diff --git a/examples/data/large_tokamak_1_MFILE.DAT b/examples/data/large_tokamak_1_MFILE.DAT new file mode 100644 index 0000000000..64ce2913b4 --- /dev/null +++ b/examples/data/large_tokamak_1_MFILE.DAT @@ -0,0 +1,1801 @@ + # PROCESS # + # Power Reactor Optimisation Code # + # PROCESS # + # Power Reactor Optimisation Code # + PROCESS_version_number__________________________________________________ (procver)_____________________ "3.0.2 R" + Date_of_run_____________________________________________________________ (date)________________________ "08/02/2024" + Time_of_run_____________________________________________________________ (time)________________________ "10:56" + User____________________________________________________________________ (username)____________________ "timothyn" + PROCESS_run_title_______________________________________________________ (runtitle)____________________ "Generic large tokamak + PROCESS_tag_number______________________________________________________ (tagno)_______________________ "v3.0.2-7-gec9530fb1" + PROCESS_git_branch_name_________________________________________________ (branch_name)_________________ "3033-inequality-constraint-for-injected-power-coded-with-the-wrong-signbug" + PROCESS_last_commit_message_____________________________________________ (commsg)______________________ "Merge branch |main| into 3033-inequality-constraint-for-injected-power-coded-with-the-wrong-signbug + Input_filename__________________________________________________________ (fileprefix)__________________ "/private/var/folders/2c/5k4t0wm94jxdmnqwdvn_h59r0000gq/T/pytest-of-timothynunn/pytest-56/test_scenario_large_tokamak_0/IN.DAT " + # Numerics # + VMCON_error_flag________________________________________________________ (ifail)_______________________ 1 + # PROCESS found a feasible solution # + Number_of_iteration_variables___________________________________________ (nvar)________________________ 45 + Number_of_constraints_(total)___________________________________________ (neqns+nineqns)_______________ 26 + Optimisation_switch_____________________________________________________ (ioptimz)_____________________ 1 + Figure_of_merit_switch__________________________________________________ (minmax)______________________ 1 + Objective_function_name_________________________________________________ (objf_name)___________________ "major radius" + Square_root_of_the_sum_of_squares_of_the_constraint_residuals___________ (sqsumsq)_____________________ 1.8713E-04 OP + VMCON_convergence_parameter_____________________________________________ (convergence_parameter)_______ 0.0000E+00 OP + Normalised_objective_function___________________________________________ (norm_objf)___________________ 1.6000E+00 OP + Number_of_VMCON_iterations______________________________________________ (nviter)______________________ 0 OP + beta____________________________________________________________________ (itvar001)____________________ 3.3648E-02 + beta_(final_value/initial_value)________________________________________ (xcm001)______________________ 1.1216E+00 + beta_(range_normalised)_________________________________________________ (nitvar001)___________________ 3.2681E-02 + dene____________________________________________________________________ (itvar002)____________________ 8.0667E+19 + dene_(final_value/initial_value)________________________________________ (xcm002)______________________ 1.0756E+00 + dene_(range_normalised)_________________________________________________ (nitvar002)___________________ 7.1381E-02 + fwalld__________________________________________________________________ (itvar003)____________________ 5.0758E-01 + fwalld_(final_value/initial_value)______________________________________ (xcm003)______________________ 5.0758E-01 + fwalld_(range_normalised)_______________________________________________ (nitvar003)___________________ 5.0709E-01 + ffuspow_________________________________________________________________ (itvar004)____________________ 5.4006E-01 + ffuspow_(final_value/initial_value)_____________________________________ (xcm004)______________________ 5.4006E-01 + ffuspow_(range_normalised)______________________________________________ (nitvar004)___________________ 5.3960E-01 + ftburn__________________________________________________________________ (itvar005)____________________ 9.9940E-01 + ftburn_(final_value/initial_value)______________________________________ (xcm005)______________________ 9.9940E-01 + ftburn_(range_normalised)_______________________________________________ (nitvar005)___________________ 9.9940E-01 + flhthresh_______________________________________________________________ (itvar006)____________________ 1.6735E+00 + flhthresh_(final_value/initial_value)___________________________________ (xcm006)______________________ 1.6735E+00 + flhthresh_(range_normalised)____________________________________________ (nitvar006)___________________ 7.4836E-02 + fpinj___________________________________________________________________ (itvar007)____________________ 4.0071E-01 + fpinj_(final_value/initial_value)_______________________________________ (xcm007)______________________ 4.0071E-01 + fpinj_(range_normalised)________________________________________________ (nitvar007)___________________ 4.0011E-01 + fpnetel_________________________________________________________________ (itvar008)____________________ 1.0000E+00 + fpnetel_(final_value/initial_value)_____________________________________ (xcm008)______________________ 1.0000E+00 + fpnetel_(range_normalised)______________________________________________ (nitvar008)___________________ 1.0000E+00 + fbetatry________________________________________________________________ (itvar009)____________________ 5.0870E-01 + fbetatry_(final_value/initial_value)____________________________________ (xcm009)______________________ 1.0174E+00 + fbetatry_(range_normalised)_____________________________________________ (nitvar009)___________________ 5.0821E-01 + fpeakb__________________________________________________________________ (itvar010)____________________ 8.6988E-01 + fpeakb_(final_value/initial_value)______________________________________ (xcm010)______________________ 8.6988E-01 + fpeakb_(range_normalised)_______________________________________________ (nitvar010)___________________ 8.6975E-01 + coheof__________________________________________________________________ (itvar011)____________________ 2.0264E+07 + coheof_(final_value/initial_value)______________________________________ (xcm011)______________________ 1.3510E+00 + coheof_(range_normalised)_______________________________________________ (nitvar011)___________________ 2.0185E-01 + fjohc___________________________________________________________________ (itvar012)____________________ 5.5541E-01 + fjohc_(final_value/initial_value)_______________________________________ (xcm012)______________________ 9.2569E-01 + fjohc_(range_normalised)________________________________________________ (nitvar012)___________________ 5.5092E-01 + fjohc0__________________________________________________________________ (itvar013)____________________ 5.4190E-01 + fjohc0_(final_value/initial_value)______________________________________ (xcm013)______________________ 9.0316E-01 + fjohc0_(range_normalised)_______________________________________________ (nitvar013)___________________ 5.4144E-01 + fcohbop_________________________________________________________________ (itvar014)____________________ 9.4380E-01 + fcohbop_(final_value/initial_value)_____________________________________ (xcm014)______________________ 1.0487E+00 + fcohbop_(range_normalised)______________________________________________ (nitvar014)___________________ 9.4374E-01 + fiooic__________________________________________________________________ (itvar015)____________________ 7.1737E-01 + fiooic_(final_value/initial_value)______________________________________ (xcm015)______________________ 1.1036E+00 + fiooic_(range_normalised)_______________________________________________ (nitvar015)___________________ 7.1709E-01 + fvdump__________________________________________________________________ (itvar016)____________________ 9.5837E-01 + fvdump_(final_value/initial_value)______________________________________ (xcm016)______________________ 9.5837E-01 + fvdump_(range_normalised)_______________________________________________ (nitvar016)___________________ 9.5833E-01 + vdalw___________________________________________________________________ (itvar017)____________________ 9.5837E+00 + vdalw_(final_value/initial_value)_______________________________________ (xcm017)______________________ 9.5837E-01 + vdalw_(range_normalised)________________________________________________ (nitvar017)___________________ 9.5837E-01 + fjprot__________________________________________________________________ (itvar018)____________________ 9.9639E-01 + fjprot_(final_value/initial_value)______________________________________ (xcm018)______________________ 9.9639E-01 + fjprot_(range_normalised)_______________________________________________ (nitvar018)___________________ 9.9639E-01 + ftmargtf________________________________________________________________ (itvar019)____________________ 9.9673E-01 + ftmargtf_(final_value/initial_value)____________________________________ (xcm019)______________________ 9.9673E-01 + ftmargtf_(range_normalised)_____________________________________________ (nitvar019)___________________ 9.9672E-01 + ftmargoh________________________________________________________________ (itvar020)____________________ 9.9653E-01 + ftmargoh_(final_value/initial_value)____________________________________ (xcm020)______________________ 9.9653E-01 + ftmargoh_(range_normalised)_____________________________________________ (nitvar020)___________________ 9.9652E-01 + ftaulimit_______________________________________________________________ (itvar021)____________________ 7.1930E-01 + ftaulimit_(final_value/initial_value)___________________________________ (xcm021)______________________ 7.1930E-01 + ftaulimit_(range_normalised)____________________________________________ (nitvar021)___________________ 7.1902E-01 + fmaxvvstress____________________________________________________________ (itvar022)____________________ 4.2966E-01 + fmaxvvstress_(final_value/initial_value)________________________________ (xcm022)______________________ 4.2966E-01 + fmaxvvstress_(range_normalised)_________________________________________ (nitvar022)___________________ 4.2909E-01 + foh_stress______________________________________________________________ (itvar023)____________________ 9.0092E-01 + foh_stress_(final_value/initial_value)__________________________________ (xcm023)______________________ 9.0092E-01 + foh_stress_(range_normalised)___________________________________________ (nitvar023)___________________ 9.0082E-01 + fne0____________________________________________________________________ (itvar024)____________________ 5.9638E-01 + fne0_(final_value/initial_value)________________________________________ (xcm024)______________________ 5.9638E-01 + fne0_(range_normalised)_________________________________________________ (nitvar024)___________________ 5.9598E-01 + fpsepbqar_______________________________________________________________ (itvar025)____________________ 1.0000E+00 + fpsepbqar_(final_value/initial_value)___________________________________ (xcm025)______________________ 1.0000E+00 + fpsepbqar_(range_normalised)____________________________________________ (nitvar025)___________________ 1.0000E+00 + fstrcase________________________________________________________________ (itvar026)____________________ 9.9670E-01 + fstrcase_(final_value/initial_value)____________________________________ (xcm026)______________________ 9.9670E-01 + fstrcase_(range_normalised)_____________________________________________ (nitvar026)___________________ 9.9670E-01 + fstrcond________________________________________________________________ (itvar027)____________________ 8.5185E-01 + fstrcond_(final_value/initial_value)____________________________________ (xcm027)______________________ 8.5185E-01 + fstrcond_(range_normalised)_____________________________________________ (nitvar027)___________________ 8.5171E-01 + bt______________________________________________________________________ (itvar028)____________________ 5.2940E+00 + bt_(final_value/initial_value)__________________________________________ (xcm028)______________________ 9.2877E-01 + bt_(range_normalised)___________________________________________________ (nitvar028)___________________ 1.7619E-01 + rmajor__________________________________________________________________ (itvar029)____________________ 8.0000E+00 + rmajor_(final_value/initial_value)______________________________________ (xcm029)______________________ 1.0000E+00 + rmajor_(range_normalised)_______________________________________________ (nitvar029)___________________ 0.0000E+00 + te______________________________________________________________________ (itvar030)____________________ 1.2489E+01 + te_(final_value/initial_value)__________________________________________ (xcm030)______________________ 1.0407E+00 + te_(range_normalised)___________________________________________________ (nitvar030)___________________ 7.3903E-02 + hfact___________________________________________________________________ (itvar031)____________________ 1.1886E+00 + hfact_(final_value/initial_value)_______________________________________ (xcm031)______________________ 1.0805E+00 + hfact_(range_normalised)________________________________________________ (nitvar031)___________________ 9.8961E-01 + tfcth___________________________________________________________________ (itvar032)____________________ 1.2000E+00 + tfcth_(final_value/initial_value)_______________________________________ (xcm032)______________________ 1.0000E+00 + tfcth_(range_normalised)________________________________________________ (nitvar032)___________________ 1.1628E-01 + ohcth___________________________________________________________________ (itvar033)____________________ 5.7587E-01 + ohcth_(final_value/initial_value)_______________________________________ (xcm033)______________________ 1.1517E+00 + ohcth_(range_normalised)________________________________________________ (nitvar033)___________________ 2.8441E-02 + q_______________________________________________________________________ (itvar034)____________________ 3.5961E+00 + q_(final_value/initial_value)___________________________________________ (xcm034)______________________ 1.0275E+00 + q_(range_normalised)____________________________________________________ (nitvar034)___________________ 1.2684E-02 + bore____________________________________________________________________ (itvar035)____________________ 1.9854E+00 + bore_(final_value/initial_value)________________________________________ (xcm035)______________________ 9.9271E-01 + bore_(range_normalised)_________________________________________________ (nitvar035)___________________ 1.9045E-01 + fvsbrnni________________________________________________________________ (itvar036)____________________ 4.3358E-01 + fvsbrnni_(final_value/initial_value)____________________________________ (xcm036)______________________ 1.0839E+00 + fvsbrnni_(range_normalised)_____________________________________________ (nitvar036)___________________ 4.3301E-01 + tdmptf__________________________________________________________________ (itvar037)____________________ 1.8429E+01 + tdmptf_(final_value/initial_value)______________________________________ (xcm037)______________________ 7.3716E-01 + tdmptf_(range_normalised)_______________________________________________ (nitvar037)___________________ 1.8347E-01 + thkcas__________________________________________________________________ (itvar038)____________________ 2.8216E-01 + thkcas_(final_value/initial_value)______________________________________ (xcm038)______________________ 5.6431E-01 + thkcas_(range_normalised)_______________________________________________ (nitvar038)___________________ 2.4437E-01 + thwcndut________________________________________________________________ (itvar039)____________________ 8.0099E-03 + thwcndut_(final_value/initial_value)____________________________________ (xcm039)______________________ 1.0012E+00 + thwcndut_(range_normalised)_____________________________________________ (nitvar039)___________________ 1.0716E-04 + fcutfsu_________________________________________________________________ (itvar040)____________________ 8.4212E-01 + fcutfsu_(final_value/initial_value)_____________________________________ (xcm040)______________________ 1.0526E+00 + fcutfsu_(range_normalised)______________________________________________ (nitvar040)___________________ 7.7755E-01 + cpttf___________________________________________________________________ (itvar041)____________________ 8.9795E+04 + cpttf_(final_value/initial_value)_______________________________________ (xcm041)______________________ 1.3815E+00 + cpttf_(range_normalised)________________________________________________ (nitvar041)___________________ 9.9182E-01 + ralpne__________________________________________________________________ (itvar042)____________________ 8.3954E-02 + ralpne_(final_value/initial_value)______________________________________ (xcm042)______________________ 8.3954E-01 + ralpne_(range_normalised)_______________________________________________ (nitvar042)___________________ 6.7908E-01 + oh_steel_frac___________________________________________________________ (itvar043)____________________ 5.1868E-01 + oh_steel_frac_(final_value/initial_value)_______________________________ (xcm043)______________________ 6.4835E-01 + oh_steel_frac_(range_normalised)________________________________________ (nitvar043)___________________ 5.4550E-01 + fimp(13)________________________________________________________________ (itvar044)____________________ 5.7149E-04 + fimp(13)_(final_value/initial_value)____________________________________ (xcm044)______________________ 1.5039E+00 + fimp(13)_(range_normalised)_____________________________________________ (nitvar044)___________________ 5.7148E-02 + dr_tf_wp________________________________________________________________ (itvar045)____________________ 5.0416E-01 + dr_tf_wp_(final_value/initial_value)____________________________________ (xcm045)______________________ 1.0083E+00 + dr_tf_wp_(range_normalised)_____________________________________________ (nitvar045)___________________ 6.5100E-02 + Beta_consistency__________________normalised_residue____________________ (normres001)__________________ 6.5770E-07 + Global_power_balance_consistency__normalised_residue____________________ (normres002)__________________ 1.2292E-07 + Radial_build_consistency__________normalised_residue____________________ (normres003)__________________ -7.3085E-11 + Density_upper_limit_______________normalised_residue____________________ (normres004)__________________ 1.6272E-08 + Neutron_wall_load_upper_limit_____normalised_residue____________________ (normres005)__________________ 1.4241E-07 + Fusion_power_upper_limit__________normalised_residue____________________ (normres006)__________________ 2.6565E-07 + Burn_time_lower_limit_____________normalised_residue____________________ (normres007)__________________ -1.2011E-04 + L-H_power_threshold_limit_________normalised_residue____________________ (normres008)__________________ -3.0891E-07 + Injection_power_upper_limit_______normalised_residue____________________ (normres009)__________________ 2.4418E-07 + Net_electric_power_lower_limit____normalised_residue____________________ (normres010)__________________ 1.5045E-05 + Beta_upper_limit__________________normalised_residue____________________ (normres011)__________________ 2.4702E-07 + Peak_toroidal_field_upper_limit___normalised_residue____________________ (normres012)__________________ 2.5809E-09 + CS_coil_EOF_current_density_limit_normalised_residue____________________ (normres013)__________________ -8.4245E-08 + CS_coil_BOP_current_density_limit_normalised_residue____________________ (normres014)__________________ 1.9393E-09 + I_op_/_I_critical_(TF_coil)_______normalised_residue____________________ (normres015)__________________ -3.8375E-07 + Dump_voltage_upper_limit__________normalised_residue____________________ (normres016)__________________ -1.5214E-04 + J_winding_pack/J_protection_limit_normalised_residue____________________ (normres017)__________________ -2.9894E-07 + TF_coil_temp._margin_lower_limit__normalised_residue____________________ (normres018)__________________ -1.0631E-06 + CS_temperature_margin_lower_limit_normalised_residue____________________ (normres019)__________________ 8.0251E-08 + taup/taueff_______________________normalised_residue____________________ (normres020)__________________ -1.8772E-08 + Dump_time_set_by_VV_stress________normalised_residue____________________ (normres021)__________________ -1.0026E-07 + CS_Tresca_yield_criterion_________normalised_residue____________________ (normres022)__________________ -1.6044E-07 + ne0_>_neped_______________________normalised_residue____________________ (normres023)__________________ -1.9637E-08 + Upper_Lim._on_Psep_*_Bt_/_q_A_R___normalised_residue____________________ (normres024)__________________ 4.9789E-07 + TF_coil_case_stress_upper_limit___normalised_residue____________________ (normres025)__________________ -4.6757E-07 + TF_coil_conduit_stress_upper_lim__normalised_residue____________________ (normres026)__________________ -4.1375E-07 + # Final Feasible Point # + # Power Reactor Costs (1990 US$) # + First_wall_/_blanket_life_(years)_______________________________________ (fwbllife)____________________ 6.1566E+00 + Divertor_life_(years)___________________________________________________ (divlife.)____________________ 3.9769E+00 + Cost_of_electricity_(m$/kWh)____________________________________________ (coe)_________________________ 5.1257E+02 + # Detailed Costings (1990 US$) # + Acc.22_multiplier_for_Nth_of_a_kind_____________________________________ (fkind)_______________________ 1.0000E+00 + Level_of_Safety_Assurance_______________________________________________ (lsa)_________________________ 4 + # Structures and Site Facilities # + Site_improvements,_facilities,_land_(M$)________________________________ (c211)________________________ 3.5200E+01 + Reactor_building_cost_(M$)______________________________________________ (c212)________________________ 4.5238E+02 + Turbine_building_cost_(M$)______________________________________________ (c213)________________________ 3.8000E+01 + Reactor_maintenance_building_cost_(M$)__________________________________ (c2141)_______________________ 1.0307E+02 + Warm_shop_cost_(M$)_____________________________________________________ (c2142)_______________________ 5.7641E+01 + Tritium_building_cost_(M$)______________________________________________ (c215)________________________ 1.4800E+01 + Electrical_equipment_building_cost_(M$)_________________________________ (c216)________________________ 1.9736E+01 + Additional_buildings_cost_(M$)__________________________________________ (c2171)_______________________ 1.8000E+01 + Control_room_buildings_cost_(M$)________________________________________ (c2172)_______________________ 2.1000E+01 + Shop_and_warehouses_cost_(M$)___________________________________________ (c2173)_______________________ 1.1500E+01 + Cryogenic_building_cost_(M$)____________________________________________ (c2174)_______________________ 6.8891E+00 + Total_account_21_cost_(M$)______________________________________________ (c21)_________________________ 7.7822E+02 + # Reactor Systems # + First_wall_cost_(M$)____________________________________________________ (c2211)_______________________ 1.9130E+02 + Blanket_beryllium_cost_(M$)_____________________________________________ (c22121)______________________ 2.6109E+02 + Blanket_breeder_material_cost_(M$)______________________________________ (c22122)______________________ 6.3985E+02 + Blanket_stainless_steel_cost_(M$)_______________________________________ (c22123)______________________ 8.0726E+01 + Blanket_vanadium_cost_(M$)______________________________________________ (c22124)______________________ 0.0000E+00 + Blanket_total_cost_(M$)_________________________________________________ (c2212)_______________________ 9.8166E+02 + Bulk_shield_cost_(M$)___________________________________________________ (c22131)______________________ 7.8394E+01 + Penetration_shielding_cost_(M$)_________________________________________ (c22132)______________________ 7.8394E+01 + Total_shield_cost_(M$)__________________________________________________ (c2213)_______________________ 1.5679E+02 + Total_support_structure_cost_(M$)_______________________________________ (c2214)_______________________ 4.0933E+01 + Divertor_cost_(M$)______________________________________________________ (c2215)_______________________ 4.1660E+01 + Total_account_221_cost_(M$)_____________________________________________ (c221)________________________ 1.4123E+03 + # Magnets # + TF_coil_conductor_cost_(M$)_____________________________________________ (c22211)______________________ 1.3230E+02 + TF_coil_winding_cost_(M$)_______________________________________________ (c22212)______________________ 5.4263E+01 + TF_coil_case_cost_(M$)__________________________________________________ (c22213)______________________ 4.4365E+02 + TF_intercoil_structure_cost_(M$)________________________________________ (c22214)______________________ 1.5066E+02 + TF_coil_gravity_support_structure_(M$)__________________________________ (c22215)______________________ 4.4659E+01 + TF_magnet_assemblies_cost_(M$)__________________________________________ (c2221)_______________________ 8.2552E+02 + PF_coil_conductor_cost_(M$)_____________________________________________ (c22221)______________________ 4.6409E+02 + PF_coil_winding_cost_(M$)_______________________________________________ (c22222)______________________ 7.6765E+01 + PF_coil_case_cost_(M$)__________________________________________________ (c22223)______________________ 9.4861E+01 + PF_coil_support_structure_cost_(M$)_____________________________________ (c22224)______________________ 8.0235E+00 + PF_magnet_assemblies_cost_(M$)__________________________________________ (c2222)_______________________ 6.4374E+02 + Vacuum_vessel_assembly_cost_(M$)________________________________________ (c2223)_______________________ 2.5404E+02 + Total_account_222_cost_(M$)_____________________________________________ (c222)________________________ 1.7233E+03 + # Power Injection # + ECH_system_cost_(M$)____________________________________________________ (c2231)_______________________ 2.4043E+02 + Lower_hybrid_system_cost_(M$)___________________________________________ (c2232)_______________________ 0.0000E+00 + Neutral_beam_system_cost_(M$)___________________________________________ (c2233)_______________________ 0.0000E+00 + Total_account_223_cost_(M$)_____________________________________________ (c223)________________________ 2.4043E+02 + # Vacuum Systems # + High_vacuum_pumps_cost_(M$)_____________________________________________ (c2241)_______________________ 1.2480E+01 + Backing_pumps_cost_(M$)_________________________________________________ (c2242)_______________________ 4.6800E+00 + Vacuum_duct_cost_(M$)___________________________________________________ (c2243)_______________________ 2.5280E+00 + Valves_cost_(M$)________________________________________________________ (c2244)_______________________ 5.7410E+00 + Duct_shielding_cost_(M$)________________________________________________ (c2245)_______________________ 0.0000E+00 + Instrumentation_cost_(M$)_______________________________________________ (c2246)_______________________ 1.3000E+00 + Total_account_224_cost_(M$)_____________________________________________ (c224)________________________ 2.6729E+01 + # Power Conditioning # + TF_coil_power_supplies_cost_(M$)________________________________________ (c22511)______________________ 4.0144E+00 + TF_coil_breakers_cost_(M$)______________________________________________ (c22512)______________________ 3.4127E+01 + TF_coil_dump_resistors_cost_(M$)________________________________________ (c22513)______________________ 2.1322E+01 + TF_coil_instrumentation_and_control_(M$)________________________________ (c22514)______________________ 4.8000E+00 + TF_coil_bussing_cost_(M$)_______________________________________________ (c22515)______________________ 3.5267E+01 + Total,_TF_coil_power_costs_(M$)_________________________________________ (c2251)_______________________ 9.9531E+01 + PF_coil_power_supplies_cost_(M$)________________________________________ (c22521)______________________ 2.9591E+00 + PF_coil_instrumentation_and_control_(M$)________________________________ (c22522)______________________ 3.6000E+00 + PF_coil_bussing_cost_(M$)_______________________________________________ (c22523)______________________ 1.1995E+01 + PF_coil_burn_power_supplies_cost_(M$)___________________________________ (c22524)______________________ 1.2679E+00 + PF_coil_breakers_cost_(M$)______________________________________________ (c22525)______________________ 1.4709E+01 + PF_coil_dump_resistors_cost_(M$)________________________________________ (c22526)______________________ 4.3206E+00 + PF_coil_ac_breakers_cost_(M$)___________________________________________ (c22527)______________________ 9.0000E-01 + Total,_PF_coil_power_costs_(M$)_________________________________________ (c2252)_______________________ 3.9752E+01 + Total,_energy_storage_cost_(M$)_________________________________________ (c2253)_______________________ 1.6864E+01 + Total_account_225_cost_(M$)_____________________________________________ (c225)________________________ 1.5615E+02 + # Heat Transport System # + Pumps_and_piping_system_cost_(M$)_______________________________________ (cpp)_________________________ 3.6795E+01 + Primary_heat_exchanger_cost_(M$)________________________________________ (chx)_________________________ 7.1692E+01 + Total,_reactor_cooling_system_cost_(M$)_________________________________ (c2261)_______________________ 1.0849E+02 + Pumps,_piping_cost_(M$)_________________________________________________ (cppa)________________________ 2.8417E+01 + Total,_auxiliary_cooling_system_cost_(M$)_______________________________ (c2262)_______________________ 2.8417E+01 + Total,_cryogenic_system_cost_(M$)_______________________________________ (c2263)_______________________ 1.7039E+02 + Total_account_226_cost_(M$)_____________________________________________ (c226)________________________ 3.0729E+02 + # Fuel Handling System # + Fuelling_system_cost_(M$)_______________________________________________ (c2271)_______________________ 2.2300E+01 + Fuel_processing_and_purification_cost_(M$)______________________________ (c2272)_______________________ 1.0229E+02 + Atmospheric_recovery_systems_cost_(M$)__________________________________ (c2273)_______________________ 5.8088E+01 + Nuclear_building_ventilation_cost_(M$)__________________________________ (c2274)_______________________ 6.9201E+01 + Total_account_227_cost_(M$)_____________________________________________ (c227)________________________ 2.5188E+02 + # Instrumentation and Control # + Instrumentation_and_control_cost_(M$)___________________________________ (c228)________________________ 1.5000E+02 + # Maintenance Equipment # + Maintenance_equipment_cost_(M$)_________________________________________ (c229)________________________ 1.2500E+02 + # Total Account 22 Cost # + Total_account_22_cost_(M$)______________________________________________ (c22)_________________________ 4.3931E+03 + # Turbine Plant Equipment # + Turbine_plant_equipment_cost_(M$)_______________________________________ (c23)_________________________ 1.7613E+02 + # Electric Plant Equipment # + Switchyard_equipment_cost_(M$)__________________________________________ (c241)________________________ 1.8400E+01 + Transformers_cost_(M$)__________________________________________________ (c242)________________________ 8.0330E+00 + Low_voltage_equipment_cost_(M$)_________________________________________ (c243)________________________ 6.4513E+00 + Diesel_backup_equipment_cost_(M$)_______________________________________ (c244)________________________ 6.8000E+00 + Auxiliary_facilities_cost_(M$)__________________________________________ (c245)________________________ 1.5000E+00 + Total_account_24_cost_(M$)______________________________________________ (c24)_________________________ 4.1184E+01 + # Miscellaneous Plant Equipment # + Miscellaneous_plant_equipment_cost_(M$)_________________________________ (c25)_________________________ 2.5000E+01 + # Heat Rejection System # + Heat_rejection_system_cost_(M$)_________________________________________ (c26)_________________________ 4.9877E+01 + # Plant Direct Cost # + Plant_direct_cost_(M$)__________________________________________________ (cdirt)_______________________ 5.4635E+03 + # Reactor Core Cost # + Reactor_core_cost_(M$)__________________________________________________ (crctcore)____________________ 3.3761E+03 + # Indirect Cost # + Indirect_cost_(M$)______________________________________________________ (c9)__________________________ 1.8221E+03 + # Total Contingency # + Total_contingency_(M$)__________________________________________________ (ccont)_______________________ 1.4207E+03 + # Constructed Cost # + Constructed_cost_(M$)___________________________________________________ (concost)_____________________ 8.7063E+03 + # Interest during Construction # + Interest_during_construction_(M$)_______________________________________ (moneyint)____________________ 1.4365E+03 + # Total Capital Investment # + Total_capital_investment_(M$)___________________________________________ (capcost)_____________________ 1.0143E+04 + # Plant Availability # + Allowable_blanket_neutron_fluence_(MW-yr/m2)____________________________ (abktflnc)____________________ 5.0000E+00 + Allowable_divertor_heat_fluence_(MW-yr/m2)______________________________ (adivflnc)____________________ 7.0000E+00 + First_wall_/_blanket_lifetime_(years)___________________________________ (bktlife)_____________________ 6.1566E+00 OP + Divertor_lifetime_(years)_______________________________________________ (divlife)_____________________ 3.9769E+00 OP + Heating/CD_system_lifetime_(years)______________________________________ (cdrlife)_____________________ 6.1566E+00 OP + Total_plant_lifetime_(years)____________________________________________ (tlife)_______________________ 3.0000E+01 + Total_plant_availability_fraction_______________________________________ (cfactr)______________________ 8.0000E-01 + Number_of_fusion_cycles_to_reach_allowable_fw/blanket_DPA_______________ (bktcycles)___________________ 1.5787E+04 + # Plasma # + Tokamak_aspect_ratio_=_Conventional,_itart_=_0__________________________ (itart)_______________________ 0.0000E+00 + Major_radius_(m)________________________________________________________ (rmajor)______________________ 8.0000E+00 ITV + Minor_radius_(m)________________________________________________________ (rminor)______________________ 2.6667E+00 + Aspect_ratio____________________________________________________________ (aspect)______________________ 3.0000E+00 + Elongation,_X-point_(input_value_used)__________________________________ (kappa)_______________________ 1.8500E+00 + Elongation,_95%_surface_(calculated_from_kappa)_________________________ (kappa95)_____________________ 1.6518E+00 + Elongation,_area_ratio_calc.____________________________________________ (kappaa)______________________ 1.7188E+00 + Triangularity,_X-point_(input_value_used)_______________________________ (triang)______________________ 5.0000E-01 + Triangularity,_95%_surface_(calculated_from_triang)_____________________ (triang95)____________________ 3.3333E-01 + Plasma_poloidal_perimeter_(m)___________________________________________ (pperim)______________________ 2.4081E+01 + Plasma_cross-sectional_area_(m2)________________________________________ (xarea)_______________________ 3.8398E+01 + Plasma_surface_area_(m2)________________________________________________ (sarea)_______________________ 1.1738E+03 OP + Plasma_volume_(m3)______________________________________________________ (vol)_________________________ 1.8882E+03 OP + Plasma_current_scaling_law_used_________________________________________ (icurr)_______________________ 4 + Plasma_current_(MA)_____________________________________________________ (plascur/1D6)_________________ 1.6631E+01 + Current_density_profile_factor__________________________________________ (alphaj)______________________ 1.9805E+00 + Plasma_internal_inductance,_li__________________________________________ (rli)_________________________ 1.2275E+00 + Vertical_field_at_plasma_(T)____________________________________________ (bvert)_______________________ -7.4373E-01 + Vacuum_toroidal_field_at_R_(T)__________________________________________ (bt)__________________________ 5.2940E+00 ITV + Average_poloidal_field_(T)______________________________________________ (bp)__________________________ 8.6787E-01 + Total_field_(sqrt(bp^2_+_bt^2))_(T)_____________________________________ (btot)________________________ 5.3647E+00 + Safety_factor_on_axis___________________________________________________ (q0)__________________________ 1.0000E+00 + Safety_factor_at_95%_flux_surface_______________________________________ (q95)_________________________ 3.5961E+00 ITV + Cylindrical_safety_factor_(qcyl)________________________________________ (qstar)_______________________ 2.9805E+00 + Total_plasma_beta_______________________________________________________ (beta)________________________ 3.3648E-02 ITV + Total_poloidal_beta_____________________________________________________ (betap)_______________________ 1.2857E+00 OP + Total_toroidal_beta_____________________________________________________ ______________________________ 3.4553E-02 OP + Fast_alpha_beta_________________________________________________________ (betaft)______________________ 4.2236E-03 OP + Beam_ion_beta___________________________________________________________ (betanb)______________________ 0.0000E+00 OP + (Fast_alpha_+_beam_physics_variables.beta)/(thermal_physics_variables.be (gammaft)_____________________ 1.4354E-01 OP + Thermal_beta____________________________________________________________ ______________________________ 2.9425E-02 OP + Thermal_poloidal_beta___________________________________________________ ______________________________ 1.1243E+00 OP + Thermal_toroidal_physics_variables.beta_(=_beta-exp)____________________ ______________________________ 3.0215E-02 OP + 2nd_stability_physics_variables.beta_:_beta_p_/_(R/a)___________________ (eps*betap)___________________ 4.2857E-01 + 2nd_stability_physics_variables.beta_upper_limit________________________ (epbetmax)____________________ 1.3800E+00 + Beta_g_coefficient______________________________________________________ (dnbeta)______________________ 4.9099E+00 + Normalised_thermal_beta_________________________________________________ ______________________________ 2.4977E+00 + Normalised_total_beta___________________________________________________ ______________________________ 2.8562E+00 + Normalised_toroidal_beta________________________________________________ (normalised_toroidal_beta)____ 2.9330E+00 + Limit_on_thermal_beta___________________________________________________ (betalim)_____________________ 5.7842E-02 + Plasma_thermal_energy_(J)_______________________________________________ ______________________________ 9.5431E+08 OP + Total_plasma_internal_energy_(J)________________________________________ (total_plasma_internal_energy) 1.0913E+09 OP + Electron_temperature_(keV)______________________________________________ (te)__________________________ 1.2489E+01 ITV + Electron_temperature_on_axis_(keV)______________________________________ (te0)_________________________ 2.5758E+01 + Ion_temperature_(keV)___________________________________________________ (ti)__________________________ 1.2489E+01 + Ion_temperature_on_axis_(keV)___________________________________________ (ti0)_________________________ 2.5758E+01 + Electron_temp.,_density_weighted_(keV)__________________________________ (ten)_________________________ 1.3805E+01 + Electron_density_(/m3)__________________________________________________ (dene)________________________ 8.0667E+19 ITV + Electron_density_on_axis_(/m3)__________________________________________ (ne0)_________________________ 1.0610E+20 OP + Line-averaged_electron_density_(/m3)____________________________________ (dnla)________________________ 8.9334E+19 OP + Line-averaged_electron_density_/_Greenwald_density______________________ (dnla_gw)_____________________ 1.2000E+00 OP + Ion_density_(/m3)_______________________________________________________ (dnitot)______________________ 7.1669E+19 OP + Fuel_density_(/m3)______________________________________________________ (deni)________________________ 6.4831E+19 OP + Total_impurity_density_with_Z_>_2_(no_He)_(/m3)_________________________ (dnz)_________________________ 4.6503E+16 OP + Helium_ion_density_(thermalised_ions_only)_(/m3)________________________ (dnalp)_______________________ 6.7723E+18 OP + Proton_density_(/m3)____________________________________________________ (dnprot)______________________ 1.8963E+16 OP + Hot_beam_density_(/m3)__________________________________________________ (dnbeam)______________________ 0.0000E+00 OP + Density_limit_from_scaling_(/m3)________________________________________ (dnelimt)_____________________ 7.4445E+19 OP + Density_limit_(enforced)_(/m3)__________________________________________ (boundu(9)*dnelimt)___________ 7.4445E+19 OP + Helium_ion_density_(thermalised_ions_only)_/_electron_density___________ (ralpne)______________________ 8.3954E-02 ITV + H__concentration________________________________________________________ (fimp(01))____________________ 8.0392E-01 OP + He_concentration________________________________________________________ (fimp(02))____________________ 8.3954E-02 + Be_concentration________________________________________________________ (fimp(03))____________________ 0.0000E+00 + C__concentration________________________________________________________ (fimp(04))____________________ 0.0000E+00 + N__concentration________________________________________________________ (fimp(05))____________________ 0.0000E+00 + O__concentration________________________________________________________ (fimp(06))____________________ 0.0000E+00 + Ne_concentration________________________________________________________ (fimp(07))____________________ 0.0000E+00 + Si_concentration________________________________________________________ (fimp(08))____________________ 0.0000E+00 + Ar_concentration________________________________________________________ (fimp(09))____________________ 0.0000E+00 + Fe_concentration________________________________________________________ (fimp(10))____________________ 0.0000E+00 + Ni_concentration________________________________________________________ (fimp(11))____________________ 0.0000E+00 + Kr_concentration________________________________________________________ (fimp(12))____________________ 0.0000E+00 + Xe_concentration________________________________________________________ (fimp(13))____________________ 5.7149E-04 ITV + W__concentration________________________________________________________ (fimp(14))____________________ 5.0000E-06 + Average_mass_of_all_ions_(amu)__________________________________________ (aion)________________________ 2.7252E+00 OP + Effective_charge________________________________________________________ (zeff)________________________ 2.5164E+00 + Density_profile_factor__________________________________________________ (alphan)______________________ 1.0000E+00 + Plasma_profile_model____________________________________________________ (ipedestal)___________________ 1 + Density_pedestal_r/a_location___________________________________________ (rhopedn)_____________________ 9.4000E-01 + Electron_density_pedestal_height_(/m3)__________________________________ (neped)_______________________ 6.3278E+19 OP + Electron_density_at_pedestal_/_nGW______________________________________ (fgwped_out)__________________ 8.5000E-01 + Temperature_pedestal_r/a_location_______________________________________ (rhopedt)_____________________ 9.4000E-01 + Pedestal_scaling_switch_________________________________________________ (ieped)_______________________ 0 + Electron_temp._pedestal_height_(keV)____________________________________ (teped)_______________________ 5.5000E+00 + Electron_temp._at_separatrix_(keV)______________________________________ (tesep)_______________________ 1.0000E-01 + Electron_density_at_separatrix_(/m3)____________________________________ (nesep)_______________________ 3.7223E+19 + Electron_density_at_separatrix_/_nGW____________________________________ (fgwsep_out)__________________ 5.0000E-01 + Temperature_profile_index_______________________________________________ (alphat)______________________ 1.4500E+00 + Temperature_profile_index_beta__________________________________________ (tbeta)_______________________ 2.0000E+00 + Old_ASDEX_model_________________________________________________________ (dlimit(1))___________________ 5.2797E+19 OP + Borrass_ITER_model_I____________________________________________________ (dlimit(2))___________________ 1.0969E+20 OP + Borrass_ITER_model_II___________________________________________________ (dlimit(3))___________________ 4.3575E+19 OP + JET_edge_radiation_model________________________________________________ (dlimit(4))___________________ 3.0227E+21 OP + JET_simplified_model____________________________________________________ (dlimit(5))___________________ 4.3397E+20 OP + Hugill-Murakami_Mq_model________________________________________________ (dlimit(6))___________________ 6.6609E+19 OP + Greenwald_model_________________________________________________________ (dlimit(7))___________________ 7.4445E+19 OP + Deuterium_fuel_fraction_________________________________________________ (fdeut)_______________________ 5.0000E-01 + Tritium_fuel_fraction___________________________________________________ (ftrit)_______________________ 5.0000E-01 + Total_fusion_power_(MW)_________________________________________________ (powfmw)______________________ 1.6202E+03 OP + _=____D-T_fusion_power_(MW)_____________________________________________ (pdt)_________________________ 1.6182E+03 OP + __+___D-D_fusion_power_(MW)_____________________________________________ (pdd)_________________________ 1.9494E+00 OP + __+_D-He3_fusion_power_(MW)_____________________________________________ (pdhe3)_______________________ 0.0000E+00 OP + Alpha_power:_total_(MW)_________________________________________________ (palpmw)______________________ 3.2365E+02 OP + Alpha_power:_beam-plasma_(MW)___________________________________________ (palpnb)______________________ 0.0000E+00 OP + Neutron_power_(MW)______________________________________________________ (pneutmw)_____________________ 1.2953E+03 OP + Charged_particle_power_(excluding_alphas)_(MW)__________________________ (pchargemw)___________________ 1.2659E+00 OP + Total_power_deposited_in_plasma_(MW)____________________________________ (tot_power_plasma)____________ 3.8950E+02 OP + Bremsstrahlung_radiation_power_(MW)_____________________________________ (pbrempv*vol)_________________ 6.5195E+01 OP + Line_radiation_power_(MW)_______________________________________________ (plinepv*vol)_________________ 1.4609E+02 OP + Synchrotron_radiation_power_(MW)________________________________________ (psyncpv*vol)_________________ 1.5187E+01 OP + Synchrotron_wall_reflectivity_factor____________________________________ (ssync)_______________________ 6.0000E-01 + Normalised_minor_radius_defining_'core'_________________________________ (coreradius)__________________ 7.5000E-01 + Fraction_of_core_radiation_subtracted_from_P_L__________________________ (coreradiationfraction)_______ 6.0000E-01 + Radiation_power_from_inner_zone_(MW)____________________________________ (pinnerzoneradmw)_____________ 9.1650E+01 OP + Radiation_power_from_outer_zone_(MW)____________________________________ (pouterzoneradmw)_____________ 1.3482E+02 OP + Total_radiation_power_from_inside_LCFS_(MW)_____________________________ (pradmw)______________________ 2.2647E+02 OP + LCFS_radiation_fraction_=_total_radiation_in_LCFS_/_total_power_deposite (rad_fraction_LCFS)___________ 5.8144E-01 OP + Nominal_mean_radiation_load_on_inside_surface_of_reactor_(MW/m2)________ (photon_wall)_________________ 1.7749E-01 OP + Peaking_factor_for_radiation_wall_load__________________________________ (peakfactrad)_________________ 3.3300E+00 IP + Maximum_permitted_radiation_wall_load_(MW/m^2)__________________________ (maxradwallload)______________ 1.0000E+00 IP + Peak_radiation_wall_load_(MW/m^2)_______________________________________ (peakradwallload)_____________ 5.9106E-01 OP + Fast_alpha_particle_power_incident_on_the_first_wall_(MW)_______________ (palpfwmw)____________________ 1.6182E+01 OP + Nominal_mean_neutron_load_on_inside_surface_of_reactor_(MW/m2)__________ (wallmw)______________________ 1.0152E+00 OP + Power_incident_on_the_divertor_targets_(MW)_____________________________ (ptarmw)______________________ 3.2606E+01 OP + Fraction_of_power_to_the_lower_divertor_________________________________ (ftar)________________________ 1.0000E+00 IP + Outboard_side_heat_flux_decay_length_(m)________________________________ (lambdaio)____________________ 1.5700E-03 OP + Fraction_of_power_on_the_inner_targets__________________________________ (fio)_________________________ 4.1000E-01 OP + Fraction_of_power_incident_on_the_lower_inner_target____________________ (fLI)_________________________ 4.1000E-01 OP + Fraction_of_power_incident_on_the_lower_outer_target____________________ (fLO)_________________________ 5.9000E-01 OP + Power_incident_on_the_lower_inner_target_(MW)___________________________ (pLImw)_______________________ 1.3368E+01 OP + Power_incident_on_the_lower_outer_target_(MW)___________________________ (pLOmw)_______________________ 1.9237E+01 OP + Ohmic_heating_power_(MW)________________________________________________ (pohmmw)______________________ 6.2284E-01 OP + Fraction_of_alpha_power_deposited_in_plasma_____________________________ (falpha)______________________ 9.5000E-01 + Fraction_of_alpha_power_to_electrons____________________________________ (falpe)_______________________ 7.1828E-01 + Fraction_of_alpha_power_to_ions_________________________________________ (falpi)_______________________ 2.8172E-01 + Ion_transport_(MW)______________________________________________________ (ptrimw)______________________ 1.4013E+02 OP + Electron_transport_(MW)_________________________________________________ (ptremw)______________________ 1.5772E+02 OP + Injection_power_to_ions_(MW)____________________________________________ (pinjimw)_____________________ 0.0000E+00 OP + Injection_power_to_electrons_(MW)_______________________________________ (pinjemw)_____________________ 8.0143E+01 OP + Ignited_plasma_switch_(0=not_ignited,_1=ignited)________________________ (ignite)______________________ 0 + Power_into_divertor_zone_via_charged_particles_(MW)_____________________ (pdivt)_______________________ 1.6303E+02 OP + Psep_/_R_ratio_(MW/m)___________________________________________________ (pdivt/rmajor)________________ 2.0378E+01 OP + Psep_Bt_/_qAR_ratio_(MWT/m)_____________________________________________ (pdivtbt/qar)_________________ 1.0000E+01 OP + ITER_1996_scaling:_nominal_(MW)_________________________________________ (pthrmw(1))___________________ 1.2978E+02 OP + ITER_1996_scaling:_upper_bound_(MW)_____________________________________ (pthrmw(2))___________________ 2.8603E+02 OP + ITER_1996_scaling:_lower_bound_(MW)_____________________________________ (pthrmw(3))___________________ 5.8098E+01 OP + ITER_1997_scaling_(1)_(MW)______________________________________________ (pthrmw(4))___________________ 2.1452E+02 OP + ITER_1997_scaling_(2)_(MW)______________________________________________ (pthrmw(5))___________________ 1.7206E+02 OP + Martin_2008_scaling:_nominal_(MW)_______________________________________ (pthrmw(6))___________________ 9.7416E+01 OP + Martin_2008_scaling:_95%_upper_bound_(MW)_______________________________ (pthrmw(7))___________________ 1.2769E+02 OP + Martin_2008_scaling:_95%_lower_bound_(MW)_______________________________ (pthrmw(8))___________________ 6.7143E+01 OP + Snipes_2000_scaling:_nominal_(MW)_______________________________________ (pthrmw(9))___________________ 6.7785E+01 OP + Snipes_2000_scaling:_upper_bound_(MW)___________________________________ (pthrmw(10))__________________ 9.9437E+01 OP + Snipes_2000_scaling:_lower_bound_(MW)___________________________________ (pthrmw(11))__________________ 4.5839E+01 OP + Snipes_2000_scaling_(closed_divertor):_nominal_(MW)_____________________ (pthrmw(12))__________________ 3.1010E+01 OP + Snipes_2000_scaling_(closed_divertor):_upper_bound_(MW)_________________ (pthrmw(13))__________________ 4.3148E+01 OP + Snipes_2000_scaling_(closed_divertor):_lower_bound_(MW)_________________ (pthrmw(14))__________________ 2.2130E+01 OP + Hubbard_2012_L-I_threshold_-_nominal_(MW)_______________________________ (pthrmw(15))__________________ 2.7549E+01 OP + Hubbard_2012_L-I_threshold_-_lower_bound_(MW)___________________________ (pthrmw(16))__________________ 1.4319E+01 OP + Hubbard_2012_L-I_threshold_-_upper_bound_(MW)___________________________ (pthrmw(17))__________________ 5.3005E+01 OP + Hubbard_2017_L-I_threshold______________________________________________ (pthrmw(18))__________________ 2.6202E+02 OP + Martin_2008_aspect_ratio_corrected_scaling:_nominal_(MW)________________ (pthrmw(19))__________________ 9.7416E+01 OP + Martin_2008_aspect_ratio_corrected_scaling:_95%_upper_bound_(MW)________ (pthrmw(20))__________________ 1.2769E+02 OP + Martin_2008_aspect_ratio_corrected_scaling:_95%_lower_bound_(MW)________ (pthrmw(21))__________________ 6.7143E+01 OP + L-H_threshold_power_(enforced)_(MW)_____________________________________ (boundl(103)*plhthresh)_______ 9.7416E+01 OP + L-H_threshold_power_(MW)________________________________________________ (plhthresh)___________________ 9.7416E+01 OP + Confinement_H_factor____________________________________________________ (hfact)_______________________ 1.1886E+00 ITV + Global_thermal_energy_confinement_time_(s)______________________________ (taueff)______________________ 3.2037E+00 + Ion_energy_confinement_time_(s)_________________________________________ (tauei)_______________________ 3.2037E+00 + Electron_energy_confinement_time_(s)____________________________________ (tauee)_______________________ 3.2037E+00 + n.tau_=_Volume-average_electron_density_x_Energy_confinement_time_(s/m3) (dntau)_______________________ 2.5843E+20 OP + Triple_product__(keV_s/m3)______________________________________________ (dntau*te)____________________ 3.2275E+21 OP + Transport_loss_power_assumed_in_scaling_law_(MW)________________________ (powerht)_____________________ 2.9785E+02 OP + Switch_for_radiation_loss_term_usage_in_power_balance___________________ (iradloss)____________________ 1 + Radiation_power_subtracted_from_plasma_power_balance_(MW)_______________ ______________________________ 9.1650E+01 OP + Alpha_particle_confinement_time_(s)_____________________________________ (taup)________________________ 2.2270E+01 + Alpha_particle/energy_confinement_time_ratio____________________________ (taup/taueff)_________________ 6.9512E+00 + Lower_limit_on_taup/taueff______________________________________________ (taulimit)____________________ 5.0000E+00 + Total_energy_confinement_time_including_radiation_loss_(s)______________ (total_energy_conf_time)______ 2.8018E+00 + Normalized_plasma_pressure_beta_as_defined_by_McDonald_et_al____________ (beta_mcdonald)_______________ 3.4553E-02 OP + Normalized_ion_Larmor_radius____________________________________________ (rho_star)____________________ 1.9603E-03 OP + Normalized_collisionality_______________________________________________ (nu_star)_____________________ 3.7266E-03 OP + Volume_measure_of_elongation____________________________________________ (kappaa_IPB)__________________ 1.6815E+00 OP + Total_volt-second_requirement_(Wb)______________________________________ (vsstt)_______________________ 5.5616E+02 OP + Inductive_volt-seconds_(Wb)_____________________________________________ (vsind)_______________________ 2.3585E+02 OP + Ejima_coefficient_______________________________________________________ (gamma)_______________________ 3.0000E-01 + Start-up_resistive_(Wb)_________________________________________________ (vsres)_______________________ 5.0159E+01 OP + Flat-top_resistive_(Wb)_________________________________________________ (vsbrn)_______________________ 2.7015E+02 OP + bootstrap_current_fraction_multiplier___________________________________ (cboot)_______________________ 1.0000E+00 + Bootstrap_fraction_(ITER_1989)__________________________________________ (bscf_iter89)_________________ 3.7098E-01 + Bootstrap_fraction_(Sauter_et_al)_______________________________________ (bscf_sauter)_________________ 4.1920E-01 + Bootstrap_fraction_(Nevins_et_al)_______________________________________ (bscf_nevins)_________________ 3.5042E-01 + Bootstrap_fraction_(Wilson)_____________________________________________ (bscf_wilson)_________________ 4.3349E-01 + Diamagnetic_fraction_(Hender)___________________________________________ (diacf_hender)________________ 1.2017E-02 + Diamagnetic_fraction_(SCENE)____________________________________________ (diacf_scene)_________________ 1.1139E-02 + Pfirsch-Schlueter_fraction_(SCENE)______________________________________ (pscf_scene)__________________ -3.0283E-03 + Bootstrap_fraction_(enforced)___________________________________________ (bootipf.)____________________ 4.1920E-01 + Diamagnetic_fraction_(enforced)_________________________________________ (diaipf.)_____________________ 0.0000E+00 + Pfirsch-Schlueter_fraction_(enforced)___________________________________ (psipf.)______________________ 0.0000E+00 + Loop_voltage_during_burn_(V)____________________________________________ (vburn)_______________________ 3.7450E-02 OP + Plasma_resistance_(ohm)_________________________________________________ (rplas)_______________________ 3.9755E-09 OP + Resistive_diffusion_time_(s)____________________________________________ (res_time)____________________ 3.0619E+03 OP + Plasma_inductance_(H)___________________________________________________ (rlp)_________________________ 1.4181E-05 OP + Coefficient_for_sawtooth_effects_on_burn_V-s_requirement________________ (csawth)______________________ 1.0000E+00 + Ratio_of_He_and_pellet_particle_confinement_times_______________________ (tauratio)____________________ 1.0000E+00 + Fuelling_rate_(nucleus-pairs/s)_________________________________________ (qfuel)_______________________ 3.3420E+21 OP + Fuel_burn-up_rate_(reactions/s)_________________________________________ (rndfuel)_____________________ 5.7755E+20 OP + Burn-up_fraction________________________________________________________ (burnup)______________________ 1.7282E-01 + # Energy confinement times, and required H-factors : # + # Current Drive System # + Current_drive_efficiency_model__________________________________________ (iefrf)_______________________ 10 + Secondary_current_drive_efficiency_model________________________________ (iefrffix)____________________ 0 + Ratio_of_power_for_flat-top_to_start-up_(MW)____________________________ (startupratio)________________ 1.0000E+00 + Auxiliary_power_used_for_plasma_heating_only_(MW)_______________________ (pheat)_______________________ 7.5000E+01 + Power_injected_for_current_drive_(MW)___________________________________ (pcurrentdrivemw)_____________ 5.1429E+00 + Maximum_Allowed_Bootstrap_current_fraction______________________________ (bscfmax)_____________________ 9.5000E-01 + Fusion_gain_factor_Q____________________________________________________ (bigq)________________________ 2.0060E+01 OP + Auxiliary_current_drive_(A)_____________________________________________ (auxiliary_cd)________________ 2.3908E+05 OP + Current_drive_efficiency_(A/W)__________________________________________ (effcd)_______________________ 4.6488E-02 OP + Normalised_current_drive_efficiency,_gamma_(10^20_A/W-m2)_______________ (gamcd)_______________________ 3.0000E-01 OP + Wall_plug_to_injector_efficiency________________________________________ (etacd)_______________________ 5.0000E-01 + ECRH_plasma_heating_efficiency__________________________________________ (gamma_ecrh)__________________ 3.0000E-01 + Bootstrap_fraction______________________________________________________ (bootipf)_____________________ 4.1920E-01 + Diamagnetic_fraction____________________________________________________ (diaipf)______________________ 0.0000E+00 + Pfirsch-Schlueter_fraction______________________________________________ (psipf)_______________________ 0.0000E+00 + Auxiliary_current_drive_fraction________________________________________ (faccd)_______________________ 1.4376E-02 + Inductive_fraction______________________________________________________ (facoh)_______________________ 5.6642E-01 + Total___________________________________________________________________ (plasipf+faccd+facoh)_________ 1.0000E+00 + Fraction_of_the_plasma_current_produced_by_non-inductive_means__________ (fvsbrnni)____________________ 4.3358E-01 ITV + Electron_cyclotron_injected_power_(MW)__________________________________ (echpwr)______________________ 8.0143E+01 OP + Maximum_allowable_ECRH_power_(MW)_______________________________________ (pinjalw)_____________________ 2.0000E+02 + ECH_wall_plug_efficiency________________________________________________ (etaech)______________________ 5.0000E-01 + ECH_wall_plug_power_(MW)________________________________________________ (echwpow)_____________________ 1.6029E+02 OP + Total_V-s_capability_of_Central_Solenoid/PF_coils_(Wb)__________________ (abs(vstot))__________________ 5.7728E+02 + Required_volt-seconds_during_start-up_(Wb)______________________________ (vssoft)______________________ 2.8601E+02 + Available_volt-seconds_during_burn_(Wb)_________________________________ (vsmax)_______________________ 2.7014E+02 + # Times # + Initial_charge_time_for_CS_from_zero_current_(s)________________________ (tramp)_______________________ 5.0000E+02 + Plasma_current_ramp-up_time_(s)_________________________________________ (tohs)________________________ 1.6631E+02 + Heating_time_(s)________________________________________________________ (theat)_______________________ 1.0000E+01 + Burn_time_(s)___________________________________________________________ (tburn)_______________________ 7.2035E+03 OP + Reset_time_to_zero_current_for_CS_(s)___________________________________ (tqnch)_______________________ 1.6631E+02 + Time_between_pulses_(s)_________________________________________________ (tdwell)______________________ 1.8000E+03 + Total_plant_cycle_time_(s)______________________________________________ (tcycle)______________________ 9.8463E+03 OP + # Radial Build # + TF_coil_radial_placement_switch_________________________________________ (tf_in_cs)____________________ 0 + TF_coil_radial_placement_switch_________________________________________ (tf_in_cs)____________________ 0 + Machine_bore_(m)________________________________________________________ (bore)________________________ 1.9854E+00 ITV + CS_radial_thickness_(m)_________________________________________________ (ohcth)_______________________ 5.7587E-01 ITV + CS_precompression_(m)___________________________________________________ (precomp)_____________________ 6.8064E-02 + CS_precompresion_to_TF_coil_radial_gap_(m)______________________________ (gapoh)_______________________ 8.0000E-02 + TF_coil_inboard_leg_(m)_________________________________________________ (tfcth)_______________________ 9.1597E-01 ITV + TF_coil_inboard_leg_insulation_gap_(m)__________________________________ (tftsgap)_____________________ 5.0000E-02 + Thermal_shield,_inboard_(m)_____________________________________________ (thshield_ib)_________________ 5.0000E-02 + thermal_shield_to_vessel_radial_gap_(m)_________________________________ (gapds)_______________________ 2.0000E-02 + Inboard_vacuum_vessel_radial_thickness_(m)______________________________ (d_vv_in)_____________________ 3.0000E-01 + Inner_radiation_shield_radial_thickness_(m)_____________________________ (shldith)_____________________ 3.0000E-01 + Gap_(m)_________________________________________________________________ (vvblgap)_____________________ 2.0000E-02 + Inboard_blanket_radial_thickness_(m)____________________________________ (blnkith)_____________________ 7.0000E-01 + Inboard_first_wall_radial_thickness_(m)_________________________________ (fwith)_______________________ 1.8000E-02 + Inboard_scrape-off_radial_thickness_(m)_________________________________ (scrapli)_____________________ 2.5000E-01 + Outboard_scrape-off_radial_thickness_(m)________________________________ (scraplo)_____________________ 2.5000E-01 + Outboard_first_wall_radial_thickness_(m)________________________________ (fwoth)_______________________ 1.8000E-02 + Outboard_blanket_radial_thickness_(m)___________________________________ (blnkoth)_____________________ 1.0000E+00 + Outer_radiation_shield_radial_thickness_(m)_____________________________ (shldoth)_____________________ 8.0000E-01 + Outboard_vacuum_vessel_radial_thickness_(m)_____________________________ (d_vv_out)____________________ 3.0000E-01 + Vessel_to_TF_radial_gap_(m)_____________________________________________ (gapsto)______________________ 1.3720E+00 + Thermal_shield,_outboard_(m)____________________________________________ (thshield_ob)_________________ 5.0000E-02 + Gap_(m)_________________________________________________________________ (tftsgap)_____________________ 5.0000E-02 + TF_coil_outboard_leg_radial_thickness_(m)_______________________________ (tfthko)______________________ 9.1597E-01 + # Vertical Build # + Divertor_null_switch____________________________________________________ (i_single_null)_______________ 1 + Vessel_-_TF_coil_vertical_gap_(m)_______________________________________ (vgap2)_______________________ 1.6300E-01 + Topside_vacuum_vessel_radial_thickness_(m)______________________________ (d_vv_top)____________________ 3.0000E-01 + Top_radiation_shield_thickness_(m)______________________________________ (shldtth)_____________________ 6.0000E-01 + Top_blanket_vertical_thickness_(m)______________________________________ (blnktth)_____________________ 8.5000E-01 + Top_first_wall_vertical_thickness_(m)___________________________________ (fwtth)_______________________ 1.8000E-02 + Top_scrape-off_vertical_thickness_(m)___________________________________ (vgaptop)_____________________ 6.0000E-01 + Plasma_half-height_(m)__________________________________________________ (rminor*kappa)________________ 4.9333E+00 + Bottom_scrape-off_vertical_thickness_(m)________________________________ (vgap)________________________ 2.0019E+00 + Divertor_structure_vertical_thickness_(m)_______________________________ (divfix)______________________ 6.2000E-01 + Bottom_radiation_shield_thickness_(m)___________________________________ (shldlth)_____________________ 7.0000E-01 + Underside_vacuum_vessel_radial_thickness_(m)____________________________ (d_vv_bot)____________________ 3.0000E-01 + External_cryostat_thickness_(m)_________________________________________ (ddwex)_______________________ 1.5000E-01 + Ratio_of_Central_solenoid_height_to_TF_coil_internal_height_____________ (ohhghf)______________________ 9.0000E-01 + Width_of_neutral_beam_duct_where_it_passes_between_the_TF_coils_(m)_____ (beamwd)______________________ 5.8000E-01 + # Divertor build and plasma position # + Plasma_top_position,_radial_(m)_________________________________________ (ptop_radial)_________________ 6.6667E+00 + Plasma_top_position,_vertical_(m)_______________________________________ (ptop_vertical)_______________ 4.9333E+00 + Plasma_geometric_centre,_radial_(m)_____________________________________ (physics_variables.rmajor.)___ 8.0000E+00 + Plasma_geometric_centre,_vertical_(m)___________________________________ (0.0)_________________________ 0.0000E+00 + Plasma_lower_physics_variables.triangularity____________________________ (tril)________________________ 5.0000E-01 + Plasma_elongation_______________________________________________________ (physics_variables.kappa.)____ 1.8500E+00 + TF_coil_vertical_offset_(m)_____________________________________________ (tfoffset)____________________ -6.1694E-01 + Plasma_outer_arc_radius_of_curvature_(m)________________________________ (rco)_________________________ 5.0422E+00 + Plasma_inner_arc_radius_of_curvature_(m)________________________________ (rci)_________________________ 9.7933E+00 + Plasma_lower_X-pt,_radial_(m)___________________________________________ (rxpt)________________________ 6.6667E+00 + Plasma_lower_X-pt,_vertical_(m)_________________________________________ (zxpt)________________________ -4.9333E+00 + Poloidal_plane_angle_between_vertical_and_inner_leg_(rad)_______________ (thetai)______________________ 2.0820E-01 + Poloidal_plane_angle_between_vertical_and_outer_leg_(rad)_______________ (thetao)______________________ 1.0429E+00 + Poloidal_plane_angle_between_inner_leg_and_plate_(rad)__________________ (betai)_______________________ 1.0000E+00 + Poloidal_plane_angle_between_outer_leg_and_plate_(rad)__________________ (betao)_______________________ 1.0000E+00 + Inner_divertor_leg_poloidal_length_(m)__________________________________ (plsepi)______________________ 1.0000E+00 + Outer_divertor_leg_poloidal_length_(m)__________________________________ (plsepo)______________________ 1.5000E+00 + Inner_divertor_plate_length_(m)_________________________________________ (plleni)______________________ 1.0000E+00 + Outer_divertor_plate_length_(m)_________________________________________ (plleno)______________________ 1.0000E+00 + Inner_strike_point,_radial_(m)__________________________________________ (rspi)________________________ 5.6883E+00 + Inner_strike_point,_vertical_(m)________________________________________ (zspi)________________________ -5.1400E+00 + Inner_plate_top,_radial_(m)_____________________________________________ (rplti)_______________________ 5.8656E+00 + Inner_plate_top,_vertical_(m)___________________________________________ (zplti)_______________________ -4.6725E+00 + Inner_plate_bottom,_radial_(m)__________________________________________ (rplbi)_______________________ 5.5109E+00 + Inner_plate_bottom,_vertical_(m)________________________________________ (zplbi)_______________________ -5.6075E+00 + Outer_strike_point,_radial_(m)__________________________________________ (rspo)________________________ 7.4223E+00 + Outer_strike_point,_vertical_(m)________________________________________ (zspo)________________________ -6.2291E+00 + Outer_plate_top,_radial_(m)_____________________________________________ (rplto)_______________________ 7.6496E+00 + Outer_plate_top,_vertical_(m)___________________________________________ (zplto)_______________________ -5.7838E+00 + Outer_plate_bottom,_radial_(m)__________________________________________ (rplbo)_______________________ 7.1949E+00 + Outer_plate_bottom,_vertical_(m)________________________________________ (zplbo)_______________________ -6.6744E+00 + Calculated_maximum_divertor_height_(m)__________________________________ (divht)_______________________ 2.0019E+00 + # TF coils # + Allowable_maximum_shear_stress_in_TF_coil_case_(Tresca_criterion)_(Pa)__ (sig_tf_case_max)_____________ 7.5000E+08 + Allowable_maximum_shear_stress_in_TF_coil_conduit_(Tresca_criterion)_(Pa (sig_tf_wp_max)_______________ 7.5000E+08 + WP_transverse_modulus_(GPa)_____________________________________________ (eyoung_wp_trans*1.0d-9)______ 4.3534E+01 OP + WP_vertical_modulus_(GPa)_______________________________________________ (eyoung_wp_axial*1.0d-9)______ 1.1510E+02 OP + WP_transverse_Poissons_ratio____________________________________________ (poisson_wp_trans)____________ 3.0390E-01 OP + WP_vertical-transverse_Pois._rat._______________________________________ (poisson_wp_axial)____________ 3.1568E-01 OP + Radial____stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_r_max(1))_____________ 4.8849E-08 + toroidal__stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_t_max(1))_____________ -4.8724E+08 + Vertical__stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_z_max(1))_____________ 2.6028E+08 + Von-Mises_stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_vmises_max(1))________ 6.5725E+08 + Maximum_shear_stress_for_the_Tresca_yield_criterion_1_(Pa)______________ (sig_tf_tresca_max(1))________ 7.4752E+08 + Radial____stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_r_max(2))_____________ -1.5411E+08 + toroidal__stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_t_max(2))_____________ -3.7861E+08 + Vertical__stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_z_max(2))_____________ 2.6028E+08 + Von-Mises_stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_vmises_max(2))________ 5.5645E+08 + Maximum_shear_stress_for_the_Tresca_yield_criterion_2_(Pa)______________ (sig_tf_tresca_max(2))________ 6.3889E+08 + Radial____stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_r_max(3))_____________ 6.1398E+06 + toroidal__stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_t_max(3))_____________ -3.6314E+08 + Vertical__stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_z_max(3))_____________ 1.4510E+08 + Von-Mises_stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_vmises_max(3))________ 4.5345E+08 + Maximum_shear_stress_for_the_Tresca_yield_criterion_3_(Pa)______________ (sig_tf_tresca_max(3))________ 5.0824E+08 + Maximum_radial_deflection_at_midplane_(m)_______________________________ (deflect)_____________________ -6.2714E-03 OP + Vertical_strain_on_casing_______________________________________________ (casestr)_____________________ 1.2697E-03 OP + Radial_strain_on_insulator______________________________________________ (insstrain)___________________ -7.6923E-03 OP + Conductor_technology____________________________________________________ (i_tf_sup)____________________ 1 + Superconductor_material_________________________________________________ (i_tf_sc_mat)_________________ 1 + Presence_of_TF_demountable_joints_______________________________________ (itart)_______________________ 0 + TF_inboard_leg_support_strategy_________________________________________ (i_tf_bucking)________________ 1 + Number_of_TF_coils______________________________________________________ (n_tf)________________________ 16 + Inboard_leg_centre_radius_(m)___________________________________________ (r_tf_inboard_mid)____________ 3.1673E+00 OP + Outboard_leg_centre_radius_(m)__________________________________________ (r_tf_outboard_mid)___________ 1.4985E+01 OP + Total_inboard_leg_radial_thickness_(m)__________________________________ (tfcth)_______________________ 9.1597E-01 ITV + Total_outboard_leg_radial_thickness_(m)_________________________________ (tfthko)______________________ 9.1597E-01 + Outboard_leg_toroidal_thickness_(m)_____________________________________ (tftort)______________________ 1.4145E+00 OP + Maximum_inboard_edge_height_(m)_________________________________________ (hmax)________________________ 8.8182E+00 OP + Mean_coil_circumference_(including_inboard_leg_length)_(m)______________ (tfleng)______________________ 4.7937E+01 OP + Vertical_TF_shape_______________________________________________________ (i_tf_shape)__________________ 1 + TF_coil_arc_point_0_R_(m)_______________________________________________ (xarc(1))_____________________ 3.6253E+00 + TF_coil_arc_point_0_Z_(m)_______________________________________________ (yarc(1))_____________________ 4.5506E+00 + TF_coil_arc_point_1_R_(m)_______________________________________________ (xarc(2))_____________________ 7.4667E+00 + TF_coil_arc_point_1_Z_(m)_______________________________________________ (yarc(2))_____________________ 7.5843E+00 + TF_coil_arc_point_2_R_(m)_______________________________________________ (xarc(3))_____________________ 1.4527E+01 + TF_coil_arc_point_2_Z_(m)_______________________________________________ (yarc(3))_____________________ 0.0000E+00 + TF_coil_arc_point_3_R_(m)_______________________________________________ (xarc(4))_____________________ 7.4667E+00 + TF_coil_arc_point_3_Z_(m)_______________________________________________ (yarc(4))_____________________ -8.8182E+00 + TF_coil_arc_point_4_R_(m)_______________________________________________ (xarc(5))_____________________ 3.6253E+00 + TF_coil_arc_point_4_Z_(m)_______________________________________________ (yarc(5))_____________________ -5.2909E+00 + TF_cross-section_(total)_(m2)___________________________________________ (tfareain)____________________ 1.8229E+01 + Total_steel_cross-section_(m2)__________________________________________ (a_tf_steel*n_tf)_____________ 1.2853E+01 + Total_steel_TF_fraction_________________________________________________ (f_tf_steel)__________________ 7.0508E-01 + Total_Insulation_cross-section_(total)_(m2)_____________________________ (a_tf_ins*n_tf)_______________ 8.4752E-01 + Total_Insulation_fraction_______________________________________________ (f_tf_ins)____________________ 4.6493E-02 + Casing_cross_section_area_(per_leg)_(m2)________________________________ (acasetf)_____________________ 5.6444E-01 + Inboard_leg_case_plasma_side_wall_thickness_(m)_________________________ (casthi)______________________ 6.0000E-02 + Inboard_leg_case_inboard_"nose"_thickness_(m)___________________________ (thkcas)______________________ 2.8216E-01 ITV + Inboard_leg_case_sidewall_thickness_at_its_narrowest_point_(m)__________ (casths)______________________ 5.0000E-02 + External_case_mass_per_coil_(kg)________________________________________ (whtcas)______________________ 5.5456E+05 OP + WP_cross_section_area_with_insulation_and_insertion_(per_coil)_(m2)_____ (awpc)________________________ 5.7486E-01 + WP_cross_section_area_(per_coil)_(m2)___________________________________ (aswp)________________________ 5.1696E-01 + Winding_pack_radial_thickness_(m)_______________________________________ (dr_tf_wp)____________________ 5.0416E-01 ITV + Winding_pack_toroidal_width_1_(m)_______________________________________ (wwp1)________________________ 1.1904E+00 OP + Winding_pack_toroidal_width_2_(m)_______________________________________ (wwp2)________________________ 1.0901E+00 OP + Ground_wall_insulation_thickness_(m)____________________________________ (tinstf)______________________ 8.0000E-03 + Winding_pack_insertion_gap_(m)__________________________________________ (tfinsgap)____________________ 1.0000E-02 + Steel_WP_cross-section_(total)_(m2)_____________________________________ (aswp*n_tf)___________________ 3.8217E+00 + Steel_WP_fraction_______________________________________________________ (aswp/awpc)___________________ 4.1550E-01 + Insulation_WP_fraction__________________________________________________ (aiwp/awpc)___________________ 4.7934E-02 + Cable_WP_fraction_______________________________________________________ ((awpc-aswp-aiwp)/awpc)_______ 5.3656E-01 + Turn_parametrisation____________________________________________________ (i_tf_turns_integer)__________ 0 + Number_of_turns_per_TF_coil_____________________________________________ (n_tf_turn)___________________ 1.4739E+02 OP + Width_of_turn_including_inter-turn_insulation_(m)_______________________ (t_turn_tf)___________________ 5.9223E-02 OP + Width_of_conductor_(square)_(m)_________________________________________ (t_conductor)_________________ 5.7623E-02 OP + Width_of_space_inside_conductor_(m)_____________________________________ (t_cable)_____________________ 4.1604E-02 OP + Steel_conduit_thickness_(m)_____________________________________________ (thwcndut)____________________ 8.0099E-03 ITV + Inter-turn_insulation_thickness_(m)_____________________________________ (thicndut)____________________ 8.0000E-04 + Diameter_of_central_helium_channel_in_cable_____________________________ (dhecoil)_____________________ 1.0000E-02 + internal_area_of_the_cable_space________________________________________ (acstf)_______________________ 1.6999E-03 + Coolant_fraction_in_conductor_excluding_central_channel_________________ (vftf)________________________ 3.0000E-01 + Copper_fraction_of_conductor____________________________________________ (fcutfsu)_____________________ 8.4212E-01 ITV + Superconductor_fraction_of_conductor____________________________________ (1-fcutfsu)___________________ 1.5788E-01 + Check_total_area_fractions_in_winding_pack_=_1__________________________ ______________________________ 1.0000E+00 + minimum_TF_conductor_temperature_margin__(K)____________________________ (tmargmin_tf)_________________ 1.5000E+00 + TF_conductor_temperature_margin_(K)_____________________________________ (tmargtf)_____________________ 1.5049E+00 + Elastic_properties_behavior_____________________________________________ (i_tf_cond_eyoung_axial)______ 0 + Conductor_axial_Youngs_modulus__________________________________________ (eyoung_cond_axial)___________ 0.0000E+00 + Conductor_transverse_Youngs_modulus_____________________________________ (eyoung_cond_trans)___________ 0.0000E+00 + Superconductor_mass_per_coil_(kg)_______________________________________ (whtconsc)____________________ 4.6964E+03 OP + Copper_mass_per_coil_(kg)_______________________________________________ (whtconcu)____________________ 5.8073E+04 OP + Steel_conduit_mass_per_coil_(kg)________________________________________ (whtconsh)____________________ 8.9310E+04 OP + Conduit_insulation_mass_per_coil_(kg)___________________________________ (whtconin)____________________ 2.3777E+03 OP + Total_conduit_mass_per_coil_(kg)________________________________________ (whtcon)______________________ 1.5446E+05 OP + Mass_of_each_TF_coil_(kg)_______________________________________________ (whttf/n_tf)__________________ 7.1402E+05 OP + Total_TF_coil_mass_(kg)_________________________________________________ (whttf)_______________________ 1.1424E+07 OP + Nominal_peak_field_assuming_toroidal_symmetry_(T)_______________________ (bmaxtf)______________________ 1.2178E+01 OP + Total_current_in_all_TF_coils_(MA)______________________________________ (ritfc/1.D6)__________________ 2.1176E+02 OP + TF_coil_current_(summed_over_all_coils)_(A)_____________________________ (ritfc)_______________________ 2.1176E+08 + Actual_peak_field_at_discrete_conductor_(T)_____________________________ (bmaxtfrp)____________________ 1.2636E+01 OP + Winding_pack_current_density_(A/m2)_____________________________________ (jwptf)_______________________ 2.5602E+07 OP + Inboard_leg_mid-plane_conductor_current_density_(A/m2)__________________ (oacdcp)______________________ 1.1617E+07 + Total_stored_energy_in_TF_coils_(GJ)____________________________________ (estotftgj)___________________ 1.2161E+02 OP + Inboard_vertical_tension_per_coil_(N)___________________________________ (vforce)______________________ 2.0908E+08 OP + Outboard_vertical_tension_per_coil_(N)__________________________________ (vforce_outboard)_____________ 2.0908E+08 OP + inboard_vertical_tension_fraction_(-)___________________________________ (f_vforce_inboard)____________ 5.0000E-01 OP + Centring_force_per_coil_(N/m)___________________________________________ (cforce)______________________ 8.0590E+07 OP + Max_allowed_tfcoil_variables.ripple_amplitude_at_plasma_outboard_midplan (ripmax)______________________ 6.0000E-01 + Ripple_amplitude_at_plasma_outboard_midplane_(%)________________________ (ripple)______________________ 6.0000E-01 OP + Actual_quench_time_(or_time_constant)_(s)_______________________________ (tdmptf)______________________ 1.8429E+01 ITV + Vacuum_Vessel_stress_on_quench_(Pa)_____________________________________ (vv_stress_quench)____________ 6.1442E+07 OP + Maximum_allowed_voltage_during_quench_due_to_insulation_(kV)____________ (vdalw)_______________________ 9.5837E+00 ITV + Actual_quench_voltage_(kV)______________________________________________ (vtfskv)______________________ 9.1862E+00 OP + Maximum_allowed_temp_rise_during_a_quench_(K)___________________________ (tmaxpro)_____________________ 1.5000E+02 + # Superconducting TF Coils # + Superconductor_switch___________________________________________________ (isumat)______________________ 1 + Critical_field_at_zero_temperature_and_strain_(T)_______________________ (bc20m)_______________________ 3.2970E+01 + Critical_temperature_at_zero_field_and_strain_(K)_______________________ (tc0m)________________________ 1.6060E+01 + Helium_temperature_at_peak_field_(=_superconductor_temperature)_(K)_____ (thelium)_____________________ 4.7500E+00 + Total_helium_fraction_inside_cable_space________________________________ (fhetot)______________________ 3.4620E-01 OP + Copper_fraction_of_conductor____________________________________________ (fcutfsu)_____________________ 8.4212E-01 ITV + Residual_manufacturing_strain_on_superconductor_________________________ (str_tf_con_res)______________ -5.0000E-03 + Self-consistent_strain_on_superconductor________________________________ (str_wp)______________________ 2.0730E-03 + Critical_current_density_in_superconductor_(A/m2)_______________________ (jcritsc)_____________________ 7.1337E+08 OP + Critical_current_density_in_strand_(A/m2)_______________________________ (jcritstr)____________________ 1.1263E+08 OP + Critical_current_density_in_winding_pack_(A/m2)_________________________ (jwdgcrt)_____________________ 3.5688E+07 OP + Actual_current_density_in_winding_pack_(A/m2)___________________________ (jwdgop)______________________ 2.5602E+07 OP + Minimum_allowed_temperature_margin_in_superconductor_(K)________________ (tmargmin_tf)_________________ 1.5000E+00 + Actual_temperature_margin_in_superconductor_(K)_________________________ (tmarg)_______________________ 1.5049E+00 OP + Critical_current_(A)____________________________________________________ (icrit)_______________________ 1.2517E+05 OP + Actual_current_(A)______________________________________________________ (cpttf)_______________________ 8.9795E+04 ITV + Actual_current_/_critical_current_______________________________________ (iooic)_______________________ 7.1737E-01 OP + # Central Solenoid and PF Coils # + Central_solenoid_superconductor_material________________________________ (isumatoh)____________________ 1 + Maximum_field_at_Beginning_Of_Pulse_(T)_________________________________ (bmaxoh0)_____________________ 1.4050E+01 OP + Critical_superconductor_current_density_at_BOP_(A/m2)___________________ (jscoh_bop)___________________ 3.4918E+08 OP + Critical_strand_current_density_at_BOP_(A/m2)___________________________ (jstrandoh_bop)_______________ 1.0475E+08 OP + Allowable_overall_current_density_at_BOP_(A/m2)_________________________ (rjohc0)______________________ 3.5294E+07 OP + Actual_overall_current_density_at_BOP_(A/m2)____________________________ (cohbop)______________________ 1.9126E+07 OP + Maximum_field_at_End_Of_Flattop_(T)_____________________________________ (bmaxoh)______________________ 1.3920E+01 OP + Critical_superconductor_current_density_at_EOF_(A/m2)___________________ (jscoh_eof)___________________ 3.6097E+08 OP + Critical_strand_current_density_at_EOF_(A/m2)___________________________ (jstrandoh_eof)_______________ 1.0829E+08 OP + Allowable_overall_current_density_at_EOF_(A/m2)_________________________ (rjohc)_______________________ 3.6485E+07 OP + Actual_overall_current_density_at_EOF_(A/m2)____________________________ (coheof)______________________ 2.0264E+07 ITV + CS_inside_radius_(m)____________________________________________________ (bore)________________________ 1.9854E+00 ITV + CS_thickness_(m)________________________________________________________ (ohcth)_______________________ 5.7587E-01 ITV + Gap_between_central_solenoid_and_TF_coil_(m)____________________________ (gapoh)_______________________ 8.0000E-02 + CS_overall_cross-sectional_area_(m2)____________________________________ (areaoh)______________________ 9.1407E+00 OP + CS_conductor+void_cross-sectional_area_(m2)_____________________________ (awpoh)_______________________ 4.3996E+00 OP + ___CS_conductor_cross-sectional_area_(m2)_______________________________ (awpoh*(1-vfohc))_____________ 3.0797E+00 OP + ___CS_void_cross-sectional_area_(m2)____________________________________ (awpoh*vfohc)_________________ 1.3199E+00 OP + CS_steel_cross-sectional_area_(m2)______________________________________ (areaoh-awpoh)________________ 4.7411E+00 OP + CS_steel_area_fraction__________________________________________________ (oh_steel_frac)_______________ 5.1868E-01 ITV + Switch_for_CS_stress_calculation________________________________________ (i_cs_stress)_________________ 0 + Allowable_stress_in_CS_steel_(Pa)_______________________________________ (alstroh)_____________________ 7.5000E+08 + Hoop_stress_in_CS_steel_(Pa)____________________________________________ (sig_hoop)____________________ 6.7569E+08 OP + Axial_stress_in_CS_steel_(Pa)___________________________________________ (sig_axial)___________________ -7.6205E+08 OP + Maximum_shear_stress_in_CS_steel_for_the_Tresca_criterion_(Pa)__________ (s_tresca_oh)_________________ 6.7569E+08 OP + Axial_force_in_CS_(N)___________________________________________________ (axial_force)_________________ -1.6256E+09 OP + Residual_manufacturing_strain_in_CS_superconductor_material_____________ (tfcoil_variables.str_cs_con_r -5.0000E-03 + Copper_fraction_in_strand_______________________________________________ (fcuohsu)_____________________ 7.0000E-01 + Void_(coolant)_fraction_in_conductor____________________________________ (vfohc)_______________________ 3.0000E-01 + Helium_coolant_temperature_(K)__________________________________________ (tftmp)_______________________ 4.7500E+00 + CS_temperature_margin_(K)_______________________________________________ (tmargoh)_____________________ 1.5052E+00 OP + Minimum_permitted_temperature_margin_(K)________________________________ (tmargmin_cs)_________________ 1.5000E+00 + Residual_hoop_stress_in_CS_Steel_(Pa)___________________________________ (residual_sig_hoop)___________ 2.4000E+08 + Minimum_burn_time_(s)___________________________________________________ (tbrnmn)______________________ 7.2000E+03 + Initial_vertical_crack_size_(m)_________________________________________ (t_crack_vertical)____________ 8.9000E-04 + Initial_radial_crack_size_(m)___________________________________________ (t_crack_radial)______________ 2.6700E-03 + CS_turn_area_(m)________________________________________________________ (a_oh_turn)___________________ 1.9739E-03 + CS_turn_length_(m)______________________________________________________ (l_cond_cst)__________________ 7.6953E-02 + CS_turn_internal_cable_space_radius_(m)_________________________________ (r_in_cst)____________________ 7.4740E-03 + CS_turn_width_(m)_______________________________________________________ (d_cond_cst)__________________ 2.5651E-02 + CS_structural_vertical_thickness_(m)____________________________________ (t_structural_vertical)_______ 5.3514E-03 + CS_structural_radial_thickness_(m)______________________________________ (t_structural_radial)_________ 5.3514E-03 + Allowable_number_of_cycles_till_CS_fracture_____________________________ (n_cycle)_____________________ 1.3378E+02 OP + Minimum_number_of_cycles_required_till_CS_fracture______________________ (n_cycle_min)_________________ 2.0000E+04 OP + PF_coil_superconductor_material_________________________________________ (isumatpf)____________________ 3 + Copper_fraction_in_conductor____________________________________________ (fcupfsu)_____________________ 6.9000E-01 + Maximum_permissible_tensile_stress_(MPa)________________________________ (sigpfcalw)___________________ 5.0000E+02 + JxB_hoop_force_fraction_supported_by_case_______________________________ (sigpfcf)_____________________ 6.6600E-01 + PF_coil_0_radius_(m)____________________________________________________ (rpf[0]_______________________ 5.5667E+00 + PF_coil_0_vertical_position_(m)_________________________________________ (zpf[0])______________________ 9.3603E+00 + PF_coil_0_radial_thickness_(m)__________________________________________ (pfdr(0))_____________________ 1.2727E+00 + PF_coil_0_vertical_thickness_(m)________________________________________ (pfdz(0))_____________________ 1.2727E+00 + PF_coil_0_turns_________________________________________________________ (turns[0])____________________ 4.4541E+02 + PF_coil_0_current_(MA)__________________________________________________ (ric[0])______________________ 1.7816E+01 + PF_coil_0_field_(T)_____________________________________________________ (bpf[0])______________________ 6.2280E+00 + PF_coil_1_radius_(m)____________________________________________________ (rpf[1]_______________________ 5.5667E+00 + PF_coil_1_vertical_position_(m)_________________________________________ (zpf[1])______________________ -1.0594E+01 + PF_coil_1_radial_thickness_(m)__________________________________________ (pfdr(1))_____________________ 1.3651E+00 + PF_coil_1_vertical_thickness_(m)________________________________________ (pfdz(1))_____________________ -1.3651E+00 + PF_coil_1_turns_________________________________________________________ (turns[1])____________________ 5.1248E+02 + PF_coil_1_current_(MA)__________________________________________________ (ric[1])______________________ 2.0499E+01 + PF_coil_1_field_(T)_____________________________________________________ (bpf[1])______________________ 6.6990E+00 + PF_coil_2_radius_(m)____________________________________________________ (rpf[2]_______________________ 1.6731E+01 + PF_coil_2_vertical_position_(m)_________________________________________ (zpf[2])______________________ 2.6667E+00 + PF_coil_2_radial_thickness_(m)__________________________________________ (pfdr(2))_____________________ 1.1332E+00 + PF_coil_2_vertical_thickness_(m)________________________________________ (pfdz(2))_____________________ 1.1332E+00 + PF_coil_2_turns_________________________________________________________ (turns[2])____________________ 1.9262E+02 + PF_coil_2_current_(MA)__________________________________________________ (ric[2])______________________ -7.7049E+00 + PF_coil_2_field_(T)_____________________________________________________ (bpf[2])______________________ 2.6389E+00 + PF_coil_3_radius_(m)____________________________________________________ (rpf[3]_______________________ 1.6731E+01 + PF_coil_3_vertical_position_(m)_________________________________________ (zpf[3])______________________ -2.6667E+00 + PF_coil_3_radial_thickness_(m)__________________________________________ (pfdr(3))_____________________ 1.1332E+00 + PF_coil_3_vertical_thickness_(m)________________________________________ (pfdz(3))_____________________ -1.1332E+00 + PF_coil_3_turns_________________________________________________________ (turns[3])____________________ 1.9262E+02 + PF_coil_3_current_(MA)__________________________________________________ (ric[3])______________________ -7.7049E+00 + PF_coil_3_field_(T)_____________________________________________________ (bpf[3])______________________ 2.6389E+00 + PF_coil_4_radius_(m)____________________________________________________ (rpf[4]_______________________ 1.5209E+01 + PF_coil_4_vertical_position_(m)_________________________________________ (zpf[4])______________________ 7.4667E+00 + PF_coil_4_radial_thickness_(m)__________________________________________ (pfdr(4))_____________________ 8.0773E-01 + PF_coil_4_vertical_thickness_(m)________________________________________ (pfdz(4))_____________________ 8.0773E-01 + PF_coil_4_turns_________________________________________________________ (turns[4])____________________ 1.3049E+02 + PF_coil_4_current_(MA)__________________________________________________ (ric[4])______________________ -5.2194E+00 + PF_coil_4_field_(T)_____________________________________________________ (bpf[4])______________________ 2.5737E+00 + PF_coil_5_radius_(m)____________________________________________________ (rpf[5]_______________________ 1.5209E+01 + PF_coil_5_vertical_position_(m)_________________________________________ (zpf[5])______________________ -7.4667E+00 + PF_coil_5_radial_thickness_(m)__________________________________________ (pfdr(5))_____________________ 8.0773E-01 + PF_coil_5_vertical_thickness_(m)________________________________________ (pfdz(5))_____________________ -8.0773E-01 + PF_coil_5_turns_________________________________________________________ (turns[5])____________________ 1.3049E+02 + PF_coil_5_current_(MA)__________________________________________________ (ric[5])______________________ -5.2194E+00 + PF_coil_5_field_(T)_____________________________________________________ (bpf[5])______________________ 2.5737E+00 + Central_solenoid_radius_(m)_____________________________________________ (rpf[nohc-1])_________________ 2.2734E+00 + Central_solenoid_vertical_position_(m)__________________________________ (zpf[nohc-1])_________________ 0.0000E+00 + Central_solenoid_radial_thickness_(m)___________________________________ (ohdr)________________________ 5.7587E-01 + Central_solenoid_vertical_thickness_(m)_________________________________ (ohdz)________________________ 1.5873E+01 + Central_solenoid_turns__________________________________________________ (turns[nohc-1])_______________ 4.6308E+03 + Central_solenoid_current_(MA)___________________________________________ (ric[nohc-1])_________________ -1.8523E+02 + Central_solenoid_field_(T)______________________________________________ (bpf[nohc-1])_________________ 1.4050E+01 + Sum_of_squares_of_residuals_____________________________________________ (ssq0)________________________ 3.5207E-04 OP + Smoothing_parameter_____________________________________________________ (alfapf)______________________ 5.0000E-10 + # Volt Second Consumption # + Total_volt-second_consumption_by_coils_(Wb)_____________________________ (vstot)_______________________ -5.8000E+02 OP + # Waveforms # + Ratio_of_central_solenoid_current_at_beginning_of_Pulse_/_end_of_flat-to (fcohbop)_____________________ 9.4380E-01 ITV + Ratio_of_central_solenoid_current_at_beginning_of_Flat-top_/_end_of_flat (fcohbof)_____________________ -1.4083E-01 OP + # PF Circuit Waveform Data # + Number_of_PF_circuits_including_CS_and_plasma___________________________ (ncirt)_______________________ 8 + PF_Circuit_0_Time_point_0_(A)___________________________________________ (pfc0t0)______________________ 0.0000E+00 + PF_Circuit_0_Time_point_1_(A)___________________________________________ (pfc0t1)______________________ 1.3971E+07 + PF_Circuit_0_Time_point_2_(A)___________________________________________ (pfc0t2)______________________ 1.7816E+07 + PF_Circuit_0_Time_point_3_(A)___________________________________________ (pfc0t3)______________________ 1.7816E+07 + PF_Circuit_0_Time_point_4_(A)___________________________________________ (pfc0t4)______________________ 9.2844E+05 + PF_Circuit_0_Time_point_5_(A)___________________________________________ (pfc0t5)______________________ 0.0000E+00 + PF_Circuit_1_Time_point_0_(A)___________________________________________ (pfc1t0)______________________ 0.0000E+00 + PF_Circuit_1_Time_point_1_(A)___________________________________________ (pfc1t1)______________________ 1.8269E+07 + PF_Circuit_1_Time_point_2_(A)___________________________________________ (pfc1t2)______________________ 2.0499E+07 + PF_Circuit_1_Time_point_3_(A)___________________________________________ (pfc1t3)______________________ 2.0499E+07 + PF_Circuit_1_Time_point_4_(A)___________________________________________ (pfc1t4)______________________ -1.5831E+06 + PF_Circuit_1_Time_point_5_(A)___________________________________________ (pfc1t5)______________________ 0.0000E+00 + PF_Circuit_2_Time_point_0_(A)___________________________________________ (pfc2t0)______________________ -0.0000E+00 + PF_Circuit_2_Time_point_1_(A)___________________________________________ (pfc2t1)______________________ 4.9542E+05 + PF_Circuit_2_Time_point_2_(A)___________________________________________ (pfc2t2)______________________ -7.1060E+06 + PF_Circuit_2_Time_point_3_(A)___________________________________________ (pfc2t3)______________________ -7.1060E+06 + PF_Circuit_2_Time_point_4_(A)___________________________________________ (pfc2t4)______________________ -7.7049E+06 + PF_Circuit_2_Time_point_5_(A)___________________________________________ (pfc2t5)______________________ -0.0000E+00 + PF_Circuit_3_Time_point_0_(A)___________________________________________ (pfc3t0)______________________ -0.0000E+00 + PF_Circuit_3_Time_point_1_(A)___________________________________________ (pfc3t1)______________________ 4.9542E+05 + PF_Circuit_3_Time_point_2_(A)___________________________________________ (pfc3t2)______________________ -7.1060E+06 + PF_Circuit_3_Time_point_3_(A)___________________________________________ (pfc3t3)______________________ -7.1060E+06 + PF_Circuit_3_Time_point_4_(A)___________________________________________ (pfc3t4)______________________ -7.7049E+06 + PF_Circuit_3_Time_point_5_(A)___________________________________________ (pfc3t5)______________________ -0.0000E+00 + PF_Circuit_4_Time_point_0_(A)___________________________________________ (pfc4t0)______________________ -0.0000E+00 + PF_Circuit_4_Time_point_1_(A)___________________________________________ (pfc4t1)______________________ 3.2650E+05 + PF_Circuit_4_Time_point_2_(A)___________________________________________ (pfc4t2)______________________ -4.8247E+06 + PF_Circuit_4_Time_point_3_(A)___________________________________________ (pfc4t3)______________________ -4.8247E+06 + PF_Circuit_4_Time_point_4_(A)___________________________________________ (pfc4t4)______________________ -5.2194E+06 + PF_Circuit_4_Time_point_5_(A)___________________________________________ (pfc4t5)______________________ -0.0000E+00 + PF_Circuit_5_Time_point_0_(A)___________________________________________ (pfc5t0)______________________ -0.0000E+00 + PF_Circuit_5_Time_point_1_(A)___________________________________________ (pfc5t1)______________________ 3.2650E+05 + PF_Circuit_5_Time_point_2_(A)___________________________________________ (pfc5t2)______________________ -4.8247E+06 + PF_Circuit_5_Time_point_3_(A)___________________________________________ (pfc5t3)______________________ -4.8247E+06 + PF_Circuit_5_Time_point_4_(A)___________________________________________ (pfc5t4)______________________ -5.2194E+06 + PF_Circuit_5_Time_point_5_(A)___________________________________________ (pfc5t5)______________________ -0.0000E+00 + CS_Circuit_Time_point_0_(A)_____________________________________________ (cs_t0)_______________________ -0.0000E+00 + CS_Circuit_Time_point_1_(A)_____________________________________________ (cs_t1)_______________________ 1.7482E+08 + CS_Circuit_Time_point_2_(A)_____________________________________________ (cs_t2)_______________________ 2.6086E+07 + CS_Circuit_Time_point_3_(A)_____________________________________________ (cs_t3)_______________________ 2.6086E+07 + CS_Circuit_Time_point_4_(A)_____________________________________________ (cs_t4)_______________________ -1.8523E+08 + CS_Circuit_Time_point_5_(A)_____________________________________________ (cs_t5)_______________________ -0.0000E+00 + Plasma_Time_point_0_(A)_________________________________________________ (plasmat0)____________________ 0.0000E+00 + Plasma_Time_point_1_(A)_________________________________________________ (plasmat1)____________________ 0.0000E+00 + Plasma_Time_point_2_(A)_________________________________________________ (plasmat2)____________________ 1.6631E+07 + Plasma_Time_point_3_(A)_________________________________________________ (plasmat3)____________________ 1.6631E+07 + Plasma_Time_point_4_(A)_________________________________________________ (plasmat4)____________________ 1.6631E+07 + Plasma_Time_point_5_(A)_________________________________________________ (plasmat5)____________________ 0.0000E+00 + # Support Structure # + Outer_PF_coil_fence_mass_(kg)___________________________________________ (fncmass)_____________________ 2.2924E+05 OP + Intercoil_support_structure_mass_(kg)___________________________________ (aintmass)____________________ 4.3045E+06 OP + Mass_of_cooled_components_(kg)__________________________________________ (coldmass)____________________ 3.4369E+07 OP + Gravity_support_structure_mass_(kg)_____________________________________ (clgsmass)____________________ 1.2760E+06 OP + Torus_leg_support_mass_(kg)_____________________________________________ (gsm1)________________________ 8.5820E+04 OP + Ring_beam_mass_(kg)_____________________________________________________ (gsm2)________________________ 4.0088E+05 OP + Ring_legs_mass_(kg)_____________________________________________________ (gsm3)________________________ 6.8283E+05 OP + # PF Coil Inductances # + # Nuclear Heating Magnets Before Renormalisation # + Shield_line_density_(tonne/m2)__________________________________________ (x_shield)____________________ 4.0560E+00 + Blanket_line_density_(tonne/m2)_________________________________________ (x_blanket)___________________ 2.2911E+00 + Unit_nuclear_heating_in_TF_coil_(W/GW)__________________________________ (tfc_nuc_heating)_____________ 1.4866E+04 + Total_nuclear_heating_in_TF_coil_(MW)___________________________________ (ptfnuc.)_____________________ 2.4085E-02 + powfmw__________________________________________________________________ (powfmw.)_____________________ 1.6202E+03 + total_mass_of_the_TF_coils_(kg)_________________________________________ (whttf)_______________________ 1.1424E+07 + # Pumping for primary coolant (helium) # + Pressure_drop_in_FW_and_blanket_coolant_incl._hx_and_pipes_(Pa)_________ (dp_he)_______________________ 5.5000E+05 + Fraction_of_FW_and_blanket_thermal_power_required_for_pumping___________ (fpump)_______________________ 8.9463E-02 OP + Total_power_absorbed_by_FW_&_blanket_(MW)_______________________________ (p_plasma)____________________ 1.6698E+03 OP + Inlet_temperature_of_FW_&_blanket_coolant_pump_(K)______________________ (t_in_compressor)_____________ 5.5703E+02 OP + Coolant_pump_outlet/Inlet_temperature_of_FW_&_blanket_(K)_______________ (t_in_bb)_____________________ 5.7313E+02 + Outlet_temperature_of_FW_&_blanket_(K)__________________________________ (t_out_bb)____________________ 7.7313E+02 + Mechanical_pumping_power_for_FW_and_blanket_cooling_loop_including_heat_ (htpmw_fw_blkt)_______________ 1.6407E+02 OP + Mechanical_pumping_power_for_divertor_(MW)______________________________ (htpmw_div)___________________ 1.6906E+00 OP + Mechanical_pumping_power_for_shield_and_vacuum_vessel_(MW)______________ (htpmw_shld)__________________ 7.0688E-03 OP + # First wall and blanket : CCFE HCPB model # + Titanium_beryllide_fraction_____________________________________________ (fbltibe12)___________________ 3.7500E-01 + Lithium_orthosilicate_fraction__________________________________________ (fblli2sio4)__________________ 3.7500E-01 + Steel_fraction__________________________________________________________ (fblss_ccfe)__________________ 9.7050E-02 + Coolant_fraction________________________________________________________ (vfcblkt)_____________________ 5.2950E-02 + Purge_gas_fraction______________________________________________________ (vfpblkt)_____________________ 1.0000E-01 + First_Wall_Armour_Volume_(m3)___________________________________________ (fw_armour_vol)_______________ 5.8692E+00 + First_Wall_Volume_(m3)__________________________________________________ (volfw)_______________________ 1.9807E+01 + Blanket_Volume_(m3)_____________________________________________________ (volblkt)_____________________ 1.1849E+03 + Shield_Volume_(m3)______________________________________________________ (volshld)_____________________ 7.8520E+02 + Vacuum_vessel_volume_(m3)_______________________________________________ (vdewin)______________________ 1.0178E+03 + First_Wall_Armour_Mass_(kg)_____________________________________________ (fw_armour_mass)______________ 1.1298E+05 OP + First_Wall_Mass,_excluding_armour_(kg)__________________________________ (fwmass)______________________ 1.5449E+05 OP + Blanket_Mass_-_Total(kg)________________________________________________ (whtblkt)_____________________ 2.9676E+06 OP + ____Blanket_Mass_-_TiBe12_(kg)__________________________________________ (whtbltibe12)_________________ 1.0042E+06 OP + ____Blanket_Mass_-_Li4SiO4_(kg)_________________________________________ (whtblli4sio4)________________ 1.0664E+06 OP + ____Blanket_Mass_-_Steel_(kg)___________________________________________ (whtblss)_____________________ 8.9696E+05 OP + Total_mass_of_armour,_first_wall_and_blanket_(kg)_______________________ (armour_fw_bl_mass)___________ 3.2350E+06 OP + Shield_Mass_(kg)________________________________________________________ (whtshld)_____________________ 2.4498E+06 OP + Vacuum_vessel_mass_(kg)_________________________________________________ (vvmass)______________________ 7.9388E+06 OP + Total_nuclear_heating_in_TF+PF_coils_(CS_is_negligible)_(MW)____________ (ptfnuc)______________________ 2.5118E-02 OP + Total_nuclear_heating_in_FW_(MW)________________________________________ (pnucfw)______________________ 1.6315E+02 OP + Total_nuclear_heating_in_the_blanket_(including_emult)_(MW)_____________ (pnucblkt)____________________ 1.2901E+03 OP + Total_nuclear_heating_in_the_shield_(MW)________________________________ (pnucshld)____________________ 1.4138E+00 OP + Total_nuclear_heating_in_the_divertor_(MW)______________________________ (pnucdiv)_____________________ 1.4906E+02 OP + Blanket_exponential_factor______________________________________________ (exp_blanket)_________________ 9.9936E-01 OP + Shield:_first_exponential_______________________________________________ (exp_shield1)_________________ 1.9523E-03 OP + Shield:_second_exponential______________________________________________ (exp_shield2)_________________ 2.5427E-01 OP + Solid_angle_fraction_taken_by_on_divertor_______________________________ (fdiv)________________________ 1.1500E-01 + Switch_for_plant_secondary_cycle________________________________________ (secondary_cycle)_____________ 2 + First_wall_coolant_pressure_(Pa)________________________________________ (fwpressure)__________________ 1.5500E+07 + Blanket_coolant_pressure_(Pa)___________________________________________ (blpressure)__________________ 1.5500E+07 + Allowable_nominal_neutron_fluence_at_first_wall_(MW.year/m2)____________ (abktflnc)____________________ 5.0000E+00 + No_of_inboard_blanket_modules_poloidally________________________________ (nblktmodpi)__________________ 7 + No_of_inboard_blanket_modules_toroidally________________________________ (nblktmodti)__________________ 32 + No_of_outboard_blanket_modules_poloidally_______________________________ (nblktmodpo)__________________ 8 + No_of_outboard_blanket_modules_toroidally_______________________________ (nblktmodto)__________________ 48 + Isentropic_efficiency_of_first_wall_/_blanket_coolant_pumps_____________ (etaiso)______________________ 9.0000E-01 + First_wall_area_(m2)____________________________________________________ (fwarea)______________________ 1.6044E+03 OP + Cryostat_internal_radius_(m)____________________________________________ (rdewex)______________________ 1.7798E+01 OP + Cryostat_internal_half-height_(m)_______________________________________ (zdewex)______________________ 1.5339E+01 OP + Vertical_clearance_from_TF_coil_to_cryostat_(m)_________________________ (clh1)________________________ 5.6044E+00 OP + Divertor_area_(m2)______________________________________________________ (divsur)______________________ 1.4879E+02 OP + Divertor_mass_(kg)______________________________________________________ (divmas)______________________ 3.6453E+04 OP + # Superconducting TF Coil Power Conversion # + TF_coil_current_(kA)____________________________________________________ (itfka)_______________________ 8.9795E+01 OP + Number_of_TF_coils______________________________________________________ (ntfc)________________________ 1.6000E+01 + Voltage_across_a_TF_coil_during_quench_(kV)_____________________________ (vtfskv)______________________ 9.1862E+00 OP + TF_coil_charge_time_(hours)_____________________________________________ (tchghr)______________________ 4.0000E+00 + Total_inductance_of_TF_coils_(H)________________________________________ (ltfth)_______________________ 3.0165E+01 OP + Total_resistance_of_TF_coils_(ohm)______________________________________ (rcoils)______________________ 0.0000E+00 OP + TF_coil_charging_voltage_(V)____________________________________________ (tfcv)________________________ 2.9268E+02 + Number_of_DC_circuit_breakers___________________________________________ (ntfbkr)______________________ 1.6000E+01 + Number_of_dump_resistors________________________________________________ (ndumpr)______________________ 6.4000E+01 + Resistance_per_dump_resistor_(ohm)______________________________________ (r1dump)______________________ 1.0230E-01 OP + Dump_resistor_peak_power_(MW)___________________________________________ (r1ppmw)______________________ 2.0622E+02 OP + Energy_supplied_per_dump_resistor_(MJ)__________________________________ (r1emj)_______________________ 1.9002E+03 OP + TF_coil_L/R_time_constant_(s)___________________________________________ (ttfsec)______________________ 1.8429E+01 OP + Power_supply_voltage_(V)________________________________________________ (tfpsv)_______________________ 3.0731E+02 OP + Power_supply_current_(kA)_______________________________________________ (tfpska)______________________ 9.4285E+01 OP + DC_power_supply_rating_(kW)_____________________________________________ (tfckw)_______________________ 2.8975E+04 OP + AC_power_for_charging_(kW)______________________________________________ (tfackw)______________________ 3.2194E+04 OP + TF_coil_resistive_power_(MW)____________________________________________ (rpower)______________________ 9.3902E+00 OP + TF_coil_inductive_power_(MVA)___________________________________________ (xpower)______________________ 1.6891E+01 OP + Aluminium_bus_current_density_(kA/cm2)__________________________________ (djmka)_______________________ 1.2500E-01 + Aluminium_bus_cross-sectional_area_(cm2)________________________________ (albusa)______________________ 7.1836E+02 OP + Total_length_of_TF_coil_bussing_(m)_____________________________________ (tfbusl)______________________ 3.1931E+03 OP + Aluminium_bus_weight_(tonnes)___________________________________________ (albuswt)_____________________ 6.1932E+02 OP + Total_TF_coil_bus_resistance_(ohm)______________________________________ (rtfbus)______________________ 1.1646E-03 OP + TF_coil_bus_voltage_drop_(V)____________________________________________ (vtfbus)______________________ 1.0457E+02 OP + Dump_resistor_floor_area_(m2)___________________________________________ (drarea)______________________ 4.9234E+03 OP + TF_coil_power_conversion_floor_space_(m2)_______________________________ (tfcfsp)______________________ 1.8228E+03 OP + TF_coil_power_conv._building_volume_(m3)________________________________ (tfcbv)_______________________ 1.0937E+04 OP + TF_coil_AC_inductive_power_demand_(MW)__________________________________ (xpwrmw)______________________ 1.8768E+01 OP + Total_steady_state_AC_power_demand_(MW)_________________________________ (tfacpd)______________________ 1.0434E+01 OP + # PF Coils and Central Solenoid: Power and Energy # + Number_of_PF_coil_circuits______________________________________________ (pfckts)______________________ 1.2000E+01 + Sum_of_PF_power_supply_ratings_(MVA)____________________________________ (spsmva)______________________ 3.0313E+02 OP + Total_PF_coil_circuit_bus_length_(m)____________________________________ (spfbusl)_____________________ 2.4480E+03 OP + Total_PF_coil_bus_resistive_power_(kW)__________________________________ (pfbuspwr)____________________ 9.6485E+02 OP + Total_PF_coil_resistive_power_(kW)______________________________________ (srcktpm)_____________________ 9.6485E+02 OP + Maximum_PF_coil_voltage_(kV)____________________________________________ (vpfskv)______________________ 2.0000E+01 + Efficiency_of_transfer_of_PF_stored_energy_into_or_out_of_storage_______ (etapsu)______________________ 9.0000E-01 + Maximum_stored_energy_in_poloidal_field_(MJ)____________________________ (ensxpfm)_____________________ 2.8804E+04 OP + Peak_absolute_rate_of_change_of_stored_energy_in_poloidal_field_(MW)____ (peakpoloidalpower)___________ 1.7319E+02 OP + # Vacuum System # + First_wall_outgassing_rate_(Pa_m/s)_____________________________________ (rat)_________________________ 1.3000E-08 + Total_outgassing_load_(Pa_m3/s)_________________________________________ (ogas)________________________ 1.6691E-04 OP + Base_pressure_required_(Pa)_____________________________________________ (pbase)_______________________ 5.0000E-04 + Required_N2_pump_speed_(m3/s)___________________________________________ (s(1))________________________ 3.3381E-01 OP + N2_pump_speed_provided_(m3/s)___________________________________________ (snet(1))_____________________ 2.3404E+01 OP + Plasma_chamber_volume_(m3)______________________________________________ (volume)______________________ 2.2588E+03 OP + Chamber_pressure_after_burn_(Pa)________________________________________ (pend)________________________ 1.6698E-01 OP + Chamber_pressure_before_burn_(Pa)_______________________________________ (pstart)______________________ 1.6698E-03 + Allowable_pumping_time_switch___________________________________________ (dwell_pump)__________________ 0 + Dwell_time_between_burns_(s)____________________________________________ (tdwell.)_____________________ 1.8000E+03 + CS_ramp-up_time_burns_(s)_______________________________________________ (tramp.)______________________ 5.0000E+02 + Allowable_pumping_time_between_burns_(s)________________________________ (tpump)_______________________ 1.8000E+03 + Required_D-T_pump_speed_(m3/s)__________________________________________ (s(2))________________________ 5.7790E+00 OP + D-T_pump_speed_provided_(m3/s)__________________________________________ (snet(2))_____________________ 5.6700E+01 OP + Divertor_chamber_gas_pressure_(Pa)______________________________________ (prdiv)_______________________ 3.6000E-01 + Helium_gas_fraction_in_divertor_chamber_________________________________ (fhe)_________________________ 1.7218E-01 OP + Required_helium_pump_speed_(m3/s)_______________________________________ (s(3))________________________ 3.8423E+01 OP + Helium_pump_speed_provided_(m3/s)_______________________________________ (snet(3))_____________________ 3.8423E+01 OP + D-T_fuelling_rate_(kg/s)________________________________________________ (frate)_______________________ 2.7747E-05 OP + Required_D-T_pump_speed_(m3/s)__________________________________________ (s(4))________________________ 3.8423E+01 OP + D-T_pump_speed_provided_(m3/s)__________________________________________ (snet(4))_____________________ 5.6700E+01 OP + Number_of_large_pump_ducts______________________________________________ (nduct)_______________________ 16 + Passage_diameter,_divertor_to_ducts_(m)_________________________________ (d(imax))_____________________ 4.7857E-01 OP + Passage_length_(m)______________________________________________________ (l1)__________________________ 1.7160E+00 OP + Diameter_of_ducts_(m)___________________________________________________ (dout)________________________ 5.7428E-01 OP + Duct_length,_divertor_to_elbow_(m)______________________________________ (l2)__________________________ 4.8000E+00 OP + Duct_length,_elbow_to_pumps_(m)_________________________________________ (l3)__________________________ 2.0000E+00 + Number_of_pumps_________________________________________________________ (pumpn)_______________________ 3.2000E+01 OP + # Plant Buildings System # + Internal_volume_of_reactor_building_(m3)________________________________ (vrci)________________________ 9.9708E+05 + Dist_from_centre_of_torus_to_bldg_wall_(m)______________________________ (wrbi)________________________ 3.9531E+01 + Effective_floor_area_(m2)_______________________________________________ (efloor)______________________ 3.3660E+05 + Reactor_building_volume_(m3)____________________________________________ (rbv)_________________________ 1.1310E+06 + Reactor_maintenance_building_volume_(m3)________________________________ (rmbv)________________________ 3.9641E+05 + Warmshop_volume_(m3)____________________________________________________ (wsv)_________________________ 1.2531E+05 + Tritium_building_volume_(m3)____________________________________________ (triv)________________________ 4.0000E+04 + Electrical_building_volume_(m3)_________________________________________ (elev)________________________ 5.1937E+04 + Control_building_volume_(m3)____________________________________________ (conv)________________________ 6.0000E+04 + Cryogenics_building_volume_(m3)_________________________________________ (cryv)________________________ 1.4976E+04 + Administration_building_volume_(m3)_____________________________________ (admv)________________________ 1.0000E+05 + Shops_volume_(m3)_______________________________________________________ (shov)________________________ 1.0000E+05 + Total_volume_of_nuclear_buildings_(m3)__________________________________ (volnucb)_____________________ 1.5738E+06 + # Electric Power Requirements # + Facility_base_load_(MW)_________________________________________________ (basemw)______________________ 5.0000E+00 + Divertor_coil_power_supplies_(MW)_______________________________________ (bdvmw)_______________________ 0.0000E+00 + Cryoplant_electric_power_(MW)___________________________________________ (crymw)_______________________ 3.6566E+01 OP + Primary_coolant_pumps_(MW)______________________________________________ (htpmw..)_____________________ 1.9053E+02 OP + PF_coil_power_supplies_(MW)_____________________________________________ (ppfmw)_______________________ 8.5511E+01 OP + TF_coil_power_supplies_(MW)_____________________________________________ (ptfmw)_______________________ 1.0434E+01 OP + Plasma_heating_supplies_(MW)____________________________________________ (pheatingmw)__________________ 1.6029E+02 OP + Tritium_processing_(MW)_________________________________________________ (trithtmw..)__________________ 1.5000E+01 + Vacuum_pumps__(MW)______________________________________________________ (vachtmw..)___________________ 5.0000E-01 + Total_pulsed_power_(MW)_________________________________________________ (pacpmw)______________________ 5.5432E+02 OP + Total_base_power_required_at_all_times_(MW)_____________________________ (fcsht)_______________________ 5.5490E+01 OP + # Cryogenics # + Conduction_and_radiation_heat_loads_on_cryogenic_components_(MW)________ (qss/1.0d6)___________________ 1.4779E-02 OP + Nuclear_heating_of_cryogenic_components_(MW)____________________________ (qnuc/1.0d6)__________________ 1.3000E-02 OP + AC_losses_in_cryogenic_components_(MW)__________________________________ (qac/1.0d6)___________________ 3.8170E-03 OP + Resistive_losses_in_current_leads_(MW)__________________________________ (qcl/1.0d6)___________________ 1.9539E-02 OP + 45%_allowance_for_heat_loads_in_transfer_lines,_storage_tanks_etc_(MW)__ (qmisc/1.0d6)_________________ 2.3011E-02 OP + Sum_=_Total_heat_removal_at_cryogenic_temperatures_(tfcoil_variables.tmp (helpow_+_helpow_cryal/1.0d6)_ 7.4146E-02 OP + Temperature_of_cryogenic_superconducting_components_(K)_________________ (tmpcry)______________________ 4.5000E+00 + Temperature_of_cryogenic_aluminium_components_(K)_______________________ (tcoolin)_____________________ 3.1315E+02 + Efficiency_(figure_of_merit)_of_cryogenic_plant_is_13%_of_ideal_Carnot_v ______________________________ 2.0277E-03 OP + Efficiency_(figure_of_merit)_of_cryogenic_aluminium_plant_is_40%_of_idea ______________________________ -2.0203E+00 OP + Electric_power_for_cryogenic_plant_(MW)_________________________________ (crypmw)______________________ 3.6566E+01 OP + # Plant Power / Heat Transport Balance # + Neutron_power_multiplication_in_blanket_________________________________ (emult)_______________________ 1.2690E+00 + Divertor_area_fraction_of_whole_toroid_surface__________________________ (fdiv)________________________ 1.1500E-01 + H/CD_apparatus_+_diagnostics_area_fraction______________________________ (fhcd)________________________ 0.0000E+00 + First_wall_area_fraction________________________________________________ (1-fdiv-fhcd)_________________ 8.8500E-01 + Switch_for_pumping_of_primary_coolant___________________________________ (primary_pumping)_____________ 3 + Mechanical_pumping_power_for_FW_cooling_loop_including_heat_exchanger_(M (htpmw_fw)____________________ 0.0000E+00 OP + Mechanical_pumping_power_for_blanket_cooling_loop_including_heat_exchang (htpmw_blkt)__________________ 0.0000E+00 OP + Mechanical_pumping_power_for_FW_and_blanket_cooling_loop_including_heat_ (htpmw_fw_blkt)_______________ 1.6407E+02 OP + Mechanical_pumping_power_for_divertor_(MW)______________________________ (htpmw_div)___________________ 1.6906E+00 OP + Mechanical_pumping_power_for_shield_and_vacuum_vessel_(MW)______________ (htpmw_shld)__________________ 7.0688E-03 OP + Electrical_pumping_power_for_FW_and_blanket_(MW)________________________ (htpmwe_fw_blkt)______________ 1.8858E+02 OP + Electrical_pumping_power_for_shield_(MW)________________________________ (htpmwe_shld)_________________ 8.1250E-03 OP + Electrical_pumping_power_for_divertor_(MW)______________________________ (htpmwe_div)__________________ 1.9433E+00 OP + Total_electrical_pumping_power_for_primary_coolant_(MW)_________________ (htpmw)_______________________ 1.9053E+02 OP + Coolant_pump_power_/_non-pumping_thermal_power_in_shield________________ (fpumpshld)___________________ 5.0000E-03 + Coolant_pump_power_/_non-pumping_thermal_power_in_divertor______________ (fpumpdiv)____________________ 5.0000E-03 + Electrical_efficiency_of_heat_transport_coolant_pumps___________________ (etahtp)______________________ 8.7000E-01 + Thermal_to_electric_conversion_efficiency_of_the_power_conversion_cycle_ (etath)_______________________ 4.0000E-01 + Fraction_of_total_high-grade_thermal_power_to_divertor__________________ (pdivfraction)________________ 1.5623E-01 + Total_power_leaving_reactor_(across_vacuum_vessel_boundary)_(MW)________ ______________________________ 2.0111E+03 + Heat_removal_from_cryogenic_plant_(MW)__________________________________ (crypmw)______________________ 3.6566E+01 + Heat_removal_from_facilities_(MW)_______________________________________ (fachtmw)_____________________ 5.5490E+01 + Coolant_pumping_efficiency_losses_(MW)__________________________________ (htpsecmw)____________________ 2.4769E+01 + Heat_removal_from_injection_power_(MW)__________________________________ (pinjht)______________________ 8.0143E+01 + Heat_removal_from_tritium_plant_(MW)____________________________________ (trithtmw)____________________ 1.5000E+01 + Heat_removal_from_vacuum_pumps_(MW)_____________________________________ (vachtmw)_____________________ 5.0000E-01 + TF_coil_resistive_power_(MW)____________________________________________ (tfcmw)_______________________ 0.0000E+00 + Total_low-grade_thermal_power_(MW)______________________________________ (psechtmw)____________________ 2.2417E+02 + Total_High-grade_thermal_power_(MW)_____________________________________ (pthermmw)____________________ 2.1751E+03 + Number_of_primary_heat_exchangers_______________________________________ (nphx)________________________ 3 OP + Transport_power_from_scaling_law_(MW)___________________________________ (pscalingmw)__________________ 2.9785E+02 + Radiation_power_from_inside_"coreradius"_(MW)___________________________ (pcoreradmw.)_________________ 9.1650E+01 + Total_(MW)______________________________________________________________ ______________________________ 3.8950E+02 + Alpha_power_deposited_in_plasma_(MW)____________________________________ (falpha*palpmw)_______________ 3.0746E+02 + Power_from_charged_products_of_DD_and/or_D-He3_fusion_(MW)______________ (pchargemw.)__________________ 1.2659E+00 + Ohmic_heating_(MW)______________________________________________________ (pohmmw.)_____________________ 6.2284E-01 + Injected_power_deposited_in_plasma_(MW)_________________________________ (pinjmw)______________________ 8.0143E+01 + Total_(MW)______________________________________________________________ ______________________________ 3.8950E+02 + Fusion_power_(MW)_______________________________________________________ (powfmw)______________________ 1.6202E+03 + Power_from_energy_multiplication_in_blanket_and_shield_(MW)_____________ (emultmw)_____________________ 3.0836E+02 + Injected_power_(MW)_____________________________________________________ (pinjmw.)_____________________ 8.0143E+01 + Ohmic_power_(MW)________________________________________________________ (pohmmw.)_____________________ 6.2284E-01 + Power_deposited_in_primary_coolant_by_pump_(MW)_________________________ (htpmw_mech)__________________ 1.6576E+02 + Total_(MW)______________________________________________________________ ______________________________ 2.1751E+03 + Heat_extracted_from_first_wall_and_blanket_(MW)_________________________ (pthermfw_blkt)_______________ 1.8339E+03 + Heat_extracted_from_shield__(MW)________________________________________ (pthermshld)__________________ 1.4208E+00 + Heat_extracted_from_divertor_(MW)_______________________________________ (pthermdiv)___________________ 3.3982E+02 + Nuclear_and_photon_power_lost_to_H/CD_system_(MW)_______________________ (psechcd)_____________________ 0.0000E+00 + Nuclear_power_lost_to_TF_(MW)___________________________________________ (ptfnuc)______________________ 2.5118E-02 + Total_(MW)______________________________________________________________ ______________________________ 2.1752E+03 + Net_electric_power_output(MW)___________________________________________ (pnetelmw.)___________________ 4.0001E+02 + Required_Net_electric_power_output(MW)__________________________________ (pnetelin)____________________ 4.0000E+02 + Electric_power_for_heating_and_current_drive_(MW)_______________________ (pinjwp)______________________ 1.6029E+02 + Electric_power_for_primary_coolant_pumps_(MW)___________________________ (htpmw)_______________________ 1.9053E+02 + Electric_power_for_vacuum_pumps_(MW)____________________________________ (vachtmw)_____________________ 5.0000E-01 + Electric_power_for_tritium_plant_(MW)___________________________________ (trithtmw)____________________ 1.5000E+01 + Electric_power_for_cryoplant_(MW)_______________________________________ (crypmw)______________________ 3.6566E+01 + Electric_power_for_TF_coils_(MW)________________________________________ (tfacpd)______________________ 1.0434E+01 + Electric_power_for_PF_coils_(MW)________________________________________ (pfwpmw)______________________ 1.2422E+00 + All_other_internal_electric_power_requirements_(MW)_____________________ (fachtmw)_____________________ 5.5490E+01 + Total_(MW)______________________________________________________________ (tot_plant_power)_____________ 8.7006E+02 + Total_(MW)______________________________________________________________ ______________________________ 8.7006E+02 + Gross_electrical_output*_(MW)___________________________________________ (pgrossmw)____________________ 8.7006E+02 + Fusion_power_(MW)_______________________________________________________ (powfmw)______________________ 1.6202E+03 + Power_from_energy_multiplication_in_blanket_and_shield_(MW)_____________ (emultmw)_____________________ 3.0836E+02 + Total_(MW)______________________________________________________________ ______________________________ 1.9285E+03 + Net_electrical_output_(MW) _____________________________________________ (pnetelmw)____________________ 4.0001E+02 + Heat_rejected_by_main_power_conversion_circuit_(MW)_____________________ (rejected_main)_______________ 1.3051E+03 + Heat_rejected_by_other_cooling_circuits_(MW)____________________________ (psechtmw)____________________ 2.2417E+02 + Total_(MW)______________________________________________________________ ______________________________ 1.9293E+03 + Net_electric_power_/_total_nuclear_power_(%)____________________________ (pnetelmw/(powfmw+emultmw)____ 2.0741E+01 + Net_electric_power_/_total_fusion_power_(%)_____________________________ (pnetelmw/powfmw)_____________ 2.4689E+01 + Gross_electric_power*_/_high_grade_heat_(%)_____________________________ (etath)_______________________ 4.0000E+01 + Recirculating_power_fraction____________________________________________ (cirpowfr)____________________ 5.4025E-01 + # Water usage during plant operation (secondary cooling) # + Volume_used_in_cooling_tower_(m3/day)___________________________________ (waterusetower)_______________ 5.5485E+04 OP + Volume_used_in_recirculating_water_system_(m3/day)______________________ (wateruserecirc)______________ 1.8617E+04 OP + Volume_used_in_once-through_water_system_(m3/day)_______________________ (wateruseonethru)_____________ 1.8244E+06 OP + # Errors and Warnings # + # Errors and Warnings # + PROCESS_error_status_flag_______________________________________________ (error_status)________________ 2 + Final_error_identifier__________________________________________________ (error_id)____________________ 244 + # End of PROCESS Output # + # End of PROCESS Output # + # Copy of PROCESS Input Follows # +************************************************************************************************************************ +***** ***** +***** Generic large tokamak file ***** +***** James Morris, UKAEA ***** +***** 28/06/23 ***** +***** ***** +************************************************************************* + +* Run Information * +******************* + +runtitle = Generic large tokamak + +* Figure of merit - minimise major radius +minmax = 1 + +* Error tolerance for VMCON +epsvmc = 1e-7 + +* Constraint Equations - Consistency Equations * +************************************************ + +* Beta consistency * +*------------------* +icc = 1 +ixc = 5 * beta +beta = 0.03 + +* Global power balance * +*----------------------* +icc = 2 + +* Radial build consistency * +*--------------------------* +icc = 11 + +* Constraint Equations - Limit Equations * +****************************************** + +* Density upper limit * +*---------------------* +icc = 5 +ixc = 6 * dene [m-3] +fdene = 1.2 +dene = 7.5E19 + +* Neutron wall load upper limit * +*-------------------------------* +icc = 8 +ixc = 14 * fwalld +fwalld = 1.0 +* wall load limit [MW/m2] +walalw = 2.0 + +* Fusion power upper limit * +*--------------------------* + +icc = 9 +ixc = 26 * ffuspow +* Maximum allowable value fusion power [MW] +powfmax = 3000 + +* Burn time lower limit * +*-----------------------* +icc = 13 +ixc = 21 * ftburn +* minimum burn time [s] +tbrnmn = 7200.0 + +* L-H threshold scaling * +*-----------------------* +icc = 15 +ixc = 103 * flhthresh +boundu(103) = 10.0 + +* Injection power upper limit * +*-----------------------------* +icc = 30 +ixc = 46 * fpinj +* Maximum allowable value for injected power [MW] +pinjalw = 200.0 + +* Net electric power lower limit * +*--------------------------------* +icc = 16 +ixc = 25 * fpnetel +* Minimum allowable value for net eletric power [MW] +pnetelin = 400.0 + +* Beta upper limit * +*------------------* +icc = 24 +ixc = 36 * fbetatry +fbetatry = 0.5 + +* Max TF field * +*--------------* +icc = 25 +ixc = 35 * fpeakb +* Maximum allowable value for toroidal magnetic field [T] +bmxlim = 14.0 + +* Central solenoid EOF current density upper limit * +*--------------------------------------------------* +icc = 26 +ixc = 37 * coheof [A/m2] +ixc = 38 * fjohc +boundu(38) = 1.0 +coheof = 1.5E7 +fjohc = 0.6 + +* Central solenoid BOP current density upper limit * +*--------------------------------------------------* +icc = 27 +ixc = 39 * fjohc0 +ixc = 41 * fcohbop +boundu(39) = 1.0 +fjohc0 = 0.6 +fcohbop = 0.9 + +* I_op/I_Crit TF coil limit * +*---------------------------* +icc = 33 +ixc = 50 * fiooic +boundu(50) = 1.0 +fiooic = 0.65 + +* Dump voltage upper limit * +*--------------------------* +icc = 34 +ixc = 51 * fvdump +ixc = 52 * vdalw [kV] +boundu(52) = 10.0 +fvdump = 1.0 +vdalw = 10.0 + +* J_winding pack protection * +*---------------------------* +icc = 35 +ixc = 53 * fjprot +fjprot = 1.0 + +* TF temp marg lower limit * +*--------------------------* +icc = 36 +ixc = 54 * ftmargtf +* Minimum allowable temperature margin [K] +tmargmin = 1.5 + +* CS coil temp margin lower limit * +*---------------------------------* +icc = 60 +ixc = 106 * ftmargoh +tmargmin_cs = 1.5 + +* Lower limit on taup/taueff (ratio alpha particle/energy confinement times) * +*-------------------------------------------------------------------------------* +icc = 62 +ixc = 110 * ftaulimit +taulimit = 5.0 + +* dump time constraint for VV stresses * +*--------------------------------------* +icc = 65 +ixc = 113 * fmaxvvstress +fmaxvvstress = 1.0 + +* CS stress limit * +*-----------------* +icc = 72 +ixc = 123 * foh_stress +foh_stress = 1.0 +* allowable hoop stress in Central Solenoid structural material [Pa] +alstroh = 7.5D8 + +* neped_neped_______________________normalised_residue____________________ (normres023)__________________ -1.9637E-08 + Upper_Lim._on_Psep_*_Bt_/_q_A_R___normalised_residue____________________ (normres024)__________________ 4.9789E-07 + TF_coil_case_stress_upper_limit___normalised_residue____________________ (normres025)__________________ -4.6757E-07 + TF_coil_conduit_stress_upper_lim__normalised_residue____________________ (normres026)__________________ -4.1375E-07 + # Final Feasible Point # + # Power Reactor Costs (1990 US$) # + First_wall_/_blanket_life_(years)_______________________________________ (fwbllife)____________________ 6.1566E+00 + Divertor_life_(years)___________________________________________________ (divlife.)____________________ 3.9769E+00 + Cost_of_electricity_(m$/kWh)____________________________________________ (coe)_________________________ 5.1257E+02 + # Detailed Costings (1990 US$) # + Acc.22_multiplier_for_Nth_of_a_kind_____________________________________ (fkind)_______________________ 1.0000E+00 + Level_of_Safety_Assurance_______________________________________________ (lsa)_________________________ 4 + # Structures and Site Facilities # + Site_improvements,_facilities,_land_(M$)________________________________ (c211)________________________ 3.5200E+01 + Reactor_building_cost_(M$)______________________________________________ (c212)________________________ 4.5238E+02 + Turbine_building_cost_(M$)______________________________________________ (c213)________________________ 3.8000E+01 + Reactor_maintenance_building_cost_(M$)__________________________________ (c2141)_______________________ 1.0307E+02 + Warm_shop_cost_(M$)_____________________________________________________ (c2142)_______________________ 5.7641E+01 + Tritium_building_cost_(M$)______________________________________________ (c215)________________________ 1.4800E+01 + Electrical_equipment_building_cost_(M$)_________________________________ (c216)________________________ 1.9736E+01 + Additional_buildings_cost_(M$)__________________________________________ (c2171)_______________________ 1.8000E+01 + Control_room_buildings_cost_(M$)________________________________________ (c2172)_______________________ 2.1000E+01 + Shop_and_warehouses_cost_(M$)___________________________________________ (c2173)_______________________ 1.1500E+01 + Cryogenic_building_cost_(M$)____________________________________________ (c2174)_______________________ 6.8891E+00 + Total_account_21_cost_(M$)______________________________________________ (c21)_________________________ 7.7822E+02 + # Reactor Systems # + First_wall_cost_(M$)____________________________________________________ (c2211)_______________________ 1.9130E+02 + Blanket_beryllium_cost_(M$)_____________________________________________ (c22121)______________________ 2.6109E+02 + Blanket_breeder_material_cost_(M$)______________________________________ (c22122)______________________ 6.3985E+02 + Blanket_stainless_steel_cost_(M$)_______________________________________ (c22123)______________________ 8.0726E+01 + Blanket_vanadium_cost_(M$)______________________________________________ (c22124)______________________ 0.0000E+00 + Blanket_total_cost_(M$)_________________________________________________ (c2212)_______________________ 9.8166E+02 + Bulk_shield_cost_(M$)___________________________________________________ (c22131)______________________ 7.8394E+01 + Penetration_shielding_cost_(M$)_________________________________________ (c22132)______________________ 7.8394E+01 + Total_shield_cost_(M$)__________________________________________________ (c2213)_______________________ 1.5679E+02 + Total_support_structure_cost_(M$)_______________________________________ (c2214)_______________________ 4.0933E+01 + Divertor_cost_(M$)______________________________________________________ (c2215)_______________________ 4.1660E+01 + Total_account_221_cost_(M$)_____________________________________________ (c221)________________________ 1.4123E+03 + # Magnets # + TF_coil_conductor_cost_(M$)_____________________________________________ (c22211)______________________ 1.3230E+02 + TF_coil_winding_cost_(M$)_______________________________________________ (c22212)______________________ 5.4263E+01 + TF_coil_case_cost_(M$)__________________________________________________ (c22213)______________________ 4.4365E+02 + TF_intercoil_structure_cost_(M$)________________________________________ (c22214)______________________ 1.5066E+02 + TF_coil_gravity_support_structure_(M$)__________________________________ (c22215)______________________ 4.4659E+01 + TF_magnet_assemblies_cost_(M$)__________________________________________ (c2221)_______________________ 8.2552E+02 + PF_coil_conductor_cost_(M$)_____________________________________________ (c22221)______________________ 4.6409E+02 + PF_coil_winding_cost_(M$)_______________________________________________ (c22222)______________________ 7.6765E+01 + PF_coil_case_cost_(M$)__________________________________________________ (c22223)______________________ 9.4861E+01 + PF_coil_support_structure_cost_(M$)_____________________________________ (c22224)______________________ 8.0235E+00 + PF_magnet_assemblies_cost_(M$)__________________________________________ (c2222)_______________________ 6.4374E+02 + Vacuum_vessel_assembly_cost_(M$)________________________________________ (c2223)_______________________ 2.5404E+02 + Total_account_222_cost_(M$)_____________________________________________ (c222)________________________ 1.7233E+03 + # Power Injection # + ECH_system_cost_(M$)____________________________________________________ (c2231)_______________________ 2.4043E+02 + Lower_hybrid_system_cost_(M$)___________________________________________ (c2232)_______________________ 0.0000E+00 + Neutral_beam_system_cost_(M$)___________________________________________ (c2233)_______________________ 0.0000E+00 + Total_account_223_cost_(M$)_____________________________________________ (c223)________________________ 2.4043E+02 + # Vacuum Systems # + High_vacuum_pumps_cost_(M$)_____________________________________________ (c2241)_______________________ 1.2480E+01 + Backing_pumps_cost_(M$)_________________________________________________ (c2242)_______________________ 4.6800E+00 + Vacuum_duct_cost_(M$)___________________________________________________ (c2243)_______________________ 2.5280E+00 + Valves_cost_(M$)________________________________________________________ (c2244)_______________________ 5.7410E+00 + Duct_shielding_cost_(M$)________________________________________________ (c2245)_______________________ 0.0000E+00 + Instrumentation_cost_(M$)_______________________________________________ (c2246)_______________________ 1.3000E+00 + Total_account_224_cost_(M$)_____________________________________________ (c224)________________________ 2.6729E+01 + # Power Conditioning # + TF_coil_power_supplies_cost_(M$)________________________________________ (c22511)______________________ 4.0144E+00 + TF_coil_breakers_cost_(M$)______________________________________________ (c22512)______________________ 3.4127E+01 + TF_coil_dump_resistors_cost_(M$)________________________________________ (c22513)______________________ 2.1322E+01 + TF_coil_instrumentation_and_control_(M$)________________________________ (c22514)______________________ 4.8000E+00 + TF_coil_bussing_cost_(M$)_______________________________________________ (c22515)______________________ 3.5267E+01 + Total,_TF_coil_power_costs_(M$)_________________________________________ (c2251)_______________________ 9.9531E+01 + PF_coil_power_supplies_cost_(M$)________________________________________ (c22521)______________________ 2.9591E+00 + PF_coil_instrumentation_and_control_(M$)________________________________ (c22522)______________________ 3.6000E+00 + PF_coil_bussing_cost_(M$)_______________________________________________ (c22523)______________________ 1.1995E+01 + PF_coil_burn_power_supplies_cost_(M$)___________________________________ (c22524)______________________ 1.2679E+00 + PF_coil_breakers_cost_(M$)______________________________________________ (c22525)______________________ 1.4709E+01 + PF_coil_dump_resistors_cost_(M$)________________________________________ (c22526)______________________ 4.3206E+00 + PF_coil_ac_breakers_cost_(M$)___________________________________________ (c22527)______________________ 9.0000E-01 + Total,_PF_coil_power_costs_(M$)_________________________________________ (c2252)_______________________ 3.9752E+01 + Total,_energy_storage_cost_(M$)_________________________________________ (c2253)_______________________ 1.6864E+01 + Total_account_225_cost_(M$)_____________________________________________ (c225)________________________ 1.5615E+02 + # Heat Transport System # + Pumps_and_piping_system_cost_(M$)_______________________________________ (cpp)_________________________ 3.6795E+01 + Primary_heat_exchanger_cost_(M$)________________________________________ (chx)_________________________ 7.1692E+01 + Total,_reactor_cooling_system_cost_(M$)_________________________________ (c2261)_______________________ 1.0849E+02 + Pumps,_piping_cost_(M$)_________________________________________________ (cppa)________________________ 2.8417E+01 + Total,_auxiliary_cooling_system_cost_(M$)_______________________________ (c2262)_______________________ 2.8417E+01 + Total,_cryogenic_system_cost_(M$)_______________________________________ (c2263)_______________________ 1.7039E+02 + Total_account_226_cost_(M$)_____________________________________________ (c226)________________________ 3.0729E+02 + # Fuel Handling System # + Fuelling_system_cost_(M$)_______________________________________________ (c2271)_______________________ 2.2300E+01 + Fuel_processing_and_purification_cost_(M$)______________________________ (c2272)_______________________ 1.0229E+02 + Atmospheric_recovery_systems_cost_(M$)__________________________________ (c2273)_______________________ 5.8088E+01 + Nuclear_building_ventilation_cost_(M$)__________________________________ (c2274)_______________________ 6.9201E+01 + Total_account_227_cost_(M$)_____________________________________________ (c227)________________________ 2.5188E+02 + # Instrumentation and Control # + Instrumentation_and_control_cost_(M$)___________________________________ (c228)________________________ 1.5000E+02 + # Maintenance Equipment # + Maintenance_equipment_cost_(M$)_________________________________________ (c229)________________________ 1.2500E+02 + # Total Account 22 Cost # + Total_account_22_cost_(M$)______________________________________________ (c22)_________________________ 4.3931E+03 + # Turbine Plant Equipment # + Turbine_plant_equipment_cost_(M$)_______________________________________ (c23)_________________________ 1.7613E+02 + # Electric Plant Equipment # + Switchyard_equipment_cost_(M$)__________________________________________ (c241)________________________ 1.8400E+01 + Transformers_cost_(M$)__________________________________________________ (c242)________________________ 8.0330E+00 + Low_voltage_equipment_cost_(M$)_________________________________________ (c243)________________________ 6.4513E+00 + Diesel_backup_equipment_cost_(M$)_______________________________________ (c244)________________________ 6.8000E+00 + Auxiliary_facilities_cost_(M$)__________________________________________ (c245)________________________ 1.5000E+00 + Total_account_24_cost_(M$)______________________________________________ (c24)_________________________ 4.1184E+01 + # Miscellaneous Plant Equipment # + Miscellaneous_plant_equipment_cost_(M$)_________________________________ (c25)_________________________ 2.5000E+01 + # Heat Rejection System # + Heat_rejection_system_cost_(M$)_________________________________________ (c26)_________________________ 4.9877E+01 + # Plant Direct Cost # + Plant_direct_cost_(M$)__________________________________________________ (cdirt)_______________________ 5.4635E+03 + # Reactor Core Cost # + Reactor_core_cost_(M$)__________________________________________________ (crctcore)____________________ 3.3761E+03 + # Indirect Cost # + Indirect_cost_(M$)______________________________________________________ (c9)__________________________ 1.8221E+03 + # Total Contingency # + Total_contingency_(M$)__________________________________________________ (ccont)_______________________ 1.4207E+03 + # Constructed Cost # + Constructed_cost_(M$)___________________________________________________ (concost)_____________________ 8.7063E+03 + # Interest during Construction # + Interest_during_construction_(M$)_______________________________________ (moneyint)____________________ 1.4365E+03 + # Total Capital Investment # + Total_capital_investment_(M$)___________________________________________ (capcost)_____________________ 1.0143E+04 + # Plant Availability # + Allowable_blanket_neutron_fluence_(MW-yr/m2)____________________________ (abktflnc)____________________ 5.0000E+00 + Allowable_divertor_heat_fluence_(MW-yr/m2)______________________________ (adivflnc)____________________ 7.0000E+00 + First_wall_/_blanket_lifetime_(years)___________________________________ (bktlife)_____________________ 6.1566E+00 OP + Divertor_lifetime_(years)_______________________________________________ (divlife)_____________________ 3.9769E+00 OP + Heating/CD_system_lifetime_(years)______________________________________ (cdrlife)_____________________ 6.1566E+00 OP + Total_plant_lifetime_(years)____________________________________________ (tlife)_______________________ 3.0000E+01 + Total_plant_availability_fraction_______________________________________ (cfactr)______________________ 8.0000E-01 + Number_of_fusion_cycles_to_reach_allowable_fw/blanket_DPA_______________ (bktcycles)___________________ 1.5787E+04 + # Plasma # + Tokamak_aspect_ratio_=_Conventional,_itart_=_0__________________________ (itart)_______________________ 0.0000E+00 + Major_radius_(m)________________________________________________________ (rmajor)______________________ 8.0000E+00 ITV + Minor_radius_(m)________________________________________________________ (rminor)______________________ 2.6667E+00 + Aspect_ratio____________________________________________________________ (aspect)______________________ 3.0000E+00 + Elongation,_X-point_(input_value_used)__________________________________ (kappa)_______________________ 1.8500E+00 + Elongation,_95%_surface_(calculated_from_kappa)_________________________ (kappa95)_____________________ 1.6518E+00 + Elongation,_area_ratio_calc.____________________________________________ (kappaa)______________________ 1.7188E+00 + Triangularity,_X-point_(input_value_used)_______________________________ (triang)______________________ 5.0000E-01 + Triangularity,_95%_surface_(calculated_from_triang)_____________________ (triang95)____________________ 3.3333E-01 + Plasma_poloidal_perimeter_(m)___________________________________________ (pperim)______________________ 2.4081E+01 + Plasma_cross-sectional_area_(m2)________________________________________ (xarea)_______________________ 3.8398E+01 + Plasma_surface_area_(m2)________________________________________________ (sarea)_______________________ 1.1738E+03 OP + Plasma_volume_(m3)______________________________________________________ (vol)_________________________ 1.8882E+03 OP + Plasma_current_scaling_law_used_________________________________________ (icurr)_______________________ 4 + Plasma_current_(MA)_____________________________________________________ (plascur/1D6)_________________ 1.6631E+01 + Current_density_profile_factor__________________________________________ (alphaj)______________________ 1.9805E+00 + Plasma_internal_inductance,_li__________________________________________ (rli)_________________________ 1.2275E+00 + Vertical_field_at_plasma_(T)____________________________________________ (bvert)_______________________ -7.4373E-01 + Vacuum_toroidal_field_at_R_(T)__________________________________________ (bt)__________________________ 5.2940E+00 ITV + Average_poloidal_field_(T)______________________________________________ (bp)__________________________ 8.6787E-01 + Total_field_(sqrt(bp^2_+_bt^2))_(T)_____________________________________ (btot)________________________ 5.3647E+00 + Safety_factor_on_axis___________________________________________________ (q0)__________________________ 1.0000E+00 + Safety_factor_at_95%_flux_surface_______________________________________ (q95)_________________________ 3.5961E+00 ITV + Cylindrical_safety_factor_(qcyl)________________________________________ (qstar)_______________________ 2.9805E+00 + Total_plasma_beta_______________________________________________________ (beta)________________________ 3.3648E-02 ITV + Total_poloidal_beta_____________________________________________________ (betap)_______________________ 1.2857E+00 OP + Total_toroidal_beta_____________________________________________________ ______________________________ 3.4553E-02 OP + Fast_alpha_beta_________________________________________________________ (betaft)______________________ 4.2236E-03 OP + Beam_ion_beta___________________________________________________________ (betanb)______________________ 0.0000E+00 OP + (Fast_alpha_+_beam_physics_variables.beta)/(thermal_physics_variables.be (gammaft)_____________________ 1.4354E-01 OP + Thermal_beta____________________________________________________________ ______________________________ 2.9425E-02 OP + Thermal_poloidal_beta___________________________________________________ ______________________________ 1.1243E+00 OP + Thermal_toroidal_physics_variables.beta_(=_beta-exp)____________________ ______________________________ 3.0215E-02 OP + 2nd_stability_physics_variables.beta_:_beta_p_/_(R/a)___________________ (eps*betap)___________________ 4.2857E-01 + 2nd_stability_physics_variables.beta_upper_limit________________________ (epbetmax)____________________ 1.3800E+00 + Beta_g_coefficient______________________________________________________ (dnbeta)______________________ 4.9099E+00 + Normalised_thermal_beta_________________________________________________ ______________________________ 2.4977E+00 + Normalised_total_beta___________________________________________________ ______________________________ 2.8562E+00 + Normalised_toroidal_beta________________________________________________ (normalised_toroidal_beta)____ 2.9330E+00 + Limit_on_thermal_beta___________________________________________________ (betalim)_____________________ 5.7842E-02 + Plasma_thermal_energy_(J)_______________________________________________ ______________________________ 9.5431E+08 OP + Total_plasma_internal_energy_(J)________________________________________ (total_plasma_internal_energy) 1.0913E+09 OP + Electron_temperature_(keV)______________________________________________ (te)__________________________ 1.2489E+01 ITV + Electron_temperature_on_axis_(keV)______________________________________ (te0)_________________________ 2.5758E+01 + Ion_temperature_(keV)___________________________________________________ (ti)__________________________ 1.2489E+01 + Ion_temperature_on_axis_(keV)___________________________________________ (ti0)_________________________ 2.5758E+01 + Electron_temp.,_density_weighted_(keV)__________________________________ (ten)_________________________ 1.3805E+01 + Electron_density_(/m3)__________________________________________________ (dene)________________________ 8.0667E+19 ITV + Electron_density_on_axis_(/m3)__________________________________________ (ne0)_________________________ 1.0610E+20 OP + Line-averaged_electron_density_(/m3)____________________________________ (dnla)________________________ 8.9334E+19 OP + Line-averaged_electron_density_/_Greenwald_density______________________ (dnla_gw)_____________________ 1.2000E+00 OP + Ion_density_(/m3)_______________________________________________________ (dnitot)______________________ 7.1669E+19 OP + Fuel_density_(/m3)______________________________________________________ (deni)________________________ 6.4831E+19 OP + Total_impurity_density_with_Z_>_2_(no_He)_(/m3)_________________________ (dnz)_________________________ 4.6503E+16 OP + Helium_ion_density_(thermalised_ions_only)_(/m3)________________________ (dnalp)_______________________ 6.7723E+18 OP + Proton_density_(/m3)____________________________________________________ (dnprot)______________________ 1.8963E+16 OP + Hot_beam_density_(/m3)__________________________________________________ (dnbeam)______________________ 0.0000E+00 OP + Density_limit_from_scaling_(/m3)________________________________________ (dnelimt)_____________________ 7.4445E+19 OP + Density_limit_(enforced)_(/m3)__________________________________________ (boundu(9)*dnelimt)___________ 7.4445E+19 OP + Helium_ion_density_(thermalised_ions_only)_/_electron_density___________ (ralpne)______________________ 8.3954E-02 ITV + H__concentration________________________________________________________ (fimp(01))____________________ 8.0392E-01 OP + He_concentration________________________________________________________ (fimp(02))____________________ 8.3954E-02 + Be_concentration________________________________________________________ (fimp(03))____________________ 0.0000E+00 + C__concentration________________________________________________________ (fimp(04))____________________ 0.0000E+00 + N__concentration________________________________________________________ (fimp(05))____________________ 0.0000E+00 + O__concentration________________________________________________________ (fimp(06))____________________ 0.0000E+00 + Ne_concentration________________________________________________________ (fimp(07))____________________ 0.0000E+00 + Si_concentration________________________________________________________ (fimp(08))____________________ 0.0000E+00 + Ar_concentration________________________________________________________ (fimp(09))____________________ 0.0000E+00 + Fe_concentration________________________________________________________ (fimp(10))____________________ 0.0000E+00 + Ni_concentration________________________________________________________ (fimp(11))____________________ 0.0000E+00 + Kr_concentration________________________________________________________ (fimp(12))____________________ 0.0000E+00 + Xe_concentration________________________________________________________ (fimp(13))____________________ 5.7149E-04 ITV + W__concentration________________________________________________________ (fimp(14))____________________ 5.0000E-06 + Average_mass_of_all_ions_(amu)__________________________________________ (aion)________________________ 2.7252E+00 OP + Effective_charge________________________________________________________ (zeff)________________________ 2.5164E+00 + Density_profile_factor__________________________________________________ (alphan)______________________ 1.0000E+00 + Plasma_profile_model____________________________________________________ (ipedestal)___________________ 1 + Density_pedestal_r/a_location___________________________________________ (rhopedn)_____________________ 9.4000E-01 + Electron_density_pedestal_height_(/m3)__________________________________ (neped)_______________________ 6.3278E+19 OP + Electron_density_at_pedestal_/_nGW______________________________________ (fgwped_out)__________________ 8.5000E-01 + Temperature_pedestal_r/a_location_______________________________________ (rhopedt)_____________________ 9.4000E-01 + Pedestal_scaling_switch_________________________________________________ (ieped)_______________________ 0 + Electron_temp._pedestal_height_(keV)____________________________________ (teped)_______________________ 5.5000E+00 + Electron_temp._at_separatrix_(keV)______________________________________ (tesep)_______________________ 1.0000E-01 + Electron_density_at_separatrix_(/m3)____________________________________ (nesep)_______________________ 3.7223E+19 + Electron_density_at_separatrix_/_nGW____________________________________ (fgwsep_out)__________________ 5.0000E-01 + Temperature_profile_index_______________________________________________ (alphat)______________________ 1.4500E+00 + Temperature_profile_index_beta__________________________________________ (tbeta)_______________________ 2.0000E+00 + Old_ASDEX_model_________________________________________________________ (dlimit(1))___________________ 5.2797E+19 OP + Borrass_ITER_model_I____________________________________________________ (dlimit(2))___________________ 1.0969E+20 OP + Borrass_ITER_model_II___________________________________________________ (dlimit(3))___________________ 4.3575E+19 OP + JET_edge_radiation_model________________________________________________ (dlimit(4))___________________ 3.0227E+21 OP + JET_simplified_model____________________________________________________ (dlimit(5))___________________ 4.3397E+20 OP + Hugill-Murakami_Mq_model________________________________________________ (dlimit(6))___________________ 6.6609E+19 OP + Greenwald_model_________________________________________________________ (dlimit(7))___________________ 7.4445E+19 OP + Deuterium_fuel_fraction_________________________________________________ (fdeut)_______________________ 5.0000E-01 + Tritium_fuel_fraction___________________________________________________ (ftrit)_______________________ 5.0000E-01 + Total_fusion_power_(MW)_________________________________________________ (powfmw)______________________ 1.6202E+03 OP + _=____D-T_fusion_power_(MW)_____________________________________________ (pdt)_________________________ 1.6182E+03 OP + __+___D-D_fusion_power_(MW)_____________________________________________ (pdd)_________________________ 1.9494E+00 OP + __+_D-He3_fusion_power_(MW)_____________________________________________ (pdhe3)_______________________ 0.0000E+00 OP + Alpha_power:_total_(MW)_________________________________________________ (palpmw)______________________ 3.2365E+02 OP + Alpha_power:_beam-plasma_(MW)___________________________________________ (palpnb)______________________ 0.0000E+00 OP + Neutron_power_(MW)______________________________________________________ (pneutmw)_____________________ 1.2953E+03 OP + Charged_particle_power_(excluding_alphas)_(MW)__________________________ (pchargemw)___________________ 1.2659E+00 OP + Total_power_deposited_in_plasma_(MW)____________________________________ (tot_power_plasma)____________ 3.8950E+02 OP + Bremsstrahlung_radiation_power_(MW)_____________________________________ (pbrempv*vol)_________________ 6.5195E+01 OP + Line_radiation_power_(MW)_______________________________________________ (plinepv*vol)_________________ 1.4609E+02 OP + Synchrotron_radiation_power_(MW)________________________________________ (psyncpv*vol)_________________ 1.5187E+01 OP + Synchrotron_wall_reflectivity_factor____________________________________ (ssync)_______________________ 6.0000E-01 + Normalised_minor_radius_defining_'core'_________________________________ (coreradius)__________________ 7.5000E-01 + Fraction_of_core_radiation_subtracted_from_P_L__________________________ (coreradiationfraction)_______ 6.0000E-01 + Radiation_power_from_inner_zone_(MW)____________________________________ (pinnerzoneradmw)_____________ 9.1650E+01 OP + Radiation_power_from_outer_zone_(MW)____________________________________ (pouterzoneradmw)_____________ 1.3482E+02 OP + Total_radiation_power_from_inside_LCFS_(MW)_____________________________ (pradmw)______________________ 2.2647E+02 OP + LCFS_radiation_fraction_=_total_radiation_in_LCFS_/_total_power_deposite (rad_fraction_LCFS)___________ 5.8144E-01 OP + Nominal_mean_radiation_load_on_inside_surface_of_reactor_(MW/m2)________ (photon_wall)_________________ 1.7749E-01 OP + Peaking_factor_for_radiation_wall_load__________________________________ (peakfactrad)_________________ 3.3300E+00 IP + Maximum_permitted_radiation_wall_load_(MW/m^2)__________________________ (maxradwallload)______________ 1.0000E+00 IP + Peak_radiation_wall_load_(MW/m^2)_______________________________________ (peakradwallload)_____________ 5.9106E-01 OP + Fast_alpha_particle_power_incident_on_the_first_wall_(MW)_______________ (palpfwmw)____________________ 1.6182E+01 OP + Nominal_mean_neutron_load_on_inside_surface_of_reactor_(MW/m2)__________ (wallmw)______________________ 1.0152E+00 OP + Power_incident_on_the_divertor_targets_(MW)_____________________________ (ptarmw)______________________ 3.2606E+01 OP + Fraction_of_power_to_the_lower_divertor_________________________________ (ftar)________________________ 1.0000E+00 IP + Outboard_side_heat_flux_decay_length_(m)________________________________ (lambdaio)____________________ 1.5700E-03 OP + Fraction_of_power_on_the_inner_targets__________________________________ (fio)_________________________ 4.1000E-01 OP + Fraction_of_power_incident_on_the_lower_inner_target____________________ (fLI)_________________________ 4.1000E-01 OP + Fraction_of_power_incident_on_the_lower_outer_target____________________ (fLO)_________________________ 5.9000E-01 OP + Power_incident_on_the_lower_inner_target_(MW)___________________________ (pLImw)_______________________ 1.3368E+01 OP + Power_incident_on_the_lower_outer_target_(MW)___________________________ (pLOmw)_______________________ 1.9237E+01 OP + Ohmic_heating_power_(MW)________________________________________________ (pohmmw)______________________ 6.2284E-01 OP + Fraction_of_alpha_power_deposited_in_plasma_____________________________ (falpha)______________________ 9.5000E-01 + Fraction_of_alpha_power_to_electrons____________________________________ (falpe)_______________________ 7.1828E-01 + Fraction_of_alpha_power_to_ions_________________________________________ (falpi)_______________________ 2.8172E-01 + Ion_transport_(MW)______________________________________________________ (ptrimw)______________________ 1.4013E+02 OP + Electron_transport_(MW)_________________________________________________ (ptremw)______________________ 1.5772E+02 OP + Injection_power_to_ions_(MW)____________________________________________ (pinjimw)_____________________ 0.0000E+00 OP + Injection_power_to_electrons_(MW)_______________________________________ (pinjemw)_____________________ 8.0143E+01 OP + Ignited_plasma_switch_(0=not_ignited,_1=ignited)________________________ (ignite)______________________ 0 + Power_into_divertor_zone_via_charged_particles_(MW)_____________________ (pdivt)_______________________ 1.6303E+02 OP + Psep_/_R_ratio_(MW/m)___________________________________________________ (pdivt/rmajor)________________ 2.0378E+01 OP + Psep_Bt_/_qAR_ratio_(MWT/m)_____________________________________________ (pdivtbt/qar)_________________ 1.0000E+01 OP + ITER_1996_scaling:_nominal_(MW)_________________________________________ (pthrmw(1))___________________ 1.2978E+02 OP + ITER_1996_scaling:_upper_bound_(MW)_____________________________________ (pthrmw(2))___________________ 2.8603E+02 OP + ITER_1996_scaling:_lower_bound_(MW)_____________________________________ (pthrmw(3))___________________ 5.8098E+01 OP + ITER_1997_scaling_(1)_(MW)______________________________________________ (pthrmw(4))___________________ 2.1452E+02 OP + ITER_1997_scaling_(2)_(MW)______________________________________________ (pthrmw(5))___________________ 1.7206E+02 OP + Martin_2008_scaling:_nominal_(MW)_______________________________________ (pthrmw(6))___________________ 9.7416E+01 OP + Martin_2008_scaling:_95%_upper_bound_(MW)_______________________________ (pthrmw(7))___________________ 1.2769E+02 OP + Martin_2008_scaling:_95%_lower_bound_(MW)_______________________________ (pthrmw(8))___________________ 6.7143E+01 OP + Snipes_2000_scaling:_nominal_(MW)_______________________________________ (pthrmw(9))___________________ 6.7785E+01 OP + Snipes_2000_scaling:_upper_bound_(MW)___________________________________ (pthrmw(10))__________________ 9.9437E+01 OP + Snipes_2000_scaling:_lower_bound_(MW)___________________________________ (pthrmw(11))__________________ 4.5839E+01 OP + Snipes_2000_scaling_(closed_divertor):_nominal_(MW)_____________________ (pthrmw(12))__________________ 3.1010E+01 OP + Snipes_2000_scaling_(closed_divertor):_upper_bound_(MW)_________________ (pthrmw(13))__________________ 4.3148E+01 OP + Snipes_2000_scaling_(closed_divertor):_lower_bound_(MW)_________________ (pthrmw(14))__________________ 2.2130E+01 OP + Hubbard_2012_L-I_threshold_-_nominal_(MW)_______________________________ (pthrmw(15))__________________ 2.7549E+01 OP + Hubbard_2012_L-I_threshold_-_lower_bound_(MW)___________________________ (pthrmw(16))__________________ 1.4319E+01 OP + Hubbard_2012_L-I_threshold_-_upper_bound_(MW)___________________________ (pthrmw(17))__________________ 5.3005E+01 OP + Hubbard_2017_L-I_threshold______________________________________________ (pthrmw(18))__________________ 2.6202E+02 OP + Martin_2008_aspect_ratio_corrected_scaling:_nominal_(MW)________________ (pthrmw(19))__________________ 9.7416E+01 OP + Martin_2008_aspect_ratio_corrected_scaling:_95%_upper_bound_(MW)________ (pthrmw(20))__________________ 1.2769E+02 OP + Martin_2008_aspect_ratio_corrected_scaling:_95%_lower_bound_(MW)________ (pthrmw(21))__________________ 6.7143E+01 OP + L-H_threshold_power_(enforced)_(MW)_____________________________________ (boundl(103)*plhthresh)_______ 9.7416E+01 OP + L-H_threshold_power_(MW)________________________________________________ (plhthresh)___________________ 9.7416E+01 OP + Confinement_H_factor____________________________________________________ (hfact)_______________________ 1.1886E+00 ITV + Global_thermal_energy_confinement_time_(s)______________________________ (taueff)______________________ 3.2037E+00 + Ion_energy_confinement_time_(s)_________________________________________ (tauei)_______________________ 3.2037E+00 + Electron_energy_confinement_time_(s)____________________________________ (tauee)_______________________ 3.2037E+00 + n.tau_=_Volume-average_electron_density_x_Energy_confinement_time_(s/m3) (dntau)_______________________ 2.5843E+20 OP + Triple_product__(keV_s/m3)______________________________________________ (dntau*te)____________________ 3.2275E+21 OP + Transport_loss_power_assumed_in_scaling_law_(MW)________________________ (powerht)_____________________ 2.9785E+02 OP + Switch_for_radiation_loss_term_usage_in_power_balance___________________ (iradloss)____________________ 1 + Radiation_power_subtracted_from_plasma_power_balance_(MW)_______________ ______________________________ 9.1650E+01 OP + Alpha_particle_confinement_time_(s)_____________________________________ (taup)________________________ 2.2270E+01 + Alpha_particle/energy_confinement_time_ratio____________________________ (taup/taueff)_________________ 6.9512E+00 + Lower_limit_on_taup/taueff______________________________________________ (taulimit)____________________ 5.0000E+00 + Total_energy_confinement_time_including_radiation_loss_(s)______________ (total_energy_conf_time)______ 2.8018E+00 + Normalized_plasma_pressure_beta_as_defined_by_McDonald_et_al____________ (beta_mcdonald)_______________ 3.4553E-02 OP + Normalized_ion_Larmor_radius____________________________________________ (rho_star)____________________ 1.9603E-03 OP + Normalized_collisionality_______________________________________________ (nu_star)_____________________ 3.7266E-03 OP + Volume_measure_of_elongation____________________________________________ (kappaa_IPB)__________________ 1.6815E+00 OP + Total_volt-second_requirement_(Wb)______________________________________ (vsstt)_______________________ 5.5616E+02 OP + Inductive_volt-seconds_(Wb)_____________________________________________ (vsind)_______________________ 2.3585E+02 OP + Ejima_coefficient_______________________________________________________ (gamma)_______________________ 3.0000E-01 + Start-up_resistive_(Wb)_________________________________________________ (vsres)_______________________ 5.0159E+01 OP + Flat-top_resistive_(Wb)_________________________________________________ (vsbrn)_______________________ 2.7015E+02 OP + bootstrap_current_fraction_multiplier___________________________________ (cboot)_______________________ 1.0000E+00 + Bootstrap_fraction_(ITER_1989)__________________________________________ (bscf_iter89)_________________ 3.7098E-01 + Bootstrap_fraction_(Sauter_et_al)_______________________________________ (bscf_sauter)_________________ 4.1920E-01 + Bootstrap_fraction_(Nevins_et_al)_______________________________________ (bscf_nevins)_________________ 3.5042E-01 + Bootstrap_fraction_(Wilson)_____________________________________________ (bscf_wilson)_________________ 4.3349E-01 + Diamagnetic_fraction_(Hender)___________________________________________ (diacf_hender)________________ 1.2017E-02 + Diamagnetic_fraction_(SCENE)____________________________________________ (diacf_scene)_________________ 1.1139E-02 + Pfirsch-Schlueter_fraction_(SCENE)______________________________________ (pscf_scene)__________________ -3.0283E-03 + Bootstrap_fraction_(enforced)___________________________________________ (bootipf.)____________________ 4.1920E-01 + Diamagnetic_fraction_(enforced)_________________________________________ (diaipf.)_____________________ 0.0000E+00 + Pfirsch-Schlueter_fraction_(enforced)___________________________________ (psipf.)______________________ 0.0000E+00 + Loop_voltage_during_burn_(V)____________________________________________ (vburn)_______________________ 3.7450E-02 OP + Plasma_resistance_(ohm)_________________________________________________ (rplas)_______________________ 3.9755E-09 OP + Resistive_diffusion_time_(s)____________________________________________ (res_time)____________________ 3.0619E+03 OP + Plasma_inductance_(H)___________________________________________________ (rlp)_________________________ 1.4181E-05 OP + Coefficient_for_sawtooth_effects_on_burn_V-s_requirement________________ (csawth)______________________ 1.0000E+00 + Ratio_of_He_and_pellet_particle_confinement_times_______________________ (tauratio)____________________ 1.0000E+00 + Fuelling_rate_(nucleus-pairs/s)_________________________________________ (qfuel)_______________________ 3.3420E+21 OP + Fuel_burn-up_rate_(reactions/s)_________________________________________ (rndfuel)_____________________ 5.7755E+20 OP + Burn-up_fraction________________________________________________________ (burnup)______________________ 1.7282E-01 + # Energy confinement times, and required H-factors : # + # Current Drive System # + Current_drive_efficiency_model__________________________________________ (iefrf)_______________________ 10 + Secondary_current_drive_efficiency_model________________________________ (iefrffix)____________________ 0 + Ratio_of_power_for_flat-top_to_start-up_(MW)____________________________ (startupratio)________________ 1.0000E+00 + Auxiliary_power_used_for_plasma_heating_only_(MW)_______________________ (pheat)_______________________ 7.5000E+01 + Power_injected_for_current_drive_(MW)___________________________________ (pcurrentdrivemw)_____________ 5.1429E+00 + Maximum_Allowed_Bootstrap_current_fraction______________________________ (bscfmax)_____________________ 9.5000E-01 + Fusion_gain_factor_Q____________________________________________________ (bigq)________________________ 2.0060E+01 OP + Auxiliary_current_drive_(A)_____________________________________________ (auxiliary_cd)________________ 2.3908E+05 OP + Current_drive_efficiency_(A/W)__________________________________________ (effcd)_______________________ 4.6488E-02 OP + Normalised_current_drive_efficiency,_gamma_(10^20_A/W-m2)_______________ (gamcd)_______________________ 3.0000E-01 OP + Wall_plug_to_injector_efficiency________________________________________ (etacd)_______________________ 5.0000E-01 + ECRH_plasma_heating_efficiency__________________________________________ (gamma_ecrh)__________________ 3.0000E-01 + Bootstrap_fraction______________________________________________________ (bootipf)_____________________ 4.1920E-01 + Diamagnetic_fraction____________________________________________________ (diaipf)______________________ 0.0000E+00 + Pfirsch-Schlueter_fraction______________________________________________ (psipf)_______________________ 0.0000E+00 + Auxiliary_current_drive_fraction________________________________________ (faccd)_______________________ 1.4376E-02 + Inductive_fraction______________________________________________________ (facoh)_______________________ 5.6642E-01 + Total___________________________________________________________________ (plasipf+faccd+facoh)_________ 1.0000E+00 + Fraction_of_the_plasma_current_produced_by_non-inductive_means__________ (fvsbrnni)____________________ 4.3358E-01 ITV + Electron_cyclotron_injected_power_(MW)__________________________________ (echpwr)______________________ 8.0143E+01 OP + Maximum_allowable_ECRH_power_(MW)_______________________________________ (pinjalw)_____________________ 2.0000E+02 + ECH_wall_plug_efficiency________________________________________________ (etaech)______________________ 5.0000E-01 + ECH_wall_plug_power_(MW)________________________________________________ (echwpow)_____________________ 1.6029E+02 OP + Total_V-s_capability_of_Central_Solenoid/PF_coils_(Wb)__________________ (abs(vstot))__________________ 5.7728E+02 + Required_volt-seconds_during_start-up_(Wb)______________________________ (vssoft)______________________ 2.8601E+02 + Available_volt-seconds_during_burn_(Wb)_________________________________ (vsmax)_______________________ 2.7014E+02 + # Times # + Initial_charge_time_for_CS_from_zero_current_(s)________________________ (tramp)_______________________ 5.0000E+02 + Plasma_current_ramp-up_time_(s)_________________________________________ (tohs)________________________ 1.6631E+02 + Heating_time_(s)________________________________________________________ (theat)_______________________ 1.0000E+01 + Burn_time_(s)___________________________________________________________ (tburn)_______________________ 7.2035E+03 OP + Reset_time_to_zero_current_for_CS_(s)___________________________________ (tqnch)_______________________ 1.6631E+02 + Time_between_pulses_(s)_________________________________________________ (tdwell)______________________ 1.8000E+03 + Total_plant_cycle_time_(s)______________________________________________ (tcycle)______________________ 9.8463E+03 OP + # Radial Build # + TF_coil_radial_placement_switch_________________________________________ (tf_in_cs)____________________ 0 + TF_coil_radial_placement_switch_________________________________________ (tf_in_cs)____________________ 0 + Machine_bore_(m)________________________________________________________ (bore)________________________ 1.9854E+00 ITV + CS_radial_thickness_(m)_________________________________________________ (ohcth)_______________________ 5.7587E-01 ITV + CS_precompression_(m)___________________________________________________ (precomp)_____________________ 6.8064E-02 + CS_precompresion_to_TF_coil_radial_gap_(m)______________________________ (gapoh)_______________________ 8.0000E-02 + TF_coil_inboard_leg_(m)_________________________________________________ (tfcth)_______________________ 9.1597E-01 ITV + TF_coil_inboard_leg_insulation_gap_(m)__________________________________ (tftsgap)_____________________ 5.0000E-02 + Thermal_shield,_inboard_(m)_____________________________________________ (thshield_ib)_________________ 5.0000E-02 + thermal_shield_to_vessel_radial_gap_(m)_________________________________ (gapds)_______________________ 2.0000E-02 + Inboard_vacuum_vessel_radial_thickness_(m)______________________________ (d_vv_in)_____________________ 3.0000E-01 + Inner_radiation_shield_radial_thickness_(m)_____________________________ (shldith)_____________________ 3.0000E-01 + Gap_(m)_________________________________________________________________ (vvblgap)_____________________ 2.0000E-02 + Inboard_blanket_radial_thickness_(m)____________________________________ (blnkith)_____________________ 7.0000E-01 + Inboard_first_wall_radial_thickness_(m)_________________________________ (fwith)_______________________ 1.8000E-02 + Inboard_scrape-off_radial_thickness_(m)_________________________________ (scrapli)_____________________ 2.5000E-01 + Outboard_scrape-off_radial_thickness_(m)________________________________ (scraplo)_____________________ 2.5000E-01 + Outboard_first_wall_radial_thickness_(m)________________________________ (fwoth)_______________________ 1.8000E-02 + Outboard_blanket_radial_thickness_(m)___________________________________ (blnkoth)_____________________ 1.0000E+00 + Outer_radiation_shield_radial_thickness_(m)_____________________________ (shldoth)_____________________ 8.0000E-01 + Outboard_vacuum_vessel_radial_thickness_(m)_____________________________ (d_vv_out)____________________ 3.0000E-01 + Vessel_to_TF_radial_gap_(m)_____________________________________________ (gapsto)______________________ 1.3720E+00 + Thermal_shield,_outboard_(m)____________________________________________ (thshield_ob)_________________ 5.0000E-02 + Gap_(m)_________________________________________________________________ (tftsgap)_____________________ 5.0000E-02 + TF_coil_outboard_leg_radial_thickness_(m)_______________________________ (tfthko)______________________ 9.1597E-01 + # Vertical Build # + Divertor_null_switch____________________________________________________ (i_single_null)_______________ 1 + Vessel_-_TF_coil_vertical_gap_(m)_______________________________________ (vgap2)_______________________ 1.6300E-01 + Topside_vacuum_vessel_radial_thickness_(m)______________________________ (d_vv_top)____________________ 3.0000E-01 + Top_radiation_shield_thickness_(m)______________________________________ (shldtth)_____________________ 6.0000E-01 + Top_blanket_vertical_thickness_(m)______________________________________ (blnktth)_____________________ 8.5000E-01 + Top_first_wall_vertical_thickness_(m)___________________________________ (fwtth)_______________________ 1.8000E-02 + Top_scrape-off_vertical_thickness_(m)___________________________________ (vgaptop)_____________________ 6.0000E-01 + Plasma_half-height_(m)__________________________________________________ (rminor*kappa)________________ 4.9333E+00 + Bottom_scrape-off_vertical_thickness_(m)________________________________ (vgap)________________________ 2.0019E+00 + Divertor_structure_vertical_thickness_(m)_______________________________ (divfix)______________________ 6.2000E-01 + Bottom_radiation_shield_thickness_(m)___________________________________ (shldlth)_____________________ 7.0000E-01 + Underside_vacuum_vessel_radial_thickness_(m)____________________________ (d_vv_bot)____________________ 3.0000E-01 + External_cryostat_thickness_(m)_________________________________________ (ddwex)_______________________ 1.5000E-01 + Ratio_of_Central_solenoid_height_to_TF_coil_internal_height_____________ (ohhghf)______________________ 9.0000E-01 + Width_of_neutral_beam_duct_where_it_passes_between_the_TF_coils_(m)_____ (beamwd)______________________ 5.8000E-01 + # Divertor build and plasma position # + Plasma_top_position,_radial_(m)_________________________________________ (ptop_radial)_________________ 6.6667E+00 + Plasma_top_position,_vertical_(m)_______________________________________ (ptop_vertical)_______________ 4.9333E+00 + Plasma_geometric_centre,_radial_(m)_____________________________________ (physics_variables.rmajor.)___ 8.0000E+00 + Plasma_geometric_centre,_vertical_(m)___________________________________ (0.0)_________________________ 0.0000E+00 + Plasma_lower_physics_variables.triangularity____________________________ (tril)________________________ 5.0000E-01 + Plasma_elongation_______________________________________________________ (physics_variables.kappa.)____ 1.8500E+00 + TF_coil_vertical_offset_(m)_____________________________________________ (tfoffset)____________________ -6.1694E-01 + Plasma_outer_arc_radius_of_curvature_(m)________________________________ (rco)_________________________ 5.0422E+00 + Plasma_inner_arc_radius_of_curvature_(m)________________________________ (rci)_________________________ 9.7933E+00 + Plasma_lower_X-pt,_radial_(m)___________________________________________ (rxpt)________________________ 6.6667E+00 + Plasma_lower_X-pt,_vertical_(m)_________________________________________ (zxpt)________________________ -4.9333E+00 + Poloidal_plane_angle_between_vertical_and_inner_leg_(rad)_______________ (thetai)______________________ 2.0820E-01 + Poloidal_plane_angle_between_vertical_and_outer_leg_(rad)_______________ (thetao)______________________ 1.0429E+00 + Poloidal_plane_angle_between_inner_leg_and_plate_(rad)__________________ (betai)_______________________ 1.0000E+00 + Poloidal_plane_angle_between_outer_leg_and_plate_(rad)__________________ (betao)_______________________ 1.0000E+00 + Inner_divertor_leg_poloidal_length_(m)__________________________________ (plsepi)______________________ 1.0000E+00 + Outer_divertor_leg_poloidal_length_(m)__________________________________ (plsepo)______________________ 1.5000E+00 + Inner_divertor_plate_length_(m)_________________________________________ (plleni)______________________ 1.0000E+00 + Outer_divertor_plate_length_(m)_________________________________________ (plleno)______________________ 1.0000E+00 + Inner_strike_point,_radial_(m)__________________________________________ (rspi)________________________ 5.6883E+00 + Inner_strike_point,_vertical_(m)________________________________________ (zspi)________________________ -5.1400E+00 + Inner_plate_top,_radial_(m)_____________________________________________ (rplti)_______________________ 5.8656E+00 + Inner_plate_top,_vertical_(m)___________________________________________ (zplti)_______________________ -4.6725E+00 + Inner_plate_bottom,_radial_(m)__________________________________________ (rplbi)_______________________ 5.5109E+00 + Inner_plate_bottom,_vertical_(m)________________________________________ (zplbi)_______________________ -5.6075E+00 + Outer_strike_point,_radial_(m)__________________________________________ (rspo)________________________ 7.4223E+00 + Outer_strike_point,_vertical_(m)________________________________________ (zspo)________________________ -6.2291E+00 + Outer_plate_top,_radial_(m)_____________________________________________ (rplto)_______________________ 7.6496E+00 + Outer_plate_top,_vertical_(m)___________________________________________ (zplto)_______________________ -5.7838E+00 + Outer_plate_bottom,_radial_(m)__________________________________________ (rplbo)_______________________ 7.1949E+00 + Outer_plate_bottom,_vertical_(m)________________________________________ (zplbo)_______________________ -6.6744E+00 + Calculated_maximum_divertor_height_(m)__________________________________ (divht)_______________________ 2.0019E+00 + # TF coils # + Allowable_maximum_shear_stress_in_TF_coil_case_(Tresca_criterion)_(Pa)__ (sig_tf_case_max)_____________ 7.5000E+08 + Allowable_maximum_shear_stress_in_TF_coil_conduit_(Tresca_criterion)_(Pa (sig_tf_wp_max)_______________ 7.5000E+08 + WP_transverse_modulus_(GPa)_____________________________________________ (eyoung_wp_trans*1.0d-9)______ 4.3534E+01 OP + WP_vertical_modulus_(GPa)_______________________________________________ (eyoung_wp_axial*1.0d-9)______ 1.1510E+02 OP + WP_transverse_Poissons_ratio____________________________________________ (poisson_wp_trans)____________ 3.0390E-01 OP + WP_vertical-transverse_Pois._rat._______________________________________ (poisson_wp_axial)____________ 3.1568E-01 OP + Radial____stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_r_max(1))_____________ 4.8849E-08 + toroidal__stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_t_max(1))_____________ -4.8724E+08 + Vertical__stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_z_max(1))_____________ 2.6028E+08 + Von-Mises_stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_vmises_max(1))________ 6.5725E+08 + Maximum_shear_stress_for_the_Tresca_yield_criterion_1_(Pa)______________ (sig_tf_tresca_max(1))________ 7.4752E+08 + Radial____stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_r_max(2))_____________ -1.5411E+08 + toroidal__stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_t_max(2))_____________ -3.7861E+08 + Vertical__stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_z_max(2))_____________ 2.6028E+08 + Von-Mises_stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_vmises_max(2))________ 5.5645E+08 + Maximum_shear_stress_for_the_Tresca_yield_criterion_2_(Pa)______________ (sig_tf_tresca_max(2))________ 6.3889E+08 + Radial____stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_r_max(3))_____________ 6.1398E+06 + toroidal__stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_t_max(3))_____________ -3.6314E+08 + Vertical__stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_z_max(3))_____________ 1.4510E+08 + Von-Mises_stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_vmises_max(3))________ 4.5345E+08 + Maximum_shear_stress_for_the_Tresca_yield_criterion_3_(Pa)______________ (sig_tf_tresca_max(3))________ 5.0824E+08 + Maximum_radial_deflection_at_midplane_(m)_______________________________ (deflect)_____________________ -6.2714E-03 OP + Vertical_strain_on_casing_______________________________________________ (casestr)_____________________ 1.2697E-03 OP + Radial_strain_on_insulator______________________________________________ (insstrain)___________________ -7.6923E-03 OP + Conductor_technology____________________________________________________ (i_tf_sup)____________________ 1 + Superconductor_material_________________________________________________ (i_tf_sc_mat)_________________ 1 + Presence_of_TF_demountable_joints_______________________________________ (itart)_______________________ 0 + TF_inboard_leg_support_strategy_________________________________________ (i_tf_bucking)________________ 1 + Number_of_TF_coils______________________________________________________ (n_tf)________________________ 16 + Inboard_leg_centre_radius_(m)___________________________________________ (r_tf_inboard_mid)____________ 3.1673E+00 OP + Outboard_leg_centre_radius_(m)__________________________________________ (r_tf_outboard_mid)___________ 1.4985E+01 OP + Total_inboard_leg_radial_thickness_(m)__________________________________ (tfcth)_______________________ 9.1597E-01 ITV + Total_outboard_leg_radial_thickness_(m)_________________________________ (tfthko)______________________ 9.1597E-01 + Outboard_leg_toroidal_thickness_(m)_____________________________________ (tftort)______________________ 1.4145E+00 OP + Maximum_inboard_edge_height_(m)_________________________________________ (hmax)________________________ 8.8182E+00 OP + Mean_coil_circumference_(including_inboard_leg_length)_(m)______________ (tfleng)______________________ 4.7937E+01 OP + Vertical_TF_shape_______________________________________________________ (i_tf_shape)__________________ 1 + TF_coil_arc_point_0_R_(m)_______________________________________________ (xarc(1))_____________________ 3.6253E+00 + TF_coil_arc_point_0_Z_(m)_______________________________________________ (yarc(1))_____________________ 4.5506E+00 + TF_coil_arc_point_1_R_(m)_______________________________________________ (xarc(2))_____________________ 7.4667E+00 + TF_coil_arc_point_1_Z_(m)_______________________________________________ (yarc(2))_____________________ 7.5843E+00 + TF_coil_arc_point_2_R_(m)_______________________________________________ (xarc(3))_____________________ 1.4527E+01 + TF_coil_arc_point_2_Z_(m)_______________________________________________ (yarc(3))_____________________ 0.0000E+00 + TF_coil_arc_point_3_R_(m)_______________________________________________ (xarc(4))_____________________ 7.4667E+00 + TF_coil_arc_point_3_Z_(m)_______________________________________________ (yarc(4))_____________________ -8.8182E+00 + TF_coil_arc_point_4_R_(m)_______________________________________________ (xarc(5))_____________________ 3.6253E+00 + TF_coil_arc_point_4_Z_(m)_______________________________________________ (yarc(5))_____________________ -5.2909E+00 + TF_cross-section_(total)_(m2)___________________________________________ (tfareain)____________________ 1.8229E+01 + Total_steel_cross-section_(m2)__________________________________________ (a_tf_steel*n_tf)_____________ 1.2853E+01 + Total_steel_TF_fraction_________________________________________________ (f_tf_steel)__________________ 7.0508E-01 + Total_Insulation_cross-section_(total)_(m2)_____________________________ (a_tf_ins*n_tf)_______________ 8.4752E-01 + Total_Insulation_fraction_______________________________________________ (f_tf_ins)____________________ 4.6493E-02 + Casing_cross_section_area_(per_leg)_(m2)________________________________ (acasetf)_____________________ 5.6444E-01 + Inboard_leg_case_plasma_side_wall_thickness_(m)_________________________ (casthi)______________________ 6.0000E-02 + Inboard_leg_case_inboard_"nose"_thickness_(m)___________________________ (thkcas)______________________ 2.8216E-01 ITV + Inboard_leg_case_sidewall_thickness_at_its_narrowest_point_(m)__________ (casths)______________________ 5.0000E-02 + External_case_mass_per_coil_(kg)________________________________________ (whtcas)______________________ 5.5456E+05 OP + WP_cross_section_area_with_insulation_and_insertion_(per_coil)_(m2)_____ (awpc)________________________ 5.7486E-01 + WP_cross_section_area_(per_coil)_(m2)___________________________________ (aswp)________________________ 5.1696E-01 + Winding_pack_radial_thickness_(m)_______________________________________ (dr_tf_wp)____________________ 5.0416E-01 ITV + Winding_pack_toroidal_width_1_(m)_______________________________________ (wwp1)________________________ 1.1904E+00 OP + Winding_pack_toroidal_width_2_(m)_______________________________________ (wwp2)________________________ 1.0901E+00 OP + Ground_wall_insulation_thickness_(m)____________________________________ (tinstf)______________________ 8.0000E-03 + Winding_pack_insertion_gap_(m)__________________________________________ (tfinsgap)____________________ 1.0000E-02 + Steel_WP_cross-section_(total)_(m2)_____________________________________ (aswp*n_tf)___________________ 3.8217E+00 + Steel_WP_fraction_______________________________________________________ (aswp/awpc)___________________ 4.1550E-01 + Insulation_WP_fraction__________________________________________________ (aiwp/awpc)___________________ 4.7934E-02 + Cable_WP_fraction_______________________________________________________ ((awpc-aswp-aiwp)/awpc)_______ 5.3656E-01 + Turn_parametrisation____________________________________________________ (i_tf_turns_integer)__________ 0 + Number_of_turns_per_TF_coil_____________________________________________ (n_tf_turn)___________________ 1.4739E+02 OP + Width_of_turn_including_inter-turn_insulation_(m)_______________________ (t_turn_tf)___________________ 5.9223E-02 OP + Width_of_conductor_(square)_(m)_________________________________________ (t_conductor)_________________ 5.7623E-02 OP + Width_of_space_inside_conductor_(m)_____________________________________ (t_cable)_____________________ 4.1604E-02 OP + Steel_conduit_thickness_(m)_____________________________________________ (thwcndut)____________________ 8.0099E-03 ITV + Inter-turn_insulation_thickness_(m)_____________________________________ (thicndut)____________________ 8.0000E-04 + Diameter_of_central_helium_channel_in_cable_____________________________ (dhecoil)_____________________ 1.0000E-02 + internal_area_of_the_cable_space________________________________________ (acstf)_______________________ 1.6999E-03 + Coolant_fraction_in_conductor_excluding_central_channel_________________ (vftf)________________________ 3.0000E-01 + Copper_fraction_of_conductor____________________________________________ (fcutfsu)_____________________ 8.4212E-01 ITV + Superconductor_fraction_of_conductor____________________________________ (1-fcutfsu)___________________ 1.5788E-01 + Check_total_area_fractions_in_winding_pack_=_1__________________________ ______________________________ 1.0000E+00 + minimum_TF_conductor_temperature_margin__(K)____________________________ (tmargmin_tf)_________________ 1.5000E+00 + TF_conductor_temperature_margin_(K)_____________________________________ (tmargtf)_____________________ 1.5049E+00 + Elastic_properties_behavior_____________________________________________ (i_tf_cond_eyoung_axial)______ 0 + Conductor_axial_Youngs_modulus__________________________________________ (eyoung_cond_axial)___________ 0.0000E+00 + Conductor_transverse_Youngs_modulus_____________________________________ (eyoung_cond_trans)___________ 0.0000E+00 + Superconductor_mass_per_coil_(kg)_______________________________________ (whtconsc)____________________ 4.6964E+03 OP + Copper_mass_per_coil_(kg)_______________________________________________ (whtconcu)____________________ 5.8073E+04 OP + Steel_conduit_mass_per_coil_(kg)________________________________________ (whtconsh)____________________ 8.9310E+04 OP + Conduit_insulation_mass_per_coil_(kg)___________________________________ (whtconin)____________________ 2.3777E+03 OP + Total_conduit_mass_per_coil_(kg)________________________________________ (whtcon)______________________ 1.5446E+05 OP + Mass_of_each_TF_coil_(kg)_______________________________________________ (whttf/n_tf)__________________ 7.1402E+05 OP + Total_TF_coil_mass_(kg)_________________________________________________ (whttf)_______________________ 1.1424E+07 OP + Nominal_peak_field_assuming_toroidal_symmetry_(T)_______________________ (bmaxtf)______________________ 1.2178E+01 OP + Total_current_in_all_TF_coils_(MA)______________________________________ (ritfc/1.D6)__________________ 2.1176E+02 OP + TF_coil_current_(summed_over_all_coils)_(A)_____________________________ (ritfc)_______________________ 2.1176E+08 + Actual_peak_field_at_discrete_conductor_(T)_____________________________ (bmaxtfrp)____________________ 1.2636E+01 OP + Winding_pack_current_density_(A/m2)_____________________________________ (jwptf)_______________________ 2.5602E+07 OP + Inboard_leg_mid-plane_conductor_current_density_(A/m2)__________________ (oacdcp)______________________ 1.1617E+07 + Total_stored_energy_in_TF_coils_(GJ)____________________________________ (estotftgj)___________________ 1.2161E+02 OP + Inboard_vertical_tension_per_coil_(N)___________________________________ (vforce)______________________ 2.0908E+08 OP + Outboard_vertical_tension_per_coil_(N)__________________________________ (vforce_outboard)_____________ 2.0908E+08 OP + inboard_vertical_tension_fraction_(-)___________________________________ (f_vforce_inboard)____________ 5.0000E-01 OP + Centring_force_per_coil_(N/m)___________________________________________ (cforce)______________________ 8.0590E+07 OP + Max_allowed_tfcoil_variables.ripple_amplitude_at_plasma_outboard_midplan (ripmax)______________________ 6.0000E-01 + Ripple_amplitude_at_plasma_outboard_midplane_(%)________________________ (ripple)______________________ 6.0000E-01 OP + Actual_quench_time_(or_time_constant)_(s)_______________________________ (tdmptf)______________________ 1.8429E+01 ITV + Vacuum_Vessel_stress_on_quench_(Pa)_____________________________________ (vv_stress_quench)____________ 6.1442E+07 OP + Maximum_allowed_voltage_during_quench_due_to_insulation_(kV)____________ (vdalw)_______________________ 9.5837E+00 ITV + Actual_quench_voltage_(kV)______________________________________________ (vtfskv)______________________ 9.1862E+00 OP + Maximum_allowed_temp_rise_during_a_quench_(K)___________________________ (tmaxpro)_____________________ 1.5000E+02 + # Superconducting TF Coils # + Superconductor_switch___________________________________________________ (isumat)______________________ 1 + Critical_field_at_zero_temperature_and_strain_(T)_______________________ (bc20m)_______________________ 3.2970E+01 + Critical_temperature_at_zero_field_and_strain_(K)_______________________ (tc0m)________________________ 1.6060E+01 + Helium_temperature_at_peak_field_(=_superconductor_temperature)_(K)_____ (thelium)_____________________ 4.7500E+00 + Total_helium_fraction_inside_cable_space________________________________ (fhetot)______________________ 3.4620E-01 OP + Copper_fraction_of_conductor____________________________________________ (fcutfsu)_____________________ 8.4212E-01 ITV + Residual_manufacturing_strain_on_superconductor_________________________ (str_tf_con_res)______________ -5.0000E-03 + Self-consistent_strain_on_superconductor________________________________ (str_wp)______________________ 2.0730E-03 + Critical_current_density_in_superconductor_(A/m2)_______________________ (jcritsc)_____________________ 7.1337E+08 OP + Critical_current_density_in_strand_(A/m2)_______________________________ (jcritstr)____________________ 1.1263E+08 OP + Critical_current_density_in_winding_pack_(A/m2)_________________________ (jwdgcrt)_____________________ 3.5688E+07 OP + Actual_current_density_in_winding_pack_(A/m2)___________________________ (jwdgop)______________________ 2.5602E+07 OP + Minimum_allowed_temperature_margin_in_superconductor_(K)________________ (tmargmin_tf)_________________ 1.5000E+00 + Actual_temperature_margin_in_superconductor_(K)_________________________ (tmarg)_______________________ 1.5049E+00 OP + Critical_current_(A)____________________________________________________ (icrit)_______________________ 1.2517E+05 OP + Actual_current_(A)______________________________________________________ (cpttf)_______________________ 8.9795E+04 ITV + Actual_current_/_critical_current_______________________________________ (iooic)_______________________ 7.1737E-01 OP + # Central Solenoid and PF Coils # + Central_solenoid_superconductor_material________________________________ (isumatoh)____________________ 1 + Maximum_field_at_Beginning_Of_Pulse_(T)_________________________________ (bmaxoh0)_____________________ 1.4050E+01 OP + Critical_superconductor_current_density_at_BOP_(A/m2)___________________ (jscoh_bop)___________________ 3.4918E+08 OP + Critical_strand_current_density_at_BOP_(A/m2)___________________________ (jstrandoh_bop)_______________ 1.0475E+08 OP + Allowable_overall_current_density_at_BOP_(A/m2)_________________________ (rjohc0)______________________ 3.5294E+07 OP + Actual_overall_current_density_at_BOP_(A/m2)____________________________ (cohbop)______________________ 1.9126E+07 OP + Maximum_field_at_End_Of_Flattop_(T)_____________________________________ (bmaxoh)______________________ 1.3920E+01 OP + Critical_superconductor_current_density_at_EOF_(A/m2)___________________ (jscoh_eof)___________________ 3.6097E+08 OP + Critical_strand_current_density_at_EOF_(A/m2)___________________________ (jstrandoh_eof)_______________ 1.0829E+08 OP + Allowable_overall_current_density_at_EOF_(A/m2)_________________________ (rjohc)_______________________ 3.6485E+07 OP + Actual_overall_current_density_at_EOF_(A/m2)____________________________ (coheof)______________________ 2.0264E+07 ITV + CS_inside_radius_(m)____________________________________________________ (bore)________________________ 1.9854E+00 ITV + CS_thickness_(m)________________________________________________________ (ohcth)_______________________ 5.7587E-01 ITV + Gap_between_central_solenoid_and_TF_coil_(m)____________________________ (gapoh)_______________________ 8.0000E-02 + CS_overall_cross-sectional_area_(m2)____________________________________ (areaoh)______________________ 9.1407E+00 OP + CS_conductor+void_cross-sectional_area_(m2)_____________________________ (awpoh)_______________________ 4.3996E+00 OP + ___CS_conductor_cross-sectional_area_(m2)_______________________________ (awpoh*(1-vfohc))_____________ 3.0797E+00 OP + ___CS_void_cross-sectional_area_(m2)____________________________________ (awpoh*vfohc)_________________ 1.3199E+00 OP + CS_steel_cross-sectional_area_(m2)______________________________________ (areaoh-awpoh)________________ 4.7411E+00 OP + CS_steel_area_fraction__________________________________________________ (oh_steel_frac)_______________ 5.1868E-01 ITV + Switch_for_CS_stress_calculation________________________________________ (i_cs_stress)_________________ 0 + Allowable_stress_in_CS_steel_(Pa)_______________________________________ (alstroh)_____________________ 7.5000E+08 + Hoop_stress_in_CS_steel_(Pa)____________________________________________ (sig_hoop)____________________ 6.7569E+08 OP + Axial_stress_in_CS_steel_(Pa)___________________________________________ (sig_axial)___________________ -7.6205E+08 OP + Maximum_shear_stress_in_CS_steel_for_the_Tresca_criterion_(Pa)__________ (s_tresca_oh)_________________ 6.7569E+08 OP + Axial_force_in_CS_(N)___________________________________________________ (axial_force)_________________ -1.6256E+09 OP + Residual_manufacturing_strain_in_CS_superconductor_material_____________ (tfcoil_variables.str_cs_con_r -5.0000E-03 + Copper_fraction_in_strand_______________________________________________ (fcuohsu)_____________________ 7.0000E-01 + Void_(coolant)_fraction_in_conductor____________________________________ (vfohc)_______________________ 3.0000E-01 + Helium_coolant_temperature_(K)__________________________________________ (tftmp)_______________________ 4.7500E+00 + CS_temperature_margin_(K)_______________________________________________ (tmargoh)_____________________ 1.5052E+00 OP + Minimum_permitted_temperature_margin_(K)________________________________ (tmargmin_cs)_________________ 1.5000E+00 + Residual_hoop_stress_in_CS_Steel_(Pa)___________________________________ (residual_sig_hoop)___________ 2.4000E+08 + Minimum_burn_time_(s)___________________________________________________ (tbrnmn)______________________ 7.2000E+03 + Initial_vertical_crack_size_(m)_________________________________________ (t_crack_vertical)____________ 8.9000E-04 + Initial_radial_crack_size_(m)___________________________________________ (t_crack_radial)______________ 2.6700E-03 + CS_turn_area_(m)________________________________________________________ (a_oh_turn)___________________ 1.9739E-03 + CS_turn_length_(m)______________________________________________________ (l_cond_cst)__________________ 7.6953E-02 + CS_turn_internal_cable_space_radius_(m)_________________________________ (r_in_cst)____________________ 7.4740E-03 + CS_turn_width_(m)_______________________________________________________ (d_cond_cst)__________________ 2.5651E-02 + CS_structural_vertical_thickness_(m)____________________________________ (t_structural_vertical)_______ 5.3514E-03 + CS_structural_radial_thickness_(m)______________________________________ (t_structural_radial)_________ 5.3514E-03 + Allowable_number_of_cycles_till_CS_fracture_____________________________ (n_cycle)_____________________ 1.3378E+02 OP + Minimum_number_of_cycles_required_till_CS_fracture______________________ (n_cycle_min)_________________ 2.0000E+04 OP + PF_coil_superconductor_material_________________________________________ (isumatpf)____________________ 3 + Copper_fraction_in_conductor____________________________________________ (fcupfsu)_____________________ 6.9000E-01 + Maximum_permissible_tensile_stress_(MPa)________________________________ (sigpfcalw)___________________ 5.0000E+02 + JxB_hoop_force_fraction_supported_by_case_______________________________ (sigpfcf)_____________________ 6.6600E-01 + PF_coil_0_radius_(m)____________________________________________________ (rpf[0]_______________________ 5.5667E+00 + PF_coil_0_vertical_position_(m)_________________________________________ (zpf[0])______________________ 9.3603E+00 + PF_coil_0_radial_thickness_(m)__________________________________________ (pfdr(0))_____________________ 1.2727E+00 + PF_coil_0_vertical_thickness_(m)________________________________________ (pfdz(0))_____________________ 1.2727E+00 + PF_coil_0_turns_________________________________________________________ (turns[0])____________________ 4.4541E+02 + PF_coil_0_current_(MA)__________________________________________________ (ric[0])______________________ 1.7816E+01 + PF_coil_0_field_(T)_____________________________________________________ (bpf[0])______________________ 6.2280E+00 + PF_coil_1_radius_(m)____________________________________________________ (rpf[1]_______________________ 5.5667E+00 + PF_coil_1_vertical_position_(m)_________________________________________ (zpf[1])______________________ -1.0594E+01 + PF_coil_1_radial_thickness_(m)__________________________________________ (pfdr(1))_____________________ 1.3651E+00 + PF_coil_1_vertical_thickness_(m)________________________________________ (pfdz(1))_____________________ -1.3651E+00 + PF_coil_1_turns_________________________________________________________ (turns[1])____________________ 5.1248E+02 + PF_coil_1_current_(MA)__________________________________________________ (ric[1])______________________ 2.0499E+01 + PF_coil_1_field_(T)_____________________________________________________ (bpf[1])______________________ 6.6990E+00 + PF_coil_2_radius_(m)____________________________________________________ (rpf[2]_______________________ 1.6731E+01 + PF_coil_2_vertical_position_(m)_________________________________________ (zpf[2])______________________ 2.6667E+00 + PF_coil_2_radial_thickness_(m)__________________________________________ (pfdr(2))_____________________ 1.1332E+00 + PF_coil_2_vertical_thickness_(m)________________________________________ (pfdz(2))_____________________ 1.1332E+00 + PF_coil_2_turns_________________________________________________________ (turns[2])____________________ 1.9262E+02 + PF_coil_2_current_(MA)__________________________________________________ (ric[2])______________________ -7.7049E+00 + PF_coil_2_field_(T)_____________________________________________________ (bpf[2])______________________ 2.6389E+00 + PF_coil_3_radius_(m)____________________________________________________ (rpf[3]_______________________ 1.6731E+01 + PF_coil_3_vertical_position_(m)_________________________________________ (zpf[3])______________________ -2.6667E+00 + PF_coil_3_radial_thickness_(m)__________________________________________ (pfdr(3))_____________________ 1.1332E+00 + PF_coil_3_vertical_thickness_(m)________________________________________ (pfdz(3))_____________________ -1.1332E+00 + PF_coil_3_turns_________________________________________________________ (turns[3])____________________ 1.9262E+02 + PF_coil_3_current_(MA)__________________________________________________ (ric[3])______________________ -7.7049E+00 + PF_coil_3_field_(T)_____________________________________________________ (bpf[3])______________________ 2.6389E+00 + PF_coil_4_radius_(m)____________________________________________________ (rpf[4]_______________________ 1.5209E+01 + PF_coil_4_vertical_position_(m)_________________________________________ (zpf[4])______________________ 7.4667E+00 + PF_coil_4_radial_thickness_(m)__________________________________________ (pfdr(4))_____________________ 8.0773E-01 + PF_coil_4_vertical_thickness_(m)________________________________________ (pfdz(4))_____________________ 8.0773E-01 + PF_coil_4_turns_________________________________________________________ (turns[4])____________________ 1.3049E+02 + PF_coil_4_current_(MA)__________________________________________________ (ric[4])______________________ -5.2194E+00 + PF_coil_4_field_(T)_____________________________________________________ (bpf[4])______________________ 2.5737E+00 + PF_coil_5_radius_(m)____________________________________________________ (rpf[5]_______________________ 1.5209E+01 + PF_coil_5_vertical_position_(m)_________________________________________ (zpf[5])______________________ -7.4667E+00 + PF_coil_5_radial_thickness_(m)__________________________________________ (pfdr(5))_____________________ 8.0773E-01 + PF_coil_5_vertical_thickness_(m)________________________________________ (pfdz(5))_____________________ -8.0773E-01 + PF_coil_5_turns_________________________________________________________ (turns[5])____________________ 1.3049E+02 + PF_coil_5_current_(MA)__________________________________________________ (ric[5])______________________ -5.2194E+00 + PF_coil_5_field_(T)_____________________________________________________ (bpf[5])______________________ 2.5737E+00 + Central_solenoid_radius_(m)_____________________________________________ (rpf[nohc-1])_________________ 2.2734E+00 + Central_solenoid_vertical_position_(m)__________________________________ (zpf[nohc-1])_________________ 0.0000E+00 + Central_solenoid_radial_thickness_(m)___________________________________ (ohdr)________________________ 5.7587E-01 + Central_solenoid_vertical_thickness_(m)_________________________________ (ohdz)________________________ 1.5873E+01 + Central_solenoid_turns__________________________________________________ (turns[nohc-1])_______________ 4.6308E+03 + Central_solenoid_current_(MA)___________________________________________ (ric[nohc-1])_________________ -1.8523E+02 + Central_solenoid_field_(T)______________________________________________ (bpf[nohc-1])_________________ 1.4050E+01 + Sum_of_squares_of_residuals_____________________________________________ (ssq0)________________________ 3.5207E-04 OP + Smoothing_parameter_____________________________________________________ (alfapf)______________________ 5.0000E-10 + # Volt Second Consumption # + Total_volt-second_consumption_by_coils_(Wb)_____________________________ (vstot)_______________________ -5.8000E+02 OP + # Waveforms # + Ratio_of_central_solenoid_current_at_beginning_of_Pulse_/_end_of_flat-to (fcohbop)_____________________ 9.4380E-01 ITV + Ratio_of_central_solenoid_current_at_beginning_of_Flat-top_/_end_of_flat (fcohbof)_____________________ -1.4083E-01 OP + # PF Circuit Waveform Data # + Number_of_PF_circuits_including_CS_and_plasma___________________________ (ncirt)_______________________ 8 + PF_Circuit_0_Time_point_0_(A)___________________________________________ (pfc0t0)______________________ 0.0000E+00 + PF_Circuit_0_Time_point_1_(A)___________________________________________ (pfc0t1)______________________ 1.3971E+07 + PF_Circuit_0_Time_point_2_(A)___________________________________________ (pfc0t2)______________________ 1.7816E+07 + PF_Circuit_0_Time_point_3_(A)___________________________________________ (pfc0t3)______________________ 1.7816E+07 + PF_Circuit_0_Time_point_4_(A)___________________________________________ (pfc0t4)______________________ 9.2844E+05 + PF_Circuit_0_Time_point_5_(A)___________________________________________ (pfc0t5)______________________ 0.0000E+00 + PF_Circuit_1_Time_point_0_(A)___________________________________________ (pfc1t0)______________________ 0.0000E+00 + PF_Circuit_1_Time_point_1_(A)___________________________________________ (pfc1t1)______________________ 1.8269E+07 + PF_Circuit_1_Time_point_2_(A)___________________________________________ (pfc1t2)______________________ 2.0499E+07 + PF_Circuit_1_Time_point_3_(A)___________________________________________ (pfc1t3)______________________ 2.0499E+07 + PF_Circuit_1_Time_point_4_(A)___________________________________________ (pfc1t4)______________________ -1.5831E+06 + PF_Circuit_1_Time_point_5_(A)___________________________________________ (pfc1t5)______________________ 0.0000E+00 + PF_Circuit_2_Time_point_0_(A)___________________________________________ (pfc2t0)______________________ -0.0000E+00 + PF_Circuit_2_Time_point_1_(A)___________________________________________ (pfc2t1)______________________ 4.9542E+05 + PF_Circuit_2_Time_point_2_(A)___________________________________________ (pfc2t2)______________________ -7.1060E+06 + PF_Circuit_2_Time_point_3_(A)___________________________________________ (pfc2t3)______________________ -7.1060E+06 + PF_Circuit_2_Time_point_4_(A)___________________________________________ (pfc2t4)______________________ -7.7049E+06 + PF_Circuit_2_Time_point_5_(A)___________________________________________ (pfc2t5)______________________ -0.0000E+00 + PF_Circuit_3_Time_point_0_(A)___________________________________________ (pfc3t0)______________________ -0.0000E+00 + PF_Circuit_3_Time_point_1_(A)___________________________________________ (pfc3t1)______________________ 4.9542E+05 + PF_Circuit_3_Time_point_2_(A)___________________________________________ (pfc3t2)______________________ -7.1060E+06 + PF_Circuit_3_Time_point_3_(A)___________________________________________ (pfc3t3)______________________ -7.1060E+06 + PF_Circuit_3_Time_point_4_(A)___________________________________________ (pfc3t4)______________________ -7.7049E+06 + PF_Circuit_3_Time_point_5_(A)___________________________________________ (pfc3t5)______________________ -0.0000E+00 + PF_Circuit_4_Time_point_0_(A)___________________________________________ (pfc4t0)______________________ -0.0000E+00 + PF_Circuit_4_Time_point_1_(A)___________________________________________ (pfc4t1)______________________ 3.2650E+05 + PF_Circuit_4_Time_point_2_(A)___________________________________________ (pfc4t2)______________________ -4.8247E+06 + PF_Circuit_4_Time_point_3_(A)___________________________________________ (pfc4t3)______________________ -4.8247E+06 + PF_Circuit_4_Time_point_4_(A)___________________________________________ (pfc4t4)______________________ -5.2194E+06 + PF_Circuit_4_Time_point_5_(A)___________________________________________ (pfc4t5)______________________ -0.0000E+00 + PF_Circuit_5_Time_point_0_(A)___________________________________________ (pfc5t0)______________________ -0.0000E+00 + PF_Circuit_5_Time_point_1_(A)___________________________________________ (pfc5t1)______________________ 3.2650E+05 + PF_Circuit_5_Time_point_2_(A)___________________________________________ (pfc5t2)______________________ -4.8247E+06 + PF_Circuit_5_Time_point_3_(A)___________________________________________ (pfc5t3)______________________ -4.8247E+06 + PF_Circuit_5_Time_point_4_(A)___________________________________________ (pfc5t4)______________________ -5.2194E+06 + PF_Circuit_5_Time_point_5_(A)___________________________________________ (pfc5t5)______________________ -0.0000E+00 + CS_Circuit_Time_point_0_(A)_____________________________________________ (cs_t0)_______________________ -0.0000E+00 + CS_Circuit_Time_point_1_(A)_____________________________________________ (cs_t1)_______________________ 1.7482E+08 + CS_Circuit_Time_point_2_(A)_____________________________________________ (cs_t2)_______________________ 2.6086E+07 + CS_Circuit_Time_point_3_(A)_____________________________________________ (cs_t3)_______________________ 2.6086E+07 + CS_Circuit_Time_point_4_(A)_____________________________________________ (cs_t4)_______________________ -1.8523E+08 + CS_Circuit_Time_point_5_(A)_____________________________________________ (cs_t5)_______________________ -0.0000E+00 + Plasma_Time_point_0_(A)_________________________________________________ (plasmat0)____________________ 0.0000E+00 + Plasma_Time_point_1_(A)_________________________________________________ (plasmat1)____________________ 0.0000E+00 + Plasma_Time_point_2_(A)_________________________________________________ (plasmat2)____________________ 1.6631E+07 + Plasma_Time_point_3_(A)_________________________________________________ (plasmat3)____________________ 1.6631E+07 + Plasma_Time_point_4_(A)_________________________________________________ (plasmat4)____________________ 1.6631E+07 + Plasma_Time_point_5_(A)_________________________________________________ (plasmat5)____________________ 0.0000E+00 + # Support Structure # + Outer_PF_coil_fence_mass_(kg)___________________________________________ (fncmass)_____________________ 2.2924E+05 OP + Intercoil_support_structure_mass_(kg)___________________________________ (aintmass)____________________ 4.3045E+06 OP + Mass_of_cooled_components_(kg)__________________________________________ (coldmass)____________________ 3.4369E+07 OP + Gravity_support_structure_mass_(kg)_____________________________________ (clgsmass)____________________ 1.2760E+06 OP + Torus_leg_support_mass_(kg)_____________________________________________ (gsm1)________________________ 8.5820E+04 OP + Ring_beam_mass_(kg)_____________________________________________________ (gsm2)________________________ 4.0088E+05 OP + Ring_legs_mass_(kg)_____________________________________________________ (gsm3)________________________ 6.8283E+05 OP + # PF Coil Inductances # + # Nuclear Heating Magnets Before Renormalisation # + Shield_line_density_(tonne/m2)__________________________________________ (x_shield)____________________ 4.0560E+00 + Blanket_line_density_(tonne/m2)_________________________________________ (x_blanket)___________________ 2.2911E+00 + Unit_nuclear_heating_in_TF_coil_(W/GW)__________________________________ (tfc_nuc_heating)_____________ 1.4866E+04 + Total_nuclear_heating_in_TF_coil_(MW)___________________________________ (ptfnuc.)_____________________ 2.4085E-02 + powfmw__________________________________________________________________ (powfmw.)_____________________ 1.6202E+03 + total_mass_of_the_TF_coils_(kg)_________________________________________ (whttf)_______________________ 1.1424E+07 + # Pumping for primary coolant (helium) # + Pressure_drop_in_FW_and_blanket_coolant_incl._hx_and_pipes_(Pa)_________ (dp_he)_______________________ 5.5000E+05 + Fraction_of_FW_and_blanket_thermal_power_required_for_pumping___________ (fpump)_______________________ 8.9463E-02 OP + Total_power_absorbed_by_FW_&_blanket_(MW)_______________________________ (p_plasma)____________________ 1.6698E+03 OP + Inlet_temperature_of_FW_&_blanket_coolant_pump_(K)______________________ (t_in_compressor)_____________ 5.5703E+02 OP + Coolant_pump_outlet/Inlet_temperature_of_FW_&_blanket_(K)_______________ (t_in_bb)_____________________ 5.7313E+02 + Outlet_temperature_of_FW_&_blanket_(K)__________________________________ (t_out_bb)____________________ 7.7313E+02 + Mechanical_pumping_power_for_FW_and_blanket_cooling_loop_including_heat_ (htpmw_fw_blkt)_______________ 1.6407E+02 OP + Mechanical_pumping_power_for_divertor_(MW)______________________________ (htpmw_div)___________________ 1.6906E+00 OP + Mechanical_pumping_power_for_shield_and_vacuum_vessel_(MW)______________ (htpmw_shld)__________________ 7.0688E-03 OP + # First wall and blanket : CCFE HCPB model # + Titanium_beryllide_fraction_____________________________________________ (fbltibe12)___________________ 3.7500E-01 + Lithium_orthosilicate_fraction__________________________________________ (fblli2sio4)__________________ 3.7500E-01 + Steel_fraction__________________________________________________________ (fblss_ccfe)__________________ 9.7050E-02 + Coolant_fraction________________________________________________________ (vfcblkt)_____________________ 5.2950E-02 + Purge_gas_fraction______________________________________________________ (vfpblkt)_____________________ 1.0000E-01 + First_Wall_Armour_Volume_(m3)___________________________________________ (fw_armour_vol)_______________ 5.8692E+00 + First_Wall_Volume_(m3)__________________________________________________ (volfw)_______________________ 1.9807E+01 + Blanket_Volume_(m3)_____________________________________________________ (volblkt)_____________________ 1.1849E+03 + Shield_Volume_(m3)______________________________________________________ (volshld)_____________________ 7.8520E+02 + Vacuum_vessel_volume_(m3)_______________________________________________ (vdewin)______________________ 1.0178E+03 + First_Wall_Armour_Mass_(kg)_____________________________________________ (fw_armour_mass)______________ 1.1298E+05 OP + First_Wall_Mass,_excluding_armour_(kg)__________________________________ (fwmass)______________________ 1.5449E+05 OP + Blanket_Mass_-_Total(kg)________________________________________________ (whtblkt)_____________________ 2.9676E+06 OP + ____Blanket_Mass_-_TiBe12_(kg)__________________________________________ (whtbltibe12)_________________ 1.0042E+06 OP + ____Blanket_Mass_-_Li4SiO4_(kg)_________________________________________ (whtblli4sio4)________________ 1.0664E+06 OP + ____Blanket_Mass_-_Steel_(kg)___________________________________________ (whtblss)_____________________ 8.9696E+05 OP + Total_mass_of_armour,_first_wall_and_blanket_(kg)_______________________ (armour_fw_bl_mass)___________ 3.2350E+06 OP + Shield_Mass_(kg)________________________________________________________ (whtshld)_____________________ 2.4498E+06 OP + Vacuum_vessel_mass_(kg)_________________________________________________ (vvmass)______________________ 7.9388E+06 OP + Total_nuclear_heating_in_TF+PF_coils_(CS_is_negligible)_(MW)____________ (ptfnuc)______________________ 2.5118E-02 OP + Total_nuclear_heating_in_FW_(MW)________________________________________ (pnucfw)______________________ 1.6315E+02 OP + Total_nuclear_heating_in_the_blanket_(including_emult)_(MW)_____________ (pnucblkt)____________________ 1.2901E+03 OP + Total_nuclear_heating_in_the_shield_(MW)________________________________ (pnucshld)____________________ 1.4138E+00 OP + Total_nuclear_heating_in_the_divertor_(MW)______________________________ (pnucdiv)_____________________ 1.4906E+02 OP + Blanket_exponential_factor______________________________________________ (exp_blanket)_________________ 9.9936E-01 OP + Shield:_first_exponential_______________________________________________ (exp_shield1)_________________ 1.9523E-03 OP + Shield:_second_exponential______________________________________________ (exp_shield2)_________________ 2.5427E-01 OP + Solid_angle_fraction_taken_by_on_divertor_______________________________ (fdiv)________________________ 1.1500E-01 + Switch_for_plant_secondary_cycle________________________________________ (secondary_cycle)_____________ 2 + First_wall_coolant_pressure_(Pa)________________________________________ (fwpressure)__________________ 1.5500E+07 + Blanket_coolant_pressure_(Pa)___________________________________________ (blpressure)__________________ 1.5500E+07 + Allowable_nominal_neutron_fluence_at_first_wall_(MW.year/m2)____________ (abktflnc)____________________ 5.0000E+00 + No_of_inboard_blanket_modules_poloidally________________________________ (nblktmodpi)__________________ 7 + No_of_inboard_blanket_modules_toroidally________________________________ (nblktmodti)__________________ 32 + No_of_outboard_blanket_modules_poloidally_______________________________ (nblktmodpo)__________________ 8 + No_of_outboard_blanket_modules_toroidally_______________________________ (nblktmodto)__________________ 48 + Isentropic_efficiency_of_first_wall_/_blanket_coolant_pumps_____________ (etaiso)______________________ 9.0000E-01 + First_wall_area_(m2)____________________________________________________ (fwarea)______________________ 1.6044E+03 OP + Cryostat_internal_radius_(m)____________________________________________ (rdewex)______________________ 1.7798E+01 OP + Cryostat_internal_half-height_(m)_______________________________________ (zdewex)______________________ 1.5339E+01 OP + Vertical_clearance_from_TF_coil_to_cryostat_(m)_________________________ (clh1)________________________ 5.6044E+00 OP + Divertor_area_(m2)______________________________________________________ (divsur)______________________ 1.4879E+02 OP + Divertor_mass_(kg)______________________________________________________ (divmas)______________________ 3.6453E+04 OP + # Superconducting TF Coil Power Conversion # + TF_coil_current_(kA)____________________________________________________ (itfka)_______________________ 8.9795E+01 OP + Number_of_TF_coils______________________________________________________ (ntfc)________________________ 1.6000E+01 + Voltage_across_a_TF_coil_during_quench_(kV)_____________________________ (vtfskv)______________________ 9.1862E+00 OP + TF_coil_charge_time_(hours)_____________________________________________ (tchghr)______________________ 4.0000E+00 + Total_inductance_of_TF_coils_(H)________________________________________ (ltfth)_______________________ 3.0165E+01 OP + Total_resistance_of_TF_coils_(ohm)______________________________________ (rcoils)______________________ 0.0000E+00 OP + TF_coil_charging_voltage_(V)____________________________________________ (tfcv)________________________ 2.9268E+02 + Number_of_DC_circuit_breakers___________________________________________ (ntfbkr)______________________ 1.6000E+01 + Number_of_dump_resistors________________________________________________ (ndumpr)______________________ 6.4000E+01 + Resistance_per_dump_resistor_(ohm)______________________________________ (r1dump)______________________ 1.0230E-01 OP + Dump_resistor_peak_power_(MW)___________________________________________ (r1ppmw)______________________ 2.0622E+02 OP + Energy_supplied_per_dump_resistor_(MJ)__________________________________ (r1emj)_______________________ 1.9002E+03 OP + TF_coil_L/R_time_constant_(s)___________________________________________ (ttfsec)______________________ 1.8429E+01 OP + Power_supply_voltage_(V)________________________________________________ (tfpsv)_______________________ 3.0731E+02 OP + Power_supply_current_(kA)_______________________________________________ (tfpska)______________________ 9.4285E+01 OP + DC_power_supply_rating_(kW)_____________________________________________ (tfckw)_______________________ 2.8975E+04 OP + AC_power_for_charging_(kW)______________________________________________ (tfackw)______________________ 3.2194E+04 OP + TF_coil_resistive_power_(MW)____________________________________________ (rpower)______________________ 9.3902E+00 OP + TF_coil_inductive_power_(MVA)___________________________________________ (xpower)______________________ 1.6891E+01 OP + Aluminium_bus_current_density_(kA/cm2)__________________________________ (djmka)_______________________ 1.2500E-01 + Aluminium_bus_cross-sectional_area_(cm2)________________________________ (albusa)______________________ 7.1836E+02 OP + Total_length_of_TF_coil_bussing_(m)_____________________________________ (tfbusl)______________________ 3.1931E+03 OP + Aluminium_bus_weight_(tonnes)___________________________________________ (albuswt)_____________________ 6.1932E+02 OP + Total_TF_coil_bus_resistance_(ohm)______________________________________ (rtfbus)______________________ 1.1646E-03 OP + TF_coil_bus_voltage_drop_(V)____________________________________________ (vtfbus)______________________ 1.0457E+02 OP + Dump_resistor_floor_area_(m2)___________________________________________ (drarea)______________________ 4.9234E+03 OP + TF_coil_power_conversion_floor_space_(m2)_______________________________ (tfcfsp)______________________ 1.8228E+03 OP + TF_coil_power_conv._building_volume_(m3)________________________________ (tfcbv)_______________________ 1.0937E+04 OP + TF_coil_AC_inductive_power_demand_(MW)__________________________________ (xpwrmw)______________________ 1.8768E+01 OP + Total_steady_state_AC_power_demand_(MW)_________________________________ (tfacpd)______________________ 1.0434E+01 OP + # PF Coils and Central Solenoid: Power and Energy # + Number_of_PF_coil_circuits______________________________________________ (pfckts)______________________ 1.2000E+01 + Sum_of_PF_power_supply_ratings_(MVA)____________________________________ (spsmva)______________________ 3.0313E+02 OP + Total_PF_coil_circuit_bus_length_(m)____________________________________ (spfbusl)_____________________ 2.4480E+03 OP + Total_PF_coil_bus_resistive_power_(kW)__________________________________ (pfbuspwr)____________________ 9.6485E+02 OP + Total_PF_coil_resistive_power_(kW)______________________________________ (srcktpm)_____________________ 9.6485E+02 OP + Maximum_PF_coil_voltage_(kV)____________________________________________ (vpfskv)______________________ 2.0000E+01 + Efficiency_of_transfer_of_PF_stored_energy_into_or_out_of_storage_______ (etapsu)______________________ 9.0000E-01 + Maximum_stored_energy_in_poloidal_field_(MJ)____________________________ (ensxpfm)_____________________ 2.8804E+04 OP + Peak_absolute_rate_of_change_of_stored_energy_in_poloidal_field_(MW)____ (peakpoloidalpower)___________ 1.7319E+02 OP + # Vacuum System # + First_wall_outgassing_rate_(Pa_m/s)_____________________________________ (rat)_________________________ 1.3000E-08 + Total_outgassing_load_(Pa_m3/s)_________________________________________ (ogas)________________________ 1.6691E-04 OP + Base_pressure_required_(Pa)_____________________________________________ (pbase)_______________________ 5.0000E-04 + Required_N2_pump_speed_(m3/s)___________________________________________ (s(1))________________________ 3.3381E-01 OP + N2_pump_speed_provided_(m3/s)___________________________________________ (snet(1))_____________________ 2.3404E+01 OP + Plasma_chamber_volume_(m3)______________________________________________ (volume)______________________ 2.2588E+03 OP + Chamber_pressure_after_burn_(Pa)________________________________________ (pend)________________________ 1.6698E-01 OP + Chamber_pressure_before_burn_(Pa)_______________________________________ (pstart)______________________ 1.6698E-03 + Allowable_pumping_time_switch___________________________________________ (dwell_pump)__________________ 0 + Dwell_time_between_burns_(s)____________________________________________ (tdwell.)_____________________ 1.8000E+03 + CS_ramp-up_time_burns_(s)_______________________________________________ (tramp.)______________________ 5.0000E+02 + Allowable_pumping_time_between_burns_(s)________________________________ (tpump)_______________________ 1.8000E+03 + Required_D-T_pump_speed_(m3/s)__________________________________________ (s(2))________________________ 5.7790E+00 OP + D-T_pump_speed_provided_(m3/s)__________________________________________ (snet(2))_____________________ 5.6700E+01 OP + Divertor_chamber_gas_pressure_(Pa)______________________________________ (prdiv)_______________________ 3.6000E-01 + Helium_gas_fraction_in_divertor_chamber_________________________________ (fhe)_________________________ 1.7218E-01 OP + Required_helium_pump_speed_(m3/s)_______________________________________ (s(3))________________________ 3.8423E+01 OP + Helium_pump_speed_provided_(m3/s)_______________________________________ (snet(3))_____________________ 3.8423E+01 OP + D-T_fuelling_rate_(kg/s)________________________________________________ (frate)_______________________ 2.7747E-05 OP + Required_D-T_pump_speed_(m3/s)__________________________________________ (s(4))________________________ 3.8423E+01 OP + D-T_pump_speed_provided_(m3/s)__________________________________________ (snet(4))_____________________ 5.6700E+01 OP + Number_of_large_pump_ducts______________________________________________ (nduct)_______________________ 16 + Passage_diameter,_divertor_to_ducts_(m)_________________________________ (d(imax))_____________________ 4.7857E-01 OP + Passage_length_(m)______________________________________________________ (l1)__________________________ 1.7160E+00 OP + Diameter_of_ducts_(m)___________________________________________________ (dout)________________________ 5.7428E-01 OP + Duct_length,_divertor_to_elbow_(m)______________________________________ (l2)__________________________ 4.8000E+00 OP + Duct_length,_elbow_to_pumps_(m)_________________________________________ (l3)__________________________ 2.0000E+00 + Number_of_pumps_________________________________________________________ (pumpn)_______________________ 3.2000E+01 OP + # Plant Buildings System # + Internal_volume_of_reactor_building_(m3)________________________________ (vrci)________________________ 9.9708E+05 + Dist_from_centre_of_torus_to_bldg_wall_(m)______________________________ (wrbi)________________________ 3.9531E+01 + Effective_floor_area_(m2)_______________________________________________ (efloor)______________________ 3.3660E+05 + Reactor_building_volume_(m3)____________________________________________ (rbv)_________________________ 1.1310E+06 + Reactor_maintenance_building_volume_(m3)________________________________ (rmbv)________________________ 3.9641E+05 + Warmshop_volume_(m3)____________________________________________________ (wsv)_________________________ 1.2531E+05 + Tritium_building_volume_(m3)____________________________________________ (triv)________________________ 4.0000E+04 + Electrical_building_volume_(m3)_________________________________________ (elev)________________________ 5.1937E+04 + Control_building_volume_(m3)____________________________________________ (conv)________________________ 6.0000E+04 + Cryogenics_building_volume_(m3)_________________________________________ (cryv)________________________ 1.4976E+04 + Administration_building_volume_(m3)_____________________________________ (admv)________________________ 1.0000E+05 + Shops_volume_(m3)_______________________________________________________ (shov)________________________ 1.0000E+05 + Total_volume_of_nuclear_buildings_(m3)__________________________________ (volnucb)_____________________ 1.5738E+06 + # Electric Power Requirements # + Facility_base_load_(MW)_________________________________________________ (basemw)______________________ 5.0000E+00 + Divertor_coil_power_supplies_(MW)_______________________________________ (bdvmw)_______________________ 0.0000E+00 + Cryoplant_electric_power_(MW)___________________________________________ (crymw)_______________________ 3.6566E+01 OP + Primary_coolant_pumps_(MW)______________________________________________ (htpmw..)_____________________ 1.9053E+02 OP + PF_coil_power_supplies_(MW)_____________________________________________ (ppfmw)_______________________ 8.5511E+01 OP + TF_coil_power_supplies_(MW)_____________________________________________ (ptfmw)_______________________ 1.0434E+01 OP + Plasma_heating_supplies_(MW)____________________________________________ (pheatingmw)__________________ 1.6029E+02 OP + Tritium_processing_(MW)_________________________________________________ (trithtmw..)__________________ 1.5000E+01 + Vacuum_pumps__(MW)______________________________________________________ (vachtmw..)___________________ 5.0000E-01 + Total_pulsed_power_(MW)_________________________________________________ (pacpmw)______________________ 5.5432E+02 OP + Total_base_power_required_at_all_times_(MW)_____________________________ (fcsht)_______________________ 5.5490E+01 OP + # Cryogenics # + Conduction_and_radiation_heat_loads_on_cryogenic_components_(MW)________ (qss/1.0d6)___________________ 1.4779E-02 OP + Nuclear_heating_of_cryogenic_components_(MW)____________________________ (qnuc/1.0d6)__________________ 1.3000E-02 OP + AC_losses_in_cryogenic_components_(MW)__________________________________ (qac/1.0d6)___________________ 3.8170E-03 OP + Resistive_losses_in_current_leads_(MW)__________________________________ (qcl/1.0d6)___________________ 1.9539E-02 OP + 45%_allowance_for_heat_loads_in_transfer_lines,_storage_tanks_etc_(MW)__ (qmisc/1.0d6)_________________ 2.3011E-02 OP + Sum_=_Total_heat_removal_at_cryogenic_temperatures_(tfcoil_variables.tmp (helpow_+_helpow_cryal/1.0d6)_ 7.4146E-02 OP + Temperature_of_cryogenic_superconducting_components_(K)_________________ (tmpcry)______________________ 4.5000E+00 + Temperature_of_cryogenic_aluminium_components_(K)_______________________ (tcoolin)_____________________ 3.1315E+02 + Efficiency_(figure_of_merit)_of_cryogenic_plant_is_13%_of_ideal_Carnot_v ______________________________ 2.0277E-03 OP + Efficiency_(figure_of_merit)_of_cryogenic_aluminium_plant_is_40%_of_idea ______________________________ -2.0203E+00 OP + Electric_power_for_cryogenic_plant_(MW)_________________________________ (crypmw)______________________ 3.6566E+01 OP + # Plant Power / Heat Transport Balance # + Neutron_power_multiplication_in_blanket_________________________________ (emult)_______________________ 1.2690E+00 + Divertor_area_fraction_of_whole_toroid_surface__________________________ (fdiv)________________________ 1.1500E-01 + H/CD_apparatus_+_diagnostics_area_fraction______________________________ (fhcd)________________________ 0.0000E+00 + First_wall_area_fraction________________________________________________ (1-fdiv-fhcd)_________________ 8.8500E-01 + Switch_for_pumping_of_primary_coolant___________________________________ (primary_pumping)_____________ 3 + Mechanical_pumping_power_for_FW_cooling_loop_including_heat_exchanger_(M (htpmw_fw)____________________ 0.0000E+00 OP + Mechanical_pumping_power_for_blanket_cooling_loop_including_heat_exchang (htpmw_blkt)__________________ 0.0000E+00 OP + Mechanical_pumping_power_for_FW_and_blanket_cooling_loop_including_heat_ (htpmw_fw_blkt)_______________ 1.6407E+02 OP + Mechanical_pumping_power_for_divertor_(MW)______________________________ (htpmw_div)___________________ 1.6906E+00 OP + Mechanical_pumping_power_for_shield_and_vacuum_vessel_(MW)______________ (htpmw_shld)__________________ 7.0688E-03 OP + Electrical_pumping_power_for_FW_and_blanket_(MW)________________________ (htpmwe_fw_blkt)______________ 1.8858E+02 OP + Electrical_pumping_power_for_shield_(MW)________________________________ (htpmwe_shld)_________________ 8.1250E-03 OP + Electrical_pumping_power_for_divertor_(MW)______________________________ (htpmwe_div)__________________ 1.9433E+00 OP + Total_electrical_pumping_power_for_primary_coolant_(MW)_________________ (htpmw)_______________________ 1.9053E+02 OP + Coolant_pump_power_/_non-pumping_thermal_power_in_shield________________ (fpumpshld)___________________ 5.0000E-03 + Coolant_pump_power_/_non-pumping_thermal_power_in_divertor______________ (fpumpdiv)____________________ 5.0000E-03 + Electrical_efficiency_of_heat_transport_coolant_pumps___________________ (etahtp)______________________ 8.7000E-01 + Thermal_to_electric_conversion_efficiency_of_the_power_conversion_cycle_ (etath)_______________________ 4.0000E-01 + Fraction_of_total_high-grade_thermal_power_to_divertor__________________ (pdivfraction)________________ 1.5623E-01 + Total_power_leaving_reactor_(across_vacuum_vessel_boundary)_(MW)________ ______________________________ 2.0111E+03 + Heat_removal_from_cryogenic_plant_(MW)__________________________________ (crypmw)______________________ 3.6566E+01 + Heat_removal_from_facilities_(MW)_______________________________________ (fachtmw)_____________________ 5.5490E+01 + Coolant_pumping_efficiency_losses_(MW)__________________________________ (htpsecmw)____________________ 2.4769E+01 + Heat_removal_from_injection_power_(MW)__________________________________ (pinjht)______________________ 8.0143E+01 + Heat_removal_from_tritium_plant_(MW)____________________________________ (trithtmw)____________________ 1.5000E+01 + Heat_removal_from_vacuum_pumps_(MW)_____________________________________ (vachtmw)_____________________ 5.0000E-01 + TF_coil_resistive_power_(MW)____________________________________________ (tfcmw)_______________________ 0.0000E+00 + Total_low-grade_thermal_power_(MW)______________________________________ (psechtmw)____________________ 2.2417E+02 + Total_High-grade_thermal_power_(MW)_____________________________________ (pthermmw)____________________ 2.1751E+03 + Number_of_primary_heat_exchangers_______________________________________ (nphx)________________________ 3 OP + Transport_power_from_scaling_law_(MW)___________________________________ (pscalingmw)__________________ 2.9785E+02 + Radiation_power_from_inside_"coreradius"_(MW)___________________________ (pcoreradmw.)_________________ 9.1650E+01 + Total_(MW)______________________________________________________________ ______________________________ 3.8950E+02 + Alpha_power_deposited_in_plasma_(MW)____________________________________ (falpha*palpmw)_______________ 3.0746E+02 + Power_from_charged_products_of_DD_and/or_D-He3_fusion_(MW)______________ (pchargemw.)__________________ 1.2659E+00 + Ohmic_heating_(MW)______________________________________________________ (pohmmw.)_____________________ 6.2284E-01 + Injected_power_deposited_in_plasma_(MW)_________________________________ (pinjmw)______________________ 8.0143E+01 + Total_(MW)______________________________________________________________ ______________________________ 3.8950E+02 + Fusion_power_(MW)_______________________________________________________ (powfmw)______________________ 1.6202E+03 + Power_from_energy_multiplication_in_blanket_and_shield_(MW)_____________ (emultmw)_____________________ 3.0836E+02 + Injected_power_(MW)_____________________________________________________ (pinjmw.)_____________________ 8.0143E+01 + Ohmic_power_(MW)________________________________________________________ (pohmmw.)_____________________ 6.2284E-01 + Power_deposited_in_primary_coolant_by_pump_(MW)_________________________ (htpmw_mech)__________________ 1.6576E+02 + Total_(MW)______________________________________________________________ ______________________________ 2.1751E+03 + Heat_extracted_from_first_wall_and_blanket_(MW)_________________________ (pthermfw_blkt)_______________ 1.8339E+03 + Heat_extracted_from_shield__(MW)________________________________________ (pthermshld)__________________ 1.4208E+00 + Heat_extracted_from_divertor_(MW)_______________________________________ (pthermdiv)___________________ 3.3982E+02 + Nuclear_and_photon_power_lost_to_H/CD_system_(MW)_______________________ (psechcd)_____________________ 0.0000E+00 + Nuclear_power_lost_to_TF_(MW)___________________________________________ (ptfnuc)______________________ 2.5118E-02 + Total_(MW)______________________________________________________________ ______________________________ 2.1752E+03 + Net_electric_power_output(MW)___________________________________________ (pnetelmw.)___________________ 4.0001E+02 + Required_Net_electric_power_output(MW)__________________________________ (pnetelin)____________________ 4.0000E+02 + Electric_power_for_heating_and_current_drive_(MW)_______________________ (pinjwp)______________________ 1.6029E+02 + Electric_power_for_primary_coolant_pumps_(MW)___________________________ (htpmw)_______________________ 1.9053E+02 + Electric_power_for_vacuum_pumps_(MW)____________________________________ (vachtmw)_____________________ 5.0000E-01 + Electric_power_for_tritium_plant_(MW)___________________________________ (trithtmw)____________________ 1.5000E+01 + Electric_power_for_cryoplant_(MW)_______________________________________ (crypmw)______________________ 3.6566E+01 + Electric_power_for_TF_coils_(MW)________________________________________ (tfacpd)______________________ 1.0434E+01 + Electric_power_for_PF_coils_(MW)________________________________________ (pfwpmw)______________________ 1.2422E+00 + All_other_internal_electric_power_requirements_(MW)_____________________ (fachtmw)_____________________ 5.5490E+01 + Total_(MW)______________________________________________________________ (tot_plant_power)_____________ 8.7006E+02 + Total_(MW)______________________________________________________________ ______________________________ 8.7006E+02 + Gross_electrical_output*_(MW)___________________________________________ (pgrossmw)____________________ 8.7006E+02 + Fusion_power_(MW)_______________________________________________________ (powfmw)______________________ 1.6202E+03 + Power_from_energy_multiplication_in_blanket_and_shield_(MW)_____________ (emultmw)_____________________ 3.0836E+02 + Total_(MW)______________________________________________________________ ______________________________ 1.9285E+03 + Net_electrical_output_(MW) _____________________________________________ (pnetelmw)____________________ 4.0001E+02 + Heat_rejected_by_main_power_conversion_circuit_(MW)_____________________ (rejected_main)_______________ 1.3051E+03 + Heat_rejected_by_other_cooling_circuits_(MW)____________________________ (psechtmw)____________________ 2.2417E+02 + Total_(MW)______________________________________________________________ ______________________________ 1.9293E+03 + Net_electric_power_/_total_nuclear_power_(%)____________________________ (pnetelmw/(powfmw+emultmw)____ 2.0741E+01 + Net_electric_power_/_total_fusion_power_(%)_____________________________ (pnetelmw/powfmw)_____________ 2.4689E+01 + Gross_electric_power*_/_high_grade_heat_(%)_____________________________ (etath)_______________________ 4.0000E+01 + Recirculating_power_fraction____________________________________________ (cirpowfr)____________________ 5.4025E-01 + # Water usage during plant operation (secondary cooling) # + Volume_used_in_cooling_tower_(m3/day)___________________________________ (waterusetower)_______________ 5.5485E+04 OP + Volume_used_in_recirculating_water_system_(m3/day)______________________ (wateruserecirc)______________ 1.8617E+04 OP + Volume_used_in_once-through_water_system_(m3/day)_______________________ (wateruseonethru)_____________ 1.8244E+06 OP + # Errors and Warnings # + # Errors and Warnings # + PROCESS_error_status_flag_______________________________________________ (error_status)________________ 2 + Final_error_identifier__________________________________________________ (error_id)____________________ 244 + # End of PROCESS Output # + # End of PROCESS Output # + # Copy of PROCESS Input Follows # +************************************************************************************************************************ +***** ***** +***** Generic large tokamak file ***** +***** James Morris, UKAEA ***** +***** 28/06/23 ***** +***** ***** +************************************************************************* + +* Run Information * +******************* + +runtitle = Generic large tokamak + +* Figure of merit - minimise major radius +minmax = 1 + +* Error tolerance for VMCON +epsvmc = 1e-7 + +* Constraint Equations - Consistency Equations * +************************************************ + +* Beta consistency * +*------------------* +icc = 1 +ixc = 5 * beta +beta = 0.03 + +* Global power balance * +*----------------------* +icc = 2 + +* Radial build consistency * +*--------------------------* +icc = 11 + +* Constraint Equations - Limit Equations * +****************************************** + +* Density upper limit * +*---------------------* +icc = 5 +ixc = 6 * dene [m-3] +fdene = 1.2 +dene = 7.5E19 + +* Neutron wall load upper limit * +*-------------------------------* +icc = 8 +ixc = 14 * fwalld +fwalld = 1.0 +* wall load limit [MW/m2] +walalw = 2.0 + +* Fusion power upper limit * +*--------------------------* + +icc = 9 +ixc = 26 * ffuspow +* Maximum allowable value fusion power [MW] +powfmax = 3000 + +* Burn time lower limit * +*-----------------------* +icc = 13 +ixc = 21 * ftburn +* minimum burn time [s] +tbrnmn = 7200.0 + +* L-H threshold scaling * +*-----------------------* +icc = 15 +ixc = 103 * flhthresh +boundu(103) = 10.0 + +* Injection power upper limit * +*-----------------------------* +icc = 30 +ixc = 46 * fpinj +* Maximum allowable value for injected power [MW] +pinjalw = 200.0 + +* Net electric power lower limit * +*--------------------------------* +icc = 16 +ixc = 25 * fpnetel +* Minimum allowable value for net eletric power [MW] +pnetelin = 400.0 + +* Beta upper limit * +*------------------* +icc = 24 +ixc = 36 * fbetatry +fbetatry = 0.5 + +* Max TF field * +*--------------* +icc = 25 +ixc = 35 * fpeakb +* Maximum allowable value for toroidal magnetic field [T] +bmxlim = 14.0 + +* Central solenoid EOF current density upper limit * +*--------------------------------------------------* +icc = 26 +ixc = 37 * coheof [A/m2] +ixc = 38 * fjohc +boundu(38) = 1.0 +coheof = 1.5E7 +fjohc = 0.6 + +* Central solenoid BOP current density upper limit * +*--------------------------------------------------* +icc = 27 +ixc = 39 * fjohc0 +ixc = 41 * fcohbop +boundu(39) = 1.0 +fjohc0 = 0.6 +fcohbop = 0.9 + +* I_op/I_Crit TF coil limit * +*---------------------------* +icc = 33 +ixc = 50 * fiooic +boundu(50) = 1.0 +fiooic = 0.65 + +* Dump voltage upper limit * +*--------------------------* +icc = 34 +ixc = 51 * fvdump +ixc = 52 * vdalw [kV] +boundu(52) = 10.0 +fvdump = 1.0 +vdalw = 10.0 + +* J_winding pack protection * +*---------------------------* +icc = 35 +ixc = 53 * fjprot +fjprot = 1.0 + +* TF temp marg lower limit * +*--------------------------* +icc = 36 +ixc = 54 * ftmargtf +* Minimum allowable temperature margin [K] +tmargmin = 1.5 + +* CS coil temp margin lower limit * +*---------------------------------* +icc = 60 +ixc = 106 * ftmargoh +tmargmin_cs = 1.5 + +* Lower limit on taup/taueff (ratio alpha particle/energy confinement times) * +*-------------------------------------------------------------------------------* +icc = 62 +ixc = 110 * ftaulimit +taulimit = 5.0 + +* dump time constraint for VV stresses * +*--------------------------------------* +icc = 65 +ixc = 113 * fmaxvvstress +fmaxvvstress = 1.0 + +* CS stress limit * +*-----------------* +icc = 72 +ixc = 123 * foh_stress +foh_stress = 1.0 +* allowable hoop stress in Central Solenoid structural material [Pa] +alstroh = 7.5D8 + +* neped_neped_______________________normalised_residue____________________ (normres023)__________________ -1.9637E-08 + Upper_Lim._on_Psep_*_Bt_/_q_A_R___normalised_residue____________________ (normres024)__________________ 4.9789E-07 + TF_coil_case_stress_upper_limit___normalised_residue____________________ (normres025)__________________ -4.6757E-07 + TF_coil_conduit_stress_upper_lim__normalised_residue____________________ (normres026)__________________ -4.1375E-07 + # Final Feasible Point # + # Power Reactor Costs (1990 US$) # + First_wall_/_blanket_life_(years)_______________________________________ (fwbllife)____________________ 6.1566E+00 + Divertor_life_(years)___________________________________________________ (divlife.)____________________ 3.9769E+00 + Cost_of_electricity_(m$/kWh)____________________________________________ (coe)_________________________ 5.1257E+02 + # Detailed Costings (1990 US$) # + Acc.22_multiplier_for_Nth_of_a_kind_____________________________________ (fkind)_______________________ 1.0000E+00 + Level_of_Safety_Assurance_______________________________________________ (lsa)_________________________ 4 + # Structures and Site Facilities # + Site_improvements,_facilities,_land_(M$)________________________________ (c211)________________________ 3.5200E+01 + Reactor_building_cost_(M$)______________________________________________ (c212)________________________ 4.5238E+02 + Turbine_building_cost_(M$)______________________________________________ (c213)________________________ 3.8000E+01 + Reactor_maintenance_building_cost_(M$)__________________________________ (c2141)_______________________ 1.0307E+02 + Warm_shop_cost_(M$)_____________________________________________________ (c2142)_______________________ 5.7641E+01 + Tritium_building_cost_(M$)______________________________________________ (c215)________________________ 1.4800E+01 + Electrical_equipment_building_cost_(M$)_________________________________ (c216)________________________ 1.9736E+01 + Additional_buildings_cost_(M$)__________________________________________ (c2171)_______________________ 1.8000E+01 + Control_room_buildings_cost_(M$)________________________________________ (c2172)_______________________ 2.1000E+01 + Shop_and_warehouses_cost_(M$)___________________________________________ (c2173)_______________________ 1.1500E+01 + Cryogenic_building_cost_(M$)____________________________________________ (c2174)_______________________ 6.8891E+00 + Total_account_21_cost_(M$)______________________________________________ (c21)_________________________ 7.7822E+02 + # Reactor Systems # + First_wall_cost_(M$)____________________________________________________ (c2211)_______________________ 1.9130E+02 + Blanket_beryllium_cost_(M$)_____________________________________________ (c22121)______________________ 2.6109E+02 + Blanket_breeder_material_cost_(M$)______________________________________ (c22122)______________________ 6.3985E+02 + Blanket_stainless_steel_cost_(M$)_______________________________________ (c22123)______________________ 8.0726E+01 + Blanket_vanadium_cost_(M$)______________________________________________ (c22124)______________________ 0.0000E+00 + Blanket_total_cost_(M$)_________________________________________________ (c2212)_______________________ 9.8166E+02 + Bulk_shield_cost_(M$)___________________________________________________ (c22131)______________________ 7.8394E+01 + Penetration_shielding_cost_(M$)_________________________________________ (c22132)______________________ 7.8394E+01 + Total_shield_cost_(M$)__________________________________________________ (c2213)_______________________ 1.5679E+02 + Total_support_structure_cost_(M$)_______________________________________ (c2214)_______________________ 4.0933E+01 + Divertor_cost_(M$)______________________________________________________ (c2215)_______________________ 4.1660E+01 + Total_account_221_cost_(M$)_____________________________________________ (c221)________________________ 1.4123E+03 + # Magnets # + TF_coil_conductor_cost_(M$)_____________________________________________ (c22211)______________________ 1.3230E+02 + TF_coil_winding_cost_(M$)_______________________________________________ (c22212)______________________ 5.4263E+01 + TF_coil_case_cost_(M$)__________________________________________________ (c22213)______________________ 4.4365E+02 + TF_intercoil_structure_cost_(M$)________________________________________ (c22214)______________________ 1.5066E+02 + TF_coil_gravity_support_structure_(M$)__________________________________ (c22215)______________________ 4.4659E+01 + TF_magnet_assemblies_cost_(M$)__________________________________________ (c2221)_______________________ 8.2552E+02 + PF_coil_conductor_cost_(M$)_____________________________________________ (c22221)______________________ 4.6409E+02 + PF_coil_winding_cost_(M$)_______________________________________________ (c22222)______________________ 7.6765E+01 + PF_coil_case_cost_(M$)__________________________________________________ (c22223)______________________ 9.4861E+01 + PF_coil_support_structure_cost_(M$)_____________________________________ (c22224)______________________ 8.0235E+00 + PF_magnet_assemblies_cost_(M$)__________________________________________ (c2222)_______________________ 6.4374E+02 + Vacuum_vessel_assembly_cost_(M$)________________________________________ (c2223)_______________________ 2.5404E+02 + Total_account_222_cost_(M$)_____________________________________________ (c222)________________________ 1.7233E+03 + # Power Injection # + ECH_system_cost_(M$)____________________________________________________ (c2231)_______________________ 2.4043E+02 + Lower_hybrid_system_cost_(M$)___________________________________________ (c2232)_______________________ 0.0000E+00 + Neutral_beam_system_cost_(M$)___________________________________________ (c2233)_______________________ 0.0000E+00 + Total_account_223_cost_(M$)_____________________________________________ (c223)________________________ 2.4043E+02 + # Vacuum Systems # + High_vacuum_pumps_cost_(M$)_____________________________________________ (c2241)_______________________ 1.2480E+01 + Backing_pumps_cost_(M$)_________________________________________________ (c2242)_______________________ 4.6800E+00 + Vacuum_duct_cost_(M$)___________________________________________________ (c2243)_______________________ 2.5280E+00 + Valves_cost_(M$)________________________________________________________ (c2244)_______________________ 5.7410E+00 + Duct_shielding_cost_(M$)________________________________________________ (c2245)_______________________ 0.0000E+00 + Instrumentation_cost_(M$)_______________________________________________ (c2246)_______________________ 1.3000E+00 + Total_account_224_cost_(M$)_____________________________________________ (c224)________________________ 2.6729E+01 + # Power Conditioning # + TF_coil_power_supplies_cost_(M$)________________________________________ (c22511)______________________ 4.0144E+00 + TF_coil_breakers_cost_(M$)______________________________________________ (c22512)______________________ 3.4127E+01 + TF_coil_dump_resistors_cost_(M$)________________________________________ (c22513)______________________ 2.1322E+01 + TF_coil_instrumentation_and_control_(M$)________________________________ (c22514)______________________ 4.8000E+00 + TF_coil_bussing_cost_(M$)_______________________________________________ (c22515)______________________ 3.5267E+01 + Total,_TF_coil_power_costs_(M$)_________________________________________ (c2251)_______________________ 9.9531E+01 + PF_coil_power_supplies_cost_(M$)________________________________________ (c22521)______________________ 2.9591E+00 + PF_coil_instrumentation_and_control_(M$)________________________________ (c22522)______________________ 3.6000E+00 + PF_coil_bussing_cost_(M$)_______________________________________________ (c22523)______________________ 1.1995E+01 + PF_coil_burn_power_supplies_cost_(M$)___________________________________ (c22524)______________________ 1.2679E+00 + PF_coil_breakers_cost_(M$)______________________________________________ (c22525)______________________ 1.4709E+01 + PF_coil_dump_resistors_cost_(M$)________________________________________ (c22526)______________________ 4.3206E+00 + PF_coil_ac_breakers_cost_(M$)___________________________________________ (c22527)______________________ 9.0000E-01 + Total,_PF_coil_power_costs_(M$)_________________________________________ (c2252)_______________________ 3.9752E+01 + Total,_energy_storage_cost_(M$)_________________________________________ (c2253)_______________________ 1.6864E+01 + Total_account_225_cost_(M$)_____________________________________________ (c225)________________________ 1.5615E+02 + # Heat Transport System # + Pumps_and_piping_system_cost_(M$)_______________________________________ (cpp)_________________________ 3.6795E+01 + Primary_heat_exchanger_cost_(M$)________________________________________ (chx)_________________________ 7.1692E+01 + Total,_reactor_cooling_system_cost_(M$)_________________________________ (c2261)_______________________ 1.0849E+02 + Pumps,_piping_cost_(M$)_________________________________________________ (cppa)________________________ 2.8417E+01 + Total,_auxiliary_cooling_system_cost_(M$)_______________________________ (c2262)_______________________ 2.8417E+01 + Total,_cryogenic_system_cost_(M$)_______________________________________ (c2263)_______________________ 1.7039E+02 + Total_account_226_cost_(M$)_____________________________________________ (c226)________________________ 3.0729E+02 + # Fuel Handling System # + Fuelling_system_cost_(M$)_______________________________________________ (c2271)_______________________ 2.2300E+01 + Fuel_processing_and_purification_cost_(M$)______________________________ (c2272)_______________________ 1.0229E+02 + Atmospheric_recovery_systems_cost_(M$)__________________________________ (c2273)_______________________ 5.8088E+01 + Nuclear_building_ventilation_cost_(M$)__________________________________ (c2274)_______________________ 6.9201E+01 + Total_account_227_cost_(M$)_____________________________________________ (c227)________________________ 2.5188E+02 + # Instrumentation and Control # + Instrumentation_and_control_cost_(M$)___________________________________ (c228)________________________ 1.5000E+02 + # Maintenance Equipment # + Maintenance_equipment_cost_(M$)_________________________________________ (c229)________________________ 1.2500E+02 + # Total Account 22 Cost # + Total_account_22_cost_(M$)______________________________________________ (c22)_________________________ 4.3931E+03 + # Turbine Plant Equipment # + Turbine_plant_equipment_cost_(M$)_______________________________________ (c23)_________________________ 1.7613E+02 + # Electric Plant Equipment # + Switchyard_equipment_cost_(M$)__________________________________________ (c241)________________________ 1.8400E+01 + Transformers_cost_(M$)__________________________________________________ (c242)________________________ 8.0330E+00 + Low_voltage_equipment_cost_(M$)_________________________________________ (c243)________________________ 6.4513E+00 + Diesel_backup_equipment_cost_(M$)_______________________________________ (c244)________________________ 6.8000E+00 + Auxiliary_facilities_cost_(M$)__________________________________________ (c245)________________________ 1.5000E+00 + Total_account_24_cost_(M$)______________________________________________ (c24)_________________________ 4.1184E+01 + # Miscellaneous Plant Equipment # + Miscellaneous_plant_equipment_cost_(M$)_________________________________ (c25)_________________________ 2.5000E+01 + # Heat Rejection System # + Heat_rejection_system_cost_(M$)_________________________________________ (c26)_________________________ 4.9877E+01 + # Plant Direct Cost # + Plant_direct_cost_(M$)__________________________________________________ (cdirt)_______________________ 5.4635E+03 + # Reactor Core Cost # + Reactor_core_cost_(M$)__________________________________________________ (crctcore)____________________ 3.3761E+03 + # Indirect Cost # + Indirect_cost_(M$)______________________________________________________ (c9)__________________________ 1.8221E+03 + # Total Contingency # + Total_contingency_(M$)__________________________________________________ (ccont)_______________________ 1.4207E+03 + # Constructed Cost # + Constructed_cost_(M$)___________________________________________________ (concost)_____________________ 8.7063E+03 + # Interest during Construction # + Interest_during_construction_(M$)_______________________________________ (moneyint)____________________ 1.4365E+03 + # Total Capital Investment # + Total_capital_investment_(M$)___________________________________________ (capcost)_____________________ 1.0143E+04 + # Plant Availability # + Allowable_blanket_neutron_fluence_(MW-yr/m2)____________________________ (abktflnc)____________________ 5.0000E+00 + Allowable_divertor_heat_fluence_(MW-yr/m2)______________________________ (adivflnc)____________________ 7.0000E+00 + First_wall_/_blanket_lifetime_(years)___________________________________ (bktlife)_____________________ 6.1566E+00 OP + Divertor_lifetime_(years)_______________________________________________ (divlife)_____________________ 3.9769E+00 OP + Heating/CD_system_lifetime_(years)______________________________________ (cdrlife)_____________________ 6.1566E+00 OP + Total_plant_lifetime_(years)____________________________________________ (tlife)_______________________ 3.0000E+01 + Total_plant_availability_fraction_______________________________________ (cfactr)______________________ 8.0000E-01 + Number_of_fusion_cycles_to_reach_allowable_fw/blanket_DPA_______________ (bktcycles)___________________ 1.5787E+04 + # Plasma # + Tokamak_aspect_ratio_=_Conventional,_itart_=_0__________________________ (itart)_______________________ 0.0000E+00 + Major_radius_(m)________________________________________________________ (rmajor)______________________ 8.0000E+00 ITV + Minor_radius_(m)________________________________________________________ (rminor)______________________ 2.6667E+00 + Aspect_ratio____________________________________________________________ (aspect)______________________ 3.0000E+00 + Elongation,_X-point_(input_value_used)__________________________________ (kappa)_______________________ 1.8500E+00 + Elongation,_95%_surface_(calculated_from_kappa)_________________________ (kappa95)_____________________ 1.6518E+00 + Elongation,_area_ratio_calc.____________________________________________ (kappaa)______________________ 1.7188E+00 + Triangularity,_X-point_(input_value_used)_______________________________ (triang)______________________ 5.0000E-01 + Triangularity,_95%_surface_(calculated_from_triang)_____________________ (triang95)____________________ 3.3333E-01 + Plasma_poloidal_perimeter_(m)___________________________________________ (pperim)______________________ 2.4081E+01 + Plasma_cross-sectional_area_(m2)________________________________________ (xarea)_______________________ 3.8398E+01 + Plasma_surface_area_(m2)________________________________________________ (sarea)_______________________ 1.1738E+03 OP + Plasma_volume_(m3)______________________________________________________ (vol)_________________________ 1.8882E+03 OP + Plasma_current_scaling_law_used_________________________________________ (icurr)_______________________ 4 + Plasma_current_(MA)_____________________________________________________ (plascur/1D6)_________________ 1.6631E+01 + Current_density_profile_factor__________________________________________ (alphaj)______________________ 1.9805E+00 + Plasma_internal_inductance,_li__________________________________________ (rli)_________________________ 1.2275E+00 + Vertical_field_at_plasma_(T)____________________________________________ (bvert)_______________________ -7.4373E-01 + Vacuum_toroidal_field_at_R_(T)__________________________________________ (bt)__________________________ 5.2940E+00 ITV + Average_poloidal_field_(T)______________________________________________ (bp)__________________________ 8.6787E-01 + Total_field_(sqrt(bp^2_+_bt^2))_(T)_____________________________________ (btot)________________________ 5.3647E+00 + Safety_factor_on_axis___________________________________________________ (q0)__________________________ 1.0000E+00 + Safety_factor_at_95%_flux_surface_______________________________________ (q95)_________________________ 3.5961E+00 ITV + Cylindrical_safety_factor_(qcyl)________________________________________ (qstar)_______________________ 2.9805E+00 + Total_plasma_beta_______________________________________________________ (beta)________________________ 3.3648E-02 ITV + Total_poloidal_beta_____________________________________________________ (betap)_______________________ 1.2857E+00 OP + Total_toroidal_beta_____________________________________________________ ______________________________ 3.4553E-02 OP + Fast_alpha_beta_________________________________________________________ (betaft)______________________ 4.2236E-03 OP + Beam_ion_beta___________________________________________________________ (betanb)______________________ 0.0000E+00 OP + (Fast_alpha_+_beam_physics_variables.beta)/(thermal_physics_variables.be (gammaft)_____________________ 1.4354E-01 OP + Thermal_beta____________________________________________________________ ______________________________ 2.9425E-02 OP + Thermal_poloidal_beta___________________________________________________ ______________________________ 1.1243E+00 OP + Thermal_toroidal_physics_variables.beta_(=_beta-exp)____________________ ______________________________ 3.0215E-02 OP + 2nd_stability_physics_variables.beta_:_beta_p_/_(R/a)___________________ (eps*betap)___________________ 4.2857E-01 + 2nd_stability_physics_variables.beta_upper_limit________________________ (epbetmax)____________________ 1.3800E+00 + Beta_g_coefficient______________________________________________________ (dnbeta)______________________ 4.9099E+00 + Normalised_thermal_beta_________________________________________________ ______________________________ 2.4977E+00 + Normalised_total_beta___________________________________________________ ______________________________ 2.8562E+00 + Normalised_toroidal_beta________________________________________________ (normalised_toroidal_beta)____ 2.9330E+00 + Limit_on_thermal_beta___________________________________________________ (betalim)_____________________ 5.7842E-02 + Plasma_thermal_energy_(J)_______________________________________________ ______________________________ 9.5431E+08 OP + Total_plasma_internal_energy_(J)________________________________________ (total_plasma_internal_energy) 1.0913E+09 OP + Electron_temperature_(keV)______________________________________________ (te)__________________________ 1.2489E+01 ITV + Electron_temperature_on_axis_(keV)______________________________________ (te0)_________________________ 2.5758E+01 + Ion_temperature_(keV)___________________________________________________ (ti)__________________________ 1.2489E+01 + Ion_temperature_on_axis_(keV)___________________________________________ (ti0)_________________________ 2.5758E+01 + Electron_temp.,_density_weighted_(keV)__________________________________ (ten)_________________________ 1.3805E+01 + Electron_density_(/m3)__________________________________________________ (dene)________________________ 8.0667E+19 ITV + Electron_density_on_axis_(/m3)__________________________________________ (ne0)_________________________ 1.0610E+20 OP + Line-averaged_electron_density_(/m3)____________________________________ (dnla)________________________ 8.9334E+19 OP + Line-averaged_electron_density_/_Greenwald_density______________________ (dnla_gw)_____________________ 1.2000E+00 OP + Ion_density_(/m3)_______________________________________________________ (dnitot)______________________ 7.1669E+19 OP + Fuel_density_(/m3)______________________________________________________ (deni)________________________ 6.4831E+19 OP + Total_impurity_density_with_Z_>_2_(no_He)_(/m3)_________________________ (dnz)_________________________ 4.6503E+16 OP + Helium_ion_density_(thermalised_ions_only)_(/m3)________________________ (dnalp)_______________________ 6.7723E+18 OP + Proton_density_(/m3)____________________________________________________ (dnprot)______________________ 1.8963E+16 OP + Hot_beam_density_(/m3)__________________________________________________ (dnbeam)______________________ 0.0000E+00 OP + Density_limit_from_scaling_(/m3)________________________________________ (dnelimt)_____________________ 7.4445E+19 OP + Density_limit_(enforced)_(/m3)__________________________________________ (boundu(9)*dnelimt)___________ 7.4445E+19 OP + Helium_ion_density_(thermalised_ions_only)_/_electron_density___________ (ralpne)______________________ 8.3954E-02 ITV + H__concentration________________________________________________________ (fimp(01))____________________ 8.0392E-01 OP + He_concentration________________________________________________________ (fimp(02))____________________ 8.3954E-02 + Be_concentration________________________________________________________ (fimp(03))____________________ 0.0000E+00 + C__concentration________________________________________________________ (fimp(04))____________________ 0.0000E+00 + N__concentration________________________________________________________ (fimp(05))____________________ 0.0000E+00 + O__concentration________________________________________________________ (fimp(06))____________________ 0.0000E+00 + Ne_concentration________________________________________________________ (fimp(07))____________________ 0.0000E+00 + Si_concentration________________________________________________________ (fimp(08))____________________ 0.0000E+00 + Ar_concentration________________________________________________________ (fimp(09))____________________ 0.0000E+00 + Fe_concentration________________________________________________________ (fimp(10))____________________ 0.0000E+00 + Ni_concentration________________________________________________________ (fimp(11))____________________ 0.0000E+00 + Kr_concentration________________________________________________________ (fimp(12))____________________ 0.0000E+00 + Xe_concentration________________________________________________________ (fimp(13))____________________ 5.7149E-04 ITV + W__concentration________________________________________________________ (fimp(14))____________________ 5.0000E-06 + Average_mass_of_all_ions_(amu)__________________________________________ (aion)________________________ 2.7252E+00 OP + Effective_charge________________________________________________________ (zeff)________________________ 2.5164E+00 + Density_profile_factor__________________________________________________ (alphan)______________________ 1.0000E+00 + Plasma_profile_model____________________________________________________ (ipedestal)___________________ 1 + Density_pedestal_r/a_location___________________________________________ (rhopedn)_____________________ 9.4000E-01 + Electron_density_pedestal_height_(/m3)__________________________________ (neped)_______________________ 6.3278E+19 OP + Electron_density_at_pedestal_/_nGW______________________________________ (fgwped_out)__________________ 8.5000E-01 + Temperature_pedestal_r/a_location_______________________________________ (rhopedt)_____________________ 9.4000E-01 + Pedestal_scaling_switch_________________________________________________ (ieped)_______________________ 0 + Electron_temp._pedestal_height_(keV)____________________________________ (teped)_______________________ 5.5000E+00 + Electron_temp._at_separatrix_(keV)______________________________________ (tesep)_______________________ 1.0000E-01 + Electron_density_at_separatrix_(/m3)____________________________________ (nesep)_______________________ 3.7223E+19 + Electron_density_at_separatrix_/_nGW____________________________________ (fgwsep_out)__________________ 5.0000E-01 + Temperature_profile_index_______________________________________________ (alphat)______________________ 1.4500E+00 + Temperature_profile_index_beta__________________________________________ (tbeta)_______________________ 2.0000E+00 + Old_ASDEX_model_________________________________________________________ (dlimit(1))___________________ 5.2797E+19 OP + Borrass_ITER_model_I____________________________________________________ (dlimit(2))___________________ 1.0969E+20 OP + Borrass_ITER_model_II___________________________________________________ (dlimit(3))___________________ 4.3575E+19 OP + JET_edge_radiation_model________________________________________________ (dlimit(4))___________________ 3.0227E+21 OP + JET_simplified_model____________________________________________________ (dlimit(5))___________________ 4.3397E+20 OP + Hugill-Murakami_Mq_model________________________________________________ (dlimit(6))___________________ 6.6609E+19 OP + Greenwald_model_________________________________________________________ (dlimit(7))___________________ 7.4445E+19 OP + Deuterium_fuel_fraction_________________________________________________ (fdeut)_______________________ 5.0000E-01 + Tritium_fuel_fraction___________________________________________________ (ftrit)_______________________ 5.0000E-01 + Total_fusion_power_(MW)_________________________________________________ (powfmw)______________________ 1.6202E+03 OP + _=____D-T_fusion_power_(MW)_____________________________________________ (pdt)_________________________ 1.6182E+03 OP + __+___D-D_fusion_power_(MW)_____________________________________________ (pdd)_________________________ 1.9494E+00 OP + __+_D-He3_fusion_power_(MW)_____________________________________________ (pdhe3)_______________________ 0.0000E+00 OP + Alpha_power:_total_(MW)_________________________________________________ (palpmw)______________________ 3.2365E+02 OP + Alpha_power:_beam-plasma_(MW)___________________________________________ (palpnb)______________________ 0.0000E+00 OP + Neutron_power_(MW)______________________________________________________ (pneutmw)_____________________ 1.2953E+03 OP + Charged_particle_power_(excluding_alphas)_(MW)__________________________ (pchargemw)___________________ 1.2659E+00 OP + Total_power_deposited_in_plasma_(MW)____________________________________ (tot_power_plasma)____________ 3.8950E+02 OP + Bremsstrahlung_radiation_power_(MW)_____________________________________ (pbrempv*vol)_________________ 6.5195E+01 OP + Line_radiation_power_(MW)_______________________________________________ (plinepv*vol)_________________ 1.4609E+02 OP + Synchrotron_radiation_power_(MW)________________________________________ (psyncpv*vol)_________________ 1.5187E+01 OP + Synchrotron_wall_reflectivity_factor____________________________________ (ssync)_______________________ 6.0000E-01 + Normalised_minor_radius_defining_'core'_________________________________ (coreradius)__________________ 7.5000E-01 + Fraction_of_core_radiation_subtracted_from_P_L__________________________ (coreradiationfraction)_______ 6.0000E-01 + Radiation_power_from_inner_zone_(MW)____________________________________ (pinnerzoneradmw)_____________ 9.1650E+01 OP + Radiation_power_from_outer_zone_(MW)____________________________________ (pouterzoneradmw)_____________ 1.3482E+02 OP + Total_radiation_power_from_inside_LCFS_(MW)_____________________________ (pradmw)______________________ 2.2647E+02 OP + LCFS_radiation_fraction_=_total_radiation_in_LCFS_/_total_power_deposite (rad_fraction_LCFS)___________ 5.8144E-01 OP + Nominal_mean_radiation_load_on_inside_surface_of_reactor_(MW/m2)________ (photon_wall)_________________ 1.7749E-01 OP + Peaking_factor_for_radiation_wall_load__________________________________ (peakfactrad)_________________ 3.3300E+00 IP + Maximum_permitted_radiation_wall_load_(MW/m^2)__________________________ (maxradwallload)______________ 1.0000E+00 IP + Peak_radiation_wall_load_(MW/m^2)_______________________________________ (peakradwallload)_____________ 5.9106E-01 OP + Fast_alpha_particle_power_incident_on_the_first_wall_(MW)_______________ (palpfwmw)____________________ 1.6182E+01 OP + Nominal_mean_neutron_load_on_inside_surface_of_reactor_(MW/m2)__________ (wallmw)______________________ 1.0152E+00 OP + Power_incident_on_the_divertor_targets_(MW)_____________________________ (ptarmw)______________________ 3.2606E+01 OP + Fraction_of_power_to_the_lower_divertor_________________________________ (ftar)________________________ 1.0000E+00 IP + Outboard_side_heat_flux_decay_length_(m)________________________________ (lambdaio)____________________ 1.5700E-03 OP + Fraction_of_power_on_the_inner_targets__________________________________ (fio)_________________________ 4.1000E-01 OP + Fraction_of_power_incident_on_the_lower_inner_target____________________ (fLI)_________________________ 4.1000E-01 OP + Fraction_of_power_incident_on_the_lower_outer_target____________________ (fLO)_________________________ 5.9000E-01 OP + Power_incident_on_the_lower_inner_target_(MW)___________________________ (pLImw)_______________________ 1.3368E+01 OP + Power_incident_on_the_lower_outer_target_(MW)___________________________ (pLOmw)_______________________ 1.9237E+01 OP + Ohmic_heating_power_(MW)________________________________________________ (pohmmw)______________________ 6.2284E-01 OP + Fraction_of_alpha_power_deposited_in_plasma_____________________________ (falpha)______________________ 9.5000E-01 + Fraction_of_alpha_power_to_electrons____________________________________ (falpe)_______________________ 7.1828E-01 + Fraction_of_alpha_power_to_ions_________________________________________ (falpi)_______________________ 2.8172E-01 + Ion_transport_(MW)______________________________________________________ (ptrimw)______________________ 1.4013E+02 OP + Electron_transport_(MW)_________________________________________________ (ptremw)______________________ 1.5772E+02 OP + Injection_power_to_ions_(MW)____________________________________________ (pinjimw)_____________________ 0.0000E+00 OP + Injection_power_to_electrons_(MW)_______________________________________ (pinjemw)_____________________ 8.0143E+01 OP + Ignited_plasma_switch_(0=not_ignited,_1=ignited)________________________ (ignite)______________________ 0 + Power_into_divertor_zone_via_charged_particles_(MW)_____________________ (pdivt)_______________________ 1.6303E+02 OP + Psep_/_R_ratio_(MW/m)___________________________________________________ (pdivt/rmajor)________________ 2.0378E+01 OP + Psep_Bt_/_qAR_ratio_(MWT/m)_____________________________________________ (pdivtbt/qar)_________________ 1.0000E+01 OP + ITER_1996_scaling:_nominal_(MW)_________________________________________ (pthrmw(1))___________________ 1.2978E+02 OP + ITER_1996_scaling:_upper_bound_(MW)_____________________________________ (pthrmw(2))___________________ 2.8603E+02 OP + ITER_1996_scaling:_lower_bound_(MW)_____________________________________ (pthrmw(3))___________________ 5.8098E+01 OP + ITER_1997_scaling_(1)_(MW)______________________________________________ (pthrmw(4))___________________ 2.1452E+02 OP + ITER_1997_scaling_(2)_(MW)______________________________________________ (pthrmw(5))___________________ 1.7206E+02 OP + Martin_2008_scaling:_nominal_(MW)_______________________________________ (pthrmw(6))___________________ 9.7416E+01 OP + Martin_2008_scaling:_95%_upper_bound_(MW)_______________________________ (pthrmw(7))___________________ 1.2769E+02 OP + Martin_2008_scaling:_95%_lower_bound_(MW)_______________________________ (pthrmw(8))___________________ 6.7143E+01 OP + Snipes_2000_scaling:_nominal_(MW)_______________________________________ (pthrmw(9))___________________ 6.7785E+01 OP + Snipes_2000_scaling:_upper_bound_(MW)___________________________________ (pthrmw(10))__________________ 9.9437E+01 OP + Snipes_2000_scaling:_lower_bound_(MW)___________________________________ (pthrmw(11))__________________ 4.5839E+01 OP + Snipes_2000_scaling_(closed_divertor):_nominal_(MW)_____________________ (pthrmw(12))__________________ 3.1010E+01 OP + Snipes_2000_scaling_(closed_divertor):_upper_bound_(MW)_________________ (pthrmw(13))__________________ 4.3148E+01 OP + Snipes_2000_scaling_(closed_divertor):_lower_bound_(MW)_________________ (pthrmw(14))__________________ 2.2130E+01 OP + Hubbard_2012_L-I_threshold_-_nominal_(MW)_______________________________ (pthrmw(15))__________________ 2.7549E+01 OP + Hubbard_2012_L-I_threshold_-_lower_bound_(MW)___________________________ (pthrmw(16))__________________ 1.4319E+01 OP + Hubbard_2012_L-I_threshold_-_upper_bound_(MW)___________________________ (pthrmw(17))__________________ 5.3005E+01 OP + Hubbard_2017_L-I_threshold______________________________________________ (pthrmw(18))__________________ 2.6202E+02 OP + Martin_2008_aspect_ratio_corrected_scaling:_nominal_(MW)________________ (pthrmw(19))__________________ 9.7416E+01 OP + Martin_2008_aspect_ratio_corrected_scaling:_95%_upper_bound_(MW)________ (pthrmw(20))__________________ 1.2769E+02 OP + Martin_2008_aspect_ratio_corrected_scaling:_95%_lower_bound_(MW)________ (pthrmw(21))__________________ 6.7143E+01 OP + L-H_threshold_power_(enforced)_(MW)_____________________________________ (boundl(103)*plhthresh)_______ 9.7416E+01 OP + L-H_threshold_power_(MW)________________________________________________ (plhthresh)___________________ 9.7416E+01 OP + Confinement_H_factor____________________________________________________ (hfact)_______________________ 1.1886E+00 ITV + Global_thermal_energy_confinement_time_(s)______________________________ (taueff)______________________ 3.2037E+00 + Ion_energy_confinement_time_(s)_________________________________________ (tauei)_______________________ 3.2037E+00 + Electron_energy_confinement_time_(s)____________________________________ (tauee)_______________________ 3.2037E+00 + n.tau_=_Volume-average_electron_density_x_Energy_confinement_time_(s/m3) (dntau)_______________________ 2.5843E+20 OP + Triple_product__(keV_s/m3)______________________________________________ (dntau*te)____________________ 3.2275E+21 OP + Transport_loss_power_assumed_in_scaling_law_(MW)________________________ (powerht)_____________________ 2.9785E+02 OP + Switch_for_radiation_loss_term_usage_in_power_balance___________________ (iradloss)____________________ 1 + Radiation_power_subtracted_from_plasma_power_balance_(MW)_______________ ______________________________ 9.1650E+01 OP + Alpha_particle_confinement_time_(s)_____________________________________ (taup)________________________ 2.2270E+01 + Alpha_particle/energy_confinement_time_ratio____________________________ (taup/taueff)_________________ 6.9512E+00 + Lower_limit_on_taup/taueff______________________________________________ (taulimit)____________________ 5.0000E+00 + Total_energy_confinement_time_including_radiation_loss_(s)______________ (total_energy_conf_time)______ 2.8018E+00 + Normalized_plasma_pressure_beta_as_defined_by_McDonald_et_al____________ (beta_mcdonald)_______________ 3.4553E-02 OP + Normalized_ion_Larmor_radius____________________________________________ (rho_star)____________________ 1.9603E-03 OP + Normalized_collisionality_______________________________________________ (nu_star)_____________________ 3.7266E-03 OP + Volume_measure_of_elongation____________________________________________ (kappaa_IPB)__________________ 1.6815E+00 OP + Total_volt-second_requirement_(Wb)______________________________________ (vsstt)_______________________ 5.5616E+02 OP + Inductive_volt-seconds_(Wb)_____________________________________________ (vsind)_______________________ 2.3585E+02 OP + Ejima_coefficient_______________________________________________________ (gamma)_______________________ 3.0000E-01 + Start-up_resistive_(Wb)_________________________________________________ (vsres)_______________________ 5.0159E+01 OP + Flat-top_resistive_(Wb)_________________________________________________ (vsbrn)_______________________ 2.7015E+02 OP + bootstrap_current_fraction_multiplier___________________________________ (cboot)_______________________ 1.0000E+00 + Bootstrap_fraction_(ITER_1989)__________________________________________ (bscf_iter89)_________________ 3.7098E-01 + Bootstrap_fraction_(Sauter_et_al)_______________________________________ (bscf_sauter)_________________ 4.1920E-01 + Bootstrap_fraction_(Nevins_et_al)_______________________________________ (bscf_nevins)_________________ 3.5042E-01 + Bootstrap_fraction_(Wilson)_____________________________________________ (bscf_wilson)_________________ 4.3349E-01 + Diamagnetic_fraction_(Hender)___________________________________________ (diacf_hender)________________ 1.2017E-02 + Diamagnetic_fraction_(SCENE)____________________________________________ (diacf_scene)_________________ 1.1139E-02 + Pfirsch-Schlueter_fraction_(SCENE)______________________________________ (pscf_scene)__________________ -3.0283E-03 + Bootstrap_fraction_(enforced)___________________________________________ (bootipf.)____________________ 4.1920E-01 + Diamagnetic_fraction_(enforced)_________________________________________ (diaipf.)_____________________ 0.0000E+00 + Pfirsch-Schlueter_fraction_(enforced)___________________________________ (psipf.)______________________ 0.0000E+00 + Loop_voltage_during_burn_(V)____________________________________________ (vburn)_______________________ 3.7450E-02 OP + Plasma_resistance_(ohm)_________________________________________________ (rplas)_______________________ 3.9755E-09 OP + Resistive_diffusion_time_(s)____________________________________________ (res_time)____________________ 3.0619E+03 OP + Plasma_inductance_(H)___________________________________________________ (rlp)_________________________ 1.4181E-05 OP + Coefficient_for_sawtooth_effects_on_burn_V-s_requirement________________ (csawth)______________________ 1.0000E+00 + Ratio_of_He_and_pellet_particle_confinement_times_______________________ (tauratio)____________________ 1.0000E+00 + Fuelling_rate_(nucleus-pairs/s)_________________________________________ (qfuel)_______________________ 3.3420E+21 OP + Fuel_burn-up_rate_(reactions/s)_________________________________________ (rndfuel)_____________________ 5.7755E+20 OP + Burn-up_fraction________________________________________________________ (burnup)______________________ 1.7282E-01 + # Energy confinement times, and required H-factors : # + # Current Drive System # + Current_drive_efficiency_model__________________________________________ (iefrf)_______________________ 10 + Secondary_current_drive_efficiency_model________________________________ (iefrffix)____________________ 0 + Ratio_of_power_for_flat-top_to_start-up_(MW)____________________________ (startupratio)________________ 1.0000E+00 + Auxiliary_power_used_for_plasma_heating_only_(MW)_______________________ (pheat)_______________________ 7.5000E+01 + Power_injected_for_current_drive_(MW)___________________________________ (pcurrentdrivemw)_____________ 5.1429E+00 + Maximum_Allowed_Bootstrap_current_fraction______________________________ (bscfmax)_____________________ 9.5000E-01 + Fusion_gain_factor_Q____________________________________________________ (bigq)________________________ 2.0060E+01 OP + Auxiliary_current_drive_(A)_____________________________________________ (auxiliary_cd)________________ 2.3908E+05 OP + Current_drive_efficiency_(A/W)__________________________________________ (effcd)_______________________ 4.6488E-02 OP + Normalised_current_drive_efficiency,_gamma_(10^20_A/W-m2)_______________ (gamcd)_______________________ 3.0000E-01 OP + Wall_plug_to_injector_efficiency________________________________________ (etacd)_______________________ 5.0000E-01 + ECRH_plasma_heating_efficiency__________________________________________ (gamma_ecrh)__________________ 3.0000E-01 + Bootstrap_fraction______________________________________________________ (bootipf)_____________________ 4.1920E-01 + Diamagnetic_fraction____________________________________________________ (diaipf)______________________ 0.0000E+00 + Pfirsch-Schlueter_fraction______________________________________________ (psipf)_______________________ 0.0000E+00 + Auxiliary_current_drive_fraction________________________________________ (faccd)_______________________ 1.4376E-02 + Inductive_fraction______________________________________________________ (facoh)_______________________ 5.6642E-01 + Total___________________________________________________________________ (plasipf+faccd+facoh)_________ 1.0000E+00 + Fraction_of_the_plasma_current_produced_by_non-inductive_means__________ (fvsbrnni)____________________ 4.3358E-01 ITV + Electron_cyclotron_injected_power_(MW)__________________________________ (echpwr)______________________ 8.0143E+01 OP + Maximum_allowable_ECRH_power_(MW)_______________________________________ (pinjalw)_____________________ 2.0000E+02 + ECH_wall_plug_efficiency________________________________________________ (etaech)______________________ 5.0000E-01 + ECH_wall_plug_power_(MW)________________________________________________ (echwpow)_____________________ 1.6029E+02 OP + Total_V-s_capability_of_Central_Solenoid/PF_coils_(Wb)__________________ (abs(vstot))__________________ 5.7728E+02 + Required_volt-seconds_during_start-up_(Wb)______________________________ (vssoft)______________________ 2.8601E+02 + Available_volt-seconds_during_burn_(Wb)_________________________________ (vsmax)_______________________ 2.7014E+02 + # Times # + Initial_charge_time_for_CS_from_zero_current_(s)________________________ (tramp)_______________________ 5.0000E+02 + Plasma_current_ramp-up_time_(s)_________________________________________ (tohs)________________________ 1.6631E+02 + Heating_time_(s)________________________________________________________ (theat)_______________________ 1.0000E+01 + Burn_time_(s)___________________________________________________________ (tburn)_______________________ 7.2035E+03 OP + Reset_time_to_zero_current_for_CS_(s)___________________________________ (tqnch)_______________________ 1.6631E+02 + Time_between_pulses_(s)_________________________________________________ (tdwell)______________________ 1.8000E+03 + Total_plant_cycle_time_(s)______________________________________________ (tcycle)______________________ 9.8463E+03 OP + # Radial Build # + TF_coil_radial_placement_switch_________________________________________ (tf_in_cs)____________________ 0 + TF_coil_radial_placement_switch_________________________________________ (tf_in_cs)____________________ 0 + Machine_bore_(m)________________________________________________________ (bore)________________________ 1.9854E+00 ITV + CS_radial_thickness_(m)_________________________________________________ (ohcth)_______________________ 5.7587E-01 ITV + CS_precompression_(m)___________________________________________________ (precomp)_____________________ 6.8064E-02 + CS_precompresion_to_TF_coil_radial_gap_(m)______________________________ (gapoh)_______________________ 8.0000E-02 + TF_coil_inboard_leg_(m)_________________________________________________ (tfcth)_______________________ 9.1597E-01 ITV + TF_coil_inboard_leg_insulation_gap_(m)__________________________________ (tftsgap)_____________________ 5.0000E-02 + Thermal_shield,_inboard_(m)_____________________________________________ (thshield_ib)_________________ 5.0000E-02 + thermal_shield_to_vessel_radial_gap_(m)_________________________________ (gapds)_______________________ 2.0000E-02 + Inboard_vacuum_vessel_radial_thickness_(m)______________________________ (d_vv_in)_____________________ 3.0000E-01 + Inner_radiation_shield_radial_thickness_(m)_____________________________ (shldith)_____________________ 3.0000E-01 + Gap_(m)_________________________________________________________________ (vvblgap)_____________________ 2.0000E-02 + Inboard_blanket_radial_thickness_(m)____________________________________ (blnkith)_____________________ 7.0000E-01 + Inboard_first_wall_radial_thickness_(m)_________________________________ (fwith)_______________________ 1.8000E-02 + Inboard_scrape-off_radial_thickness_(m)_________________________________ (scrapli)_____________________ 2.5000E-01 + Outboard_scrape-off_radial_thickness_(m)________________________________ (scraplo)_____________________ 2.5000E-01 + Outboard_first_wall_radial_thickness_(m)________________________________ (fwoth)_______________________ 1.8000E-02 + Outboard_blanket_radial_thickness_(m)___________________________________ (blnkoth)_____________________ 1.0000E+00 + Outer_radiation_shield_radial_thickness_(m)_____________________________ (shldoth)_____________________ 8.0000E-01 + Outboard_vacuum_vessel_radial_thickness_(m)_____________________________ (d_vv_out)____________________ 3.0000E-01 + Vessel_to_TF_radial_gap_(m)_____________________________________________ (gapsto)______________________ 1.3720E+00 + Thermal_shield,_outboard_(m)____________________________________________ (thshield_ob)_________________ 5.0000E-02 + Gap_(m)_________________________________________________________________ (tftsgap)_____________________ 5.0000E-02 + TF_coil_outboard_leg_radial_thickness_(m)_______________________________ (tfthko)______________________ 9.1597E-01 + # Vertical Build # + Divertor_null_switch____________________________________________________ (i_single_null)_______________ 1 + Vessel_-_TF_coil_vertical_gap_(m)_______________________________________ (vgap2)_______________________ 1.6300E-01 + Topside_vacuum_vessel_radial_thickness_(m)______________________________ (d_vv_top)____________________ 3.0000E-01 + Top_radiation_shield_thickness_(m)______________________________________ (shldtth)_____________________ 6.0000E-01 + Top_blanket_vertical_thickness_(m)______________________________________ (blnktth)_____________________ 8.5000E-01 + Top_first_wall_vertical_thickness_(m)___________________________________ (fwtth)_______________________ 1.8000E-02 + Top_scrape-off_vertical_thickness_(m)___________________________________ (vgaptop)_____________________ 6.0000E-01 + Plasma_half-height_(m)__________________________________________________ (rminor*kappa)________________ 4.9333E+00 + Bottom_scrape-off_vertical_thickness_(m)________________________________ (vgap)________________________ 2.0019E+00 + Divertor_structure_vertical_thickness_(m)_______________________________ (divfix)______________________ 6.2000E-01 + Bottom_radiation_shield_thickness_(m)___________________________________ (shldlth)_____________________ 7.0000E-01 + Underside_vacuum_vessel_radial_thickness_(m)____________________________ (d_vv_bot)____________________ 3.0000E-01 + External_cryostat_thickness_(m)_________________________________________ (ddwex)_______________________ 1.5000E-01 + Ratio_of_Central_solenoid_height_to_TF_coil_internal_height_____________ (ohhghf)______________________ 9.0000E-01 + Width_of_neutral_beam_duct_where_it_passes_between_the_TF_coils_(m)_____ (beamwd)______________________ 5.8000E-01 + # Divertor build and plasma position # + Plasma_top_position,_radial_(m)_________________________________________ (ptop_radial)_________________ 6.6667E+00 + Plasma_top_position,_vertical_(m)_______________________________________ (ptop_vertical)_______________ 4.9333E+00 + Plasma_geometric_centre,_radial_(m)_____________________________________ (physics_variables.rmajor.)___ 8.0000E+00 + Plasma_geometric_centre,_vertical_(m)___________________________________ (0.0)_________________________ 0.0000E+00 + Plasma_lower_physics_variables.triangularity____________________________ (tril)________________________ 5.0000E-01 + Plasma_elongation_______________________________________________________ (physics_variables.kappa.)____ 1.8500E+00 + TF_coil_vertical_offset_(m)_____________________________________________ (tfoffset)____________________ -6.1694E-01 + Plasma_outer_arc_radius_of_curvature_(m)________________________________ (rco)_________________________ 5.0422E+00 + Plasma_inner_arc_radius_of_curvature_(m)________________________________ (rci)_________________________ 9.7933E+00 + Plasma_lower_X-pt,_radial_(m)___________________________________________ (rxpt)________________________ 6.6667E+00 + Plasma_lower_X-pt,_vertical_(m)_________________________________________ (zxpt)________________________ -4.9333E+00 + Poloidal_plane_angle_between_vertical_and_inner_leg_(rad)_______________ (thetai)______________________ 2.0820E-01 + Poloidal_plane_angle_between_vertical_and_outer_leg_(rad)_______________ (thetao)______________________ 1.0429E+00 + Poloidal_plane_angle_between_inner_leg_and_plate_(rad)__________________ (betai)_______________________ 1.0000E+00 + Poloidal_plane_angle_between_outer_leg_and_plate_(rad)__________________ (betao)_______________________ 1.0000E+00 + Inner_divertor_leg_poloidal_length_(m)__________________________________ (plsepi)______________________ 1.0000E+00 + Outer_divertor_leg_poloidal_length_(m)__________________________________ (plsepo)______________________ 1.5000E+00 + Inner_divertor_plate_length_(m)_________________________________________ (plleni)______________________ 1.0000E+00 + Outer_divertor_plate_length_(m)_________________________________________ (plleno)______________________ 1.0000E+00 + Inner_strike_point,_radial_(m)__________________________________________ (rspi)________________________ 5.6883E+00 + Inner_strike_point,_vertical_(m)________________________________________ (zspi)________________________ -5.1400E+00 + Inner_plate_top,_radial_(m)_____________________________________________ (rplti)_______________________ 5.8656E+00 + Inner_plate_top,_vertical_(m)___________________________________________ (zplti)_______________________ -4.6725E+00 + Inner_plate_bottom,_radial_(m)__________________________________________ (rplbi)_______________________ 5.5109E+00 + Inner_plate_bottom,_vertical_(m)________________________________________ (zplbi)_______________________ -5.6075E+00 + Outer_strike_point,_radial_(m)__________________________________________ (rspo)________________________ 7.4223E+00 + Outer_strike_point,_vertical_(m)________________________________________ (zspo)________________________ -6.2291E+00 + Outer_plate_top,_radial_(m)_____________________________________________ (rplto)_______________________ 7.6496E+00 + Outer_plate_top,_vertical_(m)___________________________________________ (zplto)_______________________ -5.7838E+00 + Outer_plate_bottom,_radial_(m)__________________________________________ (rplbo)_______________________ 7.1949E+00 + Outer_plate_bottom,_vertical_(m)________________________________________ (zplbo)_______________________ -6.6744E+00 + Calculated_maximum_divertor_height_(m)__________________________________ (divht)_______________________ 2.0019E+00 + # TF coils # + Allowable_maximum_shear_stress_in_TF_coil_case_(Tresca_criterion)_(Pa)__ (sig_tf_case_max)_____________ 7.5000E+08 + Allowable_maximum_shear_stress_in_TF_coil_conduit_(Tresca_criterion)_(Pa (sig_tf_wp_max)_______________ 7.5000E+08 + WP_transverse_modulus_(GPa)_____________________________________________ (eyoung_wp_trans*1.0d-9)______ 4.3534E+01 OP + WP_vertical_modulus_(GPa)_______________________________________________ (eyoung_wp_axial*1.0d-9)______ 1.1510E+02 OP + WP_transverse_Poissons_ratio____________________________________________ (poisson_wp_trans)____________ 3.0390E-01 OP + WP_vertical-transverse_Pois._rat._______________________________________ (poisson_wp_axial)____________ 3.1568E-01 OP + Radial____stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_r_max(1))_____________ 4.8849E-08 + toroidal__stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_t_max(1))_____________ -4.8724E+08 + Vertical__stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_z_max(1))_____________ 2.6028E+08 + Von-Mises_stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_vmises_max(1))________ 6.5725E+08 + Maximum_shear_stress_for_the_Tresca_yield_criterion_1_(Pa)______________ (sig_tf_tresca_max(1))________ 7.4752E+08 + Radial____stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_r_max(2))_____________ -1.5411E+08 + toroidal__stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_t_max(2))_____________ -3.7861E+08 + Vertical__stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_z_max(2))_____________ 2.6028E+08 + Von-Mises_stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_vmises_max(2))________ 5.5645E+08 + Maximum_shear_stress_for_the_Tresca_yield_criterion_2_(Pa)______________ (sig_tf_tresca_max(2))________ 6.3889E+08 + Radial____stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_r_max(3))_____________ 6.1398E+06 + toroidal__stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_t_max(3))_____________ -3.6314E+08 + Vertical__stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_z_max(3))_____________ 1.4510E+08 + Von-Mises_stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_vmises_max(3))________ 4.5345E+08 + Maximum_shear_stress_for_the_Tresca_yield_criterion_3_(Pa)______________ (sig_tf_tresca_max(3))________ 5.0824E+08 + Maximum_radial_deflection_at_midplane_(m)_______________________________ (deflect)_____________________ -6.2714E-03 OP + Vertical_strain_on_casing_______________________________________________ (casestr)_____________________ 1.2697E-03 OP + Radial_strain_on_insulator______________________________________________ (insstrain)___________________ -7.6923E-03 OP + Conductor_technology____________________________________________________ (i_tf_sup)____________________ 1 + Superconductor_material_________________________________________________ (i_tf_sc_mat)_________________ 1 + Presence_of_TF_demountable_joints_______________________________________ (itart)_______________________ 0 + TF_inboard_leg_support_strategy_________________________________________ (i_tf_bucking)________________ 1 + Number_of_TF_coils______________________________________________________ (n_tf)________________________ 16 + Inboard_leg_centre_radius_(m)___________________________________________ (r_tf_inboard_mid)____________ 3.1673E+00 OP + Outboard_leg_centre_radius_(m)__________________________________________ (r_tf_outboard_mid)___________ 1.4985E+01 OP + Total_inboard_leg_radial_thickness_(m)__________________________________ (tfcth)_______________________ 9.1597E-01 ITV + Total_outboard_leg_radial_thickness_(m)_________________________________ (tfthko)______________________ 9.1597E-01 + Outboard_leg_toroidal_thickness_(m)_____________________________________ (tftort)______________________ 1.4145E+00 OP + Maximum_inboard_edge_height_(m)_________________________________________ (hmax)________________________ 8.8182E+00 OP + Mean_coil_circumference_(including_inboard_leg_length)_(m)______________ (tfleng)______________________ 4.7937E+01 OP + Vertical_TF_shape_______________________________________________________ (i_tf_shape)__________________ 1 + TF_coil_arc_point_0_R_(m)_______________________________________________ (xarc(1))_____________________ 3.6253E+00 + TF_coil_arc_point_0_Z_(m)_______________________________________________ (yarc(1))_____________________ 4.5506E+00 + TF_coil_arc_point_1_R_(m)_______________________________________________ (xarc(2))_____________________ 7.4667E+00 + TF_coil_arc_point_1_Z_(m)_______________________________________________ (yarc(2))_____________________ 7.5843E+00 + TF_coil_arc_point_2_R_(m)_______________________________________________ (xarc(3))_____________________ 1.4527E+01 + TF_coil_arc_point_2_Z_(m)_______________________________________________ (yarc(3))_____________________ 0.0000E+00 + TF_coil_arc_point_3_R_(m)_______________________________________________ (xarc(4))_____________________ 7.4667E+00 + TF_coil_arc_point_3_Z_(m)_______________________________________________ (yarc(4))_____________________ -8.8182E+00 + TF_coil_arc_point_4_R_(m)_______________________________________________ (xarc(5))_____________________ 3.6253E+00 + TF_coil_arc_point_4_Z_(m)_______________________________________________ (yarc(5))_____________________ -5.2909E+00 + TF_cross-section_(total)_(m2)___________________________________________ (tfareain)____________________ 1.8229E+01 + Total_steel_cross-section_(m2)__________________________________________ (a_tf_steel*n_tf)_____________ 1.2853E+01 + Total_steel_TF_fraction_________________________________________________ (f_tf_steel)__________________ 7.0508E-01 + Total_Insulation_cross-section_(total)_(m2)_____________________________ (a_tf_ins*n_tf)_______________ 8.4752E-01 + Total_Insulation_fraction_______________________________________________ (f_tf_ins)____________________ 4.6493E-02 + Casing_cross_section_area_(per_leg)_(m2)________________________________ (acasetf)_____________________ 5.6444E-01 + Inboard_leg_case_plasma_side_wall_thickness_(m)_________________________ (casthi)______________________ 6.0000E-02 + Inboard_leg_case_inboard_"nose"_thickness_(m)___________________________ (thkcas)______________________ 2.8216E-01 ITV + Inboard_leg_case_sidewall_thickness_at_its_narrowest_point_(m)__________ (casths)______________________ 5.0000E-02 + External_case_mass_per_coil_(kg)________________________________________ (whtcas)______________________ 5.5456E+05 OP + WP_cross_section_area_with_insulation_and_insertion_(per_coil)_(m2)_____ (awpc)________________________ 5.7486E-01 + WP_cross_section_area_(per_coil)_(m2)___________________________________ (aswp)________________________ 5.1696E-01 + Winding_pack_radial_thickness_(m)_______________________________________ (dr_tf_wp)____________________ 5.0416E-01 ITV + Winding_pack_toroidal_width_1_(m)_______________________________________ (wwp1)________________________ 1.1904E+00 OP + Winding_pack_toroidal_width_2_(m)_______________________________________ (wwp2)________________________ 1.0901E+00 OP + Ground_wall_insulation_thickness_(m)____________________________________ (tinstf)______________________ 8.0000E-03 + Winding_pack_insertion_gap_(m)__________________________________________ (tfinsgap)____________________ 1.0000E-02 + Steel_WP_cross-section_(total)_(m2)_____________________________________ (aswp*n_tf)___________________ 3.8217E+00 + Steel_WP_fraction_______________________________________________________ (aswp/awpc)___________________ 4.1550E-01 + Insulation_WP_fraction__________________________________________________ (aiwp/awpc)___________________ 4.7934E-02 + Cable_WP_fraction_______________________________________________________ ((awpc-aswp-aiwp)/awpc)_______ 5.3656E-01 + Turn_parametrisation____________________________________________________ (i_tf_turns_integer)__________ 0 + Number_of_turns_per_TF_coil_____________________________________________ (n_tf_turn)___________________ 1.4739E+02 OP + Width_of_turn_including_inter-turn_insulation_(m)_______________________ (t_turn_tf)___________________ 5.9223E-02 OP + Width_of_conductor_(square)_(m)_________________________________________ (t_conductor)_________________ 5.7623E-02 OP + Width_of_space_inside_conductor_(m)_____________________________________ (t_cable)_____________________ 4.1604E-02 OP + Steel_conduit_thickness_(m)_____________________________________________ (thwcndut)____________________ 8.0099E-03 ITV + Inter-turn_insulation_thickness_(m)_____________________________________ (thicndut)____________________ 8.0000E-04 + Diameter_of_central_helium_channel_in_cable_____________________________ (dhecoil)_____________________ 1.0000E-02 + internal_area_of_the_cable_space________________________________________ (acstf)_______________________ 1.6999E-03 + Coolant_fraction_in_conductor_excluding_central_channel_________________ (vftf)________________________ 3.0000E-01 + Copper_fraction_of_conductor____________________________________________ (fcutfsu)_____________________ 8.4212E-01 ITV + Superconductor_fraction_of_conductor____________________________________ (1-fcutfsu)___________________ 1.5788E-01 + Check_total_area_fractions_in_winding_pack_=_1__________________________ ______________________________ 1.0000E+00 + minimum_TF_conductor_temperature_margin__(K)____________________________ (tmargmin_tf)_________________ 1.5000E+00 + TF_conductor_temperature_margin_(K)_____________________________________ (tmargtf)_____________________ 1.5049E+00 + Elastic_properties_behavior_____________________________________________ (i_tf_cond_eyoung_axial)______ 0 + Conductor_axial_Youngs_modulus__________________________________________ (eyoung_cond_axial)___________ 0.0000E+00 + Conductor_transverse_Youngs_modulus_____________________________________ (eyoung_cond_trans)___________ 0.0000E+00 + Superconductor_mass_per_coil_(kg)_______________________________________ (whtconsc)____________________ 4.6964E+03 OP + Copper_mass_per_coil_(kg)_______________________________________________ (whtconcu)____________________ 5.8073E+04 OP + Steel_conduit_mass_per_coil_(kg)________________________________________ (whtconsh)____________________ 8.9310E+04 OP + Conduit_insulation_mass_per_coil_(kg)___________________________________ (whtconin)____________________ 2.3777E+03 OP + Total_conduit_mass_per_coil_(kg)________________________________________ (whtcon)______________________ 1.5446E+05 OP + Mass_of_each_TF_coil_(kg)_______________________________________________ (whttf/n_tf)__________________ 7.1402E+05 OP + Total_TF_coil_mass_(kg)_________________________________________________ (whttf)_______________________ 1.1424E+07 OP + Nominal_peak_field_assuming_toroidal_symmetry_(T)_______________________ (bmaxtf)______________________ 1.2178E+01 OP + Total_current_in_all_TF_coils_(MA)______________________________________ (ritfc/1.D6)__________________ 2.1176E+02 OP + TF_coil_current_(summed_over_all_coils)_(A)_____________________________ (ritfc)_______________________ 2.1176E+08 + Actual_peak_field_at_discrete_conductor_(T)_____________________________ (bmaxtfrp)____________________ 1.2636E+01 OP + Winding_pack_current_density_(A/m2)_____________________________________ (jwptf)_______________________ 2.5602E+07 OP + Inboard_leg_mid-plane_conductor_current_density_(A/m2)__________________ (oacdcp)______________________ 1.1617E+07 + Total_stored_energy_in_TF_coils_(GJ)____________________________________ (estotftgj)___________________ 1.2161E+02 OP + Inboard_vertical_tension_per_coil_(N)___________________________________ (vforce)______________________ 2.0908E+08 OP + Outboard_vertical_tension_per_coil_(N)__________________________________ (vforce_outboard)_____________ 2.0908E+08 OP + inboard_vertical_tension_fraction_(-)___________________________________ (f_vforce_inboard)____________ 5.0000E-01 OP + Centring_force_per_coil_(N/m)___________________________________________ (cforce)______________________ 8.0590E+07 OP + Max_allowed_tfcoil_variables.ripple_amplitude_at_plasma_outboard_midplan (ripmax)______________________ 6.0000E-01 + Ripple_amplitude_at_plasma_outboard_midplane_(%)________________________ (ripple)______________________ 6.0000E-01 OP + Actual_quench_time_(or_time_constant)_(s)_______________________________ (tdmptf)______________________ 1.8429E+01 ITV + Vacuum_Vessel_stress_on_quench_(Pa)_____________________________________ (vv_stress_quench)____________ 6.1442E+07 OP + Maximum_allowed_voltage_during_quench_due_to_insulation_(kV)____________ (vdalw)_______________________ 9.5837E+00 ITV + Actual_quench_voltage_(kV)______________________________________________ (vtfskv)______________________ 9.1862E+00 OP + Maximum_allowed_temp_rise_during_a_quench_(K)___________________________ (tmaxpro)_____________________ 1.5000E+02 + # Superconducting TF Coils # + Superconductor_switch___________________________________________________ (isumat)______________________ 1 + Critical_field_at_zero_temperature_and_strain_(T)_______________________ (bc20m)_______________________ 3.2970E+01 + Critical_temperature_at_zero_field_and_strain_(K)_______________________ (tc0m)________________________ 1.6060E+01 + Helium_temperature_at_peak_field_(=_superconductor_temperature)_(K)_____ (thelium)_____________________ 4.7500E+00 + Total_helium_fraction_inside_cable_space________________________________ (fhetot)______________________ 3.4620E-01 OP + Copper_fraction_of_conductor____________________________________________ (fcutfsu)_____________________ 8.4212E-01 ITV + Residual_manufacturing_strain_on_superconductor_________________________ (str_tf_con_res)______________ -5.0000E-03 + Self-consistent_strain_on_superconductor________________________________ (str_wp)______________________ 2.0730E-03 + Critical_current_density_in_superconductor_(A/m2)_______________________ (jcritsc)_____________________ 7.1337E+08 OP + Critical_current_density_in_strand_(A/m2)_______________________________ (jcritstr)____________________ 1.1263E+08 OP + Critical_current_density_in_winding_pack_(A/m2)_________________________ (jwdgcrt)_____________________ 3.5688E+07 OP + Actual_current_density_in_winding_pack_(A/m2)___________________________ (jwdgop)______________________ 2.5602E+07 OP + Minimum_allowed_temperature_margin_in_superconductor_(K)________________ (tmargmin_tf)_________________ 1.5000E+00 + Actual_temperature_margin_in_superconductor_(K)_________________________ (tmarg)_______________________ 1.5049E+00 OP + Critical_current_(A)____________________________________________________ (icrit)_______________________ 1.2517E+05 OP + Actual_current_(A)______________________________________________________ (cpttf)_______________________ 8.9795E+04 ITV + Actual_current_/_critical_current_______________________________________ (iooic)_______________________ 7.1737E-01 OP + # Central Solenoid and PF Coils # + Central_solenoid_superconductor_material________________________________ (isumatoh)____________________ 1 + Maximum_field_at_Beginning_Of_Pulse_(T)_________________________________ (bmaxoh0)_____________________ 1.4050E+01 OP + Critical_superconductor_current_density_at_BOP_(A/m2)___________________ (jscoh_bop)___________________ 3.4918E+08 OP + Critical_strand_current_density_at_BOP_(A/m2)___________________________ (jstrandoh_bop)_______________ 1.0475E+08 OP + Allowable_overall_current_density_at_BOP_(A/m2)_________________________ (rjohc0)______________________ 3.5294E+07 OP + Actual_overall_current_density_at_BOP_(A/m2)____________________________ (cohbop)______________________ 1.9126E+07 OP + Maximum_field_at_End_Of_Flattop_(T)_____________________________________ (bmaxoh)______________________ 1.3920E+01 OP + Critical_superconductor_current_density_at_EOF_(A/m2)___________________ (jscoh_eof)___________________ 3.6097E+08 OP + Critical_strand_current_density_at_EOF_(A/m2)___________________________ (jstrandoh_eof)_______________ 1.0829E+08 OP + Allowable_overall_current_density_at_EOF_(A/m2)_________________________ (rjohc)_______________________ 3.6485E+07 OP + Actual_overall_current_density_at_EOF_(A/m2)____________________________ (coheof)______________________ 2.0264E+07 ITV + CS_inside_radius_(m)____________________________________________________ (bore)________________________ 1.9854E+00 ITV + CS_thickness_(m)________________________________________________________ (ohcth)_______________________ 5.7587E-01 ITV + Gap_between_central_solenoid_and_TF_coil_(m)____________________________ (gapoh)_______________________ 8.0000E-02 + CS_overall_cross-sectional_area_(m2)____________________________________ (areaoh)______________________ 9.1407E+00 OP + CS_conductor+void_cross-sectional_area_(m2)_____________________________ (awpoh)_______________________ 4.3996E+00 OP + ___CS_conductor_cross-sectional_area_(m2)_______________________________ (awpoh*(1-vfohc))_____________ 3.0797E+00 OP + ___CS_void_cross-sectional_area_(m2)____________________________________ (awpoh*vfohc)_________________ 1.3199E+00 OP + CS_steel_cross-sectional_area_(m2)______________________________________ (areaoh-awpoh)________________ 4.7411E+00 OP + CS_steel_area_fraction__________________________________________________ (oh_steel_frac)_______________ 5.1868E-01 ITV + Switch_for_CS_stress_calculation________________________________________ (i_cs_stress)_________________ 0 + Allowable_stress_in_CS_steel_(Pa)_______________________________________ (alstroh)_____________________ 7.5000E+08 + Hoop_stress_in_CS_steel_(Pa)____________________________________________ (sig_hoop)____________________ 6.7569E+08 OP + Axial_stress_in_CS_steel_(Pa)___________________________________________ (sig_axial)___________________ -7.6205E+08 OP + Maximum_shear_stress_in_CS_steel_for_the_Tresca_criterion_(Pa)__________ (s_tresca_oh)_________________ 6.7569E+08 OP + Axial_force_in_CS_(N)___________________________________________________ (axial_force)_________________ -1.6256E+09 OP + Residual_manufacturing_strain_in_CS_superconductor_material_____________ (tfcoil_variables.str_cs_con_r -5.0000E-03 + Copper_fraction_in_strand_______________________________________________ (fcuohsu)_____________________ 7.0000E-01 + Void_(coolant)_fraction_in_conductor____________________________________ (vfohc)_______________________ 3.0000E-01 + Helium_coolant_temperature_(K)__________________________________________ (tftmp)_______________________ 4.7500E+00 + CS_temperature_margin_(K)_______________________________________________ (tmargoh)_____________________ 1.5052E+00 OP + Minimum_permitted_temperature_margin_(K)________________________________ (tmargmin_cs)_________________ 1.5000E+00 + Residual_hoop_stress_in_CS_Steel_(Pa)___________________________________ (residual_sig_hoop)___________ 2.4000E+08 + Minimum_burn_time_(s)___________________________________________________ (tbrnmn)______________________ 7.2000E+03 + Initial_vertical_crack_size_(m)_________________________________________ (t_crack_vertical)____________ 8.9000E-04 + Initial_radial_crack_size_(m)___________________________________________ (t_crack_radial)______________ 2.6700E-03 + CS_turn_area_(m)________________________________________________________ (a_oh_turn)___________________ 1.9739E-03 + CS_turn_length_(m)______________________________________________________ (l_cond_cst)__________________ 7.6953E-02 + CS_turn_internal_cable_space_radius_(m)_________________________________ (r_in_cst)____________________ 7.4740E-03 + CS_turn_width_(m)_______________________________________________________ (d_cond_cst)__________________ 2.5651E-02 + CS_structural_vertical_thickness_(m)____________________________________ (t_structural_vertical)_______ 5.3514E-03 + CS_structural_radial_thickness_(m)______________________________________ (t_structural_radial)_________ 5.3514E-03 + Allowable_number_of_cycles_till_CS_fracture_____________________________ (n_cycle)_____________________ 1.3378E+02 OP + Minimum_number_of_cycles_required_till_CS_fracture______________________ (n_cycle_min)_________________ 2.0000E+04 OP + PF_coil_superconductor_material_________________________________________ (isumatpf)____________________ 3 + Copper_fraction_in_conductor____________________________________________ (fcupfsu)_____________________ 6.9000E-01 + Maximum_permissible_tensile_stress_(MPa)________________________________ (sigpfcalw)___________________ 5.0000E+02 + JxB_hoop_force_fraction_supported_by_case_______________________________ (sigpfcf)_____________________ 6.6600E-01 + PF_coil_0_radius_(m)____________________________________________________ (rpf[0]_______________________ 5.5667E+00 + PF_coil_0_vertical_position_(m)_________________________________________ (zpf[0])______________________ 9.3603E+00 + PF_coil_0_radial_thickness_(m)__________________________________________ (pfdr(0))_____________________ 1.2727E+00 + PF_coil_0_vertical_thickness_(m)________________________________________ (pfdz(0))_____________________ 1.2727E+00 + PF_coil_0_turns_________________________________________________________ (turns[0])____________________ 4.4541E+02 + PF_coil_0_current_(MA)__________________________________________________ (ric[0])______________________ 1.7816E+01 + PF_coil_0_field_(T)_____________________________________________________ (bpf[0])______________________ 6.2280E+00 + PF_coil_1_radius_(m)____________________________________________________ (rpf[1]_______________________ 5.5667E+00 + PF_coil_1_vertical_position_(m)_________________________________________ (zpf[1])______________________ -1.0594E+01 + PF_coil_1_radial_thickness_(m)__________________________________________ (pfdr(1))_____________________ 1.3651E+00 + PF_coil_1_vertical_thickness_(m)________________________________________ (pfdz(1))_____________________ -1.3651E+00 + PF_coil_1_turns_________________________________________________________ (turns[1])____________________ 5.1248E+02 + PF_coil_1_current_(MA)__________________________________________________ (ric[1])______________________ 2.0499E+01 + PF_coil_1_field_(T)_____________________________________________________ (bpf[1])______________________ 6.6990E+00 + PF_coil_2_radius_(m)____________________________________________________ (rpf[2]_______________________ 1.6731E+01 + PF_coil_2_vertical_position_(m)_________________________________________ (zpf[2])______________________ 2.6667E+00 + PF_coil_2_radial_thickness_(m)__________________________________________ (pfdr(2))_____________________ 1.1332E+00 + PF_coil_2_vertical_thickness_(m)________________________________________ (pfdz(2))_____________________ 1.1332E+00 + PF_coil_2_turns_________________________________________________________ (turns[2])____________________ 1.9262E+02 + PF_coil_2_current_(MA)__________________________________________________ (ric[2])______________________ -7.7049E+00 + PF_coil_2_field_(T)_____________________________________________________ (bpf[2])______________________ 2.6389E+00 + PF_coil_3_radius_(m)____________________________________________________ (rpf[3]_______________________ 1.6731E+01 + PF_coil_3_vertical_position_(m)_________________________________________ (zpf[3])______________________ -2.6667E+00 + PF_coil_3_radial_thickness_(m)__________________________________________ (pfdr(3))_____________________ 1.1332E+00 + PF_coil_3_vertical_thickness_(m)________________________________________ (pfdz(3))_____________________ -1.1332E+00 + PF_coil_3_turns_________________________________________________________ (turns[3])____________________ 1.9262E+02 + PF_coil_3_current_(MA)__________________________________________________ (ric[3])______________________ -7.7049E+00 + PF_coil_3_field_(T)_____________________________________________________ (bpf[3])______________________ 2.6389E+00 + PF_coil_4_radius_(m)____________________________________________________ (rpf[4]_______________________ 1.5209E+01 + PF_coil_4_vertical_position_(m)_________________________________________ (zpf[4])______________________ 7.4667E+00 + PF_coil_4_radial_thickness_(m)__________________________________________ (pfdr(4))_____________________ 8.0773E-01 + PF_coil_4_vertical_thickness_(m)________________________________________ (pfdz(4))_____________________ 8.0773E-01 + PF_coil_4_turns_________________________________________________________ (turns[4])____________________ 1.3049E+02 + PF_coil_4_current_(MA)__________________________________________________ (ric[4])______________________ -5.2194E+00 + PF_coil_4_field_(T)_____________________________________________________ (bpf[4])______________________ 2.5737E+00 + PF_coil_5_radius_(m)____________________________________________________ (rpf[5]_______________________ 1.5209E+01 + PF_coil_5_vertical_position_(m)_________________________________________ (zpf[5])______________________ -7.4667E+00 + PF_coil_5_radial_thickness_(m)__________________________________________ (pfdr(5))_____________________ 8.0773E-01 + PF_coil_5_vertical_thickness_(m)________________________________________ (pfdz(5))_____________________ -8.0773E-01 + PF_coil_5_turns_________________________________________________________ (turns[5])____________________ 1.3049E+02 + PF_coil_5_current_(MA)__________________________________________________ (ric[5])______________________ -5.2194E+00 + PF_coil_5_field_(T)_____________________________________________________ (bpf[5])______________________ 2.5737E+00 + Central_solenoid_radius_(m)_____________________________________________ (rpf[nohc-1])_________________ 2.2734E+00 + Central_solenoid_vertical_position_(m)__________________________________ (zpf[nohc-1])_________________ 0.0000E+00 + Central_solenoid_radial_thickness_(m)___________________________________ (ohdr)________________________ 5.7587E-01 + Central_solenoid_vertical_thickness_(m)_________________________________ (ohdz)________________________ 1.5873E+01 + Central_solenoid_turns__________________________________________________ (turns[nohc-1])_______________ 4.6308E+03 + Central_solenoid_current_(MA)___________________________________________ (ric[nohc-1])_________________ -1.8523E+02 + Central_solenoid_field_(T)______________________________________________ (bpf[nohc-1])_________________ 1.4050E+01 + Sum_of_squares_of_residuals_____________________________________________ (ssq0)________________________ 3.5207E-04 OP + Smoothing_parameter_____________________________________________________ (alfapf)______________________ 5.0000E-10 + # Volt Second Consumption # + Total_volt-second_consumption_by_coils_(Wb)_____________________________ (vstot)_______________________ -5.8000E+02 OP + # Waveforms # + Ratio_of_central_solenoid_current_at_beginning_of_Pulse_/_end_of_flat-to (fcohbop)_____________________ 9.4380E-01 ITV + Ratio_of_central_solenoid_current_at_beginning_of_Flat-top_/_end_of_flat (fcohbof)_____________________ -1.4083E-01 OP + # PF Circuit Waveform Data # + Number_of_PF_circuits_including_CS_and_plasma___________________________ (ncirt)_______________________ 8 + PF_Circuit_0_Time_point_0_(A)___________________________________________ (pfc0t0)______________________ 0.0000E+00 + PF_Circuit_0_Time_point_1_(A)___________________________________________ (pfc0t1)______________________ 1.3971E+07 + PF_Circuit_0_Time_point_2_(A)___________________________________________ (pfc0t2)______________________ 1.7816E+07 + PF_Circuit_0_Time_point_3_(A)___________________________________________ (pfc0t3)______________________ 1.7816E+07 + PF_Circuit_0_Time_point_4_(A)___________________________________________ (pfc0t4)______________________ 9.2844E+05 + PF_Circuit_0_Time_point_5_(A)___________________________________________ (pfc0t5)______________________ 0.0000E+00 + PF_Circuit_1_Time_point_0_(A)___________________________________________ (pfc1t0)______________________ 0.0000E+00 + PF_Circuit_1_Time_point_1_(A)___________________________________________ (pfc1t1)______________________ 1.8269E+07 + PF_Circuit_1_Time_point_2_(A)___________________________________________ (pfc1t2)______________________ 2.0499E+07 + PF_Circuit_1_Time_point_3_(A)___________________________________________ (pfc1t3)______________________ 2.0499E+07 + PF_Circuit_1_Time_point_4_(A)___________________________________________ (pfc1t4)______________________ -1.5831E+06 + PF_Circuit_1_Time_point_5_(A)___________________________________________ (pfc1t5)______________________ 0.0000E+00 + PF_Circuit_2_Time_point_0_(A)___________________________________________ (pfc2t0)______________________ -0.0000E+00 + PF_Circuit_2_Time_point_1_(A)___________________________________________ (pfc2t1)______________________ 4.9542E+05 + PF_Circuit_2_Time_point_2_(A)___________________________________________ (pfc2t2)______________________ -7.1060E+06 + PF_Circuit_2_Time_point_3_(A)___________________________________________ (pfc2t3)______________________ -7.1060E+06 + PF_Circuit_2_Time_point_4_(A)___________________________________________ (pfc2t4)______________________ -7.7049E+06 + PF_Circuit_2_Time_point_5_(A)___________________________________________ (pfc2t5)______________________ -0.0000E+00 + PF_Circuit_3_Time_point_0_(A)___________________________________________ (pfc3t0)______________________ -0.0000E+00 + PF_Circuit_3_Time_point_1_(A)___________________________________________ (pfc3t1)______________________ 4.9542E+05 + PF_Circuit_3_Time_point_2_(A)___________________________________________ (pfc3t2)______________________ -7.1060E+06 + PF_Circuit_3_Time_point_3_(A)___________________________________________ (pfc3t3)______________________ -7.1060E+06 + PF_Circuit_3_Time_point_4_(A)___________________________________________ (pfc3t4)______________________ -7.7049E+06 + PF_Circuit_3_Time_point_5_(A)___________________________________________ (pfc3t5)______________________ -0.0000E+00 + PF_Circuit_4_Time_point_0_(A)___________________________________________ (pfc4t0)______________________ -0.0000E+00 + PF_Circuit_4_Time_point_1_(A)___________________________________________ (pfc4t1)______________________ 3.2650E+05 + PF_Circuit_4_Time_point_2_(A)___________________________________________ (pfc4t2)______________________ -4.8247E+06 + PF_Circuit_4_Time_point_3_(A)___________________________________________ (pfc4t3)______________________ -4.8247E+06 + PF_Circuit_4_Time_point_4_(A)___________________________________________ (pfc4t4)______________________ -5.2194E+06 + PF_Circuit_4_Time_point_5_(A)___________________________________________ (pfc4t5)______________________ -0.0000E+00 + PF_Circuit_5_Time_point_0_(A)___________________________________________ (pfc5t0)______________________ -0.0000E+00 + PF_Circuit_5_Time_point_1_(A)___________________________________________ (pfc5t1)______________________ 3.2650E+05 + PF_Circuit_5_Time_point_2_(A)___________________________________________ (pfc5t2)______________________ -4.8247E+06 + PF_Circuit_5_Time_point_3_(A)___________________________________________ (pfc5t3)______________________ -4.8247E+06 + PF_Circuit_5_Time_point_4_(A)___________________________________________ (pfc5t4)______________________ -5.2194E+06 + PF_Circuit_5_Time_point_5_(A)___________________________________________ (pfc5t5)______________________ -0.0000E+00 + CS_Circuit_Time_point_0_(A)_____________________________________________ (cs_t0)_______________________ -0.0000E+00 + CS_Circuit_Time_point_1_(A)_____________________________________________ (cs_t1)_______________________ 1.7482E+08 + CS_Circuit_Time_point_2_(A)_____________________________________________ (cs_t2)_______________________ 2.6086E+07 + CS_Circuit_Time_point_3_(A)_____________________________________________ (cs_t3)_______________________ 2.6086E+07 + CS_Circuit_Time_point_4_(A)_____________________________________________ (cs_t4)_______________________ -1.8523E+08 + CS_Circuit_Time_point_5_(A)_____________________________________________ (cs_t5)_______________________ -0.0000E+00 + Plasma_Time_point_0_(A)_________________________________________________ (plasmat0)____________________ 0.0000E+00 + Plasma_Time_point_1_(A)_________________________________________________ (plasmat1)____________________ 0.0000E+00 + Plasma_Time_point_2_(A)_________________________________________________ (plasmat2)____________________ 1.6631E+07 + Plasma_Time_point_3_(A)_________________________________________________ (plasmat3)____________________ 1.6631E+07 + Plasma_Time_point_4_(A)_________________________________________________ (plasmat4)____________________ 1.6631E+07 + Plasma_Time_point_5_(A)_________________________________________________ (plasmat5)____________________ 0.0000E+00 + # Support Structure # + Outer_PF_coil_fence_mass_(kg)___________________________________________ (fncmass)_____________________ 2.2924E+05 OP + Intercoil_support_structure_mass_(kg)___________________________________ (aintmass)____________________ 4.3045E+06 OP + Mass_of_cooled_components_(kg)__________________________________________ (coldmass)____________________ 3.4369E+07 OP + Gravity_support_structure_mass_(kg)_____________________________________ (clgsmass)____________________ 1.2760E+06 OP + Torus_leg_support_mass_(kg)_____________________________________________ (gsm1)________________________ 8.5820E+04 OP + Ring_beam_mass_(kg)_____________________________________________________ (gsm2)________________________ 4.0088E+05 OP + Ring_legs_mass_(kg)_____________________________________________________ (gsm3)________________________ 6.8283E+05 OP + # PF Coil Inductances # + # Nuclear Heating Magnets Before Renormalisation # + Shield_line_density_(tonne/m2)__________________________________________ (x_shield)____________________ 4.0560E+00 + Blanket_line_density_(tonne/m2)_________________________________________ (x_blanket)___________________ 2.2911E+00 + Unit_nuclear_heating_in_TF_coil_(W/GW)__________________________________ (tfc_nuc_heating)_____________ 1.4866E+04 + Total_nuclear_heating_in_TF_coil_(MW)___________________________________ (ptfnuc.)_____________________ 2.4085E-02 + powfmw__________________________________________________________________ (powfmw.)_____________________ 1.6202E+03 + total_mass_of_the_TF_coils_(kg)_________________________________________ (whttf)_______________________ 1.1424E+07 + # Pumping for primary coolant (helium) # + Pressure_drop_in_FW_and_blanket_coolant_incl._hx_and_pipes_(Pa)_________ (dp_he)_______________________ 5.5000E+05 + Fraction_of_FW_and_blanket_thermal_power_required_for_pumping___________ (fpump)_______________________ 8.9463E-02 OP + Total_power_absorbed_by_FW_&_blanket_(MW)_______________________________ (p_plasma)____________________ 1.6698E+03 OP + Inlet_temperature_of_FW_&_blanket_coolant_pump_(K)______________________ (t_in_compressor)_____________ 5.5703E+02 OP + Coolant_pump_outlet/Inlet_temperature_of_FW_&_blanket_(K)_______________ (t_in_bb)_____________________ 5.7313E+02 + Outlet_temperature_of_FW_&_blanket_(K)__________________________________ (t_out_bb)____________________ 7.7313E+02 + Mechanical_pumping_power_for_FW_and_blanket_cooling_loop_including_heat_ (htpmw_fw_blkt)_______________ 1.6407E+02 OP + Mechanical_pumping_power_for_divertor_(MW)______________________________ (htpmw_div)___________________ 1.6906E+00 OP + Mechanical_pumping_power_for_shield_and_vacuum_vessel_(MW)______________ (htpmw_shld)__________________ 7.0688E-03 OP + # First wall and blanket : CCFE HCPB model # + Titanium_beryllide_fraction_____________________________________________ (fbltibe12)___________________ 3.7500E-01 + Lithium_orthosilicate_fraction__________________________________________ (fblli2sio4)__________________ 3.7500E-01 + Steel_fraction__________________________________________________________ (fblss_ccfe)__________________ 9.7050E-02 + Coolant_fraction________________________________________________________ (vfcblkt)_____________________ 5.2950E-02 + Purge_gas_fraction______________________________________________________ (vfpblkt)_____________________ 1.0000E-01 + First_Wall_Armour_Volume_(m3)___________________________________________ (fw_armour_vol)_______________ 5.8692E+00 + First_Wall_Volume_(m3)__________________________________________________ (volfw)_______________________ 1.9807E+01 + Blanket_Volume_(m3)_____________________________________________________ (volblkt)_____________________ 1.1849E+03 + Shield_Volume_(m3)______________________________________________________ (volshld)_____________________ 7.8520E+02 + Vacuum_vessel_volume_(m3)_______________________________________________ (vdewin)______________________ 1.0178E+03 + First_Wall_Armour_Mass_(kg)_____________________________________________ (fw_armour_mass)______________ 1.1298E+05 OP + First_Wall_Mass,_excluding_armour_(kg)__________________________________ (fwmass)______________________ 1.5449E+05 OP + Blanket_Mass_-_Total(kg)________________________________________________ (whtblkt)_____________________ 2.9676E+06 OP + ____Blanket_Mass_-_TiBe12_(kg)__________________________________________ (whtbltibe12)_________________ 1.0042E+06 OP + ____Blanket_Mass_-_Li4SiO4_(kg)_________________________________________ (whtblli4sio4)________________ 1.0664E+06 OP + ____Blanket_Mass_-_Steel_(kg)___________________________________________ (whtblss)_____________________ 8.9696E+05 OP + Total_mass_of_armour,_first_wall_and_blanket_(kg)_______________________ (armour_fw_bl_mass)___________ 3.2350E+06 OP + Shield_Mass_(kg)________________________________________________________ (whtshld)_____________________ 2.4498E+06 OP + Vacuum_vessel_mass_(kg)_________________________________________________ (vvmass)______________________ 7.9388E+06 OP + Total_nuclear_heating_in_TF+PF_coils_(CS_is_negligible)_(MW)____________ (ptfnuc)______________________ 2.5118E-02 OP + Total_nuclear_heating_in_FW_(MW)________________________________________ (pnucfw)______________________ 1.6315E+02 OP + Total_nuclear_heating_in_the_blanket_(including_emult)_(MW)_____________ (pnucblkt)____________________ 1.2901E+03 OP + Total_nuclear_heating_in_the_shield_(MW)________________________________ (pnucshld)____________________ 1.4138E+00 OP + Total_nuclear_heating_in_the_divertor_(MW)______________________________ (pnucdiv)_____________________ 1.4906E+02 OP + Blanket_exponential_factor______________________________________________ (exp_blanket)_________________ 9.9936E-01 OP + Shield:_first_exponential_______________________________________________ (exp_shield1)_________________ 1.9523E-03 OP + Shield:_second_exponential______________________________________________ (exp_shield2)_________________ 2.5427E-01 OP + Solid_angle_fraction_taken_by_on_divertor_______________________________ (fdiv)________________________ 1.1500E-01 + Switch_for_plant_secondary_cycle________________________________________ (secondary_cycle)_____________ 2 + First_wall_coolant_pressure_(Pa)________________________________________ (fwpressure)__________________ 1.5500E+07 + Blanket_coolant_pressure_(Pa)___________________________________________ (blpressure)__________________ 1.5500E+07 + Allowable_nominal_neutron_fluence_at_first_wall_(MW.year/m2)____________ (abktflnc)____________________ 5.0000E+00 + No_of_inboard_blanket_modules_poloidally________________________________ (nblktmodpi)__________________ 7 + No_of_inboard_blanket_modules_toroidally________________________________ (nblktmodti)__________________ 32 + No_of_outboard_blanket_modules_poloidally_______________________________ (nblktmodpo)__________________ 8 + No_of_outboard_blanket_modules_toroidally_______________________________ (nblktmodto)__________________ 48 + Isentropic_efficiency_of_first_wall_/_blanket_coolant_pumps_____________ (etaiso)______________________ 9.0000E-01 + First_wall_area_(m2)____________________________________________________ (fwarea)______________________ 1.6044E+03 OP + Cryostat_internal_radius_(m)____________________________________________ (rdewex)______________________ 1.7798E+01 OP + Cryostat_internal_half-height_(m)_______________________________________ (zdewex)______________________ 1.5339E+01 OP + Vertical_clearance_from_TF_coil_to_cryostat_(m)_________________________ (clh1)________________________ 5.6044E+00 OP + Divertor_area_(m2)______________________________________________________ (divsur)______________________ 1.4879E+02 OP + Divertor_mass_(kg)______________________________________________________ (divmas)______________________ 3.6453E+04 OP + # Superconducting TF Coil Power Conversion # + TF_coil_current_(kA)____________________________________________________ (itfka)_______________________ 8.9795E+01 OP + Number_of_TF_coils______________________________________________________ (ntfc)________________________ 1.6000E+01 + Voltage_across_a_TF_coil_during_quench_(kV)_____________________________ (vtfskv)______________________ 9.1862E+00 OP + TF_coil_charge_time_(hours)_____________________________________________ (tchghr)______________________ 4.0000E+00 + Total_inductance_of_TF_coils_(H)________________________________________ (ltfth)_______________________ 3.0165E+01 OP + Total_resistance_of_TF_coils_(ohm)______________________________________ (rcoils)______________________ 0.0000E+00 OP + TF_coil_charging_voltage_(V)____________________________________________ (tfcv)________________________ 2.9268E+02 + Number_of_DC_circuit_breakers___________________________________________ (ntfbkr)______________________ 1.6000E+01 + Number_of_dump_resistors________________________________________________ (ndumpr)______________________ 6.4000E+01 + Resistance_per_dump_resistor_(ohm)______________________________________ (r1dump)______________________ 1.0230E-01 OP + Dump_resistor_peak_power_(MW)___________________________________________ (r1ppmw)______________________ 2.0622E+02 OP + Energy_supplied_per_dump_resistor_(MJ)__________________________________ (r1emj)_______________________ 1.9002E+03 OP + TF_coil_L/R_time_constant_(s)___________________________________________ (ttfsec)______________________ 1.8429E+01 OP + Power_supply_voltage_(V)________________________________________________ (tfpsv)_______________________ 3.0731E+02 OP + Power_supply_current_(kA)_______________________________________________ (tfpska)______________________ 9.4285E+01 OP + DC_power_supply_rating_(kW)_____________________________________________ (tfckw)_______________________ 2.8975E+04 OP + AC_power_for_charging_(kW)______________________________________________ (tfackw)______________________ 3.2194E+04 OP + TF_coil_resistive_power_(MW)____________________________________________ (rpower)______________________ 9.3902E+00 OP + TF_coil_inductive_power_(MVA)___________________________________________ (xpower)______________________ 1.6891E+01 OP + Aluminium_bus_current_density_(kA/cm2)__________________________________ (djmka)_______________________ 1.2500E-01 + Aluminium_bus_cross-sectional_area_(cm2)________________________________ (albusa)______________________ 7.1836E+02 OP + Total_length_of_TF_coil_bussing_(m)_____________________________________ (tfbusl)______________________ 3.1931E+03 OP + Aluminium_bus_weight_(tonnes)___________________________________________ (albuswt)_____________________ 6.1932E+02 OP + Total_TF_coil_bus_resistance_(ohm)______________________________________ (rtfbus)______________________ 1.1646E-03 OP + TF_coil_bus_voltage_drop_(V)____________________________________________ (vtfbus)______________________ 1.0457E+02 OP + Dump_resistor_floor_area_(m2)___________________________________________ (drarea)______________________ 4.9234E+03 OP + TF_coil_power_conversion_floor_space_(m2)_______________________________ (tfcfsp)______________________ 1.8228E+03 OP + TF_coil_power_conv._building_volume_(m3)________________________________ (tfcbv)_______________________ 1.0937E+04 OP + TF_coil_AC_inductive_power_demand_(MW)__________________________________ (xpwrmw)______________________ 1.8768E+01 OP + Total_steady_state_AC_power_demand_(MW)_________________________________ (tfacpd)______________________ 1.0434E+01 OP + # PF Coils and Central Solenoid: Power and Energy # + Number_of_PF_coil_circuits______________________________________________ (pfckts)______________________ 1.2000E+01 + Sum_of_PF_power_supply_ratings_(MVA)____________________________________ (spsmva)______________________ 3.0313E+02 OP + Total_PF_coil_circuit_bus_length_(m)____________________________________ (spfbusl)_____________________ 2.4480E+03 OP + Total_PF_coil_bus_resistive_power_(kW)__________________________________ (pfbuspwr)____________________ 9.6485E+02 OP + Total_PF_coil_resistive_power_(kW)______________________________________ (srcktpm)_____________________ 9.6485E+02 OP + Maximum_PF_coil_voltage_(kV)____________________________________________ (vpfskv)______________________ 2.0000E+01 + Efficiency_of_transfer_of_PF_stored_energy_into_or_out_of_storage_______ (etapsu)______________________ 9.0000E-01 + Maximum_stored_energy_in_poloidal_field_(MJ)____________________________ (ensxpfm)_____________________ 2.8804E+04 OP + Peak_absolute_rate_of_change_of_stored_energy_in_poloidal_field_(MW)____ (peakpoloidalpower)___________ 1.7319E+02 OP + # Vacuum System # + First_wall_outgassing_rate_(Pa_m/s)_____________________________________ (rat)_________________________ 1.3000E-08 + Total_outgassing_load_(Pa_m3/s)_________________________________________ (ogas)________________________ 1.6691E-04 OP + Base_pressure_required_(Pa)_____________________________________________ (pbase)_______________________ 5.0000E-04 + Required_N2_pump_speed_(m3/s)___________________________________________ (s(1))________________________ 3.3381E-01 OP + N2_pump_speed_provided_(m3/s)___________________________________________ (snet(1))_____________________ 2.3404E+01 OP + Plasma_chamber_volume_(m3)______________________________________________ (volume)______________________ 2.2588E+03 OP + Chamber_pressure_after_burn_(Pa)________________________________________ (pend)________________________ 1.6698E-01 OP + Chamber_pressure_before_burn_(Pa)_______________________________________ (pstart)______________________ 1.6698E-03 + Allowable_pumping_time_switch___________________________________________ (dwell_pump)__________________ 0 + Dwell_time_between_burns_(s)____________________________________________ (tdwell.)_____________________ 1.8000E+03 + CS_ramp-up_time_burns_(s)_______________________________________________ (tramp.)______________________ 5.0000E+02 + Allowable_pumping_time_between_burns_(s)________________________________ (tpump)_______________________ 1.8000E+03 + Required_D-T_pump_speed_(m3/s)__________________________________________ (s(2))________________________ 5.7790E+00 OP + D-T_pump_speed_provided_(m3/s)__________________________________________ (snet(2))_____________________ 5.6700E+01 OP + Divertor_chamber_gas_pressure_(Pa)______________________________________ (prdiv)_______________________ 3.6000E-01 + Helium_gas_fraction_in_divertor_chamber_________________________________ (fhe)_________________________ 1.7218E-01 OP + Required_helium_pump_speed_(m3/s)_______________________________________ (s(3))________________________ 3.8423E+01 OP + Helium_pump_speed_provided_(m3/s)_______________________________________ (snet(3))_____________________ 3.8423E+01 OP + D-T_fuelling_rate_(kg/s)________________________________________________ (frate)_______________________ 2.7747E-05 OP + Required_D-T_pump_speed_(m3/s)__________________________________________ (s(4))________________________ 3.8423E+01 OP + D-T_pump_speed_provided_(m3/s)__________________________________________ (snet(4))_____________________ 5.6700E+01 OP + Number_of_large_pump_ducts______________________________________________ (nduct)_______________________ 16 + Passage_diameter,_divertor_to_ducts_(m)_________________________________ (d(imax))_____________________ 4.7857E-01 OP + Passage_length_(m)______________________________________________________ (l1)__________________________ 1.7160E+00 OP + Diameter_of_ducts_(m)___________________________________________________ (dout)________________________ 5.7428E-01 OP + Duct_length,_divertor_to_elbow_(m)______________________________________ (l2)__________________________ 4.8000E+00 OP + Duct_length,_elbow_to_pumps_(m)_________________________________________ (l3)__________________________ 2.0000E+00 + Number_of_pumps_________________________________________________________ (pumpn)_______________________ 3.2000E+01 OP + # Plant Buildings System # + Internal_volume_of_reactor_building_(m3)________________________________ (vrci)________________________ 9.9708E+05 + Dist_from_centre_of_torus_to_bldg_wall_(m)______________________________ (wrbi)________________________ 3.9531E+01 + Effective_floor_area_(m2)_______________________________________________ (efloor)______________________ 3.3660E+05 + Reactor_building_volume_(m3)____________________________________________ (rbv)_________________________ 1.1310E+06 + Reactor_maintenance_building_volume_(m3)________________________________ (rmbv)________________________ 3.9641E+05 + Warmshop_volume_(m3)____________________________________________________ (wsv)_________________________ 1.2531E+05 + Tritium_building_volume_(m3)____________________________________________ (triv)________________________ 4.0000E+04 + Electrical_building_volume_(m3)_________________________________________ (elev)________________________ 5.1937E+04 + Control_building_volume_(m3)____________________________________________ (conv)________________________ 6.0000E+04 + Cryogenics_building_volume_(m3)_________________________________________ (cryv)________________________ 1.4976E+04 + Administration_building_volume_(m3)_____________________________________ (admv)________________________ 1.0000E+05 + Shops_volume_(m3)_______________________________________________________ (shov)________________________ 1.0000E+05 + Total_volume_of_nuclear_buildings_(m3)__________________________________ (volnucb)_____________________ 1.5738E+06 + # Electric Power Requirements # + Facility_base_load_(MW)_________________________________________________ (basemw)______________________ 5.0000E+00 + Divertor_coil_power_supplies_(MW)_______________________________________ (bdvmw)_______________________ 0.0000E+00 + Cryoplant_electric_power_(MW)___________________________________________ (crymw)_______________________ 3.6566E+01 OP + Primary_coolant_pumps_(MW)______________________________________________ (htpmw..)_____________________ 1.9053E+02 OP + PF_coil_power_supplies_(MW)_____________________________________________ (ppfmw)_______________________ 8.5511E+01 OP + TF_coil_power_supplies_(MW)_____________________________________________ (ptfmw)_______________________ 1.0434E+01 OP + Plasma_heating_supplies_(MW)____________________________________________ (pheatingmw)__________________ 1.6029E+02 OP + Tritium_processing_(MW)_________________________________________________ (trithtmw..)__________________ 1.5000E+01 + Vacuum_pumps__(MW)______________________________________________________ (vachtmw..)___________________ 5.0000E-01 + Total_pulsed_power_(MW)_________________________________________________ (pacpmw)______________________ 5.5432E+02 OP + Total_base_power_required_at_all_times_(MW)_____________________________ (fcsht)_______________________ 5.5490E+01 OP + # Cryogenics # + Conduction_and_radiation_heat_loads_on_cryogenic_components_(MW)________ (qss/1.0d6)___________________ 1.4779E-02 OP + Nuclear_heating_of_cryogenic_components_(MW)____________________________ (qnuc/1.0d6)__________________ 1.3000E-02 OP + AC_losses_in_cryogenic_components_(MW)__________________________________ (qac/1.0d6)___________________ 3.8170E-03 OP + Resistive_losses_in_current_leads_(MW)__________________________________ (qcl/1.0d6)___________________ 1.9539E-02 OP + 45%_allowance_for_heat_loads_in_transfer_lines,_storage_tanks_etc_(MW)__ (qmisc/1.0d6)_________________ 2.3011E-02 OP + Sum_=_Total_heat_removal_at_cryogenic_temperatures_(tfcoil_variables.tmp (helpow_+_helpow_cryal/1.0d6)_ 7.4146E-02 OP + Temperature_of_cryogenic_superconducting_components_(K)_________________ (tmpcry)______________________ 4.5000E+00 + Temperature_of_cryogenic_aluminium_components_(K)_______________________ (tcoolin)_____________________ 3.1315E+02 + Efficiency_(figure_of_merit)_of_cryogenic_plant_is_13%_of_ideal_Carnot_v ______________________________ 2.0277E-03 OP + Efficiency_(figure_of_merit)_of_cryogenic_aluminium_plant_is_40%_of_idea ______________________________ -2.0203E+00 OP + Electric_power_for_cryogenic_plant_(MW)_________________________________ (crypmw)______________________ 3.6566E+01 OP + # Plant Power / Heat Transport Balance # + Neutron_power_multiplication_in_blanket_________________________________ (emult)_______________________ 1.2690E+00 + Divertor_area_fraction_of_whole_toroid_surface__________________________ (fdiv)________________________ 1.1500E-01 + H/CD_apparatus_+_diagnostics_area_fraction______________________________ (fhcd)________________________ 0.0000E+00 + First_wall_area_fraction________________________________________________ (1-fdiv-fhcd)_________________ 8.8500E-01 + Switch_for_pumping_of_primary_coolant___________________________________ (primary_pumping)_____________ 3 + Mechanical_pumping_power_for_FW_cooling_loop_including_heat_exchanger_(M (htpmw_fw)____________________ 0.0000E+00 OP + Mechanical_pumping_power_for_blanket_cooling_loop_including_heat_exchang (htpmw_blkt)__________________ 0.0000E+00 OP + Mechanical_pumping_power_for_FW_and_blanket_cooling_loop_including_heat_ (htpmw_fw_blkt)_______________ 1.6407E+02 OP + Mechanical_pumping_power_for_divertor_(MW)______________________________ (htpmw_div)___________________ 1.6906E+00 OP + Mechanical_pumping_power_for_shield_and_vacuum_vessel_(MW)______________ (htpmw_shld)__________________ 7.0688E-03 OP + Electrical_pumping_power_for_FW_and_blanket_(MW)________________________ (htpmwe_fw_blkt)______________ 1.8858E+02 OP + Electrical_pumping_power_for_shield_(MW)________________________________ (htpmwe_shld)_________________ 8.1250E-03 OP + Electrical_pumping_power_for_divertor_(MW)______________________________ (htpmwe_div)__________________ 1.9433E+00 OP + Total_electrical_pumping_power_for_primary_coolant_(MW)_________________ (htpmw)_______________________ 1.9053E+02 OP + Coolant_pump_power_/_non-pumping_thermal_power_in_shield________________ (fpumpshld)___________________ 5.0000E-03 + Coolant_pump_power_/_non-pumping_thermal_power_in_divertor______________ (fpumpdiv)____________________ 5.0000E-03 + Electrical_efficiency_of_heat_transport_coolant_pumps___________________ (etahtp)______________________ 8.7000E-01 + Thermal_to_electric_conversion_efficiency_of_the_power_conversion_cycle_ (etath)_______________________ 4.0000E-01 + Fraction_of_total_high-grade_thermal_power_to_divertor__________________ (pdivfraction)________________ 1.5623E-01 + Total_power_leaving_reactor_(across_vacuum_vessel_boundary)_(MW)________ ______________________________ 2.0111E+03 + Heat_removal_from_cryogenic_plant_(MW)__________________________________ (crypmw)______________________ 3.6566E+01 + Heat_removal_from_facilities_(MW)_______________________________________ (fachtmw)_____________________ 5.5490E+01 + Coolant_pumping_efficiency_losses_(MW)__________________________________ (htpsecmw)____________________ 2.4769E+01 + Heat_removal_from_injection_power_(MW)__________________________________ (pinjht)______________________ 8.0143E+01 + Heat_removal_from_tritium_plant_(MW)____________________________________ (trithtmw)____________________ 1.5000E+01 + Heat_removal_from_vacuum_pumps_(MW)_____________________________________ (vachtmw)_____________________ 5.0000E-01 + TF_coil_resistive_power_(MW)____________________________________________ (tfcmw)_______________________ 0.0000E+00 + Total_low-grade_thermal_power_(MW)______________________________________ (psechtmw)____________________ 2.2417E+02 + Total_High-grade_thermal_power_(MW)_____________________________________ (pthermmw)____________________ 2.1751E+03 + Number_of_primary_heat_exchangers_______________________________________ (nphx)________________________ 3 OP + Transport_power_from_scaling_law_(MW)___________________________________ (pscalingmw)__________________ 2.9785E+02 + Radiation_power_from_inside_"coreradius"_(MW)___________________________ (pcoreradmw.)_________________ 9.1650E+01 + Total_(MW)______________________________________________________________ ______________________________ 3.8950E+02 + Alpha_power_deposited_in_plasma_(MW)____________________________________ (falpha*palpmw)_______________ 3.0746E+02 + Power_from_charged_products_of_DD_and/or_D-He3_fusion_(MW)______________ (pchargemw.)__________________ 1.2659E+00 + Ohmic_heating_(MW)______________________________________________________ (pohmmw.)_____________________ 6.2284E-01 + Injected_power_deposited_in_plasma_(MW)_________________________________ (pinjmw)______________________ 8.0143E+01 + Total_(MW)______________________________________________________________ ______________________________ 3.8950E+02 + Fusion_power_(MW)_______________________________________________________ (powfmw)______________________ 1.6202E+03 + Power_from_energy_multiplication_in_blanket_and_shield_(MW)_____________ (emultmw)_____________________ 3.0836E+02 + Injected_power_(MW)_____________________________________________________ (pinjmw.)_____________________ 8.0143E+01 + Ohmic_power_(MW)________________________________________________________ (pohmmw.)_____________________ 6.2284E-01 + Power_deposited_in_primary_coolant_by_pump_(MW)_________________________ (htpmw_mech)__________________ 1.6576E+02 + Total_(MW)______________________________________________________________ ______________________________ 2.1751E+03 + Heat_extracted_from_first_wall_and_blanket_(MW)_________________________ (pthermfw_blkt)_______________ 1.8339E+03 + Heat_extracted_from_shield__(MW)________________________________________ (pthermshld)__________________ 1.4208E+00 + Heat_extracted_from_divertor_(MW)_______________________________________ (pthermdiv)___________________ 3.3982E+02 + Nuclear_and_photon_power_lost_to_H/CD_system_(MW)_______________________ (psechcd)_____________________ 0.0000E+00 + Nuclear_power_lost_to_TF_(MW)___________________________________________ (ptfnuc)______________________ 2.5118E-02 + Total_(MW)______________________________________________________________ ______________________________ 2.1752E+03 + Net_electric_power_output(MW)___________________________________________ (pnetelmw.)___________________ 4.0001E+02 + Required_Net_electric_power_output(MW)__________________________________ (pnetelin)____________________ 4.0000E+02 + Electric_power_for_heating_and_current_drive_(MW)_______________________ (pinjwp)______________________ 1.6029E+02 + Electric_power_for_primary_coolant_pumps_(MW)___________________________ (htpmw)_______________________ 1.9053E+02 + Electric_power_for_vacuum_pumps_(MW)____________________________________ (vachtmw)_____________________ 5.0000E-01 + Electric_power_for_tritium_plant_(MW)___________________________________ (trithtmw)____________________ 1.5000E+01 + Electric_power_for_cryoplant_(MW)_______________________________________ (crypmw)______________________ 3.6566E+01 + Electric_power_for_TF_coils_(MW)________________________________________ (tfacpd)______________________ 1.0434E+01 + Electric_power_for_PF_coils_(MW)________________________________________ (pfwpmw)______________________ 1.2422E+00 + All_other_internal_electric_power_requirements_(MW)_____________________ (fachtmw)_____________________ 5.5490E+01 + Total_(MW)______________________________________________________________ (tot_plant_power)_____________ 8.7006E+02 + Total_(MW)______________________________________________________________ ______________________________ 8.7006E+02 + Gross_electrical_output*_(MW)___________________________________________ (pgrossmw)____________________ 8.7006E+02 + Fusion_power_(MW)_______________________________________________________ (powfmw)______________________ 1.6202E+03 + Power_from_energy_multiplication_in_blanket_and_shield_(MW)_____________ (emultmw)_____________________ 3.0836E+02 + Total_(MW)______________________________________________________________ ______________________________ 1.9285E+03 + Net_electrical_output_(MW) _____________________________________________ (pnetelmw)____________________ 4.0001E+02 + Heat_rejected_by_main_power_conversion_circuit_(MW)_____________________ (rejected_main)_______________ 1.3051E+03 + Heat_rejected_by_other_cooling_circuits_(MW)____________________________ (psechtmw)____________________ 2.2417E+02 + Total_(MW)______________________________________________________________ ______________________________ 1.9293E+03 + Net_electric_power_/_total_nuclear_power_(%)____________________________ (pnetelmw/(powfmw+emultmw)____ 2.0741E+01 + Net_electric_power_/_total_fusion_power_(%)_____________________________ (pnetelmw/powfmw)_____________ 2.4689E+01 + Gross_electric_power*_/_high_grade_heat_(%)_____________________________ (etath)_______________________ 4.0000E+01 + Recirculating_power_fraction____________________________________________ (cirpowfr)____________________ 5.4025E-01 + # Water usage during plant operation (secondary cooling) # + Volume_used_in_cooling_tower_(m3/day)___________________________________ (waterusetower)_______________ 5.5485E+04 OP + Volume_used_in_recirculating_water_system_(m3/day)______________________ (wateruserecirc)______________ 1.8617E+04 OP + Volume_used_in_once-through_water_system_(m3/day)_______________________ (wateruseonethru)_____________ 1.8244E+06 OP + # Errors and Warnings # + # Errors and Warnings # + PROCESS_error_status_flag_______________________________________________ (error_status)________________ 2 + Final_error_identifier__________________________________________________ (error_id)____________________ 244 + # End of PROCESS Output # + # End of PROCESS Output # + # Copy of PROCESS Input Follows # +************************************************************************************************************************ +***** ***** +***** Generic large tokamak file ***** +***** James Morris, UKAEA ***** +***** 28/06/23 ***** +***** ***** +************************************************************************* + +* Run Information * +******************* + +runtitle = Generic large tokamak + +* Figure of merit - minimise major radius +minmax = 1 + +* Error tolerance for VMCON +epsvmc = 1e-7 + +* Constraint Equations - Consistency Equations * +************************************************ + +* Beta consistency * +*------------------* +icc = 1 +ixc = 5 * beta +beta = 0.03 + +* Global power balance * +*----------------------* +icc = 2 + +* Radial build consistency * +*--------------------------* +icc = 11 + +* Constraint Equations - Limit Equations * +****************************************** + +* Density upper limit * +*---------------------* +icc = 5 +ixc = 6 * dene [m-3] +fdene = 1.2 +dene = 7.5E19 + +* Neutron wall load upper limit * +*-------------------------------* +icc = 8 +ixc = 14 * fwalld +fwalld = 1.0 +* wall load limit [MW/m2] +walalw = 2.0 + +* Fusion power upper limit * +*--------------------------* + +icc = 9 +ixc = 26 * ffuspow +* Maximum allowable value fusion power [MW] +powfmax = 3000 + +* Burn time lower limit * +*-----------------------* +icc = 13 +ixc = 21 * ftburn +* minimum burn time [s] +tbrnmn = 7200.0 + +* L-H threshold scaling * +*-----------------------* +icc = 15 +ixc = 103 * flhthresh +boundu(103) = 10.0 + +* Injection power upper limit * +*-----------------------------* +icc = 30 +ixc = 46 * fpinj +* Maximum allowable value for injected power [MW] +pinjalw = 200.0 + +* Net electric power lower limit * +*--------------------------------* +icc = 16 +ixc = 25 * fpnetel +* Minimum allowable value for net eletric power [MW] +pnetelin = 400.0 + +* Beta upper limit * +*------------------* +icc = 24 +ixc = 36 * fbetatry +fbetatry = 0.5 + +* Max TF field * +*--------------* +icc = 25 +ixc = 35 * fpeakb +* Maximum allowable value for toroidal magnetic field [T] +bmxlim = 14.0 + +* Central solenoid EOF current density upper limit * +*--------------------------------------------------* +icc = 26 +ixc = 37 * coheof [A/m2] +ixc = 38 * fjohc +boundu(38) = 1.0 +coheof = 1.5E7 +fjohc = 0.6 + +* Central solenoid BOP current density upper limit * +*--------------------------------------------------* +icc = 27 +ixc = 39 * fjohc0 +ixc = 41 * fcohbop +boundu(39) = 1.0 +fjohc0 = 0.6 +fcohbop = 0.9 + +* I_op/I_Crit TF coil limit * +*---------------------------* +icc = 33 +ixc = 50 * fiooic +boundu(50) = 1.0 +fiooic = 0.65 + +* Dump voltage upper limit * +*--------------------------* +icc = 34 +ixc = 51 * fvdump +ixc = 52 * vdalw [kV] +boundu(52) = 10.0 +fvdump = 1.0 +vdalw = 10.0 + +* J_winding pack protection * +*---------------------------* +icc = 35 +ixc = 53 * fjprot +fjprot = 1.0 + +* TF temp marg lower limit * +*--------------------------* +icc = 36 +ixc = 54 * ftmargtf +* Minimum allowable temperature margin [K] +tmargmin = 1.5 + +* CS coil temp margin lower limit * +*---------------------------------* +icc = 60 +ixc = 106 * ftmargoh +tmargmin_cs = 1.5 + +* Lower limit on taup/taueff (ratio alpha particle/energy confinement times) * +*-------------------------------------------------------------------------------* +icc = 62 +ixc = 110 * ftaulimit +taulimit = 5.0 + +* dump time constraint for VV stresses * +*--------------------------------------* +icc = 65 +ixc = 113 * fmaxvvstress +fmaxvvstress = 1.0 + +* CS stress limit * +*-----------------* +icc = 72 +ixc = 123 * foh_stress +foh_stress = 1.0 +* allowable hoop stress in Central Solenoid structural material [Pa] +alstroh = 7.5D8 + +* neped_neped_______________________normalised_residue____________________ (normres023)__________________ -1.9637E-08 + Upper_Lim._on_Psep_*_Bt_/_q_A_R___normalised_residue____________________ (normres024)__________________ 4.9789E-07 + TF_coil_case_stress_upper_limit___normalised_residue____________________ (normres025)__________________ -4.6757E-07 + TF_coil_conduit_stress_upper_lim__normalised_residue____________________ (normres026)__________________ -4.1375E-07 + # Final Feasible Point # + # Power Reactor Costs (1990 US$) # + First_wall_/_blanket_life_(years)_______________________________________ (fwbllife)____________________ 6.1566E+00 + Divertor_life_(years)___________________________________________________ (divlife.)____________________ 3.9769E+00 + Cost_of_electricity_(m$/kWh)____________________________________________ (coe)_________________________ 5.1257E+02 + # Detailed Costings (1990 US$) # + Acc.22_multiplier_for_Nth_of_a_kind_____________________________________ (fkind)_______________________ 1.0000E+00 + Level_of_Safety_Assurance_______________________________________________ (lsa)_________________________ 4 + # Structures and Site Facilities # + Site_improvements,_facilities,_land_(M$)________________________________ (c211)________________________ 3.5200E+01 + Reactor_building_cost_(M$)______________________________________________ (c212)________________________ 4.5238E+02 + Turbine_building_cost_(M$)______________________________________________ (c213)________________________ 3.8000E+01 + Reactor_maintenance_building_cost_(M$)__________________________________ (c2141)_______________________ 1.0307E+02 + Warm_shop_cost_(M$)_____________________________________________________ (c2142)_______________________ 5.7641E+01 + Tritium_building_cost_(M$)______________________________________________ (c215)________________________ 1.4800E+01 + Electrical_equipment_building_cost_(M$)_________________________________ (c216)________________________ 1.9736E+01 + Additional_buildings_cost_(M$)__________________________________________ (c2171)_______________________ 1.8000E+01 + Control_room_buildings_cost_(M$)________________________________________ (c2172)_______________________ 2.1000E+01 + Shop_and_warehouses_cost_(M$)___________________________________________ (c2173)_______________________ 1.1500E+01 + Cryogenic_building_cost_(M$)____________________________________________ (c2174)_______________________ 6.8891E+00 + Total_account_21_cost_(M$)______________________________________________ (c21)_________________________ 7.7822E+02 + # Reactor Systems # + First_wall_cost_(M$)____________________________________________________ (c2211)_______________________ 1.9130E+02 + Blanket_beryllium_cost_(M$)_____________________________________________ (c22121)______________________ 2.6109E+02 + Blanket_breeder_material_cost_(M$)______________________________________ (c22122)______________________ 6.3985E+02 + Blanket_stainless_steel_cost_(M$)_______________________________________ (c22123)______________________ 8.0726E+01 + Blanket_vanadium_cost_(M$)______________________________________________ (c22124)______________________ 0.0000E+00 + Blanket_total_cost_(M$)_________________________________________________ (c2212)_______________________ 9.8166E+02 + Bulk_shield_cost_(M$)___________________________________________________ (c22131)______________________ 7.8394E+01 + Penetration_shielding_cost_(M$)_________________________________________ (c22132)______________________ 7.8394E+01 + Total_shield_cost_(M$)__________________________________________________ (c2213)_______________________ 1.5679E+02 + Total_support_structure_cost_(M$)_______________________________________ (c2214)_______________________ 4.0933E+01 + Divertor_cost_(M$)______________________________________________________ (c2215)_______________________ 4.1660E+01 + Total_account_221_cost_(M$)_____________________________________________ (c221)________________________ 1.4123E+03 + # Magnets # + TF_coil_conductor_cost_(M$)_____________________________________________ (c22211)______________________ 1.3230E+02 + TF_coil_winding_cost_(M$)_______________________________________________ (c22212)______________________ 5.4263E+01 + TF_coil_case_cost_(M$)__________________________________________________ (c22213)______________________ 4.4365E+02 + TF_intercoil_structure_cost_(M$)________________________________________ (c22214)______________________ 1.5066E+02 + TF_coil_gravity_support_structure_(M$)__________________________________ (c22215)______________________ 4.4659E+01 + TF_magnet_assemblies_cost_(M$)__________________________________________ (c2221)_______________________ 8.2552E+02 + PF_coil_conductor_cost_(M$)_____________________________________________ (c22221)______________________ 4.6409E+02 + PF_coil_winding_cost_(M$)_______________________________________________ (c22222)______________________ 7.6765E+01 + PF_coil_case_cost_(M$)__________________________________________________ (c22223)______________________ 9.4861E+01 + PF_coil_support_structure_cost_(M$)_____________________________________ (c22224)______________________ 8.0235E+00 + PF_magnet_assemblies_cost_(M$)__________________________________________ (c2222)_______________________ 6.4374E+02 + Vacuum_vessel_assembly_cost_(M$)________________________________________ (c2223)_______________________ 2.5404E+02 + Total_account_222_cost_(M$)_____________________________________________ (c222)________________________ 1.7233E+03 + # Power Injection # + ECH_system_cost_(M$)____________________________________________________ (c2231)_______________________ 2.4043E+02 + Lower_hybrid_system_cost_(M$)___________________________________________ (c2232)_______________________ 0.0000E+00 + Neutral_beam_system_cost_(M$)___________________________________________ (c2233)_______________________ 0.0000E+00 + Total_account_223_cost_(M$)_____________________________________________ (c223)________________________ 2.4043E+02 + # Vacuum Systems # + High_vacuum_pumps_cost_(M$)_____________________________________________ (c2241)_______________________ 1.2480E+01 + Backing_pumps_cost_(M$)_________________________________________________ (c2242)_______________________ 4.6800E+00 + Vacuum_duct_cost_(M$)___________________________________________________ (c2243)_______________________ 2.5280E+00 + Valves_cost_(M$)________________________________________________________ (c2244)_______________________ 5.7410E+00 + Duct_shielding_cost_(M$)________________________________________________ (c2245)_______________________ 0.0000E+00 + Instrumentation_cost_(M$)_______________________________________________ (c2246)_______________________ 1.3000E+00 + Total_account_224_cost_(M$)_____________________________________________ (c224)________________________ 2.6729E+01 + # Power Conditioning # + TF_coil_power_supplies_cost_(M$)________________________________________ (c22511)______________________ 4.0144E+00 + TF_coil_breakers_cost_(M$)______________________________________________ (c22512)______________________ 3.4127E+01 + TF_coil_dump_resistors_cost_(M$)________________________________________ (c22513)______________________ 2.1322E+01 + TF_coil_instrumentation_and_control_(M$)________________________________ (c22514)______________________ 4.8000E+00 + TF_coil_bussing_cost_(M$)_______________________________________________ (c22515)______________________ 3.5267E+01 + Total,_TF_coil_power_costs_(M$)_________________________________________ (c2251)_______________________ 9.9531E+01 + PF_coil_power_supplies_cost_(M$)________________________________________ (c22521)______________________ 2.9591E+00 + PF_coil_instrumentation_and_control_(M$)________________________________ (c22522)______________________ 3.6000E+00 + PF_coil_bussing_cost_(M$)_______________________________________________ (c22523)______________________ 1.1995E+01 + PF_coil_burn_power_supplies_cost_(M$)___________________________________ (c22524)______________________ 1.2679E+00 + PF_coil_breakers_cost_(M$)______________________________________________ (c22525)______________________ 1.4709E+01 + PF_coil_dump_resistors_cost_(M$)________________________________________ (c22526)______________________ 4.3206E+00 + PF_coil_ac_breakers_cost_(M$)___________________________________________ (c22527)______________________ 9.0000E-01 + Total,_PF_coil_power_costs_(M$)_________________________________________ (c2252)_______________________ 3.9752E+01 + Total,_energy_storage_cost_(M$)_________________________________________ (c2253)_______________________ 1.6864E+01 + Total_account_225_cost_(M$)_____________________________________________ (c225)________________________ 1.5615E+02 + # Heat Transport System # + Pumps_and_piping_system_cost_(M$)_______________________________________ (cpp)_________________________ 3.6795E+01 + Primary_heat_exchanger_cost_(M$)________________________________________ (chx)_________________________ 7.1692E+01 + Total,_reactor_cooling_system_cost_(M$)_________________________________ (c2261)_______________________ 1.0849E+02 + Pumps,_piping_cost_(M$)_________________________________________________ (cppa)________________________ 2.8417E+01 + Total,_auxiliary_cooling_system_cost_(M$)_______________________________ (c2262)_______________________ 2.8417E+01 + Total,_cryogenic_system_cost_(M$)_______________________________________ (c2263)_______________________ 1.7039E+02 + Total_account_226_cost_(M$)_____________________________________________ (c226)________________________ 3.0729E+02 + # Fuel Handling System # + Fuelling_system_cost_(M$)_______________________________________________ (c2271)_______________________ 2.2300E+01 + Fuel_processing_and_purification_cost_(M$)______________________________ (c2272)_______________________ 1.0229E+02 + Atmospheric_recovery_systems_cost_(M$)__________________________________ (c2273)_______________________ 5.8088E+01 + Nuclear_building_ventilation_cost_(M$)__________________________________ (c2274)_______________________ 6.9201E+01 + Total_account_227_cost_(M$)_____________________________________________ (c227)________________________ 2.5188E+02 + # Instrumentation and Control # + Instrumentation_and_control_cost_(M$)___________________________________ (c228)________________________ 1.5000E+02 + # Maintenance Equipment # + Maintenance_equipment_cost_(M$)_________________________________________ (c229)________________________ 1.2500E+02 + # Total Account 22 Cost # + Total_account_22_cost_(M$)______________________________________________ (c22)_________________________ 4.3931E+03 + # Turbine Plant Equipment # + Turbine_plant_equipment_cost_(M$)_______________________________________ (c23)_________________________ 1.7613E+02 + # Electric Plant Equipment # + Switchyard_equipment_cost_(M$)__________________________________________ (c241)________________________ 1.8400E+01 + Transformers_cost_(M$)__________________________________________________ (c242)________________________ 8.0330E+00 + Low_voltage_equipment_cost_(M$)_________________________________________ (c243)________________________ 6.4513E+00 + Diesel_backup_equipment_cost_(M$)_______________________________________ (c244)________________________ 6.8000E+00 + Auxiliary_facilities_cost_(M$)__________________________________________ (c245)________________________ 1.5000E+00 + Total_account_24_cost_(M$)______________________________________________ (c24)_________________________ 4.1184E+01 + # Miscellaneous Plant Equipment # + Miscellaneous_plant_equipment_cost_(M$)_________________________________ (c25)_________________________ 2.5000E+01 + # Heat Rejection System # + Heat_rejection_system_cost_(M$)_________________________________________ (c26)_________________________ 4.9877E+01 + # Plant Direct Cost # + Plant_direct_cost_(M$)__________________________________________________ (cdirt)_______________________ 5.4635E+03 + # Reactor Core Cost # + Reactor_core_cost_(M$)__________________________________________________ (crctcore)____________________ 3.3761E+03 + # Indirect Cost # + Indirect_cost_(M$)______________________________________________________ (c9)__________________________ 1.8221E+03 + # Total Contingency # + Total_contingency_(M$)__________________________________________________ (ccont)_______________________ 1.4207E+03 + # Constructed Cost # + Constructed_cost_(M$)___________________________________________________ (concost)_____________________ 8.7063E+03 + # Interest during Construction # + Interest_during_construction_(M$)_______________________________________ (moneyint)____________________ 1.4365E+03 + # Total Capital Investment # + Total_capital_investment_(M$)___________________________________________ (capcost)_____________________ 1.0143E+04 + # Plant Availability # + Allowable_blanket_neutron_fluence_(MW-yr/m2)____________________________ (abktflnc)____________________ 5.0000E+00 + Allowable_divertor_heat_fluence_(MW-yr/m2)______________________________ (adivflnc)____________________ 7.0000E+00 + First_wall_/_blanket_lifetime_(years)___________________________________ (bktlife)_____________________ 6.1566E+00 OP + Divertor_lifetime_(years)_______________________________________________ (divlife)_____________________ 3.9769E+00 OP + Heating/CD_system_lifetime_(years)______________________________________ (cdrlife)_____________________ 6.1566E+00 OP + Total_plant_lifetime_(years)____________________________________________ (tlife)_______________________ 3.0000E+01 + Total_plant_availability_fraction_______________________________________ (cfactr)______________________ 8.0000E-01 + Number_of_fusion_cycles_to_reach_allowable_fw/blanket_DPA_______________ (bktcycles)___________________ 1.5787E+04 + # Plasma # + Tokamak_aspect_ratio_=_Conventional,_itart_=_0__________________________ (itart)_______________________ 0.0000E+00 + Major_radius_(m)________________________________________________________ (rmajor)______________________ 8.0000E+00 ITV + Minor_radius_(m)________________________________________________________ (rminor)______________________ 2.6667E+00 + Aspect_ratio____________________________________________________________ (aspect)______________________ 3.0000E+00 + Elongation,_X-point_(input_value_used)__________________________________ (kappa)_______________________ 1.8500E+00 + Elongation,_95%_surface_(calculated_from_kappa)_________________________ (kappa95)_____________________ 1.6518E+00 + Elongation,_area_ratio_calc.____________________________________________ (kappaa)______________________ 1.7188E+00 + Triangularity,_X-point_(input_value_used)_______________________________ (triang)______________________ 5.0000E-01 + Triangularity,_95%_surface_(calculated_from_triang)_____________________ (triang95)____________________ 3.3333E-01 + Plasma_poloidal_perimeter_(m)___________________________________________ (pperim)______________________ 2.4081E+01 + Plasma_cross-sectional_area_(m2)________________________________________ (xarea)_______________________ 3.8398E+01 + Plasma_surface_area_(m2)________________________________________________ (sarea)_______________________ 1.1738E+03 OP + Plasma_volume_(m3)______________________________________________________ (vol)_________________________ 1.8882E+03 OP + Plasma_current_scaling_law_used_________________________________________ (icurr)_______________________ 4 + Plasma_current_(MA)_____________________________________________________ (plascur/1D6)_________________ 1.6631E+01 + Current_density_profile_factor__________________________________________ (alphaj)______________________ 1.9805E+00 + Plasma_internal_inductance,_li__________________________________________ (rli)_________________________ 1.2275E+00 + Vertical_field_at_plasma_(T)____________________________________________ (bvert)_______________________ -7.4373E-01 + Vacuum_toroidal_field_at_R_(T)__________________________________________ (bt)__________________________ 5.2940E+00 ITV + Average_poloidal_field_(T)______________________________________________ (bp)__________________________ 8.6787E-01 + Total_field_(sqrt(bp^2_+_bt^2))_(T)_____________________________________ (btot)________________________ 5.3647E+00 + Safety_factor_on_axis___________________________________________________ (q0)__________________________ 1.0000E+00 + Safety_factor_at_95%_flux_surface_______________________________________ (q95)_________________________ 3.5961E+00 ITV + Cylindrical_safety_factor_(qcyl)________________________________________ (qstar)_______________________ 2.9805E+00 + Total_plasma_beta_______________________________________________________ (beta)________________________ 3.3648E-02 ITV + Total_poloidal_beta_____________________________________________________ (betap)_______________________ 1.2857E+00 OP + Total_toroidal_beta_____________________________________________________ ______________________________ 3.4553E-02 OP + Fast_alpha_beta_________________________________________________________ (betaft)______________________ 4.2236E-03 OP + Beam_ion_beta___________________________________________________________ (betanb)______________________ 0.0000E+00 OP + (Fast_alpha_+_beam_physics_variables.beta)/(thermal_physics_variables.be (gammaft)_____________________ 1.4354E-01 OP + Thermal_beta____________________________________________________________ ______________________________ 2.9425E-02 OP + Thermal_poloidal_beta___________________________________________________ ______________________________ 1.1243E+00 OP + Thermal_toroidal_physics_variables.beta_(=_beta-exp)____________________ ______________________________ 3.0215E-02 OP + 2nd_stability_physics_variables.beta_:_beta_p_/_(R/a)___________________ (eps*betap)___________________ 4.2857E-01 + 2nd_stability_physics_variables.beta_upper_limit________________________ (epbetmax)____________________ 1.3800E+00 + Beta_g_coefficient______________________________________________________ (dnbeta)______________________ 4.9099E+00 + Normalised_thermal_beta_________________________________________________ ______________________________ 2.4977E+00 + Normalised_total_beta___________________________________________________ ______________________________ 2.8562E+00 + Normalised_toroidal_beta________________________________________________ (normalised_toroidal_beta)____ 2.9330E+00 + Limit_on_thermal_beta___________________________________________________ (betalim)_____________________ 5.7842E-02 + Plasma_thermal_energy_(J)_______________________________________________ ______________________________ 9.5431E+08 OP + Total_plasma_internal_energy_(J)________________________________________ (total_plasma_internal_energy) 1.0913E+09 OP + Electron_temperature_(keV)______________________________________________ (te)__________________________ 1.2489E+01 ITV + Electron_temperature_on_axis_(keV)______________________________________ (te0)_________________________ 2.5758E+01 + Ion_temperature_(keV)___________________________________________________ (ti)__________________________ 1.2489E+01 + Ion_temperature_on_axis_(keV)___________________________________________ (ti0)_________________________ 2.5758E+01 + Electron_temp.,_density_weighted_(keV)__________________________________ (ten)_________________________ 1.3805E+01 + Electron_density_(/m3)__________________________________________________ (dene)________________________ 8.0667E+19 ITV + Electron_density_on_axis_(/m3)__________________________________________ (ne0)_________________________ 1.0610E+20 OP + Line-averaged_electron_density_(/m3)____________________________________ (dnla)________________________ 8.9334E+19 OP + Line-averaged_electron_density_/_Greenwald_density______________________ (dnla_gw)_____________________ 1.2000E+00 OP + Ion_density_(/m3)_______________________________________________________ (dnitot)______________________ 7.1669E+19 OP + Fuel_density_(/m3)______________________________________________________ (deni)________________________ 6.4831E+19 OP + Total_impurity_density_with_Z_>_2_(no_He)_(/m3)_________________________ (dnz)_________________________ 4.6503E+16 OP + Helium_ion_density_(thermalised_ions_only)_(/m3)________________________ (dnalp)_______________________ 6.7723E+18 OP + Proton_density_(/m3)____________________________________________________ (dnprot)______________________ 1.8963E+16 OP + Hot_beam_density_(/m3)__________________________________________________ (dnbeam)______________________ 0.0000E+00 OP + Density_limit_from_scaling_(/m3)________________________________________ (dnelimt)_____________________ 7.4445E+19 OP + Density_limit_(enforced)_(/m3)__________________________________________ (boundu(9)*dnelimt)___________ 7.4445E+19 OP + Helium_ion_density_(thermalised_ions_only)_/_electron_density___________ (ralpne)______________________ 8.3954E-02 ITV + H__concentration________________________________________________________ (fimp(01))____________________ 8.0392E-01 OP + He_concentration________________________________________________________ (fimp(02))____________________ 8.3954E-02 + Be_concentration________________________________________________________ (fimp(03))____________________ 0.0000E+00 + C__concentration________________________________________________________ (fimp(04))____________________ 0.0000E+00 + N__concentration________________________________________________________ (fimp(05))____________________ 0.0000E+00 + O__concentration________________________________________________________ (fimp(06))____________________ 0.0000E+00 + Ne_concentration________________________________________________________ (fimp(07))____________________ 0.0000E+00 + Si_concentration________________________________________________________ (fimp(08))____________________ 0.0000E+00 + Ar_concentration________________________________________________________ (fimp(09))____________________ 0.0000E+00 + Fe_concentration________________________________________________________ (fimp(10))____________________ 0.0000E+00 + Ni_concentration________________________________________________________ (fimp(11))____________________ 0.0000E+00 + Kr_concentration________________________________________________________ (fimp(12))____________________ 0.0000E+00 + Xe_concentration________________________________________________________ (fimp(13))____________________ 5.7149E-04 ITV + W__concentration________________________________________________________ (fimp(14))____________________ 5.0000E-06 + Average_mass_of_all_ions_(amu)__________________________________________ (aion)________________________ 2.7252E+00 OP + Effective_charge________________________________________________________ (zeff)________________________ 2.5164E+00 + Density_profile_factor__________________________________________________ (alphan)______________________ 1.0000E+00 + Plasma_profile_model____________________________________________________ (ipedestal)___________________ 1 + Density_pedestal_r/a_location___________________________________________ (rhopedn)_____________________ 9.4000E-01 + Electron_density_pedestal_height_(/m3)__________________________________ (neped)_______________________ 6.3278E+19 OP + Electron_density_at_pedestal_/_nGW______________________________________ (fgwped_out)__________________ 8.5000E-01 + Temperature_pedestal_r/a_location_______________________________________ (rhopedt)_____________________ 9.4000E-01 + Pedestal_scaling_switch_________________________________________________ (ieped)_______________________ 0 + Electron_temp._pedestal_height_(keV)____________________________________ (teped)_______________________ 5.5000E+00 + Electron_temp._at_separatrix_(keV)______________________________________ (tesep)_______________________ 1.0000E-01 + Electron_density_at_separatrix_(/m3)____________________________________ (nesep)_______________________ 3.7223E+19 + Electron_density_at_separatrix_/_nGW____________________________________ (fgwsep_out)__________________ 5.0000E-01 + Temperature_profile_index_______________________________________________ (alphat)______________________ 1.4500E+00 + Temperature_profile_index_beta__________________________________________ (tbeta)_______________________ 2.0000E+00 + Old_ASDEX_model_________________________________________________________ (dlimit(1))___________________ 5.2797E+19 OP + Borrass_ITER_model_I____________________________________________________ (dlimit(2))___________________ 1.0969E+20 OP + Borrass_ITER_model_II___________________________________________________ (dlimit(3))___________________ 4.3575E+19 OP + JET_edge_radiation_model________________________________________________ (dlimit(4))___________________ 3.0227E+21 OP + JET_simplified_model____________________________________________________ (dlimit(5))___________________ 4.3397E+20 OP + Hugill-Murakami_Mq_model________________________________________________ (dlimit(6))___________________ 6.6609E+19 OP + Greenwald_model_________________________________________________________ (dlimit(7))___________________ 7.4445E+19 OP + Deuterium_fuel_fraction_________________________________________________ (fdeut)_______________________ 5.0000E-01 + Tritium_fuel_fraction___________________________________________________ (ftrit)_______________________ 5.0000E-01 + Total_fusion_power_(MW)_________________________________________________ (powfmw)______________________ 1.6202E+03 OP + _=____D-T_fusion_power_(MW)_____________________________________________ (pdt)_________________________ 1.6182E+03 OP + __+___D-D_fusion_power_(MW)_____________________________________________ (pdd)_________________________ 1.9494E+00 OP + __+_D-He3_fusion_power_(MW)_____________________________________________ (pdhe3)_______________________ 0.0000E+00 OP + Alpha_power:_total_(MW)_________________________________________________ (palpmw)______________________ 3.2365E+02 OP + Alpha_power:_beam-plasma_(MW)___________________________________________ (palpnb)______________________ 0.0000E+00 OP + Neutron_power_(MW)______________________________________________________ (pneutmw)_____________________ 1.2953E+03 OP + Charged_particle_power_(excluding_alphas)_(MW)__________________________ (pchargemw)___________________ 1.2659E+00 OP + Total_power_deposited_in_plasma_(MW)____________________________________ (tot_power_plasma)____________ 3.8950E+02 OP + Bremsstrahlung_radiation_power_(MW)_____________________________________ (pbrempv*vol)_________________ 6.5195E+01 OP + Line_radiation_power_(MW)_______________________________________________ (plinepv*vol)_________________ 1.4609E+02 OP + Synchrotron_radiation_power_(MW)________________________________________ (psyncpv*vol)_________________ 1.5187E+01 OP + Synchrotron_wall_reflectivity_factor____________________________________ (ssync)_______________________ 6.0000E-01 + Normalised_minor_radius_defining_'core'_________________________________ (coreradius)__________________ 7.5000E-01 + Fraction_of_core_radiation_subtracted_from_P_L__________________________ (coreradiationfraction)_______ 6.0000E-01 + Radiation_power_from_inner_zone_(MW)____________________________________ (pinnerzoneradmw)_____________ 9.1650E+01 OP + Radiation_power_from_outer_zone_(MW)____________________________________ (pouterzoneradmw)_____________ 1.3482E+02 OP + Total_radiation_power_from_inside_LCFS_(MW)_____________________________ (pradmw)______________________ 2.2647E+02 OP + LCFS_radiation_fraction_=_total_radiation_in_LCFS_/_total_power_deposite (rad_fraction_LCFS)___________ 5.8144E-01 OP + Nominal_mean_radiation_load_on_inside_surface_of_reactor_(MW/m2)________ (photon_wall)_________________ 1.7749E-01 OP + Peaking_factor_for_radiation_wall_load__________________________________ (peakfactrad)_________________ 3.3300E+00 IP + Maximum_permitted_radiation_wall_load_(MW/m^2)__________________________ (maxradwallload)______________ 1.0000E+00 IP + Peak_radiation_wall_load_(MW/m^2)_______________________________________ (peakradwallload)_____________ 5.9106E-01 OP + Fast_alpha_particle_power_incident_on_the_first_wall_(MW)_______________ (palpfwmw)____________________ 1.6182E+01 OP + Nominal_mean_neutron_load_on_inside_surface_of_reactor_(MW/m2)__________ (wallmw)______________________ 1.0152E+00 OP + Power_incident_on_the_divertor_targets_(MW)_____________________________ (ptarmw)______________________ 3.2606E+01 OP + Fraction_of_power_to_the_lower_divertor_________________________________ (ftar)________________________ 1.0000E+00 IP + Outboard_side_heat_flux_decay_length_(m)________________________________ (lambdaio)____________________ 1.5700E-03 OP + Fraction_of_power_on_the_inner_targets__________________________________ (fio)_________________________ 4.1000E-01 OP + Fraction_of_power_incident_on_the_lower_inner_target____________________ (fLI)_________________________ 4.1000E-01 OP + Fraction_of_power_incident_on_the_lower_outer_target____________________ (fLO)_________________________ 5.9000E-01 OP + Power_incident_on_the_lower_inner_target_(MW)___________________________ (pLImw)_______________________ 1.3368E+01 OP + Power_incident_on_the_lower_outer_target_(MW)___________________________ (pLOmw)_______________________ 1.9237E+01 OP + Ohmic_heating_power_(MW)________________________________________________ (pohmmw)______________________ 6.2284E-01 OP + Fraction_of_alpha_power_deposited_in_plasma_____________________________ (falpha)______________________ 9.5000E-01 + Fraction_of_alpha_power_to_electrons____________________________________ (falpe)_______________________ 7.1828E-01 + Fraction_of_alpha_power_to_ions_________________________________________ (falpi)_______________________ 2.8172E-01 + Ion_transport_(MW)______________________________________________________ (ptrimw)______________________ 1.4013E+02 OP + Electron_transport_(MW)_________________________________________________ (ptremw)______________________ 1.5772E+02 OP + Injection_power_to_ions_(MW)____________________________________________ (pinjimw)_____________________ 0.0000E+00 OP + Injection_power_to_electrons_(MW)_______________________________________ (pinjemw)_____________________ 8.0143E+01 OP + Ignited_plasma_switch_(0=not_ignited,_1=ignited)________________________ (ignite)______________________ 0 + Power_into_divertor_zone_via_charged_particles_(MW)_____________________ (pdivt)_______________________ 1.6303E+02 OP + Psep_/_R_ratio_(MW/m)___________________________________________________ (pdivt/rmajor)________________ 2.0378E+01 OP + Psep_Bt_/_qAR_ratio_(MWT/m)_____________________________________________ (pdivtbt/qar)_________________ 1.0000E+01 OP + ITER_1996_scaling:_nominal_(MW)_________________________________________ (pthrmw(1))___________________ 1.2978E+02 OP + ITER_1996_scaling:_upper_bound_(MW)_____________________________________ (pthrmw(2))___________________ 2.8603E+02 OP + ITER_1996_scaling:_lower_bound_(MW)_____________________________________ (pthrmw(3))___________________ 5.8098E+01 OP + ITER_1997_scaling_(1)_(MW)______________________________________________ (pthrmw(4))___________________ 2.1452E+02 OP + ITER_1997_scaling_(2)_(MW)______________________________________________ (pthrmw(5))___________________ 1.7206E+02 OP + Martin_2008_scaling:_nominal_(MW)_______________________________________ (pthrmw(6))___________________ 9.7416E+01 OP + Martin_2008_scaling:_95%_upper_bound_(MW)_______________________________ (pthrmw(7))___________________ 1.2769E+02 OP + Martin_2008_scaling:_95%_lower_bound_(MW)_______________________________ (pthrmw(8))___________________ 6.7143E+01 OP + Snipes_2000_scaling:_nominal_(MW)_______________________________________ (pthrmw(9))___________________ 6.7785E+01 OP + Snipes_2000_scaling:_upper_bound_(MW)___________________________________ (pthrmw(10))__________________ 9.9437E+01 OP + Snipes_2000_scaling:_lower_bound_(MW)___________________________________ (pthrmw(11))__________________ 4.5839E+01 OP + Snipes_2000_scaling_(closed_divertor):_nominal_(MW)_____________________ (pthrmw(12))__________________ 3.1010E+01 OP + Snipes_2000_scaling_(closed_divertor):_upper_bound_(MW)_________________ (pthrmw(13))__________________ 4.3148E+01 OP + Snipes_2000_scaling_(closed_divertor):_lower_bound_(MW)_________________ (pthrmw(14))__________________ 2.2130E+01 OP + Hubbard_2012_L-I_threshold_-_nominal_(MW)_______________________________ (pthrmw(15))__________________ 2.7549E+01 OP + Hubbard_2012_L-I_threshold_-_lower_bound_(MW)___________________________ (pthrmw(16))__________________ 1.4319E+01 OP + Hubbard_2012_L-I_threshold_-_upper_bound_(MW)___________________________ (pthrmw(17))__________________ 5.3005E+01 OP + Hubbard_2017_L-I_threshold______________________________________________ (pthrmw(18))__________________ 2.6202E+02 OP + Martin_2008_aspect_ratio_corrected_scaling:_nominal_(MW)________________ (pthrmw(19))__________________ 9.7416E+01 OP + Martin_2008_aspect_ratio_corrected_scaling:_95%_upper_bound_(MW)________ (pthrmw(20))__________________ 1.2769E+02 OP + Martin_2008_aspect_ratio_corrected_scaling:_95%_lower_bound_(MW)________ (pthrmw(21))__________________ 6.7143E+01 OP + L-H_threshold_power_(enforced)_(MW)_____________________________________ (boundl(103)*plhthresh)_______ 9.7416E+01 OP + L-H_threshold_power_(MW)________________________________________________ (plhthresh)___________________ 9.7416E+01 OP + Confinement_H_factor____________________________________________________ (hfact)_______________________ 1.1886E+00 ITV + Global_thermal_energy_confinement_time_(s)______________________________ (taueff)______________________ 3.2037E+00 + Ion_energy_confinement_time_(s)_________________________________________ (tauei)_______________________ 3.2037E+00 + Electron_energy_confinement_time_(s)____________________________________ (tauee)_______________________ 3.2037E+00 + n.tau_=_Volume-average_electron_density_x_Energy_confinement_time_(s/m3) (dntau)_______________________ 2.5843E+20 OP + Triple_product__(keV_s/m3)______________________________________________ (dntau*te)____________________ 3.2275E+21 OP + Transport_loss_power_assumed_in_scaling_law_(MW)________________________ (powerht)_____________________ 2.9785E+02 OP + Switch_for_radiation_loss_term_usage_in_power_balance___________________ (iradloss)____________________ 1 + Radiation_power_subtracted_from_plasma_power_balance_(MW)_______________ ______________________________ 9.1650E+01 OP + Alpha_particle_confinement_time_(s)_____________________________________ (taup)________________________ 2.2270E+01 + Alpha_particle/energy_confinement_time_ratio____________________________ (taup/taueff)_________________ 6.9512E+00 + Lower_limit_on_taup/taueff______________________________________________ (taulimit)____________________ 5.0000E+00 + Total_energy_confinement_time_including_radiation_loss_(s)______________ (total_energy_conf_time)______ 2.8018E+00 + Normalized_plasma_pressure_beta_as_defined_by_McDonald_et_al____________ (beta_mcdonald)_______________ 3.4553E-02 OP + Normalized_ion_Larmor_radius____________________________________________ (rho_star)____________________ 1.9603E-03 OP + Normalized_collisionality_______________________________________________ (nu_star)_____________________ 3.7266E-03 OP + Volume_measure_of_elongation____________________________________________ (kappaa_IPB)__________________ 1.6815E+00 OP + Total_volt-second_requirement_(Wb)______________________________________ (vsstt)_______________________ 5.5616E+02 OP + Inductive_volt-seconds_(Wb)_____________________________________________ (vsind)_______________________ 2.3585E+02 OP + Ejima_coefficient_______________________________________________________ (gamma)_______________________ 3.0000E-01 + Start-up_resistive_(Wb)_________________________________________________ (vsres)_______________________ 5.0159E+01 OP + Flat-top_resistive_(Wb)_________________________________________________ (vsbrn)_______________________ 2.7015E+02 OP + bootstrap_current_fraction_multiplier___________________________________ (cboot)_______________________ 1.0000E+00 + Bootstrap_fraction_(ITER_1989)__________________________________________ (bscf_iter89)_________________ 3.7098E-01 + Bootstrap_fraction_(Sauter_et_al)_______________________________________ (bscf_sauter)_________________ 4.1920E-01 + Bootstrap_fraction_(Nevins_et_al)_______________________________________ (bscf_nevins)_________________ 3.5042E-01 + Bootstrap_fraction_(Wilson)_____________________________________________ (bscf_wilson)_________________ 4.3349E-01 + Diamagnetic_fraction_(Hender)___________________________________________ (diacf_hender)________________ 1.2017E-02 + Diamagnetic_fraction_(SCENE)____________________________________________ (diacf_scene)_________________ 1.1139E-02 + Pfirsch-Schlueter_fraction_(SCENE)______________________________________ (pscf_scene)__________________ -3.0283E-03 + Bootstrap_fraction_(enforced)___________________________________________ (bootipf.)____________________ 4.1920E-01 + Diamagnetic_fraction_(enforced)_________________________________________ (diaipf.)_____________________ 0.0000E+00 + Pfirsch-Schlueter_fraction_(enforced)___________________________________ (psipf.)______________________ 0.0000E+00 + Loop_voltage_during_burn_(V)____________________________________________ (vburn)_______________________ 3.7450E-02 OP + Plasma_resistance_(ohm)_________________________________________________ (rplas)_______________________ 3.9755E-09 OP + Resistive_diffusion_time_(s)____________________________________________ (res_time)____________________ 3.0619E+03 OP + Plasma_inductance_(H)___________________________________________________ (rlp)_________________________ 1.4181E-05 OP + Coefficient_for_sawtooth_effects_on_burn_V-s_requirement________________ (csawth)______________________ 1.0000E+00 + Ratio_of_He_and_pellet_particle_confinement_times_______________________ (tauratio)____________________ 1.0000E+00 + Fuelling_rate_(nucleus-pairs/s)_________________________________________ (qfuel)_______________________ 3.3420E+21 OP + Fuel_burn-up_rate_(reactions/s)_________________________________________ (rndfuel)_____________________ 5.7755E+20 OP + Burn-up_fraction________________________________________________________ (burnup)______________________ 1.7282E-01 + # Energy confinement times, and required H-factors : # + # Current Drive System # + Current_drive_efficiency_model__________________________________________ (iefrf)_______________________ 10 + Secondary_current_drive_efficiency_model________________________________ (iefrffix)____________________ 0 + Ratio_of_power_for_flat-top_to_start-up_(MW)____________________________ (startupratio)________________ 1.0000E+00 + Auxiliary_power_used_for_plasma_heating_only_(MW)_______________________ (pheat)_______________________ 7.5000E+01 + Power_injected_for_current_drive_(MW)___________________________________ (pcurrentdrivemw)_____________ 5.1429E+00 + Maximum_Allowed_Bootstrap_current_fraction______________________________ (bscfmax)_____________________ 9.5000E-01 + Fusion_gain_factor_Q____________________________________________________ (bigq)________________________ 2.0060E+01 OP + Auxiliary_current_drive_(A)_____________________________________________ (auxiliary_cd)________________ 2.3908E+05 OP + Current_drive_efficiency_(A/W)__________________________________________ (effcd)_______________________ 4.6488E-02 OP + Normalised_current_drive_efficiency,_gamma_(10^20_A/W-m2)_______________ (gamcd)_______________________ 3.0000E-01 OP + Wall_plug_to_injector_efficiency________________________________________ (etacd)_______________________ 5.0000E-01 + ECRH_plasma_heating_efficiency__________________________________________ (gamma_ecrh)__________________ 3.0000E-01 + Bootstrap_fraction______________________________________________________ (bootipf)_____________________ 4.1920E-01 + Diamagnetic_fraction____________________________________________________ (diaipf)______________________ 0.0000E+00 + Pfirsch-Schlueter_fraction______________________________________________ (psipf)_______________________ 0.0000E+00 + Auxiliary_current_drive_fraction________________________________________ (faccd)_______________________ 1.4376E-02 + Inductive_fraction______________________________________________________ (facoh)_______________________ 5.6642E-01 + Total___________________________________________________________________ (plasipf+faccd+facoh)_________ 1.0000E+00 + Fraction_of_the_plasma_current_produced_by_non-inductive_means__________ (fvsbrnni)____________________ 4.3358E-01 ITV + Electron_cyclotron_injected_power_(MW)__________________________________ (echpwr)______________________ 8.0143E+01 OP + Maximum_allowable_ECRH_power_(MW)_______________________________________ (pinjalw)_____________________ 2.0000E+02 + ECH_wall_plug_efficiency________________________________________________ (etaech)______________________ 5.0000E-01 + ECH_wall_plug_power_(MW)________________________________________________ (echwpow)_____________________ 1.6029E+02 OP + Total_V-s_capability_of_Central_Solenoid/PF_coils_(Wb)__________________ (abs(vstot))__________________ 5.7728E+02 + Required_volt-seconds_during_start-up_(Wb)______________________________ (vssoft)______________________ 2.8601E+02 + Available_volt-seconds_during_burn_(Wb)_________________________________ (vsmax)_______________________ 2.7014E+02 + # Times # + Initial_charge_time_for_CS_from_zero_current_(s)________________________ (tramp)_______________________ 5.0000E+02 + Plasma_current_ramp-up_time_(s)_________________________________________ (tohs)________________________ 1.6631E+02 + Heating_time_(s)________________________________________________________ (theat)_______________________ 1.0000E+01 + Burn_time_(s)___________________________________________________________ (tburn)_______________________ 7.2035E+03 OP + Reset_time_to_zero_current_for_CS_(s)___________________________________ (tqnch)_______________________ 1.6631E+02 + Time_between_pulses_(s)_________________________________________________ (tdwell)______________________ 1.8000E+03 + Total_plant_cycle_time_(s)______________________________________________ (tcycle)______________________ 9.8463E+03 OP + # Radial Build # + TF_coil_radial_placement_switch_________________________________________ (tf_in_cs)____________________ 0 + TF_coil_radial_placement_switch_________________________________________ (tf_in_cs)____________________ 0 + Machine_bore_(m)________________________________________________________ (bore)________________________ 1.9854E+00 ITV + CS_radial_thickness_(m)_________________________________________________ (ohcth)_______________________ 5.7587E-01 ITV + CS_precompression_(m)___________________________________________________ (precomp)_____________________ 6.8064E-02 + CS_precompresion_to_TF_coil_radial_gap_(m)______________________________ (gapoh)_______________________ 8.0000E-02 + TF_coil_inboard_leg_(m)_________________________________________________ (tfcth)_______________________ 9.1597E-01 ITV + TF_coil_inboard_leg_insulation_gap_(m)__________________________________ (tftsgap)_____________________ 5.0000E-02 + Thermal_shield,_inboard_(m)_____________________________________________ (thshield_ib)_________________ 5.0000E-02 + thermal_shield_to_vessel_radial_gap_(m)_________________________________ (gapds)_______________________ 2.0000E-02 + Inboard_vacuum_vessel_radial_thickness_(m)______________________________ (d_vv_in)_____________________ 3.0000E-01 + Inner_radiation_shield_radial_thickness_(m)_____________________________ (shldith)_____________________ 3.0000E-01 + Gap_(m)_________________________________________________________________ (vvblgap)_____________________ 2.0000E-02 + Inboard_blanket_radial_thickness_(m)____________________________________ (blnkith)_____________________ 7.0000E-01 + Inboard_first_wall_radial_thickness_(m)_________________________________ (fwith)_______________________ 1.8000E-02 + Inboard_scrape-off_radial_thickness_(m)_________________________________ (scrapli)_____________________ 2.5000E-01 + Outboard_scrape-off_radial_thickness_(m)________________________________ (scraplo)_____________________ 2.5000E-01 + Outboard_first_wall_radial_thickness_(m)________________________________ (fwoth)_______________________ 1.8000E-02 + Outboard_blanket_radial_thickness_(m)___________________________________ (blnkoth)_____________________ 1.0000E+00 + Outer_radiation_shield_radial_thickness_(m)_____________________________ (shldoth)_____________________ 8.0000E-01 + Outboard_vacuum_vessel_radial_thickness_(m)_____________________________ (d_vv_out)____________________ 3.0000E-01 + Vessel_to_TF_radial_gap_(m)_____________________________________________ (gapsto)______________________ 1.3720E+00 + Thermal_shield,_outboard_(m)____________________________________________ (thshield_ob)_________________ 5.0000E-02 + Gap_(m)_________________________________________________________________ (tftsgap)_____________________ 5.0000E-02 + TF_coil_outboard_leg_radial_thickness_(m)_______________________________ (tfthko)______________________ 9.1597E-01 + # Vertical Build # + Divertor_null_switch____________________________________________________ (i_single_null)_______________ 1 + Vessel_-_TF_coil_vertical_gap_(m)_______________________________________ (vgap2)_______________________ 1.6300E-01 + Topside_vacuum_vessel_radial_thickness_(m)______________________________ (d_vv_top)____________________ 3.0000E-01 + Top_radiation_shield_thickness_(m)______________________________________ (shldtth)_____________________ 6.0000E-01 + Top_blanket_vertical_thickness_(m)______________________________________ (blnktth)_____________________ 8.5000E-01 + Top_first_wall_vertical_thickness_(m)___________________________________ (fwtth)_______________________ 1.8000E-02 + Top_scrape-off_vertical_thickness_(m)___________________________________ (vgaptop)_____________________ 6.0000E-01 + Plasma_half-height_(m)__________________________________________________ (rminor*kappa)________________ 4.9333E+00 + Bottom_scrape-off_vertical_thickness_(m)________________________________ (vgap)________________________ 2.0019E+00 + Divertor_structure_vertical_thickness_(m)_______________________________ (divfix)______________________ 6.2000E-01 + Bottom_radiation_shield_thickness_(m)___________________________________ (shldlth)_____________________ 7.0000E-01 + Underside_vacuum_vessel_radial_thickness_(m)____________________________ (d_vv_bot)____________________ 3.0000E-01 + External_cryostat_thickness_(m)_________________________________________ (ddwex)_______________________ 1.5000E-01 + Ratio_of_Central_solenoid_height_to_TF_coil_internal_height_____________ (ohhghf)______________________ 9.0000E-01 + Width_of_neutral_beam_duct_where_it_passes_between_the_TF_coils_(m)_____ (beamwd)______________________ 5.8000E-01 + # Divertor build and plasma position # + Plasma_top_position,_radial_(m)_________________________________________ (ptop_radial)_________________ 6.6667E+00 + Plasma_top_position,_vertical_(m)_______________________________________ (ptop_vertical)_______________ 4.9333E+00 + Plasma_geometric_centre,_radial_(m)_____________________________________ (physics_variables.rmajor.)___ 8.0000E+00 + Plasma_geometric_centre,_vertical_(m)___________________________________ (0.0)_________________________ 0.0000E+00 + Plasma_lower_physics_variables.triangularity____________________________ (tril)________________________ 5.0000E-01 + Plasma_elongation_______________________________________________________ (physics_variables.kappa.)____ 1.8500E+00 + TF_coil_vertical_offset_(m)_____________________________________________ (tfoffset)____________________ -6.1694E-01 + Plasma_outer_arc_radius_of_curvature_(m)________________________________ (rco)_________________________ 5.0422E+00 + Plasma_inner_arc_radius_of_curvature_(m)________________________________ (rci)_________________________ 9.7933E+00 + Plasma_lower_X-pt,_radial_(m)___________________________________________ (rxpt)________________________ 6.6667E+00 + Plasma_lower_X-pt,_vertical_(m)_________________________________________ (zxpt)________________________ -4.9333E+00 + Poloidal_plane_angle_between_vertical_and_inner_leg_(rad)_______________ (thetai)______________________ 2.0820E-01 + Poloidal_plane_angle_between_vertical_and_outer_leg_(rad)_______________ (thetao)______________________ 1.0429E+00 + Poloidal_plane_angle_between_inner_leg_and_plate_(rad)__________________ (betai)_______________________ 1.0000E+00 + Poloidal_plane_angle_between_outer_leg_and_plate_(rad)__________________ (betao)_______________________ 1.0000E+00 + Inner_divertor_leg_poloidal_length_(m)__________________________________ (plsepi)______________________ 1.0000E+00 + Outer_divertor_leg_poloidal_length_(m)__________________________________ (plsepo)______________________ 1.5000E+00 + Inner_divertor_plate_length_(m)_________________________________________ (plleni)______________________ 1.0000E+00 + Outer_divertor_plate_length_(m)_________________________________________ (plleno)______________________ 1.0000E+00 + Inner_strike_point,_radial_(m)__________________________________________ (rspi)________________________ 5.6883E+00 + Inner_strike_point,_vertical_(m)________________________________________ (zspi)________________________ -5.1400E+00 + Inner_plate_top,_radial_(m)_____________________________________________ (rplti)_______________________ 5.8656E+00 + Inner_plate_top,_vertical_(m)___________________________________________ (zplti)_______________________ -4.6725E+00 + Inner_plate_bottom,_radial_(m)__________________________________________ (rplbi)_______________________ 5.5109E+00 + Inner_plate_bottom,_vertical_(m)________________________________________ (zplbi)_______________________ -5.6075E+00 + Outer_strike_point,_radial_(m)__________________________________________ (rspo)________________________ 7.4223E+00 + Outer_strike_point,_vertical_(m)________________________________________ (zspo)________________________ -6.2291E+00 + Outer_plate_top,_radial_(m)_____________________________________________ (rplto)_______________________ 7.6496E+00 + Outer_plate_top,_vertical_(m)___________________________________________ (zplto)_______________________ -5.7838E+00 + Outer_plate_bottom,_radial_(m)__________________________________________ (rplbo)_______________________ 7.1949E+00 + Outer_plate_bottom,_vertical_(m)________________________________________ (zplbo)_______________________ -6.6744E+00 + Calculated_maximum_divertor_height_(m)__________________________________ (divht)_______________________ 2.0019E+00 + # TF coils # + Allowable_maximum_shear_stress_in_TF_coil_case_(Tresca_criterion)_(Pa)__ (sig_tf_case_max)_____________ 7.5000E+08 + Allowable_maximum_shear_stress_in_TF_coil_conduit_(Tresca_criterion)_(Pa (sig_tf_wp_max)_______________ 7.5000E+08 + WP_transverse_modulus_(GPa)_____________________________________________ (eyoung_wp_trans*1.0d-9)______ 4.3534E+01 OP + WP_vertical_modulus_(GPa)_______________________________________________ (eyoung_wp_axial*1.0d-9)______ 1.1510E+02 OP + WP_transverse_Poissons_ratio____________________________________________ (poisson_wp_trans)____________ 3.0390E-01 OP + WP_vertical-transverse_Pois._rat._______________________________________ (poisson_wp_axial)____________ 3.1568E-01 OP + Radial____stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_r_max(1))_____________ 4.8849E-08 + toroidal__stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_t_max(1))_____________ -4.8724E+08 + Vertical__stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_z_max(1))_____________ 2.6028E+08 + Von-Mises_stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_vmises_max(1))________ 6.5725E+08 + Maximum_shear_stress_for_the_Tresca_yield_criterion_1_(Pa)______________ (sig_tf_tresca_max(1))________ 7.4752E+08 + Radial____stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_r_max(2))_____________ -1.5411E+08 + toroidal__stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_t_max(2))_____________ -3.7861E+08 + Vertical__stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_z_max(2))_____________ 2.6028E+08 + Von-Mises_stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_vmises_max(2))________ 5.5645E+08 + Maximum_shear_stress_for_the_Tresca_yield_criterion_2_(Pa)______________ (sig_tf_tresca_max(2))________ 6.3889E+08 + Radial____stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_r_max(3))_____________ 6.1398E+06 + toroidal__stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_t_max(3))_____________ -3.6314E+08 + Vertical__stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_z_max(3))_____________ 1.4510E+08 + Von-Mises_stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_vmises_max(3))________ 4.5345E+08 + Maximum_shear_stress_for_the_Tresca_yield_criterion_3_(Pa)______________ (sig_tf_tresca_max(3))________ 5.0824E+08 + Maximum_radial_deflection_at_midplane_(m)_______________________________ (deflect)_____________________ -6.2714E-03 OP + Vertical_strain_on_casing_______________________________________________ (casestr)_____________________ 1.2697E-03 OP + Radial_strain_on_insulator______________________________________________ (insstrain)___________________ -7.6923E-03 OP + Conductor_technology____________________________________________________ (i_tf_sup)____________________ 1 + Superconductor_material_________________________________________________ (i_tf_sc_mat)_________________ 1 + Presence_of_TF_demountable_joints_______________________________________ (itart)_______________________ 0 + TF_inboard_leg_support_strategy_________________________________________ (i_tf_bucking)________________ 1 + Number_of_TF_coils______________________________________________________ (n_tf)________________________ 16 + Inboard_leg_centre_radius_(m)___________________________________________ (r_tf_inboard_mid)____________ 3.1673E+00 OP + Outboard_leg_centre_radius_(m)__________________________________________ (r_tf_outboard_mid)___________ 1.4985E+01 OP + Total_inboard_leg_radial_thickness_(m)__________________________________ (tfcth)_______________________ 9.1597E-01 ITV + Total_outboard_leg_radial_thickness_(m)_________________________________ (tfthko)______________________ 9.1597E-01 + Outboard_leg_toroidal_thickness_(m)_____________________________________ (tftort)______________________ 1.4145E+00 OP + Maximum_inboard_edge_height_(m)_________________________________________ (hmax)________________________ 8.8182E+00 OP + Mean_coil_circumference_(including_inboard_leg_length)_(m)______________ (tfleng)______________________ 4.7937E+01 OP + Vertical_TF_shape_______________________________________________________ (i_tf_shape)__________________ 1 + TF_coil_arc_point_0_R_(m)_______________________________________________ (xarc(1))_____________________ 3.6253E+00 + TF_coil_arc_point_0_Z_(m)_______________________________________________ (yarc(1))_____________________ 4.5506E+00 + TF_coil_arc_point_1_R_(m)_______________________________________________ (xarc(2))_____________________ 7.4667E+00 + TF_coil_arc_point_1_Z_(m)_______________________________________________ (yarc(2))_____________________ 7.5843E+00 + TF_coil_arc_point_2_R_(m)_______________________________________________ (xarc(3))_____________________ 1.4527E+01 + TF_coil_arc_point_2_Z_(m)_______________________________________________ (yarc(3))_____________________ 0.0000E+00 + TF_coil_arc_point_3_R_(m)_______________________________________________ (xarc(4))_____________________ 7.4667E+00 + TF_coil_arc_point_3_Z_(m)_______________________________________________ (yarc(4))_____________________ -8.8182E+00 + TF_coil_arc_point_4_R_(m)_______________________________________________ (xarc(5))_____________________ 3.6253E+00 + TF_coil_arc_point_4_Z_(m)_______________________________________________ (yarc(5))_____________________ -5.2909E+00 + TF_cross-section_(total)_(m2)___________________________________________ (tfareain)____________________ 1.8229E+01 + Total_steel_cross-section_(m2)__________________________________________ (a_tf_steel*n_tf)_____________ 1.2853E+01 + Total_steel_TF_fraction_________________________________________________ (f_tf_steel)__________________ 7.0508E-01 + Total_Insulation_cross-section_(total)_(m2)_____________________________ (a_tf_ins*n_tf)_______________ 8.4752E-01 + Total_Insulation_fraction_______________________________________________ (f_tf_ins)____________________ 4.6493E-02 + Casing_cross_section_area_(per_leg)_(m2)________________________________ (acasetf)_____________________ 5.6444E-01 + Inboard_leg_case_plasma_side_wall_thickness_(m)_________________________ (casthi)______________________ 6.0000E-02 + Inboard_leg_case_inboard_"nose"_thickness_(m)___________________________ (thkcas)______________________ 2.8216E-01 ITV + Inboard_leg_case_sidewall_thickness_at_its_narrowest_point_(m)__________ (casths)______________________ 5.0000E-02 + External_case_mass_per_coil_(kg)________________________________________ (whtcas)______________________ 5.5456E+05 OP + WP_cross_section_area_with_insulation_and_insertion_(per_coil)_(m2)_____ (awpc)________________________ 5.7486E-01 + WP_cross_section_area_(per_coil)_(m2)___________________________________ (aswp)________________________ 5.1696E-01 + Winding_pack_radial_thickness_(m)_______________________________________ (dr_tf_wp)____________________ 5.0416E-01 ITV + Winding_pack_toroidal_width_1_(m)_______________________________________ (wwp1)________________________ 1.1904E+00 OP + Winding_pack_toroidal_width_2_(m)_______________________________________ (wwp2)________________________ 1.0901E+00 OP + Ground_wall_insulation_thickness_(m)____________________________________ (tinstf)______________________ 8.0000E-03 + Winding_pack_insertion_gap_(m)__________________________________________ (tfinsgap)____________________ 1.0000E-02 + Steel_WP_cross-section_(total)_(m2)_____________________________________ (aswp*n_tf)___________________ 3.8217E+00 + Steel_WP_fraction_______________________________________________________ (aswp/awpc)___________________ 4.1550E-01 + Insulation_WP_fraction__________________________________________________ (aiwp/awpc)___________________ 4.7934E-02 + Cable_WP_fraction_______________________________________________________ ((awpc-aswp-aiwp)/awpc)_______ 5.3656E-01 + Turn_parametrisation____________________________________________________ (i_tf_turns_integer)__________ 0 + Number_of_turns_per_TF_coil_____________________________________________ (n_tf_turn)___________________ 1.4739E+02 OP + Width_of_turn_including_inter-turn_insulation_(m)_______________________ (t_turn_tf)___________________ 5.9223E-02 OP + Width_of_conductor_(square)_(m)_________________________________________ (t_conductor)_________________ 5.7623E-02 OP + Width_of_space_inside_conductor_(m)_____________________________________ (t_cable)_____________________ 4.1604E-02 OP + Steel_conduit_thickness_(m)_____________________________________________ (thwcndut)____________________ 8.0099E-03 ITV + Inter-turn_insulation_thickness_(m)_____________________________________ (thicndut)____________________ 8.0000E-04 + Diameter_of_central_helium_channel_in_cable_____________________________ (dhecoil)_____________________ 1.0000E-02 + internal_area_of_the_cable_space________________________________________ (acstf)_______________________ 1.6999E-03 + Coolant_fraction_in_conductor_excluding_central_channel_________________ (vftf)________________________ 3.0000E-01 + Copper_fraction_of_conductor____________________________________________ (fcutfsu)_____________________ 8.4212E-01 ITV + Superconductor_fraction_of_conductor____________________________________ (1-fcutfsu)___________________ 1.5788E-01 + Check_total_area_fractions_in_winding_pack_=_1__________________________ ______________________________ 1.0000E+00 + minimum_TF_conductor_temperature_margin__(K)____________________________ (tmargmin_tf)_________________ 1.5000E+00 + TF_conductor_temperature_margin_(K)_____________________________________ (tmargtf)_____________________ 1.5049E+00 + Elastic_properties_behavior_____________________________________________ (i_tf_cond_eyoung_axial)______ 0 + Conductor_axial_Youngs_modulus__________________________________________ (eyoung_cond_axial)___________ 0.0000E+00 + Conductor_transverse_Youngs_modulus_____________________________________ (eyoung_cond_trans)___________ 0.0000E+00 + Superconductor_mass_per_coil_(kg)_______________________________________ (whtconsc)____________________ 4.6964E+03 OP + Copper_mass_per_coil_(kg)_______________________________________________ (whtconcu)____________________ 5.8073E+04 OP + Steel_conduit_mass_per_coil_(kg)________________________________________ (whtconsh)____________________ 8.9310E+04 OP + Conduit_insulation_mass_per_coil_(kg)___________________________________ (whtconin)____________________ 2.3777E+03 OP + Total_conduit_mass_per_coil_(kg)________________________________________ (whtcon)______________________ 1.5446E+05 OP + Mass_of_each_TF_coil_(kg)_______________________________________________ (whttf/n_tf)__________________ 7.1402E+05 OP + Total_TF_coil_mass_(kg)_________________________________________________ (whttf)_______________________ 1.1424E+07 OP + Nominal_peak_field_assuming_toroidal_symmetry_(T)_______________________ (bmaxtf)______________________ 1.2178E+01 OP + Total_current_in_all_TF_coils_(MA)______________________________________ (ritfc/1.D6)__________________ 2.1176E+02 OP + TF_coil_current_(summed_over_all_coils)_(A)_____________________________ (ritfc)_______________________ 2.1176E+08 + Actual_peak_field_at_discrete_conductor_(T)_____________________________ (bmaxtfrp)____________________ 1.2636E+01 OP + Winding_pack_current_density_(A/m2)_____________________________________ (jwptf)_______________________ 2.5602E+07 OP + Inboard_leg_mid-plane_conductor_current_density_(A/m2)__________________ (oacdcp)______________________ 1.1617E+07 + Total_stored_energy_in_TF_coils_(GJ)____________________________________ (estotftgj)___________________ 1.2161E+02 OP + Inboard_vertical_tension_per_coil_(N)___________________________________ (vforce)______________________ 2.0908E+08 OP + Outboard_vertical_tension_per_coil_(N)__________________________________ (vforce_outboard)_____________ 2.0908E+08 OP + inboard_vertical_tension_fraction_(-)___________________________________ (f_vforce_inboard)____________ 5.0000E-01 OP + Centring_force_per_coil_(N/m)___________________________________________ (cforce)______________________ 8.0590E+07 OP + Max_allowed_tfcoil_variables.ripple_amplitude_at_plasma_outboard_midplan (ripmax)______________________ 6.0000E-01 + Ripple_amplitude_at_plasma_outboard_midplane_(%)________________________ (ripple)______________________ 6.0000E-01 OP + Actual_quench_time_(or_time_constant)_(s)_______________________________ (tdmptf)______________________ 1.8429E+01 ITV + Vacuum_Vessel_stress_on_quench_(Pa)_____________________________________ (vv_stress_quench)____________ 6.1442E+07 OP + Maximum_allowed_voltage_during_quench_due_to_insulation_(kV)____________ (vdalw)_______________________ 9.5837E+00 ITV + Actual_quench_voltage_(kV)______________________________________________ (vtfskv)______________________ 9.1862E+00 OP + Maximum_allowed_temp_rise_during_a_quench_(K)___________________________ (tmaxpro)_____________________ 1.5000E+02 + # Superconducting TF Coils # + Superconductor_switch___________________________________________________ (isumat)______________________ 1 + Critical_field_at_zero_temperature_and_strain_(T)_______________________ (bc20m)_______________________ 3.2970E+01 + Critical_temperature_at_zero_field_and_strain_(K)_______________________ (tc0m)________________________ 1.6060E+01 + Helium_temperature_at_peak_field_(=_superconductor_temperature)_(K)_____ (thelium)_____________________ 4.7500E+00 + Total_helium_fraction_inside_cable_space________________________________ (fhetot)______________________ 3.4620E-01 OP + Copper_fraction_of_conductor____________________________________________ (fcutfsu)_____________________ 8.4212E-01 ITV + Residual_manufacturing_strain_on_superconductor_________________________ (str_tf_con_res)______________ -5.0000E-03 + Self-consistent_strain_on_superconductor________________________________ (str_wp)______________________ 2.0730E-03 + Critical_current_density_in_superconductor_(A/m2)_______________________ (jcritsc)_____________________ 7.1337E+08 OP + Critical_current_density_in_strand_(A/m2)_______________________________ (jcritstr)____________________ 1.1263E+08 OP + Critical_current_density_in_winding_pack_(A/m2)_________________________ (jwdgcrt)_____________________ 3.5688E+07 OP + Actual_current_density_in_winding_pack_(A/m2)___________________________ (jwdgop)______________________ 2.5602E+07 OP + Minimum_allowed_temperature_margin_in_superconductor_(K)________________ (tmargmin_tf)_________________ 1.5000E+00 + Actual_temperature_margin_in_superconductor_(K)_________________________ (tmarg)_______________________ 1.5049E+00 OP + Critical_current_(A)____________________________________________________ (icrit)_______________________ 1.2517E+05 OP + Actual_current_(A)______________________________________________________ (cpttf)_______________________ 8.9795E+04 ITV + Actual_current_/_critical_current_______________________________________ (iooic)_______________________ 7.1737E-01 OP + # Central Solenoid and PF Coils # + Central_solenoid_superconductor_material________________________________ (isumatoh)____________________ 1 + Maximum_field_at_Beginning_Of_Pulse_(T)_________________________________ (bmaxoh0)_____________________ 1.4050E+01 OP + Critical_superconductor_current_density_at_BOP_(A/m2)___________________ (jscoh_bop)___________________ 3.4918E+08 OP + Critical_strand_current_density_at_BOP_(A/m2)___________________________ (jstrandoh_bop)_______________ 1.0475E+08 OP + Allowable_overall_current_density_at_BOP_(A/m2)_________________________ (rjohc0)______________________ 3.5294E+07 OP + Actual_overall_current_density_at_BOP_(A/m2)____________________________ (cohbop)______________________ 1.9126E+07 OP + Maximum_field_at_End_Of_Flattop_(T)_____________________________________ (bmaxoh)______________________ 1.3920E+01 OP + Critical_superconductor_current_density_at_EOF_(A/m2)___________________ (jscoh_eof)___________________ 3.6097E+08 OP + Critical_strand_current_density_at_EOF_(A/m2)___________________________ (jstrandoh_eof)_______________ 1.0829E+08 OP + Allowable_overall_current_density_at_EOF_(A/m2)_________________________ (rjohc)_______________________ 3.6485E+07 OP + Actual_overall_current_density_at_EOF_(A/m2)____________________________ (coheof)______________________ 2.0264E+07 ITV + CS_inside_radius_(m)____________________________________________________ (bore)________________________ 1.9854E+00 ITV + CS_thickness_(m)________________________________________________________ (ohcth)_______________________ 5.7587E-01 ITV + Gap_between_central_solenoid_and_TF_coil_(m)____________________________ (gapoh)_______________________ 8.0000E-02 + CS_overall_cross-sectional_area_(m2)____________________________________ (areaoh)______________________ 9.1407E+00 OP + CS_conductor+void_cross-sectional_area_(m2)_____________________________ (awpoh)_______________________ 4.3996E+00 OP + ___CS_conductor_cross-sectional_area_(m2)_______________________________ (awpoh*(1-vfohc))_____________ 3.0797E+00 OP + ___CS_void_cross-sectional_area_(m2)____________________________________ (awpoh*vfohc)_________________ 1.3199E+00 OP + CS_steel_cross-sectional_area_(m2)______________________________________ (areaoh-awpoh)________________ 4.7411E+00 OP + CS_steel_area_fraction__________________________________________________ (oh_steel_frac)_______________ 5.1868E-01 ITV + Switch_for_CS_stress_calculation________________________________________ (i_cs_stress)_________________ 0 + Allowable_stress_in_CS_steel_(Pa)_______________________________________ (alstroh)_____________________ 7.5000E+08 + Hoop_stress_in_CS_steel_(Pa)____________________________________________ (sig_hoop)____________________ 6.7569E+08 OP + Axial_stress_in_CS_steel_(Pa)___________________________________________ (sig_axial)___________________ -7.6205E+08 OP + Maximum_shear_stress_in_CS_steel_for_the_Tresca_criterion_(Pa)__________ (s_tresca_oh)_________________ 6.7569E+08 OP + Axial_force_in_CS_(N)___________________________________________________ (axial_force)_________________ -1.6256E+09 OP + Residual_manufacturing_strain_in_CS_superconductor_material_____________ (tfcoil_variables.str_cs_con_r -5.0000E-03 + Copper_fraction_in_strand_______________________________________________ (fcuohsu)_____________________ 7.0000E-01 + Void_(coolant)_fraction_in_conductor____________________________________ (vfohc)_______________________ 3.0000E-01 + Helium_coolant_temperature_(K)__________________________________________ (tftmp)_______________________ 4.7500E+00 + CS_temperature_margin_(K)_______________________________________________ (tmargoh)_____________________ 1.5052E+00 OP + Minimum_permitted_temperature_margin_(K)________________________________ (tmargmin_cs)_________________ 1.5000E+00 + Residual_hoop_stress_in_CS_Steel_(Pa)___________________________________ (residual_sig_hoop)___________ 2.4000E+08 + Minimum_burn_time_(s)___________________________________________________ (tbrnmn)______________________ 7.2000E+03 + Initial_vertical_crack_size_(m)_________________________________________ (t_crack_vertical)____________ 8.9000E-04 + Initial_radial_crack_size_(m)___________________________________________ (t_crack_radial)______________ 2.6700E-03 + CS_turn_area_(m)________________________________________________________ (a_oh_turn)___________________ 1.9739E-03 + CS_turn_length_(m)______________________________________________________ (l_cond_cst)__________________ 7.6953E-02 + CS_turn_internal_cable_space_radius_(m)_________________________________ (r_in_cst)____________________ 7.4740E-03 + CS_turn_width_(m)_______________________________________________________ (d_cond_cst)__________________ 2.5651E-02 + CS_structural_vertical_thickness_(m)____________________________________ (t_structural_vertical)_______ 5.3514E-03 + CS_structural_radial_thickness_(m)______________________________________ (t_structural_radial)_________ 5.3514E-03 + Allowable_number_of_cycles_till_CS_fracture_____________________________ (n_cycle)_____________________ 1.3378E+02 OP + Minimum_number_of_cycles_required_till_CS_fracture______________________ (n_cycle_min)_________________ 2.0000E+04 OP + PF_coil_superconductor_material_________________________________________ (isumatpf)____________________ 3 + Copper_fraction_in_conductor____________________________________________ (fcupfsu)_____________________ 6.9000E-01 + Maximum_permissible_tensile_stress_(MPa)________________________________ (sigpfcalw)___________________ 5.0000E+02 + JxB_hoop_force_fraction_supported_by_case_______________________________ (sigpfcf)_____________________ 6.6600E-01 + PF_coil_0_radius_(m)____________________________________________________ (rpf[0]_______________________ 5.5667E+00 + PF_coil_0_vertical_position_(m)_________________________________________ (zpf[0])______________________ 9.3603E+00 + PF_coil_0_radial_thickness_(m)__________________________________________ (pfdr(0))_____________________ 1.2727E+00 + PF_coil_0_vertical_thickness_(m)________________________________________ (pfdz(0))_____________________ 1.2727E+00 + PF_coil_0_turns_________________________________________________________ (turns[0])____________________ 4.4541E+02 + PF_coil_0_current_(MA)__________________________________________________ (ric[0])______________________ 1.7816E+01 + PF_coil_0_field_(T)_____________________________________________________ (bpf[0])______________________ 6.2280E+00 + PF_coil_1_radius_(m)____________________________________________________ (rpf[1]_______________________ 5.5667E+00 + PF_coil_1_vertical_position_(m)_________________________________________ (zpf[1])______________________ -1.0594E+01 + PF_coil_1_radial_thickness_(m)__________________________________________ (pfdr(1))_____________________ 1.3651E+00 + PF_coil_1_vertical_thickness_(m)________________________________________ (pfdz(1))_____________________ -1.3651E+00 + PF_coil_1_turns_________________________________________________________ (turns[1])____________________ 5.1248E+02 + PF_coil_1_current_(MA)__________________________________________________ (ric[1])______________________ 2.0499E+01 + PF_coil_1_field_(T)_____________________________________________________ (bpf[1])______________________ 6.6990E+00 + PF_coil_2_radius_(m)____________________________________________________ (rpf[2]_______________________ 1.6731E+01 + PF_coil_2_vertical_position_(m)_________________________________________ (zpf[2])______________________ 2.6667E+00 + PF_coil_2_radial_thickness_(m)__________________________________________ (pfdr(2))_____________________ 1.1332E+00 + PF_coil_2_vertical_thickness_(m)________________________________________ (pfdz(2))_____________________ 1.1332E+00 + PF_coil_2_turns_________________________________________________________ (turns[2])____________________ 1.9262E+02 + PF_coil_2_current_(MA)__________________________________________________ (ric[2])______________________ -7.7049E+00 + PF_coil_2_field_(T)_____________________________________________________ (bpf[2])______________________ 2.6389E+00 + PF_coil_3_radius_(m)____________________________________________________ (rpf[3]_______________________ 1.6731E+01 + PF_coil_3_vertical_position_(m)_________________________________________ (zpf[3])______________________ -2.6667E+00 + PF_coil_3_radial_thickness_(m)__________________________________________ (pfdr(3))_____________________ 1.1332E+00 + PF_coil_3_vertical_thickness_(m)________________________________________ (pfdz(3))_____________________ -1.1332E+00 + PF_coil_3_turns_________________________________________________________ (turns[3])____________________ 1.9262E+02 + PF_coil_3_current_(MA)__________________________________________________ (ric[3])______________________ -7.7049E+00 + PF_coil_3_field_(T)_____________________________________________________ (bpf[3])______________________ 2.6389E+00 + PF_coil_4_radius_(m)____________________________________________________ (rpf[4]_______________________ 1.5209E+01 + PF_coil_4_vertical_position_(m)_________________________________________ (zpf[4])______________________ 7.4667E+00 + PF_coil_4_radial_thickness_(m)__________________________________________ (pfdr(4))_____________________ 8.0773E-01 + PF_coil_4_vertical_thickness_(m)________________________________________ (pfdz(4))_____________________ 8.0773E-01 + PF_coil_4_turns_________________________________________________________ (turns[4])____________________ 1.3049E+02 + PF_coil_4_current_(MA)__________________________________________________ (ric[4])______________________ -5.2194E+00 + PF_coil_4_field_(T)_____________________________________________________ (bpf[4])______________________ 2.5737E+00 + PF_coil_5_radius_(m)____________________________________________________ (rpf[5]_______________________ 1.5209E+01 + PF_coil_5_vertical_position_(m)_________________________________________ (zpf[5])______________________ -7.4667E+00 + PF_coil_5_radial_thickness_(m)__________________________________________ (pfdr(5))_____________________ 8.0773E-01 + PF_coil_5_vertical_thickness_(m)________________________________________ (pfdz(5))_____________________ -8.0773E-01 + PF_coil_5_turns_________________________________________________________ (turns[5])____________________ 1.3049E+02 + PF_coil_5_current_(MA)__________________________________________________ (ric[5])______________________ -5.2194E+00 + PF_coil_5_field_(T)_____________________________________________________ (bpf[5])______________________ 2.5737E+00 + Central_solenoid_radius_(m)_____________________________________________ (rpf[nohc-1])_________________ 2.2734E+00 + Central_solenoid_vertical_position_(m)__________________________________ (zpf[nohc-1])_________________ 0.0000E+00 + Central_solenoid_radial_thickness_(m)___________________________________ (ohdr)________________________ 5.7587E-01 + Central_solenoid_vertical_thickness_(m)_________________________________ (ohdz)________________________ 1.5873E+01 + Central_solenoid_turns__________________________________________________ (turns[nohc-1])_______________ 4.6308E+03 + Central_solenoid_current_(MA)___________________________________________ (ric[nohc-1])_________________ -1.8523E+02 + Central_solenoid_field_(T)______________________________________________ (bpf[nohc-1])_________________ 1.4050E+01 + Sum_of_squares_of_residuals_____________________________________________ (ssq0)________________________ 3.5207E-04 OP + Smoothing_parameter_____________________________________________________ (alfapf)______________________ 5.0000E-10 + # Volt Second Consumption # + Total_volt-second_consumption_by_coils_(Wb)_____________________________ (vstot)_______________________ -5.8000E+02 OP + # Waveforms # + Ratio_of_central_solenoid_current_at_beginning_of_Pulse_/_end_of_flat-to (fcohbop)_____________________ 9.4380E-01 ITV + Ratio_of_central_solenoid_current_at_beginning_of_Flat-top_/_end_of_flat (fcohbof)_____________________ -1.4083E-01 OP + # PF Circuit Waveform Data # + Number_of_PF_circuits_including_CS_and_plasma___________________________ (ncirt)_______________________ 8 + PF_Circuit_0_Time_point_0_(A)___________________________________________ (pfc0t0)______________________ 0.0000E+00 + PF_Circuit_0_Time_point_1_(A)___________________________________________ (pfc0t1)______________________ 1.3971E+07 + PF_Circuit_0_Time_point_2_(A)___________________________________________ (pfc0t2)______________________ 1.7816E+07 + PF_Circuit_0_Time_point_3_(A)___________________________________________ (pfc0t3)______________________ 1.7816E+07 + PF_Circuit_0_Time_point_4_(A)___________________________________________ (pfc0t4)______________________ 9.2844E+05 + PF_Circuit_0_Time_point_5_(A)___________________________________________ (pfc0t5)______________________ 0.0000E+00 + PF_Circuit_1_Time_point_0_(A)___________________________________________ (pfc1t0)______________________ 0.0000E+00 + PF_Circuit_1_Time_point_1_(A)___________________________________________ (pfc1t1)______________________ 1.8269E+07 + PF_Circuit_1_Time_point_2_(A)___________________________________________ (pfc1t2)______________________ 2.0499E+07 + PF_Circuit_1_Time_point_3_(A)___________________________________________ (pfc1t3)______________________ 2.0499E+07 + PF_Circuit_1_Time_point_4_(A)___________________________________________ (pfc1t4)______________________ -1.5831E+06 + PF_Circuit_1_Time_point_5_(A)___________________________________________ (pfc1t5)______________________ 0.0000E+00 + PF_Circuit_2_Time_point_0_(A)___________________________________________ (pfc2t0)______________________ -0.0000E+00 + PF_Circuit_2_Time_point_1_(A)___________________________________________ (pfc2t1)______________________ 4.9542E+05 + PF_Circuit_2_Time_point_2_(A)___________________________________________ (pfc2t2)______________________ -7.1060E+06 + PF_Circuit_2_Time_point_3_(A)___________________________________________ (pfc2t3)______________________ -7.1060E+06 + PF_Circuit_2_Time_point_4_(A)___________________________________________ (pfc2t4)______________________ -7.7049E+06 + PF_Circuit_2_Time_point_5_(A)___________________________________________ (pfc2t5)______________________ -0.0000E+00 + PF_Circuit_3_Time_point_0_(A)___________________________________________ (pfc3t0)______________________ -0.0000E+00 + PF_Circuit_3_Time_point_1_(A)___________________________________________ (pfc3t1)______________________ 4.9542E+05 + PF_Circuit_3_Time_point_2_(A)___________________________________________ (pfc3t2)______________________ -7.1060E+06 + PF_Circuit_3_Time_point_3_(A)___________________________________________ (pfc3t3)______________________ -7.1060E+06 + PF_Circuit_3_Time_point_4_(A)___________________________________________ (pfc3t4)______________________ -7.7049E+06 + PF_Circuit_3_Time_point_5_(A)___________________________________________ (pfc3t5)______________________ -0.0000E+00 + PF_Circuit_4_Time_point_0_(A)___________________________________________ (pfc4t0)______________________ -0.0000E+00 + PF_Circuit_4_Time_point_1_(A)___________________________________________ (pfc4t1)______________________ 3.2650E+05 + PF_Circuit_4_Time_point_2_(A)___________________________________________ (pfc4t2)______________________ -4.8247E+06 + PF_Circuit_4_Time_point_3_(A)___________________________________________ (pfc4t3)______________________ -4.8247E+06 + PF_Circuit_4_Time_point_4_(A)___________________________________________ (pfc4t4)______________________ -5.2194E+06 + PF_Circuit_4_Time_point_5_(A)___________________________________________ (pfc4t5)______________________ -0.0000E+00 + PF_Circuit_5_Time_point_0_(A)___________________________________________ (pfc5t0)______________________ -0.0000E+00 + PF_Circuit_5_Time_point_1_(A)___________________________________________ (pfc5t1)______________________ 3.2650E+05 + PF_Circuit_5_Time_point_2_(A)___________________________________________ (pfc5t2)______________________ -4.8247E+06 + PF_Circuit_5_Time_point_3_(A)___________________________________________ (pfc5t3)______________________ -4.8247E+06 + PF_Circuit_5_Time_point_4_(A)___________________________________________ (pfc5t4)______________________ -5.2194E+06 + PF_Circuit_5_Time_point_5_(A)___________________________________________ (pfc5t5)______________________ -0.0000E+00 + CS_Circuit_Time_point_0_(A)_____________________________________________ (cs_t0)_______________________ -0.0000E+00 + CS_Circuit_Time_point_1_(A)_____________________________________________ (cs_t1)_______________________ 1.7482E+08 + CS_Circuit_Time_point_2_(A)_____________________________________________ (cs_t2)_______________________ 2.6086E+07 + CS_Circuit_Time_point_3_(A)_____________________________________________ (cs_t3)_______________________ 2.6086E+07 + CS_Circuit_Time_point_4_(A)_____________________________________________ (cs_t4)_______________________ -1.8523E+08 + CS_Circuit_Time_point_5_(A)_____________________________________________ (cs_t5)_______________________ -0.0000E+00 + Plasma_Time_point_0_(A)_________________________________________________ (plasmat0)____________________ 0.0000E+00 + Plasma_Time_point_1_(A)_________________________________________________ (plasmat1)____________________ 0.0000E+00 + Plasma_Time_point_2_(A)_________________________________________________ (plasmat2)____________________ 1.6631E+07 + Plasma_Time_point_3_(A)_________________________________________________ (plasmat3)____________________ 1.6631E+07 + Plasma_Time_point_4_(A)_________________________________________________ (plasmat4)____________________ 1.6631E+07 + Plasma_Time_point_5_(A)_________________________________________________ (plasmat5)____________________ 0.0000E+00 + # Support Structure # + Outer_PF_coil_fence_mass_(kg)___________________________________________ (fncmass)_____________________ 2.2924E+05 OP + Intercoil_support_structure_mass_(kg)___________________________________ (aintmass)____________________ 4.3045E+06 OP + Mass_of_cooled_components_(kg)__________________________________________ (coldmass)____________________ 3.4369E+07 OP + Gravity_support_structure_mass_(kg)_____________________________________ (clgsmass)____________________ 1.2760E+06 OP + Torus_leg_support_mass_(kg)_____________________________________________ (gsm1)________________________ 8.5820E+04 OP + Ring_beam_mass_(kg)_____________________________________________________ (gsm2)________________________ 4.0088E+05 OP + Ring_legs_mass_(kg)_____________________________________________________ (gsm3)________________________ 6.8283E+05 OP + # PF Coil Inductances # + # Nuclear Heating Magnets Before Renormalisation # + Shield_line_density_(tonne/m2)__________________________________________ (x_shield)____________________ 4.0560E+00 + Blanket_line_density_(tonne/m2)_________________________________________ (x_blanket)___________________ 2.2911E+00 + Unit_nuclear_heating_in_TF_coil_(W/GW)__________________________________ (tfc_nuc_heating)_____________ 1.4866E+04 + Total_nuclear_heating_in_TF_coil_(MW)___________________________________ (ptfnuc.)_____________________ 2.4085E-02 + powfmw__________________________________________________________________ (powfmw.)_____________________ 1.6202E+03 + total_mass_of_the_TF_coils_(kg)_________________________________________ (whttf)_______________________ 1.1424E+07 + # Pumping for primary coolant (helium) # + Pressure_drop_in_FW_and_blanket_coolant_incl._hx_and_pipes_(Pa)_________ (dp_he)_______________________ 5.5000E+05 + Fraction_of_FW_and_blanket_thermal_power_required_for_pumping___________ (fpump)_______________________ 8.9463E-02 OP + Total_power_absorbed_by_FW_&_blanket_(MW)_______________________________ (p_plasma)____________________ 1.6698E+03 OP + Inlet_temperature_of_FW_&_blanket_coolant_pump_(K)______________________ (t_in_compressor)_____________ 5.5703E+02 OP + Coolant_pump_outlet/Inlet_temperature_of_FW_&_blanket_(K)_______________ (t_in_bb)_____________________ 5.7313E+02 + Outlet_temperature_of_FW_&_blanket_(K)__________________________________ (t_out_bb)____________________ 7.7313E+02 + Mechanical_pumping_power_for_FW_and_blanket_cooling_loop_including_heat_ (htpmw_fw_blkt)_______________ 1.6407E+02 OP + Mechanical_pumping_power_for_divertor_(MW)______________________________ (htpmw_div)___________________ 1.6906E+00 OP + Mechanical_pumping_power_for_shield_and_vacuum_vessel_(MW)______________ (htpmw_shld)__________________ 7.0688E-03 OP + # First wall and blanket : CCFE HCPB model # + Titanium_beryllide_fraction_____________________________________________ (fbltibe12)___________________ 3.7500E-01 + Lithium_orthosilicate_fraction__________________________________________ (fblli2sio4)__________________ 3.7500E-01 + Steel_fraction__________________________________________________________ (fblss_ccfe)__________________ 9.7050E-02 + Coolant_fraction________________________________________________________ (vfcblkt)_____________________ 5.2950E-02 + Purge_gas_fraction______________________________________________________ (vfpblkt)_____________________ 1.0000E-01 + First_Wall_Armour_Volume_(m3)___________________________________________ (fw_armour_vol)_______________ 5.8692E+00 + First_Wall_Volume_(m3)__________________________________________________ (volfw)_______________________ 1.9807E+01 + Blanket_Volume_(m3)_____________________________________________________ (volblkt)_____________________ 1.1849E+03 + Shield_Volume_(m3)______________________________________________________ (volshld)_____________________ 7.8520E+02 + Vacuum_vessel_volume_(m3)_______________________________________________ (vdewin)______________________ 1.0178E+03 + First_Wall_Armour_Mass_(kg)_____________________________________________ (fw_armour_mass)______________ 1.1298E+05 OP + First_Wall_Mass,_excluding_armour_(kg)__________________________________ (fwmass)______________________ 1.5449E+05 OP + Blanket_Mass_-_Total(kg)________________________________________________ (whtblkt)_____________________ 2.9676E+06 OP + ____Blanket_Mass_-_TiBe12_(kg)__________________________________________ (whtbltibe12)_________________ 1.0042E+06 OP + ____Blanket_Mass_-_Li4SiO4_(kg)_________________________________________ (whtblli4sio4)________________ 1.0664E+06 OP + ____Blanket_Mass_-_Steel_(kg)___________________________________________ (whtblss)_____________________ 8.9696E+05 OP + Total_mass_of_armour,_first_wall_and_blanket_(kg)_______________________ (armour_fw_bl_mass)___________ 3.2350E+06 OP + Shield_Mass_(kg)________________________________________________________ (whtshld)_____________________ 2.4498E+06 OP + Vacuum_vessel_mass_(kg)_________________________________________________ (vvmass)______________________ 7.9388E+06 OP + Total_nuclear_heating_in_TF+PF_coils_(CS_is_negligible)_(MW)____________ (ptfnuc)______________________ 2.5118E-02 OP + Total_nuclear_heating_in_FW_(MW)________________________________________ (pnucfw)______________________ 1.6315E+02 OP + Total_nuclear_heating_in_the_blanket_(including_emult)_(MW)_____________ (pnucblkt)____________________ 1.2901E+03 OP + Total_nuclear_heating_in_the_shield_(MW)________________________________ (pnucshld)____________________ 1.4138E+00 OP + Total_nuclear_heating_in_the_divertor_(MW)______________________________ (pnucdiv)_____________________ 1.4906E+02 OP + Blanket_exponential_factor______________________________________________ (exp_blanket)_________________ 9.9936E-01 OP + Shield:_first_exponential_______________________________________________ (exp_shield1)_________________ 1.9523E-03 OP + Shield:_second_exponential______________________________________________ (exp_shield2)_________________ 2.5427E-01 OP + Solid_angle_fraction_taken_by_on_divertor_______________________________ (fdiv)________________________ 1.1500E-01 + Switch_for_plant_secondary_cycle________________________________________ (secondary_cycle)_____________ 2 + First_wall_coolant_pressure_(Pa)________________________________________ (fwpressure)__________________ 1.5500E+07 + Blanket_coolant_pressure_(Pa)___________________________________________ (blpressure)__________________ 1.5500E+07 + Allowable_nominal_neutron_fluence_at_first_wall_(MW.year/m2)____________ (abktflnc)____________________ 5.0000E+00 + No_of_inboard_blanket_modules_poloidally________________________________ (nblktmodpi)__________________ 7 + No_of_inboard_blanket_modules_toroidally________________________________ (nblktmodti)__________________ 32 + No_of_outboard_blanket_modules_poloidally_______________________________ (nblktmodpo)__________________ 8 + No_of_outboard_blanket_modules_toroidally_______________________________ (nblktmodto)__________________ 48 + Isentropic_efficiency_of_first_wall_/_blanket_coolant_pumps_____________ (etaiso)______________________ 9.0000E-01 + First_wall_area_(m2)____________________________________________________ (fwarea)______________________ 1.6044E+03 OP + Cryostat_internal_radius_(m)____________________________________________ (rdewex)______________________ 1.7798E+01 OP + Cryostat_internal_half-height_(m)_______________________________________ (zdewex)______________________ 1.5339E+01 OP + Vertical_clearance_from_TF_coil_to_cryostat_(m)_________________________ (clh1)________________________ 5.6044E+00 OP + Divertor_area_(m2)______________________________________________________ (divsur)______________________ 1.4879E+02 OP + Divertor_mass_(kg)______________________________________________________ (divmas)______________________ 3.6453E+04 OP + # Superconducting TF Coil Power Conversion # + TF_coil_current_(kA)____________________________________________________ (itfka)_______________________ 8.9795E+01 OP + Number_of_TF_coils______________________________________________________ (ntfc)________________________ 1.6000E+01 + Voltage_across_a_TF_coil_during_quench_(kV)_____________________________ (vtfskv)______________________ 9.1862E+00 OP + TF_coil_charge_time_(hours)_____________________________________________ (tchghr)______________________ 4.0000E+00 + Total_inductance_of_TF_coils_(H)________________________________________ (ltfth)_______________________ 3.0165E+01 OP + Total_resistance_of_TF_coils_(ohm)______________________________________ (rcoils)______________________ 0.0000E+00 OP + TF_coil_charging_voltage_(V)____________________________________________ (tfcv)________________________ 2.9268E+02 + Number_of_DC_circuit_breakers___________________________________________ (ntfbkr)______________________ 1.6000E+01 + Number_of_dump_resistors________________________________________________ (ndumpr)______________________ 6.4000E+01 + Resistance_per_dump_resistor_(ohm)______________________________________ (r1dump)______________________ 1.0230E-01 OP + Dump_resistor_peak_power_(MW)___________________________________________ (r1ppmw)______________________ 2.0622E+02 OP + Energy_supplied_per_dump_resistor_(MJ)__________________________________ (r1emj)_______________________ 1.9002E+03 OP + TF_coil_L/R_time_constant_(s)___________________________________________ (ttfsec)______________________ 1.8429E+01 OP + Power_supply_voltage_(V)________________________________________________ (tfpsv)_______________________ 3.0731E+02 OP + Power_supply_current_(kA)_______________________________________________ (tfpska)______________________ 9.4285E+01 OP + DC_power_supply_rating_(kW)_____________________________________________ (tfckw)_______________________ 2.8975E+04 OP + AC_power_for_charging_(kW)______________________________________________ (tfackw)______________________ 3.2194E+04 OP + TF_coil_resistive_power_(MW)____________________________________________ (rpower)______________________ 9.3902E+00 OP + TF_coil_inductive_power_(MVA)___________________________________________ (xpower)______________________ 1.6891E+01 OP + Aluminium_bus_current_density_(kA/cm2)__________________________________ (djmka)_______________________ 1.2500E-01 + Aluminium_bus_cross-sectional_area_(cm2)________________________________ (albusa)______________________ 7.1836E+02 OP + Total_length_of_TF_coil_bussing_(m)_____________________________________ (tfbusl)______________________ 3.1931E+03 OP + Aluminium_bus_weight_(tonnes)___________________________________________ (albuswt)_____________________ 6.1932E+02 OP + Total_TF_coil_bus_resistance_(ohm)______________________________________ (rtfbus)______________________ 1.1646E-03 OP + TF_coil_bus_voltage_drop_(V)____________________________________________ (vtfbus)______________________ 1.0457E+02 OP + Dump_resistor_floor_area_(m2)___________________________________________ (drarea)______________________ 4.9234E+03 OP + TF_coil_power_conversion_floor_space_(m2)_______________________________ (tfcfsp)______________________ 1.8228E+03 OP + TF_coil_power_conv._building_volume_(m3)________________________________ (tfcbv)_______________________ 1.0937E+04 OP + TF_coil_AC_inductive_power_demand_(MW)__________________________________ (xpwrmw)______________________ 1.8768E+01 OP + Total_steady_state_AC_power_demand_(MW)_________________________________ (tfacpd)______________________ 1.0434E+01 OP + # PF Coils and Central Solenoid: Power and Energy # + Number_of_PF_coil_circuits______________________________________________ (pfckts)______________________ 1.2000E+01 + Sum_of_PF_power_supply_ratings_(MVA)____________________________________ (spsmva)______________________ 3.0313E+02 OP + Total_PF_coil_circuit_bus_length_(m)____________________________________ (spfbusl)_____________________ 2.4480E+03 OP + Total_PF_coil_bus_resistive_power_(kW)__________________________________ (pfbuspwr)____________________ 9.6485E+02 OP + Total_PF_coil_resistive_power_(kW)______________________________________ (srcktpm)_____________________ 9.6485E+02 OP + Maximum_PF_coil_voltage_(kV)____________________________________________ (vpfskv)______________________ 2.0000E+01 + Efficiency_of_transfer_of_PF_stored_energy_into_or_out_of_storage_______ (etapsu)______________________ 9.0000E-01 + Maximum_stored_energy_in_poloidal_field_(MJ)____________________________ (ensxpfm)_____________________ 2.8804E+04 OP + Peak_absolute_rate_of_change_of_stored_energy_in_poloidal_field_(MW)____ (peakpoloidalpower)___________ 1.7319E+02 OP + # Vacuum System # + First_wall_outgassing_rate_(Pa_m/s)_____________________________________ (rat)_________________________ 1.3000E-08 + Total_outgassing_load_(Pa_m3/s)_________________________________________ (ogas)________________________ 1.6691E-04 OP + Base_pressure_required_(Pa)_____________________________________________ (pbase)_______________________ 5.0000E-04 + Required_N2_pump_speed_(m3/s)___________________________________________ (s(1))________________________ 3.3381E-01 OP + N2_pump_speed_provided_(m3/s)___________________________________________ (snet(1))_____________________ 2.3404E+01 OP + Plasma_chamber_volume_(m3)______________________________________________ (volume)______________________ 2.2588E+03 OP + Chamber_pressure_after_burn_(Pa)________________________________________ (pend)________________________ 1.6698E-01 OP + Chamber_pressure_before_burn_(Pa)_______________________________________ (pstart)______________________ 1.6698E-03 + Allowable_pumping_time_switch___________________________________________ (dwell_pump)__________________ 0 + Dwell_time_between_burns_(s)____________________________________________ (tdwell.)_____________________ 1.8000E+03 + CS_ramp-up_time_burns_(s)_______________________________________________ (tramp.)______________________ 5.0000E+02 + Allowable_pumping_time_between_burns_(s)________________________________ (tpump)_______________________ 1.8000E+03 + Required_D-T_pump_speed_(m3/s)__________________________________________ (s(2))________________________ 5.7790E+00 OP + D-T_pump_speed_provided_(m3/s)__________________________________________ (snet(2))_____________________ 5.6700E+01 OP + Divertor_chamber_gas_pressure_(Pa)______________________________________ (prdiv)_______________________ 3.6000E-01 + Helium_gas_fraction_in_divertor_chamber_________________________________ (fhe)_________________________ 1.7218E-01 OP + Required_helium_pump_speed_(m3/s)_______________________________________ (s(3))________________________ 3.8423E+01 OP + Helium_pump_speed_provided_(m3/s)_______________________________________ (snet(3))_____________________ 3.8423E+01 OP + D-T_fuelling_rate_(kg/s)________________________________________________ (frate)_______________________ 2.7747E-05 OP + Required_D-T_pump_speed_(m3/s)__________________________________________ (s(4))________________________ 3.8423E+01 OP + D-T_pump_speed_provided_(m3/s)__________________________________________ (snet(4))_____________________ 5.6700E+01 OP + Number_of_large_pump_ducts______________________________________________ (nduct)_______________________ 16 + Passage_diameter,_divertor_to_ducts_(m)_________________________________ (d(imax))_____________________ 4.7857E-01 OP + Passage_length_(m)______________________________________________________ (l1)__________________________ 1.7160E+00 OP + Diameter_of_ducts_(m)___________________________________________________ (dout)________________________ 5.7428E-01 OP + Duct_length,_divertor_to_elbow_(m)______________________________________ (l2)__________________________ 4.8000E+00 OP + Duct_length,_elbow_to_pumps_(m)_________________________________________ (l3)__________________________ 2.0000E+00 + Number_of_pumps_________________________________________________________ (pumpn)_______________________ 3.2000E+01 OP + # Plant Buildings System # + Internal_volume_of_reactor_building_(m3)________________________________ (vrci)________________________ 9.9708E+05 + Dist_from_centre_of_torus_to_bldg_wall_(m)______________________________ (wrbi)________________________ 3.9531E+01 + Effective_floor_area_(m2)_______________________________________________ (efloor)______________________ 3.3660E+05 + Reactor_building_volume_(m3)____________________________________________ (rbv)_________________________ 1.1310E+06 + Reactor_maintenance_building_volume_(m3)________________________________ (rmbv)________________________ 3.9641E+05 + Warmshop_volume_(m3)____________________________________________________ (wsv)_________________________ 1.2531E+05 + Tritium_building_volume_(m3)____________________________________________ (triv)________________________ 4.0000E+04 + Electrical_building_volume_(m3)_________________________________________ (elev)________________________ 5.1937E+04 + Control_building_volume_(m3)____________________________________________ (conv)________________________ 6.0000E+04 + Cryogenics_building_volume_(m3)_________________________________________ (cryv)________________________ 1.4976E+04 + Administration_building_volume_(m3)_____________________________________ (admv)________________________ 1.0000E+05 + Shops_volume_(m3)_______________________________________________________ (shov)________________________ 1.0000E+05 + Total_volume_of_nuclear_buildings_(m3)__________________________________ (volnucb)_____________________ 1.5738E+06 + # Electric Power Requirements # + Facility_base_load_(MW)_________________________________________________ (basemw)______________________ 5.0000E+00 + Divertor_coil_power_supplies_(MW)_______________________________________ (bdvmw)_______________________ 0.0000E+00 + Cryoplant_electric_power_(MW)___________________________________________ (crymw)_______________________ 3.6566E+01 OP + Primary_coolant_pumps_(MW)______________________________________________ (htpmw..)_____________________ 1.9053E+02 OP + PF_coil_power_supplies_(MW)_____________________________________________ (ppfmw)_______________________ 8.5511E+01 OP + TF_coil_power_supplies_(MW)_____________________________________________ (ptfmw)_______________________ 1.0434E+01 OP + Plasma_heating_supplies_(MW)____________________________________________ (pheatingmw)__________________ 1.6029E+02 OP + Tritium_processing_(MW)_________________________________________________ (trithtmw..)__________________ 1.5000E+01 + Vacuum_pumps__(MW)______________________________________________________ (vachtmw..)___________________ 5.0000E-01 + Total_pulsed_power_(MW)_________________________________________________ (pacpmw)______________________ 5.5432E+02 OP + Total_base_power_required_at_all_times_(MW)_____________________________ (fcsht)_______________________ 5.5490E+01 OP + # Cryogenics # + Conduction_and_radiation_heat_loads_on_cryogenic_components_(MW)________ (qss/1.0d6)___________________ 1.4779E-02 OP + Nuclear_heating_of_cryogenic_components_(MW)____________________________ (qnuc/1.0d6)__________________ 1.3000E-02 OP + AC_losses_in_cryogenic_components_(MW)__________________________________ (qac/1.0d6)___________________ 3.8170E-03 OP + Resistive_losses_in_current_leads_(MW)__________________________________ (qcl/1.0d6)___________________ 1.9539E-02 OP + 45%_allowance_for_heat_loads_in_transfer_lines,_storage_tanks_etc_(MW)__ (qmisc/1.0d6)_________________ 2.3011E-02 OP + Sum_=_Total_heat_removal_at_cryogenic_temperatures_(tfcoil_variables.tmp (helpow_+_helpow_cryal/1.0d6)_ 7.4146E-02 OP + Temperature_of_cryogenic_superconducting_components_(K)_________________ (tmpcry)______________________ 4.5000E+00 + Temperature_of_cryogenic_aluminium_components_(K)_______________________ (tcoolin)_____________________ 3.1315E+02 + Efficiency_(figure_of_merit)_of_cryogenic_plant_is_13%_of_ideal_Carnot_v ______________________________ 2.0277E-03 OP + Efficiency_(figure_of_merit)_of_cryogenic_aluminium_plant_is_40%_of_idea ______________________________ -2.0203E+00 OP + Electric_power_for_cryogenic_plant_(MW)_________________________________ (crypmw)______________________ 3.6566E+01 OP + # Plant Power / Heat Transport Balance # + Neutron_power_multiplication_in_blanket_________________________________ (emult)_______________________ 1.2690E+00 + Divertor_area_fraction_of_whole_toroid_surface__________________________ (fdiv)________________________ 1.1500E-01 + H/CD_apparatus_+_diagnostics_area_fraction______________________________ (fhcd)________________________ 0.0000E+00 + First_wall_area_fraction________________________________________________ (1-fdiv-fhcd)_________________ 8.8500E-01 + Switch_for_pumping_of_primary_coolant___________________________________ (primary_pumping)_____________ 3 + Mechanical_pumping_power_for_FW_cooling_loop_including_heat_exchanger_(M (htpmw_fw)____________________ 0.0000E+00 OP + Mechanical_pumping_power_for_blanket_cooling_loop_including_heat_exchang (htpmw_blkt)__________________ 0.0000E+00 OP + Mechanical_pumping_power_for_FW_and_blanket_cooling_loop_including_heat_ (htpmw_fw_blkt)_______________ 1.6407E+02 OP + Mechanical_pumping_power_for_divertor_(MW)______________________________ (htpmw_div)___________________ 1.6906E+00 OP + Mechanical_pumping_power_for_shield_and_vacuum_vessel_(MW)______________ (htpmw_shld)__________________ 7.0688E-03 OP + Electrical_pumping_power_for_FW_and_blanket_(MW)________________________ (htpmwe_fw_blkt)______________ 1.8858E+02 OP + Electrical_pumping_power_for_shield_(MW)________________________________ (htpmwe_shld)_________________ 8.1250E-03 OP + Electrical_pumping_power_for_divertor_(MW)______________________________ (htpmwe_div)__________________ 1.9433E+00 OP + Total_electrical_pumping_power_for_primary_coolant_(MW)_________________ (htpmw)_______________________ 1.9053E+02 OP + Coolant_pump_power_/_non-pumping_thermal_power_in_shield________________ (fpumpshld)___________________ 5.0000E-03 + Coolant_pump_power_/_non-pumping_thermal_power_in_divertor______________ (fpumpdiv)____________________ 5.0000E-03 + Electrical_efficiency_of_heat_transport_coolant_pumps___________________ (etahtp)______________________ 8.7000E-01 + Thermal_to_electric_conversion_efficiency_of_the_power_conversion_cycle_ (etath)_______________________ 4.0000E-01 + Fraction_of_total_high-grade_thermal_power_to_divertor__________________ (pdivfraction)________________ 1.5623E-01 + Total_power_leaving_reactor_(across_vacuum_vessel_boundary)_(MW)________ ______________________________ 2.0111E+03 + Heat_removal_from_cryogenic_plant_(MW)__________________________________ (crypmw)______________________ 3.6566E+01 + Heat_removal_from_facilities_(MW)_______________________________________ (fachtmw)_____________________ 5.5490E+01 + Coolant_pumping_efficiency_losses_(MW)__________________________________ (htpsecmw)____________________ 2.4769E+01 + Heat_removal_from_injection_power_(MW)__________________________________ (pinjht)______________________ 8.0143E+01 + Heat_removal_from_tritium_plant_(MW)____________________________________ (trithtmw)____________________ 1.5000E+01 + Heat_removal_from_vacuum_pumps_(MW)_____________________________________ (vachtmw)_____________________ 5.0000E-01 + TF_coil_resistive_power_(MW)____________________________________________ (tfcmw)_______________________ 0.0000E+00 + Total_low-grade_thermal_power_(MW)______________________________________ (psechtmw)____________________ 2.2417E+02 + Total_High-grade_thermal_power_(MW)_____________________________________ (pthermmw)____________________ 2.1751E+03 + Number_of_primary_heat_exchangers_______________________________________ (nphx)________________________ 3 OP + Transport_power_from_scaling_law_(MW)___________________________________ (pscalingmw)__________________ 2.9785E+02 + Radiation_power_from_inside_"coreradius"_(MW)___________________________ (pcoreradmw.)_________________ 9.1650E+01 + Total_(MW)______________________________________________________________ ______________________________ 3.8950E+02 + Alpha_power_deposited_in_plasma_(MW)____________________________________ (falpha*palpmw)_______________ 3.0746E+02 + Power_from_charged_products_of_DD_and/or_D-He3_fusion_(MW)______________ (pchargemw.)__________________ 1.2659E+00 + Ohmic_heating_(MW)______________________________________________________ (pohmmw.)_____________________ 6.2284E-01 + Injected_power_deposited_in_plasma_(MW)_________________________________ (pinjmw)______________________ 8.0143E+01 + Total_(MW)______________________________________________________________ ______________________________ 3.8950E+02 + Fusion_power_(MW)_______________________________________________________ (powfmw)______________________ 1.6202E+03 + Power_from_energy_multiplication_in_blanket_and_shield_(MW)_____________ (emultmw)_____________________ 3.0836E+02 + Injected_power_(MW)_____________________________________________________ (pinjmw.)_____________________ 8.0143E+01 + Ohmic_power_(MW)________________________________________________________ (pohmmw.)_____________________ 6.2284E-01 + Power_deposited_in_primary_coolant_by_pump_(MW)_________________________ (htpmw_mech)__________________ 1.6576E+02 + Total_(MW)______________________________________________________________ ______________________________ 2.1751E+03 + Heat_extracted_from_first_wall_and_blanket_(MW)_________________________ (pthermfw_blkt)_______________ 1.8339E+03 + Heat_extracted_from_shield__(MW)________________________________________ (pthermshld)__________________ 1.4208E+00 + Heat_extracted_from_divertor_(MW)_______________________________________ (pthermdiv)___________________ 3.3982E+02 + Nuclear_and_photon_power_lost_to_H/CD_system_(MW)_______________________ (psechcd)_____________________ 0.0000E+00 + Nuclear_power_lost_to_TF_(MW)___________________________________________ (ptfnuc)______________________ 2.5118E-02 + Total_(MW)______________________________________________________________ ______________________________ 2.1752E+03 + Net_electric_power_output(MW)___________________________________________ (pnetelmw.)___________________ 4.0001E+02 + Required_Net_electric_power_output(MW)__________________________________ (pnetelin)____________________ 4.0000E+02 + Electric_power_for_heating_and_current_drive_(MW)_______________________ (pinjwp)______________________ 1.6029E+02 + Electric_power_for_primary_coolant_pumps_(MW)___________________________ (htpmw)_______________________ 1.9053E+02 + Electric_power_for_vacuum_pumps_(MW)____________________________________ (vachtmw)_____________________ 5.0000E-01 + Electric_power_for_tritium_plant_(MW)___________________________________ (trithtmw)____________________ 1.5000E+01 + Electric_power_for_cryoplant_(MW)_______________________________________ (crypmw)______________________ 3.6566E+01 + Electric_power_for_TF_coils_(MW)________________________________________ (tfacpd)______________________ 1.0434E+01 + Electric_power_for_PF_coils_(MW)________________________________________ (pfwpmw)______________________ 1.2422E+00 + All_other_internal_electric_power_requirements_(MW)_____________________ (fachtmw)_____________________ 5.5490E+01 + Total_(MW)______________________________________________________________ (tot_plant_power)_____________ 8.7006E+02 + Total_(MW)______________________________________________________________ ______________________________ 8.7006E+02 + Gross_electrical_output*_(MW)___________________________________________ (pgrossmw)____________________ 8.7006E+02 + Fusion_power_(MW)_______________________________________________________ (powfmw)______________________ 1.6202E+03 + Power_from_energy_multiplication_in_blanket_and_shield_(MW)_____________ (emultmw)_____________________ 3.0836E+02 + Total_(MW)______________________________________________________________ ______________________________ 1.9285E+03 + Net_electrical_output_(MW) _____________________________________________ (pnetelmw)____________________ 4.0001E+02 + Heat_rejected_by_main_power_conversion_circuit_(MW)_____________________ (rejected_main)_______________ 1.3051E+03 + Heat_rejected_by_other_cooling_circuits_(MW)____________________________ (psechtmw)____________________ 2.2417E+02 + Total_(MW)______________________________________________________________ ______________________________ 1.9293E+03 + Net_electric_power_/_total_nuclear_power_(%)____________________________ (pnetelmw/(powfmw+emultmw)____ 2.0741E+01 + Net_electric_power_/_total_fusion_power_(%)_____________________________ (pnetelmw/powfmw)_____________ 2.4689E+01 + Gross_electric_power*_/_high_grade_heat_(%)_____________________________ (etath)_______________________ 4.0000E+01 + Recirculating_power_fraction____________________________________________ (cirpowfr)____________________ 5.4025E-01 + # Water usage during plant operation (secondary cooling) # + Volume_used_in_cooling_tower_(m3/day)___________________________________ (waterusetower)_______________ 5.5485E+04 OP + Volume_used_in_recirculating_water_system_(m3/day)______________________ (wateruserecirc)______________ 1.8617E+04 OP + Volume_used_in_once-through_water_system_(m3/day)_______________________ (wateruseonethru)_____________ 1.8244E+06 OP + # Errors and Warnings # + # Errors and Warnings # + PROCESS_error_status_flag_______________________________________________ (error_status)________________ 2 + Final_error_identifier__________________________________________________ (error_id)____________________ 244 + # End of PROCESS Output # + # End of PROCESS Output # + # Copy of PROCESS Input Follows # +************************************************************************************************************************ +***** ***** +***** Generic large tokamak file ***** +***** James Morris, UKAEA ***** +***** 28/06/23 ***** +***** ***** +************************************************************************* + +* Run Information * +******************* + +runtitle = Generic large tokamak + +* Figure of merit - minimise major radius +minmax = 1 + +* Error tolerance for VMCON +epsvmc = 1e-7 + +* Constraint Equations - Consistency Equations * +************************************************ + +* Beta consistency * +*------------------* +icc = 1 +ixc = 5 * beta +beta = 0.03 + +* Global power balance * +*----------------------* +icc = 2 + +* Radial build consistency * +*--------------------------* +icc = 11 + +* Constraint Equations - Limit Equations * +****************************************** + +* Density upper limit * +*---------------------* +icc = 5 +ixc = 6 * dene [m-3] +fdene = 1.2 +dene = 7.5E19 + +* Neutron wall load upper limit * +*-------------------------------* +icc = 8 +ixc = 14 * fwalld +fwalld = 1.0 +* wall load limit [MW/m2] +walalw = 2.0 + +* Fusion power upper limit * +*--------------------------* + +icc = 9 +ixc = 26 * ffuspow +* Maximum allowable value fusion power [MW] +powfmax = 3000 + +* Burn time lower limit * +*-----------------------* +icc = 13 +ixc = 21 * ftburn +* minimum burn time [s] +tbrnmn = 7200.0 + +* L-H threshold scaling * +*-----------------------* +icc = 15 +ixc = 103 * flhthresh +boundu(103) = 10.0 + +* Injection power upper limit * +*-----------------------------* +icc = 30 +ixc = 46 * fpinj +* Maximum allowable value for injected power [MW] +pinjalw = 200.0 + +* Net electric power lower limit * +*--------------------------------* +icc = 16 +ixc = 25 * fpnetel +* Minimum allowable value for net eletric power [MW] +pnetelin = 400.0 + +* Beta upper limit * +*------------------* +icc = 24 +ixc = 36 * fbetatry +fbetatry = 0.5 + +* Max TF field * +*--------------* +icc = 25 +ixc = 35 * fpeakb +* Maximum allowable value for toroidal magnetic field [T] +bmxlim = 14.0 + +* Central solenoid EOF current density upper limit * +*--------------------------------------------------* +icc = 26 +ixc = 37 * coheof [A/m2] +ixc = 38 * fjohc +boundu(38) = 1.0 +coheof = 1.5E7 +fjohc = 0.6 + +* Central solenoid BOP current density upper limit * +*--------------------------------------------------* +icc = 27 +ixc = 39 * fjohc0 +ixc = 41 * fcohbop +boundu(39) = 1.0 +fjohc0 = 0.6 +fcohbop = 0.9 + +* I_op/I_Crit TF coil limit * +*---------------------------* +icc = 33 +ixc = 50 * fiooic +boundu(50) = 1.0 +fiooic = 0.65 + +* Dump voltage upper limit * +*--------------------------* +icc = 34 +ixc = 51 * fvdump +ixc = 52 * vdalw [kV] +boundu(52) = 10.0 +fvdump = 1.0 +vdalw = 10.0 + +* J_winding pack protection * +*---------------------------* +icc = 35 +ixc = 53 * fjprot +fjprot = 1.0 + +* TF temp marg lower limit * +*--------------------------* +icc = 36 +ixc = 54 * ftmargtf +* Minimum allowable temperature margin [K] +tmargmin = 1.5 + +* CS coil temp margin lower limit * +*---------------------------------* +icc = 60 +ixc = 106 * ftmargoh +tmargmin_cs = 1.5 + +* Lower limit on taup/taueff (ratio alpha particle/energy confinement times) * +*-------------------------------------------------------------------------------* +icc = 62 +ixc = 110 * ftaulimit +taulimit = 5.0 + +* dump time constraint for VV stresses * +*--------------------------------------* +icc = 65 +ixc = 113 * fmaxvvstress +fmaxvvstress = 1.0 + +* CS stress limit * +*-----------------* +icc = 72 +ixc = 123 * foh_stress +foh_stress = 1.0 +* allowable hoop stress in Central Solenoid structural material [Pa] +alstroh = 7.5D8 + +* neped\n", + "\n", + "\n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + " \n", + "
tagobjf_namenorm_objfitvar001_namexcm001itvar002_namexcm002itvar003_namexcm003itvar004_name...itvar041_namexcm041itvar042_namexcm042itvar043_namexcm043itvar044_namexcm044itvar045_namexcm045
0large tokamak 1major radius1.6beta1.1216dene1.0756fwalld0.50758ffuspow...cpttf1.3815ralpne0.83954oh_steel_frac0.64835fimp(13)1.5039dr_tf_wp1.0083
\n", + "

1 rows × 93 columns

\n", + "" + ], + "text/plain": [ + " tag objf_name norm_objf itvar001_name xcm001 \\\n", + "0 large tokamak 1 major radius 1.6 beta 1.1216 \n", + "\n", + " itvar002_name xcm002 itvar003_name xcm003 itvar004_name ... \\\n", + "0 dene 1.0756 fwalld 0.50758 ffuspow ... \n", + "\n", + " itvar041_name xcm041 itvar042_name xcm042 itvar043_name xcm043 \\\n", + "0 cpttf 1.3815 ralpne 0.83954 oh_steel_frac 0.64835 \n", + "\n", + " itvar044_name xcm044 itvar045_name xcm045 \n", + "0 fimp(13) 1.5039 dr_tf_wp 1.0083 \n", + "\n", + "[1 rows x 93 columns]" + ] + }, + "execution_count": 2, + "metadata": {}, + "output_type": "execute_result" + }, + { + "data": { + "image/png": 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", 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" + ] + }, + "metadata": {}, + "output_type": "display_data" + } + ], + "source": [ + "data_dir = Path(\"data\")\n", + "runs_metadata = [\n", + " RunMetadata(data_dir / \"large_tokamak_1_MFILE.DAT\", \"large tokamak 1\"),\n", + "]\n", + "\n", + "# Figure and dataframe returned for optional further modification\n", + "fig1, df1 = plot_mfile_solutions(\n", + " runs_metadata=runs_metadata,\n", + " plot_title=\"Large tokamak solution 1\",\n", + ")\n", + "df1" + ] + }, + { + "attachments": {}, + "cell_type": "markdown", + "metadata": {}, + "source": [ + "## Plot two solutions\n", + "\n", + "Plot two MFILEs together, showing normalised values of the optimisation parameters at the solution points, as well as the objective function values." + ] + }, + { + "cell_type": "code", + "execution_count": 3, + "metadata": {}, + "outputs": [ + { + "data": { + "text/html": [ + "
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tagobjf_namenorm_objfitvar001_namexcm001itvar002_namexcm002itvar003_namexcm003itvar004_name...itvar041_namexcm041itvar042_namexcm042itvar043_namexcm043itvar044_namexcm044itvar045_namexcm045
0large tokamak 1major radius1.60beta1.1216dene1.0756fwalld0.50758ffuspow...cpttf1.3815ralpne0.83954oh_steel_frac0.64835fimp(13)1.5039dr_tf_wp1.0083
1large tokamak 2major radius1.63beta1.3216dene1.0756fwalld0.51758ffuspow...cpttf1.3815ralpne0.83954oh_steel_frac0.64835fimp(13)1.5039dr_tf_wp1.1083
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" + ], + "text/plain": [ + " tag objf_name norm_objf itvar001_name xcm001 \\\n", + "0 large tokamak 1 major radius 1.60 beta 1.1216 \n", + "1 large tokamak 2 major radius 1.63 beta 1.3216 \n", + "\n", + " itvar002_name xcm002 itvar003_name xcm003 itvar004_name ... \\\n", + "0 dene 1.0756 fwalld 0.50758 ffuspow ... \n", + "1 dene 1.0756 fwalld 0.51758 ffuspow ... \n", + "\n", + " itvar041_name xcm041 itvar042_name xcm042 itvar043_name xcm043 \\\n", + "0 cpttf 1.3815 ralpne 0.83954 oh_steel_frac 0.64835 \n", + "1 cpttf 1.3815 ralpne 0.83954 oh_steel_frac 0.64835 \n", + "\n", + " itvar044_name xcm044 itvar045_name xcm045 \n", + "0 fimp(13) 1.5039 dr_tf_wp 1.0083 \n", + "1 fimp(13) 1.5039 dr_tf_wp 1.1083 \n", + "\n", + "[2 rows x 93 columns]" + ] + }, + "execution_count": 3, + "metadata": {}, + "output_type": "execute_result" + }, + { + "data": { + "image/png": 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" + ] + }, + "metadata": {}, + "output_type": "display_data" + } + ], + "source": [ + "runs_metadata = [\n", + " RunMetadata(data_dir / \"large_tokamak_1_MFILE.DAT\", \"large tokamak 1\"),\n", + " RunMetadata(data_dir / \"large_tokamak_2_MFILE.DAT\", \"large tokamak 2\"),\n", + "]\n", + "\n", + "fig2, df2 = plot_mfile_solutions(\n", + " runs_metadata=runs_metadata,\n", + " plot_title=\"2 large tokamak solutions\",\n", + ")\n", + "df2" + ] + }, + { + "attachments": {}, + "cell_type": "markdown", + "metadata": {}, + "source": [ + "## Plot one solution normalised to another\n", + "\n", + "Normalised differences, relative to the a given solution, can also be plotted:" + ] + }, + { + "cell_type": "code", + "execution_count": 4, + "metadata": {}, + "outputs": [ + { + "data": { + "text/html": [ + "
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tagobjf_namenorm_objfitvar001_namexcm001itvar002_namexcm002itvar003_namexcm003itvar004_name...itvar041_namexcm041itvar042_namexcm042itvar043_namexcm043itvar044_namexcm044itvar045_namexcm045
0large tokamak 1major radius1.60beta1.1216dene1.0756fwalld0.50758ffuspow...cpttf1.3815ralpne0.83954oh_steel_frac0.64835fimp(13)1.5039dr_tf_wp1.0083
1large tokamak 2major radius1.63beta1.3216dene1.0756fwalld0.51758ffuspow...cpttf1.3815ralpne0.83954oh_steel_frac0.64835fimp(13)1.5039dr_tf_wp1.1083
\n", + "

2 rows × 93 columns

\n", + "
" + ], + "text/plain": [ + " tag objf_name norm_objf itvar001_name xcm001 \\\n", + "0 large tokamak 1 major radius 1.60 beta 1.1216 \n", + "1 large tokamak 2 major radius 1.63 beta 1.3216 \n", + "\n", + " itvar002_name xcm002 itvar003_name xcm003 itvar004_name ... \\\n", + "0 dene 1.0756 fwalld 0.50758 ffuspow ... \n", + "1 dene 1.0756 fwalld 0.51758 ffuspow ... \n", + "\n", + " itvar041_name xcm041 itvar042_name xcm042 itvar043_name xcm043 \\\n", + "0 cpttf 1.3815 ralpne 0.83954 oh_steel_frac 0.64835 \n", + "1 cpttf 1.3815 ralpne 0.83954 oh_steel_frac 0.64835 \n", + "\n", + " itvar044_name xcm044 itvar045_name xcm045 \n", + "0 fimp(13) 1.5039 dr_tf_wp 1.0083 \n", + "1 fimp(13) 1.5039 dr_tf_wp 1.1083 \n", + "\n", + "[2 rows x 93 columns]" + ] + }, + "execution_count": 4, + "metadata": {}, + "output_type": "execute_result" + }, + { + "data": { + "image/png": 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PPvsM7777LkaOHKmVvJVn4MCB+PDDDzFq1Ci8/fbb6N69O/r164fXX39d/cvsjz/+gJeXl9Yvt7KviR+9/tWt7HiNGzfWKDc1NYWHh4dWPPXr19caG//CCy/gzJkzTx1DrVq1UL9+fY2yrKwsFBQUoE6dOuXuk5+f/9g6K3Of6mrgwIGYOXMmcnNzUa9ePaSlpSE/Px8DBw7UW9wV+eOPP+Di4qI1hrQqn5vdu3dj3rx5OHXqlMb4/vKefSjvuv3xxx/o1KmTVnl5P8sAIDAwsNw4bGxsKhX3w8cHdP/sXr58GcOGDUP//v2xatWqcuuszOemMj/LAGiMOc/MzMS7776LgwcPQi6Xa2z/6B/6usRNpA9MjumpbNu2DeHh4ejbty+mTp2KOnXqQCKRYMGCBcjOztba/uHegcpSqVQQBAHff/99uePKrKysnrpuoPxfgOXx8fHBrVu3sHXrVowZM0brl8T8+fPx3nvv4a233sLcuXNhb28PExMTREdHl9t7WtEYuYrKxdKHjbKzs9G9e3c0adIEy5Ytg6urK0xNTZGUlITly5drHetJcT9JSkoKhg8fjp49e2L9+vU67WNubo4ffvgBqamp2LNnD/bu3YvPPvsMgYGB2LdvX5XHB1bUZro8xKMvT2qnp/Hwtw9lVCoV6tSpg+3bt5e7T3lj9MtU9j7V1cCBAzFjxgx88cUXiI6Oxueffw5bW1uEhobqJe6a9OOPP+KVV15B165dsXbtWjg7O0MqlWLz5s3YsWOH1vZV/VkGPBh3/PB47TI1NSuIs7MznJ2dkZSUhBMnTqBt27Ya6yv7uXnan2W3bt2Cv78/bGxsMGfOHHh6esLMzAy//PILpk+frvWz7ElxE+kLk2N6Kl9++SU8PDzw1VdfaSQqs2fP1mn/OnXqwMzMDJcuXdJa92iZp6cnRFFEw4YN4e3tXelYK0qkGjRoAJVKhaysLI25L2/cuIFbt25pzX/r6OiIL7/8El26dEH37t3x008/aQwJ+fLLL9GtWzds2rRJY79bt2498QG2yvjuu++gUCjw7bffavTYVPSV7JPifpxjx47h1VdfRdu2bfH5559X6pe3iYkJunfvju7du2PZsmWYP38+3nnnHaSmpqJHjx5o0KABzpw5A5VKpZEQln2V+rj5h1944YVyn8Ivr9dQ1z9+yo538eJFeHh4qMuLi4tx+fJlg01d5+npif3796Nz586VTsx0vU8r+wa8hg0bon379vjss88QFRWFr776Cn379tV4AK0qcT8upgYNGmD//v24ffu2Ru+xLp+b8uzcuRNmZmZITk7WiH/z5s0619GgQQOdf5YBD37+Pc3n6XHXBND9s2tmZobdu3cjMDAQoaGhOHToEHx8fNTrq/rzXVdpaWn4559/8NVXX6Fr167q8suXL5e7/ZPiJtIXDtahp1LWI/BwL9mxY8dw5MgRnffv0aMHdu3ahWvXrqnLL126pDVmsF+/fpBIJIiLi9PqlRNFEf/8889jj1U2T+yjyVRYWBgAICEhQaN82bJlAKD1lDrw4Kv0/fv34+7duwgKCtI4tkQi0Yrviy++0Bhfpw/lXfuCgoLH/jJ/XNwVOX/+PHr27Al3d3fs3r27UgnOo9M1AVCPxyz72josLAx5eXkaY1fv37+PVatWwcrKCv7+/hXW7+npiYKCAo0hDNevXy93hhFLS0udprPq0aMHTE1NsXLlSo1ru2nTJhQUFJT7eagJAwYMQElJCebOnau17v79+489N13v07JZMSrzopyBAwfi6NGj+Oijj/D3339rDKmoatzA4+/bkpISrF69WqN8+fLlEASh0jOFSCQSCIKg8a3DlStXKvVWxZCQEBw5ckRj/tx///1Xq9c8JCQENjY2mD9/vsZQhTJ//fXXY49T0TV5ms+ura0tkpOTUadOHQQFBWn0CFf157uuyjtOcXEx1q5dW+E+j4ubSF/Yc0wV+uijj9RzeD5s0qRJ6NWrF7766iu8+uqr6NmzJy5fvoz169ejWbNmKCws1Kn+2NhY7Nu3D507d8bYsWPVv/CaN2+u8UvG09MT8+bNw4wZM3DlyhX07dsX1tbWuHz5Mr7++mtERERgypQpFR6nTZs2AIB33nkHgwYNglQqRe/evdGqVSuMGDECGzduVH+9d/z4cWzZsgV9+/Ytdy5X4ME4wn379iEgIAAhISE4ePAgbGxs0KtXL8yZMwdvvvkm/Pz8cPbsWWzfvl2jJ0cfgoODYWpqit69e2PMmDEoLCzEBx98gDp16uD69esV7ldR3OW5ffs2QkJCcPPmTUydOlXrgR5PT89yx1iWmTNnDn744Qf07NkTDRo0QH5+PtauXYv69eujS5cuAICIiAhs2LAB4eHhyMjIgLu7O7788kscPnwYCQkJj52XdNCgQZg+fTpeffVVTJw4UT0dlre3t9YDQ23atMH+/fuxbNkyuLi4oGHDhuoHhh5Wu3ZtzJgxA3FxcQgNDcUrr7yCixcvYu3atWjXrp3Gw3eVERAQgEOHDj31cAt/f3+MGTMGCxYswKlTpxAcHAypVIqsrCx88cUXWLFihcbcwg/T9T41NzdHs2bN8Nlnn8Hb2xv29vZo3rw5mjdvXmFcAwYMwJQpUzBlyhTY29tr9U5WJW7gf/ftxIkTERISAolEgkGDBqF3797o1q0b3nnnHVy5cgWtWrXCvn378M033yA6OvqxU/WVp2fPnli2bBlCQ0MxZMgQ5OfnY82aNWjUqJHO48enTZuGbdu2ISgoCBMmTFBP5ebm5oZ///1X3ftqY2ODdevW4Y033sCLL76IQYMGoXbt2sjJycGePXvQuXNnraT/Yb6+vpBIJFi0aBEKCgogk8nU850/zWfX0dFRPR95jx498NNPP6FevXp6+fmuCz8/P7zwwgsYMWIEJk6cCEEQsHXr1ifeKxXFXZGCggL1GOWy6SRXr14NOzs72NnZISoqSm/nREaihmfHoGdA2RRXFf139epVUaVSifPnzxcbNGggymQysXXr1uLu3bu1pkkqm+pnyZIl5R7rwIEDYuvWrUVTU1PR09NT/PDDD8XJkyeLZmZmWtvu3LlT7NKli2hpaSlaWlqKTZo0EcePHy9evHjxiec0d+5csV69eqKJiYnGND5KpVKMi4sTGzZsKEqlUtHV1VWcMWOGxhRCoqg5JVqZY8eOidbW1mLXrl3FoqIi8d69e+LkyZNFZ2dn0dzcXOzcubN45MgRrem1yqZy++KLL8q97o9OoVc2ldbD06J9++23YsuWLUUzMzPR3d1dXLRokfjRRx9pTVGkS9zlKWu3iv4rb2q0hx04cEDs06eP6OLiIpqamoouLi7i4MGDxd9++01juxs3bohvvvmm6OjoKJqamootWrQQN2/erFUfyplmbN++fWLz5s1FU1NTsXHjxuK2bdvKncrtwoULYteuXUVzc3ON2B+dyq3M6tWrxSZNmohSqVSsW7euOHbsWK2p6x6eVuph5U0T1qZNG9HJyanCa/XwvpaWlhWu37hxo9imTRvR3NxctLa2Flu0aCFOmzZNvHbtmkZcD3/WdL1PRVEUf/75Z7FNmzaiqampxvUu75qW6dy5c7nTIVY27vLcv39fnDBhgli7dm1REASNGG7fvi3+3//9n+ji4iJKpVLRy8tLXLJkiahSqR5bpyiW30abNm0Svby8RJlMJjZp0kTcvHlzuecNQBw/fny59Z48eVJ86aWXRJlMJtavX19csGCBuHLlShGAmJeXp7FtamqqGBISItra2opmZmaip6enGB4eLp44ceKJ8X/wwQeih4eHKJFItKZ1e9rP7qVLl0RnZ2exadOm4l9//VXln++V+Rl3+PBhsWPHjqK5ubno4uIiTps2TUxOTtY6N13irsjjfp6VNyUkkSCKVXh6hKga9O3bF5mZmeonu4meVbdv34a9vT0SEhIe+3IWMk7R0dHYsGEDCgsL+ZIKomcIxxyTQd29e1djOSsrC0lJSQgICDBMQER69MMPP6BevXoYPXq0oUOhavboz7J//vkHW7duRZcuXZgYEz1j2HNMBuXs7Izw8HD1XJzr1q2DQqHAyZMnK5zXmIjov8bX1xcBAQFo2rQpbty4gU2bNuHatWs4cOCAxkwMRPTfxwfyyKBCQ0PxySefIC8vDzKZDJ06dcL8+fOZGBPRMyUsLAxffvklNm7cCEEQ8OKLL2LTpk1MjImeQew5JiIiIiIqxTHHRERERESlmBwTEREREZVickxEREREVIrJMRERERFRKSbHRERERESlmBwTEREREZXiPMekplKpcO3aNVhbW0MQBEOHQ0RERKQ3oiji9u3bcHFxgYlJxf3DTI5J7dq1a3B1dTV0GERERETV5urVq6hfv36F65kck5q1tTWABx8aGxubKtenVCqxb98+BAcHQyqVVrk+Mhy2pfFgWxoHtqPxYFvWHLlcDldXV3W+UxEmx6RWNpTCxsZGb8mxhYUFbGxseMM/49iWxoNtaRzYjsaDbVnznjR0lA/kERERERGVYnJcwwICAhAdHW3oMIiIiIioHEyOnzGJiYmws7MzdBhERERERoljjomIiIjIIJIz87A29RJ+u1EI77pWGNetEUJ8nAwaE3uODeD+/fuIioqCra0tHB0d8d5770EURQCAQqHAlClTUK9ePVhaWqJDhw5IS0sDAKSlpeHNN99EQUEBBEGAIAiIjY0FAGzduhVt27aFtbU1nJycMGTIEOTn5xvoDImIiIgeLzkzD2O2ZuD0nwW4qyzB6T8LELktA8mZeQaNiz3HBrBlyxaMHDkSx48fx4kTJxAREQE3NzeMHj0aUVFROHfuHD799FO4uLjg66+/RmhoKM6ePQs/Pz8kJCRg1qxZuHjxIgDAysoKwIOnXefOnYvGjRsjPz8fMTExCA8PR1JSUoVxKBQKKBQK9bJcLlfXpVQqq3yeZXXooy4yLLal8WBbGge2o/F4nttyzcEsrTJRBNakZiHQ20Hvx9P1GgtiWZcl1YiAgADk5+cjMzNTPZXI22+/jW+//RZ79+6Fh4cHcnJy4OLiot6nR48eaN++PebPn4/ExERER0fj1q1bjz3OiRMn0K5dO9y+fVudQD8qNjYWcXFxWuU7duyAhYXF058kERER0RNMPSZBsUp7WjVTExFLOpTo/XhFRUUYMmQICgoKHjtlLXuODaBjx44ac+x16tQJ8fHxOHv2LEpKSuDt7a2xvUKhgIPD4/+CysjIQGxsLE6fPo2bN29CpVIBAHJyctCsWbNy95kxYwZiYmLUy2WTYwcHB+ttnuOUlBQEBQVx7sZnHNvSeLAtjQPb0Xg8z225KecozuTKtcqbuNgiLKyj3o9X9g35kzA5/g8pLCyERCJBRkYGJBKJxrqKen8B4M6dOwgJCUFISAi2b9+O2rVrIycnByEhISguLq5wP5lMBplMplUulUr1eoPquz4yHLal8WBbGge2o/F4HttyfKAXIrdl4OExDIIARHXzqpZroWudTI4N4NixYxrLR48ehZeXF1q3bo2SkhLk5+fjpZdeKndfU1NTlJRoftVw4cIF/PPPP1i4cCFcXV0BPBhWQURERPRfFeLjhPXD2mBtWjaybtyGV11rjA/wRLCBZ6tgcmwAOTk5iImJwZgxY/DLL79g1apViI+Ph7e3N4YOHYrhw4cjPj4erVu3xl9//YUDBw6gZcuW6NmzJ9zd3VFYWIgDBw6gVatWsLCwgJubG0xNTbFq1SpERkbi119/xdy5cw19mkRERESPFeLjZPCp2x7FqdwMYPjw4bh79y7at2+P8ePHY9KkSYiIiAAAbN68GcOHD8fkyZPRuHFj9O3bF+np6XBzcwMA+Pn5ITIyEgMHDkTt2rWxePFi1K5dG4mJifjiiy/QrFkzLFy4EEuXLjXkKRIRERE9k9hzXMPK5iwGgHXr1mmtl0qliIuLK3cWiYf3e3TfwYMHY/DgwRplnIiEiIiIqHLYc0xEREREVIrJMRERERFRKSbHRERERESlmBwTEREREZVickxEREREVIrJMRERERFRKSbHBhIQEIDo6GhDh0FERERED2FyTERERERUiskxET1WcmYeXlt/FFOPSfDa+qNIzswzdEhERETVhslxDbhz5w6GDx8OKysrODs7Iz4+XmO9QqHAlClTUK9ePVhaWqJDhw4ab9JLTEyEnZ0dkpOT0bRpU1hZWSE0NBTXr1/XqOfDDz9E06ZNYWZmhiZNmmDt2rU1cXpkxJIz8zBmawbO5MpRrBJwJleOyG0ZTJCJiMho8fXRNWDq1Kk4dOgQvvnmG9SpUwczZ87EL7/8Al9fXwBAVFQUzp07h08//RQuLi74+uuvERoairNnz8LLywsAUFRUhKVLl2Lr1q0wMTHBsGHDMGXKFGzfvh0AsH37dsyaNQurV69G69atcfLkSYwePRqWlpYYMWJEuXEpFAooFAr1slwuBwAolUoolcoqn3dZHfqoiwxjzcEsrTJRBNakZiHQ28EAEVFV8b40DmxH48G2rDm6XmNBFEWxmmN5rhUWFsLBwQHbtm1D//79AQD//vsv6tevj4iICMTExMDDwwM5OTlwcXFR79ejRw+0b98e8+fPR2JiIt58801cunQJnp6eAIC1a9dizpw5yMt70IPXqFEjzJ07F4MHD1bXMW/ePCQlJeHnn38uN7bY2FjExcVple/YsQMWFhZ6uwb07Jp6TIJilaBVbmoiYkmHEgNERERE9HSKioowZMgQFBQUwMbGpsLt2HNczbKzs1FcXIwOHTqoy+zt7dG4cWMAwNmzZ1FSUgJvb2+N/RQKBRwc/tczZ2FhoU6MAcDZ2Rn5+fkAHgzbyM7OxsiRIzF69Gj1Nvfv34etrW2Fsc2YMQMxMTHqZblcDldXVwQHBz/2Q6MrpVKJlJQUBAUFQSqVVrk+qnmbco7iTK5cq7yJiy3CwjoaICKqKt6XxoHtaDzYljWn7BvyJ2FybGCFhYWQSCTIyMiARCLRWGdlZaX+96M3jCAIKOv0LywsBAB88MEHGkk4AK06HyaTySCTybTKpVKpXm9QfddHNWd8oBcit2Xg4e+XBAGI6ubFNn3G8b40DmxH48G2rH66Xl8mx9XM09MTUqkUx44dg5ubGwDg5s2b+O233+Dv74/WrVujpKQE+fn5eOmll57qGHXr1oWLiwt+//13DB06VJ/h03MuxMcJ64e1wZrULFy4VoAmLraI6uaFYB8nQ4dGRERULZgcVzMrKyuMHDkSU6dOhYODA+rUqYN33nkHJiYPJgrx9vbG0KFDMXz4cMTHx6N169b466+/cODAAbRs2RI9e/bU6ThxcXGYOHEibG1tERoaCoVCgRMnTuDmzZsaQyeIKivExwmB3g5ISkpCWFhH9mwQEZFRY3JcA5YsWYLCwkL07t0b1tbWmDx5MgoKCtTrN2/ejHnz5mHy5MnIzc2Fo6MjOnbsiF69eul8jFGjRsHCwgJLlizB1KlTYWlpiRYtWvAtfERERESVwNkqSE0ul8PW1vaJT3HqSqlUlvY2hrG38RnHtjQebEvjwHY0HmzLmqNrnsOXgBARERERlWJyTERERERUiskxEREREVEpJsdERERERKWYHBMRERERlWJyTERERERUismxnoiiiIiICNjb20MQBJw6dUqv9QuCgF27dgEArly58sRjpKWlQRAE3Lp1S69xEBERERkzvgRET/bu3YvExESkpaXBw8MDjo6Ohg6JiIiIiCqJybGeZGdnw9nZGX5+foYOhei5l5yZh7Wpl/DbjUJ417XCuG6NEOLjZOiwiIjoGcBhFXoQHh6OCRMmICcnB4IgwNHRUePVzwkJCRAEAXv37lWXNWrUCB9++CEAID09HUFBQXB0dIStrS38/f3xyy+/VCqGpKQkeHt7w9zcHN26dcOVK1f0cm5Ez5rkzDyM2ZqB038W4K6yBKf/LEDktgwkZ+YZOjQiInoGsOdYD1asWAFPT09s3LgR6enpSElJwYQJE1BSUgKJRIJDhw7B0dERaWlpCA0NRW5uLrKzsxEQEAAAuH37NkaMGIFVq1ZBFEXEx8cjLCwMWVlZsLa2fuLxr169in79+mH8+PGIiIjAiRMnMHny5Cfup1AooFAo1MtyuRzAg1dZKpXKp7sYDymrQx91kWE9S2255mCWVpkoAmtSsxDo7WCAiP5bnqW2pIqxHY0H27Lm6HqNmRzrga2tLaytrSGRSODk5ITevXsjPDwcJ0+eRJs2bfDDDz9g6tSp6gfq0tLSUK9ePTRq1AgAEBgYqFHfxo0bYWdnh0OHDmn0QFdk3bp18PT0RHx8PACgcePGOHv2LBYtWvTY/RYsWIC4uDit8n379sHCwkKXU9dJSkqK3uoiw3oW2vLCdQkAQbv8WgGSkpJqPqD/qGehLenJ2I7Gg21Z/YqKinTajslxNbCzs0OrVq2QlpYGU1NTmJqaIiIiArNnz0ZhYSEOHToEf39/9fY3btzAu+++i7S0NOTn56OkpARFRUXIycnR6Xjnz59Hhw4dNMo6der0xP1mzJiBmJgY9bJcLoerqyuCg4NhY2Oj49lWTKlUIiUlBUFBQZBKpVWujwznWWrLTTlHcSZXrlXexMUWYWEdDRDRf8uz1JZUMbaj8WBb1pyyb8ifhMlxNQkICEBaWhpkMhn8/f1hb2+Ppk2b4qeffsKhQ4c0hj2MGDEC//zzD1asWIEGDRpAJpOhU6dOKC4urtYYZTIZZDKZVrlUKtXrDarv+shwnoW2HB/ohchtGRDF/5UJAhDVzes/H3tNehbakp6M7Wg82JbVT9frywfyqom/vz9++uknHDhwQD22OCAgAJ988gl+++03dRkAHD58GBMnTkRYWBh8fHwgk8nw999/63yspk2b4vjx4xplR48e1cdpED1zQnycsH5YG7RytYOFqQStXO2wYVgbBHO2CiIi0gF7jqtJ165dcfv2bezevRsLFy4E8CA5fv311+Hs7Axvb2/1tl5eXti6dSvatm0LuVyOqVOnwtzcXOdjRUZGIj4+HlOnTsWoUaOQkZGBxMREfZ8S0TMjxMeJU7cREdFTYc9xNXnhhRfQokUL1K5dG02aNAHwIGFWqVQa440BYNOmTbh58yZefPFFvPHGG5g4cSLq1Kmj87Hc3Nywc+dO7Nq1C61atcL69esxf/58vZ4PERER0fOAPcd6Eh0djejoaI2yR1/vbG9vD5VKpbVv69atkZ6erlH2+uuvayyLDw2gdHd311gGgF69emnNbPHmm2/qGj4RERERgT3HRERERERqTI6JiIiIiEoxOSYiIiIiKsXkmIiIiIioFJNjIiIiIqJSTI6JiIiIiEoxOS6HKIqIiIiAvb09BEHAyZMnNZYfnaKNiIiIiIwD5zkux969e5GYmIi0tDR4eHggPT1dY9nR0dHQIRIRERFRNWByXI7s7Gw4OzvDz88PAPDHH39oLBM9T5Iz87DmYBYuXJdgU85RjA/04quZiYjIaHFYxSPCw8MxYcIE5OTkQBAEuLu7ay0DD95Sl5CQoLGvr68vYmNjATwYmhEbGws3NzfIZDK4uLhg4sSJ6m3d3d0xd+5cDB48GJaWlqhXrx7WrFmjUV9OTg769OkDKysr2NjYYMCAAbhx4wYAoKCgABKJBCdOnAAAqFQq2Nvbo2PHjur9t23bBldXVz1fIXqeJGfmYczWDJzJlaNYJeBMrhyR2zKQnJln6NCIiIiqBXuOH7FixQp4enpi48aNSE9Ph0KhwMcff6xelkgkOtWzc+dOLF++HJ9++il8fHyQl5eH06dPa2yzZMkSzJw5E3FxcUhOTsakSZPg7e2NoKAgqFQqdWJ86NAh3L9/H+PHj8fAgQORlpYGW1tb+Pr6Ii0tDW3btsXZs2fV46MLCwvV+/n7+1cYo0KhgEKhUC/L5XIAgFKphFKpfIqrp6msDn3URYax5mCWVpkoAmtSsxDo7WCAiKiqeF8aB7aj8WBb1hxdrzGT40fY2trC2toaEokETk4Pvjp+dFkXOTk5cHJyQo8ePSCVSuHm5ob27dtrbNO5c2e8/fbbAABvb28cPnwYy5cvR1BQEA4cOICzZ8/i8uXL6t7fjz/+GD4+PkhPT0e7du0QEBCAtLQ0TJkyBWlpaQgKCsKFCxfw008/ITQ0FGlpaZg2bVqFMS5YsABxcXFa5fv27YOFhYXO5/okKSkpequLataF6xIAgnb5tQIkJSXVfECkN7wvjQPb0XiwLatfUVGRTtsxOa4m/fv3R0JCAjw8PBAaGoqwsDD07t0btWr975J36tRJY59OnTqph2qcP38erq6uGsMimjVrBjs7O5w/fx7t2rWDv78/Nm3ahJKSEhw6dAjBwcFwcnJCWloaWrZsiUuXLiEgIKDCGGfMmIGYmBj1slwuh6urK4KDg2FjY1Pla6BUKpGSkoKgoCBIpdIq10c1b1POUZzJlWuVN3GxRVhYx3L2oP863pfGge1oPNiWNafsG/InYXL8lExMTCCKokbZw931rq6uuHjxIvbv34+UlBSMGzcOS5YswaFDh/T24e/atStu376NX375BT/88APmz58PJycnLFy4EK1atYKLiwu8vLwq3F8mk0Emk2mVS6VSvd6g+q6Pas74QC9EbsvAwx91QQCiunmxTZ9xvC+NA9vReLAtq5+u15cP5D2l2rVr4/r16+pluVyOy5cva2xjbm6O3r17Y+XKlUhLS8ORI0dw9uxZ9fqjR49qbH/06FE0bdoUANC0aVNcvXoVV69eVa8/d+4cbt26hWbNmgEA7Ozs0LJlS6xevRpSqRRNmjRB165dcfLkSezevfux442JdBHi44T1w9qgZX0bmJqIaFnfBhuGtUEwZ6sgIiIjxZ7jpxQYGIjExET07t0bdnZ2mDVrlsbDeomJiSgpKUGHDh1gYWGBbdu2wdzcHA0aNFBvc/jwYSxevBh9+/ZFSkoKvvjiC+zZswcA0KNHD7Ro0QJDhw5FQkIC7t+/j3HjxsHf3x9t27ZV1xEQEIBVq1bh9ddfBwDY29ujadOm+Oyzz7RmvyB6GiE+Tgj0dkBSUhLCwjqyZ4OIiIwae46f0owZM+Dv749evXqhZ8+e6Nu3Lzw9PdXr7ezs8MEHH6Bz585o2bIl9u/fj++++w4ODv97wn/y5Mk4ceIEWrdujXnz5mHZsmUICQkBAAiCgG+++QYvvPACunbtih49esDDwwOfffaZRhz+/v4oKSnRGFscEBCgVUZERERETyaIjw6cpRrh7u6O6OhoREdHGzoUNblcDltbWxQUFOjtgbwHvY1h7G18xrEtjQfb0jiwHY0H27Lm6JrnsOeYiIiIiKgUk2MiIiIiolJ8IM9Arly5YugQiIiIiOgR7DkmIiIiIirF5JiIiIiIqBSTYyIiIiKiUkyO9UQURURERMDe3h6CIODUqVNa28TGxsLX17fGYyMiIiIi3TA51pO9e/ciMTERu3fvxvXr19G6dWvs2rXL0GERERERUSVwtgo9yc7OhrOzM/z8/Gr82MXFxTA1Na3x49LzITkzD2sOZuHCdQk25RzF+EAvhPg4GTosIiKiasGeYz0IDw/HhAkTkJOTA0EQ4O7uDgB49dVXNZbLbNiwAa6urrCwsMCAAQNQUFCgXhcQEKD11ry+ffsiPDxcvezu7o65c+di+PDhsLGxQUREBBITE2FnZ4fk5GQ0bdoUVlZWCA0NxfXr16vprOl5kJyZhzFbM3AmV45ilYAzuXJEbstAcmaeoUMjIiKqFuw51oMVK1bA09MTGzduRHp6OiQSCerUqYPNmzcjNDQUEolEve2lS5fw+eef47vvvoNcLsfIkSMxbtw4bN++vVLHXLp0KWbNmoXZs2cDAH788UcUFRVh6dKl2Lp1K0xMTDBs2DBMmTKlwroVCgUUCoV6WS6XA3jwKkulUlnZy6ClrA591EWGseZgllaZKAJrUrMQ6O1ggIioqnhfGge2o/FgW9YcXa8xk2M9sLW1hbW1NSQSCZyc/vd1s52dncYyANy7dw8ff/wx6tWrBwBYtWoVevbsifj4eK1tHycwMBCTJ09WL//4449QKpVYv349PD09AQBRUVGYM2dOhXUsWLAAcXFxWuX79u2DhYWFzrE8SUpKit7qopp14boEgKBdfq0ASUlJNR8Q6Q3vS+PAdjQebMvqV1RUpNN2TI5rmJubmzoxBoBOnTpBpVLh4sWLlUqO27Ztq1VmYWGhTowBwNnZGfn5+RXWMWPGDMTExKiX5XI5XF1dERwcDBsbG51jqYhSqURKSgqCgoIglUqrXB/VvE05R3EmV65V3sTFFmFhHQ0QEVUV70vjwHY0HmzLmlP2DfmTMDn+jzExMYEoihpl5X0NYGlpqVX26E0lCIJWXQ+TyWSQyWTl1qPPG1Tf9VHNGR/ohchtGXj4YyQIQFQ3L7bpM473pXFgOxoPtmX10/X68oG8aiKVSlFSUqJVnpOTg2vXrqmXjx49ChMTEzRu3BgAULt2bY2H6EpKSvDrr79Wf8BE5QjxccL6YW3Qsr4NTE1EtKxvgw3D2iCYs1UQEZGRYnJcTdzd3XHgwAHk5eXh5s2b6nIzMzOMGDECp0+fxo8//oiJEydiwIAB6iEVgYGB2LNnD/bs2YMLFy5g7NixuHXrloHOguhBgrxzTEcs6VCCnWM6MjEmIiKjxuS4msTHxyMlJQWurq5o3bq1urxRo0bo168fwsLCEBwcjJYtW2Lt2rXq9W+99RZGjBiB4cOHw9/fHx4eHujWrZshToGIiIjouSOIjxuUSs8VuVwOW1tbFBQU6O2BvKSkJISFhXEc1TOObWk82JbGge1oPNiWNUfXPIc9x0REREREpZgcExERERGVYnJMRERERFSKyTERERERUSkmx0REREREpZgcExERERGVem6TY1EUERERAXt7ewiCADs7O0RHR6vXu7u7IyEhodL1hoeHo2/fvnqLU1cBAQEa8RMRERFR5T23yfHevXuRmJiI3bt34/r162jevHml9r9y5QoEQcCpU6eqJ0AiIiIiqnG1DB2AoWRnZ8PZ2Rl+fn4AgFq1DHcpiouLYWpqarDjEz1OcmYe1hzMwoXrEmzKOYrxgV4I4SukiYjISD2XPcfh4eGYMGECcnJyIAgC3N3dy92uqKgIb731FqytreHm5oaNGzeq1zVs2BAA0Lp1awiCgICAAI19ly5dCmdnZzg4OGD8+PFQKpXqde7u7pg7dy6GDx8OGxsbREREAAB++uknvPTSSzA3N4erqysmTpyIO3fuqPdbu3YtvLy8YGZmhrp16+L111/XOKZKpcK0adNgb28PJycnxMbGVuEqET1IjMdszcCZXDmKVQLO5MoRuS0DyZl5hg6NiIioWjyXPccrVqyAp6cnNm7ciPT0dEgkEvTv319ru/j4eMydOxczZ87El19+ibFjx8Lf3x+NGzfG8ePH0b59e+zfvx8+Pj4aPb+pqalwdnZGamoqLl26hIEDB8LX1xejR49Wb7N06VLMmjULs2fPBvCgJzs0NBTz5s3DRx99hL/++gtRUVGIiorC5s2bceLECUycOBFbt26Fn58f/v33X/z4448a8W7ZsgUxMTE4duwYjhw5gvDwcHTu3BlBQUHlXgeFQgGFQqFelsvlAB68yvLhZP5pldWhj7rIMNYczNIqE0VgTWoWAr0dDBARVRXvS+PAdjQebMuao+s1FkRRFKs5lv+khIQEJCQk4MqVKwAePNDm6+urfgjP3d0dL730ErZu3QrgwQN8Tk5OiIuLQ2RkJK5cuYKGDRvi5MmT8PX1VdcbHh6OtLQ0ZGdnQyKRAAAGDBgAExMTfPrpp+q6W7duja+//lq936hRoyCRSLBhwwZ12U8//QR/f3/cuXMHSUlJePPNN/Hnn3/C2tpa63wCAgJQUlKikTC3b98egYGBWLhwYbnXIDY2FnFxcVrlO3bsgIWFhQ5XkYzd1GMSFKsErXJTExFLOpQYICIiIqKnU1RUhCFDhqCgoAA2NjYVbvdc9hzrqmXLlup/C4IAJycn5OfnP3E/Hx8fdWIMAM7Ozjh79qzGNm3bttVYPn36NM6cOYPt27ery0RRhEqlwuXLlxEUFIQGDRrAw8MDoaGhCA0NxauvvqqRxD4cb9lxHxfvjBkzEBMTo16Wy+VwdXVFcHDwYz80ulIqlUhJSUFQUBCkUmmV66OatynnKM7kyrXKm7jYIiysowEioqrifWkc2I7Gg21Zc8q+IX8SJseP8eiHVBAEqFQqvexnaWmpsVxYWIgxY8Zg4sSJWvW5ubnB1NQUv/zyC9LS0rBv3z7MmjULsbGxSE9Ph52d3VPFK5PJIJPJyo1fnzeovuujmjM+0AuR2zLw8PdLggBEdfNimz7jeF8aB7aj8WBbVj9dry+T46dUNsa4pEQ/Xy2/+OKLOHfuHBo1alThNrVq1UKPHj3Qo0cPzJ49G3Z2djh48CD69eunlxiIHhXi44T1w9pgTWoWLlwrQBMXW0R180IwZ6sgIiIjxeT4KdWpUwfm5ubYu3cv6tevDzMzM9ja2j51fdOnT0fHjh0RFRWFUaNGwdLSEufOnUNKSgpWr16N3bt34/fff0fXrl3xwgsvICkpCSqVCo0bN9bjWRFpC/FxQqC3A5KSkhAW1pE9G0REZNSey6nc9KFWrVpYuXIlNmzYABcXF/Tp06dK9bVs2RKHDh3Cb7/9hpdeegmtW7fGrFmz4OLiAgCws7PDV199hcDAQDRt2hTr16/HJ598Ah8fH32cDhERERHhOZ6tgrTJ5XLY2to+8SlOXSmVytLexjD2Nj7j2JbGg21pHNiOxoNtWXN0zXPYc0xEREREVIrJMRERERFRKSbHRERERESlmBwTEREREZVickxEREREVIrJMRERERFRKSbHRERERESlmBwbgCiKiIiIgL29PQRBwKlTp564j7u7OxISEnQ+xpUrV3Sum4iIiIge4OujDWDv3r1ITExEWloaPDw84Ojo+MR90tPTYWlpqfMxXF1dcf36dZ3qJnqc5Mw8rDmYhQvXJdiUcxTjA70Q4uNk6LCIiIiqBXuODSA7OxvOzs7w8/ODk5MTatV68t8otWvXhoWFhc7HkEgkOtdNVJHkzDyM2ZqBM7lyFKsEnMmVI3JbBpIz8wwdGhERUbVg5lTDwsPDsWXLFgCAIAho0KAB3N3d0bx5cwDA1q1bIZVKMXbsWMyZMweCIAB4MKwiOjoa0dHR6n0/+OAD7NmzB8nJyahXrx7i4+PxyiuvAHgwrKJhw4Y4efIkfH19y41FoVBAoVCol+VyOYAHr7JUKpVVPteyOvRRFxnGmoNZWmWiCKxJzUKgt4MBIqKq4n1pHNiOxoNtWXN0vcZMjmvYihUr4OnpiY0bNyI9PR0SiQT9+/fHli1bMHLkSBw/fhwnTpxAREQE3NzcMHr06ArriouLw+LFi7FkyRKsWrUKQ4cOxR9//AF7e3udYlmwYAHi4uK0yvft21epXuonSUlJ0VtdVLMuXJcAELTLrxUgKSmp5gMiveF9aRzYjsaDbVn9ioqKdNqOyXENs7W1hbW1tXrYQxlXV1csX74cgiCgcePGOHv2LJYvX/7Y5Dg8PByDBw8GAMyfPx8rV67E8ePHERoaqlMsM2bMQExMjHpZLpfD1dUVwcHBsLGxecoz/B+lUomUlBQEBQVBKpVWuT6qeZtyjuJMrlyrvImLLcLCOhogIqoq3pfGge1oPNiWNafsG/InYXL8H9GxY0f1EAoA6NSpE+Lj41FSUgKJRFLuPi1btlT/29LSEjY2NsjPz9f5mDKZDDKZTKtcKpXq9QbVd31Uc8YHeiFyWwZE8X9lggBEdfNimz7jeF8aB7aj8WBbVj9dry8fyHuGPdrIgiBApVIZKBoyRiE+Tlg/rA1a1reBqYmIlvVtsGFYGwRztgoiIjJS7Dn+jzh27JjG8tGjR+Hl5VVhrzFRTQnxcUKgtwOSkpIQFtaRPRtERGTU2HP8H5GTk4OYmBhcvHgRn3zyCVatWoVJkyYZOiwiIiKi5wp7jv8jhg8fjrt376J9+/aQSCSYNGkSIiIiDB0WERER0XOFybEBPDxfcRmpVIqEhASsW7eu3H2uXLmisSw+/IRUqVu3bqn/XTZ/sZWVVZViJSIiInqecFiFEfr333/x5ZdfwsbGBq6uroYOh4iIiOiZwZ5jIzRy5EhkZGRg3bp15U7VRkRERETlY3L8H5CWlqbX+r7++mu91kdERET0vOCwCiIiIiKiUkyOiYiIiIhKMTkmIiIiIirF5LgSRFFEREQE7O3tIQgCTp06ZeiQHis8PBx9+/Y1dBhEREREzww+kFcJe/fuRWJiItLS0uDh4QFHR8caOW54eDhu3bqFXbt21cjxiIiIiJ5XTI4rITs7G87OzvDz8zN0KEQ1JjkzD2sOZuHCdQk25RzF+EAvhPg4GTosIiKiasFhFToKDw/HhAkTkJOTA0EQ4O7ujoCAAERFRSEqKgq2trZwdHTEe++9p/H2Ond3d8yfPx9vvfUWrK2t4ebmho0bN2rUffXqVQwYMAB2dnawt7dHnz591G/Ei42NxZYtW/DNN99AEAQIgqCe+u1x+xHpQ3JmHsZszcCZXDmKVQLO5MoRuS0DyZl5hg6NiIioWrDnWEcrVqyAp6cnNm7ciPT0dEgkEvTv3x9btmzByJEjcfz4cZw4cQIRERFwc3PD6NGj1fvGx8dj7ty5mDlzJr788kuMHTsW/v7+aNy4MZRKJUJCQtCpUyf8+OOPqFWrFubNm4fQ0FCcOXMGU6ZMwfnz5yGXy7F582YAgL29/RP3MzU1feI5KRQK9WumAUAulwMAlEollEplla9ZWR36qIsMY83BLK0yUQTWpGYh0NvBABFRVfG+NA5sR+PBtqw5ul5jJsc6srW1hbW1NSQSCZyc/veVsqurK5YvXw5BENC4cWOcPXsWy5cv10iOw8LCMG7cOADA9OnTsXz5cqSmpqJx48b47LPPoFKp8OGHH0IQBADA5s2bYWdnh7S0NAQHB8Pc3BwKhULjuNu2bXvifk+yYMECxMXFaZXv27cPFhYWT3ehypGSkqK3uqhmXbguASBol18rQFJSUs0HRHrD+9I4sB2NB9uy+hUVFem0HZPjKurYsaM6OQWATp06IT4+HiUlJZBIJACAli1bqtcLggAnJyfk5+cDAE6fPo1Lly7B2tpao9579+4hOzu7wuM+7X4PmzFjBmJiYtTLcrkcrq6uCA4Oho2NjU51PI5SqURKSgqCgoIglUqrXB/VvE05R3EmV65V3sTFFmFhHQ0QEVUV70vjwHY0HmzLmlP2DfmTMDmuAY9+2AVBgEqlAgAUFhaiTZs22L59u9Z+tWvXrrDOp93vYTKZDDKZrNx49XmD6rs+qjnjA70QuS0DDw2jhyAAUd282KbPON6XxoHtaDzYltVP1+vL5LiKjh07prF89OhReHl5qXuNn+TFF1/EZ599hjp16lTYW2tqaoqSkpJK70dUVSE+Tlg/rA3WpGbhwrUCNHGxRVQ3LwRztgoiIjJSnK2iinJychATE4OLFy/ik08+wapVqzBp0iSd9x86dCgcHR3Rp08f/Pjjj7h8+TLS0tIwceJE/PnnnwAezHhx5swZXLx4EX///TeUSqVO+xHpQ4iPE3aO6YglHUqwc0xHJsZERGTUmBxX0fDhw3H37l20b98e48ePx6RJkxAREaHz/hYWFvjhhx/g5uaGfv36oWnTphg5ciTu3bun7hEePXo0GjdujLZt26J27do4fPiwTvsRERERUeVwWEUlREdHIzo6WqNMKpUiISEB69atK3ef8uYdfvS1005OTtiyZUuFx61duzb27dunVf6k/RITEytcR0RERETa2HNMRERERFSKyTERERERUSkOq6iCstc4ExEREZFxYM8xEREREVEpJsdERERERKWYHBMRERERlWJy/AhRFBEREQF7e3sIggA7Ozut6duIiIiIyDgxOX7E3r17kZiYiN27d+P69eto3rx5letMTEyEnZ1dpfdLS0uDIAi4detWlWMgIiIioifjbBWPyM7OhrOzM/z8/AAAtWr99y9RcXExTE1NDR0GGankzDysOZiFC9cl2JRzFOMDvRDCV0gTEZGRYs/xQ8LDwzFhwgTk5ORAEAS4u7sDAO7fv4+oqCjY2trC0dER7733HkRRVO+nUCgwZcoU1KtXD5aWlujQoYN6mre0tDS8+eabKCgogCAIEAQBsbGxAICtW7eibdu2sLa2hpOTE4YMGYL8/HwAD96s161bNwDACy+8AEEQEB4eDgAICAhAVFQUoqOj4ejoiJCQELz11lvo1auXxvkolUrUqVMHmzZtqr6LRkYtOTMPY7Zm4EyuHMUqAWdy5YjcloHkzDxDh0ZERFQt/vvdojVoxYoV8PT0xMaNG5Geng6JRIL+/ftjy5YtGDlyJI4fP44TJ04gIiICbm5uGD16NAAgKioK586dw6effgoXFxd8/fXXCA0NxdmzZ+Hn54eEhATMmjULFy9eBABYWVkBeJC8zp07F40bN0Z+fj5iYmIQHh6OpKQkuLq6YufOnXjttddw8eJF2NjYwNzcXB3rli1bMHbsWBw+fBgA8M8//6Br1664fv06nJ2dAQC7d+9GUVERBg4cWO75KhQKKBQK9bJcLlfHpVQqq3w9y+rQR11kGGsOZmmViSKwJjULgd4OBoiIqor3pXFgOxoPtmXN0fUaC+LDXaCEhIQEJCQk4MqVKwAe9NLm5+cjMzMTgiAAAN5++218++23OHfuHHJycuDh4YGcnBy4uLio6+nRowfat2+P+fPnIzExEdHR0U8cO3zixAm0a9cOt2/fhpWVFdLS0tCtWzfcvHlTY8xyQEAA5HI5fvnlF439fXx8MGLECEybNg0A8Morr8DBwQGbN28u93ixsbGIi4vTKt+xYwcsLCyedKnoOTD1mATFKkGr3NRExJIOJQaIiIiI6OkUFRVhyJAhKCgogI2NTYXbsedYBx07dlQnxgDQqVMnxMfHo6SkBGfPnkVJSQm8vb019lEoFHBweHzPWkZGBmJjY3H69GncvHkTKpUKAJCTk4NmzZo9dt82bdpolY0aNQobN27EtGnTcOPGDXz//fc4ePBghXXMmDEDMTEx6mW5XA5XV1cEBwc/9kOjK6VSiZSUFAQFBUEqlVa5Pqp5m3KO4kyuXKu8iYstwsI6GiAiqirel8aB7Wg82JY1p+wb8idhclxFhYWFkEgkyMjIgEQi0VhXNnyiPHfu3EFISAhCQkKwfft21K5dGzk5OQgJCUFxcfETj2tpaalVNnz4cLz99ts4cuQIfv75ZzRs2BAvvfRShXXIZDLIZDKtcqlUqtcbVN/1Uc0ZH+iFyG0ZePj7JUEAorp5sU2fcbwvjQPb0XiwLaufrteXybEOjh07prF89OhReHl5QSKRoHXr1igpKUF+fn6FiaipqSlKSjS/gr5w4QL++ecfLFy4EK6urgAeDKt4dD8AWvtWxMHBAX379sXmzZtx5MgRvPnmmzrtR1SREB8nrB/WBmtSs3DhWgGauNgiqpsXgjlbBRERGSnOVqGDnJwcxMTE4OLFi/jkk0+watUqTJo0CQDg7e2NoUOHYvjw4fjqq69w+fJlHD9+HAsWLMCePXsAAO7u7igsLMSBAwfw999/o6ioCG5ubjA1NcWqVavw+++/49tvv8XcuXM1jtugQQMIgoDdu3fjr7/+QmFh4RNjHTVqFLZs2YLz589jxIgR+r8Y9NwJ8XHCzjEdsaRDCXaO6cjEmIiIjBqTYx0MHz4cd+/eRfv27TF+/HhMmjQJERER6vWbN2/G8OHDMXnyZDRu3Bh9+/ZFeno63NzcAAB+fn6IjIzEwIEDUbt2bSxevBi1a9dGYmIivvjiCzRr1gwLFy7E0qVLNY5br149xMXF4e2330bdunURFRX1xFh79OgBZ2dnhISEaDwgSERERERPxtkqjExhYSHq1auHzZs3o1+/fpXaVy6Xw9bW9olPcepKqVQiKSkJYWFhHEf1jGNbGg+2pXFgOxoPtmXN0TXP4ZhjI6FSqfD3338jPj4ednZ2eOWVVwwdEhEREdEzh8mxkcjJyUHDhg1Rv359JCYmPhOvvSYiIiL6r2EGZSTc3d3BETJEREREVcMH8oiIiIiISjE5JiIiIiIqxeSYiIiIiKgUk+NKEkURERERsLe3hyAIOHXqVI0cNyAgANHR0RWuDw8PR9++fWskFiIiIiJjxQfyKmnv3r1ITExEWloaPDw84OjoaOiQiIiIiEhPmBxXUnZ2NpydneHn52foUIhqRHJmHtYczMKF6xJsyjmK8YFeCOErpImIyEhxWEUlhIeHY8KECcjJyYEgCHB3d0dAQACioqIQFRUFW1tbODo64r333tOYVk2hUGDKlCmoV68eLC0t0aFDB6SlpanX//PPPxg8eDDq1asHCwsLtGjRAp988sljY9mzZw9sbW2xfft2jfK4uDjUrl0bNjY2iIyMRHFxsV6vAT1fkjPzMGZrBs7kylGsEnAmV47IbRlIzswzdGhERETVgj3HlbBixQp4enpi48aNSE9Ph0QiQf/+/bFlyxaMHDkSx48fx4kTJxAREQE3NzeMHj0aABAVFYVz587h008/hYuLC77++muEhobi7Nmz8PLywr1799CmTRtMnz4dNjY22LNnD9544w14enqiffv2WnHs2LEDkZGR2LFjB3r16qUuP3DgAMzMzJCWloYrV67gzTffhIODA95///1yz0ehUEChUKiX5XI5gAevslQqlVW+XmV16KMuMow1B7O0ykQRWJOahUBvBwNERFXF+9I4sB2NB9uy5uh6jQWRb46olISEBCQkJODKlSsAHjwol5+fj8zMTAiCAAB4++238e233+LcuXPIycmBh4cHcnJy4OLioq6nR48eaN++PebPn1/ucXr16oUmTZpg6dKl6uP4+vrCy8sL77zzDr755hv4+/urtw8PD8d3332Hq1evwsLCAgCwfv16TJ06FQUFBTAx0f6SIDY2FnFxcVrlO3bsUNdBz7epxyQoVgla5aYmIpZ0KDFARERERE+nqKgIQ4YMQUFBAWxsbCrcjj3HetCxY0d1YgwAnTp1Qnx8PEpKSnD27FmUlJTA29tbYx+FQgEHhwc9byUlJZg/fz4+//xz5Obmori4GAqFQitB/fLLL5Gfn4/Dhw+jXbt2WnG0atVKY59OnTqhsLAQV69eRYMGDbS2nzFjBmJiYtTLcrkcrq6uCA4OfuyHRldKpRIpKSkICgqCVCqtcn1U8zblHMWZXLlWeRMXW4SFdTRARFRVvC+NA9vReLAta07ZN+RPwuS4mhUWFkIikSAjIwMSiURjnZWVFQBgyZIlWLFiBRISEtCiRQtYWloiOjpaa7xw69at8csvv+Cjjz5C27ZtNRLypyGTySCTybTKpVKpXm9QfddHNWd8oBcit2Xg4e+XBAGI6ubFNn3G8b40DmxH48G2rH66Xl8mx3pw7NgxjeWjR4/Cy8sLEokErVu3RklJCfLz8/HSSy+Vu//hw4fRp08fDBs2DACgUqnw22+/oVmzZhrbeXp6Ij4+HgEBAZBIJFi9erXG+tOnT+Pu3bswNzdXx2FlZQVXV1d9nSo9Z0J8nLB+WBusSc3ChWsFaOJii6huXgjmbBVERGSkOFuFHuTk5CAmJgYXL17EJ598glWrVmHSpEkAAG9vbwwdOhTDhw/HV199hcuXL+P48eNYsGAB9uzZAwDw8vJCSkoKfv75Z5w/fx5jxozBjRs3yj2Wt7c3UlNTsXPnTq2XghQXF2PkyJE4d+4ckpKSMHv2bERFRZU73phIVyE+Ttg5piOWdCjBzjEdmRgTEZFRY8+xHgwfPhx3795F+/btIZFIMGnSJERERKjXb968GfPmzcPkyZORm5sLR0dHdOzYUT3TxLvvvovff/8dISEhsLCwQEREBPr27YuCgoJyj9e4cWMcPHhQ3YMcHx8PAOjevTu8vLzQtWtXKBQKDB48GLGxsdV+/kRERETGgrNVVFHZLBIJCQmGDqXK5HI5bG1tn/gUp66USiWSkpIQFhbGcVTPOLal8WBbGge2o/FgW9YcXfMcft9ORERERFSKyTERERERUSmOOa6ih18DTURERETPNvYcExERERGVYnJMRERERFSKyTERERERUSkmxzUsPDwcffv2rfbjFBUV4bXXXoONjQ0EQcCtW7eq/ZhEREREzzo+kGektmzZgh9//BE///wzHB0dYWtra+iQiIiIiP7zmBwbqezsbDRt2hTNmzc3dCj0jEvOzMOag1m4cF2CTTlHMT7QCyF8hTQRERkpDqt4CiqVCosXL0ajRo0gk8ng5uaG999/HwBw9uxZBAYGwtzcHA4ODoiIiEBhYaFWHUuXLoWzszMcHBwwfvx4KJVK9TqFQoEpU6agXr16sLS0RIcOHbSmjNu5cyd8fHwgk8ng7u6ufoU08OCtffHx8fjhhx8gCAICAgKq5TqQ8UvOzMOYrRk4kytHsUrAmVw5IrdlIDkzz9ChERERVQv2HD+FGTNm4IMPPsDy5cvRpUsXXL9+HRcuXMCdO3cQEhKCTp06IT09Hfn5+Rg1ahSioqKQmJio3j81NRXOzs5ITU3FpUuXMHDgQPj6+mL06NEAgKioKJw7dw6ffvopXFxc8PXXXyM0NBRnz56Fl5cXMjIyMGDAAMTGxmLgwIH4+eefMW7cODg4OCA8PBxfffUV3n77bfz666/46quvYGpqWu55KBQKKBQK9bJcLgfw4FWWDyfrT6usDn3URYax5mCWVpkoAmtSsxDo7WCAiKiqeF8aB7aj8WBb1hxdr7EgiqJYzbEYldu3b6N27dpYvXo1Ro0apbHugw8+wPTp03H16lVYWloCAJKSktC7d29cu3YNdevWRXh4ONLS0pCdnQ2JRAIAGDBgAExMTPDpp58iJycHHh4eyMnJgYuLi7ruHj16oH379pg/fz6GDh2Kv/76C/v27VOvnzZtGvbs2YPMzEwAQHR0NE6dOvXYl5TExsYiLi5Oq3zHjh2wsLB46mtExmPqMQmKVYJWuamJiCUdSgwQERER0dMpKirCkCFDUFBQABsbmwq3Y89xJZ0/fx4KhQLdu3cvd12rVq3UiTEAdO7cGSqVChcvXkTdunUBAD4+PurEGACcnZ1x9uxZAA+GZZSUlMDb21ujboVCAQcHB/Vx+vTpo7G+c+fOSEhIQElJiUbdjzNjxgzExMSol+VyOVxdXREcHPzYD42ulEolUlJSEBQUBKlUWuX6qOZtyjmKM7lyrfImLrYIC+togIioqnhfGge2o/FgW9acsm/In4TJcSWZm5tXuY5HP/yCIEClUgEACgsLIZFIkJGRoZXkWllZVfnYD5PJZJDJZOXGp88bVN/1Uc0ZH+iFyG0ZePj7JUEAorp5sU2fcbwvjQPb0XiwLaufrteXD+RVkpeXF8zNzXHgwAGtdU2bNsXp06dx584dddnhw4dhYmKCxo0b61R/69atUVJSgvz8fDRq1EjjPycnJ/VxDh8+rLHf4cOH4e3trXOvMZEuQnycsH5YG7SsbwNTExEt69tgw7A2COZsFUREZKTYc1xJZmZmmD59OqZNmwZTU1N07twZf/31FzIzMzF06FDMnj0bI0aMQGxsLP766y9MmDABb7zxhnpIxZN4e3tj6NChGD58OOLj49G6dWv89ddfOHDgAFq2bImePXti8uTJaNeuHebOnYuBAwfiyJEjWL16NdauXVvNZ0/PoxAfJwR6OyApKQlhYR3Zs0FEREaNyfFTeO+991CrVi3MmjUL165dg7OzMyIjI2FhYYHk5GRMmjQJ7dq1g4WFBV577TUsW7asUvVv3rwZ8+bNw+TJk5GbmwtHR0d07NgRvXr1AgC8+OKL+PzzzzFr1izMnTsXzs7OmDNnDsLDw6vhbImIiIieH5ytgtTkcjlsbW2f+BSnrpRKZWlvYxh7G59xbEvjwbY0DmxH48G2rDm65jkcc0xEREREVIrJMRERERFRKSbHRERERESlmBwTEREREZVickxEREREVIrJMRERERFRKSbHNUQURURERMDe3h6CIKBv377o27evzvunpaVBEATcunWr2mIkIiIiet7xJSA1ZO/evUhMTERaWho8PDxgbm4OTjFNRERE9N/C5LiGZGdnw9nZGX5+foYOhahSkjPzsOZgFi5cl2BTzlGMD/RCiI+TocMiIiKqFhxWUQPCw8MxYcIE5OTkQBAEuLu7Izw8XGNYhUKhwMSJE1GnTh2YmZmhS5cuSE9P16orIyMDbdu2hYWFBfz8/HDx4kWN9d999x3atWsHMzMzODo64tVXX63u0yMjlpyZhzFbM3AmV45ilYAzuXJEbstAcmaeoUMjIiKqFuw5rgErVqyAp6cnNm7ciPT0dEgkEkydOlVjm2nTpmHnzp3YsmULGjRogMWLFyMkJASXLl2Cvb29ert33nkH8fHxqF27NiIjI/HWW2/h8OHDAIA9e/bg1VdfxTvvvIOPP/4YxcXFSEpKqjAuhUIBhUKhXpbL5QAevMpSqVRW+bzL6tBHXWQYaw5maZWJIrAmNQuB3g4GiIiqivelcWA7Gg+2Zc3R9RoLIge+1oiEhAQkJCTgypUrAB70Jt+6dQu7du3CnTt38MILLyAxMRFDhgwB8KAB3d3dER0djalTpyItLQ3dunXD/v370b17dwBAUlISevbsibt378LMzAx+fn7w8PDAtm3bdIopNjYWcXFxWuU7duyAhYWFfk6cnmlTj0lQrBK0yk1NRCzpUGKAiIiIiJ5OUVERhgwZgoKCAtjY2FS4HXuO/wOys7OhVCrRuXNndZlUKkX79u1x/vx5jW1btmyp/rezszMAID8/H25ubjh16hRGjx6t83FnzJiBmJgY9bJcLoerqyuCg4Mf+6HRlVKpREpKCoKCgiCVSqtcH9W8TTlHcSZXrlXexMUWYWEdDRARVRXvS+PAdjQebMuaU/YN+ZMwOX7GPHzjCMKDHj2VSgUAMDc3r1RdMpkMMpms3GPo8wbVd31Uc8YHeiFyWwYe/n5JEICobl5s02cc70vjwHY0HmzL6qfr9eUDef8Bnp6eMDU1VY8dBh78JZmeno5mzZrpXE/Lli1x4MCB6giRnlMhPk5YP6wNWta3gamJiJb1bbBhWBsEc7YKIiIyUuw5/g+wtLTE2LFjMXXqVNjb28PNzQ2LFy9GUVERRo4cqXM9s2fPRvfu3eHp6YlBgwbh/v37SEpKwvTp06sxejJ2IT5OCPR2QFJSEsLCOrJng4iIjBqT4/+IhQsXQqVS4Y033sDt27fRtm1bJCcn44UXXtC5joCAAHzxxReYO3cuFi5cCBsbG3Tt2rUaoyYiIiIyLkyOa0h0dDSio6PVywqFAlZWVuplMzMzrFy5EitXrix3/4CAAK036vn6+mqV9evXD/369dNf4ERERETPEY45rmH379/HuXPncOTIEfj4+Bg6HCIiIiJ6CJPjGvbrr7+ibdu28PHxQWRkpKHDISIiIqKHcFhFDfP19UVRUZGhwyAiIiKicrDnmIiIiIioFJNjIiIiIqJSTI6JiIiIiEoxOdYDURQREREBe3t7CIKAvn37om/fvjrvn5aWBkEQcOvWrWqLkYiIiIiejA/k6cHevXuRmJiItLQ0eHh4wNzcXGv+4eomiiJmz56NDz74ALdu3ULnzp2xbt06eHl51WgcRERERM8y9hzrQXZ2NpydneHn5wcnJyfY2trCzs6uRmNYvHgxVq5cifXr1+PYsWOwtLRESEgI7t27V6NxkPFJzszDa+uPYuoxCV5bfxTJmXmGDomIiKjaMDmuovDwcEyYMAE5OTkQBAHu7u4IDw/XGFahUCgwceJE1KlTB2ZmZujSpQvS09O16srIyEDbtm1hYWEBPz8/XLx4UWP9d999h3bt2sHMzAyOjo549dVXATzoNU5ISMC7776LPn36oGXLlvj4449x7do17Nq1qzpPn4xccmYexmzNwJlcOYpVAs7kyhG5LYMJMhERGS0Oq6iiFStWwNPTExs3bkR6ejokEgmmTp2qsc20adOwc+dObNmyBQ0aNMDixYsREhKCS5cuwd7eXr3dO++8g/j4eNSuXRuRkZF46623cPjwYQDAnj178Oqrr+Kdd97Bxx9/jOLiYiQlJQEALl++jLy8PPTo0UNdl62tLTp06IAjR45g0KBB5cauUCigUCjUy3K5HACgVCqhVCqrfG3K6tBHXWQYaw5maZWJIrAmNQuB3g4GiIiqivelcWA7Gg+2Zc3R9RozOa4iW1tbWFtbQyKRwMnJSWv9nTt3sG7dOiQmJuLll18GAHzwwQdISUnBpk2bNBLp999/H/7+/gCAt99+Gz179sS9e/dgZmaG999/H4MGDUJcXJx6+1atWgEA8vIe9OLVrVtX49h169ZVryvPggULNOors2/fPlhYWOh6CZ4oJSVFb3VRzbpwXQJA0C6/VqD+44yeTbwvjQPb0XiwLaufri9hY3JczbKzs6FUKtG5c2d1mVQqRfv27XH+/HmNbVu2bKn+t7OzMwAgPz8fbm5uOHXqFEaPHq3X2GbMmIGYmBj1slwuh6urK4KDg2FjY1Pl+pVKJVJSUhAUFASpVFrl+qjmbco5ijO5cq3yJi62CAvraICIqKp4XxoHtqPxYFvWnLJvyJ+EyfF/yMM3hSA86K1TqVQAAHNz8wr3K+uxvnHjhjqpLlv29fWtcD+ZTAaZTFZuHPq8QfVdH9Wc8YFeiNyWgYcnXxEEIKqbF9v0Gcf70jiwHY0H27L66Xp9+UBeNfP09ISpqal67DDw4K/E9PR0NGvWTOd6WrZsiQMHDpS7rmHDhnByctJYL5fLcezYMXTq1Onpg6fnXoiPE9YPa4OW9W1gaiKiZX0bbBjWBsE+2kOIiIiIjAF7jquZpaUlxo4di6lTp8Le3h5ubm5YvHgxioqKMHLkSJ3rmT17Nrp37w5PT08MGjQI9+/fR1JSEqZPnw5BEBAdHY158+bBy8sLDRs2xHvvvQcXF5dKvYyEqDwhPk4I9HZAUlISwsI6smeDiIiMGpPjGrBw4UKoVCq88cYbuH37Ntq2bYvk5GS88MILOtcREBCAL774AnPnzsXChQthY2ODrl27qtdPmzYNd+7cQUREBG7duoUuXbpg7969MDMzq45TIiIiIjJKTI71IDo6GtHR0eplhUIBKysr9bKZmRlWrlyJlStXlrt/QECA1hv1fH19tcr69euHfv36lVuHIAiYM2cO5syZ85RnQUREREQcc6xH9+/fx7lz53DkyBH4+PgYOhwiIiIiqiQmx3r066+/om3btvDx8UFkZKShwyEiIiKiSuKwCj3y9fXVeYJpIiIiIvrvYc8xEREREVEpJsdERERERKWYHBMRERERlWJy/AhRFBEREQF7e3sIgoBTp05Vqb7w8PAnvojD3d0dCQkJVToOEREREVUdH8h7xN69e5GYmIi0tDR4eHjA0dHR0CERERERUQ1hcvyI7OxsODs7w8/Pz9ChEP0nJGfmYc3BLFy4LsGmnKMYH+iFEB8nQ4dFRERULTis4iHh4eGYMGECcnJyIAgC3N3doVKpsHjxYjRq1AgymQxubm54//331fucPXsWgYGBMDc3h4ODAyIiIlBYWKhV99KlS+Hs7AwHBweMHz8eSqVSY/3t27cxePBgWFpaol69elizZo3G+pycHPTp0wdWVlawsbHBgAEDcOPGDfX62NhY+Pr6YsOGDXB1dYWFhQUGDBiAgoICPV8lep4kZ+ZhzNYMnMmVo1gl4EyuHJHbMpCcmWfo0IiIiKoFe44fsmLFCnh6emLjxo1IT0+HRCLBjBkz8MEHH2D58uXo0qULrl+/jgsXLgAA7ty5g5CQEHTq1Anp6enIz8/HqFGjEBUVhcTERHW9qampcHZ2RmpqKi5duoSBAwfC19cXo0ePVm+zZMkSzJw5E3FxcUhOTsakSZPg7e2NoKAgqFQqdWJ86NAh3L9/H+PHj8fAgQORlpamruPSpUv4/PPP8d1330Eul2PkyJEYN24ctm/fXu75KhQKKBQK9bJcLgcAKJVKreT9aZTVoY+6yDDWHMzSKhNFYE1qFgK9HQwQEVUV70vjwHY0HmzLmqPrNRZEURSrOZZnSkJCAhISEnDlyhXcvn0btWvXxurVqzFq1CitbT/44ANMnz4dV69ehaWlJQAgKSkJvXv3xrVr11C3bl2Eh4cjLS0N2dnZkEgkAIABAwbAxMQEn376KYAHD+Q1bdoU33//vbruQYMGQS6XIykpCSkpKXj55Zdx+fJluLq6AgDOnTsHHx8fHD9+HO3atUNsbCzmzZuHP/74A/Xq1QPwYPx0z549kZubCycn7a/BY2NjERcXp1W+Y8cOWFhYVPFKkjGYekyCYpWgVW5qImJJhxIDRERERPR0ioqKMGTIEBQUFMDGxqbC7dhz/Bjnz5+HQqFA9+7dK1zfqlUrdWIMAJ07d4ZKpcLFixdRt25dAICPj486MQYAZ2dnnD17VqOuTp06aS2XzWBx/vx5uLq6qhNjAGjWrBns7Oxw/vx5tGvXDgDg5uamTozL6iiLpbzkeMaMGYiJiVEvy+VyuLq6Ijg4+LEfGl0plUqkpKQgKCgIUqm0yvVRzduUcxRncuVa5U1cbBEW1tEAEVFV8b40DmxH48G2rDll35A/CZPjxzA3N9dLPY9+2AVBgEql0kvdVSGTySCTybTKpVKpXm9QfddHNWd8oBcit2Xg4e+XBAGI6ubFNn3G8b40DmxH48G2rH66Xl8+kPcYXl5eMDc3x4EDB8pd37RpU5w+fRp37txRlx0+fBgmJiZo3LhxpY519OhRreWmTZuqj3P16lVcvXpVvf7cuXO4desWmjVrpi7LycnBtWvXNOp4mliIyoT4OGH9sDZoWd8GpiYiWta3wYZhbRDM2SqIiMhIMTl+DDMzM0yfPh3Tpk3Dxx9/jOzsbBw9ehSbNm0CAAwdOhRmZmYYMWIEfv31V6SmpmLChAl444031EMqdHX48GEsXrwYv/32G9asWYMvvvgCkyZNAgD06NEDLVq0wNChQ/HLL7/g+PHjGD58OPz9/dG2bVuNeEeMGIHTp0/jxx9/xMSJEzFgwIByh1QQ6SrExwk7x3TEkg4l2DmmIxNjIiIyahxW8QTvvfceatWqhVmzZuHatWtwdnZGZGQkAMDCwkI9s0S7du1gYWGB1157DcuWLav0cSZPnowTJ04gLi4ONjY2WLZsGUJCQgA8GIbxzTffYMKECejatStMTEwQGhqKVatWadTRqFEj9OvXD2FhYfj333/Rq1cvrF27tuoXgYiIiOg5weT4EdHR0YiOjlYvm5iY4J133sE777xT7vYtWrTAwYMHK6zv4Sndyjz6qugrV648MS43Nzd88803T9xu7NixGDt27BO3IyIiIiJtHFZBRERERFSKyTERERERUSkmx0YiNjYWp06dMnQYRERERM80JsdERERERKWYHBMRERERlWJyTERERERUislxNRFFEREREbC3t4cgCLCzs9OYIk4f3N3dtaaFIyIiIqKnx3mOq8nevXuRmJiItLQ0eHh4wMTEBObm5no9Rnp6OiwtLfVaJxEREdHzjMlxNcnOzoazszP8/Pyq7Ri1a9eutrqJyiRn5mHNwSxcuC7BppyjGB/ohRC+QpqIiIwUh1VUg/DwcEyYMAE5OTkQBAHu7u4ICAjQGFZx8+ZNDB8+HC+88AIsLCzw8ssvIysrS6OenTt3wsfHBzKZDO7u7oiPj9dY/+iwilu3bmHMmDGoW7cuzMzM0Lx5c+zevbs6T5WMXHJmHsZszcCZXDmKVQLO5MoRuS0DyZl5hg6NiIioWrDnuBqsWLECnp6e2LhxI9LT0yGRSNC/f3+NbcLDw5GVlYVvv/0WNjY2mD59OsLCwnDu3DlIpVJkZGRgwIABiI2NxcCBA/Hzzz9j3LhxcHBwQHh4uNYxVSoVXn75Zdy+fRvbtm2Dp6cnzp07B4lEUmGcCoUCCoVCvSyXywEASqUSSqWyytehrA591EWGseZgllaZKAJrUrMQ6O1ggIioqnhfGge2o/FgW9YcXa8xk+NqYGtrC2tra0gkEjg5aX/9XJYUHz58WD3sYvv27XB1dcWuXbvQv39/LFu2DN27d8d7770HAPD29sa5c+ewZMmScpPj/fv34/jx4zh//jy8vb0BAB4eHo+Nc8GCBYiLi9Mq37dvHywsLCp72hVKSUnRW11Usy5clwAQtMuvFSApKanmAyK94X1pHNiOxoNtWf2Kiop02o7JsQGcP38etWrVQocOHdRlDg4OaNy4Mc6fP6/epk+fPhr7de7cGQkJCSgpKdHqET516hTq16+vTox1MWPGDMTExKiX5XI5XF1dERwcDBsbm6c5NQ1KpRIpKSkICgqCVCqtcn1U8zblHMWZXLlWeRMXW4SFdTRARFRVvC+NA9vReLAta07ZN+RPwuTYSDzNTBgymQwymUyrXCqV6vUG1Xd9VHPGB3ohclsGRPF/ZYIARHXzYps+43hfGge2o/FgW1Y/Xa8vH8gzgKZNm+L+/fs4duyYuuyff/7BxYsX0axZM/U2hw8f1tjv8OHD8Pb2LnccccuWLfHnn3/it99+q97g6bkS4uOE9cPaoGV9G5iaiGhZ3wYbhrVBMGerICIiI8WeYwPw8vJCnz59MHr0aGzYsAHW1tZ4++23Ua9ePfVQismTJ6Ndu3aYO3cuBg4ciCNHjmD16tVYu3ZtuXX6+/uja9eueO2117Bs2TI0atQIFy5cgCAICA0NrcnTIyMT4uOEQG8HJCUlISysI3s2iIjIqLHn2EA2b96MNm3aoFevXujUqRNEUURSUpI68XjxxRfx+eef49NPP0Xz5s0xa9YszJkzp9yH8crs3LkT7dq1w+DBg9GsWTNMmzYNJSUlNXRGRERERM8+9hxXk+joaI15jdPS0jTWv/DCC/j4448fW8drr72G1157rcL1V65c0Vi2t7fHRx99VNlQiYiIiKgUe46JiIiIiEoxOSYiIiIiKsXkmIiIiIioFJNjIiIiIqJSTI6JiIiIiEoxOSYiIiIiKsXkmIiIiIioFJPjCoiiiIiICNjb20MQBJw6darSdcTGxsLX11fvsRERERFR9eBLQCqwd+9eJCYmIi0tDR4eHnB0dDR0SEQGkZyZhzUHs3DhugSbco5ifKAXQnycDB0WERFRtWDPcQWys7Ph7OwMPz8/ODk5oVYt/h1Bz5/kzDyM2ZqBM7lyFKsEnMmVI3JbBpIz8wwdGhERUbVgxleO8PBwbNmyBQAgCAKcnZ0BAH/++SdMTP7390SfPn3g4OCgfmXzwoULsXz5chQVFWHAgAGoXbu2Rr0BAQHw9fVFQkKCuqxv376ws7NDYmIiAMDd3R2jRo3Cb7/9hq+++goODg5YtWoVOnXqhFGjRuHAgQPw8PDARx99hLZt2wIAEhMTER0djcTEREydOhVXr16Fv78/PvzwQ7i6ulZ4ngqFAgqFQr0sl8sBAEqlEkql8imv3v+U1aGPusgw1hzM0ioTRWBNahYCvR0MEBFVFe9L48B2NB5sy5qj6zVmclyOFStWwNPTExs3bkR6ejokEgnq16+P1NRUdO/eHQDw77//Yu/evUhKSgIAfP7554iNjcWaNWvQpUsXbN26FStXroSHh0elj798+XLMnz8f7733HpYvX4433ngDfn5+eOutt7BkyRJMnz4dw4cPR2ZmJgRBAAAUFRXh/fffx8cffwxTU1OMGzcOgwYNwuHDhys8zoIFCxAXF6dVvm/fPlhYWFQ67oqkpKTorS6qWReuSwAI2uXXCtSffXo28b40DmxH48G2rH5FRUU6bcfkuBy2trawtraGRCKBk9ODsZUvv/wyduzYoU6Ov/zySzg6OqJbt24AgISEBIwcORIjR44EAMybNw/79+/HvXv3Kn38sLAwjBkzBgAwa9YsrFu3Du3atUP//v0BANOnT0enTp1w48YNdXxKpRKrV69Ghw4dAABbtmxB06ZNcfz4cbRv377c48yYMQMxMTHqZblcDldXVwQHB8PGxqbScT9KqVQiJSUFQUFBkEqlVa6Pat6mnKM4kyvXKm/iYouwsI4GiIiqivelcWA7Gg+2Zc0p+4b8SZgc62jo0KEYPXo01q5dC5lMhu3bt2PQoEHqYRbnz59HZGSkxj6dOnVCampqpY/VsmVL9b/r1q0LAGjRooVWWX5+vjo5rlWrFtq1a6fepkmTJrCzs8P58+crTI5lMhlkMplWuVQq1esNqu/6qOaMD/RC5LYMiOL/ygQBiOrmxTZ9xvG+NA5sR+PBtqx+ul5fPpCno969e0MURezZswdXr17Fjz/+iKFDh1aqDhMTE4gPZxkof/zLw41XNmyivDKVSlWp4xNVVoiPE9YPa4OW9W1gaiKiZX0bbBjWBsGcrYKIiIwUk2MdmZmZoV+/fti+fTs++eQTNG7cGC+++KJ6fdOmTXHs2DGNfY4ePaqxXLt2bVy/fl29XFJSgl9//VUv8d2/fx8nTpxQL1+8eBG3bt1C06ZN9VI/Pb9CfJywc0xHLOlQgp1jOjIxJiIio8ZhFZUwdOhQ9OrVC5mZmRg2bJjGukmTJiE8PBxt27ZF586dsX37dmRmZmo8kBcYGIiYmBjs2bMHnp6eWLZsGW7duqWX2KRSKSZMmICVK1eiVq1aiIqKQseOHSscUkFERERE2pgcV0JgYCDs7e1x8eJFDBkyRGPdwIEDkZ2djWnTpuHevXt47bXXMHbsWCQnJ6u3eeutt3D69GkMHz4ctWrVwv/93/+pH+irKgsLC0yfPh1DhgxBbm4uXnrpJWzatEkvdRMRERE9L5gcVyA6OhrR0dEaZSYmJrh27VqF+8ycORMzZ87UKFu0aJH631KpFGvXrsXatWsrrOPKlStaZY+OU3Z3d9cqA4B+/fqhX79+FdZNRERERI/HMcdERERERKWYHBMRERERlWJybATCw8P19mAfERER0fOMyTERERERUSkmx0REREREpZgcExERERGVYnJsQLGxsfD19a3UPoIgYNeuXdUSDxEREdHzjskxEREREVEpJsdE9FjJmXl4bf1RTD0mwWvrjyI5M8/QIREREVUbJsd6snHjRri4uEClUmmU9+nTB2+99RYAYOHChahbty6sra0xcuRI3Lt3T2Pb9PR0BAUFwdHREba2tvD398cvv/xS4TFff/11REVFqZejo6MhCAIuXLgAACguLoalpSX279+vr9Ok50xyZh7GbM3AmVw5ilUCzuTKEbktgwkyEREZLb4+Wk/69++PCRMmIDU1Fd27dwcA/Pvvv9i7dy+SkpLw+eefIzY2FmvWrEGXLl2wdetWrFy5Eh4eHuo6bt++jREjRmDVqlUQRRHx8fEICwtDVlYWrK2ttY7p7++PDRs2qJcPHToER0dHpKWloUmTJkhPT4dSqYSfn1+5MSsUCigUCvWyXC4HACiVSiiVyipfk7I69FEXGcaag1laZaIIrEnNQqC3gwEioqrifWkc2I7Gg21Zc3S9xoIoimI1x/Lc6Nu3LxwcHLBp0yYAD3qT4+LicPXqVXTp0gWtW7fGmjVr1Nt37NgR9+7dw6lTp8qtT6VSwc7ODjt27ECvXr0APHgg7+uvv0bfvn1x9uxZtGrVCjdu3ECtWrXg5OSE9957D7/++is+/fRTvP/++0hKSsLhw4fLrT82NhZxcXFa5Tt27ICFhUUVrwYZg6nHJChWCVrlpiYilnQoMUBERERET6eoqAhDhgxBQUEBbGxsKtyOPcd6NHToUIwePRpr166FTCbD9u3bMWjQIJiYmOD8+fOIjIzU2L5Tp05ITU1VL9+4cQPvvvsu0tLSkJ+fj5KSEhQVFSEnJ6fc4zVv3hz29vY4dOgQTE1N0bp1a/Tq1UudgB86dAgBAQEVxjtjxgzExMSol+VyOVxdXREcHPzYD42ulEolUlJSEBQUBKlUWuX6qOZtyjmKM7lyrfImLrYIC+togIioqnhfGge2o/FgW9acsm/In4TJsR717t0boihiz549aNeuHX788UcsX75c5/1HjBiBf/75BytWrECDBg0gk8nQqVMnFBcXl7u9IAjo2rUr0tLSIJPJEBAQgJYtW0KhUODXX3/Fzz//jClTplR4PJlMBplMplUulUr1eoPquz6qOeMDvRC5LQMPf78kCEBUNy+26TOO96VxYDsaD7Zl9dP1+vKBPD0yMzNDv379sH37dnzyySdo3LgxXnzxRQBA06ZNcezYMY3tjx49qrF8+PBhTJw4EWFhYfDx8YFMJsPff//92GP6+/sjLS0NaWlpCAgIgImJCbp27YolS5ZAoVCgc+fO+j1Jeq6E+Dhh/bA2aFnfBqYmIlrWt8GGYW0Q7ONk6NCIiIiqBXuO9Wzo0KHo1asXMjMzMWzYMHX5pEmTEB4ejrZt26Jz587Yvn07MjMzNR7I8/LywtatW9G2bVvI5XJMnToV5ubmjz1eQEAA/u///g+mpqbo0qWLumzKlClo164dLC0tq+dE6bkR4uOEQG8HJCUlISysI3s2iIjIqLHnWM8CAwNhb2+PixcvYsiQIerygQMH4r333sO0adPQpk0b/PHHHxg7dqzGvps2bcLNmzfx4osv4o033sDEiRNRp06dxx6vRYsWsLOzg6+vL6ysrAA8SI5LSkoeO96YiIiIiLSx51jPTExMcO3atXLXzZw5EzNnztQoW7RokfrfrVu3Rnp6usb6119/XWP50clFTExM8O+//2qU+fr6am1HRERERE/GnmMiIiIiolJMjomIiIiISjE5JiIiIiIqxeSYiIiIiKgUk2MiIiIiolJMjomIiIiISjE5riaiKCIiIgL29vYQBAF9+/ZF3759DR0WERERET0G5zmuJnv37kViYiLS0tLg4eEBc3PzGpt72N3dHdHR0YiOjq6R4xEREREZCybH1SQ7OxvOzs7w8/PTW53FxcUwNTXVW32kLTkzD2tTL+G3G4XwrmuFcd0aIcTHydBhERERUQ3hsIpqEB4ejgkTJiAnJweCIMDd3R3h4eEawyoCAgIQFRWFqKgo2NrawtHREe+9955G77K7uzvmzp2L4cOHw8bGBhEREQCAnTt3wsfHBzKZDO7u7oiPj9eo948//sD//d//QRAECIJQY+f9rEvOzMOYrRk4/WcB7ipLcPrPAkRuy0ByZp6hQyMiIqIawp7jarBixQp4enpi48aNSE9Ph0QiwdSpU7W227JlC0aOHInjx4/jxIkTiIiIgJubG0aPHq3eZunSpZg1axZmz54NAMjIyMCAAQMQGxuLgQMH4ueff8a4cePg4OCA8PBwfPXVV2jVqhUiIiI06imPQqGAQqFQL8vlcgCAUqmEUqms8nUoq0MfddWENQeztMpEEViTmoVAbwcDRPTf8ay1JVWMbWkc2I7Gg21Zc3S9xkyOq4GtrS2sra0hkUjg5FTxV/Kurq5Yvnw5BEFA48aNcfbsWSxfvlwjqQ0MDMTkyZPVy0OHDkX37t3x3nvvAQC8vb1x7tw5LFmyBOHh4bC3t4dEIoG1tfVjjw0ACxYsQFxcnFb5vn37YGFhUdnTrlBKSore6qpOF65LAGj3tF+4VoCkpKSaD+g/6FlpS3oytqVxYDsaD7Zl9SsqKtJpOybHBtSxY0eNYQ+dOnVCfHw8SkpKIJFIAABt27bV2Of8+fPo06ePRlnnzp2RkJCgsZ8uZsyYgZiYGPWyXC6Hq6srgoODYWNj8zSnpEGpVCIlJQVBQUGQSqVVrq+6bco5ijO5cq3yJi62CAvraICI/juetbakirEtjQPb0XiwLWtO2TfkT8Lk+D/O0tKy2uqWyWSQyWRa5VKpVK83qL7rqy7jA70QuS0DD08qIghAVDevZyL+mvCstCU9GdvSOLAdjQfbsvrpen35QJ4BHTt2TGP56NGj8PLyemzvb9OmTXH48GGNssOHD8Pb21u9n6mpKUpKSvQfsJEL8XHC+mFt0MrVDhamErRytcOGYW0QzNkqiIiInhvsOTagnJwcxMTEYMyYMfjll1+watUqjZknyjN58mS0a9cOc+fOxcCBA3HkyBGsXr0aa9euVW/j7u6OH374AYMGDYJMJoOjo2N1n4rRCPFx4tRtREREzzEmxwY0fPhw3L17F+3bt4dEIsGkSZPU07VV5MUXX8Tnn3+OWbNmYe7cuXB2dsacOXMQHh6u3mbOnDkYM2YMPD09oVAoauzlI0RERETPOibH1eTRN9QpFApYWVlpbCOVSpGQkIB169aVW8eVK1fKLX/ttdfw2muvVXjsjh074vTp05WOmYiIiOh5xzHH1ez+/fs4d+4cjhw5Ah8fH0OHQ0RERESPUankWKlUwtPTE+fPn6+ueIzOr7/+irZt28LHxweRkZGGDoeIiIiIHqNSwyqkUinu3btXXbEYJV9f33InnU5LS6v5YIiIiIjosSo9rGL8+PFYtGgR7t+/Xx3xEBEREREZTKUfyEtPT8eBAwewb98+tGjRQuslFV999ZXegiMiIiIiqkmVTo7t7OweO1MCEREREdGzqtLJ8ebNm6sjDoMTRRFjxozBl19+iZs3b+LkyZPw9fU1dFhPbePGjZg7dy5yc3OxbNkyjWnliIiIiKh8TzWV2/3797F//35s2LABt2/fBgBcu3YNhYWFeg2uJu3duxeJiYnYvXs3rl+/jtatW2PXrl2GDuuJBEHQilMulyMqKgrTp09Hbm7uE18sQkREREQPVLrn+I8//kBoaChycnKgUCgQFBQEa2trLFq0CAqFAuvXr6+OOKtddnY2nJ2d4efnZ+hQUFJSAkEQYGLydNNQ5+TkQKlUomfPnnB2dtZzdPS8Sc7Mw5qDWbhwXYJNOUcxPtCLr9gmIiKjVensa9KkSWjbti1u3rwJc3Nzdfmrr76KAwcO6DW4mhIeHo4JEyYgJycHgiDA3d0dwINzeng5NjYWvr6++Oijj+Dm5gYrKyuMGzcOJSUlWLx4MZycnFCnTh28//77GvUvW7ZM/fCiq6srxo0bp9HLnpiYCDs7O3z77bdo1qwZZDIZcnJycP36dfTs2RPm5uZo2LAhduzYAXd3dyQkJABAuXEmJiaiRYsWAAAPDw8IglDhm/aIniQ5Mw9jtmbgTK4cxSoBZ3LliNyWgeTMPEOHRkREVC0q3XP8448/4ueff4apqalGubu7O3Jzc/UWWE1asWIFPD09sXHjRqSnp0MikaBOnTrYvHkzQkNDIZFI1NtmZ2fj+++/x969e5GdnY3XX38dv//+O7y9vXHo0CH8/PPPeOutt9CjRw906NABAGBiYoKVK1eiYcOG+P333zFu3DhMmzYNa9euVddbVFSERYsW4cMPP4SDgwPq1KmDPn364O+//0ZaWhqkUiliYmKQn5+v3ic9PV0rTisrK7i6uqJHjx44fvw4XF1dUbt27XLPW6FQQKFQqJflcjmABy97USqVVb6uZXXooy4yjDUHs7TKRBFYk5qFQG8HA0REVcX70jiwHY0H27Lm6HqNK50cq1QqlJSUaJX/+eefsLa2rmx1/wm2trawtraGRCKBk9P/vi62s7PTWAYenP9HH30Ea2trNGvWDN26dcPFixeRlJQEExMTNG7cGIsWLUJqaqo6OX74YTh3d3fMmzcPkZGRGsmxUqnE2rVr0apVKwDAhQsXsH//fqSnp6Nt27YAgA8//BBeXl7qfcqS3kfjdHBwUK9/NP6HLViwAHFxcVrl+/btg4WFxeMvWiWkpKTorS6qWReuSwAI2uXXCpCUlFTzAZHe8L40DmxH48G2rH7lvZStPJVOjoODg5GQkICNGzcCePBAWGFhIWbPno2wsLDKVvfMcXd31/gjoG7dupBIJBrjg+vWravRw7t//34sWLAAFy5cgFwux/3793Hv3j0UFRWpk1BTU1O0bNlSvc/FixdRq1YtvPjii+qyRo0a4YUXXtDbucyYMQMxMTHqZblcDldXVwQHB8PGxqbK9SuVSqSkpCAoKAhSqbTK9VHN25RzFGdy5VrlTVxsERbW0QARUVXxvjQObEfjwbasOWXfkD9JpZPj+Ph4hISEoFmzZrh37x6GDBmCrKwsODo64pNPPql0oM+aRz+4giCUW6ZSqQAAV65cQa9evTB27Fi8//77sLe3x08//YSRI0eiuLhYnRybm5tDELR76KqTTCaDTCbTKpdKpXq9QfVdH9Wc8YFeiNyWAVH8X5kgAFHdvNimzzjel8aB7Wg82JbVT9frW+nkuH79+jh9+jQ+++wznD59GoWFhRg5ciSGDh2q8YDes04qlZY7fKSyMjIyoFKpEB8fr+5d/vzzz5+4X+PGjXH//n2cPHkSbdq0AQBcunQJN2/erJY4icoT4uOE9cPaYE1qFi5cK0ATF1tEdfNCMGerICIiI1Xp5PiHH36An58fhg4diqFDh6rL79+/jx9++AFdu3bVa4CG4u7ujgMHDqBz586QyWRPPZyhUaNGUCqVWLVqFXr37o3Dhw/rNN1dkyZN0KNHD0RERGDdunWQSqWYPHmyVg+zvuIkqkiIjxMCvR2QlJSEsLCO7NkgIiKjVump3Lp164Z///1Xq7ygoADdunXTS1D/BfHx8UhJSYGrqytat2791PW0atUKy5Ytw6JFi9C8eXNs374dCxYs0Gnfjz/+GHXr1kXXrl3x6quvYvTo0bC2toaZmZne4yQiIiIiQBDFh0cTPpmJiQlu3LihNT3Yb7/9hrZt2+o82Jkq788//4Srqyv279+P7t27671+uVwOW1tbFBQU6O2BvAe9jWHsbXzGsS2NB9vSOLAdjQfbsubomufoPKyiX79+AB48bBYeHq7xIFdJSQnOnDnzn3i7nDE5ePAgCgsL0aJFC1y/fh3Tpk2Du7u70QxdISIiIvqv0Tk5trW1BQCIoghra2uNh+9MTU3RsWNHjB49Wv8RPseUSiVmzpyJ33//HdbW1vDz88P27dv5lyURERFRNdE5Od68eTOABw+ATZkyBZaWltUWFD0QEhKCkJAQQ4dBRERE9Nyo9AN5s2fPhkwmw/79+7Fhwwbcvn0bAHDt2jUUFhbqPUAiIiIioppS6anc/vjjD4SGhiInJwcKhQJBQUGwtrbGokWLoFAodJqmjIiIiIjov6jSPceTJk1C27ZtcfPmTY1xx6+++ioOHDig1+CIiIiIiGpSpZPjH3/8Ee+++y5MTU01yt3d3ZGbm6u3wKqLKIqIiIiAvb09BEHAqVOnDB2SXsTGxsLX19fQYRARERE90yqdHKtUqnJfV/znn3/C2tpaL0FVp7179yIxMRG7d+/G9evX0bp1a+zatcvQYRERERHRf0Clk+Pg4GAkJCSolwVBQGFhIWbPno2wsDB9xlYtsrOz4ezsDD8/Pzg5ORk0lpKSEqhUKoPGQPQkyZl5eG39UUw9JsFr648iOTPP0CERERFVm0onx/Hx8Th8+DCaNWuGe/fuYciQIeohFYsWLaqOGPUmPDwcEyZMQE5ODgRBgLu7O4AH46UfXi4bovDRRx/Bzc0NVlZWGDduHEpKSrB48WI4OTmhTp06eP/99zXqX7ZsGVq0aAFLS0u4urpi3LhxGjN4JCYmws7ODt9++y2aNWsGmUyGnJwcXL9+HT179oS5uTkaNmyIHTt2wN3dXeOPkJycHPTp0wdWVlawsbHBgAEDcOPGDa1z3Lp1K9zd3WFra4tBgwapZxMhehrJmXkYszUDZ3LlKFYJOJMrR+S2DCbIRERktCo9W0X9+vVx+vRpfPrppzhz5gwKCwsxcuRIDB06VOMBvf+iFStWwNPTExs3bkR6ejokEgnq1KmDzZs3IzQ0FBKJRL1tdnY2vv/+e+zduxfZ2dl4/fXX8fvvv8Pb2xuHDh3Czz//jLfeegs9evRAhw4dADx4tfbKlSvRsGFD/P777xg3bhymTZuGtWvXqustKirCokWL8OGHH8LBwQF16tRBnz598PfffyMtLQ1SqRQxMTHIz89X76NSqdSJ8aFDh3D//n2MHz8eAwcORFpamkbMu3btwu7du3Hz5k0MGDAACxcu1EriyygUCigUCvVy2au/lUollEplla93WR36qIsMY83BLK0yUQTWpGYh0NvBABFRVfG+NA5sR+PBtqw5ul7jSifHAFCrVi0MGzbsaXY1KFtbW1hbW0MikWgMqbCzs9MaYqFSqfDRRx/B2toazZo1Q7du3XDx4kUkJSXBxMQEjRs3xqJFi5CamqpOjv+fvTuPy6Lc/z/+GhBQREAQBRPFBVxQ1DTXSkQBRT25VJaaUZZiLhlpZZ4MPZlmh9zSbDExl6yjZX6NRFxo8SQpZnZww4UolcxSbpWCW+D3h3r/JFxAbiDu3s/Hw8dhrpn7ms/Mhzl9uO5rZiZMmGD5vJ+fHy+99BJRUVGFimOz2cyiRYto3bo1AAcOHGDz5s3s3LmT9u3bA/DOO+/g7+9v+cyWLVv4/vvvOXbsGL6+vgC89957BAYGsnPnTu644w5LzHFxcZa53w899BBbtmy5bnE8c+ZMpk2bVqR906ZNODs7F++kFkNiYqLV+pLydeCkPWAUbT+RRXx8fPkHJFaj69I2KI+2Q7kse9nZ2cXa7paK4xMnTvDVV19x6tSpInNmx48ffytd/uX4+fkVusGwTp062NvbY2dnV6jt6hHezZs3M3PmTA4cOIDJZOLixYv88ccfZGdnW4pNR0dHgoKCLJ85ePAgVapU4fbbb7e0NWnShJo1a1qW9+/fj6+vr6UwBmjRogXu7u7s37/fUhz/OWYfH59C8f3Z5MmTiY6OtiybTCZ8fX0JCwvD1dW1eCfqBsxmM4mJiYSGhuqV15XUkowd7D1uKtLerK4bERGdKiAiKS1dl7ZBebQdymX5ufIN+c2UuDiOi4tj1KhRODo64unpiWH8/1ElwzBspjj+8y+oYRjXbLvyx0F6ejp9+/Zl9OjRzJgxAw8PD7766itGjBhBbm6upTiuVq1aoXNW1jHf6IY/JycnnJycrtmPNS9Qa/cn5WdMiD9RK1IoKPj/bYYBY7v7K6eVnK5L26A82g7lsuwV9/yW+Ia8F154galTp5KVlUV6ejrHjh2z/Dt69GiJA61oDg4O13w0XUmlpKSQn59PbGwsnTp1IiAggBMnTtz0c02bNuXixYt8++23lrbDhw9z5swZy3Lz5s358ccf+fHHHy1t+/bt4+zZs7Ro0aLUsYtcT3igN4uHtSOoniuOdgUE1XPlzWHtCAus2Ce9iIiIlJUSF8fZ2dk88MADhaYXVGZ+fn5s2bKFzMzMQgVpSTVp0gSz2cyCBQs4evQoy5cvL9artJs1a0bPnj0ZOXIk33zzDd9++y0jR44sNMLcs2dPWrVqxdChQ9m9ezfffPMNw4cPp1u3bpZ5yiJlJTzQm7WjOvFqxzzWjuqkwlhERGxaiSvcESNG8J///KcsYqkQsbGxJCYm4uvrS9u2bW+5n9atW/Paa6/xyiuv0LJlS1auXMnMmTOL9dn33nuPOnXqcPfddzNgwAAef/xxatSoQdWqVYFL0yM++eQTatasyd13303Pnj1p1KgRH3zwwS3HKyIiIiJFGQUFV88mvLm8vDz69u3L77//TqtWrYrM33jttdesGuDf0U8//YSvry+bN2+mR48e5bZfk8mEm5sbWVlZVrshLz4+noiICM2jquSUS9uhXNoG5dF2KJflp7h1TolvyJs5cyYJCQk0bdoUoMgNeVJyW7du5fz587Rq1YqTJ0/yzDPP4Ofnx913313RoYmIiIj8rZS4OI6NjeXdd98lMjKyDML5ezKbzTz//PMcPXqUGjVq0KVLF1auXKm/IEVERETKWYmLYycnJ7p27VoWsfxthYeHEx4eXtFhiIiIiPztlfiGvCeffJIFCxaURSwiIiIiIhWqxCPH33zzDVu3bmXDhg0EBgYW+er/o48+slpwIiIiIiLlqcTFsbu7OwMHDiyLWEREREREKlSJi+OlS5eWRRwVqqCggFGjRrFmzRrOnDnDt99+S5s2bay+n/T0dBo2bGjpPykpie7du3PmzBnc3d1vuV8/Pz8mTJjAhAkTrBariIiIyN+RbbzmrpQ2btxIXFwcGzZs4OTJk7Rt25Z169aV+X67dOnCyZMncXNzK1U/O3fuZOTIkZZlwzDKJX4RERERW1PikWOANWvW8OGHH5KRkUFubm6hdbt377ZKYOXpyJEj+Pj40KVLl3Ldr6OjI97epX8Vr5eXlxWiEbm2hNRMFm5N48BJe5Zk7GBMiD/heoW0iIjYqBKPHM+fP59HHnmEOnXq8O2339KhQwc8PT05evQovXv3LosYy1RkZCTjxo0jIyMDwzDw8/MDYMCAAYWWjxw5wj333EOdOnVwcXHhjjvuYPPmzYX6utaIrbu7O3Fxcdfcd1JSEoZhcPbsWQDi4uJwd3dnw4YNNG3aFGdnZ+69916ys7NZtmwZfn5+1KxZk/Hjx5OXl2fpx8/Pj7lz51p+vlb8IrciITWTUctT2HvcRG6+wd7jJqJWpJCQmlnRoYmIiJSJEo8cL1q0iLfeeosHH3yQuLg4nnnmGRo1asTUqVP57bffyiLGMjVv3jwaN27MW2+9xc6dO7G3t6d27dosXbqUXr16YW9vD8D58+eJiIhgxowZODk58d5779GvXz8OHjxI/fr1rRZPdnY28+fPZ/Xq1Zw7d46BAwcyYMAA3N3diY+P5+jRowwaNIiuXbsyePDgIp/fuXPnNeO/lpycHHJycizLJpMJuPRSErPZXOpjudKHNfqSirFwa1qRtoICWLgtjZAAzwqISEpL16VtUB5th3JZfop7jktcHGdkZFimH1SrVo1z584B8NBDD9GpUydef/31knZZodzc3KhRowb29vaFpji4u7sXWm7dujWtW7e2LP/rX//i448/Zv369YwdO9Zq8ZjNZt544w0aN24MwL333svy5cv5+eefcXFxoUWLFnTv3p1t27Zdszi+MsXiz/Ffy8yZM5k2bVqR9k2bNuHs7GyFo7kkMTHRan1J+Tpw0h4o+lr4AyeyiI+PL/+AxGp0XdoG5dF2KJdlLzs7u1jblbg49vb25rfffqNBgwbUr1+fHTt20Lp1a44dO0ZBQUGJA60szp8/T0xMDJ9++iknT57k4sWL/P7772RkZFh1P87OzpbCGKBOnTr4+fnh4uJSqO3UqVOl3tfkyZOJjo62LJtMJnx9fQkLC8PV1bXU/ZvNZhITEwkNDdWrsCupJRk72HvcVKS9WV03IiI6VUBEUlq6Lm2D8mg7lMvyc+Ub8pspcXEcEhLC+vXradu2LY888ghPPfUUa9asYdeuXTb9/OOJEyeSmJjIv//9b5o0aUK1atW49957C92QaBhGkT8QSvo1yZ8vDMMwrtmWn59fwiMoysnJCScnp2vGYM0L1Nr9SfkZE+JP1IoUrv61NgwY291fOa3kdF3aBuXRdiiXZa+457fExfFbb71lKczGjBmDp6cn//3vf/nHP/7BqFGjStrdX5KDg0OhG94Atm/fTmRkJAMGDAAujSSnp6cX2sbLy4uTJ09altPS0oo9hG9N14pf5FaEB3qzeFg7Fm5L48CJLJrVdWNsd3/C9LQKERGxUSUqji9evMjLL7/Mo48+Sr169QB44IEHeOCBB8okuIri5+fHli1b6Nq1K05OTtSsWRN/f38++ugj+vXrh2EYvPDCC0VGb0NCQnj99dfp3LkzeXl5PPvssxXyV+C14he5VeGB3oQEeBIfH09ERCeNbIiIiE0r0aPcqlSpwuzZs7l48WJZxfOXEBsbS2JiIr6+vrRt2xaA1157jZo1a9KlSxf69etHeHg4t99+e5HP+fr6ctdddzFkyBAmTpxo1RvbShO/iIiIiNycUVDCu+juueceBg4cyMMPP1xWMUkFMZlMuLm5kZWVZbUb8i6NNkZotLGSUy5th3JpG5RH26Fclp/i1jklnnPcu3dvnnvuOb7//nvatWtH9erVC63/xz/+UfJoRURERET+AkpcHD/xxBPApWkGf2YYhm4EExEREZFKq8TFsTUeISYiIiIi8ldUohvyRERERERsWYlHjgEuXLjA559/TkZGRqGXYACMHz/eKoGJiIiIiJS3EhfH3377LREREWRnZ3PhwgU8PDw4ffo0zs7O1K5dW8WxiIiIiFRaJZ5W8dRTT9GvXz/OnDlDtWrV2LFjBz/88APt2rXj3//+d4n6KigoYOTIkXh4eGAYBnv27ClpOCIiIiIiVlPi4njPnj08/fTT2NnZYW9vT05ODr6+vsyePZvnn3++RH1t3LiRuLg4NmzYwMmTJ2nZsmVJw6kUgoODmTBhQkWHISIiIiI3UeLi2MHBATu7Sx+rXbs2GRkZALi5ufHjjz+WqK8jR47g4+NDly5d8Pb2pkqVW5oCbRMKCgps/s2DUjklpGYyaPEOJiXbM2jxDhJSMys6JBERkTJT4uK4bdu27Ny5E4Bu3boxdepUVq5cyYQJE0o08hsZGcm4cePIyMjAMAz8/PwIDg5m3LhxTJgwgZo1a1KnTh3efvttLly4wCOPPEKNGjVo0qQJn332maWfvLw8RowYQcOGDalWrRpNmzZl3rx5lvV//PEHgYGBjBw50tJ25MgRatSowbvvvovJZKJatWqF+gT4+OOPqVGjBtnZ2XTp0oVnn3220PpffvkFBwcHvvjiCwAWLVqEv78/VatWpU6dOtx7772W4/z888+ZN28ehmFgGAbp6ekkJSVhGAafffYZ7dq1w8nJia+++or8/HxmzpxpOZ7WrVuzZs0ay37PnDnD0KFD8fLyolq1avj7+7N06VIAcnNzGTt2LD4+PlStWpUGDRowc+bMYudE5M8SUjMZtTyFvcdN5OYb7D1uImpFigpkERGxWSUeqn355Zc5d+4cADNmzGD48OGMHj0af39/3n333WL3M2/ePBo3bsxbb73Fzp07sbe357777mPZsmU888wzfPPNN3zwwQeMHj2ajz/+mAEDBvD8888zZ84cHnroITIyMnB2diY/P5969erxn//8B09PT/773/8ycuRIfHx8uP/++6latSorV66kY8eO9OnTh759+zJs2DBCQ0N59NFHAejbty+rVq2id+/elvhWrlxJ//79cXZ2ZujQocyePZtZs2ZhGAYAH3zwAXXr1uWuu+5i165djB8/nuXLl9OlSxd+++03vvzyS8txHjp0iJYtWzJ9+nQAvLy8SE9PB+C5557j3//+N40aNaJmzZrMnDmTFStWsHjxYvz9/fniiy8YNmwYXl5edOvWjRdeeIF9+/bx2WefUatWLQ4fPszvv/8OwPz581m/fj0ffvgh9evX58cff7zhaH5OTg45OTmWZZPJBFx6laXZbC52Lq/nSh/W6EsqxsKtaUXaCgpg4bY0QgI8KyAiKS1dl7ZBebQdymX5Ke45NgoKCgrKOJbrmjt3LnPnzrUUisHBweTl5VkKy7y8PNzc3Bg4cCDvvfceAJmZmfj4+PD111/TqVOna/Y7duxYMjMzC424vvrqq8yePZsHHniAtWvX8v333+Ppeek/7uvWreOhhx7i559/xtnZGZPJRJ06dfj444/p1asXv/zyC3Xr1mXr1q3cddddAHTp0oW7776bWbNm8dFHH/HII4/w008/UaNGjSLxBAcH06ZNG+bOnWtpS0pKonv37qxbt4577rkHuFSsenh4sHnzZjp37mzZ9rHHHiM7O5tVq1bxj3/8g1q1al3zD5Hx48eTmprK5s2bLUX8jcTExDBt2rQi7atWrcLZ2fmmnxfbNynZntz8or9LjnYFvNpRb8MUEZHKIzs7myFDhpCVlYWrq+t1t7vlSb6nTp3i4MGDADRr1gwvL69b7aqQoKAgy8/29vZ4enrSqlUrS1udOnUs+79i4cKFvPvuu2RkZPD777+Tm5tLmzZtCvX79NNPs27dOl5//XU+++wzS2EMEBERgYODA+vXr7cUz66urvTs2RO4NNIbFhbGypUrueuuuzh27Bhff/01b775JgChoaE0aNCARo0a0atXL3r16sWAAQOKVWC2b9/e8vPhw4fJzs4mNDS00Da5ubm0bdsWgNGjRzNo0CB2795NWFgY/fv3p0uXLsClKRyhoaE0bdqUXr160bdvX8LCwq6778mTJxMdHW1ZNplM+Pr6EhYWdsNfmuIym80kJiYSGhqKg4NDqfuT8rckYwd7j5uKtDer60ZExLX/OJW/Nl2XtkF5tB3KZfm58g35zZS4OD537hxPPPEEq1evJi/v0siRvb09gwcPZuHChbi5uZW0y0L+/IthGEahtisjoldeY7169WomTpxIbGwsnTt3pkaNGrz66qskJycX6ufUqVMcOnQIe3t70tLS6NWrl2Wdo6Mj9957L6tWreKBBx5g1apVDB48uNANgkOHDmX8+PEsWLCAVatW0apVK0vRXqNGDXbv3k1SUhKbNm1i6tSpxMTEsHPnTtzd3W94vNWrV7f8fP78eQA+/fRTbrvttkLbOTk5AdC7d29++OEH4uPjSUxMpEePHowZM4Z///vf3H777Rw7dozPPvuMzZs3c//999OzZ89CI+h/7vNKv1dzcHCw6gVq7f6k/IwJ8SdqRQpXf79kGDC2u79yWsnpurQNyqPtUC7LXnHPb4lvyHvsscdITk5mw4YNnD17lrNnz7JhwwZ27drFqFGjShxoaW3fvp0uXbrwxBNP0LZtW5o0acKRI0eKbPfoo4/SqlUrli1bxrPPPsv+/fsLrR86dCgbN24kNTWVrVu3MnTo0ELr77nnHv744w82btzIqlWriqyvUqUKPXv2ZPbs2ezdu5f09HS2bt0KXCq+r/whcSMtWrTAycmJjIwMmjRpUuifr6+vZTsvLy8efvhhVqxYwdy5c3nrrbcs61xdXRk8eDBvv/02H3zwAWvXruW33367+YkUuYbwQG8WD2tHUD1XHO0KCKrnypvD2hEW6F3RoYmIiJSJEo8cb9iwgYSEBO68805LW3h4OG+//Xah0djy4u/vz3vvvUdCQgINGzZk+fLl7Ny5k4YNG1q2WbhwIV9//TV79+7F19eXTz/9lKFDh7Jjxw4cHR0BuPvuu/H29mbo0KE0bNiQjh07FtpP9erV6d+/Py+88AL79+/nwQcftKzbsGEDR48e5e6776ZmzZrEx8eTn59P06ZNAfDz8yM5OZn09HRcXFzw8PC45rHUqFGDiRMn8tRTT5Gfn8+dd95JVlYW27dvx9XVlYcffpipU6fSrl07AgMDycnJYcOGDTRv3hyA1157DR8fH9q2bYudnR3/+c9/8Pb2vunotciNhAd6ExLgSXx8PBERnTSyISIiNq3EI8eenp7XnDrh5uZGzZo1rRJUSYwaNYqBAwcyePBgOnbsyK+//soTTzxhWX/gwAEmTZrEokWLLKOvixYt4vTp07zwwguW7QzD4MEHH+S7774rMip8xdChQ/nuu++46667qF+/vqXd3d2djz76iJCQEJo3b87ixYt5//33CQwMBGDixInY29vTokULvLy8LM+GvpZ//etfvPDCC8ycOZPmzZvTq1cvPv30U0ux7+joyOTJkwkKCuLuu+/G3t6e1atXA5eK69mzZ9O+fXvuuOMO0tPTiY+PtzyXWkRERERurMRPq3jrrbf4z3/+w/Lly/H2vvTVamZmJg8//DADBw6skKkVYh0mkwk3N7eb3sVZXGaz+fJoY4RGGys55dJ2KJe2QXm0Hcpl+SlunVPiaRVvvPEGhw8fpn79+pbR04yMDJycnPjll18sT3AA2L179y2ELiIiIiJSMUpcHPfv378MwhARERERqXglLo5ffPHFsohDRERERKTC6U4tEREREZHLVByLiIiIiFym4lhERERE5DIVxyIiIiIil9lscVxQUMDIkSPx8PDAMAz27Nlzw+2TkpIwDIOzZ8+WS3wiIiIi8tdT4qdV5OXlERcXx5YtWzh16hT5+fmF1m/dutVqwZXGxo0biYuLIykpiUaNGlGrVq0KiyUuLo4JEyao8JZKKSE1k4Vb0zhw0p4lGTsYE+JPeKB3RYclIiJSJkpcHD/55JPExcXRp08fWrZsiWEYZRFXqR05cgQfHx+6dOlS0aEUW25uLo6OjhUdhohFQmomo5anXF4y2HvcRNSKFBYPa6cCWUREbFKJi+PVq1fz4YcfEhERURbxWEVkZCTLli0DwDAMGjRowMGDB5k0aRKrV6/GZDLRvn175syZwx133FHosykpKTz77LPs27ePNm3asHTpUpo2bXrTfX733XdMmDCBXbt2YRgG/v7+vPnmm5w/f55HHnnEEgtcelZ0TEwMfn5+jBgxgrS0NNatW8fAgQOJi4vjq6++YvLkyezatYtatWoxYMAAZs6cSfXq1QFYtGgRc+bM4ccff8TNzY277rqLNWvWALBmzRqmTZvG4cOHcXZ2pm3btnzyySeWz14tJyeHnJwcy7LJZAIuvcrSbDaX9LQXcaUPa/QlFWPh1rQibQUFsHBbGiEBnhUQkZSWrkvboDzaDuWy/BT3HBsFBQUFJem4bt26JCUlERAQcEuBlYesrCzmz5/PW2+9xc6dO7G3t+ell15izZo1vPPOOzRo0IDZs2ezfv16Dh8+jIeHB0lJSXTv3p2OHTvyyiuv4OXlRVRUFHl5eWzfvv2m+2zZsiVt27ZlypQp2Nvbs2fPHgICAmjevDlvvPEGU6dO5eDBgwC4uLjg4uKCn58fZ86cYerUqYXePNi6dWteeukl+vTpwy+//MLYsWNp3bo1S5cuZdeuXXTq1Inly5fTpUsXfvvtN7788kvGjx/PyZMnqV+/PrNnz2bAgAGcO3eOL7/8kuHDh+Pi4lIk5piYGKZNm1akfdWqVTg7O996AsRmTEq2Jze/6LdDjnYFvNoxrwIiEhERuTXZ2dkMGTKErKwsXF1dr7tdiYvj2NhYjh49yuuvv/6XnVIBMHfuXObOnUt6ejoXLlygZs2axMXFMWTIEODSXw9+fn5MmDCBSZMmWYrjzZs306NHDwDi4+Pp06cPv//+O1WrVr3h/lxdXVmwYAEPP/xwkXXXm3Ps5+dH27Zt+fjjjy1tjz32GPb29rz55puWtq+++opu3bpx4cIF4uPjeeSRR/jpp5+oUaNGof52795Nu3btSE9Pp0GDBjc9R9caOfb19eX06dM3/KUpLrPZTGJiIqGhoTg4OJS6Pyl/gxbvYO9xU5H2oHqurB3VqQIiktLSdWkblEfboVyWH5PJRK1atW5aHJd4WsVXX33Ftm3b+OyzzwgMDCySyI8++qjk0ZaxI0eOYDab6dq1q6XNwcGBDh06sH///kLbBgUFWX728fEB4NSpU9SvX/+G+4iOjuaxxx5j+fLl9OzZk/vuu4/GjRvfNLb27dsXWv7uu+/Yu3cvK1eutLQVFBSQn5/PsWPHCA0NpUGDBjRq1IhevXrRq1cvBgwYgLOzM61bt6ZHjx60atWK8PBwwsLCuPfee6lZs+Y19+3k5ISTk1ORdgcHB6teoNbuT8rPmBB/olakcPWf0IYBY7v7K6eVnK5L26A82g7lsuwV9/yW+FFu7u7uDBgwgG7dulGrVi3c3NwK/avsrj5xV0bG//xEjmuJiYkhNTWVPn36sHXrVlq0aFFoRPh6/jwX+Pz584waNYo9e/ZY/n333XekpaXRuHFjatSowe7du3n//ffx8fFh6tSptG7dmrNnz2Jvb09iYiKfffYZLVq0YMGCBTRt2pRjx46V8CyIXBIe6M3iYe0IqueKo10BQfVceXNYO8J0M56IiNioEo8cL126tCziKFONGzfG0dGR7du3W6YbmM1mdu7cyYQJE6y2n4CAAAICAnjqqad48MEHWbp0KQMGDMDR0ZG8vOLNz7z99tvZt28fTZo0ue42VapUoWfPnvTs2ZMXX3wRd3d3tm7dysCBAzEMg65du9K1a1emTp1KgwYN+Pjjj4mOjrbWYcrfTHigNyEBnsTHxxMR0UkjGyIiYtNKXBxf8csvv1huMGvatCleXl5WC8raqlevzujRo5k0aRIeHh6Wm9ays7MZMWJEqfv//fffmTRpEvfeey8NGzbkp59+YufOnQwaNAi4NLf4/PnzbNmyhdatW+Ps7HzdG96effZZOnXqxNixY3nssceoXr06+/btIzExkddff50NGzZw9OhR7r77bmrWrEl8fDz5+fk0bdqU5ORktmzZQlhYGLVr1yY5OZlffvmF5s2bl/oYRURERP4OSlwcX7hwgXHjxvHee+9ZphvY29szfPhwFixY8Jd9ysGsWbPIz8/noYce4ty5c7Rv356EhITrzsctCXt7e3799VeGDx/Ozz//TK1atRg4cKDlSRBdunQhKiqKwYMH8+uvv1oe5XYtQUFBfP7550yZMoW77rqLgoICGjduzODBg4FL01o++ugjYmJi+OOPP/D39+f9998nMDCQ/fv388UXXzB37lxMJhMNGjQgNjaW3r17l/oYRURERP4OSvy0ilGjRrF582Zef/11yw1uX331FePHjyc0NJQ33nijTAKVsmcymXBzc7vpXZzFZTabL38VH6Gv4is55dJ2KJe2QXm0Hcpl+SlunVPikeO1a9eyZs0agoODLW0RERFUq1aN+++/X8WxiIiIiFRaJX5aRXZ2NnXq1CnSXrt2bbKzs60S1F9RYGCg5eUdf/539WPXRERERKTyKvHIcefOnXnxxRd57733LC/G+P3335k2bRqdO3e2eoB/FfHx8dd97eC1/lgQERERkcqnxMXxvHnzCA8Pp169erRu3Rq49OKKqlWrkpCQYPUA/yqK88Y5EREREancSlwct2zZkrS0NFauXMmBAwcAePDBBxk6dCjVqlWzeoAiIiIiIuXllp5z7OzszOOPP27tWP42CgoKGDVqFGvWrOHMmTN8++23tGnTpqLDEhEREfnbK1ZxvH79enr37o2DgwPr16+/4bb/+Mc/rBKYLdu4cSNxcXEkJSXRqFEjatWqZZV+k5KSiI6OJjU1FV9fX/75z38SGRlplb5FRERE/g6KVRz379+fzMxMateuTf/+/a+7nWEYxX5N8t/ZkSNH8PHxoUuXLlbr89ixY/Tp04eoqChWrlzJli1beOyxx/Dx8SE8PNxq+5G/n4TUTBZuTePASXuWZOxgTIg/4YHeFR2WiIhImSjWo9zy8/OpXbu25efr/VNhfHORkZGMGzeOjIwMDMPAz8+P4OBgxo8fzzPPPIOHhwfe3t5F3qB39uxZHnvsMby8vHB1dSUkJITvvvvOsn7x4sU0bNiQ2NhYmjdvztixY7n33nuZM2dOOR+h2JKE1ExGLU9h73ETufkGe4+biFqRQkJqZkWHJiIiUiZKPOf4vffeY/DgwTg5ORVqz83NZfXq1QwfPtxqwdmiefPm0bhxY9566y127tyJvb099913H8uWLSM6Oprk5GS+/vprIiMj6dq1K6GhoQDcd999VKtWjc8++ww3NzfefPNNevTowaFDh/Dw8ODrr7+mZ8+ehfYVHh7OhAkTrhtLTk4OOTk5lmWTyQRcelvP9R5bVxJX+rBGX1IxFm5NK9JWUAALt6UREuBZARFJaem6tA3Ko+1QLstPcc9xiV8fbW9vz8mTJy0jyVf8+uuv1K5dW6PHxTB37lzmzp1Leno6AMHBweTl5fHll19atunQoQMhISHMmjWLr776ij59+nDq1KlCf5Q0adKEZ555hpEjRxIQEMAjjzzC5MmTLevj4+Pp06cP2dnZ13ySSExMDNOmTSvSvmrVKpydna14xFJZTUq2JzffKNLuaFfAqx11rYuISOWRnZ3NkCFDrP/66IKCAgyj6H8sf/rpJ9zc3EranVwWFBRUaNnHx4dTp04Bl54jff78eTw9C4/U/f777xw5cuSW9zl58mSio6MtyyaTCV9fX8LCwm74S1NcZrOZxMREQkND9b74SmpJxg72HjcVaW9W142IiE4VEJGUlq5L26A82g7lsvxc+Yb8ZopdHLdt2xbDMDAMgx49elClyv//aF5eHseOHaNXr14lj1QAilwQhmGQn58PwPnz5/Hx8SEpKanI59zd3QHw9vbm559/LrTu559/xtXV9brPn3ZycioyPeZKLNa8QK3dn5SfMSH+RK1I4ervlwwDxnb3V04rOV2XtkF5tB3KZdkr7vktdnF85SkVe/bsITw8HBcXF8s6R0dH/Pz8GDRoUMmilGK5/fbbyczMpEqVKvj5+V1zm86dOxMfH1+oLTEx0aZf6S1lLzzQm8XD2rFwWxoHTmTRrK4bY7v7E6anVYiIiI0qdnH84osvAuDn58fgwYOpWrVqmQUlhfXs2ZPOnTvTv39/Zs+eTUBAACdOnODTTz9lwIABtG/fnqioKF5//XWeeeYZHn30UbZu3cqHH37Ip59+WtHhSyUXHuhNSIAn8fHxRER00siGiIjYtGI9yu1qDz/8sArjcmYYBvHx8dx999088sgjBAQE8MADD/DDDz9Qp04dABo2bMinn35KYmIirVu3JjY2lnfeeUfPOBYREREpgRLfkJeXl8ecOXP48MMPycjIIDc3t9D63377zWrB2aoJEyYUesTateYSr1u3rtByjRo1mD9/PvPnz79uv8HBwXz77bdWilJERETk76fEI8fTpk3jtddeY/DgwWRlZREdHc3AgQOxs7Mr8uIKEREREZHKpMTF8cqVK3n77bd5+umnqVKlCg8++CDvvPMOU6dOZceOHWURo4iIiIhIuShxcZyZmUmrVq0AcHFxISsrC4C+ffvq5i8RERERqdRKXBzXq1ePkydPAtC4cWM2bdoEwM6dO6/5zFwRERERkcqixMXxgAED2LJlCwDjxo3jhRdewN/fn+HDh/Poo49aPUARERERkfJS4qdVzJo1y/Lz4MGDqV+/Pl9//TX+/v7069fPqsGJiIiIiJSnEhfHf9a5c2e9hU1EREREbEKJp1UsW7as0I13zzzzDO7u7nTp0oUffvjBqsHdqoKCAkaOHImHhweGYbBnz56KDom4uDjc3d0rOgwRERERuYESF8cvv/wy1apVA+Drr7/m9ddfZ/bs2dSqVYunnnrK6gHeio0bNxIXF8eGDRs4efIkLVu2rOiQRCqthNRMBi3ewaRkewYt3kFCamZFhyQiIlJmSjyt4scff6RJkybApbe43XvvvYwcOZKuXbsSHBxs7fhuyZEjR/Dx8aFLly4VHcpfgtlsxsHBoaLDkEooITWTUctTLi8Z7D1uImpFCouHtSM80LtCYxMRESkLJS6OXVxc+PXXX6lfvz6bNm0iOjoagKpVq/L7779bPcCSioyMZNmyZQAYhkGDBg3w8/OzjB4vX74cBwcHRo8ezfTp0zEMA4BFixYxZ84cfvzxR9zc3LjrrrtYs2YNAPn5+bzyyiu89dZbZGZmEhAQwAsvvMC9994LXHr9c/fu3dmwYQOTJ0/m0KFDtGnThnfeeafIqPW6deuYNGkSP/74I926deOdd97B19fXsn7WrFnMmTOH7Oxs7r//fry8vNi4caNlasjOnTt5/vnn+fbbbzGbzbRp04Y5c+Zw++23W/owDINFixbx2WefsWXLFiZNmnTNtxfm5OSQk5NjWTaZTMClYtpsNpcmDZZ+rv5fqXwWbk0r0lZQAAu3pRES4FkBEUlp6bq0Dcqj7VAuy09xz3GJi+PQ0FAee+wx2rZty6FDh4iIiAAgNTUVPz+/knZndfPmzaNx48a89dZb7Ny5E3t7e+677z6WLVvGiBEj+Oabb9i1axcjR46kfv36PP744+zatYvx48ezfPlyunTpwm+//caXX35p6XPmzJmsWLGCxYsX4+/vzxdffMGwYcPw8vKiW7dulu0mTZrEvHnz8Pb25vnnn6dfv34cOnTIMmqbnZ3NjBkzeO+993B0dOSJJ57ggQceYPv27QB8+OGHxMTEsHDhQu68806WL1/O/PnzadSokWUf586d4+GHH2bBggUUFBQQGxtLREQEaWlp1KhRw7JdTEwMs2bNYu7cuVSpcu00z5w5k2nTphVp37RpE87OzqVLxFUSExOt1peUrwMn7QGjaPuJLOLj48s/ILEaXZe2QXm0Hcpl2cvOzi7WdkZBQUFBSTo+e/Ys//znP/nxxx8ZPXo0vXr1AuDFF1/E0dGRKVOmlDxaK5s7dy5z584lPT0dgODgYE6dOkVqaqplpPi5555j/fr17Nu3j48++ohHHnmEn376qVCBCZdGVz08PNi8eXOhp3I89thjZGdns2rVKsvI8erVqxk8eDAAv/32G/Xq1SMuLo7777+fuLg4HnnkEXbs2EHHjh0BOHDgAM2bNyc5OZkOHTrQpUsX2rZty8KFCy376dSpE3/88cd1byrMz8/H3d2dVatW0bdvX+DSyPGECROYM2fODc/TtUaOfX19OX36NK6ursU40zdmNptJTEwkNDRU0zoqqUGLd7D3uKlIe1A9V9aO6lQBEUlp6bq0Dcqj7VAuy4/JZKJWrVpkZWXdsM4p8cixu7s7r7/+epH2a41A/pV06tTJUhjDpUfQxcbGkpeXR2hoKA0aNKBRo0b06tWLXr16MWDAAJydnTl8+DDZ2dmEhoYW6i83N5e2bdsWaru6ePbw8KBp06bs37/f0lalShXuuOMOy3KzZs1wd3dn//79dOjQgf379xMVFVWkz23btlmWf/75Z/75z3+SlJTEqVOnyMvLIzs7m4yMjEKfa9++/U3PiZOT0zXfaujg4GDVC9Ta/Un5GRPiT9SKFK7+E9owYGx3f+W0ktN1aRuUR9uhXJa94p7fYhXHe/fupWXLltjZ2bF3794bbhsUFFSsHf+V1KhRg927d5OUlMSmTZuYOnUqMTEx7Ny5k/PnzwPw6aefcttttxX6XEW8Lvvhhx/m119/Zd68eTRo0AAnJyc6d+5Mbm5uoe2qV69e7rGJ7QkP9GbxsHYs3JbGgRNZNKvrxtju/oTpZjwREbFRxSqO27RpQ2ZmJrVr16ZNmzYYhsHVszGuLBuGQV5eXpkFWxrJycmFlnfs2IG/vz/29vbApVHdnj170rNnT1588UXc3d3ZunUroaGhODk5kZGRUWh+8bXs2LGD+vXrA3DmzBkOHTpE8+bNLesvXrzIrl276NChAwAHDx7k7Nmzlm2uTLEYPnx4oT6vtn37dhYtWmSZ6/3jjz9y+vTpWzklIsUSHuhNSIAn8fHxRER00siGiIjYtGIVx8eOHcPLy8vyc2WUkZFBdHQ0o0aNYvfu3SxYsIDY2FgANmzYwNGjR7n77rupWbMm8fHx5Ofn07RpU2rUqMHEiRN56qmnyM/P58477yQrK4vt27fj6urKww8/bNnH9OnT8fT0pE6dOkyZMoVatWrRv39/y3oHBwfGjRvH/PnzqVKlCmPHjqVTp06WYvnJJ58kMjKS9u3b07VrV1auXElqamqhG/L8/f1Zvnw57du3x2QyMWnSJMtzp0VERESkdIpVHDdo0OCaP1cmw4cP5/fff6dDhw7Y29vz5JNPMnLkSODSPOqPPvqImJgY/vjjD/z9/Xn//fcJDAwE4F//+hdeXl7MnDmTo0eP4u7uzu23387zzz9faB+zZs3iySefJC0tjTZt2vB///d/ODo6WtY7Ozvz7LPPMmTIEI4fP85dd93FkiVLLOsHDx7MkSNHeOaZZ/jjjz8YNGgQo0ePJiEhwbLNkiVLGDlyJLfffju+vr68/PLLTJw4sSxPnYiIiMjfRomfVgFw4sQJvvrqK06dOkV+fn6hdePHj7dacNYSHBxMmzZtmDt3bpn0f+VpFWfOnLH6K6JjYmJYt25dubwC22Qy4ebmdtO7OIvLbDZf/io+Ql/FV3LKpe1QLm2D8mg7lMvyU9w6p8RPq4iLi2PUqFE4Ojri6elZ6AkQhmH8JYtjEREREZHiKHFx/MILLzB16lQmT56MnZ1dWcQkIiIiIlIhSlwcZ2dn88ADD1SqwjgpKalM+w8ODuYWZqcUS0xMzDVf/SwiIiIi1lfiCnfEiBH85z//KYtYREREREQqVIlHjmfOnEnfvn3ZuHEjrVq1KjJ5/LXXXrNacCIiIiIi5emWiuOEhASaNm0KUOSGPBERERGRyqrExXFsbCzvvvsukZGRZRDOX0NBQQGjRo1izZo1nDlzhm+//ZY2bdpUdFgiIiIiUsZKXBw7OTnRtWvXsojlL2Pjxo3ExcWRlJREo0aNqFWr1nW3jYyM5OzZs6xbt678AhQRERGRMlHiG/KefPJJFixYUBax/GUcOXIEHx8funTpgre3N1WqlPhviCLMZrMVIhMpfwmpmQxavINJyfYMWryDhNTMig5JRESkzJS4OP7mm29YtmwZjRo1ol+/fgwcOLDQv8ouMjKScePGkZGRgWEY+Pn5sWbNGlq1akW1atXw9PSkZ8+eXLhwgZiYGJYtW8Ynn3yCYRgYhkFSUhLp6ekYhsEHH3xAt27dqFq1KitXrgTg3XffJTAwECcnJ3x8fBg7dqxl36+99hqtWrWievXq+Pr68sQTT3D+/HnL+h9++IF+/fpRs2ZNqlevTmBgIPHx8Zb1//vf/+jduzcuLi7UqVOHhx56iNOnT5ffyRObk5CayajlKew9biI332DvcRNRK1JUIIuIiM0q8ZCou7u7TRTB1zNv3jwaN27MW2+9xc6dOzGbzTRq1IjZs2czYMAAzp07x5dffklBQQETJ05k//79mEwmli5dCoCHhwcnTpwA4LnnniM2Npa2bdtStWpV3njjDaKjo5k1axa9e/cmKyuL7du3W/ZtZ2fH/PnzadiwIUePHuWJJ57gmWeeYdGiRQCMGTOG3NxcvvjiC6pXr86+fftwcXEB4OzZs4SEhPDYY48xZ84cfv/9d5599lnuv/9+tm7des1jzcnJIScnx7JsMpmAS6Pc1hjpvtKHRs0rr4Vb04q0FRTAwm1phAR4VkBEUlq6Lm2D8mg7lMvyU9xzbBSU1dsrKrG5c+cyd+5c0tPT2b17N+3atSM9PZ0GDRoU2fZac47T09Np2LAhc+fO5cknn7S033bbbTzyyCO89NJLxYpjzZo1REVFWUZ/g4KCGDRoEC+++GKRbV966SW+/PJLEhISLG0//fQTvr6+HDx4kICAgCKfiYmJYdq0aUXaV61ahbOzc7FiFNs2Kdme3PyiT6FxtCvg1Y55FRCRiIjIrcnOzmbIkCFkZWXh6up63e1KP5nWxrVu3ZoePXrQqlUrwsPDCQsL495776VmzZo3/Wz79u0tP586dYoTJ07Qo0eP626/efNmZs6cyYEDBzCZTFy8eJE//viD7OxsnJ2dGT9+PKNHj2bTpk307NmTQYMGERQUBMB3333Htm3bLCPJVzty5Mg1i+PJkycTHR1tWTaZTPj6+hIWFnbDX5riMpvNJCYmEhoaWuR52FI5LMnYwd7jpiLtzeq6ERHRqQIiktLSdWkblEfboVyWnyvfkN9MsYrj22+/nS1btlCzZk3atm17w+cZ7969u3gRVhL29vYkJiby3//+l02bNrFgwQKmTJlCcnIyDRs2vOFnq1evbvm5WrVqN9w2PT2dvn37Mnr0aGbMmIGHhwdfffUVI0aMIDc3F2dnZx577DHCw8P59NNP2bRpEzNnziQ2NpZx48Zx/vx5+vXrxyuvvFKkbx8fn2vu08nJCScnpyLtDg4OVr1Ard2flJ8xIf5ErUjh6u+XDAPGdvdXTis5XZe2QXm0Hcpl2Svu+S1WcXzPPfdYiqh77rnnb/eyD8Mw6Nq1K127dmXq1Kk0aNCAjz/+mOjoaBwdHcnLu/nXyzVq1MDPz48tW7bQvXv3IutTUlLIz88nNjYWO7tL90l++OGHRbbz9fUlKiqKqKgoJk+ezNtvv824ceO4/fbbWbt2LX5+flZ5uoYIQHigN4uHtWPhtjQOnMiiWV03xnb3JyzQu6JDExERKRPFqqKunuMaExNTVrH8JSUnJ7NlyxbCwsKoXbs2ycnJ/PLLLzRv3hwAPz8/EhISOHjwIJ6enri5uV23r5iYGKKioqhduza9e/fm3LlzbN++nXHjxtGkSRPMZjMLFiygX79+bN++ncWLFxf6/IQJE+jduzcBAQGcOXOGbdu2WeIYM2YMb7/9Ng8++CDPPPMMHh4eHD58mNWrV/POO+9gb29fdidJbFp4oDchAZ7Ex8cTEdFJIxsiImLTSvwot0aNGvHrr78WaT979iyNGjWySlB/Ja6urnzxxRdEREQQEBDAP//5T2JjY+nduzcAjz/+OE2bNqV9+/Z4eXkVevrEnz388MPMnTuXRYsWERgYSN++fUlLu/Q0gNatW/Paa6/xyiuv0LJlS1auXMnMmTMLfT4vL48xY8bQvHlzevXqRUBAgOVJFnXr1mX79u3k5eURFhZGq1atmDBhAu7u7paRaBERERG5sRI/rcLOzo7MzExq165dqP3nn3/G19eX3NxcqwYo5cdkMuHm5nbTuziLy2w2Xx5tjNBoYyWnXNoO5dI2KI+2Q7ksP8Wtc4o9OXX9+vWWnxMSEgpNH8jLy2PLli03vUFNREREROSvrNjFcf/+/YFLN6c9/PDDhdY5ODjg5+dHbGysVYMTERERESlPxS6O8/PzAWjYsCE7d+6kVq1aZRaUiIiIiEhFKPEzv44dO1YWcYiIiIiIVLhbeozBli1b6Nu3L40bN6Zx48b07duXzZs3Wzs2EREREZFyVeLieNGiRfTq1YsaNWrw5JNP8uSTT+Lq6kpERAQLFy4sixhFRERERMpFiYvjl19+mTlz5vD+++8zfvx4xo8fz6pVq5gzZw4vv/xyWcRYbgoKChg5ciQeHh4YhsGePXsqOqRSCQ4OZsKECRUdhoiIiEilUeLi+OzZs/Tq1atIe1hYGFlZWVYJqqJs3LiRuLg4NmzYwMmTJ2nZsuV1t42MjLQ8wUNEREREbEOJi+N//OMffPzxx0XaP/nkE/r27WuVoCrKkSNH8PHxoUuXLnh7e1OlSonvVyzCbDZbITKRipOQmsmgxTuYlGzPoMU7SEjNrOiQREREykyJi+MWLVowY8YM+vTpw0svvcRLL71E3759mTFjBi1btmT+/PmWf5VJZGQk48aNIyMjA8Mw8PPzY82aNbRq1Ypq1arh6elJz549uXDhAjExMSxbtoxPPvkEwzAwDIOkpCTS09MxDIMPPviAbt26UbVqVVauXAnAu+++S2BgIE5OTvj4+DB27FjLvjMyMrjnnntwcXHB1dWV+++/n59//tmyPiYmhjZt2rB8+XL8/Pxwc3PjgQce4Ny5c5ZtLly4wPDhw3FxccHHx0fPnBarSEjNZNTyFPYeN5Gbb7D3uImoFSkqkEVExGaVeGh0yZIl1KxZk3379rFv3z5Lu7u7O0uWLLEsG4bB+PHjrRNlOZg3bx6NGzfmrbfeYufOnZjNZho1asTs2bMZMGAA586d48svv6SgoICJEyeyf/9+TCYTS5cuBcDDw4MTJ04A8NxzzxEbG0vbtm2pWrUqb7zxBtHR0cyaNYvevXuTlZXF9u3bgUvPj75SGH/++edcvHiRMWPGMHjwYJKSkizxHTlyhHXr1rFhwwbOnDnD/fffz6xZs5gxYwYAkyZN4vPPP+eTTz6hdu3aPP/88+zevZs2bdpc95hzcnLIycmxLJtMJuDSaLc1Rryv9KHR88pr4da0Im0FBbBwWxohAZ4VEJGUlq5L26A82g7lsvwU9xzrOceXubm5UaNGDezt7fH29mb37t1cvHiRgQMH0qBBAwBatWpl2b5atWrk5OTg7e1dpK8JEyYwcOBAy/JLL73E008/zZNPPmlpu+OOO4BLj8X7/vvvOXbsGL6+vgC89957BAYGsnPnTst2+fn5xMXFUaNGDQAeeughtmzZwowZMzh//jxLlixhxYoV9OjRA4Bly5ZRr169Gx7zzJkzmTZtWpH2TZs24ezsfPOTVkyJiYlW60vK14GT9oBRtP1EFvHx8eUfkFiNrkvboDzaDuWy7GVnZxdru1ueVHv69GkAm31TXuvWrenRowetWrUiPDycsLAw7r33XmrWrHnTz7Zv397y86lTpzhx4oSlaP2z/fv34+vraymM4dLUFXd3d/bv328pjv38/CyFMYCPjw+nTp0CLo0q5+bm0rFjR8t6Dw8PmjZtesM4J0+eTHR0tGXZZDLh6+tLWFgYrq6uNz3OmzGbzSQmJhIaGoqDg0Op+5PytyRjB3uPm4q0N6vrRkREpwqISEpL16VtUB5th3JZfq58Q34zJSqOz549y5QpU/jggw84c+YMADVr1uSBBx7gpZdewt3dvcSB/lXZ29uTmJjIf//7XzZt2sSCBQuYMmUKycnJNGzY8IafrV69uuXnatWqWSWeP18whmFYXul9q5ycnHBycrrmvqx5gVq7Pyk/Y0L8iVqRQkHB/28zDBjb3V85reR0XdoG5dF2KJdlr7jnt9g35P3222907NiRZcuWMWjQIGJjY4mNjWXgwIHExcXRuXNnS8FsKwzDoGvXrkybNo1vv/0WR0dHy5M6HB0dycvLu2kfNWrUwM/Pjy1btlxzffPmzfnxxx/58ccfLW379u3j7NmztGjRolhxNm7cGAcHB5KTky1tZ86c4dChQ8X6vMj1hAd6s3hYO4LqueJoV0BQPVfeHNaOsMCi04lERERsQbFHjqdPn46joyNHjhyhTp06RdaFhYUxffp05syZY/UgK0JycjJbtmwhLCyM2rVrk5yczC+//ELz5s2BS9McEhISOHjwIJ6enri5uV23r5iYGKKioqhduza9e/fm3LlzbN++nXHjxtGzZ09atWrF0KFDmTt3LhcvXuSJJ56gW7duhaZn3IiLiwsjRoxg0qRJeHp6Urt2baZMmYKd3S29HVykkPBAb0ICPImPjyciopNGNkRExKYVu3pat24d//73v4sUxgDe3t7Mnj37ms8/rqxcXV354osviIiIICAggH/+85/ExsbSu3dvAB5//HGaNm1K+/bt8fLysjx94loefvhh5s6dy6JFiwgMDKRv376kpV16CoBhGHzyySfUrFmTu+++m549e9KoUSM++OCDEsX76quvctddd9GvXz969uzJnXfeSbt27W79BIiIiIj8DRkFBVfPJrw+Jycnjhw5ct0nIPz00080adKEP/74w6oBSvkxmUy4ubmRlZVltRvyLo02Rmi0sZJTLm2HcmkblEfboVyWn+LWOcUeOa5Vqxbp6enXXX/s2DE8PDxKFKSIiIiIyF9JsYvj8PBwpkyZQm5ubpF1OTk5vPDCC/Tq1cuqwYmIiIiIlKcS3ZDXvn17/P39GTNmDM2aNaOgoID9+/ezaNEicnJyWL58eVnGKiIiIiJSpopdHNerV4+vv/6aJ554gsmTJ3NlqrJhGISGhvL6668XepGFiIiIiEhlU6KXgDRs2JDPPvuMM2fOWJ620KRJE801FhERERGbcEuvj65ZsyYdOnSwdiwiIiIiIhVKb4mohIKDg5kwYUJFhyEiIiJic1Qc2yA/Pz/mzp1b0WGIiIiIVDoqjkXkhhJSMxm0eAeTku0ZtHgHCamZFR2SiIhImVFxXEldvHiRsWPH4ubmRq1atXjhhRcoKCggODiYH374gaeeegrDMDAMo6JDlUosITWTUctT2HvcRG6+wd7jJqJWpKhAFhERm3VLN+RJxVu2bBkjRozgm2++YdeuXYwcOZL69evz0Ucf0bp1a0aOHMnjjz9+wz5ycnLIycmxLJtMJuDSqyzNZnOpY7zShzX6koqxcGtakbaCAli4LY2QAM8KiEhKS9elbVAebYdyWX6Ke45VHFdSvr6+zJkzB8MwaNq0Kd9//z1z5szh8ccfx97enho1auDt7X3DPmbOnMm0adOKtG/atAlnZ2erxZqYmGi1vqR8HThpDxT99uHAiSzi4+PLPyCxGl2XtkF5tB3KZdnLzs4u1nYqjiupTp06FZoy0blzZ2JjY8nLyyt2H5MnTyY6OtqybDKZ8PX1JSwsDFdX11LHaDabSUxMJDQ0FAcHh1L3J+VvScYO9h43FWlvVteNiIhOFRCRlJauS9ugPNoO5bL8XPmG/GZUHP+NOTk54eTkVKTdwcHBqheotfuT8jMmxJ+oFSlcfiEmAIYBY7v7K6eVnK5L26A82g7lsuwV9/zqhrxKKjk5udDyjh078Pf3x97eHkdHxxKNIItcT3igN4uHtSOoniuOdgUE1XPlzWHtCAu88ZQdERGRykrFcSWVkZFBdHQ0Bw8e5P3332fBggU8+eSTwKXnHH/xxRccP36c06dPV3CkUtmFB3qzdlQnXu2Yx9pRnVQYi4iITdO0ikpq+PDh/P7773To0AF7e3uefPJJRo4cCcD06dMZNWoUjRs3Jicnh4KrvxMXERERketScVwJJSUlWX5+4403iqzv1KkT3333XTlGJCIiImIbNK1CREREROQyFcciIiIiIpepOBYRERERuUzFsYiIiIjIZSqORUREREQuU3EsIiIiInKZiuNKwDAM1q1bV9FhiIiIiNg8Pee4Ejh58iQ1a9as6DBEREREbJ5Gjq0kNze3zPr29vbGycnplj9flrGJiEj5SkjNZNDiHUxKtmfQ4h0kpGZWdEgiNkXF8S0KDg5m7NixTJgwgVq1auHk5IRhGCQkJNC2bVuqVatGSEgIp06d4rPPPqN58+a4uroyZMgQsrOzLf1s3LiRO++8E3d3dzw9Penbty9HjhwptK8/T6v4/vvvCQkJoVq1anh6ejJy5EjOnz9vWR8ZGUn//v2ZMWMGdevWpWnTpmV+PkREpOwlpGYyankKe4+byM032HvcRNSKFBXIIlakaRWlsGzZMkaPHs327dtJSkoiKiqKmJgYXn/9dZydnbn//vu5//77cXJyYtWqVZw/f54BAwawYMECnn32WQAuXLhAdHQ0QUFBnD9/nqlTpzJgwAD27NmDnV3Rv10uXLhAeHg4nTt3ZufOnZw6dYrHHnuMsWPHEhcXZ9luy5YtuLq6kpiYeN34c3JyyMnJsSybTCYAzGYzZrO51OfnSh/W6EsqlnJpO5TLym3h1rQibQUFsHBbGiEBnhUQkZSWrsnyU9xzbBQUFBSUcSw2KTg4GJPJxO7duwFISkqie/fubN68mR49egAwa9YsJk+ezJEjR2jUqBEAUVFRpKens3Hjxmv2e/r0aby8vPj+++9p2bIlcGnk+OOPP6Z///68/fbbPPvss/z4449Ur14dgPj4ePr168eJEyeoU6cOkZGRbNy4kYyMDBwdHa97DDExMUybNq1I+6pVq3B2dr71kyMiImViUrI9uflGkXZHuwJe7ZhXARGJVB7Z2dkMGTKErKwsXF1dr7udRo5LoV27dkXagoKCLD/XqVMHZ2dnS2F8pe2bb76xLKelpTF16lSSk5M5ffo0+fn5AGRkZFiK46vt37+f1q1bWwpjgK5du5Kfn8/BgwepU6cOAK1atbphYQwwefJkoqOjLcsmkwlfX1/CwsJu+EtTXGazmcTEREJDQ3FwcCh1f1JxlEvboVxWbksydrD3uKlIe7O6bkREdKqAiKS0dE2WnyvfkN+MiuNSuLpAveLqX2zDMIr8ohuGYSmAAfr160eDBg14++23qVu3Lvn5+bRs2bLUN9FdK7Y/c3JyuuaNfg4ODla9QK3dn1Qc5dJ2KJeV05gQf6JWpHD1d76GAWO7+yuflZyuybJX3POrG/Iq0K+//srBgwf55z//SY8ePWjevDlnzpy54WeaN2/Od999x4ULFyxt27dvx87OTjfeiYjYuPBAbxYPa0dQPVcc7QoIqufKm8PaERboXdGhidgMFccVqGbNmnh6evLWW29x+PBhtm7dWmiaw7UMHTqUqlWr8vDDD/O///2Pbdu2MW7cOB566CHLlAoREbFd4YHerB3ViVc75rF2VCcVxiJWpuK4AtnZ2bF69WpSUlJo2bIlTz31FK+++uoNP+Ps7ExCQgK//fYbd9xxB/feey89evTg9ddfL6eoRURERGyX5hzfoqSkpELLwcHB/PnBH5GRkURGRhZqi4mJISYmxrLcs2dP9u3bV2ibq/u58qg1FxcXS1urVq3YunXrdWO7+pFuIiIiIlJ8Ko7/wkwmEx999BF2dnY0a9asosMRERERsXkqjv/CXnzxRVatWsUrr7xCvXr1KjocEREREZun4vgvbM6cOcyZM6eiwxARERH529ANeSIiIiIil6k4FhERERG5TMWxiIiIiMhlKo5FRERERC5TcVxJBQcHM2HChIoOQ0RERMSmqDgWkRtKSM1k0OIdTEq2Z9DiHSSkZlZ0SCIiImVGxXElFBkZyeeff868efMwDAPDMEhPT+d///sfvXv3xsXFhTp16vDQQw9x+vTpig5XKrGE1ExGLU9h73ETufkGe4+biFqRogJZRERslp5zXAnNmzePQ4cO0bJlS6ZPnw6Ag4MDHTp04LHHHmPOnDn8/vvvPPvss9x///3XfdV0Tk6O5fXUcOmNfABmsxmz2VzqOK/0YY2+pGIs3JpWpK2gABZuSyMkwLMCIpLS0nVpG5RH26Fclp/inmOjoKCgoIxjkTIQHBxMmzZtmDt3LgAvvfQSX375JQkJCZZtfvrpJ3x9fTl48CABAQFF+oiJiWHatGlF2letWoWzs3OZxS6Vx6Rke3LzjSLtjnYFvNoxrwIiEhERuTXZ2dkMGTKErKwsXF1dr7udRo5txHfffce2bdtwcXEpsu7IkSPXLI4nT55MdHS0ZdlkMuHr60tYWNgNf2mKy2w2k5iYSGhoKA4ODqXuT8rfkowd7D1uKtLerK4bERGdKiAiKS1dl7ZBebQdymX5ufIN+c2oOLYR58+fp1+/frzyyitF1vn4+FzzM05OTjg5ORVpd3BwsOoFau3+pPyMCfEnakUKV3+/ZBgwtru/clrJ6bq0Dcqj7VAuy15xz6+K40rK0dGRvLz//7X27bffztq1a/Hz86NKFaVVrCM80JvFw9qxcFsaB05k0ayuG2O7+xMW6F3RoYmIiJQJPa2ikvLz8yM5OZn09HROnz7NmDFj+O2333jwwQfZuXMnR44cISEhgUceeaRQES1SUuGB3qwd1YlXO+axdlQnFcYiImLTVBxXUhMnTsTe3p4WLVrg5eVFbm4u27dvJy8vj7CwMFq1asWECRNwd3fHzk5pFhERESkOff9eSQUEBPD1118Xaf/oo48qIBoRERER26AhRRERERGRy1Qci4iIiIhcpuJYREREROQyFcciIiIiIpepOBYRERERuUzFsYiIiIjIZSqOy1hwcDATJky47vrMzExCQ0OpXr067u7u5RaXiIiIiBSl4riCzZkzh5MnT7Jnzx4OHTpklT5vVpCLiIiIyLXpJSAV7MiRI7Rr1w5/f/+KDkXkmhJSM1m4NY0DJ+1ZkrGDMSH+hOsV0iIiYqM0clwO8vPzeeaZZ/Dw8MDb25uYmBgA/Pz8WLt2Le+99x6GYRAZGQnAa6+9RqtWrahevTq+vr488cQTnD9/vlCf27dvJzg4GGdnZ2rWrEl4eDhnzpwhMjKSzz//nHnz5mEYBoZhkJ6eXr4HLDYjITWTUctT2HvcRG6+wd7jJqJWpJCQmlnRoYmIiJQJjRyXg2XLlhEdHU1ycjJff/01kZGRdO3alZ07dzJ8+HBcXV2ZN28e1apVA8DOzo758+fTsGFDjh49yhNPPMEzzzzDokWLANizZw89evTg0UcfZd68eVSpUoVt27aRl5fHvHnzOHToEC1btmT69OkAeHl5XTOunJwccnJyLMsmkwkAs9mM2Wwu9XFf6cMafUnFWLg1rUhbQQEs3JZGSIBnBUQkpaXr0jYoj7ZDuSw/xT3HRkFBQUEZx/K3FhwcTF5eHl9++aWlrUOHDoSEhDBr1iz69++Pu7s7cXFx1+1jzZo1REVFcfr0aQCGDBlCRkYGX3311XX32aZNG+bOnXvD2GJiYpg2bVqR9lWrVuHs7HzzgxObNynZntx8o0i7o10Br3bMq4CIREREbk12djZDhgwhKysLV1fX626nkeNyEBQUVGjZx8eHU6dOXXf7zZs3M3PmTA4cOIDJZOLixYv88ccfZGdn4+zszJ49e7jvvvtKHdfkyZOJjo62LJtMJnx9fQkLC7vhL01xmc1mEhMTCQ0NxcHBodT9SflbkrGDvcdNRdqb1XUjIqJTBUQkpaXr0jYoj7ZDuSw/V74hvxkVx+Xgz7/shmGQn59/zW3T09Pp27cvo0ePZsaMGXh4ePDVV18xYsQIcnNzcXZ2tky/KC0nJyecnJyuGa81L1Br9yflZ0yIP1ErUrj6+yXDgLHd/ZXTSk7XpW1QHm2Hcln2int+dUPeX0xKSgr5+fnExsbSqVMnAgICOHHiRKFtgoKC2LJly3X7cHR0JC9PX3lL6YUHerN4WDuC6rniaFdAUD1X3hzWjjA9rUJERGyUiuO/mCZNmmA2m1mwYAFHjx5l+fLlLF68uNA2kydPZufOnTzxxBPs3buXAwcO8MYbb1jmJPv5+ZGcnEx6ejqnT5++7ii1SHGEB3qzdlQnXu2Yx9pRnVQYi4iITVNx/BfTunVrXnvtNV555RVatmzJypUrmTlzZqFtAgIC2LRpE9999x0dOnSgc+fOfPLJJ1SpcmmWzMSJE7G3t6dFixZ4eXmRkZFREYciIiIiUuloznEZS0pKKtK2bt26a/58xVNPPcVTTz1VqO2hhx4qtNytWze2b99+zX0GBATw9ddflzhWERERkb87jRyLiIiIiFym4lhERERE5DIVxyIiIiIil6k4FhERERG5TMWxiIiIiMhlKo5FRERERC5TcVzBtm/fTqtWrXBwcKB///631Ed6ejqGYbBnzx6rxiYiIiLyd6PiuBwFBwczYcKEQm3R0dG0adOGY8eOERcXd9M+IiMjb7mIFhEREZEbU3FcwY4cOUJISAj16tXD3d29osMRKSIhNZNBi3cwKdmeQYt3kJCaWdEhiYiIlBkVx+UkMjKSzz//nHnz5mEYhuXfr7/+yqOPPophGJaR49TUVPr27Yurqys1atTgrrvu4siRI8TExLBs2TI++eQTy+evfgPf0aNH6d69O87OzrRu3VpvyZNSS0jNZNTyFPYeN5Gbb7D3uImoFSkqkEVExGbp9dHlZN68eRw6dIiWLVsyffp08vLyAGjRogXTp09n8ODBuLm5cfz4ce6++26Cg4PZunUrrq6ubN++nYsXLzJx4kT279+PyWRi6dKlAHh4eHDixAkApkyZwr///W/8/f2ZMmUKDz74IIcPH6ZKlWunOScnh5ycHMuyyWQCwGw2YzabS33MV/qwRl9SMRZuTSvSVlAAC7elERLgWQERSWnpurQNyqPtUC7LT3HPsYrjcuLm5oajoyPOzs54e3tb2g3DwM3NzdK2cOFC3NzcWL16NQ4ODgAEBARYtq9WrRo5OTmF+rhi4sSJ9OnTB4Bp06YRGBjI4cOHadas2TVjmjlzJtOmTSvSvmnTJpydnW/9YP8kMTHRan1J+Tpw0h4wirafyCI+Pr78AxKr0XVpG5RH26Fclr3s7Oxibafi+C9mz5493HXXXZbCuCSCgoIsP/v4+ABw6tSp6xbHkydPJjo62rJsMpnw9fUlLCwMV1fXEu//z8xmM4mJiYSGht7S8UjFW5Kxg73HTUXam9V1IyKiUwVEJKWl69I2KI+2Q7ksP1e+Ib8ZFcd/MdWqVbvlz159URnGpdG+/Pz8627v5OSEk5PTNfux5gVq7f6k/IwJ8SdqRQoFBf+/zTBgbHd/5bSS03VpG5RH26Fclr3inl/dkFeOHB0dLXONrycoKIgvv/zyuvNiitOHiLWEB3qzeFg7guq54mhXQFA9V94c1o6wwKLTekRERGyBiuNy5OfnR3JyMunp6Zw+ffqao7pjx47FZDLxwAMPsGvXLtLS0li+fDkHDx609LF3714OHjzI6dOnNYFfylx4oDdrR3Xi1Y55rB3VSYWxiIjYNBXH5WjixInY29vTokULvLy8yMjIKLKNp6cnW7du5fz583Tr1o127drx9ttvW74KePzxx2natCnt27fHy8uL7du3l/dhiIiIiNgszTkuRwEBAUWePXz27Nki2wUFBZGQkHDNPry8vNi0aVOR9oKrJ4UC7u7uRdpERERE5MY0ciwiIiIicpmKYxERERGRy1Qci4iIiIhcpuJYREREROQyFcciIiIiIpepOBYRERERuUzFsYiIiIjIZSqOy1lSUhKGYVzz+calERcXh7u7u1X7FBEREfm7UXFcCfn5+TF37tyKDkP+JhJSMxm0eAeTku0ZtHgHCamZFR2SiIhImVFxLCLXlZCayajlKew9biI332DvcRNRK1JUIIuIiM3S66PLQE5ODpMmTWL16tWYTCbat2/PnDlzuOOOOyzbpKSk8Oyzz7Jv3z7atGnD0qVLadq0qWX9//3f/zF9+nS+//57XFxcuOuuu/j4448JDg7mhx9+4KmnnuKpp54CCr86OiEhgQkTJvDjjz9y5513snTpUnx8fK4bZ05OjmXZZDIBYDabMZvNpT4PV/qwRl9SMRZuTSvSVlAAC7elERLgWQERSWnpurQNyqPtUC7LT3HPsVFwdWUlVvHkk0+yZs0a3nnnHRo0aMDs2bNZv349hw8fZu/evXTv3p2OHTvyyiuv4OXlRVRUFHl5eWzfvh2ATz/9lHvuuYcpU6bwwAMPkJubS3x8PJMnT+a3336jdevWjBw5kscffxwAb29v4uLiGDlyJN26dWPmzJnY2dkxbNgw2rZty8qVK68ZZ0xMDNOmTSvSvmrVKpydncvuBEmlMSnZntx8o0i7o10Br3bMq4CIREREbk12djZDhgwhKysLV1fX626n4tjKLly4QM2aNYmLi2PIkCHApb9U/Pz8mDBhAnfccQfdu3dn8+bN9OjRA4D4+Hj69OnD77//TtWqVenSpQuNGjVixYoV19zHlb4mTJhgaYuLi+ORRx7h8OHDNG7cGIBFixYxffp0MjOv/RX4tUaOfX19OX369A1/aYrLbDaTmJhIaGgoDg4Ope5Pyt+gxTvYe9xUpD2onitrR3WqgIiktHRd2gbl0XYol+XHZDJRq1atmxbHmlZhZUeOHMFsNtO1a1dLm4ODAx06dGD//v2WqRVBQUGW9VemPZw6dYr69euzZ88ey6hwSTg7O1sK4yv9njp16rrbOzk54eTkVKTdwcHBqheotfuT8jMmxJ+oFSlc/Se0YcDY7v7KaSWn69I2KI+2Q7kse8U9v7ohr4JcnSDDuPS1dX5+PgDVqlUrdZ9X+tUXA1Ia4YHeLB7WjqB6rjjaFRBUz5U3h7UjLNC7okMTEREpEyqOraxx48Y4Ojpa5g/Dpa9Mdu7cSYsWLYrVR1BQEFu2bLnuekdHR/LyNN9Tykd4oDdrR3Xi1Y55rB3VSYWxiIjYNBXHVla9enVGjx7NpEmT2LhxI/v27ePxxx8nOzubESNGFKuPF198kffff58XX3yR/fv38/333/PKK69Y1vv5+fHFF19w/PhxTp8+XVaHIiIiIvK3o+K4DMyaNYtBgwbx0EMPcfvtt3P48GESEhKoWbNmsT4fHBzMf/7zH9avX0+bNm0ICQnhm2++sayfPn066enpNG7cGC8vr7I6DBEREZG/Hd2QVwaqVq3K/PnzmT9/fpF1wcHBReYBt2nTpkjbwIEDGThw4DX779SpE999912htsjISCIjIwu19e/fX3OORUREREpAI8ciIiIiIpepOBYRERERuUzFsYiIiIjIZSqORUREREQuU3EsIiIiInKZimMRERERkctUHIuIiIiIXKbiWERuKCE1k0GLdzAp2Z5Bi3eQkJpZ0SGJiIiUGRXHInJdCamZjFqewt7jJnLzDfYeNxG1IkUFsoiI2Cy9Ic+GXLhwgdGjR/PRRx9Ro0YNJk6cyP/93//Rpk0b5s6dW2T7nJwccnJyLMsmkwkAs9mM2WwudTxX+rBGX1IxFm5NK9JWUAALt6UREuBZARFJaem6tA3Ko+1QLstPcc+ximMbMmnSJD7//HM++eQTateuzfPPP8/u3btp06bNNbefOXMm06ZNK9K+adMmnJ2drRZXYmKi1fqS8nXgpD1gFG0/kUV8fHz5ByRWo+vSNiiPtkO5LHvZ2dnF2s4oKCgoKONYpBycP38eT09PVqxYwX333QfAb7/9Rr169Rg5cmSxR459fX05ffo0rq6upY7JbDaTmJhIaGgoDg4Ope5Pyt+gxTvYe9xUpD2onitrR3WqgIiktHRd2gbl0XYol+XHZDJRq1YtsrKybljnaOTYRhw5coTc3Fw6duxoafPw8KBp06bX/YyTkxNOTk5F2h0cHKx6gVq7Pyk/Y0L8iVqRwtV/QhsGjO3ur5xWcroubYPyaDuUy7JX3POrG/JE5LrCA71ZPKwdQfVccbQrIKieK28Oa0dYoHdFhyYiIlImVBzbiMaNG+Pg4EBycrKl7cyZMxw6dKgCoxJbEB7ozdpRnXi1Yx5rR3VSYSwiIjZN0ypshIuLCyNGjGDSpEl4enpSu3ZtpkyZgp2d/v4RERERKS4Vxzbk1Vdf5fz58/Tr148aNWrw9NNPk5WVVdFhiYiIiFQaGla0IS4uLixfvpwLFy6QmZnJpEmTKjokERERkUpFxbGIiIiIyGUqjkVERERELtOcYxuXlJRU0SGIiIiIVBoaORYRERERuUzFsYiIiIjIZSqORUREREQuU3FczoKDg5kwYUJFhyEiIiIi16DiWERERETkMhXHlVxeXh75+fkVHYbYsITUTAYt3sGkZHsGLd5BQmpmRYckIiJSZlQcV4CLFy8yduxY3NzcqFWrFi+88AIFBQUAnDlzhuHDh1OzZk2cnZ3p3bs3aWlpls/GxcXh7u7O+vXradGiBU5OTmRkZJCTk8PEiRO57bbbqF69Oh07dtRj3KTUElIzGbU8hb3HTeTmG+w9biJqRYoKZBERsVl6znEFWLZsGSNGjOCbb75h165djBw5kvr16/P4448TGRlJWloa69evx9XVlWeffZaIiAj27duHg4MDANnZ2bzyyiu88847eHp6Urt2bcaOHcu+fftYvXo1devW5eOPP6ZXr158//33+Pv7XzOOnJwccnJyLMsmkwkAs9mM2Wwu9XFe6cMafUnFWLg1rUhbQQEs3JZGSIBnBUQkpaXr0jYoj7ZDuSw/xT3HRsGVIUspF8HBwZw6dYrU1FQMwwDgueeeY/369XzyyScEBASwfft2unTpAsCvv/6Kr68vy5Yt47777iMuLo5HHnmEPXv20Lp1awAyMjJo1KgRGRkZ1K1b17Kvnj170qFDB15++eVrxhITE8O0adOKtK9atQpnZ2drH7pUQpOS7cnNN4q0O9oV8GrHvAqISERE5NZkZ2czZMgQsrKycHV1ve52GjmuAJ06dbIUxgCdO3cmNjaWffv2UaVKFTp27GhZ5+npSdOmTdm/f7+lzdHRkaCgIMvy999/T15eHgEBAYX2k5OTg6fn9Uf3Jk+eTHR0tGXZZDLh6+tLWFjYDX9pistsNpOYmEhoaKhl1FsqlyUZO9h73FSkvVldNyIiOlVARFJaui5tg/JoO5TL8nPlG/KbUXFcCVWrVq1QcX3+/Hns7e1JSUnB3t6+0LYuLi7X7cfJyQknJ6ci7Q4ODla9QK3dn5SfMSH+RK1I4ervlwwDxnb3V04rOV2XtkF5tB3KZdkr7vnVDXkVIDk5udDyjh078Pf3p0WLFly8eLHQ+l9//ZWDBw/SokWL6/bXtm1b8vLyOHXqFE2aNCn0z9vbu8yOQ2xfeKA3i4e1I6ieK452BQTVc+XNYe0IC9TvlYiI2CaNHFeAjIwMoqOjGTVqFLt372bBggXExsbi7+/PPffcw+OPP86bb75JjRo1eO6557jtttu45557rttfQEAAQ4cOZfjw4cTGxtK2bVt++eUXtmzZQlBQEH369CnHoxNbEx7oTUiAJ/Hx8UREdNLIhoiI2DQVxxVg+PDh/P7773To0AF7e3uefPJJRo4cCcDSpUt58skn6du3L7m5udx9993Ex8fftCBZunQpL730Ek8//TTHjx+nVq1adOrUib59+5bHIYmIiIjYBBXH5ezqZw+/8cYbRdbXrFmT995777qfj4yMJDIyski7g4MD06ZNu+bTJ0RERESkeDTnWERERETkMhXHIiIiIiKXqTgWEREREblMxbGIiIiIyGUqjkVERERELlNxLCIiIiJymYrjPykoKGDkyJF4eHhgGAZ79uy55b7i4uJwd3e3WmwlFRMTQ5s2bSps/yIiIiKVjYrjP9m4cSNxcXFs2LCBkydP0rJly4oO6ZZNnDiRLVu2VHQYIiIiIpWGXgLyJ0eOHMHHx4cuXbpUyP5zc3NxdHS0Sl8uLi64uLhYpS/5+0pIzWTh1jQOnLRnScYOxoT4Ex7oXdFhiYiIlAmNHF8lMjKScePGkZGRgWEY1K1bl7p165Kfn19ou3vuuYdHH30UgO+++47u3btTo0YNXF1dadeuHbt27Sq0/bp16/D396dq1aqEh4fz448/WtZdmfrwzjvv0LBhQ6pWrQqAYRi88847DBgwAGdnZ/z9/Vm/fr3lc0lJSRiGwZYtW2jfvj3Ozs506dKFgwcPFulb5FYlpGYyankKe4+byM032HvcRNSKFBJSMys6NBERkTKhkeOrzJs3j8aNG/PWW2+xc+dO7O3tqVevHtu2baNHjx4A/Pbbb2zcuJH4+HgAhg4dStu2bXnjjTewt7dnz549ODg4WPrMzs5mxowZvPfeezg6OvLEE0/wwAMPsH37dss2hw8fZu3atXz00UfY29tb2qdNm8bs2bN59dVXWbBgAUOHDuWHH37Aw8PDss2UKVOIjY3Fy8uLqKgoHn300UJ930hOTg45OTmWZZPJBIDZbMZsNt/CGSzsSh/W6EsqxsKtaUXaCgpg4bY0QgI8KyAiKS1dl7ZBebQdymX5Ke45VnF8FTc3N2rUqIG9vT3e3pe+Nu7duzerVq2yFMdr1qyhVq1adO/eHYCMjAwmTZpEs2bNAPD39y/Up9ls5vXXX6djx44ALFu2jObNm/PNN9/QoUMH4NJUivfeew8vL69Cn42MjOTBBx8E4OWXX2b+/Pl888039OrVy7LNjBkz6NatGwDPPfccffr04Y8//rCMQN/IzJkzmTZtWpH2TZs24ezsfNPPF1diYqLV+pLydeCkPWAUbT+RZfkDUSonXZe2QXm0Hcpl2cvOzi7WdiqOb2Lo0KE8/vjjLFq0CCcnJ1auXMkDDzyAnd2lGSnR0dE89thjLF++nJ49e3LffffRuHFjy+erVKnCHXfcYVlu1qwZ7u7u7N+/31IcN2jQoEhhDBAUFGT5uXr16ri6unLq1KnrbuPj4wPAqVOnqF+//k2PbfLkyURHR1uWTSYTvr6+hIWF4erqetPP34zZbCYxMZHQ0NBCo+lSeSzJ2MHe46Yi7c3quhER0akCIpLS0nVpG5RH26Fclp8r35DfjIrjm+jXrx8FBQV8+umn3HHHHXz55ZfMmTPHsj4mJoYhQ4bw6aef8tlnn/Hiiy+yevVqBgwYUOx9VK9e/Zrtf75IDMMoMv/56m0M49II35+3uR4nJyecnJyuuV9rXqDW7k/Kz5gQf6JWpFBQ8P/bDAPGdvdXTis5XZe2QXm0Hcpl2Svu+dUNeTdRtWpVBg4cyMqVK3n//fdp2rQpt99+e6FtAgICeOqpp9i0aRMDBw5k6dKllnUXL14sdIPewYMHOXv2LM2bNy+3YxC5VeGB3iwe1o6geq442hUQVM+VN4e1I0xPqxARERulkeNiGDp0KH379iU1NZVhw4ZZ2n///XcmTZrEvffeS8OGDfnpp5/YuXMngwYNsmzj4ODAuHHjmD9/PlWqVGHs2LF06tTJMqVC5K8uPNCbkABP4uPjiYjopJENERGxaSqOiyEkJAQPDw8OHjzIkCFDLO329vb8+uuvDB8+nJ9//platWoxcODAQje5OTs78+yzzzJkyBCOHz/OXXfdxZIlSyriMERERETkJoyCgqtnE8rfmclkws3NjaysLKvdkHdptDFCo42VnHJpO5RL26A82g7lsvwUt87RnGMRERERkctUHIuIiIiIXKbiWERERETkMhXHIiIiIiKXqTgWEREREblMxbGIiIiIyGUqjstAUlIShmFw9uzZCovhrbfewtfXFzs7O+bOnVthcYiIiIhUJiqOSyg4OJgJEyZUdBgWhmGwbt26Qm0mk4mxY8fy7LPPcvz4cUaOHFkxwYmIiIhUMnpDng3KyMjAbDbTp08ffHx8KjocqeQSUjNZuDWNAyftWZKxgzEh/oQHeld0WCIiImVCI8clEBkZyeeff868efMwDAPDMEhPTyc+Pp6AgACqVatG9+7dSU9PL/S5uLg43N3d2bBhA02bNsXZ2Zl7772X7Oxsli1bhp+fHzVr1mT8+PHk5eVZPufn58e//vUvHnzwQapXr85tt93GwoULC60HGDBgAIZh4OfnR1xcHK1atQKgUaNGlhhFbkVCaiajlqew97iJ3HyDvcdNRK1IISE1s6JDExERKRMaOS6BefPmcejQIVq2bMn06dMByMnJYeDAgYwZM4aRI0eya9cunn766SKfzc7OZv78+axevZpz584xcOBABgwYgLu7O/Hx8Rw9epRBgwbRtWtXBg8ebPncq6++yvPPP8+0adNISEjgySefJCAggNDQUHbu3Ent2rVZunQpvXr1wt7eHhcXF3x9fenZsyfffPMNvr6+eHl5XfN4cnJyyMnJsSybTCbg0qsszWZzqc/XlT6s0ZdUjIVb04q0FRTAwm1phAR4VkBEUlq6Lm2D8mg7lMvyU9xzrOK4BNzc3HB0dMTZ2Rlv70tfKz///PM0btyY2NhYAJo2bcr333/PK6+8UuizZrOZN954g8aNGwNw7733snz5cn7++WdcXFxo0aIF3bt3Z9u2bYWK465du/Lcc88BEBAQwPbt25kzZw6hoaGWotfd3d0SD4Cn56WixcvLq1D7n82cOZNp06YVad+0aRPOzs4lPj/Xk5iYaLW+pHwdOGkPGEXbT2QRHx9f/gGJ1ei6tA3Ko+1QLstednZ2sbZTcVxK+/fvp2PHjoXaOnfuXGQ7Z2dnS2EMUKdOHfz8/HBxcSnUdurUqRv21blzZ6s9fWLy5MlER0dblk0mE76+voSFheHq6lrq/s1mM4mJiYSGhuLg4FDq/qT8LcnYwd7jpiLtzeq6ERHRqQIiktLSdWkblEfboVyWnyvfkN+MiuNy8udfeMMwrtmWn59fbjE5OTnh5ORUpN3BwcGqF6i1+5PyMybEn6gVKRQU/P82w4Cx3f2V00pO16VtUB5th3JZ9op7fnVDXgk5OjoWummuefPmfPPNN4W22bFjh9X29+e+duzYQfPmzS3LDg4OheIRsabwQG8WD2tHUD1XHO0KCKrnypvD2hGmp1WIiIiNUnFcQn5+fiQnJ5Oens7p06eJiooiLS2NSZMmcfDgQVatWkVcXJzV9rd9+3Zmz57NoUOHWLhwIf/5z3948sknC8WzZcsWMjMzOXPmjNX2K3JFeKA3a0d14tWOeawd1UmFsYiI2DQVxyU0ceJE7O3tadGiBV5eXuTn57N27VrWrVtH69atWbx4MS+//LLV9vf000+za9cu2rZty0svvcRrr71GeHi4ZX1sbCyJiYn4+vrStm1bq+1XRERE5O9Ic45LKCAggK+//rpQm5+fH3379i3U9sgjj1h+joyMJDIystD6mJgYYmJiCrVda8TZ1dWVDz/88Lrx9OvXj379+hVqa9OmDQVXTxIVERERkWLRyLGIiIiIyGUqjkVERERELtO0ir8wvfZZREREpHxp5FhERERE5DIVxyIiIiIil6k4FhERERG5TMWxlSQlJWEYBmfPnr3uNjExMbRp06bcYhIRERGRklFxfIuCg4OZMGFCRYchIiIiIlak4lhEbighNZNBi3cwKdmeQYt3kJCaWdEhiYiIlBkVx7cgMjKSzz//nHnz5mEYBoZhWB67lpKSQvv27XF2dqZLly4cPHjwuv0cOXKERo0aMXbsWMsb7bZv305wcDDOzs7UrFmT8PBwzpw5A8DGjRu58847cXd3x9PTk759+3LkyBFLf7m5uYwdOxYfHx+qVq1KgwYNmDlzZtmdCLF5CamZjFqewt7jJnLzDfYeNxG1IkUFsoiI2Cw95/gWzJs3j0OHDtGyZUumT58OQGpqKgBTpkwhNjYWLy8voqKiePTRR9m+fXuRPvbu3Ut4eDgjRozgpZdeAmDPnj306NGDRx99lHnz5lGlShW2bdtGXl4eABcuXCA6OpqgoCDOnz/P1KlTGTBgAHv27MHOzo758+ezfv16PvzwQ+rXr8+PP/7Ijz/+eN3jyMnJIScnx7JsMpkAMJvNmM3mUp+nK31Yoy+pGAu3phVpKyiAhdvSCAnwrICIpLR0XdoG5dF2KJflp7jnWMXxLXBzc8PR0RFnZ2e8vb0BOHDgAAAzZsygW7duADz33HP06dOHP/74g6pVq1o+/9///pe+ffsyZcoUnn76aUv77Nmzad++PYsWLbK0BQYGWn4eNGhQoTjeffddvLy82LdvHy1btiQjIwN/f3/uvPNODMOgQYMGNzyOmTNnMm3atCLtmzZtwtnZubin46YSExOt1peUrwMn7QGjaPuJLOLj48s/ILEaXZe2QXm0Hcpl2cvOzi7WdiqOrSwoKMjys4+PDwCnTp2ifv36AGRkZBAaGsqMGTOK3NC3Z88e7rvvvuv2nZaWxtSpU0lOTub06dPk5+db+mzZsiWRkZGEhobStGlTevXqRd++fQkLC7tuf5MnTyY6OtqybDKZ8PX1JSwsDFdX1xIf+5+ZzWYSExMJDQ3FwcGh1P1J+VuSsYO9x01F2pvVdSMiolMFRCSlpevSNiiPtkO5LD9XviG/GRXHVnb1L7ZhXBpxu1LEAnh5eVG3bl3ef/99Hn300UJFaLVq1W7Yd79+/WjQoAFvv/02devWJT8/n5YtW5KbmwvA7bffzrFjx/jss8/YvHkz999/Pz179mTNmjXX7M/JyQknJ6drHoM1L1Br9yflZ0yIP1ErUrg8JR4Aw4Cx3f2V00pO16VtUB5th3JZ9op7fnVD3i1ydHS0zAUuiWrVqrFhwwaqVq1KeHg4586ds6wLCgpiy5Yt1/zcr7/+ysGDB/nnP/9Jjx49aN68ueVGvau5uroyePBg3n77bT744APWrl3Lb7/9VuI4RQDCA71ZPKwdQfVccbQrIKieK28Oa0dYoHdFhyYiIlImNHJ8i/z8/EhOTiY9PR0XF5dCo8M3U716dT799FN69+5N79692bhxIy4uLkyePJlWrVrxxBNPEBUVhaOjI9u2beO+++7Dw8MDT09P3nrrLXx8fMjIyOC5554r1O9rr72Gj48Pbdu2xc7Ojv/85z94e3vj7u5u5aOXv5PwQG9CAjyJj48nIqKTRjZERMSmaeT4Fk2cOBF7e3tatGiBl5cXGRkZJfq8i4sLn332GQUFBfTp04cLFy4QEBDApk2b+O677+jQoQOdO3fmk08+oUqVKtjZ2bF69WpSUlJo2bIlTz31FK+++mqhPmvUqGG5qe+OO+4gPT2d+Ph47OyUZhEREZHiMAoKrp5NKH9nJpMJNzc3srKyrHZD3qXRxgiNNlZyyqXtUC5tg/JoO5TL8lPcOkdDiiIiIiIil6k4FhERERG5TMWxiIiIiMhlKo5FRERERC5TcSwiIiIicpmKYxERERGRy/7WxXFSUhKGYXD27NmKDuWGgoODmTBhQkWHISIiImLz/lbF8d+lyExPT8cwDPbs2VPRoYiIiIhUKn+r4lhESi4hNZNBi3cwKdmeQYt3kJCaWdEhiYiIlJm/TXEcGRnJ559/zrx58zAMA8MwSE9PByAlJYX27dvj7OxMly5dOHjwIABZWVnY29uza9cuAPLz8/Hw8KBTp06WflesWIGvr69l+aeffuLBBx/Ew8OD6tWr0759e5KTkwGIiYmhTZs2LF++HD8/P9zc3HjggQc4d+6c5fMXLlxg+PDhuLi44OPjQ2xsbJFjMQyDdevWFWpzd3cnLi4OgIYNGwLQtm1bDMMgODi4VOdO/r4SUjMZtTyFvcdN5OYb7D1uImpFigpkERGxWVUqOoDyMm/ePA4dOkTLli2ZPn06AKmpqQBMmTKF2NhYvLy8iIqK4tFHH2X79u24ubnRpk0bkpKSaN++Pd9//z2GYfDtt99y/vx5XFxc+Pzzz+nWrRsA58+fp1u3btx2222sX78eb29vdu/eTX5+viWOI0eOsG7dOjZs2MCZM2e4//77mTVrFjNmzABg0qRJfP7553zyySfUrl2b559/nt27d9OmTZtiH+s333xDhw4d2Lx5M4GBgTg6Ol5zu5ycHHJycizLJpMJuPQqS7PZXPyTex1X+rBGX1IxFm5NK9JWUAALt6UREuBZARFJaem6tA3Ko+1QLstPcc/x36Y4dnNzw9HREWdnZ7y9vQE4cOAAADNmzLAUuM899xx9+vThjz/+oGrVqgQHB5OUlMTEiRNJSkoiNDSUAwcO8NVXX9GrVy+SkpJ45plnAFi1ahW//PILO3fuxMPDA4AmTZoUiiM/P5+4uDhq1KgBwEMPPcSWLVuYMWMG58+fZ8mSJaxYsYIePXoAsGzZMurVq1eiY/Xy8gLA09PTcqzXMnPmTKZNm1akfdOmTTg7O5donzeSmJhotb6kfB04aQ8YRdtPZBEfH1/+AYnV6Lq0Dcqj7VAuy152dnaxtvvbFMc3EhQUZPnZx8cHgFOnTlG/fn26devGkiVLyMvL4/PPPycsLAxvb2+SkpIICgri8OHDlmkLe/bsoW3btpbC+Fr8/PwshfGV/Z06dQq4NKqcm5tLx44dLes9PDxo2rSpNQ/XYvLkyURHR1uWTSYTvr6+hIWF4erqWur+zWYziYmJhIaG4uDgUOr+pPwtydjB3uOmIu3N6roREdHpGp+Qvzpdl7ZBebQdymX5ufIN+c2oOIZCv4yGcWmU7MpUiLvvvptz586xe/duvvjiC15++WW8vb2ZNWsWrVu3pm7duvj7+wNQrVq1Eu3ryv6unnZRHIZhUFBQUKjtVr6OcXJywsnJ6ZoxWvMCtXZ/Un7GhPgTtSKFq3/dDAPGdvdXTis5XZe2QXm0Hcpl2Svu+f3b3JAH4OjoSF5eXok+4+7uTlBQEK+//joODg40a9aMu+++m2+//ZYNGzZYpmPApRHoPXv28Ntvv91SfI0bN8bBwcFyAx/AmTNnOHToUKHtvLy8OHnypGU5LS2t0FcFV+YYl/RYRf4sPNCbxcPaEVTPFUe7AoLqufLmsHaEBV5/uo6IiEhl9rcqjv38/EhOTiY9PZ3Tp08Xe8Q2ODiYlStXWgphDw8PmjdvzgcffFCoOH7wwQfx9vamf//+bN++naNHj7J27Vq+/vrrYu3HxcWFESNGMGnSJLZu3cr//vc/IiMjsbMrnKaQkBBef/11vv32W3bt2kVUVFShv4Zq165NtWrV2LhxIz///DNZWVnF2r/ItYQHerN2VCde7ZjH2lGdVBiLiIhN+1sVxxMnTsTe3p4WLVrg5eVFRkZGsT7XrVs38vLyCj0SLTg4uEibo6MjmzZtonbt2kRERNCqVStmzZqFvb19sWN89dVXueuuu+jXrx89e/bkzjvvpF27doW2iY2NxdfXl7vuuoshQ4YwceLEQjfQValShfnz5/Pmm29St25d7rnnnmLvX0REROTvzCj48+RV+dsymUy4ubmRlZVltRvy4uPjiYiI0DyqSk65tB3KpW1QHm2Hcll+ilvn/K1GjkVEREREbkTFsYiIiIjIZSqORUREREQuU3EsIiIiInKZimMRERERkctUHIuIiIiIXKbiuIQKCgoYOXIkHh4eGIbBnj17ymQ/2dnZDBo0CFdXVwzD4OzZs2WyHxERERH5/1Qcl9DGjRuJi4tjw4YNnDx5kpYtW5aqv7i4ONzd3Yu0L1u2jC+//JL//ve/nDx5Ejc3t1LtR0RERERurkpFB1DZHDlyBB8fH7p06VLm+2nevHmpi++/moTUTBZtO8yhn88TUMeFJ7o3IVyvIxYREZG/CI0cl0BkZCTjxo0jIyMDwzDw8/MjPz+f2bNn06RJE5ycnKhfvz4zZswAICkpqciUiD179mAYBunp6SQlJfHII4+QlZWFYRgYhkFMTAzBwcHExsbyxRdfYBiG5RXVixYtwt/fn6pVq1KnTh3uvfdeS79+fn7MnTu3ULxt2rQhJiamjM9K8SWkZjJqeQrf/ZTF7+Y8vvspi6gVKSSkZlZ0aCIiIiKARo5LZN68eTRu3Ji33nqLnTt3Ym9vz+TJk3n77beZM2cOd955JydPnuTAgQPF6q9Lly7MnTuXqVOncvDgQQBcXFwYP348zz33HP/73//46KOPcHR0ZNeuXYwfP57ly5fTpUsXfvvtN7788stSHU9OTg45OTmWZZPJBFx6laXZbC5V31f6ufp/F25NK7JNQQEs3JZGSIBnqfcnZefPuZTKS7m0Dcqj7VAuy09xz7GK4xJwc3OjRo0a2Nvb4+3tzblz55g3bx6vv/46Dz/8MACNGzfmzjvvLFZ/jo6OuLm5YRgG3t6FpxY4Ozvj6OhoaU9KSqJ69er07duXGjVq0KBBA9q2bVuq45k5cybTpk0r0r5p0yacnZ1L1ffVEhMTAThw0h4wiqw/cCKL+Ph4q+1Pys6VXErlp1zaBuXRdiiXZS87O7tY26k4LoX9+/eTk5NDjx49ynxfoaGhNGjQgEaNGtGrVy969erFgAEDSlXETp48mejoaMuyyWTC19eXsLAwXF1dSx2z2WwmMTGR0NBQHBwcWJKxg73HTUW2a1bXjYiITqXen5SdP+dSKi/l0jYoj7ZDuSw/V74hvxkVx6VQrVq1G663s7s0pbugoMDSdqtfm9SoUYPdu3eTlJTEpk2bmDp1KjExMezcuRN3d3fs7OwK7ac4+3JycsLJyalIu4ODg1Uv0Cv9jQnxJ2pFCleHaRgwtru//g+hkrD274ZUHOXSNiiPtkO5LHvFPb+6Ia8U/P39qVatGlu2bLnmei8vLwBOnjxpafvzc5EdHR3Jy8sr1v6qVKlCz549mT17Nnv37iU9PZ2tW7da9nX1fkwmE8eOHSvJ4ZS58EBvFg9rR2tfd5wd7Wnt686bw9oRpqdViIiIyF+ERo5LoWrVqjz77LM888wzODo60rVrV3755RdSU1MZMWIETZo0wdfXl5iYGGbMmMGhQ4eIjY0t1Iefnx/nz59ny5YttG7dGmdn52tOldiwYQNHjx7l7rvvpmbNmsTHx5Ofn0/Tpk0BCAkJIS4ujn79+uHu7s7UqVOxt7cvl/NQEuGB3np0m4iIiPxlaeS4lF544QWefvpppk6dSvPmzRk8eDCnTp0CLg3fv//++xw4cICgoCBeeeUVXnrppUKf79KlC1FRUQwePBgvLy9mz559zf24u7vz0UcfERISQvPmzVm8eDHvv/8+gYGBwKX5w926daNv37706dOH/v3707hx47I9eBEREREbYxT8eaKq/G2ZTCbc3NzIysqy2g158fHxREREaB5VJadc2g7l0jYoj7ZDuSw/xa1zNHIsIiIiInKZimMRERERkctUHIuIiIiIXKbiWERERETkMhXHIiIiIiKXqTgWEREREblMxbEN2759O61atcLBwYH+/ftXdDgiIiIif3kqjiuRpKQkDMPg7NmzhdqDg4OZMGFCke2jo6Np06YNx44dIy4urlxiFBEREanMVBzbsCNHjhASEkK9evVwd3ev6HCkkkpIzWTQ4h1MSrZn0OIdJKRmVnRIIiIiZUbFcTnLz89n9uzZNGnSBCcnJ+rXr8+MGTNIT0/HMAxWr15Nly5dqFq1Ki1btuTzzz8HID09ne7duwNQs2ZNDMMgMjKSyMhIPv/8c+bNm4dhGBiGYenr119/5dFHH8UwDI0cyy1JSM1k1PIU9h43kZtvsPe4iagVKSqQRUTEZlWp6AD+biZPnszbb7/NnDlzuPPOOzl58iQHDhywrJ80aRJz586lRYsWvPbaa/Tr149jx47h6+vL2rVrGTRoEAcPHsTV1ZVq1aoBcOjQIVq2bMn06dMB8PLy4uTJkzRt2pTp06czePBg3NzcisSSk5NDTk6OZdlkMgGXXmVpNptLfaxX+rBGX1IxFm5NK9JWUAALt6UREuBZARFJaem6tA3Ko+1QLstPcc+xiuNydO7cOebNm8frr7/Oww8/DEDjxo258847SU9PB2Ds2LEMGjQIgDfeeIONGzeyZMkSnnnmGTw8PACoXbt2oWkSjo6OODs74+3tbWnz9vbGMAzc3NwKtV9t5syZTJs2rUj7pk2bcHZ2tsYhA5CYmGi1vqR8HThpDxhF209kER8fX/4BidXourQNyqPtUC7LXnZ2drG2U3Fcjvbv309OTg49evS47jadO3e2/FylShXat2/P/v37yySeyZMnEx0dbVk2mUz4+voSFhaGq6trqfs3m80kJiYSGhqKg4NDqfuT8rckYwd7j5uKtDer60ZERKcKiEhKS9elbVAebYdyWX6ufEN+MyqOy9GVaRB/FU5OTjg5ORVpd3BwsOoFau3+pPyMCfEnakUKBQX/v80wYGx3oaQvNgAAZAdJREFUf+W0ktN1aRuUR9uhXJa94p5f3ZBXjvz9/alWrRpbtmy57jY7duyw/Hzx4kVSUlJo3rw5cGn6BEBeXl6hzzg6OhZpE7GG8EBvFg9rR1A9VxztCgiq58qbw9oRFnjtqToiIiKVnUaOy1HVqlV59tlneeaZZ3B0dKRr16788ssvpKamWqZaLFy4EH9/f5o3b86cOXM4c+YMjz76KAANGjTAMAw2bNhAREQE1apVw8XFBT8/P5KTk0lPT8fFxQUPDw/s7PR3j1hHeKA3IQGexMfHExHRSSMbIiJi01RBlbMXXniBp59+mqlTp9K8eXMGDx7MqVOnLOtnzZrFrFmzaN26NV999RXr16+nVq1aANx2221MmzaN5557jjp16jB27FgAJk6ciL29PS1atMDLy4uMjIwKOTYRERGRyk4jx+XMzs6OKVOmMGXKlELtV55W0bx5c5KTk6/7+RdeeIEXXnihUFtAQABff/11kW3//CY9EREREbkxjRyLiIiIiFym4lhERERE5DJNq/iL8PPzo+Dq52WJiIiISLnTyLGIiIiIyGUqjkVERERELlNxLCIiIiJymYpjEREREZHLVByXs7i4ONzd3Ss6DBERERG5BhXHInJDCamZDFq8g0nJ9gxavIOE1MyKDklERKTMqDi2otzc3IoOQcSqElIzGbU8hb3HTeTmG+w9biJqRYoKZBERsVl6znEpBAcH07JlS6pUqcKKFSto1aoV/fr1Y+nSpRw9ehQPDw/69evH7NmzcXFxuWYfMTExrFu3jtGjR/PSSy/x66+/0rdvX95++23c3NwAiIyM5OzZs9x5553ExsaSm5vLAw88wNy5c3FwcAAgJyeHKVOm8P7773P27FlatmzJK6+8QnBw8HXjz8nJIScnx7JsMpkAMJvNmM3mUp+fK31Yoy+pGAu3phVpKyiAhdvSCAnwrICIpLR0XdoG5dF2KJflp7jnWMVxKS1btozRo0ezfft2AD777DPmz59Pw4YNOXr0KE888QTPPPMMixYtum4fhw8f5sMPP+T//u//MJlMjBgxgieeeIKVK1dattm2bRs+Pj5s27aNw4cPM3jwYNq0acPjjz8OwNixY9m3bx+rV6+mbt26fPzxx/Tq1Yvvv/8ef3//a+535syZTJs2rUj7pk2bcHZ2Ls1pKSQxMdFqfUn5OnDSHjCKtp/IIj4+vvwDEqvRdWkblEfboVyWvezs7GJtZxTotWy3LDg4GJPJxO7du6+7zZo1a4iKiuL06dPApRvyJkyYwNmzZ4FLI8cvvfQSP/zwA7fddhsAGzdupE+fPhw/fhxvb28iIyNJSkriyJEj2NvbA3D//fdjZ2fH6tWrycjIoFGjRmRkZFC3bl3Lvnv27EmHDh14+eWXrxnbtUaOfX19OX36NK6urqU6N3DpL7TExERCQ0MtI9xSuQxavIO9x01F2oPqubJ2VKcKiEhKS9elbVAebYdyWX5MJhO1atUiKyvrhnWORo5LqV27doWWN2/ezMyZMzlw4AAmk4mLFy/yxx9/kJ2dfd3R2Pr161sKY4DOnTuTn5/PwYMH8fb2BiAwMNBSGAP4+Pjw/fffA/D999+Tl5dHQEBAoX5zcnLw9Lz+V99OTk44OTkVaXdwcLDqBWrt/qT8jAnxJ2pFClf/CW0YMLa7v3Jayem6tA3Ko+1QLstecc+viuNSql69uuXn9PR0+vbty+jRo5kxYwYeHh589dVXjBgxgtzc3FJNVfhzQg3DID8/H4Dz589jb29PSkpKoQIauO5cZ5HiCA/0ZvGwdizclsaBE1k0q+vG2O7+hAV6V3RoIiIiZULFsRWlpKSQn59PbGwsdnaXHgTy4Ycf3vRzGRkZnDhxwjIlYseOHdjZ2dG0adNi7bdt27bk5eVx6tQp7rrrrls/AJFrCA/0JiTAk/j4eCIiOmlkQ0REbJoe5WZFTZo0wWw2s2DBAo4ePcry5ctZvHjxTT9XtWpVHn74Yb777ju+/PJLxo8fz/3332+ZUnEzAQEBDB06lOHD/1979x0WxfH/Afx99N47IigCIhYUpFlAxGBvsROxYIlYQMUexRLFii3GkiiowRpL/NqxYMEKghUBkWIBuwIifX5/APvzpB1wxyl8Xs/Dozs7O/vZmd1jmJvd9cThw4eRmJiIW7duISAgACdOnKjpYRFCCCGE1BvUORaiVq1aITAwECtWrEDz5s0REhKCgICASrdr0qQJ+vfvj+7du+Onn35Cy5YtK3y6RVmCgoLg6emJ6dOnw8LCAn379sXt27fRsGHD6h4OIYQQQki9Q0+rELOS5xxHR0eLOxSkp6dDVVW10rs4BZWXl1f8VXx3+ir+B0dtWXdQW9YN1I51B7Vl7RG0n0Mjx4QQQgghhBSjzjEhhBBCCCHFqHMsZgsXLvwuplQQQgghhBDqHBNCCCGEEMKhzjEhhBBCCCHFqHNMCCGEEEJIse+6cxwWFgYej4ePHz+KO5QqMTExwbp16wTKm5aWhi5dukBRURFqamoijYsQQgghhFTsu+4ci1JwcPB30Rldu3YtUlNTER0djbi4OHGHQ0gpZx6m4ectNzDjpiR+3nIDZx6miTskQgghRGTqbef4e5GQkAAbGxuYmZlBR0enzDx5eXm1HBUhRc48TMP43ZG49yIduYU83HuRjl//iaQOMiGEkDpLStwB5OTkYMaMGdi3bx/S09Nha2uLtWvXom3btlyeyMhIzJo1C48ePYK1tTWCgoJgYWFRadl3796Fr68vIiIiwOPxYGZmhq1btyIzMxOjRo0CAPB4PACAv78/Fi5ciJycHMybNw979+7Fx48f0bx5c6xYsQIuLi5cuVevXsWcOXMQEREBLS0t9OvXDwEBAVBUVKzSsZuYmCA5ORkAsGvXLowYMQLBwcHg8Xj4888/cerUKZw/fx4zZszA/PnzMW7cOFy4cAFpaWlo2LAhvL294ePjw1fmjh07sGbNGjx58gQaGhr4+eef8ccff5Rb9zk5Odxyeno6gKLOuDA65CVlUOf+x7XpQnypNMaATRfj4WquKYaISE3RdVk3UDvWHdSWtUfQOhZ753jmzJk4dOgQdu7cCWNjY6xcuRLu7u548uQJl2fevHlYs2YNtLW18euvv2L06NEIDw+vtGwPDw+0bt0amzdvhqSkJKKjoyEtLQ0nJyesW7cOCxYsQGxsLABASUkJADBp0iQ8evQI+/btg4GBAY4cOYKuXbvi/v37MDMzQ0JCArp27Yrff/8dO3bswJs3bzBp0iRMmjQJQUFBVTr227dvw9PTEyoqKli/fj3k5eW5dQsXLsTy5cuxbt06SElJobCwEA0aNMDBgwehqamJa9euYdy4cdDX18egQYMAAJs3b8a0adOwfPlydOvWDZ8+faqwngICArBo0aJS6WfPnoWCgkKVjqUioaGhQiuL1K7HqZIAeKXTX37CyZMnaz8gIjR0XdYN1I51B7Wl6GVlZQmUj8cYYyKOpVyfP3+Guro6goODMWzYMABFvXoTExP4+vqibdu26NSpE86dO4fOnTsDAE6ePIkePXrgy5cvkJOTq7B8FRUVbNy4ESNGjCi1Ljg4GL6+vnw3+6WkpKBx48ZISUmBgYEBl+7m5gY7OzssW7YMY8aMgaSkJLZu3cqtv3r1KpydnfH582fIyclx8fv6+lZaB3379oWamhqCg4O5NB6PB19fX6xdu7bCbSdNmoS0tDT8+++/AABDQ0OMGjUKv//+e6X7BcoeOTYyMsLbt28rfOe4oPLy8hAaGoouXbrQ++J/UD9vuYF7L9JLpbdsoIJD4x3EEBGpKbou6wZqx7qD2rL2pKenQ0tLC58+faqwnyPWkeOEhATk5eWhXbt2XJq0tDTs7OwQExPDTa1o2bIlt15fXx8A8Pr1azRs2LDC8qdNm4YxY8Zg9+7dcHNzw8CBA2Fqalpu/vv376OgoADm5uZ86Tk5OdDULPoK+e7du7h37x5CQkK49YwxFBYWIjExEZaWlgIefcVsbW1LpW3atAk7duxASkoKvnz5gtzcXFhbWwMoqo+XL19yf0QIQlZWFrKysqXSpaWlhXqBCrs8Unsmuprh138i8fWf0DweMKmTGbXpD46uy7qB2rHuoLYUPUHrV+zTKgTx9cGUzBEuLCysdLuFCxdi2LBhOHHiBE6dOgV/f3/s27cP/fr1KzN/ZmYmJCUlERkZCUlJSb51JdMuMjMzMX78eEyZMqXU9pV11qvi2/nL+/btg5+fH9asWQNHR0coKytj1apVuHnzJgDwTckgRFjcrfSw5RcbbLoYj8cvP6GpgSomdTLDT1Z64g6NEEIIEQmxdo5NTU0hIyOD8PBwGBsbAyj6euH27dsCTUkQhLm5OczNzTF16lQMHToUQUFB6NevH2RkZFBQUMCXt3Xr1igoKMDr16/RoUOHMstr06YNHj16hCZNmgglPkGFh4fDyckJ3t7eXFpCQgL3f2VlZZiYmOD8+fPo1KlTrcZG6jZ3Kz24mmvi5MmT6N7dgUY2CCGE1GlifZSboqIiJkyYgBkzZuD06dN49OgRxo4di6ysLHh5edWo7C9fvmDSpEkICwtDcnIywsPDcfv2bW7ag4mJCTIzM3H+/Hm8ffsWWVlZMDc3h4eHBzw9PXH48GEkJibi1q1bCAgIwIkTJwAAs2bNwrVr1zBp0iRER0cjPj4e//33HyZNmlTj+qiImZkZIiIicObMGcTFxWH+/Pm4ffs2X56FCxdizZo12LBhA+Lj43Hnzh1s3LhRpHERQgghhNQlYp9WsXz5chQWFmL48OHIyMiAra0tzpw5A3V19RqVKykpiXfv3sHT0xOvXr2ClpYW+vfvzz2dwcnJCb/++isGDx6Md+/ecY9yCwoKwu+//47p06fjxYsX0NLSgoODA3r27AmgaP7zpUuXMG/ePHTo0AGMMZiammLw4ME1rouKjB8/HlFRURg8eDB4PB6GDh0Kb29vnDp1isszYsQIZGdnY+3atfDz84OWlhYGDBgg0rgIIYQQQuoSsT6tgnxf0tPToaqqWuldnILKy8sr/iq+O30V/4Ojtqw7qC3rBmrHuoPasvYI2s+hN+QRQgghhBBS7IfuHFtZWUFJSanMn68ftSYuISEh5cZnZWUl7vAIIYQQQsg3xD7nuCZOnjxZ7qsAdXV1azma0nr37g17e/sy19FXJ4QQQggh358funNc8vi375WysjKUlZXFHQYhhBBCCBHQDz2tghBCCCGEEGH6oUeOCSGEEPJ9YIwhPz+/1Au2SMXy8vIgJSWF7OxsqrsakpSUhJSUFPc25eqq951jxhjGjx+Pf//9Fx8+fICqqipGjhyJdevW1cr+O3bsiF9//RXDhg0TWpmnT5/G7NmzcefOHUhI0JcDhBBCRCs3NxepqanIysoSdyg/HMYY9PT08OzZsxp36gigoKAAfX19yMjIVLuMet85Pn36NIKDgxEWFobGjRtDQkIC8vLytbLvY8eO4dWrVxgyZAiXtm3bNuzZswd37txBRkYGPnz4ADU1Nb7tevfujejoaLx+/Rrq6upwc3PDihUrYGBgAADo2rUr5s+fj5CQEAwfPrxWjoUQQkj9VFhYiMTEREhKSsLAwAAyMjLUyauCwsJCZGZmQklJiQa0aoAxhtzcXLx58waJiYkwMzOrdn3W+85xQkIC9PX14eTkVOv73rBhA0aNGsXXeFlZWejatSu6du2KOXPmlLldp06dMHfuXOjr6+PFixfw8/PDgAEDcO3aNS7PyJEjsWHDBuockxo78zANmy7E43GqJLan3MBEVzO4W+mJOyxCyHciNzcXhYWFMDIygoKCgrjD+eEUFhYiNzcXcnJy1DmuIXl5eUhLSyM5OZmr0+qo160wcuRITJ48GSkpKeDxeDAxMYGLiwt8fX25PCYmJvj999/h6ekJJSUlGBsb49ixY3jz5g369OkDJSUltGzZEhEREdw2wcHBUFNTw9GjR2FmZgY5OTm4u7vj2bNnXJ43b97gwoUL6NWrF19Mvr6+mD17NhwcHMqNe+rUqXBwcICxsTGcnJwwe/Zs3Lhxg++xdr169UJERAQSEhKEUFOkvjrzMA3jd0fi3ot05BbycO9FOn79JxJnHqaJOzRCyHeGOnbkeyCM87BejxyvX78epqam2LZtG27fvg1JSUkMHDiwVL61a9di2bJlmD9/PtauXYvhw4fDyckJo0ePxqpVqzBr1ix4enri4cOH3FdJWVlZWLp0KXbt2gUZGRl4e3tjyJAhCA8PBwBcvXoVCgoKsLS0rNExvH//HiEhIXBycuJ7dnLDhg2hq6uLK1euwNTUtMxtc3JykJOTwy2np6cDKLo5oLznR1dFSRnCKIuIx6YL8aXSGAM2XYyHq7mmGCIiNUXXZd3wPbVjXl4eGGMoLCxEYWGhuMP54TDGuH+p/mqusLAQjDHk5eVBUlKSb52g10u97hyrqqpCWVkZkpKS0NMr/2vi7t27Y/z48QCABQsWYPPmzWjbti3XkZ41axYcHR3x6tUrrpy8vDz88ccf3EtAdu7cCUtLS9y6dQt2dnZITk6Grq5utf/CmTVrFv744w9kZWXBwcEBx48fL5XHwMAAycnJ5ZYREBCARYsWlUo/e/asUL8aCw0NFVpZpHY9TpUEUHru4OOXn3Dy5MnaD4gIDV2XdcP30I5SUlLQ09NDZmYmcnNzxR3ODysjI0PcIdQJubm5+PLlCy5fvoz8/Hy+dYLeMFqvO8eCatmyJff/kjfvtWjRolTa69evuc6xlJQU2rZty+Vp2rQp1NTUEBMTAzs7O3z58qXac2EAYMaMGfDy8kJycjIWLVoET09PHD9+nO8mCHl5+QpPhDlz5mDatGnccnp6OoyMjPDTTz9BRUWl2rGVyMvLQ2hoKLp06UJvBPxBbU+5gXsv0kulNzVQRffu5U/9Id8vui7rhu+pHbOzs/Hs2TMoKSnV6PeaOLi6uqJVq1ZYu3at2GJgjCEjIwPKyspCu5FRUlIShw4dQt++fYVSnrAEBwdj2rRpeP/+vcj2kZ2dDXl5eXTs2LHU+VjyDXllqHMsgK8/eEpO3LLSqvJ1iJaWFj58+FDtmLS0tKClpQVzc3NYWlrCyMgIN27cgKOjI5fn/fv30NbWLrcMWVlZyMrKlkqXlpYW6oetsMsjtWeiqxl+/ScSxd/6AQB4PGBSJzNq0x8cXZd1w/fQjgUFBeDxeJCQkPgh5x2XxC4uJX2HsuLg8Xg4cuRItTq532N7lMQjaFx5eXn47bffcPLkSTx9+hSqqqpwc3PD8uXLuSd0lbUPHo9X5rUh6LXyfdVaHZKfn893k15sbCw+fvzIzTFu3bo10tLSatRBLlFyYX09fzg7OxsJCQlo3bp1jcsn9Ze7lR62/GKDlg1UICPB0LKBCrb+YoOf6GkVhBARKChkuJ7wDv9Fv8D1hHcoKGSVbyRGJS8+IaKRlZWFO3fuYP78+bhz5w4OHz6M2NhY9O7dW6T7pc6xiEhLS2Py5Mm4efMmIiMjMXLkSDg4OMDOzg5AUedYS0uLu0GvRFpaGqKjo/HkyRMAwP379xEdHc19BXHz5k388ccfiI6ORnJyMi5cuIChQ4fC1NSUb9T4xo0bkJWV5UsjpDrcrfRwaLwDVtkX4NB4B+oYE0JE4vSDVLRfcQFD/7oBn33RGPrXDbRfcQGnH6TWWgy7d++Gra0tlJWVoaenh2HDhuH169fc+rCwMPB4PJw6dQo2NjaQlZXF1atXkZGRAQ8PDygqKkJfXx9r164t9fSrnJwc+Pn5wdDQEIqKirC3t0dYWFi5sZiYmAAA+vXrxz1Rq8TmzZthamoKGRkZWFhYYPfu3RUel7+/P/T19XHv3j0ARfctmZubQ0FBAY0bN8b8+fP5blZbuHAhrK2tsWPHDjRs2BBKSkrw9vZGQUEBVq5cCT09Pejo6GDp0qV8+wkMDESLFi2gqKgIIyMjeHt7IzMzs9y43rx5A1tbW/Tr149vgK+EqqoqQkNDMWjQIFhYWMDBwQF//PEHIiMjkZKSUuEx1wR1jkVEQUEBs2bNwrBhw9CuXTsoKSlh//793HpJSUmMGjUKISEhfNtt2bIFrVu3xtixYwEUvUGvdevWOHbsGFfu4cOH0blzZ1hYWMDLywstW7bEpUuX+KZI7N27Fx4eHvTMSUIIId+90w9SMeGfO0j9lM2XnvYpGxP+uVNrHeS8vDwsWbIEd+/exdGjR5GUlISRI0eWyjd79mwsX74cMTExaNmyJaZNm4bw8HAcO3YMoaGhuHLlCu7cucO3zaRJk3D9+nXs27cP9+7dw8CBA9G1a1fEx5d+KhAA3L59GwAQFBSE1NRUbvnIkSPw8fHB9OnT8eDBA4wfPx6jRo3CxYsXS5XBGMPkyZOxa9cuXLlyhbuHSllZGcHBwXj06BHWr1+Pv/76q9S864SEBJw6dQqnT5/G3r17sX37dvTo0QPPnz/HpUuXsGLFCvz222+4efMmt42EhAQ2bNiAhw8fYufOnbhw4QJmzpxZ5vE9e/YMHTp0QPPmzfHvv/+WOc2zLJ8+fQKPxyv1gjShYkTogoKCmKqqaqX5UlNTmYaGBktKShLq/t+8ecM0NDTY06dPq7Tdp0+fGAD26dMnocSRm5vLjh49ynJzc4VSHhEfasu6g9qybvie2vHLly/s0aNH7MuXL9XaPr+gkDksO8eMZx0v88dk1nHmsOwcyy8oFHLkjDk7OzMfH59y19++fZsBYBkZGYwxxi5evMgAsKNHj3J50tPTmbS0NDt48CCX9vHjR6agoMCVnZyczCQlJdmLFy/4yu/cuTObPXs2+/DhAysoKCi1fwDsyJEjfGlOTk5s7NixfGkDBw5k3bt359vu4MGDbNiwYczS0pI9f/68wnpYtWoVs7Gx4Zb9/f2ZgoICS09P59Lc3d2ZiYkJX5wWFhYsICCg3HIPHjzINDU1ueWS/tHjx4+ZkZERmzJlCissFLxdv3z5wtq0acOGDRtWYZ7yzkdB+zl0Q54Y6enpYfv27UhJSYGxsbHQyk1KSsKff/6JRo0aCa1MQgghRBRuJb4vNWL8NQYg9VM2biW+h6OpaJ+vHhkZiYULF+Lu3bv48OEDd09PSkoKmjVrxuWztbXl/v/06VPk5eVx0yaBoukAFhYW3PL9+/dRUFAAc3Nzvv3l5ORAQ0OjSjHGxMRg3LhxfGnt2rXD+vXr+dKmTp0KWVlZ3LhxA1paWnzr9u/fjw0bNiAhIQGZmZnIz88v9ZQqExMTKCsrc8u6urqQlJTku5lOV1eXb9rJuXPnEBAQgMePHyM9PR35+fnIzs5GVlYW9032ly9f0KFDBwwbNgzr1q0T+Ljz8vIwaNAgMMawefNmgberDppWIWZ9+/ZFhw4dhFqmra0tBg8eLNQyCSGEEFF4nVF+x7g6+arr8+fPcHd3h4qKCkJCQnD79m0cOXIEAEo9v1lRUbFKZWdmZkJSUhKRkZGIjo7mfmJiYqrUQayKLl264MWLFzhz5gxf+vXr1+Hh4YHu3bvj+PHjiIqKwrx580od47dPdih5AsS3aSV/QCQlJaFnz55o2bIlDh06hMjISGzatAkAf/3JysrCzc0Nx48fx4sXLwQ6lpKOcXJyMkJDQ4XyuNmKUOdYBEaOHImPHz+KOwxCCCHku6ejLNizkQXNV12PHz/Gu3fvsHz5cnTo0AFNmzblGxUtT+PGjSEtLc3NCQaK5sXGxcVxy61bt0ZBQQFev36NJk2a8P1U9BIyaWlpFBQU8KVZWlqWupk/PDycb2QbAHr37o09e/ZgzJgx2LdvH5d+7do1GBsbY968ebC1tYWZmVmFLwwTVGRkJAoLC7FmzRo4ODjA3NwcL1++LJVPQkICu3fvho2NDTp16lRmnq+VdIzj4+Nx7tw5aGqK/u2s1DkmhBBCiNjYNdKAvqpcGe/iLMIDoK8qB7tGVZt+UFUNGzaEjIwMNm7ciKdPn+LYsWNYsmRJpdspKytjxIgRmDFjBi5evIiHDx/Cy8uLe94uAJibm8PDwwOenp44fPgwEhMTcevWLQQEBODEiRPllm1iYoLz58/zPfp1xowZCA4OxubNmxEfH4/AwEAcPnwYfn5+pbbv168fdu/ejVGjRuHff/8FAJiZmSElJQX79u1DQkICNmzYwI2Q10STJk2Ql5fH1d/u3buxZcuWMvNKSkoiJCQErVq1gqurK9LS0srMl5eXhwEDBiAiIgIhISEoKChAWloa0tLSRPo2RuocE0IIIURsJCV48O9VNOr5bQe5ZNm/VzNISgjn7XHl0dbWRnBwMA4ePIhmzZph+fLlWL16tUDbBgYGwtHRET179oSbmxvatWsHS0tLvje0BQUFwdPTE9OnT4eFhQX69u2L27dvo2HDhuWWu2bNGoSGhsLIyIh7b0Hfvn2xfv16rF69GlZWVti6dSuCgoLg4uJSZhkDBgzAzp07MXz4cBw+fBi9e/fG1KlTMWnSJFhbW+PatWuYP3++4BVVjlatWiEwMBArVqxA8+bNERISgoCAgHLzS0lJYe/evbCysoKrq2uZo/QvXrzAsWPH8Pz5c1hbW0NfX5/7uXbtWo1jLg+PMfZ9P2Gb1Jr09HSoqqri06dPQnt99MmTJ9G9e3exv8GJ1Ay1Zd1BbVk3fE/tmJ2djcTERDRq1KhGr48+/SAVi/73iO/mPH1VOfj3aoauzfWFEWqt+fz5MwwNDbFmzRp4eXlVmLewsBDp6elQUVH57t5o9yOq6HwUtJ9DT6soh4uLC6ytrYU+UX7hwoXYvHkzXr9+Xe1XQhJCCCF1Tdfm+ujSTA+3Et/jdUY2dJSLplKIesRYGKKiovD48WPY2dnh06dPWLx4MQCgT58+Yo6MVAd1jkUgKSkJjRo1QlRUFKytrbn0mJgYLFq0CEeOHIGDgwPU1dXFFyQhhBDynZGU4In8cW2isnr1asTGxkJGRgY2Nja4cuVKqUeokR8DdY6rITc3FzIyMlXeLiEhAUDRX5Ilk/QJIYQQQZx5mIY/Lz5B3KtMmOkooq0SD93FHRQBUPQ0isjISHGHQYSEJregaG6Qp6cnlJSUoK+vjzVr1vCtNzExwZIlS+Dp6QkVFZVSD9/+VsnLN1q3bg0ejwcXFxcsXLgQvXr1AgC+O1jL8+DBA0hISODNmzcAgPfv30NCQgJDhgzh8vz+++9o3749gP9/3/uJEyfQsmVLyMnJwcHBAQ8ePKhaZRBCCPnunHmYhvG7I3H3+Sd8ySvAvRfp2BErgdBHlT9qjBBSNTRyjKLHoly6dAn//fcfdHR0MHfuXNy5c4dvSsTq1auxYMEC+Pv7V1rerVu3YGdnh3PnzsHKygoyMjKQkZGBiYkJRo0ahdTUyt8Rb2VlBU1NTVy6dAkDBgzAlStXuOUSly5dKnV36owZM7B+/Xro6elh7ty56NWrF+Li4sq8YSMnJwc5OTnccnp6OoCiGz3y8vIqjbEyJWUIoywiXtSWdQe15Y9p04X4UmkMPGy+lIAuzXTEENH/y8/PB2MMBQUF3AshiOBKnovAGKP6E4KCggIwxpCfn1/qc07Qz7163znOzMzE9u3b8c8//6Bz584AgJ07d6JBgwZ8+VxdXTF9+nSBytTW1gYAaGpq8j3cW01NDQAqfOB3CR6Ph44dOyIsLAwDBgxAWFgYRo0ahb///huPHz+Gqakprl27hpkzZ/Jt5+/vjy5duvAdx5EjRzBo0KBS+wgICMCiRYtKpZ89e5Z7zaMwhIaGCq0sIl7UlnUHteWP5XGqJEo/6AyITUvHyZMnaz+gr/B4POjr6+P9+/d8rxsmVZORkSHuEOqEjIwMfP78GRcuXMC3D2TLysoSqIx63zlOSEhAbm4u7O3tuTQNDQ2+d6ID/O9Rry3Ozs7Ytm0bgKJR4mXLliEuLg5hYWF4//498vLy0K5dO75tHB0duf+XHEdMTEyZ5c+ZMwfTpk3jltPT02FkZISffvpJaI9yCw0NRZcuXcT+qCFSM9SWdQe15Y9pe8oN3HuRXirdQk8F3bs7lrFF7Xr16hXS09MhJycHBQUFuq+mChhj+Pz5MxQVFaneaoAxhqysLGRkZEBfX5/v2/8SJd+QV6bed44FVdX3qAuDi4sLfH19ER8fj0ePHqF9+/Z4/PgxwsLC8OHDB9ja2tZohFdWVhaysrKl0qWlpYX6S1PY5RHxobasO6gtfywTXc3w6z+R+HogjAcGbxfT76IdDQ0NISkpibdv34o7lB8OYwxfvnyBvLw8dY6FQF1dHXp6emXWpaDXSr3vHJuaFn2w3Lx5k3tLzYcPHxAXFwdnZ+dqlVnyJItv34deVS1atIC6ujp+//13WFtbQ0lJCS4uLlixYgU+fPhQ5ttwbty4Ueo4LC0taxQHIYQQ8XK30sOWX2zwZ1gC4l9loImOIuwUP8DNUrzzjUuUTK3Q0dGh+exVlJeXh8uXL6Njx47fxR86PzJpaWlISkrWuJx63zlWUlKCl5cXZsyYAU1NTejo6GDevHk1ekuNjo4O5OXlcfr0aTRo0ABycnJQVVWtcjkl845DQkK4d6a3bNkSOTk5OH/+PN+UiBKLFy+GpqYmdHV1MW/ePGhpadGLRgghpA5wt9KDu1XRPSslb8j73khKSgqlc1KfSEpKIj8/H3JyctQ5/k7Qo9wArFq1Ch06dECvXr3g5uaG9u3bw8bGptrlSUlJYcOGDdi6dSsMDAxq9IYcZ2dnFBQUcKPEEhIS6NixI3g8Xqn5xgCwfPly+Pj4wMbGBmlpafjf//5XrWcyE0IIIYTUR/V+5BgoGj3evXs3du/ezaXNmDGD+39SUlKVyxwzZgzGjBnDl9a3b99Sd05WxtfXF76+vnxpR48eLTd/+/bt6dnGhBBCCCHVRCPHhBBCCCGEFKOR42pYtmwZli1bVua6Dh064NSpUwKVo6SkVO66U6dOoUOHDtWKr7pKRrUFfdRJZfLy8pCVlYX09HSaR/WDo7asO6gt6wZqx7qD2rL2lPRvKvsWn8eq+j0/wfv37/H+/fsy18nLy8PQ0FCgcp48eVLuOkNDQ8jLy1crvup6/vw5jIyManWfhBBCCCG16dmzZ6Ve9vY16hwTTmFhIV6+fAllZWWhPGux5KUiz549E8pLRYj4UFvWHdSWdQO1Y91BbVl7GGPIyMiAgYFBhU8lo2kVhCMhIVHhX1LVpaKiQhd8HUFtWXdQW9YN1I51B7Vl7RDk0bp0Qx4hhBBCCCHFqHNMCCGEEEJIMeocE5GRlZWFv78/ZGVlxR0KqSFqy7qD2rJuoHasO6gtvz90Qx4hhBBCCCHFaOSYEEIIIYSQYtQ5JoQQQgghpBh1jgkhhBBCCClGnWNCCCGEEEKKUeeY1Mj79+/h4eEBFRUVqKmpwcvLC5mZmRVuk52djYkTJ0JTUxNKSkr4+eef8erVK748PB6v1M++fftEeSj1yqZNm2BiYgI5OTnY29vj1q1bFeY/ePAgmjZtCjk5ObRo0QInT57kW88Yw4IFC6Cvrw95eXm4ubkhPj5elIdAigm7LUeOHFnq2uvatasoD4EUq0pbPnz4ED///DNMTEzA4/Gwbt26GpdJhEPY7bhw4cJS12TTpk1FeASEOsekRjw8PPDw4UOEhobi+PHjuHz5MsaNG1fhNlOnTsX//vc/HDx4EJcuXcLLly/Rv3//UvmCgoKQmprK/fTt21dER1G/7N+/H9OmTYO/vz/u3LmDVq1awd3dHa9fvy4z/7Vr1zB06FB4eXkhKioKffv2Rd++ffHgwQMuz8qVK7FhwwZs2bIFN2/ehKKiItzd3ZGdnV1bh1UviaItAaBr1658197evXtr43Dqtaq2ZVZWFho3bozly5dDT09PKGWSmhNFOwKAlZUV3zV59epVUR0CAQBGSDU9evSIAWC3b9/m0k6dOsV4PB578eJFmdt8/PiRSUtLs4MHD3JpMTExDAC7fv06lwaAHTlyRGSx12d2dnZs4sSJ3HJBQQEzMDBgAQEBZeYfNGgQ69GjB1+avb09Gz9+PGOMscLCQqanp8dWrVrFrf/48SOTlZVle/fuFcERkBLCbkvGGBsxYgTr06ePSOIl5atqW37N2NiYrV27VqhlkuoRRTv6+/uzVq1aCTFKUhkaOSbVdv36daipqcHW1pZLc3Nzg4SEBG7evFnmNpGRkcjLy4ObmxuX1rRpUzRs2BDXr1/nyztx4kRoaWnBzs4OO3bsAKNHctdYbm4uIiMj+epfQkICbm5upeq/xPXr1/nyA4C7uzuXPzExEWlpaXx5VFVVYW9vX26ZpOZE0ZYlwsLCoKOjAwsLC0yYMAHv3r0T/gEQTnXaUhxlkoqJss7j4+NhYGCAxo0bw8PDAykpKTUNl1SAOsek2tLS0qCjo8OXJiUlBQ0NDaSlpZW7jYyMDNTU1PjSdXV1+bZZvHgxDhw4gNDQUPz888/w9vbGxo0bhX4M9c3bt29RUFAAXV1dvvRv6/9raWlpFeYv+bcqZZKaE0VbAkVTKnbt2oXz589jxYoVuHTpErp164aCggLhHwQBUL22FEeZpGKiqnN7e3sEBwfj9OnT2Lx5MxITE9GhQwdkZGTUNGRSDilxB0C+P7Nnz8aKFSsqzBMTEyPSGObPn8/9v3Xr1vj8+TNWrVqFKVOmiHS/hNR3Q4YM4f7fokULtGzZEqampggLC0Pnzp3FGBkh9VO3bt24/7ds2RL29vYwNjbGgQMH4OXlJcbI6i4aOSalTJ8+HTExMRX+NG7cGHp6eqVuMsjPz8f79+/LvbFAT08Pubm5+PjxI1/6q1evKrwZwd7eHs+fP0dOTk6Nj68+09LSgqSkZKmng1RU/3p6ehXmL/m3KmWSmhNFW5alcePG0NLSwpMnT2oeNClTddpSHGWSitVWnaupqcHc3JyuSRGizjEpRVtbG02bNq3wR0ZGBo6Ojvj48SMiIyO5bS9cuIDCwkLY29uXWbaNjQ2kpaVx/vx5Li02NhYpKSlwdHQsN6bo6Gioq6tDVlZWeAdaD8nIyMDGxoav/gsLC3H+/Ply69/R0ZEvPwCEhoZy+Rs1agQ9PT2+POnp6bh582aFbUpqRhRtWZbnz5/j3bt30NfXF07gpJTqtKU4yiQVq606z8zMREJCAl2ToiTuOwLJj61r166sdevW7ObNm+zq1avMzMyMDR06lFv//PlzZmFhwW7evMml/frrr6xhw4bswoULLCIigjk6OjJHR0du/bFjx9hff/3F7t+/z+Lj49mff/7JFBQU2IIFC2r12Oqqffv2MVlZWRYcHMwePXrExo0bx9TU1FhaWhpjjLHhw4ez2bNnc/nDw8OZlJQUW716NYuJiWH+/v5MWlqa3b9/n8uzfPlypqamxv777z9279491qdPH9aoUSP25cuXWj+++kTYbZmRkcH8/PzY9evXWWJiIjt37hxr06YNMzMzY9nZ2WI5xvqiqm2Zk5PDoqKiWFRUFNPX12d+fn4sKiqKxcfHC1wmET5RtOP06dNZWFgYS0xMZOHh4czNzY1paWmx169f1/rx1RfUOSY18u7dOzZ06FCmpKTEVFRU2KhRo1hGRga3PjExkQFgFy9e5NK+fPnCvL29mbq6OlNQUGD9+vVjqamp3PpTp04xa2trpqSkxBQVFVmrVq3Yli1bWEFBQW0eWp22ceNG1rBhQyYjI8Ps7OzYjRs3uHXOzs5sxIgRfPkPHDjAzM3NmYyMDLOysmInTpzgW19YWMjmz5/PdHV1maysLOvcuTOLjY2tjUOp94TZlllZWeynn35i2traTFpamhkbG7OxY8dSZ6qWVKUtSz5bv/1xdnYWuEwiGsJux8GDBzN9fX0mIyPDDA0N2eDBg9mTJ09q8YjqHx5j9HwsQgghhBBCAJpzTAghhBBCCIc6x4QQQgghhBSjzjEhhBBCCCHFqHNMCCGEEEJIMeocE0IIIYQQUow6x4QQQgghhBSjzjEhhBBCCCHFqHNMCCGEEEJIMeocEyIkLi4u8PX1FXcY353g4GCoqalxywsXLoS1tbVI98nj8XD06NFy14uircLCwsDj8fDx40eBtxk5ciT69u0r9HJr41wUJHZSxMTEBOvWreOWKzs/a6o2rrES3x5bXZCUlAQej4fo6Ghxh1JKbbZtfUadY1Lv9erVC127di1z3ZUrV8Dj8XDv3r1ajqru8vPzw/nz58UdhtA5OTkhNTUVqqqqAm+zfv16BAcHc8tldWqrUy75vqWmpqJbt25i2391/uD6EX3PndzatG3bNri4uEBFRaVetLswUOeY1HteXl4IDQ3F8+fPS60LCgqCra0tWrZsKYbIak9eXl6t7UtJSQmampq1tr/aIiMjAz09PfB4PIG3UVVV5RtVF1a5pGpyc3NrdX96enqQlZWt1X1+rwoKClBYWCjuMOq0rKwsdO3aFXPnzhV3KD8M6hyTeq9nz57Q1tbmG8EDgMzMTBw8eBBeXl549+4dhg4dCkNDQygoKKBFixbYu3dvheWW9dWpmpoa336ePXuGQYMGQU1NDRoaGujTpw+SkpLKLbNkxOf8+fOwtbWFgoICnJycEBsby5dv8+bNMDU1hYyMDCwsLLB79+5SsW3evBm9e/eGoqIili5dyn1dt2PHDjRs2BBKSkrw9vZGQUEBVq5cCT09Pejo6GDp0qV8ZQUGBqJFixZQVFSEkZERvL29kZmZWe4xfPu1YFhYGOzs7KCoqAg1NTW0a9cOycnJ3Pr//vsPbdq0gZycHBo3boxFixYhPz+fWx8fH4+OHTtCTk4OzZo1Q2hoaLn7/lp+fj4mTZoEVVVVaGlpYf78+WCMAQAWL16M5s2bl9rG2toa8+fPL7O8b0fjSqaTnDlzBpaWllBSUkLXrl2RmprKbfP11ISRI0fi0qVLWL9+PXg8Hng8HpKSkkqVW51z8WtxcXHg8Xh4/PgxX/ratWthamoKoKjD4uXlhUaNGkFeXh4WFhZYv359heWW9fW6tbU1Fi5cyC1//PgRY8aMgba2NlRUVODq6oq7d+8KHDtQNLo+ZcoUzJw5ExoaGtDT0+PbBwCkpKSgT58+UFJSgoqKCgYNGoRXr15x60vOwb///huNGjWCnJwcgKLrYuvWrejZsycUFBRgaWmJ69ev48mTJ3BxcYGioiKcnJyQkJDAlZWQkIA+ffpAV1cXSkpKaNu2Lc6dO1fhMXz92ZCbm4tJkyZBX18fcnJyMDY2RkBAQJXqbPny5dDV1YWysjK8vLyQnZ1d7r6TkpLQqVMnAIC6ujp4PB5GjhwJAMjJycGUKVOgo6MDOTk5tG/fHrdv367wWL5V2edByXVx7NgxNGvWDLKyskhJSUFqaip69OgBeXl5NGrUCHv27Cl1TlX1/GnUqBEAoHXr1uDxeHBxcQEAFBYWYvHixWjQoAFkZWVhbW2N06dPl1tOQUEBRo8ejaZNmyIlJUWg66Pk2l62bBl0dXWhpqaGxYsXIz8/HzNmzICGhgYaNGiAoKAgvu1mzZoFc3NzKCgooHHjxpg/f36FgxcJCQlo3LgxJk2axH1+fcvX1xezZ8+Gg4NDueUQftQ5JvWelJQUPD09ERwczPfhcvDgQRQUFGDo0KHIzs6GjY0NTpw4gQcPHmDcuHEYPnw4bt26Ve395uXlwd3dHcrKyrhy5QrCw8O5DlRlI1nz5s3DmjVrEBERASkpKYwePZpbd+TIEfj4+GD69Ol48OABxo8fj1GjRuHixYt8ZSxcuBD9+vXD/fv3ue0TEhJw6tQpnD59Gnv37sX27dvRo0cPPH/+HJcuXcKKFSvw22+/4ebNm1w5EhIS2LBhAx4+fIidO3fiwoULmDlzpkB1kJ+fj759+8LZ2Rn37t3D9evXMW7cOG6U9MqVK/D09ISPjw8ePXqErVu3Ijg4mOugFxYWon///pCRkcHNmzexZcsWzJo1S6B979y5E1JSUrh16xbWr1+PwMBA/P333wCA0aNHIyYmhq9jEBUVhXv37mHUqFEClQ8UjdisXr0au3fvxuXLl5GSkgI/P78y865fvx6Ojo4YO3YsUlNTkZqaCiMjo1L5anoumpubw9bWFiEhIXzpISEhGDZsGICiem3QoAEOHjyIR48eYcGCBZg7dy4OHDgg8LGXZeDAgXj9+jVOnTqFyMhItGnTBp07d8b79++rVM7OnTuhqKiImzdvYuXKlVi8eDH3R1FhYSH69OmD9+/f49KlSwgNDcXTp08xePBgvjKePHmCQ4cO4fDhw3xfuy9ZsgSenp6Ijo5G06ZNMWzYMIwfPx5z5sxBREQEGGOYNGkSlz8zMxPdu3fH+fPnERUVha5du6JXr15ISUkR6Fg2bNiAY8eO4cCBA4iNjUVISAhMTEwErrMDBw5g4cKFWLZsGSIiIqCvr48///yz3P0ZGRnh0KFDAIDY2FikpqZyHbuZM2fi0KFD2LlzJ+7cuYMmTZrA3d29Su0jyOdBVlYWVqxYgb///hsPHz6Ejo4OPD098fLlS4SFheHQoUPYtm0bXr9+zbddVc+fkmvi3LlzSE1NxeHDhwEUXWtr1qzB6tWrce/ePbi7u6N3796Ij48vVUZOTg4GDhyI6OhoXLlyBQ0bNhT4+rhw4QJevnyJy5cvIzAwEP7+/ujZsyfU1dVx8+ZN/Prrrxg/fjzft5bKysoIDg7Go0ePsH79evz1119Yu3Ztmcd37949tG/fHsOGDcMff/xB3y4JEyOEsJiYGAaAXbx4kUvr0KED++WXX8rdpkePHmz69OncsrOzM/Px8eGWAbAjR47wbaOqqsqCgoIYY4zt3r2bWVhYsMLCQm59Tk4Ok5eXZ2fOnClznxcvXmQA2Llz57i0EydOMADsy5cvjDHGnJyc2NixY/m2GzhwIOvevTtfbL6+vnx5/P39mYKCAktPT+fS3N3dmYmJCSsoKODSLCwsWEBAQJnxMcbYwYMHmaamJrccFBTEVFVV+fbTqlUrxhhj7969YwBYWFhYmWV17tyZLVu2jC9t9+7dTF9fnzHG2JkzZ5iUlBR78eIFt/7UqVNl1v3XnJ2dmaWlJV/dz5o1i1laWnLL3bp1YxMmTOCWJ0+ezFxcXMots6RtPnz4wB03APbkyRMuz6ZNm5iuri63PGLECNanTx++uL4+h8oqtyyVnYvfWrt2LTM1NeWWY2NjGQAWExNT7jYTJ05kP//8c7mxGxsbs7Vr1/Jt06pVK+bv788YY+zKlStMRUWFZWdn8+UxNTVlW7duLXe/33J2dmbt27fnS2vbti2bNWsWY4yxs2fPMklJSZaSksKtf/jwIQPAbt26xRgrOgelpaXZ69ev+coBwH777Tdu+fr16wwA2759O5e2d+9eJicnV2GMVlZWbOPGjdzyt3Xz9fk5efJk5urqynculhCkzhwdHZm3tzffent7e+4aK0tZ51RmZiaTlpZmISEhXFpubi4zMDBgK1euLLesstr9a2V9HgBg0dHRXFrJ5+/t27e5tPj4eAaAK7s6509iYiIDwKKiovjSDQwM2NKlS/nS2rZty9VjyXZXrlxhnTt3Zu3bt2cfP34s9xgZK/v6MDY2LvXZ2aFDB245Pz+fKSoqsr1795Zb7qpVq5iNjQ23XPL5GR4eztTV1dnq1asrjOtrgnyWkCI0ckwIgKZNm8LJyQk7duwAUDSqdOXKFXh5eQEo+lptyZIlaNGiBTQ0NKCkpIQzZ84IPDpUlrt37+LJkydQVlaGkpISlJSUoKGhgezsbL6vbcvy9RxofX19AOBGWWJiYtCuXTu+/O3atUNMTAxfmq2tbalyTUxMoKyszC3r6uqiWbNmkJCQ4Ev7ekTn3Llz6Ny5MwwNDaGsrIzhw4fj3bt3yMrKqqwKoKGhgZEjR8Ld3R29evXC+vXr+aYd3L17F4sXL+bqR0lJiRtZzcrKQkxMDIyMjGBgYMBt4+joWOl+AcDBwYFvpMXR0RHx8fEoKCgAAIwdOxZ79+5FdnY2cnNzsWfPHr4RekEoKChwUxWAorb6djSsqoRxLg4ZMgRJSUm4ceMGgKJR4zZt2qBp06Zcnk2bNsHGxgba2tpQUlLCtm3bany+Z2ZmQlNTk689ExMTKz3fv/XtPQBf12vJOfH1qHuzZs2gpqbGdw0YGxtDW1u7wrJ1dXUBAC1atOBLy87ORnp6OoCikWM/Pz9YWlpCTU0NSkpKiImJEbiuRo4ciejoaFhYWGDKlCk4e/Yst06QOouJiYG9vT1fmYJeA19LSEhAXl4e32eHtLQ07OzsSn12VESQzwMZGRm+eo6NjYWUlBTatGnDpTVp0gTq6urcsrDOn/T0dLx8+VKgz8ihQ4fi8+fPOHv2bKkbYgW5PqysrEp9dn59LklKSkJTU5PvM2H//v1o164d9PT0oKSkhN9++61UuSkpKejSpQsWLFiA6dOnC3zsRHBS4g6AkO+Fl5cXJk+ejE2bNiEoKAimpqZwdnYGAKxatQrr16/HunXruPl0vr6+FU5/4PF4peaAfT13LDMzEzY2NqW+3gZQ5i/tr0lLS/PtB0CVb2pRVFSssNySsstKK9lXUlISevbsiQkTJmDp0qXQ0NDA1atX4eXlhdzcXCgoKFQaR1BQEKZMmYLTp09j//79+O233xAaGgoHBwdkZmZi0aJF6N+/f6ntSuaJikqvXr0gKyuLI0eOQEZGBnl5eRgwYECVyiir7r49J6qqOufit/T09ODq6oo9e/bAwcEBe/bswYQJE7j1+/btg5+fH9asWQNHR0coKytj1apVfNNpviUhIVHp+a6vr4+wsLBS21Z2U+K3KjonBVXW+f9t2SXXVkXXm5+fH0JDQ7F69Wo0adIE8vLyGDBggMDt0aZNGyQmJuLUqVM4d+4cBg0aBDc3N/z7779CrbPaIOjngby8fJWnAIijLrp3745//vkH169fh6urK5cu6PVR1c/T69evw8PDA4sWLYK7uztUVVWxb98+rFmzhm8bbW1tGBgYYO/evRg9ejRUVFSEedgE1DkmhDNo0CD4+Phgz5492LVrFyZMmMB9gIeHh6NPnz745ZdfABT9YoyLi0OzZs3KLU9bW5tvFDQ+Pp5v9KRNmzbYv38/dHR0hPrhZmlpifDwcIwYMYJLCw8PrzDW6oqMjERhYSHWrFnDjZBUZ15q69at0bp1a8yZMweOjo5cp61NmzaIjY1FkyZNytzO0tISz549Q2pqKjeCXjIaWplvf5HduHEDZmZmkJSUBFA0F33EiBEICgqCjIwMhgwZAnl5+SofW1XIyMhwI9flqc65WBYPDw/MnDkTQ4cOxdOnTzFkyBC+fTg5OcHb25tLq2x07tvzPT09HYmJidxymzZtkJaWBikpKb45tcJWck48e/aMGz1+9OgRPn78KJJrIDw8HCNHjkS/fv0AFHXiKrqptiwqKioYPHgwBg8ejAEDBqBr1654//69QHVmaWmJmzdvwtPTk0ur7BqQkZEBAL5zreQG3vDwcBgbGwMo+uPm9u3bAj8zu7qfBxYWFsjPz0dUVBRsbGwAFH179+HDBy5Pdc6fso5TRUUFBgYGCA8P5wY/gKJ2tLOz49t+woQJaN68OXr37o0TJ05w+atzfQji2rVrMDY2xrx587i0r29OLiEvL4/jx4+je/fucHd3x9mzZ/m+8SM1R9MqCCmmpKSEwYMHY86cOUhNTeXu4AYAMzMzhIaG4tq1a4iJicH48eP57n4vi6urK/744w9ERUUhIiICv/76K9+ogYeHB7S0tNCnTx9cuXIFiYmJCAsLw5QpU8p8rJygZsyYgeDgYGzevBnx8fEIDAzE4cOHy70RrCaaNGmCvLw8bNy4EU+fPsXu3buxZcsWgbdPTEzEnDlzcP36dSQnJ+Ps2bOIj4+HpaUlAGDBggXYtWsXFi1ahIcPHyImJgb79u3Db7/9BgBwc3ODubk5RowYgbt37+LKlSt8v1gqkpKSgmnTpiE2NhZ79+7Fxo0b4ePjw5dnzJgxuHDhAk6fPl3lKRXVYWJigps3byIpKQlv374tczS0OudiWfr374+MjAxMmDABnTp14puaYmZmhoiICJw5cwZxcXGYP39+pU8tcHV1xe7du3HlyhXcv38fI0aM4P7QAIraytHREX379sXZs2eRlJSEa9euYd68eYiIiKhy/OVxc3NDixYt4OHhgTt37uDWrVvw9PSEs7NzmVOJasrMzIy7qe/u3bsYNmxYlUaxAwMDsXfvXjx+/BhxcXE4ePAg9PT0oKamJlCd+fj4YMeOHQgKCkJcXBz8/f3x8OHDCvdpbGwMHo+H48eP482bN8jMzISioiImTJiAGTNm4PTp03j06BHGjh2LrKwsbnpZZar7edC0aVO4ublh3LhxuHXrFqKiojBu3Di+EebqnD86OjqQl5fH6dOn8erVK3z69AlA0WfkihUrsH//fsTGxmL27NmIjo4udf0DwOTJk/H777+jZ8+euHr1KoDqXR+CMDMzQ0pKCvbt24eEhARs2LABR44cKTOvoqIiTpw4ASkpKXTr1q3CJwSlpaUhOjoaT548AQDcv38f0dHRVb4Rtj6hzjEhX/Hy8sKHDx/g7u7O11n47bff0KZNG7i7u8PFxQV6enqVvh1szZo1MDIyQocOHTBs2DD4+fnxTTNQUFDA5cuX0bBhQ/Tv3x+WlpbcY5hqMpLct29frF+/HqtXr4aVlRW2bt2KoKAg7jFGwtSqVSsEBgZixYoVaN68OUJCQvgeQ1UZBQUFPH78GD///DPMzc0xbtw4TJw4EePHjwcAuLu74/jx4zh79izatm0LBwcHrF27lhvZkpCQwJEjR/DlyxfY2dlhzJgxpR41Vx5PT09uu4kTJ8LHxwfjxo3jy2NmZgYnJyc0bdq01LxOUfDz84OkpCSaNWsGbW3tMuetVudcLIuysjJ69eqFu3fvwsPDg2/d+PHj0b9/fwwePBj29vZ49+4d3yhZWebMmQNnZ2f07NkTPXr0QN++ffnmW/N4PJw8eRIdO3bEqFGjYG5ujiFDhiA5OZmb21vy0oayvjoXFI/Hw3///Qd1dXV07NgRbm5uaNy4Mfbv31/tMisSGBgIdXV1ODk5oVevXnB3d+ebO1sZZWVlrFy5Era2tmjbti2SkpJw8uRJSEhICFRngwcPxvz58zFz5kzY2NggOTmZb4pMWQwNDbFo0SLMnj0burq63NM3li9fjp9//hnDhw9HmzZt8OTJE5w5c4Zv7m9FavJ5sGvXLujq6qJjx47o168fxo4dC2VlZb7H7FVWF9+SkpLChg0bsHXrVhgYGKBPnz4AgClTpmDatGmYPn06WrRogdOnT+PYsWMwMzMrsxxfX18sWrQI3bt3x7Vr16p1fQiid+/emDp1KiZNmgRra2tcu3at3EdHAkUDOqdOnQJjDD169MDnz5/LzLdlyxa0bt0aY8eOBQB07NgRrVu3xrFjx2occ13FYzWdAEcIIXUUYwxmZmbw9vbGtGnTxB1OnXfx4kX0798fT58+FbhDRuqm58+fw8jIiLvBj5DaRHOOCSGkDG/evMG+ffuQlpZWpWcbk+o7efIk5s6dSx3jeujChQvIzMxEixYtkJqaipkzZ8LExAQdO3YUd2ikHqLOMSGElEFHRwdaWlrYtm0bddZqyapVq8QdAhGTvLw8zJ07F0+fPoWysjKcnJwQEhJS6ukOhNQGmlZBCCGEEEJIMbohjxBCCCGEkGLUOSaEEEIIIaQYdY4JIYQQQggpRp1jQgghhBBCilHnmBBCCCGEkGLUOSaEEEIIIaQYdY4JIYQQQggpRp1jQgghhBBCilHnmBBCCCGEkGLUOSaEEEIIIaQYdY4JIYQQQggpRp1jQgghhBBCilHnmBBCCCGEkGLUOSaEEEIIIaQYdY4JIYQQQggpJiXuAIhgCgsL8fLlSygrK4PH44k7HEIIIYSQHwpjDBkZGTAwMICERPnjw9Q5/kG8fPkSRkZG4g6DEEIIIeSH9uzZMzRo0KDc9dQ5/kEoKysDKGpQFRUVMUdDCCGEEPJjSU9Ph5GREdenKg91jn8QJVMpVFRUqHNMCCGEEFJNlU1PpRvyCCGEEEIIKUadY0IIIYQQQopR55gQQgghhJBi30XneOHChbC2thZ3GJUaOXIk+vbtyy27uLjA19dXbPEQQgghhBDh+i5uyPPz88PkyZPFHUaVHT58GNLS0uIOgxBCxO7MwzT8efEJ4l5lwlxXCd6dmsDdSk/cYRFCSJV9FyPHSkpK0NTUrFEZeXl5Qs0nCA0NjUofB0IIIXXdmYdpGL87Eneff8KXvALcff4Jv/4TiTMP08QdGiGEVFmVOscuLi6YPHkyfH19oa6uDl1dXfz111/4/PkzRo0aBWVlZTRp0gSnTp3itikoKICXlxcaNWoEeXl5WFhYYP369XzlfjutorCwEIsXL0aDBg0gKysLa2trnD59mluflJQEHo+H/fv3w9nZGXJycggJCSkzZh6Ph82bN6N3795QVFTE0qVLBYqpoKAA06ZNg5qaGjQ1NTFz5kwwxkrVx9fTKng8Ho4ePcqXR01NDcHBwQCA3NxcTJo0Cfr6+pCTk4OxsTECAgLKjDsnJwfp6el8P4QQ8j368+KTUmmMAX+GJYghGkIIqZkqjxzv3LkTWlpauHXrFiZPnowJEyZg4MCBcHJywp07d/DTTz9h+PDhyMrKAlDU0W3QoAEOHjyIR48eYcGCBZg7dy4OHDhQ7j7Wr1+PNWvWYPXq1bh37x7c3d3Ru3dvxMfH8+WbPXs2fHx8EBMTA3d393LLW7hwIfr164f79+9j9OjRAsW0Zs0aBAcHY8eOHbh69Srev3+PI0eOVLW6+GzYsAHHjh3DgQMHEBsbi5CQEJiYmJSZNyAgAKqqqtwPvR2PEPK9inuVWWZ6/KuMWo6EEEJqrspzjlu1aoXffvsNADBnzhwsX74cWlpaGDt2LABgwYIF2Lx5M+7duwcHBwdIS0tj0aJF3PaNGjXC9evXceDAAQwaNKjMfaxevRqzZs3CkCFDAAArVqzAxYsXsW7dOmzatInL5+vri/79+1ca87BhwzBq1Ci+tMpiWrduHebMmcOVv2XLFpw5c6bSfVUkJSUFZmZmaN++PXg8HoyNjcvNO2fOHEybNo1bLnmrCyGEfG/MdZVw9/mnUulmujTtjBDy46nyyHHLli25/0tKSkJTUxMtWrTg0nR1dQEAr1+/5tI2bdoEGxsbaGtrQ0lJCdu2bUNKSkqZ5aenp+Ply5do164dX3q7du0QExPDl2ZraytQzGXlqyimT58+ITU1Ffb29lx+KSkpgfdXnpEjRyI6OhoWFhaYMmUKzp49W25eWVlZ7m149FY8Qsj3zLtTE3z7wikeD5joYiqegAghpAaq3Dn+9ukMPB6PL63klXyFhYUAgH379sHPzw9eXl44e/YsoqOjMWrUKOTm5tYkbgCAoqJitfKJKiYej1dqXvLXNwC2adMGiYmJWLJkCb58+YJBgwZhwIABNdonIYSIm7uVHrb8YoNWRmpQkJFEKyM1bP3FBj/R0yoIIT8gkT/KLTw8HE5OTvD29ubSEhLKv0lDRUUFBgYGCA8Ph7OzM185dnZ2tRKTqqoq9PX1cfPmTXTs2BEAkJ+fj8jISLRp06bccrW1tZGamsotx8fHc3OvS6ioqGDw4MEYPHgwBgwYgK5du+L9+/fQ0NAQyrERQog4uFvp0aPbCCF1gsg7x2ZmZti1axfOnDmDRo0aYffu3bh9+zYaNWpU7jYzZsyAv78/TE1NYW1tjaCgIERHR5f7RApRxOTj44Ply5fDzMwMTZs2RWBgID5+/Fhhua6urvjjjz/g6OiIgoICzJo1i29UPTAwEPr6+mjdujUkJCRw8OBB6OnpQU1NTSjHRQghhBBCakbknePx48cjKioKgwcPBo/Hw9ChQ+Ht7c33uLdvTZkyBZ8+fcL06dPx+vVrNGvWDMeOHYOZmVmtxTR9+nSkpqZixIgRkJCQwOjRo9GvXz98+lT6ppMSa9aswahRo9ChQwcYGBhg/fr1iIyM5NYrKytj5cqViI+Ph6SkJNq2bYuTJ09CQuK7eNw0IYQQQki9x2PfTpIVgzlz5uDKlSu4evWquEP5bqWnp0NVVRWfPn2im/MIIYQQQqpI0L6UWIcsGWNISEjA+fPnYWVlJc5QCCGEEEIIEW/n+NOnT2jWrBlkZGQwd+5ccYZCCCGEEEKI6OccV0RNTQ05OTniDOGHUTL7hV4jTQghhBBSdSV9qMpmFIu1c0wEl5FR9BpWekseIYQQQkj1ZWRkQFVVtdz138UNeaRyhYWFePnyJZSVlbkXrdRHJa/RfvbsWb2+MZHqoQjVQxGqh/9HdVGE6qEI1cP/o7ooGjHOyMiAgYFBhU8Ko5HjH4SEhAQaNGgg7jC+G/RK7SJUD0WoHopQPfw/qosiVA9FqB7+X32vi4pGjEvQA3YJIYQQQggpRp1jQgghhBBCilHnmPxQZGVl4e/vD1lZWXGHIlZUD0WoHopQPfw/qosiVA9FqB7+H9WF4OiGPEIIIYQQQorRyDEhhBBCCCHFqHNMCCGEEEJIMeocE0IIIYQQUow6x4QQQgghhBSjzjERm8uXL6NXr14wMDAAj8fD0aNHK8wfFhYGHo9X6ictLY0v34sXL/DLL79AU1MT8vLyaNGiBSIiIkR4JDUjinooKCjA/Pnz0ahRI8jLy8PU1BRLliyp9H3y4lTVegCAnJwczJs3D8bGxpCVlYWJiQl27NjBl+fgwYNo2rQp5OTk0KJFC5w8eVJERyA8oqiLv/76Cx06dIC6ujrU1dXh5uaGW7duifAoak5U50SJffv2gcfjoW/fvsINXMhEVQ8fP37ExIkToa+vD1lZWZibm3/X14eo6mHdunWwsLCAvLw8jIyMMHXqVGRnZ4voKISjqnUxcuTIMn9vWFlZ8eXbtGkTTExMICcnB3t7++/+M0JU6A15RGw+f/6MVq1aYfTo0ejfv7/A28XGxvK93UdHR4f7/4cPH9CuXTt06tQJp06dgra2NuLj46Guri7U2IVJFPWwYsUKbN68GTt37oSVlRUiIiIwatQoqKqqYsqUKUKNX1iqUw+DBg3Cq1evsH37djRp0gSpqakoLCzk1l+7dg1Dhw5FQEAAevbsiT179qBv3764c+cOmjdvLqpDqTFR1EVYWBiGDh0KJycnyMnJYcWKFfjpp5/w8OFDGBoaiupQakQU9VAiKSkJfn5+6NChg7DDFjpR1ENubi66dOkCHR0d/PvvvzA0NERycjLU1NREdBQ1J4p62LNnD2bPno0dO3bAyckJcXFxXEcyMDBQVIdSY1Wti/Xr12P58uXccn5+Plq1aoWBAwdyafv378e0adOwZcsW2NvbY926dXB3d0dsbCzf75d6gRHyHQDAjhw5UmGeixcvMgDsw4cP5eaZNWsWa9++vXCDq0XCqocePXqw0aNH86X179+feXh4CCFK0ROkHk6dOsVUVVXZu3fvys0zaNAg1qNHD740e3t7Nn78eGGEWSuEVRffys/PZ8rKymznzp01jLB2CLMe8vPzmZOTE/v777/ZiBEjWJ8+fYQXqIgJqx42b97MGjduzHJzc4UcYe0QVj1MnDiRubq68qVNmzaNtWvXThhh1gpB6uJbR44cYTwejyUlJXFpdnZ2bOLEidxyQUEBMzAwYAEBAcIK9YdB0yrID8fa2hr6+vro0qULwsPD+dYdO3YMtra2GDhwIHR0dNC6dWv89ddfYopUtCqqBycnJ5w/fx5xcXEAgLt37+Lq1avo1q2bOEIViZK2XrlyJQwNDWFubg4/Pz98+fKFy3P9+nW4ubnxbefu7o7r16/XdrgiJUhdfCsrKwt5eXnQ0NCoxUhFS9B6WLx4MXR0dODl5SWmSEVLkHo4duwYHB0dMXHiROjq6qJ58+ZYtmwZCgoKxBi5cAlSD05OToiMjOSmDzx9+hQnT55E9+7dxRV2rdi+fTvc3NxgbGwMoOibhMjISL7PSwkJCbi5udW5z0tB0LQK8sPQ19fHli1bYGtri5ycHPz9999wcXHBzZs30aZNGwBFH2ybN2/GtGnTMHfuXNy+fRtTpkyBjIwMRowYIeYjEA5B6mH27NlIT09H06ZNISkpiYKCAixduhQeHh5ijl54nj59iqtXr0JOTg5HjhzB27dv4e3tjXfv3iEoKAgAkJaWBl1dXb7tdHV1S81T/9EJUhffmjVrFgwMDEr98fAjE6Qerl69iu3btyM6Olq8wYqQIPXw9OlTXLhwAR4eHjh58iSePHkCb29v5OXlwd/fX8xHIByC1MOwYcPw9u1btG/fHowx5Ofn49dff8XcuXPFHL3ovHz5EqdOncKePXu4tLdv36KgoKDMz8vHjx/XdojiJ+6ha0IYq97XQowx1rFjR/bLL79wy9LS0szR0ZEvz+TJk5mDg0NNQ6wVwqqHvXv3sgYNGrC9e/eye/fusV27djENDQ0WHBwsxGhFR5B66NKlC5OTk2MfP37k0g4dOsR4PB7LyspijBWdD3v27OHbbtOmTUxHR0foMYuKsOriawEBAUxdXZ3dvXtX2OGKjDDqIT09nZmYmLCTJ09y6+vitApBzgczMzNmZGTE8vPzuTxr1qxhenp6Iolb2IRVDxcvXmS6urrsr7/+Yvfu3WOHDx9mRkZGbPHixaIMX6iq+ntj2bJlTFNTk+Xk5HBpL168YADYtWvX+PLOmDGD2dnZCSvUHwaNHJMfmp2dHa5evcot6+vro1mzZnx5LC0tcejQodoOrVZ9Ww8zZszA7NmzMWTIEABAixYtkJycjICAgDo1gm5oaAhVVVUuzdLSEowxPH/+HGZmZtDT08OrV6/4tnv16hX09PRqO1yREqQuSqxevRrLly/HuXPn0LJlS3GEKzKV1cPnz5+RlJSEXr16cetLbs6SkpJCbGwsTE1Naz1uYRPkfNDX14e0tDQkJSX58qSlpSE3NxcyMjLiCF2oBKmH+fPnY/jw4RgzZgyAos/Kz58/Y9y4cZg3bx4kJOrW7FPGGHbs2IHhw4fztbGWlhYkJSXrxeelIOpWq5N6Jzo6Gvr6+txyu3btEBsby5cnLi6Om1dVV31bD1lZWaU+1CUlJcu8a/9H1a5dO7x8+RKZmZlcWlxcHCQkJNCgQQMAgKOjI86fP8+3XWhoKBwdHWs1VlETpC4AYOXKlViyZAlOnz4NW1tbcYQqUpXVQ9OmTXH//n1ER0dzP71790anTp0QHR0NIyMjMUYvPIKcD+3atcOTJ0/4PhPi4uKgr69fJzrGgGD1UN5nJYDv+tGX1XXp0iU8efKk1Hx7GRkZ2NjY8H1eFhYW4vz583Xu81IgYhy1JvVcRkYGi4qKYlFRUQwACwwMZFFRUSw5OZkxxtjs2bPZ8OHDufxr165lR48eZfHx8ez+/fvMx8eHSUhIsHPnznF5bt26xaSkpNjSpUtZfHw8CwkJYQoKCuyff/6p9eMTlCjqYcSIEczQ0JAdP36cJSYmssOHDzMtLS02c+bMWj8+QVW1HjIyMliDBg3YgAED2MOHD9mlS5eYmZkZGzNmDJcnPDycSUlJsdWrV7OYmBjm7+/PpKWl2f3792v9+KpCFHWxfPlyJiMjw/7991+WmprK/WRkZNT68QlKFPXwrR9hWoUo6iElJYUpKyuzSZMmsdjYWHb8+HGmo6PDfv/991o/PkGJoh78/f2ZsrIy27t3L3v69Ck7e/YsMzU1ZYMGDar146uKqtZFiV9++YXZ29uXWea+ffuYrKwsCw4OZo8ePWLjxo1jampqLC0tTaTH8j2izjERm5JHkn37M2LECMZY0S8tZ2dnLv+KFSuYqakpk5OTYxoaGszFxYVduHChVLn/+9//WPPmzZmsrCxr2rQp27ZtWy0dUfWIoh7S09OZj48Pa9iwIZOTk2ONGzdm8+bN45tj9r2paj0wxlhMTAxzc3Nj8vLyrEGDBmzatGml5tgeOHCAmZubMxkZGWZlZcVOnDhRS0dUfaKoC2Nj4zLL9Pf3r70DqyJRnRNf+xE6x6Kqh2vXrjF7e3smKyvLGjduzJYuXco3B/l7I4p6yMvLYwsXLuQ+U42MjJi3t3eFj8r8HlSnLj5+/Mjk5eUr/J24ceNG1rBhQyYjI8Ps7OzYjRs3RHgU3y8eY3XwewNCCCGEEEKqgeYcE0IIIYQQUow6x4QQQgghhBSjzjEhhBBCCCHFqHNMCCGEEEJIMeocE0IIIYQQUow6x4QQQgghhBSjzjEhhBBCCCHFqHNMCCGEEEJIMeocE0KIgExMTLBu3boa56mp4OBgqKmpiXQfAHD06FE0adIEkpKS8PX1Ffn+KuLi4iL2GARRW21DCBEd6hwTQuq9Z8+eYfTo0TAwMICMjAyMjY3h4+ODd+/eVbms27dvY9y4cUKLrazO9uDBgxEXFye0fZRn/PjxGDBgAJ49e4YlS5aIfH8AEBYWBh6Ph48fP/KlHz58uNZiIITUb9Q5JoTUa0+fPoWtrS3i4+Oxd+9ePHnyBFu2bMH58+fh6OiI9+/fV6k8bW1tKCgoiCjaIvLy8tDR0RHpPjIzM/H69Wu4u7vDwMAAysrKIt1fZTQ0NMQeAyGkfqDOMSGkXps4cSJkZGRw9uxZODs7o2HDhujWrRvOnTuHFy9eYN68eXz5MzIyMHToUCgqKsLQ0BCbNm3iW//tSO/Hjx8xZswYaGtrQ0VFBa6urrh79y7fNv/73//Qtm1byMnJQUtLC/369QNQNJUgOTkZU6dOBY/HA4/HA8D/1X1cXBx4PB4eP37MV+batWthamrKLT948ADdunWDkpISdHV1MXz4cLx9+7bMOgkLC+M6oq6uruDxeAgLC8PChQthbW3Nl3fdunUwMTHhlkeOHIm+ffti9erV0NfXh6amJiZOnIi8vDwuT05ODmbNmgUjIyPIysqiSZMm2L59O5KSktCpUycAgLq6Ong8HkaOHMnVxdfTKj58+ABPT0+oq6tDQUEB3bp1Q3x8PLe+pI7OnDkDS0tLKCkpoWvXrkhNTS3zmAsLC9GgQQNs3ryZLz0qKgoSEhJITk4GAAQGBqJFixZQVFSEkZERvL29kZmZWWaZX9fH13x9feHi4sK374CAADRq1Ajy8vJo1aoV/v3333LLJISIFnWOCSH11vv373HmzBl4e3tDXl6eb52enh48PDywf/9+MMa49FWrVqFVq1aIiorC7Nmz4ePjg9DQ0HL3MXDgQLx+/RqnTp1CZGQk2rRpg86dO3Mj0idOnEC/fv3QvXt3REVF4fz587CzswNQNJWgQYMGWLx4MVJTU8vs2Jmbm8PW1hYhISF86SEhIRg2bBiAog66q6srWrdujYiICJw+fRqvXr3CoEGDyozZyckJsbGxAIBDhw4hNTUVTk5OlVUn5+LFi0hISMDFixexc+dOBAcHIzg4mFvv6emJvXv3YsOGDYiJicHWrVuhpKQEIyMjHDp0CAAQGxuL1NRUrF+/vsx9jBw5EhERETh27BiuX78Oxhi6d+/O1wnPysrC6tWrsXv3bly+fBkpKSnw8/MrszwJCQkMHToUe/bs4UsPCQlBu3btYGxszOXbsGEDHj58iJ07d+LChQuYOXOmwHVTloCAAOzatQtbtmzBw4cPMXXqVPzyyy+4dOlSjcolhFQTI4SQeurGjRsMADty5EiZ6wMDAxkA9urVK8YYY8bGxqxr1658eQYPHsy6devGLRsbG7O1a9cyxhi7cuUKU1FRYdnZ2XzbmJqasq1btzLGGHN0dGQeHh7lxvh1eSWCgoKYqqoqt7x27VpmamrKLcfGxjIALCYmhjHG2JIlS9hPP/3EV8azZ88YABYbG1vmfj98+MAAsIsXL3Jp/v7+rFWrVnz51q5dy4yNjbnlESNGMGNjY5afn8+lDRw4kA0ePJgvttDQ0DL3e/HiRQaAffjwgS/d2dmZ+fj4MMYYi4uLYwBYeHg4t/7t27dMXl6eHThwgDFWVEcA2JMnT7g8mzZtYrq6umXulzHGoqKiGI/HY8nJyYwxxgoKCpihoSHbvHlzudscPHiQaWpqcsvfts2IESNYnz59+Lbx8fFhzs7OjDHGsrOzmYKCArt27RpfHi8vLzZ06NBy90sIER0aOSaE1Hvsq5Hhyjg6OpZajomJKTPv3bt3kZmZCU1NTSgpKXE/iYmJSEhIAABER0ejc+fO1Q8ewJAhQ5CUlIQbN24AKBrtbNOmDZo2bcrFcfHiRb4YStaVxCFMVlZWkJSU5Jb19fXx+vVrAEXHKykpCWdn52qXHxMTAykpKdjb23NpmpqasLCw4GsLBQUFvqklX8dRFmtra1haWnKjx5cuXcLr168xcOBALs+5c+fQuXNnGBoaQllZGcOHD8e7d++QlZVVrWN58uQJsrKy0KVLF7722bVrl0jahhBSOSlxB0AIIeLSpEkT8Hg8xMTEcPN8vxYTEwN1dXVoa2tXq/zMzEzo6+sjLCys1LqSOcPfTueoDj09Pbi6umLPnj1wcHDAnj17MGHCBL44evX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" + ] + }, + "metadata": {}, + "output_type": "display_data" + } + ], + "source": [ + "fig3, df3 = plot_mfile_solutions(\n", + " runs_metadata=runs_metadata,\n", + " plot_title=\"Large tokamak 2 solution, relative to large tokamak 1\",\n", + " normalising_tag=\"large tokamak 1\",\n", + ")\n", + "df3" + ] + }, + { + "attachments": {}, + "cell_type": "markdown", + "metadata": {}, + "source": [ + "## Plot multiple solutions normalised by one\n", + "\n", + "Plot two MFILEs, normalised by a third MFILE." + ] + }, + { + "cell_type": "code", + "execution_count": 5, + "metadata": {}, + "outputs": [ + { + "data": { + "text/html": [ + "
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tagobjf_namenorm_objfitvar001_namexcm001itvar002_namexcm002itvar003_namexcm003itvar004_name...itvar041_namexcm041itvar042_namexcm042itvar043_namexcm043itvar044_namexcm044itvar045_namexcm045
0large tokamak 1major radius1.60beta1.1216dene1.0756fwalld0.50758ffuspow...cpttf1.3815ralpne0.83954oh_steel_frac0.64835fimp(13)1.5039dr_tf_wp1.0083
1large tokamak 2major radius1.63beta1.3216dene1.0756fwalld0.51758ffuspow...cpttf1.3815ralpne0.83954oh_steel_frac0.64835fimp(13)1.5039dr_tf_wp1.1083
2large tokamak 3major radius1.50beta1.1216dene1.0756fwalld0.50758ffuspow...cpttf1.3815ralpne0.83954oh_steel_frac0.64835fimp(13)1.5039dr_tf_wp1.0083
\n", + "

3 rows × 93 columns

\n", + "
" + ], + "text/plain": [ + " tag objf_name norm_objf itvar001_name xcm001 \\\n", + "0 large tokamak 1 major radius 1.60 beta 1.1216 \n", + "1 large tokamak 2 major radius 1.63 beta 1.3216 \n", + "2 large tokamak 3 major radius 1.50 beta 1.1216 \n", + "\n", + " itvar002_name xcm002 itvar003_name xcm003 itvar004_name ... \\\n", + "0 dene 1.0756 fwalld 0.50758 ffuspow ... \n", + "1 dene 1.0756 fwalld 0.51758 ffuspow ... \n", + "2 dene 1.0756 fwalld 0.50758 ffuspow ... \n", + "\n", + " itvar041_name xcm041 itvar042_name xcm042 itvar043_name xcm043 \\\n", + "0 cpttf 1.3815 ralpne 0.83954 oh_steel_frac 0.64835 \n", + "1 cpttf 1.3815 ralpne 0.83954 oh_steel_frac 0.64835 \n", + "2 cpttf 1.3815 ralpne 0.83954 oh_steel_frac 0.64835 \n", + "\n", + " itvar044_name xcm044 itvar045_name xcm045 \n", + "0 fimp(13) 1.5039 dr_tf_wp 1.0083 \n", + "1 fimp(13) 1.5039 dr_tf_wp 1.1083 \n", + "2 fimp(13) 1.5039 dr_tf_wp 1.0083 \n", + "\n", + "[3 rows x 93 columns]" + ] + }, + "execution_count": 5, + "metadata": {}, + "output_type": "execute_result" + }, + { + "data": { + "image/png": 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" + ] + }, + "metadata": {}, + "output_type": "display_data" + } + ], + "source": [ + "runs_metadata = [\n", + " RunMetadata(data_dir / \"large_tokamak_1_MFILE.DAT\", \"large tokamak 1\"),\n", + " RunMetadata(data_dir / \"large_tokamak_2_MFILE.DAT\", \"large tokamak 2\"),\n", + " RunMetadata(data_dir / \"large_tokamak_3_MFILE.DAT\", \"large tokamak 3\"),\n", + "]\n", + "\n", + "fig4, df4 = plot_mfile_solutions(\n", + " runs_metadata,\n", + " \"2 large tokamak solutions, relative to large tokamak 1\",\n", + " normalising_tag=\"large tokamak 1\",\n", + ")\n", + "df4" + ] + }, + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "## RMS Errors\n", + "\n", + "Plot RMS errors of multiple solutions relative to a reference solution." + ] + }, + { + "cell_type": "code", + "execution_count": 6, + "metadata": {}, + "outputs": [ + { + "data": { + "text/html": [ + "
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tagobjf_namenorm_objfitvar001_namexcm001itvar002_namexcm002itvar003_namexcm003itvar004_name...itvar041_namexcm041itvar042_namexcm042itvar043_namexcm043itvar044_namexcm044itvar045_namexcm045
0large tokamak 1major radius1.60beta1.1216dene1.0756fwalld0.50758ffuspow...cpttf1.3815ralpne0.83954oh_steel_frac0.64835fimp(13)1.5039dr_tf_wp1.0083
1large tokamak 2major radius1.63beta1.3216dene1.0756fwalld0.51758ffuspow...cpttf1.3815ralpne0.83954oh_steel_frac0.64835fimp(13)1.5039dr_tf_wp1.1083
2large tokamak 3major radius1.50beta1.1216dene1.0756fwalld0.50758ffuspow...cpttf1.3815ralpne0.83954oh_steel_frac0.64835fimp(13)1.5039dr_tf_wp1.0083
3large tokamak 4major radius1.52beta1.1216dene1.0756fwalld0.50758ffuspow...cpttf1.3815ralpne0.83954oh_steel_frac0.64835fimp(13)1.5039dr_tf_wp1.0083
\n", + "

4 rows × 93 columns

\n", + "
" + ], + "text/plain": [ + " tag objf_name norm_objf itvar001_name xcm001 \\\n", + "0 large tokamak 1 major radius 1.60 beta 1.1216 \n", + "1 large tokamak 2 major radius 1.63 beta 1.3216 \n", + "2 large tokamak 3 major radius 1.50 beta 1.1216 \n", + "3 large tokamak 4 major radius 1.52 beta 1.1216 \n", + "\n", + " itvar002_name xcm002 itvar003_name xcm003 itvar004_name ... \\\n", + "0 dene 1.0756 fwalld 0.50758 ffuspow ... \n", + "1 dene 1.0756 fwalld 0.51758 ffuspow ... \n", + "2 dene 1.0756 fwalld 0.50758 ffuspow ... \n", + "3 dene 1.0756 fwalld 0.50758 ffuspow ... \n", + "\n", + " itvar041_name xcm041 itvar042_name xcm042 itvar043_name xcm043 \\\n", + "0 cpttf 1.3815 ralpne 0.83954 oh_steel_frac 0.64835 \n", + "1 cpttf 1.3815 ralpne 0.83954 oh_steel_frac 0.64835 \n", + "2 cpttf 1.3815 ralpne 0.83954 oh_steel_frac 0.64835 \n", + "3 cpttf 1.3815 ralpne 0.83954 oh_steel_frac 0.64835 \n", + "\n", + " itvar044_name xcm044 itvar045_name xcm045 \n", + "0 fimp(13) 1.5039 dr_tf_wp 1.0083 \n", + "1 fimp(13) 1.5039 dr_tf_wp 1.1083 \n", + "2 fimp(13) 1.5039 dr_tf_wp 1.0083 \n", + "3 fimp(13) 1.5039 dr_tf_wp 1.0083 \n", + "\n", + "[4 rows x 93 columns]" + ] + }, + "execution_count": 6, + "metadata": {}, + "output_type": "execute_result" + }, + { + "data": { + "image/png": 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" + ] + }, + "metadata": {}, + "output_type": "display_data" + } + ], + "source": [ + "runs_metadata = [\n", + " RunMetadata(data_dir / \"large_tokamak_1_MFILE.DAT\", \"large tokamak 1\"),\n", + " RunMetadata(data_dir / \"large_tokamak_2_MFILE.DAT\", \"large tokamak 2\"),\n", + " RunMetadata(data_dir / \"large_tokamak_3_MFILE.DAT\", \"large tokamak 3\"),\n", + " RunMetadata(data_dir / \"large_tokamak_4_MFILE.DAT\", \"large tokamak 4\"),\n", + "]\n", + "\n", + "fig5, df5 = plot_mfile_solutions(\n", + " runs_metadata,\n", + " \"3 large tokamak solutions with RMS errors normalised to large tokamak 1\",\n", + " normalising_tag=\"large tokamak 1\",\n", + " rmse=True,\n", + ")\n", + "df5" + ] + }, + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "## Solutions normalised by range\n", + "\n", + "Use `nitvar` values instead; the solution optimisation parameters are normalised to the range of their upper and lower bounds." + ] + }, + { + "cell_type": "code", + "execution_count": 7, + "metadata": {}, + "outputs": [ + { + "data": { + "text/html": [ + "
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tagobjf_namenorm_objfitvar001_namenitvar001itvar002_namenitvar002itvar003_namenitvar003itvar004_name...itvar041_namenitvar041itvar042_namenitvar042itvar043_namenitvar043itvar044_namenitvar044itvar045_namenitvar045
0large tokamak 1major radius1.60beta0.032681dene0.071381fwalld0.50709ffuspow...cpttf0.99182ralpne0.67908oh_steel_frac0.5455fimp(13)0.057148dr_tf_wp0.0651
1large tokamak 2major radius1.63beta0.042681dene0.071381fwalld0.70709ffuspow...cpttf0.99182ralpne0.67908oh_steel_frac0.5455fimp(13)0.057148dr_tf_wp0.0651
2large tokamak 3major radius1.50beta0.022681dene0.071381fwalld0.50709ffuspow...cpttf0.99182ralpne0.67908oh_steel_frac0.5455fimp(13)0.057148dr_tf_wp0.0651
3large tokamak 4major radius1.52beta0.032681dene0.071381fwalld0.40709ffuspow...cpttf0.99182ralpne0.67908oh_steel_frac0.5455fimp(13)0.057148dr_tf_wp0.0651
\n", + "

4 rows × 93 columns

\n", + "
" + ], + "text/plain": [ + " tag objf_name norm_objf itvar001_name nitvar001 \\\n", + "0 large tokamak 1 major radius 1.60 beta 0.032681 \n", + "1 large tokamak 2 major radius 1.63 beta 0.042681 \n", + "2 large tokamak 3 major radius 1.50 beta 0.022681 \n", + "3 large tokamak 4 major radius 1.52 beta 0.032681 \n", + "\n", + " itvar002_name nitvar002 itvar003_name nitvar003 itvar004_name ... \\\n", + "0 dene 0.071381 fwalld 0.50709 ffuspow ... \n", + "1 dene 0.071381 fwalld 0.70709 ffuspow ... \n", + "2 dene 0.071381 fwalld 0.50709 ffuspow ... \n", + "3 dene 0.071381 fwalld 0.40709 ffuspow ... \n", + "\n", + " itvar041_name nitvar041 itvar042_name nitvar042 itvar043_name nitvar043 \\\n", + "0 cpttf 0.99182 ralpne 0.67908 oh_steel_frac 0.5455 \n", + "1 cpttf 0.99182 ralpne 0.67908 oh_steel_frac 0.5455 \n", + "2 cpttf 0.99182 ralpne 0.67908 oh_steel_frac 0.5455 \n", + "3 cpttf 0.99182 ralpne 0.67908 oh_steel_frac 0.5455 \n", + "\n", + " itvar044_name nitvar044 itvar045_name nitvar045 \n", + "0 fimp(13) 0.057148 dr_tf_wp 0.0651 \n", + "1 fimp(13) 0.057148 dr_tf_wp 0.0651 \n", + "2 fimp(13) 0.057148 dr_tf_wp 0.0651 \n", + "3 fimp(13) 0.057148 dr_tf_wp 0.0651 \n", + "\n", + "[4 rows x 93 columns]" + ] + }, + "execution_count": 7, + "metadata": {}, + "output_type": "execute_result" + }, + { + "data": { + "image/png": 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+ "text/plain": [ + "
" + ] + }, + "metadata": {}, + "output_type": "display_data" + } + ], + "source": [ + "runs_metadata = [\n", + " RunMetadata(data_dir / \"large_tokamak_1_MFILE.DAT\", \"large tokamak 1\"),\n", + " RunMetadata(data_dir / \"large_tokamak_2_MFILE.DAT\", \"large tokamak 2\"),\n", + " RunMetadata(data_dir / \"large_tokamak_3_MFILE.DAT\", \"large tokamak 3\"),\n", + " RunMetadata(data_dir / \"large_tokamak_4_MFILE.DAT\", \"large tokamak 4\"),\n", + "]\n", + "\n", + "fig6, df6 = plot_mfile_solutions(\n", + " runs_metadata,\n", + " \"4 large tokamak solutions normalised to the range of the optimisation parameters\",\n", + " normalisation_type=\"range\",\n", + ")\n", + "df6" + ] + }, + { + "cell_type": "markdown", + "metadata": {}, + "source": [ + "## Actual values" + ] + }, + { + "cell_type": "code", + "execution_count": 8, + "metadata": {}, + "outputs": [ + { + "data": { + "text/html": [ + "
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tagobjf_namenorm_objfitvar001_nameitvar001itvar002_nameitvar002itvar003_nameitvar003itvar004_name...itvar041_nameitvar041itvar042_nameitvar042itvar043_nameitvar043itvar044_nameitvar044itvar045_nameitvar045
0large tokamak 1major radius1.60beta0.033648dene8.066700e+19fwalld0.50758ffuspow...cpttf89795.0ralpne0.083954oh_steel_frac0.51868fimp(13)0.000571dr_tf_wp0.50416
1large tokamak 2major radius1.63beta0.034648dene8.056700e+19fwalld0.50258ffuspow...cpttf89795.0ralpne0.083954oh_steel_frac0.51868fimp(13)0.000571dr_tf_wp0.50416
2large tokamak 3major radius1.50beta0.033648dene8.066700e+19fwalld0.50758ffuspow...cpttf88795.0ralpne0.081954oh_steel_frac0.52868fimp(13)0.000531dr_tf_wp0.57416
3large tokamak 4major radius1.52beta0.037648dene8.366700e+19fwalld0.55758ffuspow...cpttf89795.0ralpne0.083954oh_steel_frac0.51868fimp(13)0.000571dr_tf_wp0.50416
\n", + "

4 rows × 93 columns

\n", + "
" + ], + "text/plain": [ + " tag objf_name norm_objf itvar001_name itvar001 \\\n", + "0 large tokamak 1 major radius 1.60 beta 0.033648 \n", + "1 large tokamak 2 major radius 1.63 beta 0.034648 \n", + "2 large tokamak 3 major radius 1.50 beta 0.033648 \n", + "3 large tokamak 4 major radius 1.52 beta 0.037648 \n", + "\n", + " itvar002_name itvar002 itvar003_name itvar003 itvar004_name ... \\\n", + "0 dene 8.066700e+19 fwalld 0.50758 ffuspow ... \n", + "1 dene 8.056700e+19 fwalld 0.50258 ffuspow ... \n", + "2 dene 8.066700e+19 fwalld 0.50758 ffuspow ... \n", + "3 dene 8.366700e+19 fwalld 0.55758 ffuspow ... \n", + "\n", + " itvar041_name itvar041 itvar042_name itvar042 itvar043_name itvar043 \\\n", + "0 cpttf 89795.0 ralpne 0.083954 oh_steel_frac 0.51868 \n", + "1 cpttf 89795.0 ralpne 0.083954 oh_steel_frac 0.51868 \n", + "2 cpttf 88795.0 ralpne 0.081954 oh_steel_frac 0.52868 \n", + "3 cpttf 89795.0 ralpne 0.083954 oh_steel_frac 0.51868 \n", + "\n", + " itvar044_name itvar044 itvar045_name itvar045 \n", + "0 fimp(13) 0.000571 dr_tf_wp 0.50416 \n", + "1 fimp(13) 0.000571 dr_tf_wp 0.50416 \n", + "2 fimp(13) 0.000531 dr_tf_wp 0.57416 \n", + "3 fimp(13) 0.000571 dr_tf_wp 0.50416 \n", + "\n", + "[4 rows x 93 columns]" + ] + }, + "execution_count": 8, + "metadata": {}, + "output_type": "execute_result" + }, + { + "data": { + "image/png": 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", + "text/plain": [ + "
" + ] + }, + "metadata": {}, + "output_type": "display_data" + } + ], + "source": [ + "runs_metadata = [\n", + " RunMetadata(data_dir / \"large_tokamak_1_MFILE.DAT\", \"large tokamak 1\"),\n", + " RunMetadata(data_dir / \"large_tokamak_2_MFILE.DAT\", \"large tokamak 2\"),\n", + " RunMetadata(data_dir / \"large_tokamak_3_MFILE.DAT\", \"large tokamak 3\"),\n", + " RunMetadata(data_dir / \"large_tokamak_4_MFILE.DAT\", \"large tokamak 4\"),\n", + "]\n", + "\n", + "fig7, df7 = plot_mfile_solutions(\n", + " runs_metadata,\n", + " \"4 large tokamak solutions normalised to the range of the optimisation parameters\",\n", + " normalisation_type=None,\n", + ")\n", + "df7" + ] + } + ], + "metadata": { + "kernelspec": { + "display_name": "process", + "language": "python", + "name": "python3" + }, + "language_info": { + "codemirror_mode": { + "name": "ipython", + "version": 3 + }, + "file_extension": ".py", + "mimetype": "text/x-python", + "name": "python", + "nbconvert_exporter": "python", + "pygments_lexer": "ipython3", + "version": "3.10.9" + }, + "orig_nbformat": 4 + }, + "nbformat": 4, + "nbformat_minor": 2 +} diff --git a/examples/plot_solutions.py b/examples/plot_solutions.py new file mode 100644 index 0000000000..1b5a7ffa68 --- /dev/null +++ b/examples/plot_solutions.py @@ -0,0 +1,142 @@ +# %% [markdown] +# # `plot_solutions` Solution Comparison Tool +# +# This tool plots the solution vectors (i.e. final values of optimisation parameters) for different runs of PROCESS. This allows visual comparisons of different solution points. +# +# It can use different intra-solution optimisation parameter normalisations (e.g. initial value, parameter range) and inter-solution normalisations (e.g. normalise to a certain solution). +# +# ### Known Limitations +# +# - The solution vectors (optimisation parameter values at the solution) currently plotted are normalised to the initial point (from the `IN.DAT`) of each solution: each element of the vector is the $x_{final}/x_{initial}$, the `xcmxxx` values in the `MFILE.DAT`. This allows all optimisation parameters to be plotted on the same axis, showing the relative changes from their initial values across multiple solutions. +# - Solutions being plotted together must also have the same optimisation parameters. +# - The solutions plotted in this example are fictitious. + +# %% +from process.io.plot_solutions import RunMetadata, plot_mfile_solutions +from pathlib import Path + +# %% [markdown] +# ## Plot single solution +# +# Plot a single solution, showing optimisation parameters normalised to their initial values. + +# %% +data_dir = Path("data") +runs_metadata = [ + RunMetadata(data_dir / "large_tokamak_1_MFILE.DAT", "large tokamak 1"), +] + +# Figure and dataframe returned for optional further modification +fig1, df1 = plot_mfile_solutions( + runs_metadata=runs_metadata, + plot_title="Large tokamak solution 1", +) +df1 + +# %% [markdown] +# ## Plot two solutions +# +# Plot two MFILEs together, showing normalised values of the optimisation parameters at the solution points, as well as the objective function values. + +# %% +runs_metadata = [ + RunMetadata(data_dir / "large_tokamak_1_MFILE.DAT", "large tokamak 1"), + RunMetadata(data_dir / "large_tokamak_2_MFILE.DAT", "large tokamak 2"), +] + +fig2, df2 = plot_mfile_solutions( + runs_metadata=runs_metadata, + plot_title="2 large tokamak solutions", +) +df2 + +# %% [markdown] +# ## Plot one solution normalised to another +# +# Normalised differences, relative to the a given solution, can also be plotted: + +# %% +fig3, df3 = plot_mfile_solutions( + runs_metadata=runs_metadata, + plot_title="Large tokamak 2 solution, relative to large tokamak 1", + normalising_tag="large tokamak 1", +) +df3 + +# %% [markdown] +# ## Plot multiple solutions normalised by one +# +# Plot two MFILEs, normalised by a third MFILE. + +# %% +runs_metadata = [ + RunMetadata(data_dir / "large_tokamak_1_MFILE.DAT", "large tokamak 1"), + RunMetadata(data_dir / "large_tokamak_2_MFILE.DAT", "large tokamak 2"), + RunMetadata(data_dir / "large_tokamak_3_MFILE.DAT", "large tokamak 3"), +] + +fig4, df4 = plot_mfile_solutions( + runs_metadata, + "2 large tokamak solutions, relative to large tokamak 1", + normalising_tag="large tokamak 1", +) +df4 + +# %% [markdown] +# ## RMS Errors +# +# Plot RMS errors of multiple solutions relative to a reference solution. + +# %% +runs_metadata = [ + RunMetadata(data_dir / "large_tokamak_1_MFILE.DAT", "large tokamak 1"), + RunMetadata(data_dir / "large_tokamak_2_MFILE.DAT", "large tokamak 2"), + RunMetadata(data_dir / "large_tokamak_3_MFILE.DAT", "large tokamak 3"), + RunMetadata(data_dir / "large_tokamak_4_MFILE.DAT", "large tokamak 4"), +] + +fig5, df5 = plot_mfile_solutions( + runs_metadata, + "3 large tokamak solutions with RMS errors normalised to large tokamak 1", + normalising_tag="large tokamak 1", + rmse=True, +) +df5 + +# %% [markdown] +# ## Solutions normalised by range +# +# Use `nitvar` values instead; the solution optimisation parameters are normalised to the range of their upper and lower bounds. + +# %% +runs_metadata = [ + RunMetadata(data_dir / "large_tokamak_1_MFILE.DAT", "large tokamak 1"), + RunMetadata(data_dir / "large_tokamak_2_MFILE.DAT", "large tokamak 2"), + RunMetadata(data_dir / "large_tokamak_3_MFILE.DAT", "large tokamak 3"), + RunMetadata(data_dir / "large_tokamak_4_MFILE.DAT", "large tokamak 4"), +] + +fig6, df6 = plot_mfile_solutions( + runs_metadata, + "4 large tokamak solutions normalised to the range of the optimisation parameters", + normalisation_type="range", +) +df6 + +# %% [markdown] +# ## Actual values + +# %% +runs_metadata = [ + RunMetadata(data_dir / "large_tokamak_1_MFILE.DAT", "large tokamak 1"), + RunMetadata(data_dir / "large_tokamak_2_MFILE.DAT", "large tokamak 2"), + RunMetadata(data_dir / "large_tokamak_3_MFILE.DAT", "large tokamak 3"), + RunMetadata(data_dir / "large_tokamak_4_MFILE.DAT", "large tokamak 4"), +] + +fig7, df7 = plot_mfile_solutions( + runs_metadata, + "4 large tokamak solutions normalised to the range of the optimisation parameters", + normalisation_type=None, +) +df7 diff --git a/process/io/mfile.py b/process/io/mfile.py index eb1e67cad1..3a44cdff98 100755 --- a/process/io/mfile.py +++ b/process/io/mfile.py @@ -28,10 +28,10 @@ from collections import OrderedDict import logging -from sys import stderr import json +from typing import List, Union -LOG = logging.getLogger("mfile") +logger = logging.getLogger(__name__) class MFileVariable(dict): @@ -60,7 +60,7 @@ def __init__( self.var_flag = var_flag self.latest_scan = 0 super().__init__(*args, **kwargs) - LOG.debug( + logger.debug( "Initialising variable '{}': {}".format(self.var_name, self.var_description) ) @@ -85,7 +85,7 @@ def set_scan(self, scan_number, scan_value): self["scan{:02}".format(scan_number)] = scan_value if scan_number > self.latest_scan: self.latest_scan = scan_number - LOG.debug( + logger.debug( "Scan {} for variable '{}' == {}".format( scan_number, self.var_name, scan_value ) @@ -146,7 +146,7 @@ def __init__(self, item): self.get_number_of_scans = self.get_error def get_error(self, *args, **kwargs): - LOG.error("Key '{}' not in MFILE. KeyError! Check MFILE".format(self.item)) + logger.error("Key '{}' not in MFILE. KeyError! Check MFILE".format(self.item)) if self.item == "error_status": # Missing error_status key means Process exited prematurely, usually @@ -230,7 +230,7 @@ def __repr__(self): class MFile(object): def __init__(self, filename="MFILE.DAT"): """Class object to store the MFile Objects""" - LOG.info("Creating MFile class for file '{}'".format(filename)) + logger.info("Creating MFile class for file '{}'".format(filename)) self.filename = filename # self.data = MFileDataDictionary() # self.data = OrderedDict() @@ -241,9 +241,9 @@ def __init__(self, filename="MFILE.DAT"): self.mfile_modules["Misc"] = list() self.current_module = "Misc" if filename is not None: - LOG.info("Opening file '{}'".format(self.filename)) + logger.info("Opening file '{}'".format(self.filename)) self.open_mfile() - LOG.info("Parsing file '{}'".format(self.filename)) + logger.info("Parsing file '{}'".format(self.filename)) self.parse_mfile() def open_mfile(self): @@ -296,7 +296,8 @@ class or create a new class if it is the first instance of it. if "runtitle" in var_name: var_value = " ".join(line[2:]) else: - var_value = sort_value(line[2]) + # Pass all value "words" + var_value = sort_value(line[2:]) var_unit = get_unit(var_des) if len(line) >= 4: var_flag = line[3] @@ -374,18 +375,25 @@ def write_to_json(self, keys_to_write={}, scan=-1, verbose=False): json.dump(dict_to_write, fp, indent=4) -def sort_value(val): - """Function to sort out value line in MFILE.""" - if '"' in val: - return str(val.strip('"')) +def sort_value(value_words: List[str]) -> Union[str, float]: + """Parse value section of a line in MFILE. + + value_words is a list of strings, which is then parsed. + :param value_words: value of var in MFILE as list of strings + :type value_words: List[str] + :return: string or float representation of value list + :rtype: Union[str, float] + """ + if '"' in value_words[0]: + # First "word" begins with ": return words as single str + return " ".join(value_words).strip().strip('"').strip() else: try: - return float(val) - except ValueError as err: - print("Please fix this!", file=stderr) - print(err, file=stderr) - print(val) - exit() + # Attempt float conversion of first word + return float(value_words[0]) + except ValueError: + logger.exception(f"Can't parse value in MFILE: {value_words}") + raise def sort_brackets(var): diff --git a/process/io/plot_solutions.py b/process/io/plot_solutions.py new file mode 100644 index 0000000000..2de7875d84 --- /dev/null +++ b/process/io/plot_solutions.py @@ -0,0 +1,579 @@ +"""Plot solution vectors from MFILEs to compare them. + +This tool plots multiple solutions, or their differences, to allow comparisons +of the solution vectors and objective function values. It allows normalisation +to a given solution as well as plotting RMSEs relative to it. + +If the MFILE is the result of a parameter scan, only the last point is plotted +currently. +""" + +from process.io.mfile import MFile +from pathlib import Path +import pandas as pd + +import numpy as np +import matplotlib.pyplot as plt +import matplotlib as mpl +import logging +import seaborn as sns +from dataclasses import dataclass, asdict +from typing import Optional, Sequence, List, Dict, Tuple, Union + + +# Variables of interest in mfiles and subsequent dataframes +# Be specific about exact names, patterns and regex +INITIAL_NORM_OPT_PARAM_VALUE_PATTERN = "xcm" +RANGE_NORM_OPT_PARAM_VALUE_PATTERN = "nitvar" +OPT_PARAM_VALUE_REGEX = r"^itvar\d{3}$" +NORM_OPT_PARAM_NAME_REGEX = r"itvar\d{3}_name" +NORM_OBJF_PATTERN = "objf" +NORM_OBJF_VALUE = "norm_objf" +NORM_OBJF_NAME = "objf_name" +TAG_REGEX = r"tag$" +TAG = "tag" + +logger = logging.getLogger(__name__) + + +@dataclass +class RunMetadata: + """Metadata for a given Process run. + + Define mfile for run and other information to identify it. Depending on + what is being run/plotted, different fields can be undefined. + """ + + mfile_path: Path + tag: str + + +def plot_mfile_solutions( + runs_metadata: Sequence[RunMetadata], + plot_title: str, + normalising_tag: Optional[str] = None, + rmse: bool = False, + normalisation_type: Optional[str] = "init", +) -> Tuple[mpl.figure.Figure, pd.DataFrame]: + """Plot multiple solutions, optionally normalised by a given solution. + + :param runs_metadata: list of RunMetadata objects + :type runs_metadata: Sequence[RunMetadata] + :param plot_title: title of plot + :type plot_title: str + :param normalising_tag: tag for solution to normalise with. If provided, + normalise, otherwise don't, defaults to None + :type normalising_tag: str, optional + :param rmse: plot RMS errors relative to reference solution, defaults to False + :type rmse: bool, optional + :param normalisation_type: opt param normalisation to use: one of ["init", "range", None], defaults to "init" + :type normalisation_type: str, optional + :return: figure and dataframe of solutions + :rtype: Tuple[mpl.figure.Figure, pd.DataFrame] + """ + # Determine type of normalised opt params to plot (i.e. itvar, xcm or nitvar) + if normalisation_type == "init": + opt_param_value_pattern = INITIAL_NORM_OPT_PARAM_VALUE_PATTERN + elif normalisation_type == "range": + opt_param_value_pattern = RANGE_NORM_OPT_PARAM_VALUE_PATTERN + else: + opt_param_value_pattern = OPT_PARAM_VALUE_REGEX + + # Create dataframe from runs metadata: mfile data with a tag for each run + results_df = _create_df_from_run_metadata(runs_metadata) + + # Filter for tag, optimisation parameters and objective function + filtered_results_df = _filter_vars_of_interest( + results_df, opt_param_value_pattern=opt_param_value_pattern + ) + + if normalising_tag is not None: + # Calculate the normalised diffs relative to the tagged solution + plot_results_df = _normalise_diffs( + filtered_results_df, + opt_param_value_pattern=opt_param_value_pattern, + normalising_tag=normalising_tag, + ) + else: + # Don't perform any processing of optimisation parameters + plot_results_df = filtered_results_df + + if rmse: + if normalising_tag is None: + raise ValueError( + "RMSE plot requires normalising_tag to be specified: which " + "solution are the errors relative to?" + ) + + # Calcualte RMS errors relative to normalising tag solution + rmse_df = _rms_errors( + results_df=results_df, + opt_param_value_pattern=opt_param_value_pattern, + normalising_tag=normalising_tag, + ) + else: + # Don't plot RMS errors + rmse_df = None + + fig = _plot_solutions( + plot_results_df, + opt_param_value_pattern=opt_param_value_pattern, + plot_title=plot_title, + rmse_df=rmse_df, + normalising_tag=normalising_tag, + normalisation_type=normalisation_type, + ) + + # Return fig for optional further customisation + # fig as varying numbers of axes depending on plot type + return fig, filtered_results_df + + +def _extract_mfile_data(mfile_path: Path) -> Dict: + """Extract data from mfile and return as dict. + + Also include the names of the optimisation parameters. + + :param mfile_path: mfile to extract data from + :type mfile_path: pathlib.Path + :return: dict of all data in mfile + :rtype: dict + """ + mfile = MFile(str(mfile_path)) + mfile_data = {} + + for var in mfile.data.keys(): + if var.startswith("itvar"): + # Iteration variable: get name too + mfile_data[f"{var}_name"] = mfile.data[var].var_description + + # Extract value + mfile_data[var] = mfile.data[var].get_scan(-1) + + return mfile_data + + +def _create_df_from_run_metadata(runs_metadata: Sequence[RunMetadata]) -> pd.DataFrame: + """Create a dataframe from multiple mfiles. + + Uses RunMetadata objects. + :param runs_metadata: scenarios and solvers that have been run + :type runs_metadata: Sequence[RunMetadata] + :return: dataframe of all results + :rtype: pandas.DataFrame + """ + results = [] + for run_metadata in runs_metadata: + if Path(run_metadata.mfile_path).exists(): + mfile_data = _extract_mfile_data(run_metadata.mfile_path) + else: + raise FileNotFoundError( + f"The MFILE {run_metadata.mfile_path} doesn't exist" + ) + # Merge each run's metadata and results into one dict + results.append({**asdict(run_metadata), **mfile_data}) + + return pd.DataFrame(results) + + +def _separate_norm_solution( + results_df: pd.DataFrame, normalising_tag: str +) -> Tuple[pd.DataFrame]: + """Separate solutions df into normalising row and rows to be normalised. + + :param results_df: multiple solutions dataframe + :type results_df: pd.DataFrame + :param normalising_tag: tag to identify row to normalise with + :type normalising_tag: str + :return: normalising row, rows to be normalised + :rtype: Tuple[pd.DataFrame] + """ + # Split results into normalising and non-normalising solutions + normalising_soln = results_df[results_df[TAG] == normalising_tag] + non_normalising_solns = results_df[results_df[TAG] != normalising_tag] + + return normalising_soln, non_normalising_solns + + +def _filter_opt_params( + results: pd.DataFrame, + opt_param_value_pattern: str, + filter_in: bool = True, +) -> pd.DataFrame: + """Filter optimsation parameters in or out of results. + + :param results: multiple solutions + :type results: pd.DataFrame + :param opt_param_value_pattern: normalisation type for opt params in mfile + :type opt_param_value_pattern: str + :param filter_in: include opt params, defaults to True + :type filter_in: bool, optional + :return: multiple solutions with opt params filtered in or out + :rtype: pd.DataFrame + """ + is_opt_param = results.columns.str.contains(opt_param_value_pattern) + if filter_in: + # TODO Check this loc can't be removed + filtered_results = results.loc[:, is_opt_param] + else: + filtered_results = results.loc[:, ~is_opt_param] + return filtered_results + + +def _normalise_diffs( + results_df: pd.DataFrame, + opt_param_value_pattern: str, + normalising_tag: str, +) -> pd.DataFrame: + """Normalise differences of multiple solutions with a normalising solution. + + :param results_df: dataframe of two solutions (same scenario, different solvers) + :type results_df: pandas.DataFrame + :param opt_param_value_pattern: normalisation type for opt params in mfile + :type opt_param_value_pattern: str + :param normalising_tag: tag to normalise other solutions with + :type normalising_tag: str + :return: normalised differences + :rtype: pandas.DataFrame + """ + normalising_soln, non_normalising_solns = _separate_norm_solution( + results_df, normalising_tag + ) + # Solution to normalise with + normalising_soln_opt_params = _filter_opt_params( + normalising_soln, opt_param_value_pattern=opt_param_value_pattern + ) + # Solutions that need normalised diffs calculating + non_normalising_solns_opt_params = _filter_opt_params( + non_normalising_solns, opt_param_value_pattern=opt_param_value_pattern + ) + + # Calculate the normalised differences between multiple solutions + # for optimisation parameters + normalising_soln_opt_params_np = normalising_soln_opt_params.to_numpy() + if (normalising_soln_opt_params_np == 0).any(): + zero_indexes = np.nonzero(normalising_soln_opt_params_np == 0)[0] + raise ValueError( + f"Can't normalise with 0-valued optimisation parameter at index {str(zero_indexes)}." + ) + + normalised_solns_opt_params = ( + non_normalising_solns_opt_params - normalising_soln_opt_params_np + ) / abs(normalising_soln_opt_params_np) + + # Combine dfs to get non-numerical info (metadata) alongside normalised diffs + # e.g. tag, objf_name + non_normalising_solns_metadata = _filter_opt_params( + non_normalising_solns, + opt_param_value_pattern=opt_param_value_pattern, + filter_in=False, + ) + normalised_solns = pd.concat( + [non_normalising_solns_metadata, normalised_solns_opt_params], axis=1 + ) + + return normalised_solns + + +def _filter_vars_of_interest( + results_df: pd.DataFrame, + opt_param_value_pattern: str, + extra_var_names: Optional[List[str]] = None, +) -> pd.DataFrame: + """Filter variables of interest from full results for all solutions. + + :param results_df: full results for all solutions + :type results_df: pandas.DataFrame + :param opt_param_value_pattern: normalisation type for opt params in mfile + :type opt_param_value_pattern: str + :param extra_var_names: other variables of interest to filter, defaults to None + :type extra_var_names: List[str], optional + :return: variables of interest + :rtype: pandas.DataFrame + """ + if extra_var_names is None: + extra_var_names = [] + + # Filter for optimisation parameters (normalised to initial value + # e.g. xcm001) values and names, objective function value and name, plus + # any extra variables + filtered_results = results_df.filter( + regex=( + f"{TAG_REGEX}|{opt_param_value_pattern}|{NORM_OPT_PARAM_NAME_REGEX}|" + f"{NORM_OBJF_PATTERN}|{'|'.join(extra_var_names)}".rstrip("|") + ) + ) + + return filtered_results + + +def _plot_solutions( + diffs_df: pd.DataFrame, + normalisation_type: str, + opt_param_value_pattern: str, + plot_title: str, + normalising_tag: Union[str, None], + rmse_df: pd.DataFrame, +) -> mpl.figure.Figure: + """Plot multiple solutions, optionally normalised by a given solution. + + :param diffs_df: normalised diffs for optimisation parameters and objective function + :type diffs_df: pandas.DataFrame + :param normalisation_type: opt param normalisation to use: ["init", "range"] + :type normalisation_type: str + :param opt_param_value_pattern: normalisation type for opt params in mfile + :type opt_param_value_pattern: str + :param plot_title: title of plot + :type plot_title: str + :param normalising_tag: tag for normalising solution, if any + :type normalising_tag: Union[str, None] + :param rmse_df: RMS errors relative to reference solution + :type rmse_df: pd.DataFrame + :return: figure containing varying numbers of axes + :rtype: mpl.figure.Figure + """ + # Separate optimisation parameters and objective dfs + opt_params_df = diffs_df.filter( + regex=f"{opt_param_value_pattern}|{NORM_OPT_PARAM_NAME_REGEX}|{TAG}" + ) + norm_objf_df = diffs_df.filter(regex=f"{NORM_OBJF_PATTERN}|{TAG}") + + # Further separate objective function values only, for plotting + norm_objf_values_df = norm_objf_df.filter(regex=f"{NORM_OBJF_VALUE}|{TAG}") + + # Acquire objective function name(s), then check only one type is being plotted + objf_list = norm_objf_df[NORM_OBJF_NAME].unique() + + if len(objf_list) != 1: + raise ValueError("Can't plot different objective functions on the same plot") + + objf_name = objf_list[0] + + # Now separate optimisation parameter values from their names + opt_params_values_df = opt_params_df.filter( + regex=f"{opt_param_value_pattern}|{TAG}" + ) + opt_params_names_df = opt_params_df.filter(regex=NORM_OPT_PARAM_NAME_REGEX) + + # Replace xcm--- optimisation parameter column headers with actual var names + # in sub-df: allows plotting showing actual var names + # eg. column headers "tag, xcm001, xcm002, ..." become + # "tag, bt, rmajor, ..." + # Normalising row may have been filtered out; reset index to ensure + # opt param names in row 0 + opt_params_names_df_reset = opt_params_names_df.reset_index(drop=True) + opt_params_names = opt_params_names_df_reset.loc[0].values.tolist() + + # Need to include tag column as first column header + opt_params_names_with_tag = opt_params_names.copy() + opt_params_names_with_tag.insert(0, TAG) + opt_params_values_with_names_df = opt_params_values_df.set_axis( + opt_params_names_with_tag, axis=1 + ) + + # Define subfig and subplot layout + # Matplotlib usually fits the subplots to the figure. However, as there are + # varying numbers of opt params and various plot options, it is necessary + # to fit the figure to the subplots, i.e. have different figure sizes + # based on what's being plotted + # Strategy: 2 subfigures (opt params and obj func/rmse), varying numbers of + # subplots in each + + # Define optimisation parameter plot + opt_param_count = len(opt_params_names) + if normalisation_type is None: + # Separate axes for each opt param: more space per param + inches_per_opt_param = 0.7 + # Add extra subplot for legend + nrows_opt_param_subplot = opt_param_count + 1 + inches_per_legend_entry = 0.5 + tag_count = diffs_df[TAG].count() + external_legend_height = tag_count * inches_per_legend_entry + else: + # Single axis for all opt params: less space per param + inches_per_opt_param = 0.20 + nrows_opt_param_subplot = 1 + external_legend_height = 0.0 + + final_subfig_height_opt_params = ( + opt_param_count * inches_per_opt_param + ) + external_legend_height + figsize = [7, final_subfig_height_opt_params] + + # Add obj func/RMSE subfig + base_subfig_height_obj_func = 0.75 + if rmse_df is not None: + nrows_obj_func_rmse_subplot = 2 + final_subfig_height_obj_func = ( + nrows_obj_func_rmse_subplot * base_subfig_height_obj_func + ) + else: + nrows_obj_func_rmse_subplot = 1 + final_subfig_height_obj_func = base_subfig_height_obj_func + + figsize[1] += final_subfig_height_obj_func + + fig = plt.figure(layout="constrained", figsize=figsize) + fig.suptitle(plot_title) + # 2 subfig rows: 1 for opt params, 1 for objective function and optional RMSE + # Use actual calculated height to define height ratios + subfigs = fig.subfigures( + nrows=2, + ncols=1, + height_ratios=[final_subfig_height_opt_params, final_subfig_height_obj_func], + ) + axs_opt_params = subfigs[0].subplots(nrows=nrows_opt_param_subplot) + + # Adapt x axis label for normalisation type + if normalisation_type == "init": + x_axis_label = "Value normalised by initial value" + elif normalisation_type == "range": + x_axis_label = "Value normalised by parameter range" + else: + x_axis_label = "Value" + + if normalising_tag is not None: + x_axis_label += f", normalised to {normalising_tag}" + + # Plot optimisation parameters + # Melt df (wide to long-form) for seaborn plotting with jitter + opt_params_values_with_names_df_melt = opt_params_values_with_names_df.melt( + id_vars=TAG + ) + + # If normalisation_type is None (no normalisation of original opt param + # values), plot strip plot with different axis for each opt param. + # Otherwise plot all params on single axis + if normalisation_type is None: + # axs_opt_params[0] reserved for legend + for i, opt_param_name in enumerate(opt_params_names): + sns.stripplot( + data=opt_params_values_with_names_df_melt[ + opt_params_values_with_names_df_melt["variable"] == opt_param_name + ], + x="value", + y="variable", + hue=TAG, + jitter=True, + ax=axs_opt_params[i + 1], + ) + axs_opt_params[i + 1].set_xlabel("") + axs_opt_params[i + 1].set_ylabel("") + axs_opt_params[i + 1].get_legend().remove() + axs_opt_params[i + 1].ticklabel_format( + axis="x", style="scientific", scilimits=(-1, 1) + ) + # Set legend for all subplots: plot in own subplot + axs_opt_params[0].axis("off") + handles, labels = axs_opt_params[1].get_legend_handles_labels() + axs_opt_params[0].legend(handles=handles, labels=labels, ncols=3, loc="center") + + subfigs[0].supxlabel(x_axis_label) + subfigs[0].supylabel("Optimisation parameter") + else: + sns.stripplot( + data=opt_params_values_with_names_df_melt, + x="value", + y="variable", + hue=TAG, + jitter=True, + ax=axs_opt_params, + ) + + axs_opt_params.set_xlabel(x_axis_label) + axs_opt_params.set_ylabel("Optimisation parameter") + axs_opt_params.legend() + axs_opt_params.grid() + + # Plot objf change separately + axs_opt_params = subfigs[1].subplots(nrows=nrows_obj_func_rmse_subplot) + if nrows_obj_func_rmse_subplot > 1: + ax_obj_func = axs_opt_params[0] + ax_rmse = axs_opt_params[1] + else: + ax_obj_func = axs_opt_params + + # Melt for seaborn stripplot + norm_objf_values_df_melt = norm_objf_values_df.melt(id_vars=TAG) + sns.stripplot( + data=norm_objf_values_df_melt, + x="value", + y="variable", + hue=TAG, + jitter=True, + ax=ax_obj_func, + formatter=lambda label: objf_name, + ) + + ax_obj_func.get_legend().remove() + # Objective function values are not normalised (no initial value): be explicit + ax_obj_func.set_xlabel("Objective function value") + ax_obj_func.set_ylabel("") + + if rmse_df is not None: + # Ensure solution legend colours are the same: tags match between opt + # params and RMS error plot. This can happen if not normalising opt + # params, but RMS error plot requested + rmse_df_matched = rmse_df[ + rmse_df["tag"].isin(opt_params_values_with_names_df["tag"]) + ] + + rmse_df_matched_melt = rmse_df_matched.melt(id_vars=TAG) + sns.stripplot( + data=rmse_df_matched_melt, + x="value", + y="variable", + hue=TAG, + jitter=True, + ax=ax_rmse, + formatter=lambda label: f"Relative to\n{normalising_tag}", + ) + ax_rmse.set_xlabel("RMS error") + ax_rmse.set_ylabel("") + ax_rmse.get_legend().remove() + + return fig + + +def _rms_errors( + results_df: pd.DataFrame, + opt_param_value_pattern: str, + normalising_tag: str, +) -> pd.DataFrame: + """Calculate RMS errors between different solutions. + + Summarise solution differences in single number. + :param results_df: df containing multiple solutions + :type results_df: pandas.DataFrame + :param opt_param_value_pattern: normalisation type for opt params in mfile + :type opt_param_value_pattern: str + :param normalising_tag: tag to calculate RMSEs against + :type normalising_tag: str + :return: RMS errors for each solution + :rtype: pandas.DataFrame + """ + normalising_soln, _ = _separate_norm_solution(results_df, normalising_tag) + # Reference solution to calculate RMS errors against + ref_soln_opt_params = _filter_opt_params( + normalising_soln, opt_param_value_pattern=opt_param_value_pattern + ) + # Solutions that need RMS errors calculating + # Include reference solution here, so that its RMS error is calculated (as 0) + # This is so that the colours in the RMSE plot match those in the main + # optimisation parameter plot's legend + all_solns_opt_params = _filter_opt_params( + results_df, opt_param_value_pattern=opt_param_value_pattern + ) + + ref_soln_opt_params_np = ref_soln_opt_params.to_numpy() + solns_opt_params_to_rms_np = all_solns_opt_params.to_numpy() + + rmses = np.sqrt( + np.mean((solns_opt_params_to_rms_np - ref_soln_opt_params_np) ** 2, axis=1) + ) + + # Create df of tags and rmses + tag_series = results_df["tag"] + rmse_series = pd.Series(rmses, name="rmse") + rmse_df = pd.concat([tag_series, rmse_series], axis=1) + return rmse_df diff --git a/requirements.txt b/requirements.txt index 7d757f5a91..f4ca6149e0 100644 --- a/requirements.txt +++ b/requirements.txt @@ -22,3 +22,4 @@ PyVMCON>=2.1.0,<3.0.0 CoolProp>=6.4 Jinja2>=3.0 cvxpy!=1.3.0,!=1.3.1 +seaborn>=0.12.2 diff --git a/setup.py b/setup.py index 62242ca2ac..2a91724ca1 100644 --- a/setup.py +++ b/setup.py @@ -45,6 +45,7 @@ "numba>=0.57", "PyVMCON>=2.1.0,<3.0.0", "CoolProp>=6.4", + "seaborn>=0.12.2", ], "extras_require": {"test": ["pytest"]}, "entry_points": { diff --git a/source/fortran/numerics.f90 b/source/fortran/numerics.f90 index ebb117193b..50d4ffca89 100755 --- a/source/fortran/numerics.f90 +++ b/source/fortran/numerics.f90 @@ -383,6 +383,8 @@ module numerics real(dp) :: sqsumsq !! sqsumsq : sqrt of the sum of the square of the constraint residuals + character(len=40) :: objf_name + !! Description of the objective function real(dp) :: norm_objf !! Normalised objective function (figure of merit) real(dp) :: epsfcn @@ -421,25 +423,25 @@ subroutine init_numerics() ioptimz = 1 minmax = 7 lablmm = (/ & - 'major radius. ', & - 'not used. ', & - 'neutron wall load. ', & - 'P_tf + P_pf. ', & - 'fusion gain. ', & - 'cost of electricity. ', & - 'capital cost. ', & - 'aspect ratio. ', & - 'divertor heat load. ', & - 'toroidal field. ', & - 'total injected power. ', & - 'H plant capital cost. ', & - 'H production rate. ', & - 'pulse length. ', & - 'plant availability. ', & - 'min R0, max tau_burn. ', & - 'net electrical output.', & - 'Null figure of merit. ', & - 'max Q, max t_burn. ' & + 'major radius ', & + 'not used ', & + 'neutron wall load ', & + 'P_tf + P_pf ', & + 'fusion gain ', & + 'cost of electricity ', & + 'capital cost ', & + 'aspect ratio ', & + 'divertor heat load ', & + 'toroidal field ', & + 'total injected power ', & + 'H plant capital cost ', & + 'H production rate ', & + 'pulse length ', & + 'plant availability ', & + 'min R0, max tau_burn ', & + 'net electrical output ', & + 'Null figure of merit ', & + 'max Q, max t_burn ' & /) ncalls = 0 @@ -558,6 +560,7 @@ subroutine init_numerics() lablxc = '' ! Issue 287 iteration variables are now defined in module define_iteration_variables in iteration variables.f90 sqsumsq = 0.0D0 + objf_name = "" norm_objf = 0.0D0 epsfcn = 1.0D-3 epsvmc = 1.0D-6 diff --git a/source/fortran/scan.f90 b/source/fortran/scan.f90 index 1bf55ca9e2..178ccf850a 100644 --- a/source/fortran/scan.f90 +++ b/source/fortran/scan.f90 @@ -886,7 +886,6 @@ subroutine post_optimise(ifail) real(dp), dimension(ipeqns) :: con1, con2, err character(len=1), dimension(ipeqns) :: sym character(len=10), dimension(ipeqns) :: lab - character(len=30) :: strfom character(len=60) :: string1, string2 ! !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! @@ -955,9 +954,12 @@ subroutine post_optimise(ifail) ! call ovarin(nout,'VMCON error flag','(ifail)',ifail) ! end if + objf_name = '"'//trim(lablmm(abs(minmax)))//'"' + ! Quotes required for string parsing in MFILE + call ovarst(nout,'Objective function name','(objf_name)',objf_name) + call ovarre(nout,'Normalised objective function','(norm_objf)',norm_objf, 'OP ') call ovarre(nout,'Square root of the sum of squares of the constraint residuals','(sqsumsq)',sqsumsq, 'OP ') call ovarre(nout,'VMCON convergence parameter','(convergence_parameter)',convergence_parameter, 'OP ') - call ovarre(nout,'Normalised objective function','(norm_objf)',norm_objf, 'OP ') call ovarin(nout,'Number of VMCON iterations','(nviter)',nviter, 'OP ') call oblnkl(nout) @@ -973,9 +975,8 @@ subroutine post_optimise(ifail) string2 = ' to maximise the figure of merit: ' end if - strfom = lablmm(abs(minmax)) - call upper_case(strfom) - write(nout,10) trim(string1) // trim(string2), trim(strfom) + call upper_case(objf_name) + write(nout,10) trim(string1) // trim(string2), trim(objf_name) 10 format(a90, t92, a22) call oblnkl(nout) diff --git a/tests/integration/data/large_tokamak_1_MFILE.DAT b/tests/integration/data/large_tokamak_1_MFILE.DAT new file mode 100644 index 0000000000..64ce2913b4 --- /dev/null +++ b/tests/integration/data/large_tokamak_1_MFILE.DAT @@ -0,0 +1,1801 @@ + # PROCESS # + # Power Reactor Optimisation Code # + # PROCESS # + # Power Reactor Optimisation Code # + PROCESS_version_number__________________________________________________ (procver)_____________________ "3.0.2 R" + Date_of_run_____________________________________________________________ (date)________________________ "08/02/2024" + Time_of_run_____________________________________________________________ (time)________________________ "10:56" + User____________________________________________________________________ (username)____________________ "timothyn" + PROCESS_run_title_______________________________________________________ (runtitle)____________________ "Generic large tokamak + PROCESS_tag_number______________________________________________________ (tagno)_______________________ "v3.0.2-7-gec9530fb1" + PROCESS_git_branch_name_________________________________________________ (branch_name)_________________ "3033-inequality-constraint-for-injected-power-coded-with-the-wrong-signbug" + PROCESS_last_commit_message_____________________________________________ (commsg)______________________ "Merge branch |main| into 3033-inequality-constraint-for-injected-power-coded-with-the-wrong-signbug + Input_filename__________________________________________________________ (fileprefix)__________________ "/private/var/folders/2c/5k4t0wm94jxdmnqwdvn_h59r0000gq/T/pytest-of-timothynunn/pytest-56/test_scenario_large_tokamak_0/IN.DAT " + # Numerics # + VMCON_error_flag________________________________________________________ (ifail)_______________________ 1 + # PROCESS found a feasible solution # + Number_of_iteration_variables___________________________________________ (nvar)________________________ 45 + Number_of_constraints_(total)___________________________________________ (neqns+nineqns)_______________ 26 + Optimisation_switch_____________________________________________________ (ioptimz)_____________________ 1 + Figure_of_merit_switch__________________________________________________ (minmax)______________________ 1 + Objective_function_name_________________________________________________ (objf_name)___________________ "major radius" + Square_root_of_the_sum_of_squares_of_the_constraint_residuals___________ (sqsumsq)_____________________ 1.8713E-04 OP + VMCON_convergence_parameter_____________________________________________ (convergence_parameter)_______ 0.0000E+00 OP + Normalised_objective_function___________________________________________ (norm_objf)___________________ 1.6000E+00 OP + Number_of_VMCON_iterations______________________________________________ (nviter)______________________ 0 OP + beta____________________________________________________________________ (itvar001)____________________ 3.3648E-02 + beta_(final_value/initial_value)________________________________________ (xcm001)______________________ 1.1216E+00 + beta_(range_normalised)_________________________________________________ (nitvar001)___________________ 3.2681E-02 + dene____________________________________________________________________ (itvar002)____________________ 8.0667E+19 + dene_(final_value/initial_value)________________________________________ (xcm002)______________________ 1.0756E+00 + dene_(range_normalised)_________________________________________________ (nitvar002)___________________ 7.1381E-02 + fwalld__________________________________________________________________ (itvar003)____________________ 5.0758E-01 + fwalld_(final_value/initial_value)______________________________________ (xcm003)______________________ 5.0758E-01 + fwalld_(range_normalised)_______________________________________________ (nitvar003)___________________ 5.0709E-01 + ffuspow_________________________________________________________________ (itvar004)____________________ 5.4006E-01 + ffuspow_(final_value/initial_value)_____________________________________ (xcm004)______________________ 5.4006E-01 + ffuspow_(range_normalised)______________________________________________ (nitvar004)___________________ 5.3960E-01 + ftburn__________________________________________________________________ (itvar005)____________________ 9.9940E-01 + ftburn_(final_value/initial_value)______________________________________ (xcm005)______________________ 9.9940E-01 + ftburn_(range_normalised)_______________________________________________ (nitvar005)___________________ 9.9940E-01 + flhthresh_______________________________________________________________ (itvar006)____________________ 1.6735E+00 + flhthresh_(final_value/initial_value)___________________________________ (xcm006)______________________ 1.6735E+00 + flhthresh_(range_normalised)____________________________________________ (nitvar006)___________________ 7.4836E-02 + fpinj___________________________________________________________________ (itvar007)____________________ 4.0071E-01 + fpinj_(final_value/initial_value)_______________________________________ (xcm007)______________________ 4.0071E-01 + fpinj_(range_normalised)________________________________________________ (nitvar007)___________________ 4.0011E-01 + fpnetel_________________________________________________________________ (itvar008)____________________ 1.0000E+00 + fpnetel_(final_value/initial_value)_____________________________________ (xcm008)______________________ 1.0000E+00 + fpnetel_(range_normalised)______________________________________________ (nitvar008)___________________ 1.0000E+00 + fbetatry________________________________________________________________ (itvar009)____________________ 5.0870E-01 + fbetatry_(final_value/initial_value)____________________________________ (xcm009)______________________ 1.0174E+00 + fbetatry_(range_normalised)_____________________________________________ (nitvar009)___________________ 5.0821E-01 + fpeakb__________________________________________________________________ (itvar010)____________________ 8.6988E-01 + fpeakb_(final_value/initial_value)______________________________________ (xcm010)______________________ 8.6988E-01 + fpeakb_(range_normalised)_______________________________________________ (nitvar010)___________________ 8.6975E-01 + coheof__________________________________________________________________ (itvar011)____________________ 2.0264E+07 + coheof_(final_value/initial_value)______________________________________ (xcm011)______________________ 1.3510E+00 + coheof_(range_normalised)_______________________________________________ (nitvar011)___________________ 2.0185E-01 + fjohc___________________________________________________________________ (itvar012)____________________ 5.5541E-01 + fjohc_(final_value/initial_value)_______________________________________ (xcm012)______________________ 9.2569E-01 + fjohc_(range_normalised)________________________________________________ (nitvar012)___________________ 5.5092E-01 + fjohc0__________________________________________________________________ (itvar013)____________________ 5.4190E-01 + fjohc0_(final_value/initial_value)______________________________________ (xcm013)______________________ 9.0316E-01 + fjohc0_(range_normalised)_______________________________________________ (nitvar013)___________________ 5.4144E-01 + fcohbop_________________________________________________________________ (itvar014)____________________ 9.4380E-01 + fcohbop_(final_value/initial_value)_____________________________________ (xcm014)______________________ 1.0487E+00 + fcohbop_(range_normalised)______________________________________________ (nitvar014)___________________ 9.4374E-01 + fiooic__________________________________________________________________ (itvar015)____________________ 7.1737E-01 + fiooic_(final_value/initial_value)______________________________________ (xcm015)______________________ 1.1036E+00 + fiooic_(range_normalised)_______________________________________________ (nitvar015)___________________ 7.1709E-01 + fvdump__________________________________________________________________ (itvar016)____________________ 9.5837E-01 + fvdump_(final_value/initial_value)______________________________________ (xcm016)______________________ 9.5837E-01 + fvdump_(range_normalised)_______________________________________________ (nitvar016)___________________ 9.5833E-01 + vdalw___________________________________________________________________ (itvar017)____________________ 9.5837E+00 + vdalw_(final_value/initial_value)_______________________________________ (xcm017)______________________ 9.5837E-01 + vdalw_(range_normalised)________________________________________________ (nitvar017)___________________ 9.5837E-01 + fjprot__________________________________________________________________ (itvar018)____________________ 9.9639E-01 + fjprot_(final_value/initial_value)______________________________________ (xcm018)______________________ 9.9639E-01 + fjprot_(range_normalised)_______________________________________________ (nitvar018)___________________ 9.9639E-01 + ftmargtf________________________________________________________________ (itvar019)____________________ 9.9673E-01 + ftmargtf_(final_value/initial_value)____________________________________ (xcm019)______________________ 9.9673E-01 + ftmargtf_(range_normalised)_____________________________________________ (nitvar019)___________________ 9.9672E-01 + ftmargoh________________________________________________________________ (itvar020)____________________ 9.9653E-01 + ftmargoh_(final_value/initial_value)____________________________________ (xcm020)______________________ 9.9653E-01 + ftmargoh_(range_normalised)_____________________________________________ (nitvar020)___________________ 9.9652E-01 + ftaulimit_______________________________________________________________ (itvar021)____________________ 7.1930E-01 + ftaulimit_(final_value/initial_value)___________________________________ (xcm021)______________________ 7.1930E-01 + ftaulimit_(range_normalised)____________________________________________ (nitvar021)___________________ 7.1902E-01 + fmaxvvstress____________________________________________________________ (itvar022)____________________ 4.2966E-01 + fmaxvvstress_(final_value/initial_value)________________________________ (xcm022)______________________ 4.2966E-01 + fmaxvvstress_(range_normalised)_________________________________________ (nitvar022)___________________ 4.2909E-01 + foh_stress______________________________________________________________ (itvar023)____________________ 9.0092E-01 + foh_stress_(final_value/initial_value)__________________________________ (xcm023)______________________ 9.0092E-01 + foh_stress_(range_normalised)___________________________________________ (nitvar023)___________________ 9.0082E-01 + fne0____________________________________________________________________ (itvar024)____________________ 5.9638E-01 + fne0_(final_value/initial_value)________________________________________ (xcm024)______________________ 5.9638E-01 + fne0_(range_normalised)_________________________________________________ (nitvar024)___________________ 5.9598E-01 + fpsepbqar_______________________________________________________________ (itvar025)____________________ 1.0000E+00 + fpsepbqar_(final_value/initial_value)___________________________________ (xcm025)______________________ 1.0000E+00 + fpsepbqar_(range_normalised)____________________________________________ (nitvar025)___________________ 1.0000E+00 + fstrcase________________________________________________________________ (itvar026)____________________ 9.9670E-01 + fstrcase_(final_value/initial_value)____________________________________ (xcm026)______________________ 9.9670E-01 + fstrcase_(range_normalised)_____________________________________________ (nitvar026)___________________ 9.9670E-01 + fstrcond________________________________________________________________ (itvar027)____________________ 8.5185E-01 + fstrcond_(final_value/initial_value)____________________________________ (xcm027)______________________ 8.5185E-01 + fstrcond_(range_normalised)_____________________________________________ (nitvar027)___________________ 8.5171E-01 + bt______________________________________________________________________ (itvar028)____________________ 5.2940E+00 + bt_(final_value/initial_value)__________________________________________ (xcm028)______________________ 9.2877E-01 + bt_(range_normalised)___________________________________________________ (nitvar028)___________________ 1.7619E-01 + rmajor__________________________________________________________________ (itvar029)____________________ 8.0000E+00 + rmajor_(final_value/initial_value)______________________________________ (xcm029)______________________ 1.0000E+00 + rmajor_(range_normalised)_______________________________________________ (nitvar029)___________________ 0.0000E+00 + te______________________________________________________________________ (itvar030)____________________ 1.2489E+01 + te_(final_value/initial_value)__________________________________________ (xcm030)______________________ 1.0407E+00 + te_(range_normalised)___________________________________________________ (nitvar030)___________________ 7.3903E-02 + hfact___________________________________________________________________ (itvar031)____________________ 1.1886E+00 + hfact_(final_value/initial_value)_______________________________________ (xcm031)______________________ 1.0805E+00 + hfact_(range_normalised)________________________________________________ (nitvar031)___________________ 9.8961E-01 + tfcth___________________________________________________________________ (itvar032)____________________ 1.2000E+00 + tfcth_(final_value/initial_value)_______________________________________ (xcm032)______________________ 1.0000E+00 + tfcth_(range_normalised)________________________________________________ (nitvar032)___________________ 1.1628E-01 + ohcth___________________________________________________________________ (itvar033)____________________ 5.7587E-01 + ohcth_(final_value/initial_value)_______________________________________ (xcm033)______________________ 1.1517E+00 + ohcth_(range_normalised)________________________________________________ (nitvar033)___________________ 2.8441E-02 + q_______________________________________________________________________ (itvar034)____________________ 3.5961E+00 + q_(final_value/initial_value)___________________________________________ (xcm034)______________________ 1.0275E+00 + q_(range_normalised)____________________________________________________ (nitvar034)___________________ 1.2684E-02 + bore____________________________________________________________________ (itvar035)____________________ 1.9854E+00 + bore_(final_value/initial_value)________________________________________ (xcm035)______________________ 9.9271E-01 + bore_(range_normalised)_________________________________________________ (nitvar035)___________________ 1.9045E-01 + fvsbrnni________________________________________________________________ (itvar036)____________________ 4.3358E-01 + fvsbrnni_(final_value/initial_value)____________________________________ (xcm036)______________________ 1.0839E+00 + fvsbrnni_(range_normalised)_____________________________________________ (nitvar036)___________________ 4.3301E-01 + tdmptf__________________________________________________________________ (itvar037)____________________ 1.8429E+01 + tdmptf_(final_value/initial_value)______________________________________ (xcm037)______________________ 7.3716E-01 + tdmptf_(range_normalised)_______________________________________________ (nitvar037)___________________ 1.8347E-01 + thkcas__________________________________________________________________ (itvar038)____________________ 2.8216E-01 + thkcas_(final_value/initial_value)______________________________________ (xcm038)______________________ 5.6431E-01 + thkcas_(range_normalised)_______________________________________________ (nitvar038)___________________ 2.4437E-01 + thwcndut________________________________________________________________ (itvar039)____________________ 8.0099E-03 + thwcndut_(final_value/initial_value)____________________________________ (xcm039)______________________ 1.0012E+00 + thwcndut_(range_normalised)_____________________________________________ (nitvar039)___________________ 1.0716E-04 + fcutfsu_________________________________________________________________ (itvar040)____________________ 8.4212E-01 + fcutfsu_(final_value/initial_value)_____________________________________ (xcm040)______________________ 1.0526E+00 + fcutfsu_(range_normalised)______________________________________________ (nitvar040)___________________ 7.7755E-01 + cpttf___________________________________________________________________ (itvar041)____________________ 8.9795E+04 + cpttf_(final_value/initial_value)_______________________________________ (xcm041)______________________ 1.3815E+00 + cpttf_(range_normalised)________________________________________________ (nitvar041)___________________ 9.9182E-01 + ralpne__________________________________________________________________ (itvar042)____________________ 8.3954E-02 + ralpne_(final_value/initial_value)______________________________________ (xcm042)______________________ 8.3954E-01 + ralpne_(range_normalised)_______________________________________________ (nitvar042)___________________ 6.7908E-01 + oh_steel_frac___________________________________________________________ (itvar043)____________________ 5.1868E-01 + oh_steel_frac_(final_value/initial_value)_______________________________ (xcm043)______________________ 6.4835E-01 + oh_steel_frac_(range_normalised)________________________________________ (nitvar043)___________________ 5.4550E-01 + fimp(13)________________________________________________________________ (itvar044)____________________ 5.7149E-04 + fimp(13)_(final_value/initial_value)____________________________________ (xcm044)______________________ 1.5039E+00 + fimp(13)_(range_normalised)_____________________________________________ (nitvar044)___________________ 5.7148E-02 + dr_tf_wp________________________________________________________________ (itvar045)____________________ 5.0416E-01 + dr_tf_wp_(final_value/initial_value)____________________________________ (xcm045)______________________ 1.0083E+00 + dr_tf_wp_(range_normalised)_____________________________________________ (nitvar045)___________________ 6.5100E-02 + Beta_consistency__________________normalised_residue____________________ (normres001)__________________ 6.5770E-07 + Global_power_balance_consistency__normalised_residue____________________ (normres002)__________________ 1.2292E-07 + Radial_build_consistency__________normalised_residue____________________ (normres003)__________________ -7.3085E-11 + Density_upper_limit_______________normalised_residue____________________ (normres004)__________________ 1.6272E-08 + Neutron_wall_load_upper_limit_____normalised_residue____________________ (normres005)__________________ 1.4241E-07 + Fusion_power_upper_limit__________normalised_residue____________________ (normres006)__________________ 2.6565E-07 + Burn_time_lower_limit_____________normalised_residue____________________ (normres007)__________________ -1.2011E-04 + L-H_power_threshold_limit_________normalised_residue____________________ (normres008)__________________ -3.0891E-07 + Injection_power_upper_limit_______normalised_residue____________________ (normres009)__________________ 2.4418E-07 + Net_electric_power_lower_limit____normalised_residue____________________ (normres010)__________________ 1.5045E-05 + Beta_upper_limit__________________normalised_residue____________________ (normres011)__________________ 2.4702E-07 + Peak_toroidal_field_upper_limit___normalised_residue____________________ (normres012)__________________ 2.5809E-09 + CS_coil_EOF_current_density_limit_normalised_residue____________________ (normres013)__________________ -8.4245E-08 + CS_coil_BOP_current_density_limit_normalised_residue____________________ (normres014)__________________ 1.9393E-09 + I_op_/_I_critical_(TF_coil)_______normalised_residue____________________ (normres015)__________________ -3.8375E-07 + Dump_voltage_upper_limit__________normalised_residue____________________ (normres016)__________________ -1.5214E-04 + J_winding_pack/J_protection_limit_normalised_residue____________________ (normres017)__________________ -2.9894E-07 + TF_coil_temp._margin_lower_limit__normalised_residue____________________ (normres018)__________________ -1.0631E-06 + CS_temperature_margin_lower_limit_normalised_residue____________________ (normres019)__________________ 8.0251E-08 + taup/taueff_______________________normalised_residue____________________ (normres020)__________________ -1.8772E-08 + Dump_time_set_by_VV_stress________normalised_residue____________________ (normres021)__________________ -1.0026E-07 + CS_Tresca_yield_criterion_________normalised_residue____________________ (normres022)__________________ -1.6044E-07 + ne0_>_neped_______________________normalised_residue____________________ (normres023)__________________ -1.9637E-08 + Upper_Lim._on_Psep_*_Bt_/_q_A_R___normalised_residue____________________ (normres024)__________________ 4.9789E-07 + TF_coil_case_stress_upper_limit___normalised_residue____________________ (normres025)__________________ -4.6757E-07 + TF_coil_conduit_stress_upper_lim__normalised_residue____________________ (normres026)__________________ -4.1375E-07 + # Final Feasible Point # + # Power Reactor Costs (1990 US$) # + First_wall_/_blanket_life_(years)_______________________________________ (fwbllife)____________________ 6.1566E+00 + Divertor_life_(years)___________________________________________________ (divlife.)____________________ 3.9769E+00 + Cost_of_electricity_(m$/kWh)____________________________________________ (coe)_________________________ 5.1257E+02 + # Detailed Costings (1990 US$) # + Acc.22_multiplier_for_Nth_of_a_kind_____________________________________ (fkind)_______________________ 1.0000E+00 + Level_of_Safety_Assurance_______________________________________________ (lsa)_________________________ 4 + # Structures and Site Facilities # + Site_improvements,_facilities,_land_(M$)________________________________ (c211)________________________ 3.5200E+01 + Reactor_building_cost_(M$)______________________________________________ (c212)________________________ 4.5238E+02 + Turbine_building_cost_(M$)______________________________________________ (c213)________________________ 3.8000E+01 + Reactor_maintenance_building_cost_(M$)__________________________________ (c2141)_______________________ 1.0307E+02 + Warm_shop_cost_(M$)_____________________________________________________ (c2142)_______________________ 5.7641E+01 + Tritium_building_cost_(M$)______________________________________________ (c215)________________________ 1.4800E+01 + Electrical_equipment_building_cost_(M$)_________________________________ (c216)________________________ 1.9736E+01 + Additional_buildings_cost_(M$)__________________________________________ (c2171)_______________________ 1.8000E+01 + Control_room_buildings_cost_(M$)________________________________________ (c2172)_______________________ 2.1000E+01 + Shop_and_warehouses_cost_(M$)___________________________________________ (c2173)_______________________ 1.1500E+01 + Cryogenic_building_cost_(M$)____________________________________________ (c2174)_______________________ 6.8891E+00 + Total_account_21_cost_(M$)______________________________________________ (c21)_________________________ 7.7822E+02 + # Reactor Systems # + First_wall_cost_(M$)____________________________________________________ (c2211)_______________________ 1.9130E+02 + Blanket_beryllium_cost_(M$)_____________________________________________ (c22121)______________________ 2.6109E+02 + Blanket_breeder_material_cost_(M$)______________________________________ (c22122)______________________ 6.3985E+02 + Blanket_stainless_steel_cost_(M$)_______________________________________ (c22123)______________________ 8.0726E+01 + Blanket_vanadium_cost_(M$)______________________________________________ (c22124)______________________ 0.0000E+00 + Blanket_total_cost_(M$)_________________________________________________ (c2212)_______________________ 9.8166E+02 + Bulk_shield_cost_(M$)___________________________________________________ (c22131)______________________ 7.8394E+01 + Penetration_shielding_cost_(M$)_________________________________________ (c22132)______________________ 7.8394E+01 + Total_shield_cost_(M$)__________________________________________________ (c2213)_______________________ 1.5679E+02 + Total_support_structure_cost_(M$)_______________________________________ (c2214)_______________________ 4.0933E+01 + Divertor_cost_(M$)______________________________________________________ (c2215)_______________________ 4.1660E+01 + Total_account_221_cost_(M$)_____________________________________________ (c221)________________________ 1.4123E+03 + # Magnets # + TF_coil_conductor_cost_(M$)_____________________________________________ (c22211)______________________ 1.3230E+02 + TF_coil_winding_cost_(M$)_______________________________________________ (c22212)______________________ 5.4263E+01 + TF_coil_case_cost_(M$)__________________________________________________ (c22213)______________________ 4.4365E+02 + TF_intercoil_structure_cost_(M$)________________________________________ (c22214)______________________ 1.5066E+02 + TF_coil_gravity_support_structure_(M$)__________________________________ (c22215)______________________ 4.4659E+01 + TF_magnet_assemblies_cost_(M$)__________________________________________ (c2221)_______________________ 8.2552E+02 + PF_coil_conductor_cost_(M$)_____________________________________________ (c22221)______________________ 4.6409E+02 + PF_coil_winding_cost_(M$)_______________________________________________ (c22222)______________________ 7.6765E+01 + PF_coil_case_cost_(M$)__________________________________________________ (c22223)______________________ 9.4861E+01 + PF_coil_support_structure_cost_(M$)_____________________________________ (c22224)______________________ 8.0235E+00 + PF_magnet_assemblies_cost_(M$)__________________________________________ (c2222)_______________________ 6.4374E+02 + Vacuum_vessel_assembly_cost_(M$)________________________________________ (c2223)_______________________ 2.5404E+02 + Total_account_222_cost_(M$)_____________________________________________ (c222)________________________ 1.7233E+03 + # Power Injection # + ECH_system_cost_(M$)____________________________________________________ (c2231)_______________________ 2.4043E+02 + Lower_hybrid_system_cost_(M$)___________________________________________ (c2232)_______________________ 0.0000E+00 + Neutral_beam_system_cost_(M$)___________________________________________ (c2233)_______________________ 0.0000E+00 + Total_account_223_cost_(M$)_____________________________________________ (c223)________________________ 2.4043E+02 + # Vacuum Systems # + High_vacuum_pumps_cost_(M$)_____________________________________________ (c2241)_______________________ 1.2480E+01 + Backing_pumps_cost_(M$)_________________________________________________ (c2242)_______________________ 4.6800E+00 + Vacuum_duct_cost_(M$)___________________________________________________ (c2243)_______________________ 2.5280E+00 + Valves_cost_(M$)________________________________________________________ (c2244)_______________________ 5.7410E+00 + Duct_shielding_cost_(M$)________________________________________________ (c2245)_______________________ 0.0000E+00 + Instrumentation_cost_(M$)_______________________________________________ (c2246)_______________________ 1.3000E+00 + Total_account_224_cost_(M$)_____________________________________________ (c224)________________________ 2.6729E+01 + # Power Conditioning # + TF_coil_power_supplies_cost_(M$)________________________________________ (c22511)______________________ 4.0144E+00 + TF_coil_breakers_cost_(M$)______________________________________________ (c22512)______________________ 3.4127E+01 + TF_coil_dump_resistors_cost_(M$)________________________________________ (c22513)______________________ 2.1322E+01 + TF_coil_instrumentation_and_control_(M$)________________________________ (c22514)______________________ 4.8000E+00 + TF_coil_bussing_cost_(M$)_______________________________________________ (c22515)______________________ 3.5267E+01 + Total,_TF_coil_power_costs_(M$)_________________________________________ (c2251)_______________________ 9.9531E+01 + PF_coil_power_supplies_cost_(M$)________________________________________ (c22521)______________________ 2.9591E+00 + PF_coil_instrumentation_and_control_(M$)________________________________ (c22522)______________________ 3.6000E+00 + PF_coil_bussing_cost_(M$)_______________________________________________ (c22523)______________________ 1.1995E+01 + PF_coil_burn_power_supplies_cost_(M$)___________________________________ (c22524)______________________ 1.2679E+00 + PF_coil_breakers_cost_(M$)______________________________________________ (c22525)______________________ 1.4709E+01 + PF_coil_dump_resistors_cost_(M$)________________________________________ (c22526)______________________ 4.3206E+00 + PF_coil_ac_breakers_cost_(M$)___________________________________________ (c22527)______________________ 9.0000E-01 + Total,_PF_coil_power_costs_(M$)_________________________________________ (c2252)_______________________ 3.9752E+01 + Total,_energy_storage_cost_(M$)_________________________________________ (c2253)_______________________ 1.6864E+01 + Total_account_225_cost_(M$)_____________________________________________ (c225)________________________ 1.5615E+02 + # Heat Transport System # + Pumps_and_piping_system_cost_(M$)_______________________________________ (cpp)_________________________ 3.6795E+01 + Primary_heat_exchanger_cost_(M$)________________________________________ (chx)_________________________ 7.1692E+01 + Total,_reactor_cooling_system_cost_(M$)_________________________________ (c2261)_______________________ 1.0849E+02 + Pumps,_piping_cost_(M$)_________________________________________________ (cppa)________________________ 2.8417E+01 + Total,_auxiliary_cooling_system_cost_(M$)_______________________________ (c2262)_______________________ 2.8417E+01 + Total,_cryogenic_system_cost_(M$)_______________________________________ (c2263)_______________________ 1.7039E+02 + Total_account_226_cost_(M$)_____________________________________________ (c226)________________________ 3.0729E+02 + # Fuel Handling System # + Fuelling_system_cost_(M$)_______________________________________________ (c2271)_______________________ 2.2300E+01 + Fuel_processing_and_purification_cost_(M$)______________________________ (c2272)_______________________ 1.0229E+02 + Atmospheric_recovery_systems_cost_(M$)__________________________________ (c2273)_______________________ 5.8088E+01 + Nuclear_building_ventilation_cost_(M$)__________________________________ (c2274)_______________________ 6.9201E+01 + Total_account_227_cost_(M$)_____________________________________________ (c227)________________________ 2.5188E+02 + # Instrumentation and Control # + Instrumentation_and_control_cost_(M$)___________________________________ (c228)________________________ 1.5000E+02 + # Maintenance Equipment # + Maintenance_equipment_cost_(M$)_________________________________________ (c229)________________________ 1.2500E+02 + # Total Account 22 Cost # + Total_account_22_cost_(M$)______________________________________________ (c22)_________________________ 4.3931E+03 + # Turbine Plant Equipment # + Turbine_plant_equipment_cost_(M$)_______________________________________ (c23)_________________________ 1.7613E+02 + # Electric Plant Equipment # + Switchyard_equipment_cost_(M$)__________________________________________ (c241)________________________ 1.8400E+01 + Transformers_cost_(M$)__________________________________________________ (c242)________________________ 8.0330E+00 + Low_voltage_equipment_cost_(M$)_________________________________________ (c243)________________________ 6.4513E+00 + Diesel_backup_equipment_cost_(M$)_______________________________________ (c244)________________________ 6.8000E+00 + Auxiliary_facilities_cost_(M$)__________________________________________ (c245)________________________ 1.5000E+00 + Total_account_24_cost_(M$)______________________________________________ (c24)_________________________ 4.1184E+01 + # Miscellaneous Plant Equipment # + Miscellaneous_plant_equipment_cost_(M$)_________________________________ (c25)_________________________ 2.5000E+01 + # Heat Rejection System # + Heat_rejection_system_cost_(M$)_________________________________________ (c26)_________________________ 4.9877E+01 + # Plant Direct Cost # + Plant_direct_cost_(M$)__________________________________________________ (cdirt)_______________________ 5.4635E+03 + # Reactor Core Cost # + Reactor_core_cost_(M$)__________________________________________________ (crctcore)____________________ 3.3761E+03 + # Indirect Cost # + Indirect_cost_(M$)______________________________________________________ (c9)__________________________ 1.8221E+03 + # Total Contingency # + Total_contingency_(M$)__________________________________________________ (ccont)_______________________ 1.4207E+03 + # Constructed Cost # + Constructed_cost_(M$)___________________________________________________ (concost)_____________________ 8.7063E+03 + # Interest during Construction # + Interest_during_construction_(M$)_______________________________________ (moneyint)____________________ 1.4365E+03 + # Total Capital Investment # + Total_capital_investment_(M$)___________________________________________ (capcost)_____________________ 1.0143E+04 + # Plant Availability # + Allowable_blanket_neutron_fluence_(MW-yr/m2)____________________________ (abktflnc)____________________ 5.0000E+00 + Allowable_divertor_heat_fluence_(MW-yr/m2)______________________________ (adivflnc)____________________ 7.0000E+00 + First_wall_/_blanket_lifetime_(years)___________________________________ (bktlife)_____________________ 6.1566E+00 OP + Divertor_lifetime_(years)_______________________________________________ (divlife)_____________________ 3.9769E+00 OP + Heating/CD_system_lifetime_(years)______________________________________ (cdrlife)_____________________ 6.1566E+00 OP + Total_plant_lifetime_(years)____________________________________________ (tlife)_______________________ 3.0000E+01 + Total_plant_availability_fraction_______________________________________ (cfactr)______________________ 8.0000E-01 + Number_of_fusion_cycles_to_reach_allowable_fw/blanket_DPA_______________ (bktcycles)___________________ 1.5787E+04 + # Plasma # + Tokamak_aspect_ratio_=_Conventional,_itart_=_0__________________________ (itart)_______________________ 0.0000E+00 + Major_radius_(m)________________________________________________________ (rmajor)______________________ 8.0000E+00 ITV + Minor_radius_(m)________________________________________________________ (rminor)______________________ 2.6667E+00 + Aspect_ratio____________________________________________________________ (aspect)______________________ 3.0000E+00 + Elongation,_X-point_(input_value_used)__________________________________ (kappa)_______________________ 1.8500E+00 + Elongation,_95%_surface_(calculated_from_kappa)_________________________ (kappa95)_____________________ 1.6518E+00 + Elongation,_area_ratio_calc.____________________________________________ (kappaa)______________________ 1.7188E+00 + Triangularity,_X-point_(input_value_used)_______________________________ (triang)______________________ 5.0000E-01 + Triangularity,_95%_surface_(calculated_from_triang)_____________________ (triang95)____________________ 3.3333E-01 + Plasma_poloidal_perimeter_(m)___________________________________________ (pperim)______________________ 2.4081E+01 + Plasma_cross-sectional_area_(m2)________________________________________ (xarea)_______________________ 3.8398E+01 + Plasma_surface_area_(m2)________________________________________________ (sarea)_______________________ 1.1738E+03 OP + Plasma_volume_(m3)______________________________________________________ (vol)_________________________ 1.8882E+03 OP + Plasma_current_scaling_law_used_________________________________________ (icurr)_______________________ 4 + Plasma_current_(MA)_____________________________________________________ (plascur/1D6)_________________ 1.6631E+01 + Current_density_profile_factor__________________________________________ (alphaj)______________________ 1.9805E+00 + Plasma_internal_inductance,_li__________________________________________ (rli)_________________________ 1.2275E+00 + Vertical_field_at_plasma_(T)____________________________________________ (bvert)_______________________ -7.4373E-01 + Vacuum_toroidal_field_at_R_(T)__________________________________________ (bt)__________________________ 5.2940E+00 ITV + Average_poloidal_field_(T)______________________________________________ (bp)__________________________ 8.6787E-01 + Total_field_(sqrt(bp^2_+_bt^2))_(T)_____________________________________ (btot)________________________ 5.3647E+00 + Safety_factor_on_axis___________________________________________________ (q0)__________________________ 1.0000E+00 + Safety_factor_at_95%_flux_surface_______________________________________ (q95)_________________________ 3.5961E+00 ITV + Cylindrical_safety_factor_(qcyl)________________________________________ (qstar)_______________________ 2.9805E+00 + Total_plasma_beta_______________________________________________________ (beta)________________________ 3.3648E-02 ITV + Total_poloidal_beta_____________________________________________________ (betap)_______________________ 1.2857E+00 OP + Total_toroidal_beta_____________________________________________________ ______________________________ 3.4553E-02 OP + Fast_alpha_beta_________________________________________________________ (betaft)______________________ 4.2236E-03 OP + Beam_ion_beta___________________________________________________________ (betanb)______________________ 0.0000E+00 OP + (Fast_alpha_+_beam_physics_variables.beta)/(thermal_physics_variables.be (gammaft)_____________________ 1.4354E-01 OP + Thermal_beta____________________________________________________________ ______________________________ 2.9425E-02 OP + Thermal_poloidal_beta___________________________________________________ ______________________________ 1.1243E+00 OP + Thermal_toroidal_physics_variables.beta_(=_beta-exp)____________________ ______________________________ 3.0215E-02 OP + 2nd_stability_physics_variables.beta_:_beta_p_/_(R/a)___________________ (eps*betap)___________________ 4.2857E-01 + 2nd_stability_physics_variables.beta_upper_limit________________________ (epbetmax)____________________ 1.3800E+00 + Beta_g_coefficient______________________________________________________ (dnbeta)______________________ 4.9099E+00 + Normalised_thermal_beta_________________________________________________ ______________________________ 2.4977E+00 + Normalised_total_beta___________________________________________________ ______________________________ 2.8562E+00 + Normalised_toroidal_beta________________________________________________ (normalised_toroidal_beta)____ 2.9330E+00 + Limit_on_thermal_beta___________________________________________________ (betalim)_____________________ 5.7842E-02 + Plasma_thermal_energy_(J)_______________________________________________ ______________________________ 9.5431E+08 OP + Total_plasma_internal_energy_(J)________________________________________ (total_plasma_internal_energy) 1.0913E+09 OP + Electron_temperature_(keV)______________________________________________ (te)__________________________ 1.2489E+01 ITV + Electron_temperature_on_axis_(keV)______________________________________ (te0)_________________________ 2.5758E+01 + Ion_temperature_(keV)___________________________________________________ (ti)__________________________ 1.2489E+01 + Ion_temperature_on_axis_(keV)___________________________________________ (ti0)_________________________ 2.5758E+01 + Electron_temp.,_density_weighted_(keV)__________________________________ (ten)_________________________ 1.3805E+01 + Electron_density_(/m3)__________________________________________________ (dene)________________________ 8.0667E+19 ITV + Electron_density_on_axis_(/m3)__________________________________________ (ne0)_________________________ 1.0610E+20 OP + Line-averaged_electron_density_(/m3)____________________________________ (dnla)________________________ 8.9334E+19 OP + Line-averaged_electron_density_/_Greenwald_density______________________ (dnla_gw)_____________________ 1.2000E+00 OP + Ion_density_(/m3)_______________________________________________________ (dnitot)______________________ 7.1669E+19 OP + Fuel_density_(/m3)______________________________________________________ (deni)________________________ 6.4831E+19 OP + Total_impurity_density_with_Z_>_2_(no_He)_(/m3)_________________________ (dnz)_________________________ 4.6503E+16 OP + Helium_ion_density_(thermalised_ions_only)_(/m3)________________________ (dnalp)_______________________ 6.7723E+18 OP + Proton_density_(/m3)____________________________________________________ (dnprot)______________________ 1.8963E+16 OP + Hot_beam_density_(/m3)__________________________________________________ (dnbeam)______________________ 0.0000E+00 OP + Density_limit_from_scaling_(/m3)________________________________________ (dnelimt)_____________________ 7.4445E+19 OP + Density_limit_(enforced)_(/m3)__________________________________________ (boundu(9)*dnelimt)___________ 7.4445E+19 OP + Helium_ion_density_(thermalised_ions_only)_/_electron_density___________ (ralpne)______________________ 8.3954E-02 ITV + H__concentration________________________________________________________ (fimp(01))____________________ 8.0392E-01 OP + He_concentration________________________________________________________ (fimp(02))____________________ 8.3954E-02 + Be_concentration________________________________________________________ (fimp(03))____________________ 0.0000E+00 + C__concentration________________________________________________________ (fimp(04))____________________ 0.0000E+00 + N__concentration________________________________________________________ (fimp(05))____________________ 0.0000E+00 + O__concentration________________________________________________________ (fimp(06))____________________ 0.0000E+00 + Ne_concentration________________________________________________________ (fimp(07))____________________ 0.0000E+00 + Si_concentration________________________________________________________ (fimp(08))____________________ 0.0000E+00 + Ar_concentration________________________________________________________ (fimp(09))____________________ 0.0000E+00 + Fe_concentration________________________________________________________ (fimp(10))____________________ 0.0000E+00 + Ni_concentration________________________________________________________ (fimp(11))____________________ 0.0000E+00 + Kr_concentration________________________________________________________ (fimp(12))____________________ 0.0000E+00 + Xe_concentration________________________________________________________ (fimp(13))____________________ 5.7149E-04 ITV + W__concentration________________________________________________________ (fimp(14))____________________ 5.0000E-06 + Average_mass_of_all_ions_(amu)__________________________________________ (aion)________________________ 2.7252E+00 OP + Effective_charge________________________________________________________ (zeff)________________________ 2.5164E+00 + Density_profile_factor__________________________________________________ (alphan)______________________ 1.0000E+00 + Plasma_profile_model____________________________________________________ (ipedestal)___________________ 1 + Density_pedestal_r/a_location___________________________________________ (rhopedn)_____________________ 9.4000E-01 + Electron_density_pedestal_height_(/m3)__________________________________ (neped)_______________________ 6.3278E+19 OP + Electron_density_at_pedestal_/_nGW______________________________________ (fgwped_out)__________________ 8.5000E-01 + Temperature_pedestal_r/a_location_______________________________________ (rhopedt)_____________________ 9.4000E-01 + Pedestal_scaling_switch_________________________________________________ (ieped)_______________________ 0 + Electron_temp._pedestal_height_(keV)____________________________________ (teped)_______________________ 5.5000E+00 + Electron_temp._at_separatrix_(keV)______________________________________ (tesep)_______________________ 1.0000E-01 + Electron_density_at_separatrix_(/m3)____________________________________ (nesep)_______________________ 3.7223E+19 + Electron_density_at_separatrix_/_nGW____________________________________ (fgwsep_out)__________________ 5.0000E-01 + Temperature_profile_index_______________________________________________ (alphat)______________________ 1.4500E+00 + Temperature_profile_index_beta__________________________________________ (tbeta)_______________________ 2.0000E+00 + Old_ASDEX_model_________________________________________________________ (dlimit(1))___________________ 5.2797E+19 OP + Borrass_ITER_model_I____________________________________________________ (dlimit(2))___________________ 1.0969E+20 OP + Borrass_ITER_model_II___________________________________________________ (dlimit(3))___________________ 4.3575E+19 OP + JET_edge_radiation_model________________________________________________ (dlimit(4))___________________ 3.0227E+21 OP + JET_simplified_model____________________________________________________ (dlimit(5))___________________ 4.3397E+20 OP + Hugill-Murakami_Mq_model________________________________________________ (dlimit(6))___________________ 6.6609E+19 OP + Greenwald_model_________________________________________________________ (dlimit(7))___________________ 7.4445E+19 OP + Deuterium_fuel_fraction_________________________________________________ (fdeut)_______________________ 5.0000E-01 + Tritium_fuel_fraction___________________________________________________ (ftrit)_______________________ 5.0000E-01 + Total_fusion_power_(MW)_________________________________________________ (powfmw)______________________ 1.6202E+03 OP + _=____D-T_fusion_power_(MW)_____________________________________________ (pdt)_________________________ 1.6182E+03 OP + __+___D-D_fusion_power_(MW)_____________________________________________ (pdd)_________________________ 1.9494E+00 OP + __+_D-He3_fusion_power_(MW)_____________________________________________ (pdhe3)_______________________ 0.0000E+00 OP + Alpha_power:_total_(MW)_________________________________________________ (palpmw)______________________ 3.2365E+02 OP + Alpha_power:_beam-plasma_(MW)___________________________________________ (palpnb)______________________ 0.0000E+00 OP + Neutron_power_(MW)______________________________________________________ (pneutmw)_____________________ 1.2953E+03 OP + Charged_particle_power_(excluding_alphas)_(MW)__________________________ (pchargemw)___________________ 1.2659E+00 OP + Total_power_deposited_in_plasma_(MW)____________________________________ (tot_power_plasma)____________ 3.8950E+02 OP + Bremsstrahlung_radiation_power_(MW)_____________________________________ (pbrempv*vol)_________________ 6.5195E+01 OP + Line_radiation_power_(MW)_______________________________________________ (plinepv*vol)_________________ 1.4609E+02 OP + Synchrotron_radiation_power_(MW)________________________________________ (psyncpv*vol)_________________ 1.5187E+01 OP + Synchrotron_wall_reflectivity_factor____________________________________ (ssync)_______________________ 6.0000E-01 + Normalised_minor_radius_defining_'core'_________________________________ (coreradius)__________________ 7.5000E-01 + Fraction_of_core_radiation_subtracted_from_P_L__________________________ (coreradiationfraction)_______ 6.0000E-01 + Radiation_power_from_inner_zone_(MW)____________________________________ (pinnerzoneradmw)_____________ 9.1650E+01 OP + Radiation_power_from_outer_zone_(MW)____________________________________ (pouterzoneradmw)_____________ 1.3482E+02 OP + Total_radiation_power_from_inside_LCFS_(MW)_____________________________ (pradmw)______________________ 2.2647E+02 OP + LCFS_radiation_fraction_=_total_radiation_in_LCFS_/_total_power_deposite (rad_fraction_LCFS)___________ 5.8144E-01 OP + Nominal_mean_radiation_load_on_inside_surface_of_reactor_(MW/m2)________ (photon_wall)_________________ 1.7749E-01 OP + Peaking_factor_for_radiation_wall_load__________________________________ (peakfactrad)_________________ 3.3300E+00 IP + Maximum_permitted_radiation_wall_load_(MW/m^2)__________________________ (maxradwallload)______________ 1.0000E+00 IP + Peak_radiation_wall_load_(MW/m^2)_______________________________________ (peakradwallload)_____________ 5.9106E-01 OP + Fast_alpha_particle_power_incident_on_the_first_wall_(MW)_______________ (palpfwmw)____________________ 1.6182E+01 OP + Nominal_mean_neutron_load_on_inside_surface_of_reactor_(MW/m2)__________ (wallmw)______________________ 1.0152E+00 OP + Power_incident_on_the_divertor_targets_(MW)_____________________________ (ptarmw)______________________ 3.2606E+01 OP + Fraction_of_power_to_the_lower_divertor_________________________________ (ftar)________________________ 1.0000E+00 IP + Outboard_side_heat_flux_decay_length_(m)________________________________ (lambdaio)____________________ 1.5700E-03 OP + Fraction_of_power_on_the_inner_targets__________________________________ (fio)_________________________ 4.1000E-01 OP + Fraction_of_power_incident_on_the_lower_inner_target____________________ (fLI)_________________________ 4.1000E-01 OP + Fraction_of_power_incident_on_the_lower_outer_target____________________ (fLO)_________________________ 5.9000E-01 OP + Power_incident_on_the_lower_inner_target_(MW)___________________________ (pLImw)_______________________ 1.3368E+01 OP + Power_incident_on_the_lower_outer_target_(MW)___________________________ (pLOmw)_______________________ 1.9237E+01 OP + Ohmic_heating_power_(MW)________________________________________________ (pohmmw)______________________ 6.2284E-01 OP + Fraction_of_alpha_power_deposited_in_plasma_____________________________ (falpha)______________________ 9.5000E-01 + Fraction_of_alpha_power_to_electrons____________________________________ (falpe)_______________________ 7.1828E-01 + Fraction_of_alpha_power_to_ions_________________________________________ (falpi)_______________________ 2.8172E-01 + Ion_transport_(MW)______________________________________________________ (ptrimw)______________________ 1.4013E+02 OP + Electron_transport_(MW)_________________________________________________ (ptremw)______________________ 1.5772E+02 OP + Injection_power_to_ions_(MW)____________________________________________ (pinjimw)_____________________ 0.0000E+00 OP + Injection_power_to_electrons_(MW)_______________________________________ (pinjemw)_____________________ 8.0143E+01 OP + Ignited_plasma_switch_(0=not_ignited,_1=ignited)________________________ (ignite)______________________ 0 + Power_into_divertor_zone_via_charged_particles_(MW)_____________________ (pdivt)_______________________ 1.6303E+02 OP + Psep_/_R_ratio_(MW/m)___________________________________________________ (pdivt/rmajor)________________ 2.0378E+01 OP + Psep_Bt_/_qAR_ratio_(MWT/m)_____________________________________________ (pdivtbt/qar)_________________ 1.0000E+01 OP + ITER_1996_scaling:_nominal_(MW)_________________________________________ (pthrmw(1))___________________ 1.2978E+02 OP + ITER_1996_scaling:_upper_bound_(MW)_____________________________________ (pthrmw(2))___________________ 2.8603E+02 OP + ITER_1996_scaling:_lower_bound_(MW)_____________________________________ (pthrmw(3))___________________ 5.8098E+01 OP + ITER_1997_scaling_(1)_(MW)______________________________________________ (pthrmw(4))___________________ 2.1452E+02 OP + ITER_1997_scaling_(2)_(MW)______________________________________________ (pthrmw(5))___________________ 1.7206E+02 OP + Martin_2008_scaling:_nominal_(MW)_______________________________________ (pthrmw(6))___________________ 9.7416E+01 OP + Martin_2008_scaling:_95%_upper_bound_(MW)_______________________________ (pthrmw(7))___________________ 1.2769E+02 OP + Martin_2008_scaling:_95%_lower_bound_(MW)_______________________________ (pthrmw(8))___________________ 6.7143E+01 OP + Snipes_2000_scaling:_nominal_(MW)_______________________________________ (pthrmw(9))___________________ 6.7785E+01 OP + Snipes_2000_scaling:_upper_bound_(MW)___________________________________ (pthrmw(10))__________________ 9.9437E+01 OP + Snipes_2000_scaling:_lower_bound_(MW)___________________________________ (pthrmw(11))__________________ 4.5839E+01 OP + Snipes_2000_scaling_(closed_divertor):_nominal_(MW)_____________________ (pthrmw(12))__________________ 3.1010E+01 OP + Snipes_2000_scaling_(closed_divertor):_upper_bound_(MW)_________________ (pthrmw(13))__________________ 4.3148E+01 OP + Snipes_2000_scaling_(closed_divertor):_lower_bound_(MW)_________________ (pthrmw(14))__________________ 2.2130E+01 OP + Hubbard_2012_L-I_threshold_-_nominal_(MW)_______________________________ (pthrmw(15))__________________ 2.7549E+01 OP + Hubbard_2012_L-I_threshold_-_lower_bound_(MW)___________________________ (pthrmw(16))__________________ 1.4319E+01 OP + Hubbard_2012_L-I_threshold_-_upper_bound_(MW)___________________________ (pthrmw(17))__________________ 5.3005E+01 OP + Hubbard_2017_L-I_threshold______________________________________________ (pthrmw(18))__________________ 2.6202E+02 OP + Martin_2008_aspect_ratio_corrected_scaling:_nominal_(MW)________________ (pthrmw(19))__________________ 9.7416E+01 OP + Martin_2008_aspect_ratio_corrected_scaling:_95%_upper_bound_(MW)________ (pthrmw(20))__________________ 1.2769E+02 OP + Martin_2008_aspect_ratio_corrected_scaling:_95%_lower_bound_(MW)________ (pthrmw(21))__________________ 6.7143E+01 OP + L-H_threshold_power_(enforced)_(MW)_____________________________________ (boundl(103)*plhthresh)_______ 9.7416E+01 OP + L-H_threshold_power_(MW)________________________________________________ (plhthresh)___________________ 9.7416E+01 OP + Confinement_H_factor____________________________________________________ (hfact)_______________________ 1.1886E+00 ITV + Global_thermal_energy_confinement_time_(s)______________________________ (taueff)______________________ 3.2037E+00 + Ion_energy_confinement_time_(s)_________________________________________ (tauei)_______________________ 3.2037E+00 + Electron_energy_confinement_time_(s)____________________________________ (tauee)_______________________ 3.2037E+00 + n.tau_=_Volume-average_electron_density_x_Energy_confinement_time_(s/m3) (dntau)_______________________ 2.5843E+20 OP + Triple_product__(keV_s/m3)______________________________________________ (dntau*te)____________________ 3.2275E+21 OP + Transport_loss_power_assumed_in_scaling_law_(MW)________________________ (powerht)_____________________ 2.9785E+02 OP + Switch_for_radiation_loss_term_usage_in_power_balance___________________ (iradloss)____________________ 1 + Radiation_power_subtracted_from_plasma_power_balance_(MW)_______________ ______________________________ 9.1650E+01 OP + Alpha_particle_confinement_time_(s)_____________________________________ (taup)________________________ 2.2270E+01 + Alpha_particle/energy_confinement_time_ratio____________________________ (taup/taueff)_________________ 6.9512E+00 + Lower_limit_on_taup/taueff______________________________________________ (taulimit)____________________ 5.0000E+00 + Total_energy_confinement_time_including_radiation_loss_(s)______________ (total_energy_conf_time)______ 2.8018E+00 + Normalized_plasma_pressure_beta_as_defined_by_McDonald_et_al____________ (beta_mcdonald)_______________ 3.4553E-02 OP + Normalized_ion_Larmor_radius____________________________________________ (rho_star)____________________ 1.9603E-03 OP + Normalized_collisionality_______________________________________________ (nu_star)_____________________ 3.7266E-03 OP + Volume_measure_of_elongation____________________________________________ (kappaa_IPB)__________________ 1.6815E+00 OP + Total_volt-second_requirement_(Wb)______________________________________ (vsstt)_______________________ 5.5616E+02 OP + Inductive_volt-seconds_(Wb)_____________________________________________ (vsind)_______________________ 2.3585E+02 OP + Ejima_coefficient_______________________________________________________ (gamma)_______________________ 3.0000E-01 + Start-up_resistive_(Wb)_________________________________________________ (vsres)_______________________ 5.0159E+01 OP + Flat-top_resistive_(Wb)_________________________________________________ (vsbrn)_______________________ 2.7015E+02 OP + bootstrap_current_fraction_multiplier___________________________________ (cboot)_______________________ 1.0000E+00 + Bootstrap_fraction_(ITER_1989)__________________________________________ (bscf_iter89)_________________ 3.7098E-01 + Bootstrap_fraction_(Sauter_et_al)_______________________________________ (bscf_sauter)_________________ 4.1920E-01 + Bootstrap_fraction_(Nevins_et_al)_______________________________________ (bscf_nevins)_________________ 3.5042E-01 + Bootstrap_fraction_(Wilson)_____________________________________________ (bscf_wilson)_________________ 4.3349E-01 + Diamagnetic_fraction_(Hender)___________________________________________ (diacf_hender)________________ 1.2017E-02 + Diamagnetic_fraction_(SCENE)____________________________________________ (diacf_scene)_________________ 1.1139E-02 + Pfirsch-Schlueter_fraction_(SCENE)______________________________________ (pscf_scene)__________________ -3.0283E-03 + Bootstrap_fraction_(enforced)___________________________________________ (bootipf.)____________________ 4.1920E-01 + Diamagnetic_fraction_(enforced)_________________________________________ (diaipf.)_____________________ 0.0000E+00 + Pfirsch-Schlueter_fraction_(enforced)___________________________________ (psipf.)______________________ 0.0000E+00 + Loop_voltage_during_burn_(V)____________________________________________ (vburn)_______________________ 3.7450E-02 OP + Plasma_resistance_(ohm)_________________________________________________ (rplas)_______________________ 3.9755E-09 OP + Resistive_diffusion_time_(s)____________________________________________ (res_time)____________________ 3.0619E+03 OP + Plasma_inductance_(H)___________________________________________________ (rlp)_________________________ 1.4181E-05 OP + Coefficient_for_sawtooth_effects_on_burn_V-s_requirement________________ (csawth)______________________ 1.0000E+00 + Ratio_of_He_and_pellet_particle_confinement_times_______________________ (tauratio)____________________ 1.0000E+00 + Fuelling_rate_(nucleus-pairs/s)_________________________________________ (qfuel)_______________________ 3.3420E+21 OP + Fuel_burn-up_rate_(reactions/s)_________________________________________ (rndfuel)_____________________ 5.7755E+20 OP + Burn-up_fraction________________________________________________________ (burnup)______________________ 1.7282E-01 + # Energy confinement times, and required H-factors : # + # Current Drive System # + Current_drive_efficiency_model__________________________________________ (iefrf)_______________________ 10 + Secondary_current_drive_efficiency_model________________________________ (iefrffix)____________________ 0 + Ratio_of_power_for_flat-top_to_start-up_(MW)____________________________ (startupratio)________________ 1.0000E+00 + Auxiliary_power_used_for_plasma_heating_only_(MW)_______________________ (pheat)_______________________ 7.5000E+01 + Power_injected_for_current_drive_(MW)___________________________________ (pcurrentdrivemw)_____________ 5.1429E+00 + Maximum_Allowed_Bootstrap_current_fraction______________________________ (bscfmax)_____________________ 9.5000E-01 + Fusion_gain_factor_Q____________________________________________________ (bigq)________________________ 2.0060E+01 OP + Auxiliary_current_drive_(A)_____________________________________________ (auxiliary_cd)________________ 2.3908E+05 OP + Current_drive_efficiency_(A/W)__________________________________________ (effcd)_______________________ 4.6488E-02 OP + Normalised_current_drive_efficiency,_gamma_(10^20_A/W-m2)_______________ (gamcd)_______________________ 3.0000E-01 OP + Wall_plug_to_injector_efficiency________________________________________ (etacd)_______________________ 5.0000E-01 + ECRH_plasma_heating_efficiency__________________________________________ (gamma_ecrh)__________________ 3.0000E-01 + Bootstrap_fraction______________________________________________________ (bootipf)_____________________ 4.1920E-01 + Diamagnetic_fraction____________________________________________________ (diaipf)______________________ 0.0000E+00 + Pfirsch-Schlueter_fraction______________________________________________ (psipf)_______________________ 0.0000E+00 + Auxiliary_current_drive_fraction________________________________________ (faccd)_______________________ 1.4376E-02 + Inductive_fraction______________________________________________________ (facoh)_______________________ 5.6642E-01 + Total___________________________________________________________________ (plasipf+faccd+facoh)_________ 1.0000E+00 + Fraction_of_the_plasma_current_produced_by_non-inductive_means__________ (fvsbrnni)____________________ 4.3358E-01 ITV + Electron_cyclotron_injected_power_(MW)__________________________________ (echpwr)______________________ 8.0143E+01 OP + Maximum_allowable_ECRH_power_(MW)_______________________________________ (pinjalw)_____________________ 2.0000E+02 + ECH_wall_plug_efficiency________________________________________________ (etaech)______________________ 5.0000E-01 + ECH_wall_plug_power_(MW)________________________________________________ (echwpow)_____________________ 1.6029E+02 OP + Total_V-s_capability_of_Central_Solenoid/PF_coils_(Wb)__________________ (abs(vstot))__________________ 5.7728E+02 + Required_volt-seconds_during_start-up_(Wb)______________________________ (vssoft)______________________ 2.8601E+02 + Available_volt-seconds_during_burn_(Wb)_________________________________ (vsmax)_______________________ 2.7014E+02 + # Times # + Initial_charge_time_for_CS_from_zero_current_(s)________________________ (tramp)_______________________ 5.0000E+02 + Plasma_current_ramp-up_time_(s)_________________________________________ (tohs)________________________ 1.6631E+02 + Heating_time_(s)________________________________________________________ (theat)_______________________ 1.0000E+01 + Burn_time_(s)___________________________________________________________ (tburn)_______________________ 7.2035E+03 OP + Reset_time_to_zero_current_for_CS_(s)___________________________________ (tqnch)_______________________ 1.6631E+02 + Time_between_pulses_(s)_________________________________________________ (tdwell)______________________ 1.8000E+03 + Total_plant_cycle_time_(s)______________________________________________ (tcycle)______________________ 9.8463E+03 OP + # Radial Build # + TF_coil_radial_placement_switch_________________________________________ (tf_in_cs)____________________ 0 + TF_coil_radial_placement_switch_________________________________________ (tf_in_cs)____________________ 0 + Machine_bore_(m)________________________________________________________ (bore)________________________ 1.9854E+00 ITV + CS_radial_thickness_(m)_________________________________________________ (ohcth)_______________________ 5.7587E-01 ITV + CS_precompression_(m)___________________________________________________ (precomp)_____________________ 6.8064E-02 + CS_precompresion_to_TF_coil_radial_gap_(m)______________________________ (gapoh)_______________________ 8.0000E-02 + TF_coil_inboard_leg_(m)_________________________________________________ (tfcth)_______________________ 9.1597E-01 ITV + TF_coil_inboard_leg_insulation_gap_(m)__________________________________ (tftsgap)_____________________ 5.0000E-02 + Thermal_shield,_inboard_(m)_____________________________________________ (thshield_ib)_________________ 5.0000E-02 + thermal_shield_to_vessel_radial_gap_(m)_________________________________ (gapds)_______________________ 2.0000E-02 + Inboard_vacuum_vessel_radial_thickness_(m)______________________________ (d_vv_in)_____________________ 3.0000E-01 + Inner_radiation_shield_radial_thickness_(m)_____________________________ (shldith)_____________________ 3.0000E-01 + Gap_(m)_________________________________________________________________ (vvblgap)_____________________ 2.0000E-02 + Inboard_blanket_radial_thickness_(m)____________________________________ (blnkith)_____________________ 7.0000E-01 + Inboard_first_wall_radial_thickness_(m)_________________________________ (fwith)_______________________ 1.8000E-02 + Inboard_scrape-off_radial_thickness_(m)_________________________________ (scrapli)_____________________ 2.5000E-01 + Outboard_scrape-off_radial_thickness_(m)________________________________ (scraplo)_____________________ 2.5000E-01 + Outboard_first_wall_radial_thickness_(m)________________________________ (fwoth)_______________________ 1.8000E-02 + Outboard_blanket_radial_thickness_(m)___________________________________ (blnkoth)_____________________ 1.0000E+00 + Outer_radiation_shield_radial_thickness_(m)_____________________________ (shldoth)_____________________ 8.0000E-01 + Outboard_vacuum_vessel_radial_thickness_(m)_____________________________ (d_vv_out)____________________ 3.0000E-01 + Vessel_to_TF_radial_gap_(m)_____________________________________________ (gapsto)______________________ 1.3720E+00 + Thermal_shield,_outboard_(m)____________________________________________ (thshield_ob)_________________ 5.0000E-02 + Gap_(m)_________________________________________________________________ (tftsgap)_____________________ 5.0000E-02 + TF_coil_outboard_leg_radial_thickness_(m)_______________________________ (tfthko)______________________ 9.1597E-01 + # Vertical Build # + Divertor_null_switch____________________________________________________ (i_single_null)_______________ 1 + Vessel_-_TF_coil_vertical_gap_(m)_______________________________________ (vgap2)_______________________ 1.6300E-01 + Topside_vacuum_vessel_radial_thickness_(m)______________________________ (d_vv_top)____________________ 3.0000E-01 + Top_radiation_shield_thickness_(m)______________________________________ (shldtth)_____________________ 6.0000E-01 + Top_blanket_vertical_thickness_(m)______________________________________ (blnktth)_____________________ 8.5000E-01 + Top_first_wall_vertical_thickness_(m)___________________________________ (fwtth)_______________________ 1.8000E-02 + Top_scrape-off_vertical_thickness_(m)___________________________________ (vgaptop)_____________________ 6.0000E-01 + Plasma_half-height_(m)__________________________________________________ (rminor*kappa)________________ 4.9333E+00 + Bottom_scrape-off_vertical_thickness_(m)________________________________ (vgap)________________________ 2.0019E+00 + Divertor_structure_vertical_thickness_(m)_______________________________ (divfix)______________________ 6.2000E-01 + Bottom_radiation_shield_thickness_(m)___________________________________ (shldlth)_____________________ 7.0000E-01 + Underside_vacuum_vessel_radial_thickness_(m)____________________________ (d_vv_bot)____________________ 3.0000E-01 + External_cryostat_thickness_(m)_________________________________________ (ddwex)_______________________ 1.5000E-01 + Ratio_of_Central_solenoid_height_to_TF_coil_internal_height_____________ (ohhghf)______________________ 9.0000E-01 + Width_of_neutral_beam_duct_where_it_passes_between_the_TF_coils_(m)_____ (beamwd)______________________ 5.8000E-01 + # Divertor build and plasma position # + Plasma_top_position,_radial_(m)_________________________________________ (ptop_radial)_________________ 6.6667E+00 + Plasma_top_position,_vertical_(m)_______________________________________ (ptop_vertical)_______________ 4.9333E+00 + Plasma_geometric_centre,_radial_(m)_____________________________________ (physics_variables.rmajor.)___ 8.0000E+00 + Plasma_geometric_centre,_vertical_(m)___________________________________ (0.0)_________________________ 0.0000E+00 + Plasma_lower_physics_variables.triangularity____________________________ (tril)________________________ 5.0000E-01 + Plasma_elongation_______________________________________________________ (physics_variables.kappa.)____ 1.8500E+00 + TF_coil_vertical_offset_(m)_____________________________________________ (tfoffset)____________________ -6.1694E-01 + Plasma_outer_arc_radius_of_curvature_(m)________________________________ (rco)_________________________ 5.0422E+00 + Plasma_inner_arc_radius_of_curvature_(m)________________________________ (rci)_________________________ 9.7933E+00 + Plasma_lower_X-pt,_radial_(m)___________________________________________ (rxpt)________________________ 6.6667E+00 + Plasma_lower_X-pt,_vertical_(m)_________________________________________ (zxpt)________________________ -4.9333E+00 + Poloidal_plane_angle_between_vertical_and_inner_leg_(rad)_______________ (thetai)______________________ 2.0820E-01 + Poloidal_plane_angle_between_vertical_and_outer_leg_(rad)_______________ (thetao)______________________ 1.0429E+00 + Poloidal_plane_angle_between_inner_leg_and_plate_(rad)__________________ (betai)_______________________ 1.0000E+00 + Poloidal_plane_angle_between_outer_leg_and_plate_(rad)__________________ (betao)_______________________ 1.0000E+00 + Inner_divertor_leg_poloidal_length_(m)__________________________________ (plsepi)______________________ 1.0000E+00 + Outer_divertor_leg_poloidal_length_(m)__________________________________ (plsepo)______________________ 1.5000E+00 + Inner_divertor_plate_length_(m)_________________________________________ (plleni)______________________ 1.0000E+00 + Outer_divertor_plate_length_(m)_________________________________________ (plleno)______________________ 1.0000E+00 + Inner_strike_point,_radial_(m)__________________________________________ (rspi)________________________ 5.6883E+00 + Inner_strike_point,_vertical_(m)________________________________________ (zspi)________________________ -5.1400E+00 + Inner_plate_top,_radial_(m)_____________________________________________ (rplti)_______________________ 5.8656E+00 + Inner_plate_top,_vertical_(m)___________________________________________ (zplti)_______________________ -4.6725E+00 + Inner_plate_bottom,_radial_(m)__________________________________________ (rplbi)_______________________ 5.5109E+00 + Inner_plate_bottom,_vertical_(m)________________________________________ (zplbi)_______________________ -5.6075E+00 + Outer_strike_point,_radial_(m)__________________________________________ (rspo)________________________ 7.4223E+00 + Outer_strike_point,_vertical_(m)________________________________________ (zspo)________________________ -6.2291E+00 + Outer_plate_top,_radial_(m)_____________________________________________ (rplto)_______________________ 7.6496E+00 + Outer_plate_top,_vertical_(m)___________________________________________ (zplto)_______________________ -5.7838E+00 + Outer_plate_bottom,_radial_(m)__________________________________________ (rplbo)_______________________ 7.1949E+00 + Outer_plate_bottom,_vertical_(m)________________________________________ (zplbo)_______________________ -6.6744E+00 + Calculated_maximum_divertor_height_(m)__________________________________ (divht)_______________________ 2.0019E+00 + # TF coils # + Allowable_maximum_shear_stress_in_TF_coil_case_(Tresca_criterion)_(Pa)__ (sig_tf_case_max)_____________ 7.5000E+08 + Allowable_maximum_shear_stress_in_TF_coil_conduit_(Tresca_criterion)_(Pa (sig_tf_wp_max)_______________ 7.5000E+08 + WP_transverse_modulus_(GPa)_____________________________________________ (eyoung_wp_trans*1.0d-9)______ 4.3534E+01 OP + WP_vertical_modulus_(GPa)_______________________________________________ (eyoung_wp_axial*1.0d-9)______ 1.1510E+02 OP + WP_transverse_Poissons_ratio____________________________________________ (poisson_wp_trans)____________ 3.0390E-01 OP + WP_vertical-transverse_Pois._rat._______________________________________ (poisson_wp_axial)____________ 3.1568E-01 OP + Radial____stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_r_max(1))_____________ 4.8849E-08 + toroidal__stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_t_max(1))_____________ -4.8724E+08 + Vertical__stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_z_max(1))_____________ 2.6028E+08 + Von-Mises_stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_vmises_max(1))________ 6.5725E+08 + Maximum_shear_stress_for_the_Tresca_yield_criterion_1_(Pa)______________ (sig_tf_tresca_max(1))________ 7.4752E+08 + Radial____stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_r_max(2))_____________ -1.5411E+08 + toroidal__stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_t_max(2))_____________ -3.7861E+08 + Vertical__stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_z_max(2))_____________ 2.6028E+08 + Von-Mises_stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_vmises_max(2))________ 5.5645E+08 + Maximum_shear_stress_for_the_Tresca_yield_criterion_2_(Pa)______________ (sig_tf_tresca_max(2))________ 6.3889E+08 + Radial____stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_r_max(3))_____________ 6.1398E+06 + toroidal__stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_t_max(3))_____________ -3.6314E+08 + Vertical__stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_z_max(3))_____________ 1.4510E+08 + Von-Mises_stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_vmises_max(3))________ 4.5345E+08 + Maximum_shear_stress_for_the_Tresca_yield_criterion_3_(Pa)______________ (sig_tf_tresca_max(3))________ 5.0824E+08 + Maximum_radial_deflection_at_midplane_(m)_______________________________ (deflect)_____________________ -6.2714E-03 OP + Vertical_strain_on_casing_______________________________________________ (casestr)_____________________ 1.2697E-03 OP + Radial_strain_on_insulator______________________________________________ (insstrain)___________________ -7.6923E-03 OP + Conductor_technology____________________________________________________ (i_tf_sup)____________________ 1 + Superconductor_material_________________________________________________ (i_tf_sc_mat)_________________ 1 + Presence_of_TF_demountable_joints_______________________________________ (itart)_______________________ 0 + TF_inboard_leg_support_strategy_________________________________________ (i_tf_bucking)________________ 1 + Number_of_TF_coils______________________________________________________ (n_tf)________________________ 16 + Inboard_leg_centre_radius_(m)___________________________________________ (r_tf_inboard_mid)____________ 3.1673E+00 OP + Outboard_leg_centre_radius_(m)__________________________________________ (r_tf_outboard_mid)___________ 1.4985E+01 OP + Total_inboard_leg_radial_thickness_(m)__________________________________ (tfcth)_______________________ 9.1597E-01 ITV + Total_outboard_leg_radial_thickness_(m)_________________________________ (tfthko)______________________ 9.1597E-01 + Outboard_leg_toroidal_thickness_(m)_____________________________________ (tftort)______________________ 1.4145E+00 OP + Maximum_inboard_edge_height_(m)_________________________________________ (hmax)________________________ 8.8182E+00 OP + Mean_coil_circumference_(including_inboard_leg_length)_(m)______________ (tfleng)______________________ 4.7937E+01 OP + Vertical_TF_shape_______________________________________________________ (i_tf_shape)__________________ 1 + TF_coil_arc_point_0_R_(m)_______________________________________________ (xarc(1))_____________________ 3.6253E+00 + TF_coil_arc_point_0_Z_(m)_______________________________________________ (yarc(1))_____________________ 4.5506E+00 + TF_coil_arc_point_1_R_(m)_______________________________________________ (xarc(2))_____________________ 7.4667E+00 + TF_coil_arc_point_1_Z_(m)_______________________________________________ (yarc(2))_____________________ 7.5843E+00 + TF_coil_arc_point_2_R_(m)_______________________________________________ (xarc(3))_____________________ 1.4527E+01 + TF_coil_arc_point_2_Z_(m)_______________________________________________ (yarc(3))_____________________ 0.0000E+00 + TF_coil_arc_point_3_R_(m)_______________________________________________ (xarc(4))_____________________ 7.4667E+00 + TF_coil_arc_point_3_Z_(m)_______________________________________________ (yarc(4))_____________________ -8.8182E+00 + TF_coil_arc_point_4_R_(m)_______________________________________________ (xarc(5))_____________________ 3.6253E+00 + TF_coil_arc_point_4_Z_(m)_______________________________________________ (yarc(5))_____________________ -5.2909E+00 + TF_cross-section_(total)_(m2)___________________________________________ (tfareain)____________________ 1.8229E+01 + Total_steel_cross-section_(m2)__________________________________________ (a_tf_steel*n_tf)_____________ 1.2853E+01 + Total_steel_TF_fraction_________________________________________________ (f_tf_steel)__________________ 7.0508E-01 + Total_Insulation_cross-section_(total)_(m2)_____________________________ (a_tf_ins*n_tf)_______________ 8.4752E-01 + Total_Insulation_fraction_______________________________________________ (f_tf_ins)____________________ 4.6493E-02 + Casing_cross_section_area_(per_leg)_(m2)________________________________ (acasetf)_____________________ 5.6444E-01 + Inboard_leg_case_plasma_side_wall_thickness_(m)_________________________ (casthi)______________________ 6.0000E-02 + Inboard_leg_case_inboard_"nose"_thickness_(m)___________________________ (thkcas)______________________ 2.8216E-01 ITV + Inboard_leg_case_sidewall_thickness_at_its_narrowest_point_(m)__________ (casths)______________________ 5.0000E-02 + External_case_mass_per_coil_(kg)________________________________________ (whtcas)______________________ 5.5456E+05 OP + WP_cross_section_area_with_insulation_and_insertion_(per_coil)_(m2)_____ (awpc)________________________ 5.7486E-01 + WP_cross_section_area_(per_coil)_(m2)___________________________________ (aswp)________________________ 5.1696E-01 + Winding_pack_radial_thickness_(m)_______________________________________ (dr_tf_wp)____________________ 5.0416E-01 ITV + Winding_pack_toroidal_width_1_(m)_______________________________________ (wwp1)________________________ 1.1904E+00 OP + Winding_pack_toroidal_width_2_(m)_______________________________________ (wwp2)________________________ 1.0901E+00 OP + Ground_wall_insulation_thickness_(m)____________________________________ (tinstf)______________________ 8.0000E-03 + Winding_pack_insertion_gap_(m)__________________________________________ (tfinsgap)____________________ 1.0000E-02 + Steel_WP_cross-section_(total)_(m2)_____________________________________ (aswp*n_tf)___________________ 3.8217E+00 + Steel_WP_fraction_______________________________________________________ (aswp/awpc)___________________ 4.1550E-01 + Insulation_WP_fraction__________________________________________________ (aiwp/awpc)___________________ 4.7934E-02 + Cable_WP_fraction_______________________________________________________ ((awpc-aswp-aiwp)/awpc)_______ 5.3656E-01 + Turn_parametrisation____________________________________________________ (i_tf_turns_integer)__________ 0 + Number_of_turns_per_TF_coil_____________________________________________ (n_tf_turn)___________________ 1.4739E+02 OP + Width_of_turn_including_inter-turn_insulation_(m)_______________________ (t_turn_tf)___________________ 5.9223E-02 OP + Width_of_conductor_(square)_(m)_________________________________________ (t_conductor)_________________ 5.7623E-02 OP + Width_of_space_inside_conductor_(m)_____________________________________ (t_cable)_____________________ 4.1604E-02 OP + Steel_conduit_thickness_(m)_____________________________________________ (thwcndut)____________________ 8.0099E-03 ITV + Inter-turn_insulation_thickness_(m)_____________________________________ (thicndut)____________________ 8.0000E-04 + Diameter_of_central_helium_channel_in_cable_____________________________ (dhecoil)_____________________ 1.0000E-02 + internal_area_of_the_cable_space________________________________________ (acstf)_______________________ 1.6999E-03 + Coolant_fraction_in_conductor_excluding_central_channel_________________ (vftf)________________________ 3.0000E-01 + Copper_fraction_of_conductor____________________________________________ (fcutfsu)_____________________ 8.4212E-01 ITV + Superconductor_fraction_of_conductor____________________________________ (1-fcutfsu)___________________ 1.5788E-01 + Check_total_area_fractions_in_winding_pack_=_1__________________________ ______________________________ 1.0000E+00 + minimum_TF_conductor_temperature_margin__(K)____________________________ (tmargmin_tf)_________________ 1.5000E+00 + TF_conductor_temperature_margin_(K)_____________________________________ (tmargtf)_____________________ 1.5049E+00 + Elastic_properties_behavior_____________________________________________ (i_tf_cond_eyoung_axial)______ 0 + Conductor_axial_Youngs_modulus__________________________________________ (eyoung_cond_axial)___________ 0.0000E+00 + Conductor_transverse_Youngs_modulus_____________________________________ (eyoung_cond_trans)___________ 0.0000E+00 + Superconductor_mass_per_coil_(kg)_______________________________________ (whtconsc)____________________ 4.6964E+03 OP + Copper_mass_per_coil_(kg)_______________________________________________ (whtconcu)____________________ 5.8073E+04 OP + Steel_conduit_mass_per_coil_(kg)________________________________________ (whtconsh)____________________ 8.9310E+04 OP + Conduit_insulation_mass_per_coil_(kg)___________________________________ (whtconin)____________________ 2.3777E+03 OP + Total_conduit_mass_per_coil_(kg)________________________________________ (whtcon)______________________ 1.5446E+05 OP + Mass_of_each_TF_coil_(kg)_______________________________________________ (whttf/n_tf)__________________ 7.1402E+05 OP + Total_TF_coil_mass_(kg)_________________________________________________ (whttf)_______________________ 1.1424E+07 OP + Nominal_peak_field_assuming_toroidal_symmetry_(T)_______________________ (bmaxtf)______________________ 1.2178E+01 OP + Total_current_in_all_TF_coils_(MA)______________________________________ (ritfc/1.D6)__________________ 2.1176E+02 OP + TF_coil_current_(summed_over_all_coils)_(A)_____________________________ (ritfc)_______________________ 2.1176E+08 + Actual_peak_field_at_discrete_conductor_(T)_____________________________ (bmaxtfrp)____________________ 1.2636E+01 OP + Winding_pack_current_density_(A/m2)_____________________________________ (jwptf)_______________________ 2.5602E+07 OP + Inboard_leg_mid-plane_conductor_current_density_(A/m2)__________________ (oacdcp)______________________ 1.1617E+07 + Total_stored_energy_in_TF_coils_(GJ)____________________________________ (estotftgj)___________________ 1.2161E+02 OP + Inboard_vertical_tension_per_coil_(N)___________________________________ (vforce)______________________ 2.0908E+08 OP + Outboard_vertical_tension_per_coil_(N)__________________________________ (vforce_outboard)_____________ 2.0908E+08 OP + inboard_vertical_tension_fraction_(-)___________________________________ (f_vforce_inboard)____________ 5.0000E-01 OP + Centring_force_per_coil_(N/m)___________________________________________ (cforce)______________________ 8.0590E+07 OP + Max_allowed_tfcoil_variables.ripple_amplitude_at_plasma_outboard_midplan (ripmax)______________________ 6.0000E-01 + Ripple_amplitude_at_plasma_outboard_midplane_(%)________________________ (ripple)______________________ 6.0000E-01 OP + Actual_quench_time_(or_time_constant)_(s)_______________________________ (tdmptf)______________________ 1.8429E+01 ITV + Vacuum_Vessel_stress_on_quench_(Pa)_____________________________________ (vv_stress_quench)____________ 6.1442E+07 OP + Maximum_allowed_voltage_during_quench_due_to_insulation_(kV)____________ (vdalw)_______________________ 9.5837E+00 ITV + Actual_quench_voltage_(kV)______________________________________________ (vtfskv)______________________ 9.1862E+00 OP + Maximum_allowed_temp_rise_during_a_quench_(K)___________________________ (tmaxpro)_____________________ 1.5000E+02 + # Superconducting TF Coils # + Superconductor_switch___________________________________________________ (isumat)______________________ 1 + Critical_field_at_zero_temperature_and_strain_(T)_______________________ (bc20m)_______________________ 3.2970E+01 + Critical_temperature_at_zero_field_and_strain_(K)_______________________ (tc0m)________________________ 1.6060E+01 + Helium_temperature_at_peak_field_(=_superconductor_temperature)_(K)_____ (thelium)_____________________ 4.7500E+00 + Total_helium_fraction_inside_cable_space________________________________ (fhetot)______________________ 3.4620E-01 OP + Copper_fraction_of_conductor____________________________________________ (fcutfsu)_____________________ 8.4212E-01 ITV + Residual_manufacturing_strain_on_superconductor_________________________ (str_tf_con_res)______________ -5.0000E-03 + Self-consistent_strain_on_superconductor________________________________ (str_wp)______________________ 2.0730E-03 + Critical_current_density_in_superconductor_(A/m2)_______________________ (jcritsc)_____________________ 7.1337E+08 OP + Critical_current_density_in_strand_(A/m2)_______________________________ (jcritstr)____________________ 1.1263E+08 OP + Critical_current_density_in_winding_pack_(A/m2)_________________________ (jwdgcrt)_____________________ 3.5688E+07 OP + Actual_current_density_in_winding_pack_(A/m2)___________________________ (jwdgop)______________________ 2.5602E+07 OP + Minimum_allowed_temperature_margin_in_superconductor_(K)________________ (tmargmin_tf)_________________ 1.5000E+00 + Actual_temperature_margin_in_superconductor_(K)_________________________ (tmarg)_______________________ 1.5049E+00 OP + Critical_current_(A)____________________________________________________ (icrit)_______________________ 1.2517E+05 OP + Actual_current_(A)______________________________________________________ (cpttf)_______________________ 8.9795E+04 ITV + Actual_current_/_critical_current_______________________________________ (iooic)_______________________ 7.1737E-01 OP + # Central Solenoid and PF Coils # + Central_solenoid_superconductor_material________________________________ (isumatoh)____________________ 1 + Maximum_field_at_Beginning_Of_Pulse_(T)_________________________________ (bmaxoh0)_____________________ 1.4050E+01 OP + Critical_superconductor_current_density_at_BOP_(A/m2)___________________ (jscoh_bop)___________________ 3.4918E+08 OP + Critical_strand_current_density_at_BOP_(A/m2)___________________________ (jstrandoh_bop)_______________ 1.0475E+08 OP + Allowable_overall_current_density_at_BOP_(A/m2)_________________________ (rjohc0)______________________ 3.5294E+07 OP + Actual_overall_current_density_at_BOP_(A/m2)____________________________ (cohbop)______________________ 1.9126E+07 OP + Maximum_field_at_End_Of_Flattop_(T)_____________________________________ (bmaxoh)______________________ 1.3920E+01 OP + Critical_superconductor_current_density_at_EOF_(A/m2)___________________ (jscoh_eof)___________________ 3.6097E+08 OP + Critical_strand_current_density_at_EOF_(A/m2)___________________________ (jstrandoh_eof)_______________ 1.0829E+08 OP + Allowable_overall_current_density_at_EOF_(A/m2)_________________________ (rjohc)_______________________ 3.6485E+07 OP + Actual_overall_current_density_at_EOF_(A/m2)____________________________ (coheof)______________________ 2.0264E+07 ITV + CS_inside_radius_(m)____________________________________________________ (bore)________________________ 1.9854E+00 ITV + CS_thickness_(m)________________________________________________________ (ohcth)_______________________ 5.7587E-01 ITV + Gap_between_central_solenoid_and_TF_coil_(m)____________________________ (gapoh)_______________________ 8.0000E-02 + CS_overall_cross-sectional_area_(m2)____________________________________ (areaoh)______________________ 9.1407E+00 OP + CS_conductor+void_cross-sectional_area_(m2)_____________________________ (awpoh)_______________________ 4.3996E+00 OP + ___CS_conductor_cross-sectional_area_(m2)_______________________________ (awpoh*(1-vfohc))_____________ 3.0797E+00 OP + ___CS_void_cross-sectional_area_(m2)____________________________________ (awpoh*vfohc)_________________ 1.3199E+00 OP + CS_steel_cross-sectional_area_(m2)______________________________________ (areaoh-awpoh)________________ 4.7411E+00 OP + CS_steel_area_fraction__________________________________________________ (oh_steel_frac)_______________ 5.1868E-01 ITV + Switch_for_CS_stress_calculation________________________________________ (i_cs_stress)_________________ 0 + Allowable_stress_in_CS_steel_(Pa)_______________________________________ (alstroh)_____________________ 7.5000E+08 + Hoop_stress_in_CS_steel_(Pa)____________________________________________ (sig_hoop)____________________ 6.7569E+08 OP + Axial_stress_in_CS_steel_(Pa)___________________________________________ (sig_axial)___________________ -7.6205E+08 OP + Maximum_shear_stress_in_CS_steel_for_the_Tresca_criterion_(Pa)__________ (s_tresca_oh)_________________ 6.7569E+08 OP + Axial_force_in_CS_(N)___________________________________________________ (axial_force)_________________ -1.6256E+09 OP + Residual_manufacturing_strain_in_CS_superconductor_material_____________ (tfcoil_variables.str_cs_con_r -5.0000E-03 + Copper_fraction_in_strand_______________________________________________ (fcuohsu)_____________________ 7.0000E-01 + Void_(coolant)_fraction_in_conductor____________________________________ (vfohc)_______________________ 3.0000E-01 + Helium_coolant_temperature_(K)__________________________________________ (tftmp)_______________________ 4.7500E+00 + CS_temperature_margin_(K)_______________________________________________ (tmargoh)_____________________ 1.5052E+00 OP + Minimum_permitted_temperature_margin_(K)________________________________ (tmargmin_cs)_________________ 1.5000E+00 + Residual_hoop_stress_in_CS_Steel_(Pa)___________________________________ (residual_sig_hoop)___________ 2.4000E+08 + Minimum_burn_time_(s)___________________________________________________ (tbrnmn)______________________ 7.2000E+03 + Initial_vertical_crack_size_(m)_________________________________________ (t_crack_vertical)____________ 8.9000E-04 + Initial_radial_crack_size_(m)___________________________________________ (t_crack_radial)______________ 2.6700E-03 + CS_turn_area_(m)________________________________________________________ (a_oh_turn)___________________ 1.9739E-03 + CS_turn_length_(m)______________________________________________________ (l_cond_cst)__________________ 7.6953E-02 + CS_turn_internal_cable_space_radius_(m)_________________________________ (r_in_cst)____________________ 7.4740E-03 + CS_turn_width_(m)_______________________________________________________ (d_cond_cst)__________________ 2.5651E-02 + CS_structural_vertical_thickness_(m)____________________________________ (t_structural_vertical)_______ 5.3514E-03 + CS_structural_radial_thickness_(m)______________________________________ (t_structural_radial)_________ 5.3514E-03 + Allowable_number_of_cycles_till_CS_fracture_____________________________ (n_cycle)_____________________ 1.3378E+02 OP + Minimum_number_of_cycles_required_till_CS_fracture______________________ (n_cycle_min)_________________ 2.0000E+04 OP + PF_coil_superconductor_material_________________________________________ (isumatpf)____________________ 3 + Copper_fraction_in_conductor____________________________________________ (fcupfsu)_____________________ 6.9000E-01 + Maximum_permissible_tensile_stress_(MPa)________________________________ (sigpfcalw)___________________ 5.0000E+02 + JxB_hoop_force_fraction_supported_by_case_______________________________ (sigpfcf)_____________________ 6.6600E-01 + PF_coil_0_radius_(m)____________________________________________________ (rpf[0]_______________________ 5.5667E+00 + PF_coil_0_vertical_position_(m)_________________________________________ (zpf[0])______________________ 9.3603E+00 + PF_coil_0_radial_thickness_(m)__________________________________________ (pfdr(0))_____________________ 1.2727E+00 + PF_coil_0_vertical_thickness_(m)________________________________________ (pfdz(0))_____________________ 1.2727E+00 + PF_coil_0_turns_________________________________________________________ (turns[0])____________________ 4.4541E+02 + PF_coil_0_current_(MA)__________________________________________________ (ric[0])______________________ 1.7816E+01 + PF_coil_0_field_(T)_____________________________________________________ (bpf[0])______________________ 6.2280E+00 + PF_coil_1_radius_(m)____________________________________________________ (rpf[1]_______________________ 5.5667E+00 + PF_coil_1_vertical_position_(m)_________________________________________ (zpf[1])______________________ -1.0594E+01 + PF_coil_1_radial_thickness_(m)__________________________________________ (pfdr(1))_____________________ 1.3651E+00 + PF_coil_1_vertical_thickness_(m)________________________________________ (pfdz(1))_____________________ -1.3651E+00 + PF_coil_1_turns_________________________________________________________ (turns[1])____________________ 5.1248E+02 + PF_coil_1_current_(MA)__________________________________________________ (ric[1])______________________ 2.0499E+01 + PF_coil_1_field_(T)_____________________________________________________ (bpf[1])______________________ 6.6990E+00 + PF_coil_2_radius_(m)____________________________________________________ (rpf[2]_______________________ 1.6731E+01 + PF_coil_2_vertical_position_(m)_________________________________________ (zpf[2])______________________ 2.6667E+00 + PF_coil_2_radial_thickness_(m)__________________________________________ (pfdr(2))_____________________ 1.1332E+00 + PF_coil_2_vertical_thickness_(m)________________________________________ (pfdz(2))_____________________ 1.1332E+00 + PF_coil_2_turns_________________________________________________________ (turns[2])____________________ 1.9262E+02 + PF_coil_2_current_(MA)__________________________________________________ (ric[2])______________________ -7.7049E+00 + PF_coil_2_field_(T)_____________________________________________________ (bpf[2])______________________ 2.6389E+00 + PF_coil_3_radius_(m)____________________________________________________ (rpf[3]_______________________ 1.6731E+01 + PF_coil_3_vertical_position_(m)_________________________________________ (zpf[3])______________________ -2.6667E+00 + PF_coil_3_radial_thickness_(m)__________________________________________ (pfdr(3))_____________________ 1.1332E+00 + PF_coil_3_vertical_thickness_(m)________________________________________ (pfdz(3))_____________________ -1.1332E+00 + PF_coil_3_turns_________________________________________________________ (turns[3])____________________ 1.9262E+02 + PF_coil_3_current_(MA)__________________________________________________ (ric[3])______________________ -7.7049E+00 + PF_coil_3_field_(T)_____________________________________________________ (bpf[3])______________________ 2.6389E+00 + PF_coil_4_radius_(m)____________________________________________________ (rpf[4]_______________________ 1.5209E+01 + PF_coil_4_vertical_position_(m)_________________________________________ (zpf[4])______________________ 7.4667E+00 + PF_coil_4_radial_thickness_(m)__________________________________________ (pfdr(4))_____________________ 8.0773E-01 + PF_coil_4_vertical_thickness_(m)________________________________________ (pfdz(4))_____________________ 8.0773E-01 + PF_coil_4_turns_________________________________________________________ (turns[4])____________________ 1.3049E+02 + PF_coil_4_current_(MA)__________________________________________________ (ric[4])______________________ -5.2194E+00 + PF_coil_4_field_(T)_____________________________________________________ (bpf[4])______________________ 2.5737E+00 + PF_coil_5_radius_(m)____________________________________________________ (rpf[5]_______________________ 1.5209E+01 + PF_coil_5_vertical_position_(m)_________________________________________ (zpf[5])______________________ -7.4667E+00 + PF_coil_5_radial_thickness_(m)__________________________________________ (pfdr(5))_____________________ 8.0773E-01 + PF_coil_5_vertical_thickness_(m)________________________________________ (pfdz(5))_____________________ -8.0773E-01 + PF_coil_5_turns_________________________________________________________ (turns[5])____________________ 1.3049E+02 + PF_coil_5_current_(MA)__________________________________________________ (ric[5])______________________ -5.2194E+00 + PF_coil_5_field_(T)_____________________________________________________ (bpf[5])______________________ 2.5737E+00 + Central_solenoid_radius_(m)_____________________________________________ (rpf[nohc-1])_________________ 2.2734E+00 + Central_solenoid_vertical_position_(m)__________________________________ (zpf[nohc-1])_________________ 0.0000E+00 + Central_solenoid_radial_thickness_(m)___________________________________ (ohdr)________________________ 5.7587E-01 + Central_solenoid_vertical_thickness_(m)_________________________________ (ohdz)________________________ 1.5873E+01 + Central_solenoid_turns__________________________________________________ (turns[nohc-1])_______________ 4.6308E+03 + Central_solenoid_current_(MA)___________________________________________ (ric[nohc-1])_________________ -1.8523E+02 + Central_solenoid_field_(T)______________________________________________ (bpf[nohc-1])_________________ 1.4050E+01 + Sum_of_squares_of_residuals_____________________________________________ (ssq0)________________________ 3.5207E-04 OP + Smoothing_parameter_____________________________________________________ (alfapf)______________________ 5.0000E-10 + # Volt Second Consumption # + Total_volt-second_consumption_by_coils_(Wb)_____________________________ (vstot)_______________________ -5.8000E+02 OP + # Waveforms # + Ratio_of_central_solenoid_current_at_beginning_of_Pulse_/_end_of_flat-to (fcohbop)_____________________ 9.4380E-01 ITV + Ratio_of_central_solenoid_current_at_beginning_of_Flat-top_/_end_of_flat (fcohbof)_____________________ -1.4083E-01 OP + # PF Circuit Waveform Data # + Number_of_PF_circuits_including_CS_and_plasma___________________________ (ncirt)_______________________ 8 + PF_Circuit_0_Time_point_0_(A)___________________________________________ (pfc0t0)______________________ 0.0000E+00 + PF_Circuit_0_Time_point_1_(A)___________________________________________ (pfc0t1)______________________ 1.3971E+07 + PF_Circuit_0_Time_point_2_(A)___________________________________________ (pfc0t2)______________________ 1.7816E+07 + PF_Circuit_0_Time_point_3_(A)___________________________________________ (pfc0t3)______________________ 1.7816E+07 + PF_Circuit_0_Time_point_4_(A)___________________________________________ (pfc0t4)______________________ 9.2844E+05 + PF_Circuit_0_Time_point_5_(A)___________________________________________ (pfc0t5)______________________ 0.0000E+00 + PF_Circuit_1_Time_point_0_(A)___________________________________________ (pfc1t0)______________________ 0.0000E+00 + PF_Circuit_1_Time_point_1_(A)___________________________________________ (pfc1t1)______________________ 1.8269E+07 + PF_Circuit_1_Time_point_2_(A)___________________________________________ (pfc1t2)______________________ 2.0499E+07 + PF_Circuit_1_Time_point_3_(A)___________________________________________ (pfc1t3)______________________ 2.0499E+07 + PF_Circuit_1_Time_point_4_(A)___________________________________________ (pfc1t4)______________________ -1.5831E+06 + PF_Circuit_1_Time_point_5_(A)___________________________________________ (pfc1t5)______________________ 0.0000E+00 + PF_Circuit_2_Time_point_0_(A)___________________________________________ (pfc2t0)______________________ -0.0000E+00 + PF_Circuit_2_Time_point_1_(A)___________________________________________ (pfc2t1)______________________ 4.9542E+05 + PF_Circuit_2_Time_point_2_(A)___________________________________________ (pfc2t2)______________________ -7.1060E+06 + PF_Circuit_2_Time_point_3_(A)___________________________________________ (pfc2t3)______________________ -7.1060E+06 + PF_Circuit_2_Time_point_4_(A)___________________________________________ (pfc2t4)______________________ -7.7049E+06 + PF_Circuit_2_Time_point_5_(A)___________________________________________ (pfc2t5)______________________ -0.0000E+00 + PF_Circuit_3_Time_point_0_(A)___________________________________________ (pfc3t0)______________________ -0.0000E+00 + PF_Circuit_3_Time_point_1_(A)___________________________________________ (pfc3t1)______________________ 4.9542E+05 + PF_Circuit_3_Time_point_2_(A)___________________________________________ (pfc3t2)______________________ -7.1060E+06 + PF_Circuit_3_Time_point_3_(A)___________________________________________ (pfc3t3)______________________ -7.1060E+06 + PF_Circuit_3_Time_point_4_(A)___________________________________________ (pfc3t4)______________________ -7.7049E+06 + PF_Circuit_3_Time_point_5_(A)___________________________________________ (pfc3t5)______________________ -0.0000E+00 + PF_Circuit_4_Time_point_0_(A)___________________________________________ (pfc4t0)______________________ -0.0000E+00 + PF_Circuit_4_Time_point_1_(A)___________________________________________ (pfc4t1)______________________ 3.2650E+05 + PF_Circuit_4_Time_point_2_(A)___________________________________________ (pfc4t2)______________________ -4.8247E+06 + PF_Circuit_4_Time_point_3_(A)___________________________________________ (pfc4t3)______________________ -4.8247E+06 + PF_Circuit_4_Time_point_4_(A)___________________________________________ (pfc4t4)______________________ -5.2194E+06 + PF_Circuit_4_Time_point_5_(A)___________________________________________ (pfc4t5)______________________ -0.0000E+00 + PF_Circuit_5_Time_point_0_(A)___________________________________________ (pfc5t0)______________________ -0.0000E+00 + PF_Circuit_5_Time_point_1_(A)___________________________________________ (pfc5t1)______________________ 3.2650E+05 + PF_Circuit_5_Time_point_2_(A)___________________________________________ (pfc5t2)______________________ -4.8247E+06 + PF_Circuit_5_Time_point_3_(A)___________________________________________ (pfc5t3)______________________ -4.8247E+06 + PF_Circuit_5_Time_point_4_(A)___________________________________________ (pfc5t4)______________________ -5.2194E+06 + PF_Circuit_5_Time_point_5_(A)___________________________________________ (pfc5t5)______________________ -0.0000E+00 + CS_Circuit_Time_point_0_(A)_____________________________________________ (cs_t0)_______________________ -0.0000E+00 + CS_Circuit_Time_point_1_(A)_____________________________________________ (cs_t1)_______________________ 1.7482E+08 + CS_Circuit_Time_point_2_(A)_____________________________________________ (cs_t2)_______________________ 2.6086E+07 + CS_Circuit_Time_point_3_(A)_____________________________________________ (cs_t3)_______________________ 2.6086E+07 + CS_Circuit_Time_point_4_(A)_____________________________________________ (cs_t4)_______________________ -1.8523E+08 + CS_Circuit_Time_point_5_(A)_____________________________________________ (cs_t5)_______________________ -0.0000E+00 + Plasma_Time_point_0_(A)_________________________________________________ (plasmat0)____________________ 0.0000E+00 + Plasma_Time_point_1_(A)_________________________________________________ (plasmat1)____________________ 0.0000E+00 + Plasma_Time_point_2_(A)_________________________________________________ (plasmat2)____________________ 1.6631E+07 + Plasma_Time_point_3_(A)_________________________________________________ (plasmat3)____________________ 1.6631E+07 + Plasma_Time_point_4_(A)_________________________________________________ (plasmat4)____________________ 1.6631E+07 + Plasma_Time_point_5_(A)_________________________________________________ (plasmat5)____________________ 0.0000E+00 + # Support Structure # + Outer_PF_coil_fence_mass_(kg)___________________________________________ (fncmass)_____________________ 2.2924E+05 OP + Intercoil_support_structure_mass_(kg)___________________________________ (aintmass)____________________ 4.3045E+06 OP + Mass_of_cooled_components_(kg)__________________________________________ (coldmass)____________________ 3.4369E+07 OP + Gravity_support_structure_mass_(kg)_____________________________________ (clgsmass)____________________ 1.2760E+06 OP + Torus_leg_support_mass_(kg)_____________________________________________ (gsm1)________________________ 8.5820E+04 OP + Ring_beam_mass_(kg)_____________________________________________________ (gsm2)________________________ 4.0088E+05 OP + Ring_legs_mass_(kg)_____________________________________________________ (gsm3)________________________ 6.8283E+05 OP + # PF Coil Inductances # + # Nuclear Heating Magnets Before Renormalisation # + Shield_line_density_(tonne/m2)__________________________________________ (x_shield)____________________ 4.0560E+00 + Blanket_line_density_(tonne/m2)_________________________________________ (x_blanket)___________________ 2.2911E+00 + Unit_nuclear_heating_in_TF_coil_(W/GW)__________________________________ (tfc_nuc_heating)_____________ 1.4866E+04 + Total_nuclear_heating_in_TF_coil_(MW)___________________________________ (ptfnuc.)_____________________ 2.4085E-02 + powfmw__________________________________________________________________ (powfmw.)_____________________ 1.6202E+03 + total_mass_of_the_TF_coils_(kg)_________________________________________ (whttf)_______________________ 1.1424E+07 + # Pumping for primary coolant (helium) # + Pressure_drop_in_FW_and_blanket_coolant_incl._hx_and_pipes_(Pa)_________ (dp_he)_______________________ 5.5000E+05 + Fraction_of_FW_and_blanket_thermal_power_required_for_pumping___________ (fpump)_______________________ 8.9463E-02 OP + Total_power_absorbed_by_FW_&_blanket_(MW)_______________________________ (p_plasma)____________________ 1.6698E+03 OP + Inlet_temperature_of_FW_&_blanket_coolant_pump_(K)______________________ (t_in_compressor)_____________ 5.5703E+02 OP + Coolant_pump_outlet/Inlet_temperature_of_FW_&_blanket_(K)_______________ (t_in_bb)_____________________ 5.7313E+02 + Outlet_temperature_of_FW_&_blanket_(K)__________________________________ (t_out_bb)____________________ 7.7313E+02 + Mechanical_pumping_power_for_FW_and_blanket_cooling_loop_including_heat_ (htpmw_fw_blkt)_______________ 1.6407E+02 OP + Mechanical_pumping_power_for_divertor_(MW)______________________________ (htpmw_div)___________________ 1.6906E+00 OP + Mechanical_pumping_power_for_shield_and_vacuum_vessel_(MW)______________ (htpmw_shld)__________________ 7.0688E-03 OP + # First wall and blanket : CCFE HCPB model # + Titanium_beryllide_fraction_____________________________________________ (fbltibe12)___________________ 3.7500E-01 + Lithium_orthosilicate_fraction__________________________________________ (fblli2sio4)__________________ 3.7500E-01 + Steel_fraction__________________________________________________________ (fblss_ccfe)__________________ 9.7050E-02 + Coolant_fraction________________________________________________________ (vfcblkt)_____________________ 5.2950E-02 + Purge_gas_fraction______________________________________________________ (vfpblkt)_____________________ 1.0000E-01 + First_Wall_Armour_Volume_(m3)___________________________________________ (fw_armour_vol)_______________ 5.8692E+00 + First_Wall_Volume_(m3)__________________________________________________ (volfw)_______________________ 1.9807E+01 + Blanket_Volume_(m3)_____________________________________________________ (volblkt)_____________________ 1.1849E+03 + Shield_Volume_(m3)______________________________________________________ (volshld)_____________________ 7.8520E+02 + Vacuum_vessel_volume_(m3)_______________________________________________ (vdewin)______________________ 1.0178E+03 + First_Wall_Armour_Mass_(kg)_____________________________________________ (fw_armour_mass)______________ 1.1298E+05 OP + First_Wall_Mass,_excluding_armour_(kg)__________________________________ (fwmass)______________________ 1.5449E+05 OP + Blanket_Mass_-_Total(kg)________________________________________________ (whtblkt)_____________________ 2.9676E+06 OP + ____Blanket_Mass_-_TiBe12_(kg)__________________________________________ (whtbltibe12)_________________ 1.0042E+06 OP + ____Blanket_Mass_-_Li4SiO4_(kg)_________________________________________ (whtblli4sio4)________________ 1.0664E+06 OP + ____Blanket_Mass_-_Steel_(kg)___________________________________________ (whtblss)_____________________ 8.9696E+05 OP + Total_mass_of_armour,_first_wall_and_blanket_(kg)_______________________ (armour_fw_bl_mass)___________ 3.2350E+06 OP + Shield_Mass_(kg)________________________________________________________ (whtshld)_____________________ 2.4498E+06 OP + Vacuum_vessel_mass_(kg)_________________________________________________ (vvmass)______________________ 7.9388E+06 OP + Total_nuclear_heating_in_TF+PF_coils_(CS_is_negligible)_(MW)____________ (ptfnuc)______________________ 2.5118E-02 OP + Total_nuclear_heating_in_FW_(MW)________________________________________ (pnucfw)______________________ 1.6315E+02 OP + Total_nuclear_heating_in_the_blanket_(including_emult)_(MW)_____________ (pnucblkt)____________________ 1.2901E+03 OP + Total_nuclear_heating_in_the_shield_(MW)________________________________ (pnucshld)____________________ 1.4138E+00 OP + Total_nuclear_heating_in_the_divertor_(MW)______________________________ (pnucdiv)_____________________ 1.4906E+02 OP + Blanket_exponential_factor______________________________________________ (exp_blanket)_________________ 9.9936E-01 OP + Shield:_first_exponential_______________________________________________ (exp_shield1)_________________ 1.9523E-03 OP + Shield:_second_exponential______________________________________________ (exp_shield2)_________________ 2.5427E-01 OP + Solid_angle_fraction_taken_by_on_divertor_______________________________ (fdiv)________________________ 1.1500E-01 + Switch_for_plant_secondary_cycle________________________________________ (secondary_cycle)_____________ 2 + First_wall_coolant_pressure_(Pa)________________________________________ (fwpressure)__________________ 1.5500E+07 + Blanket_coolant_pressure_(Pa)___________________________________________ (blpressure)__________________ 1.5500E+07 + Allowable_nominal_neutron_fluence_at_first_wall_(MW.year/m2)____________ (abktflnc)____________________ 5.0000E+00 + No_of_inboard_blanket_modules_poloidally________________________________ (nblktmodpi)__________________ 7 + No_of_inboard_blanket_modules_toroidally________________________________ (nblktmodti)__________________ 32 + No_of_outboard_blanket_modules_poloidally_______________________________ (nblktmodpo)__________________ 8 + No_of_outboard_blanket_modules_toroidally_______________________________ (nblktmodto)__________________ 48 + Isentropic_efficiency_of_first_wall_/_blanket_coolant_pumps_____________ (etaiso)______________________ 9.0000E-01 + First_wall_area_(m2)____________________________________________________ (fwarea)______________________ 1.6044E+03 OP + Cryostat_internal_radius_(m)____________________________________________ (rdewex)______________________ 1.7798E+01 OP + Cryostat_internal_half-height_(m)_______________________________________ (zdewex)______________________ 1.5339E+01 OP + Vertical_clearance_from_TF_coil_to_cryostat_(m)_________________________ (clh1)________________________ 5.6044E+00 OP + Divertor_area_(m2)______________________________________________________ (divsur)______________________ 1.4879E+02 OP + Divertor_mass_(kg)______________________________________________________ (divmas)______________________ 3.6453E+04 OP + # Superconducting TF Coil Power Conversion # + TF_coil_current_(kA)____________________________________________________ (itfka)_______________________ 8.9795E+01 OP + Number_of_TF_coils______________________________________________________ (ntfc)________________________ 1.6000E+01 + Voltage_across_a_TF_coil_during_quench_(kV)_____________________________ (vtfskv)______________________ 9.1862E+00 OP + TF_coil_charge_time_(hours)_____________________________________________ (tchghr)______________________ 4.0000E+00 + Total_inductance_of_TF_coils_(H)________________________________________ (ltfth)_______________________ 3.0165E+01 OP + Total_resistance_of_TF_coils_(ohm)______________________________________ (rcoils)______________________ 0.0000E+00 OP + TF_coil_charging_voltage_(V)____________________________________________ (tfcv)________________________ 2.9268E+02 + Number_of_DC_circuit_breakers___________________________________________ (ntfbkr)______________________ 1.6000E+01 + Number_of_dump_resistors________________________________________________ (ndumpr)______________________ 6.4000E+01 + Resistance_per_dump_resistor_(ohm)______________________________________ (r1dump)______________________ 1.0230E-01 OP + Dump_resistor_peak_power_(MW)___________________________________________ (r1ppmw)______________________ 2.0622E+02 OP + Energy_supplied_per_dump_resistor_(MJ)__________________________________ (r1emj)_______________________ 1.9002E+03 OP + TF_coil_L/R_time_constant_(s)___________________________________________ (ttfsec)______________________ 1.8429E+01 OP + Power_supply_voltage_(V)________________________________________________ (tfpsv)_______________________ 3.0731E+02 OP + Power_supply_current_(kA)_______________________________________________ (tfpska)______________________ 9.4285E+01 OP + DC_power_supply_rating_(kW)_____________________________________________ (tfckw)_______________________ 2.8975E+04 OP + AC_power_for_charging_(kW)______________________________________________ (tfackw)______________________ 3.2194E+04 OP + TF_coil_resistive_power_(MW)____________________________________________ (rpower)______________________ 9.3902E+00 OP + TF_coil_inductive_power_(MVA)___________________________________________ (xpower)______________________ 1.6891E+01 OP + Aluminium_bus_current_density_(kA/cm2)__________________________________ (djmka)_______________________ 1.2500E-01 + Aluminium_bus_cross-sectional_area_(cm2)________________________________ (albusa)______________________ 7.1836E+02 OP + Total_length_of_TF_coil_bussing_(m)_____________________________________ (tfbusl)______________________ 3.1931E+03 OP + Aluminium_bus_weight_(tonnes)___________________________________________ (albuswt)_____________________ 6.1932E+02 OP + Total_TF_coil_bus_resistance_(ohm)______________________________________ (rtfbus)______________________ 1.1646E-03 OP + TF_coil_bus_voltage_drop_(V)____________________________________________ (vtfbus)______________________ 1.0457E+02 OP + Dump_resistor_floor_area_(m2)___________________________________________ (drarea)______________________ 4.9234E+03 OP + TF_coil_power_conversion_floor_space_(m2)_______________________________ (tfcfsp)______________________ 1.8228E+03 OP + TF_coil_power_conv._building_volume_(m3)________________________________ (tfcbv)_______________________ 1.0937E+04 OP + TF_coil_AC_inductive_power_demand_(MW)__________________________________ (xpwrmw)______________________ 1.8768E+01 OP + Total_steady_state_AC_power_demand_(MW)_________________________________ (tfacpd)______________________ 1.0434E+01 OP + # PF Coils and Central Solenoid: Power and Energy # + Number_of_PF_coil_circuits______________________________________________ (pfckts)______________________ 1.2000E+01 + Sum_of_PF_power_supply_ratings_(MVA)____________________________________ (spsmva)______________________ 3.0313E+02 OP + Total_PF_coil_circuit_bus_length_(m)____________________________________ (spfbusl)_____________________ 2.4480E+03 OP + Total_PF_coil_bus_resistive_power_(kW)__________________________________ (pfbuspwr)____________________ 9.6485E+02 OP + Total_PF_coil_resistive_power_(kW)______________________________________ (srcktpm)_____________________ 9.6485E+02 OP + Maximum_PF_coil_voltage_(kV)____________________________________________ (vpfskv)______________________ 2.0000E+01 + Efficiency_of_transfer_of_PF_stored_energy_into_or_out_of_storage_______ (etapsu)______________________ 9.0000E-01 + Maximum_stored_energy_in_poloidal_field_(MJ)____________________________ (ensxpfm)_____________________ 2.8804E+04 OP + Peak_absolute_rate_of_change_of_stored_energy_in_poloidal_field_(MW)____ (peakpoloidalpower)___________ 1.7319E+02 OP + # Vacuum System # + First_wall_outgassing_rate_(Pa_m/s)_____________________________________ (rat)_________________________ 1.3000E-08 + Total_outgassing_load_(Pa_m3/s)_________________________________________ (ogas)________________________ 1.6691E-04 OP + Base_pressure_required_(Pa)_____________________________________________ (pbase)_______________________ 5.0000E-04 + Required_N2_pump_speed_(m3/s)___________________________________________ (s(1))________________________ 3.3381E-01 OP + N2_pump_speed_provided_(m3/s)___________________________________________ (snet(1))_____________________ 2.3404E+01 OP + Plasma_chamber_volume_(m3)______________________________________________ (volume)______________________ 2.2588E+03 OP + Chamber_pressure_after_burn_(Pa)________________________________________ (pend)________________________ 1.6698E-01 OP + Chamber_pressure_before_burn_(Pa)_______________________________________ (pstart)______________________ 1.6698E-03 + Allowable_pumping_time_switch___________________________________________ (dwell_pump)__________________ 0 + Dwell_time_between_burns_(s)____________________________________________ (tdwell.)_____________________ 1.8000E+03 + CS_ramp-up_time_burns_(s)_______________________________________________ (tramp.)______________________ 5.0000E+02 + Allowable_pumping_time_between_burns_(s)________________________________ (tpump)_______________________ 1.8000E+03 + Required_D-T_pump_speed_(m3/s)__________________________________________ (s(2))________________________ 5.7790E+00 OP + D-T_pump_speed_provided_(m3/s)__________________________________________ (snet(2))_____________________ 5.6700E+01 OP + Divertor_chamber_gas_pressure_(Pa)______________________________________ (prdiv)_______________________ 3.6000E-01 + Helium_gas_fraction_in_divertor_chamber_________________________________ (fhe)_________________________ 1.7218E-01 OP + Required_helium_pump_speed_(m3/s)_______________________________________ (s(3))________________________ 3.8423E+01 OP + Helium_pump_speed_provided_(m3/s)_______________________________________ (snet(3))_____________________ 3.8423E+01 OP + D-T_fuelling_rate_(kg/s)________________________________________________ (frate)_______________________ 2.7747E-05 OP + Required_D-T_pump_speed_(m3/s)__________________________________________ (s(4))________________________ 3.8423E+01 OP + D-T_pump_speed_provided_(m3/s)__________________________________________ (snet(4))_____________________ 5.6700E+01 OP + Number_of_large_pump_ducts______________________________________________ (nduct)_______________________ 16 + Passage_diameter,_divertor_to_ducts_(m)_________________________________ (d(imax))_____________________ 4.7857E-01 OP + Passage_length_(m)______________________________________________________ (l1)__________________________ 1.7160E+00 OP + Diameter_of_ducts_(m)___________________________________________________ (dout)________________________ 5.7428E-01 OP + Duct_length,_divertor_to_elbow_(m)______________________________________ (l2)__________________________ 4.8000E+00 OP + Duct_length,_elbow_to_pumps_(m)_________________________________________ (l3)__________________________ 2.0000E+00 + Number_of_pumps_________________________________________________________ (pumpn)_______________________ 3.2000E+01 OP + # Plant Buildings System # + Internal_volume_of_reactor_building_(m3)________________________________ (vrci)________________________ 9.9708E+05 + Dist_from_centre_of_torus_to_bldg_wall_(m)______________________________ (wrbi)________________________ 3.9531E+01 + Effective_floor_area_(m2)_______________________________________________ (efloor)______________________ 3.3660E+05 + Reactor_building_volume_(m3)____________________________________________ (rbv)_________________________ 1.1310E+06 + Reactor_maintenance_building_volume_(m3)________________________________ (rmbv)________________________ 3.9641E+05 + Warmshop_volume_(m3)____________________________________________________ (wsv)_________________________ 1.2531E+05 + Tritium_building_volume_(m3)____________________________________________ (triv)________________________ 4.0000E+04 + Electrical_building_volume_(m3)_________________________________________ (elev)________________________ 5.1937E+04 + Control_building_volume_(m3)____________________________________________ (conv)________________________ 6.0000E+04 + Cryogenics_building_volume_(m3)_________________________________________ (cryv)________________________ 1.4976E+04 + Administration_building_volume_(m3)_____________________________________ (admv)________________________ 1.0000E+05 + Shops_volume_(m3)_______________________________________________________ (shov)________________________ 1.0000E+05 + Total_volume_of_nuclear_buildings_(m3)__________________________________ (volnucb)_____________________ 1.5738E+06 + # Electric Power Requirements # + Facility_base_load_(MW)_________________________________________________ (basemw)______________________ 5.0000E+00 + Divertor_coil_power_supplies_(MW)_______________________________________ (bdvmw)_______________________ 0.0000E+00 + Cryoplant_electric_power_(MW)___________________________________________ (crymw)_______________________ 3.6566E+01 OP + Primary_coolant_pumps_(MW)______________________________________________ (htpmw..)_____________________ 1.9053E+02 OP + PF_coil_power_supplies_(MW)_____________________________________________ (ppfmw)_______________________ 8.5511E+01 OP + TF_coil_power_supplies_(MW)_____________________________________________ (ptfmw)_______________________ 1.0434E+01 OP + Plasma_heating_supplies_(MW)____________________________________________ (pheatingmw)__________________ 1.6029E+02 OP + Tritium_processing_(MW)_________________________________________________ (trithtmw..)__________________ 1.5000E+01 + Vacuum_pumps__(MW)______________________________________________________ (vachtmw..)___________________ 5.0000E-01 + Total_pulsed_power_(MW)_________________________________________________ (pacpmw)______________________ 5.5432E+02 OP + Total_base_power_required_at_all_times_(MW)_____________________________ (fcsht)_______________________ 5.5490E+01 OP + # Cryogenics # + Conduction_and_radiation_heat_loads_on_cryogenic_components_(MW)________ (qss/1.0d6)___________________ 1.4779E-02 OP + Nuclear_heating_of_cryogenic_components_(MW)____________________________ (qnuc/1.0d6)__________________ 1.3000E-02 OP + AC_losses_in_cryogenic_components_(MW)__________________________________ (qac/1.0d6)___________________ 3.8170E-03 OP + Resistive_losses_in_current_leads_(MW)__________________________________ (qcl/1.0d6)___________________ 1.9539E-02 OP + 45%_allowance_for_heat_loads_in_transfer_lines,_storage_tanks_etc_(MW)__ (qmisc/1.0d6)_________________ 2.3011E-02 OP + Sum_=_Total_heat_removal_at_cryogenic_temperatures_(tfcoil_variables.tmp (helpow_+_helpow_cryal/1.0d6)_ 7.4146E-02 OP + Temperature_of_cryogenic_superconducting_components_(K)_________________ (tmpcry)______________________ 4.5000E+00 + Temperature_of_cryogenic_aluminium_components_(K)_______________________ (tcoolin)_____________________ 3.1315E+02 + Efficiency_(figure_of_merit)_of_cryogenic_plant_is_13%_of_ideal_Carnot_v ______________________________ 2.0277E-03 OP + Efficiency_(figure_of_merit)_of_cryogenic_aluminium_plant_is_40%_of_idea ______________________________ -2.0203E+00 OP + Electric_power_for_cryogenic_plant_(MW)_________________________________ (crypmw)______________________ 3.6566E+01 OP + # Plant Power / Heat Transport Balance # + Neutron_power_multiplication_in_blanket_________________________________ (emult)_______________________ 1.2690E+00 + Divertor_area_fraction_of_whole_toroid_surface__________________________ (fdiv)________________________ 1.1500E-01 + H/CD_apparatus_+_diagnostics_area_fraction______________________________ (fhcd)________________________ 0.0000E+00 + First_wall_area_fraction________________________________________________ (1-fdiv-fhcd)_________________ 8.8500E-01 + Switch_for_pumping_of_primary_coolant___________________________________ (primary_pumping)_____________ 3 + Mechanical_pumping_power_for_FW_cooling_loop_including_heat_exchanger_(M (htpmw_fw)____________________ 0.0000E+00 OP + Mechanical_pumping_power_for_blanket_cooling_loop_including_heat_exchang (htpmw_blkt)__________________ 0.0000E+00 OP + Mechanical_pumping_power_for_FW_and_blanket_cooling_loop_including_heat_ (htpmw_fw_blkt)_______________ 1.6407E+02 OP + Mechanical_pumping_power_for_divertor_(MW)______________________________ (htpmw_div)___________________ 1.6906E+00 OP + Mechanical_pumping_power_for_shield_and_vacuum_vessel_(MW)______________ (htpmw_shld)__________________ 7.0688E-03 OP + Electrical_pumping_power_for_FW_and_blanket_(MW)________________________ (htpmwe_fw_blkt)______________ 1.8858E+02 OP + Electrical_pumping_power_for_shield_(MW)________________________________ (htpmwe_shld)_________________ 8.1250E-03 OP + Electrical_pumping_power_for_divertor_(MW)______________________________ (htpmwe_div)__________________ 1.9433E+00 OP + Total_electrical_pumping_power_for_primary_coolant_(MW)_________________ (htpmw)_______________________ 1.9053E+02 OP + Coolant_pump_power_/_non-pumping_thermal_power_in_shield________________ (fpumpshld)___________________ 5.0000E-03 + Coolant_pump_power_/_non-pumping_thermal_power_in_divertor______________ (fpumpdiv)____________________ 5.0000E-03 + Electrical_efficiency_of_heat_transport_coolant_pumps___________________ (etahtp)______________________ 8.7000E-01 + Thermal_to_electric_conversion_efficiency_of_the_power_conversion_cycle_ (etath)_______________________ 4.0000E-01 + Fraction_of_total_high-grade_thermal_power_to_divertor__________________ (pdivfraction)________________ 1.5623E-01 + Total_power_leaving_reactor_(across_vacuum_vessel_boundary)_(MW)________ ______________________________ 2.0111E+03 + Heat_removal_from_cryogenic_plant_(MW)__________________________________ (crypmw)______________________ 3.6566E+01 + Heat_removal_from_facilities_(MW)_______________________________________ (fachtmw)_____________________ 5.5490E+01 + Coolant_pumping_efficiency_losses_(MW)__________________________________ (htpsecmw)____________________ 2.4769E+01 + Heat_removal_from_injection_power_(MW)__________________________________ (pinjht)______________________ 8.0143E+01 + Heat_removal_from_tritium_plant_(MW)____________________________________ (trithtmw)____________________ 1.5000E+01 + Heat_removal_from_vacuum_pumps_(MW)_____________________________________ (vachtmw)_____________________ 5.0000E-01 + TF_coil_resistive_power_(MW)____________________________________________ (tfcmw)_______________________ 0.0000E+00 + Total_low-grade_thermal_power_(MW)______________________________________ (psechtmw)____________________ 2.2417E+02 + Total_High-grade_thermal_power_(MW)_____________________________________ (pthermmw)____________________ 2.1751E+03 + Number_of_primary_heat_exchangers_______________________________________ (nphx)________________________ 3 OP + Transport_power_from_scaling_law_(MW)___________________________________ (pscalingmw)__________________ 2.9785E+02 + Radiation_power_from_inside_"coreradius"_(MW)___________________________ (pcoreradmw.)_________________ 9.1650E+01 + Total_(MW)______________________________________________________________ ______________________________ 3.8950E+02 + Alpha_power_deposited_in_plasma_(MW)____________________________________ (falpha*palpmw)_______________ 3.0746E+02 + Power_from_charged_products_of_DD_and/or_D-He3_fusion_(MW)______________ (pchargemw.)__________________ 1.2659E+00 + Ohmic_heating_(MW)______________________________________________________ (pohmmw.)_____________________ 6.2284E-01 + Injected_power_deposited_in_plasma_(MW)_________________________________ (pinjmw)______________________ 8.0143E+01 + Total_(MW)______________________________________________________________ ______________________________ 3.8950E+02 + Fusion_power_(MW)_______________________________________________________ (powfmw)______________________ 1.6202E+03 + Power_from_energy_multiplication_in_blanket_and_shield_(MW)_____________ (emultmw)_____________________ 3.0836E+02 + Injected_power_(MW)_____________________________________________________ (pinjmw.)_____________________ 8.0143E+01 + Ohmic_power_(MW)________________________________________________________ (pohmmw.)_____________________ 6.2284E-01 + Power_deposited_in_primary_coolant_by_pump_(MW)_________________________ (htpmw_mech)__________________ 1.6576E+02 + Total_(MW)______________________________________________________________ ______________________________ 2.1751E+03 + Heat_extracted_from_first_wall_and_blanket_(MW)_________________________ (pthermfw_blkt)_______________ 1.8339E+03 + Heat_extracted_from_shield__(MW)________________________________________ (pthermshld)__________________ 1.4208E+00 + Heat_extracted_from_divertor_(MW)_______________________________________ (pthermdiv)___________________ 3.3982E+02 + Nuclear_and_photon_power_lost_to_H/CD_system_(MW)_______________________ (psechcd)_____________________ 0.0000E+00 + Nuclear_power_lost_to_TF_(MW)___________________________________________ (ptfnuc)______________________ 2.5118E-02 + Total_(MW)______________________________________________________________ ______________________________ 2.1752E+03 + Net_electric_power_output(MW)___________________________________________ (pnetelmw.)___________________ 4.0001E+02 + Required_Net_electric_power_output(MW)__________________________________ (pnetelin)____________________ 4.0000E+02 + Electric_power_for_heating_and_current_drive_(MW)_______________________ (pinjwp)______________________ 1.6029E+02 + Electric_power_for_primary_coolant_pumps_(MW)___________________________ (htpmw)_______________________ 1.9053E+02 + Electric_power_for_vacuum_pumps_(MW)____________________________________ (vachtmw)_____________________ 5.0000E-01 + Electric_power_for_tritium_plant_(MW)___________________________________ (trithtmw)____________________ 1.5000E+01 + Electric_power_for_cryoplant_(MW)_______________________________________ (crypmw)______________________ 3.6566E+01 + Electric_power_for_TF_coils_(MW)________________________________________ (tfacpd)______________________ 1.0434E+01 + Electric_power_for_PF_coils_(MW)________________________________________ (pfwpmw)______________________ 1.2422E+00 + All_other_internal_electric_power_requirements_(MW)_____________________ (fachtmw)_____________________ 5.5490E+01 + Total_(MW)______________________________________________________________ (tot_plant_power)_____________ 8.7006E+02 + Total_(MW)______________________________________________________________ ______________________________ 8.7006E+02 + Gross_electrical_output*_(MW)___________________________________________ (pgrossmw)____________________ 8.7006E+02 + Fusion_power_(MW)_______________________________________________________ (powfmw)______________________ 1.6202E+03 + Power_from_energy_multiplication_in_blanket_and_shield_(MW)_____________ (emultmw)_____________________ 3.0836E+02 + Total_(MW)______________________________________________________________ ______________________________ 1.9285E+03 + Net_electrical_output_(MW) _____________________________________________ (pnetelmw)____________________ 4.0001E+02 + Heat_rejected_by_main_power_conversion_circuit_(MW)_____________________ (rejected_main)_______________ 1.3051E+03 + Heat_rejected_by_other_cooling_circuits_(MW)____________________________ (psechtmw)____________________ 2.2417E+02 + Total_(MW)______________________________________________________________ ______________________________ 1.9293E+03 + Net_electric_power_/_total_nuclear_power_(%)____________________________ (pnetelmw/(powfmw+emultmw)____ 2.0741E+01 + Net_electric_power_/_total_fusion_power_(%)_____________________________ (pnetelmw/powfmw)_____________ 2.4689E+01 + Gross_electric_power*_/_high_grade_heat_(%)_____________________________ (etath)_______________________ 4.0000E+01 + Recirculating_power_fraction____________________________________________ (cirpowfr)____________________ 5.4025E-01 + # Water usage during plant operation (secondary cooling) # + Volume_used_in_cooling_tower_(m3/day)___________________________________ (waterusetower)_______________ 5.5485E+04 OP + Volume_used_in_recirculating_water_system_(m3/day)______________________ (wateruserecirc)______________ 1.8617E+04 OP + Volume_used_in_once-through_water_system_(m3/day)_______________________ (wateruseonethru)_____________ 1.8244E+06 OP + # Errors and Warnings # + # Errors and Warnings # + PROCESS_error_status_flag_______________________________________________ (error_status)________________ 2 + Final_error_identifier__________________________________________________ (error_id)____________________ 244 + # End of PROCESS Output # + # End of PROCESS Output # + # Copy of PROCESS Input Follows # +************************************************************************************************************************ +***** ***** +***** Generic large tokamak file ***** +***** James Morris, UKAEA ***** +***** 28/06/23 ***** +***** ***** +************************************************************************* + +* Run Information * +******************* + +runtitle = Generic large tokamak + +* Figure of merit - minimise major radius +minmax = 1 + +* Error tolerance for VMCON +epsvmc = 1e-7 + +* Constraint Equations - Consistency Equations * +************************************************ + +* Beta consistency * +*------------------* +icc = 1 +ixc = 5 * beta +beta = 0.03 + +* Global power balance * +*----------------------* +icc = 2 + +* Radial build consistency * +*--------------------------* +icc = 11 + +* Constraint Equations - Limit Equations * +****************************************** + +* Density upper limit * +*---------------------* +icc = 5 +ixc = 6 * dene [m-3] +fdene = 1.2 +dene = 7.5E19 + +* Neutron wall load upper limit * +*-------------------------------* +icc = 8 +ixc = 14 * fwalld +fwalld = 1.0 +* wall load limit [MW/m2] +walalw = 2.0 + +* Fusion power upper limit * +*--------------------------* + +icc = 9 +ixc = 26 * ffuspow +* Maximum allowable value fusion power [MW] +powfmax = 3000 + +* Burn time lower limit * +*-----------------------* +icc = 13 +ixc = 21 * ftburn +* minimum burn time [s] +tbrnmn = 7200.0 + +* L-H threshold scaling * +*-----------------------* +icc = 15 +ixc = 103 * flhthresh +boundu(103) = 10.0 + +* Injection power upper limit * +*-----------------------------* +icc = 30 +ixc = 46 * fpinj +* Maximum allowable value for injected power [MW] +pinjalw = 200.0 + +* Net electric power lower limit * +*--------------------------------* +icc = 16 +ixc = 25 * fpnetel +* Minimum allowable value for net eletric power [MW] +pnetelin = 400.0 + +* Beta upper limit * +*------------------* +icc = 24 +ixc = 36 * fbetatry +fbetatry = 0.5 + +* Max TF field * +*--------------* +icc = 25 +ixc = 35 * fpeakb +* Maximum allowable value for toroidal magnetic field [T] +bmxlim = 14.0 + +* Central solenoid EOF current density upper limit * +*--------------------------------------------------* +icc = 26 +ixc = 37 * coheof [A/m2] +ixc = 38 * fjohc +boundu(38) = 1.0 +coheof = 1.5E7 +fjohc = 0.6 + +* Central solenoid BOP current density upper limit * +*--------------------------------------------------* +icc = 27 +ixc = 39 * fjohc0 +ixc = 41 * fcohbop +boundu(39) = 1.0 +fjohc0 = 0.6 +fcohbop = 0.9 + +* I_op/I_Crit TF coil limit * +*---------------------------* +icc = 33 +ixc = 50 * fiooic +boundu(50) = 1.0 +fiooic = 0.65 + +* Dump voltage upper limit * +*--------------------------* +icc = 34 +ixc = 51 * fvdump +ixc = 52 * vdalw [kV] +boundu(52) = 10.0 +fvdump = 1.0 +vdalw = 10.0 + +* J_winding pack protection * +*---------------------------* +icc = 35 +ixc = 53 * fjprot +fjprot = 1.0 + +* TF temp marg lower limit * +*--------------------------* +icc = 36 +ixc = 54 * ftmargtf +* Minimum allowable temperature margin [K] +tmargmin = 1.5 + +* CS coil temp margin lower limit * +*---------------------------------* +icc = 60 +ixc = 106 * ftmargoh +tmargmin_cs = 1.5 + +* Lower limit on taup/taueff (ratio alpha particle/energy confinement times) * +*-------------------------------------------------------------------------------* +icc = 62 +ixc = 110 * ftaulimit +taulimit = 5.0 + +* dump time constraint for VV stresses * +*--------------------------------------* +icc = 65 +ixc = 113 * fmaxvvstress +fmaxvvstress = 1.0 + +* CS stress limit * +*-----------------* +icc = 72 +ixc = 123 * foh_stress +foh_stress = 1.0 +* allowable hoop stress in Central Solenoid structural material [Pa] +alstroh = 7.5D8 + +* neped_neped_______________________normalised_residue____________________ (normres023)__________________ -1.9637E-08 + Upper_Lim._on_Psep_*_Bt_/_q_A_R___normalised_residue____________________ (normres024)__________________ 4.9789E-07 + TF_coil_case_stress_upper_limit___normalised_residue____________________ (normres025)__________________ -4.6757E-07 + TF_coil_conduit_stress_upper_lim__normalised_residue____________________ (normres026)__________________ -4.1375E-07 + # Final Feasible Point # + # Power Reactor Costs (1990 US$) # + First_wall_/_blanket_life_(years)_______________________________________ (fwbllife)____________________ 6.1566E+00 + Divertor_life_(years)___________________________________________________ (divlife.)____________________ 3.9769E+00 + Cost_of_electricity_(m$/kWh)____________________________________________ (coe)_________________________ 5.1257E+02 + # Detailed Costings (1990 US$) # + Acc.22_multiplier_for_Nth_of_a_kind_____________________________________ (fkind)_______________________ 1.0000E+00 + Level_of_Safety_Assurance_______________________________________________ (lsa)_________________________ 4 + # Structures and Site Facilities # + Site_improvements,_facilities,_land_(M$)________________________________ (c211)________________________ 3.5200E+01 + Reactor_building_cost_(M$)______________________________________________ (c212)________________________ 4.5238E+02 + Turbine_building_cost_(M$)______________________________________________ (c213)________________________ 3.8000E+01 + Reactor_maintenance_building_cost_(M$)__________________________________ (c2141)_______________________ 1.0307E+02 + Warm_shop_cost_(M$)_____________________________________________________ (c2142)_______________________ 5.7641E+01 + Tritium_building_cost_(M$)______________________________________________ (c215)________________________ 1.4800E+01 + Electrical_equipment_building_cost_(M$)_________________________________ (c216)________________________ 1.9736E+01 + Additional_buildings_cost_(M$)__________________________________________ (c2171)_______________________ 1.8000E+01 + Control_room_buildings_cost_(M$)________________________________________ (c2172)_______________________ 2.1000E+01 + Shop_and_warehouses_cost_(M$)___________________________________________ (c2173)_______________________ 1.1500E+01 + Cryogenic_building_cost_(M$)____________________________________________ (c2174)_______________________ 6.8891E+00 + Total_account_21_cost_(M$)______________________________________________ (c21)_________________________ 7.7822E+02 + # Reactor Systems # + First_wall_cost_(M$)____________________________________________________ (c2211)_______________________ 1.9130E+02 + Blanket_beryllium_cost_(M$)_____________________________________________ (c22121)______________________ 2.6109E+02 + Blanket_breeder_material_cost_(M$)______________________________________ (c22122)______________________ 6.3985E+02 + Blanket_stainless_steel_cost_(M$)_______________________________________ (c22123)______________________ 8.0726E+01 + Blanket_vanadium_cost_(M$)______________________________________________ (c22124)______________________ 0.0000E+00 + Blanket_total_cost_(M$)_________________________________________________ (c2212)_______________________ 9.8166E+02 + Bulk_shield_cost_(M$)___________________________________________________ (c22131)______________________ 7.8394E+01 + Penetration_shielding_cost_(M$)_________________________________________ (c22132)______________________ 7.8394E+01 + Total_shield_cost_(M$)__________________________________________________ (c2213)_______________________ 1.5679E+02 + Total_support_structure_cost_(M$)_______________________________________ (c2214)_______________________ 4.0933E+01 + Divertor_cost_(M$)______________________________________________________ (c2215)_______________________ 4.1660E+01 + Total_account_221_cost_(M$)_____________________________________________ (c221)________________________ 1.4123E+03 + # Magnets # + TF_coil_conductor_cost_(M$)_____________________________________________ (c22211)______________________ 1.3230E+02 + TF_coil_winding_cost_(M$)_______________________________________________ (c22212)______________________ 5.4263E+01 + TF_coil_case_cost_(M$)__________________________________________________ (c22213)______________________ 4.4365E+02 + TF_intercoil_structure_cost_(M$)________________________________________ (c22214)______________________ 1.5066E+02 + TF_coil_gravity_support_structure_(M$)__________________________________ (c22215)______________________ 4.4659E+01 + TF_magnet_assemblies_cost_(M$)__________________________________________ (c2221)_______________________ 8.2552E+02 + PF_coil_conductor_cost_(M$)_____________________________________________ (c22221)______________________ 4.6409E+02 + PF_coil_winding_cost_(M$)_______________________________________________ (c22222)______________________ 7.6765E+01 + PF_coil_case_cost_(M$)__________________________________________________ (c22223)______________________ 9.4861E+01 + PF_coil_support_structure_cost_(M$)_____________________________________ (c22224)______________________ 8.0235E+00 + PF_magnet_assemblies_cost_(M$)__________________________________________ (c2222)_______________________ 6.4374E+02 + Vacuum_vessel_assembly_cost_(M$)________________________________________ (c2223)_______________________ 2.5404E+02 + Total_account_222_cost_(M$)_____________________________________________ (c222)________________________ 1.7233E+03 + # Power Injection # + ECH_system_cost_(M$)____________________________________________________ (c2231)_______________________ 2.4043E+02 + Lower_hybrid_system_cost_(M$)___________________________________________ (c2232)_______________________ 0.0000E+00 + Neutral_beam_system_cost_(M$)___________________________________________ (c2233)_______________________ 0.0000E+00 + Total_account_223_cost_(M$)_____________________________________________ (c223)________________________ 2.4043E+02 + # Vacuum Systems # + High_vacuum_pumps_cost_(M$)_____________________________________________ (c2241)_______________________ 1.2480E+01 + Backing_pumps_cost_(M$)_________________________________________________ (c2242)_______________________ 4.6800E+00 + Vacuum_duct_cost_(M$)___________________________________________________ (c2243)_______________________ 2.5280E+00 + Valves_cost_(M$)________________________________________________________ (c2244)_______________________ 5.7410E+00 + Duct_shielding_cost_(M$)________________________________________________ (c2245)_______________________ 0.0000E+00 + Instrumentation_cost_(M$)_______________________________________________ (c2246)_______________________ 1.3000E+00 + Total_account_224_cost_(M$)_____________________________________________ (c224)________________________ 2.6729E+01 + # Power Conditioning # + TF_coil_power_supplies_cost_(M$)________________________________________ (c22511)______________________ 4.0144E+00 + TF_coil_breakers_cost_(M$)______________________________________________ (c22512)______________________ 3.4127E+01 + TF_coil_dump_resistors_cost_(M$)________________________________________ (c22513)______________________ 2.1322E+01 + TF_coil_instrumentation_and_control_(M$)________________________________ (c22514)______________________ 4.8000E+00 + TF_coil_bussing_cost_(M$)_______________________________________________ (c22515)______________________ 3.5267E+01 + Total,_TF_coil_power_costs_(M$)_________________________________________ (c2251)_______________________ 9.9531E+01 + PF_coil_power_supplies_cost_(M$)________________________________________ (c22521)______________________ 2.9591E+00 + PF_coil_instrumentation_and_control_(M$)________________________________ (c22522)______________________ 3.6000E+00 + PF_coil_bussing_cost_(M$)_______________________________________________ (c22523)______________________ 1.1995E+01 + PF_coil_burn_power_supplies_cost_(M$)___________________________________ (c22524)______________________ 1.2679E+00 + PF_coil_breakers_cost_(M$)______________________________________________ (c22525)______________________ 1.4709E+01 + PF_coil_dump_resistors_cost_(M$)________________________________________ (c22526)______________________ 4.3206E+00 + PF_coil_ac_breakers_cost_(M$)___________________________________________ (c22527)______________________ 9.0000E-01 + Total,_PF_coil_power_costs_(M$)_________________________________________ (c2252)_______________________ 3.9752E+01 + Total,_energy_storage_cost_(M$)_________________________________________ (c2253)_______________________ 1.6864E+01 + Total_account_225_cost_(M$)_____________________________________________ (c225)________________________ 1.5615E+02 + # Heat Transport System # + Pumps_and_piping_system_cost_(M$)_______________________________________ (cpp)_________________________ 3.6795E+01 + Primary_heat_exchanger_cost_(M$)________________________________________ (chx)_________________________ 7.1692E+01 + Total,_reactor_cooling_system_cost_(M$)_________________________________ (c2261)_______________________ 1.0849E+02 + Pumps,_piping_cost_(M$)_________________________________________________ (cppa)________________________ 2.8417E+01 + Total,_auxiliary_cooling_system_cost_(M$)_______________________________ (c2262)_______________________ 2.8417E+01 + Total,_cryogenic_system_cost_(M$)_______________________________________ (c2263)_______________________ 1.7039E+02 + Total_account_226_cost_(M$)_____________________________________________ (c226)________________________ 3.0729E+02 + # Fuel Handling System # + Fuelling_system_cost_(M$)_______________________________________________ (c2271)_______________________ 2.2300E+01 + Fuel_processing_and_purification_cost_(M$)______________________________ (c2272)_______________________ 1.0229E+02 + Atmospheric_recovery_systems_cost_(M$)__________________________________ (c2273)_______________________ 5.8088E+01 + Nuclear_building_ventilation_cost_(M$)__________________________________ (c2274)_______________________ 6.9201E+01 + Total_account_227_cost_(M$)_____________________________________________ (c227)________________________ 2.5188E+02 + # Instrumentation and Control # + Instrumentation_and_control_cost_(M$)___________________________________ (c228)________________________ 1.5000E+02 + # Maintenance Equipment # + Maintenance_equipment_cost_(M$)_________________________________________ (c229)________________________ 1.2500E+02 + # Total Account 22 Cost # + Total_account_22_cost_(M$)______________________________________________ (c22)_________________________ 4.3931E+03 + # Turbine Plant Equipment # + Turbine_plant_equipment_cost_(M$)_______________________________________ (c23)_________________________ 1.7613E+02 + # Electric Plant Equipment # + Switchyard_equipment_cost_(M$)__________________________________________ (c241)________________________ 1.8400E+01 + Transformers_cost_(M$)__________________________________________________ (c242)________________________ 8.0330E+00 + Low_voltage_equipment_cost_(M$)_________________________________________ (c243)________________________ 6.4513E+00 + Diesel_backup_equipment_cost_(M$)_______________________________________ (c244)________________________ 6.8000E+00 + Auxiliary_facilities_cost_(M$)__________________________________________ (c245)________________________ 1.5000E+00 + Total_account_24_cost_(M$)______________________________________________ (c24)_________________________ 4.1184E+01 + # Miscellaneous Plant Equipment # + Miscellaneous_plant_equipment_cost_(M$)_________________________________ (c25)_________________________ 2.5000E+01 + # Heat Rejection System # + Heat_rejection_system_cost_(M$)_________________________________________ (c26)_________________________ 4.9877E+01 + # Plant Direct Cost # + Plant_direct_cost_(M$)__________________________________________________ (cdirt)_______________________ 5.4635E+03 + # Reactor Core Cost # + Reactor_core_cost_(M$)__________________________________________________ (crctcore)____________________ 3.3761E+03 + # Indirect Cost # + Indirect_cost_(M$)______________________________________________________ (c9)__________________________ 1.8221E+03 + # Total Contingency # + Total_contingency_(M$)__________________________________________________ (ccont)_______________________ 1.4207E+03 + # Constructed Cost # + Constructed_cost_(M$)___________________________________________________ (concost)_____________________ 8.7063E+03 + # Interest during Construction # + Interest_during_construction_(M$)_______________________________________ (moneyint)____________________ 1.4365E+03 + # Total Capital Investment # + Total_capital_investment_(M$)___________________________________________ (capcost)_____________________ 1.0143E+04 + # Plant Availability # + Allowable_blanket_neutron_fluence_(MW-yr/m2)____________________________ (abktflnc)____________________ 5.0000E+00 + Allowable_divertor_heat_fluence_(MW-yr/m2)______________________________ (adivflnc)____________________ 7.0000E+00 + First_wall_/_blanket_lifetime_(years)___________________________________ (bktlife)_____________________ 6.1566E+00 OP + Divertor_lifetime_(years)_______________________________________________ (divlife)_____________________ 3.9769E+00 OP + Heating/CD_system_lifetime_(years)______________________________________ (cdrlife)_____________________ 6.1566E+00 OP + Total_plant_lifetime_(years)____________________________________________ (tlife)_______________________ 3.0000E+01 + Total_plant_availability_fraction_______________________________________ (cfactr)______________________ 8.0000E-01 + Number_of_fusion_cycles_to_reach_allowable_fw/blanket_DPA_______________ (bktcycles)___________________ 1.5787E+04 + # Plasma # + Tokamak_aspect_ratio_=_Conventional,_itart_=_0__________________________ (itart)_______________________ 0.0000E+00 + Major_radius_(m)________________________________________________________ (rmajor)______________________ 8.0000E+00 ITV + Minor_radius_(m)________________________________________________________ (rminor)______________________ 2.6667E+00 + Aspect_ratio____________________________________________________________ (aspect)______________________ 3.0000E+00 + Elongation,_X-point_(input_value_used)__________________________________ (kappa)_______________________ 1.8500E+00 + Elongation,_95%_surface_(calculated_from_kappa)_________________________ (kappa95)_____________________ 1.6518E+00 + Elongation,_area_ratio_calc.____________________________________________ (kappaa)______________________ 1.7188E+00 + Triangularity,_X-point_(input_value_used)_______________________________ (triang)______________________ 5.0000E-01 + Triangularity,_95%_surface_(calculated_from_triang)_____________________ (triang95)____________________ 3.3333E-01 + Plasma_poloidal_perimeter_(m)___________________________________________ (pperim)______________________ 2.4081E+01 + Plasma_cross-sectional_area_(m2)________________________________________ (xarea)_______________________ 3.8398E+01 + Plasma_surface_area_(m2)________________________________________________ (sarea)_______________________ 1.1738E+03 OP + Plasma_volume_(m3)______________________________________________________ (vol)_________________________ 1.8882E+03 OP + Plasma_current_scaling_law_used_________________________________________ (icurr)_______________________ 4 + Plasma_current_(MA)_____________________________________________________ (plascur/1D6)_________________ 1.6631E+01 + Current_density_profile_factor__________________________________________ (alphaj)______________________ 1.9805E+00 + Plasma_internal_inductance,_li__________________________________________ (rli)_________________________ 1.2275E+00 + Vertical_field_at_plasma_(T)____________________________________________ (bvert)_______________________ -7.4373E-01 + Vacuum_toroidal_field_at_R_(T)__________________________________________ (bt)__________________________ 5.2940E+00 ITV + Average_poloidal_field_(T)______________________________________________ (bp)__________________________ 8.6787E-01 + Total_field_(sqrt(bp^2_+_bt^2))_(T)_____________________________________ (btot)________________________ 5.3647E+00 + Safety_factor_on_axis___________________________________________________ (q0)__________________________ 1.0000E+00 + Safety_factor_at_95%_flux_surface_______________________________________ (q95)_________________________ 3.5961E+00 ITV + Cylindrical_safety_factor_(qcyl)________________________________________ (qstar)_______________________ 2.9805E+00 + Total_plasma_beta_______________________________________________________ (beta)________________________ 3.3648E-02 ITV + Total_poloidal_beta_____________________________________________________ (betap)_______________________ 1.2857E+00 OP + Total_toroidal_beta_____________________________________________________ ______________________________ 3.4553E-02 OP + Fast_alpha_beta_________________________________________________________ (betaft)______________________ 4.2236E-03 OP + Beam_ion_beta___________________________________________________________ (betanb)______________________ 0.0000E+00 OP + (Fast_alpha_+_beam_physics_variables.beta)/(thermal_physics_variables.be (gammaft)_____________________ 1.4354E-01 OP + Thermal_beta____________________________________________________________ ______________________________ 2.9425E-02 OP + Thermal_poloidal_beta___________________________________________________ ______________________________ 1.1243E+00 OP + Thermal_toroidal_physics_variables.beta_(=_beta-exp)____________________ ______________________________ 3.0215E-02 OP + 2nd_stability_physics_variables.beta_:_beta_p_/_(R/a)___________________ (eps*betap)___________________ 4.2857E-01 + 2nd_stability_physics_variables.beta_upper_limit________________________ (epbetmax)____________________ 1.3800E+00 + Beta_g_coefficient______________________________________________________ (dnbeta)______________________ 4.9099E+00 + Normalised_thermal_beta_________________________________________________ ______________________________ 2.4977E+00 + Normalised_total_beta___________________________________________________ ______________________________ 2.8562E+00 + Normalised_toroidal_beta________________________________________________ (normalised_toroidal_beta)____ 2.9330E+00 + Limit_on_thermal_beta___________________________________________________ (betalim)_____________________ 5.7842E-02 + Plasma_thermal_energy_(J)_______________________________________________ ______________________________ 9.5431E+08 OP + Total_plasma_internal_energy_(J)________________________________________ (total_plasma_internal_energy) 1.0913E+09 OP + Electron_temperature_(keV)______________________________________________ (te)__________________________ 1.2489E+01 ITV + Electron_temperature_on_axis_(keV)______________________________________ (te0)_________________________ 2.5758E+01 + Ion_temperature_(keV)___________________________________________________ (ti)__________________________ 1.2489E+01 + Ion_temperature_on_axis_(keV)___________________________________________ (ti0)_________________________ 2.5758E+01 + Electron_temp.,_density_weighted_(keV)__________________________________ (ten)_________________________ 1.3805E+01 + Electron_density_(/m3)__________________________________________________ (dene)________________________ 8.0667E+19 ITV + Electron_density_on_axis_(/m3)__________________________________________ (ne0)_________________________ 1.0610E+20 OP + Line-averaged_electron_density_(/m3)____________________________________ (dnla)________________________ 8.9334E+19 OP + Line-averaged_electron_density_/_Greenwald_density______________________ (dnla_gw)_____________________ 1.2000E+00 OP + Ion_density_(/m3)_______________________________________________________ (dnitot)______________________ 7.1669E+19 OP + Fuel_density_(/m3)______________________________________________________ (deni)________________________ 6.4831E+19 OP + Total_impurity_density_with_Z_>_2_(no_He)_(/m3)_________________________ (dnz)_________________________ 4.6503E+16 OP + Helium_ion_density_(thermalised_ions_only)_(/m3)________________________ (dnalp)_______________________ 6.7723E+18 OP + Proton_density_(/m3)____________________________________________________ (dnprot)______________________ 1.8963E+16 OP + Hot_beam_density_(/m3)__________________________________________________ (dnbeam)______________________ 0.0000E+00 OP + Density_limit_from_scaling_(/m3)________________________________________ (dnelimt)_____________________ 7.4445E+19 OP + Density_limit_(enforced)_(/m3)__________________________________________ (boundu(9)*dnelimt)___________ 7.4445E+19 OP + Helium_ion_density_(thermalised_ions_only)_/_electron_density___________ (ralpne)______________________ 8.3954E-02 ITV + H__concentration________________________________________________________ (fimp(01))____________________ 8.0392E-01 OP + He_concentration________________________________________________________ (fimp(02))____________________ 8.3954E-02 + Be_concentration________________________________________________________ (fimp(03))____________________ 0.0000E+00 + C__concentration________________________________________________________ (fimp(04))____________________ 0.0000E+00 + N__concentration________________________________________________________ (fimp(05))____________________ 0.0000E+00 + O__concentration________________________________________________________ (fimp(06))____________________ 0.0000E+00 + Ne_concentration________________________________________________________ (fimp(07))____________________ 0.0000E+00 + Si_concentration________________________________________________________ (fimp(08))____________________ 0.0000E+00 + Ar_concentration________________________________________________________ (fimp(09))____________________ 0.0000E+00 + Fe_concentration________________________________________________________ (fimp(10))____________________ 0.0000E+00 + Ni_concentration________________________________________________________ (fimp(11))____________________ 0.0000E+00 + Kr_concentration________________________________________________________ (fimp(12))____________________ 0.0000E+00 + Xe_concentration________________________________________________________ (fimp(13))____________________ 5.7149E-04 ITV + W__concentration________________________________________________________ (fimp(14))____________________ 5.0000E-06 + Average_mass_of_all_ions_(amu)__________________________________________ (aion)________________________ 2.7252E+00 OP + Effective_charge________________________________________________________ (zeff)________________________ 2.5164E+00 + Density_profile_factor__________________________________________________ (alphan)______________________ 1.0000E+00 + Plasma_profile_model____________________________________________________ (ipedestal)___________________ 1 + Density_pedestal_r/a_location___________________________________________ (rhopedn)_____________________ 9.4000E-01 + Electron_density_pedestal_height_(/m3)__________________________________ (neped)_______________________ 6.3278E+19 OP + Electron_density_at_pedestal_/_nGW______________________________________ (fgwped_out)__________________ 8.5000E-01 + Temperature_pedestal_r/a_location_______________________________________ (rhopedt)_____________________ 9.4000E-01 + Pedestal_scaling_switch_________________________________________________ (ieped)_______________________ 0 + Electron_temp._pedestal_height_(keV)____________________________________ (teped)_______________________ 5.5000E+00 + Electron_temp._at_separatrix_(keV)______________________________________ (tesep)_______________________ 1.0000E-01 + Electron_density_at_separatrix_(/m3)____________________________________ (nesep)_______________________ 3.7223E+19 + Electron_density_at_separatrix_/_nGW____________________________________ (fgwsep_out)__________________ 5.0000E-01 + Temperature_profile_index_______________________________________________ (alphat)______________________ 1.4500E+00 + Temperature_profile_index_beta__________________________________________ (tbeta)_______________________ 2.0000E+00 + Old_ASDEX_model_________________________________________________________ (dlimit(1))___________________ 5.2797E+19 OP + Borrass_ITER_model_I____________________________________________________ (dlimit(2))___________________ 1.0969E+20 OP + Borrass_ITER_model_II___________________________________________________ (dlimit(3))___________________ 4.3575E+19 OP + JET_edge_radiation_model________________________________________________ (dlimit(4))___________________ 3.0227E+21 OP + JET_simplified_model____________________________________________________ (dlimit(5))___________________ 4.3397E+20 OP + Hugill-Murakami_Mq_model________________________________________________ (dlimit(6))___________________ 6.6609E+19 OP + Greenwald_model_________________________________________________________ (dlimit(7))___________________ 7.4445E+19 OP + Deuterium_fuel_fraction_________________________________________________ (fdeut)_______________________ 5.0000E-01 + Tritium_fuel_fraction___________________________________________________ (ftrit)_______________________ 5.0000E-01 + Total_fusion_power_(MW)_________________________________________________ (powfmw)______________________ 1.6202E+03 OP + _=____D-T_fusion_power_(MW)_____________________________________________ (pdt)_________________________ 1.6182E+03 OP + __+___D-D_fusion_power_(MW)_____________________________________________ (pdd)_________________________ 1.9494E+00 OP + __+_D-He3_fusion_power_(MW)_____________________________________________ (pdhe3)_______________________ 0.0000E+00 OP + Alpha_power:_total_(MW)_________________________________________________ (palpmw)______________________ 3.2365E+02 OP + Alpha_power:_beam-plasma_(MW)___________________________________________ (palpnb)______________________ 0.0000E+00 OP + Neutron_power_(MW)______________________________________________________ (pneutmw)_____________________ 1.2953E+03 OP + Charged_particle_power_(excluding_alphas)_(MW)__________________________ (pchargemw)___________________ 1.2659E+00 OP + Total_power_deposited_in_plasma_(MW)____________________________________ (tot_power_plasma)____________ 3.8950E+02 OP + Bremsstrahlung_radiation_power_(MW)_____________________________________ (pbrempv*vol)_________________ 6.5195E+01 OP + Line_radiation_power_(MW)_______________________________________________ (plinepv*vol)_________________ 1.4609E+02 OP + Synchrotron_radiation_power_(MW)________________________________________ (psyncpv*vol)_________________ 1.5187E+01 OP + Synchrotron_wall_reflectivity_factor____________________________________ (ssync)_______________________ 6.0000E-01 + Normalised_minor_radius_defining_'core'_________________________________ (coreradius)__________________ 7.5000E-01 + Fraction_of_core_radiation_subtracted_from_P_L__________________________ (coreradiationfraction)_______ 6.0000E-01 + Radiation_power_from_inner_zone_(MW)____________________________________ (pinnerzoneradmw)_____________ 9.1650E+01 OP + Radiation_power_from_outer_zone_(MW)____________________________________ (pouterzoneradmw)_____________ 1.3482E+02 OP + Total_radiation_power_from_inside_LCFS_(MW)_____________________________ (pradmw)______________________ 2.2647E+02 OP + LCFS_radiation_fraction_=_total_radiation_in_LCFS_/_total_power_deposite (rad_fraction_LCFS)___________ 5.8144E-01 OP + Nominal_mean_radiation_load_on_inside_surface_of_reactor_(MW/m2)________ (photon_wall)_________________ 1.7749E-01 OP + Peaking_factor_for_radiation_wall_load__________________________________ (peakfactrad)_________________ 3.3300E+00 IP + Maximum_permitted_radiation_wall_load_(MW/m^2)__________________________ (maxradwallload)______________ 1.0000E+00 IP + Peak_radiation_wall_load_(MW/m^2)_______________________________________ (peakradwallload)_____________ 5.9106E-01 OP + Fast_alpha_particle_power_incident_on_the_first_wall_(MW)_______________ (palpfwmw)____________________ 1.6182E+01 OP + Nominal_mean_neutron_load_on_inside_surface_of_reactor_(MW/m2)__________ (wallmw)______________________ 1.0152E+00 OP + Power_incident_on_the_divertor_targets_(MW)_____________________________ (ptarmw)______________________ 3.2606E+01 OP + Fraction_of_power_to_the_lower_divertor_________________________________ (ftar)________________________ 1.0000E+00 IP + Outboard_side_heat_flux_decay_length_(m)________________________________ (lambdaio)____________________ 1.5700E-03 OP + Fraction_of_power_on_the_inner_targets__________________________________ (fio)_________________________ 4.1000E-01 OP + Fraction_of_power_incident_on_the_lower_inner_target____________________ (fLI)_________________________ 4.1000E-01 OP + Fraction_of_power_incident_on_the_lower_outer_target____________________ (fLO)_________________________ 5.9000E-01 OP + Power_incident_on_the_lower_inner_target_(MW)___________________________ (pLImw)_______________________ 1.3368E+01 OP + Power_incident_on_the_lower_outer_target_(MW)___________________________ (pLOmw)_______________________ 1.9237E+01 OP + Ohmic_heating_power_(MW)________________________________________________ (pohmmw)______________________ 6.2284E-01 OP + Fraction_of_alpha_power_deposited_in_plasma_____________________________ (falpha)______________________ 9.5000E-01 + Fraction_of_alpha_power_to_electrons____________________________________ (falpe)_______________________ 7.1828E-01 + Fraction_of_alpha_power_to_ions_________________________________________ (falpi)_______________________ 2.8172E-01 + Ion_transport_(MW)______________________________________________________ (ptrimw)______________________ 1.4013E+02 OP + Electron_transport_(MW)_________________________________________________ (ptremw)______________________ 1.5772E+02 OP + Injection_power_to_ions_(MW)____________________________________________ (pinjimw)_____________________ 0.0000E+00 OP + Injection_power_to_electrons_(MW)_______________________________________ (pinjemw)_____________________ 8.0143E+01 OP + Ignited_plasma_switch_(0=not_ignited,_1=ignited)________________________ (ignite)______________________ 0 + Power_into_divertor_zone_via_charged_particles_(MW)_____________________ (pdivt)_______________________ 1.6303E+02 OP + Psep_/_R_ratio_(MW/m)___________________________________________________ (pdivt/rmajor)________________ 2.0378E+01 OP + Psep_Bt_/_qAR_ratio_(MWT/m)_____________________________________________ (pdivtbt/qar)_________________ 1.0000E+01 OP + ITER_1996_scaling:_nominal_(MW)_________________________________________ (pthrmw(1))___________________ 1.2978E+02 OP + ITER_1996_scaling:_upper_bound_(MW)_____________________________________ (pthrmw(2))___________________ 2.8603E+02 OP + ITER_1996_scaling:_lower_bound_(MW)_____________________________________ (pthrmw(3))___________________ 5.8098E+01 OP + ITER_1997_scaling_(1)_(MW)______________________________________________ (pthrmw(4))___________________ 2.1452E+02 OP + ITER_1997_scaling_(2)_(MW)______________________________________________ (pthrmw(5))___________________ 1.7206E+02 OP + Martin_2008_scaling:_nominal_(MW)_______________________________________ (pthrmw(6))___________________ 9.7416E+01 OP + Martin_2008_scaling:_95%_upper_bound_(MW)_______________________________ (pthrmw(7))___________________ 1.2769E+02 OP + Martin_2008_scaling:_95%_lower_bound_(MW)_______________________________ (pthrmw(8))___________________ 6.7143E+01 OP + Snipes_2000_scaling:_nominal_(MW)_______________________________________ (pthrmw(9))___________________ 6.7785E+01 OP + Snipes_2000_scaling:_upper_bound_(MW)___________________________________ (pthrmw(10))__________________ 9.9437E+01 OP + Snipes_2000_scaling:_lower_bound_(MW)___________________________________ (pthrmw(11))__________________ 4.5839E+01 OP + Snipes_2000_scaling_(closed_divertor):_nominal_(MW)_____________________ (pthrmw(12))__________________ 3.1010E+01 OP + Snipes_2000_scaling_(closed_divertor):_upper_bound_(MW)_________________ (pthrmw(13))__________________ 4.3148E+01 OP + Snipes_2000_scaling_(closed_divertor):_lower_bound_(MW)_________________ (pthrmw(14))__________________ 2.2130E+01 OP + Hubbard_2012_L-I_threshold_-_nominal_(MW)_______________________________ (pthrmw(15))__________________ 2.7549E+01 OP + Hubbard_2012_L-I_threshold_-_lower_bound_(MW)___________________________ (pthrmw(16))__________________ 1.4319E+01 OP + Hubbard_2012_L-I_threshold_-_upper_bound_(MW)___________________________ (pthrmw(17))__________________ 5.3005E+01 OP + Hubbard_2017_L-I_threshold______________________________________________ (pthrmw(18))__________________ 2.6202E+02 OP + Martin_2008_aspect_ratio_corrected_scaling:_nominal_(MW)________________ (pthrmw(19))__________________ 9.7416E+01 OP + Martin_2008_aspect_ratio_corrected_scaling:_95%_upper_bound_(MW)________ (pthrmw(20))__________________ 1.2769E+02 OP + Martin_2008_aspect_ratio_corrected_scaling:_95%_lower_bound_(MW)________ (pthrmw(21))__________________ 6.7143E+01 OP + L-H_threshold_power_(enforced)_(MW)_____________________________________ (boundl(103)*plhthresh)_______ 9.7416E+01 OP + L-H_threshold_power_(MW)________________________________________________ (plhthresh)___________________ 9.7416E+01 OP + Confinement_H_factor____________________________________________________ (hfact)_______________________ 1.1886E+00 ITV + Global_thermal_energy_confinement_time_(s)______________________________ (taueff)______________________ 3.2037E+00 + Ion_energy_confinement_time_(s)_________________________________________ (tauei)_______________________ 3.2037E+00 + Electron_energy_confinement_time_(s)____________________________________ (tauee)_______________________ 3.2037E+00 + n.tau_=_Volume-average_electron_density_x_Energy_confinement_time_(s/m3) (dntau)_______________________ 2.5843E+20 OP + Triple_product__(keV_s/m3)______________________________________________ (dntau*te)____________________ 3.2275E+21 OP + Transport_loss_power_assumed_in_scaling_law_(MW)________________________ (powerht)_____________________ 2.9785E+02 OP + Switch_for_radiation_loss_term_usage_in_power_balance___________________ (iradloss)____________________ 1 + Radiation_power_subtracted_from_plasma_power_balance_(MW)_______________ ______________________________ 9.1650E+01 OP + Alpha_particle_confinement_time_(s)_____________________________________ (taup)________________________ 2.2270E+01 + Alpha_particle/energy_confinement_time_ratio____________________________ (taup/taueff)_________________ 6.9512E+00 + Lower_limit_on_taup/taueff______________________________________________ (taulimit)____________________ 5.0000E+00 + Total_energy_confinement_time_including_radiation_loss_(s)______________ (total_energy_conf_time)______ 2.8018E+00 + Normalized_plasma_pressure_beta_as_defined_by_McDonald_et_al____________ (beta_mcdonald)_______________ 3.4553E-02 OP + Normalized_ion_Larmor_radius____________________________________________ (rho_star)____________________ 1.9603E-03 OP + Normalized_collisionality_______________________________________________ (nu_star)_____________________ 3.7266E-03 OP + Volume_measure_of_elongation____________________________________________ (kappaa_IPB)__________________ 1.6815E+00 OP + Total_volt-second_requirement_(Wb)______________________________________ (vsstt)_______________________ 5.5616E+02 OP + Inductive_volt-seconds_(Wb)_____________________________________________ (vsind)_______________________ 2.3585E+02 OP + Ejima_coefficient_______________________________________________________ (gamma)_______________________ 3.0000E-01 + Start-up_resistive_(Wb)_________________________________________________ (vsres)_______________________ 5.0159E+01 OP + Flat-top_resistive_(Wb)_________________________________________________ (vsbrn)_______________________ 2.7015E+02 OP + bootstrap_current_fraction_multiplier___________________________________ (cboot)_______________________ 1.0000E+00 + Bootstrap_fraction_(ITER_1989)__________________________________________ (bscf_iter89)_________________ 3.7098E-01 + Bootstrap_fraction_(Sauter_et_al)_______________________________________ (bscf_sauter)_________________ 4.1920E-01 + Bootstrap_fraction_(Nevins_et_al)_______________________________________ (bscf_nevins)_________________ 3.5042E-01 + Bootstrap_fraction_(Wilson)_____________________________________________ (bscf_wilson)_________________ 4.3349E-01 + Diamagnetic_fraction_(Hender)___________________________________________ (diacf_hender)________________ 1.2017E-02 + Diamagnetic_fraction_(SCENE)____________________________________________ (diacf_scene)_________________ 1.1139E-02 + Pfirsch-Schlueter_fraction_(SCENE)______________________________________ (pscf_scene)__________________ -3.0283E-03 + Bootstrap_fraction_(enforced)___________________________________________ (bootipf.)____________________ 4.1920E-01 + Diamagnetic_fraction_(enforced)_________________________________________ (diaipf.)_____________________ 0.0000E+00 + Pfirsch-Schlueter_fraction_(enforced)___________________________________ (psipf.)______________________ 0.0000E+00 + Loop_voltage_during_burn_(V)____________________________________________ (vburn)_______________________ 3.7450E-02 OP + Plasma_resistance_(ohm)_________________________________________________ (rplas)_______________________ 3.9755E-09 OP + Resistive_diffusion_time_(s)____________________________________________ (res_time)____________________ 3.0619E+03 OP + Plasma_inductance_(H)___________________________________________________ (rlp)_________________________ 1.4181E-05 OP + Coefficient_for_sawtooth_effects_on_burn_V-s_requirement________________ (csawth)______________________ 1.0000E+00 + Ratio_of_He_and_pellet_particle_confinement_times_______________________ (tauratio)____________________ 1.0000E+00 + Fuelling_rate_(nucleus-pairs/s)_________________________________________ (qfuel)_______________________ 3.3420E+21 OP + Fuel_burn-up_rate_(reactions/s)_________________________________________ (rndfuel)_____________________ 5.7755E+20 OP + Burn-up_fraction________________________________________________________ (burnup)______________________ 1.7282E-01 + # Energy confinement times, and required H-factors : # + # Current Drive System # + Current_drive_efficiency_model__________________________________________ (iefrf)_______________________ 10 + Secondary_current_drive_efficiency_model________________________________ (iefrffix)____________________ 0 + Ratio_of_power_for_flat-top_to_start-up_(MW)____________________________ (startupratio)________________ 1.0000E+00 + Auxiliary_power_used_for_plasma_heating_only_(MW)_______________________ (pheat)_______________________ 7.5000E+01 + Power_injected_for_current_drive_(MW)___________________________________ (pcurrentdrivemw)_____________ 5.1429E+00 + Maximum_Allowed_Bootstrap_current_fraction______________________________ (bscfmax)_____________________ 9.5000E-01 + Fusion_gain_factor_Q____________________________________________________ (bigq)________________________ 2.0060E+01 OP + Auxiliary_current_drive_(A)_____________________________________________ (auxiliary_cd)________________ 2.3908E+05 OP + Current_drive_efficiency_(A/W)__________________________________________ (effcd)_______________________ 4.6488E-02 OP + Normalised_current_drive_efficiency,_gamma_(10^20_A/W-m2)_______________ (gamcd)_______________________ 3.0000E-01 OP + Wall_plug_to_injector_efficiency________________________________________ (etacd)_______________________ 5.0000E-01 + ECRH_plasma_heating_efficiency__________________________________________ (gamma_ecrh)__________________ 3.0000E-01 + Bootstrap_fraction______________________________________________________ (bootipf)_____________________ 4.1920E-01 + Diamagnetic_fraction____________________________________________________ (diaipf)______________________ 0.0000E+00 + Pfirsch-Schlueter_fraction______________________________________________ (psipf)_______________________ 0.0000E+00 + Auxiliary_current_drive_fraction________________________________________ (faccd)_______________________ 1.4376E-02 + Inductive_fraction______________________________________________________ (facoh)_______________________ 5.6642E-01 + Total___________________________________________________________________ (plasipf+faccd+facoh)_________ 1.0000E+00 + Fraction_of_the_plasma_current_produced_by_non-inductive_means__________ (fvsbrnni)____________________ 4.3358E-01 ITV + Electron_cyclotron_injected_power_(MW)__________________________________ (echpwr)______________________ 8.0143E+01 OP + Maximum_allowable_ECRH_power_(MW)_______________________________________ (pinjalw)_____________________ 2.0000E+02 + ECH_wall_plug_efficiency________________________________________________ (etaech)______________________ 5.0000E-01 + ECH_wall_plug_power_(MW)________________________________________________ (echwpow)_____________________ 1.6029E+02 OP + Total_V-s_capability_of_Central_Solenoid/PF_coils_(Wb)__________________ (abs(vstot))__________________ 5.7728E+02 + Required_volt-seconds_during_start-up_(Wb)______________________________ (vssoft)______________________ 2.8601E+02 + Available_volt-seconds_during_burn_(Wb)_________________________________ (vsmax)_______________________ 2.7014E+02 + # Times # + Initial_charge_time_for_CS_from_zero_current_(s)________________________ (tramp)_______________________ 5.0000E+02 + Plasma_current_ramp-up_time_(s)_________________________________________ (tohs)________________________ 1.6631E+02 + Heating_time_(s)________________________________________________________ (theat)_______________________ 1.0000E+01 + Burn_time_(s)___________________________________________________________ (tburn)_______________________ 7.2035E+03 OP + Reset_time_to_zero_current_for_CS_(s)___________________________________ (tqnch)_______________________ 1.6631E+02 + Time_between_pulses_(s)_________________________________________________ (tdwell)______________________ 1.8000E+03 + Total_plant_cycle_time_(s)______________________________________________ (tcycle)______________________ 9.8463E+03 OP + # Radial Build # + TF_coil_radial_placement_switch_________________________________________ (tf_in_cs)____________________ 0 + TF_coil_radial_placement_switch_________________________________________ (tf_in_cs)____________________ 0 + Machine_bore_(m)________________________________________________________ (bore)________________________ 1.9854E+00 ITV + CS_radial_thickness_(m)_________________________________________________ (ohcth)_______________________ 5.7587E-01 ITV + CS_precompression_(m)___________________________________________________ (precomp)_____________________ 6.8064E-02 + CS_precompresion_to_TF_coil_radial_gap_(m)______________________________ (gapoh)_______________________ 8.0000E-02 + TF_coil_inboard_leg_(m)_________________________________________________ (tfcth)_______________________ 9.1597E-01 ITV + TF_coil_inboard_leg_insulation_gap_(m)__________________________________ (tftsgap)_____________________ 5.0000E-02 + Thermal_shield,_inboard_(m)_____________________________________________ (thshield_ib)_________________ 5.0000E-02 + thermal_shield_to_vessel_radial_gap_(m)_________________________________ (gapds)_______________________ 2.0000E-02 + Inboard_vacuum_vessel_radial_thickness_(m)______________________________ (d_vv_in)_____________________ 3.0000E-01 + Inner_radiation_shield_radial_thickness_(m)_____________________________ (shldith)_____________________ 3.0000E-01 + Gap_(m)_________________________________________________________________ (vvblgap)_____________________ 2.0000E-02 + Inboard_blanket_radial_thickness_(m)____________________________________ (blnkith)_____________________ 7.0000E-01 + Inboard_first_wall_radial_thickness_(m)_________________________________ (fwith)_______________________ 1.8000E-02 + Inboard_scrape-off_radial_thickness_(m)_________________________________ (scrapli)_____________________ 2.5000E-01 + Outboard_scrape-off_radial_thickness_(m)________________________________ (scraplo)_____________________ 2.5000E-01 + Outboard_first_wall_radial_thickness_(m)________________________________ (fwoth)_______________________ 1.8000E-02 + Outboard_blanket_radial_thickness_(m)___________________________________ (blnkoth)_____________________ 1.0000E+00 + Outer_radiation_shield_radial_thickness_(m)_____________________________ (shldoth)_____________________ 8.0000E-01 + Outboard_vacuum_vessel_radial_thickness_(m)_____________________________ (d_vv_out)____________________ 3.0000E-01 + Vessel_to_TF_radial_gap_(m)_____________________________________________ (gapsto)______________________ 1.3720E+00 + Thermal_shield,_outboard_(m)____________________________________________ (thshield_ob)_________________ 5.0000E-02 + Gap_(m)_________________________________________________________________ (tftsgap)_____________________ 5.0000E-02 + TF_coil_outboard_leg_radial_thickness_(m)_______________________________ (tfthko)______________________ 9.1597E-01 + # Vertical Build # + Divertor_null_switch____________________________________________________ (i_single_null)_______________ 1 + Vessel_-_TF_coil_vertical_gap_(m)_______________________________________ (vgap2)_______________________ 1.6300E-01 + Topside_vacuum_vessel_radial_thickness_(m)______________________________ (d_vv_top)____________________ 3.0000E-01 + Top_radiation_shield_thickness_(m)______________________________________ (shldtth)_____________________ 6.0000E-01 + Top_blanket_vertical_thickness_(m)______________________________________ (blnktth)_____________________ 8.5000E-01 + Top_first_wall_vertical_thickness_(m)___________________________________ (fwtth)_______________________ 1.8000E-02 + Top_scrape-off_vertical_thickness_(m)___________________________________ (vgaptop)_____________________ 6.0000E-01 + Plasma_half-height_(m)__________________________________________________ (rminor*kappa)________________ 4.9333E+00 + Bottom_scrape-off_vertical_thickness_(m)________________________________ (vgap)________________________ 2.0019E+00 + Divertor_structure_vertical_thickness_(m)_______________________________ (divfix)______________________ 6.2000E-01 + Bottom_radiation_shield_thickness_(m)___________________________________ (shldlth)_____________________ 7.0000E-01 + Underside_vacuum_vessel_radial_thickness_(m)____________________________ (d_vv_bot)____________________ 3.0000E-01 + External_cryostat_thickness_(m)_________________________________________ (ddwex)_______________________ 1.5000E-01 + Ratio_of_Central_solenoid_height_to_TF_coil_internal_height_____________ (ohhghf)______________________ 9.0000E-01 + Width_of_neutral_beam_duct_where_it_passes_between_the_TF_coils_(m)_____ (beamwd)______________________ 5.8000E-01 + # Divertor build and plasma position # + Plasma_top_position,_radial_(m)_________________________________________ (ptop_radial)_________________ 6.6667E+00 + Plasma_top_position,_vertical_(m)_______________________________________ (ptop_vertical)_______________ 4.9333E+00 + Plasma_geometric_centre,_radial_(m)_____________________________________ (physics_variables.rmajor.)___ 8.0000E+00 + Plasma_geometric_centre,_vertical_(m)___________________________________ (0.0)_________________________ 0.0000E+00 + Plasma_lower_physics_variables.triangularity____________________________ (tril)________________________ 5.0000E-01 + Plasma_elongation_______________________________________________________ (physics_variables.kappa.)____ 1.8500E+00 + TF_coil_vertical_offset_(m)_____________________________________________ (tfoffset)____________________ -6.1694E-01 + Plasma_outer_arc_radius_of_curvature_(m)________________________________ (rco)_________________________ 5.0422E+00 + Plasma_inner_arc_radius_of_curvature_(m)________________________________ (rci)_________________________ 9.7933E+00 + Plasma_lower_X-pt,_radial_(m)___________________________________________ (rxpt)________________________ 6.6667E+00 + Plasma_lower_X-pt,_vertical_(m)_________________________________________ (zxpt)________________________ -4.9333E+00 + Poloidal_plane_angle_between_vertical_and_inner_leg_(rad)_______________ (thetai)______________________ 2.0820E-01 + Poloidal_plane_angle_between_vertical_and_outer_leg_(rad)_______________ (thetao)______________________ 1.0429E+00 + Poloidal_plane_angle_between_inner_leg_and_plate_(rad)__________________ (betai)_______________________ 1.0000E+00 + Poloidal_plane_angle_between_outer_leg_and_plate_(rad)__________________ (betao)_______________________ 1.0000E+00 + Inner_divertor_leg_poloidal_length_(m)__________________________________ (plsepi)______________________ 1.0000E+00 + Outer_divertor_leg_poloidal_length_(m)__________________________________ (plsepo)______________________ 1.5000E+00 + Inner_divertor_plate_length_(m)_________________________________________ (plleni)______________________ 1.0000E+00 + Outer_divertor_plate_length_(m)_________________________________________ (plleno)______________________ 1.0000E+00 + Inner_strike_point,_radial_(m)__________________________________________ (rspi)________________________ 5.6883E+00 + Inner_strike_point,_vertical_(m)________________________________________ (zspi)________________________ -5.1400E+00 + Inner_plate_top,_radial_(m)_____________________________________________ (rplti)_______________________ 5.8656E+00 + Inner_plate_top,_vertical_(m)___________________________________________ (zplti)_______________________ -4.6725E+00 + Inner_plate_bottom,_radial_(m)__________________________________________ (rplbi)_______________________ 5.5109E+00 + Inner_plate_bottom,_vertical_(m)________________________________________ (zplbi)_______________________ -5.6075E+00 + Outer_strike_point,_radial_(m)__________________________________________ (rspo)________________________ 7.4223E+00 + Outer_strike_point,_vertical_(m)________________________________________ (zspo)________________________ -6.2291E+00 + Outer_plate_top,_radial_(m)_____________________________________________ (rplto)_______________________ 7.6496E+00 + Outer_plate_top,_vertical_(m)___________________________________________ (zplto)_______________________ -5.7838E+00 + Outer_plate_bottom,_radial_(m)__________________________________________ (rplbo)_______________________ 7.1949E+00 + Outer_plate_bottom,_vertical_(m)________________________________________ (zplbo)_______________________ -6.6744E+00 + Calculated_maximum_divertor_height_(m)__________________________________ (divht)_______________________ 2.0019E+00 + # TF coils # + Allowable_maximum_shear_stress_in_TF_coil_case_(Tresca_criterion)_(Pa)__ (sig_tf_case_max)_____________ 7.5000E+08 + Allowable_maximum_shear_stress_in_TF_coil_conduit_(Tresca_criterion)_(Pa (sig_tf_wp_max)_______________ 7.5000E+08 + WP_transverse_modulus_(GPa)_____________________________________________ (eyoung_wp_trans*1.0d-9)______ 4.3534E+01 OP + WP_vertical_modulus_(GPa)_______________________________________________ (eyoung_wp_axial*1.0d-9)______ 1.1510E+02 OP + WP_transverse_Poissons_ratio____________________________________________ (poisson_wp_trans)____________ 3.0390E-01 OP + WP_vertical-transverse_Pois._rat._______________________________________ (poisson_wp_axial)____________ 3.1568E-01 OP + Radial____stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_r_max(1))_____________ 4.8849E-08 + toroidal__stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_t_max(1))_____________ -4.8724E+08 + Vertical__stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_z_max(1))_____________ 2.6028E+08 + Von-Mises_stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_vmises_max(1))________ 6.5725E+08 + Maximum_shear_stress_for_the_Tresca_yield_criterion_1_(Pa)______________ (sig_tf_tresca_max(1))________ 7.4752E+08 + Radial____stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_r_max(2))_____________ -1.5411E+08 + toroidal__stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_t_max(2))_____________ -3.7861E+08 + Vertical__stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_z_max(2))_____________ 2.6028E+08 + Von-Mises_stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_vmises_max(2))________ 5.5645E+08 + Maximum_shear_stress_for_the_Tresca_yield_criterion_2_(Pa)______________ (sig_tf_tresca_max(2))________ 6.3889E+08 + Radial____stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_r_max(3))_____________ 6.1398E+06 + toroidal__stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_t_max(3))_____________ -3.6314E+08 + Vertical__stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_z_max(3))_____________ 1.4510E+08 + Von-Mises_stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_vmises_max(3))________ 4.5345E+08 + Maximum_shear_stress_for_the_Tresca_yield_criterion_3_(Pa)______________ (sig_tf_tresca_max(3))________ 5.0824E+08 + Maximum_radial_deflection_at_midplane_(m)_______________________________ (deflect)_____________________ -6.2714E-03 OP + Vertical_strain_on_casing_______________________________________________ (casestr)_____________________ 1.2697E-03 OP + Radial_strain_on_insulator______________________________________________ (insstrain)___________________ -7.6923E-03 OP + Conductor_technology____________________________________________________ (i_tf_sup)____________________ 1 + Superconductor_material_________________________________________________ (i_tf_sc_mat)_________________ 1 + Presence_of_TF_demountable_joints_______________________________________ (itart)_______________________ 0 + TF_inboard_leg_support_strategy_________________________________________ (i_tf_bucking)________________ 1 + Number_of_TF_coils______________________________________________________ (n_tf)________________________ 16 + Inboard_leg_centre_radius_(m)___________________________________________ (r_tf_inboard_mid)____________ 3.1673E+00 OP + Outboard_leg_centre_radius_(m)__________________________________________ (r_tf_outboard_mid)___________ 1.4985E+01 OP + Total_inboard_leg_radial_thickness_(m)__________________________________ (tfcth)_______________________ 9.1597E-01 ITV + Total_outboard_leg_radial_thickness_(m)_________________________________ (tfthko)______________________ 9.1597E-01 + Outboard_leg_toroidal_thickness_(m)_____________________________________ (tftort)______________________ 1.4145E+00 OP + Maximum_inboard_edge_height_(m)_________________________________________ (hmax)________________________ 8.8182E+00 OP + Mean_coil_circumference_(including_inboard_leg_length)_(m)______________ (tfleng)______________________ 4.7937E+01 OP + Vertical_TF_shape_______________________________________________________ (i_tf_shape)__________________ 1 + TF_coil_arc_point_0_R_(m)_______________________________________________ (xarc(1))_____________________ 3.6253E+00 + TF_coil_arc_point_0_Z_(m)_______________________________________________ (yarc(1))_____________________ 4.5506E+00 + TF_coil_arc_point_1_R_(m)_______________________________________________ (xarc(2))_____________________ 7.4667E+00 + TF_coil_arc_point_1_Z_(m)_______________________________________________ (yarc(2))_____________________ 7.5843E+00 + TF_coil_arc_point_2_R_(m)_______________________________________________ (xarc(3))_____________________ 1.4527E+01 + TF_coil_arc_point_2_Z_(m)_______________________________________________ (yarc(3))_____________________ 0.0000E+00 + TF_coil_arc_point_3_R_(m)_______________________________________________ (xarc(4))_____________________ 7.4667E+00 + TF_coil_arc_point_3_Z_(m)_______________________________________________ (yarc(4))_____________________ -8.8182E+00 + TF_coil_arc_point_4_R_(m)_______________________________________________ (xarc(5))_____________________ 3.6253E+00 + TF_coil_arc_point_4_Z_(m)_______________________________________________ (yarc(5))_____________________ -5.2909E+00 + TF_cross-section_(total)_(m2)___________________________________________ (tfareain)____________________ 1.8229E+01 + Total_steel_cross-section_(m2)__________________________________________ (a_tf_steel*n_tf)_____________ 1.2853E+01 + Total_steel_TF_fraction_________________________________________________ (f_tf_steel)__________________ 7.0508E-01 + Total_Insulation_cross-section_(total)_(m2)_____________________________ (a_tf_ins*n_tf)_______________ 8.4752E-01 + Total_Insulation_fraction_______________________________________________ (f_tf_ins)____________________ 4.6493E-02 + Casing_cross_section_area_(per_leg)_(m2)________________________________ (acasetf)_____________________ 5.6444E-01 + Inboard_leg_case_plasma_side_wall_thickness_(m)_________________________ (casthi)______________________ 6.0000E-02 + Inboard_leg_case_inboard_"nose"_thickness_(m)___________________________ (thkcas)______________________ 2.8216E-01 ITV + Inboard_leg_case_sidewall_thickness_at_its_narrowest_point_(m)__________ (casths)______________________ 5.0000E-02 + External_case_mass_per_coil_(kg)________________________________________ (whtcas)______________________ 5.5456E+05 OP + WP_cross_section_area_with_insulation_and_insertion_(per_coil)_(m2)_____ (awpc)________________________ 5.7486E-01 + WP_cross_section_area_(per_coil)_(m2)___________________________________ (aswp)________________________ 5.1696E-01 + Winding_pack_radial_thickness_(m)_______________________________________ (dr_tf_wp)____________________ 5.0416E-01 ITV + Winding_pack_toroidal_width_1_(m)_______________________________________ (wwp1)________________________ 1.1904E+00 OP + Winding_pack_toroidal_width_2_(m)_______________________________________ (wwp2)________________________ 1.0901E+00 OP + Ground_wall_insulation_thickness_(m)____________________________________ (tinstf)______________________ 8.0000E-03 + Winding_pack_insertion_gap_(m)__________________________________________ (tfinsgap)____________________ 1.0000E-02 + Steel_WP_cross-section_(total)_(m2)_____________________________________ (aswp*n_tf)___________________ 3.8217E+00 + Steel_WP_fraction_______________________________________________________ (aswp/awpc)___________________ 4.1550E-01 + Insulation_WP_fraction__________________________________________________ (aiwp/awpc)___________________ 4.7934E-02 + Cable_WP_fraction_______________________________________________________ ((awpc-aswp-aiwp)/awpc)_______ 5.3656E-01 + Turn_parametrisation____________________________________________________ (i_tf_turns_integer)__________ 0 + Number_of_turns_per_TF_coil_____________________________________________ (n_tf_turn)___________________ 1.4739E+02 OP + Width_of_turn_including_inter-turn_insulation_(m)_______________________ (t_turn_tf)___________________ 5.9223E-02 OP + Width_of_conductor_(square)_(m)_________________________________________ (t_conductor)_________________ 5.7623E-02 OP + Width_of_space_inside_conductor_(m)_____________________________________ (t_cable)_____________________ 4.1604E-02 OP + Steel_conduit_thickness_(m)_____________________________________________ (thwcndut)____________________ 8.0099E-03 ITV + Inter-turn_insulation_thickness_(m)_____________________________________ (thicndut)____________________ 8.0000E-04 + Diameter_of_central_helium_channel_in_cable_____________________________ (dhecoil)_____________________ 1.0000E-02 + internal_area_of_the_cable_space________________________________________ (acstf)_______________________ 1.6999E-03 + Coolant_fraction_in_conductor_excluding_central_channel_________________ (vftf)________________________ 3.0000E-01 + Copper_fraction_of_conductor____________________________________________ (fcutfsu)_____________________ 8.4212E-01 ITV + Superconductor_fraction_of_conductor____________________________________ (1-fcutfsu)___________________ 1.5788E-01 + Check_total_area_fractions_in_winding_pack_=_1__________________________ ______________________________ 1.0000E+00 + minimum_TF_conductor_temperature_margin__(K)____________________________ (tmargmin_tf)_________________ 1.5000E+00 + TF_conductor_temperature_margin_(K)_____________________________________ (tmargtf)_____________________ 1.5049E+00 + Elastic_properties_behavior_____________________________________________ (i_tf_cond_eyoung_axial)______ 0 + Conductor_axial_Youngs_modulus__________________________________________ (eyoung_cond_axial)___________ 0.0000E+00 + Conductor_transverse_Youngs_modulus_____________________________________ (eyoung_cond_trans)___________ 0.0000E+00 + Superconductor_mass_per_coil_(kg)_______________________________________ (whtconsc)____________________ 4.6964E+03 OP + Copper_mass_per_coil_(kg)_______________________________________________ (whtconcu)____________________ 5.8073E+04 OP + Steel_conduit_mass_per_coil_(kg)________________________________________ (whtconsh)____________________ 8.9310E+04 OP + Conduit_insulation_mass_per_coil_(kg)___________________________________ (whtconin)____________________ 2.3777E+03 OP + Total_conduit_mass_per_coil_(kg)________________________________________ (whtcon)______________________ 1.5446E+05 OP + Mass_of_each_TF_coil_(kg)_______________________________________________ (whttf/n_tf)__________________ 7.1402E+05 OP + Total_TF_coil_mass_(kg)_________________________________________________ (whttf)_______________________ 1.1424E+07 OP + Nominal_peak_field_assuming_toroidal_symmetry_(T)_______________________ (bmaxtf)______________________ 1.2178E+01 OP + Total_current_in_all_TF_coils_(MA)______________________________________ (ritfc/1.D6)__________________ 2.1176E+02 OP + TF_coil_current_(summed_over_all_coils)_(A)_____________________________ (ritfc)_______________________ 2.1176E+08 + Actual_peak_field_at_discrete_conductor_(T)_____________________________ (bmaxtfrp)____________________ 1.2636E+01 OP + Winding_pack_current_density_(A/m2)_____________________________________ (jwptf)_______________________ 2.5602E+07 OP + Inboard_leg_mid-plane_conductor_current_density_(A/m2)__________________ (oacdcp)______________________ 1.1617E+07 + Total_stored_energy_in_TF_coils_(GJ)____________________________________ (estotftgj)___________________ 1.2161E+02 OP + Inboard_vertical_tension_per_coil_(N)___________________________________ (vforce)______________________ 2.0908E+08 OP + Outboard_vertical_tension_per_coil_(N)__________________________________ (vforce_outboard)_____________ 2.0908E+08 OP + inboard_vertical_tension_fraction_(-)___________________________________ (f_vforce_inboard)____________ 5.0000E-01 OP + Centring_force_per_coil_(N/m)___________________________________________ (cforce)______________________ 8.0590E+07 OP + Max_allowed_tfcoil_variables.ripple_amplitude_at_plasma_outboard_midplan (ripmax)______________________ 6.0000E-01 + Ripple_amplitude_at_plasma_outboard_midplane_(%)________________________ (ripple)______________________ 6.0000E-01 OP + Actual_quench_time_(or_time_constant)_(s)_______________________________ (tdmptf)______________________ 1.8429E+01 ITV + Vacuum_Vessel_stress_on_quench_(Pa)_____________________________________ (vv_stress_quench)____________ 6.1442E+07 OP + Maximum_allowed_voltage_during_quench_due_to_insulation_(kV)____________ (vdalw)_______________________ 9.5837E+00 ITV + Actual_quench_voltage_(kV)______________________________________________ (vtfskv)______________________ 9.1862E+00 OP + Maximum_allowed_temp_rise_during_a_quench_(K)___________________________ (tmaxpro)_____________________ 1.5000E+02 + # Superconducting TF Coils # + Superconductor_switch___________________________________________________ (isumat)______________________ 1 + Critical_field_at_zero_temperature_and_strain_(T)_______________________ (bc20m)_______________________ 3.2970E+01 + Critical_temperature_at_zero_field_and_strain_(K)_______________________ (tc0m)________________________ 1.6060E+01 + Helium_temperature_at_peak_field_(=_superconductor_temperature)_(K)_____ (thelium)_____________________ 4.7500E+00 + Total_helium_fraction_inside_cable_space________________________________ (fhetot)______________________ 3.4620E-01 OP + Copper_fraction_of_conductor____________________________________________ (fcutfsu)_____________________ 8.4212E-01 ITV + Residual_manufacturing_strain_on_superconductor_________________________ (str_tf_con_res)______________ -5.0000E-03 + Self-consistent_strain_on_superconductor________________________________ (str_wp)______________________ 2.0730E-03 + Critical_current_density_in_superconductor_(A/m2)_______________________ (jcritsc)_____________________ 7.1337E+08 OP + Critical_current_density_in_strand_(A/m2)_______________________________ (jcritstr)____________________ 1.1263E+08 OP + Critical_current_density_in_winding_pack_(A/m2)_________________________ (jwdgcrt)_____________________ 3.5688E+07 OP + Actual_current_density_in_winding_pack_(A/m2)___________________________ (jwdgop)______________________ 2.5602E+07 OP + Minimum_allowed_temperature_margin_in_superconductor_(K)________________ (tmargmin_tf)_________________ 1.5000E+00 + Actual_temperature_margin_in_superconductor_(K)_________________________ (tmarg)_______________________ 1.5049E+00 OP + Critical_current_(A)____________________________________________________ (icrit)_______________________ 1.2517E+05 OP + Actual_current_(A)______________________________________________________ (cpttf)_______________________ 8.9795E+04 ITV + Actual_current_/_critical_current_______________________________________ (iooic)_______________________ 7.1737E-01 OP + # Central Solenoid and PF Coils # + Central_solenoid_superconductor_material________________________________ (isumatoh)____________________ 1 + Maximum_field_at_Beginning_Of_Pulse_(T)_________________________________ (bmaxoh0)_____________________ 1.4050E+01 OP + Critical_superconductor_current_density_at_BOP_(A/m2)___________________ (jscoh_bop)___________________ 3.4918E+08 OP + Critical_strand_current_density_at_BOP_(A/m2)___________________________ (jstrandoh_bop)_______________ 1.0475E+08 OP + Allowable_overall_current_density_at_BOP_(A/m2)_________________________ (rjohc0)______________________ 3.5294E+07 OP + Actual_overall_current_density_at_BOP_(A/m2)____________________________ (cohbop)______________________ 1.9126E+07 OP + Maximum_field_at_End_Of_Flattop_(T)_____________________________________ (bmaxoh)______________________ 1.3920E+01 OP + Critical_superconductor_current_density_at_EOF_(A/m2)___________________ (jscoh_eof)___________________ 3.6097E+08 OP + Critical_strand_current_density_at_EOF_(A/m2)___________________________ (jstrandoh_eof)_______________ 1.0829E+08 OP + Allowable_overall_current_density_at_EOF_(A/m2)_________________________ (rjohc)_______________________ 3.6485E+07 OP + Actual_overall_current_density_at_EOF_(A/m2)____________________________ (coheof)______________________ 2.0264E+07 ITV + CS_inside_radius_(m)____________________________________________________ (bore)________________________ 1.9854E+00 ITV + CS_thickness_(m)________________________________________________________ (ohcth)_______________________ 5.7587E-01 ITV + Gap_between_central_solenoid_and_TF_coil_(m)____________________________ (gapoh)_______________________ 8.0000E-02 + CS_overall_cross-sectional_area_(m2)____________________________________ (areaoh)______________________ 9.1407E+00 OP + CS_conductor+void_cross-sectional_area_(m2)_____________________________ (awpoh)_______________________ 4.3996E+00 OP + ___CS_conductor_cross-sectional_area_(m2)_______________________________ (awpoh*(1-vfohc))_____________ 3.0797E+00 OP + ___CS_void_cross-sectional_area_(m2)____________________________________ (awpoh*vfohc)_________________ 1.3199E+00 OP + CS_steel_cross-sectional_area_(m2)______________________________________ (areaoh-awpoh)________________ 4.7411E+00 OP + CS_steel_area_fraction__________________________________________________ (oh_steel_frac)_______________ 5.1868E-01 ITV + Switch_for_CS_stress_calculation________________________________________ (i_cs_stress)_________________ 0 + Allowable_stress_in_CS_steel_(Pa)_______________________________________ (alstroh)_____________________ 7.5000E+08 + Hoop_stress_in_CS_steel_(Pa)____________________________________________ (sig_hoop)____________________ 6.7569E+08 OP + Axial_stress_in_CS_steel_(Pa)___________________________________________ (sig_axial)___________________ -7.6205E+08 OP + Maximum_shear_stress_in_CS_steel_for_the_Tresca_criterion_(Pa)__________ (s_tresca_oh)_________________ 6.7569E+08 OP + Axial_force_in_CS_(N)___________________________________________________ (axial_force)_________________ -1.6256E+09 OP + Residual_manufacturing_strain_in_CS_superconductor_material_____________ (tfcoil_variables.str_cs_con_r -5.0000E-03 + Copper_fraction_in_strand_______________________________________________ (fcuohsu)_____________________ 7.0000E-01 + Void_(coolant)_fraction_in_conductor____________________________________ (vfohc)_______________________ 3.0000E-01 + Helium_coolant_temperature_(K)__________________________________________ (tftmp)_______________________ 4.7500E+00 + CS_temperature_margin_(K)_______________________________________________ (tmargoh)_____________________ 1.5052E+00 OP + Minimum_permitted_temperature_margin_(K)________________________________ (tmargmin_cs)_________________ 1.5000E+00 + Residual_hoop_stress_in_CS_Steel_(Pa)___________________________________ (residual_sig_hoop)___________ 2.4000E+08 + Minimum_burn_time_(s)___________________________________________________ (tbrnmn)______________________ 7.2000E+03 + Initial_vertical_crack_size_(m)_________________________________________ (t_crack_vertical)____________ 8.9000E-04 + Initial_radial_crack_size_(m)___________________________________________ (t_crack_radial)______________ 2.6700E-03 + CS_turn_area_(m)________________________________________________________ (a_oh_turn)___________________ 1.9739E-03 + CS_turn_length_(m)______________________________________________________ (l_cond_cst)__________________ 7.6953E-02 + CS_turn_internal_cable_space_radius_(m)_________________________________ (r_in_cst)____________________ 7.4740E-03 + CS_turn_width_(m)_______________________________________________________ (d_cond_cst)__________________ 2.5651E-02 + CS_structural_vertical_thickness_(m)____________________________________ (t_structural_vertical)_______ 5.3514E-03 + CS_structural_radial_thickness_(m)______________________________________ (t_structural_radial)_________ 5.3514E-03 + Allowable_number_of_cycles_till_CS_fracture_____________________________ (n_cycle)_____________________ 1.3378E+02 OP + Minimum_number_of_cycles_required_till_CS_fracture______________________ (n_cycle_min)_________________ 2.0000E+04 OP + PF_coil_superconductor_material_________________________________________ (isumatpf)____________________ 3 + Copper_fraction_in_conductor____________________________________________ (fcupfsu)_____________________ 6.9000E-01 + Maximum_permissible_tensile_stress_(MPa)________________________________ (sigpfcalw)___________________ 5.0000E+02 + JxB_hoop_force_fraction_supported_by_case_______________________________ (sigpfcf)_____________________ 6.6600E-01 + PF_coil_0_radius_(m)____________________________________________________ (rpf[0]_______________________ 5.5667E+00 + PF_coil_0_vertical_position_(m)_________________________________________ (zpf[0])______________________ 9.3603E+00 + PF_coil_0_radial_thickness_(m)__________________________________________ (pfdr(0))_____________________ 1.2727E+00 + PF_coil_0_vertical_thickness_(m)________________________________________ (pfdz(0))_____________________ 1.2727E+00 + PF_coil_0_turns_________________________________________________________ (turns[0])____________________ 4.4541E+02 + PF_coil_0_current_(MA)__________________________________________________ (ric[0])______________________ 1.7816E+01 + PF_coil_0_field_(T)_____________________________________________________ (bpf[0])______________________ 6.2280E+00 + PF_coil_1_radius_(m)____________________________________________________ (rpf[1]_______________________ 5.5667E+00 + PF_coil_1_vertical_position_(m)_________________________________________ (zpf[1])______________________ -1.0594E+01 + PF_coil_1_radial_thickness_(m)__________________________________________ (pfdr(1))_____________________ 1.3651E+00 + PF_coil_1_vertical_thickness_(m)________________________________________ (pfdz(1))_____________________ -1.3651E+00 + PF_coil_1_turns_________________________________________________________ (turns[1])____________________ 5.1248E+02 + PF_coil_1_current_(MA)__________________________________________________ (ric[1])______________________ 2.0499E+01 + PF_coil_1_field_(T)_____________________________________________________ (bpf[1])______________________ 6.6990E+00 + PF_coil_2_radius_(m)____________________________________________________ (rpf[2]_______________________ 1.6731E+01 + PF_coil_2_vertical_position_(m)_________________________________________ (zpf[2])______________________ 2.6667E+00 + PF_coil_2_radial_thickness_(m)__________________________________________ (pfdr(2))_____________________ 1.1332E+00 + PF_coil_2_vertical_thickness_(m)________________________________________ (pfdz(2))_____________________ 1.1332E+00 + PF_coil_2_turns_________________________________________________________ (turns[2])____________________ 1.9262E+02 + PF_coil_2_current_(MA)__________________________________________________ (ric[2])______________________ -7.7049E+00 + PF_coil_2_field_(T)_____________________________________________________ (bpf[2])______________________ 2.6389E+00 + PF_coil_3_radius_(m)____________________________________________________ (rpf[3]_______________________ 1.6731E+01 + PF_coil_3_vertical_position_(m)_________________________________________ (zpf[3])______________________ -2.6667E+00 + PF_coil_3_radial_thickness_(m)__________________________________________ (pfdr(3))_____________________ 1.1332E+00 + PF_coil_3_vertical_thickness_(m)________________________________________ (pfdz(3))_____________________ -1.1332E+00 + PF_coil_3_turns_________________________________________________________ (turns[3])____________________ 1.9262E+02 + PF_coil_3_current_(MA)__________________________________________________ (ric[3])______________________ -7.7049E+00 + PF_coil_3_field_(T)_____________________________________________________ (bpf[3])______________________ 2.6389E+00 + PF_coil_4_radius_(m)____________________________________________________ (rpf[4]_______________________ 1.5209E+01 + PF_coil_4_vertical_position_(m)_________________________________________ (zpf[4])______________________ 7.4667E+00 + PF_coil_4_radial_thickness_(m)__________________________________________ (pfdr(4))_____________________ 8.0773E-01 + PF_coil_4_vertical_thickness_(m)________________________________________ (pfdz(4))_____________________ 8.0773E-01 + PF_coil_4_turns_________________________________________________________ (turns[4])____________________ 1.3049E+02 + PF_coil_4_current_(MA)__________________________________________________ (ric[4])______________________ -5.2194E+00 + PF_coil_4_field_(T)_____________________________________________________ (bpf[4])______________________ 2.5737E+00 + PF_coil_5_radius_(m)____________________________________________________ (rpf[5]_______________________ 1.5209E+01 + PF_coil_5_vertical_position_(m)_________________________________________ (zpf[5])______________________ -7.4667E+00 + PF_coil_5_radial_thickness_(m)__________________________________________ (pfdr(5))_____________________ 8.0773E-01 + PF_coil_5_vertical_thickness_(m)________________________________________ (pfdz(5))_____________________ -8.0773E-01 + PF_coil_5_turns_________________________________________________________ (turns[5])____________________ 1.3049E+02 + PF_coil_5_current_(MA)__________________________________________________ (ric[5])______________________ -5.2194E+00 + PF_coil_5_field_(T)_____________________________________________________ (bpf[5])______________________ 2.5737E+00 + Central_solenoid_radius_(m)_____________________________________________ (rpf[nohc-1])_________________ 2.2734E+00 + Central_solenoid_vertical_position_(m)__________________________________ (zpf[nohc-1])_________________ 0.0000E+00 + Central_solenoid_radial_thickness_(m)___________________________________ (ohdr)________________________ 5.7587E-01 + Central_solenoid_vertical_thickness_(m)_________________________________ (ohdz)________________________ 1.5873E+01 + Central_solenoid_turns__________________________________________________ (turns[nohc-1])_______________ 4.6308E+03 + Central_solenoid_current_(MA)___________________________________________ (ric[nohc-1])_________________ -1.8523E+02 + Central_solenoid_field_(T)______________________________________________ (bpf[nohc-1])_________________ 1.4050E+01 + Sum_of_squares_of_residuals_____________________________________________ (ssq0)________________________ 3.5207E-04 OP + Smoothing_parameter_____________________________________________________ (alfapf)______________________ 5.0000E-10 + # Volt Second Consumption # + Total_volt-second_consumption_by_coils_(Wb)_____________________________ (vstot)_______________________ -5.8000E+02 OP + # Waveforms # + Ratio_of_central_solenoid_current_at_beginning_of_Pulse_/_end_of_flat-to (fcohbop)_____________________ 9.4380E-01 ITV + Ratio_of_central_solenoid_current_at_beginning_of_Flat-top_/_end_of_flat (fcohbof)_____________________ -1.4083E-01 OP + # PF Circuit Waveform Data # + Number_of_PF_circuits_including_CS_and_plasma___________________________ (ncirt)_______________________ 8 + PF_Circuit_0_Time_point_0_(A)___________________________________________ (pfc0t0)______________________ 0.0000E+00 + PF_Circuit_0_Time_point_1_(A)___________________________________________ (pfc0t1)______________________ 1.3971E+07 + PF_Circuit_0_Time_point_2_(A)___________________________________________ (pfc0t2)______________________ 1.7816E+07 + PF_Circuit_0_Time_point_3_(A)___________________________________________ (pfc0t3)______________________ 1.7816E+07 + PF_Circuit_0_Time_point_4_(A)___________________________________________ (pfc0t4)______________________ 9.2844E+05 + PF_Circuit_0_Time_point_5_(A)___________________________________________ (pfc0t5)______________________ 0.0000E+00 + PF_Circuit_1_Time_point_0_(A)___________________________________________ (pfc1t0)______________________ 0.0000E+00 + PF_Circuit_1_Time_point_1_(A)___________________________________________ (pfc1t1)______________________ 1.8269E+07 + PF_Circuit_1_Time_point_2_(A)___________________________________________ (pfc1t2)______________________ 2.0499E+07 + PF_Circuit_1_Time_point_3_(A)___________________________________________ (pfc1t3)______________________ 2.0499E+07 + PF_Circuit_1_Time_point_4_(A)___________________________________________ (pfc1t4)______________________ -1.5831E+06 + PF_Circuit_1_Time_point_5_(A)___________________________________________ (pfc1t5)______________________ 0.0000E+00 + PF_Circuit_2_Time_point_0_(A)___________________________________________ (pfc2t0)______________________ -0.0000E+00 + PF_Circuit_2_Time_point_1_(A)___________________________________________ (pfc2t1)______________________ 4.9542E+05 + PF_Circuit_2_Time_point_2_(A)___________________________________________ (pfc2t2)______________________ -7.1060E+06 + PF_Circuit_2_Time_point_3_(A)___________________________________________ (pfc2t3)______________________ -7.1060E+06 + PF_Circuit_2_Time_point_4_(A)___________________________________________ (pfc2t4)______________________ -7.7049E+06 + PF_Circuit_2_Time_point_5_(A)___________________________________________ (pfc2t5)______________________ -0.0000E+00 + PF_Circuit_3_Time_point_0_(A)___________________________________________ (pfc3t0)______________________ -0.0000E+00 + PF_Circuit_3_Time_point_1_(A)___________________________________________ (pfc3t1)______________________ 4.9542E+05 + PF_Circuit_3_Time_point_2_(A)___________________________________________ (pfc3t2)______________________ -7.1060E+06 + PF_Circuit_3_Time_point_3_(A)___________________________________________ (pfc3t3)______________________ -7.1060E+06 + PF_Circuit_3_Time_point_4_(A)___________________________________________ (pfc3t4)______________________ -7.7049E+06 + PF_Circuit_3_Time_point_5_(A)___________________________________________ (pfc3t5)______________________ -0.0000E+00 + PF_Circuit_4_Time_point_0_(A)___________________________________________ (pfc4t0)______________________ -0.0000E+00 + PF_Circuit_4_Time_point_1_(A)___________________________________________ (pfc4t1)______________________ 3.2650E+05 + PF_Circuit_4_Time_point_2_(A)___________________________________________ (pfc4t2)______________________ -4.8247E+06 + PF_Circuit_4_Time_point_3_(A)___________________________________________ (pfc4t3)______________________ -4.8247E+06 + PF_Circuit_4_Time_point_4_(A)___________________________________________ (pfc4t4)______________________ -5.2194E+06 + PF_Circuit_4_Time_point_5_(A)___________________________________________ (pfc4t5)______________________ -0.0000E+00 + PF_Circuit_5_Time_point_0_(A)___________________________________________ (pfc5t0)______________________ -0.0000E+00 + PF_Circuit_5_Time_point_1_(A)___________________________________________ (pfc5t1)______________________ 3.2650E+05 + PF_Circuit_5_Time_point_2_(A)___________________________________________ (pfc5t2)______________________ -4.8247E+06 + PF_Circuit_5_Time_point_3_(A)___________________________________________ (pfc5t3)______________________ -4.8247E+06 + PF_Circuit_5_Time_point_4_(A)___________________________________________ (pfc5t4)______________________ -5.2194E+06 + PF_Circuit_5_Time_point_5_(A)___________________________________________ (pfc5t5)______________________ -0.0000E+00 + CS_Circuit_Time_point_0_(A)_____________________________________________ (cs_t0)_______________________ -0.0000E+00 + CS_Circuit_Time_point_1_(A)_____________________________________________ (cs_t1)_______________________ 1.7482E+08 + CS_Circuit_Time_point_2_(A)_____________________________________________ (cs_t2)_______________________ 2.6086E+07 + CS_Circuit_Time_point_3_(A)_____________________________________________ (cs_t3)_______________________ 2.6086E+07 + CS_Circuit_Time_point_4_(A)_____________________________________________ (cs_t4)_______________________ -1.8523E+08 + CS_Circuit_Time_point_5_(A)_____________________________________________ (cs_t5)_______________________ -0.0000E+00 + Plasma_Time_point_0_(A)_________________________________________________ (plasmat0)____________________ 0.0000E+00 + Plasma_Time_point_1_(A)_________________________________________________ (plasmat1)____________________ 0.0000E+00 + Plasma_Time_point_2_(A)_________________________________________________ (plasmat2)____________________ 1.6631E+07 + Plasma_Time_point_3_(A)_________________________________________________ (plasmat3)____________________ 1.6631E+07 + Plasma_Time_point_4_(A)_________________________________________________ (plasmat4)____________________ 1.6631E+07 + Plasma_Time_point_5_(A)_________________________________________________ (plasmat5)____________________ 0.0000E+00 + # Support Structure # + Outer_PF_coil_fence_mass_(kg)___________________________________________ (fncmass)_____________________ 2.2924E+05 OP + Intercoil_support_structure_mass_(kg)___________________________________ (aintmass)____________________ 4.3045E+06 OP + Mass_of_cooled_components_(kg)__________________________________________ (coldmass)____________________ 3.4369E+07 OP + Gravity_support_structure_mass_(kg)_____________________________________ (clgsmass)____________________ 1.2760E+06 OP + Torus_leg_support_mass_(kg)_____________________________________________ (gsm1)________________________ 8.5820E+04 OP + Ring_beam_mass_(kg)_____________________________________________________ (gsm2)________________________ 4.0088E+05 OP + Ring_legs_mass_(kg)_____________________________________________________ (gsm3)________________________ 6.8283E+05 OP + # PF Coil Inductances # + # Nuclear Heating Magnets Before Renormalisation # + Shield_line_density_(tonne/m2)__________________________________________ (x_shield)____________________ 4.0560E+00 + Blanket_line_density_(tonne/m2)_________________________________________ (x_blanket)___________________ 2.2911E+00 + Unit_nuclear_heating_in_TF_coil_(W/GW)__________________________________ (tfc_nuc_heating)_____________ 1.4866E+04 + Total_nuclear_heating_in_TF_coil_(MW)___________________________________ (ptfnuc.)_____________________ 2.4085E-02 + powfmw__________________________________________________________________ (powfmw.)_____________________ 1.6202E+03 + total_mass_of_the_TF_coils_(kg)_________________________________________ (whttf)_______________________ 1.1424E+07 + # Pumping for primary coolant (helium) # + Pressure_drop_in_FW_and_blanket_coolant_incl._hx_and_pipes_(Pa)_________ (dp_he)_______________________ 5.5000E+05 + Fraction_of_FW_and_blanket_thermal_power_required_for_pumping___________ (fpump)_______________________ 8.9463E-02 OP + Total_power_absorbed_by_FW_&_blanket_(MW)_______________________________ (p_plasma)____________________ 1.6698E+03 OP + Inlet_temperature_of_FW_&_blanket_coolant_pump_(K)______________________ (t_in_compressor)_____________ 5.5703E+02 OP + Coolant_pump_outlet/Inlet_temperature_of_FW_&_blanket_(K)_______________ (t_in_bb)_____________________ 5.7313E+02 + Outlet_temperature_of_FW_&_blanket_(K)__________________________________ (t_out_bb)____________________ 7.7313E+02 + Mechanical_pumping_power_for_FW_and_blanket_cooling_loop_including_heat_ (htpmw_fw_blkt)_______________ 1.6407E+02 OP + Mechanical_pumping_power_for_divertor_(MW)______________________________ (htpmw_div)___________________ 1.6906E+00 OP + Mechanical_pumping_power_for_shield_and_vacuum_vessel_(MW)______________ (htpmw_shld)__________________ 7.0688E-03 OP + # First wall and blanket : CCFE HCPB model # + Titanium_beryllide_fraction_____________________________________________ (fbltibe12)___________________ 3.7500E-01 + Lithium_orthosilicate_fraction__________________________________________ (fblli2sio4)__________________ 3.7500E-01 + Steel_fraction__________________________________________________________ (fblss_ccfe)__________________ 9.7050E-02 + Coolant_fraction________________________________________________________ (vfcblkt)_____________________ 5.2950E-02 + Purge_gas_fraction______________________________________________________ (vfpblkt)_____________________ 1.0000E-01 + First_Wall_Armour_Volume_(m3)___________________________________________ (fw_armour_vol)_______________ 5.8692E+00 + First_Wall_Volume_(m3)__________________________________________________ (volfw)_______________________ 1.9807E+01 + Blanket_Volume_(m3)_____________________________________________________ (volblkt)_____________________ 1.1849E+03 + Shield_Volume_(m3)______________________________________________________ (volshld)_____________________ 7.8520E+02 + Vacuum_vessel_volume_(m3)_______________________________________________ (vdewin)______________________ 1.0178E+03 + First_Wall_Armour_Mass_(kg)_____________________________________________ (fw_armour_mass)______________ 1.1298E+05 OP + First_Wall_Mass,_excluding_armour_(kg)__________________________________ (fwmass)______________________ 1.5449E+05 OP + Blanket_Mass_-_Total(kg)________________________________________________ (whtblkt)_____________________ 2.9676E+06 OP + ____Blanket_Mass_-_TiBe12_(kg)__________________________________________ (whtbltibe12)_________________ 1.0042E+06 OP + ____Blanket_Mass_-_Li4SiO4_(kg)_________________________________________ (whtblli4sio4)________________ 1.0664E+06 OP + ____Blanket_Mass_-_Steel_(kg)___________________________________________ (whtblss)_____________________ 8.9696E+05 OP + Total_mass_of_armour,_first_wall_and_blanket_(kg)_______________________ (armour_fw_bl_mass)___________ 3.2350E+06 OP + Shield_Mass_(kg)________________________________________________________ (whtshld)_____________________ 2.4498E+06 OP + Vacuum_vessel_mass_(kg)_________________________________________________ (vvmass)______________________ 7.9388E+06 OP + Total_nuclear_heating_in_TF+PF_coils_(CS_is_negligible)_(MW)____________ (ptfnuc)______________________ 2.5118E-02 OP + Total_nuclear_heating_in_FW_(MW)________________________________________ (pnucfw)______________________ 1.6315E+02 OP + Total_nuclear_heating_in_the_blanket_(including_emult)_(MW)_____________ (pnucblkt)____________________ 1.2901E+03 OP + Total_nuclear_heating_in_the_shield_(MW)________________________________ (pnucshld)____________________ 1.4138E+00 OP + Total_nuclear_heating_in_the_divertor_(MW)______________________________ (pnucdiv)_____________________ 1.4906E+02 OP + Blanket_exponential_factor______________________________________________ (exp_blanket)_________________ 9.9936E-01 OP + Shield:_first_exponential_______________________________________________ (exp_shield1)_________________ 1.9523E-03 OP + Shield:_second_exponential______________________________________________ (exp_shield2)_________________ 2.5427E-01 OP + Solid_angle_fraction_taken_by_on_divertor_______________________________ (fdiv)________________________ 1.1500E-01 + Switch_for_plant_secondary_cycle________________________________________ (secondary_cycle)_____________ 2 + First_wall_coolant_pressure_(Pa)________________________________________ (fwpressure)__________________ 1.5500E+07 + Blanket_coolant_pressure_(Pa)___________________________________________ (blpressure)__________________ 1.5500E+07 + Allowable_nominal_neutron_fluence_at_first_wall_(MW.year/m2)____________ (abktflnc)____________________ 5.0000E+00 + No_of_inboard_blanket_modules_poloidally________________________________ (nblktmodpi)__________________ 7 + No_of_inboard_blanket_modules_toroidally________________________________ (nblktmodti)__________________ 32 + No_of_outboard_blanket_modules_poloidally_______________________________ (nblktmodpo)__________________ 8 + No_of_outboard_blanket_modules_toroidally_______________________________ (nblktmodto)__________________ 48 + Isentropic_efficiency_of_first_wall_/_blanket_coolant_pumps_____________ (etaiso)______________________ 9.0000E-01 + First_wall_area_(m2)____________________________________________________ (fwarea)______________________ 1.6044E+03 OP + Cryostat_internal_radius_(m)____________________________________________ (rdewex)______________________ 1.7798E+01 OP + Cryostat_internal_half-height_(m)_______________________________________ (zdewex)______________________ 1.5339E+01 OP + Vertical_clearance_from_TF_coil_to_cryostat_(m)_________________________ (clh1)________________________ 5.6044E+00 OP + Divertor_area_(m2)______________________________________________________ (divsur)______________________ 1.4879E+02 OP + Divertor_mass_(kg)______________________________________________________ (divmas)______________________ 3.6453E+04 OP + # Superconducting TF Coil Power Conversion # + TF_coil_current_(kA)____________________________________________________ (itfka)_______________________ 8.9795E+01 OP + Number_of_TF_coils______________________________________________________ (ntfc)________________________ 1.6000E+01 + Voltage_across_a_TF_coil_during_quench_(kV)_____________________________ (vtfskv)______________________ 9.1862E+00 OP + TF_coil_charge_time_(hours)_____________________________________________ (tchghr)______________________ 4.0000E+00 + Total_inductance_of_TF_coils_(H)________________________________________ (ltfth)_______________________ 3.0165E+01 OP + Total_resistance_of_TF_coils_(ohm)______________________________________ (rcoils)______________________ 0.0000E+00 OP + TF_coil_charging_voltage_(V)____________________________________________ (tfcv)________________________ 2.9268E+02 + Number_of_DC_circuit_breakers___________________________________________ (ntfbkr)______________________ 1.6000E+01 + Number_of_dump_resistors________________________________________________ (ndumpr)______________________ 6.4000E+01 + Resistance_per_dump_resistor_(ohm)______________________________________ (r1dump)______________________ 1.0230E-01 OP + Dump_resistor_peak_power_(MW)___________________________________________ (r1ppmw)______________________ 2.0622E+02 OP + Energy_supplied_per_dump_resistor_(MJ)__________________________________ (r1emj)_______________________ 1.9002E+03 OP + TF_coil_L/R_time_constant_(s)___________________________________________ (ttfsec)______________________ 1.8429E+01 OP + Power_supply_voltage_(V)________________________________________________ (tfpsv)_______________________ 3.0731E+02 OP + Power_supply_current_(kA)_______________________________________________ (tfpska)______________________ 9.4285E+01 OP + DC_power_supply_rating_(kW)_____________________________________________ (tfckw)_______________________ 2.8975E+04 OP + AC_power_for_charging_(kW)______________________________________________ (tfackw)______________________ 3.2194E+04 OP + TF_coil_resistive_power_(MW)____________________________________________ (rpower)______________________ 9.3902E+00 OP + TF_coil_inductive_power_(MVA)___________________________________________ (xpower)______________________ 1.6891E+01 OP + Aluminium_bus_current_density_(kA/cm2)__________________________________ (djmka)_______________________ 1.2500E-01 + Aluminium_bus_cross-sectional_area_(cm2)________________________________ (albusa)______________________ 7.1836E+02 OP + Total_length_of_TF_coil_bussing_(m)_____________________________________ (tfbusl)______________________ 3.1931E+03 OP + Aluminium_bus_weight_(tonnes)___________________________________________ (albuswt)_____________________ 6.1932E+02 OP + Total_TF_coil_bus_resistance_(ohm)______________________________________ (rtfbus)______________________ 1.1646E-03 OP + TF_coil_bus_voltage_drop_(V)____________________________________________ (vtfbus)______________________ 1.0457E+02 OP + Dump_resistor_floor_area_(m2)___________________________________________ (drarea)______________________ 4.9234E+03 OP + TF_coil_power_conversion_floor_space_(m2)_______________________________ (tfcfsp)______________________ 1.8228E+03 OP + TF_coil_power_conv._building_volume_(m3)________________________________ (tfcbv)_______________________ 1.0937E+04 OP + TF_coil_AC_inductive_power_demand_(MW)__________________________________ (xpwrmw)______________________ 1.8768E+01 OP + Total_steady_state_AC_power_demand_(MW)_________________________________ (tfacpd)______________________ 1.0434E+01 OP + # PF Coils and Central Solenoid: Power and Energy # + Number_of_PF_coil_circuits______________________________________________ (pfckts)______________________ 1.2000E+01 + Sum_of_PF_power_supply_ratings_(MVA)____________________________________ (spsmva)______________________ 3.0313E+02 OP + Total_PF_coil_circuit_bus_length_(m)____________________________________ (spfbusl)_____________________ 2.4480E+03 OP + Total_PF_coil_bus_resistive_power_(kW)__________________________________ (pfbuspwr)____________________ 9.6485E+02 OP + Total_PF_coil_resistive_power_(kW)______________________________________ (srcktpm)_____________________ 9.6485E+02 OP + Maximum_PF_coil_voltage_(kV)____________________________________________ (vpfskv)______________________ 2.0000E+01 + Efficiency_of_transfer_of_PF_stored_energy_into_or_out_of_storage_______ (etapsu)______________________ 9.0000E-01 + Maximum_stored_energy_in_poloidal_field_(MJ)____________________________ (ensxpfm)_____________________ 2.8804E+04 OP + Peak_absolute_rate_of_change_of_stored_energy_in_poloidal_field_(MW)____ (peakpoloidalpower)___________ 1.7319E+02 OP + # Vacuum System # + First_wall_outgassing_rate_(Pa_m/s)_____________________________________ (rat)_________________________ 1.3000E-08 + Total_outgassing_load_(Pa_m3/s)_________________________________________ (ogas)________________________ 1.6691E-04 OP + Base_pressure_required_(Pa)_____________________________________________ (pbase)_______________________ 5.0000E-04 + Required_N2_pump_speed_(m3/s)___________________________________________ (s(1))________________________ 3.3381E-01 OP + N2_pump_speed_provided_(m3/s)___________________________________________ (snet(1))_____________________ 2.3404E+01 OP + Plasma_chamber_volume_(m3)______________________________________________ (volume)______________________ 2.2588E+03 OP + Chamber_pressure_after_burn_(Pa)________________________________________ (pend)________________________ 1.6698E-01 OP + Chamber_pressure_before_burn_(Pa)_______________________________________ (pstart)______________________ 1.6698E-03 + Allowable_pumping_time_switch___________________________________________ (dwell_pump)__________________ 0 + Dwell_time_between_burns_(s)____________________________________________ (tdwell.)_____________________ 1.8000E+03 + CS_ramp-up_time_burns_(s)_______________________________________________ (tramp.)______________________ 5.0000E+02 + Allowable_pumping_time_between_burns_(s)________________________________ (tpump)_______________________ 1.8000E+03 + Required_D-T_pump_speed_(m3/s)__________________________________________ (s(2))________________________ 5.7790E+00 OP + D-T_pump_speed_provided_(m3/s)__________________________________________ (snet(2))_____________________ 5.6700E+01 OP + Divertor_chamber_gas_pressure_(Pa)______________________________________ (prdiv)_______________________ 3.6000E-01 + Helium_gas_fraction_in_divertor_chamber_________________________________ (fhe)_________________________ 1.7218E-01 OP + Required_helium_pump_speed_(m3/s)_______________________________________ (s(3))________________________ 3.8423E+01 OP + Helium_pump_speed_provided_(m3/s)_______________________________________ (snet(3))_____________________ 3.8423E+01 OP + D-T_fuelling_rate_(kg/s)________________________________________________ (frate)_______________________ 2.7747E-05 OP + Required_D-T_pump_speed_(m3/s)__________________________________________ (s(4))________________________ 3.8423E+01 OP + D-T_pump_speed_provided_(m3/s)__________________________________________ (snet(4))_____________________ 5.6700E+01 OP + Number_of_large_pump_ducts______________________________________________ (nduct)_______________________ 16 + Passage_diameter,_divertor_to_ducts_(m)_________________________________ (d(imax))_____________________ 4.7857E-01 OP + Passage_length_(m)______________________________________________________ (l1)__________________________ 1.7160E+00 OP + Diameter_of_ducts_(m)___________________________________________________ (dout)________________________ 5.7428E-01 OP + Duct_length,_divertor_to_elbow_(m)______________________________________ (l2)__________________________ 4.8000E+00 OP + Duct_length,_elbow_to_pumps_(m)_________________________________________ (l3)__________________________ 2.0000E+00 + Number_of_pumps_________________________________________________________ (pumpn)_______________________ 3.2000E+01 OP + # Plant Buildings System # + Internal_volume_of_reactor_building_(m3)________________________________ (vrci)________________________ 9.9708E+05 + Dist_from_centre_of_torus_to_bldg_wall_(m)______________________________ (wrbi)________________________ 3.9531E+01 + Effective_floor_area_(m2)_______________________________________________ (efloor)______________________ 3.3660E+05 + Reactor_building_volume_(m3)____________________________________________ (rbv)_________________________ 1.1310E+06 + Reactor_maintenance_building_volume_(m3)________________________________ (rmbv)________________________ 3.9641E+05 + Warmshop_volume_(m3)____________________________________________________ (wsv)_________________________ 1.2531E+05 + Tritium_building_volume_(m3)____________________________________________ (triv)________________________ 4.0000E+04 + Electrical_building_volume_(m3)_________________________________________ (elev)________________________ 5.1937E+04 + Control_building_volume_(m3)____________________________________________ (conv)________________________ 6.0000E+04 + Cryogenics_building_volume_(m3)_________________________________________ (cryv)________________________ 1.4976E+04 + Administration_building_volume_(m3)_____________________________________ (admv)________________________ 1.0000E+05 + Shops_volume_(m3)_______________________________________________________ (shov)________________________ 1.0000E+05 + Total_volume_of_nuclear_buildings_(m3)__________________________________ (volnucb)_____________________ 1.5738E+06 + # Electric Power Requirements # + Facility_base_load_(MW)_________________________________________________ (basemw)______________________ 5.0000E+00 + Divertor_coil_power_supplies_(MW)_______________________________________ (bdvmw)_______________________ 0.0000E+00 + Cryoplant_electric_power_(MW)___________________________________________ (crymw)_______________________ 3.6566E+01 OP + Primary_coolant_pumps_(MW)______________________________________________ (htpmw..)_____________________ 1.9053E+02 OP + PF_coil_power_supplies_(MW)_____________________________________________ (ppfmw)_______________________ 8.5511E+01 OP + TF_coil_power_supplies_(MW)_____________________________________________ (ptfmw)_______________________ 1.0434E+01 OP + Plasma_heating_supplies_(MW)____________________________________________ (pheatingmw)__________________ 1.6029E+02 OP + Tritium_processing_(MW)_________________________________________________ (trithtmw..)__________________ 1.5000E+01 + Vacuum_pumps__(MW)______________________________________________________ (vachtmw..)___________________ 5.0000E-01 + Total_pulsed_power_(MW)_________________________________________________ (pacpmw)______________________ 5.5432E+02 OP + Total_base_power_required_at_all_times_(MW)_____________________________ (fcsht)_______________________ 5.5490E+01 OP + # Cryogenics # + Conduction_and_radiation_heat_loads_on_cryogenic_components_(MW)________ (qss/1.0d6)___________________ 1.4779E-02 OP + Nuclear_heating_of_cryogenic_components_(MW)____________________________ (qnuc/1.0d6)__________________ 1.3000E-02 OP + AC_losses_in_cryogenic_components_(MW)__________________________________ (qac/1.0d6)___________________ 3.8170E-03 OP + Resistive_losses_in_current_leads_(MW)__________________________________ (qcl/1.0d6)___________________ 1.9539E-02 OP + 45%_allowance_for_heat_loads_in_transfer_lines,_storage_tanks_etc_(MW)__ (qmisc/1.0d6)_________________ 2.3011E-02 OP + Sum_=_Total_heat_removal_at_cryogenic_temperatures_(tfcoil_variables.tmp (helpow_+_helpow_cryal/1.0d6)_ 7.4146E-02 OP + Temperature_of_cryogenic_superconducting_components_(K)_________________ (tmpcry)______________________ 4.5000E+00 + Temperature_of_cryogenic_aluminium_components_(K)_______________________ (tcoolin)_____________________ 3.1315E+02 + Efficiency_(figure_of_merit)_of_cryogenic_plant_is_13%_of_ideal_Carnot_v ______________________________ 2.0277E-03 OP + Efficiency_(figure_of_merit)_of_cryogenic_aluminium_plant_is_40%_of_idea ______________________________ -2.0203E+00 OP + Electric_power_for_cryogenic_plant_(MW)_________________________________ (crypmw)______________________ 3.6566E+01 OP + # Plant Power / Heat Transport Balance # + Neutron_power_multiplication_in_blanket_________________________________ (emult)_______________________ 1.2690E+00 + Divertor_area_fraction_of_whole_toroid_surface__________________________ (fdiv)________________________ 1.1500E-01 + H/CD_apparatus_+_diagnostics_area_fraction______________________________ (fhcd)________________________ 0.0000E+00 + First_wall_area_fraction________________________________________________ (1-fdiv-fhcd)_________________ 8.8500E-01 + Switch_for_pumping_of_primary_coolant___________________________________ (primary_pumping)_____________ 3 + Mechanical_pumping_power_for_FW_cooling_loop_including_heat_exchanger_(M (htpmw_fw)____________________ 0.0000E+00 OP + Mechanical_pumping_power_for_blanket_cooling_loop_including_heat_exchang (htpmw_blkt)__________________ 0.0000E+00 OP + Mechanical_pumping_power_for_FW_and_blanket_cooling_loop_including_heat_ (htpmw_fw_blkt)_______________ 1.6407E+02 OP + Mechanical_pumping_power_for_divertor_(MW)______________________________ (htpmw_div)___________________ 1.6906E+00 OP + Mechanical_pumping_power_for_shield_and_vacuum_vessel_(MW)______________ (htpmw_shld)__________________ 7.0688E-03 OP + Electrical_pumping_power_for_FW_and_blanket_(MW)________________________ (htpmwe_fw_blkt)______________ 1.8858E+02 OP + Electrical_pumping_power_for_shield_(MW)________________________________ (htpmwe_shld)_________________ 8.1250E-03 OP + Electrical_pumping_power_for_divertor_(MW)______________________________ (htpmwe_div)__________________ 1.9433E+00 OP + Total_electrical_pumping_power_for_primary_coolant_(MW)_________________ (htpmw)_______________________ 1.9053E+02 OP + Coolant_pump_power_/_non-pumping_thermal_power_in_shield________________ (fpumpshld)___________________ 5.0000E-03 + Coolant_pump_power_/_non-pumping_thermal_power_in_divertor______________ (fpumpdiv)____________________ 5.0000E-03 + Electrical_efficiency_of_heat_transport_coolant_pumps___________________ (etahtp)______________________ 8.7000E-01 + Thermal_to_electric_conversion_efficiency_of_the_power_conversion_cycle_ (etath)_______________________ 4.0000E-01 + Fraction_of_total_high-grade_thermal_power_to_divertor__________________ (pdivfraction)________________ 1.5623E-01 + Total_power_leaving_reactor_(across_vacuum_vessel_boundary)_(MW)________ ______________________________ 2.0111E+03 + Heat_removal_from_cryogenic_plant_(MW)__________________________________ (crypmw)______________________ 3.6566E+01 + Heat_removal_from_facilities_(MW)_______________________________________ (fachtmw)_____________________ 5.5490E+01 + Coolant_pumping_efficiency_losses_(MW)__________________________________ (htpsecmw)____________________ 2.4769E+01 + Heat_removal_from_injection_power_(MW)__________________________________ (pinjht)______________________ 8.0143E+01 + Heat_removal_from_tritium_plant_(MW)____________________________________ (trithtmw)____________________ 1.5000E+01 + Heat_removal_from_vacuum_pumps_(MW)_____________________________________ (vachtmw)_____________________ 5.0000E-01 + TF_coil_resistive_power_(MW)____________________________________________ (tfcmw)_______________________ 0.0000E+00 + Total_low-grade_thermal_power_(MW)______________________________________ (psechtmw)____________________ 2.2417E+02 + Total_High-grade_thermal_power_(MW)_____________________________________ (pthermmw)____________________ 2.1751E+03 + Number_of_primary_heat_exchangers_______________________________________ (nphx)________________________ 3 OP + Transport_power_from_scaling_law_(MW)___________________________________ (pscalingmw)__________________ 2.9785E+02 + Radiation_power_from_inside_"coreradius"_(MW)___________________________ (pcoreradmw.)_________________ 9.1650E+01 + Total_(MW)______________________________________________________________ ______________________________ 3.8950E+02 + Alpha_power_deposited_in_plasma_(MW)____________________________________ (falpha*palpmw)_______________ 3.0746E+02 + Power_from_charged_products_of_DD_and/or_D-He3_fusion_(MW)______________ (pchargemw.)__________________ 1.2659E+00 + Ohmic_heating_(MW)______________________________________________________ (pohmmw.)_____________________ 6.2284E-01 + Injected_power_deposited_in_plasma_(MW)_________________________________ (pinjmw)______________________ 8.0143E+01 + Total_(MW)______________________________________________________________ ______________________________ 3.8950E+02 + Fusion_power_(MW)_______________________________________________________ (powfmw)______________________ 1.6202E+03 + Power_from_energy_multiplication_in_blanket_and_shield_(MW)_____________ (emultmw)_____________________ 3.0836E+02 + Injected_power_(MW)_____________________________________________________ (pinjmw.)_____________________ 8.0143E+01 + Ohmic_power_(MW)________________________________________________________ (pohmmw.)_____________________ 6.2284E-01 + Power_deposited_in_primary_coolant_by_pump_(MW)_________________________ (htpmw_mech)__________________ 1.6576E+02 + Total_(MW)______________________________________________________________ ______________________________ 2.1751E+03 + Heat_extracted_from_first_wall_and_blanket_(MW)_________________________ (pthermfw_blkt)_______________ 1.8339E+03 + Heat_extracted_from_shield__(MW)________________________________________ (pthermshld)__________________ 1.4208E+00 + Heat_extracted_from_divertor_(MW)_______________________________________ (pthermdiv)___________________ 3.3982E+02 + Nuclear_and_photon_power_lost_to_H/CD_system_(MW)_______________________ (psechcd)_____________________ 0.0000E+00 + Nuclear_power_lost_to_TF_(MW)___________________________________________ (ptfnuc)______________________ 2.5118E-02 + Total_(MW)______________________________________________________________ ______________________________ 2.1752E+03 + Net_electric_power_output(MW)___________________________________________ (pnetelmw.)___________________ 4.0001E+02 + Required_Net_electric_power_output(MW)__________________________________ (pnetelin)____________________ 4.0000E+02 + Electric_power_for_heating_and_current_drive_(MW)_______________________ (pinjwp)______________________ 1.6029E+02 + Electric_power_for_primary_coolant_pumps_(MW)___________________________ (htpmw)_______________________ 1.9053E+02 + Electric_power_for_vacuum_pumps_(MW)____________________________________ (vachtmw)_____________________ 5.0000E-01 + Electric_power_for_tritium_plant_(MW)___________________________________ (trithtmw)____________________ 1.5000E+01 + Electric_power_for_cryoplant_(MW)_______________________________________ (crypmw)______________________ 3.6566E+01 + Electric_power_for_TF_coils_(MW)________________________________________ (tfacpd)______________________ 1.0434E+01 + Electric_power_for_PF_coils_(MW)________________________________________ (pfwpmw)______________________ 1.2422E+00 + All_other_internal_electric_power_requirements_(MW)_____________________ (fachtmw)_____________________ 5.5490E+01 + Total_(MW)______________________________________________________________ (tot_plant_power)_____________ 8.7006E+02 + Total_(MW)______________________________________________________________ ______________________________ 8.7006E+02 + Gross_electrical_output*_(MW)___________________________________________ (pgrossmw)____________________ 8.7006E+02 + Fusion_power_(MW)_______________________________________________________ (powfmw)______________________ 1.6202E+03 + Power_from_energy_multiplication_in_blanket_and_shield_(MW)_____________ (emultmw)_____________________ 3.0836E+02 + Total_(MW)______________________________________________________________ ______________________________ 1.9285E+03 + Net_electrical_output_(MW) _____________________________________________ (pnetelmw)____________________ 4.0001E+02 + Heat_rejected_by_main_power_conversion_circuit_(MW)_____________________ (rejected_main)_______________ 1.3051E+03 + Heat_rejected_by_other_cooling_circuits_(MW)____________________________ (psechtmw)____________________ 2.2417E+02 + Total_(MW)______________________________________________________________ ______________________________ 1.9293E+03 + Net_electric_power_/_total_nuclear_power_(%)____________________________ (pnetelmw/(powfmw+emultmw)____ 2.0741E+01 + Net_electric_power_/_total_fusion_power_(%)_____________________________ (pnetelmw/powfmw)_____________ 2.4689E+01 + Gross_electric_power*_/_high_grade_heat_(%)_____________________________ (etath)_______________________ 4.0000E+01 + Recirculating_power_fraction____________________________________________ (cirpowfr)____________________ 5.4025E-01 + # Water usage during plant operation (secondary cooling) # + Volume_used_in_cooling_tower_(m3/day)___________________________________ (waterusetower)_______________ 5.5485E+04 OP + Volume_used_in_recirculating_water_system_(m3/day)______________________ (wateruserecirc)______________ 1.8617E+04 OP + Volume_used_in_once-through_water_system_(m3/day)_______________________ (wateruseonethru)_____________ 1.8244E+06 OP + # Errors and Warnings # + # Errors and Warnings # + PROCESS_error_status_flag_______________________________________________ (error_status)________________ 2 + Final_error_identifier__________________________________________________ (error_id)____________________ 244 + # End of PROCESS Output # + # End of PROCESS Output # + # Copy of PROCESS Input Follows # +************************************************************************************************************************ +***** ***** +***** Generic large tokamak file ***** +***** James Morris, UKAEA ***** +***** 28/06/23 ***** +***** ***** +************************************************************************* + +* Run Information * +******************* + +runtitle = Generic large tokamak + +* Figure of merit - minimise major radius +minmax = 1 + +* Error tolerance for VMCON +epsvmc = 1e-7 + +* Constraint Equations - Consistency Equations * +************************************************ + +* Beta consistency * +*------------------* +icc = 1 +ixc = 5 * beta +beta = 0.03 + +* Global power balance * +*----------------------* +icc = 2 + +* Radial build consistency * +*--------------------------* +icc = 11 + +* Constraint Equations - Limit Equations * +****************************************** + +* Density upper limit * +*---------------------* +icc = 5 +ixc = 6 * dene [m-3] +fdene = 1.2 +dene = 7.5E19 + +* Neutron wall load upper limit * +*-------------------------------* +icc = 8 +ixc = 14 * fwalld +fwalld = 1.0 +* wall load limit [MW/m2] +walalw = 2.0 + +* Fusion power upper limit * +*--------------------------* + +icc = 9 +ixc = 26 * ffuspow +* Maximum allowable value fusion power [MW] +powfmax = 3000 + +* Burn time lower limit * +*-----------------------* +icc = 13 +ixc = 21 * ftburn +* minimum burn time [s] +tbrnmn = 7200.0 + +* L-H threshold scaling * +*-----------------------* +icc = 15 +ixc = 103 * flhthresh +boundu(103) = 10.0 + +* Injection power upper limit * +*-----------------------------* +icc = 30 +ixc = 46 * fpinj +* Maximum allowable value for injected power [MW] +pinjalw = 200.0 + +* Net electric power lower limit * +*--------------------------------* +icc = 16 +ixc = 25 * fpnetel +* Minimum allowable value for net eletric power [MW] +pnetelin = 400.0 + +* Beta upper limit * +*------------------* +icc = 24 +ixc = 36 * fbetatry +fbetatry = 0.5 + +* Max TF field * +*--------------* +icc = 25 +ixc = 35 * fpeakb +* Maximum allowable value for toroidal magnetic field [T] +bmxlim = 14.0 + +* Central solenoid EOF current density upper limit * +*--------------------------------------------------* +icc = 26 +ixc = 37 * coheof [A/m2] +ixc = 38 * fjohc +boundu(38) = 1.0 +coheof = 1.5E7 +fjohc = 0.6 + +* Central solenoid BOP current density upper limit * +*--------------------------------------------------* +icc = 27 +ixc = 39 * fjohc0 +ixc = 41 * fcohbop +boundu(39) = 1.0 +fjohc0 = 0.6 +fcohbop = 0.9 + +* I_op/I_Crit TF coil limit * +*---------------------------* +icc = 33 +ixc = 50 * fiooic +boundu(50) = 1.0 +fiooic = 0.65 + +* Dump voltage upper limit * +*--------------------------* +icc = 34 +ixc = 51 * fvdump +ixc = 52 * vdalw [kV] +boundu(52) = 10.0 +fvdump = 1.0 +vdalw = 10.0 + +* J_winding pack protection * +*---------------------------* +icc = 35 +ixc = 53 * fjprot +fjprot = 1.0 + +* TF temp marg lower limit * +*--------------------------* +icc = 36 +ixc = 54 * ftmargtf +* Minimum allowable temperature margin [K] +tmargmin = 1.5 + +* CS coil temp margin lower limit * +*---------------------------------* +icc = 60 +ixc = 106 * ftmargoh +tmargmin_cs = 1.5 + +* Lower limit on taup/taueff (ratio alpha particle/energy confinement times) * +*-------------------------------------------------------------------------------* +icc = 62 +ixc = 110 * ftaulimit +taulimit = 5.0 + +* dump time constraint for VV stresses * +*--------------------------------------* +icc = 65 +ixc = 113 * fmaxvvstress +fmaxvvstress = 1.0 + +* CS stress limit * +*-----------------* +icc = 72 +ixc = 123 * foh_stress +foh_stress = 1.0 +* allowable hoop stress in Central Solenoid structural material [Pa] +alstroh = 7.5D8 + +* neped_neped_______________________normalised_residue____________________ (normres023)__________________ -1.9637E-08 + Upper_Lim._on_Psep_*_Bt_/_q_A_R___normalised_residue____________________ (normres024)__________________ 4.9789E-07 + TF_coil_case_stress_upper_limit___normalised_residue____________________ (normres025)__________________ -4.6757E-07 + TF_coil_conduit_stress_upper_lim__normalised_residue____________________ (normres026)__________________ -4.1375E-07 + # Final Feasible Point # + # Power Reactor Costs (1990 US$) # + First_wall_/_blanket_life_(years)_______________________________________ (fwbllife)____________________ 6.1566E+00 + Divertor_life_(years)___________________________________________________ (divlife.)____________________ 3.9769E+00 + Cost_of_electricity_(m$/kWh)____________________________________________ (coe)_________________________ 5.1257E+02 + # Detailed Costings (1990 US$) # + Acc.22_multiplier_for_Nth_of_a_kind_____________________________________ (fkind)_______________________ 1.0000E+00 + Level_of_Safety_Assurance_______________________________________________ (lsa)_________________________ 4 + # Structures and Site Facilities # + Site_improvements,_facilities,_land_(M$)________________________________ (c211)________________________ 3.5200E+01 + Reactor_building_cost_(M$)______________________________________________ (c212)________________________ 4.5238E+02 + Turbine_building_cost_(M$)______________________________________________ (c213)________________________ 3.8000E+01 + Reactor_maintenance_building_cost_(M$)__________________________________ (c2141)_______________________ 1.0307E+02 + Warm_shop_cost_(M$)_____________________________________________________ (c2142)_______________________ 5.7641E+01 + Tritium_building_cost_(M$)______________________________________________ (c215)________________________ 1.4800E+01 + Electrical_equipment_building_cost_(M$)_________________________________ (c216)________________________ 1.9736E+01 + Additional_buildings_cost_(M$)__________________________________________ (c2171)_______________________ 1.8000E+01 + Control_room_buildings_cost_(M$)________________________________________ (c2172)_______________________ 2.1000E+01 + Shop_and_warehouses_cost_(M$)___________________________________________ (c2173)_______________________ 1.1500E+01 + Cryogenic_building_cost_(M$)____________________________________________ (c2174)_______________________ 6.8891E+00 + Total_account_21_cost_(M$)______________________________________________ (c21)_________________________ 7.7822E+02 + # Reactor Systems # + First_wall_cost_(M$)____________________________________________________ (c2211)_______________________ 1.9130E+02 + Blanket_beryllium_cost_(M$)_____________________________________________ (c22121)______________________ 2.6109E+02 + Blanket_breeder_material_cost_(M$)______________________________________ (c22122)______________________ 6.3985E+02 + Blanket_stainless_steel_cost_(M$)_______________________________________ (c22123)______________________ 8.0726E+01 + Blanket_vanadium_cost_(M$)______________________________________________ (c22124)______________________ 0.0000E+00 + Blanket_total_cost_(M$)_________________________________________________ (c2212)_______________________ 9.8166E+02 + Bulk_shield_cost_(M$)___________________________________________________ (c22131)______________________ 7.8394E+01 + Penetration_shielding_cost_(M$)_________________________________________ (c22132)______________________ 7.8394E+01 + Total_shield_cost_(M$)__________________________________________________ (c2213)_______________________ 1.5679E+02 + Total_support_structure_cost_(M$)_______________________________________ (c2214)_______________________ 4.0933E+01 + Divertor_cost_(M$)______________________________________________________ (c2215)_______________________ 4.1660E+01 + Total_account_221_cost_(M$)_____________________________________________ (c221)________________________ 1.4123E+03 + # Magnets # + TF_coil_conductor_cost_(M$)_____________________________________________ (c22211)______________________ 1.3230E+02 + TF_coil_winding_cost_(M$)_______________________________________________ (c22212)______________________ 5.4263E+01 + TF_coil_case_cost_(M$)__________________________________________________ (c22213)______________________ 4.4365E+02 + TF_intercoil_structure_cost_(M$)________________________________________ (c22214)______________________ 1.5066E+02 + TF_coil_gravity_support_structure_(M$)__________________________________ (c22215)______________________ 4.4659E+01 + TF_magnet_assemblies_cost_(M$)__________________________________________ (c2221)_______________________ 8.2552E+02 + PF_coil_conductor_cost_(M$)_____________________________________________ (c22221)______________________ 4.6409E+02 + PF_coil_winding_cost_(M$)_______________________________________________ (c22222)______________________ 7.6765E+01 + PF_coil_case_cost_(M$)__________________________________________________ (c22223)______________________ 9.4861E+01 + PF_coil_support_structure_cost_(M$)_____________________________________ (c22224)______________________ 8.0235E+00 + PF_magnet_assemblies_cost_(M$)__________________________________________ (c2222)_______________________ 6.4374E+02 + Vacuum_vessel_assembly_cost_(M$)________________________________________ (c2223)_______________________ 2.5404E+02 + Total_account_222_cost_(M$)_____________________________________________ (c222)________________________ 1.7233E+03 + # Power Injection # + ECH_system_cost_(M$)____________________________________________________ (c2231)_______________________ 2.4043E+02 + Lower_hybrid_system_cost_(M$)___________________________________________ (c2232)_______________________ 0.0000E+00 + Neutral_beam_system_cost_(M$)___________________________________________ (c2233)_______________________ 0.0000E+00 + Total_account_223_cost_(M$)_____________________________________________ (c223)________________________ 2.4043E+02 + # Vacuum Systems # + High_vacuum_pumps_cost_(M$)_____________________________________________ (c2241)_______________________ 1.2480E+01 + Backing_pumps_cost_(M$)_________________________________________________ (c2242)_______________________ 4.6800E+00 + Vacuum_duct_cost_(M$)___________________________________________________ (c2243)_______________________ 2.5280E+00 + Valves_cost_(M$)________________________________________________________ (c2244)_______________________ 5.7410E+00 + Duct_shielding_cost_(M$)________________________________________________ (c2245)_______________________ 0.0000E+00 + Instrumentation_cost_(M$)_______________________________________________ (c2246)_______________________ 1.3000E+00 + Total_account_224_cost_(M$)_____________________________________________ (c224)________________________ 2.6729E+01 + # Power Conditioning # + TF_coil_power_supplies_cost_(M$)________________________________________ (c22511)______________________ 4.0144E+00 + TF_coil_breakers_cost_(M$)______________________________________________ (c22512)______________________ 3.4127E+01 + TF_coil_dump_resistors_cost_(M$)________________________________________ (c22513)______________________ 2.1322E+01 + TF_coil_instrumentation_and_control_(M$)________________________________ (c22514)______________________ 4.8000E+00 + TF_coil_bussing_cost_(M$)_______________________________________________ (c22515)______________________ 3.5267E+01 + Total,_TF_coil_power_costs_(M$)_________________________________________ (c2251)_______________________ 9.9531E+01 + PF_coil_power_supplies_cost_(M$)________________________________________ (c22521)______________________ 2.9591E+00 + PF_coil_instrumentation_and_control_(M$)________________________________ (c22522)______________________ 3.6000E+00 + PF_coil_bussing_cost_(M$)_______________________________________________ (c22523)______________________ 1.1995E+01 + PF_coil_burn_power_supplies_cost_(M$)___________________________________ (c22524)______________________ 1.2679E+00 + PF_coil_breakers_cost_(M$)______________________________________________ (c22525)______________________ 1.4709E+01 + PF_coil_dump_resistors_cost_(M$)________________________________________ (c22526)______________________ 4.3206E+00 + PF_coil_ac_breakers_cost_(M$)___________________________________________ (c22527)______________________ 9.0000E-01 + Total,_PF_coil_power_costs_(M$)_________________________________________ (c2252)_______________________ 3.9752E+01 + Total,_energy_storage_cost_(M$)_________________________________________ (c2253)_______________________ 1.6864E+01 + Total_account_225_cost_(M$)_____________________________________________ (c225)________________________ 1.5615E+02 + # Heat Transport System # + Pumps_and_piping_system_cost_(M$)_______________________________________ (cpp)_________________________ 3.6795E+01 + Primary_heat_exchanger_cost_(M$)________________________________________ (chx)_________________________ 7.1692E+01 + Total,_reactor_cooling_system_cost_(M$)_________________________________ (c2261)_______________________ 1.0849E+02 + Pumps,_piping_cost_(M$)_________________________________________________ (cppa)________________________ 2.8417E+01 + Total,_auxiliary_cooling_system_cost_(M$)_______________________________ (c2262)_______________________ 2.8417E+01 + Total,_cryogenic_system_cost_(M$)_______________________________________ (c2263)_______________________ 1.7039E+02 + Total_account_226_cost_(M$)_____________________________________________ (c226)________________________ 3.0729E+02 + # Fuel Handling System # + Fuelling_system_cost_(M$)_______________________________________________ (c2271)_______________________ 2.2300E+01 + Fuel_processing_and_purification_cost_(M$)______________________________ (c2272)_______________________ 1.0229E+02 + Atmospheric_recovery_systems_cost_(M$)__________________________________ (c2273)_______________________ 5.8088E+01 + Nuclear_building_ventilation_cost_(M$)__________________________________ (c2274)_______________________ 6.9201E+01 + Total_account_227_cost_(M$)_____________________________________________ (c227)________________________ 2.5188E+02 + # Instrumentation and Control # + Instrumentation_and_control_cost_(M$)___________________________________ (c228)________________________ 1.5000E+02 + # Maintenance Equipment # + Maintenance_equipment_cost_(M$)_________________________________________ (c229)________________________ 1.2500E+02 + # Total Account 22 Cost # + Total_account_22_cost_(M$)______________________________________________ (c22)_________________________ 4.3931E+03 + # Turbine Plant Equipment # + Turbine_plant_equipment_cost_(M$)_______________________________________ (c23)_________________________ 1.7613E+02 + # Electric Plant Equipment # + Switchyard_equipment_cost_(M$)__________________________________________ (c241)________________________ 1.8400E+01 + Transformers_cost_(M$)__________________________________________________ (c242)________________________ 8.0330E+00 + Low_voltage_equipment_cost_(M$)_________________________________________ (c243)________________________ 6.4513E+00 + Diesel_backup_equipment_cost_(M$)_______________________________________ (c244)________________________ 6.8000E+00 + Auxiliary_facilities_cost_(M$)__________________________________________ (c245)________________________ 1.5000E+00 + Total_account_24_cost_(M$)______________________________________________ (c24)_________________________ 4.1184E+01 + # Miscellaneous Plant Equipment # + Miscellaneous_plant_equipment_cost_(M$)_________________________________ (c25)_________________________ 2.5000E+01 + # Heat Rejection System # + Heat_rejection_system_cost_(M$)_________________________________________ (c26)_________________________ 4.9877E+01 + # Plant Direct Cost # + Plant_direct_cost_(M$)__________________________________________________ (cdirt)_______________________ 5.4635E+03 + # Reactor Core Cost # + Reactor_core_cost_(M$)__________________________________________________ (crctcore)____________________ 3.3761E+03 + # Indirect Cost # + Indirect_cost_(M$)______________________________________________________ (c9)__________________________ 1.8221E+03 + # Total Contingency # + Total_contingency_(M$)__________________________________________________ (ccont)_______________________ 1.4207E+03 + # Constructed Cost # + Constructed_cost_(M$)___________________________________________________ (concost)_____________________ 8.7063E+03 + # Interest during Construction # + Interest_during_construction_(M$)_______________________________________ (moneyint)____________________ 1.4365E+03 + # Total Capital Investment # + Total_capital_investment_(M$)___________________________________________ (capcost)_____________________ 1.0143E+04 + # Plant Availability # + Allowable_blanket_neutron_fluence_(MW-yr/m2)____________________________ (abktflnc)____________________ 5.0000E+00 + Allowable_divertor_heat_fluence_(MW-yr/m2)______________________________ (adivflnc)____________________ 7.0000E+00 + First_wall_/_blanket_lifetime_(years)___________________________________ (bktlife)_____________________ 6.1566E+00 OP + Divertor_lifetime_(years)_______________________________________________ (divlife)_____________________ 3.9769E+00 OP + Heating/CD_system_lifetime_(years)______________________________________ (cdrlife)_____________________ 6.1566E+00 OP + Total_plant_lifetime_(years)____________________________________________ (tlife)_______________________ 3.0000E+01 + Total_plant_availability_fraction_______________________________________ (cfactr)______________________ 8.0000E-01 + Number_of_fusion_cycles_to_reach_allowable_fw/blanket_DPA_______________ (bktcycles)___________________ 1.5787E+04 + # Plasma # + Tokamak_aspect_ratio_=_Conventional,_itart_=_0__________________________ (itart)_______________________ 0.0000E+00 + Major_radius_(m)________________________________________________________ (rmajor)______________________ 8.0000E+00 ITV + Minor_radius_(m)________________________________________________________ (rminor)______________________ 2.6667E+00 + Aspect_ratio____________________________________________________________ (aspect)______________________ 3.0000E+00 + Elongation,_X-point_(input_value_used)__________________________________ (kappa)_______________________ 1.8500E+00 + Elongation,_95%_surface_(calculated_from_kappa)_________________________ (kappa95)_____________________ 1.6518E+00 + Elongation,_area_ratio_calc.____________________________________________ (kappaa)______________________ 1.7188E+00 + Triangularity,_X-point_(input_value_used)_______________________________ (triang)______________________ 5.0000E-01 + Triangularity,_95%_surface_(calculated_from_triang)_____________________ (triang95)____________________ 3.3333E-01 + Plasma_poloidal_perimeter_(m)___________________________________________ (pperim)______________________ 2.4081E+01 + Plasma_cross-sectional_area_(m2)________________________________________ (xarea)_______________________ 3.8398E+01 + Plasma_surface_area_(m2)________________________________________________ (sarea)_______________________ 1.1738E+03 OP + Plasma_volume_(m3)______________________________________________________ (vol)_________________________ 1.8882E+03 OP + Plasma_current_scaling_law_used_________________________________________ (icurr)_______________________ 4 + Plasma_current_(MA)_____________________________________________________ (plascur/1D6)_________________ 1.6631E+01 + Current_density_profile_factor__________________________________________ (alphaj)______________________ 1.9805E+00 + Plasma_internal_inductance,_li__________________________________________ (rli)_________________________ 1.2275E+00 + Vertical_field_at_plasma_(T)____________________________________________ (bvert)_______________________ -7.4373E-01 + Vacuum_toroidal_field_at_R_(T)__________________________________________ (bt)__________________________ 5.2940E+00 ITV + Average_poloidal_field_(T)______________________________________________ (bp)__________________________ 8.6787E-01 + Total_field_(sqrt(bp^2_+_bt^2))_(T)_____________________________________ (btot)________________________ 5.3647E+00 + Safety_factor_on_axis___________________________________________________ (q0)__________________________ 1.0000E+00 + Safety_factor_at_95%_flux_surface_______________________________________ (q95)_________________________ 3.5961E+00 ITV + Cylindrical_safety_factor_(qcyl)________________________________________ (qstar)_______________________ 2.9805E+00 + Total_plasma_beta_______________________________________________________ (beta)________________________ 3.3648E-02 ITV + Total_poloidal_beta_____________________________________________________ (betap)_______________________ 1.2857E+00 OP + Total_toroidal_beta_____________________________________________________ ______________________________ 3.4553E-02 OP + Fast_alpha_beta_________________________________________________________ (betaft)______________________ 4.2236E-03 OP + Beam_ion_beta___________________________________________________________ (betanb)______________________ 0.0000E+00 OP + (Fast_alpha_+_beam_physics_variables.beta)/(thermal_physics_variables.be (gammaft)_____________________ 1.4354E-01 OP + Thermal_beta____________________________________________________________ ______________________________ 2.9425E-02 OP + Thermal_poloidal_beta___________________________________________________ ______________________________ 1.1243E+00 OP + Thermal_toroidal_physics_variables.beta_(=_beta-exp)____________________ ______________________________ 3.0215E-02 OP + 2nd_stability_physics_variables.beta_:_beta_p_/_(R/a)___________________ (eps*betap)___________________ 4.2857E-01 + 2nd_stability_physics_variables.beta_upper_limit________________________ (epbetmax)____________________ 1.3800E+00 + Beta_g_coefficient______________________________________________________ (dnbeta)______________________ 4.9099E+00 + Normalised_thermal_beta_________________________________________________ ______________________________ 2.4977E+00 + Normalised_total_beta___________________________________________________ ______________________________ 2.8562E+00 + Normalised_toroidal_beta________________________________________________ (normalised_toroidal_beta)____ 2.9330E+00 + Limit_on_thermal_beta___________________________________________________ (betalim)_____________________ 5.7842E-02 + Plasma_thermal_energy_(J)_______________________________________________ ______________________________ 9.5431E+08 OP + Total_plasma_internal_energy_(J)________________________________________ (total_plasma_internal_energy) 1.0913E+09 OP + Electron_temperature_(keV)______________________________________________ (te)__________________________ 1.2489E+01 ITV + Electron_temperature_on_axis_(keV)______________________________________ (te0)_________________________ 2.5758E+01 + Ion_temperature_(keV)___________________________________________________ (ti)__________________________ 1.2489E+01 + Ion_temperature_on_axis_(keV)___________________________________________ (ti0)_________________________ 2.5758E+01 + Electron_temp.,_density_weighted_(keV)__________________________________ (ten)_________________________ 1.3805E+01 + Electron_density_(/m3)__________________________________________________ (dene)________________________ 8.0667E+19 ITV + Electron_density_on_axis_(/m3)__________________________________________ (ne0)_________________________ 1.0610E+20 OP + Line-averaged_electron_density_(/m3)____________________________________ (dnla)________________________ 8.9334E+19 OP + Line-averaged_electron_density_/_Greenwald_density______________________ (dnla_gw)_____________________ 1.2000E+00 OP + Ion_density_(/m3)_______________________________________________________ (dnitot)______________________ 7.1669E+19 OP + Fuel_density_(/m3)______________________________________________________ (deni)________________________ 6.4831E+19 OP + Total_impurity_density_with_Z_>_2_(no_He)_(/m3)_________________________ (dnz)_________________________ 4.6503E+16 OP + Helium_ion_density_(thermalised_ions_only)_(/m3)________________________ (dnalp)_______________________ 6.7723E+18 OP + Proton_density_(/m3)____________________________________________________ (dnprot)______________________ 1.8963E+16 OP + Hot_beam_density_(/m3)__________________________________________________ (dnbeam)______________________ 0.0000E+00 OP + Density_limit_from_scaling_(/m3)________________________________________ (dnelimt)_____________________ 7.4445E+19 OP + Density_limit_(enforced)_(/m3)__________________________________________ (boundu(9)*dnelimt)___________ 7.4445E+19 OP + Helium_ion_density_(thermalised_ions_only)_/_electron_density___________ (ralpne)______________________ 8.3954E-02 ITV + H__concentration________________________________________________________ (fimp(01))____________________ 8.0392E-01 OP + He_concentration________________________________________________________ (fimp(02))____________________ 8.3954E-02 + Be_concentration________________________________________________________ (fimp(03))____________________ 0.0000E+00 + C__concentration________________________________________________________ (fimp(04))____________________ 0.0000E+00 + N__concentration________________________________________________________ (fimp(05))____________________ 0.0000E+00 + O__concentration________________________________________________________ (fimp(06))____________________ 0.0000E+00 + Ne_concentration________________________________________________________ (fimp(07))____________________ 0.0000E+00 + Si_concentration________________________________________________________ (fimp(08))____________________ 0.0000E+00 + Ar_concentration________________________________________________________ (fimp(09))____________________ 0.0000E+00 + Fe_concentration________________________________________________________ (fimp(10))____________________ 0.0000E+00 + Ni_concentration________________________________________________________ (fimp(11))____________________ 0.0000E+00 + Kr_concentration________________________________________________________ (fimp(12))____________________ 0.0000E+00 + Xe_concentration________________________________________________________ (fimp(13))____________________ 5.7149E-04 ITV + W__concentration________________________________________________________ (fimp(14))____________________ 5.0000E-06 + Average_mass_of_all_ions_(amu)__________________________________________ (aion)________________________ 2.7252E+00 OP + Effective_charge________________________________________________________ (zeff)________________________ 2.5164E+00 + Density_profile_factor__________________________________________________ (alphan)______________________ 1.0000E+00 + Plasma_profile_model____________________________________________________ (ipedestal)___________________ 1 + Density_pedestal_r/a_location___________________________________________ (rhopedn)_____________________ 9.4000E-01 + Electron_density_pedestal_height_(/m3)__________________________________ (neped)_______________________ 6.3278E+19 OP + Electron_density_at_pedestal_/_nGW______________________________________ (fgwped_out)__________________ 8.5000E-01 + Temperature_pedestal_r/a_location_______________________________________ (rhopedt)_____________________ 9.4000E-01 + Pedestal_scaling_switch_________________________________________________ (ieped)_______________________ 0 + Electron_temp._pedestal_height_(keV)____________________________________ (teped)_______________________ 5.5000E+00 + Electron_temp._at_separatrix_(keV)______________________________________ (tesep)_______________________ 1.0000E-01 + Electron_density_at_separatrix_(/m3)____________________________________ (nesep)_______________________ 3.7223E+19 + Electron_density_at_separatrix_/_nGW____________________________________ (fgwsep_out)__________________ 5.0000E-01 + Temperature_profile_index_______________________________________________ (alphat)______________________ 1.4500E+00 + Temperature_profile_index_beta__________________________________________ (tbeta)_______________________ 2.0000E+00 + Old_ASDEX_model_________________________________________________________ (dlimit(1))___________________ 5.2797E+19 OP + Borrass_ITER_model_I____________________________________________________ (dlimit(2))___________________ 1.0969E+20 OP + Borrass_ITER_model_II___________________________________________________ (dlimit(3))___________________ 4.3575E+19 OP + JET_edge_radiation_model________________________________________________ (dlimit(4))___________________ 3.0227E+21 OP + JET_simplified_model____________________________________________________ (dlimit(5))___________________ 4.3397E+20 OP + Hugill-Murakami_Mq_model________________________________________________ (dlimit(6))___________________ 6.6609E+19 OP + Greenwald_model_________________________________________________________ (dlimit(7))___________________ 7.4445E+19 OP + Deuterium_fuel_fraction_________________________________________________ (fdeut)_______________________ 5.0000E-01 + Tritium_fuel_fraction___________________________________________________ (ftrit)_______________________ 5.0000E-01 + Total_fusion_power_(MW)_________________________________________________ (powfmw)______________________ 1.6202E+03 OP + _=____D-T_fusion_power_(MW)_____________________________________________ (pdt)_________________________ 1.6182E+03 OP + __+___D-D_fusion_power_(MW)_____________________________________________ (pdd)_________________________ 1.9494E+00 OP + __+_D-He3_fusion_power_(MW)_____________________________________________ (pdhe3)_______________________ 0.0000E+00 OP + Alpha_power:_total_(MW)_________________________________________________ (palpmw)______________________ 3.2365E+02 OP + Alpha_power:_beam-plasma_(MW)___________________________________________ (palpnb)______________________ 0.0000E+00 OP + Neutron_power_(MW)______________________________________________________ (pneutmw)_____________________ 1.2953E+03 OP + Charged_particle_power_(excluding_alphas)_(MW)__________________________ (pchargemw)___________________ 1.2659E+00 OP + Total_power_deposited_in_plasma_(MW)____________________________________ (tot_power_plasma)____________ 3.8950E+02 OP + Bremsstrahlung_radiation_power_(MW)_____________________________________ (pbrempv*vol)_________________ 6.5195E+01 OP + Line_radiation_power_(MW)_______________________________________________ (plinepv*vol)_________________ 1.4609E+02 OP + Synchrotron_radiation_power_(MW)________________________________________ (psyncpv*vol)_________________ 1.5187E+01 OP + Synchrotron_wall_reflectivity_factor____________________________________ (ssync)_______________________ 6.0000E-01 + Normalised_minor_radius_defining_'core'_________________________________ (coreradius)__________________ 7.5000E-01 + Fraction_of_core_radiation_subtracted_from_P_L__________________________ (coreradiationfraction)_______ 6.0000E-01 + Radiation_power_from_inner_zone_(MW)____________________________________ (pinnerzoneradmw)_____________ 9.1650E+01 OP + Radiation_power_from_outer_zone_(MW)____________________________________ (pouterzoneradmw)_____________ 1.3482E+02 OP + Total_radiation_power_from_inside_LCFS_(MW)_____________________________ (pradmw)______________________ 2.2647E+02 OP + LCFS_radiation_fraction_=_total_radiation_in_LCFS_/_total_power_deposite (rad_fraction_LCFS)___________ 5.8144E-01 OP + Nominal_mean_radiation_load_on_inside_surface_of_reactor_(MW/m2)________ (photon_wall)_________________ 1.7749E-01 OP + Peaking_factor_for_radiation_wall_load__________________________________ (peakfactrad)_________________ 3.3300E+00 IP + Maximum_permitted_radiation_wall_load_(MW/m^2)__________________________ (maxradwallload)______________ 1.0000E+00 IP + Peak_radiation_wall_load_(MW/m^2)_______________________________________ (peakradwallload)_____________ 5.9106E-01 OP + Fast_alpha_particle_power_incident_on_the_first_wall_(MW)_______________ (palpfwmw)____________________ 1.6182E+01 OP + Nominal_mean_neutron_load_on_inside_surface_of_reactor_(MW/m2)__________ (wallmw)______________________ 1.0152E+00 OP + Power_incident_on_the_divertor_targets_(MW)_____________________________ (ptarmw)______________________ 3.2606E+01 OP + Fraction_of_power_to_the_lower_divertor_________________________________ (ftar)________________________ 1.0000E+00 IP + Outboard_side_heat_flux_decay_length_(m)________________________________ (lambdaio)____________________ 1.5700E-03 OP + Fraction_of_power_on_the_inner_targets__________________________________ (fio)_________________________ 4.1000E-01 OP + Fraction_of_power_incident_on_the_lower_inner_target____________________ (fLI)_________________________ 4.1000E-01 OP + Fraction_of_power_incident_on_the_lower_outer_target____________________ (fLO)_________________________ 5.9000E-01 OP + Power_incident_on_the_lower_inner_target_(MW)___________________________ (pLImw)_______________________ 1.3368E+01 OP + Power_incident_on_the_lower_outer_target_(MW)___________________________ (pLOmw)_______________________ 1.9237E+01 OP + Ohmic_heating_power_(MW)________________________________________________ (pohmmw)______________________ 6.2284E-01 OP + Fraction_of_alpha_power_deposited_in_plasma_____________________________ (falpha)______________________ 9.5000E-01 + Fraction_of_alpha_power_to_electrons____________________________________ (falpe)_______________________ 7.1828E-01 + Fraction_of_alpha_power_to_ions_________________________________________ (falpi)_______________________ 2.8172E-01 + Ion_transport_(MW)______________________________________________________ (ptrimw)______________________ 1.4013E+02 OP + Electron_transport_(MW)_________________________________________________ (ptremw)______________________ 1.5772E+02 OP + Injection_power_to_ions_(MW)____________________________________________ (pinjimw)_____________________ 0.0000E+00 OP + Injection_power_to_electrons_(MW)_______________________________________ (pinjemw)_____________________ 8.0143E+01 OP + Ignited_plasma_switch_(0=not_ignited,_1=ignited)________________________ (ignite)______________________ 0 + Power_into_divertor_zone_via_charged_particles_(MW)_____________________ (pdivt)_______________________ 1.6303E+02 OP + Psep_/_R_ratio_(MW/m)___________________________________________________ (pdivt/rmajor)________________ 2.0378E+01 OP + Psep_Bt_/_qAR_ratio_(MWT/m)_____________________________________________ (pdivtbt/qar)_________________ 1.0000E+01 OP + ITER_1996_scaling:_nominal_(MW)_________________________________________ (pthrmw(1))___________________ 1.2978E+02 OP + ITER_1996_scaling:_upper_bound_(MW)_____________________________________ (pthrmw(2))___________________ 2.8603E+02 OP + ITER_1996_scaling:_lower_bound_(MW)_____________________________________ (pthrmw(3))___________________ 5.8098E+01 OP + ITER_1997_scaling_(1)_(MW)______________________________________________ (pthrmw(4))___________________ 2.1452E+02 OP + ITER_1997_scaling_(2)_(MW)______________________________________________ (pthrmw(5))___________________ 1.7206E+02 OP + Martin_2008_scaling:_nominal_(MW)_______________________________________ (pthrmw(6))___________________ 9.7416E+01 OP + Martin_2008_scaling:_95%_upper_bound_(MW)_______________________________ (pthrmw(7))___________________ 1.2769E+02 OP + Martin_2008_scaling:_95%_lower_bound_(MW)_______________________________ (pthrmw(8))___________________ 6.7143E+01 OP + Snipes_2000_scaling:_nominal_(MW)_______________________________________ (pthrmw(9))___________________ 6.7785E+01 OP + Snipes_2000_scaling:_upper_bound_(MW)___________________________________ (pthrmw(10))__________________ 9.9437E+01 OP + Snipes_2000_scaling:_lower_bound_(MW)___________________________________ (pthrmw(11))__________________ 4.5839E+01 OP + Snipes_2000_scaling_(closed_divertor):_nominal_(MW)_____________________ (pthrmw(12))__________________ 3.1010E+01 OP + Snipes_2000_scaling_(closed_divertor):_upper_bound_(MW)_________________ (pthrmw(13))__________________ 4.3148E+01 OP + Snipes_2000_scaling_(closed_divertor):_lower_bound_(MW)_________________ (pthrmw(14))__________________ 2.2130E+01 OP + Hubbard_2012_L-I_threshold_-_nominal_(MW)_______________________________ (pthrmw(15))__________________ 2.7549E+01 OP + Hubbard_2012_L-I_threshold_-_lower_bound_(MW)___________________________ (pthrmw(16))__________________ 1.4319E+01 OP + Hubbard_2012_L-I_threshold_-_upper_bound_(MW)___________________________ (pthrmw(17))__________________ 5.3005E+01 OP + Hubbard_2017_L-I_threshold______________________________________________ (pthrmw(18))__________________ 2.6202E+02 OP + Martin_2008_aspect_ratio_corrected_scaling:_nominal_(MW)________________ (pthrmw(19))__________________ 9.7416E+01 OP + Martin_2008_aspect_ratio_corrected_scaling:_95%_upper_bound_(MW)________ (pthrmw(20))__________________ 1.2769E+02 OP + Martin_2008_aspect_ratio_corrected_scaling:_95%_lower_bound_(MW)________ (pthrmw(21))__________________ 6.7143E+01 OP + L-H_threshold_power_(enforced)_(MW)_____________________________________ (boundl(103)*plhthresh)_______ 9.7416E+01 OP + L-H_threshold_power_(MW)________________________________________________ (plhthresh)___________________ 9.7416E+01 OP + Confinement_H_factor____________________________________________________ (hfact)_______________________ 1.1886E+00 ITV + Global_thermal_energy_confinement_time_(s)______________________________ (taueff)______________________ 3.2037E+00 + Ion_energy_confinement_time_(s)_________________________________________ (tauei)_______________________ 3.2037E+00 + Electron_energy_confinement_time_(s)____________________________________ (tauee)_______________________ 3.2037E+00 + n.tau_=_Volume-average_electron_density_x_Energy_confinement_time_(s/m3) (dntau)_______________________ 2.5843E+20 OP + Triple_product__(keV_s/m3)______________________________________________ (dntau*te)____________________ 3.2275E+21 OP + Transport_loss_power_assumed_in_scaling_law_(MW)________________________ (powerht)_____________________ 2.9785E+02 OP + Switch_for_radiation_loss_term_usage_in_power_balance___________________ (iradloss)____________________ 1 + Radiation_power_subtracted_from_plasma_power_balance_(MW)_______________ ______________________________ 9.1650E+01 OP + Alpha_particle_confinement_time_(s)_____________________________________ (taup)________________________ 2.2270E+01 + Alpha_particle/energy_confinement_time_ratio____________________________ (taup/taueff)_________________ 6.9512E+00 + Lower_limit_on_taup/taueff______________________________________________ (taulimit)____________________ 5.0000E+00 + Total_energy_confinement_time_including_radiation_loss_(s)______________ (total_energy_conf_time)______ 2.8018E+00 + Normalized_plasma_pressure_beta_as_defined_by_McDonald_et_al____________ (beta_mcdonald)_______________ 3.4553E-02 OP + Normalized_ion_Larmor_radius____________________________________________ (rho_star)____________________ 1.9603E-03 OP + Normalized_collisionality_______________________________________________ (nu_star)_____________________ 3.7266E-03 OP + Volume_measure_of_elongation____________________________________________ (kappaa_IPB)__________________ 1.6815E+00 OP + Total_volt-second_requirement_(Wb)______________________________________ (vsstt)_______________________ 5.5616E+02 OP + Inductive_volt-seconds_(Wb)_____________________________________________ (vsind)_______________________ 2.3585E+02 OP + Ejima_coefficient_______________________________________________________ (gamma)_______________________ 3.0000E-01 + Start-up_resistive_(Wb)_________________________________________________ (vsres)_______________________ 5.0159E+01 OP + Flat-top_resistive_(Wb)_________________________________________________ (vsbrn)_______________________ 2.7015E+02 OP + bootstrap_current_fraction_multiplier___________________________________ (cboot)_______________________ 1.0000E+00 + Bootstrap_fraction_(ITER_1989)__________________________________________ (bscf_iter89)_________________ 3.7098E-01 + Bootstrap_fraction_(Sauter_et_al)_______________________________________ (bscf_sauter)_________________ 4.1920E-01 + Bootstrap_fraction_(Nevins_et_al)_______________________________________ (bscf_nevins)_________________ 3.5042E-01 + Bootstrap_fraction_(Wilson)_____________________________________________ (bscf_wilson)_________________ 4.3349E-01 + Diamagnetic_fraction_(Hender)___________________________________________ (diacf_hender)________________ 1.2017E-02 + Diamagnetic_fraction_(SCENE)____________________________________________ (diacf_scene)_________________ 1.1139E-02 + Pfirsch-Schlueter_fraction_(SCENE)______________________________________ (pscf_scene)__________________ -3.0283E-03 + Bootstrap_fraction_(enforced)___________________________________________ (bootipf.)____________________ 4.1920E-01 + Diamagnetic_fraction_(enforced)_________________________________________ (diaipf.)_____________________ 0.0000E+00 + Pfirsch-Schlueter_fraction_(enforced)___________________________________ (psipf.)______________________ 0.0000E+00 + Loop_voltage_during_burn_(V)____________________________________________ (vburn)_______________________ 3.7450E-02 OP + Plasma_resistance_(ohm)_________________________________________________ (rplas)_______________________ 3.9755E-09 OP + Resistive_diffusion_time_(s)____________________________________________ (res_time)____________________ 3.0619E+03 OP + Plasma_inductance_(H)___________________________________________________ (rlp)_________________________ 1.4181E-05 OP + Coefficient_for_sawtooth_effects_on_burn_V-s_requirement________________ (csawth)______________________ 1.0000E+00 + Ratio_of_He_and_pellet_particle_confinement_times_______________________ (tauratio)____________________ 1.0000E+00 + Fuelling_rate_(nucleus-pairs/s)_________________________________________ (qfuel)_______________________ 3.3420E+21 OP + Fuel_burn-up_rate_(reactions/s)_________________________________________ (rndfuel)_____________________ 5.7755E+20 OP + Burn-up_fraction________________________________________________________ (burnup)______________________ 1.7282E-01 + # Energy confinement times, and required H-factors : # + # Current Drive System # + Current_drive_efficiency_model__________________________________________ (iefrf)_______________________ 10 + Secondary_current_drive_efficiency_model________________________________ (iefrffix)____________________ 0 + Ratio_of_power_for_flat-top_to_start-up_(MW)____________________________ (startupratio)________________ 1.0000E+00 + Auxiliary_power_used_for_plasma_heating_only_(MW)_______________________ (pheat)_______________________ 7.5000E+01 + Power_injected_for_current_drive_(MW)___________________________________ (pcurrentdrivemw)_____________ 5.1429E+00 + Maximum_Allowed_Bootstrap_current_fraction______________________________ (bscfmax)_____________________ 9.5000E-01 + Fusion_gain_factor_Q____________________________________________________ (bigq)________________________ 2.0060E+01 OP + Auxiliary_current_drive_(A)_____________________________________________ (auxiliary_cd)________________ 2.3908E+05 OP + Current_drive_efficiency_(A/W)__________________________________________ (effcd)_______________________ 4.6488E-02 OP + Normalised_current_drive_efficiency,_gamma_(10^20_A/W-m2)_______________ (gamcd)_______________________ 3.0000E-01 OP + Wall_plug_to_injector_efficiency________________________________________ (etacd)_______________________ 5.0000E-01 + ECRH_plasma_heating_efficiency__________________________________________ (gamma_ecrh)__________________ 3.0000E-01 + Bootstrap_fraction______________________________________________________ (bootipf)_____________________ 4.1920E-01 + Diamagnetic_fraction____________________________________________________ (diaipf)______________________ 0.0000E+00 + Pfirsch-Schlueter_fraction______________________________________________ (psipf)_______________________ 0.0000E+00 + Auxiliary_current_drive_fraction________________________________________ (faccd)_______________________ 1.4376E-02 + Inductive_fraction______________________________________________________ (facoh)_______________________ 5.6642E-01 + Total___________________________________________________________________ (plasipf+faccd+facoh)_________ 1.0000E+00 + Fraction_of_the_plasma_current_produced_by_non-inductive_means__________ (fvsbrnni)____________________ 4.3358E-01 ITV + Electron_cyclotron_injected_power_(MW)__________________________________ (echpwr)______________________ 8.0143E+01 OP + Maximum_allowable_ECRH_power_(MW)_______________________________________ (pinjalw)_____________________ 2.0000E+02 + ECH_wall_plug_efficiency________________________________________________ (etaech)______________________ 5.0000E-01 + ECH_wall_plug_power_(MW)________________________________________________ (echwpow)_____________________ 1.6029E+02 OP + Total_V-s_capability_of_Central_Solenoid/PF_coils_(Wb)__________________ (abs(vstot))__________________ 5.7728E+02 + Required_volt-seconds_during_start-up_(Wb)______________________________ (vssoft)______________________ 2.8601E+02 + Available_volt-seconds_during_burn_(Wb)_________________________________ (vsmax)_______________________ 2.7014E+02 + # Times # + Initial_charge_time_for_CS_from_zero_current_(s)________________________ (tramp)_______________________ 5.0000E+02 + Plasma_current_ramp-up_time_(s)_________________________________________ (tohs)________________________ 1.6631E+02 + Heating_time_(s)________________________________________________________ (theat)_______________________ 1.0000E+01 + Burn_time_(s)___________________________________________________________ (tburn)_______________________ 7.2035E+03 OP + Reset_time_to_zero_current_for_CS_(s)___________________________________ (tqnch)_______________________ 1.6631E+02 + Time_between_pulses_(s)_________________________________________________ (tdwell)______________________ 1.8000E+03 + Total_plant_cycle_time_(s)______________________________________________ (tcycle)______________________ 9.8463E+03 OP + # Radial Build # + TF_coil_radial_placement_switch_________________________________________ (tf_in_cs)____________________ 0 + TF_coil_radial_placement_switch_________________________________________ (tf_in_cs)____________________ 0 + Machine_bore_(m)________________________________________________________ (bore)________________________ 1.9854E+00 ITV + CS_radial_thickness_(m)_________________________________________________ (ohcth)_______________________ 5.7587E-01 ITV + CS_precompression_(m)___________________________________________________ (precomp)_____________________ 6.8064E-02 + CS_precompresion_to_TF_coil_radial_gap_(m)______________________________ (gapoh)_______________________ 8.0000E-02 + TF_coil_inboard_leg_(m)_________________________________________________ (tfcth)_______________________ 9.1597E-01 ITV + TF_coil_inboard_leg_insulation_gap_(m)__________________________________ (tftsgap)_____________________ 5.0000E-02 + Thermal_shield,_inboard_(m)_____________________________________________ (thshield_ib)_________________ 5.0000E-02 + thermal_shield_to_vessel_radial_gap_(m)_________________________________ (gapds)_______________________ 2.0000E-02 + Inboard_vacuum_vessel_radial_thickness_(m)______________________________ (d_vv_in)_____________________ 3.0000E-01 + Inner_radiation_shield_radial_thickness_(m)_____________________________ (shldith)_____________________ 3.0000E-01 + Gap_(m)_________________________________________________________________ (vvblgap)_____________________ 2.0000E-02 + Inboard_blanket_radial_thickness_(m)____________________________________ (blnkith)_____________________ 7.0000E-01 + Inboard_first_wall_radial_thickness_(m)_________________________________ (fwith)_______________________ 1.8000E-02 + Inboard_scrape-off_radial_thickness_(m)_________________________________ (scrapli)_____________________ 2.5000E-01 + Outboard_scrape-off_radial_thickness_(m)________________________________ (scraplo)_____________________ 2.5000E-01 + Outboard_first_wall_radial_thickness_(m)________________________________ (fwoth)_______________________ 1.8000E-02 + Outboard_blanket_radial_thickness_(m)___________________________________ (blnkoth)_____________________ 1.0000E+00 + Outer_radiation_shield_radial_thickness_(m)_____________________________ (shldoth)_____________________ 8.0000E-01 + Outboard_vacuum_vessel_radial_thickness_(m)_____________________________ (d_vv_out)____________________ 3.0000E-01 + Vessel_to_TF_radial_gap_(m)_____________________________________________ (gapsto)______________________ 1.3720E+00 + Thermal_shield,_outboard_(m)____________________________________________ (thshield_ob)_________________ 5.0000E-02 + Gap_(m)_________________________________________________________________ (tftsgap)_____________________ 5.0000E-02 + TF_coil_outboard_leg_radial_thickness_(m)_______________________________ (tfthko)______________________ 9.1597E-01 + # Vertical Build # + Divertor_null_switch____________________________________________________ (i_single_null)_______________ 1 + Vessel_-_TF_coil_vertical_gap_(m)_______________________________________ (vgap2)_______________________ 1.6300E-01 + Topside_vacuum_vessel_radial_thickness_(m)______________________________ (d_vv_top)____________________ 3.0000E-01 + Top_radiation_shield_thickness_(m)______________________________________ (shldtth)_____________________ 6.0000E-01 + Top_blanket_vertical_thickness_(m)______________________________________ (blnktth)_____________________ 8.5000E-01 + Top_first_wall_vertical_thickness_(m)___________________________________ (fwtth)_______________________ 1.8000E-02 + Top_scrape-off_vertical_thickness_(m)___________________________________ (vgaptop)_____________________ 6.0000E-01 + Plasma_half-height_(m)__________________________________________________ (rminor*kappa)________________ 4.9333E+00 + Bottom_scrape-off_vertical_thickness_(m)________________________________ (vgap)________________________ 2.0019E+00 + Divertor_structure_vertical_thickness_(m)_______________________________ (divfix)______________________ 6.2000E-01 + Bottom_radiation_shield_thickness_(m)___________________________________ (shldlth)_____________________ 7.0000E-01 + Underside_vacuum_vessel_radial_thickness_(m)____________________________ (d_vv_bot)____________________ 3.0000E-01 + External_cryostat_thickness_(m)_________________________________________ (ddwex)_______________________ 1.5000E-01 + Ratio_of_Central_solenoid_height_to_TF_coil_internal_height_____________ (ohhghf)______________________ 9.0000E-01 + Width_of_neutral_beam_duct_where_it_passes_between_the_TF_coils_(m)_____ (beamwd)______________________ 5.8000E-01 + # Divertor build and plasma position # + Plasma_top_position,_radial_(m)_________________________________________ (ptop_radial)_________________ 6.6667E+00 + Plasma_top_position,_vertical_(m)_______________________________________ (ptop_vertical)_______________ 4.9333E+00 + Plasma_geometric_centre,_radial_(m)_____________________________________ (physics_variables.rmajor.)___ 8.0000E+00 + Plasma_geometric_centre,_vertical_(m)___________________________________ (0.0)_________________________ 0.0000E+00 + Plasma_lower_physics_variables.triangularity____________________________ (tril)________________________ 5.0000E-01 + Plasma_elongation_______________________________________________________ (physics_variables.kappa.)____ 1.8500E+00 + TF_coil_vertical_offset_(m)_____________________________________________ (tfoffset)____________________ -6.1694E-01 + Plasma_outer_arc_radius_of_curvature_(m)________________________________ (rco)_________________________ 5.0422E+00 + Plasma_inner_arc_radius_of_curvature_(m)________________________________ (rci)_________________________ 9.7933E+00 + Plasma_lower_X-pt,_radial_(m)___________________________________________ (rxpt)________________________ 6.6667E+00 + Plasma_lower_X-pt,_vertical_(m)_________________________________________ (zxpt)________________________ -4.9333E+00 + Poloidal_plane_angle_between_vertical_and_inner_leg_(rad)_______________ (thetai)______________________ 2.0820E-01 + Poloidal_plane_angle_between_vertical_and_outer_leg_(rad)_______________ (thetao)______________________ 1.0429E+00 + Poloidal_plane_angle_between_inner_leg_and_plate_(rad)__________________ (betai)_______________________ 1.0000E+00 + Poloidal_plane_angle_between_outer_leg_and_plate_(rad)__________________ (betao)_______________________ 1.0000E+00 + Inner_divertor_leg_poloidal_length_(m)__________________________________ (plsepi)______________________ 1.0000E+00 + Outer_divertor_leg_poloidal_length_(m)__________________________________ (plsepo)______________________ 1.5000E+00 + Inner_divertor_plate_length_(m)_________________________________________ (plleni)______________________ 1.0000E+00 + Outer_divertor_plate_length_(m)_________________________________________ (plleno)______________________ 1.0000E+00 + Inner_strike_point,_radial_(m)__________________________________________ (rspi)________________________ 5.6883E+00 + Inner_strike_point,_vertical_(m)________________________________________ (zspi)________________________ -5.1400E+00 + Inner_plate_top,_radial_(m)_____________________________________________ (rplti)_______________________ 5.8656E+00 + Inner_plate_top,_vertical_(m)___________________________________________ (zplti)_______________________ -4.6725E+00 + Inner_plate_bottom,_radial_(m)__________________________________________ (rplbi)_______________________ 5.5109E+00 + Inner_plate_bottom,_vertical_(m)________________________________________ (zplbi)_______________________ -5.6075E+00 + Outer_strike_point,_radial_(m)__________________________________________ (rspo)________________________ 7.4223E+00 + Outer_strike_point,_vertical_(m)________________________________________ (zspo)________________________ -6.2291E+00 + Outer_plate_top,_radial_(m)_____________________________________________ (rplto)_______________________ 7.6496E+00 + Outer_plate_top,_vertical_(m)___________________________________________ (zplto)_______________________ -5.7838E+00 + Outer_plate_bottom,_radial_(m)__________________________________________ (rplbo)_______________________ 7.1949E+00 + Outer_plate_bottom,_vertical_(m)________________________________________ (zplbo)_______________________ -6.6744E+00 + Calculated_maximum_divertor_height_(m)__________________________________ (divht)_______________________ 2.0019E+00 + # TF coils # + Allowable_maximum_shear_stress_in_TF_coil_case_(Tresca_criterion)_(Pa)__ (sig_tf_case_max)_____________ 7.5000E+08 + Allowable_maximum_shear_stress_in_TF_coil_conduit_(Tresca_criterion)_(Pa (sig_tf_wp_max)_______________ 7.5000E+08 + WP_transverse_modulus_(GPa)_____________________________________________ (eyoung_wp_trans*1.0d-9)______ 4.3534E+01 OP + WP_vertical_modulus_(GPa)_______________________________________________ (eyoung_wp_axial*1.0d-9)______ 1.1510E+02 OP + WP_transverse_Poissons_ratio____________________________________________ (poisson_wp_trans)____________ 3.0390E-01 OP + WP_vertical-transverse_Pois._rat._______________________________________ (poisson_wp_axial)____________ 3.1568E-01 OP + Radial____stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_r_max(1))_____________ 4.8849E-08 + toroidal__stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_t_max(1))_____________ -4.8724E+08 + Vertical__stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_z_max(1))_____________ 2.6028E+08 + Von-Mises_stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_vmises_max(1))________ 6.5725E+08 + Maximum_shear_stress_for_the_Tresca_yield_criterion_1_(Pa)______________ (sig_tf_tresca_max(1))________ 7.4752E+08 + Radial____stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_r_max(2))_____________ -1.5411E+08 + toroidal__stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_t_max(2))_____________ -3.7861E+08 + Vertical__stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_z_max(2))_____________ 2.6028E+08 + Von-Mises_stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_vmises_max(2))________ 5.5645E+08 + Maximum_shear_stress_for_the_Tresca_yield_criterion_2_(Pa)______________ (sig_tf_tresca_max(2))________ 6.3889E+08 + Radial____stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_r_max(3))_____________ 6.1398E+06 + toroidal__stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_t_max(3))_____________ -3.6314E+08 + Vertical__stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_z_max(3))_____________ 1.4510E+08 + Von-Mises_stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_vmises_max(3))________ 4.5345E+08 + Maximum_shear_stress_for_the_Tresca_yield_criterion_3_(Pa)______________ (sig_tf_tresca_max(3))________ 5.0824E+08 + Maximum_radial_deflection_at_midplane_(m)_______________________________ (deflect)_____________________ -6.2714E-03 OP + Vertical_strain_on_casing_______________________________________________ (casestr)_____________________ 1.2697E-03 OP + Radial_strain_on_insulator______________________________________________ (insstrain)___________________ -7.6923E-03 OP + Conductor_technology____________________________________________________ (i_tf_sup)____________________ 1 + Superconductor_material_________________________________________________ (i_tf_sc_mat)_________________ 1 + Presence_of_TF_demountable_joints_______________________________________ (itart)_______________________ 0 + TF_inboard_leg_support_strategy_________________________________________ (i_tf_bucking)________________ 1 + Number_of_TF_coils______________________________________________________ (n_tf)________________________ 16 + Inboard_leg_centre_radius_(m)___________________________________________ (r_tf_inboard_mid)____________ 3.1673E+00 OP + Outboard_leg_centre_radius_(m)__________________________________________ (r_tf_outboard_mid)___________ 1.4985E+01 OP + Total_inboard_leg_radial_thickness_(m)__________________________________ (tfcth)_______________________ 9.1597E-01 ITV + Total_outboard_leg_radial_thickness_(m)_________________________________ (tfthko)______________________ 9.1597E-01 + Outboard_leg_toroidal_thickness_(m)_____________________________________ (tftort)______________________ 1.4145E+00 OP + Maximum_inboard_edge_height_(m)_________________________________________ (hmax)________________________ 8.8182E+00 OP + Mean_coil_circumference_(including_inboard_leg_length)_(m)______________ (tfleng)______________________ 4.7937E+01 OP + Vertical_TF_shape_______________________________________________________ (i_tf_shape)__________________ 1 + TF_coil_arc_point_0_R_(m)_______________________________________________ (xarc(1))_____________________ 3.6253E+00 + TF_coil_arc_point_0_Z_(m)_______________________________________________ (yarc(1))_____________________ 4.5506E+00 + TF_coil_arc_point_1_R_(m)_______________________________________________ (xarc(2))_____________________ 7.4667E+00 + TF_coil_arc_point_1_Z_(m)_______________________________________________ (yarc(2))_____________________ 7.5843E+00 + TF_coil_arc_point_2_R_(m)_______________________________________________ (xarc(3))_____________________ 1.4527E+01 + TF_coil_arc_point_2_Z_(m)_______________________________________________ (yarc(3))_____________________ 0.0000E+00 + TF_coil_arc_point_3_R_(m)_______________________________________________ (xarc(4))_____________________ 7.4667E+00 + TF_coil_arc_point_3_Z_(m)_______________________________________________ (yarc(4))_____________________ -8.8182E+00 + TF_coil_arc_point_4_R_(m)_______________________________________________ (xarc(5))_____________________ 3.6253E+00 + TF_coil_arc_point_4_Z_(m)_______________________________________________ (yarc(5))_____________________ -5.2909E+00 + TF_cross-section_(total)_(m2)___________________________________________ (tfareain)____________________ 1.8229E+01 + Total_steel_cross-section_(m2)__________________________________________ (a_tf_steel*n_tf)_____________ 1.2853E+01 + Total_steel_TF_fraction_________________________________________________ (f_tf_steel)__________________ 7.0508E-01 + Total_Insulation_cross-section_(total)_(m2)_____________________________ (a_tf_ins*n_tf)_______________ 8.4752E-01 + Total_Insulation_fraction_______________________________________________ (f_tf_ins)____________________ 4.6493E-02 + Casing_cross_section_area_(per_leg)_(m2)________________________________ (acasetf)_____________________ 5.6444E-01 + Inboard_leg_case_plasma_side_wall_thickness_(m)_________________________ (casthi)______________________ 6.0000E-02 + Inboard_leg_case_inboard_"nose"_thickness_(m)___________________________ (thkcas)______________________ 2.8216E-01 ITV + Inboard_leg_case_sidewall_thickness_at_its_narrowest_point_(m)__________ (casths)______________________ 5.0000E-02 + External_case_mass_per_coil_(kg)________________________________________ (whtcas)______________________ 5.5456E+05 OP + WP_cross_section_area_with_insulation_and_insertion_(per_coil)_(m2)_____ (awpc)________________________ 5.7486E-01 + WP_cross_section_area_(per_coil)_(m2)___________________________________ (aswp)________________________ 5.1696E-01 + Winding_pack_radial_thickness_(m)_______________________________________ (dr_tf_wp)____________________ 5.0416E-01 ITV + Winding_pack_toroidal_width_1_(m)_______________________________________ (wwp1)________________________ 1.1904E+00 OP + Winding_pack_toroidal_width_2_(m)_______________________________________ (wwp2)________________________ 1.0901E+00 OP + Ground_wall_insulation_thickness_(m)____________________________________ (tinstf)______________________ 8.0000E-03 + Winding_pack_insertion_gap_(m)__________________________________________ (tfinsgap)____________________ 1.0000E-02 + Steel_WP_cross-section_(total)_(m2)_____________________________________ (aswp*n_tf)___________________ 3.8217E+00 + Steel_WP_fraction_______________________________________________________ (aswp/awpc)___________________ 4.1550E-01 + Insulation_WP_fraction__________________________________________________ (aiwp/awpc)___________________ 4.7934E-02 + Cable_WP_fraction_______________________________________________________ ((awpc-aswp-aiwp)/awpc)_______ 5.3656E-01 + Turn_parametrisation____________________________________________________ (i_tf_turns_integer)__________ 0 + Number_of_turns_per_TF_coil_____________________________________________ (n_tf_turn)___________________ 1.4739E+02 OP + Width_of_turn_including_inter-turn_insulation_(m)_______________________ (t_turn_tf)___________________ 5.9223E-02 OP + Width_of_conductor_(square)_(m)_________________________________________ (t_conductor)_________________ 5.7623E-02 OP + Width_of_space_inside_conductor_(m)_____________________________________ (t_cable)_____________________ 4.1604E-02 OP + Steel_conduit_thickness_(m)_____________________________________________ (thwcndut)____________________ 8.0099E-03 ITV + Inter-turn_insulation_thickness_(m)_____________________________________ (thicndut)____________________ 8.0000E-04 + Diameter_of_central_helium_channel_in_cable_____________________________ (dhecoil)_____________________ 1.0000E-02 + internal_area_of_the_cable_space________________________________________ (acstf)_______________________ 1.6999E-03 + Coolant_fraction_in_conductor_excluding_central_channel_________________ (vftf)________________________ 3.0000E-01 + Copper_fraction_of_conductor____________________________________________ (fcutfsu)_____________________ 8.4212E-01 ITV + Superconductor_fraction_of_conductor____________________________________ (1-fcutfsu)___________________ 1.5788E-01 + Check_total_area_fractions_in_winding_pack_=_1__________________________ ______________________________ 1.0000E+00 + minimum_TF_conductor_temperature_margin__(K)____________________________ (tmargmin_tf)_________________ 1.5000E+00 + TF_conductor_temperature_margin_(K)_____________________________________ (tmargtf)_____________________ 1.5049E+00 + Elastic_properties_behavior_____________________________________________ (i_tf_cond_eyoung_axial)______ 0 + Conductor_axial_Youngs_modulus__________________________________________ (eyoung_cond_axial)___________ 0.0000E+00 + Conductor_transverse_Youngs_modulus_____________________________________ (eyoung_cond_trans)___________ 0.0000E+00 + Superconductor_mass_per_coil_(kg)_______________________________________ (whtconsc)____________________ 4.6964E+03 OP + Copper_mass_per_coil_(kg)_______________________________________________ (whtconcu)____________________ 5.8073E+04 OP + Steel_conduit_mass_per_coil_(kg)________________________________________ (whtconsh)____________________ 8.9310E+04 OP + Conduit_insulation_mass_per_coil_(kg)___________________________________ (whtconin)____________________ 2.3777E+03 OP + Total_conduit_mass_per_coil_(kg)________________________________________ (whtcon)______________________ 1.5446E+05 OP + Mass_of_each_TF_coil_(kg)_______________________________________________ (whttf/n_tf)__________________ 7.1402E+05 OP + Total_TF_coil_mass_(kg)_________________________________________________ (whttf)_______________________ 1.1424E+07 OP + Nominal_peak_field_assuming_toroidal_symmetry_(T)_______________________ (bmaxtf)______________________ 1.2178E+01 OP + Total_current_in_all_TF_coils_(MA)______________________________________ (ritfc/1.D6)__________________ 2.1176E+02 OP + TF_coil_current_(summed_over_all_coils)_(A)_____________________________ (ritfc)_______________________ 2.1176E+08 + Actual_peak_field_at_discrete_conductor_(T)_____________________________ (bmaxtfrp)____________________ 1.2636E+01 OP + Winding_pack_current_density_(A/m2)_____________________________________ (jwptf)_______________________ 2.5602E+07 OP + Inboard_leg_mid-plane_conductor_current_density_(A/m2)__________________ (oacdcp)______________________ 1.1617E+07 + Total_stored_energy_in_TF_coils_(GJ)____________________________________ (estotftgj)___________________ 1.2161E+02 OP + Inboard_vertical_tension_per_coil_(N)___________________________________ (vforce)______________________ 2.0908E+08 OP + Outboard_vertical_tension_per_coil_(N)__________________________________ (vforce_outboard)_____________ 2.0908E+08 OP + inboard_vertical_tension_fraction_(-)___________________________________ (f_vforce_inboard)____________ 5.0000E-01 OP + Centring_force_per_coil_(N/m)___________________________________________ (cforce)______________________ 8.0590E+07 OP + Max_allowed_tfcoil_variables.ripple_amplitude_at_plasma_outboard_midplan (ripmax)______________________ 6.0000E-01 + Ripple_amplitude_at_plasma_outboard_midplane_(%)________________________ (ripple)______________________ 6.0000E-01 OP + Actual_quench_time_(or_time_constant)_(s)_______________________________ (tdmptf)______________________ 1.8429E+01 ITV + Vacuum_Vessel_stress_on_quench_(Pa)_____________________________________ (vv_stress_quench)____________ 6.1442E+07 OP + Maximum_allowed_voltage_during_quench_due_to_insulation_(kV)____________ (vdalw)_______________________ 9.5837E+00 ITV + Actual_quench_voltage_(kV)______________________________________________ (vtfskv)______________________ 9.1862E+00 OP + Maximum_allowed_temp_rise_during_a_quench_(K)___________________________ (tmaxpro)_____________________ 1.5000E+02 + # Superconducting TF Coils # + Superconductor_switch___________________________________________________ (isumat)______________________ 1 + Critical_field_at_zero_temperature_and_strain_(T)_______________________ (bc20m)_______________________ 3.2970E+01 + Critical_temperature_at_zero_field_and_strain_(K)_______________________ (tc0m)________________________ 1.6060E+01 + Helium_temperature_at_peak_field_(=_superconductor_temperature)_(K)_____ (thelium)_____________________ 4.7500E+00 + Total_helium_fraction_inside_cable_space________________________________ (fhetot)______________________ 3.4620E-01 OP + Copper_fraction_of_conductor____________________________________________ (fcutfsu)_____________________ 8.4212E-01 ITV + Residual_manufacturing_strain_on_superconductor_________________________ (str_tf_con_res)______________ -5.0000E-03 + Self-consistent_strain_on_superconductor________________________________ (str_wp)______________________ 2.0730E-03 + Critical_current_density_in_superconductor_(A/m2)_______________________ (jcritsc)_____________________ 7.1337E+08 OP + Critical_current_density_in_strand_(A/m2)_______________________________ (jcritstr)____________________ 1.1263E+08 OP + Critical_current_density_in_winding_pack_(A/m2)_________________________ (jwdgcrt)_____________________ 3.5688E+07 OP + Actual_current_density_in_winding_pack_(A/m2)___________________________ (jwdgop)______________________ 2.5602E+07 OP + Minimum_allowed_temperature_margin_in_superconductor_(K)________________ (tmargmin_tf)_________________ 1.5000E+00 + Actual_temperature_margin_in_superconductor_(K)_________________________ (tmarg)_______________________ 1.5049E+00 OP + Critical_current_(A)____________________________________________________ (icrit)_______________________ 1.2517E+05 OP + Actual_current_(A)______________________________________________________ (cpttf)_______________________ 8.9795E+04 ITV + Actual_current_/_critical_current_______________________________________ (iooic)_______________________ 7.1737E-01 OP + # Central Solenoid and PF Coils # + Central_solenoid_superconductor_material________________________________ (isumatoh)____________________ 1 + Maximum_field_at_Beginning_Of_Pulse_(T)_________________________________ (bmaxoh0)_____________________ 1.4050E+01 OP + Critical_superconductor_current_density_at_BOP_(A/m2)___________________ (jscoh_bop)___________________ 3.4918E+08 OP + Critical_strand_current_density_at_BOP_(A/m2)___________________________ (jstrandoh_bop)_______________ 1.0475E+08 OP + Allowable_overall_current_density_at_BOP_(A/m2)_________________________ (rjohc0)______________________ 3.5294E+07 OP + Actual_overall_current_density_at_BOP_(A/m2)____________________________ (cohbop)______________________ 1.9126E+07 OP + Maximum_field_at_End_Of_Flattop_(T)_____________________________________ (bmaxoh)______________________ 1.3920E+01 OP + Critical_superconductor_current_density_at_EOF_(A/m2)___________________ (jscoh_eof)___________________ 3.6097E+08 OP + Critical_strand_current_density_at_EOF_(A/m2)___________________________ (jstrandoh_eof)_______________ 1.0829E+08 OP + Allowable_overall_current_density_at_EOF_(A/m2)_________________________ (rjohc)_______________________ 3.6485E+07 OP + Actual_overall_current_density_at_EOF_(A/m2)____________________________ (coheof)______________________ 2.0264E+07 ITV + CS_inside_radius_(m)____________________________________________________ (bore)________________________ 1.9854E+00 ITV + CS_thickness_(m)________________________________________________________ (ohcth)_______________________ 5.7587E-01 ITV + Gap_between_central_solenoid_and_TF_coil_(m)____________________________ (gapoh)_______________________ 8.0000E-02 + CS_overall_cross-sectional_area_(m2)____________________________________ (areaoh)______________________ 9.1407E+00 OP + CS_conductor+void_cross-sectional_area_(m2)_____________________________ (awpoh)_______________________ 4.3996E+00 OP + ___CS_conductor_cross-sectional_area_(m2)_______________________________ (awpoh*(1-vfohc))_____________ 3.0797E+00 OP + ___CS_void_cross-sectional_area_(m2)____________________________________ (awpoh*vfohc)_________________ 1.3199E+00 OP + CS_steel_cross-sectional_area_(m2)______________________________________ (areaoh-awpoh)________________ 4.7411E+00 OP + CS_steel_area_fraction__________________________________________________ (oh_steel_frac)_______________ 5.1868E-01 ITV + Switch_for_CS_stress_calculation________________________________________ (i_cs_stress)_________________ 0 + Allowable_stress_in_CS_steel_(Pa)_______________________________________ (alstroh)_____________________ 7.5000E+08 + Hoop_stress_in_CS_steel_(Pa)____________________________________________ (sig_hoop)____________________ 6.7569E+08 OP + Axial_stress_in_CS_steel_(Pa)___________________________________________ (sig_axial)___________________ -7.6205E+08 OP + Maximum_shear_stress_in_CS_steel_for_the_Tresca_criterion_(Pa)__________ (s_tresca_oh)_________________ 6.7569E+08 OP + Axial_force_in_CS_(N)___________________________________________________ (axial_force)_________________ -1.6256E+09 OP + Residual_manufacturing_strain_in_CS_superconductor_material_____________ (tfcoil_variables.str_cs_con_r -5.0000E-03 + Copper_fraction_in_strand_______________________________________________ (fcuohsu)_____________________ 7.0000E-01 + Void_(coolant)_fraction_in_conductor____________________________________ (vfohc)_______________________ 3.0000E-01 + Helium_coolant_temperature_(K)__________________________________________ (tftmp)_______________________ 4.7500E+00 + CS_temperature_margin_(K)_______________________________________________ (tmargoh)_____________________ 1.5052E+00 OP + Minimum_permitted_temperature_margin_(K)________________________________ (tmargmin_cs)_________________ 1.5000E+00 + Residual_hoop_stress_in_CS_Steel_(Pa)___________________________________ (residual_sig_hoop)___________ 2.4000E+08 + Minimum_burn_time_(s)___________________________________________________ (tbrnmn)______________________ 7.2000E+03 + Initial_vertical_crack_size_(m)_________________________________________ (t_crack_vertical)____________ 8.9000E-04 + Initial_radial_crack_size_(m)___________________________________________ (t_crack_radial)______________ 2.6700E-03 + CS_turn_area_(m)________________________________________________________ (a_oh_turn)___________________ 1.9739E-03 + CS_turn_length_(m)______________________________________________________ (l_cond_cst)__________________ 7.6953E-02 + CS_turn_internal_cable_space_radius_(m)_________________________________ (r_in_cst)____________________ 7.4740E-03 + CS_turn_width_(m)_______________________________________________________ (d_cond_cst)__________________ 2.5651E-02 + CS_structural_vertical_thickness_(m)____________________________________ (t_structural_vertical)_______ 5.3514E-03 + CS_structural_radial_thickness_(m)______________________________________ (t_structural_radial)_________ 5.3514E-03 + Allowable_number_of_cycles_till_CS_fracture_____________________________ (n_cycle)_____________________ 1.3378E+02 OP + Minimum_number_of_cycles_required_till_CS_fracture______________________ (n_cycle_min)_________________ 2.0000E+04 OP + PF_coil_superconductor_material_________________________________________ (isumatpf)____________________ 3 + Copper_fraction_in_conductor____________________________________________ (fcupfsu)_____________________ 6.9000E-01 + Maximum_permissible_tensile_stress_(MPa)________________________________ (sigpfcalw)___________________ 5.0000E+02 + JxB_hoop_force_fraction_supported_by_case_______________________________ (sigpfcf)_____________________ 6.6600E-01 + PF_coil_0_radius_(m)____________________________________________________ (rpf[0]_______________________ 5.5667E+00 + PF_coil_0_vertical_position_(m)_________________________________________ (zpf[0])______________________ 9.3603E+00 + PF_coil_0_radial_thickness_(m)__________________________________________ (pfdr(0))_____________________ 1.2727E+00 + PF_coil_0_vertical_thickness_(m)________________________________________ (pfdz(0))_____________________ 1.2727E+00 + PF_coil_0_turns_________________________________________________________ (turns[0])____________________ 4.4541E+02 + PF_coil_0_current_(MA)__________________________________________________ (ric[0])______________________ 1.7816E+01 + PF_coil_0_field_(T)_____________________________________________________ (bpf[0])______________________ 6.2280E+00 + PF_coil_1_radius_(m)____________________________________________________ (rpf[1]_______________________ 5.5667E+00 + PF_coil_1_vertical_position_(m)_________________________________________ (zpf[1])______________________ -1.0594E+01 + PF_coil_1_radial_thickness_(m)__________________________________________ (pfdr(1))_____________________ 1.3651E+00 + PF_coil_1_vertical_thickness_(m)________________________________________ (pfdz(1))_____________________ -1.3651E+00 + PF_coil_1_turns_________________________________________________________ (turns[1])____________________ 5.1248E+02 + PF_coil_1_current_(MA)__________________________________________________ (ric[1])______________________ 2.0499E+01 + PF_coil_1_field_(T)_____________________________________________________ (bpf[1])______________________ 6.6990E+00 + PF_coil_2_radius_(m)____________________________________________________ (rpf[2]_______________________ 1.6731E+01 + PF_coil_2_vertical_position_(m)_________________________________________ (zpf[2])______________________ 2.6667E+00 + PF_coil_2_radial_thickness_(m)__________________________________________ (pfdr(2))_____________________ 1.1332E+00 + PF_coil_2_vertical_thickness_(m)________________________________________ (pfdz(2))_____________________ 1.1332E+00 + PF_coil_2_turns_________________________________________________________ (turns[2])____________________ 1.9262E+02 + PF_coil_2_current_(MA)__________________________________________________ (ric[2])______________________ -7.7049E+00 + PF_coil_2_field_(T)_____________________________________________________ (bpf[2])______________________ 2.6389E+00 + PF_coil_3_radius_(m)____________________________________________________ (rpf[3]_______________________ 1.6731E+01 + PF_coil_3_vertical_position_(m)_________________________________________ (zpf[3])______________________ -2.6667E+00 + PF_coil_3_radial_thickness_(m)__________________________________________ (pfdr(3))_____________________ 1.1332E+00 + PF_coil_3_vertical_thickness_(m)________________________________________ (pfdz(3))_____________________ -1.1332E+00 + PF_coil_3_turns_________________________________________________________ (turns[3])____________________ 1.9262E+02 + PF_coil_3_current_(MA)__________________________________________________ (ric[3])______________________ -7.7049E+00 + PF_coil_3_field_(T)_____________________________________________________ (bpf[3])______________________ 2.6389E+00 + PF_coil_4_radius_(m)____________________________________________________ (rpf[4]_______________________ 1.5209E+01 + PF_coil_4_vertical_position_(m)_________________________________________ (zpf[4])______________________ 7.4667E+00 + PF_coil_4_radial_thickness_(m)__________________________________________ (pfdr(4))_____________________ 8.0773E-01 + PF_coil_4_vertical_thickness_(m)________________________________________ (pfdz(4))_____________________ 8.0773E-01 + PF_coil_4_turns_________________________________________________________ (turns[4])____________________ 1.3049E+02 + PF_coil_4_current_(MA)__________________________________________________ (ric[4])______________________ -5.2194E+00 + PF_coil_4_field_(T)_____________________________________________________ (bpf[4])______________________ 2.5737E+00 + PF_coil_5_radius_(m)____________________________________________________ (rpf[5]_______________________ 1.5209E+01 + PF_coil_5_vertical_position_(m)_________________________________________ (zpf[5])______________________ -7.4667E+00 + PF_coil_5_radial_thickness_(m)__________________________________________ (pfdr(5))_____________________ 8.0773E-01 + PF_coil_5_vertical_thickness_(m)________________________________________ (pfdz(5))_____________________ -8.0773E-01 + PF_coil_5_turns_________________________________________________________ (turns[5])____________________ 1.3049E+02 + PF_coil_5_current_(MA)__________________________________________________ (ric[5])______________________ -5.2194E+00 + PF_coil_5_field_(T)_____________________________________________________ (bpf[5])______________________ 2.5737E+00 + Central_solenoid_radius_(m)_____________________________________________ (rpf[nohc-1])_________________ 2.2734E+00 + Central_solenoid_vertical_position_(m)__________________________________ (zpf[nohc-1])_________________ 0.0000E+00 + Central_solenoid_radial_thickness_(m)___________________________________ (ohdr)________________________ 5.7587E-01 + Central_solenoid_vertical_thickness_(m)_________________________________ (ohdz)________________________ 1.5873E+01 + Central_solenoid_turns__________________________________________________ (turns[nohc-1])_______________ 4.6308E+03 + Central_solenoid_current_(MA)___________________________________________ (ric[nohc-1])_________________ -1.8523E+02 + Central_solenoid_field_(T)______________________________________________ (bpf[nohc-1])_________________ 1.4050E+01 + Sum_of_squares_of_residuals_____________________________________________ (ssq0)________________________ 3.5207E-04 OP + Smoothing_parameter_____________________________________________________ (alfapf)______________________ 5.0000E-10 + # Volt Second Consumption # + Total_volt-second_consumption_by_coils_(Wb)_____________________________ (vstot)_______________________ -5.8000E+02 OP + # Waveforms # + Ratio_of_central_solenoid_current_at_beginning_of_Pulse_/_end_of_flat-to (fcohbop)_____________________ 9.4380E-01 ITV + Ratio_of_central_solenoid_current_at_beginning_of_Flat-top_/_end_of_flat (fcohbof)_____________________ -1.4083E-01 OP + # PF Circuit Waveform Data # + Number_of_PF_circuits_including_CS_and_plasma___________________________ (ncirt)_______________________ 8 + PF_Circuit_0_Time_point_0_(A)___________________________________________ (pfc0t0)______________________ 0.0000E+00 + PF_Circuit_0_Time_point_1_(A)___________________________________________ (pfc0t1)______________________ 1.3971E+07 + PF_Circuit_0_Time_point_2_(A)___________________________________________ (pfc0t2)______________________ 1.7816E+07 + PF_Circuit_0_Time_point_3_(A)___________________________________________ (pfc0t3)______________________ 1.7816E+07 + PF_Circuit_0_Time_point_4_(A)___________________________________________ (pfc0t4)______________________ 9.2844E+05 + PF_Circuit_0_Time_point_5_(A)___________________________________________ (pfc0t5)______________________ 0.0000E+00 + PF_Circuit_1_Time_point_0_(A)___________________________________________ (pfc1t0)______________________ 0.0000E+00 + PF_Circuit_1_Time_point_1_(A)___________________________________________ (pfc1t1)______________________ 1.8269E+07 + PF_Circuit_1_Time_point_2_(A)___________________________________________ (pfc1t2)______________________ 2.0499E+07 + PF_Circuit_1_Time_point_3_(A)___________________________________________ (pfc1t3)______________________ 2.0499E+07 + PF_Circuit_1_Time_point_4_(A)___________________________________________ (pfc1t4)______________________ -1.5831E+06 + PF_Circuit_1_Time_point_5_(A)___________________________________________ (pfc1t5)______________________ 0.0000E+00 + PF_Circuit_2_Time_point_0_(A)___________________________________________ (pfc2t0)______________________ -0.0000E+00 + PF_Circuit_2_Time_point_1_(A)___________________________________________ (pfc2t1)______________________ 4.9542E+05 + PF_Circuit_2_Time_point_2_(A)___________________________________________ (pfc2t2)______________________ -7.1060E+06 + PF_Circuit_2_Time_point_3_(A)___________________________________________ (pfc2t3)______________________ -7.1060E+06 + PF_Circuit_2_Time_point_4_(A)___________________________________________ (pfc2t4)______________________ -7.7049E+06 + PF_Circuit_2_Time_point_5_(A)___________________________________________ (pfc2t5)______________________ -0.0000E+00 + PF_Circuit_3_Time_point_0_(A)___________________________________________ (pfc3t0)______________________ -0.0000E+00 + PF_Circuit_3_Time_point_1_(A)___________________________________________ (pfc3t1)______________________ 4.9542E+05 + PF_Circuit_3_Time_point_2_(A)___________________________________________ (pfc3t2)______________________ -7.1060E+06 + PF_Circuit_3_Time_point_3_(A)___________________________________________ (pfc3t3)______________________ -7.1060E+06 + PF_Circuit_3_Time_point_4_(A)___________________________________________ (pfc3t4)______________________ -7.7049E+06 + PF_Circuit_3_Time_point_5_(A)___________________________________________ (pfc3t5)______________________ -0.0000E+00 + PF_Circuit_4_Time_point_0_(A)___________________________________________ (pfc4t0)______________________ -0.0000E+00 + PF_Circuit_4_Time_point_1_(A)___________________________________________ (pfc4t1)______________________ 3.2650E+05 + PF_Circuit_4_Time_point_2_(A)___________________________________________ (pfc4t2)______________________ -4.8247E+06 + PF_Circuit_4_Time_point_3_(A)___________________________________________ (pfc4t3)______________________ -4.8247E+06 + PF_Circuit_4_Time_point_4_(A)___________________________________________ (pfc4t4)______________________ -5.2194E+06 + PF_Circuit_4_Time_point_5_(A)___________________________________________ (pfc4t5)______________________ -0.0000E+00 + PF_Circuit_5_Time_point_0_(A)___________________________________________ (pfc5t0)______________________ -0.0000E+00 + PF_Circuit_5_Time_point_1_(A)___________________________________________ (pfc5t1)______________________ 3.2650E+05 + PF_Circuit_5_Time_point_2_(A)___________________________________________ (pfc5t2)______________________ -4.8247E+06 + PF_Circuit_5_Time_point_3_(A)___________________________________________ (pfc5t3)______________________ -4.8247E+06 + PF_Circuit_5_Time_point_4_(A)___________________________________________ (pfc5t4)______________________ -5.2194E+06 + PF_Circuit_5_Time_point_5_(A)___________________________________________ (pfc5t5)______________________ -0.0000E+00 + CS_Circuit_Time_point_0_(A)_____________________________________________ (cs_t0)_______________________ -0.0000E+00 + CS_Circuit_Time_point_1_(A)_____________________________________________ (cs_t1)_______________________ 1.7482E+08 + CS_Circuit_Time_point_2_(A)_____________________________________________ (cs_t2)_______________________ 2.6086E+07 + CS_Circuit_Time_point_3_(A)_____________________________________________ (cs_t3)_______________________ 2.6086E+07 + CS_Circuit_Time_point_4_(A)_____________________________________________ (cs_t4)_______________________ -1.8523E+08 + CS_Circuit_Time_point_5_(A)_____________________________________________ (cs_t5)_______________________ -0.0000E+00 + Plasma_Time_point_0_(A)_________________________________________________ (plasmat0)____________________ 0.0000E+00 + Plasma_Time_point_1_(A)_________________________________________________ (plasmat1)____________________ 0.0000E+00 + Plasma_Time_point_2_(A)_________________________________________________ (plasmat2)____________________ 1.6631E+07 + Plasma_Time_point_3_(A)_________________________________________________ (plasmat3)____________________ 1.6631E+07 + Plasma_Time_point_4_(A)_________________________________________________ (plasmat4)____________________ 1.6631E+07 + Plasma_Time_point_5_(A)_________________________________________________ (plasmat5)____________________ 0.0000E+00 + # Support Structure # + Outer_PF_coil_fence_mass_(kg)___________________________________________ (fncmass)_____________________ 2.2924E+05 OP + Intercoil_support_structure_mass_(kg)___________________________________ (aintmass)____________________ 4.3045E+06 OP + Mass_of_cooled_components_(kg)__________________________________________ (coldmass)____________________ 3.4369E+07 OP + Gravity_support_structure_mass_(kg)_____________________________________ (clgsmass)____________________ 1.2760E+06 OP + Torus_leg_support_mass_(kg)_____________________________________________ (gsm1)________________________ 8.5820E+04 OP + Ring_beam_mass_(kg)_____________________________________________________ (gsm2)________________________ 4.0088E+05 OP + Ring_legs_mass_(kg)_____________________________________________________ (gsm3)________________________ 6.8283E+05 OP + # PF Coil Inductances # + # Nuclear Heating Magnets Before Renormalisation # + Shield_line_density_(tonne/m2)__________________________________________ (x_shield)____________________ 4.0560E+00 + Blanket_line_density_(tonne/m2)_________________________________________ (x_blanket)___________________ 2.2911E+00 + Unit_nuclear_heating_in_TF_coil_(W/GW)__________________________________ (tfc_nuc_heating)_____________ 1.4866E+04 + Total_nuclear_heating_in_TF_coil_(MW)___________________________________ (ptfnuc.)_____________________ 2.4085E-02 + powfmw__________________________________________________________________ (powfmw.)_____________________ 1.6202E+03 + total_mass_of_the_TF_coils_(kg)_________________________________________ (whttf)_______________________ 1.1424E+07 + # Pumping for primary coolant (helium) # + Pressure_drop_in_FW_and_blanket_coolant_incl._hx_and_pipes_(Pa)_________ (dp_he)_______________________ 5.5000E+05 + Fraction_of_FW_and_blanket_thermal_power_required_for_pumping___________ (fpump)_______________________ 8.9463E-02 OP + Total_power_absorbed_by_FW_&_blanket_(MW)_______________________________ (p_plasma)____________________ 1.6698E+03 OP + Inlet_temperature_of_FW_&_blanket_coolant_pump_(K)______________________ (t_in_compressor)_____________ 5.5703E+02 OP + Coolant_pump_outlet/Inlet_temperature_of_FW_&_blanket_(K)_______________ (t_in_bb)_____________________ 5.7313E+02 + Outlet_temperature_of_FW_&_blanket_(K)__________________________________ (t_out_bb)____________________ 7.7313E+02 + Mechanical_pumping_power_for_FW_and_blanket_cooling_loop_including_heat_ (htpmw_fw_blkt)_______________ 1.6407E+02 OP + Mechanical_pumping_power_for_divertor_(MW)______________________________ (htpmw_div)___________________ 1.6906E+00 OP + Mechanical_pumping_power_for_shield_and_vacuum_vessel_(MW)______________ (htpmw_shld)__________________ 7.0688E-03 OP + # First wall and blanket : CCFE HCPB model # + Titanium_beryllide_fraction_____________________________________________ (fbltibe12)___________________ 3.7500E-01 + Lithium_orthosilicate_fraction__________________________________________ (fblli2sio4)__________________ 3.7500E-01 + Steel_fraction__________________________________________________________ (fblss_ccfe)__________________ 9.7050E-02 + Coolant_fraction________________________________________________________ (vfcblkt)_____________________ 5.2950E-02 + Purge_gas_fraction______________________________________________________ (vfpblkt)_____________________ 1.0000E-01 + First_Wall_Armour_Volume_(m3)___________________________________________ (fw_armour_vol)_______________ 5.8692E+00 + First_Wall_Volume_(m3)__________________________________________________ (volfw)_______________________ 1.9807E+01 + Blanket_Volume_(m3)_____________________________________________________ (volblkt)_____________________ 1.1849E+03 + Shield_Volume_(m3)______________________________________________________ (volshld)_____________________ 7.8520E+02 + Vacuum_vessel_volume_(m3)_______________________________________________ (vdewin)______________________ 1.0178E+03 + First_Wall_Armour_Mass_(kg)_____________________________________________ (fw_armour_mass)______________ 1.1298E+05 OP + First_Wall_Mass,_excluding_armour_(kg)__________________________________ (fwmass)______________________ 1.5449E+05 OP + Blanket_Mass_-_Total(kg)________________________________________________ (whtblkt)_____________________ 2.9676E+06 OP + ____Blanket_Mass_-_TiBe12_(kg)__________________________________________ (whtbltibe12)_________________ 1.0042E+06 OP + ____Blanket_Mass_-_Li4SiO4_(kg)_________________________________________ (whtblli4sio4)________________ 1.0664E+06 OP + ____Blanket_Mass_-_Steel_(kg)___________________________________________ (whtblss)_____________________ 8.9696E+05 OP + Total_mass_of_armour,_first_wall_and_blanket_(kg)_______________________ (armour_fw_bl_mass)___________ 3.2350E+06 OP + Shield_Mass_(kg)________________________________________________________ (whtshld)_____________________ 2.4498E+06 OP + Vacuum_vessel_mass_(kg)_________________________________________________ (vvmass)______________________ 7.9388E+06 OP + Total_nuclear_heating_in_TF+PF_coils_(CS_is_negligible)_(MW)____________ (ptfnuc)______________________ 2.5118E-02 OP + Total_nuclear_heating_in_FW_(MW)________________________________________ (pnucfw)______________________ 1.6315E+02 OP + Total_nuclear_heating_in_the_blanket_(including_emult)_(MW)_____________ (pnucblkt)____________________ 1.2901E+03 OP + Total_nuclear_heating_in_the_shield_(MW)________________________________ (pnucshld)____________________ 1.4138E+00 OP + Total_nuclear_heating_in_the_divertor_(MW)______________________________ (pnucdiv)_____________________ 1.4906E+02 OP + Blanket_exponential_factor______________________________________________ (exp_blanket)_________________ 9.9936E-01 OP + Shield:_first_exponential_______________________________________________ (exp_shield1)_________________ 1.9523E-03 OP + Shield:_second_exponential______________________________________________ (exp_shield2)_________________ 2.5427E-01 OP + Solid_angle_fraction_taken_by_on_divertor_______________________________ (fdiv)________________________ 1.1500E-01 + Switch_for_plant_secondary_cycle________________________________________ (secondary_cycle)_____________ 2 + First_wall_coolant_pressure_(Pa)________________________________________ (fwpressure)__________________ 1.5500E+07 + Blanket_coolant_pressure_(Pa)___________________________________________ (blpressure)__________________ 1.5500E+07 + Allowable_nominal_neutron_fluence_at_first_wall_(MW.year/m2)____________ (abktflnc)____________________ 5.0000E+00 + No_of_inboard_blanket_modules_poloidally________________________________ (nblktmodpi)__________________ 7 + No_of_inboard_blanket_modules_toroidally________________________________ (nblktmodti)__________________ 32 + No_of_outboard_blanket_modules_poloidally_______________________________ (nblktmodpo)__________________ 8 + No_of_outboard_blanket_modules_toroidally_______________________________ (nblktmodto)__________________ 48 + Isentropic_efficiency_of_first_wall_/_blanket_coolant_pumps_____________ (etaiso)______________________ 9.0000E-01 + First_wall_area_(m2)____________________________________________________ (fwarea)______________________ 1.6044E+03 OP + Cryostat_internal_radius_(m)____________________________________________ (rdewex)______________________ 1.7798E+01 OP + Cryostat_internal_half-height_(m)_______________________________________ (zdewex)______________________ 1.5339E+01 OP + Vertical_clearance_from_TF_coil_to_cryostat_(m)_________________________ (clh1)________________________ 5.6044E+00 OP + Divertor_area_(m2)______________________________________________________ (divsur)______________________ 1.4879E+02 OP + Divertor_mass_(kg)______________________________________________________ (divmas)______________________ 3.6453E+04 OP + # Superconducting TF Coil Power Conversion # + TF_coil_current_(kA)____________________________________________________ (itfka)_______________________ 8.9795E+01 OP + Number_of_TF_coils______________________________________________________ (ntfc)________________________ 1.6000E+01 + Voltage_across_a_TF_coil_during_quench_(kV)_____________________________ (vtfskv)______________________ 9.1862E+00 OP + TF_coil_charge_time_(hours)_____________________________________________ (tchghr)______________________ 4.0000E+00 + Total_inductance_of_TF_coils_(H)________________________________________ (ltfth)_______________________ 3.0165E+01 OP + Total_resistance_of_TF_coils_(ohm)______________________________________ (rcoils)______________________ 0.0000E+00 OP + TF_coil_charging_voltage_(V)____________________________________________ (tfcv)________________________ 2.9268E+02 + Number_of_DC_circuit_breakers___________________________________________ (ntfbkr)______________________ 1.6000E+01 + Number_of_dump_resistors________________________________________________ (ndumpr)______________________ 6.4000E+01 + Resistance_per_dump_resistor_(ohm)______________________________________ (r1dump)______________________ 1.0230E-01 OP + Dump_resistor_peak_power_(MW)___________________________________________ (r1ppmw)______________________ 2.0622E+02 OP + Energy_supplied_per_dump_resistor_(MJ)__________________________________ (r1emj)_______________________ 1.9002E+03 OP + TF_coil_L/R_time_constant_(s)___________________________________________ (ttfsec)______________________ 1.8429E+01 OP + Power_supply_voltage_(V)________________________________________________ (tfpsv)_______________________ 3.0731E+02 OP + Power_supply_current_(kA)_______________________________________________ (tfpska)______________________ 9.4285E+01 OP + DC_power_supply_rating_(kW)_____________________________________________ (tfckw)_______________________ 2.8975E+04 OP + AC_power_for_charging_(kW)______________________________________________ (tfackw)______________________ 3.2194E+04 OP + TF_coil_resistive_power_(MW)____________________________________________ (rpower)______________________ 9.3902E+00 OP + TF_coil_inductive_power_(MVA)___________________________________________ (xpower)______________________ 1.6891E+01 OP + Aluminium_bus_current_density_(kA/cm2)__________________________________ (djmka)_______________________ 1.2500E-01 + Aluminium_bus_cross-sectional_area_(cm2)________________________________ (albusa)______________________ 7.1836E+02 OP + Total_length_of_TF_coil_bussing_(m)_____________________________________ (tfbusl)______________________ 3.1931E+03 OP + Aluminium_bus_weight_(tonnes)___________________________________________ (albuswt)_____________________ 6.1932E+02 OP + Total_TF_coil_bus_resistance_(ohm)______________________________________ (rtfbus)______________________ 1.1646E-03 OP + TF_coil_bus_voltage_drop_(V)____________________________________________ (vtfbus)______________________ 1.0457E+02 OP + Dump_resistor_floor_area_(m2)___________________________________________ (drarea)______________________ 4.9234E+03 OP + TF_coil_power_conversion_floor_space_(m2)_______________________________ (tfcfsp)______________________ 1.8228E+03 OP + TF_coil_power_conv._building_volume_(m3)________________________________ (tfcbv)_______________________ 1.0937E+04 OP + TF_coil_AC_inductive_power_demand_(MW)__________________________________ (xpwrmw)______________________ 1.8768E+01 OP + Total_steady_state_AC_power_demand_(MW)_________________________________ (tfacpd)______________________ 1.0434E+01 OP + # PF Coils and Central Solenoid: Power and Energy # + Number_of_PF_coil_circuits______________________________________________ (pfckts)______________________ 1.2000E+01 + Sum_of_PF_power_supply_ratings_(MVA)____________________________________ (spsmva)______________________ 3.0313E+02 OP + Total_PF_coil_circuit_bus_length_(m)____________________________________ (spfbusl)_____________________ 2.4480E+03 OP + Total_PF_coil_bus_resistive_power_(kW)__________________________________ (pfbuspwr)____________________ 9.6485E+02 OP + Total_PF_coil_resistive_power_(kW)______________________________________ (srcktpm)_____________________ 9.6485E+02 OP + Maximum_PF_coil_voltage_(kV)____________________________________________ (vpfskv)______________________ 2.0000E+01 + Efficiency_of_transfer_of_PF_stored_energy_into_or_out_of_storage_______ (etapsu)______________________ 9.0000E-01 + Maximum_stored_energy_in_poloidal_field_(MJ)____________________________ (ensxpfm)_____________________ 2.8804E+04 OP + Peak_absolute_rate_of_change_of_stored_energy_in_poloidal_field_(MW)____ (peakpoloidalpower)___________ 1.7319E+02 OP + # Vacuum System # + First_wall_outgassing_rate_(Pa_m/s)_____________________________________ (rat)_________________________ 1.3000E-08 + Total_outgassing_load_(Pa_m3/s)_________________________________________ (ogas)________________________ 1.6691E-04 OP + Base_pressure_required_(Pa)_____________________________________________ (pbase)_______________________ 5.0000E-04 + Required_N2_pump_speed_(m3/s)___________________________________________ (s(1))________________________ 3.3381E-01 OP + N2_pump_speed_provided_(m3/s)___________________________________________ (snet(1))_____________________ 2.3404E+01 OP + Plasma_chamber_volume_(m3)______________________________________________ (volume)______________________ 2.2588E+03 OP + Chamber_pressure_after_burn_(Pa)________________________________________ (pend)________________________ 1.6698E-01 OP + Chamber_pressure_before_burn_(Pa)_______________________________________ (pstart)______________________ 1.6698E-03 + Allowable_pumping_time_switch___________________________________________ (dwell_pump)__________________ 0 + Dwell_time_between_burns_(s)____________________________________________ (tdwell.)_____________________ 1.8000E+03 + CS_ramp-up_time_burns_(s)_______________________________________________ (tramp.)______________________ 5.0000E+02 + Allowable_pumping_time_between_burns_(s)________________________________ (tpump)_______________________ 1.8000E+03 + Required_D-T_pump_speed_(m3/s)__________________________________________ (s(2))________________________ 5.7790E+00 OP + D-T_pump_speed_provided_(m3/s)__________________________________________ (snet(2))_____________________ 5.6700E+01 OP + Divertor_chamber_gas_pressure_(Pa)______________________________________ (prdiv)_______________________ 3.6000E-01 + Helium_gas_fraction_in_divertor_chamber_________________________________ (fhe)_________________________ 1.7218E-01 OP + Required_helium_pump_speed_(m3/s)_______________________________________ (s(3))________________________ 3.8423E+01 OP + Helium_pump_speed_provided_(m3/s)_______________________________________ (snet(3))_____________________ 3.8423E+01 OP + D-T_fuelling_rate_(kg/s)________________________________________________ (frate)_______________________ 2.7747E-05 OP + Required_D-T_pump_speed_(m3/s)__________________________________________ (s(4))________________________ 3.8423E+01 OP + D-T_pump_speed_provided_(m3/s)__________________________________________ (snet(4))_____________________ 5.6700E+01 OP + Number_of_large_pump_ducts______________________________________________ (nduct)_______________________ 16 + Passage_diameter,_divertor_to_ducts_(m)_________________________________ (d(imax))_____________________ 4.7857E-01 OP + Passage_length_(m)______________________________________________________ (l1)__________________________ 1.7160E+00 OP + Diameter_of_ducts_(m)___________________________________________________ (dout)________________________ 5.7428E-01 OP + Duct_length,_divertor_to_elbow_(m)______________________________________ (l2)__________________________ 4.8000E+00 OP + Duct_length,_elbow_to_pumps_(m)_________________________________________ (l3)__________________________ 2.0000E+00 + Number_of_pumps_________________________________________________________ (pumpn)_______________________ 3.2000E+01 OP + # Plant Buildings System # + Internal_volume_of_reactor_building_(m3)________________________________ (vrci)________________________ 9.9708E+05 + Dist_from_centre_of_torus_to_bldg_wall_(m)______________________________ (wrbi)________________________ 3.9531E+01 + Effective_floor_area_(m2)_______________________________________________ (efloor)______________________ 3.3660E+05 + Reactor_building_volume_(m3)____________________________________________ (rbv)_________________________ 1.1310E+06 + Reactor_maintenance_building_volume_(m3)________________________________ (rmbv)________________________ 3.9641E+05 + Warmshop_volume_(m3)____________________________________________________ (wsv)_________________________ 1.2531E+05 + Tritium_building_volume_(m3)____________________________________________ (triv)________________________ 4.0000E+04 + Electrical_building_volume_(m3)_________________________________________ (elev)________________________ 5.1937E+04 + Control_building_volume_(m3)____________________________________________ (conv)________________________ 6.0000E+04 + Cryogenics_building_volume_(m3)_________________________________________ (cryv)________________________ 1.4976E+04 + Administration_building_volume_(m3)_____________________________________ (admv)________________________ 1.0000E+05 + Shops_volume_(m3)_______________________________________________________ (shov)________________________ 1.0000E+05 + Total_volume_of_nuclear_buildings_(m3)__________________________________ (volnucb)_____________________ 1.5738E+06 + # Electric Power Requirements # + Facility_base_load_(MW)_________________________________________________ (basemw)______________________ 5.0000E+00 + Divertor_coil_power_supplies_(MW)_______________________________________ (bdvmw)_______________________ 0.0000E+00 + Cryoplant_electric_power_(MW)___________________________________________ (crymw)_______________________ 3.6566E+01 OP + Primary_coolant_pumps_(MW)______________________________________________ (htpmw..)_____________________ 1.9053E+02 OP + PF_coil_power_supplies_(MW)_____________________________________________ (ppfmw)_______________________ 8.5511E+01 OP + TF_coil_power_supplies_(MW)_____________________________________________ (ptfmw)_______________________ 1.0434E+01 OP + Plasma_heating_supplies_(MW)____________________________________________ (pheatingmw)__________________ 1.6029E+02 OP + Tritium_processing_(MW)_________________________________________________ (trithtmw..)__________________ 1.5000E+01 + Vacuum_pumps__(MW)______________________________________________________ (vachtmw..)___________________ 5.0000E-01 + Total_pulsed_power_(MW)_________________________________________________ (pacpmw)______________________ 5.5432E+02 OP + Total_base_power_required_at_all_times_(MW)_____________________________ (fcsht)_______________________ 5.5490E+01 OP + # Cryogenics # + Conduction_and_radiation_heat_loads_on_cryogenic_components_(MW)________ (qss/1.0d6)___________________ 1.4779E-02 OP + Nuclear_heating_of_cryogenic_components_(MW)____________________________ (qnuc/1.0d6)__________________ 1.3000E-02 OP + AC_losses_in_cryogenic_components_(MW)__________________________________ (qac/1.0d6)___________________ 3.8170E-03 OP + Resistive_losses_in_current_leads_(MW)__________________________________ (qcl/1.0d6)___________________ 1.9539E-02 OP + 45%_allowance_for_heat_loads_in_transfer_lines,_storage_tanks_etc_(MW)__ (qmisc/1.0d6)_________________ 2.3011E-02 OP + Sum_=_Total_heat_removal_at_cryogenic_temperatures_(tfcoil_variables.tmp (helpow_+_helpow_cryal/1.0d6)_ 7.4146E-02 OP + Temperature_of_cryogenic_superconducting_components_(K)_________________ (tmpcry)______________________ 4.5000E+00 + Temperature_of_cryogenic_aluminium_components_(K)_______________________ (tcoolin)_____________________ 3.1315E+02 + Efficiency_(figure_of_merit)_of_cryogenic_plant_is_13%_of_ideal_Carnot_v ______________________________ 2.0277E-03 OP + Efficiency_(figure_of_merit)_of_cryogenic_aluminium_plant_is_40%_of_idea ______________________________ -2.0203E+00 OP + Electric_power_for_cryogenic_plant_(MW)_________________________________ (crypmw)______________________ 3.6566E+01 OP + # Plant Power / Heat Transport Balance # + Neutron_power_multiplication_in_blanket_________________________________ (emult)_______________________ 1.2690E+00 + Divertor_area_fraction_of_whole_toroid_surface__________________________ (fdiv)________________________ 1.1500E-01 + H/CD_apparatus_+_diagnostics_area_fraction______________________________ (fhcd)________________________ 0.0000E+00 + First_wall_area_fraction________________________________________________ (1-fdiv-fhcd)_________________ 8.8500E-01 + Switch_for_pumping_of_primary_coolant___________________________________ (primary_pumping)_____________ 3 + Mechanical_pumping_power_for_FW_cooling_loop_including_heat_exchanger_(M (htpmw_fw)____________________ 0.0000E+00 OP + Mechanical_pumping_power_for_blanket_cooling_loop_including_heat_exchang (htpmw_blkt)__________________ 0.0000E+00 OP + Mechanical_pumping_power_for_FW_and_blanket_cooling_loop_including_heat_ (htpmw_fw_blkt)_______________ 1.6407E+02 OP + Mechanical_pumping_power_for_divertor_(MW)______________________________ (htpmw_div)___________________ 1.6906E+00 OP + Mechanical_pumping_power_for_shield_and_vacuum_vessel_(MW)______________ (htpmw_shld)__________________ 7.0688E-03 OP + Electrical_pumping_power_for_FW_and_blanket_(MW)________________________ (htpmwe_fw_blkt)______________ 1.8858E+02 OP + Electrical_pumping_power_for_shield_(MW)________________________________ (htpmwe_shld)_________________ 8.1250E-03 OP + Electrical_pumping_power_for_divertor_(MW)______________________________ (htpmwe_div)__________________ 1.9433E+00 OP + Total_electrical_pumping_power_for_primary_coolant_(MW)_________________ (htpmw)_______________________ 1.9053E+02 OP + Coolant_pump_power_/_non-pumping_thermal_power_in_shield________________ (fpumpshld)___________________ 5.0000E-03 + Coolant_pump_power_/_non-pumping_thermal_power_in_divertor______________ (fpumpdiv)____________________ 5.0000E-03 + Electrical_efficiency_of_heat_transport_coolant_pumps___________________ (etahtp)______________________ 8.7000E-01 + Thermal_to_electric_conversion_efficiency_of_the_power_conversion_cycle_ (etath)_______________________ 4.0000E-01 + Fraction_of_total_high-grade_thermal_power_to_divertor__________________ (pdivfraction)________________ 1.5623E-01 + Total_power_leaving_reactor_(across_vacuum_vessel_boundary)_(MW)________ ______________________________ 2.0111E+03 + Heat_removal_from_cryogenic_plant_(MW)__________________________________ (crypmw)______________________ 3.6566E+01 + Heat_removal_from_facilities_(MW)_______________________________________ (fachtmw)_____________________ 5.5490E+01 + Coolant_pumping_efficiency_losses_(MW)__________________________________ (htpsecmw)____________________ 2.4769E+01 + Heat_removal_from_injection_power_(MW)__________________________________ (pinjht)______________________ 8.0143E+01 + Heat_removal_from_tritium_plant_(MW)____________________________________ (trithtmw)____________________ 1.5000E+01 + Heat_removal_from_vacuum_pumps_(MW)_____________________________________ (vachtmw)_____________________ 5.0000E-01 + TF_coil_resistive_power_(MW)____________________________________________ (tfcmw)_______________________ 0.0000E+00 + Total_low-grade_thermal_power_(MW)______________________________________ (psechtmw)____________________ 2.2417E+02 + Total_High-grade_thermal_power_(MW)_____________________________________ (pthermmw)____________________ 2.1751E+03 + Number_of_primary_heat_exchangers_______________________________________ (nphx)________________________ 3 OP + Transport_power_from_scaling_law_(MW)___________________________________ (pscalingmw)__________________ 2.9785E+02 + Radiation_power_from_inside_"coreradius"_(MW)___________________________ (pcoreradmw.)_________________ 9.1650E+01 + Total_(MW)______________________________________________________________ ______________________________ 3.8950E+02 + Alpha_power_deposited_in_plasma_(MW)____________________________________ (falpha*palpmw)_______________ 3.0746E+02 + Power_from_charged_products_of_DD_and/or_D-He3_fusion_(MW)______________ (pchargemw.)__________________ 1.2659E+00 + Ohmic_heating_(MW)______________________________________________________ (pohmmw.)_____________________ 6.2284E-01 + Injected_power_deposited_in_plasma_(MW)_________________________________ (pinjmw)______________________ 8.0143E+01 + Total_(MW)______________________________________________________________ ______________________________ 3.8950E+02 + Fusion_power_(MW)_______________________________________________________ (powfmw)______________________ 1.6202E+03 + Power_from_energy_multiplication_in_blanket_and_shield_(MW)_____________ (emultmw)_____________________ 3.0836E+02 + Injected_power_(MW)_____________________________________________________ (pinjmw.)_____________________ 8.0143E+01 + Ohmic_power_(MW)________________________________________________________ (pohmmw.)_____________________ 6.2284E-01 + Power_deposited_in_primary_coolant_by_pump_(MW)_________________________ (htpmw_mech)__________________ 1.6576E+02 + Total_(MW)______________________________________________________________ ______________________________ 2.1751E+03 + Heat_extracted_from_first_wall_and_blanket_(MW)_________________________ (pthermfw_blkt)_______________ 1.8339E+03 + Heat_extracted_from_shield__(MW)________________________________________ (pthermshld)__________________ 1.4208E+00 + Heat_extracted_from_divertor_(MW)_______________________________________ (pthermdiv)___________________ 3.3982E+02 + Nuclear_and_photon_power_lost_to_H/CD_system_(MW)_______________________ (psechcd)_____________________ 0.0000E+00 + Nuclear_power_lost_to_TF_(MW)___________________________________________ (ptfnuc)______________________ 2.5118E-02 + Total_(MW)______________________________________________________________ ______________________________ 2.1752E+03 + Net_electric_power_output(MW)___________________________________________ (pnetelmw.)___________________ 4.0001E+02 + Required_Net_electric_power_output(MW)__________________________________ (pnetelin)____________________ 4.0000E+02 + Electric_power_for_heating_and_current_drive_(MW)_______________________ (pinjwp)______________________ 1.6029E+02 + Electric_power_for_primary_coolant_pumps_(MW)___________________________ (htpmw)_______________________ 1.9053E+02 + Electric_power_for_vacuum_pumps_(MW)____________________________________ (vachtmw)_____________________ 5.0000E-01 + Electric_power_for_tritium_plant_(MW)___________________________________ (trithtmw)____________________ 1.5000E+01 + Electric_power_for_cryoplant_(MW)_______________________________________ (crypmw)______________________ 3.6566E+01 + Electric_power_for_TF_coils_(MW)________________________________________ (tfacpd)______________________ 1.0434E+01 + Electric_power_for_PF_coils_(MW)________________________________________ (pfwpmw)______________________ 1.2422E+00 + All_other_internal_electric_power_requirements_(MW)_____________________ (fachtmw)_____________________ 5.5490E+01 + Total_(MW)______________________________________________________________ (tot_plant_power)_____________ 8.7006E+02 + Total_(MW)______________________________________________________________ ______________________________ 8.7006E+02 + Gross_electrical_output*_(MW)___________________________________________ (pgrossmw)____________________ 8.7006E+02 + Fusion_power_(MW)_______________________________________________________ (powfmw)______________________ 1.6202E+03 + Power_from_energy_multiplication_in_blanket_and_shield_(MW)_____________ (emultmw)_____________________ 3.0836E+02 + Total_(MW)______________________________________________________________ ______________________________ 1.9285E+03 + Net_electrical_output_(MW) _____________________________________________ (pnetelmw)____________________ 4.0001E+02 + Heat_rejected_by_main_power_conversion_circuit_(MW)_____________________ (rejected_main)_______________ 1.3051E+03 + Heat_rejected_by_other_cooling_circuits_(MW)____________________________ (psechtmw)____________________ 2.2417E+02 + Total_(MW)______________________________________________________________ ______________________________ 1.9293E+03 + Net_electric_power_/_total_nuclear_power_(%)____________________________ (pnetelmw/(powfmw+emultmw)____ 2.0741E+01 + Net_electric_power_/_total_fusion_power_(%)_____________________________ (pnetelmw/powfmw)_____________ 2.4689E+01 + Gross_electric_power*_/_high_grade_heat_(%)_____________________________ (etath)_______________________ 4.0000E+01 + Recirculating_power_fraction____________________________________________ (cirpowfr)____________________ 5.4025E-01 + # Water usage during plant operation (secondary cooling) # + Volume_used_in_cooling_tower_(m3/day)___________________________________ (waterusetower)_______________ 5.5485E+04 OP + Volume_used_in_recirculating_water_system_(m3/day)______________________ (wateruserecirc)______________ 1.8617E+04 OP + Volume_used_in_once-through_water_system_(m3/day)_______________________ (wateruseonethru)_____________ 1.8244E+06 OP + # Errors and Warnings # + # Errors and Warnings # + PROCESS_error_status_flag_______________________________________________ (error_status)________________ 2 + Final_error_identifier__________________________________________________ (error_id)____________________ 244 + # End of PROCESS Output # + # End of PROCESS Output # + # Copy of PROCESS Input Follows # +************************************************************************************************************************ +***** ***** +***** Generic large tokamak file ***** +***** James Morris, UKAEA ***** +***** 28/06/23 ***** +***** ***** +************************************************************************* + +* Run Information * +******************* + +runtitle = Generic large tokamak + +* Figure of merit - minimise major radius +minmax = 1 + +* Error tolerance for VMCON +epsvmc = 1e-7 + +* Constraint Equations - Consistency Equations * +************************************************ + +* Beta consistency * +*------------------* +icc = 1 +ixc = 5 * beta +beta = 0.03 + +* Global power balance * +*----------------------* +icc = 2 + +* Radial build consistency * +*--------------------------* +icc = 11 + +* Constraint Equations - Limit Equations * +****************************************** + +* Density upper limit * +*---------------------* +icc = 5 +ixc = 6 * dene [m-3] +fdene = 1.2 +dene = 7.5E19 + +* Neutron wall load upper limit * +*-------------------------------* +icc = 8 +ixc = 14 * fwalld +fwalld = 1.0 +* wall load limit [MW/m2] +walalw = 2.0 + +* Fusion power upper limit * +*--------------------------* + +icc = 9 +ixc = 26 * ffuspow +* Maximum allowable value fusion power [MW] +powfmax = 3000 + +* Burn time lower limit * +*-----------------------* +icc = 13 +ixc = 21 * ftburn +* minimum burn time [s] +tbrnmn = 7200.0 + +* L-H threshold scaling * +*-----------------------* +icc = 15 +ixc = 103 * flhthresh +boundu(103) = 10.0 + +* Injection power upper limit * +*-----------------------------* +icc = 30 +ixc = 46 * fpinj +* Maximum allowable value for injected power [MW] +pinjalw = 200.0 + +* Net electric power lower limit * +*--------------------------------* +icc = 16 +ixc = 25 * fpnetel +* Minimum allowable value for net eletric power [MW] +pnetelin = 400.0 + +* Beta upper limit * +*------------------* +icc = 24 +ixc = 36 * fbetatry +fbetatry = 0.5 + +* Max TF field * +*--------------* +icc = 25 +ixc = 35 * fpeakb +* Maximum allowable value for toroidal magnetic field [T] +bmxlim = 14.0 + +* Central solenoid EOF current density upper limit * +*--------------------------------------------------* +icc = 26 +ixc = 37 * coheof [A/m2] +ixc = 38 * fjohc +boundu(38) = 1.0 +coheof = 1.5E7 +fjohc = 0.6 + +* Central solenoid BOP current density upper limit * +*--------------------------------------------------* +icc = 27 +ixc = 39 * fjohc0 +ixc = 41 * fcohbop +boundu(39) = 1.0 +fjohc0 = 0.6 +fcohbop = 0.9 + +* I_op/I_Crit TF coil limit * +*---------------------------* +icc = 33 +ixc = 50 * fiooic +boundu(50) = 1.0 +fiooic = 0.65 + +* Dump voltage upper limit * +*--------------------------* +icc = 34 +ixc = 51 * fvdump +ixc = 52 * vdalw [kV] +boundu(52) = 10.0 +fvdump = 1.0 +vdalw = 10.0 + +* J_winding pack protection * +*---------------------------* +icc = 35 +ixc = 53 * fjprot +fjprot = 1.0 + +* TF temp marg lower limit * +*--------------------------* +icc = 36 +ixc = 54 * ftmargtf +* Minimum allowable temperature margin [K] +tmargmin = 1.5 + +* CS coil temp margin lower limit * +*---------------------------------* +icc = 60 +ixc = 106 * ftmargoh +tmargmin_cs = 1.5 + +* Lower limit on taup/taueff (ratio alpha particle/energy confinement times) * +*-------------------------------------------------------------------------------* +icc = 62 +ixc = 110 * ftaulimit +taulimit = 5.0 + +* dump time constraint for VV stresses * +*--------------------------------------* +icc = 65 +ixc = 113 * fmaxvvstress +fmaxvvstress = 1.0 + +* CS stress limit * +*-----------------* +icc = 72 +ixc = 123 * foh_stress +foh_stress = 1.0 +* allowable hoop stress in Central Solenoid structural material [Pa] +alstroh = 7.5D8 + +* neped_neped_______________________normalised_residue____________________ (normres023)__________________ -1.9637E-08 + Upper_Lim._on_Psep_*_Bt_/_q_A_R___normalised_residue____________________ (normres024)__________________ 4.9789E-07 + TF_coil_case_stress_upper_limit___normalised_residue____________________ (normres025)__________________ -4.6757E-07 + TF_coil_conduit_stress_upper_lim__normalised_residue____________________ (normres026)__________________ -4.1375E-07 + # Final Feasible Point # + # Power Reactor Costs (1990 US$) # + First_wall_/_blanket_life_(years)_______________________________________ (fwbllife)____________________ 6.1566E+00 + Divertor_life_(years)___________________________________________________ (divlife.)____________________ 3.9769E+00 + Cost_of_electricity_(m$/kWh)____________________________________________ (coe)_________________________ 5.1257E+02 + # Detailed Costings (1990 US$) # + Acc.22_multiplier_for_Nth_of_a_kind_____________________________________ (fkind)_______________________ 1.0000E+00 + Level_of_Safety_Assurance_______________________________________________ (lsa)_________________________ 4 + # Structures and Site Facilities # + Site_improvements,_facilities,_land_(M$)________________________________ (c211)________________________ 3.5200E+01 + Reactor_building_cost_(M$)______________________________________________ (c212)________________________ 4.5238E+02 + Turbine_building_cost_(M$)______________________________________________ (c213)________________________ 3.8000E+01 + Reactor_maintenance_building_cost_(M$)__________________________________ (c2141)_______________________ 1.0307E+02 + Warm_shop_cost_(M$)_____________________________________________________ (c2142)_______________________ 5.7641E+01 + Tritium_building_cost_(M$)______________________________________________ (c215)________________________ 1.4800E+01 + Electrical_equipment_building_cost_(M$)_________________________________ (c216)________________________ 1.9736E+01 + Additional_buildings_cost_(M$)__________________________________________ (c2171)_______________________ 1.8000E+01 + Control_room_buildings_cost_(M$)________________________________________ (c2172)_______________________ 2.1000E+01 + Shop_and_warehouses_cost_(M$)___________________________________________ (c2173)_______________________ 1.1500E+01 + Cryogenic_building_cost_(M$)____________________________________________ (c2174)_______________________ 6.8891E+00 + Total_account_21_cost_(M$)______________________________________________ (c21)_________________________ 7.7822E+02 + # Reactor Systems # + First_wall_cost_(M$)____________________________________________________ (c2211)_______________________ 1.9130E+02 + Blanket_beryllium_cost_(M$)_____________________________________________ (c22121)______________________ 2.6109E+02 + Blanket_breeder_material_cost_(M$)______________________________________ (c22122)______________________ 6.3985E+02 + Blanket_stainless_steel_cost_(M$)_______________________________________ (c22123)______________________ 8.0726E+01 + Blanket_vanadium_cost_(M$)______________________________________________ (c22124)______________________ 0.0000E+00 + Blanket_total_cost_(M$)_________________________________________________ (c2212)_______________________ 9.8166E+02 + Bulk_shield_cost_(M$)___________________________________________________ (c22131)______________________ 7.8394E+01 + Penetration_shielding_cost_(M$)_________________________________________ (c22132)______________________ 7.8394E+01 + Total_shield_cost_(M$)__________________________________________________ (c2213)_______________________ 1.5679E+02 + Total_support_structure_cost_(M$)_______________________________________ (c2214)_______________________ 4.0933E+01 + Divertor_cost_(M$)______________________________________________________ (c2215)_______________________ 4.1660E+01 + Total_account_221_cost_(M$)_____________________________________________ (c221)________________________ 1.4123E+03 + # Magnets # + TF_coil_conductor_cost_(M$)_____________________________________________ (c22211)______________________ 1.3230E+02 + TF_coil_winding_cost_(M$)_______________________________________________ (c22212)______________________ 5.4263E+01 + TF_coil_case_cost_(M$)__________________________________________________ (c22213)______________________ 4.4365E+02 + TF_intercoil_structure_cost_(M$)________________________________________ (c22214)______________________ 1.5066E+02 + TF_coil_gravity_support_structure_(M$)__________________________________ (c22215)______________________ 4.4659E+01 + TF_magnet_assemblies_cost_(M$)__________________________________________ (c2221)_______________________ 8.2552E+02 + PF_coil_conductor_cost_(M$)_____________________________________________ (c22221)______________________ 4.6409E+02 + PF_coil_winding_cost_(M$)_______________________________________________ (c22222)______________________ 7.6765E+01 + PF_coil_case_cost_(M$)__________________________________________________ (c22223)______________________ 9.4861E+01 + PF_coil_support_structure_cost_(M$)_____________________________________ (c22224)______________________ 8.0235E+00 + PF_magnet_assemblies_cost_(M$)__________________________________________ (c2222)_______________________ 6.4374E+02 + Vacuum_vessel_assembly_cost_(M$)________________________________________ (c2223)_______________________ 2.5404E+02 + Total_account_222_cost_(M$)_____________________________________________ (c222)________________________ 1.7233E+03 + # Power Injection # + ECH_system_cost_(M$)____________________________________________________ (c2231)_______________________ 2.4043E+02 + Lower_hybrid_system_cost_(M$)___________________________________________ (c2232)_______________________ 0.0000E+00 + Neutral_beam_system_cost_(M$)___________________________________________ (c2233)_______________________ 0.0000E+00 + Total_account_223_cost_(M$)_____________________________________________ (c223)________________________ 2.4043E+02 + # Vacuum Systems # + High_vacuum_pumps_cost_(M$)_____________________________________________ (c2241)_______________________ 1.2480E+01 + Backing_pumps_cost_(M$)_________________________________________________ (c2242)_______________________ 4.6800E+00 + Vacuum_duct_cost_(M$)___________________________________________________ (c2243)_______________________ 2.5280E+00 + Valves_cost_(M$)________________________________________________________ (c2244)_______________________ 5.7410E+00 + Duct_shielding_cost_(M$)________________________________________________ (c2245)_______________________ 0.0000E+00 + Instrumentation_cost_(M$)_______________________________________________ (c2246)_______________________ 1.3000E+00 + Total_account_224_cost_(M$)_____________________________________________ (c224)________________________ 2.6729E+01 + # Power Conditioning # + TF_coil_power_supplies_cost_(M$)________________________________________ (c22511)______________________ 4.0144E+00 + TF_coil_breakers_cost_(M$)______________________________________________ (c22512)______________________ 3.4127E+01 + TF_coil_dump_resistors_cost_(M$)________________________________________ (c22513)______________________ 2.1322E+01 + TF_coil_instrumentation_and_control_(M$)________________________________ (c22514)______________________ 4.8000E+00 + TF_coil_bussing_cost_(M$)_______________________________________________ (c22515)______________________ 3.5267E+01 + Total,_TF_coil_power_costs_(M$)_________________________________________ (c2251)_______________________ 9.9531E+01 + PF_coil_power_supplies_cost_(M$)________________________________________ (c22521)______________________ 2.9591E+00 + PF_coil_instrumentation_and_control_(M$)________________________________ (c22522)______________________ 3.6000E+00 + PF_coil_bussing_cost_(M$)_______________________________________________ (c22523)______________________ 1.1995E+01 + PF_coil_burn_power_supplies_cost_(M$)___________________________________ (c22524)______________________ 1.2679E+00 + PF_coil_breakers_cost_(M$)______________________________________________ (c22525)______________________ 1.4709E+01 + PF_coil_dump_resistors_cost_(M$)________________________________________ (c22526)______________________ 4.3206E+00 + PF_coil_ac_breakers_cost_(M$)___________________________________________ (c22527)______________________ 9.0000E-01 + Total,_PF_coil_power_costs_(M$)_________________________________________ (c2252)_______________________ 3.9752E+01 + Total,_energy_storage_cost_(M$)_________________________________________ (c2253)_______________________ 1.6864E+01 + Total_account_225_cost_(M$)_____________________________________________ (c225)________________________ 1.5615E+02 + # Heat Transport System # + Pumps_and_piping_system_cost_(M$)_______________________________________ (cpp)_________________________ 3.6795E+01 + Primary_heat_exchanger_cost_(M$)________________________________________ (chx)_________________________ 7.1692E+01 + Total,_reactor_cooling_system_cost_(M$)_________________________________ (c2261)_______________________ 1.0849E+02 + Pumps,_piping_cost_(M$)_________________________________________________ (cppa)________________________ 2.8417E+01 + Total,_auxiliary_cooling_system_cost_(M$)_______________________________ (c2262)_______________________ 2.8417E+01 + Total,_cryogenic_system_cost_(M$)_______________________________________ (c2263)_______________________ 1.7039E+02 + Total_account_226_cost_(M$)_____________________________________________ (c226)________________________ 3.0729E+02 + # Fuel Handling System # + Fuelling_system_cost_(M$)_______________________________________________ (c2271)_______________________ 2.2300E+01 + Fuel_processing_and_purification_cost_(M$)______________________________ (c2272)_______________________ 1.0229E+02 + Atmospheric_recovery_systems_cost_(M$)__________________________________ (c2273)_______________________ 5.8088E+01 + Nuclear_building_ventilation_cost_(M$)__________________________________ (c2274)_______________________ 6.9201E+01 + Total_account_227_cost_(M$)_____________________________________________ (c227)________________________ 2.5188E+02 + # Instrumentation and Control # + Instrumentation_and_control_cost_(M$)___________________________________ (c228)________________________ 1.5000E+02 + # Maintenance Equipment # + Maintenance_equipment_cost_(M$)_________________________________________ (c229)________________________ 1.2500E+02 + # Total Account 22 Cost # + Total_account_22_cost_(M$)______________________________________________ (c22)_________________________ 4.3931E+03 + # Turbine Plant Equipment # + Turbine_plant_equipment_cost_(M$)_______________________________________ (c23)_________________________ 1.7613E+02 + # Electric Plant Equipment # + Switchyard_equipment_cost_(M$)__________________________________________ (c241)________________________ 1.8400E+01 + Transformers_cost_(M$)__________________________________________________ (c242)________________________ 8.0330E+00 + Low_voltage_equipment_cost_(M$)_________________________________________ (c243)________________________ 6.4513E+00 + Diesel_backup_equipment_cost_(M$)_______________________________________ (c244)________________________ 6.8000E+00 + Auxiliary_facilities_cost_(M$)__________________________________________ (c245)________________________ 1.5000E+00 + Total_account_24_cost_(M$)______________________________________________ (c24)_________________________ 4.1184E+01 + # Miscellaneous Plant Equipment # + Miscellaneous_plant_equipment_cost_(M$)_________________________________ (c25)_________________________ 2.5000E+01 + # Heat Rejection System # + Heat_rejection_system_cost_(M$)_________________________________________ (c26)_________________________ 4.9877E+01 + # Plant Direct Cost # + Plant_direct_cost_(M$)__________________________________________________ (cdirt)_______________________ 5.4635E+03 + # Reactor Core Cost # + Reactor_core_cost_(M$)__________________________________________________ (crctcore)____________________ 3.3761E+03 + # Indirect Cost # + Indirect_cost_(M$)______________________________________________________ (c9)__________________________ 1.8221E+03 + # Total Contingency # + Total_contingency_(M$)__________________________________________________ (ccont)_______________________ 1.4207E+03 + # Constructed Cost # + Constructed_cost_(M$)___________________________________________________ (concost)_____________________ 8.7063E+03 + # Interest during Construction # + Interest_during_construction_(M$)_______________________________________ (moneyint)____________________ 1.4365E+03 + # Total Capital Investment # + Total_capital_investment_(M$)___________________________________________ (capcost)_____________________ 1.0143E+04 + # Plant Availability # + Allowable_blanket_neutron_fluence_(MW-yr/m2)____________________________ (abktflnc)____________________ 5.0000E+00 + Allowable_divertor_heat_fluence_(MW-yr/m2)______________________________ (adivflnc)____________________ 7.0000E+00 + First_wall_/_blanket_lifetime_(years)___________________________________ (bktlife)_____________________ 6.1566E+00 OP + Divertor_lifetime_(years)_______________________________________________ (divlife)_____________________ 3.9769E+00 OP + Heating/CD_system_lifetime_(years)______________________________________ (cdrlife)_____________________ 6.1566E+00 OP + Total_plant_lifetime_(years)____________________________________________ (tlife)_______________________ 3.0000E+01 + Total_plant_availability_fraction_______________________________________ (cfactr)______________________ 8.0000E-01 + Number_of_fusion_cycles_to_reach_allowable_fw/blanket_DPA_______________ (bktcycles)___________________ 1.5787E+04 + # Plasma # + Tokamak_aspect_ratio_=_Conventional,_itart_=_0__________________________ (itart)_______________________ 0.0000E+00 + Major_radius_(m)________________________________________________________ (rmajor)______________________ 8.0000E+00 ITV + Minor_radius_(m)________________________________________________________ (rminor)______________________ 2.6667E+00 + Aspect_ratio____________________________________________________________ (aspect)______________________ 3.0000E+00 + Elongation,_X-point_(input_value_used)__________________________________ (kappa)_______________________ 1.8500E+00 + Elongation,_95%_surface_(calculated_from_kappa)_________________________ (kappa95)_____________________ 1.6518E+00 + Elongation,_area_ratio_calc.____________________________________________ (kappaa)______________________ 1.7188E+00 + Triangularity,_X-point_(input_value_used)_______________________________ (triang)______________________ 5.0000E-01 + Triangularity,_95%_surface_(calculated_from_triang)_____________________ (triang95)____________________ 3.3333E-01 + Plasma_poloidal_perimeter_(m)___________________________________________ (pperim)______________________ 2.4081E+01 + Plasma_cross-sectional_area_(m2)________________________________________ (xarea)_______________________ 3.8398E+01 + Plasma_surface_area_(m2)________________________________________________ (sarea)_______________________ 1.1738E+03 OP + Plasma_volume_(m3)______________________________________________________ (vol)_________________________ 1.8882E+03 OP + Plasma_current_scaling_law_used_________________________________________ (icurr)_______________________ 4 + Plasma_current_(MA)_____________________________________________________ (plascur/1D6)_________________ 1.6631E+01 + Current_density_profile_factor__________________________________________ (alphaj)______________________ 1.9805E+00 + Plasma_internal_inductance,_li__________________________________________ (rli)_________________________ 1.2275E+00 + Vertical_field_at_plasma_(T)____________________________________________ (bvert)_______________________ -7.4373E-01 + Vacuum_toroidal_field_at_R_(T)__________________________________________ (bt)__________________________ 5.2940E+00 ITV + Average_poloidal_field_(T)______________________________________________ (bp)__________________________ 8.6787E-01 + Total_field_(sqrt(bp^2_+_bt^2))_(T)_____________________________________ (btot)________________________ 5.3647E+00 + Safety_factor_on_axis___________________________________________________ (q0)__________________________ 1.0000E+00 + Safety_factor_at_95%_flux_surface_______________________________________ (q95)_________________________ 3.5961E+00 ITV + Cylindrical_safety_factor_(qcyl)________________________________________ (qstar)_______________________ 2.9805E+00 + Total_plasma_beta_______________________________________________________ (beta)________________________ 3.3648E-02 ITV + Total_poloidal_beta_____________________________________________________ (betap)_______________________ 1.2857E+00 OP + Total_toroidal_beta_____________________________________________________ ______________________________ 3.4553E-02 OP + Fast_alpha_beta_________________________________________________________ (betaft)______________________ 4.2236E-03 OP + Beam_ion_beta___________________________________________________________ (betanb)______________________ 0.0000E+00 OP + (Fast_alpha_+_beam_physics_variables.beta)/(thermal_physics_variables.be (gammaft)_____________________ 1.4354E-01 OP + Thermal_beta____________________________________________________________ ______________________________ 2.9425E-02 OP + Thermal_poloidal_beta___________________________________________________ ______________________________ 1.1243E+00 OP + Thermal_toroidal_physics_variables.beta_(=_beta-exp)____________________ ______________________________ 3.0215E-02 OP + 2nd_stability_physics_variables.beta_:_beta_p_/_(R/a)___________________ (eps*betap)___________________ 4.2857E-01 + 2nd_stability_physics_variables.beta_upper_limit________________________ (epbetmax)____________________ 1.3800E+00 + Beta_g_coefficient______________________________________________________ (dnbeta)______________________ 4.9099E+00 + Normalised_thermal_beta_________________________________________________ ______________________________ 2.4977E+00 + Normalised_total_beta___________________________________________________ ______________________________ 2.8562E+00 + Normalised_toroidal_beta________________________________________________ (normalised_toroidal_beta)____ 2.9330E+00 + Limit_on_thermal_beta___________________________________________________ (betalim)_____________________ 5.7842E-02 + Plasma_thermal_energy_(J)_______________________________________________ ______________________________ 9.5431E+08 OP + Total_plasma_internal_energy_(J)________________________________________ (total_plasma_internal_energy) 1.0913E+09 OP + Electron_temperature_(keV)______________________________________________ (te)__________________________ 1.2489E+01 ITV + Electron_temperature_on_axis_(keV)______________________________________ (te0)_________________________ 2.5758E+01 + Ion_temperature_(keV)___________________________________________________ (ti)__________________________ 1.2489E+01 + Ion_temperature_on_axis_(keV)___________________________________________ (ti0)_________________________ 2.5758E+01 + Electron_temp.,_density_weighted_(keV)__________________________________ (ten)_________________________ 1.3805E+01 + Electron_density_(/m3)__________________________________________________ (dene)________________________ 8.0667E+19 ITV + Electron_density_on_axis_(/m3)__________________________________________ (ne0)_________________________ 1.0610E+20 OP + Line-averaged_electron_density_(/m3)____________________________________ (dnla)________________________ 8.9334E+19 OP + Line-averaged_electron_density_/_Greenwald_density______________________ (dnla_gw)_____________________ 1.2000E+00 OP + Ion_density_(/m3)_______________________________________________________ (dnitot)______________________ 7.1669E+19 OP + Fuel_density_(/m3)______________________________________________________ (deni)________________________ 6.4831E+19 OP + Total_impurity_density_with_Z_>_2_(no_He)_(/m3)_________________________ (dnz)_________________________ 4.6503E+16 OP + Helium_ion_density_(thermalised_ions_only)_(/m3)________________________ (dnalp)_______________________ 6.7723E+18 OP + Proton_density_(/m3)____________________________________________________ (dnprot)______________________ 1.8963E+16 OP + Hot_beam_density_(/m3)__________________________________________________ (dnbeam)______________________ 0.0000E+00 OP + Density_limit_from_scaling_(/m3)________________________________________ (dnelimt)_____________________ 7.4445E+19 OP + Density_limit_(enforced)_(/m3)__________________________________________ (boundu(9)*dnelimt)___________ 7.4445E+19 OP + Helium_ion_density_(thermalised_ions_only)_/_electron_density___________ (ralpne)______________________ 8.3954E-02 ITV + H__concentration________________________________________________________ (fimp(01))____________________ 8.0392E-01 OP + He_concentration________________________________________________________ (fimp(02))____________________ 8.3954E-02 + Be_concentration________________________________________________________ (fimp(03))____________________ 0.0000E+00 + C__concentration________________________________________________________ (fimp(04))____________________ 0.0000E+00 + N__concentration________________________________________________________ (fimp(05))____________________ 0.0000E+00 + O__concentration________________________________________________________ (fimp(06))____________________ 0.0000E+00 + Ne_concentration________________________________________________________ (fimp(07))____________________ 0.0000E+00 + Si_concentration________________________________________________________ (fimp(08))____________________ 0.0000E+00 + Ar_concentration________________________________________________________ (fimp(09))____________________ 0.0000E+00 + Fe_concentration________________________________________________________ (fimp(10))____________________ 0.0000E+00 + Ni_concentration________________________________________________________ (fimp(11))____________________ 0.0000E+00 + Kr_concentration________________________________________________________ (fimp(12))____________________ 0.0000E+00 + Xe_concentration________________________________________________________ (fimp(13))____________________ 5.7149E-04 ITV + W__concentration________________________________________________________ (fimp(14))____________________ 5.0000E-06 + Average_mass_of_all_ions_(amu)__________________________________________ (aion)________________________ 2.7252E+00 OP + Effective_charge________________________________________________________ (zeff)________________________ 2.5164E+00 + Density_profile_factor__________________________________________________ (alphan)______________________ 1.0000E+00 + Plasma_profile_model____________________________________________________ (ipedestal)___________________ 1 + Density_pedestal_r/a_location___________________________________________ (rhopedn)_____________________ 9.4000E-01 + Electron_density_pedestal_height_(/m3)__________________________________ (neped)_______________________ 6.3278E+19 OP + Electron_density_at_pedestal_/_nGW______________________________________ (fgwped_out)__________________ 8.5000E-01 + Temperature_pedestal_r/a_location_______________________________________ (rhopedt)_____________________ 9.4000E-01 + Pedestal_scaling_switch_________________________________________________ (ieped)_______________________ 0 + Electron_temp._pedestal_height_(keV)____________________________________ (teped)_______________________ 5.5000E+00 + Electron_temp._at_separatrix_(keV)______________________________________ (tesep)_______________________ 1.0000E-01 + Electron_density_at_separatrix_(/m3)____________________________________ (nesep)_______________________ 3.7223E+19 + Electron_density_at_separatrix_/_nGW____________________________________ (fgwsep_out)__________________ 5.0000E-01 + Temperature_profile_index_______________________________________________ (alphat)______________________ 1.4500E+00 + Temperature_profile_index_beta__________________________________________ (tbeta)_______________________ 2.0000E+00 + Old_ASDEX_model_________________________________________________________ (dlimit(1))___________________ 5.2797E+19 OP + Borrass_ITER_model_I____________________________________________________ (dlimit(2))___________________ 1.0969E+20 OP + Borrass_ITER_model_II___________________________________________________ (dlimit(3))___________________ 4.3575E+19 OP + JET_edge_radiation_model________________________________________________ (dlimit(4))___________________ 3.0227E+21 OP + JET_simplified_model____________________________________________________ (dlimit(5))___________________ 4.3397E+20 OP + Hugill-Murakami_Mq_model________________________________________________ (dlimit(6))___________________ 6.6609E+19 OP + Greenwald_model_________________________________________________________ (dlimit(7))___________________ 7.4445E+19 OP + Deuterium_fuel_fraction_________________________________________________ (fdeut)_______________________ 5.0000E-01 + Tritium_fuel_fraction___________________________________________________ (ftrit)_______________________ 5.0000E-01 + Total_fusion_power_(MW)_________________________________________________ (powfmw)______________________ 1.6202E+03 OP + _=____D-T_fusion_power_(MW)_____________________________________________ (pdt)_________________________ 1.6182E+03 OP + __+___D-D_fusion_power_(MW)_____________________________________________ (pdd)_________________________ 1.9494E+00 OP + __+_D-He3_fusion_power_(MW)_____________________________________________ (pdhe3)_______________________ 0.0000E+00 OP + Alpha_power:_total_(MW)_________________________________________________ (palpmw)______________________ 3.2365E+02 OP + Alpha_power:_beam-plasma_(MW)___________________________________________ (palpnb)______________________ 0.0000E+00 OP + Neutron_power_(MW)______________________________________________________ (pneutmw)_____________________ 1.2953E+03 OP + Charged_particle_power_(excluding_alphas)_(MW)__________________________ (pchargemw)___________________ 1.2659E+00 OP + Total_power_deposited_in_plasma_(MW)____________________________________ (tot_power_plasma)____________ 3.8950E+02 OP + Bremsstrahlung_radiation_power_(MW)_____________________________________ (pbrempv*vol)_________________ 6.5195E+01 OP + Line_radiation_power_(MW)_______________________________________________ (plinepv*vol)_________________ 1.4609E+02 OP + Synchrotron_radiation_power_(MW)________________________________________ (psyncpv*vol)_________________ 1.5187E+01 OP + Synchrotron_wall_reflectivity_factor____________________________________ (ssync)_______________________ 6.0000E-01 + Normalised_minor_radius_defining_'core'_________________________________ (coreradius)__________________ 7.5000E-01 + Fraction_of_core_radiation_subtracted_from_P_L__________________________ (coreradiationfraction)_______ 6.0000E-01 + Radiation_power_from_inner_zone_(MW)____________________________________ (pinnerzoneradmw)_____________ 9.1650E+01 OP + Radiation_power_from_outer_zone_(MW)____________________________________ (pouterzoneradmw)_____________ 1.3482E+02 OP + Total_radiation_power_from_inside_LCFS_(MW)_____________________________ (pradmw)______________________ 2.2647E+02 OP + LCFS_radiation_fraction_=_total_radiation_in_LCFS_/_total_power_deposite (rad_fraction_LCFS)___________ 5.8144E-01 OP + Nominal_mean_radiation_load_on_inside_surface_of_reactor_(MW/m2)________ (photon_wall)_________________ 1.7749E-01 OP + Peaking_factor_for_radiation_wall_load__________________________________ (peakfactrad)_________________ 3.3300E+00 IP + Maximum_permitted_radiation_wall_load_(MW/m^2)__________________________ (maxradwallload)______________ 1.0000E+00 IP + Peak_radiation_wall_load_(MW/m^2)_______________________________________ (peakradwallload)_____________ 5.9106E-01 OP + Fast_alpha_particle_power_incident_on_the_first_wall_(MW)_______________ (palpfwmw)____________________ 1.6182E+01 OP + Nominal_mean_neutron_load_on_inside_surface_of_reactor_(MW/m2)__________ (wallmw)______________________ 1.0152E+00 OP + Power_incident_on_the_divertor_targets_(MW)_____________________________ (ptarmw)______________________ 3.2606E+01 OP + Fraction_of_power_to_the_lower_divertor_________________________________ (ftar)________________________ 1.0000E+00 IP + Outboard_side_heat_flux_decay_length_(m)________________________________ (lambdaio)____________________ 1.5700E-03 OP + Fraction_of_power_on_the_inner_targets__________________________________ (fio)_________________________ 4.1000E-01 OP + Fraction_of_power_incident_on_the_lower_inner_target____________________ (fLI)_________________________ 4.1000E-01 OP + Fraction_of_power_incident_on_the_lower_outer_target____________________ (fLO)_________________________ 5.9000E-01 OP + Power_incident_on_the_lower_inner_target_(MW)___________________________ (pLImw)_______________________ 1.3368E+01 OP + Power_incident_on_the_lower_outer_target_(MW)___________________________ (pLOmw)_______________________ 1.9237E+01 OP + Ohmic_heating_power_(MW)________________________________________________ (pohmmw)______________________ 6.2284E-01 OP + Fraction_of_alpha_power_deposited_in_plasma_____________________________ (falpha)______________________ 9.5000E-01 + Fraction_of_alpha_power_to_electrons____________________________________ (falpe)_______________________ 7.1828E-01 + Fraction_of_alpha_power_to_ions_________________________________________ (falpi)_______________________ 2.8172E-01 + Ion_transport_(MW)______________________________________________________ (ptrimw)______________________ 1.4013E+02 OP + Electron_transport_(MW)_________________________________________________ (ptremw)______________________ 1.5772E+02 OP + Injection_power_to_ions_(MW)____________________________________________ (pinjimw)_____________________ 0.0000E+00 OP + Injection_power_to_electrons_(MW)_______________________________________ (pinjemw)_____________________ 8.0143E+01 OP + Ignited_plasma_switch_(0=not_ignited,_1=ignited)________________________ (ignite)______________________ 0 + Power_into_divertor_zone_via_charged_particles_(MW)_____________________ (pdivt)_______________________ 1.6303E+02 OP + Psep_/_R_ratio_(MW/m)___________________________________________________ (pdivt/rmajor)________________ 2.0378E+01 OP + Psep_Bt_/_qAR_ratio_(MWT/m)_____________________________________________ (pdivtbt/qar)_________________ 1.0000E+01 OP + ITER_1996_scaling:_nominal_(MW)_________________________________________ (pthrmw(1))___________________ 1.2978E+02 OP + ITER_1996_scaling:_upper_bound_(MW)_____________________________________ (pthrmw(2))___________________ 2.8603E+02 OP + ITER_1996_scaling:_lower_bound_(MW)_____________________________________ (pthrmw(3))___________________ 5.8098E+01 OP + ITER_1997_scaling_(1)_(MW)______________________________________________ (pthrmw(4))___________________ 2.1452E+02 OP + ITER_1997_scaling_(2)_(MW)______________________________________________ (pthrmw(5))___________________ 1.7206E+02 OP + Martin_2008_scaling:_nominal_(MW)_______________________________________ (pthrmw(6))___________________ 9.7416E+01 OP + Martin_2008_scaling:_95%_upper_bound_(MW)_______________________________ (pthrmw(7))___________________ 1.2769E+02 OP + Martin_2008_scaling:_95%_lower_bound_(MW)_______________________________ (pthrmw(8))___________________ 6.7143E+01 OP + Snipes_2000_scaling:_nominal_(MW)_______________________________________ (pthrmw(9))___________________ 6.7785E+01 OP + Snipes_2000_scaling:_upper_bound_(MW)___________________________________ (pthrmw(10))__________________ 9.9437E+01 OP + Snipes_2000_scaling:_lower_bound_(MW)___________________________________ (pthrmw(11))__________________ 4.5839E+01 OP + Snipes_2000_scaling_(closed_divertor):_nominal_(MW)_____________________ (pthrmw(12))__________________ 3.1010E+01 OP + Snipes_2000_scaling_(closed_divertor):_upper_bound_(MW)_________________ (pthrmw(13))__________________ 4.3148E+01 OP + Snipes_2000_scaling_(closed_divertor):_lower_bound_(MW)_________________ (pthrmw(14))__________________ 2.2130E+01 OP + Hubbard_2012_L-I_threshold_-_nominal_(MW)_______________________________ (pthrmw(15))__________________ 2.7549E+01 OP + Hubbard_2012_L-I_threshold_-_lower_bound_(MW)___________________________ (pthrmw(16))__________________ 1.4319E+01 OP + Hubbard_2012_L-I_threshold_-_upper_bound_(MW)___________________________ (pthrmw(17))__________________ 5.3005E+01 OP + Hubbard_2017_L-I_threshold______________________________________________ (pthrmw(18))__________________ 2.6202E+02 OP + Martin_2008_aspect_ratio_corrected_scaling:_nominal_(MW)________________ (pthrmw(19))__________________ 9.7416E+01 OP + Martin_2008_aspect_ratio_corrected_scaling:_95%_upper_bound_(MW)________ (pthrmw(20))__________________ 1.2769E+02 OP + Martin_2008_aspect_ratio_corrected_scaling:_95%_lower_bound_(MW)________ (pthrmw(21))__________________ 6.7143E+01 OP + L-H_threshold_power_(enforced)_(MW)_____________________________________ (boundl(103)*plhthresh)_______ 9.7416E+01 OP + L-H_threshold_power_(MW)________________________________________________ (plhthresh)___________________ 9.7416E+01 OP + Confinement_H_factor____________________________________________________ (hfact)_______________________ 1.1886E+00 ITV + Global_thermal_energy_confinement_time_(s)______________________________ (taueff)______________________ 3.2037E+00 + Ion_energy_confinement_time_(s)_________________________________________ (tauei)_______________________ 3.2037E+00 + Electron_energy_confinement_time_(s)____________________________________ (tauee)_______________________ 3.2037E+00 + n.tau_=_Volume-average_electron_density_x_Energy_confinement_time_(s/m3) (dntau)_______________________ 2.5843E+20 OP + Triple_product__(keV_s/m3)______________________________________________ (dntau*te)____________________ 3.2275E+21 OP + Transport_loss_power_assumed_in_scaling_law_(MW)________________________ (powerht)_____________________ 2.9785E+02 OP + Switch_for_radiation_loss_term_usage_in_power_balance___________________ (iradloss)____________________ 1 + Radiation_power_subtracted_from_plasma_power_balance_(MW)_______________ ______________________________ 9.1650E+01 OP + Alpha_particle_confinement_time_(s)_____________________________________ (taup)________________________ 2.2270E+01 + Alpha_particle/energy_confinement_time_ratio____________________________ (taup/taueff)_________________ 6.9512E+00 + Lower_limit_on_taup/taueff______________________________________________ (taulimit)____________________ 5.0000E+00 + Total_energy_confinement_time_including_radiation_loss_(s)______________ (total_energy_conf_time)______ 2.8018E+00 + Normalized_plasma_pressure_beta_as_defined_by_McDonald_et_al____________ (beta_mcdonald)_______________ 3.4553E-02 OP + Normalized_ion_Larmor_radius____________________________________________ (rho_star)____________________ 1.9603E-03 OP + Normalized_collisionality_______________________________________________ (nu_star)_____________________ 3.7266E-03 OP + Volume_measure_of_elongation____________________________________________ (kappaa_IPB)__________________ 1.6815E+00 OP + Total_volt-second_requirement_(Wb)______________________________________ (vsstt)_______________________ 5.5616E+02 OP + Inductive_volt-seconds_(Wb)_____________________________________________ (vsind)_______________________ 2.3585E+02 OP + Ejima_coefficient_______________________________________________________ (gamma)_______________________ 3.0000E-01 + Start-up_resistive_(Wb)_________________________________________________ (vsres)_______________________ 5.0159E+01 OP + Flat-top_resistive_(Wb)_________________________________________________ (vsbrn)_______________________ 2.7015E+02 OP + bootstrap_current_fraction_multiplier___________________________________ (cboot)_______________________ 1.0000E+00 + Bootstrap_fraction_(ITER_1989)__________________________________________ (bscf_iter89)_________________ 3.7098E-01 + Bootstrap_fraction_(Sauter_et_al)_______________________________________ (bscf_sauter)_________________ 4.1920E-01 + Bootstrap_fraction_(Nevins_et_al)_______________________________________ (bscf_nevins)_________________ 3.5042E-01 + Bootstrap_fraction_(Wilson)_____________________________________________ (bscf_wilson)_________________ 4.3349E-01 + Diamagnetic_fraction_(Hender)___________________________________________ (diacf_hender)________________ 1.2017E-02 + Diamagnetic_fraction_(SCENE)____________________________________________ (diacf_scene)_________________ 1.1139E-02 + Pfirsch-Schlueter_fraction_(SCENE)______________________________________ (pscf_scene)__________________ -3.0283E-03 + Bootstrap_fraction_(enforced)___________________________________________ (bootipf.)____________________ 4.1920E-01 + Diamagnetic_fraction_(enforced)_________________________________________ (diaipf.)_____________________ 0.0000E+00 + Pfirsch-Schlueter_fraction_(enforced)___________________________________ (psipf.)______________________ 0.0000E+00 + Loop_voltage_during_burn_(V)____________________________________________ (vburn)_______________________ 3.7450E-02 OP + Plasma_resistance_(ohm)_________________________________________________ (rplas)_______________________ 3.9755E-09 OP + Resistive_diffusion_time_(s)____________________________________________ (res_time)____________________ 3.0619E+03 OP + Plasma_inductance_(H)___________________________________________________ (rlp)_________________________ 1.4181E-05 OP + Coefficient_for_sawtooth_effects_on_burn_V-s_requirement________________ (csawth)______________________ 1.0000E+00 + Ratio_of_He_and_pellet_particle_confinement_times_______________________ (tauratio)____________________ 1.0000E+00 + Fuelling_rate_(nucleus-pairs/s)_________________________________________ (qfuel)_______________________ 3.3420E+21 OP + Fuel_burn-up_rate_(reactions/s)_________________________________________ (rndfuel)_____________________ 5.7755E+20 OP + Burn-up_fraction________________________________________________________ (burnup)______________________ 1.7282E-01 + # Energy confinement times, and required H-factors : # + # Current Drive System # + Current_drive_efficiency_model__________________________________________ (iefrf)_______________________ 10 + Secondary_current_drive_efficiency_model________________________________ (iefrffix)____________________ 0 + Ratio_of_power_for_flat-top_to_start-up_(MW)____________________________ (startupratio)________________ 1.0000E+00 + Auxiliary_power_used_for_plasma_heating_only_(MW)_______________________ (pheat)_______________________ 7.5000E+01 + Power_injected_for_current_drive_(MW)___________________________________ (pcurrentdrivemw)_____________ 5.1429E+00 + Maximum_Allowed_Bootstrap_current_fraction______________________________ (bscfmax)_____________________ 9.5000E-01 + Fusion_gain_factor_Q____________________________________________________ (bigq)________________________ 2.0060E+01 OP + Auxiliary_current_drive_(A)_____________________________________________ (auxiliary_cd)________________ 2.3908E+05 OP + Current_drive_efficiency_(A/W)__________________________________________ (effcd)_______________________ 4.6488E-02 OP + Normalised_current_drive_efficiency,_gamma_(10^20_A/W-m2)_______________ (gamcd)_______________________ 3.0000E-01 OP + Wall_plug_to_injector_efficiency________________________________________ (etacd)_______________________ 5.0000E-01 + ECRH_plasma_heating_efficiency__________________________________________ (gamma_ecrh)__________________ 3.0000E-01 + Bootstrap_fraction______________________________________________________ (bootipf)_____________________ 4.1920E-01 + Diamagnetic_fraction____________________________________________________ (diaipf)______________________ 0.0000E+00 + Pfirsch-Schlueter_fraction______________________________________________ (psipf)_______________________ 0.0000E+00 + Auxiliary_current_drive_fraction________________________________________ (faccd)_______________________ 1.4376E-02 + Inductive_fraction______________________________________________________ (facoh)_______________________ 5.6642E-01 + Total___________________________________________________________________ (plasipf+faccd+facoh)_________ 1.0000E+00 + Fraction_of_the_plasma_current_produced_by_non-inductive_means__________ (fvsbrnni)____________________ 4.3358E-01 ITV + Electron_cyclotron_injected_power_(MW)__________________________________ (echpwr)______________________ 8.0143E+01 OP + Maximum_allowable_ECRH_power_(MW)_______________________________________ (pinjalw)_____________________ 2.0000E+02 + ECH_wall_plug_efficiency________________________________________________ (etaech)______________________ 5.0000E-01 + ECH_wall_plug_power_(MW)________________________________________________ (echwpow)_____________________ 1.6029E+02 OP + Total_V-s_capability_of_Central_Solenoid/PF_coils_(Wb)__________________ (abs(vstot))__________________ 5.7728E+02 + Required_volt-seconds_during_start-up_(Wb)______________________________ (vssoft)______________________ 2.8601E+02 + Available_volt-seconds_during_burn_(Wb)_________________________________ (vsmax)_______________________ 2.7014E+02 + # Times # + Initial_charge_time_for_CS_from_zero_current_(s)________________________ (tramp)_______________________ 5.0000E+02 + Plasma_current_ramp-up_time_(s)_________________________________________ (tohs)________________________ 1.6631E+02 + Heating_time_(s)________________________________________________________ (theat)_______________________ 1.0000E+01 + Burn_time_(s)___________________________________________________________ (tburn)_______________________ 7.2035E+03 OP + Reset_time_to_zero_current_for_CS_(s)___________________________________ (tqnch)_______________________ 1.6631E+02 + Time_between_pulses_(s)_________________________________________________ (tdwell)______________________ 1.8000E+03 + Total_plant_cycle_time_(s)______________________________________________ (tcycle)______________________ 9.8463E+03 OP + # Radial Build # + TF_coil_radial_placement_switch_________________________________________ (tf_in_cs)____________________ 0 + TF_coil_radial_placement_switch_________________________________________ (tf_in_cs)____________________ 0 + Machine_bore_(m)________________________________________________________ (bore)________________________ 1.9854E+00 ITV + CS_radial_thickness_(m)_________________________________________________ (ohcth)_______________________ 5.7587E-01 ITV + CS_precompression_(m)___________________________________________________ (precomp)_____________________ 6.8064E-02 + CS_precompresion_to_TF_coil_radial_gap_(m)______________________________ (gapoh)_______________________ 8.0000E-02 + TF_coil_inboard_leg_(m)_________________________________________________ (tfcth)_______________________ 9.1597E-01 ITV + TF_coil_inboard_leg_insulation_gap_(m)__________________________________ (tftsgap)_____________________ 5.0000E-02 + Thermal_shield,_inboard_(m)_____________________________________________ (thshield_ib)_________________ 5.0000E-02 + thermal_shield_to_vessel_radial_gap_(m)_________________________________ (gapds)_______________________ 2.0000E-02 + Inboard_vacuum_vessel_radial_thickness_(m)______________________________ (d_vv_in)_____________________ 3.0000E-01 + Inner_radiation_shield_radial_thickness_(m)_____________________________ (shldith)_____________________ 3.0000E-01 + Gap_(m)_________________________________________________________________ (vvblgap)_____________________ 2.0000E-02 + Inboard_blanket_radial_thickness_(m)____________________________________ (blnkith)_____________________ 7.0000E-01 + Inboard_first_wall_radial_thickness_(m)_________________________________ (fwith)_______________________ 1.8000E-02 + Inboard_scrape-off_radial_thickness_(m)_________________________________ (scrapli)_____________________ 2.5000E-01 + Outboard_scrape-off_radial_thickness_(m)________________________________ (scraplo)_____________________ 2.5000E-01 + Outboard_first_wall_radial_thickness_(m)________________________________ (fwoth)_______________________ 1.8000E-02 + Outboard_blanket_radial_thickness_(m)___________________________________ (blnkoth)_____________________ 1.0000E+00 + Outer_radiation_shield_radial_thickness_(m)_____________________________ (shldoth)_____________________ 8.0000E-01 + Outboard_vacuum_vessel_radial_thickness_(m)_____________________________ (d_vv_out)____________________ 3.0000E-01 + Vessel_to_TF_radial_gap_(m)_____________________________________________ (gapsto)______________________ 1.3720E+00 + Thermal_shield,_outboard_(m)____________________________________________ (thshield_ob)_________________ 5.0000E-02 + Gap_(m)_________________________________________________________________ (tftsgap)_____________________ 5.0000E-02 + TF_coil_outboard_leg_radial_thickness_(m)_______________________________ (tfthko)______________________ 9.1597E-01 + # Vertical Build # + Divertor_null_switch____________________________________________________ (i_single_null)_______________ 1 + Vessel_-_TF_coil_vertical_gap_(m)_______________________________________ (vgap2)_______________________ 1.6300E-01 + Topside_vacuum_vessel_radial_thickness_(m)______________________________ (d_vv_top)____________________ 3.0000E-01 + Top_radiation_shield_thickness_(m)______________________________________ (shldtth)_____________________ 6.0000E-01 + Top_blanket_vertical_thickness_(m)______________________________________ (blnktth)_____________________ 8.5000E-01 + Top_first_wall_vertical_thickness_(m)___________________________________ (fwtth)_______________________ 1.8000E-02 + Top_scrape-off_vertical_thickness_(m)___________________________________ (vgaptop)_____________________ 6.0000E-01 + Plasma_half-height_(m)__________________________________________________ (rminor*kappa)________________ 4.9333E+00 + Bottom_scrape-off_vertical_thickness_(m)________________________________ (vgap)________________________ 2.0019E+00 + Divertor_structure_vertical_thickness_(m)_______________________________ (divfix)______________________ 6.2000E-01 + Bottom_radiation_shield_thickness_(m)___________________________________ (shldlth)_____________________ 7.0000E-01 + Underside_vacuum_vessel_radial_thickness_(m)____________________________ (d_vv_bot)____________________ 3.0000E-01 + External_cryostat_thickness_(m)_________________________________________ (ddwex)_______________________ 1.5000E-01 + Ratio_of_Central_solenoid_height_to_TF_coil_internal_height_____________ (ohhghf)______________________ 9.0000E-01 + Width_of_neutral_beam_duct_where_it_passes_between_the_TF_coils_(m)_____ (beamwd)______________________ 5.8000E-01 + # Divertor build and plasma position # + Plasma_top_position,_radial_(m)_________________________________________ (ptop_radial)_________________ 6.6667E+00 + Plasma_top_position,_vertical_(m)_______________________________________ (ptop_vertical)_______________ 4.9333E+00 + Plasma_geometric_centre,_radial_(m)_____________________________________ (physics_variables.rmajor.)___ 8.0000E+00 + Plasma_geometric_centre,_vertical_(m)___________________________________ (0.0)_________________________ 0.0000E+00 + Plasma_lower_physics_variables.triangularity____________________________ (tril)________________________ 5.0000E-01 + Plasma_elongation_______________________________________________________ (physics_variables.kappa.)____ 1.8500E+00 + TF_coil_vertical_offset_(m)_____________________________________________ (tfoffset)____________________ -6.1694E-01 + Plasma_outer_arc_radius_of_curvature_(m)________________________________ (rco)_________________________ 5.0422E+00 + Plasma_inner_arc_radius_of_curvature_(m)________________________________ (rci)_________________________ 9.7933E+00 + Plasma_lower_X-pt,_radial_(m)___________________________________________ (rxpt)________________________ 6.6667E+00 + Plasma_lower_X-pt,_vertical_(m)_________________________________________ (zxpt)________________________ -4.9333E+00 + Poloidal_plane_angle_between_vertical_and_inner_leg_(rad)_______________ (thetai)______________________ 2.0820E-01 + Poloidal_plane_angle_between_vertical_and_outer_leg_(rad)_______________ (thetao)______________________ 1.0429E+00 + Poloidal_plane_angle_between_inner_leg_and_plate_(rad)__________________ (betai)_______________________ 1.0000E+00 + Poloidal_plane_angle_between_outer_leg_and_plate_(rad)__________________ (betao)_______________________ 1.0000E+00 + Inner_divertor_leg_poloidal_length_(m)__________________________________ (plsepi)______________________ 1.0000E+00 + Outer_divertor_leg_poloidal_length_(m)__________________________________ (plsepo)______________________ 1.5000E+00 + Inner_divertor_plate_length_(m)_________________________________________ (plleni)______________________ 1.0000E+00 + Outer_divertor_plate_length_(m)_________________________________________ (plleno)______________________ 1.0000E+00 + Inner_strike_point,_radial_(m)__________________________________________ (rspi)________________________ 5.6883E+00 + Inner_strike_point,_vertical_(m)________________________________________ (zspi)________________________ -5.1400E+00 + Inner_plate_top,_radial_(m)_____________________________________________ (rplti)_______________________ 5.8656E+00 + Inner_plate_top,_vertical_(m)___________________________________________ (zplti)_______________________ -4.6725E+00 + Inner_plate_bottom,_radial_(m)__________________________________________ (rplbi)_______________________ 5.5109E+00 + Inner_plate_bottom,_vertical_(m)________________________________________ (zplbi)_______________________ -5.6075E+00 + Outer_strike_point,_radial_(m)__________________________________________ (rspo)________________________ 7.4223E+00 + Outer_strike_point,_vertical_(m)________________________________________ (zspo)________________________ -6.2291E+00 + Outer_plate_top,_radial_(m)_____________________________________________ (rplto)_______________________ 7.6496E+00 + Outer_plate_top,_vertical_(m)___________________________________________ (zplto)_______________________ -5.7838E+00 + Outer_plate_bottom,_radial_(m)__________________________________________ (rplbo)_______________________ 7.1949E+00 + Outer_plate_bottom,_vertical_(m)________________________________________ (zplbo)_______________________ -6.6744E+00 + Calculated_maximum_divertor_height_(m)__________________________________ (divht)_______________________ 2.0019E+00 + # TF coils # + Allowable_maximum_shear_stress_in_TF_coil_case_(Tresca_criterion)_(Pa)__ (sig_tf_case_max)_____________ 7.5000E+08 + Allowable_maximum_shear_stress_in_TF_coil_conduit_(Tresca_criterion)_(Pa (sig_tf_wp_max)_______________ 7.5000E+08 + WP_transverse_modulus_(GPa)_____________________________________________ (eyoung_wp_trans*1.0d-9)______ 4.3534E+01 OP + WP_vertical_modulus_(GPa)_______________________________________________ (eyoung_wp_axial*1.0d-9)______ 1.1510E+02 OP + WP_transverse_Poissons_ratio____________________________________________ (poisson_wp_trans)____________ 3.0390E-01 OP + WP_vertical-transverse_Pois._rat._______________________________________ (poisson_wp_axial)____________ 3.1568E-01 OP + Radial____stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_r_max(1))_____________ 4.8849E-08 + toroidal__stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_t_max(1))_____________ -4.8724E+08 + Vertical__stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_z_max(1))_____________ 2.6028E+08 + Von-Mises_stress_at_maximum_shear_of_layer_1_(Pa)_______________________ (sig_tf_vmises_max(1))________ 6.5725E+08 + Maximum_shear_stress_for_the_Tresca_yield_criterion_1_(Pa)______________ (sig_tf_tresca_max(1))________ 7.4752E+08 + Radial____stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_r_max(2))_____________ -1.5411E+08 + toroidal__stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_t_max(2))_____________ -3.7861E+08 + Vertical__stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_z_max(2))_____________ 2.6028E+08 + Von-Mises_stress_at_maximum_shear_of_layer_2_(Pa)_______________________ (sig_tf_vmises_max(2))________ 5.5645E+08 + Maximum_shear_stress_for_the_Tresca_yield_criterion_2_(Pa)______________ (sig_tf_tresca_max(2))________ 6.3889E+08 + Radial____stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_r_max(3))_____________ 6.1398E+06 + toroidal__stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_t_max(3))_____________ -3.6314E+08 + Vertical__stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_z_max(3))_____________ 1.4510E+08 + Von-Mises_stress_at_maximum_shear_of_layer_3_(Pa)_______________________ (sig_tf_vmises_max(3))________ 4.5345E+08 + Maximum_shear_stress_for_the_Tresca_yield_criterion_3_(Pa)______________ (sig_tf_tresca_max(3))________ 5.0824E+08 + Maximum_radial_deflection_at_midplane_(m)_______________________________ (deflect)_____________________ -6.2714E-03 OP + Vertical_strain_on_casing_______________________________________________ (casestr)_____________________ 1.2697E-03 OP + Radial_strain_on_insulator______________________________________________ (insstrain)___________________ -7.6923E-03 OP + Conductor_technology____________________________________________________ (i_tf_sup)____________________ 1 + Superconductor_material_________________________________________________ (i_tf_sc_mat)_________________ 1 + Presence_of_TF_demountable_joints_______________________________________ (itart)_______________________ 0 + TF_inboard_leg_support_strategy_________________________________________ (i_tf_bucking)________________ 1 + Number_of_TF_coils______________________________________________________ (n_tf)________________________ 16 + Inboard_leg_centre_radius_(m)___________________________________________ (r_tf_inboard_mid)____________ 3.1673E+00 OP + Outboard_leg_centre_radius_(m)__________________________________________ (r_tf_outboard_mid)___________ 1.4985E+01 OP + Total_inboard_leg_radial_thickness_(m)__________________________________ (tfcth)_______________________ 9.1597E-01 ITV + Total_outboard_leg_radial_thickness_(m)_________________________________ (tfthko)______________________ 9.1597E-01 + Outboard_leg_toroidal_thickness_(m)_____________________________________ (tftort)______________________ 1.4145E+00 OP + Maximum_inboard_edge_height_(m)_________________________________________ (hmax)________________________ 8.8182E+00 OP + Mean_coil_circumference_(including_inboard_leg_length)_(m)______________ (tfleng)______________________ 4.7937E+01 OP + Vertical_TF_shape_______________________________________________________ (i_tf_shape)__________________ 1 + TF_coil_arc_point_0_R_(m)_______________________________________________ (xarc(1))_____________________ 3.6253E+00 + TF_coil_arc_point_0_Z_(m)_______________________________________________ (yarc(1))_____________________ 4.5506E+00 + TF_coil_arc_point_1_R_(m)_______________________________________________ (xarc(2))_____________________ 7.4667E+00 + TF_coil_arc_point_1_Z_(m)_______________________________________________ (yarc(2))_____________________ 7.5843E+00 + TF_coil_arc_point_2_R_(m)_______________________________________________ (xarc(3))_____________________ 1.4527E+01 + TF_coil_arc_point_2_Z_(m)_______________________________________________ (yarc(3))_____________________ 0.0000E+00 + TF_coil_arc_point_3_R_(m)_______________________________________________ (xarc(4))_____________________ 7.4667E+00 + TF_coil_arc_point_3_Z_(m)_______________________________________________ (yarc(4))_____________________ -8.8182E+00 + TF_coil_arc_point_4_R_(m)_______________________________________________ (xarc(5))_____________________ 3.6253E+00 + TF_coil_arc_point_4_Z_(m)_______________________________________________ (yarc(5))_____________________ -5.2909E+00 + TF_cross-section_(total)_(m2)___________________________________________ (tfareain)____________________ 1.8229E+01 + Total_steel_cross-section_(m2)__________________________________________ (a_tf_steel*n_tf)_____________ 1.2853E+01 + Total_steel_TF_fraction_________________________________________________ (f_tf_steel)__________________ 7.0508E-01 + Total_Insulation_cross-section_(total)_(m2)_____________________________ (a_tf_ins*n_tf)_______________ 8.4752E-01 + Total_Insulation_fraction_______________________________________________ (f_tf_ins)____________________ 4.6493E-02 + Casing_cross_section_area_(per_leg)_(m2)________________________________ (acasetf)_____________________ 5.6444E-01 + Inboard_leg_case_plasma_side_wall_thickness_(m)_________________________ (casthi)______________________ 6.0000E-02 + Inboard_leg_case_inboard_"nose"_thickness_(m)___________________________ (thkcas)______________________ 2.8216E-01 ITV + Inboard_leg_case_sidewall_thickness_at_its_narrowest_point_(m)__________ (casths)______________________ 5.0000E-02 + External_case_mass_per_coil_(kg)________________________________________ (whtcas)______________________ 5.5456E+05 OP + WP_cross_section_area_with_insulation_and_insertion_(per_coil)_(m2)_____ (awpc)________________________ 5.7486E-01 + WP_cross_section_area_(per_coil)_(m2)___________________________________ (aswp)________________________ 5.1696E-01 + Winding_pack_radial_thickness_(m)_______________________________________ (dr_tf_wp)____________________ 5.0416E-01 ITV + Winding_pack_toroidal_width_1_(m)_______________________________________ (wwp1)________________________ 1.1904E+00 OP + Winding_pack_toroidal_width_2_(m)_______________________________________ (wwp2)________________________ 1.0901E+00 OP + Ground_wall_insulation_thickness_(m)____________________________________ (tinstf)______________________ 8.0000E-03 + Winding_pack_insertion_gap_(m)__________________________________________ (tfinsgap)____________________ 1.0000E-02 + Steel_WP_cross-section_(total)_(m2)_____________________________________ (aswp*n_tf)___________________ 3.8217E+00 + Steel_WP_fraction_______________________________________________________ (aswp/awpc)___________________ 4.1550E-01 + Insulation_WP_fraction__________________________________________________ (aiwp/awpc)___________________ 4.7934E-02 + Cable_WP_fraction_______________________________________________________ ((awpc-aswp-aiwp)/awpc)_______ 5.3656E-01 + Turn_parametrisation____________________________________________________ (i_tf_turns_integer)__________ 0 + Number_of_turns_per_TF_coil_____________________________________________ (n_tf_turn)___________________ 1.4739E+02 OP + Width_of_turn_including_inter-turn_insulation_(m)_______________________ (t_turn_tf)___________________ 5.9223E-02 OP + Width_of_conductor_(square)_(m)_________________________________________ (t_conductor)_________________ 5.7623E-02 OP + Width_of_space_inside_conductor_(m)_____________________________________ (t_cable)_____________________ 4.1604E-02 OP + Steel_conduit_thickness_(m)_____________________________________________ (thwcndut)____________________ 8.0099E-03 ITV + Inter-turn_insulation_thickness_(m)_____________________________________ (thicndut)____________________ 8.0000E-04 + Diameter_of_central_helium_channel_in_cable_____________________________ (dhecoil)_____________________ 1.0000E-02 + internal_area_of_the_cable_space________________________________________ (acstf)_______________________ 1.6999E-03 + Coolant_fraction_in_conductor_excluding_central_channel_________________ (vftf)________________________ 3.0000E-01 + Copper_fraction_of_conductor____________________________________________ (fcutfsu)_____________________ 8.4212E-01 ITV + Superconductor_fraction_of_conductor____________________________________ (1-fcutfsu)___________________ 1.5788E-01 + Check_total_area_fractions_in_winding_pack_=_1__________________________ ______________________________ 1.0000E+00 + minimum_TF_conductor_temperature_margin__(K)____________________________ (tmargmin_tf)_________________ 1.5000E+00 + TF_conductor_temperature_margin_(K)_____________________________________ (tmargtf)_____________________ 1.5049E+00 + Elastic_properties_behavior_____________________________________________ (i_tf_cond_eyoung_axial)______ 0 + Conductor_axial_Youngs_modulus__________________________________________ (eyoung_cond_axial)___________ 0.0000E+00 + Conductor_transverse_Youngs_modulus_____________________________________ (eyoung_cond_trans)___________ 0.0000E+00 + Superconductor_mass_per_coil_(kg)_______________________________________ (whtconsc)____________________ 4.6964E+03 OP + Copper_mass_per_coil_(kg)_______________________________________________ (whtconcu)____________________ 5.8073E+04 OP + Steel_conduit_mass_per_coil_(kg)________________________________________ (whtconsh)____________________ 8.9310E+04 OP + Conduit_insulation_mass_per_coil_(kg)___________________________________ (whtconin)____________________ 2.3777E+03 OP + Total_conduit_mass_per_coil_(kg)________________________________________ (whtcon)______________________ 1.5446E+05 OP + Mass_of_each_TF_coil_(kg)_______________________________________________ (whttf/n_tf)__________________ 7.1402E+05 OP + Total_TF_coil_mass_(kg)_________________________________________________ (whttf)_______________________ 1.1424E+07 OP + Nominal_peak_field_assuming_toroidal_symmetry_(T)_______________________ (bmaxtf)______________________ 1.2178E+01 OP + Total_current_in_all_TF_coils_(MA)______________________________________ (ritfc/1.D6)__________________ 2.1176E+02 OP + TF_coil_current_(summed_over_all_coils)_(A)_____________________________ (ritfc)_______________________ 2.1176E+08 + Actual_peak_field_at_discrete_conductor_(T)_____________________________ (bmaxtfrp)____________________ 1.2636E+01 OP + Winding_pack_current_density_(A/m2)_____________________________________ (jwptf)_______________________ 2.5602E+07 OP + Inboard_leg_mid-plane_conductor_current_density_(A/m2)__________________ (oacdcp)______________________ 1.1617E+07 + Total_stored_energy_in_TF_coils_(GJ)____________________________________ (estotftgj)___________________ 1.2161E+02 OP + Inboard_vertical_tension_per_coil_(N)___________________________________ (vforce)______________________ 2.0908E+08 OP + Outboard_vertical_tension_per_coil_(N)__________________________________ (vforce_outboard)_____________ 2.0908E+08 OP + inboard_vertical_tension_fraction_(-)___________________________________ (f_vforce_inboard)____________ 5.0000E-01 OP + Centring_force_per_coil_(N/m)___________________________________________ (cforce)______________________ 8.0590E+07 OP + Max_allowed_tfcoil_variables.ripple_amplitude_at_plasma_outboard_midplan (ripmax)______________________ 6.0000E-01 + Ripple_amplitude_at_plasma_outboard_midplane_(%)________________________ (ripple)______________________ 6.0000E-01 OP + Actual_quench_time_(or_time_constant)_(s)_______________________________ (tdmptf)______________________ 1.8429E+01 ITV + Vacuum_Vessel_stress_on_quench_(Pa)_____________________________________ (vv_stress_quench)____________ 6.1442E+07 OP + Maximum_allowed_voltage_during_quench_due_to_insulation_(kV)____________ (vdalw)_______________________ 9.5837E+00 ITV + Actual_quench_voltage_(kV)______________________________________________ (vtfskv)______________________ 9.1862E+00 OP + Maximum_allowed_temp_rise_during_a_quench_(K)___________________________ (tmaxpro)_____________________ 1.5000E+02 + # Superconducting TF Coils # + Superconductor_switch___________________________________________________ (isumat)______________________ 1 + Critical_field_at_zero_temperature_and_strain_(T)_______________________ (bc20m)_______________________ 3.2970E+01 + Critical_temperature_at_zero_field_and_strain_(K)_______________________ (tc0m)________________________ 1.6060E+01 + Helium_temperature_at_peak_field_(=_superconductor_temperature)_(K)_____ (thelium)_____________________ 4.7500E+00 + Total_helium_fraction_inside_cable_space________________________________ (fhetot)______________________ 3.4620E-01 OP + Copper_fraction_of_conductor____________________________________________ (fcutfsu)_____________________ 8.4212E-01 ITV + Residual_manufacturing_strain_on_superconductor_________________________ (str_tf_con_res)______________ -5.0000E-03 + Self-consistent_strain_on_superconductor________________________________ (str_wp)______________________ 2.0730E-03 + Critical_current_density_in_superconductor_(A/m2)_______________________ (jcritsc)_____________________ 7.1337E+08 OP + Critical_current_density_in_strand_(A/m2)_______________________________ (jcritstr)____________________ 1.1263E+08 OP + Critical_current_density_in_winding_pack_(A/m2)_________________________ (jwdgcrt)_____________________ 3.5688E+07 OP + Actual_current_density_in_winding_pack_(A/m2)___________________________ (jwdgop)______________________ 2.5602E+07 OP + Minimum_allowed_temperature_margin_in_superconductor_(K)________________ (tmargmin_tf)_________________ 1.5000E+00 + Actual_temperature_margin_in_superconductor_(K)_________________________ (tmarg)_______________________ 1.5049E+00 OP + Critical_current_(A)____________________________________________________ (icrit)_______________________ 1.2517E+05 OP + Actual_current_(A)______________________________________________________ (cpttf)_______________________ 8.9795E+04 ITV + Actual_current_/_critical_current_______________________________________ (iooic)_______________________ 7.1737E-01 OP + # Central Solenoid and PF Coils # + Central_solenoid_superconductor_material________________________________ (isumatoh)____________________ 1 + Maximum_field_at_Beginning_Of_Pulse_(T)_________________________________ (bmaxoh0)_____________________ 1.4050E+01 OP + Critical_superconductor_current_density_at_BOP_(A/m2)___________________ (jscoh_bop)___________________ 3.4918E+08 OP + Critical_strand_current_density_at_BOP_(A/m2)___________________________ (jstrandoh_bop)_______________ 1.0475E+08 OP + Allowable_overall_current_density_at_BOP_(A/m2)_________________________ (rjohc0)______________________ 3.5294E+07 OP + Actual_overall_current_density_at_BOP_(A/m2)____________________________ (cohbop)______________________ 1.9126E+07 OP + Maximum_field_at_End_Of_Flattop_(T)_____________________________________ (bmaxoh)______________________ 1.3920E+01 OP + Critical_superconductor_current_density_at_EOF_(A/m2)___________________ (jscoh_eof)___________________ 3.6097E+08 OP + Critical_strand_current_density_at_EOF_(A/m2)___________________________ (jstrandoh_eof)_______________ 1.0829E+08 OP + Allowable_overall_current_density_at_EOF_(A/m2)_________________________ (rjohc)_______________________ 3.6485E+07 OP + Actual_overall_current_density_at_EOF_(A/m2)____________________________ (coheof)______________________ 2.0264E+07 ITV + CS_inside_radius_(m)____________________________________________________ (bore)________________________ 1.9854E+00 ITV + CS_thickness_(m)________________________________________________________ (ohcth)_______________________ 5.7587E-01 ITV + Gap_between_central_solenoid_and_TF_coil_(m)____________________________ (gapoh)_______________________ 8.0000E-02 + CS_overall_cross-sectional_area_(m2)____________________________________ (areaoh)______________________ 9.1407E+00 OP + CS_conductor+void_cross-sectional_area_(m2)_____________________________ (awpoh)_______________________ 4.3996E+00 OP + ___CS_conductor_cross-sectional_area_(m2)_______________________________ (awpoh*(1-vfohc))_____________ 3.0797E+00 OP + ___CS_void_cross-sectional_area_(m2)____________________________________ (awpoh*vfohc)_________________ 1.3199E+00 OP + CS_steel_cross-sectional_area_(m2)______________________________________ (areaoh-awpoh)________________ 4.7411E+00 OP + CS_steel_area_fraction__________________________________________________ (oh_steel_frac)_______________ 5.1868E-01 ITV + Switch_for_CS_stress_calculation________________________________________ (i_cs_stress)_________________ 0 + Allowable_stress_in_CS_steel_(Pa)_______________________________________ (alstroh)_____________________ 7.5000E+08 + Hoop_stress_in_CS_steel_(Pa)____________________________________________ (sig_hoop)____________________ 6.7569E+08 OP + Axial_stress_in_CS_steel_(Pa)___________________________________________ (sig_axial)___________________ -7.6205E+08 OP + Maximum_shear_stress_in_CS_steel_for_the_Tresca_criterion_(Pa)__________ (s_tresca_oh)_________________ 6.7569E+08 OP + Axial_force_in_CS_(N)___________________________________________________ (axial_force)_________________ -1.6256E+09 OP + Residual_manufacturing_strain_in_CS_superconductor_material_____________ (tfcoil_variables.str_cs_con_r -5.0000E-03 + Copper_fraction_in_strand_______________________________________________ (fcuohsu)_____________________ 7.0000E-01 + Void_(coolant)_fraction_in_conductor____________________________________ (vfohc)_______________________ 3.0000E-01 + Helium_coolant_temperature_(K)__________________________________________ (tftmp)_______________________ 4.7500E+00 + CS_temperature_margin_(K)_______________________________________________ (tmargoh)_____________________ 1.5052E+00 OP + Minimum_permitted_temperature_margin_(K)________________________________ (tmargmin_cs)_________________ 1.5000E+00 + Residual_hoop_stress_in_CS_Steel_(Pa)___________________________________ (residual_sig_hoop)___________ 2.4000E+08 + Minimum_burn_time_(s)___________________________________________________ (tbrnmn)______________________ 7.2000E+03 + Initial_vertical_crack_size_(m)_________________________________________ (t_crack_vertical)____________ 8.9000E-04 + Initial_radial_crack_size_(m)___________________________________________ (t_crack_radial)______________ 2.6700E-03 + CS_turn_area_(m)________________________________________________________ (a_oh_turn)___________________ 1.9739E-03 + CS_turn_length_(m)______________________________________________________ (l_cond_cst)__________________ 7.6953E-02 + CS_turn_internal_cable_space_radius_(m)_________________________________ (r_in_cst)____________________ 7.4740E-03 + CS_turn_width_(m)_______________________________________________________ (d_cond_cst)__________________ 2.5651E-02 + CS_structural_vertical_thickness_(m)____________________________________ (t_structural_vertical)_______ 5.3514E-03 + CS_structural_radial_thickness_(m)______________________________________ (t_structural_radial)_________ 5.3514E-03 + Allowable_number_of_cycles_till_CS_fracture_____________________________ (n_cycle)_____________________ 1.3378E+02 OP + Minimum_number_of_cycles_required_till_CS_fracture______________________ (n_cycle_min)_________________ 2.0000E+04 OP + PF_coil_superconductor_material_________________________________________ (isumatpf)____________________ 3 + Copper_fraction_in_conductor____________________________________________ (fcupfsu)_____________________ 6.9000E-01 + Maximum_permissible_tensile_stress_(MPa)________________________________ (sigpfcalw)___________________ 5.0000E+02 + JxB_hoop_force_fraction_supported_by_case_______________________________ (sigpfcf)_____________________ 6.6600E-01 + PF_coil_0_radius_(m)____________________________________________________ (rpf[0]_______________________ 5.5667E+00 + PF_coil_0_vertical_position_(m)_________________________________________ (zpf[0])______________________ 9.3603E+00 + PF_coil_0_radial_thickness_(m)__________________________________________ (pfdr(0))_____________________ 1.2727E+00 + PF_coil_0_vertical_thickness_(m)________________________________________ (pfdz(0))_____________________ 1.2727E+00 + PF_coil_0_turns_________________________________________________________ (turns[0])____________________ 4.4541E+02 + PF_coil_0_current_(MA)__________________________________________________ (ric[0])______________________ 1.7816E+01 + PF_coil_0_field_(T)_____________________________________________________ (bpf[0])______________________ 6.2280E+00 + PF_coil_1_radius_(m)____________________________________________________ (rpf[1]_______________________ 5.5667E+00 + PF_coil_1_vertical_position_(m)_________________________________________ (zpf[1])______________________ -1.0594E+01 + PF_coil_1_radial_thickness_(m)__________________________________________ (pfdr(1))_____________________ 1.3651E+00 + PF_coil_1_vertical_thickness_(m)________________________________________ (pfdz(1))_____________________ -1.3651E+00 + PF_coil_1_turns_________________________________________________________ (turns[1])____________________ 5.1248E+02 + PF_coil_1_current_(MA)__________________________________________________ (ric[1])______________________ 2.0499E+01 + PF_coil_1_field_(T)_____________________________________________________ (bpf[1])______________________ 6.6990E+00 + PF_coil_2_radius_(m)____________________________________________________ (rpf[2]_______________________ 1.6731E+01 + PF_coil_2_vertical_position_(m)_________________________________________ (zpf[2])______________________ 2.6667E+00 + PF_coil_2_radial_thickness_(m)__________________________________________ (pfdr(2))_____________________ 1.1332E+00 + PF_coil_2_vertical_thickness_(m)________________________________________ (pfdz(2))_____________________ 1.1332E+00 + PF_coil_2_turns_________________________________________________________ (turns[2])____________________ 1.9262E+02 + PF_coil_2_current_(MA)__________________________________________________ (ric[2])______________________ -7.7049E+00 + PF_coil_2_field_(T)_____________________________________________________ (bpf[2])______________________ 2.6389E+00 + PF_coil_3_radius_(m)____________________________________________________ (rpf[3]_______________________ 1.6731E+01 + PF_coil_3_vertical_position_(m)_________________________________________ (zpf[3])______________________ -2.6667E+00 + PF_coil_3_radial_thickness_(m)__________________________________________ (pfdr(3))_____________________ 1.1332E+00 + PF_coil_3_vertical_thickness_(m)________________________________________ (pfdz(3))_____________________ -1.1332E+00 + PF_coil_3_turns_________________________________________________________ (turns[3])____________________ 1.9262E+02 + PF_coil_3_current_(MA)__________________________________________________ (ric[3])______________________ -7.7049E+00 + PF_coil_3_field_(T)_____________________________________________________ (bpf[3])______________________ 2.6389E+00 + PF_coil_4_radius_(m)____________________________________________________ (rpf[4]_______________________ 1.5209E+01 + PF_coil_4_vertical_position_(m)_________________________________________ (zpf[4])______________________ 7.4667E+00 + PF_coil_4_radial_thickness_(m)__________________________________________ (pfdr(4))_____________________ 8.0773E-01 + PF_coil_4_vertical_thickness_(m)________________________________________ (pfdz(4))_____________________ 8.0773E-01 + PF_coil_4_turns_________________________________________________________ (turns[4])____________________ 1.3049E+02 + PF_coil_4_current_(MA)__________________________________________________ (ric[4])______________________ -5.2194E+00 + PF_coil_4_field_(T)_____________________________________________________ (bpf[4])______________________ 2.5737E+00 + PF_coil_5_radius_(m)____________________________________________________ (rpf[5]_______________________ 1.5209E+01 + PF_coil_5_vertical_position_(m)_________________________________________ (zpf[5])______________________ -7.4667E+00 + PF_coil_5_radial_thickness_(m)__________________________________________ (pfdr(5))_____________________ 8.0773E-01 + PF_coil_5_vertical_thickness_(m)________________________________________ (pfdz(5))_____________________ -8.0773E-01 + PF_coil_5_turns_________________________________________________________ (turns[5])____________________ 1.3049E+02 + PF_coil_5_current_(MA)__________________________________________________ (ric[5])______________________ -5.2194E+00 + PF_coil_5_field_(T)_____________________________________________________ (bpf[5])______________________ 2.5737E+00 + Central_solenoid_radius_(m)_____________________________________________ (rpf[nohc-1])_________________ 2.2734E+00 + Central_solenoid_vertical_position_(m)__________________________________ (zpf[nohc-1])_________________ 0.0000E+00 + Central_solenoid_radial_thickness_(m)___________________________________ (ohdr)________________________ 5.7587E-01 + Central_solenoid_vertical_thickness_(m)_________________________________ (ohdz)________________________ 1.5873E+01 + Central_solenoid_turns__________________________________________________ (turns[nohc-1])_______________ 4.6308E+03 + Central_solenoid_current_(MA)___________________________________________ (ric[nohc-1])_________________ -1.8523E+02 + Central_solenoid_field_(T)______________________________________________ (bpf[nohc-1])_________________ 1.4050E+01 + Sum_of_squares_of_residuals_____________________________________________ (ssq0)________________________ 3.5207E-04 OP + Smoothing_parameter_____________________________________________________ (alfapf)______________________ 5.0000E-10 + # Volt Second Consumption # + Total_volt-second_consumption_by_coils_(Wb)_____________________________ (vstot)_______________________ -5.8000E+02 OP + # Waveforms # + Ratio_of_central_solenoid_current_at_beginning_of_Pulse_/_end_of_flat-to (fcohbop)_____________________ 9.4380E-01 ITV + Ratio_of_central_solenoid_current_at_beginning_of_Flat-top_/_end_of_flat (fcohbof)_____________________ -1.4083E-01 OP + # PF Circuit Waveform Data # + Number_of_PF_circuits_including_CS_and_plasma___________________________ (ncirt)_______________________ 8 + PF_Circuit_0_Time_point_0_(A)___________________________________________ (pfc0t0)______________________ 0.0000E+00 + PF_Circuit_0_Time_point_1_(A)___________________________________________ (pfc0t1)______________________ 1.3971E+07 + PF_Circuit_0_Time_point_2_(A)___________________________________________ (pfc0t2)______________________ 1.7816E+07 + PF_Circuit_0_Time_point_3_(A)___________________________________________ (pfc0t3)______________________ 1.7816E+07 + PF_Circuit_0_Time_point_4_(A)___________________________________________ (pfc0t4)______________________ 9.2844E+05 + PF_Circuit_0_Time_point_5_(A)___________________________________________ (pfc0t5)______________________ 0.0000E+00 + PF_Circuit_1_Time_point_0_(A)___________________________________________ (pfc1t0)______________________ 0.0000E+00 + PF_Circuit_1_Time_point_1_(A)___________________________________________ (pfc1t1)______________________ 1.8269E+07 + PF_Circuit_1_Time_point_2_(A)___________________________________________ (pfc1t2)______________________ 2.0499E+07 + PF_Circuit_1_Time_point_3_(A)___________________________________________ (pfc1t3)______________________ 2.0499E+07 + PF_Circuit_1_Time_point_4_(A)___________________________________________ (pfc1t4)______________________ -1.5831E+06 + PF_Circuit_1_Time_point_5_(A)___________________________________________ (pfc1t5)______________________ 0.0000E+00 + PF_Circuit_2_Time_point_0_(A)___________________________________________ (pfc2t0)______________________ -0.0000E+00 + PF_Circuit_2_Time_point_1_(A)___________________________________________ (pfc2t1)______________________ 4.9542E+05 + PF_Circuit_2_Time_point_2_(A)___________________________________________ (pfc2t2)______________________ -7.1060E+06 + PF_Circuit_2_Time_point_3_(A)___________________________________________ (pfc2t3)______________________ -7.1060E+06 + PF_Circuit_2_Time_point_4_(A)___________________________________________ (pfc2t4)______________________ -7.7049E+06 + PF_Circuit_2_Time_point_5_(A)___________________________________________ (pfc2t5)______________________ -0.0000E+00 + PF_Circuit_3_Time_point_0_(A)___________________________________________ (pfc3t0)______________________ -0.0000E+00 + PF_Circuit_3_Time_point_1_(A)___________________________________________ (pfc3t1)______________________ 4.9542E+05 + PF_Circuit_3_Time_point_2_(A)___________________________________________ (pfc3t2)______________________ -7.1060E+06 + PF_Circuit_3_Time_point_3_(A)___________________________________________ (pfc3t3)______________________ -7.1060E+06 + PF_Circuit_3_Time_point_4_(A)___________________________________________ (pfc3t4)______________________ -7.7049E+06 + PF_Circuit_3_Time_point_5_(A)___________________________________________ (pfc3t5)______________________ -0.0000E+00 + PF_Circuit_4_Time_point_0_(A)___________________________________________ (pfc4t0)______________________ -0.0000E+00 + PF_Circuit_4_Time_point_1_(A)___________________________________________ (pfc4t1)______________________ 3.2650E+05 + PF_Circuit_4_Time_point_2_(A)___________________________________________ (pfc4t2)______________________ -4.8247E+06 + PF_Circuit_4_Time_point_3_(A)___________________________________________ (pfc4t3)______________________ -4.8247E+06 + PF_Circuit_4_Time_point_4_(A)___________________________________________ (pfc4t4)______________________ -5.2194E+06 + PF_Circuit_4_Time_point_5_(A)___________________________________________ (pfc4t5)______________________ -0.0000E+00 + PF_Circuit_5_Time_point_0_(A)___________________________________________ (pfc5t0)______________________ -0.0000E+00 + PF_Circuit_5_Time_point_1_(A)___________________________________________ (pfc5t1)______________________ 3.2650E+05 + PF_Circuit_5_Time_point_2_(A)___________________________________________ (pfc5t2)______________________ -4.8247E+06 + PF_Circuit_5_Time_point_3_(A)___________________________________________ (pfc5t3)______________________ -4.8247E+06 + PF_Circuit_5_Time_point_4_(A)___________________________________________ (pfc5t4)______________________ -5.2194E+06 + PF_Circuit_5_Time_point_5_(A)___________________________________________ (pfc5t5)______________________ -0.0000E+00 + CS_Circuit_Time_point_0_(A)_____________________________________________ (cs_t0)_______________________ -0.0000E+00 + CS_Circuit_Time_point_1_(A)_____________________________________________ (cs_t1)_______________________ 1.7482E+08 + CS_Circuit_Time_point_2_(A)_____________________________________________ (cs_t2)_______________________ 2.6086E+07 + CS_Circuit_Time_point_3_(A)_____________________________________________ (cs_t3)_______________________ 2.6086E+07 + CS_Circuit_Time_point_4_(A)_____________________________________________ (cs_t4)_______________________ -1.8523E+08 + CS_Circuit_Time_point_5_(A)_____________________________________________ (cs_t5)_______________________ -0.0000E+00 + Plasma_Time_point_0_(A)_________________________________________________ (plasmat0)____________________ 0.0000E+00 + Plasma_Time_point_1_(A)_________________________________________________ (plasmat1)____________________ 0.0000E+00 + Plasma_Time_point_2_(A)_________________________________________________ (plasmat2)____________________ 1.6631E+07 + Plasma_Time_point_3_(A)_________________________________________________ (plasmat3)____________________ 1.6631E+07 + Plasma_Time_point_4_(A)_________________________________________________ (plasmat4)____________________ 1.6631E+07 + Plasma_Time_point_5_(A)_________________________________________________ (plasmat5)____________________ 0.0000E+00 + # Support Structure # + Outer_PF_coil_fence_mass_(kg)___________________________________________ (fncmass)_____________________ 2.2924E+05 OP + Intercoil_support_structure_mass_(kg)___________________________________ (aintmass)____________________ 4.3045E+06 OP + Mass_of_cooled_components_(kg)__________________________________________ (coldmass)____________________ 3.4369E+07 OP + Gravity_support_structure_mass_(kg)_____________________________________ (clgsmass)____________________ 1.2760E+06 OP + Torus_leg_support_mass_(kg)_____________________________________________ (gsm1)________________________ 8.5820E+04 OP + Ring_beam_mass_(kg)_____________________________________________________ (gsm2)________________________ 4.0088E+05 OP + Ring_legs_mass_(kg)_____________________________________________________ (gsm3)________________________ 6.8283E+05 OP + # PF Coil Inductances # + # Nuclear Heating Magnets Before Renormalisation # + Shield_line_density_(tonne/m2)__________________________________________ (x_shield)____________________ 4.0560E+00 + Blanket_line_density_(tonne/m2)_________________________________________ (x_blanket)___________________ 2.2911E+00 + Unit_nuclear_heating_in_TF_coil_(W/GW)__________________________________ (tfc_nuc_heating)_____________ 1.4866E+04 + Total_nuclear_heating_in_TF_coil_(MW)___________________________________ (ptfnuc.)_____________________ 2.4085E-02 + powfmw__________________________________________________________________ (powfmw.)_____________________ 1.6202E+03 + total_mass_of_the_TF_coils_(kg)_________________________________________ (whttf)_______________________ 1.1424E+07 + # Pumping for primary coolant (helium) # + Pressure_drop_in_FW_and_blanket_coolant_incl._hx_and_pipes_(Pa)_________ (dp_he)_______________________ 5.5000E+05 + Fraction_of_FW_and_blanket_thermal_power_required_for_pumping___________ (fpump)_______________________ 8.9463E-02 OP + Total_power_absorbed_by_FW_&_blanket_(MW)_______________________________ (p_plasma)____________________ 1.6698E+03 OP + Inlet_temperature_of_FW_&_blanket_coolant_pump_(K)______________________ (t_in_compressor)_____________ 5.5703E+02 OP + Coolant_pump_outlet/Inlet_temperature_of_FW_&_blanket_(K)_______________ (t_in_bb)_____________________ 5.7313E+02 + Outlet_temperature_of_FW_&_blanket_(K)__________________________________ (t_out_bb)____________________ 7.7313E+02 + Mechanical_pumping_power_for_FW_and_blanket_cooling_loop_including_heat_ (htpmw_fw_blkt)_______________ 1.6407E+02 OP + Mechanical_pumping_power_for_divertor_(MW)______________________________ (htpmw_div)___________________ 1.6906E+00 OP + Mechanical_pumping_power_for_shield_and_vacuum_vessel_(MW)______________ (htpmw_shld)__________________ 7.0688E-03 OP + # First wall and blanket : CCFE HCPB model # + Titanium_beryllide_fraction_____________________________________________ (fbltibe12)___________________ 3.7500E-01 + Lithium_orthosilicate_fraction__________________________________________ (fblli2sio4)__________________ 3.7500E-01 + Steel_fraction__________________________________________________________ (fblss_ccfe)__________________ 9.7050E-02 + Coolant_fraction________________________________________________________ (vfcblkt)_____________________ 5.2950E-02 + Purge_gas_fraction______________________________________________________ (vfpblkt)_____________________ 1.0000E-01 + First_Wall_Armour_Volume_(m3)___________________________________________ (fw_armour_vol)_______________ 5.8692E+00 + First_Wall_Volume_(m3)__________________________________________________ (volfw)_______________________ 1.9807E+01 + Blanket_Volume_(m3)_____________________________________________________ (volblkt)_____________________ 1.1849E+03 + Shield_Volume_(m3)______________________________________________________ (volshld)_____________________ 7.8520E+02 + Vacuum_vessel_volume_(m3)_______________________________________________ (vdewin)______________________ 1.0178E+03 + First_Wall_Armour_Mass_(kg)_____________________________________________ (fw_armour_mass)______________ 1.1298E+05 OP + First_Wall_Mass,_excluding_armour_(kg)__________________________________ (fwmass)______________________ 1.5449E+05 OP + Blanket_Mass_-_Total(kg)________________________________________________ (whtblkt)_____________________ 2.9676E+06 OP + ____Blanket_Mass_-_TiBe12_(kg)__________________________________________ (whtbltibe12)_________________ 1.0042E+06 OP + ____Blanket_Mass_-_Li4SiO4_(kg)_________________________________________ (whtblli4sio4)________________ 1.0664E+06 OP + ____Blanket_Mass_-_Steel_(kg)___________________________________________ (whtblss)_____________________ 8.9696E+05 OP + Total_mass_of_armour,_first_wall_and_blanket_(kg)_______________________ (armour_fw_bl_mass)___________ 3.2350E+06 OP + Shield_Mass_(kg)________________________________________________________ (whtshld)_____________________ 2.4498E+06 OP + Vacuum_vessel_mass_(kg)_________________________________________________ (vvmass)______________________ 7.9388E+06 OP + Total_nuclear_heating_in_TF+PF_coils_(CS_is_negligible)_(MW)____________ (ptfnuc)______________________ 2.5118E-02 OP + Total_nuclear_heating_in_FW_(MW)________________________________________ (pnucfw)______________________ 1.6315E+02 OP + Total_nuclear_heating_in_the_blanket_(including_emult)_(MW)_____________ (pnucblkt)____________________ 1.2901E+03 OP + Total_nuclear_heating_in_the_shield_(MW)________________________________ (pnucshld)____________________ 1.4138E+00 OP + Total_nuclear_heating_in_the_divertor_(MW)______________________________ (pnucdiv)_____________________ 1.4906E+02 OP + Blanket_exponential_factor______________________________________________ (exp_blanket)_________________ 9.9936E-01 OP + Shield:_first_exponential_______________________________________________ (exp_shield1)_________________ 1.9523E-03 OP + Shield:_second_exponential______________________________________________ (exp_shield2)_________________ 2.5427E-01 OP + Solid_angle_fraction_taken_by_on_divertor_______________________________ (fdiv)________________________ 1.1500E-01 + Switch_for_plant_secondary_cycle________________________________________ (secondary_cycle)_____________ 2 + First_wall_coolant_pressure_(Pa)________________________________________ (fwpressure)__________________ 1.5500E+07 + Blanket_coolant_pressure_(Pa)___________________________________________ (blpressure)__________________ 1.5500E+07 + Allowable_nominal_neutron_fluence_at_first_wall_(MW.year/m2)____________ (abktflnc)____________________ 5.0000E+00 + No_of_inboard_blanket_modules_poloidally________________________________ (nblktmodpi)__________________ 7 + No_of_inboard_blanket_modules_toroidally________________________________ (nblktmodti)__________________ 32 + No_of_outboard_blanket_modules_poloidally_______________________________ (nblktmodpo)__________________ 8 + No_of_outboard_blanket_modules_toroidally_______________________________ (nblktmodto)__________________ 48 + Isentropic_efficiency_of_first_wall_/_blanket_coolant_pumps_____________ (etaiso)______________________ 9.0000E-01 + First_wall_area_(m2)____________________________________________________ (fwarea)______________________ 1.6044E+03 OP + Cryostat_internal_radius_(m)____________________________________________ (rdewex)______________________ 1.7798E+01 OP + Cryostat_internal_half-height_(m)_______________________________________ (zdewex)______________________ 1.5339E+01 OP + Vertical_clearance_from_TF_coil_to_cryostat_(m)_________________________ (clh1)________________________ 5.6044E+00 OP + Divertor_area_(m2)______________________________________________________ (divsur)______________________ 1.4879E+02 OP + Divertor_mass_(kg)______________________________________________________ (divmas)______________________ 3.6453E+04 OP + # Superconducting TF Coil Power Conversion # + TF_coil_current_(kA)____________________________________________________ (itfka)_______________________ 8.9795E+01 OP + Number_of_TF_coils______________________________________________________ (ntfc)________________________ 1.6000E+01 + Voltage_across_a_TF_coil_during_quench_(kV)_____________________________ (vtfskv)______________________ 9.1862E+00 OP + TF_coil_charge_time_(hours)_____________________________________________ (tchghr)______________________ 4.0000E+00 + Total_inductance_of_TF_coils_(H)________________________________________ (ltfth)_______________________ 3.0165E+01 OP + Total_resistance_of_TF_coils_(ohm)______________________________________ (rcoils)______________________ 0.0000E+00 OP + TF_coil_charging_voltage_(V)____________________________________________ (tfcv)________________________ 2.9268E+02 + Number_of_DC_circuit_breakers___________________________________________ (ntfbkr)______________________ 1.6000E+01 + Number_of_dump_resistors________________________________________________ (ndumpr)______________________ 6.4000E+01 + Resistance_per_dump_resistor_(ohm)______________________________________ (r1dump)______________________ 1.0230E-01 OP + Dump_resistor_peak_power_(MW)___________________________________________ (r1ppmw)______________________ 2.0622E+02 OP + Energy_supplied_per_dump_resistor_(MJ)__________________________________ (r1emj)_______________________ 1.9002E+03 OP + TF_coil_L/R_time_constant_(s)___________________________________________ (ttfsec)______________________ 1.8429E+01 OP + Power_supply_voltage_(V)________________________________________________ (tfpsv)_______________________ 3.0731E+02 OP + Power_supply_current_(kA)_______________________________________________ (tfpska)______________________ 9.4285E+01 OP + DC_power_supply_rating_(kW)_____________________________________________ (tfckw)_______________________ 2.8975E+04 OP + AC_power_for_charging_(kW)______________________________________________ (tfackw)______________________ 3.2194E+04 OP + TF_coil_resistive_power_(MW)____________________________________________ (rpower)______________________ 9.3902E+00 OP + TF_coil_inductive_power_(MVA)___________________________________________ (xpower)______________________ 1.6891E+01 OP + Aluminium_bus_current_density_(kA/cm2)__________________________________ (djmka)_______________________ 1.2500E-01 + Aluminium_bus_cross-sectional_area_(cm2)________________________________ (albusa)______________________ 7.1836E+02 OP + Total_length_of_TF_coil_bussing_(m)_____________________________________ (tfbusl)______________________ 3.1931E+03 OP + Aluminium_bus_weight_(tonnes)___________________________________________ (albuswt)_____________________ 6.1932E+02 OP + Total_TF_coil_bus_resistance_(ohm)______________________________________ (rtfbus)______________________ 1.1646E-03 OP + TF_coil_bus_voltage_drop_(V)____________________________________________ (vtfbus)______________________ 1.0457E+02 OP + Dump_resistor_floor_area_(m2)___________________________________________ (drarea)______________________ 4.9234E+03 OP + TF_coil_power_conversion_floor_space_(m2)_______________________________ (tfcfsp)______________________ 1.8228E+03 OP + TF_coil_power_conv._building_volume_(m3)________________________________ (tfcbv)_______________________ 1.0937E+04 OP + TF_coil_AC_inductive_power_demand_(MW)__________________________________ (xpwrmw)______________________ 1.8768E+01 OP + Total_steady_state_AC_power_demand_(MW)_________________________________ (tfacpd)______________________ 1.0434E+01 OP + # PF Coils and Central Solenoid: Power and Energy # + Number_of_PF_coil_circuits______________________________________________ (pfckts)______________________ 1.2000E+01 + Sum_of_PF_power_supply_ratings_(MVA)____________________________________ (spsmva)______________________ 3.0313E+02 OP + Total_PF_coil_circuit_bus_length_(m)____________________________________ (spfbusl)_____________________ 2.4480E+03 OP + Total_PF_coil_bus_resistive_power_(kW)__________________________________ (pfbuspwr)____________________ 9.6485E+02 OP + Total_PF_coil_resistive_power_(kW)______________________________________ (srcktpm)_____________________ 9.6485E+02 OP + Maximum_PF_coil_voltage_(kV)____________________________________________ (vpfskv)______________________ 2.0000E+01 + Efficiency_of_transfer_of_PF_stored_energy_into_or_out_of_storage_______ (etapsu)______________________ 9.0000E-01 + Maximum_stored_energy_in_poloidal_field_(MJ)____________________________ (ensxpfm)_____________________ 2.8804E+04 OP + Peak_absolute_rate_of_change_of_stored_energy_in_poloidal_field_(MW)____ (peakpoloidalpower)___________ 1.7319E+02 OP + # Vacuum System # + First_wall_outgassing_rate_(Pa_m/s)_____________________________________ (rat)_________________________ 1.3000E-08 + Total_outgassing_load_(Pa_m3/s)_________________________________________ (ogas)________________________ 1.6691E-04 OP + Base_pressure_required_(Pa)_____________________________________________ (pbase)_______________________ 5.0000E-04 + Required_N2_pump_speed_(m3/s)___________________________________________ (s(1))________________________ 3.3381E-01 OP + N2_pump_speed_provided_(m3/s)___________________________________________ (snet(1))_____________________ 2.3404E+01 OP + Plasma_chamber_volume_(m3)______________________________________________ (volume)______________________ 2.2588E+03 OP + Chamber_pressure_after_burn_(Pa)________________________________________ (pend)________________________ 1.6698E-01 OP + Chamber_pressure_before_burn_(Pa)_______________________________________ (pstart)______________________ 1.6698E-03 + Allowable_pumping_time_switch___________________________________________ (dwell_pump)__________________ 0 + Dwell_time_between_burns_(s)____________________________________________ (tdwell.)_____________________ 1.8000E+03 + CS_ramp-up_time_burns_(s)_______________________________________________ (tramp.)______________________ 5.0000E+02 + Allowable_pumping_time_between_burns_(s)________________________________ (tpump)_______________________ 1.8000E+03 + Required_D-T_pump_speed_(m3/s)__________________________________________ (s(2))________________________ 5.7790E+00 OP + D-T_pump_speed_provided_(m3/s)__________________________________________ (snet(2))_____________________ 5.6700E+01 OP + Divertor_chamber_gas_pressure_(Pa)______________________________________ (prdiv)_______________________ 3.6000E-01 + Helium_gas_fraction_in_divertor_chamber_________________________________ (fhe)_________________________ 1.7218E-01 OP + Required_helium_pump_speed_(m3/s)_______________________________________ (s(3))________________________ 3.8423E+01 OP + Helium_pump_speed_provided_(m3/s)_______________________________________ (snet(3))_____________________ 3.8423E+01 OP + D-T_fuelling_rate_(kg/s)________________________________________________ (frate)_______________________ 2.7747E-05 OP + Required_D-T_pump_speed_(m3/s)__________________________________________ (s(4))________________________ 3.8423E+01 OP + D-T_pump_speed_provided_(m3/s)__________________________________________ (snet(4))_____________________ 5.6700E+01 OP + Number_of_large_pump_ducts______________________________________________ (nduct)_______________________ 16 + Passage_diameter,_divertor_to_ducts_(m)_________________________________ (d(imax))_____________________ 4.7857E-01 OP + Passage_length_(m)______________________________________________________ (l1)__________________________ 1.7160E+00 OP + Diameter_of_ducts_(m)___________________________________________________ (dout)________________________ 5.7428E-01 OP + Duct_length,_divertor_to_elbow_(m)______________________________________ (l2)__________________________ 4.8000E+00 OP + Duct_length,_elbow_to_pumps_(m)_________________________________________ (l3)__________________________ 2.0000E+00 + Number_of_pumps_________________________________________________________ (pumpn)_______________________ 3.2000E+01 OP + # Plant Buildings System # + Internal_volume_of_reactor_building_(m3)________________________________ (vrci)________________________ 9.9708E+05 + Dist_from_centre_of_torus_to_bldg_wall_(m)______________________________ (wrbi)________________________ 3.9531E+01 + Effective_floor_area_(m2)_______________________________________________ (efloor)______________________ 3.3660E+05 + Reactor_building_volume_(m3)____________________________________________ (rbv)_________________________ 1.1310E+06 + Reactor_maintenance_building_volume_(m3)________________________________ (rmbv)________________________ 3.9641E+05 + Warmshop_volume_(m3)____________________________________________________ (wsv)_________________________ 1.2531E+05 + Tritium_building_volume_(m3)____________________________________________ (triv)________________________ 4.0000E+04 + Electrical_building_volume_(m3)_________________________________________ (elev)________________________ 5.1937E+04 + Control_building_volume_(m3)____________________________________________ (conv)________________________ 6.0000E+04 + Cryogenics_building_volume_(m3)_________________________________________ (cryv)________________________ 1.4976E+04 + Administration_building_volume_(m3)_____________________________________ (admv)________________________ 1.0000E+05 + Shops_volume_(m3)_______________________________________________________ (shov)________________________ 1.0000E+05 + Total_volume_of_nuclear_buildings_(m3)__________________________________ (volnucb)_____________________ 1.5738E+06 + # Electric Power Requirements # + Facility_base_load_(MW)_________________________________________________ (basemw)______________________ 5.0000E+00 + Divertor_coil_power_supplies_(MW)_______________________________________ (bdvmw)_______________________ 0.0000E+00 + Cryoplant_electric_power_(MW)___________________________________________ (crymw)_______________________ 3.6566E+01 OP + Primary_coolant_pumps_(MW)______________________________________________ (htpmw..)_____________________ 1.9053E+02 OP + PF_coil_power_supplies_(MW)_____________________________________________ (ppfmw)_______________________ 8.5511E+01 OP + TF_coil_power_supplies_(MW)_____________________________________________ (ptfmw)_______________________ 1.0434E+01 OP + Plasma_heating_supplies_(MW)____________________________________________ (pheatingmw)__________________ 1.6029E+02 OP + Tritium_processing_(MW)_________________________________________________ (trithtmw..)__________________ 1.5000E+01 + Vacuum_pumps__(MW)______________________________________________________ (vachtmw..)___________________ 5.0000E-01 + Total_pulsed_power_(MW)_________________________________________________ (pacpmw)______________________ 5.5432E+02 OP + Total_base_power_required_at_all_times_(MW)_____________________________ (fcsht)_______________________ 5.5490E+01 OP + # Cryogenics # + Conduction_and_radiation_heat_loads_on_cryogenic_components_(MW)________ (qss/1.0d6)___________________ 1.4779E-02 OP + Nuclear_heating_of_cryogenic_components_(MW)____________________________ (qnuc/1.0d6)__________________ 1.3000E-02 OP + AC_losses_in_cryogenic_components_(MW)__________________________________ (qac/1.0d6)___________________ 3.8170E-03 OP + Resistive_losses_in_current_leads_(MW)__________________________________ (qcl/1.0d6)___________________ 1.9539E-02 OP + 45%_allowance_for_heat_loads_in_transfer_lines,_storage_tanks_etc_(MW)__ (qmisc/1.0d6)_________________ 2.3011E-02 OP + Sum_=_Total_heat_removal_at_cryogenic_temperatures_(tfcoil_variables.tmp (helpow_+_helpow_cryal/1.0d6)_ 7.4146E-02 OP + Temperature_of_cryogenic_superconducting_components_(K)_________________ (tmpcry)______________________ 4.5000E+00 + Temperature_of_cryogenic_aluminium_components_(K)_______________________ (tcoolin)_____________________ 3.1315E+02 + Efficiency_(figure_of_merit)_of_cryogenic_plant_is_13%_of_ideal_Carnot_v ______________________________ 2.0277E-03 OP + Efficiency_(figure_of_merit)_of_cryogenic_aluminium_plant_is_40%_of_idea ______________________________ -2.0203E+00 OP + Electric_power_for_cryogenic_plant_(MW)_________________________________ (crypmw)______________________ 3.6566E+01 OP + # Plant Power / Heat Transport Balance # + Neutron_power_multiplication_in_blanket_________________________________ (emult)_______________________ 1.2690E+00 + Divertor_area_fraction_of_whole_toroid_surface__________________________ (fdiv)________________________ 1.1500E-01 + H/CD_apparatus_+_diagnostics_area_fraction______________________________ (fhcd)________________________ 0.0000E+00 + First_wall_area_fraction________________________________________________ (1-fdiv-fhcd)_________________ 8.8500E-01 + Switch_for_pumping_of_primary_coolant___________________________________ (primary_pumping)_____________ 3 + Mechanical_pumping_power_for_FW_cooling_loop_including_heat_exchanger_(M (htpmw_fw)____________________ 0.0000E+00 OP + Mechanical_pumping_power_for_blanket_cooling_loop_including_heat_exchang (htpmw_blkt)__________________ 0.0000E+00 OP + Mechanical_pumping_power_for_FW_and_blanket_cooling_loop_including_heat_ (htpmw_fw_blkt)_______________ 1.6407E+02 OP + Mechanical_pumping_power_for_divertor_(MW)______________________________ (htpmw_div)___________________ 1.6906E+00 OP + Mechanical_pumping_power_for_shield_and_vacuum_vessel_(MW)______________ (htpmw_shld)__________________ 7.0688E-03 OP + Electrical_pumping_power_for_FW_and_blanket_(MW)________________________ (htpmwe_fw_blkt)______________ 1.8858E+02 OP + Electrical_pumping_power_for_shield_(MW)________________________________ (htpmwe_shld)_________________ 8.1250E-03 OP + Electrical_pumping_power_for_divertor_(MW)______________________________ (htpmwe_div)__________________ 1.9433E+00 OP + Total_electrical_pumping_power_for_primary_coolant_(MW)_________________ (htpmw)_______________________ 1.9053E+02 OP + Coolant_pump_power_/_non-pumping_thermal_power_in_shield________________ (fpumpshld)___________________ 5.0000E-03 + Coolant_pump_power_/_non-pumping_thermal_power_in_divertor______________ (fpumpdiv)____________________ 5.0000E-03 + Electrical_efficiency_of_heat_transport_coolant_pumps___________________ (etahtp)______________________ 8.7000E-01 + Thermal_to_electric_conversion_efficiency_of_the_power_conversion_cycle_ (etath)_______________________ 4.0000E-01 + Fraction_of_total_high-grade_thermal_power_to_divertor__________________ (pdivfraction)________________ 1.5623E-01 + Total_power_leaving_reactor_(across_vacuum_vessel_boundary)_(MW)________ ______________________________ 2.0111E+03 + Heat_removal_from_cryogenic_plant_(MW)__________________________________ (crypmw)______________________ 3.6566E+01 + Heat_removal_from_facilities_(MW)_______________________________________ (fachtmw)_____________________ 5.5490E+01 + Coolant_pumping_efficiency_losses_(MW)__________________________________ (htpsecmw)____________________ 2.4769E+01 + Heat_removal_from_injection_power_(MW)__________________________________ (pinjht)______________________ 8.0143E+01 + Heat_removal_from_tritium_plant_(MW)____________________________________ (trithtmw)____________________ 1.5000E+01 + Heat_removal_from_vacuum_pumps_(MW)_____________________________________ (vachtmw)_____________________ 5.0000E-01 + TF_coil_resistive_power_(MW)____________________________________________ (tfcmw)_______________________ 0.0000E+00 + Total_low-grade_thermal_power_(MW)______________________________________ (psechtmw)____________________ 2.2417E+02 + Total_High-grade_thermal_power_(MW)_____________________________________ (pthermmw)____________________ 2.1751E+03 + Number_of_primary_heat_exchangers_______________________________________ (nphx)________________________ 3 OP + Transport_power_from_scaling_law_(MW)___________________________________ (pscalingmw)__________________ 2.9785E+02 + Radiation_power_from_inside_"coreradius"_(MW)___________________________ (pcoreradmw.)_________________ 9.1650E+01 + Total_(MW)______________________________________________________________ ______________________________ 3.8950E+02 + Alpha_power_deposited_in_plasma_(MW)____________________________________ (falpha*palpmw)_______________ 3.0746E+02 + Power_from_charged_products_of_DD_and/or_D-He3_fusion_(MW)______________ (pchargemw.)__________________ 1.2659E+00 + Ohmic_heating_(MW)______________________________________________________ (pohmmw.)_____________________ 6.2284E-01 + Injected_power_deposited_in_plasma_(MW)_________________________________ (pinjmw)______________________ 8.0143E+01 + Total_(MW)______________________________________________________________ ______________________________ 3.8950E+02 + Fusion_power_(MW)_______________________________________________________ (powfmw)______________________ 1.6202E+03 + Power_from_energy_multiplication_in_blanket_and_shield_(MW)_____________ (emultmw)_____________________ 3.0836E+02 + Injected_power_(MW)_____________________________________________________ (pinjmw.)_____________________ 8.0143E+01 + Ohmic_power_(MW)________________________________________________________ (pohmmw.)_____________________ 6.2284E-01 + Power_deposited_in_primary_coolant_by_pump_(MW)_________________________ (htpmw_mech)__________________ 1.6576E+02 + Total_(MW)______________________________________________________________ ______________________________ 2.1751E+03 + Heat_extracted_from_first_wall_and_blanket_(MW)_________________________ (pthermfw_blkt)_______________ 1.8339E+03 + Heat_extracted_from_shield__(MW)________________________________________ (pthermshld)__________________ 1.4208E+00 + Heat_extracted_from_divertor_(MW)_______________________________________ (pthermdiv)___________________ 3.3982E+02 + Nuclear_and_photon_power_lost_to_H/CD_system_(MW)_______________________ (psechcd)_____________________ 0.0000E+00 + Nuclear_power_lost_to_TF_(MW)___________________________________________ (ptfnuc)______________________ 2.5118E-02 + Total_(MW)______________________________________________________________ ______________________________ 2.1752E+03 + Net_electric_power_output(MW)___________________________________________ (pnetelmw.)___________________ 4.0001E+02 + Required_Net_electric_power_output(MW)__________________________________ (pnetelin)____________________ 4.0000E+02 + Electric_power_for_heating_and_current_drive_(MW)_______________________ (pinjwp)______________________ 1.6029E+02 + Electric_power_for_primary_coolant_pumps_(MW)___________________________ (htpmw)_______________________ 1.9053E+02 + Electric_power_for_vacuum_pumps_(MW)____________________________________ (vachtmw)_____________________ 5.0000E-01 + Electric_power_for_tritium_plant_(MW)___________________________________ (trithtmw)____________________ 1.5000E+01 + Electric_power_for_cryoplant_(MW)_______________________________________ (crypmw)______________________ 3.6566E+01 + Electric_power_for_TF_coils_(MW)________________________________________ (tfacpd)______________________ 1.0434E+01 + Electric_power_for_PF_coils_(MW)________________________________________ (pfwpmw)______________________ 1.2422E+00 + All_other_internal_electric_power_requirements_(MW)_____________________ (fachtmw)_____________________ 5.5490E+01 + Total_(MW)______________________________________________________________ (tot_plant_power)_____________ 8.7006E+02 + Total_(MW)______________________________________________________________ ______________________________ 8.7006E+02 + Gross_electrical_output*_(MW)___________________________________________ (pgrossmw)____________________ 8.7006E+02 + Fusion_power_(MW)_______________________________________________________ (powfmw)______________________ 1.6202E+03 + Power_from_energy_multiplication_in_blanket_and_shield_(MW)_____________ (emultmw)_____________________ 3.0836E+02 + Total_(MW)______________________________________________________________ ______________________________ 1.9285E+03 + Net_electrical_output_(MW) _____________________________________________ (pnetelmw)____________________ 4.0001E+02 + Heat_rejected_by_main_power_conversion_circuit_(MW)_____________________ (rejected_main)_______________ 1.3051E+03 + Heat_rejected_by_other_cooling_circuits_(MW)____________________________ (psechtmw)____________________ 2.2417E+02 + Total_(MW)______________________________________________________________ ______________________________ 1.9293E+03 + Net_electric_power_/_total_nuclear_power_(%)____________________________ (pnetelmw/(powfmw+emultmw)____ 2.0741E+01 + Net_electric_power_/_total_fusion_power_(%)_____________________________ (pnetelmw/powfmw)_____________ 2.4689E+01 + Gross_electric_power*_/_high_grade_heat_(%)_____________________________ (etath)_______________________ 4.0000E+01 + Recirculating_power_fraction____________________________________________ (cirpowfr)____________________ 5.4025E-01 + # Water usage during plant operation (secondary cooling) # + Volume_used_in_cooling_tower_(m3/day)___________________________________ (waterusetower)_______________ 5.5485E+04 OP + Volume_used_in_recirculating_water_system_(m3/day)______________________ (wateruserecirc)______________ 1.8617E+04 OP + Volume_used_in_once-through_water_system_(m3/day)_______________________ (wateruseonethru)_____________ 1.8244E+06 OP + # Errors and Warnings # + # Errors and Warnings # + PROCESS_error_status_flag_______________________________________________ (error_status)________________ 2 + Final_error_identifier__________________________________________________ (error_id)____________________ 244 + # End of PROCESS Output # + # End of PROCESS Output # + # Copy of PROCESS Input Follows # +************************************************************************************************************************ +***** ***** +***** Generic large tokamak file ***** +***** James Morris, UKAEA ***** +***** 28/06/23 ***** +***** ***** +************************************************************************* + +* Run Information * +******************* + +runtitle = Generic large tokamak + +* Figure of merit - minimise major radius +minmax = 1 + +* Error tolerance for VMCON +epsvmc = 1e-7 + +* Constraint Equations - Consistency Equations * +************************************************ + +* Beta consistency * +*------------------* +icc = 1 +ixc = 5 * beta +beta = 0.03 + +* Global power balance * +*----------------------* +icc = 2 + +* Radial build consistency * +*--------------------------* +icc = 11 + +* Constraint Equations - Limit Equations * +****************************************** + +* Density upper limit * +*---------------------* +icc = 5 +ixc = 6 * dene [m-3] +fdene = 1.2 +dene = 7.5E19 + +* Neutron wall load upper limit * +*-------------------------------* +icc = 8 +ixc = 14 * fwalld +fwalld = 1.0 +* wall load limit [MW/m2] +walalw = 2.0 + +* Fusion power upper limit * +*--------------------------* + +icc = 9 +ixc = 26 * ffuspow +* Maximum allowable value fusion power [MW] +powfmax = 3000 + +* Burn time lower limit * +*-----------------------* +icc = 13 +ixc = 21 * ftburn +* minimum burn time [s] +tbrnmn = 7200.0 + +* L-H threshold scaling * +*-----------------------* +icc = 15 +ixc = 103 * flhthresh +boundu(103) = 10.0 + +* Injection power upper limit * +*-----------------------------* +icc = 30 +ixc = 46 * fpinj +* Maximum allowable value for injected power [MW] +pinjalw = 200.0 + +* Net electric power lower limit * +*--------------------------------* +icc = 16 +ixc = 25 * fpnetel +* Minimum allowable value for net eletric power [MW] +pnetelin = 400.0 + +* Beta upper limit * +*------------------* +icc = 24 +ixc = 36 * fbetatry +fbetatry = 0.5 + +* Max TF field * +*--------------* +icc = 25 +ixc = 35 * fpeakb +* Maximum allowable value for toroidal magnetic field [T] +bmxlim = 14.0 + +* Central solenoid EOF current density upper limit * +*--------------------------------------------------* +icc = 26 +ixc = 37 * coheof [A/m2] +ixc = 38 * fjohc +boundu(38) = 1.0 +coheof = 1.5E7 +fjohc = 0.6 + +* Central solenoid BOP current density upper limit * +*--------------------------------------------------* +icc = 27 +ixc = 39 * fjohc0 +ixc = 41 * fcohbop +boundu(39) = 1.0 +fjohc0 = 0.6 +fcohbop = 0.9 + +* I_op/I_Crit TF coil limit * +*---------------------------* +icc = 33 +ixc = 50 * fiooic +boundu(50) = 1.0 +fiooic = 0.65 + +* Dump voltage upper limit * +*--------------------------* +icc = 34 +ixc = 51 * fvdump +ixc = 52 * vdalw [kV] +boundu(52) = 10.0 +fvdump = 1.0 +vdalw = 10.0 + +* J_winding pack protection * +*---------------------------* +icc = 35 +ixc = 53 * fjprot +fjprot = 1.0 + +* TF temp marg lower limit * +*--------------------------* +icc = 36 +ixc = 54 * ftmargtf +* Minimum allowable temperature margin [K] +tmargmin = 1.5 + +* CS coil temp margin lower limit * +*---------------------------------* +icc = 60 +ixc = 106 * ftmargoh +tmargmin_cs = 1.5 + +* Lower limit on taup/taueff (ratio alpha particle/energy confinement times) * +*-------------------------------------------------------------------------------* +icc = 62 +ixc = 110 * ftaulimit +taulimit = 5.0 + +* dump time constraint for VV stresses * +*--------------------------------------* +icc = 65 +ixc = 113 * fmaxvvstress +fmaxvvstress = 1.0 + +* CS stress limit * +*-----------------* +icc = 72 +ixc = 123 * foh_stress +foh_stress = 1.0 +* allowable hoop stress in Central Solenoid structural material [Pa] +alstroh = 7.5D8 + +* neped List[RunMetadata]: + """Return runs metadata. + + :param temp_data: temporary dir containing data files + :type temp_data: Path + :return: list of solutions and their tags + :rtype: List[RunMetadata] + """ + run_metadata = [ + RunMetadata(temp_data / "large_tokamak_1_MFILE.DAT", "large tokamak 1"), + RunMetadata(temp_data / "large_tokamak_2_MFILE.DAT", "large tokamak 2"), + RunMetadata(temp_data / "large_tokamak_3_MFILE.DAT", "large tokamak 3"), + ] + + return run_metadata + + +def test_plot_mfile_solutions(run_metadata: Sequence[RunMetadata]): + """Plot three mfile solutions and their differences using RunMetadata objects. + + :param run_metadata: run_metadata for plotting + :type run_metadata: Sequence[RunMetadata] + """ + + _, results_df = plot_mfile_solutions( + runs_metadata=run_metadata, plot_title="3 large tokamak solutions" + ) + + # Check shape of solution df as evidence of plotting without error + assert results_df.shape == (3, 93)