rundke_epsi

Script for running the DKE solver (can be modified by the user for specific simulations)
by Y.Peysson CEA-DRFC <yves.peysson@cea.fr> and Joan Decker MIT-RLE (jodecker@mit.edu)

0001 %Script for running the DKE solver (can be modified by the user for specific simulations)
0002 %by Y.Peysson CEA-DRFC <yves.peysson@cea.fr> and Joan Decker MIT-RLE (jodecker@mit.edu)
0003 %
0004 clear all
0005 clear mex
0006 clear functions
0007 close all
0008 warning off
0009 global nfig
0010 %
0011 p_opt = 2;
0012 %
0013 permission = test_permissions_yp;
0014 %
0015 if ~permission 
0016     disp('Please move the script to a local folder where you have write permission before to run it')
0017     return;
0018 end
0019 %
0020 % ***********************This part must be specified by the user, run make files if necessary) *****************************
0021 %
0022 id_simul = 'Ohm_epsi';%Simulation ID
0023 path_simul = '';%if nothing is specified, the working directory is first used and then MatLab is looking in all the path
0024 %
0025 psin_S = [];%Normalized poloidal flux grid where calculations are performed (0 < psin_S < 1) (If one value: local calculation only, not used if empty)
0026 rho_S = [0.5];%Normalized radial flux grid where calculations are performed (0 < rho_S < 1) (If one value: local calculation only, not used if empty)
0027 %
0028 id_path = '';%For all paths used by DKE solver
0029 path_path = '';%if nothing is specified, the working directory is first used and then MatLab is looking in all the path
0030 %
0031 id_equil = 'TScyl';%For plasma equilibrium
0032 path_equil = '';%if nothing is specified, the working directory is first used and then MatLab is looking in all the path
0033 %
0034 id_dkeparam = 'UNIFORM10010020';%For DKE code parameters
0035 path_dkeparam = '';%if nothing is specified, the working directory is first used and then MatLab is looking in all the path
0036 %
0037 id_display = 'NO_DISPLAY';%For output code display
0038 path_display = '';%if nothing is specified, the working directory is first used and then MatLab is looking in all the path
0039 %
0040 id_ohm = '';%For Ohmic electric contribution
0041 path_ohm = '';%if nothing is specified, the working directory is first used and then MatLab is looking in all the path
0042 %
0043 ids_wave = {''};%For RF waves contribution (put all the type of waves needed)
0044 paths_wave = {''};%if nothing is specified, the working directory is first used and then MatLab is looking in all the path
0045 %
0046 id_transpfaste = '';%For fast electron radial transport
0047 path_transpfaste = '';%if nothing is specified, the working directory is first used and then MatLab is looking in all the path
0048 %
0049 id_ripple = '';%For fast electron magnetic ripple losses
0050 path_ripple = '';%if nothing is specified, the working directory is first used and then MatLab is looking in all the path
0051 %
0052 %************************************************************************************************************************************
0053 %************************************************************************************************************************************
0054 %************************************************************************************************************************************
0055 %
0056 [dkepath,equil,dkeparam,dkedisplay,ohm,waves,transpfaste,ripple] = load_structures_yp('dkepath',id_path,path_path,'equil',id_equil,path_equil,'dkeparam',id_dkeparam,path_dkeparam,'dkedisplay',id_display,path_display,'ohm',id_ohm,path_ohm,'waves',ids_wave,paths_wave,'transpfaste',id_transpfaste,path_transpfaste,'ripple',id_ripple,path_ripple);
0057 %
0058 %************************************************************************************************************************************
0059 %
0060 if exist('dmumpsmex');dkeparam.invproc = -2;end
0061 %
0062 dkeparam.boundary_mode_f = 0;%Number of points where the Maxwellian distribution is enforced from p = 0 (p=0, free conservative mode but param_inv(1) must be less than 1e-4, otherwise 1e-3 is OK most of the time. Sensitive to the number of points in p)
0063 dkeparam.tn = [1000:1000:10000];% coupled particle loss after 10000 tauc - warning : runaway contribution to sigma not accounted for
0064 %
0065 dkeparam.psin_S = psin_S;
0066 dkeparam.rho_S = rho_S;
0067 %
0068 betath = 0.01;%validated for NR limit
0069 %
0070 epsi_list = logspace(-5,-1,21);
0071 %
0072 [qe,me,mp,mn,e0,mu0,re,mc2] = pc_dke_yp;%Universal physics constants
0073 %
0074 equil.pTe = betath^2*mc2*ones(size(equil.pTe));
0075 equil.pzTi = betath^2*mc2*ones(size(equil.pzTi));
0076 %equil.pzTi = 1e-10*ones(size(equil.pzTi));
0077 %
0078 for iepsi = 1:length(epsi_list),
0079     %
0080     epsi = epsi_list(iepsi);
0081     %
0082     ohm = ohm_flat(equil,epsi);
0083     %
0084     dkeparam.coll_mode = 0;% Relativistic Maxwellian background
0085     [dummy,Zcurr] = main_dke_yp(id_simul,dkepath,equil,dkeparam,dkedisplay,ohm,waves,transpfaste,ripple,[],[]);
0086     sigma_0(iepsi) = Zcurr.x_0/epsi;
0087     %
0088     dkeparam.coll_mode = 1;% High-velocity limit
0089     [dummy,Zcurr] = main_dke_yp(id_simul,dkepath,equil,dkeparam,dkedisplay,ohm,waves,transpfaste,ripple,[],[]);
0090     sigma_1(iepsi) = Zcurr.x_0/epsi;
0091     %
0092     dkeparam.coll_mode = 2;% Linearized Belaiev-Budker
0093     [dummy,Zcurr,dummy,dke_out] = main_dke_yp(id_simul,dkepath,equil,dkeparam,dkedisplay,ohm,waves,transpfaste,ripple,[],[]);
0094     if dke_out.residu_f{end}(end) <= dkeparam.prec0_f,
0095         sigma_2(iepsi) = Zcurr.x_0/epsi;
0096         sigma_2_noconv(iepsi) = NaN;
0097     else
0098         sigma_2(iepsi) = NaN;
0099         sigma_2_noconv(iepsi) = Zcurr.x_0/epsi;
0100     end        
0101     %
0102 end
0103 %
0104 sigma_2_noconv(max(find(~isnan(sigma_2)))) = sigma_2(max(find(~isnan(sigma_2))));
0105 %
0106 sigma_Z1s = 1/100*sqrt(me*qe/10)/(1.65*mu0*e0^2);%Spitzer conductivity (from 'Tokamaks' by J. Wesson, Oxford Science Publication, 3rd Eds., 2004)
0107 %
0108 sigma_Karney_nr_0 = [3.773];
0109 sigma_Karney_nr_1 = [2.837];
0110 sigma_Karney_nr_2 = [7.429];
0111 %
0112 %************************************************************************************************************************************
0113 %
0114 figure(1),clf
0115 %
0116 leg = {'Linearized','High v limit','Maxwellian'};
0117 xlim = 10.^[-5,0];
0118 ylim = [0,10];
0119 xlab = 'E/E_D';
0120 ylab = '\sigma';
0121 tit = '';
0122 siz = 20+14i;
0123 %
0124 graph1D_jd(epsi_list,sigma_2,1,0,xlab,ylab,tit,NaN,xlim,ylim,'-','none','r',2,siz,gca,0.9,0.7,0.7);
0125 graph1D_jd(epsi_list,sigma_1,1,0,'','','',NaN,xlim,ylim,'-','none','b',2,siz,gca);
0126 graph1D_jd(epsi_list,sigma_0,1,0,'','','',leg,xlim,ylim,'-','none','g',2,siz,gca);
0127 graph1D_jd(epsi_list,sigma_2_noconv,1,0,'','','',NaN,xlim,ylim,'--','none','r',2,siz,gca);
0128 graph1D_jd(xlim,[sigma_Z1s,sigma_Z1s],1,0,'','','',NaN,xlim,ylim,'-','none','k',0.5,siz,gca);
0129 graph1D_jd(xlim,[sigma_Karney_nr_2,sigma_Karney_nr_2],0,0,'','','',NaN,xlim,ylim,'--','none','r',0.5,siz,gca);
0130 graph1D_jd(xlim,[sigma_Karney_nr_1,sigma_Karney_nr_1],0,0,'','','',NaN,xlim,ylim,'--','none','b',0.5,siz,gca);
0131 graph1D_jd(xlim,[sigma_Karney_nr_0,sigma_Karney_nr_0],0,0,'','','',NaN,xlim,ylim,'--','none','g',0.5,siz,gca);
0132 graph1D_jd([1,1]/dkeparam.pnmax_S^2,ylim,0,0,'','','',NaN,xlim,ylim,'--','none','k',2,siz,gca);
0133 %
0134 set(gca,'ytick',[0:2:10])
0135 set(gca,'xtick',[1e-06 1e-5 0.0001 0.001 0.01 0.1 1])
0136 %set(gca,'XTickLabel',{'10^{-5}','10^{-4}','10^{-3}','10^{-2}','10^{-1}','1'})
0137 set(gca,'XMinorGrid','off')
0138 set(gca,'XMinorTick','on')
0139 %
0140 print_jd(p_opt,'fig_sigma_epsi','./figures',1)
0141 %
0142 %************************************************************************************************************************************
0143 %
0144 eval(['save ',path_simul,'DKE_RESULTS_',id_equil,'_',id_simul,'.mat']);
0145 info_dke_yp(2,['Data saved in ',path_simul,'DKE_RESULTS_',id_equil,'_',id_simul,'.mat']);