Newer
Older
MODULE moments_eq_rhs
IMPLICIT NONE
PUBLIC :: compute_moments_eq_rhs
SUBROUTINE compute_moments_eq_rhs

Antoine Cyril David Hoffmann
committed
USE array
USE fields

Antoine Cyril David Hoffmann
committed
USE basic
USE prec_const
USE collision

Antoine Cyril David Hoffmann
committed
USE time_integration
USE geometry, ONLY: gradz_coeff, dBdz, Ckxky, Gamma_NL!, Gamma_phipar
USE calculus, ONLY : interp_z, grad_z, grad_z2
IMPLICIT NONE

Antoine Cyril David Hoffmann
committed
!compute ion moments_eq_rhs
CALL moments_eq_rhs(ips_i,ipe_i,ipgs_i,ipge_i,ijs_i,ije_i,ijgs_i,ijge_i,jarray_i,parray_i,&
xnipj, xnipp2j, xnipm2j, xnipjp1, xnipjm1, xnipp1j, xnipm1j,&
ynipp1j, ynipp1jm1, ynipm1j, ynipm1jm1, &
znipm1j, znipm1jp1, znipm1jm1, &
xphij_i, xphijp1_i, xphijm1_i, xpsij_i, xpsijp1_i, xpsijm1_i,&
kernel_i, nadiab_moments_i, ddz_nipj, interp_nipj, Sipj,&
moments_i(ipgs_i:ipge_i,ijgs_i:ijge_i,ikys:ikye,ikxs:ikxe,izgs:izge,updatetlevel),&
TColl_i, ddzND_nipj, &
moments_rhs_i(ips_i:ipe_i,ijs_i:ije_i,ikys:ikye,ikxs:ikxe,izs:ize,updatetlevel))

Antoine Cyril David Hoffmann
committed
!compute ion moments_eq_rhs
IF(KIN_E) &
CALL moments_eq_rhs(ips_e,ipe_e,ipgs_e,ipge_e,ijs_e,ije_e,ijgs_e,ijge_e,jarray_e,parray_e,&
xnepj, xnepp2j, xnepm2j, xnepjp1, xnepjm1, xnepp1j, xnepm1j,&
ynepp1j, ynepp1jm1, ynepm1j, ynepm1jm1, &
znepm1j, znepm1jp1, znepm1jm1, &
xphij_e, xphijp1_e, xphijm1_e, xpsij_e, xpsijp1_e, xpsijm1_e,&
kernel_e, nadiab_moments_e, ddz_nepj, interp_nepj, Sepj,&
moments_e(ipgs_e:ipge_e,ijgs_e:ijge_e,ikys:ikye,ikxs:ikxe,izgs:izge,updatetlevel),&
TColl_e, ddzND_nepj,&
moments_rhs_e(ips_e:ipe_e,ijs_e:ije_e,ikys:ikye,ikxs:ikxe,izs:ize,updatetlevel))

Antoine Cyril David Hoffmann
committed
CONTAINS
!_____________________________________________________________________________!
!_____________________________________________________________________________!
!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!
!!! moments_ RHS computation !!!!!!!
!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!
! This routine assemble the RHS of the moment hierarchy equations. It uses
! linear coefficients that are stored in arrays (xn*, yn* and zn*) computed in
! numerics_mod.F90. Otherwise it simply adds the collision term TColl that is
! computed in collision_mod.F90 and the nonlinear term Sapj computed in
! nonlinear_mod.F90.
! All arguments of the subroutines are inputs only except the last one,
! moments_rhs_ that will contain the sum of every terms in the RHS.

Antoine Cyril David Hoffmann
committed
!_____________________________________________________________________________!
SUBROUTINE moments_eq_rhs(ips,ipe,ipgs,ipge,ijs,ije,ijgs,ijge,jarray,parray,&
xnapj, xnapp2j, xnapm2j, xnapjp1, xnapjm1, xnapp1j, xnapm1j,&
ynapp1j, ynapp1jm1, ynapm1j, ynapm1jm1, &
znapm1j, znapm1jp1, znapm1jm1, &
xphij, xphijp1, xphijm1, xpsij, xpsijp1, xpsijm1,&
kernel, nadiab_moments, ddz_napj, interp_napj, Sapj,&
moments_, TColl_, ddzND_napj, moments_rhs_)
IMPLICIT NONE
!! INPUTS
INTEGER, INTENT(IN) :: ips, ipe, ipgs, ipge, ijs, ije, ijgs, ijge
INTEGER, DIMENSION(ips:ipe), INTENT(IN) :: parray
INTEGER, DIMENSION(ijs:ije), INTENT(IN) :: jarray
REAL(dp), DIMENSION(ips:ipe,ijs:ije), INTENT(IN) :: xnapj
REAL(dp), DIMENSION(ips:ipe), INTENT(IN) :: xnapp2j, xnapm2j
REAL(dp), DIMENSION(ijs:ije), INTENT(IN) :: xnapjp1, xnapjm1
REAL(dp), DIMENSION(ips:ipe), INTENT(IN) :: xnapp1j, xnapm1j
REAL(dp), DIMENSION(ips:ipe,ijs:ije), INTENT(IN) :: ynapp1j, ynapp1jm1, ynapm1j, ynapm1jm1
REAL(dp), DIMENSION(ips:ipe,ijs:ije), INTENT(IN) :: znapm1j, znapm1jp1, znapm1jm1
REAL(dp), DIMENSION(ips:ipe,ijs:ije), INTENT(IN) :: xphij, xphijp1, xphijm1
REAL(dp), DIMENSION(ips:ipe,ijs:ije), INTENT(IN) :: xpsij, xpsijp1, xpsijm1

Antoine Cyril David Hoffmann
committed
REAL(dp), DIMENSION(ijgs:ijge,ikys:ikye,ikxs:ikxe,izgs:izge,0:1),INTENT(IN) :: kernel
COMPLEX(dp), DIMENSION(ipgs:ipge,ijgs:ijge,ikys:ikye,ikxs:ikxe,izgs:izge),INTENT(IN) :: nadiab_moments
COMPLEX(dp), DIMENSION(ipgs:ipge,ijgs:ijge,ikys:ikye,ikxs:ikxe,izgs:izge),INTENT(IN) :: ddz_napj
COMPLEX(dp), DIMENSION(ipgs:ipge,ijgs:ijge,ikys:ikye,ikxs:ikxe,izgs:izge),INTENT(IN) :: interp_napj
COMPLEX(dp), DIMENSION( ips:ipe, ijs:ije, ikys:ikye,ikxs:ikxe, izs:ize), INTENT(IN) :: Sapj
COMPLEX(dp), DIMENSION(ipgs:ipge,ijgs:ijge,ikys:ikye,ikxs:ikxe,izgs:izge),INTENT(IN) :: moments_
COMPLEX(dp), DIMENSION( ips:ipe, ijs:ije, ikys:ikye,ikxs:ikxe, izs:ize), INTENT(IN) :: TColl_
COMPLEX(dp), DIMENSION(ipgs:ipge,ijgs:ijge,ikys:ikye,ikxs:ikxe,izgs:izge),INTENT(IN) :: ddzND_napj

Antoine Cyril David Hoffmann
committed
!! OUTPUT
COMPLEX(dp), DIMENSION( ips:ipe, ijs:ije, ikys:ikye,ikxs:ikxe, izs:ize),INTENT(OUT) :: moments_rhs_

Antoine Cyril David Hoffmann
committed
INTEGER :: p_int, j_int ! loops indices and polynom. degrees
REAL(dp) :: kx, ky, kperp2
COMPLEX(dp) :: Tnapj, Tnapp2j, Tnapm2j, Tnapjp1, Tnapjm1 ! Terms from b x gradB and drives
COMPLEX(dp) :: Tnapp1j, Tnapm1j, Tnapp1jm1, Tnapm1jm1 ! Terms from mirror force with non adiab moments_
COMPLEX(dp) :: Tperp, Tpar, Tmir, Tphi, Tpsi
COMPLEX(dp) :: Unapm1j, Unapm1jp1, Unapm1jm1 ! Terms from mirror force with adiab moments_
COMPLEX(dp) :: i_kx,i_ky,phikykxz, psikykxz
! Measuring execution time
CALL cpu_time(t0_rhs)
! Spatial loops
zloop : DO iz = izs,ize
kxloop : DO ikx = ikxs,ikxe
kx = kxarray(ikx) ! radial wavevector
i_kx = imagu * kx ! radial derivative
kyloop : DO iky = ikys,ikye
ky = kyarray(iky) ! binormal wavevector
i_ky = imagu * ky ! binormal derivative

Antoine Cyril David Hoffmann
committed
psikykxz = psi(iky,ikx,iz)! tmp psi value

Antoine Cyril David Hoffmann
committed
! Kinetic loops
jloop : DO ij = ijs, ije ! This loop is from 1 to jmaxi+1
j_int = jarray(ij)

Antoine Cyril David Hoffmann
committed
ploop : DO ip = ips, ipe ! Hermite loop
p_int = parray(ip) ! Hermite degree
eo = MODULO(p_int,2) ! Indicates if we are on odd or even z grid
kperp2= kparray(iky,ikx,iz,eo)**2
IF((CLOS .NE. 1) .OR. (p_int+2*j_int .LE. dmaxe)) THEN ! for the closure scheme

Antoine Cyril David Hoffmann
committed
!! Compute moments_ mixing terms
Tperp = 0._dp; Tpar = 0._dp; Tmir = 0._dp
! Perpendicular dynamic

Antoine Cyril David Hoffmann
committed
! term propto n^{p,j}
Tnapj = xnapj(ip,ij)* nadiab_moments(ip,ij,iky,ikx,iz)
! term propto n^{p+2,j}
Tnapp2j = xnapp2j(ip) * nadiab_moments(ip+pp2,ij,iky,ikx,iz)
! term propto n^{p-2,j}
Tnapm2j = xnapm2j(ip) * nadiab_moments(ip-pp2,ij,iky,ikx,iz)
! term propto n^{p,j+1}
Tnapjp1 = xnapjp1(ij) * nadiab_moments(ip,ij+1,iky,ikx,iz)
! term propto n^{p,j-1}
Tnapjm1 = xnapjm1(ij) * nadiab_moments(ip,ij-1,iky,ikx,iz)

Antoine Cyril David Hoffmann
committed
Tperp = Tnapj + Tnapp2j + Tnapm2j + Tnapjp1 + Tnapjm1
! Parallel dynamic
! ddz derivative for Landau damping term

Antoine Cyril David Hoffmann
committed
Tpar = xnapp1j(ip) * ddz_napj(ip+1,ij,iky,ikx,iz) &
+ xnapm1j(ip) * ddz_napj(ip-1,ij,iky,ikx,iz)

Antoine Cyril David Hoffmann
committed
Tnapp1j = ynapp1j (ip,ij) * interp_napj(ip+1,ij ,iky,ikx,iz)
Tnapp1jm1 = ynapp1jm1(ip,ij) * interp_napj(ip+1,ij-1,iky,ikx,iz)
Tnapm1j = ynapm1j (ip,ij) * interp_napj(ip-1,ij ,iky,ikx,iz)
Tnapm1jm1 = ynapm1jm1(ip,ij) * interp_napj(ip-1,ij-1,iky,ikx,iz)

Antoine Cyril David Hoffmann
committed
Unapm1j = znapm1j (ip,ij) * interp_napj(ip-1,ij ,iky,ikx,iz)
Unapm1jp1 = znapm1jp1(ip,ij) * interp_napj(ip-1,ij+1,iky,ikx,iz)
Unapm1jm1 = znapm1jm1(ip,ij) * interp_napj(ip-1,ij-1,iky,ikx,iz)

Antoine Cyril David Hoffmann
committed
Tmir = Tnapp1j + Tnapp1jm1 + Tnapm1j + Tnapm1jm1 + Unapm1j + Unapm1jp1 + Unapm1jm1
!! Electrical potential term
IF ( p_int .LE. 2 ) THEN ! kronecker p0 p1 p2

Antoine Cyril David Hoffmann
committed
Tphi = (xphij (ip,ij)*kernel(ij ,iky,ikx,iz,eo) &
+ xphijp1(ip,ij)*kernel(ij+1,iky,ikx,iz,eo) &

Antoine Cyril David Hoffmann
committed
+ xphijm1(ip,ij)*kernel(ij-1,iky,ikx,iz,eo))
ELSE
Tphi = 0._dp
ENDIF
!! Vector potential term
IF ( (p_int .LE. 3) .AND. (p_int .GE. 1) ) THEN ! Kronecker p1 or p3

Antoine Cyril David Hoffmann
committed
Tpsi = (xpsij (ip,ij)*kernel(ij ,iky,ikx,iz,eo) &
+ xpsijp1(ip,ij)*kernel(ij+1,iky,ikx,iz,eo) &

Antoine Cyril David Hoffmann
committed
+ xpsijm1(ip,ij)*kernel(ij-1,iky,ikx,iz,eo))
ELSE
Tpsi = 0._dp
ENDIF
!! Sum of all RHS terms

Antoine Cyril David Hoffmann
committed
moments_rhs_(ip,ij,iky,ikx,iz) = &
! Perpendicular magnetic gradient/curvature effects

Antoine Cyril David Hoffmann
committed
-imagu*Ckxky(iky,ikx,iz,eo) * Tperp&
! Perpendicular pressure effects
-i_ky*beta*dpdx * Tperp&

Antoine Cyril David Hoffmann
committed
! Parallel coupling (Landau Damping)
-gradz_coeff(iz,eo) * Tpar &
! Mirror term (parallel magnetic gradient)

Antoine Cyril David Hoffmann
committed
-dBdz(iz,eo)*gradz_coeff(iz,eo) * Tmir&
! Drives (density + temperature gradients)

Antoine Cyril David Hoffmann
committed
-i_ky * (Tphi*phikykxz - Tpsi*psikykxz) &
! Parallel drive term (should be negligible, test)
! -Gamma_phipar(iz,eo)*Tphi*ddz_phi(iky,ikx,iz) &

Antoine Cyril David Hoffmann
committed
! Numerical Hermite hyperdiffusion (GX version)
-mu_p*diff_pe_coeff*p_int**4*moments_(ip,ij,iky,ikx,iz)&
! Numerical Laguerre hyperdiffusion (GX version)
-mu_j*diff_je_coeff*j_int**4*moments_(ip,ij,iky,ikx,iz)&
! Numerical perpendicular hyperdiffusion (totally artificial, for stability purpose)
-mu_x*diff_kx_coeff*kx**N_HD*moments_(ip,ij,iky,ikx,iz) &
-mu_y*diff_ky_coeff*ky**N_HD*moments_(ip,ij,iky,ikx,iz) &
! Numerical parallel hyperdiffusion "mu_z*ddz**4" see Pueschel 2010 (eq 25)
-mu_z*diff_dz_coeff*ddzND_napj(ip,ij,iky,ikx,iz) &

Antoine Cyril David Hoffmann
committed
+TColl_(ip,ij,iky,ikx,iz) &
! Nonlinear term

Antoine Cyril David Hoffmann
committed
-Gamma_NL(iz,eo)*Sapj(ip,ij,iky,ikx,iz)

Antoine Cyril David Hoffmann
committed
! IF( (ip-4 .GT. 0) .AND. (num_procs_p .EQ. 1) ) &
! ! Numerical parallel velocity hyperdiffusion "+ dvpar4 g_a" see Pueschel 2010 (eq 33)
! ! (not used often so not parallelized)
! moments_rhs_(ip,ij,iky,ikx,iz) = &
! moments_rhs_(ip,ij,iky,ikx,iz) &
! + mu_p * moments_(ip-4,ij,iky,ikx,iz)

Antoine Cyril David Hoffmann
committed
ELSE
moments_rhs_(ip,ij,iky,ikx,iz) = 0._dp
ENDIF
END DO ploop
END DO jloop
END DO kyloop
END DO kxloop
END DO zloop
! Execution time end
CALL cpu_time(t1_rhs)
tc_rhs = tc_rhs + (t1_rhs-t0_rhs)

Antoine Cyril David Hoffmann
committed
END SUBROUTINE moments_eq_rhs
!_____________________________________________________________________________!
!_____________________________________________________________________________!
END SUBROUTINE compute_moments_eq_rhs
SUBROUTINE add_Maxwellian_background_terms
! This routine is meant to add the terms rising from the magnetic operator,
! i.e. (B x GradB) Grad, applied on the background Maxwellian distribution
! (x_a + spar^2)(b x GradB) GradFaM
! It gives birth to kx=ky=0 sources terms (averages) that hit moments 00, 20,
! 40, 01,02, 21 with background gradient dependences.
USE prec_const
USE time_integration, ONLY : updatetlevel
USE model, ONLY: taue_qe, taui_qi, k_Ni, k_Ne, k_Ti, k_Te, KIN_E
USE array, ONLY: moments_rhs_e, moments_rhs_i
USE grid, ONLY: contains_kx0, contains_ky0, ikx_0, iky_0,&
ips_e,ipe_e,ijs_e,ije_e,ips_i,ipe_i,ijs_i,ije_i,&

Antoine Cyril David Hoffmann
committed
zarray, izs,ize,&
ip,ij
IMPLICIT NONE
real(dp), DIMENSION(izs:ize) :: sinz
sinz(izs:ize) = SIN(zarray(izs:ize,0))
IF(contains_kx0 .AND. contains_ky0) THEN
IF(KIN_E) THEN
DO ip = ips_e,ipe_e
DO ij = ijs_e,ije_e
SELECT CASE(ij-1)
CASE(0) ! j = 0
SELECT CASE (ip-1)
CASE(0) ! Na00 term
moments_rhs_e(ip,ij,iky_0,ikx_0,izs:ize,updatetlevel) = moments_rhs_e(ip,ij,iky_0,ikx_0,izs:ize,updatetlevel)&
+taue_qe * sinz(izs:ize) * (1.5_dp*k_Ne - 1.125_dp*k_Te)
CASE(2) ! Na20 term
moments_rhs_e(ip,ij,iky_0,ikx_0,izs:ize,updatetlevel) = moments_rhs_e(ip,ij,iky_0,ikx_0,izs:ize,updatetlevel)&
+taue_qe * sinz(izs:ize) * (SQRT2*0.5_dp*k_Ne - 2.75_dp*k_Te)
CASE(4) ! Na40 term
moments_rhs_e(ip,ij,iky_0,ikx_0,izs:ize,updatetlevel) = moments_rhs_e(ip,ij,iky_0,ikx_0,izs:ize,updatetlevel)&
+taue_qe * sinz(izs:ize) * SQRT6*0.75_dp*k_Te
END SELECT
CASE(1) ! j = 1
SELECT CASE (ip-1)
CASE(0) ! Na01 term
moments_rhs_e(ip,ij,iky_0,ikx_0,izs:ize,updatetlevel) = moments_rhs_e(ip,ij,iky_0,ikx_0,izs:ize,updatetlevel)&
-taue_qe * sinz(izs:ize) * (k_Ne + 3.5_dp*k_Te)
CASE(2) ! Na21 term
moments_rhs_e(ip,ij,iky_0,ikx_0,izs:ize,updatetlevel) = moments_rhs_e(ip,ij,iky_0,ikx_0,izs:ize,updatetlevel)&
-taue_qe * sinz(izs:ize) * SQRT2*k_Te
END SELECT
CASE(2) ! j = 2
SELECT CASE (ip-1)
CASE(0) ! Na02 term
moments_rhs_e(ip,ij,iky_0,ikx_0,izs:ize,updatetlevel) = moments_rhs_e(ip,ij,iky_0,ikx_0,izs:ize,updatetlevel)&
+taue_qe * sinz(izs:ize) * 2._dp*k_Te
END SELECT
END SELECT
ENDDO
ENDDO
ENDIF
DO ip = ips_i,ipe_i
DO ij = ijs_i,ije_i
SELECT CASE(ij-1)
CASE(0) ! j = 0
SELECT CASE (ip-1)
CASE(0) ! Na00 term
moments_rhs_i(ip,ij,iky_0,ikx_0,izs:ize,updatetlevel) = moments_rhs_i(ip,ij,iky_0,ikx_0,izs:ize,updatetlevel)&
+taui_qi * sinz(izs:ize) * (1.5_dp*k_Ni - 1.125_dp*k_Ti)
CASE(2) ! Na20 term
moments_rhs_i(ip,ij,iky_0,ikx_0,izs:ize,updatetlevel) = moments_rhs_i(ip,ij,iky_0,ikx_0,izs:ize,updatetlevel)&
+taui_qi * sinz(izs:ize) * (SQRT2*0.5_dp*k_Ni - 2.75_dp*k_Ti)
CASE(4) ! Na40 term
moments_rhs_i(ip,ij,iky_0,ikx_0,izs:ize,updatetlevel) = moments_rhs_i(ip,ij,iky_0,ikx_0,izs:ize,updatetlevel)&
+taui_qi * sinz(izs:ize) * SQRT6*0.75_dp*k_Ti
END SELECT
CASE(1) ! j = 1
SELECT CASE (ip-1)
CASE(0) ! Na01 term
moments_rhs_i(ip,ij,iky_0,ikx_0,izs:ize,updatetlevel) = moments_rhs_i(ip,ij,iky_0,ikx_0,izs:ize,updatetlevel)&
-taui_qi * sinz(izs:ize) * (k_Ni + 3.5_dp*k_Ti)
CASE(2) ! Na21 term
moments_rhs_i(ip,ij,iky_0,ikx_0,izs:ize,updatetlevel) = moments_rhs_i(ip,ij,iky_0,ikx_0,izs:ize,updatetlevel)&
-taui_qi * sinz(izs:ize) * SQRT2*k_Ti
END SELECT
CASE(2) ! j = 2
SELECT CASE (ip-1)
CASE(0) ! Na02 term
moments_rhs_i(ip,ij,iky_0,ikx_0,izs:ize,updatetlevel) = moments_rhs_i(ip,ij,iky_0,ikx_0,izs:ize,updatetlevel)&
+taui_qi * sinz(izs:ize) * 2._dp*k_Ti
END SELECT
END SELECT
ENDDO
ENDDO
ENDIF
END SUBROUTINE
END MODULE moments_eq_rhs