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!-------------------------------------------------------------------------------
!VERS
! This file is part of Code_Saturne, a general-purpose CFD tool.
!
! Copyright (C) 1998-2016 EDF S.A.
!
! This program 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 2 of the License, or (at your option) any later
! version.
!
! This program 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
! this program; if not, write to the Free Software Foundation, Inc., 51 Franklin
! Street, Fifth Floor, Boston, MA 02110-1301, USA.
!-------------------------------------------------------------------------------
!===============================================================================
! Purpose:
! -------
!> \file cs_user_source_terms-richards_decay.f90
!>
!> \brief User source terms example.
!>
!> See \subpage cs_user_source_terms and \subpage cs_user_source_terms-scalar_in_a_channel
!> for examples.
!>
!> \brief Additional right-hand side source terms for velocity components equation
!> (Navier-Stokes)
!>
!> \section ustsnv_use Usage
!>
!> The additional source term is decomposed into an explicit part (\c crvexp) and
!> an implicit part (\c crvimp) that must be provided here.
!> The resulting equation solved by the code for a velocity is:
!> \f[
!> \rho \norm{\vol{\celli}} \DP{\vect{u}} + ....
!> = \tens{crvimp} \cdot \vect{u} + \vect{crvexp}
!> \f]
!>
!> Note that \c crvexp and \c crvimp are defined after the Finite Volume integration
!> over the cells, so they include the "volume" term. More precisely:
!> - crvexp is expressed in kg.m/s2
!> - crvimp is expressed in kg/s
!>
!> The \c crvexp and \c crvimp arrays are already initialized to 0
!> before entering the
!> the routine. It is not needed to do it in the routine (waste of CPU time).
!>
!> \remark The additional force on \f$ x_i \f$ direction is given by
!> \c crvexp(i, iel) + vel(j, iel)* crvimp(j, i).
!>
!> For stability reasons, Code_Saturne will not add -crvimp directly to the
!> diagonal of the matrix, but Max(-crvimp,0). This way, the crvimp term is
!> treated implicitely only if it strengthens the diagonal of the matrix.
!> However, when using the second-order in time scheme, this limitation cannot
!> be done anymore and -crvimp is added directly. The user should therefore test
!> the negativity of crvimp by himself.
!>
!> When using the second-order in time scheme, one should supply:
!> - crvexp at time n
!> - crvimp at time n+1/2
!>
!> The selection of cells where to apply the source terms is based on a
!> \ref getcel command. For more info on the syntax of the \ref getcel command,
!> refer to the user manual or to the comments on the similar command
!> \ref getfbr in the routine \ref cs_user_boundary_conditions.
!
!-------------------------------------------------------------------------------
subroutine ustssc &
!================
( nvar , nscal , ncepdp , ncesmp , &
iscal , &
icepdc , icetsm , itypsm , &
dt , &
ckupdc , smacel , &
crvexp , crvimp )
!===============================================================================
! Module files
!===============================================================================
use paramx
use numvar
use entsor
use optcal
use cstphy
use parall
use period
use mesh
use field
use darcy_module
!===============================================================================
implicit none
integer nvar , nscal
integer ncepdp , ncesmp
integer iscal
integer icepdc(ncepdp)
integer icetsm(ncesmp), itypsm(ncesmp,nvar)
double precision dt(ncelet)
double precision ckupdc(ncepdp,6), smacel(ncesmp,nvar)
double precision crvexp(ncelet), crvimp(ncelet)
character*80 chaine
integer iiscvr, iel
integer ilelt, nlelt
double precision lambda
integer, allocatable, dimension(:) :: lstelt
double precision, dimension(:), pointer :: cpro_rom
integer delay_id
double precision, dimension(:), pointer :: delay, saturation
character*80 fname
!===============================================================================
! In groundwater module flow, the radioactive decay of solute is treated as a
! source term in the transport equation
allocate(lstelt(ncel))
call field_get_label(ivarfl(isca(iscal)), chaine)
iiscvr = iscavr(iscal)
if (iwarni(isca(iscal)).ge.1) then
write(nfecra,1000) chaine(1:8)
endif
!< [richards_decay]
! Set the first order decay coefficient
lambda = 1.d-2
! Set radioactive decay for the first solute
if (isca(iscal).eq.1) then
do iel = 1, ncel
crvimp(iel) = -volume(iel)*lambda
enddo
endif
!< [richards_decay]
1000 format(' User source terms for variable ',A8,/)
deallocate(lstelt)
return
end subroutine ustssc
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