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pyramid_photo_rate.f90
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pyramid_photo_rate.f90
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module pyramid_photo_rate
use precision, only: dp
use input, only: level_py, partition ,volume_factor, use_which_source, pi
use array, only: pyramid_grid, &
px_py_pz_dx, px_py_pz_dy, px_py_pz_dz, &
px_py_nz_dx, px_py_nz_dy, px_py_nz_dz, &
px_ny_pz_dx, px_ny_pz_dy, px_ny_pz_dz, &
px_ny_nz_dx, px_ny_nz_dy, px_ny_nz_dz, &
nx_py_pz_dx, nx_py_pz_dy, nx_py_pz_dz, &
nx_py_nz_dx, nx_py_nz_dy, nx_py_nz_dz, &
nx_ny_pz_dx, nx_ny_pz_dy, nx_ny_pz_dz, &
nx_ny_nz_dx, nx_ny_nz_dy, nx_ny_nz_dz
use radiation, only: photoion_solid_angle, photrates
contains
subroutine pyramid_domain_photo_rate_calculation()
call px_py_pz_dx_photo_rate_calculation ()
call px_py_pz_dy_photo_rate_calculation ()
call px_py_pz_dz_photo_rate_calculation ()
call px_py_nz_dx_photo_rate_calculation ()
call px_py_nz_dy_photo_rate_calculation ()
call px_py_nz_dz_photo_rate_calculation ()
call px_ny_pz_dx_photo_rate_calculation ()
call px_ny_pz_dy_photo_rate_calculation ()
call px_ny_pz_dz_photo_rate_calculation ()
call px_ny_nz_dx_photo_rate_calculation ()
call px_ny_nz_dy_photo_rate_calculation ()
call px_ny_nz_dz_photo_rate_calculation ()
call nx_py_pz_dx_photo_rate_calculation ()
call nx_py_pz_dy_photo_rate_calculation ()
call nx_py_pz_dz_photo_rate_calculation ()
call nx_py_nz_dx_photo_rate_calculation ()
call nx_py_nz_dy_photo_rate_calculation ()
call nx_py_nz_dz_photo_rate_calculation ()
call nx_ny_pz_dx_photo_rate_calculation ()
call nx_ny_pz_dy_photo_rate_calculation ()
call nx_ny_pz_dz_photo_rate_calculation ()
call nx_ny_nz_dx_photo_rate_calculation ()
call nx_ny_nz_dy_photo_rate_calculation ()
call nx_ny_nz_dz_photo_rate_calculation ()
end subroutine pyramid_domain_photo_rate_calculation
!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!
subroutine px_py_pz_dx_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
real(kind=dp) :: HeI_column_density_in
real(kind=dp) :: HeI_column_density_out
real(kind=dp) :: HeII_column_density_in
real(kind=dp) :: HeII_column_density_out
type(photrates) :: phi
real(kind=dp) :: i,j,k,x,y,z,n
do i_level_py = 1,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
i = real(i_level_py)
j = real(i_primary)
k = real(i_secondary)
n = real(partition(i_level_py))
x = (2.0*i-1.0)/2.0
y = (2.0*j-1.0)*(2.0*i-1.0)/(4.0*n)
z = (2.0*k-1.0)*(2.0*i-1.0)/(4.0*n)
HI_column_density_in = px_py_pz_dx(i_level_py)%HI_column_density_in(i_primary,i_secondary)
HeI_column_density_in = px_py_pz_dx(i_level_py)%HeI_column_density_in(i_primary,i_secondary)
HeII_column_density_in = px_py_pz_dx(i_level_py)%HeII_column_density_in(i_primary,i_secondary)
HI_column_density_out = px_py_pz_dx(i_level_py)%HI_column_density_out(i_primary,i_secondary)
HeI_column_density_out = px_py_pz_dx(i_level_py)%HeI_column_density_out(i_primary,i_secondary)
HeII_column_density_out = px_py_pz_dx(i_level_py)%HeII_column_density_out(i_primary,i_secondary)
!call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
! HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,correction (x,y,z))
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,1.0_dp)
px_py_pz_dx(i_level_py)%HI_photoionization_rate(i_primary,i_secondary) = 1.0!phi%photo_cell_HI
px_py_pz_dx(i_level_py)%HeI_photoionization_rate(i_primary,i_secondary) = phi%photo_cell_HeI
px_py_pz_dx(i_level_py)%HeII_photoionization_rate(i_primary,i_secondary) = phi%photo_cell_HeII
px_py_pz_dx(i_level_py)%photoheating_rate(i_primary,i_secondary) = phi%heat
enddo
enddo
enddo
write(*,*)'py HI rate near source is ', px_py_pz_dx(1)%HI_photoionization_rate(1,1)
end subroutine px_py_pz_dx_photo_rate_calculation
subroutine px_py_pz_dy_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
real(kind=dp) :: HeI_column_density_in
real(kind=dp) :: HeI_column_density_out
real(kind=dp) :: HeII_column_density_in
real(kind=dp) :: HeII_column_density_out
type(photrates) :: phi
real(kind=dp) :: i,j,k,x,y,z,n
do i_level_py = 1,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
i = real(i_secondary)
j = real(i_level_py)
k = real(i_primary)
n = real(partition(i_level_py))
x = (2.0*i-1.0)*(2.0*j-1.0)/(4.0*n)
y = (2.0*j-1.0)/2.0
z = (2.0*k-1.0)*(2.0*j-1.0)/(4.0*n)
HI_column_density_in = px_py_pz_dy(i_level_py)%HI_column_density_in(i_primary,i_secondary)
HeI_column_density_in = px_py_pz_dy(i_level_py)%HeI_column_density_in(i_primary,i_secondary)
HeII_column_density_in = px_py_pz_dy(i_level_py)%HeII_column_density_in(i_primary,i_secondary)
HI_column_density_out = px_py_pz_dy(i_level_py)%HI_column_density_out(i_primary,i_secondary)
HeI_column_density_out = px_py_pz_dy(i_level_py)%HeI_column_density_out(i_primary,i_secondary)
HeII_column_density_out = px_py_pz_dy(i_level_py)%HeII_column_density_out(i_primary,i_secondary)
!call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
! HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,correction (x,y,z))
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,1.0_dp)
px_py_pz_dy(i_level_py)%HI_photoionization_rate(i_primary,i_secondary) = 1.0!phi%photo_cell_HI
px_py_pz_dy(i_level_py)%HeI_photoionization_rate(i_primary,i_secondary) = phi%photo_cell_HeI
px_py_pz_dy(i_level_py)%HeII_photoionization_rate(i_primary,i_secondary) = phi%photo_cell_HeII
px_py_pz_dy(i_level_py)%photoheating_rate(i_primary,i_secondary) = phi%heat
enddo
enddo
enddo
end subroutine px_py_pz_dy_photo_rate_calculation
subroutine px_py_pz_dz_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
real(kind=dp) :: HeI_column_density_in
real(kind=dp) :: HeI_column_density_out
real(kind=dp) :: HeII_column_density_in
real(kind=dp) :: HeII_column_density_out
type(photrates) :: phi
real(kind=dp) :: i,j,k,x,y,z,n
do i_level_py = 1,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
i = real(i_primary)
j = real(i_secondary)
k = real(i_level_py)
n = real(partition(i_level_py))
x = (2.0*i-1.0)*(2.0*k-1.0)/(4.0*n)
y = (2.0*j-1.0)*(2.0*k-1.0)/(4.0*n)
z = (2.0*k-1.0)/2.0
HI_column_density_in = px_py_pz_dz(i_level_py)%HI_column_density_in(i_primary,i_secondary)
HeI_column_density_in = px_py_pz_dz(i_level_py)%HeI_column_density_in(i_primary,i_secondary)
HeII_column_density_in = px_py_pz_dz(i_level_py)%HeII_column_density_in(i_primary,i_secondary)
HI_column_density_out = px_py_pz_dz(i_level_py)%HI_column_density_out(i_primary,i_secondary)
HeI_column_density_out = px_py_pz_dz(i_level_py)%HeI_column_density_out(i_primary,i_secondary)
HeII_column_density_out = px_py_pz_dz(i_level_py)%HeII_column_density_out(i_primary,i_secondary)
!call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
! HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,correction (x,y,z))
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,1.0_dp)
px_py_pz_dz(i_level_py)%HI_photoionization_rate(i_primary,i_secondary) = 1.0!phi%photo_cell_HI
px_py_pz_dz(i_level_py)%HeI_photoionization_rate(i_primary,i_secondary) = phi%photo_cell_HeI
px_py_pz_dz(i_level_py)%HeII_photoionization_rate(i_primary,i_secondary) = phi%photo_cell_HeII
px_py_pz_dz(i_level_py)%photoheating_rate(i_primary,i_secondary) = phi%heat
enddo
enddo
enddo
end subroutine px_py_pz_dz_photo_rate_calculation
subroutine px_py_nz_dx_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
real(kind=dp) :: HeI_column_density_in
real(kind=dp) :: HeI_column_density_out
real(kind=dp) :: HeII_column_density_in
real(kind=dp) :: HeII_column_density_out
type(photrates) :: phi
real(kind=dp) :: i,j,k,x,y,z,n
do i_level_py = 1,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
i = real(i_level_py)
j = real(i_primary)
k = real(i_secondary)
n = real(partition(i_level_py))
x = (2.0*i-1.0)/2.0
y = (2.0*j-1.0)*(2.0*i-1.0)/(4.0*n)
z = -(2.0*k-1.0)*(2.0*i-1.0)/(4.0*n)
HI_column_density_in = px_py_nz_dx(i_level_py)%HI_column_density_in(i_primary,-i_secondary)
HeI_column_density_in = px_py_nz_dx(i_level_py)%HeI_column_density_in(i_primary,-i_secondary)
HeII_column_density_in = px_py_nz_dx(i_level_py)%HeII_column_density_in(i_primary,-i_secondary)
HI_column_density_out = px_py_nz_dx(i_level_py)%HI_column_density_out(i_primary,-i_secondary)
HeI_column_density_out = px_py_nz_dx(i_level_py)%HeI_column_density_out(i_primary,-i_secondary)
HeII_column_density_out = px_py_nz_dx(i_level_py)%HeII_column_density_out(i_primary,-i_secondary)
!call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
! HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,correction (x,y,z))
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,1.0_dp)
px_py_nz_dx(i_level_py)%HI_photoionization_rate(i_primary,-i_secondary) = 1.0!phi%photo_cell_HI
px_py_nz_dx(i_level_py)%HeI_photoionization_rate(i_primary,-i_secondary) = phi%photo_cell_HeI
px_py_nz_dx(i_level_py)%HeII_photoionization_rate(i_primary,-i_secondary) = phi%photo_cell_HeII
px_py_nz_dx(i_level_py)%photoheating_rate(i_primary,-i_secondary) = phi%heat
enddo
enddo
enddo
end subroutine px_py_nz_dx_photo_rate_calculation
subroutine px_py_nz_dy_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
real(kind=dp) :: HeI_column_density_in
real(kind=dp) :: HeI_column_density_out
real(kind=dp) :: HeII_column_density_in
real(kind=dp) :: HeII_column_density_out
type(photrates) :: phi
real(kind=dp) :: i,j,k,x,y,z,n
do i_level_py = 1,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
i = real(i_secondary)
j = real(i_level_py)
k = real(i_primary)
n = real(partition(i_level_py))
x = (2.0*i-1.0)*(2.0*j-1.0)/(4.0*n)
y = (2.0*j-1.0)/2.0
z = -(2.0*k-1.0)*(2.0*j-1.0)/(4.0*n)
HI_column_density_in = px_py_nz_dy(i_level_py)%HI_column_density_in(-i_primary,i_secondary)
HeI_column_density_in = px_py_nz_dy(i_level_py)%HeI_column_density_in(-i_primary,i_secondary)
HeII_column_density_in = px_py_nz_dy(i_level_py)%HeII_column_density_in(-i_primary,i_secondary)
HI_column_density_out = px_py_nz_dy(i_level_py)%HI_column_density_out(-i_primary,i_secondary)
HeI_column_density_out = px_py_nz_dy(i_level_py)%HeI_column_density_out(-i_primary,i_secondary)
HeII_column_density_out = px_py_nz_dy(i_level_py)%HeII_column_density_out(-i_primary,i_secondary)
!call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
! HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,correction (x,y,z))
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,1.0_dp)
px_py_nz_dy(i_level_py)%HI_photoionization_rate(-i_primary,i_secondary) = 1.0!phi%photo_cell_HI
px_py_nz_dy(i_level_py)%HeI_photoionization_rate(-i_primary,i_secondary) = phi%photo_cell_HeI
px_py_nz_dy(i_level_py)%HeII_photoionization_rate(-i_primary,i_secondary) = phi%photo_cell_HeII
px_py_nz_dy(i_level_py)%photoheating_rate(-i_primary,i_secondary) = phi%heat
enddo
enddo
enddo
end subroutine px_py_nz_dy_photo_rate_calculation
subroutine px_py_nz_dz_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
real(kind=dp) :: HeI_column_density_in
real(kind=dp) :: HeI_column_density_out
real(kind=dp) :: HeII_column_density_in
real(kind=dp) :: HeII_column_density_out
type(photrates) :: phi
real(kind=dp) :: i,j,k,x,y,z,n
do i_level_py = 1,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
i = real(i_primary)
j = real(i_secondary)
k = real(i_level_py)
n = real(partition(i_level_py))
x = (2.0*i-1.0)*(2.0*k-1.0)/(4.0*n)
y = (2.0*j-1.0)*(2.0*k-1.0)/(4.0*n)
z = -(2.0*k-1.0)/2.0
HI_column_density_in = px_py_nz_dz(-i_level_py)%HI_column_density_in(i_primary,i_secondary)
HeI_column_density_in = px_py_nz_dz(-i_level_py)%HeI_column_density_in(i_primary,i_secondary)
HeII_column_density_in = px_py_nz_dz(-i_level_py)%HeII_column_density_in(i_primary,i_secondary)
HI_column_density_out = px_py_nz_dz(-i_level_py)%HI_column_density_out(i_primary,i_secondary)
HeI_column_density_out = px_py_nz_dz(-i_level_py)%HeI_column_density_out(i_primary,i_secondary)
HeII_column_density_out = px_py_nz_dz(-i_level_py)%HeII_column_density_out(i_primary,i_secondary)
!call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
! HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,correction (x,y,z))
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,1.0_dp)
px_py_nz_dz(-i_level_py)%HI_photoionization_rate(i_primary,i_secondary) = 1.0!phi%photo_cell_HI
px_py_nz_dz(-i_level_py)%HeI_photoionization_rate(i_primary,i_secondary) = phi%photo_cell_HeI
px_py_nz_dz(-i_level_py)%HeII_photoionization_rate(i_primary,i_secondary) = phi%photo_cell_HeII
px_py_nz_dz(-i_level_py)%photoheating_rate(i_primary,i_secondary) = phi%heat
enddo
enddo
enddo
end subroutine px_py_nz_dz_photo_rate_calculation
subroutine px_ny_pz_dx_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
real(kind=dp) :: HeI_column_density_in
real(kind=dp) :: HeI_column_density_out
real(kind=dp) :: HeII_column_density_in
real(kind=dp) :: HeII_column_density_out
type(photrates) :: phi
real(kind=dp) :: i,j,k,x,y,z,n
do i_level_py = 1,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
i = real(i_level_py)
j = real(i_primary)
k = real(i_secondary)
n = real(partition(i_level_py))
x = (2.0*i-1.0)/2.0
y = -(2.0*j-1.0)*(2.0*i-1.0)/(4.0*n)
z = (2.0*k-1.0)*(2.0*i-1.0)/(4.0*n)
HI_column_density_in = px_ny_pz_dx(i_level_py)%HI_column_density_in(-i_primary,i_secondary)
HeI_column_density_in = px_ny_pz_dx(i_level_py)%HeI_column_density_in(-i_primary,i_secondary)
HeII_column_density_in = px_ny_pz_dx(i_level_py)%HeII_column_density_in(-i_primary,i_secondary)
HI_column_density_out = px_ny_pz_dx(i_level_py)%HI_column_density_out(-i_primary,i_secondary)
HeI_column_density_out = px_ny_pz_dx(i_level_py)%HeI_column_density_out(-i_primary,i_secondary)
HeII_column_density_out = px_ny_pz_dx(i_level_py)%HeII_column_density_out(-i_primary,i_secondary)
!call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
! HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,correction (x,y,z))
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,1.0_dp)
px_ny_pz_dx(i_level_py)%HI_photoionization_rate(-i_primary,i_secondary) = 1.0!phi%photo_cell_HI
px_ny_pz_dx(i_level_py)%HeI_photoionization_rate(-i_primary,i_secondary) = phi%photo_cell_HeI
px_ny_pz_dx(i_level_py)%HeII_photoionization_rate(-i_primary,i_secondary) = phi%photo_cell_HeII
px_ny_pz_dx(i_level_py)%photoheating_rate(-i_primary,i_secondary) = phi%heat
enddo
enddo
enddo
end subroutine px_ny_pz_dx_photo_rate_calculation
subroutine px_ny_pz_dy_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
real(kind=dp) :: HeI_column_density_in
real(kind=dp) :: HeI_column_density_out
real(kind=dp) :: HeII_column_density_in
real(kind=dp) :: HeII_column_density_out
type(photrates) :: phi
real(kind=dp) :: i,j,k,x,y,z,n
do i_level_py = 1,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
i = real(i_secondary)
j = real(i_level_py)
k = real(i_primary)
n = real(partition(i_level_py))
x = (2.0*i-1.0)*(2.0*j-1.0)/(4.0*n)
y = -(2.0*j-1.0)/2.0
z = (2.0*k-1.0)*(2.0*j-1.0)/(4.0*n)
HI_column_density_in = px_ny_pz_dy(-i_level_py)%HI_column_density_in(i_primary,i_secondary)
HeI_column_density_in = px_ny_pz_dy(-i_level_py)%HeI_column_density_in(i_primary,i_secondary)
HeII_column_density_in = px_ny_pz_dy(-i_level_py)%HeII_column_density_in(i_primary,i_secondary)
HI_column_density_out = px_ny_pz_dy(-i_level_py)%HI_column_density_out(i_primary,i_secondary)
HeI_column_density_out = px_ny_pz_dy(-i_level_py)%HeI_column_density_out(i_primary,i_secondary)
HeII_column_density_out = px_ny_pz_dy(-i_level_py)%HeII_column_density_out(i_primary,i_secondary)
!call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
! HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,correction (x,y,z))
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,1.0_dp)
px_ny_pz_dy(-i_level_py)%HI_photoionization_rate(i_primary,i_secondary) = 1.0!phi%photo_cell_HI
px_ny_pz_dy(-i_level_py)%HeI_photoionization_rate(i_primary,i_secondary) = phi%photo_cell_HeI
px_ny_pz_dy(-i_level_py)%HeII_photoionization_rate(i_primary,i_secondary) = phi%photo_cell_HeII
px_ny_pz_dy(-i_level_py)%photoheating_rate(i_primary,i_secondary) = phi%heat
enddo
enddo
enddo
end subroutine px_ny_pz_dy_photo_rate_calculation
subroutine px_ny_pz_dz_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
real(kind=dp) :: HeI_column_density_in
real(kind=dp) :: HeI_column_density_out
real(kind=dp) :: HeII_column_density_in
real(kind=dp) :: HeII_column_density_out
type(photrates) :: phi
real(kind=dp) :: i,j,k,x,y,z,n
do i_level_py = 1,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
i = real(i_primary)
j = real(i_secondary)
k = real(i_level_py)
n = real(partition(i_level_py))
x = (2.0*i-1.0)*(2.0*k-1.0)/(4.0*n)
y = -(2.0*j-1.0)*(2.0*k-1.0)/(4.0*n)
z = (2.0*k-1.0)/2.0
HI_column_density_in = px_ny_pz_dz(i_level_py)%HI_column_density_in(i_primary,-i_secondary)
HeI_column_density_in = px_ny_pz_dz(i_level_py)%HeI_column_density_in(i_primary,-i_secondary)
HeII_column_density_in = px_ny_pz_dz(i_level_py)%HeII_column_density_in(i_primary,-i_secondary)
HI_column_density_out = px_ny_pz_dz(i_level_py)%HI_column_density_out(i_primary,-i_secondary)
HeI_column_density_out = px_ny_pz_dz(i_level_py)%HeI_column_density_out(i_primary,-i_secondary)
HeII_column_density_out = px_ny_pz_dz(i_level_py)%HeII_column_density_out(i_primary,-i_secondary)
!call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
! HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,correction (x,y,z))
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,1.0_dp)
px_ny_pz_dz(i_level_py)%HI_photoionization_rate(i_primary,-i_secondary) = 1.0!phi%photo_cell_HI
px_ny_pz_dz(i_level_py)%HeI_photoionization_rate(i_primary,-i_secondary) = phi%photo_cell_HeI
px_ny_pz_dz(i_level_py)%HeII_photoionization_rate(i_primary,-i_secondary) = phi%photo_cell_HeII
px_ny_pz_dz(i_level_py)%photoheating_rate(i_primary,-i_secondary) = phi%heat
enddo
enddo
enddo
end subroutine px_ny_pz_dz_photo_rate_calculation
subroutine px_ny_nz_dx_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
real(kind=dp) :: HeI_column_density_in
real(kind=dp) :: HeI_column_density_out
real(kind=dp) :: HeII_column_density_in
real(kind=dp) :: HeII_column_density_out
type(photrates) :: phi
real(kind=dp) :: i,j,k,x,y,z,n
do i_level_py = 1,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
i = real(i_level_py)
j = real(i_primary)
k = real(i_secondary)
n = real(partition(i_level_py))
x = (2.0*i-1.0)/2.0
y = -(2.0*j-1.0)*(2.0*i-1.0)/(4.0*n)
z = -(2.0*k-1.0)*(2.0*i-1.0)/(4.0*n)
HI_column_density_in = px_ny_nz_dx(i_level_py)%HI_column_density_in(-i_primary,-i_secondary)
HeI_column_density_in = px_ny_nz_dx(i_level_py)%HeI_column_density_in(-i_primary,-i_secondary)
HeII_column_density_in = px_ny_nz_dx(i_level_py)%HeII_column_density_in(-i_primary,-i_secondary)
HI_column_density_out = px_ny_nz_dx(i_level_py)%HI_column_density_out(-i_primary,-i_secondary)
HeI_column_density_out = px_ny_nz_dx(i_level_py)%HeI_column_density_out(-i_primary,-i_secondary)
HeII_column_density_out = px_ny_nz_dx(i_level_py)%HeII_column_density_out(-i_primary,-i_secondary)
!call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
! HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,correction (x,y,z))
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,1.0_dp)
px_ny_nz_dx(i_level_py)%HI_photoionization_rate(-i_primary,-i_secondary) = 1.0!phi%photo_cell_HI
px_ny_nz_dx(i_level_py)%HeI_photoionization_rate(-i_primary,-i_secondary) = phi%photo_cell_HeI
px_ny_nz_dx(i_level_py)%HeII_photoionization_rate(-i_primary,-i_secondary) = phi%photo_cell_HeII
px_ny_nz_dx(i_level_py)%photoheating_rate(-i_primary,-i_secondary) = phi%heat
enddo
enddo
enddo
end subroutine px_ny_nz_dx_photo_rate_calculation
subroutine px_ny_nz_dy_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
real(kind=dp) :: HeI_column_density_in
real(kind=dp) :: HeI_column_density_out
real(kind=dp) :: HeII_column_density_in
real(kind=dp) :: HeII_column_density_out
type(photrates) :: phi
real(kind=dp) :: i,j,k,x,y,z,n
do i_level_py = 1,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
i = real(i_secondary)
j = real(i_level_py)
k = real(i_primary)
n = real(partition(i_level_py))
x = (2.0*i-1.0)*(2.0*j-1.0)/(4.0*n)
y = -(2.0*j-1.0)/2.0
z = -(2.0*k-1.0)*(2.0*j-1.0)/(4.0*n)
HI_column_density_in = px_ny_nz_dy(-i_level_py)%HI_column_density_in(-i_primary,i_secondary)
HeI_column_density_in = px_ny_nz_dy(-i_level_py)%HeI_column_density_in(-i_primary,i_secondary)
HeII_column_density_in = px_ny_nz_dy(-i_level_py)%HeII_column_density_in(-i_primary,i_secondary)
HI_column_density_out = px_ny_nz_dy(-i_level_py)%HI_column_density_out(-i_primary,i_secondary)
HeI_column_density_out = px_ny_nz_dy(-i_level_py)%HeI_column_density_out(-i_primary,i_secondary)
HeII_column_density_out = px_ny_nz_dy(-i_level_py)%HeII_column_density_out(-i_primary,i_secondary)
!call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
! HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,correction (x,y,z))
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,1.0_dp)
px_ny_nz_dy(-i_level_py)%HI_photoionization_rate(-i_primary,i_secondary) = 1.0!phi%photo_cell_HI
px_ny_nz_dy(-i_level_py)%HeI_photoionization_rate(-i_primary,i_secondary) = phi%photo_cell_HeI
px_ny_nz_dy(-i_level_py)%HeII_photoionization_rate(-i_primary,i_secondary) = phi%photo_cell_HeII
px_ny_nz_dy(-i_level_py)%photoheating_rate(-i_primary,i_secondary) = phi%heat
enddo
enddo
enddo
end subroutine px_ny_nz_dy_photo_rate_calculation
subroutine px_ny_nz_dz_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
real(kind=dp) :: HeI_column_density_in
real(kind=dp) :: HeI_column_density_out
real(kind=dp) :: HeII_column_density_in
real(kind=dp) :: HeII_column_density_out
type(photrates) :: phi
real(kind=dp) :: i,j,k,x,y,z,n
do i_level_py = 1,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
i = real(i_primary)
j = real(i_secondary)
k = real(i_level_py)
n = real(partition(i_level_py))
x = (2.0*i-1.0)*(2.0*k-1.0)/(4.0*n)
y = -(2.0*j-1.0)*(2.0*k-1.0)/(4.0*n)
z = -(2.0*k-1.0)/2.0
HI_column_density_in = px_ny_nz_dz(-i_level_py)%HI_column_density_in(i_primary,-i_secondary)
HeI_column_density_in = px_ny_nz_dz(-i_level_py)%HeI_column_density_in(i_primary,-i_secondary)
HeII_column_density_in = px_ny_nz_dz(-i_level_py)%HeII_column_density_in(i_primary,-i_secondary)
HI_column_density_out = px_ny_nz_dz(-i_level_py)%HI_column_density_out(i_primary,-i_secondary)
HeI_column_density_out = px_ny_nz_dz(-i_level_py)%HeI_column_density_out(i_primary,-i_secondary)
HeII_column_density_out = px_ny_nz_dz(-i_level_py)%HeII_column_density_out(i_primary,-i_secondary)
!call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
! HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,correction (x,y,z))
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,1.0_dp)
px_ny_nz_dz(-i_level_py)%HI_photoionization_rate(i_primary,-i_secondary) = 1.0!phi%photo_cell_HI
px_ny_nz_dz(-i_level_py)%HeI_photoionization_rate(i_primary,-i_secondary) = phi%photo_cell_HeI
px_ny_nz_dz(-i_level_py)%HeII_photoionization_rate(i_primary,-i_secondary) = phi%photo_cell_HeII
px_ny_nz_dz(-i_level_py)%photoheating_rate(i_primary,-i_secondary) = phi%heat
enddo
enddo
enddo
end subroutine px_ny_nz_dz_photo_rate_calculation
subroutine nx_py_pz_dx_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
real(kind=dp) :: HeI_column_density_in
real(kind=dp) :: HeI_column_density_out
real(kind=dp) :: HeII_column_density_in
real(kind=dp) :: HeII_column_density_out
type(photrates) :: phi
real(kind=dp) :: i,j,k,x,y,z,n
do i_level_py = 1,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
i = real(i_level_py)
j = real(i_primary)
k = real(i_secondary)
n = real(partition(i_level_py))
x = -(2.0*i-1.0)/2.0
y = (2.0*j-1.0)*(2.0*i-1.0)/(4.0*n)
z = (2.0*k-1.0)*(2.0*i-1.0)/(4.0*n)
HI_column_density_in = nx_py_pz_dx(-i_level_py)%HI_column_density_in(i_primary,i_secondary)
HeI_column_density_in = nx_py_pz_dx(-i_level_py)%HeI_column_density_in(i_primary,i_secondary)
HeII_column_density_in = nx_py_pz_dx(-i_level_py)%HeII_column_density_in(i_primary,i_secondary)
HI_column_density_out = nx_py_pz_dx(-i_level_py)%HI_column_density_out(i_primary,i_secondary)
HeI_column_density_out = nx_py_pz_dx(-i_level_py)%HeI_column_density_out(i_primary,i_secondary)
HeII_column_density_out = nx_py_pz_dx(-i_level_py)%HeII_column_density_out(i_primary,i_secondary)
!call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
! HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,correction (x,y,z))
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,1.0_dp)
nx_py_pz_dx(-i_level_py)%HI_photoionization_rate(i_primary,i_secondary) = 1.0!phi%photo_cell_HI
nx_py_pz_dx(-i_level_py)%HeI_photoionization_rate(i_primary,i_secondary) = phi%photo_cell_HeI
nx_py_pz_dx(-i_level_py)%HeII_photoionization_rate(i_primary,i_secondary) = phi%photo_cell_HeII
nx_py_pz_dx(-i_level_py)%photoheating_rate(i_primary,i_secondary) = phi%heat
enddo
enddo
enddo
end subroutine nx_py_pz_dx_photo_rate_calculation
subroutine nx_py_pz_dy_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
real(kind=dp) :: HeI_column_density_in
real(kind=dp) :: HeI_column_density_out
real(kind=dp) :: HeII_column_density_in
real(kind=dp) :: HeII_column_density_out
type(photrates) :: phi
real(kind=dp) :: i,j,k,x,y,z,n
do i_level_py = 1,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
i = real(i_secondary)
j = real(i_level_py)
k = real(i_primary)
n = real(partition(i_level_py))
x = -(2.0*i-1.0)*(2.0*j-1.0)/(4.0*n)
y = (2.0*j-1.0)/2.0
z = (2.0*k-1.0)*(2.0*j-1.0)/(4.0*n)
HI_column_density_in = nx_py_pz_dy(i_level_py)%HI_column_density_in(i_primary,-i_secondary)
HeI_column_density_in = nx_py_pz_dy(i_level_py)%HeI_column_density_in(i_primary,-i_secondary)
HeII_column_density_in = nx_py_pz_dy(i_level_py)%HeII_column_density_in(i_primary,-i_secondary)
HI_column_density_out = nx_py_pz_dy(i_level_py)%HI_column_density_out(i_primary,-i_secondary)
HeI_column_density_out = nx_py_pz_dy(i_level_py)%HeI_column_density_out(i_primary,-i_secondary)
HeII_column_density_out = nx_py_pz_dy(i_level_py)%HeII_column_density_out(i_primary,-i_secondary)
!call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
! HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,correction (x,y,z))
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,1.0_dp)
nx_py_pz_dy(i_level_py)%HI_photoionization_rate(i_primary,-i_secondary) = 1.0!phi%photo_cell_HI
nx_py_pz_dy(i_level_py)%HeI_photoionization_rate(i_primary,-i_secondary) = phi%photo_cell_HeI
nx_py_pz_dy(i_level_py)%HeII_photoionization_rate(i_primary,-i_secondary) = phi%photo_cell_HeII
nx_py_pz_dy(i_level_py)%photoheating_rate(i_primary,-i_secondary) = phi%heat
enddo
enddo
enddo
end subroutine nx_py_pz_dy_photo_rate_calculation
subroutine nx_py_pz_dz_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
real(kind=dp) :: HeI_column_density_in
real(kind=dp) :: HeI_column_density_out
real(kind=dp) :: HeII_column_density_in
real(kind=dp) :: HeII_column_density_out
type(photrates) :: phi
real(kind=dp) :: i,j,k,x,y,z,n
do i_level_py = 1,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
i = real(i_primary)
j = real(i_secondary)
k = real(i_level_py)
n = real(partition(i_level_py))
x = -(2.0*i-1.0)*(2.0*k-1.0)/(4.0*n)
y = (2.0*j-1.0)*(2.0*k-1.0)/(4.0*n)
z = (2.0*k-1.0)/2.0
HI_column_density_in = nx_py_pz_dz(i_level_py)%HI_column_density_in(-i_primary,i_secondary)
HeI_column_density_in = nx_py_pz_dz(i_level_py)%HeI_column_density_in(-i_primary,i_secondary)
HeII_column_density_in = nx_py_pz_dz(i_level_py)%HeII_column_density_in(-i_primary,i_secondary)
HI_column_density_out = nx_py_pz_dz(i_level_py)%HI_column_density_out(-i_primary,i_secondary)
HeI_column_density_out = nx_py_pz_dz(i_level_py)%HeI_column_density_out(-i_primary,i_secondary)
HeII_column_density_out = nx_py_pz_dz(i_level_py)%HeII_column_density_out(-i_primary,i_secondary)
!call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
! HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,correction (x,y,z))
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,1.0_dp)
nx_py_pz_dz(i_level_py)%HI_photoionization_rate(-i_primary,i_secondary) = 1.0!phi%photo_cell_HI
nx_py_pz_dz(i_level_py)%HeI_photoionization_rate(-i_primary,i_secondary) = phi%photo_cell_HeI
nx_py_pz_dz(i_level_py)%HeII_photoionization_rate(-i_primary,i_secondary) = phi%photo_cell_HeII
nx_py_pz_dz(i_level_py)%photoheating_rate(-i_primary,i_secondary) = phi%heat
enddo
enddo
enddo
end subroutine nx_py_pz_dz_photo_rate_calculation
subroutine nx_py_nz_dx_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
real(kind=dp) :: HeI_column_density_in
real(kind=dp) :: HeI_column_density_out
real(kind=dp) :: HeII_column_density_in
real(kind=dp) :: HeII_column_density_out
type(photrates) :: phi
real(kind=dp) :: i,j,k,x,y,z,n
do i_level_py = 1,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
i = real(i_level_py)
j = real(i_primary)
k = real(i_secondary)
n = real(partition(i_level_py))
x = -(2.0*i-1.0)/2.0
y = (2.0*j-1.0)*(2.0*i-1.0)/(4.0*n)
z = -(2.0*k-1.0)*(2.0*i-1.0)/(4.0*n)
HI_column_density_in = nx_py_nz_dx(-i_level_py)%HI_column_density_in(i_primary,-i_secondary)
HeI_column_density_in = nx_py_nz_dx(-i_level_py)%HeI_column_density_in(i_primary,-i_secondary)
HeII_column_density_in = nx_py_nz_dx(-i_level_py)%HeII_column_density_in(i_primary,-i_secondary)
HI_column_density_out = nx_py_nz_dx(-i_level_py)%HI_column_density_out(i_primary,-i_secondary)
HeI_column_density_out = nx_py_nz_dx(-i_level_py)%HeI_column_density_out(i_primary,-i_secondary)
HeII_column_density_out = nx_py_nz_dx(-i_level_py)%HeII_column_density_out(i_primary,-i_secondary)
!call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
! HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,correction (x,y,z))
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,1.0_dp)
nx_py_nz_dx(-i_level_py)%HI_photoionization_rate(i_primary,-i_secondary) = 1.0!phi%photo_cell_HI
nx_py_nz_dx(-i_level_py)%HeI_photoionization_rate(i_primary,-i_secondary) = phi%photo_cell_HeI
nx_py_nz_dx(-i_level_py)%HeII_photoionization_rate(i_primary,-i_secondary) = phi%photo_cell_HeII
nx_py_nz_dx(-i_level_py)%photoheating_rate(i_primary,-i_secondary) = phi%heat
enddo
enddo
enddo
end subroutine nx_py_nz_dx_photo_rate_calculation
subroutine nx_py_nz_dy_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
real(kind=dp) :: HeI_column_density_in
real(kind=dp) :: HeI_column_density_out
real(kind=dp) :: HeII_column_density_in
real(kind=dp) :: HeII_column_density_out
type(photrates) :: phi
real(kind=dp) :: i,j,k,x,y,z,n
do i_level_py = 1,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
i = real(i_secondary)
j = real(i_level_py)
k = real(i_primary)
n = real(partition(i_level_py))
x = -(2.0*i-1.0)*(2.0*j-1.0)/(4.0*n)
y = (2.0*j-1.0)/2.0
z = -(2.0*k-1.0)*(2.0*j-1.0)/(4.0*n)
HI_column_density_in = nx_py_nz_dy(i_level_py)%HI_column_density_in(-i_primary,-i_secondary)
HeI_column_density_in = nx_py_nz_dy(i_level_py)%HeI_column_density_in(-i_primary,-i_secondary)
HeII_column_density_in = nx_py_nz_dy(i_level_py)%HeII_column_density_in(-i_primary,-i_secondary)
HI_column_density_out = nx_py_nz_dy(i_level_py)%HI_column_density_out(-i_primary,-i_secondary)
HeI_column_density_out = nx_py_nz_dy(i_level_py)%HeI_column_density_out(-i_primary,-i_secondary)
HeII_column_density_out = nx_py_nz_dy(i_level_py)%HeII_column_density_out(-i_primary,-i_secondary)
!call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
! HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,correction (x,y,z))
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,1.0_dp)
nx_py_nz_dy(i_level_py)%HI_photoionization_rate(-i_primary,-i_secondary) = 1.0!phi%photo_cell_HI
nx_py_nz_dy(i_level_py)%HeI_photoionization_rate(-i_primary,-i_secondary) = phi%photo_cell_HeI
nx_py_nz_dy(i_level_py)%HeII_photoionization_rate(-i_primary,-i_secondary) = phi%photo_cell_HeII
nx_py_nz_dy(i_level_py)%photoheating_rate(-i_primary,-i_secondary) = phi%heat
enddo
enddo
enddo
end subroutine nx_py_nz_dy_photo_rate_calculation
subroutine nx_py_nz_dz_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
real(kind=dp) :: HeI_column_density_in
real(kind=dp) :: HeI_column_density_out
real(kind=dp) :: HeII_column_density_in
real(kind=dp) :: HeII_column_density_out
type(photrates) :: phi
real(kind=dp) :: i,j,k,x,y,z,n
do i_level_py = 1,level_py
do i_primary = 1,partition(i_level_py)
do i_secondary = 1,partition(i_level_py)
solid_angle = pyramid_grid(i_level_py)%solid_angle(i_primary,i_secondary)
i = real(i_primary)
j = real(i_secondary)
k = real(i_level_py)
n = real(partition(i_level_py))
x = -(2.0*i-1.0)*(2.0*k-1.0)/(4.0*n)
y = (2.0*j-1.0)*(2.0*k-1.0)/(4.0*n)
z = -(2.0*k-1.0)/2.0
HI_column_density_in = nx_py_nz_dz(-i_level_py)%HI_column_density_in(-i_primary,i_secondary)
HeI_column_density_in = nx_py_nz_dz(-i_level_py)%HeI_column_density_in(-i_primary,i_secondary)
HeII_column_density_in = nx_py_nz_dz(-i_level_py)%HeII_column_density_in(-i_primary,i_secondary)
HI_column_density_out = nx_py_nz_dz(-i_level_py)%HI_column_density_out(-i_primary,i_secondary)
HeI_column_density_out = nx_py_nz_dz(-i_level_py)%HeI_column_density_out(-i_primary,i_secondary)
HeII_column_density_out = nx_py_nz_dz(-i_level_py)%HeII_column_density_out(-i_primary,i_secondary)
!call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
! HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,correction (x,y,z))
call photoion_solid_angle(phi,HI_column_density_in,HI_column_density_out,HeI_column_density_in,HeI_column_density_out,&
HeII_column_density_in,HeII_column_density_out,solid_angle,use_which_source,1.0_dp)
nx_py_nz_dz(-i_level_py)%HI_photoionization_rate(-i_primary,i_secondary) = 1.0!phi%photo_cell_HI
nx_py_nz_dz(-i_level_py)%HeI_photoionization_rate(-i_primary,i_secondary) = phi%photo_cell_HeI
nx_py_nz_dz(-i_level_py)%HeII_photoionization_rate(-i_primary,i_secondary) = phi%photo_cell_HeII
nx_py_nz_dz(-i_level_py)%photoheating_rate(-i_primary,i_secondary) = phi%heat
enddo
enddo
enddo
end subroutine nx_py_nz_dz_photo_rate_calculation
subroutine nx_ny_pz_dx_photo_rate_calculation ()
implicit none
integer :: i_primary,i_secondary,i_level_py
integer :: o_primary,o_secondary
real(kind=dp) :: solid_angle
real(kind=dp) :: HI_column_density_in
real(kind=dp) :: HI_column_density_out
real(kind=dp) :: HeI_column_density_in
real(kind=dp) :: HeI_column_density_out
real(kind=dp) :: HeII_column_density_in
real(kind=dp) :: HeII_column_density_out
type(photrates) :: phi
real(kind=dp) :: i,j,k,x,y,z,n