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pytests/pytests/unittests/D+C/nonog_carbon/default/C_rates.strahl
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pytests/pytests/unittests/D+C/nonog_carbon/default/conftest.py
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import pytest | ||
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@pytest.fixture(autouse=True) | ||
def change_test_dir(request, monkeypatch): | ||
monkeypatch.chdir(request.fspath.dirname) |
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pytests/pytests/unittests/D+C/nonog_carbon/default/ehr2.dat
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pytests/pytests/unittests/D+C/nonog_carbon/default/gridue_8x4
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pytests/pytests/unittests/D+C/nonog_carbon/default/input.py
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# This is the test header file | ||
# It is copied into the start of every test case | ||
# created from this subdirectory. It is the | ||
# best place to include lines common to | ||
# all test cases, such as rate paths etc. | ||
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from uedge import * | ||
from uedge.hdf5 import hdf5_restore | ||
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try: | ||
bbb.oldseec = 0 | ||
bbb.jhswitch = 0 | ||
except: | ||
pass | ||
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bbb.mhdgeo = 1 #use MHD equilibrium | ||
bbb.gengrid=0 #read mesh from gridue file | ||
com.geometry = "snull" # Defines a LSN geometry for the problem | ||
bbb.GridFileName = "gridue_8x4" # Defines the gridue file name | ||
com.isnonog = 1 #nonorthogal differencing used | ||
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bbb.methn = 33 #ion continuty eqn | ||
bbb.methu = 33 #ion parallel momentum eqn | ||
bbb.methe = 33 #electron energy eqn | ||
bbb.methi = 33 #ion energy eqn | ||
bbb.methg = 66 #neutral gas continuity eqn | ||
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# templates/D+C/inputs/1_basecase/default.py | ||
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# Boundary conditions | ||
bbb.ncore[0] = 2.e19 #hydrogen ion density on core | ||
bbb.iflcore = 0 #flag; =0, fixed Te,i; =1, fixed power on core | ||
bbb.tcoree = 250. #core Te | ||
bbb.tcorei = 250. #core Ti | ||
bbb.tedge = 2. #fixed wall,pf Te,i if istewcon=1, etc | ||
bbb.recycp[0] = 0.95 #hydrogen recycling coeff at plates | ||
bbb.recycm = 0.1 | ||
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# Transport coefficients (m**2/s) | ||
bbb.difni[0] = 1. #D for radial hydrogen diffusion | ||
bbb.kye = 1. #chi_e for radial elec energy diffusion | ||
bbb.kyi = 1. #chi_i for radial ion energy diffusion | ||
bbb.travis[0] = 1. #eta_a for radial ion momentum diffusion | ||
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# Flux limits | ||
bbb.flalfe = 0.21 #electron parallel thermal conduct. coeff | ||
bbb.flalfi = 0.21 #ion parallel thermal conduct. coeff | ||
bbb.flalfv = 0.5 #ion parallel viscosity coeff | ||
bbb.flalfgx = 1. #neut. gas part. flux in poloidal direction | ||
bbb.flalfgy = 1. #neut. gas part. flux in radial direction | ||
bbb.flalfgxy = 1. #neut. gas part. flux in mixed derivatives | ||
bbb.flalftgx = 1. #neut. gas thermal flux, poloidal direction | ||
bbb.flalftgy = 1. #neut. gas thermal flux, radial direction | ||
bbb.lgmax = 0.1 #max scale length for flalfgx,y | ||
bbb.lgtmax = 0.1 #max scale length for flalftgx,y | ||
bbb.lgvmax = 0.1 #max scale length for flalfvgx,y | ||
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# Solver package | ||
bbb.svrpkg = "nksol" #Newton solver using Krylov method | ||
bbb.premeth = "ilut" #Solution method for precond. Jacobian matrix | ||
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# Parallel neutral momentum equation | ||
bbb.isupgon[0] = 1 | ||
bbb.ineudif = 2 #=2 for evolving pg=ng*tg variable | ||
bbb.isngon[0] = 0 | ||
com.ngsp = 1 | ||
com.nhsp = 2 | ||
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bbb.ziin[1] = 0 | ||
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# Atomic data switches | ||
com.istabon = 10 #=10 specifics hydrogen data file ehr2.dat | ||
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# templates/D+C/inputs/2_C/default.py | ||
# This part sets up carbon. | ||
# Should be split into smaller parts, each part tested | ||
## Impurity gas basics | ||
com.ngsp = 2 #total number of gas species | ||
bbb.isngon[1] = 1 #turns on impurity gas | ||
bbb.ngbackg[1] = 1.e9 #neutral impurity background for added source | ||
bbb.ingb = 2 #exponent for strength of ngbackg turn-on | ||
bbb.istgcon[1] = 1 #=1 for constant tg(2) at tgas(2) | ||
bbb.tgas[1] = 1. #value for tg when istgcon=1 | ||
bbb.rcxighg = 0. # best value; ratio of imp cx to hyd cx | ||
bbb.kelighi[1] = 5.e-16 #elastic sig_v for imp_gas/h_ion | ||
bbb.kelighg[1] = 5.e-16 #elastic sig_v for imp_gas/h_gas | ||
bbb.n0g[1] = 1.e16 #imp. gas density normalization | ||
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# Impurity gas boundary conditions | ||
bbb.recycp[1] = 0.01 #plate recycling of impurities | ||
bbb.recycw[1] = 1e-4 #wall recycling; matwsi,o set above for hyd | ||
bbb.isch_sput[1]=7 # Haasz/Davis chemical sputtering model | ||
bbb.isph_sput[1]=3 # physical sputtering model | ||
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# Reduce C isputtering owing to boronization | ||
bbb.fphysylb[1,0] = 0.5 | ||
bbb.fphysyrb[1,0] = 0.5 | ||
bbb.fchemylb[1,0] = 0.1 | ||
bbb.fchemyrb[1,0] = 0.1 | ||
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bbb.t_wall = 300. | ||
bbb.t_plat = 500. | ||
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## Impurity ions | ||
bbb.isimpon = 6 #Use force-balance only | ||
com.nzsp[0] = 6 #number chrg states impurity isotope #1 | ||
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bbb.csfaclb[2:8,0] = 2.191 | ||
bbb.csfacrb[2:8,0] = 2.191 | ||
bbb.minu[2:8] = 12. | ||
bbb.ziin[:2] = [1, 0] | ||
bbb.ziin[2:8] = list(range(1,7)) | ||
bbb.znuclin[:2] = 1 | ||
bbb.znuclin[2:8] = 6 | ||
bbb.n0[2:8] = 1.e17 | ||
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bbb.nzbackg = 1.e9 #background density for impurities | ||
bbb.inzb = 2 #exponent for switching on nzbackg | ||
bbb.ismctab = 2 # use Braams" rate tables | ||
com.mcfilename[0] = "C_rates.strahl" # Imp rate file name | ||
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bbb.isnicore[7] = 3 | ||
bbb.curcore[7] = 0. | ||
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bbb.isnwcono[2:8] = 3 | ||
bbb.isnwconi[2:8] = 3 | ||
bbb.nwomin[2:8] = 1.e7 | ||
bbb.nwimin[2:8] = 1.e7 | ||
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# Scale factor converting (upi-upg)**2 energy to thermal energy | ||
bbb.cfnidh = 0.2 | ||
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# templates/restore/default.py | ||
bbb.restart = 1 #Begin from savefile | ||
bbb.allocate() #allocate plasma/neutral arrays | ||
hdf5_restore("solution.h5") #read in the solution from pfb file |
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