Skip to content
Snippets Groups Projects
moments_eq_rhs.F90 12.2 KiB
Newer Older
!_____________________________________________________________________________!
!_____________________________________________________________________________!
!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!
!!!!!! Electrons moments RHS !!!!!!!
!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!
!_____________________________________________________________________________!
SUBROUTINE moments_eq_rhs_e

  USE basic
  USE time_integration
  USE array
  USE fields
  USE model
  USE prec_const
  IMPLICIT NONE

  INTEGER     :: p_int, j_int ! loops indices and polynom. degrees
  REAL(dp)    :: kx, ky, kperp2, dzlnB_o_J
  COMPLEX(dp) :: Tnepj, Tnepp2j, Tnepm2j, Tnepjp1, Tnepjm1, Tpare, Tphi ! Terms from b x gradB and drives
  COMPLEX(dp) :: Tmir, Tnepp1j, Tnepm1j, Tnepp1jm1, Tnepm1jm1 ! Terms from mirror force with non adiab moments
  COMPLEX(dp) :: UNepm1j, UNepm1jp1, UNepm1jm1 ! Terms from mirror force with adiab moments
  INTEGER     :: izm2, izm1, izp1, izp2 ! indices for centered FDF ddz
  ! To store derivatives and odd-even z grid interpolations
  COMPLEX(dp), DIMENSION(izs:ize) :: ddznepp1j, ddznepm1j, &
              nepp1j, nepp1jm1, nepm1j, nepm1jm1, nepm1jp1
  CALL cpu_time(t0_rhs)

  ploope : DO ip = ips_e, ipe_e ! loop over Hermite degree indices
    p_int = parray_e(ip)    ! Hermite polynom. degree
    eo    = MODULO(p_int,2) ! Indicates if we are on even or odd z grid
    jloope : DO ij = ijs_e, ije_e ! loop over Laguerre degree indices
    j_int = jarray_e(ij)
      ! Spatial loops
      kxloope : DO ikx = ikxs,ikxe
      kx     = kxarray(ikx)   ! radial wavevector
      kyloope : DO iky = ikys,ikye
      ky     = kyarray(iky)   ! toroidal wavevector
        i_ky   = imagu * ky     ! toroidal derivative
        IF (Nky .EQ. 1) i_ky = imagu * kxarray(ikx) ! If 1D simulation we put kx as ky
        ! Compute z derivatives and odd-even z interpolations
        CALL   grad_z(eo,nadiab_moments_e(ip+1,ij  ,ikx,iky,:),ddznepp1j(:))
        CALL   grad_z(eo,nadiab_moments_e(ip-1,ij  ,ikx,iky,:),ddznepm1j(:))
        CALL interp_z(eo,nadiab_moments_e(ip+1,ij  ,ikx,iky,:),   nepp1j  (:))
        CALL interp_z(eo,nadiab_moments_e(ip+1,ij-1,ikx,iky,:),   nepp1jm1(:))
        CALL interp_z(eo,nadiab_moments_e(ip-1,ij  ,ikx,iky,:),   nepm1j  (:))
        CALL interp_z(eo,nadiab_moments_e(ip-1,ij+1,ikx,iky,:),   nepm1jp1(:))
        CALL interp_z(eo,nadiab_moments_e(ip-1,ij-1,ikx,iky,:),   nepm1jm1(:))
        zloope : DO  iz = izs,ize
          ! Obtain the index with an array that accounts for boundary conditions
          !   e.g. : 4 stencil with periodic BC, izarray(Nz+2) = 2, izarray(-1) = Nz-1
          izp1 = izarray(iz+1); izp2 = izarray(iz+2);
          izm1 = izarray(iz-1); izm2 = izarray(iz-2);
            !
          kperp2= kparray(ikx,iky,iz,eo)**2
          !! Compute moments mixing terms
          ! Perpendicular dynamic
          ! term propto n_e^{p,j}
          Tnepj   = xnepj(ip,ij)* nadiab_moments_e(ip,ij,ikx,iky,iz)
          Tnepp2j = xnepp2j(ip) * nadiab_moments_e(ip+pp2,ij,ikx,iky,iz)
          Tnepm2j = xnepm2j(ip) * nadiab_moments_e(ip-pp2,ij,ikx,iky,iz)
          Tnepjp1 = xnepjp1(ij) * nadiab_moments_e(ip,ij+1,ikx,iky,iz)
          Tnepjm1 = xnepjm1(ij) * nadiab_moments_e(ip,ij-1,ikx,iky,iz)
          Tpare = 0._dp; Tmir = 0._dp
          IF(Nz .GT. 1) THEN
          ! ddz derivative for Landau damping term
          Tpare = xnepp1j(ip) * ddznepp1j(iz) + xnepm1j(ip) * ddznepm1j(iz)
          Tnepp1j   = ynepp1j  (ip,ij) * nepp1j  (iz)
          Tnepp1jm1 = ynepp1jm1(ip,ij) * nepp1jm1(iz)
          Tnepm1j   = ynepm1j  (ip,ij) * nepm1j  (iz)
          Tnepm1jm1 = ynepm1jm1(ip,ij) * nepm1jm1(iz)
          UNepm1j   = znepm1j  (ip,ij) * nepm1j  (iz)
          UNepm1jp1 = znepm1jp1(ip,ij) * nepm1jp1(iz)
          UNepm1jm1 = znepm1jm1(ip,ij) * nepm1jm1(iz)

          Tmir = Tnepp1j + Tnepp1jm1 + Tnepm1j + Tnepm1jm1 + UNepm1j + UNepm1jp1 + UNepm1jm1
          IF ( p_int .LE. 2 ) THEN ! kronecker p0 p1 p2
          Tphi = phi(ikx,iky,iz) * (xphij(ip,ij)*kernel_e(ij,ikx,iky,iz,eo) &
                   + xphijp1(ip,ij)*kernel_e(ij+1,ikx,iky,iz,eo) &
                   + xphijm1(ip,ij)*kernel_e(ij-1,ikx,iky,iz,eo) )
          ! IF (CO .EQ. 0) THEN ! Lenard Bernstein
          !   CALL LenardBernstein_e(ip,ij,ikx,iky,iz,TColl)
          ! ELSEIF (CO .EQ. 1) THEN ! GK Dougherty
          !   CALL DoughertyGK_e(ip,ij,ikx,iky,iz,TColl)
          ! ELSE ! COSOLver matrix
          !   TColl = TColl_e(ip,ij,ikx,iky,iz)
          ! ENDIF
          !! Sum of all linear terms (the sign is inverted to match RHS)
          moments_rhs_e(ip,ij,ikx,iky,iz,updatetlevel) = &
              ! Perpendicular magnetic gradient/curvature effects
              - imagu*Ckxky(ikx,iky,iz,eo)*hatR(iz,eo)* (Tnepj + Tnepp2j + Tnepm2j + Tnepjp1 + Tnepjm1)&
              ! Parallel coupling (Landau Damping)
              ! Mirror term (parallel magnetic gradient)
              ! Drives (density + temperature gradients)
              - i_ky * Tphi &
              ! Electrostatic background gradients
              - i_ky * K_E * moments_e(ip,ij,ikx,iky,iz,updatetlevel) &
              ! Numerical hyperdiffusion (totally artificial, for stability purpose)
              - (mu_x*kx**4 + mu_y*ky**4)*moments_e(ip,ij,ikx,iky,iz,updatetlevel) &
          !! Adding non linearity
            moments_rhs_e(ip,ij,ikx,iky,iz,updatetlevel) = &
              moments_rhs_e(ip,ij,ikx,iky,iz,updatetlevel) - Sepj(ip,ij,ikx,iky,iz)
  ! Execution time end
  CALL cpu_time(t1_rhs)
  tc_rhs = tc_rhs + (t1_rhs-t0_rhs)

END SUBROUTINE moments_eq_rhs_e
!_____________________________________________________________________________!
!_____________________________________________________________________________!
!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!
!!!!!!!!! Ions moments RHS !!!!!!!!!
!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!
!_____________________________________________________________________________!
SUBROUTINE moments_eq_rhs_i

  USE basic
  USE time_integration, ONLY: updatetlevel
  USE array
  USE fields
  USE grid
  USE model
  USE prec_const
  USE collision
  INTEGER     :: p_int, j_int ! loops indices and polynom. degrees
  REAL(dp)    :: kx, ky, kperp2
  COMPLEX(dp) :: Tnipj, Tnipp2j, Tnipm2j, Tnipjp1, Tnipjm1, Tpari, Tphi
  COMPLEX(dp) :: Tmir, Tnipp1j, Tnipm1j, Tnipp1jm1, Tnipm1jm1 ! Terms from mirror force with non adiab moments
  COMPLEX(dp) :: UNipm1j, UNipm1jp1, UNipm1jm1 ! Terms from mirror force with adiab moments
  INTEGER     :: izm2, izm1, izp1, izp2 ! indices for centered FDF ddz
  ! To store derivatives and odd-even z grid interpolations
  COMPLEX(dp), DIMENSION(izs:ize) :: ddznipp1j, ddznipm1j, &
              nipp1j, nipp1jm1, nipm1j, nipm1jm1, nipm1jp1
  ! Measuring execution time
  CALL cpu_time(t0_rhs)

  ploopi : DO ip = ips_i, ipe_i  ! Hermite loop
    p_int = parray_i(ip)    ! Hermite degree
    eo    = MODULO(p_int,2) ! Indicates if we are on odd or even z grid
    jloopi : DO ij = ijs_i, ije_i  ! This loop is from 1 to jmaxi+1
      j_int = jarray_i(ij)
      ! Spatial loops
      kxloopi : DO ikx = ikxs,ikxe
      kx     = kxarray(ikx)   ! radial wavevector
      kyloopi : DO iky = ikys,ikye
      ky     = kyarray(iky)   ! toroidal wavevector
        i_ky   = imagu * ky     ! toroidal derivative
        IF (Nky .EQ. 1) i_ky = imagu * kxarray(ikx) ! If 1D simulation we put kx as ky
        ! Compute z derivatives and odd-even z interpolations
        CALL   grad_z(eo,nadiab_moments_i(ip+1,ij  ,ikx,iky,:),ddznipp1j(:))
        CALL   grad_z(eo,nadiab_moments_i(ip-1,ij  ,ikx,iky,:),ddznipm1j(:))
        CALL interp_z(eo,nadiab_moments_i(ip+1,ij  ,ikx,iky,:), nipp1j  (:))
        CALL interp_z(eo,nadiab_moments_i(ip+1,ij-1,ikx,iky,:), nipp1jm1(:))
        CALL interp_z(eo,nadiab_moments_i(ip-1,ij  ,ikx,iky,:), nipm1j  (:))
        CALL interp_z(eo,nadiab_moments_i(ip-1,ij+1,ikx,iky,:), nipm1jp1(:))
        CALL interp_z(eo,nadiab_moments_i(ip-1,ij-1,ikx,iky,:), nipm1jm1(:))
        zloopi : DO  iz = izs,ize
          ! kperp2= gxx(iz)*kx**2 + 2._dp*gxy(iz)*kx*ky + gyy(iz)*ky**2
          !! Compute moments mixing terms
          ! Perpendicular dynamic
          ! term propto n_i^{p,j}
          Tnipj   = xnipj(ip,ij) * nadiab_moments_i(ip    ,ij  ,ikx,iky,iz)
          Tnipp2j = xnipp2j(ip)  * nadiab_moments_i(ip+pp2,ij  ,ikx,iky,iz)
          Tnipm2j = xnipm2j(ip)  * nadiab_moments_i(ip-pp2,ij  ,ikx,iky,iz)
          Tnipjp1 = xnipjp1(ij)  * nadiab_moments_i(ip    ,ij+1,ikx,iky,iz)
          Tnipjm1 = xnipjm1(ij)  * nadiab_moments_i(ip    ,ij-1,ikx,iky,iz)
          Tpari = 0._dp; Tmir = 0._dp
          IF(Nz .GT. 1) THEN
          ! term propto N_i^{p,j+1}, centered FDF
          Tpari = xnipp1j(ip) * ddznipp1j(iz) + xnipm1j(ip) * ddznipm1j(iz)

          Tnipp1j   = ynipp1j  (ip,ij) * nipp1j  (iz)
          Tnipp1jm1 = ynipp1jm1(ip,ij) * nipp1jm1(iz)
          Tnipm1j   = ynipm1j  (ip,ij) * nipm1j  (iz)
          Tnipm1jm1 = ynipm1jm1(ip,ij) * nipm1jm1(iz)
          UNipm1j   = znipm1j  (ip,ij) * nipm1j  (iz)
          UNipm1jp1 = znipm1jp1(ip,ij) * nipm1jp1(iz)
          UNipm1jm1 = znipm1jm1(ip,ij) * nipm1jm1(iz)

          Tmir = Tnipp1j + Tnipp1jm1 + Tnipm1j + Tnipm1jm1 + UNipm1j + UNipm1jp1 + UNipm1jm1
          IF ( p_int .LE. 2 ) THEN ! kronecker p0 p1 p2
            Tphi = phi(ikx,iky,iz) * (xphij(ip,ij)*kernel_i(ij,ikx,iky,iz,eo) &
                     + xphijp1(ip,ij)*kernel_i(ij+1,ikx,iky,iz,eo) &
                     + xphijm1(ip,ij)*kernel_i(ij-1,ikx,iky,iz,eo) )
          ! IF     (CO .EQ. 0) THEN ! Lenard Bernstein
          !   CALL LenardBernstein_i(ip,ij,ikx,iky,iz,TColl)
          ! ELSEIF (CO .EQ. 1) THEN ! GK Dougherty
          !   CALL DoughertyGK_i(ip,ij,ikx,iky,iz,TColl)
          ! ELSE! COSOLver matrix (Sugama, Coulomb)
          !   TColl = TColl_i(ip,ij,ikx,iky,iz)
          ! ENDIF
          !! Sum of all linear terms (the sign is inverted to match RHS)
          moments_rhs_i(ip,ij,ikx,iky,iz,updatetlevel) = &
              ! Perpendicular magnetic gradient/curvature effects
              - imagu*Ckxky(ikx,iky,iz,eo)*hatR(iz,eo)*(Tnipj + Tnipp2j + Tnipm2j + Tnipjp1 + Tnipjm1)&
              ! Parallel coupling (Landau Damping)
              ! Mirror term (parallel magnetic gradient)
              ! Drives (density + temperature gradients)
              - i_ky * Tphi &
              ! Electrostatic background gradients
              - i_ky * K_E * moments_i(ip,ij,ikx,iky,iz,updatetlevel) &
              ! Numerical hyperdiffusion (totally artificial, for stability purpose)
              - (mu_x*kx**4 + mu_y*ky**4)*moments_i(ip,ij,ikx,iky,iz,updatetlevel) &
          !! Adding non linearity
           moments_rhs_i(ip,ij,ikx,iky,iz,updatetlevel) = &
             moments_rhs_i(ip,ij,ikx,iky,iz,updatetlevel) - Sipj(ip,ij,ikx,iky,iz)
  ! Execution time end
  CALL cpu_time(t1_rhs)
  tc_rhs = tc_rhs + (t1_rhs-t0_rhs)

END SUBROUTINE moments_eq_rhs_i