diff --git a/wk/lin_run_script.m b/wk/lin_run_script.m
index 0eb275e6621f04545cda7df520fc2f4520732f0d..f549d7b8fed3daaf318e12b01da0b91b120db6ae 100644
--- a/wk/lin_run_script.m
+++ b/wk/lin_run_script.m
@@ -21,10 +21,22 @@ EXECNAME = 'gyacomo23_sp'; % single precision
% EXECNAME = 'gyacomo23_dp'; % double precision
%% Setup parameters
-% run lin_DTT_AB_rho85_PT
+% run lin_DTT_AB_rho85
+% run lin_DTT_AB_rho98
+run lin_JET_rho97
% run lin_Entropy
% run lin_ITG
-
+%% Change parameters
+NY = 2;
+PMAX = 4;
+JMAX = 2;
+ky = 10.0;
+LY = 2*pi/ky;
+DT = 1e-3/ky;
+SIGMA_E = 0.023;
+TMAX = 1.5/ky;
+DTSAVE0D = 0.01;
+DTSAVE3D = 0.01;
%%-------------------------------------------------------------------------
%% RUN
setup
@@ -32,9 +44,9 @@ setup
% Run linear simulation
if RUN
MVIN =['cd ../results/',SIMID,'/',PARAMS,'/;'];
-% RUN =['time ',mpirun,' -np 2 ',gyacomodir,'bin/',EXECNAME,' 1 2 1 0;'];
+ RUN =['time ',mpirun,' -np 2 ',gyacomodir,'bin/',EXECNAME,' 1 2 1 0;'];
% RUN =['time ',mpirun,' -np 4 ',gyacomodir,'bin/',EXECNAME,' 1 2 2 0;'];
- RUN =['time ',mpirun,' -np 8 ',gyacomodir,'bin/',EXECNAME,' 1 4 2 0;'];
+ % RUN =['time ',mpirun,' -np 8 ',gyacomodir,'bin/',EXECNAME,' 1 4 2 0;'];
% RUN =['time ',mpirun,' -np 1 ',gyacomodir,'bin/',EXECNAME,' 1 1 1 0;'];
% RUN = ['./../../../bin/gyacomo23_sp 0;'];
MVOUT='cd ../../../wk;';
@@ -53,7 +65,7 @@ data = {}; % Initialize data as an empty cell array
data = compile_results_low_mem(data,LOCALDIR,J0,J1);
-if 0 % Activate or not
+if 1 % Activate or not
%% plot mode evolution and growth rates
% Load phi
[data.PHI, data.Ts3D] = compile_results_3D(LOCALDIR,J0,J1,'phi');
@@ -70,7 +82,7 @@ options.fftz.flag = 0; % Set fftz.flag option to 0
fig = mode_growth_meter(data,options); % Call the function mode_growth_meter with data and options as input arguments, and store the result in fig
end
-if 1
+if (1 && NZ>4)
%% Ballooning plot
[data.PHI, data.Ts3D] = compile_results_3D(LOCALDIR,J0,J1,'phi');
if data.inputs.BETA > 0
diff --git a/wk/lin_scan_script.m b/wk/lin_scan_script.m
index a10d35fa9c82b68f585c143c1b5e0a19e643cd3b..a587fc23207dbe35794a5f3d5bc7092aa80b128d 100644
--- a/wk/lin_scan_script.m
+++ b/wk/lin_scan_script.m
@@ -16,7 +16,7 @@ addpath(genpath([gyacomodir,'wk/parameters'])) % Add parameters folder
%% Setup run or load an executable
RUN = 1; % To run or just to load
-RERUN = 0; % rerun if the data does not exist
+RERUN = 1; % rerun if the data does not exist
default_plots_options
EXECNAME = 'gyacomo23_sp'; % single precision
% EXECNAME = 'gyacomo23_dp'; % double precision
@@ -29,13 +29,13 @@ run lin_DTT_AB_rho85_PT
%% Modify parameters
% NZ = 1;
NY = 2;
-DT = 2e-3;
-
+DT = 0.5e-3;
+TMAX = 50;
+MU_X = 0.1; MU_Y = 0.1;
%% Scan parameters
SIMID = [SIMID,'_scan'];
-P_a = [2 4 8];
-ky_a= 0.1:0.1:0.5;
-
+P_a = [2 4 6 8];
+ky_a = 0.05:0.05:1.5;
%% Scan loop
% arrays for the result
g_ky = zeros(numel(ky_a),numel(P_a),2);
@@ -47,63 +47,63 @@ for PMAX = P_a
i = 1;
for ky = ky_a
LY = 2*pi/ky;
- %% RUN
- setup
- % naming
- filename = [SIMID,'/',PARAMS,'/'];
- LOCALDIR = [gyacomodir,'results/',filename,'/'];
- % check if data exist to run if no data
- data_ = {};
- try
- data_ = compile_results_low_mem(data_,LOCALDIR,00,00);
- Ntime = numel(data_.Ts0D);
- catch
- data_.outfilenames = [];
- end
- if RUN && (RERUN || isempty(data_.outfilenames) || Ntime < 10)
- % system(['cd ../results/',SIMID,'/',PARAMS,'/; mpirun -np 2 ',gyacomodir,'bin/',EXECNAME,' 1 2 1 0; cd ../../../wk'])
- system(['cd ../results/',SIMID,'/',PARAMS,'/; mpirun -np 4 ',gyacomodir,'bin/',EXECNAME,' 1 2 2 0; cd ../../../wk'])
- % system(['cd ../results/',SIMID,'/',PARAMS,'/; mpirun -np 6 ',gyacomodir,'bin/',EXECNAME,' 3 2 1 0; cd ../../../wk'])
- end
- data_ = compile_results_low_mem(data_,LOCALDIR,00,00);
- [data_.PHI, data_.Ts3D] = compile_results_3D(LOCALDIR,00,00,'phi');
- if numel(data_.Ts3D)>10
- if numel(data_.Ts3D)>5
- % Load results after trying to run
+ %% RUN
+ setup
+ % naming
filename = [SIMID,'/',PARAMS,'/'];
LOCALDIR = [gyacomodir,'results/',filename,'/'];
-
+ % check if data exist to run if no data
+ data_ = {};
+ try
+ data_ = compile_results_low_mem(data_,LOCALDIR,00,00);
+ Ntime = numel(data_.Ts0D);
+ catch
+ data_.outfilenames = [];
+ end
+ if RUN && (RERUN || isempty(data_.outfilenames) || Ntime < 10)
+ % system(['cd ../results/',SIMID,'/',PARAMS,'/; mpirun -np 2 ',gyacomodir,'bin/',EXECNAME,' 1 2 1 0; cd ../../../wk'])
+ system(['cd ../results/',SIMID,'/',PARAMS,'/; mpirun -np 4 ',gyacomodir,'bin/',EXECNAME,' 1 2 2 0; cd ../../../wk'])
+ % system(['cd ../results/',SIMID,'/',PARAMS,'/; mpirun -np 6 ',gyacomodir,'bin/',EXECNAME,' 3 2 1 0; cd ../../../wk'])
+ end
data_ = compile_results_low_mem(data_,LOCALDIR,00,00);
[data_.PHI, data_.Ts3D] = compile_results_3D(LOCALDIR,00,00,'phi');
-
- % linear growth rate (adapted for 2D zpinch and fluxtube)
- options.TRANGE = [0.5 1]*data_.Ts3D(end);
- options.NPLOTS = 0; % 1 for only growth rate and error, 2 for omega local evolution, 3 for plot according to z
- options.GOK = 0; %plot 0: gamma 1: gamma/k 2: gamma^2/k^3
-
- [~,it1] = min(abs(data_.Ts3D-0.5*data_.Ts3D(end))); % start of the measurement time window
- [~,it2] = min(abs(data_.Ts3D-1.0*data_.Ts3D(end))); % end of ...
- field = 0;
- field_t = 0;
- for ik = 2:NY/2+1
- field = squeeze(sum(abs(data_.PHI),3)); % take the sum over z
- field_t = squeeze(field(ik,1,:)); % take the kx =0, ky = ky mode only
- to_measure = log(field_t(it1:it2));
- tw = double(data_.Ts3D(it1:it2));
- % gr = polyfit(tw,to_measure,1);
- gr = fit(tw,to_measure,'poly1');
- err= confint(gr);
- g_ky(i,j,ik) = gr.p1;
- g_std(i,j,ik) = abs(err(2,1)-err(1,1))/2;
- end
- [gmax, ikmax] = max(g_ky(i,j,:));
-
- msg = sprintf('gmax = %2.2f, kmax = %2.2f',gmax,data_.grids.ky(ikmax)); disp(msg);
+ if numel(data_.Ts3D)>10
+ if numel(data_.Ts3D)>5
+ % Load results after trying to run
+ filename = [SIMID,'/',PARAMS,'/'];
+ LOCALDIR = [gyacomodir,'results/',filename,'/'];
+
+ data_ = compile_results_low_mem(data_,LOCALDIR,00,00);
+ [data_.PHI, data_.Ts3D] = compile_results_3D(LOCALDIR,00,00,'phi');
+
+ % linear growth rate (adapted for 2D zpinch and fluxtube)
+ options.TRANGE = [0.5 1]*data_.Ts3D(end);
+ options.NPLOTS = 0; % 1 for only growth rate and error, 2 for omega local evolution, 3 for plot according to z
+ options.GOK = 0; %plot 0: gamma 1: gamma/k 2: gamma^2/k^3
+
+ [~,it1] = min(abs(data_.Ts3D-0.5*data_.Ts3D(end))); % start of the measurement time window
+ [~,it2] = min(abs(data_.Ts3D-1.0*data_.Ts3D(end))); % end of ...
+ field = 0;
+ field_t = 0;
+ for ik = 2:NY/2+1
+ field = squeeze(sum(abs(data_.PHI),3)); % take the sum over z
+ field_t = squeeze(field(ik,1,:)); % take the kx =0, ky = ky mode only
+ to_measure = log(field_t(it1:it2));
+ tw = double(data_.Ts3D(it1:it2));
+ % gr = polyfit(tw,to_measure,1);
+ gr = fit(tw,to_measure,'poly1');
+ err= confint(gr);
+ g_ky(i,j,ik) = gr.p1;
+ g_std(i,j,ik) = abs(err(2,1)-err(1,1))/2;
+ end
+ [gmax, ikmax] = max(g_ky(i,j,:));
+
+ msg = sprintf('gmax = %2.2f, kmax = %2.2f',gmax,data_.grids.ky(ikmax)); disp(msg);
+ end
end
+ i = i + 1;
end
- i = i + 1;
-end
-j = j + 1;
+ j = j + 1;
end
%% take max growth rate among z coordinate
@@ -114,8 +114,11 @@ e_ = g_std(:,:,2);
if(numel(ky_a)>1 && numel(P_a)>1)
pmin = num2str(min(P_a)); pmax = num2str(max(P_a));
kymin = num2str(min(ky_a)); kymax= num2str(max(ky_a));
- filename = [num2str(NX),'x',num2str(NZ),'_ky_',kymin,'_',kymax,...
- '_P_',pmin,'_',pmax,'_',CONAME,'_',num2str(NU),'_be_',num2str(BETA),'.mat'];
+ filename = [num2str(NX),'x',num2str(NZ),...
+ '_ky_',kymin,'_',kymax,...
+ '_P_',pmin,'_',pmax,...
+ '_kN_',num2str(K_Ni),...
+ '_',CONAME,'_',num2str(NU),'_be_',num2str(BETA),'.mat'];
metadata.name = filename;
metadata.kymin = ky;
metadata.title = ['$\nu_{',CONAME,'}=$',num2str(NU),'$\kappa_T=$',num2str(K_Ti),', $\kappa_N=$',num2str(K_Ni)];
diff --git a/wk/parameters/lin_DTT_AB_rho85_PT.m b/wk/parameters/lin_DTT_AB_rho85.m
similarity index 92%
rename from wk/parameters/lin_DTT_AB_rho85_PT.m
rename to wk/parameters/lin_DTT_AB_rho85.m
index f950920ec2285b2acbbd676c255369a752a94028..dfdf7fa1bace13a36b1e225ef8f5a0375ba59252 100644
--- a/wk/parameters/lin_DTT_AB_rho85_PT.m
+++ b/wk/parameters/lin_DTT_AB_rho85.m
@@ -14,8 +14,8 @@ dpdx_gn =0.086;
SIMID = 'lin_DTT_AB_rho85_PT'; % Name of the simulation
%% Set up physical parameters
CLUSTER.TIME = '99:00:00'; % Allocation time hh:mm:ss
-nu = nu_ei; %(0.00235 in GENE)
-TAU = 0.9360; % e/i temperature ratio
+NU = 0.1; %(0.00235 or 0.56 in GENE?)
+TAU = 0.9360; % e/i temperature ratio
K_Ne = 1.33; % ele Density '''
K_Te = 12.0; % ele Temperature '''
K_Ni = 1.33; % ion Density gradient drive
@@ -26,12 +26,11 @@ ADIAB_E = (NA==1); % adiabatic electron model
BETA = b_gn; % electron plasma beta
MHD_PD = 0;
%% Set up grid parameters
-P = 4;
-J = P/2;%P/2;
-PMAX = P; % Hermite basis size
-JMAX = J; % Laguerre basis size
-NX = 16; % real space x-gridpoints
-NY = 16; % real space y-gridpoints
+
+PMAX = 4; % Hermite basis size
+JMAX = PMAX/2; % Laguerre basis size
+NX = 4; % real space x-gridpoints
+NY = 24; % real space y-gridpoints
LX = 2*pi/0.1; % Size of the squared frequency domain in x direction
LY = 2*pi/0.2; % Size of the squared frequency domain in y direction
NZ = 24; % number of perpendicular planes (parallel grid)
@@ -55,7 +54,7 @@ SHIFT_Y = 0.0; % Shift in the periodic BC in z
NPOL = 1; % Number of poloidal turns
PB_PHASE = 0;
%% TIME PARAMETERS
-TMAX = 15; % Maximal time unit
+TMAX = 25; % Maximal time unit
DT = 1e-3; % Time step
DTSAVE0D = 0.5; % Sampling time for 0D arrays
DTSAVE2D = -1; % Sampling time for 2D arrays
diff --git a/wk/parameters/lin_DTT_AB_rho98_PT.m b/wk/parameters/lin_DTT_AB_rho98.m
similarity index 91%
rename from wk/parameters/lin_DTT_AB_rho98_PT.m
rename to wk/parameters/lin_DTT_AB_rho98.m
index 55352cd11ae29c5743ed4c35b455bc215998412b..12c49a63686d0bd9a563732f8917fae00b93b94c 100644
--- a/wk/parameters/lin_DTT_AB_rho98_PT.m
+++ b/wk/parameters/lin_DTT_AB_rho98.m
@@ -7,11 +7,11 @@ mref = 2.0; % in proton mass
lnLAMBDA = 13; % Coulomb logarithm
nuref = 0.45*2.3031e-5*lnLAMBDA*nref*Lref/Tref/Tref; %(0.00235 in GENE)
nu_ei = 0.569013;
-nu_gn = 0.00235;
+nu_gn = 0.235;
b_gn = 0.0039;
dpdx_gn =0.086;
%% Set simulation parameters
-SIMID = 'lin_DTT_AB_rho85_PT'; % Name of the simulation
+SIMID = 'lin_DTT_AB_rho98_PT'; % Name of the simulation
%% Set up physical parameters
CLUSTER.TIME = '99:00:00'; % Allocation time hh:mm:ss
nu = nu_ei; %(0.00235 in GENE)
@@ -20,7 +20,7 @@ K_Ne = 65; % ele Density '''
K_Te = 350; % ele Temperature '''
K_Ni = K_Ne; % ion Density gradient drive
K_Ti = 350; % ion Temperature '''
-SIGMA_E = 0.0233380/sqrt(mref); % mass ratio sqrt(m_a/m_i) (correct = 0.0233380)
+SIGMA_E = 0.0233380; % mass ratio sqrt(m_a/m_i) (correct = 0.0233380)
NA = 2; % number of kinetic species
ADIAB_E = (NA==1); % adiabatic electron model
BETA = b_gn; % electron plasma beta
@@ -30,11 +30,11 @@ P = 4;
J = P/2;%P/2;
PMAX = P; % Hermite basis size
JMAX = J; % Laguerre basis size
-NX = 16; % real space x-gridpoints
-NY = 16; % real space y-gridpoints
+NX = 8; % real space x-gridpoints
+NY = 2; % real space y-gridpoints
LX = 2*pi/0.1; % Size of the squared frequency domain in x direction
-LY = 2*pi/0.2; % Size of the squared frequency domain in y direction
-NZ = 24; % number of perpendicular planes (parallel grid)
+LY = 2*pi/0.5; % Size of the squared frequency domain in y direction
+NZ = 32; % number of perpendicular planes (parallel grid)
SG = 0; % Staggered z grids option
NEXC = 1; % To extend Lx if needed (Lx = Nexc/(kymin*shear))
diff --git a/wk/parameters/lin_Entropy.m b/wk/parameters/lin_Entropy.m
index ea0b655db7e4e66f06ff53dea77bfe562c9ac8ce..31c57f712dffb8b3b1066087d95e926458cafc50 100644
--- a/wk/parameters/lin_Entropy.m
+++ b/wk/parameters/lin_Entropy.m
@@ -14,17 +14,17 @@ NA = 2; % number of kinetic species
ADIAB_E = 0; % adiabatic electron model
ADIAB_I = 0; % adiabatic ion model
BETA = 0.000; % electron plasma beta
-MHD_PD = 0; % MHD pressure drift
+MHD_PD = 1; % MHD pressure drift
%% Set up grid parameters
P = 4;
J = P/2;%P/2;
PMAX = P; % Hermite basis size
JMAX = J; % Laguerre basis size
NX = 2; % real space x-gridpoints
-NY = 12; % real space y-gridpoints
+NY = 40; % real space y-gridpoints
LX = 2*pi/0.05; % Size of the squared frequency domain in x direction
-LY = 2*pi/0.2; % Size of the squared frequency domain in y direction
-NZ = 16; % number of perpendicular planes (parallel grid)
+LY = 2*pi/0.1; % Size of the squared frequency domain in y direction
+NZ = 1; % number of perpendicular planes (parallel grid)
SG = 0; % Staggered z grids option
NEXC = 1; % To extend Lx if needed (Lx = Nexc/(kymin*shear))
%% GEOMETRY
@@ -45,8 +45,8 @@ SHIFT_Y = 0.0; % Shift in the periodic BC in z
NPOL = 1; % Number of poloidal turns
PB_PHASE= 0;
%% TIME PARAMETERS
-TMAX = 100; % Maximal time unit
-DT = 1e-3; % Time step
+TMAX = 50; % Maximal time unit
+DT = 1e-2; % Time step
DTSAVE0D = 1.0; % Sampling time for 0D arrays
DTSAVE2D = -1; % Sampling time for 2D arrays
DTSAVE3D = 2.0; % Sampling time for 3D arrays
diff --git a/wk/parameters/lin_JET_rho97.m b/wk/parameters/lin_JET_rho97.m
new file mode 100644
index 0000000000000000000000000000000000000000..5047e578535c447cb450728dbe55acf7513e2753
--- /dev/null
+++ b/wk/parameters/lin_JET_rho97.m
@@ -0,0 +1,101 @@
+% Parameters found in Parisi et al. 2020
+% Jet shot 92174
+%% Set simulation parameters
+SIMID = 'lin_JET_rho97'; % Name of the simulation
+%% Set up physical parameters
+CLUSTER.TIME = '99:00:00'; % Allocation time hh:mm:ss
+nu = 0.83; %(0.00235 in GENE)
+TAU = 0.56; % e/i temperature ratio
+K_Ne = 10; % ele Density '''
+K_Te = 42; % ele Temperature '''
+K_Ni = 10; % ion Density gradient drive
+K_Ti = 11; % ion Temperature '''
+SIGMA_E = 0.0233380; % mass ratio sqrt(m_a/m_i) (correct = 0.0233380)
+NA = 2; % number of kinetic species
+ADIAB_E = (NA==1); % adiabatic electron model
+BETA = 0.0031; % electron plasma beta
+MHD_PD = 0;
+
+%% GEOMETRY
+% GEOMETRY= 's-alpha';
+GEOMETRY= 'miller';
+EPS = 0.9753*0.91/2.91; % inverse aspect ratio
+Q0 = 5.10; % safety factor
+SHEAR = 3.36; % magnetic shear
+KAPPA = 1.55; % elongation
+S_KAPPA = 0.95;
+DELTA = 0.26; % triangularity
+S_DELTA = 0.74;
+ZETA = 0; % squareness
+S_ZETA = 0;
+PARALLEL_BC = 'dirichlet'; % Boundary condition for parallel direction ('dirichlet','periodic','shearless','disconnected')
+SHIFT_Y = 0.0; % Shift in the periodic BC in z
+NPOL = 1; % Number of poloidal turns
+PB_PHASE = 0;
+
+%% Set up grid parameters
+P = 4;
+J = P/2;%P/2;
+PMAX = P; % Hermite basis size
+JMAX = J; % Laguerre basis size
+NX = 8; % real space x-gridpoints
+NY = 2; % real space y-gridpoints
+LX = 2*pi/0.1; % Size of the squared frequency domain in x direction
+LY = 2*pi/0.5; % Size of the squared frequency domain in y direction
+NZ = 32; % number of perpendicular planes (parallel grid)
+SG = 0; % Staggered z grids option
+NEXC = 1; % To extend Lx if needed (Lx = Nexc/(kymin*shear))
+
+%% TIME PARAMETERS
+TMAX = 15; % Maximal time unit
+DT = 1e-3; % Time step
+DTSAVE0D = 0.5; % Sampling time for 0D arrays
+DTSAVE2D = -1; % Sampling time for 2D arrays
+DTSAVE3D = 0.5; % Sampling time for 3D arrays
+DTSAVE5D = 100; % Sampling time for 5D arrays
+JOB2LOAD = -1; % Start a new simulation serie
+
+%% OPTIONS
+LINEARITY = 'linear'; % activate non-linearity (is cancelled if KXEQ0 = 1)
+CO = 'DG'; % Collision operator (LB:L.Bernstein, DG:Dougherty, SG:Sugama, LR: Lorentz, LD: Landau)
+GKCO = 1; % Gyrokinetic operator
+ABCO = 1; % INTERSPECIES collisions
+INIT_ZF = 0; % Initialize zero-field quantities
+HRCY_CLOS = 'truncation'; % Closure model for higher order moments
+DMAX = -1;
+NLIN_CLOS = 'truncation'; % Nonlinear closure model for higher order moments
+NMAX = 0;
+KERN = 0; % Kernel model (0 : GK)
+INIT_OPT = 'phi'; % Start simulation with a noisy mom00/phi/allmom
+NUMERICAL_SCHEME = 'RK4'; % Numerical integration scheme (RK2,SSPx_RK2,RK3,SSP_RK3,SSPx_RK3,IMEX_SSP2,ARK2,RK4,DOPRI5)
+
+%% OUTPUTS
+W_DOUBLE = 1; % Output flag for double moments
+W_GAMMA = 1; % Output flag for gamma (Gyrokinetic Energy)
+W_HF = 1; % Output flag for high-frequency potential energy
+W_PHI = 1; % Output flag for potential
+W_NA00 = 1; % Output flag for nalpha00 (density of species alpha)
+W_DENS = 1; % Output flag for total density
+W_TEMP = 1; % Output flag for temperature
+W_NAPJ = 1; % Output flag for nalphaparallel (parallel momentum of species alpha)
+W_SAPJ = 0; % Output flag for saparallel (parallel current of species alpha)
+
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
+%% UNUSED PARAMETERS
+% These parameters are usually not to play with in linear runs
+MU = 0.0; % Hyperdiffusivity coefficient
+MU_X = MU; % Hyperdiffusivity coefficient in x direction
+MU_Y = MU; % Hyperdiffusivity coefficient in y direction
+N_HD = 4; % Degree of spatial-hyperdiffusivity
+MU_Z = 2.0; % Hyperdiffusivity coefficient in z direction
+HYP_V = 'hypcoll'; % Kinetic-hyperdiffusivity model
+MU_P = 0.0; % Hyperdiffusivity coefficient for Hermite
+MU_J = 0.0; % Hyperdiffusivity coefficient for Laguerre
+LAMBDAD = 0.0; % Lambda Debye
+NOISE0 = 1.0e-5; % Initial noise amplitude
+BCKGD0 = 0.0e-5; % Initial background
+k_gB = 1.0; % Magnetic gradient strength
+k_cB = 1.0; % Magnetic curvature strength
+COLL_KCUT = 1; % Cutoff for collision operator
+ADIAB_I = 0; % adiabatic ion model
\ No newline at end of file