Moved calculation of S(a,b) cross sections into separate subroutine.

This commit is contained in:
Paul Romano 2011-12-16 16:18:53 -06:00
parent 56de9654ad
commit 9e30afb733

View file

@ -226,13 +226,8 @@ contains
integer, intent(in) :: index_sab ! index into sab_tables array
integer :: IE ! index on nuclide energy grid
integer :: IE_sab ! index on S(a,b) energy grid
real(8) :: f ! interp factor on nuclide energy grid
real(8) :: f_sab ! interp factor on S(a,b) energy grid
real(8) :: inelastic ! S(a,b) inelastic cross section
real(8) :: elastic ! S(a,b) elastic cross section
type(Nuclide), pointer :: nuc => null()
type(SAB_Table), pointer :: sab => null()
! Set pointer to nuclide
nuc => nuclides(index_nuclide)
@ -282,76 +277,97 @@ contains
! need to correct it by subtracting the non-S(a,b) elastic cross section and
! then add back in the calculated S(a,b) elastic+inelastic cross section.
if (index_sab > 0) then
micro_xs(index_nuclide) % use_sab = .true.
! Get pointer to S(a,b) table
sab => sab_tables(index_sab)
! Get index and interpolation factor for inelastic grid
if (p%E < sab % inelastic_e_in(1)) then
IE_sab = 1
f_sab = ZERO
else
IE_sab = binary_search(sab % inelastic_e_in, sab % n_inelastic_e_in, p%E)
f_sab = (p%E - sab%inelastic_e_in(IE_sab)) / &
(sab%inelastic_e_in(IE_sab+1) - sab%inelastic_e_in(IE_sab))
end if
! Calculate S(a,b) inelastic scattering cross section
inelastic = (ONE-f_sab) * sab % inelastic_sigma(IE_sab) + f_sab * &
sab % inelastic_sigma(IE_sab + 1)
! Check for elastic data
if (p % E < sab % threshold_elastic) then
! Determine whether elastic scattering is given in the coherent or
! incoherent approximation. For coherent, the cross section is
! represented as P/E whereas for incoherent, it is simply P
if (sab % elastic_mode == SAB_ELASTIC_EXACT) then
if (p % E < sab % elastic_e_in(1)) then
! If energy is below that of the lowest Bragg peak, the elastic
! cross section will be zero
elastic = ZERO
else
IE_sab = binary_search(sab % elastic_e_in, sab % n_elastic_e_in, p%E)
elastic = sab % elastic_P(IE_sab) / p % E
end if
else
! Determine index on elastic energy grid
if (p % E < sab % elastic_e_in(1)) then
IE_sab = 1
else
IE_sab = binary_search(sab % elastic_e_in, sab % n_elastic_e_in, p%E)
end if
! Get interpolation factor for elastic grid
f_sab = (p%E - sab%elastic_e_in(IE_sab))/(sab%elastic_e_in(IE_sab+1) - &
sab%elastic_e_in(IE_sab))
! Calculate S(a,b) elastic scattering cross section
elastic = (ONE-f_sab) * sab % elastic_P(IE_sab) + f_sab * &
sab % elastic_P(IE_sab + 1)
end if
else
! No elastic data
elastic = ZERO
end if
! Correct total and elastic cross sections
micro_xs(index_nuclide) % total = micro_xs(index_nuclide) % total - &
micro_xs(index_nuclide) % elastic + inelastic + elastic
micro_xs(index_nuclide) % elastic = inelastic + elastic
! Store S(a,b) elastic cross section for sampling later
micro_xs(index_nuclide) % elastic_sab = elastic
end if
if (index_sab > 0) call calculate_sab_xs(p, index_nuclide, index_sab)
! Set last evaluated energy
micro_xs(index_nuclide) % last_E = p % E
end subroutine calculate_nuclide_xs
!===============================================================================
! CALCULATE_SAB_XS determines the elastic and inelastic scattering
! cross-sections in the thermal energy range. These cross sections replace
! whatever data were taken from the normal Nuclide table.
!===============================================================================
subroutine calculate_sab_xs(p, index_nuclide, index_sab)
type(Particle), pointer :: p
integer, intent(in) :: index_nuclide ! index into nuclides array
integer, intent(in) :: index_sab ! index into sab_tables array
integer :: IE_sab ! index on S(a,b) energy grid
real(8) :: f_sab ! interp factor on S(a,b) energy grid
real(8) :: inelastic ! S(a,b) inelastic cross section
real(8) :: elastic ! S(a,b) elastic cross section
type(SAB_Table), pointer :: sab => null()
! Set flag that S(a,b) treatment should be used for scattering
micro_xs(index_nuclide) % use_sab = .true.
! Get pointer to S(a,b) table
sab => sab_tables(index_sab)
! Get index and interpolation factor for inelastic grid
if (p%E < sab % inelastic_e_in(1)) then
IE_sab = 1
f_sab = ZERO
else
IE_sab = binary_search(sab % inelastic_e_in, sab % n_inelastic_e_in, p%E)
f_sab = (p%E - sab%inelastic_e_in(IE_sab)) / &
(sab%inelastic_e_in(IE_sab+1) - sab%inelastic_e_in(IE_sab))
end if
! Calculate S(a,b) inelastic scattering cross section
inelastic = (ONE-f_sab) * sab % inelastic_sigma(IE_sab) + f_sab * &
sab % inelastic_sigma(IE_sab + 1)
! Check for elastic data
if (p % E < sab % threshold_elastic) then
! Determine whether elastic scattering is given in the coherent or
! incoherent approximation. For coherent, the cross section is
! represented as P/E whereas for incoherent, it is simply P
if (sab % elastic_mode == SAB_ELASTIC_EXACT) then
if (p % E < sab % elastic_e_in(1)) then
! If energy is below that of the lowest Bragg peak, the elastic
! cross section will be zero
elastic = ZERO
else
IE_sab = binary_search(sab % elastic_e_in, sab % n_elastic_e_in, p%E)
elastic = sab % elastic_P(IE_sab) / p % E
end if
else
! Determine index on elastic energy grid
if (p % E < sab % elastic_e_in(1)) then
IE_sab = 1
else
IE_sab = binary_search(sab % elastic_e_in, sab % n_elastic_e_in, p%E)
end if
! Get interpolation factor for elastic grid
f_sab = (p%E - sab%elastic_e_in(IE_sab))/(sab%elastic_e_in(IE_sab+1) - &
sab%elastic_e_in(IE_sab))
! Calculate S(a,b) elastic scattering cross section
elastic = (ONE-f_sab) * sab % elastic_P(IE_sab) + f_sab * &
sab % elastic_P(IE_sab + 1)
end if
else
! No elastic data
elastic = ZERO
end if
! Correct total and elastic cross sections
micro_xs(index_nuclide) % total = micro_xs(index_nuclide) % total - &
micro_xs(index_nuclide) % elastic + inelastic + elastic
micro_xs(index_nuclide) % elastic = inelastic + elastic
! Store S(a,b) elastic cross section for sampling later
micro_xs(index_nuclide) % elastic_sab = elastic
end subroutine calculate_sab_xs
!===============================================================================
! FIND_ENERGY_INDEX determines the index on the union energy grid and the
! interpolation factor for a particle at a certain energy