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Antoine Cyril David Hoffmann
Gyacomo
Commits
7ed60f68
Commit
7ed60f68
authored
1 year ago
by
Antoine Cyril David Hoffmann
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wk/paper_2_scripts_and_results/fast_analysis.m
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7ed60f68
gyacomodir
=
pwd
;
gyacomodir
=
gyacomodir
(
1
:
end
-
2
);
% get code directory
addpath
(
genpath
([
gyacomodir
,
'matlab'
]))
% ... add
addpath
(
genpath
([
gyacomodir
,
'matlab/plot'
]))
% ... add
addpath
(
genpath
([
gyacomodir
,
'matlab/compute'
]))
% ... add
addpath
(
genpath
([
gyacomodir
,
'matlab/load'
]))
% ... add
default_plots_options
% Partition of the computer where the data have to be searched
PARTITION
=
'/misc/gyacomo23_outputs/'
;
% PARTITION = '/home/ahoffman/gyacomo/';
%% Tests
% resdir = 'test_stepon_AA/CBC_stepon_AA';
% resdir = 'test_stepon_AA/CBC_no_stepon_AA'; % No clear conclusions
%% CBC benchmark
% resdir = 'paper_2_GYAC23/CBC/3x2x128x64x24';
% resdir = 'paper_2_GYAC23/CBC/3x2x128x64x24_nu_5e-2';
% resdir = 'paper_2_GYAC23/CBC/5x3x128x64x24';
% resdir = 'paper_2_GYAC23/CBC/7x4x128x64x24';
% resdir = 'paper_2_GYAC23/CBC/21x6x192x96x24';
%% low precision kT scan
% resdir = 'paper_2_GYAC23/local_runs/1x2x64x48x16/CBC';
% resdir = 'paper_2_GYAC23/local_runs/1x2x64x48x16/CBC_dp';
% resdir = 'paper_2_GYAC23/local_runs/1x2x128x64x16/CBC';
% resdir = 'paper_2_GYAC23/local_runs/nu=0.05/5x2x64x48x16/kT_3.5';
% resdir = 'paper_2_GYAC23/local_runs/nu=0.05/5x2x64x48x16/kT_4.0';
% resdir = 'paper_2_GYAC23/local_runs/nu=0.05/5x2x64x48x16/kT_4.5';
% resdir = 'paper_2_GYAC23/local_runs/nu=0.05/5x2x64x48x16/kT_5.3';
% resdir = 'paper_2_GYAC23/local_runs/5x2x64x48x16/CBC';
% resdir = 'paper_2_GYAC23/local_runs/5x2x64x48x16/CBC_noise_init';
% resdir = 'paper_2_GYAC23/local_runs/nu=0.05/9x2x64x48x16/kT_3.5';
% resdir = 'paper_2_GYAC23/local_runs/nu=0.05/9x2x64x48x16/kT_4.0';
% resdir = 'paper_2_GYAC23/local_runs/nu=0.05/9x2x64x48x16/kT_4.5';
% resdir = 'paper_2_GYAC23/local_runs/nu=0.05/9x2x64x48x16/kT_5.3';
% resdir = 'paper_2_GYAC23/local_runs/9x2x64x48x16/CBC';
% resdir = 'paper_2_GYAC23/local_runs/nu=0.05/11x2x64x48x16/kT_4.0';
% resdir = 'paper_2_GYAC23/local_runs/nu=0.05/11x2x64x48x16/kT_4.5';
% resdir = 'paper_2_GYAC23/local_runs/nu=0.05/11x2x64x48x16/kT_5.3';
% resdir = 'paper_2_GYAC23/local_runs/nu=0.05/11x2x64x48x16/CBC';
% resdir = 'paper_2_GYAC23/local_runs/11x2x64x48x16/CBC';
%% Collision scan
% resdir = 'paper_2_GYAC23/collision_study/nuLDGK_scan_CBC/7x2x64x48x16/nu_0.1';
% resdir = 'paper_2_GYAC23/collision_study/nuLDGK_scan_CBC/9x2x64x48x16/nu_0.1';
% resdir = 'paper_2_GYAC23/collision_study/nuLDGK_scan_CBC/9x2x64x48x16/nu_0.1';
% resdir = 'paper_2_GYAC23/collision_study/nuDGGK_scan_kT_5.3/9x5x128x64x24/nu_0.5';
% resdir = 'paper_2_GYAC23/collision_study/nuDGGK_scan_kT_5.3/5x3x128x64x24/nu_0.5';
% resdir = 'paper_2_GYAC23/collision_study/nuSGGK_scan_kT_5.3/9x5x128x64x24/nu_0.5';
% resdir = 'paper_2_GYAC23/collision_study/nuSGGK_scan_kT_5.3/9x5x128x64x24_Lx200/nu_0.5';
% resdir = 'paper_2_GYAC23/collision_study/nuLDGK_scan_kT_5.3/9x5x128x64x24/nu_0.005';
% resdir = 'paper_2_GYAC23/collision_study/nuDGGK_scan_kT_5.3/11x6x192x96x24/nu_0.1';
% resdir = 'paper_2_GYAC23/collision_study/nuDGGK_scan_kT_5.3/9x5x192x96x24/nu_0.2';
% resdir = 'paper_2_GYAC23/collision_study/nuDGGK_scan_kT_5.3/17x9x192x96x24/nu_0.2';
% resdir = 'paper_2_GYAC23/collision_study/nuDGGK_scan_kT_5.3/17x9x192x96x24/nu_0.02';
% resdir = 'paper_2_GYAC23/collision_study/nuSGGK_scan_kT_5.3/17x9x192x96x24/nu_0.02';
% resdir = 'paper_2_GYAC23/collision_study/nuSGGK_scan_kT_5.3/9x5x192x96x24/nu_0.2';
% resdir = 'paper_2_GYAC23/collision_study/nuDGGK_scan_kT_5.3/17x9x192x96x24/continue_SG_nu_0.02';
% resdir = 'paper_2_GYAC23/collision_study/nuSGGK_scan_kT_5.3/5x3x192x96x24/nu_0.02';
% resdir = 'paper_2_GYAC23/collision_study/nuSGGK_scan_kT_5.3/9x5x192x96x24/nu_0.02';
% resdir = 'paper_2_GYAC23/collision_study/nuSGGK_scan_kT_5.3/17x9x192x96x24/nu_0.02';
% resdir = 'paper_2_GYAC23/collision_study/nuSGGK_scan_kT_5.3/17x9x192x96x24/nu_0.005';
% resdir = 'paper_2_GYAC23/collision_study/nuLDGK_scan_kT_5.3/5x3x192x96x24/nu_0.005';
% resdir = 'paper_2_GYAC23/collision_study/nuLDGK_scan_kT_5.3/9x5x192x96x24/nu_0.005';
% resdir = 'paper_2_GYAC23/collision_study/nuLDGK_scan_kT_5.3/17x9x128x64x24/nu_0.005';
% resdir = 'paper_2_GYAC23/collision_study/nuLDGK_scan_kT_5.3/17x9x128x64x24_large_box/nu_0.005';
% resdir = 'paper_2_GYAC23/collision_study/nuLDGK_scan_kT_5.3/17x9x128x64x24_ckcut_0.8/nu_0.005';
%% kT eff study
% resdir = 'paper_2_GYAC23/kT_eff_study/1x3x128x64x24_kT_3.0/Lx120';
% resdir = 'paper_2_GYAC23/kT_eff_study/1x3x128x64x24_kT_3.0/Lx240';
% resdir = 'paper_2_GYAC23/kT_eff_study/3x3x128x64x24_kT_3.4/Lx120';
% resdir = 'paper_2_GYAC23/kT_eff_study/3x3x128x64x24_kT_3.4/Lx240';
% resdir = 'paper_2_GYAC23/kT_eff_study/5x3x128x64x24_kT_3.5';
% resdir = 'paper_2_GYAC23/kT_eff_study/7x3x128x64x24_kT_3.6/truncation';
% resdir = 'paper_2_GYAC23/kT_eff_study/7x3x128x64x24_kT_3.6/dmax';
%% dev
PARTITION
=
''
;
% resdir = '/home/ahoffman/gyacomo/testcases/zpinch_3D';
% resdir = '/home/ahoffman/gyacomo/results/dev/3D_kine_zpinch_test';
%% CBC benchmark
% resdir = '/misc/gyacomo23_outputs/paper_2_GYAC23/kT_scan_nu_1e-3/3x2x128x64x24/kT_7.0';
% resdir = '/misc/gyacomo23_outputs/paper_2_GYAC23/kT_scan_nu_1e-3/5x3x128x64x24/kT_7.0';
% resdir = '/misc/gyacomo23_outputs/paper_2_GYAC23/kT_scan_nu_1e-3/9x5x128x64x24/kT_7.0';
% resdir = '/misc/gyacomo23_outputs/paper_2_GYAC23/kT_scan_nu_1e-3/17x9x128x64x24/kT_7.0';
% resdir = '/misc/gyacomo23_outputs/paper_2_GYAC23/kT_scan_nu_1e-3/31x16x128x64x24/kT_7.0';
%% Paper 3
resdir
=
'/misc/gyacomo23_outputs/paper_3_GYAC23/CBC_kine'
;
%%
J0
=
00
;
J1
=
20
;
% Load basic info (grids and time traces)
DATADIR
=
[
PARTITION
,
resdir
,
'/'
];
data
=
{};
data
=
compile_results_low_mem
(
data
,
DATADIR
,
J0
,
J1
);
if
1
%% Plot transport and phi radial profile
[
data
.
PHI
,
data
.
Ts3D
]
=
compile_results_3D
(
DATADIR
,
J0
,
J1
,
'phi'
);
options
.
TAVG_0
=
100
;
options
.
TAVG_1
=
1000
;
options
.
NCUT
=
5
;
% Number of cuts for averaging and error estimation
options
.
NMVA
=
1
;
% Moving average for time traces
% options.ST_FIELD = '\Gamma_x'; % chose your field to plot in spacetime diag (e.g \phi,v_x,G_x)
options
.
ST_FIELD
=
'\phi'
;
% chose your field to plot in spacetime diag (e.g \phi,v_x,G_x)
options
.
INTERP
=
0
;
options
.
RESOLUTION
=
256
;
plot_radial_transport_and_spacetime
(
data
,
options
);
end
if
0
%% MOVIES %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
% Options
% [data.PHI, data.Ts3D] = compile_results_3D(DATADIR,J0,J1,'phi');
% [data.Na00, data.Ts3D] = compile_results_3Da(DATADIR,J0,J1,'Na00');
% data.Ni00 = reshape(data.Na00(1,:,:,:,:),data.grids.Nky,data.grids.Nkx,data.grids.Nz,numel(data.Ts3D));
options
.
INTERP
=
1
;
options
.
POLARPLOT
=
0
;
options
.
NAME
=
'\phi'
;
% options.NAME = '\phi^{NZ}';
% options.NAME = '\omega_z';
% options.NAME = 'N_i^{00}';
% options.NAME = 's_{Ey}';
% options.NAME = 'n_i^{NZ}';
% options.NAME = 'Q_x';
% options.NAME = 'n_i';
% options.NAME = 'n_i-n_e';
options
.
PLAN
=
'yz'
;
% options.NAME = 'f_i';
% options.PLAN = 'sx';
options
.
COMP
=
'avg'
;
% options.TIME = data.Ts5D(end-30:end);
options
.
TIME
=
data
.
Ts3D
(
1
:
1
:
end
);
% options.TIME = [0:1500];
data
.
EPS
=
0.1
;
data
.
a
=
data
.
EPS
*
2000
;
options
.
RESOLUTION
=
256
;
create_film
(
data
,
options
,
'.gif'
)
end
if
0
%% fields snapshots
% Options
[
data
.
Na00
,
data
.
Ts3D
]
=
compile_results_3Da
(
DATADIR
,
J0
,
J1
,
'Na00'
);
[
data
.
PHI
,
data
.
Ts3D
]
=
compile_results_3D
(
DATADIR
,
J0
,
J1
,
'phi'
);
data
.
Ni00
=
reshape
(
data
.
Na00
(
1
,:,:,:,:),
data
.
grids
.
Nky
,
data
.
grids
.
Nkx
,
data
.
grids
.
Nz
,
numel
(
data
.
Ts3D
));
options
.
INTERP
=
0
;
options
.
POLARPLOT
=
0
;
options
.
AXISEQUAL
=
0
;
options
.
NORMALIZE
=
0
;
% options.NAME = 'N_i^{00}';
options
.
NAME
=
'\phi'
;
options
.
PLAN
=
'kxky'
;
options
.
COMP
=
'avg'
;
options
.
TIME
=
[
0
:
0.02
:
0.14
];
% options.TIME = data.Ts3D(1:2:end);
options
.
RESOLUTION
=
256
;
fig
=
photomaton
(
data
,
options
);
% save_figure(data,fig)
end
if
0
%% Performance profiler
profiler
(
data
)
end
if
1
%% Hermite-Laguerre spectrum
[
data
.
Napjz
,
data
.
Ts3D
]
=
compile_results_3Da
(
DATADIR
,
J0
,
J1
,
'Napjz'
);
% [data.Napjz, data.Ts3D] = compile_results_3D(DATADIR,J0,J1,'Nipjz');
options
.
ST
=
1
;
options
.
NORMALIZED
=
0
;
options
.
LOGSCALE
=
1
;
options
.
FILTER
=
0
;
%filter the 50% time-average of the spectrum from
options
.
TAVG_2D
=
0
;
%Show a 2D plot of the modes, 50% time averaged
options
.
TAVG_2D_CTR
=
0
;
%make it contour plot
fig
=
show_moments_spectrum
(
data
,
options
);
end
if
0
%% Mode evolution
[
data
.
PHI
,
data
.
Ts3D
]
=
compile_results_3D
(
DATADIR
,
J0
,
J1
,
'phi'
);
options
.
NORMALIZED
=
0
;
options
.
TIME
=
[
000
:
9000
];
options
.
KX_TW
=
[
30
40
];
%kx Growth rate time window
options
.
KY_TW
=
[
10
20
];
%ky Growth rate time window
options
.
NMA
=
1
;
options
.
NMODES
=
800
;
options
.
iz
=
'avg'
;
% avg or index
options
.
ik
=
1
;
% sum, max or index
options
.
fftz
.
flag
=
0
;
fig
=
mode_growth_meter
(
data
,
options
);
% save_figure(data,fig,'.png')
end
if
0
%% Study singular values
[
data
.
SV_ky_pj
,
data
.
Ts2D
]
=
compile_results_2D
(
DATADIR
,
J0
,
J1
,
'sv_ky_pj'
);
nSV
=
data
.
grids
.
Np
*
data
.
grids
.
Nj
;
colors_
=
jet
(
nSV
);
figure
for
i
=
1
:
nSV
sv
=
squeeze
(
data
.
SV_ky_pj
(
i
,:));
semilogy
(
data
.
Ts2D
,
sv
,
...
'color'
,
colors_
(
i
,:),
'DisplayName'
,[
'SV '
,
num2str
(
i
)]);
hold
on
end
legend
(
'show'
);
end
\ No newline at end of file
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