lion
This documentation is generated from the XML schema, the xsd-file, for the code parameters.
Namespace:
Code parameter tree
| Name | Type | Restrictions |
|---|---|---|
| COCOS_IN | integer | Expected Cocos number in the input CPOs
|
| COCOS_OUT | integer | Requested Cocos number for the output CPOs
|
| ACHARG | FloatList | The charge of each ion species, given in atomic units. The length of this vector should be NRSPEC
|
| AD | FloatList | Coefficient for polynomial density profile
|
| AHEIGT | float | HEIGHT OF 2-D PLOTS
|
| ALARG | float | WIDTH OF 2-D PLOTS
|
| AMASS | FloatList | The mass of each ion species, given in atomic units. The length of this vector should be NRSPEC
|
| AMASSE | float | ATOMIC MASS OF ELECTRON
|
| ANGLET | FloatList | Toroidal cuts, in degrees.
|
| ANTRAD | float | ANTRAD-1.=DISTANCE ANTENNA-PLASMA
|
| ANTRADMAX | float |
|
| ANTUP | float | UPPER RIGHT POSITION OF TOP/BOTTOM ANTENNA
|
| ANU | float | COLLISIONAL DAMPING NU/OMEGA
|
| ARSIZE | float | SIZE OF ARROWS
|
| ASPCT | float | INVERSE ASPECT RATIO FOR SOLOVEV EQUILIBRIU
|
| ASYMB | float | SIZE OF SYMBOLS
|
| ATE | FloatList |
|
| ATI | FloatList |
|
| ATIP | FloatList |
|
| BNOT | float | MAGNETIC FIELD AT MAGNETIC AXIS (TESLA)
|
| CEN0 | FloatList | DENSITIES FOR CONST BETA SCAN OF DKE STAB
|
| CENDEN | FloatList | DENSITIES OF ION SPECIES AT MAGN.AXIS (M-3)
|
| CENTE | float | ELECTRON TEMPERATURE AT MAGNETIC AXIS
|
| CENTI | FloatList | ION TEMPERATURES AT MAGN.AXIS (EV)
|
| CENTIP | FloatList | PERP.ION TEMPERATURES AT MAGN. AXIS (EV)
|
| CEOMCI | FloatList | NORMALIZED ION CYCLOTRON FREQUENCIES
|
| CPSRF | float | PSI AT PLASMA SURFACE
|
| CURASY | FloatList | AMPLITUDE OF SIN ANTENNA CURRENT (HELICAL)
|
| CURSYM | FloatList | AMPLITUDE OF ANTENNA CURRENT
|
| DELTA | float | PHENOMENOLOGICAL DAMPING
|
| DELTAF | float | FREQUENCY INCREMENT FOR FREQUENCY TRACE
|
| ELLIPT | float | ELLIPTICITY SQUARED FOR SOLOVEV EQUILIBRIUM
|
| EPSMAC | float | ROUND-OFF ERROR OF COMPUTER
|
| EQALFD | float | PROFILE PARAMETER OF TOTAL MASS DENSITY
|
| EQDENS | float | PROFILE PARAMETER OF TOTAL MASS DENSITY
|
| EQFAST | float | PROFILE PARAMETER OF FAST PARTICLE DENSITY
|
| EQKAPD | float | PROFILE PARAMETER OF TOTAL MASS DENSITY
|
| EQKAPF | FloatList | PROFILE PARAMETER OF FAST PARTICLE DENSITY
|
| EQKAPT | FloatList | Parameter describing the ion temperature profile; TI(PARALLEL) = CENTI(I) * (1.-EQTI(I)*S*S) **EQKAPT(I)
|
| EQKPTE | float | PROFILE PARAMETER OF ELECTRON TEMPERATURE
|
| EQTE | float | PROFILE PARAMETER OF ELECTRON TEMPERATURE
|
| EQTI | FloatList | Parameter describing the ion temperature profiles; TI(PARALLEL) = CENTI(I) * (1.-EQTI(I)*S*S) **EQKAPT(I)
|
| FEEDUP | float | POSITION OF UPPER RIGHT FEED OF T/B ANTENNA
|
| FRAC | FloatList | MASS FRACTION OF ION SPECIES
|
| FRCEN | FloatList | CENTER OF ION DENSITY PROFILE
|
| FRDEL | FloatList | WIDTH OF ION DENSITY PROFILE
|
| FREQCY | float | FREQUENCY OF GENERATOR (HZ)
|
| OMEGA | float | NORMALIZED FREQUENCY (*RMAJOR/ALFV.SPEED)
|
| QIAXE | float | 1./Q(AXIS) FOR SOLOVEV EQUILIBRIUM
|
| RMAJOR | float | MAJOR RADIUS (M)
|
| SAMIN | float | INSIDE EDGE OF ANTENNA INSIDE PLASMA (S)
|
| SAMAX | float | OUTSIDE EDGE OF ANTENNA INSIDE PLASMA (S)
|
| SIGMA | float | NORM FACTOR FOR V-THEMAL (IONS)
|
| THANT | FloatList | THANT(J) are angles given in degrees, with values between 0 and 360. THANT(J) are measured from the magnetic axis horizontal.
|
| THANTW | float | THETA OF SADDLE COILS TOROIDAL SECTIONS
|
| TIME_ITM | FloatList | Time for slicing ITM CPO data (s).
|
| VBIRTH | float | THE BIRTH VELOCITY OF FAST PARTICLES [M/S]
|
| WALRAD | float | DISTANCE WALL-MAGNETIC AXIS IN UNITS OF THE MINOR RADIUS IN THE Z=0 PLANE.
|
| WNTDEL | float | THE TOROIDAL WAVENUMBER INCREMENT FOR TOROIDAL WN SCANS
|
| WNTORO | float | THE TOROIDAL WAVE NUMBER.
|
| LENGTH | integer | Number of elements of a matrix block
|
| MANCMP | integer | Number of poloidal wave numbers for helical antennas
|
| MEQ | integer | Equilibrium quantities (i,jchi),js=1,npsi+1 ; EQ(i,jchi,js)
|
| MFL | integer | Lower m value for fourier analysis
|
| MPOLWN | IntegerList | Poloidal wave numbers for helical antenna
|
| NANTSHEET | integer | Number of antenna current sheets.
For NANTSHEET>1, the "power at antenna" might be wrong ...
and hopefully the "power at plasma surface" is right.
The current sheets are placed equidistantly between ANTRAD and ANTRADMAX.
The current distribution as function of theta is identical for all sheets.
|
| NANTYP | integer |
The variable 'nantyp' selects the type of antenna.
(A) NANTYP=-1: "Helical volume antenna". Volume antenna currents in
the plasma between s=SAMIN and s=SAMAX, directed
along psi=const surfaces, defined by:
"j_a = grad psi x grad sigma",
with sigma(s,chi,phi) = H(s-SAMIN) * H(SAMAX-s) *
( sum[j=1..MANCMP] { CURSYM(j)*cos(MPOLWN(j)*chi)
+ CURASY(j)*sin(MPOLWN(j)*chi) } )
* exp{i*WNTORO*phi}.
Note that in this case there is no antenna in the
vacuum region: the vacuum contribution to the right-
hand side is put to zero by setting SAUTR(j) to zero.
(B) NANTYP = 1 ==== "Helical antenna". current sheet at a constant
distance of the plasma surface. The currents
are harmonic functions of the poloidal angle
theta, with poloidal wavenumbers given by
'MPOLWN(J)':
SAUTR(THETA) = SUM(J=1 TO MANCMP) OF
CURSYM(J)*COS(MPOLWN(J)*THETA) +
I*CURASY(J)*SIN(MPOLWN(J)*THETA).
There are no feeders.
(C) NANTYP = 2 ==== LFS or HFS antenna. Specified by the input
parameters THANT(J), J=1,4 and CURSYM(1).
THANT(J) ARE ANGLES GIVEN IN DEGREES, WITH VALUES
BETWEEN 0 AND 360. THANT(J) ARE MEASURED FROM THE
MAGNETIC AXIS HORIZONTAL.
THE LFS OR HFS ANTENNA IS A CURRENT SHEET WHICH,
BETWEEN THETA = THANT(2) AND THANT(3), IS AT A
CONSTANT DISTANCE OF THE PLASMA SURFACE AND
CARRIES CONSTANT PURE POLOIDAL CURRENTS :
SAUTR(THETA) = CURSYM(1)
BETWEEN THETA = THANT(1) AND THETA = THANT(2)
AND THETA = THANT(3) AND THETA = THANT(4) ARE
THE FEEDERS, WHERE THE DISTANCE FROM THE
PLASMA SURFACE INCREASES SMOOTHLY UP TO THE
WALL SURFACE.
THE LFS ANTENNA EXTENDS ACROSS THE THETA=0
LINE. THEREFORE THANT(3) < THANT(4) < THANT(1)
< THANT(2).
THE HFS ANTENNA CANNOT CROSS THE THETA=0
LINE. THEREFORE THANT(1) < THANT(2) < THANT(3)
< THANT(4).
THE SELECTION OF EITHER LFS OR HFS ANTENNA
AUTOMATIC :
THANT(3).LT.THANT(2) SELECTS LFS ANTENNA
THANT(2).GT.THANT(3) SELECTS HFS ANTENNA
NOTE THAT WE MUST HAVE THANT(1) < THANT(2)
AND THANT(3) < THANT(4).
(D) NANTYP = 3 ==== TOP/BOTTOM ANTENNA. THE ANTENNA SURFACE IS UP/
DOWN SYMMETRIC, AT CONSTANT DISTANCE OF THE
PLASMA SURFACE BETWEEN THETA = ANTUP AND
THETA = PI - ANTUP. THE CURRENTS ARE DEFINED
AS FOR NANTYP = 1.
(E) NANTYP = 4 ==== SADDLE COIL ANTENNA. THE ANTENNA SURFACE IS THE
SAME AS FOR THE HELICAL ANTENNA: CURRENT SHEET
AT A DISTANCE ANTRAD-1 OF THE PLASMA SURFACE.
THE CURRENT = CURSYM(1) IN [THANT(1),THANT(2)]
AND IN [THANT(3),THANT(4)], SMOOTHLY DECAYING
TO ZERO NEAR THANT(J).
|
| NANT_ITM | integer | 0 (default), 1 if uses antennas_in and antennas_tools to define the antenna geometry
|
| NBCASE | integer | Number of cases for the constant beta scan
|
| NBTYPE | integer | TYPE OF CONSTANT BETA SCAN:
1 == n_i(o) IS VARIED (CEN0()),
T_i(o) and T_e(o) as 1/n_i(o),
Bo is kept constant. ==> v_A(o) is varied
2 == n_i(o) IS VARIED (CEN0()),
Bo as sqrt(n_i(o)), ==> v_A(o) constant
T_i(o) and T_e(o) are kept constant
'NLTTMP': .F. ==> SWITCH OFF TTMP BY PUTTING B_PARALLEL TO 0 IN DKE
POWER EXPRESSIONS.
|
| NCHI | integer | Number of poloidal intervals all around (please note
that in LION this becomes variable NPOL, and that
NCHI is defined in lion as the number of poloidal
intervals in the upper half-plane)
|
| NCOLMN | integer | Rank of a matrix block
|
| NCONTR | integer | Number of contour lines
|
| NCUT | integer | Number of toroidal cuts for plots
|
| NDA | integer | Matrix a I/O channel
|
| NDARG | integer | Argument for polynomial density profile
|
| NDDEG | integer | Degree of polynomial density profile
|
| NDENS | integer | Selects type of density profile
|
| NDES | integer | R,Z coordinates and normals i/o channel
|
| NDLT | integer | Decomposed matrix L,D,U I/O channel
|
| NDS | integer | Solution vector
|
| NELDTTMP | integer | Type of model for Electron Landau and TTMP damping
1 ==> Additional damping term in epsilon_{perp,perp},
with k_perp from Fast Wave dispersion relation;
see WEPSEL in subroutine QUAEQU
2 ==> Additional damping term propto B_parallel,
consistent in the weak variational form;
see WEPSTTMP in subroutine QUAEQU, CONST1,2,3, etc.
Factor 1/2 for combined ELD and TTMP of fast waves
|
| NELDTTMPCOR | integer | Correction (perturbative) to electron Landau and TTMP damping diagnostics
0 (default): do not correct
1 : do the correction; option valid only for NELDTTMP=1;
WARNING: the powers will not be consistent
|
| NFAKAP | integer | Number of fast particle density profiles
|
| NHARM | integer | Maximum absolute value of the harmonic number used in constructing
the warm plasma dielectric tensor, i.e. the tensor includes components for
harmonic numbers from -NHARM to +NHARM.
|
| NPLTYP | integer | 2-D GRAPHICAL PLOTS SELECTED IN NLPL05(4):
- IF NPLTYP = 1 (DEFAULT): PREPARES PLOT FILES FOR USE
WITH THE GRAPHICAL PACKAGE BASPL:
WRITES A FILE coords (TAPE18) OF (R,Z)
COORDINATES OF MESH CELLS CENTERS AND A FILE fields
(TAPE19)
OF (R,Z) COMPONENTS OF E, POWER ABSORPTION DENSITY,
NORMAL AND BINORMAL COMPONENTS OF E, NORMAL, BINORMAL
AND PARALLEL COMPONEMTS OF B. THE
PLOTS ARE THEN DONE WITH THE GRAPHICAL PACKAGE BASPL.
IT ALLOWS TO MAKE COLOR PLOTS, ARROW PLOTS, CONTOUR
PLOTS, ... INTERACTIVELY.
- IF NPLTYP = 2 : PLOT FILE FOR USE WITH THE GRAPHICAL
PACKAGE explorer:
WRITES A FILE corfields (TAPE19) CONTAINING COORDINATES
AND FIELDS.
|
| NPOL | integer | Total number of chi intervals
|
| NPRNT | integer | Line-printer output
|
| NPSI | integer | Number of s intervals
|
| NREAD | integer | -documentation missing-
|
| NRSPEC | integer | Number of ion species
|
| NRUN | integer | The number of runs for frequency traces
|
| NSADDL | integer |
SELECTS THE TYPE OF SADDLE COIL PHASING IN THE POLOIDAL PLANE.
THIS IS DISCARDED UNLESS NANTYP = 4.
NSADDL = 0 === ONLY 1 SADDLE COIL ANTENNA IS CONNECTED:
BETWEEN THANT(1) AND THANT(2).
NSADDL = 1 === 2 SADDLE COILS ARE CONNECTED. THE CONNECTION
IS DONE IN OPPOSITE DIRECTIONS FOR THE 2
COILS, THUS DEFINING A PREDOMINANTLY 'M=1'
ANTENNA CURRENT COMPONENT: (+-) PHASING.
NSADDL = 2 === 2 SADDLE COILS ARE CONNECTED. THE CONNECTION
IS DONE IN THE SAME DIRECTION FOR THE 2
COILS, THUS DEFINING A PREDOMINANTLY 'M=2'
ANTENNA CURRENT COMPONENT: (++) PHASING.
THIS IS THE DEFAULT VALUE.
|
| NSAVE | integer | NAMELIST I/O CHANNEL
|
| NSOURC | integer | NAMELIST I/O CHANNEL
|
| NTEMP | integer |
'EQTI()', EQKAPT()', 'NTEMP':
SPECIFY THE ION PARALLEL AND PERPENDICULAR
TEMPERATURE PROFILES [EV] :
NTEMP = -2 ==> PROPORTIONAL TO SQRT(EQUILIBRIUM_PRESSURE)
TI(PARALLEL) = CENTI(I) * SQRT (P/P_AXIS)
NTEMP = -1 ==> POLYNOMIAL FUNCTION OF
S**2 IF NDARG = 1
S IF NDARG = 2
TE/TI()/TIP() = CENTE/CENTI()/CENTIP() *
(1. + SUM(J=1,NDDEG) {ATE/ATI/ATIP(J)*ARG**J})
NTEMP # -1 OR -2 ==>
TI(PARALLEL) = CENTI(I) * (1.-EQTI(I)*S*S) **EQKAPT(I)
(SUBROUTINE TEMPI)
NTEMP = -2 ==> PROPORTIONAL TO SQRT(EQUILIBRIUM_PRESSURE)
TI(PERP) = CENTIP(I) * SQRT (P/P_AXIS)
NTEMP=-1 ==> POLYNOMIAL (SEE ABOVE)
NTEMP # -2 ==>
TI(PERP) = CENTIP(I) * (1.-EQTI(I)*S*S) **EQKAPT(I)
(SUBROUTINE TEMPRP)
|
| NTORSP | integer | The number of toroidal WN's for toroidal WN scans
|
| NUMBER | integer | Run number
|
| NVERBOSE | integer | Select verbosity of output to STDOUT
|
| NVAC | integer | VACUUM QUANTITIES I/O CHANNEL
|
| NLCOLD | boolean |
Switch off electron Landau and TTMP damping of fast wave:
If .TRUE. then no additionnal term in EPSILON_PERPPERP
If .FALSE. then additionnal damping term in EPSILON_PERPPERP.
Note that the alfven wave electron landau damping rate
is evaluated as a diagnostic of the obtained solution
irrespectively of the value of NLCOLE.
|
| NLCOLE | boolean |
Switch off electron Landau and TTMP damping of fast wave.
If .TRUE. then no additionnal term in EPSILON_PERPPERP
If .FALSE. then additionnal damping term in EPSILON_PERPPERP.
Note that the alfven wave electron landau damping rate
is evaluated as a diagnostic of the obtained solution
irrespectively of the value of NLCOLE.
|
| NLDIP | boolean | Selects monopole or dipole antenna. the dipole option has not been programmed yet. DEFAULT: FALSE , i.e. monopole.
|
| NLDISO | boolean |
Switch computation and diagnostics of the solution.
If NLDISO=.TRUE. then the solution is computed everywhere.
Diagnostics are performed, printed and/or
plotted according to NLOTP5() and NLPLO5()
(see below).
With this option (which is the default)
running the LION code requires scratch
disk space for matrix storage:
96 * NPSI * NPOL**2 (bytes)
If NLDISO=.FALSE. then the solution is computed only at the plasma-vacuum interface.
The only diagnostic is the total power,
which is permanent output. It is correct
as long as there is no source inside the
plasma.
No other diagnostics are perfomed, irrespectively of NLOTP5() and NLPLO5().
With this option the lion code does not
use disk space for matrix storage, therefore
the turnaround time is reduced.
|
| NLPHAS | boolean | Switch poloidal phase extraction
|
| NLFAST | boolean | If TRUE, then introduce fast particles
|
| NLOTP0 | boolean | General switch for line-printer output and graphics
|
| NLOTP1 | BooleanList | LINE-PRINTER OUTPUT FOR EQUILIBRIUM QUANTITIES (LION1); LENGTH 5.
|
| NLOTP2 | BooleanList |
LINE-PRINTER OUTPUT FOR VACUUM QUANTITIES (LION2).
(1) : GEOMETRICAL QUANTITIES AT PLASMA SURFACE.
(2) : POSITIONS OF PLASMA SURFACE, ANTENNA AND WALL.
(3) : ANTENNA CURRENT POTENTIAL VS CHI AND THETA.
(4) : NON-HERMICITY OF VACUUM MATRIX.
(5) :
|
| NLOTP3 | BooleanList | LINE-PRINTER OUTPUT FOR MATRIX CONSTRUCTION (LION3). LENGTH 2.
|
| NLOTP4 | BooleanList |
LINE-PRINTER OUTPUT FOR MATRIX SOLVER (LION4).
(1) : NAMELIST
(2) : OHM-VECTOR
(3) : SOLUTION AT PLASMA BOUNDARY
(4) :
(5) :
|
| NLOTP5 | BooleanList |
LINE-PRINTER OUTPUT FOR SOLUTION DIAGNOSTICS (LION5).
(1) : NAMELIST
(2) : RADIAL POWER ABSORPTIONS AND OTHER DIAGNOSTICS
(3) : EXTENDED OUTPUT OF RADIAL DIAGNOSTICS
(4) : 2-D POWER ABSORPTION DENSITY
(5) : 2-D POWER ABSORBED IN EACH CELL
(6) : 2-D NORMAL COMPONENT OF POYNTING
(7) : 2-D PERP COMPONENT OF POYNTING
(8) : 2-D PARALLEL COMPONENT OF POYNTING
(9) :
(10) : 2-D REAL PART OF E-NORMAL
(11) : 2-D REAL PART OF E-PERP
(12) : 2-D IMAGINARY PART OF E-NORMAL
(13) : 2-D IMAGINARY PART OF E-PERP
(14) : 2-D POLARAZATION NORM OF E-PLUS SQUARED
(15) : 2-D POLARIZATION NORM OF E-MINUS SQUARED
(16) : ELECTRIC FIELD ON OUTER EQUATORIAL PLANE (CHI=0)
(17) :
(18) : POLOIDAL FOURIER COMPONENTS OF E-NORMAL IN THETA
FOR M = 'MFL', MFL+1, .., MFU(=MFL+MD2FP1-1)
(19) : POLOIDAL FOURIER COMPONENTS OF E-PERP IN THETA
(20) : POLOIDAL FOURIER COMPONENTS OF E-NORMAL IN CHI
(21) : POLOIDAL FOURIER COMPONENTS OF E-PERP IN CHI
(22) : 2-D EPSILON SUB-N-N - N**2 / R**2
(23) : 2-D IMAGINARY PART OF EPSILON SUB N-N
(24) : 2-D OMEGA - OMEGACI
(25) : SHEAR ALFVEN FREQUENCIES (NEGLECTING TOROIDAL
COUPLING; FOR SINGLE SPECIES PLASMA ONLY),
FOR M = 'MFL', MFL+1, .., MFU(=MFL+MD2FP1-1)
(26) : DENSITY, MINOR AND MAJOR RADIUS, IN NORMALISED AND
S.I. UNITS, ON THE OUTER EQUATORIAL PLANE (CHI=0).
(31) : POLOIDAL FOURIER COMPONENTS OF B_N IN THETA
FOR M = 'MFL', MFL+1, .., MFU(=MFL+MD2FP1-1)
(32) : POLOIDAL FOURIER COMPONENTS OF B_B IN THETA
(33) : POLOIDAL FOURIER COMPONENTS OF B_PAR IN THETA
(34) : POLOIDAL FOURIER COMPONENTS OF B_N IN CHI
(35) : POLOIDAL FOURIER COMPONENTS OF B_B IN CHI
(36) : POLOIDAL FOURIER COMPONENTS OF B_PAR IN CHI
THE 2-D TABLES GIVE THE VALUES ON THE CENTERS OF THE CELLS
OF THE (S,CHI) MESH. A LINE IN THE TABLE CORRESPONDS TO A PSI =
CONST SURFACE. IT GOES FROM CHI=0 TO CHI=PI IN THE UPPER HALF-PLANE
AND FROM CHI=PI TO CHI=2*PI IN THE LOWER HALF-PLANE. THE VALUES
ARE NORMALIZED TO THEIR MAXIMUM VALUE. THE FIRST AND THE LAST LINES
OF THE TABLES GIVE THE POLOIDAL NUMBERING OF THE CELLS. THE FIRST
COLUMN GIVES THE RADIAL NUMBERING OF THE CELLS. ALL OUTPUT IS IN
CODE-NORMALIZED UNITS UNLESS SPECIFIED.
|
| NLPLO5 | BooleanList |
GRAPHICAL OUTPUT FOR LION5
(1) : GENERAL SWITCH FOR GRAPHICAL PLOTS
(2) : RADIAL POWER ABSORPTION AND FLUX
(3) : FAST ION BETA_CRITICAL AND P_DK(S). WRITES TABLES
ON TAPE26 AND TAPE27
=> MATLAB (plotfast.m AND plotpdks(.,.).m)
(4) : 2-D GRAPHICAL PLOTS :
- IF NPLTYP = 1 (DEFAULT): PREPARES PLOT FILES FOR USE
WITH THE GRAPHICAL PACKAGE BASPL:
WRITES A FILE coords (TAPE18) OF (R,Z)
COORDINATES OF MESH CELLS CENTERS AND A FILE fields
(TAPE19)
OF (R,Z) COMPONENTS OF E, POWER ABSORPTION DENSITY,
NORMAL AND BINORMAL COMPONENTS OF E, NORMAL, BINORMAL
AND PARALLEL COMPONEMTS OF B. THE
PLOTS ARE THEN DONE WITH THE GRAPHICAL PACKAGE BASPL.
IT ALLOWS TO MAKE COLOR PLOTS, ARROW PLOTS, CONTOUR
PLOTS, ... INTERACTIVELY.
- IF NPLTYP = 2 : PLOT FILE FOR USE WITH THE GRAPHICAL
PACKAGE explorer:
WRITES A FILE corfields (TAPE19) CONTAINING COORDINATES
AND FIELDS.
(5) : POLOIDAL FOURIER COMPONENTS (CABS) OF E_n, E_b, B_n,
B_b AND B_//. WRITES A TABLE ON TAPE25 =>
=> MATLAB (plotfour.m).
|
| NLTTMP | boolean | Switch on/off TTMP by putting B_parallel to 0 in DKE power expressions.
|
| NITMOPT | integer | Uses ITM database: 0 (default) = no, 1 =reads from ITM, 10=writes on ITM, 11=reads and writes, 22=LION run as module within Kepler
|
| NITMRUN | IntegerList | ITM run number
|
| NITMSHOT | IntegerList | ITM shot number
|
Locally defined types
| Name | Type | Descriptions |
|---|---|---|
| IntegerList | integer | |
| FloatList | float | |
| BooleanList | boolean |
last update: 2015-08-07 by dpc