The inputs structure contains the basic information needed by FIDASIM.
| Variable | Type | Rank | Dimensions | Units | Description |
|---|---|---|---|---|---|
shot |
Int32 | 0 | NA | NA | Shot Number |
time |
Float64 | 0 | NA | s | Time |
runid |
String | 0 | NA | NA | Run ID |
comment |
String | 0 | NA | NA | Comment |
result_dir |
String | 0 | NA | NA | Result directory |
tables_file |
String | 0 | NA | NA | Atomic Tables file |
The simulation switches can take values 0, 1, or 2. A value of zero and one will turn the calculation off and on respectively. A value of two will turn on additional functionality.
| Variable | Type | Rank | Dimensions | Units | Description |
|---|---|---|---|---|---|
calc_bes |
Int16 | 0 | NA | NA | Calculate Beam Emission and Halo spectra |
calc_brems |
Int16 | 0 | NA | NA | Calculate Bremsstrahlung |
calc_fida |
Int16 | 0 | NA | NA | Calculate FIDA spectra |
calc_npa |
Int16 | 0 | NA | NA | Calculate NPA flux |
calc_birth |
Int16 | 0 | NA | NA | Calculate Birth profile |
calc_fida_wght |
Int16 | 0 | NA | NA | Calculate FIDA weight functions |
calc_npa_wght |
Int16 | 0 | NA | NA | Calculate NPA weight functions |
dump_dcx |
Int16 | 0 | NA | NA | Dump DCX neutrals and spectra |
These settings control the number of Monte Carlo particles used by FIDASIM. Using too few particles will execute quickly but will be extremely noisy. Contrarily, using too many particles will increase runtime but will have small Monte Carlo noise. The following settings provide a good balance between runtime and Monte Carlo noise.
n_fida = 5000000Ln_npa = 5000000Ln_nbi = 50000Ln_dcx = 500000Ln_halo = 500000Ln_birth = 50000L| Variable | Type | Rank | Dimensions | Units | Description |
|---|---|---|---|---|---|
n_fida |
Int32 | 0 | NA | NA | Number of FIDA MC particles |
n_npa |
Int32 | 0 | NA | NA | Number of NPA MC particles |
n_nbi |
Int32 | 0 | NA | NA | Number of NBI MC particles |
n_dcx |
Int32 | 0 | NA | NA | Number of DCX MC particles |
n_halo |
Int32 | 0 | NA | NA | Number of HALO MC particles |
n_birth |
Int32 | 0 | NA | NA | Number of Birth particles outputed |
These variables define the neutral beam properties.
Currently the mass of the beam species, ab, can only be the mass either protium or deuterium.
The current_fractions variable must sum to one.
Click here for more information.
| Variable | Type | Rank | Dimensions | Units | Description |
|---|---|---|---|---|---|
ab |
Float64 | 0 | NA | amu | Beam species mass |
pinj |
Float64 | 0 | NA | MW | Beam power |
einj |
Float64 | 0 | NA | keV | Beam energy |
current_fractions |
Float64 | 1 | [3] | NA | Current fractions (Full, Half, Third) |
These variables define the properties of the thermal plasma species.
Like the ab variable, ai can only be the mass of either protium or deuterium
Click here for more information.
| Variable | Type | Rank | Dimensions | Units | Description |
|---|---|---|---|---|---|
ai |
Float64 | 0 | NA | amu | Thermal Ion species mass |
impurity_charge |
Int16 | 0 | NA | NA | Impurity Charge |
These variables define a rotated coordinate system. Click here for more details.
| Variable | Type | Rank | Dimensions | Units | Description |
|---|---|---|---|---|---|
nx |
Int16 | 0 | NA | NA | Number of cells in the X direction |
ny |
Int16 | 0 | NA | NA | Number of cells in the Y direction |
nz |
Int16 | 0 | NA | NA | Number of cells in the Z direction |
xmin |
Float64 | 0 | NA | cm | Minimum X value in beam grid coordinates |
xmax |
Float64 | 0 | NA | cm | Maximum X value in beam grid coordinates |
ymin |
Float64 | 0 | NA | cm | Minimum Y value in beam grid coordinates |
ymax |
Float64 | 0 | NA | cm | Maximum Y value in beam grid coordinates |
zmin |
Float64 | 0 | NA | cm | Minimum Z value in beam grid coordinates |
zmax |
Float64 | 0 | NA | cm | Maximum Z value in beam grid coordinates |
alpha |
Float64 | 0 | NA | rad | Tait-Bryan rotation angle about z-axis |
beta |
Float64 | 0 | NA | rad | Tait-Bryan rotation angle about y'-axis |
gamma |
Float64 | 0 | NA | rad | Tait-Bryan rotation angle about x"-axis |
origin |
Float64 | 1 | [3] | cm | Beam grid origin in Machine Coordinates |
These variables define the wavelength grid. Using a fine wavelength has no performance penalty. Click here for more more information.
| Variable | Type | Rank | Dimensions | Units | Description |
|---|---|---|---|---|---|
nlambda |
Int16 | 0 | NA | NA | Number of wavelengths |
lambdamin |
Float64 | 0 | NA | nm | Minimum wavelength |
lambdamax |
Float64 | 0 | NA | nm | Maximum wavelength |
These variables define the setting for the calculation of weight functions. Click here for more information.
| Variable | Type | Rank | Dimensions | Units | Description |
|---|---|---|---|---|---|
ne_wght |
Int16 | 0 | NA | NA | Number of weight function energies |
np_wght |
Int16 | 0 | NA | NA | Number of weight function pitches |
nphi_wght |
Int16 | 0 | NA | NA | Number of gyro-angles |
emax_wght |
Float64 | 0 | NA | keV | Maximum energy of weight functions |
nlambda_wght |
Int16 | 0 | NA | NA | Number of weight function wavelengths |
lambdamin_wght |
Float64 | 0 | NA | nm | Minimum weight function wavelength |
lambdamax_wght |
Float64 | 0 | NA | nm | Maximum weight function wavelength |
The grid structure contains the definition of the 2D R-Z grid that the plasma parameters and electromagnetic fields are mapped onto.
| Variable | Type | Rank | Dimensions | Units | Description |
|---|---|---|---|---|---|
nr |
Int16 | 0 | NA | NA | Number of radii |
nz |
Int16 | 0 | NA | NA | Number of z values |
r |
Float64 | 1 | [nr] |
cm | Array of radii |
z |
Float64 | 1 | [nz] |
cm | Array of z values |
r2d |
Float64 | 2 | [nr,nz] |
cm | 2D array of radii r = r2d(r,z) |
z2d |
Float64 | 2 | [nr,nz] |
cm | 2D array of z values z = z2d(r,z) |
The nbi structure contains the neutral beam geometry.
The (a)shape of the source grid and apertures take the value of 1 or 2 for a rectangular and circular respectively.
Click here for more information.
| Variable | Type | Rank | Dimensions | Units | Description |
|---|---|---|---|---|---|
name |
String | 0 | NA | NA | Name of the neutral beam |
shape |
Int16 | 0 | NA | NA | Shape of the beam source grid (1 or 2) |
data_source |
String | 0 | NA | NA | Source of the neutral beam geometry |
src |
Float64 | 1 | [3] | cm | Position of the source grid in machine coordinates |
axis |
Float64 | 1 | [3] | NA | Direction of the beam center line |
widy |
Float64 | 0 | NA | cm | Source grid half-width in the horizontal direction |
widz |
Float64 | 0 | NA | cm | Source grid half-height in the vertical direction |
divy |
Float64 | 1 | [3] | rad | Horizontal beam divergence |
divz |
Float64 | 1 | [3] | rad | Vertical beam divergence |
focy |
Float64 | 0 | NA | cm | Horizontal focal length |
focz |
Float64 | 0 | NA | cm | Vertical focal length |
naperture |
Int16 | 0 | NA | NA | Number of apertures |
ashape |
Int16 | 1 | [naperture] |
NA | Shape of the aperture(s) (1 or 2) |
awidy |
Float64 | 1 | [naperture] |
cm | Half-width of the aperture(s) |
awidz |
Float64 | 1 | [naperture] |
cm | Half-height of the aperture(s) |
aoffy |
Float64 | 1 | [naperture] |
cm | Horizontal (y) offset of the aperture(s) relative to the +x aligned beam centerline |
aoffz |
Float64 | 1 | [naperture] |
cm | Vertical (z) offset of the aperture(s) relative to the +x aligned beam centerline |
adist |
Float64 | 1 | [naperture] |
cm | Distance from the center of the beam source grid to the aperture(s) plane |
This structure contain the electromagnetic fields mapped onto the interpolation grid. Click here for more information.
| Variable | Type | Rank | Dimensions | Units | Description |
|---|---|---|---|---|---|
time |
Float64 | 0 | NA | s | Time when the fields data were collected/reconstructed |
data_source |
String | 0 | NA | NA | Source of the fields data |
mask |
Int16 | 2 | [nr,nz] |
NA | Boolean mask that indicates where the fields are well defined |
br |
Float64 | 2 | [nr,nz] |
T | Radial component of the magnetic field |
bt |
Float64 | 2 | [nr,nz] |
T | Torodial/Phi component of the magnetic field |
bz |
Float64 | 2 | [nr,nz] |
T | Z component of the magnetic field |
er |
Float64 | 2 | [nr,nz] |
V/m | Radial component of the electric field |
et |
Float64 | 2 | [nr,nz] |
V/m | Torodial/Phi component of the electric field |
ez |
Float64 | 2 | [nr,nz] |
V/m | Z component of the electric field |
This structure contain the plasma parameters mapped onto the interpolation grid. Click here for more information.
| Variable | Type | Rank | Dimensions | Units | Description |
|---|---|---|---|---|---|
time |
Float64 | 0 | NA | s | Time when the plasma parameter data was collected |
data_source |
String | 0 | NA | NA | Source of the plasma parameter data |
mask |
Int16 | 2 | [nr,nz] |
NA | Boolean mask that indicates where the plasma is well defined |
te |
Float64 | 2 | [nr,nz] |
keV | Electron temperature |
ti |
Float64 | 2 | [nr,nz] |
keV | Ion temperature |
dene |
Float64 | 2 | [nr,nz] |
cm^-3 | Electron density |
zeff |
Float64 | 2 | [nr,nz] |
NA | Z-effective |
vr |
Float64 | 2 | [nr,nz] |
cm/s | Radial component of the bulk plasma rotation/flow |
vt |
Float64 | 2 | [nr,nz] |
cm/s | Torodial/Phi component of the bulk plasma rotation/flow |
vz |
Float64 | 2 | [nr,nz] |
cm/s | Z component of the bulk plasma rotation/flow |
The dist structure contains the fast-ion distribution which can be one of three different types.
Click here for more information.
| Variable | Type | Rank | Dimensions | Units | Description |
|---|---|---|---|---|---|
type |
Int16 | 0 | NA | NA | Distribution type (1) |
time |
Float64 | 0 | NA | s | Time of the distribution |
data_source |
String | 0 | NA | NA | Source of the distribution data |
nenergy |
Int16 | 0 | NA | NA | Number of energy values |
npitch |
Int16 | 0 | NA | NA | Number of pitch values |
energy |
Float64 | 1 | [nenergy] |
keV | Energy array |
pitch |
Float64 | 1 | [npitch] |
NA | Pitch array w.r.t magnetic field |
denf |
Float64 | 2 | [nr,nz] |
cm^-3 | Fast-ion density |
f |
Float64 | 4 | [nenergy,npitch,nr,nz] |
fast-ions/(dE dP cm^3) | Fast-ion distribution F(E,p,R,Z) |
The sum(weight) = # of Fast-ions in phase space sampled by the MC particles.
The class variable can take values in the range of 1:nclass.
| Variable | Type | Rank | Dimensions | Units | Description |
|---|---|---|---|---|---|
type |
Int16 | 0 | NA | NA | Distribution type (2) |
time |
Float64 | 0 | NA | s | Time of the distribution |
data_source |
String | 0 | NA | NA | Source of the distribution data |
nparticle |
Int32 | 0 | NA | NA | Number of MC particles |
nclass |
Int16 | 0 | NA | NA | Number of orbit classes |
class |
Int16 | 1 | [nparticle] |
NA | Orbit class of the MC particle |
weight |
Float64 | 1 | [nparticle] |
fast-ions | Weight of the MC particle |
r |
Float64 | 1 | [nparticle] |
cm | R positions of the MC particle |
z |
Float64 | 1 | [nparticle] |
cm | Z positions of the MC particle |
energy |
Float64 | 1 | [nparticle] |
keV | Energy of the MC particle |
pitch |
Float64 | 1 | [nparticle] |
NA | Pitch w.r.t the magnetic field of the MC particle |
The sum(weight) = # of Fast-ions in phase space sampled by the MC particles
The class variable can take values in the range of 1:nclass.
| Variable | Type | Rank | Dimensions | Units | Description |
|---|---|---|---|---|---|
type |
Int16 | 0 | NA | NA | Distribution type (3) |
time |
Float64 | 0 | NA | s | Time of the distribution |
data_source |
String | 0 | NA | NA | Source of the distribution data |
nparticle |
Int32 | 0 | NA | NA | Number of MC particles |
nclass |
Int16 | 0 | NA | NA | Number of orbit classes |
class |
Int16 | 1 | [nparticle] |
NA | Orbit class of the MC particle |
weight |
Float64 | 1 | [nparticle] |
fast-ions | Weight of the MC particle |
r |
Float64 | 1 | [nparticle] |
cm | R positions of the MC particle |
z |
Float64 | 1 | [nparticle] |
cm | Z positions of the MC particle |
vr |
Float64 | 1 | [nparticle] |
cm/s | Radial component of the MC particle velocity |
vt |
Float64 | 1 | [nparticle] |
cm/s | Torodial/Phi component of the MC particle velocity |
vz |
Float64 | 1 | [nparticle] |
cm/s | Z component of the MC particle velocity |
This structure contains the geometry of the spectroscopic systems Click here for more more information.
| Variable | Type | Rank | Dimensions | Units | Description |
|---|---|---|---|---|---|
nchan |
Int32 | 0 | NA | NA | Number of channels |
system |
String | 0 | NA | NA | Name of the spectrocopic system(s) |
data_source |
String | 0 | NA | NA | Source of the spectral geometry data |
id |
String | 1 | [nchan] |
NA | Channel ID |
radius |
Float64 | 1 | [nchan] |
cm | Line of sight radius at midplane or tangency point |
lens |
Float64 | 2 | [3,nchan] |
cm | Lens location in machine coordinates |
axis |
Float64 | 2 | [3,nchan] |
NA | Optical axis/direction of the lines of sight |
spot_size |
Float64 | 1 | [nchan] |
cm | Radius of the collecting volume |
sigma_pi |
Float64 | 1 | [nchan] |
NA | Ratio of the intensities of the sigma and pi stark lines |
This structure contains the geometry of the spectroscopic systems The shapes of the detector and aperture can take the value 1 or 2 for a rectangular and circular aperture/detector respectively. Click here for more more information.
| Variable | Type | Rank | Dimensions | Units | Description |
|---|---|---|---|---|---|
nchan |
Int32 | 0 | NA | NA | Number of channels |
system |
String | 0 | NA | NA | Name of the NPA system(s) |
data_source |
String | 0 | NA | NA | Source of the NPA geometry data |
id |
String | 1 | [nchan] |
NA | Channel ID |
radius |
Float64 | 1 | [nchan] |
cm | Line of sight radius at midplane or tangency point |
a_shape |
Int16 | 1 | [nchan] |
NA | Shape of the aperture |
d_shape |
Int16 | 1 | [nchan] |
NA | Shape of the detector |
a_cent |
Float64 | 2 | [3,nchan] |
cm | Position of the center of the aperture |
a_redge |
Float64 | 2 | [3,nchan] |
cm | Position of the apertures right edge |
a_tedge |
Float64 | 2 | [3,nchan] |
cm | Position of the apertures top edge |
d_cent |
Float64 | 2 | [3,nchan] |
cm | Position of the center of the detector |
d_redge |
Float64 | 2 | [3,nchan] |
cm | Position of the detectors right edge |
d_tedge |
Float64 | 2 | [3,nchan] |
cm | Position of the detectors top edge |