helio_gr.f90 Source File


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sourcefile~~helio_gr.f90~~EfferentGraph sourcefile~helio_gr.f90 helio_gr.f90 sourcefile~helio_module.f90 helio_module.f90 sourcefile~helio_gr.f90->sourcefile~helio_module.f90 sourcefile~swiftest_module.f90 swiftest_module.f90 sourcefile~helio_gr.f90->sourcefile~swiftest_module.f90 sourcefile~helio_module.f90->sourcefile~swiftest_module.f90 sourcefile~whm_module.f90 whm_module.f90 sourcefile~helio_module.f90->sourcefile~whm_module.f90 sourcefile~operator_module.f90 operator_module.f90 sourcefile~swiftest_module.f90->sourcefile~operator_module.f90 sourcefile~base_module.f90 base_module.f90 sourcefile~swiftest_module.f90->sourcefile~base_module.f90 sourcefile~collision_module.f90 collision_module.f90 sourcefile~swiftest_module.f90->sourcefile~collision_module.f90 sourcefile~lambda_function_module.f90 lambda_function_module.f90 sourcefile~swiftest_module.f90->sourcefile~lambda_function_module.f90 sourcefile~encounter_module.f90 encounter_module.f90 sourcefile~swiftest_module.f90->sourcefile~encounter_module.f90 sourcefile~walltime_module.f90 walltime_module.f90 sourcefile~swiftest_module.f90->sourcefile~walltime_module.f90 sourcefile~io_progress_bar_module.f90 io_progress_bar_module.f90 sourcefile~swiftest_module.f90->sourcefile~io_progress_bar_module.f90 sourcefile~netcdf_io_module.f90 netcdf_io_module.f90 sourcefile~swiftest_module.f90->sourcefile~netcdf_io_module.f90 sourcefile~solver_module.f90 solver_module.f90 sourcefile~swiftest_module.f90->sourcefile~solver_module.f90 sourcefile~whm_module.f90->sourcefile~swiftest_module.f90 sourcefile~coarray_module.f90 coarray_module.f90 sourcefile~base_module.f90->sourcefile~coarray_module.f90 sourcefile~collision_module.f90->sourcefile~base_module.f90 sourcefile~collision_module.f90->sourcefile~encounter_module.f90 sourcefile~encounter_module.f90->sourcefile~base_module.f90 sourcefile~encounter_module.f90->sourcefile~netcdf_io_module.f90 sourcefile~walltime_module.f90->sourcefile~base_module.f90 sourcefile~io_progress_bar_module.f90->sourcefile~base_module.f90 sourcefile~netcdf_io_module.f90->sourcefile~base_module.f90 sourcefile~solver_module.f90->sourcefile~base_module.f90 sourcefile~solver_module.f90->sourcefile~lambda_function_module.f90

Contents

Source Code


Source Code

! Copyright 2024 - The Minton Group at Purdue University
! This file is part of Swiftest.
! Swiftest is free software: you can redistribute it and/or modify it under the terms of the GNU General Public License 
! as published by the Free Software Foundation, either version 3 of the License, or (at your option) any later version.
! Swiftest is distributed in the hope that it will be useful, but WITHOUT ANY WARRANTY; without even the implied warranty 
! of MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public License for more details.
! You should have received a copy of the GNU General Public License along with Swiftest. 
! If not, see: https://www.gnu.org/licenses. 

submodule(helio) s_helio_gr
   use swiftest
contains

   pure module subroutine helio_gr_kick_getacch_pl(self, param) 
      !! author: David A. Minton
      !!
      !! Compute relativisitic accelerations of massive bodies
      !!    Based on Saha & Tremaine (1994) Eq. 28
      !!
      !! Adapted from David A. Minton's Swifter routine routine gr_whm_kick_getacch.f90
      implicit none
      ! Arguments
      class(helio_pl),            intent(inout) :: self   
         !! Helio massive body particle data structure
      class(swiftest_parameters), intent(in)    :: param 
         !! Current run configuration parameters 
      
      if (self%nbody == 0) return

      associate(pl => self, npl => self%nbody)
         call swiftest_gr_kick_getacch(pl%mu, pl%rh, pl%lmask, npl, param%inv_c2, pl%agr) 
         pl%ah(:,1:npl) = pl%ah(:,1:npl) + pl%agr(:,1:npl)
      end associate

      return
   end subroutine helio_gr_kick_getacch_pl


   pure module subroutine helio_gr_kick_getacch_tp(self, param)
      !! author: David A. Minton
      !!
      !! Compute relativisitic accelerations of test particles
      !!    Based on Saha & Tremaine (1994) Eq. 28
      !!
      !! Adapted from David A. Minton's Swifter routine routine gr_helio_kick_getacch.f90
      implicit none
      ! Arguments
      class(helio_tp),            intent(inout) :: self   
         !! Helio massive body particle data structure
      class(swiftest_parameters), intent(in)    :: param  
         !! Current run configuration parameters 
      
      if (self%nbody == 0) return

      associate(tp => self, ntp => self%nbody)
         call swiftest_gr_kick_getacch(tp%mu, tp%rh, tp%lmask, ntp, param%inv_c2, tp%agr) 
         tp%ah(:,1:ntp) = tp%ah(:,1:ntp) + tp%agr(:,1:ntp)
      end associate

      return
   end subroutine helio_gr_kick_getacch_tp
   

   pure module subroutine helio_gr_p4_pl(self, nbody_system, param, dt)
      !! author: David A. Minton
      !!
      !! Position kick to massive bodies due to p**4 term in the post-Newtonian correction
      !!    Based on Saha & Tremaine (1994) Eq. 28
      !!
      !! Adapted from David A. Minton's Swifter routine routine gr_helio_p4.f90
      implicit none
      ! Arguments
      class(helio_pl),              intent(inout) :: self  
          !! Swiftest particle object
      class(swiftest_nbody_system), intent(inout) :: nbody_system 
         !! Swiftest nbody system object
      class(swiftest_parameters),   intent(in)    :: param 
         !! Current run configuration parameters 
      real(DP),                     intent(in)    :: dt     
         !! Step size
      ! Internals
      integer(I4B) :: i, npl

      if (self%nbody == 0) return

      associate(lmask => self%lmask, rh => self%rh, vb => self%vb, inv_c2 => param%inv_c2)
         npl = self%nbody
#ifdef DOCONLOC
         do concurrent(i = 1:npl, lmask(i)) shared(inv_c2, lmask, rh, vb, dt)
#else
         do concurrent(i = 1:npl, lmask(i))
#endif
            call swiftest_gr_p4_pos_kick(inv_c2, rh(1,i), rh(2,i), rh(3,i), vb(1,i), vb(2,i), vb(3,i), dt)
         end do
      end associate
 
     return
   end subroutine helio_gr_p4_pl


   pure module subroutine helio_gr_p4_tp(self, nbody_system, param, dt)
      !! author: David A. Minton
      !!
      !! Position kick to test particles due to p**4 term in the post-Newtonian correction
      !!    Based on Saha & Tremaine (1994) Eq. 28
      !!
      !! Adapted from David A. Minton's Swifter routine routine gr_helio_p4.f90
      implicit none
      ! Arguments
      class(helio_tp),              intent(inout) :: self   
         !! Swiftest particle object
      class(swiftest_nbody_system), intent(inout) :: nbody_system 
         !! Swiftest nbody system object
      class(swiftest_parameters),   intent(in)    :: param  
         !! Current run configuration parameters 
      real(DP),                     intent(in)    :: dt     
         !! Step size
      ! Internals
      integer(I4B) :: i, ntp

      if (self%nbody == 0) return

      associate(rh => self%rh, vb => self%vb, lmask => self%lmask, inv_c2 => param%inv_c2)
         ntp = self%nbody
#ifdef DOCONLOC
         do concurrent(i = 1:ntp, lmask(i)) shared(inv_c2, lmask, rh, vb, dt)
#else
         do concurrent(i = 1:ntp, lmask(i))
#endif
            call swiftest_gr_p4_pos_kick(inv_c2, rh(1,i), rh(2,i), rh(3,i), vb(1,i), vb(2,i), vb(3,i), dt)
         end do
      end associate
 
     return
   end subroutine helio_gr_p4_tp

end submodule s_helio_gr