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gray/src/gray_core.f90

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src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
! This modules contains the core GRAY routines
src/graycore.f90 -> src/gray_core.f90 Rename for consistency with other modules.
2021-12-15 02:31:14 +01:00
module gray_core
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
use const_and_precisions, only : wp_
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
implicit none
contains
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
subroutine gray_main(params, data, results, error, rhout)
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
use const_and_precisions, only : zero, one, degree, comp_tiny
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
use coreprofiles, only : temp, fzeff
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
use dispersion, only : expinit
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
use gray_params, only : gray_parameters, gray_data, gray_results, &
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
print_parameters
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
use beams, only : xgygcoeff, launchangles2n
use beamdata, only : pweight, rayi2jk
improve error handling in the gray_main routine - rename errocodes → gray_errors - restructure the errors into a `error_spec` type - make the list of errors easily extensible - rewrite the `print_errn`, `print_errhcd` (now `print_err_raytracing`, `print_err_ecrh_cd`) subroutine to handle arbitrary errors - add functions to easily manipulate errors (`raise_error`, `has_error`, `is_critical`) - remove print statements from quadpack - log all errors to stderr using the logger module
2022-07-14 00:38:34 +02:00
use gray_errors, only : is_critical, print_err_raytracing, print_err_ecrh_cd
fixed incompatibilities with allocatable arrays (pgf90 compiler, JETTO); fixed input/output scaling (gray/jetto interface); fixed error in read_beams2 for small beam tables
2016-06-01 15:49:35 +02:00
use magsurf_data, only : flux_average, dealloc_surfvec
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
use beamdata, only : init_btr, dealloc_beam
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
use pec, only : pec_init, spec, postproc_profiles, dealloc_pec, &
rhop_tab, rhot_tab
use utils, only : vmaxmin
use reflections, only : inside
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
use multipass, only : alloc_multipass, dealloc_multipass, initbeam, &
initmultipass, turnoffray, plasma_in, plasma_out, &
wall_out
src: use the logging system everywhere
2021-12-18 18:57:38 +01:00
use logger, only : log_info, log_debug
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
implicit none
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
! subroutine arguments
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
type(gray_parameters), intent(inout) :: params
type(gray_data), intent(in) :: data
type(gray_results), intent(out) :: results
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
! Predefined grid for the output profiles (optional)
gray/jetto interface reverted to F77 (removed use of modules), adding an intermediate F90 subroutine handling the reading of parameters/beams files. pec_init now uses optional input rho grid
2015-11-24 17:36:20 +01:00
real(wp_), dimension(:), intent(in), optional :: rhout
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
! Exit code
integer, intent(out) :: error
! local variables
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
real(wp_), parameter :: taucr = 12._wp_, etaucr = exp(-taucr)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
character, dimension(2), parameter :: mode=['O','X']
src: use the logging system everywhere
2021-12-18 18:57:38 +01:00
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
integer :: sox
real(wp_) :: ak0,bres,xgcn,xg,yg,rrm,zzm,alpha,didp,anpl,anpr,anprim,anprre
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
real(wp_) :: chipol,psipol,btot,psinv,dens,tekev,dersdst,derdnm
* reduced arrays required for dI/ds,dP/ds integration * new module for error handling * input parameters collected in a single file * fixed uninitialized pabs,icd
2015-11-19 19:20:58 +01:00
real(wp_) :: tau,pow,dids,ddr,ddi,taumn,taumx
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
real(wp_) :: rhotpav,drhotpav,rhotjava,drhotjava,dpdvp,jphip
real(wp_) :: rhotp,drhotp,rhotj,drhotj,dpdvmx,jphimx,ratjamx,ratjbmx
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
real(wp_) :: pabs_beam,icd_beam,cpl_beam1,cpl_beam2,cpl_cbeam1,cpl_cbeam2
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
real(wp_), dimension(2) :: pabs_pass,icd_pass,cpl,cpl0
added further output prints to fort.4
2017-09-12 21:37:06 +02:00
real(wp_), dimension(3) :: xv,anv0,anv,bv,derxg
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
! Ray variables
real(wp_), dimension(:,:), pointer :: yw=>null(),ypw=>null(),gri=>null()
fixed incompatibilities with allocatable arrays (pgf90 compiler, JETTO); fixed input/output scaling (gray/jetto interface); fixed error in read_beams2 for small beam tables
2016-06-01 15:49:35 +02:00
real(wp_), dimension(:,:,:), pointer :: xc=>null(),du1=>null(),ggri=>null()
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
! i: integration step, jk: global ray index
integer :: i, jk
improve error handling in the gray_main routine - rename errocodes → gray_errors - restructure the errors into a `error_spec` type - make the list of errors easily extensible - rewrite the `print_errn`, `print_errhcd` (now `print_err_raytracing`, `print_err_ecrh_cd`) subroutine to handle arbitrary errors - add functions to easily manipulate errors (`raise_error`, `has_error`, `is_critical`) - remove print statements from quadpack - log all errors to stderr using the logger module
2022-07-14 00:38:34 +02:00
integer :: iox,nharm,nhf,nnd,iokhawa,ierrn,ierrhcd,index_rt
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
integer :: ip,ib,iopmin,ipar,iO
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
integer :: igrad_b,istop_pass,nbeam_pass,nlim
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
logical :: ins_pl,ins_wl,ent_pl,ext_pl,ent_wl,ext_wl,iboff
real(wp_), dimension(:,:,:), pointer :: yynext=>null(),yypnext=>null()
real(wp_), dimension(:,:), pointer :: psjki=>null(),ppabs=>null(),ccci=>null()
real(wp_), dimension(:,:), pointer :: taus=>null(),stnext=>null(), &
yw0=>null(),ypw0=>null(),cpls=>null()
real(wp_), dimension(:), pointer :: p0ray=>null(),tau0=>null(),alphaabs0=>null(), &
dids0=>null(),ccci0=>null(),tau1=>null(),etau1=>null(),cpl1=>null(),lgcpl1=>null()
real(wp_), dimension(:), pointer :: p0jk=>null()
real(wp_), dimension(:), pointer :: jphi_beam=>null(),pins_beam=>null(), &
currins_beam=>null(), dpdv_beam=>null(),jcd_beam=>null(),stv=>null(), &
psipv=>null(),chipv=>null()
complex(wp_), dimension(:), pointer :: ext=>null(), eyt=>null()
integer, dimension(:), pointer :: iiv=>null(),iop=>null(),iow=>null()
logical, dimension(:), pointer :: iwait=>null()
logical, dimension(:,:), pointer :: iroff=>null()
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
src: use the logging system everywhere
2021-12-18 18:57:38 +01:00
! buffer for formatting log messages
character(256) :: msg
added file headers with input parameters
2016-04-27 16:37:57 +02:00
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
! ======== set environment BEGIN ========
! Number of limiter contourn points
nlim = size(data%equilibrium%zlim)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
! Compute X=ω/ω_ce and Y=(ω/ω_pe)² (with B=1)
call xgygcoeff(params%antenna%fghz, ak0, bres, xgcn)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
! Compute the initial cartesian wavevector (anv0)
src/beams.f90: document read_beam{0,1} formats
2023-03-26 16:03:57 +02:00
! from launch angles α,β and the position
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
call launchangles2n(params%antenna, anv0)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
! Initialise the ray variables (beamtracing)
call init_btr(params%raytracing, yw, ypw, xc, du1, gri, ggri, psjki, ppabs, ccci, &
tau0, alphaabs0, dids0, ccci0, p0jk, ext, eyt, iiv)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
! Initialise the dispersion module
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
if(params%ecrh_cd%iwarm > 1) call expinit
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
! Initialise the magsurf_data module
call flux_average ! requires frhotor for dadrhot,dvdrhot
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
! Initialise the output profiles
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
call pec_init(params%output%ipec, rhout)
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
nnd = size(rhop_tab) ! number of radial profile points
call alloc_multipass(nnd, iwait, iroff, iop, iow, yynext, yypnext, yw0, ypw0, stnext, &
stv, p0ray, taus, tau1, etau1, cpls, cpl1, lgcpl1, jphi_beam, &
pins_beam, currins_beam, dpdv_beam, jcd_beam, psipv, chipv)
! Allocate memory for the results...
allocate(results%dpdv(params%output%nrho))
allocate(results%jcd(params%output%nrho))
! ...and initialise them
results%pabs = zero
results%icd = zero
results%dpdv = zero
results%jcd = zero
! ========= set environment END =========
! ======== pre-proc prints BEGIN ========
skip print_headers with no active units
2022-05-03 23:16:21 +02:00
call print_headers(params)
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
src: use the logging system everywhere
2021-12-18 18:57:38 +01:00
! print ψ surface for q=1.5 and q=2 on file and log psi,rhot,rhop
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
call print_surfq([1.5_wp_, 2.0_wp_])
! print initial position
src: use the logging system everywhere
2021-12-18 18:57:38 +01:00
write (msg, '("initial position:",3(x,g0.3))') params%antenna%pos
call log_info(msg, mod='gray_core', proc='gray_main')
write (msg, '("initial direction:",2(x,a,"=",g0.2))') &
'α', params%antenna%alpha, 'β', params%antenna%beta
call log_info(msg, mod='gray_core', proc='gray_main')
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
! print Btot=Bres
! print ne, Te, q, Jphi versus psi, rhop, rhot
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
call print_bres(bres)
src/gray_core.f90: print profiles up to ψ_bnd
2023-05-23 17:49:51 +02:00
call print_prof(params%profiles)
src: use hypot and norm2 when possible
2021-12-19 02:35:24 +01:00
call print_maps(bres, xgcn, &
norm2(params%antenna%pos(1:2)) * 0.01_wp_, &
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
sin(params%antenna%beta*degree))
! ========= pre-proc prints END =========
! =========== main loop BEGIN ===========
call initmultipass(params%raytracing%ipol, params%antenna%iox, &
iroff,yynext,yypnext,yw0,ypw0, &
stnext,p0ray,taus,tau1,etau1,cpls,cpl1,lgcpl1,psipv,chipv)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
if(params%raytracing%ipol == 0) then
if(params%antenna%iox == 2) then ! only X mode on 1st pass
cpl0 = [zero, one]
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
else ! only O mode on 1st pass
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
cpl0 = [one, zero]
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
end if
end if
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
sox=1 ! mode inverted for each beam
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
iox=2 ! start with O: sox=-1, iox=1
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
psipol = params%antenna%psi
chipol = params%antenna%chi
call pweight(params%antenna%power, p0jk)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
nbeam_pass=1 ! max n of beam per pass
index_rt=0 ! global beam index: 1,O 2,X 1st pass
trunk/graycore: minor fixes
2019-03-28 10:50:28 +01:00
! | | | |
src: use the logging system everywhere
2021-12-18 18:57:38 +01:00
call log_debug('pass loop start', mod='gray_core', proc='gray_main') ! 3,O 4,X 5,O 6,X 2nd pass
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
main_loop: do ip=1,params%raytracing%ipass
src: use the logging system everywhere
2021-12-18 18:57:38 +01:00
write (msg, '("pass: ",g0)') ip
call log_info(msg, mod='gray_core', proc='gray_main')
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
pabs_pass = zero
icd_pass = zero
istop_pass = 0 ! stop flag for current pass
nbeam_pass = 2*nbeam_pass ! max n of beams in current pass
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
if(ip > 1) then
trunk/graycore: minor fixes
2019-03-28 10:50:28 +01:00
du1 = zero
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
gri = zero
ggri = zero
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
if(ip == params%raytracing%ipass) cpl = [zero, zero] ! no successive passes
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
end if
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! =========== beam loop BEGIN ===========
src: use the logging system everywhere
2021-12-18 18:57:38 +01:00
call log_debug('beam loop start', mod='gray_core', proc='gray_main')
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
beam_loop: do ib=1,nbeam_pass
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
sox = -sox ! invert mode
iox = 3-iox ! O-mode at ip=1,ib=1
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
index_rt = index_rt +1
iO = 2*index_rt +1 ! * index_rt of O-mode derived ray (iX=iO+1)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
call initbeam(index_rt,iroff,iboff,iwait,stv,jphi_beam, &
pins_beam,currins_beam,dpdv_beam,jcd_beam)
src: use the logging system everywhere
2021-12-18 18:57:38 +01:00
write(msg, '(" beam: ",g0," (",a1," mode)")') index_rt, mode(iox)
call log_info(msg, mod='gray_core', proc='gray_main')
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
if(iboff) then ! no propagation for current beam
istop_pass = istop_pass +1 ! * +1 non propagating beam
src: use the logging system everywhere
2021-12-18 18:57:38 +01:00
call log_info(" beam is off", mod='gray_core', proc='gray_main')
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
cycle
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
end if
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
call vectinit(psjki,ppabs,ccci,tau0,alphaabs0,dids0,ccci0,iiv)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
if(ip == 1) then ! 1st pass
igrad_b = params%raytracing%igrad ! * input value, igrad_b=0 from 2nd pass
trunk/graycore: minor fixes
2019-03-28 10:50:28 +01:00
tau1 = zero ! * tau from previous passes
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
etau1 = one
trunk/graycore: minor fixes
2019-03-28 10:50:28 +01:00
cpl1 = one ! * coupling from previous passes
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
lgcpl1 = zero
p0ray = p0jk ! * initial beam power
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
call ic_gb(params, anv0, ak0, yw, ypw, & ! * initial conditions
xc, du1, gri, ggri, index_rt)
call set_pol(yw, bres, sox, params%raytracing%ipol, & ! * initial polarization
psipol, chipol, ext, eyt)
do jk=1,params%raytracing%nray
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
zzm = yw(3,jk)*0.01_wp_
rrm = sqrt(yw(1,jk)*yw(1,jk)+yw(2,jk)*yw(2,jk))*0.01_wp_
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
if(inside(data%equilibrium%rlim, data%equilibrium%zlim, &
nlim, rrm, zzm)) then ! * start propagation in/outside vessel?
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
iow(jk) = 1 ! + inside
else
iow(jk) = 0 ! + outside
end if
end do
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
trunk/graycore: minor fixes
2019-03-28 10:50:28 +01:00
else ! 2nd+ passes
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
ipar = (index_rt+1)/2-1 ! * parent beam index
yw = yynext(:,:,ipar) ! * starting coordinates from
ypw = yypnext(:,:,ipar) ! parent beam last step
stv = stnext(:,ipar) ! * starting step from parent beam last step
iow = 1 ! * start propagation inside vessel
tau1 = taus(:,index_rt) ! * tau from previous passes
etau1 = exp(-tau1)
cpl1 = cpls(:,index_rt) ! * coupling from previous passes
lgcpl1 = -log(cpl1)
p0ray = p0jk * etau1 * cpl1 ! * initial beam power
end if
iop = 0 ! start propagation outside plasma
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
if(params%raytracing%nray>1 .and. all(.not.iwait)) & ! iproj=0 ==> nfilp=8
call print_projxyzt(stv,yw,0)
! ======= propagation loop BEGIN =======
src: use the logging system everywhere
2021-12-18 18:57:38 +01:00
call log_debug(' propagation loop start', mod='gray_core', proc='gray_main')
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
propagation_loop: do i=1,params%raytracing%nstep
! advance one step with "frozen" grad(S_I)
do jk=1,params%raytracing%nray
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
if(iwait(jk)) cycle ! jk ray is waiting for next pass
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
stv(jk) = stv(jk) + params%raytracing%dst ! current ray step
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
call rkstep(sox,bres,xgcn,yw(:,jk),ypw(:,jk),gri(:,jk),ggri(:,:,jk),igrad_b)
end do
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! update position and grad
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
if(igrad_b == 1) call gradi_upd(yw,ak0,xc,du1,gri,ggri)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
error = 0
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
iopmin = 10
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! =========== rays loop BEGIN ===========
rays_loop: do jk=1,params%raytracing%nray
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
if(iwait(jk)) cycle ! jk ray is waiting for next pass
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! compute derivatives with updated gradient and local plasma values
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
xv = yw(1:3,jk)
anv = yw(4:6,jk)
call ywppla_upd(xv,anv,gri(:,jk),ggri(:,:,jk),sox,bres,xgcn,ypw(:,jk), &
psinv,dens,btot,bv,xg,yg,derxg,anpl,anpr,ddr,ddi,dersdst,derdnm, &
ierrn,igrad_b)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! update global error code and print message
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
if(ierrn/=0) then
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
error = ior(error,ierrn)
improve error handling in the gray_main routine - rename errocodes → gray_errors - restructure the errors into a `error_spec` type - make the list of errors easily extensible - rewrite the `print_errn`, `print_errhcd` (now `print_err_raytracing`, `print_err_ecrh_cd`) subroutine to handle arbitrary errors - add functions to easily manipulate errors (`raise_error`, `has_error`, `is_critical`) - remove print statements from quadpack - log all errors to stderr using the logger module
2022-07-14 00:38:34 +02:00
call print_err_raytracing(ierrn, i, anpl)
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
end if
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! check entrance/exit plasma/wall
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
zzm = xv(3)*0.01_wp_
rrm = sqrt(xv(1)*xv(1)+xv(2)*xv(2))*0.01_wp_
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
ins_pl = (psinv>=zero .and. psinv<params%profiles%psnbnd) ! in/out plasma?
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
ins_wl = inside(data%equilibrium%rlim, data%equilibrium%zlim, &
nlim,rrm,zzm) ! in/out vessel?
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
ent_pl = (mod(iop(jk),2) == 0 .and. ins_pl) ! enter plasma
ext_pl = (mod(iop(jk),2) == 1 .and. .not.ins_pl) ! exit plasma
ent_wl = (mod(iow(jk),2) == 0 .and. ins_wl) ! enter vessel
ext_wl = (mod(iow(jk),2) == 1 .and. .not.ins_wl) ! exit vessel
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
if(ent_pl) then ! ray enters plasma
add some useful debug messages
2022-05-26 02:33:55 +02:00
write (msg, '(" ray ",g0," entered plasma (",g0," steps)")') jk, i
call log_debug(msg, mod='gray_core', proc='gray_main')
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
call plasma_in(jk,xv,anv,bres,sox,cpl,psipol,chipol,iop,ext,eyt)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
if(iop(jk) == 1 .and. ip==1) then ! * 1st entrance on 1st pass (ray hasn't entered in plasma yet) => continue current pass
if(params%raytracing%ipol == 0) then ! + IF single mode propagation
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
cpl = cpl0
p0ray(jk) = p0ray(jk)*cpl(iox)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
else if(cpl(iox) < etaucr) then ! + ELSE IF low coupled power for current mode => de-activate derived rays
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
call turnoffray(jk,ip+1,2*ib+2-iox,iroff)
iwait(jk) = .true. ! . stop advancement and H&CD computation for current ray
if(cpl(iox).le.comp_tiny) cpl(iox)=etaucr
else ! + ELSE assign coupled power to current ray
p0ray(jk) = p0ray(jk)*cpl(iox)
end if
cpls(jk,index_rt) = cpl(iox)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
if(jk == 1) then
src: use the logging system everywhere
2021-12-18 18:57:38 +01:00
write (msg,'(" 1st pass - central ray (",a1,"-mode) c=",g0.4)') &
mode(iox), cpl(iox)
call log_info(msg, mod='gray_core', proc='gray_main')
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
psipv(index_rt) = psipol ! + polarization angles at plasma boundary for central ray
chipv(index_rt) = chipol
end if
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
else if(iop(jk) > 2) then ! * 2nd entrance on 1st pass / entrance on 2nd+ pass => end of current pass for ray jk
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
igrad_b = 0 ! + switch to ray-tracing
iwait(jk) = .true. ! + stop advancement and H&CD computation for current ray
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
if(ip < params%raytracing%ipass) then ! + not last pass
trunk/graycore: minor fixes
2019-03-28 10:50:28 +01:00
yynext(:,jk,index_rt) = yw0(:,jk) ! . copy starting coordinates
yypnext(:,jk,index_rt) = ypw0(:,jk) ! for next pass from last step
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
stnext(jk,index_rt) = stv(jk) - params%raytracing%dst ! . starting step for next pass = last step
if(cpl(1) < etaucr) then ! . low coupled power for O-mode => de-activate derived rays
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
call turnoffray(jk,ip+1,2*ib-1,iroff)
if(cpl(1).le.comp_tiny) cpl(1)=etaucr
end if
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
if(cpl(2) < etaucr) then ! . low coupled power for X-mode => de-activate derived rays
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
call turnoffray(jk,ip+1,2*ib,iroff)
if(cpl(2).le.comp_tiny) cpl(2)=etaucr
end if
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
trunk/graycore: minor fixes
2019-03-28 10:50:28 +01:00
taus(jk,iO:iO+1) = tau1(jk) + tau0(jk) ! . starting tau for next O-mode pass
cpls(jk,iO) = cpl1(jk) * cpl(1) ! . cumulative coupling for next O-mode pass
cpls(jk,iO+1) = cpl1(jk) * cpl(2) ! . cumulative coupling for next X-mode pass
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
if(jk == 1) then ! . polarization angles at plasma boundary for central ray
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
psipv(iO:iO+1) = psipol
chipv(iO:iO+1) = chipol
end if
trunk/graycore: minor fixes
2019-03-28 10:50:28 +01:00
else ! * 1st entrance on 2nd+ pass (ray hasn't entered in plasma since end of previous pass) => continue current pass
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
cpl = [zero, zero]
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
end if
end if
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
else if(ext_pl) then ! ray exits plasma
add some useful debug messages
2022-05-26 02:33:55 +02:00
write (msg, '(" ray ", g0, " left plasma")') jk
call log_debug(msg, mod='gray_core', proc='gray_main')
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
call plasma_out(jk,xv,anv,bres,sox,iop,ext,eyt)
end if
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
if(ent_wl) then ! ray enters vessel
trunk/graycore: minor fixes
2019-03-28 10:50:28 +01:00
iow(jk)=iow(jk)+1 ! * out->in
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
else if(ext_wl) then ! ray exit vessel
call wall_out(jk,ins_pl,xv,anv,bres,sox,psipol,chipol,iow,iop,ext,eyt)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
yw(:,jk) = [xv, anv] ! * updated coordinates (reflected)
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
igrad_b = 0 ! * switch to ray-tracing
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
call ywppla_upd(xv,anv,gri(:,jk),ggri(:,:,jk),sox,bres,xgcn,ypw(:,jk), &
psinv,dens,btot,bv,xg,yg,derxg,anpl,anpr,ddr,ddi,dersdst,derdnm, &
ierrn,igrad_b) ! * update derivatives after reflection
if(ierrn/=0) then ! * update global error code and print message
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
error = ior(error,ierrn)
improve error handling in the gray_main routine - rename errocodes → gray_errors - restructure the errors into a `error_spec` type - make the list of errors easily extensible - rewrite the `print_errn`, `print_errhcd` (now `print_err_raytracing`, `print_err_ecrh_cd`) subroutine to handle arbitrary errors - add functions to easily manipulate errors (`raise_error`, `has_error`, `is_critical`) - remove print statements from quadpack - log all errors to stderr using the logger module
2022-07-14 00:38:34 +02:00
call print_err_raytracing(ierrn, i, anpl)
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
end if
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
if(jk == 1 .and. ip == 1) then ! * 1st pass, polarization angles at reflection for central ray
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
psipv(index_rt) = psipol
chipv(index_rt) = chipol
end if
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
trunk/graycore: minor fixes
2019-03-28 10:50:28 +01:00
if(ins_pl) then ! * plasma-wall overlapping => wall+plasma crossing => end of current pass
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
iwait(jk) = .true. ! + stop advancement and H&CD computation for current ray
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
if(ip < params%raytracing%ipass) then ! + not last pass
yynext(:,jk,index_rt) = [xv, anv] ! . starting coordinates
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
yypnext(:,jk,index_rt) = ypw(:,jk) ! for next pass = reflection point
stnext(jk,index_rt) = stv(jk) ! . starting step for next pass = step after reflection
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
call plasma_in(jk,xv,anv,bres,sox,cpl,psipol,chipol,iop,ext,eyt) ! . ray re-enters plasma after reflection
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
if(cpl(1) < etaucr) then ! . low coupled power for O-mode? => de-activate derived rays
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
call turnoffray(jk,ip+1,2*ib-1,iroff)
if(cpl(1).le.comp_tiny) cpl(1)=etaucr
end if
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
if(cpl(2) < etaucr) then ! . low coupled power for X-mode? => de-activate derived rays
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
call turnoffray(jk,ip+1,2*ib,iroff)
if(cpl(2).le.comp_tiny) cpl(2)=etaucr
end if
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
taus(jk,iO:iO+1) = tau1(jk) + tau0(jk) ! . starting tau for next O-mode pass
cpls(jk,iO) = cpl1(jk) * cpl(1) ! . cumulative coupling for next O-mode pass
cpls(jk,iO+1) = cpl1(jk) * cpl(2) ! . cumulative coupling for next X-mode pass
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
if(jk == 1) then ! + polarization angles at plasma boundary for central ray
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
psipv(iO:iO+1) = psipol
chipv(iO:iO+1) = chipol
end if
end if
end if
end if
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
iopmin = min(iopmin,iop(jk))
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
if(ip < params%raytracing%ipass) then ! not last pass
trunk/graycore: minor fixes
2019-03-28 10:50:28 +01:00
yw0(:,jk) = yw(:,jk) ! * store current coordinates in case
ypw0(:,jk) = ypw(:,jk) ! current pass ends on next step
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
end if
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! Compute ECRH&CD if (inside plasma & power available>0 & ray still active)
! Note: power check is τ + τ₀ + log(coupling O/X) < τ_critic
if(ierrn==0 .and. params%ecrh_cd%iwarm>0 .and. ins_pl .and. &
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
(tau1(jk)+tau0(jk)+lgcpl1(jk))<=taucr .and. .not.iwait(jk)) then ! H&CD computation check
tekev=temp(psinv)
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
block
complex(wp_) :: Npr_warm
call alpha_effj(params%ecrh_cd, psinv, xg, yg, dens, tekev, &
ak0, bres, derdnm, anpl, anpr, sox, Npr_warm, &
alpha, didp, nharm, nhf, iokhawa, ierrhcd)
anprre = Npr_warm%re
anprim = Npr_warm%im
improve error handling in the gray_main routine - rename errocodes → gray_errors - restructure the errors into a `error_spec` type - make the list of errors easily extensible - rewrite the `print_errn`, `print_errhcd` (now `print_err_raytracing`, `print_err_ecrh_cd`) subroutine to handle arbitrary errors - add functions to easily manipulate errors (`raise_error`, `has_error`, `is_critical`) - remove print statements from quadpack - log all errors to stderr using the logger module
2022-07-14 00:38:34 +02:00
if(ierrhcd /= 0) then
error = ior(error, ierrhcd)
call print_err_ecrh_cd(ierrhcd, i, Npr_warm, alpha)
end if
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
end block
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
else
tekev=zero
alpha=zero
didp=zero
anprim=zero
anprre=anpr
nharm=0
nhf=0
iokhawa=0
end if
if(nharm>0) iiv(jk)=i
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
psjki(jk,i) = psinv
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! Computation of the ray τ, dP/ds, P(s), dI/ds, I(s)
! optical depth: τ = ∫α(s)ds using the trapezoid rule
tau = tau0(jk) + 0.5_wp_*(alphaabs0(jk) + alpha) * dersdst * params%raytracing%dst
pow = p0ray(jk) * exp(-tau) ! residual power: P = P₀exp(-τ)
ppabs(jk,i) = p0ray(jk) - pow ! absorbed power: P_abs = P₀ - P
improve some comments
2023-03-29 11:19:00 +02:00
dids = didp * pow * alpha ! current driven: dI/ds = dI/dP⋅dP/ds = dI/dP⋅P⋅α
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! current: I = ∫dI/ds⋅ds using the trapezoid rule
ccci(jk,i) = ccci0(jk) + 0.5_wp_*(dids0(jk) + dids) * dersdst * params%raytracing%dst
tau0(jk) = tau
alphaabs0(jk) = alpha
dids0(jk) = dids
ccci0(jk) = ccci(jk,i)
trunk/graycore: minor fixes
2019-03-28 10:50:28 +01:00
if(iwait(jk)) then ! copy values from last pass for inactive ray
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
ppabs(jk,i:params%raytracing%nstep) = ppabs(jk,i-1)
ccci(jk,i:params%raytracing%nstep) = ccci(jk,i-1)
psjki(jk,i:params%raytracing%nstep) = psjki(jk,i-1)
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
else
updated makefile, added manpage, fixed few print statements
2019-12-09 15:49:37 +01:00
call print_output(i,jk,stv(jk),p0ray(jk),xv,psinv, &
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
btot,bv,ak0,anpl,anpr,anv,anprim,dens,tekev,alpha,tau,dids, &
trunk/graycore: minor fixes
2019-03-28 10:50:28 +01:00
nharm,nhf,iokhawa,index_rt,ddr,ddi,xg,yg,derxg) ! p0ray/etau1 [dids normalization] = fraction of p0 coupled to this ray (not including absorption from previous passes)
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
end if
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
end do rays_loop
! ============ rays loop END ============
if(i==params%raytracing%nstep) then ! step limit reached?
do jk=1,params%raytracing%nray
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
if(iop(jk)<3) call turnoffray(jk,ip,ib,iroff) ! * ray hasn't exited+reentered the plasma by last step => stop ray
end do
end if
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! print ray positions for j=nrayr in local reference system
if(mod(i,params%output%istpr) == 0) then
if(params%raytracing%nray > 1 .and. all(.not.iwait)) &
call print_projxyzt(stv,yw,0)
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
end if
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! test whether further trajectory integration is unnecessary
call vmaxmin(tau1+tau0+lgcpl1,params%raytracing%nray,taumn,taumx) ! test on tau + coupling
improve error handling in the gray_main routine - rename errocodes → gray_errors - restructure the errors into a `error_spec` type - make the list of errors easily extensible - rewrite the `print_errn`, `print_errhcd` (now `print_err_raytracing`, `print_err_ecrh_cd`) subroutine to handle arbitrary errors - add functions to easily manipulate errors (`raise_error`, `has_error`, `is_critical`) - remove print statements from quadpack - log all errors to stderr using the logger module
2022-07-14 00:38:34 +02:00
if(is_critical(error)) then ! stop propagation for current beam
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
istop_pass = istop_pass +1 ! * +1 non propagating beam
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
if(ip < params%raytracing%ipass) call turnoffray(0,ip,ib,iroff) ! * de-activate derived beams
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
exit
trunk/graycore: minor fixes
2019-03-28 10:50:28 +01:00
else if(all(iwait)) then ! all rays in current beam are waiting for next pass => do not increase istop_pass
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
exit
* reduced arrays required for dI/ds,dP/ds integration * new module for error handling * input parameters collected in a single file * fixed uninitialized pabs,icd
2015-11-19 19:20:58 +01:00
end if
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
end do propagation_loop
src: use the logging system everywhere
2021-12-18 18:57:38 +01:00
call log_debug(' propagation loop end', mod='gray_core', proc='gray_main')
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! ======== propagation loop END ========
! print all ray positions in local reference system
if(params%raytracing%nray > 1 .and. all(.not.iwait)) call print_projxyzt(stv,yw,1)
! =========== post-proc BEGIN ===========
! compute total absorbed power and driven current for current beam
if(i>params%raytracing%nstep) i=params%raytracing%nstep
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
pabs_beam = sum(ppabs(:,i))
icd_beam = sum(ccci(:,i))
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
call vmaxmin(tau0,params%raytracing%nray,taumn,taumx) ! taumn,taumx for print
! compute power and current density profiles for all rays
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
call spec(psjki,ppabs,ccci,iiv,pabs_beam,icd_beam,dpdv_beam,jphi_beam,jcd_beam, &
pins_beam,currins_beam)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
pabs_pass(iox) = pabs_pass(iox) + pabs_beam ! 0D results for current pass, sum on O/X mode beams
icd_pass(iox) = icd_pass(iox) + icd_beam
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
if(ip < params%raytracing%ipass .and. iopmin > 2) then ! not last pass AND at least one ray re-entered plasma
cpl_beam1 = sum(p0ray * exp(-tau0) * cpls(:,iO)/cpl1, MASK=iop > 2) / &
sum(p0ray * exp(-tau0), MASK=iop > 2) ! * average O-mode coupling for next beam (on active rays)
trunk/graycore: fix to coupling calculation for on-screen print
2019-03-28 12:33:43 +01:00
cpl_beam2 = one - cpl_beam1 ! * average X-mode coupling for next beam
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
if(iop(1) > 2) then ! * central ray O/X-mode coupling for next beam
trunk/graycore: fix to coupling calculation for on-screen print
2019-03-28 12:33:43 +01:00
cpl_cbeam1 = cpls(1,iO)/cpl1(1)
cpl_cbeam2 = one - cpl_cbeam1
end if
else ! last pass OR no ray re-entered plasma
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
cpl_beam1 = zero
cpl_beam2 = zero
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
end if
src: use the logging system everywhere
2021-12-18 18:57:38 +01:00
! print final results for pass on screen
call log_info(' partial results:', mod='gray_core', proc='gray_main')
add some useful debug messages
2022-05-26 02:33:55 +02:00
write(msg, '(" final step:", x,a,g0, x,a,g0.4)') 'n=', i, '(s, ct, Sr)=', stv(1)
src: use the logging system everywhere
2021-12-18 18:57:38 +01:00
call log_info(msg, mod='gray_core', proc='gray_main')
write(msg, '(3x,a,2(x,a,"=",g0.4))') 'optical depth:', 'τ_min', taumn, 'τ_max', taumx
call log_info(msg, mod='gray_core', proc='gray_main')
write(msg, '(3x,a,g0.3," MW")') 'absoption: P=', pabs_beam
call log_info(msg, mod='gray_core', proc='gray_main')
write(msg, '(3x,a,g0.3," MW")') 'current drive: I=', icd_beam*1.0e3_wp_
call log_info(msg, mod='gray_core', proc='gray_main')
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
if(ip < params%raytracing%ipass) then
src: use the logging system everywhere
2021-12-18 18:57:38 +01:00
write (msg,'(3x,a,(g0.4,", ",g0.4))') & ! average coupling for next O/X beams (=0 if no ray re-entered plasma)
'next couplings [O,X mode]: c=', cpl_beam1, cpl_beam2
call log_info(msg, mod='gray_core', proc='gray_main')
if(iop(1) > 2) then
write(msg, '(3x,a,(g0.4,", ",g0.4))') &
'coupling [ctr ray, O/X]:', cpl_cbeam1, cpl_cbeam2 ! central ray coupling for next O/X beams
end if
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
end if
src: use the logging system everywhere
2021-12-18 18:57:38 +01:00
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
call print_pec(rhop_tab,rhot_tab,jphi_beam,jcd_beam,dpdv_beam,currins_beam, &
pins_beam,ip) ! *print power and current density profiles for current beam
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
call postproc_profiles(pabs_beam,icd_beam,rhot_tab,dpdv_beam,jphi_beam, &
rhotpav,drhotpav,rhotjava,drhotjava,dpdvp,jphip,rhotp,drhotp,rhotj, &
drhotj,dpdvmx,jphimx,ratjamx,ratjbmx) ! *compute profiles width for current beam
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
call print_finals(pabs_beam,icd_beam,dpdvp,jphip,rhotpav,rhotjava, &
drhotpav,drhotjava,dpdvmx,jphimx,rhotp,rhotj,drhotp,drhotj,ratjamx, &
ratjbmx,stv(1),psipv(index_rt),chipv(index_rt),index_rt,sum(p0ray), &
cpl_beam1,cpl_beam2) ! *print 0D results for current beam
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! ============ post-proc END ============
end do beam_loop
src: use the logging system everywhere
2021-12-18 18:57:38 +01:00
call log_debug('beam loop end', mod='gray_core', proc='gray_main')
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! ============ beam loop END ============
! ======= cumulative prints BEGIN =======
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
results%pabs = results%pabs + sum(pabs_pass) ! *final results (O+X) [gray_main output]
results%icd = results%icd + sum(icd_pass)
src: use the logging system everywhere
2021-12-18 18:57:38 +01:00
! print final results for pass on screen
call log_info(' comulative results:', mod='gray_core', proc='gray_main')
write(msg, '(" absoption [O,X mode] P=",g0.4,", ",g0.4," MW")') &
pabs_pass(1), pabs_pass(2)
call log_info(msg, mod='gray_core', proc='gray_main')
write(msg, '(" current drive [O,X mode] I=",g0.4,", ",g0.4," kA")') &
icd_pass(1)*1.0e3_wp_, icd_pass(2)*1.0e3_wp_
call log_info(msg, mod='gray_core', proc='gray_main')
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! ======== cumulative prints END ========
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
if(istop_pass == nbeam_pass) exit ! no active beams
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
end do main_loop
src: use the logging system everywhere
2021-12-18 18:57:38 +01:00
call log_debug('pass loop end', mod='gray_core', proc='gray_main')
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! ============ main loop END ============
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! ========== free memory BEGIN ==========
fixed incompatibilities with allocatable arrays (pgf90 compiler, JETTO); fixed input/output scaling (gray/jetto interface); fixed error in read_beams2 for small beam tables
2016-06-01 15:49:35 +02:00
call dealloc_surfvec
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
call dealloc_beam(yw,ypw,xc,du1,gri,ggri,psjki,ppabs,ccci,tau0, &
alphaabs0,dids0,ccci0,p0jk,ext,eyt,iiv)
fixed incompatibilities with allocatable arrays (pgf90 compiler, JETTO); fixed input/output scaling (gray/jetto interface); fixed error in read_beams2 for small beam tables
2016-06-01 15:49:35 +02:00
call dealloc_pec
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
call dealloc_multipass(iwait,iroff,iop,iow,yynext,yypnext,yw0,ypw0, &
stnext,stv,p0ray,taus,tau1,etau1,cpls,cpl1,lgcpl1,jphi_beam, &
pins_beam,currins_beam,dpdv_beam,jcd_beam,psipv,chipv)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! =========== free memory END ===========
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
end subroutine gray_main
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
merge graysum and gray Note that graysum, now as sum_mode, still doesn't support multipass.
2021-12-15 02:30:55 +01:00
* reduced arrays required for dI/ds,dP/ds integration * new module for error handling * input parameters collected in a single file * fixed uninitialized pabs,icd
2015-11-19 19:20:58 +01:00
subroutine vectinit(psjki,ppabs,ccci,tau0,alphaabs0,dids0,ccci0,iiv)
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
use const_and_precisions, only : zero
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
implicit none
! arguments
* reduced arrays required for dI/ds,dP/ds integration * new module for error handling * input parameters collected in a single file * fixed uninitialized pabs,icd
2015-11-19 19:20:58 +01:00
real(wp_), dimension(:,:), intent(out) :: psjki,ppabs,ccci
real(wp_), dimension(:), intent(out) :: tau0,alphaabs0,dids0,ccci0
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
integer, dimension(:), intent(out) :: iiv
!! common/external functions/variables
! integer :: jclosest
! real(wp_), dimension(3) :: anwcl,xwcl
!
! common/refln/anwcl,xwcl,jclosest
!
! jclosest=nrayr+1
! anwcl(1:3)=0.0_wp_
! xwcl(1:3)=0.0_wp_
* reduced arrays required for dI/ds,dP/ds integration * new module for error handling * input parameters collected in a single file * fixed uninitialized pabs,icd
2015-11-19 19:20:58 +01:00
psjki = zero
ppabs = zero
ccci = zero
tau0 = zero
alphaabs0 = zero
dids0 = zero
ccci0 = zero
iiv = 1
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
end subroutine vectinit
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
subroutine ic_gb(params, anv0c, ak0, ywrk0, ypwrk0, &
xc0, du10, gri, ggri, index_rt)
! beam tracing initial conditions igrad=1
! !!!!!! check ray tracing initial conditions igrad=0 !!!!!!
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
use const_and_precisions, only : zero,one,pi,half,two,degree,ui=>im
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
use gray_params, only : gray_parameters
use beamdata, only : nray,nrayr,nrayth,rwmax
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
implicit none
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! subroutine arguments
type(gray_parameters), intent(in) :: params
real(wp_), dimension(3), intent(in) :: anv0c
real(wp_), intent(in) :: ak0
real(wp_), dimension(6, nray), intent(out) :: ywrk0, ypwrk0
real(wp_), dimension(3, nrayth, nrayr), intent(out) :: xc0, du10
real(wp_), dimension(3, nray), intent(out) :: gri
real(wp_), dimension(3, 3, nray), intent(out) :: ggri
integer, intent(in) :: index_rt
! local variables
real(wp_), dimension(3) :: xv0c
real(wp_) :: wcsi,weta,rcicsi,rcieta,phiw,phir
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
integer :: j,k,jk
real(wp_) :: csth,snth,csps,snps,phiwrad,phirrad,csphiw,snphiw,alfak
real(wp_) :: wwcsi,wweta,sk,sw,dk,dw,rci1,ww1,rci2,ww2,wwxx,wwyy,wwxy
real(wp_) :: rcixx,rciyy,rcixy,dwwxx,dwwyy,dwwxy,d2wwxx,d2wwyy,d2wwxy
real(wp_) :: drcixx,drciyy,drcixy,dr,da,ddfu,dcsiw,detaw,dx0t,dy0t
real(wp_) :: x0t,y0t,z0t,dx0,dy0,dz0,x0,y0,z0,gxt,gyt,gzt,gr2
real(wp_) :: gxxt,gyyt,gzzt,gxyt,gxzt,gyzt,dgr2xt,dgr2yt,dgr2zt
real(wp_) :: dgr2x,dgr2y,dgr2z,pppx,pppy,denpp,ppx,ppy
real(wp_) :: anzt,anxt,anyt,anx,any,anz,an20,an0
real(wp_) :: du1tx,du1ty,du1tz,denom,ddr,ddi
real(wp_), dimension(nrayr) :: uj
real(wp_), dimension(nrayth) :: sna,csa
complex(wp_) :: sss,ddd,phic,qi1,qi2,tc,ts,qqxx,qqxy,qqyy,dqi1,dqi2
complex(wp_) :: dqqxx,dqqyy,dqqxy,d2qi1,d2qi2,d2qqxx,d2qqyy,d2qqxy
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! initial beam parameters
xv0c = params%antenna%pos
wcsi = params%antenna%w(1)
weta = params%antenna%w(2)
rcicsi = params%antenna%ri(1)
rcieta = params%antenna%ri(2)
phiw = params%antenna%phi(1)
phir = params%antenna%phi(2)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
csth=anv0c(3)
snth=sqrt(one-csth**2)
if(snth > zero) then
csps=anv0c(2)/snth
snps=anv0c(1)/snth
else
csps=one
snps=zero
end if
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! Gaussian beam: exp[-ik0 zt] exp[-i k0/2 S(xt,yt,zt)]
! xt,yt,zt, cartesian coordinate system with zt along the beamline and xt in the z = 0 plane
! S(xt,yt,zt) = S_real +i S_imag = Qxx(zt) xt^2 + Qyy(zt) yt^2 + 2 Qxy(zt) xt yt
! (csiw, etaw) and (csiR, etaR) intensity and phase ellipse, rotated by angle phiw and phiR
! S(xt,yt,zt) = csiR^2 / Rccsi +etaR^2 /Rceta - i (csiw^2 Wcsi +etaw^2 Weta)
! Rccsi,eta curvature radius at the launching point
! Wcsi,eta =2/(k0 wcsi,eta^2) with wcsi,eta^2 beam size at the launching point
updated prfile subr, added comments and minor changes in ic_gb
2015-11-19 18:44:17 +01:00
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
phiwrad = phiw*degree
phirrad = phir*degree
csphiw = cos(phiwrad)
snphiw = sin(phiwrad)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
!csphir = cos(phirrad)
!snphir = sin(phirrad)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
wwcsi = two/(ak0*wcsi**2)
wweta = two/(ak0*weta**2)
if(phir/=phiw) then
updated prfile subr, added comments and minor changes in ic_gb
2015-11-19 18:44:17 +01:00
sk = rcicsi + rcieta
sw = wwcsi + wweta
dk = rcicsi - rcieta
dw = wwcsi - wweta
ts = -(dk*sin(2*phirrad) - ui*dw*sin(2*phiwrad))
tc = (dk*cos(2*phirrad) - ui*dw*cos(2*phiwrad))
use the logger everywhere This converts the last remaining warnings to use the logging system. Also drops `catand` and replace it with the intrinsic `atan`, which supports complex as well as real numbers. Note: before 3eab989d the `catand` function was actually incorrent! The definition of arctan(z) can be obtained starting from the identity d/dz arctan(z) = 1/(1 + z²) = ½ [1/(1 + iz) + 1/(1 - iz)], integrating and using the definition log(z) = ∫₁^z dz/z, arctan(z) = -i/2 [log(1 + iz) - log(1 - iz)]. If log is the principal branch, log(z) = log|z| + i arg(z), then arctan(z) = -i/2 log(w) = 1/2 arg(w) -i/2 log|w| where w = (1 + iz)/(1 - iz). Finally, the real part is Re arctan(z) = 1/2 atan2(2Re(z), 1 - |z|²). The term -|z|² is missing from the `catand` definition of GRAY, but is present in the original Fortran 77 code from [SLATEC]: it has probably been lost in the translation. [SLATEC]: https://people.math.sc.edu/Burkardt/f_src/slatec/slatec.f90
2022-07-15 00:09:36 +02:00
phic = half*atan(ts/tc)
updated prfile subr, added comments and minor changes in ic_gb
2015-11-19 18:44:17 +01:00
ddd = dk*cos(2*(phirrad+phic)) - ui*dw*cos(2*(phiwrad+phic))
sss = sk - ui*sw
qi1 = half*(sss + ddd)
qi2 = half*(sss - ddd)
always use generic math functions This replaces double precision-specific function in order to allow building GRAY with other real kinds, for example single or quadruple precision.
2023-09-20 16:03:08 +02:00
rci1 = real(qi1)
rci2 = real(qi2)
ww1 = -imag(qi1)
ww2 = -imag(qi2)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
else
rci1 = rcicsi
rci2 = rcieta
ww1 = wwcsi
ww2 = wweta
phic = -phiwrad
qi1 = rci1 - ui*ww1
qi2 = rci2 - ui*ww2
end if
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
!w01=sqrt(2.0_wp_/(ak0*ww1))
!d01=-rci1/(rci1**2+ww1**2)
!w02=sqrt(2.0_wp_/(ak0*ww2))
!d02=-rci2/(rci2**2+ww2**2)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
qqxx = qi1*cos(phic)**2 + qi2*sin(phic)**2
qqyy = qi1*sin(phic)**2 + qi2*cos(phic)**2
updated prfile subr, added comments and minor changes in ic_gb
2015-11-19 18:44:17 +01:00
qqxy = -(qi1 - qi2)*sin(phic)*cos(phic)
always use generic math functions This replaces double precision-specific function in order to allow building GRAY with other real kinds, for example single or quadruple precision.
2023-09-20 16:03:08 +02:00
wwxx = -imag(qqxx)
wwyy = -imag(qqyy)
wwxy = -imag(qqxy)
rcixx = real(qqxx)
rciyy = real(qqyy)
rcixy = real(qqxy)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
dqi1 = -qi1**2
dqi2 = -qi2**2
d2qi1 = 2*qi1**3
d2qi2 = 2*qi2**3
dqqxx = dqi1*cos(phic)**2 + dqi2*sin(phic)**2
dqqyy = dqi1*sin(phic)**2 + dqi2*cos(phic)**2
updated prfile subr, added comments and minor changes in ic_gb
2015-11-19 18:44:17 +01:00
dqqxy = -(dqi1 - dqi2)*sin(phic)*cos(phic)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
d2qqxx = d2qi1*cos(phic)**2 + d2qi2*sin(phic)**2
d2qqyy = d2qi1*sin(phic)**2 + d2qi2*cos(phic)**2
updated prfile subr, added comments and minor changes in ic_gb
2015-11-19 18:44:17 +01:00
d2qqxy = -(d2qi1 - d2qi2)*sin(phic)*cos(phic)
always use generic math functions This replaces double precision-specific function in order to allow building GRAY with other real kinds, for example single or quadruple precision.
2023-09-20 16:03:08 +02:00
dwwxx = -imag(dqqxx)
dwwyy = -imag(dqqyy)
dwwxy = -imag(dqqxy)
d2wwxx = -imag(d2qqxx)
d2wwyy = -imag(d2qqyy)
d2wwxy = -imag(d2qqxy)
drcixx = real(dqqxx)
drciyy = real(dqqyy)
drcixy = real(dqqxy)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
if(nrayr > 1) then
always use generic math functions This replaces double precision-specific function in order to allow building GRAY with other real kinds, for example single or quadruple precision.
2023-09-20 16:03:08 +02:00
dr = rwmax/(nrayr-1)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
else
dr = one
end if
always use generic math functions This replaces double precision-specific function in order to allow building GRAY with other real kinds, for example single or quadruple precision.
2023-09-20 16:03:08 +02:00
ddfu = two*dr**2/ak0 ! twodr2 = 2*dr**2 = 2*rwmax/real(nrayr-1)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
do j = 1, nrayr
always use generic math functions This replaces double precision-specific function in order to allow building GRAY with other real kinds, for example single or quadruple precision.
2023-09-20 16:03:08 +02:00
uj(j) = real(j-1, wp_)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
end do
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
always use generic math functions This replaces double precision-specific function in order to allow building GRAY with other real kinds, for example single or quadruple precision.
2023-09-20 16:03:08 +02:00
da=2*pi/nrayth
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
do k=1,nrayth
alfak = (k-1)*da
sna(k) = sin(alfak)
csa(k) = cos(alfak)
end do
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! central ray
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
jk=1
gri(:,1) = zero
ggri(:,:,1) = zero
ywrk0(1:3,1) = xv0c
ywrk0(4:6,1) = anv0c
ypwrk0(1:3,1) = anv0c
ypwrk0(4:6,1) = zero
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
do k=1,nrayth
dcsiw = dr*csa(k)*wcsi
detaw = dr*sna(k)*weta
dx0t = dcsiw*csphiw - detaw*snphiw
dy0t = dcsiw*snphiw + detaw*csphiw
du1tx = (dx0t*wwxx + dy0t*wwxy)/ddfu
du1ty = (dx0t*wwxy + dy0t*wwyy)/ddfu
xc0(:,k,1) = xv0c
du10(1,k,1) = du1tx*csps + snps*du1ty*csth
du10(2,k,1) = -du1tx*snps + csps*du1ty*csth
du10(3,k,1) = -du1ty*snth
end do
ddr = zero
ddi = zero
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! loop on rays jk>1
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
j=2
k=0
do jk=2,nray
k=k+1
if(k > nrayth) then
j=j+1
k=1
end if
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
!csiw=u*dcsiw
!etaw=u*detaw
!csir=x0t*csphir+y0t*snphir
!etar=-x0t*snphir+y0t*csphir
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
dcsiw = dr*csa(k)*wcsi
detaw = dr*sna(k)*weta
dx0t = dcsiw*csphiw - detaw*snphiw
dy0t = dcsiw*snphiw + detaw*csphiw
x0t = uj(j)*dx0t
y0t = uj(j)*dy0t
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
z0t = -(half*(rcixx*x0t**2 + rciyy*y0t**2) + rcixy*x0t*y0t)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
dx0 = x0t*csps + snps*(y0t*csth + z0t*snth)
dy0 = -x0t*snps + csps*(y0t*csth + z0t*snth)
dz0 = z0t*csth - y0t*snth
x0 = xv0c(1) + dx0
y0 = xv0c(2) + dy0
z0 = xv0c(3) + dz0
gxt = x0t*wwxx + y0t*wwxy
gyt = x0t*wwxy + y0t*wwyy
gzt = half*(x0t**2*dwwxx + y0t**2*dwwyy ) + x0t*y0t*dwwxy
gr2 = gxt*gxt + gyt*gyt + gzt*gzt
gxxt = wwxx
gyyt = wwyy
gzzt = half*(x0t**2*d2wwxx + y0t**2*d2wwyy) + x0t*y0t*d2wwxy
gxyt = wwxy
gxzt = x0t*dwwxx + y0t*dwwxy
gyzt = x0t*dwwxy + y0t*dwwyy
dgr2xt = 2*(gxt*gxxt + gyt*gxyt + gzt*gxzt)
dgr2yt = 2*(gxt*gxyt + gyt*gyyt + gzt*gyzt)
dgr2zt = 2*(gxt*gxzt + gyt*gyzt + gzt*gzzt)
dgr2x = dgr2xt*csps + snps*(dgr2yt*csth + dgr2zt*snth)
dgr2y = -dgr2xt*snps + csps*(dgr2yt*csth + dgr2zt*snth)
dgr2z = dgr2zt*csth - dgr2yt*snth
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
gri(1,jk) = gxt*csps + snps*(gyt*csth + gzt*snth)
gri(2,jk) = -gxt*snps + csps*(gyt*csth + gzt*snth)
gri(3,jk) = gzt*csth - gyt*snth
ggri(1,1,jk) = gxxt*csps**2 &
+ snps**2 *(gyyt*csth**2 + gzzt*snth**2 + 2*snth*csth*gyzt) &
+2*snps*csps*(gxyt*csth + gxzt*snth)
ggri(2,1,jk) = csps*snps &
*(-gxxt+csth**2*gyyt + snth**2*gzzt + 2*csth*snth*gyzt) &
+(csps**2 - snps**2)*(snth*gxzt + csth*gxyt)
ggri(3,1,jk) = csth*snth*snps*(gzzt - gyyt) + (csth**2 - snth**2) &
*snps*gyzt + csps*(csth*gxzt - snth*gxyt)
ggri(1,2,jk) = ggri(2,1,jk)
ggri(2,2,jk) = gxxt*snps**2 &
+ csps**2 *(gyyt*csth**2 + gzzt*snth**2 + 2*snth*csth*gyzt) &
-2*snps*csps*(gxyt*csth + gxzt*snth)
ggri(3,2,jk) = csth*snth*csps*(gzzt - gyyt) + (csth**2-snth**2) &
*csps*gyzt + snps*(snth*gxyt - csth*gxzt)
ggri(1,3,jk) = ggri(3,1,jk)
ggri(2,3,jk) = ggri(3,2,jk)
ggri(3,3,jk) = gzzt*csth**2 + gyyt*snth**2 - 2*csth*snth*gyzt
du1tx = (dx0t*wwxx + dy0t*wwxy)/ddfu
du1ty = (dx0t*wwxy + dy0t*wwyy)/ddfu
du1tz = half*uj(j)*(dx0t**2*dwwxx + dy0t**2*dwwyy + 2*dx0t*dy0t*dwwxy)/ddfu
du10(1,k,j) = du1tx*csps + snps*(du1ty*csth + du1tz*snth)
du10(2,k,j) = -du1tx*snps + csps*(du1ty*csth + du1tz*snth)
du10(3,k,j) = du1tz*csth - du1ty*snth
pppx = x0t*rcixx + y0t*rcixy
pppy = x0t*rcixy + y0t*rciyy
denpp = pppx*gxt + pppy*gyt
if (denpp/=zero) then
ppx = -pppx*gzt/denpp
ppy = -pppy*gzt/denpp
else
ppx = zero
ppy = zero
end if
anzt = sqrt((one + gr2)/(one + ppx**2 + ppy**2))
anxt = ppx*anzt
anyt = ppy*anzt
anx = anxt*csps + snps*(anyt*csth + anzt*snth)
any =-anxt*snps + csps*(anyt*csth + anzt*snth)
anz = anzt*csth - anyt*snth
an20 = one + gr2
an0 = sqrt(an20)
xc0(1,k,j) = x0
xc0(2,k,j) = y0
xc0(3,k,j) = z0
ywrk0(1,jk) = x0
ywrk0(2,jk) = y0
ywrk0(3,jk) = z0
ywrk0(4,jk) = anx
ywrk0(5,jk) = any
ywrk0(6,jk) = anz
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! integration variable
select case(params%raytracing%idst)
case(0)
! optical path: s
denom = an0
case(1)
! "time": c⋅t
denom = one
case(2)
! real eikonal: S_R
denom = an20
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
end select
ypwrk0(1,jk) = anx/denom
ypwrk0(2,jk) = any/denom
ypwrk0(3,jk) = anz/denom
ypwrk0(4,jk) = dgr2x/(2*denom)
ypwrk0(5,jk) = dgr2y/(2*denom)
ypwrk0(6,jk) = dgr2z/(2*denom)
ddr = anx**2 + any**2 + anz**2 - an20
ddi = 2*(anxt*gxt + anyt*gyt + anzt*gzt)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! st=0, index_rt=1, B=0, N=0, psin=-1, Xg=0, Yg=0, gradXg=0
call print_output(0,jk,zero,one,xc0(:,k,j),-one,zero,[zero,zero,zero], &
ak0,zero,zero,[zero,zero,zero],zero,zero,zero,zero,zero,zero, &
0,0,0,index_rt,ddr,ddi,zero,zero,[zero,zero,zero])
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
end do
end subroutine ic_gb
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
subroutine rkstep(sox,bres,xgcn,y,yp,dgr,ddgr,igrad)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
! Runge-Kutta integrator
! use gray_params, only : igrad
use beamdata, only : h,hh,h6
implicit none
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
real(wp_), intent(in) :: bres,xgcn
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
real(wp_), dimension(6), intent(inout) :: y
real(wp_), dimension(6), intent(in) :: yp
real(wp_), dimension(3), intent(in) :: dgr
real(wp_), dimension(3,3), intent(in) :: ddgr
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
integer, intent(in) :: igrad,sox
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
real(wp_), dimension(6) :: yy,fk1,fk2,fk3,fk4
src/gray_core.f90: remove unused variables in rhs
2023-09-21 13:59:21 +02:00
fk1 = yp
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
yy = y + fk1*hh
src/gray_core.f90: remove unused variables in rhs
2023-09-21 13:59:21 +02:00
call rhs(sox,bres,xgcn,yy,dgr,ddgr,fk2,igrad)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
yy = y + fk2*hh
src/gray_core.f90: remove unused variables in rhs
2023-09-21 13:59:21 +02:00
call rhs(sox,bres,xgcn,yy,dgr,ddgr,fk3,igrad)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
yy = y + fk3*h
src/gray_core.f90: remove unused variables in rhs
2023-09-21 13:59:21 +02:00
call rhs(sox,bres,xgcn,yy,dgr,ddgr,fk4,igrad)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
y = y + h6*(fk1 + 2*fk2 + 2*fk3 + fk4)
end subroutine rkstep
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
src/gray_core.f90: remove unused variables in rhs
2023-09-21 13:59:21 +02:00
subroutine rhs(sox,bres,xgcn,y,dgr,ddgr,dery,igrad)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
! Compute right-hand side terms of the ray equations (dery)
! used in R-K integrator
implicit none
! arguments
real(wp_), dimension(6), intent(in) :: y
src/gray_core.f90: remove unused variables in rhs
2023-09-21 13:59:21 +02:00
real(wp_), intent(in) :: bres,xgcn
real(wp_), dimension(3), intent(in) :: dgr
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
real(wp_), dimension(3,3), intent(in) :: ddgr
real(wp_), dimension(6), intent(out) :: dery
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
integer, intent(in) :: igrad,sox
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
! local variables
src/gray_core.f90: remove unused variables in rhs
2023-09-21 13:59:21 +02:00
real(wp_) :: dens,btot,xg,yg
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
real(wp_), dimension(3) :: xv,anv,bv,derxg,deryg
real(wp_), dimension(3,3) :: derbv
xv = y(1:3)
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
call plas_deriv(xv,bres,xgcn,dens,btot,bv,derbv,xg,yg,derxg,deryg)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
anv = y(4:6)
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
call disp_deriv(anv,sox,xg,yg,derxg,deryg,bv,derbv,dgr,ddgr,igrad,dery)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
end subroutine rhs
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
subroutine ywppla_upd(xv,anv,dgr,ddgr,sox,bres,xgcn,dery,psinv,dens,btot, &
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
bv,xg,yg,derxg,anpl,anpr,ddr,ddi,dersdst,derdnm,error,igrad)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
! Compute right-hand side terms of the ray equations (dery)
! used after full R-K step and grad(S_I) update
improve error handling in the gray_main routine - rename errocodes → gray_errors - restructure the errors into a `error_spec` type - make the list of errors easily extensible - rewrite the `print_errn`, `print_errhcd` (now `print_err_raytracing`, `print_err_ecrh_cd`) subroutine to handle arbitrary errors - add functions to easily manipulate errors (`raise_error`, `has_error`, `is_critical`) - remove print statements from quadpack - log all errors to stderr using the logger module
2022-07-14 00:38:34 +02:00
use gray_errors, only : raise_error, large_npl
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
implicit none
! arguments
real(wp_), dimension(3), intent(in) :: xv,anv
real(wp_), dimension(3), intent(in) :: dgr
real(wp_), dimension(3,3), intent(in) :: ddgr
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
integer, intent(in) :: sox
real(wp_), intent(in) :: bres,xgcn
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
real(wp_), dimension(6), intent(out) :: dery
real(wp_), intent(out) :: psinv,dens,btot,xg,yg,anpl,anpr
real(wp_), intent(out) :: ddr,ddi,dersdst,derdnm
some additional output prints (2D maps and Bcart, Ncart along central ray)
2016-02-12 17:49:00 +01:00
real(wp_), dimension(3), intent(out) :: bv
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
integer, intent(out) :: error
added further output prints to fort.4
2017-09-12 21:37:06 +02:00
real(wp_), dimension(3), intent(out) :: derxg
trunk: added multiple passes calculation; added multipass module; graycore/gray_main: subroutine rewritten; equilibrium/read_equil_an: limiter coordinates read from equilibrium file for ipass>1; err_codes/check_err: istop=1 only for alpha<0; pec/pec_tab: fixed index assignements in loops; polarization/pol_limit: fixed ext,eyt normalization
2019-03-26 15:21:22 +01:00
integer, intent(in) :: igrad
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
! local variables
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
real(wp_), dimension(3) :: deryg
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
real(wp_), dimension(3,3) :: derbv
* reduced arrays required for dI/ds,dP/ds integration * new module for error handling * input parameters collected in a single file * fixed uninitialized pabs,icd
2015-11-19 19:20:58 +01:00
real(wp_), parameter :: anplth1 = 0.99_wp_, anplth2 = 1.05_wp_
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
call plas_deriv(xv,bres,xgcn,dens,btot,bv,derbv,xg,yg,derxg,deryg,psinv)
call disp_deriv(anv,sox,xg,yg,derxg,deryg,bv,derbv,dgr,ddgr,igrad, &
dery,anpl,anpr,ddr,ddi,dersdst,derdnm)
* reduced arrays required for dI/ds,dP/ds integration * new module for error handling * input parameters collected in a single file * fixed uninitialized pabs,icd
2015-11-19 19:20:58 +01:00
improve error handling in the gray_main routine - rename errocodes → gray_errors - restructure the errors into a `error_spec` type - make the list of errors easily extensible - rewrite the `print_errn`, `print_errhcd` (now `print_err_raytracing`, `print_err_ecrh_cd`) subroutine to handle arbitrary errors - add functions to easily manipulate errors (`raise_error`, `has_error`, `is_critical`) - remove print statements from quadpack - log all errors to stderr using the logger module
2022-07-14 00:38:34 +02:00
if (abs(anpl) > anplth2) then
error = raise_error(error, large_npl, 1)
else if (abs(anpl) > anplth1) then
error = raise_error(error, large_npl, 0)
else
error = 0
* reduced arrays required for dI/ds,dP/ds integration * new module for error handling * input parameters collected in a single file * fixed uninitialized pabs,icd
2015-11-19 19:20:58 +01:00
end if
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
end subroutine ywppla_upd
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
subroutine gradi_upd(ywrk,ak0,xc,du1,gri,ggri)
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
use const_and_precisions, only : zero,half
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
use beamdata, only : nray,nrayr,nrayth,twodr2
implicit none
real(wp_), intent(in) :: ak0
real(wp_), dimension(6,nray), intent(in) :: ywrk
real(wp_), dimension(3,nrayth,nrayr), intent(inout) :: xc,du1
real(wp_), dimension(3,nray), intent(out) :: gri
real(wp_), dimension(3,3,nray), intent(out) :: ggri
! local variables
real(wp_), dimension(3,nrayth,nrayr) :: xco,du1o
integer :: jk,j,jm,jp,k,km,kp
real(wp_) :: ux,uxx,uxy,uxz,uy,uyy,uyz,uz,uzz
real(wp_) :: dfuu,dffiu,gx,gxx,gxy,gxz,gy,gyy,gyz,gz,gzz
real(wp_), dimension(3) :: dxv1,dxv2,dxv3,dgu
real(wp_), dimension(3,3) :: dgg,dff
! update position and du1 vectors
xco = xc
du1o = du1
jk = 1
do j=1,nrayr
do k=1,nrayth
if(j>1) jk=jk+1
xc(1:3,k,j)=ywrk(1:3,jk)
end do
end do
! compute grad u1 for central ray
j = 1
jp = 2
do k=1,nrayth
if(k == 1) then
km = nrayth
else
km = k-1
end if
if(k == nrayth) then
kp = 1
else
kp = k+1
end if
dxv1 = xc(:,k ,jp) - xc(:,k ,j)
dxv2 = xc(:,kp,jp) - xc(:,km,jp)
dxv3 = xc(:,k ,j) - xco(:,k ,j)
call solg0(dxv1,dxv2,dxv3,dgu)
du1(:,k,j) = dgu
end do
gri(:,1) = zero
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
! compute grad u1 and grad(S_I) for all the other rays
dfuu=twodr2/ak0 ! twodr2 = 2*dr**2 = 2*(rwmax/(nrayr-1))**2
jm=1
j=2
k=0
dffiu = dfuu
do jk=2,nray
k=k+1
if(k > nrayth) then
jm = j
j = j+1
k = 1
dffiu = dfuu*jm
end if
kp = k+1
km = k-1
if (k == 1) then
km=nrayth
else if (k == nrayth) then
kp=1
end if
dxv1 = xc(:,k ,j) - xc(:,k ,jm)
dxv2 = xc(:,kp,j) - xc(:,km,j)
dxv3 = xc(:,k ,j) - xco(:,k ,j)
call solg0(dxv1,dxv2,dxv3,dgu)
du1(:,k,j) = dgu
gri(:,jk) = dgu(:)*dffiu
end do
! compute derivatives of grad u and grad(S_I) for rays jk>1
ggri(:,:,1) = zero
jm=1
j=2
k=0
dffiu = dfuu
do jk=2,nray
k=k+1
if(k > nrayth) then
jm=j
j=j+1
k=1
dffiu = dfuu*jm
end if
kp=k+1
km=k-1
if (k == 1) then
km=nrayth
else if (k == nrayth) then
kp=1
end if
dxv1 = xc(:,k ,j) - xc(:,k ,jm)
dxv2 = xc(:,kp,j) - xc(:,km,j)
dxv3 = xc(:,k ,j) - xco(:,k ,j)
dff(:,1) = du1(:,k ,j) - du1(:,k ,jm)
dff(:,2) = du1(:,kp,j) - du1(:,km,j)
dff(:,3) = du1(:,k ,j) - du1o(:,k ,j)
call solg3(dxv1,dxv2,dxv3,dff,dgg)
! derivatives of u
ux = du1(1,k,j)
uy = du1(2,k,j)
uz = du1(3,k,j)
uxx = dgg(1,1)
uyy = dgg(2,2)
uzz = dgg(3,3)
uxy = (dgg(1,2) + dgg(2,1))*half
uxz = (dgg(1,3) + dgg(3,1))*half
uyz = (dgg(2,3) + dgg(3,2))*half
! derivatives of S_I and Grad(S_I)
gx = ux*dffiu
gy = uy*dffiu
gz = uz*dffiu
gxx = dfuu*ux*ux + dffiu*uxx
gyy = dfuu*uy*uy + dffiu*uyy
gzz = dfuu*uz*uz + dffiu*uzz
gxy = dfuu*ux*uy + dffiu*uxy
gxz = dfuu*ux*uz + dffiu*uxz
gyz = dfuu*uy*uz + dffiu*uyz
ggri(1,1,jk)=gxx
ggri(2,1,jk)=gxy
ggri(3,1,jk)=gxz
ggri(1,2,jk)=gxy
ggri(2,2,jk)=gyy
ggri(3,2,jk)=gyz
ggri(1,3,jk)=gxz
ggri(2,3,jk)=gyz
ggri(3,3,jk)=gzz
end do
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
end subroutine gradi_upd
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
subroutine solg0(dxv1,dxv2,dxv3,dgg)
! solution of the linear system of 3 eqs : dgg . dxv = dff
! input vectors : dxv1, dxv2, dxv3, dff
! output vector : dgg
! dff=(1,0,0)
implicit none
! arguments
real(wp_), dimension(3), intent(in) :: dxv1,dxv2,dxv3
real(wp_), dimension(3), intent(out) :: dgg
! local variables
real(wp_) :: denom,aa1,aa2,aa3
aa1 = (dxv2(2)*dxv3(3) - dxv3(2)*dxv2(3))
aa2 = (dxv1(2)*dxv3(3) - dxv3(2)*dxv1(3))
aa3 = (dxv1(2)*dxv2(3) - dxv2(2)*dxv1(3))
denom = dxv1(1)*aa1 - dxv2(1)*aa2 + dxv3(1)*aa3
dgg(1) = aa1/denom
dgg(2) = -(dxv2(1)*dxv3(3) - dxv3(1)*dxv2(3))/denom
dgg(3) = (dxv2(1)*dxv3(2) - dxv3(1)*dxv2(2))/denom
end subroutine solg0
subroutine solg3(dxv1,dxv2,dxv3,dff,dgg)
! rhs "matrix" dff, result in dgg
implicit none
! arguments
real(wp_), dimension(3), intent(in) :: dxv1,dxv2,dxv3
real(wp_), dimension(3,3), intent(in) :: dff
real(wp_), dimension(3,3), intent(out) :: dgg
! local variables
real(wp_) denom,a11,a21,a31,a12,a22,a32,a13,a23,a33
a11 = (dxv2(2)*dxv3(3) - dxv3(2)*dxv2(3))
a21 = (dxv1(2)*dxv3(3) - dxv3(2)*dxv1(3))
a31 = (dxv1(2)*dxv2(3) - dxv2(2)*dxv1(3))
a12 = (dxv2(1)*dxv3(3) - dxv3(1)*dxv2(3))
a22 = (dxv1(1)*dxv3(3) - dxv3(1)*dxv1(3))
a32 = (dxv1(1)*dxv2(3) - dxv2(1)*dxv1(3))
a13 = (dxv2(1)*dxv3(2) - dxv3(1)*dxv2(2))
a23 = (dxv1(1)*dxv3(2) - dxv3(1)*dxv1(2))
a33 = (dxv1(1)*dxv2(2) - dxv2(1)*dxv1(2))
denom = dxv1(1)*a11 - dxv2(1)*a21 + dxv3(1)*a31
dgg(:,1) = ( dff(:,1)*a11 - dff(:,2)*a21 + dff(:,3)*a31)/denom
dgg(:,2) = (-dff(:,1)*a12 + dff(:,2)*a22 - dff(:,3)*a32)/denom
dgg(:,3) = ( dff(:,1)*a13 - dff(:,2)*a23 + dff(:,3)*a33)/denom
end subroutine solg3
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
subroutine plas_deriv(xv, bres, xgcn, dens, btot, bv, derbv, &
xg, yg, derxg, deryg, psinv_opt)
use const_and_precisions, only : zero
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
use gray_params, only : iequil
use equilibrium, only : psia, equinum_fpol, equinum_psi, equian, sgnbphi
use coreprofiles, only : density
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
implicit none
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! subroutine arguments
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
real(wp_), dimension(3), intent(in) :: xv
real(wp_), intent(in) :: xgcn, bres
real(wp_), intent(out) :: dens, btot, xg, yg
real(wp_), dimension(3), intent(out) :: bv, derxg, deryg
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
real(wp_), dimension(3,3), intent(out) :: derbv
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
real(wp_), optional, intent(out) :: psinv_opt
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! local variables
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
integer :: jv
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
real(wp_) :: xx,yy,zz
real(wp_) :: psinv
src/gray_core.f90: use intrinsic linear algebra functions
2022-05-06 00:31:18 +02:00
real(wp_) :: csphi,drrdx,drrdy,dphidx,dphidy,rr,rr2,rrm,snphi,zzm
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
real(wp_), dimension(3) :: dbtot,bvc
real(wp_), dimension(3,3) :: dbvcdc,dbvdc,dbv
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
real(wp_) :: brr,bphi,bzz,dxgdpsi
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
real(wp_) :: dpsidr,dpsidz,ddpsidrr,ddpsidzz,ddpsidrz,fpolv,dfpv,ddenspsin
xg = zero
yg = 99._wp_
psinv = -1._wp_
dens = zero
btot = zero
derxg = zero
deryg = zero
bv = zero
derbv = zero
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
if(iequil==0) then
! copy optional output
if (present(psinv_opt)) psinv_opt = psinv
return
end if
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
dbtot = zero
dbv = zero
dbvcdc = zero
dbvcdc = zero
dbvdc = zero
xx = xv(1)
yy = xv(2)
zz = xv(3)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! cylindrical coordinates
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
rr2 = xx**2 + yy**2
rr = sqrt(rr2)
csphi = xx/rr
snphi = yy/rr
bv(1) = -snphi*sgnbphi
bv(2) = csphi*sgnbphi
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! convert from cm to meters
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
zzm = 1.0e-2_wp_*zz
rrm = 1.0e-2_wp_*rr
if(iequil==1) then
call equian(rrm,zzm,psinv,fpolv,dfpv,dpsidr,dpsidz, &
ddpsidrr,ddpsidzz,ddpsidrz)
else
call equinum_psi(rrm,zzm,psinv,dpsidr,dpsidz,ddpsidrr,ddpsidzz,ddpsidrz)
call equinum_fpol(psinv,fpolv,dfpv)
end if
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
! copy optional output
if (present(psinv_opt)) psinv_opt = psinv
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! compute yg and derivative
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
if(psinv < zero) then
bphi = fpolv/rrm
btot = abs(bphi)
yg = btot/bres
return
end if
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! compute xg and derivative
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
call density(psinv,dens,ddenspsin)
xg = xgcn*dens
dxgdpsi = xgcn*ddenspsin/psia
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! B = f(psi)/R e_phi+ grad psi x e_phi/R
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
bphi = fpolv/rrm
brr =-dpsidz/rrm
bzz = dpsidr/rrm
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! bvc(i) = B_i in cylindrical coordinates
bvc = [brr, bphi, bzz]
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! bv(i) = B_i in cartesian coordinates
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
bv(1)=bvc(1)*csphi - bvc(2)*snphi
bv(2)=bvc(1)*snphi + bvc(2)*csphi
bv(3)=bvc(3)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! dbvcdc(iv,jv) = d Bcil(iv) / dxvcil(jv)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
dbvcdc(1,1) = -ddpsidrz/rrm - brr/rrm
dbvcdc(2,1) = dfpv*dpsidr/rrm - bphi/rrm
dbvcdc(3,1) = ddpsidrr/rrm - bzz/rrm
dbvcdc(1,3) = -ddpsidzz/rrm
dbvcdc(2,3) = dfpv*dpsidz/rrm
dbvcdc(3,3) = ddpsidrz/rrm
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! dbvdc(iv,jv) = d Bcart(iv) / dxvcil(jv)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
dbvdc(1,1) = dbvcdc(1,1)*csphi - dbvcdc(2,1)*snphi
dbvdc(2,1) = dbvcdc(1,1)*snphi + dbvcdc(2,1)*csphi
dbvdc(3,1) = dbvcdc(3,1)
dbvdc(1,2) = -bv(2)
dbvdc(2,2) = bv(1)
dbvdc(3,2) = dbvcdc(3,2)
dbvdc(1,3) = dbvcdc(1,3)*csphi - dbvcdc(2,3)*snphi
dbvdc(2,3) = dbvcdc(1,3)*snphi + dbvcdc(2,3)*csphi
dbvdc(3,3) = dbvcdc(3,3)
drrdx = csphi
drrdy = snphi
dphidx = -snphi/rrm
dphidy = csphi/rrm
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! dbv(iv,jv) = d Bcart(iv) / dxvcart(jv)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
dbv(:,1) = drrdx*dbvdc(:,1) + dphidx*dbvdc(:,2)
dbv(:,2) = drrdy*dbvdc(:,1) + dphidy*dbvdc(:,2)
dbv(:,3) = dbvdc(:,3)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! B magnitude and derivatives
src/gray_core.f90: use intrinsic linear algebra functions
2022-05-06 00:31:18 +02:00
btot = norm2(bv)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
src/gray_core.f90: use intrinsic linear algebra functions
2022-05-06 00:31:18 +02:00
dbtot = matmul(bv, dbv)/btot
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
yg = btot/Bres
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! convert spatial derivatives from dummy/m -> dummy/cm
! to be used in rhs
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! bv(i) = B_i / B ; derbv(i,j) = d (B_i / B) /d x,y,z
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
deryg = 1.0e-2_wp_*dbtot/Bres
bv = bv/btot
do jv=1,3
derbv(:,jv) = 1.0e-2_wp_*(dbv(:,jv) - bv(:)*dbtot(jv))/btot
end do
derxg(1) = 1.0e-2_wp_*drrdx*dpsidr*dxgdpsi
derxg(2) = 1.0e-2_wp_*drrdy*dpsidr*dxgdpsi
derxg(3) = 1.0e-2_wp_*dpsidz *dxgdpsi
end subroutine plas_deriv
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
subroutine disp_deriv(anv, sox, xg, yg, derxg, deryg, bv, derbv, &
dgr, ddgr, igrad, dery, anpl_, anpr, ddr, ddi, &
dersdst, derdnm_)
! Computes the dispersion relation, derivatives and other
! related quantities
!
! The mandatory outputs are used for both integrating the ray
! trajectory (`rhs` subroutine) and updating the ray state
! (`ywppla_upd` suborutine); while the optional ones are used for
! computing the absoprtion and current drive.
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
use const_and_precisions, only : zero, one, half, two
use gray_params, only : idst
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
implicit none
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! subroutine arguments
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
! Inputs
! refractive index N̅ vector, b̅ = B̅/B magnetic field direction
real(wp_), dimension(3), intent(in) :: anv, bv
! sign of polarisation mode: -1 ⇒ O, +1 ⇒ X
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
integer, intent(in) :: sox
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
! CMA diagram variables: X=(ω_pe/ω)², Y=ω_ce/ω
real(wp_), intent(in) :: xg, yg
! gradients of X, Y
real(wp_), dimension(3), intent(in) :: derxg, deryg
! gradients of the complex eikonal
real(wp_), dimension(3), intent(in) :: dgr ! ∇S_I
real(wp_), dimension(3, 3), intent(in) :: ddgr ! ∇∇S_I
! gradient of the magnetic field direction
real(wp_), dimension(3, 3), intent(in) :: derbv ! ∇b̅
! raytracing/beamtracing switch
integer, intent(in) :: igrad
! Outputs
! the actual derivatives: (∂Λ/∂x̅, -∂Λ/∂N̅)
real(wp_), dimension(6), intent(out) :: dery
! additional quantities:
! refractive index
real(wp_), optional, intent(out) :: anpl_, anpr ! N∥, N⊥
! real and imaginary part of the dispersion
real(wp_), optional, intent(out) :: ddr, ddi ! Λ, ∂Λ/∂N̅⋅∇S_I
! Jacobian ds/dσ, where s arclength, σ integration variable
real(wp_), optional, intent(out) :: dersdst
! |∂Λ/∂N̅|
real(wp_), optional, intent(out) :: derdnm_
! Note: assign values to missing optional arguments results in a segfault.
! Since some are always needed anyway, we store them here and copy
! them later, if needed:
real(wp_) :: anpl, derdnm
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! local variables
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
real(wp_) :: gr2, yg2, anpl2, del, dnl, duh, dan2sdnpl, an2, an2s
real(wp_) :: dan2sdxg, dan2sdyg, denom
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
real(wp_) :: derdom, dfdiadnpl, dfdiadxg, dfdiadyg, fdia, bdotgr
real(wp_), dimension(3) :: derdxv, danpldxv, derdnv, dbgr
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
an2 = dot_product(anv, anv) ! N²
anpl = dot_product(anv, bv) ! N∥ = N̅⋅B̅
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
! Shorthands used in the expressions below
yg2 = yg**2 ! Y²
anpl2 = anpl**2 ! N∥²
dnl = one - anpl2 ! 1 - N∥²
duh = one - xg - yg2 ! UH denom (duh=0 on the upper-hybrid resonance)
! Compute/copy optional outputs
if (present(anpr)) anpr = sqrt(max(an2 - anpl2, zero)) ! N⊥
if (present(anpl_)) anpl_ = anpl ! N∥
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
an2s = one
dan2sdxg = zero
dan2sdyg = zero
dan2sdnpl = zero
del = zero
fdia = zero
dfdiadnpl = zero
dfdiadxg = zero
dfdiadyg = zero
if(xg > zero) then
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
! Derivatives of the cold plasma refractive index
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
!
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
! N²s = 1 - X - XY²⋅(1 + N∥² ± √Δ)/[2(1 - X - Y²)]
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
!
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
! where Δ = (1 - N∥²)² + 4N∥²⋅(1 - X)/Y²
! + for the X mode, - for the O mode
! √Δ
del = sqrt(dnl**2 + 4.0_wp_*anpl2*(one - xg)/yg2)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! ∂(N²s)/∂X
improve some comments
2023-03-29 11:19:00 +02:00
! Note: this term is nonzero for X=0, but it multiplies terms
! proportional to X or ∂X/∂ψ which are zero outside the plasma.
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
dan2sdxg = - half*yg2*(one - yg2)*(one + anpl2 + sox*del)/duh**2 &
+ sox*xg*anpl2/(del*duh) - one
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! ∂(N²s)/∂Y
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
dan2sdyg = - xg*yg*(one - xg)*(one + anpl2 + sox*del)/duh**2 &
+ two*sox*xg*(one - xg)*anpl2/(yg*del*duh)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! ∂(N²s)/∂N∥
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
dan2sdnpl = - xg*yg2*anpl/duh &
- sox*xg*anpl*(two*(one - xg) - yg2*dnl)/(del*duh)
if(igrad > 0) then
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
! Derivatives used in the complex eikonal terms (beamtracing only)
block
real(wp_) :: ddelnpl2, ddelnpl2x, ddelnpl2y, derdel
! ∂²Δ/∂N∥²
ddelnpl2 = two*(two*(one - xg)*(one + 3.0_wp_*anpl2**2) &
- yg2*dnl**3)/yg2/del**3
! ∂²(N²s)/∂N∥²
fdia = - xg*yg2*(one + half*sox*ddelnpl2)/duh
! Intermediates results used right below
derdel = two*(one - xg)*anpl2*(one + 3.0_wp_*anpl2**2) &
- dnl**2*(one + 3.0_wp_*anpl2)*yg2
derdel = 4.0_wp_*derdel/(yg*del)**5
ddelnpl2y = two*(one - xg)*derdel
ddelnpl2x = yg*derdel
! ∂³(N²s)/∂N∥³
dfdiadnpl = 24.0_wp_*sox*xg*(one - xg)*anpl*(one - anpl2**2) &
/(yg2*del**5)
! ∂³(N²s)/∂N∥²∂X
dfdiadxg = - yg2*(one - yg2)/duh**2 - sox*yg2*((one - yg2) &
*ddelnpl2 + xg*duh*ddelnpl2x)/(two*duh**2)
! ∂³(N²s)/∂N∥²∂Y
dfdiadyg = - two*yg*xg*(one - xg)/duh**2 &
- sox*xg*yg*(two*(one - xg)*ddelnpl2 &
+ yg*duh*ddelnpl2y)/(two*duh**2)
end block
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
end if
end if
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
! ∇(N∥) = ∇(N̅⋅b̅) = N̅⋅∇b̅
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
danpldxv = matmul(anv, derbv)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
! ∂Λ/∂x̅ = - ∇(N²s) = -∂Λ/∂X ∇X - ∂Λ/∂Y ∇Y - ∂Λ/∂N∥ ∇(N∥)
derdxv = -(derxg*dan2sdxg + deryg*dan2sdyg + danpldxv*dan2sdnpl)
! ∂Λ/∂N̅ = 2N̅ - ∂(N²s)/∂N̅ = 2N̅ - ∂(N²s)/∂N∥ b̅
! Note: we used the identity ∇f(v̅⋅b̅) = f' ∇(v̅⋅b̅) = f'b̅.
derdnv = two*anv - dan2sdnpl*bv
! ∂Λ/∂ω = ∂N²/∂ω - ∂N²s/∂X⋅∂X/∂ω - ∂N²s/∂Y⋅∂Y/∂ω - ∂N²s/∂N∥⋅∂N∥/∂ω
! Notes: 1. N depends on ω: N²=c²k²/ω² ⇒ ∂N²/∂ω = -2N²/ω
! N∥=ck∥/ω ⇒ ∂N∥/∂ω = -N∥/ω
! 2. derdom is actually ω⋅∂Λ/∂ω, see below for the reason.
! 3. N gains a dependency on ω because Λ(∇S, ω) is computed
! on the constrains Λ=0.
derdom = -two*an2 + two*xg*dan2sdxg + yg*dan2sdyg + anpl*dan2sdnpl
if (igrad > 0) then
! Complex eikonal terms added to the above expressions
block
real(wp_) :: dgr2(3)
bdotgr = dot_product(bv, dgr) ! b̅⋅∇S_I
gr2 = dot_product(dgr, dgr) ! |∇S_I|²
dgr2 = 2 * matmul(ddgr, dgr) ! ∇|∇S_I|² = 2 ∇∇S_I⋅∇S_I
! ∇(b̅⋅∇S_I) = ∇b̅ᵗ ∇S_I + b̅ᵗ ∇∇S_I
! Notes: 1. We are using the convention ∇b̅_ij = ∂b_i/∂x_j.
! 2. Fortran doesn't distinguish between column/row vectors,
! so matmul(A, v̅) ≅ Av̅ and matmul(v̅, A) ≅ v̅ᵗA ≅ Aᵗv̅.
dbgr = matmul(dgr, derbv) + matmul(bv, ddgr)
! ∂Λ/∂x̅ += - ∇(|∇S_I|²) + ½ ∇[(b̅⋅∇S_I)² ∂²N²s/∂N∥²]
derdxv = derdxv - dgr2 + fdia*bdotgr*dbgr + half*bdotgr**2 &
* (derxg*dfdiadxg + deryg*dfdiadyg + danpldxv*dfdiadnpl)
! ∂Λ/∂N̅ += ½(b̅⋅∇S_I)² ∂³(N²s)/∂N∥³ b̅
! Note: we used again the identity ∇f(v̅⋅b̅) = f'b̅.
derdnv = derdnv + half*bdotgr**2*dfdiadnpl*bv
! ∂Λ/∂ω += ∂|∇S_I|²/∂ω + ½∂(b⋅∇S_I)²/∂ω + ½(b̅⋅∇S_I)² ∂/∂ω (∂²N²s/∂N∥²)
! Note: as above ∇S_I gains a dependency on ω
derdom = derdom + two*gr2 - bdotgr**2 &
* (fdia + xg*dfdiadxg + half*yg*dfdiadyg &
+ half*anpl*dfdiadnpl)
end block
end if
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
derdnm = norm2(derdnv)
! Denominator of the r.h.s, depending on the
! choice of the integration variable σ:
!
! dx̅/dσ = + ∂Λ/∂N̅ / denom
! dN̅/dσ = - ∂Λ/∂x̅ / denom
!
select case (idst)
case (0) ! σ=s, arclength
! denom = |∂Λ/∂N̅|
! Proof: Normalising ∂Λ/∂N̅ (∥ to the group velocity)
! simply makes σ the arclength parameter s.
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
denom = derdnm
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
case (1) ! σ=ct, time
! denom = -ω⋅∂Λ/∂ω
! Proof: The Hamilton equations are
!
! dx̅/dt = + ∂H/∂k̅ (H=ℏΩ, p=ℏk̅)
! dp̅/dt = - ∂H/∂x̅
!
! where Ω(x̅, k̅) is implicitely defined by the dispersion
! D(k̅, ω, x̅) = 0. By differentiating the latter we get:
!
! ∂Ω/∂x̅ = - ∂D/∂x̅ / ∂D/∂ω = - ∂Λ/∂x̅ / ∂Λ/∂ω
! ∂Ω/∂k̅ = - ∂D/∂k̅ / ∂D/∂ω = - ∂Λ/∂k̅ / ∂Λ/∂ω
!
! with Λ=D/k₀, k₀=ω/c. Finally, substituting k̅=k₀N̅:
!
! dx̅/d(ct) = + ∂Λ/∂N̅ / (-ω⋅∂Λ/∂ω)
! dN̅/d(ct) = - ∂Λ/∂x̅ / (-ω⋅∂Λ/∂ω)
!
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
denom = -derdom
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
case (2) ! s=S_R, phase
! denom = N̅⋅∂Λ/∂N̅
! Note: This parametrises the curve by the value
! of the (real) phase, with the wave frozen in time.
! Proof: By definition N̅ = k̅/k₀ = ∇S. Using the gradient
! theorem on the ray curve parametrised by the arclength
!
! S(s) = ∫₀^x̅(s) N̅⋅dl̅ = ∫₀^s N̅(σ)⋅dx̅/ds ds
!
! Differentiating gives dS = N̅⋅dx̅/ds ds, so
!
! dS = N̅⋅∂Λ/∂N̅ / |∂Λ/∂N̅| ds ⇒
!
! dx̅/dS = + ∂Λ/∂N̅ / N̅⋅∂Λ/∂N̅
! dN̅/dS = - ∂Λ/∂x̅ / N̅⋅∂Λ/∂N̅
!
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
denom = dot_product(anv, derdnv)
end select
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
! Jacobian ds/dσ, where s is the arclength,
! for computing integrals in dσ, like:
!
! τ = ∫α(s)ds = ∫α(σ)(ds/dσ)dσ
!
if (present(dersdst)) dersdst = derdnm/denom
! |∂Λ/∂N̅|: used in the α computation (see alpha_effj)
if (present(derdnm_)) derdnm_ = derdnm
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! r.h.s. vector
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
dery(1:3) = derdnv(:)/denom ! +∂Λ/∂N̅
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
dery(4:6) = -derdxv(:)/denom ! -∂Λ/∂x̅
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
src/gray_core.f90: make some {disp,plas}_deriv outputs optional Some of the outputs of disp_deriv and plas_deriv are only needed when updating the local plasma quantities (ywppla_upd) and not when integrating the raytracing equations (rkstep). This change save some unnecessary computations and variable definitions. Also add some comments to disp_deriv
2023-03-29 22:13:43 +02:00
if (present(ddr) .or. present(ddi)) then
! Dispersion relation (geometric optics)
! ddr ← Λ = N² - N²s(X,Y,N∥) = 0
an2s = one - xg - half*xg*yg2*(one + anpl2 + sox*del)/duh
ddr = an2 - an2s
end if
if (present(ddr) .and. igrad > 0) then
! Dispersion relation (complex eikonal)
! ddr ← Λ = N² - N²s - |∇S_I|² + ½ (b̅⋅∇S_I)² ∂²N²s/∂N∥²
ddr = ddr - gr2 - half*bdotgr**2*fdia ! real part
end if
! Note: we have to return ddi even for igrad=0 because
! it's printed to udisp unconditionally
if (present(ddi)) then
! Dispersion relation (complex eikonal)
! ddi ← ∂Λ/∂N̅⋅∇S_I
ddi = merge(dot_product(derdnv, dgr), zero, igrad > 0) ! imaginary part
end if
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
end subroutine disp_deriv
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
subroutine alpha_effj(params, psinv, X, Y, density, temperature, &
k0, Bres, derdnm, Npl, Npr_cold, sox, &
Npr, alpha, dIdp, nhmin, nhmax, iokhawa, error)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! Computes the absorption coefficient and effective current
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
use const_and_precisions, only : pi, mc2=>mc2_
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
use gray_params, only : ecrh_cd_parameters
use coreprofiles, only : fzeff
use equilibrium, only : sgnbphi
use dispersion, only : harmnumber, warmdisp
use eccd, only : setcdcoeff, eccdeff, fjch0, fjch, fjncl
improve error handling in the gray_main routine - rename errocodes → gray_errors - restructure the errors into a `error_spec` type - make the list of errors easily extensible - rewrite the `print_errn`, `print_errhcd` (now `print_err_raytracing`, `print_err_ecrh_cd`) subroutine to handle arbitrary errors - add functions to easily manipulate errors (`raise_error`, `has_error`, `is_critical`) - remove print statements from quadpack - log all errors to stderr using the logger module
2022-07-14 00:38:34 +02:00
use gray_errors, only : negative_absorption, raise_error
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
use magsurf_data, only : fluxval
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
implicit none
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! subroutine arguments
! Inputs
! ECRH & CD parameters
type(ecrh_cd_parameters) :: params
! poloidal flux ψ
real(wp_), intent(in) :: psinv
! CMA diagram variables: X=(ω_pe/ω)², Y=ω_ce/ω
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
real(wp_), intent(in) :: X, Y
! densityity [10¹⁹ m⁻³], temperature [keV]
real(wp_), intent(in) :: density, temperature
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! vacuum wavenumber k₀=ω/c, resonant B field
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
real(wp_), intent(in) :: k0, Bres
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! group velocity: |∂Λ/∂N̅| where Λ=c²/ω²⋅D_R
real(wp_), intent(in) :: derdnm
! refractive index: N∥, N⊥ (cold dispersion)
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
real(wp_), intent(in) :: Npl, Npr_cold
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! sign of polarisation mode: -1 ⇒ O, +1 ⇒ X
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
integer, intent(in) :: sox
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! Outputs
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
! orthogonal refractive index N⊥ (solution of the warm dispersion)
complex(wp_), intent(out) :: Npr
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! absorption coefficient, current density
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
real(wp_), intent(out) :: alpha, dIdp
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! lowest/highest resonant harmonic numbers
integer, intent(out) :: nhmin, nhmax
! ECCD/overall error codes
integer, intent(out) :: iokhawa, error
! local variables
real(wp_) :: rbavi, rrii, rhop
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
integer :: nlarmor, ithn, ierrcd
real(wp_) :: mu, rbn, rbx
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
real(wp_) :: zeff, cst2, bmxi, bmni, fci
real(wp_), dimension(:), pointer :: eccdpar=>null()
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
real(wp_) :: effjcd, effjcdav, Btot
complex(wp_) :: e(3)
alpha = 0
Npr = 0
dIdp = 0
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
nhmin = 0
nhmax = 0
iokhawa = 0
error = 0
! Absorption computation
! Skip when the temperature is zero (no plasma)
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
if (temperature <= 0) return
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! Skip when the lowest resonant harmonic number is zero
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
mu = mc2/temperature ! μ=(mc²/kT)
call harmnumber(Y, mu, Npl**2, params%iwarm == 1, nhmin, nhmax)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
if (nhmin <= 0) return
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
! Solve the full dispersion only when needed
if (params%iwarm /= 4 .or. params%ieccd /= 0) then
nlarmor = max(params%ilarm, nhmax)
if (params%ieccd /= 0) then
! Compute the polarisation vector only when current drive is on
call warmdisp(X, Y, mu, Npl, Npr_cold, sox, error, Npr, e, &
model=params%iwarm, nlarmor=nlarmor, &
max_iters=abs(params%imx), fallback=params%imx < 0)
else
call warmdisp(X, Y, mu, Npl, Npr_cold, sox, error, Npr, &
model=params%iwarm, nlarmor=nlarmor, &
max_iters=abs(params%imx), fallback=params%imx < 0)
end if
end if
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
! Compute α from the solution of the dispersion relation
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! The absoption coefficient is defined as
!
! α = 2 Im(k̅)⋅s̅
!
! where s̅ = v̅_g/|v_g|, the direction of the energy flow.
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
! Since v̅_g = - ∂Λ/∂N̅ / ∂Λ/∂ω, using the cold dispersion
! relation, we have that
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
!
! s̅ = ∂Λ/∂N̅ / |∂Λ/∂N̅|
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
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! = [2N̅ - ∂(N²s)/∂N∥ b̅
! + ½(b̅⋅∇S_I)² ∂³(N²s)/∂N∥³ b̅] / |∂Λ/∂N̅|
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
!
! Assuming Im(k∥)=0:
!
! α = 4 Im(k⊥)⋅N⊥ / |∂Λ/∂N̅|
!
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
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block
real(wp_) :: k_im
k_im = k0 * Npr%im ! imaginary part of k⊥
alpha = 4 * k_im*Npr_cold / derdnm
end block
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
if (alpha < 0) then
improve error handling in the gray_main routine - rename errocodes → gray_errors - restructure the errors into a `error_spec` type - make the list of errors easily extensible - rewrite the `print_errn`, `print_errhcd` (now `print_err_raytracing`, `print_err_ecrh_cd`) subroutine to handle arbitrary errors - add functions to easily manipulate errors (`raise_error`, `has_error`, `is_critical`) - remove print statements from quadpack - log all errors to stderr using the logger module
2022-07-14 00:38:34 +02:00
error = raise_error(error, negative_absorption)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
return
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
end if
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! Current drive computation
if (params%ieccd <= 0) return
zeff = fzeff(psinv)
ithn = 1
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
if (nlarmor > nhmin) ithn = 2
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
rhop = sqrt(psinv)
call fluxval(rhop, rri=rrii, rbav=rbavi, bmn=bmni, bmx=bmxi, fc=fci)
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
Btot = Y*Bres
rbn = Btot/bmni
rbx = Btot/bmxi
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
select case(params%ieccd)
case(1)
! Cohen model
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
call setcdcoeff(zeff, rbn, rbx, cst2, eccdpar)
call eccdeff(Y, Npl, Npr%re, density, mu, e, nhmin, nhmax, &
ithn, cst2, fjch, eccdpar, effjcd, iokhawa, ierrcd)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
case(2)
! No trapping
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
call setcdcoeff(zeff, cst2, eccdpar)
call eccdeff(Y, Npl, Npr%re, density, mu, e, nhmin, nhmax, &
ithn, cst2, fjch0, eccdpar, effjcd, iokhawa, ierrcd)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
case default
! Neoclassical model
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
call setcdcoeff(zeff, rbx, fci, mu, rhop, cst2, eccdpar)
call eccdeff(Y, Npl, Npr%re, density, mu, e, nhmin, nhmax, &
ithn, cst2, fjncl, eccdpar, effjcd, iokhawa, ierrcd)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
end select
error = error + ierrcd
if (associated(eccdpar)) deallocate(eccdpar)
! current drive efficiency <j/p> [A⋅m/W]
effjcdav = rbavi*effjcd
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
dIdp = sgnbphi * effjcdav / (2*pi*rrii)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
end subroutine alpha_effj
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
subroutine set_pol(ywrk0, bres, sox, ipol, psipol0, chipol0, ext0, eyt0)
use const_and_precisions, only : degree, zero, one, half, im
use beamdata, only : nray,nrayth
use equilibrium, only : bfield
use polarization, only : pol_limit, polellipse, &
stokes_ce, stokes_ell
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
implicit none
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! subroutine arguments
real(wp_), dimension(6, nray), intent(in) :: ywrk0
src/dispersion.f90: cleanup - merge branch with a method to control the speed of iteration and improve the convergence of `warmdisp` (thanks Thomas) - unify `diel_tens_fr` and `diel_tens_wr` into a single subroutine, `dielectric_tensor` - stay as close as possible to the notation of Daniela Farina's paper - make `sox` an integer - mark more subroutines as pure - add more comments
2022-05-20 13:10:49 +02:00
real(wp_), intent(in) :: bres
integer, intent(in) :: sox, ipol
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
real(wp_), intent(inout) :: psipol0, chipol0
complex(wp_), dimension(nray), intent(out) :: ext0, eyt0
! local variables
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
integer :: j,k,jk
real(wp_), dimension(3) :: xmv, anv, bv
real(wp_) :: rm, csphi, snphi, bphi, br, bz, qq, uu, vv, deltapol
j=1
k=0
do jk=1,nray
k=k+1
if(jk == 2 .or. k > nrayth) then
j=j+1
k=1
end if
if(ipol == 0) then
xmv=ywrk0(1:3,jk)*0.01_wp_ ! convert from cm to m
anv=ywrk0(4:6,jk)
rm=sqrt(xmv(1)**2+xmv(2)**2)
csphi=xmv(1)/rm
snphi=xmv(2)/rm
call bfield(rm,xmv(3),bphi,br,bz)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
! bv(i) = B_i in cartesian coordinates
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
bv(1)=br*csphi-bphi*snphi
bv(2)=br*snphi+bphi*csphi
bv(3)=bz
call pol_limit(anv,bv,bres,sox,ext0(jk),eyt0(jk))
if (jk == 1) then
call stokes_ce(ext0(jk),eyt0(jk),qq,uu,vv)
call polellipse(qq,uu,vv,psipol0,chipol0)
psipol0=psipol0/degree ! convert from rad to degree
chipol0=chipol0/degree
end if
else
call stokes_ell(chipol0*degree,psipol0*degree,qq,uu,vv)
if(qq**2 < one) then
deltapol=asin(vv/sqrt(one - qq**2))
ext0(jk)= sqrt(half*(one + qq))
eyt0(jk)= sqrt(half*(one - qq))*exp(-im*deltapol)
else
ext0(jk)= one
eyt0(jk)= zero
end if
endif
end do
end subroutine set_pol
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
subroutine cniteq(rqgrid,zqgrid,matr2dgrid,nr,nz,h,ncon,npts,icount,rcon,zcon)
! v2.01 12/07/95 -- written by d v bartlett, jet joint undertaking.
! (based on an older code)
implicit none
! arguments
integer, intent(in) :: nr,nz
real(wp_), dimension(nr), intent(in) :: rqgrid
real(wp_), dimension(nz), intent(in) :: zqgrid
real(wp_), dimension(nr,nz), intent(in) :: matr2dgrid
real(wp_), intent(in) :: h
integer, intent(inout) :: ncon, icount
integer, dimension(ncon), intent(out) :: npts
real(wp_), dimension(icount), intent(out) :: rcon,zcon
! local variables
integer :: i,j,k,l,nrqmax,iclast,mpl,ix,jx,mxr,n1,jm,jfor,lda,ldb
integer :: jabs,jnb,kx,ikx,itm,inext,in
integer, dimension(3,2) :: ja
integer, dimension(icount/2-1) :: lx
real(wp_) :: drgrd,dzgrd,ah,adn,px,x,y
real(wp_), dimension(nr*nz) :: a
logical :: flag1
px = 0.5_wp_
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
a = reshape(matr2dgrid, [nr*nz])
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
rcon = 0.0_wp_
zcon = 0.0_wp_
nrqmax = nr
drgrd = rqgrid(2) - rqgrid(1)
dzgrd = zqgrid(2) - zqgrid(1)
ncon = 0
npts = 0
iclast = 0
icount = 0
mpl = 0
ix = 0
mxr = nrqmax * (nz - 1)
n1 = nr - 1
do jx=2,n1
do jm=jx,mxr,nrqmax
j = jm + nrqmax
ah=a(j)-h
if (ah <= 0.0_wp_ .and. a(jm) > h .or. &
ah > 0.0_wp_ .and. a(jm) <= h) then
ix=ix+1
lx(ix)=-j
end if
if (ah <= 0.0_wp_ .and. a(j-1) > h .or. &
ah > 0.0_wp_ .and. a(j-1) <= h) then
ix=ix+1
lx(ix)=j
end if
end do
end do
do jm=nr,mxr,nrqmax
j = jm + nrqmax
ah=a(j)-h
if (ah <= 0.0_wp_ .and. a(j-1) > h .or. &
ah > 0.0_wp_ .and. a(j-1) <= h) then
ix=ix+1
lx(ix)=j
end if
if (ah <= 0.0_wp_ .and. a(jm) > h .or. &
ah > 0.0_wp_ .and. a(jm) <= h) then
ix=ix+1
lx(ix)=-j
end if
end do
do jm=1,mxr,nrqmax
j = jm + nrqmax
if (a(j) <= h .and. a(jm) > h .or. &
a(j) > h .and. a(jm) <= h) then
ix=ix+1
lx(ix) =-j
end if
end do
do j=2,nr
if (a(j) <= h .and. a(j-1) > h .or. &
a(j) > h .and. a(j-1) <= h) then
ix=ix+1
lx(ix)=j
end if
end do
if(ix<=0) return
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
bb: do
in=ix
jx=lx(in)
jfor=0
lda=1
ldb=2
do
if(jx<0) then
jabs=-jx
jnb = jabs - nrqmax
else
jabs=jx
jnb=jabs-1
end if
adn=a(jabs)-a(jnb)
if(adn/=0) px=(a(jabs)-h)/adn
kx = (jabs - 1) / nrqmax
ikx = jabs - nrqmax * kx - 1
if(jx<0) then
x = drgrd * ikx
y = dzgrd * (kx - px)
else
x = drgrd * (ikx - px)
y = dzgrd * kx
end if
icount = icount + 1
rcon(icount) = x + rqgrid(1)
zcon(icount) = y + zqgrid(1)
mpl= icount
itm = 1
ja(1,1) = jabs + nrqmax
j=1
if(jx<=0) then
ja(1,1) = -jabs-1
j=2
end if
ja(2,1) = -ja(1,1)
ja(3,1) = -jx + 1 - nrqmax
ja(3,2) = -jx
ja(j,2) = jabs - nrqmax
k= 3-j
ja(k,2) = 1-jabs
if (kx<=0 .or. ikx<=0) then
lda=1
ldb=lda
else if (ikx + 1 - nr >= 0 .and. jx <= 0) then
lda=2
ldb=lda
else if(jfor/=0) then
lda=2
do i=1,3
if(jfor==ja(i,2)) then
lda=1
exit
end if
end do
ldb=lda
end if
flag1=.false.
aa: do k=1,3
do l=lda,ldb
do i=1,ix
if(lx(i)==ja(k,l)) then
itm=itm+1
inext= i
if(jfor/=0) exit aa
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
if(itm > 3) then
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
flag1=.true.
exit aa
end if
end if
end do
end do
end do aa
if(.not.flag1) then
lx(in)=0
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
if(itm == 1) exit
end if
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
jfor=jx
jx=lx(inext)
in = inext
end do
do
if(lx(ix)/=0) then
if(mpl>=4) then
ncon = ncon + 1
npts(ncon) = icount - iclast
iclast = icount
end if
exit
end if
ix= ix-1
if(ix<=0) exit bb
end do
end do bb
if(mpl >= 4) then
ncon = ncon + 1
npts(ncon) = icount - iclast
iclast = icount
end if
end subroutine cniteq
skip print_headers with no active units
2022-05-03 23:16:21 +02:00
subroutine print_headers(params)
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
! Prints the headers of all gray_main output tables
skip print_headers with no active units
2022-05-03 23:16:21 +02:00
use units, only : uprj0, uwbm, udisp, ucenr, uoutr, upec, usumm, &
unit_active, active_units
use gray_params, only : gray_parameters, headw, headl, print_parameters
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
implicit none
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
2021-12-15 02:31:09 +01:00
! subroutine arguments
skip print_headers with no active units
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type(gray_parameters), intent(in) :: params
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
src: use derived type arguments (work in progress) This change structures the arguments of most functions, in particular gray_main, into well-defined categories using derived types. All types are defined in the gray_params.f90 (location subject to change) and are organised as follows: gray_parameters (statically allocated data) ├── antenna_parameters ├── ecrh_cd_parameters ├── equilibrium_parameters ├── misc_parameters ├── output_parameters ├── profiles_parameters └── raytracing_parameters gray_data - inputs of gray_main (dynamically-allocated arrays) ├── equilibrium_data └── profiles_data gray_results - outputs of gray_main (dynamically-allocated arrays)
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! local variables
src: implement toggling of output units This actually implements the --units option
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integer :: i, j
integer :: main_units(8)
character(256) :: main_headers(8)
skip print_headers with no active units
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character(len=headw), dimension(headl) :: header
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
main_units = [uprj0, uprj0+1, uwbm, udisp, ucenr, uoutr, upec, usumm]
main_headers(1) = '#sst j k xt yt zt rt'
main_headers(2) = '#sst j k xt yt zt rt'
main_headers(3) = '#sst w1 w2'
main_headers(4) = '#sst Dr_Nr Di_Nr'
main_headers(5) = '#sst R z phi psin rhot ne Te Btot Bx By Bz Nperp ' &
// 'Npl Nx Ny Nz ki alpha tau Pt dIds nhmin nhmax ' &
// 'iohkw index_rt ddr Xg Yg dXgdx dXgdy dXgdz'
main_headers(6) = '#i k sst x y R z psin tau Npl alpha index_rt'
main_headers(7) = '#rhop rhot Jphi Jcdb dPdV Icdins Pins index_rt'
main_headers(8) = '#Icd Pa Jphip dPdVp rhotj rhotjava rhotp rhotpav ' &
// 'drhotjava drhotpav ratjamx ratjbmx stmx psipol ' &
// 'chipol index_rt Jphimx dPdVmx drhotj drhotp P0 ' &
// 'cplO cplX'
skip print_headers with no active units
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if (all(active_units == 0)) return
call print_parameters(params, header)
src: implement toggling of output units This actually implements the --units option
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do i=1,size(main_units)
if (unit_active(main_units(i))) then
skip print_headers with no active units
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do j=1,size(header)
write (main_units(i), '(1x,a)') header(j)
src: implement toggling of output units This actually implements the --units option
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end do
write (main_units(i), '(1x,a)') trim(main_headers(i))
end if
added file headers with input parameters
2016-04-27 16:37:57 +02:00
end do
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
end subroutine print_headers
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
src/gray_core.f90: print profiles up to ψ_bnd
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subroutine print_prof(params)
! Prints the (input) plasma kinetic profiles (unit 55)
src: implement toggling of output units This actually implements the --units option
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src/gray_core.f90: print profiles up to ψ_bnd
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use gray_params, only : profiles_parameters
simplify handling of splines This adds a new `splines` module which implements a high-level interface for creating and evaluating splines and rewrite almost all modules to use it. Also, notably: 1. both `simplespline` and DIERCKX splines can now used with a uniform interface 2. most complexity due to handling working space arrays is gone 3. memory management has been significantly simplified too
2022-12-18 14:09:40 +01:00
use equilibrium, only : q_spline, fq, frhotor, tor_curr_psi
use coreprofiles, only : density, temp
use units, only : uprfin, unit_active
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
implicit none
src: implement toggling of output units This actually implements the --units option
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src/gray_core.f90: print profiles up to ψ_bnd
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! suborutine arguments
type(profiles_parameters), intent(in) :: params
src: implement toggling of output units This actually implements the --units option
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! local constants
real(wp_), parameter :: eps = 1.e-4_wp_
! local variables
src/gray_core.f90: print profiles up to ψ_bnd
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integer :: i, N_data, N_tail
real(wp_) :: rhot, jphi, dens, ddens
real(wp_) :: psin, dpsin, psin_last
src: implement toggling of output units This actually implements the --units option
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if (.not. unit_active(uprfin)) return
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
src/gray_core.f90: print profiles up to ψ_bnd
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! N of profiles data points
N_data = q_spline%ndata
! parameters for the density tail (numerical profiles only)
if (params%iprof == 1) then
N_tail = N_data / 10 ! N of density tail points
psin_last = q_spline%data(N_data) ! last data point
dpsin = (params%psnbnd - psin_last) / N_tail ! Δψ for uniform grid
else
N_tail = 0
end if
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
write (uprfin, *) '#psi rhot ne Te q Jphi'
src/gray_core.f90: print profiles up to ψ_bnd
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do i = 1, N_data + N_tail
if (i > N_data) then
psin = psin_last + dpsin*(i - N_data)
else
psin = q_spline%data(i)
end if
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
rhot = frhotor(sqrt(psin))
call density(psin, dens, ddens)
simplify handling of splines This adds a new `splines` module which implements a high-level interface for creating and evaluating splines and rewrite almost all modules to use it. Also, notably: 1. both `simplespline` and DIERCKX splines can now used with a uniform interface 2. most complexity due to handling working space arrays is gone 3. memory management has been significantly simplified too
2022-12-18 14:09:40 +01:00
jphi = tor_curr_psi(max(eps, psin))
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
write (uprfin, '(12(1x,e12.5))') &
simplify handling of splines This adds a new `splines` module which implements a high-level interface for creating and evaluating splines and rewrite almost all modules to use it. Also, notably: 1. both `simplespline` and DIERCKX splines can now used with a uniform interface 2. most complexity due to handling working space arrays is gone 3. memory management has been significantly simplified too
2022-12-18 14:09:40 +01:00
psin, rhot, dens, temp(psin), fq(psin), jphi*1.e-6_wp_
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
end do
end subroutine print_prof
subroutine print_bres(bres)
src: implement toggling of output units This actually implements the --units option
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! Prints the EC resonance surface table (unit 70)
simplify handling of splines This adds a new `splines` module which implements a high-level interface for creating and evaluating splines and rewrite almost all modules to use it. Also, notably: 1. both `simplespline` and DIERCKX splines can now used with a uniform interface 2. most complexity due to handling working space arrays is gone 3. memory management has been significantly simplified too
2022-12-18 14:09:40 +01:00
use equilibrium, only : rmnm, rmxm, zmnm, zmxm, bfield, q_spline
use units, only : ubres, unit_active
src: implement toggling of output units This actually implements the --units option
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re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
implicit none
src: implement toggling of output units This actually implements the --units option
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! subroutine arguments
real(wp_), intent(in) :: bres
! local constants
integer, parameter :: icmx = 2002
! local variables
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
integer :: j,k,n,nconts,nctot
integer, dimension(10) :: ncpts
real(wp_) :: dr,dz,btmx,btmn,zzk,rrj,bbphi,bbr,bbz,bbb
real(wp_), dimension(icmx) :: rrcb,zzcb
simplify handling of splines This adds a new `splines` module which implements a high-level interface for creating and evaluating splines and rewrite almost all modules to use it. Also, notably: 1. both `simplespline` and DIERCKX splines can now used with a uniform interface 2. most complexity due to handling working space arrays is gone 3. memory management has been significantly simplified too
2022-12-18 14:09:40 +01:00
real(wp_) :: rv(q_spline%ndata), zv(q_spline%ndata)
real(wp_), dimension(q_spline%ndata,q_spline%ndata) :: btotal
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
if (.not. unit_active(ubres)) return
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
simplify handling of splines This adds a new `splines` module which implements a high-level interface for creating and evaluating splines and rewrite almost all modules to use it. Also, notably: 1. both `simplespline` and DIERCKX splines can now used with a uniform interface 2. most complexity due to handling working space arrays is gone 3. memory management has been significantly simplified too
2022-12-18 14:09:40 +01:00
dr = (rmxm - rmnm)/(q_spline%ndata - 1)
dz = (zmxm - zmnm)/(q_spline%ndata - 1)
do j=1,q_spline%ndata
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
rv(j) = rmnm + dr*(j - 1)
zv(j) = zmnm + dz*(j - 1)
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
end do
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
! Btotal on psi grid
btmx = -1.0e30_wp_
btmn = 1.0e30_wp_
simplify handling of splines This adds a new `splines` module which implements a high-level interface for creating and evaluating splines and rewrite almost all modules to use it. Also, notably: 1. both `simplespline` and DIERCKX splines can now used with a uniform interface 2. most complexity due to handling working space arrays is gone 3. memory management has been significantly simplified too
2022-12-18 14:09:40 +01:00
do k = 1, q_spline%ndata
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
zzk = zv(k)
simplify handling of splines This adds a new `splines` module which implements a high-level interface for creating and evaluating splines and rewrite almost all modules to use it. Also, notably: 1. both `simplespline` and DIERCKX splines can now used with a uniform interface 2. most complexity due to handling working space arrays is gone 3. memory management has been significantly simplified too
2022-12-18 14:09:40 +01:00
do j = 1, q_spline%ndata
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
rrj = rv(j)
call bfield(rrj, zzk, bbphi, bbr, bbz)
btotal(j,k) = sqrt(bbr**2 + bbz**2 + bbphi**2)
if(btotal(j,k) >= btmx) btmx = btotal(j,k)
if(btotal(j,k) <= btmn) btmn = btotal(j,k)
end do
end do
! compute Btot=Bres/n with n=1,5
write (ubres, *) '#i Btot R z'
simplify handling of splines This adds a new `splines` module which implements a high-level interface for creating and evaluating splines and rewrite almost all modules to use it. Also, notably: 1. both `simplespline` and DIERCKX splines can now used with a uniform interface 2. most complexity due to handling working space arrays is gone 3. memory management has been significantly simplified too
2022-12-18 14:09:40 +01:00
do n = 1, 5
always use generic math functions This replaces double precision-specific function in order to allow building GRAY with other real kinds, for example single or quadruple precision.
2023-09-20 16:03:08 +02:00
bbb = bres/n
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
if (bbb >= btmn .and. bbb <= btmx) then
nconts = size(ncpts)
nctot = size(rrcb)
simplify handling of splines This adds a new `splines` module which implements a high-level interface for creating and evaluating splines and rewrite almost all modules to use it. Also, notably: 1. both `simplespline` and DIERCKX splines can now used with a uniform interface 2. most complexity due to handling working space arrays is gone 3. memory management has been significantly simplified too
2022-12-18 14:09:40 +01:00
call cniteq(rv, zv, btotal, q_spline%ndata, q_spline%ndata, bbb, &
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
nconts, ncpts, nctot, rrcb, zzcb)
simplify handling of splines This adds a new `splines` module which implements a high-level interface for creating and evaluating splines and rewrite almost all modules to use it. Also, notably: 1. both `simplespline` and DIERCKX splines can now used with a uniform interface 2. most complexity due to handling working space arrays is gone 3. memory management has been significantly simplified too
2022-12-18 14:09:40 +01:00
do j = 1, nctot
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
write (ubres, '(i6,12(1x,e12.5))') j, bbb, rrcb(j), zzcb(j)
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
end do
end if
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
write (ubres, *)
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
end do
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
end subroutine print_bres
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
subroutine print_maps(bres, xgcn, r0, anpl0)
! Prints several input quantities on a regular grid (unit 72)
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
use gray_params, only : iequil
use equilibrium, only : rmnm, rmxm, zmnm, zmxm, equian, equinum_psi, &
simplify handling of splines This adds a new `splines` module which implements a high-level interface for creating and evaluating splines and rewrite almost all modules to use it. Also, notably: 1. both `simplespline` and DIERCKX splines can now used with a uniform interface 2. most complexity due to handling working space arrays is gone 3. memory management has been significantly simplified too
2022-12-18 14:09:40 +01:00
equinum_fpol, q_spline
some additional output prints (2D maps and Bcart, Ncart along central ray)
2016-02-12 17:49:00 +01:00
use coreprofiles, only : density, temp
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
use units, only : umaps, unit_active
some additional output prints (2D maps and Bcart, Ncart along central ray)
2016-02-12 17:49:00 +01:00
implicit none
src: implement toggling of output units This actually implements the --units option
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! subroutine arguments
some additional output prints (2D maps and Bcart, Ncart along central ray)
2016-02-12 17:49:00 +01:00
real(wp_), intent(in) :: bres,xgcn,r0,anpl0
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
! local variables
some additional output prints (2D maps and Bcart, Ncart along central ray)
2016-02-12 17:49:00 +01:00
integer :: j,k
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
real(wp_) :: dr, dz, zk, rj, bphi, br, bz, btot, &
psin, ne, dne, te, xg, yg, anpl
simplify handling of splines This adds a new `splines` module which implements a high-level interface for creating and evaluating splines and rewrite almost all modules to use it. Also, notably: 1. both `simplespline` and DIERCKX splines can now used with a uniform interface 2. most complexity due to handling working space arrays is gone 3. memory management has been significantly simplified too
2022-12-18 14:09:40 +01:00
real(wp_), dimension(q_spline%ndata) :: r, z
some additional output prints (2D maps and Bcart, Ncart along central ray)
2016-02-12 17:49:00 +01:00
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
if (.not. unit_active(umaps)) return
simplify handling of splines This adds a new `splines` module which implements a high-level interface for creating and evaluating splines and rewrite almost all modules to use it. Also, notably: 1. both `simplespline` and DIERCKX splines can now used with a uniform interface 2. most complexity due to handling working space arrays is gone 3. memory management has been significantly simplified too
2022-12-18 14:09:40 +01:00
dr = (rmxm-rmnm)/(q_spline%ndata - 1)
dz = (zmxm-zmnm)/(q_spline%ndata - 1)
do j=1,q_spline%ndata
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
r(j) = rmnm + dr*(j - 1)
z(j) = zmnm + dz*(j - 1)
some additional output prints (2D maps and Bcart, Ncart along central ray)
2016-02-12 17:49:00 +01:00
end do
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
write (umaps, *) '#R z psin Br Bphi Bz Btot ne Te X Y Npl'
simplify handling of splines This adds a new `splines` module which implements a high-level interface for creating and evaluating splines and rewrite almost all modules to use it. Also, notably: 1. both `simplespline` and DIERCKX splines can now used with a uniform interface 2. most complexity due to handling working space arrays is gone 3. memory management has been significantly simplified too
2022-12-18 14:09:40 +01:00
do j = 1, q_spline%ndata
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
rj = r(j)
anpl = anpl0 * r0/rj
simplify handling of splines This adds a new `splines` module which implements a high-level interface for creating and evaluating splines and rewrite almost all modules to use it. Also, notably: 1. both `simplespline` and DIERCKX splines can now used with a uniform interface 2. most complexity due to handling working space arrays is gone 3. memory management has been significantly simplified too
2022-12-18 14:09:40 +01:00
do k = 1, q_spline%ndata
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
zk = z(k)
some additional output prints (2D maps and Bcart, Ncart along central ray)
2016-02-12 17:49:00 +01:00
if (iequil < 2) then
simplify handling of splines This adds a new `splines` module which implements a high-level interface for creating and evaluating splines and rewrite almost all modules to use it. Also, notably: 1. both `simplespline` and DIERCKX splines can now used with a uniform interface 2. most complexity due to handling working space arrays is gone 3. memory management has been significantly simplified too
2022-12-18 14:09:40 +01:00
call equian(rj, zk, psi=psin, fpolv=bphi, dpsidr=bz, dpsidz=br)
some additional output prints (2D maps and Bcart, Ncart along central ray)
2016-02-12 17:49:00 +01:00
else
simplify handling of splines This adds a new `splines` module which implements a high-level interface for creating and evaluating splines and rewrite almost all modules to use it. Also, notably: 1. both `simplespline` and DIERCKX splines can now used with a uniform interface 2. most complexity due to handling working space arrays is gone 3. memory management has been significantly simplified too
2022-12-18 14:09:40 +01:00
call equinum_psi(rj, zk, psi=psin, dpsidr=bz, dpsidz=br)
call equinum_fpol(psin, fpol=bphi)
some additional output prints (2D maps and Bcart, Ncart along central ray)
2016-02-12 17:49:00 +01:00
end if
br = -br/rj
bphi = bphi/rj
bz = bz/rj
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
btot = sqrt(br**2 + bphi**2 + bz**2)
some additional output prints (2D maps and Bcart, Ncart along central ray)
2016-02-12 17:49:00 +01:00
yg = btot/bres
te = temp(psin)
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
call density(psin, ne, dne)
some additional output prints (2D maps and Bcart, Ncart along central ray)
2016-02-12 17:49:00 +01:00
xg = xgcn*ne
src: implement toggling of output units This actually implements the --units option
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write (umaps,'(12(x,e12.5))') &
rj, zk, psin, br, bphi, bz, btot, ne, te, xg, yg, anpl
end do
write (umaps,*)
end do
some additional output prints (2D maps and Bcart, Ncart along central ray)
2016-02-12 17:49:00 +01:00
end subroutine print_maps
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
subroutine print_surfq(qval)
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
! Print constant ψ surfaces for a given `q` value
simplify handling of splines This adds a new `splines` module which implements a high-level interface for creating and evaluating splines and rewrite almost all modules to use it. Also, notably: 1. both `simplespline` and DIERCKX splines can now used with a uniform interface 2. most complexity due to handling working space arrays is gone 3. memory management has been significantly simplified too
2022-12-18 14:09:40 +01:00
use equilibrium, only : q_spline, fq, frhotor, &
src: use the logging system everywhere
2021-12-18 18:57:38 +01:00
rmaxis, zmaxis, zbsup, zbinf
use magsurf_data, only : contours_psi, npoints, print_contour
use utils, only : locate, intlin
use logger, only : log_info
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
implicit none
src: use the logging system everywhere
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! subroutine arguments
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
real(wp_), dimension(:), intent(in) :: qval
src: use the logging system everywhere
2021-12-18 18:57:38 +01:00
! local variables
fixed incompatibilities with allocatable arrays (pgf90 compiler, JETTO); fixed input/output scaling (gray/jetto interface); fixed error in read_beams2 for small beam tables
2016-06-01 15:49:35 +02:00
integer :: i1,i
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
real(wp_) :: rup,zup,rlw,zlw,rhot,psival
real(wp_), dimension(npoints) :: rcn,zcn
simplify handling of splines This adds a new `splines` module which implements a high-level interface for creating and evaluating splines and rewrite almost all modules to use it. Also, notably: 1. both `simplespline` and DIERCKX splines can now used with a uniform interface 2. most complexity due to handling working space arrays is gone 3. memory management has been significantly simplified too
2022-12-18 14:09:40 +01:00
real(wp_), dimension(q_spline%ndata) :: qpsi
src: use the logging system everywhere
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character(256) :: msg ! for log messages formatting
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
simplify handling of splines This adds a new `splines` module which implements a high-level interface for creating and evaluating splines and rewrite almost all modules to use it. Also, notably: 1. both `simplespline` and DIERCKX splines can now used with a uniform interface 2. most complexity due to handling working space arrays is gone 3. memory management has been significantly simplified too
2022-12-18 14:09:40 +01:00
! build the q profile on the ψ grid
do i = 1, q_spline%ndata
qpsi(i) = fq(q_spline%data(i))
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
end do
src: use the logging system everywhere
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! locate ψ surface for q=qval
call log_info('constant ψ surfaces for:', &
mod='gray_core', proc='print_surfq')
simplify handling of splines This adds a new `splines` module which implements a high-level interface for creating and evaluating splines and rewrite almost all modules to use it. Also, notably: 1. both `simplespline` and DIERCKX splines can now used with a uniform interface 2. most complexity due to handling working space arrays is gone 3. memory management has been significantly simplified too
2022-12-18 14:09:40 +01:00
do i=1, size(qval)
src: use the logging system everywhere
2021-12-18 18:57:38 +01:00
! FIXME: check for non monotonous q profile
simplify handling of splines This adds a new `splines` module which implements a high-level interface for creating and evaluating splines and rewrite almost all modules to use it. Also, notably: 1. both `simplespline` and DIERCKX splines can now used with a uniform interface 2. most complexity due to handling working space arrays is gone 3. memory management has been significantly simplified too
2022-12-18 14:09:40 +01:00
call locate(abs(qpsi), q_spline%ndata, qval(i), i1)
if (i1 > 0 .and. i1 < q_spline%ndata) then
call intlin(abs(qpsi(i1)), q_spline%data(i1), abs(qpsi(i1+1)), &
q_spline%data(i1+1), qval(i), psival)
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
rup = rmaxis
rlw = rmaxis
zup = (zbsup + zmaxis)/2.0_wp_
zlw = (zmaxis + zbinf)/2.0_wp_
call contours_psi(psival, rcn, zcn, rup, zup, rlw, zlw)
call print_contour(psival, rcn, zcn)
rhot = frhotor(sqrt(psival))
src: use the logging system everywhere
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write (msg, '(4(x,a,"=",g0.3))') &
'q', qval(i), 'ψ', psival, 'rhop', sqrt(psival), 'rhot', rhot
call log_info(msg, mod='gray_core', proc='print_surfq')
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
end if
end do
src: use the logging system everywhere
2021-12-18 18:57:38 +01:00
end subroutine print_surfq
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
subroutine print_projxyzt(stv, ywrk, iproj)
! Prints the beam shape tables (unit 8, 12)
use const_and_precisions, only : comp_huge, zero, one
use beamdata, only : nray, nrayr, nrayth, rayi2jk
use units, only : uprj0, uwbm, unit_active
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
implicit none
src: implement toggling of output units This actually implements the --units option
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! subroutine arguments
real(wp_), dimension(:), intent(in) :: stv
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
real(wp_), dimension(:,:), intent(in) :: ywrk
src: implement toggling of output units This actually implements the --units option
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integer, intent(in) :: iproj
! local variables
integer :: jk, jkz, uprj
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
integer, dimension(2) ::jkv
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
real(wp_), dimension(3) :: xv1, dir, dxv
real(wp_) :: rtimn, rtimx, csth1, snth1, &
csps1, snps1, xti, yti, zti, rti
if (.not.(unit_active(uprj0) .or. unit_active(uwbm))) return
! common/external functions/variables
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
uprj = uprj0 + iproj
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
xv1 = ywrk(1:3, 1)
dir = ywrk(4:6, 1)
dir = dir/norm2(dir)
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
csth1 = dir(3)
snth1 = sqrt(one - csth1**2)
if(snth1 > zero) then
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
csps1 = dir(2)/snth1
snps1 = dir(1)/snth1
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
else
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
csps1 = one
snps1 = zero
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
end if
if(iproj==0) then
jkz = nray - nrayth + 1
else
jkz = 1
end if
rtimn = comp_huge
rtimx = zero
do jk = jkz, nray
dxv = ywrk(1:3,jk) - xv1
xti = dxv(1)*csps1 - dxv(2)*snps1
yti =(dxv(1)*snps1 + dxv(2)*csps1)*csth1 - dxv(3)*snth1
zti =(dxv(1)*snps1 + dxv(2)*csps1)*snth1 + dxv(3)*csth1
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
rti = hypot(xti, yti)
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
jkv=rayi2jk(jk)
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
if(.not.(iproj==0 .and. jk==1)) &
write(uprj, '(1x,e16.8e3,2i5,4(1x,e16.8e3))') &
stv(jk), jkv, xti, yti, zti, rti
if(iproj==1 .and. jkv(2)==nrayth) write (uprj, *)
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
if(rti>=rtimx .and. jkv(1)==nrayr) rtimx = rti
if(rti<=rtimn .and. jkv(1)==nrayr) rtimn = rti
end do
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
write (uprj, *)
write (uwbm, '(3(1x,e16.8e3))') stv(1), rtimn, rtimx
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
end subroutine print_projxyzt
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
subroutine print_output(i, jk, st, qj, xv, psinv, btot, bv, ak0, &
anpl, anpr, anv, anprim, dens, tekev, &
alpha, tau, dids, nhm, nhf, iokhawa, &
index_rt, ddr, ddi, xg, yg, derxg)
! Prints the ray variables and Hamiltonian error (units 4, 33, 17)
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
use const_and_precisions, only : degree,zero,one
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
use equilibrium, only : frhotor
use gray_params, only : istpl0
use beamdata, only : nray,nrayth,jkray1
use units, only : ucenr, uoutr, udisp, unit_active
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
implicit none
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
! subroutine arguments
integer, intent(in) :: i, jk, nhm, nhf, iokhawa, index_rt
real(wp_), dimension(3), intent(in) :: xv, bv, anv
real(wp_), intent(in) :: st, qj, psinv, btot, ak0, anpl, anpr, anprim
real(wp_), intent(in) :: dens, tekev, alpha, tau, dids, ddr, ddi
real(wp_), intent(in) :: xg, yg
added further output prints to fort.4
2017-09-12 21:37:06 +02:00
real(wp_), dimension(3), intent(in) :: derxg
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
! local variables
real(wp_) :: stm, xxm, yym, zzm, rrm, phideg, rhot, akim, pt, didsn
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
integer :: k
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
stm = st * 1.0e-2_wp_
xxm = xv(1) * 1.0e-2_wp_
yym = xv(2) * 1.0e-2_wp_
zzm = xv(3) * 1.0e-2_wp_
rrm = hypot(xxm, yym)
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
! print central ray trajectory. dIds in A/m/W, ki in m⁻¹
if(jk == 1) then
phideg = atan2(yym, xxm)/degree
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
if(psinv>=zero .and. psinv<=one) then
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
rhot = frhotor(sqrt(psinv))
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
else
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
rhot = 1.0_wp_
end if
akim = anprim * ak0 * 1.0e2_wp_
pt = qj*exp(-tau)
didsn = dids * 1.0e2_wp_/qj
! print central ray data
if (unit_active(ucenr)) then
write (ucenr,'(22(1x,e16.8e3),4i5,6(1x,e16.8e3))') &
stm, rrm, zzm, phideg, psinv, rhot, dens, tekev, &
btot, bv, anpr, anpl, anv, akim, alpha, tau, pt, &
didsn, nhm, nhf, iokhawa, index_rt, ddr, xg, yg, &
derxg
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
end if
end if
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
! print conservation of dispersion relation (Hamiltonian error)
if(unit_active(udisp) .and. jk==nray) then
write(udisp,'(30(1x,e16.8e3))') st,ddr,ddi
end if
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
! print outer ray trajectories
if(mod(i, istpl0) == 0) then
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
k = jk - jkray1 + 1
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
if(unit_active(uoutr) .and. k>0 .and. k<=nrayth) then
write(uoutr, '(2i5,9(1x,e16.8e3),i5)') &
i, k, stm, xxm, yym, rrm, zzm, &
psinv, tau, anpl, alpha, index_rt
nocommon branch merged back into trunk
2015-11-18 17:34:33 +01:00
end if
end if
end subroutine print_output
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
subroutine print_pec(rhop_tab, rhot_tab, jphi, jcd, &
dpdv, currins, pins, index_rt)
! Prints the ECRH and CD profiles (unit 48)
use units, only : upec, unit_active
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
implicit none
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
! subroutine arguments
real(wp_), dimension(:), intent(in) :: rhop_tab, rhot_tab, jphi, jcd, &
dpdv, currins, pins
integer, intent(in) :: index_rt
! local variables
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
integer :: i
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
if (.not. unit_active(upec)) return
do i=1, size(rhop_tab)
write(upec, '(7(1x, e16.8e3), i5)') rhop_tab(i), rhot_tab(i), &
jphi(i), jcd(i), dpdv(i), currins(i), pins(i), index_rt
src/gray_core.f90: cleanup - add some comments - annotate loops - indent comments - remove trailing whitespace - reduce usage of opaque global variables - use Fortran 90 logical operators - use Fortran 2003 array syntax
2022-05-10 12:36:37 +02:00
end do
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
write(upec, *) ''
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
end subroutine print_pec
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
subroutine print_finals(pabs, icd, dpdvp, jphip, rhotpav, rhotjava, drhotpav, &
drhotjava, dpdvmx, jphimx, rhotp, rhotj, drhotp, &
drhotj, ratjamx, ratjbmx, stmx, psipol, chipol, &
index_rt, p0, cpl1, cpl2)
! Prints global data and final results (unit 7)
use units, only : ucenr, usumm, unit_active
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
implicit none
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
! subroutine arguments
real(wp_), intent(in) :: pabs, icd, dpdvp, jphip, rhotpav, rhotjava, &
drhotpav, drhotjava, dpdvmx, jphimx, rhotp, &
rhotj, drhotp, drhotj, ratjamx, ratjbmx, &
stmx, psipol, chipol, p0, cpl1, cpl2
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
integer, intent(in) :: index_rt
src: implement toggling of output units This actually implements the --units option
2021-12-19 16:39:19 +01:00
if (unit_active(ucenr)) then
write(ucenr, *) ''
end if
if (unit_active(usumm)) then
write(usumm,'(15(1x,e12.5),i5,7(1x,e12.5))') &
icd, pabs, jphip, dpdvp, rhotj, rhotjava, rhotp, rhotpav, &
drhotjava, drhotpav, ratjamx, ratjbmx, stmx, psipol, &
chipol, index_rt, jphimx, dpdvmx, drhotj, drhotp, &
p0, cpl1, cpl2
end if
re-added missing output files, file units specified in dedicated module, added option iequil=3 for partially filled psi(R,z) grid on input: required for integration in JETTO
2015-11-23 18:55:27 +01:00
end subroutine print_finals
src/graycore.f90 -> src/gray_core.f90 Rename for consistency with other modules.
2021-12-15 02:31:14 +01:00
end module gray_core
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