/usr/share/code_saturne/user/ustsma.f90 is in code-saturne-data 3.3.2-4.
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! Code_Saturne version 3.3.2
! --------------------------
! This file is part of Code_Saturne, a general-purpose CFD tool.
!
! Copyright (C) 1998-2014 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.
!-------------------------------------------------------------------------------
subroutine ustsma &
!================
( nvar , nscal , ncepdp , &
ncesmp , iappel , &
icepdc , icetsm , itypsm , izctsm , &
dt , &
ckupdc , smacel )
!===============================================================================
! Purpose:
! -------
! User subroutine.
! Mass source term
! The subroutine ustsma is called at three different stages in the code
! (iappel = 1, 2 or 3)
! iappel = 1
! Calculation of the number of cells where a mass source term is
! imposed: ncesmp
! Called once at the beginning of the calculation
! iappel = 2
! Identification of the cells where a mass source term is imposed:
! array icesmp(ncesmp)
! Called once at the beginning of the calculation
! iappel = 3
! Calculation of the values of the mass source term
! Called at each time step
! The equation for mass conservation becomes
! d(rho)/dt + div(rho u) = gamma
! The equation for a variable f becomes
! d(f)/dt = ..... + gamma*(f_i - f)
! discretized as
! rho*(f^(n+1) - f^(n))/dt = .....
! + gamma*(f_i - f^(n+1))
! f_i is the value of f associated to the injected mass.
! Two options are available:
! - the mass flux is injected with the local value of variable f
! --> f_i = f^(n+1)
! (the equation for f is therefore not modified)
!
! - the mass flux is injected with a specific value for f
! --> f_i is specified by the user
! Variables to be specified by the user
! =====================================
! ncesmp: number of cells where a mass source term is imposed
! icetsm(ieltsm): identification of the cells where a mass source
! term is imposed.
! For each cell where a mass source term is imposed
! (ielstm in [1;ncesmp]), icetsm(ieltsm) is the
! global index number of the corresponding cell
! (icestm(ieltsm) in [1;ncel])
! smacel(ieltsm,ipr): value of the injection mass rate gamma (kg/m3/s)
! in the ieltsm cell with mass source term
! itypsm(ieltsm,ivar): type of treatment for variable ivar in the
! ieltsm cell with mass source term.
! * itypsm = 0 --> injection of ivar at local value
! * itypsm = 1 --> injection of ivar at user
! specified value
! smacel(ieltsm,ivar): specified value for variable ivar associated
! to the injected mass in the ieltsm cell with
! a mass source term
! except for ivar=ipr
!
! Remarks
! =======
!
! - if itypsm(ieltsm,ivar)=0, smacel(ieltsm,ivar) is not used
! - if smacel(ieltsm,ipr)<0, mass is removed from the system,
! therefore Code_Saturna automatically considers f_i=f^(n+1),
! whatever the values of itypsm or smacel specified by the user
! - if a value ivar is not linked for a mass source
! term is imposed, no source term will be taen into account.
! - if a scalar doesn't evolve following the standard equation
! d(rho f)/dt + d(rho U f)/dx = ...
! (alternate convective field for instance), the source term
! set by this routine will nto be correct (except in case of
! injection at the local value of the variable). The proper source
! term should be added directly in ustssc.
! Identification of cells
! =======================
! The selection of cells where to apply the source terms is based on a getcel
! command. For more info on the syntax of the getcel command, refer to the
! user manual or to the comments on the similar command getfbr in the routine
! cs_user_boundary_conditions.
!-------------------------------------------------------------------------------
! Arguments
!__________________.____._____.________________________________________________.
! name !type!mode ! role !
!__________________!____!_____!________________________________________________!
! nvar ! i ! <-- ! total number of variables !
! nscal ! i ! <-- ! total number of scalars !
! ncepdp ! i ! <-- ! number of cells with head loss terms !
! ncssmp ! i ! <-- ! number of cells with mass source terms !
! iappel ! i ! <-- ! indicates which at which stage the routine is !
! ! ! ! is called !
! icepdc(ncepdp) ! ia ! <-- ! index number of cells with head loss terms !
! ! ! ! (usable only for iappel > 1) !
! icetsm(ncesmp) ! ia ! <-- ! index number of cells with mass source terms !
! itypsm ! ia ! <-- ! type of mass source term for each variable !
! (ncesmp,nvar) ! ! ! (see uttsma.f90) !
! izctsm(ncelet) ! ia ! <-- ! cells zone for mass source terms definition !
! dt(ncelet) ! ra ! <-- ! time step (per cell) !
! ckupdc(ncepdp,6) ! ra ! <-- ! head loss coefficient !
! smacel ! ra ! <-- ! value associated to each variable in the mass !
! (ncesmp,nvar) ! ! ! source terms or mass rate !
!__________________!____!_____!________________________________________________!
! Type: i (integer), r (real), s (string), a (array), l (logical),
! and composite types (ex: ra real array)
! mode: <-- input, --> output, <-> modifies data, --- work array
!===============================================================================
!===============================================================================
! Module files
!===============================================================================
use paramx
use numvar
use entsor
use optcal
use cstphy
use cstnum
use parall
use period
use mesh
!===============================================================================
implicit none
! Arguments
integer nvar , nscal
integer ncepdp , ncesmp
integer iappel
integer icepdc(*)
integer icetsm(ncesmp), itypsm(ncesmp,nvar)
integer izctsm(ncel)
double precision dt(ncelet)
double precision ckupdc(ncepdp,6)
double precision smacel(ncesmp,nvar)
! Local variables
integer ieltsm
integer ifac, ii
integer ilelt, nlelt
integer izone
double precision vent, vent2
double precision dh, ustar2
double precision xkent, xeent
double precision flucel
double precision vtot , gamma
integer, allocatable, dimension(:) :: lstelt
!===============================================================================
! Allocate a temporary array for cells selection
allocate(lstelt(ncel))
if (iappel.eq.1.or.iappel.eq.2) then
!===============================================================================
! 1. One or two calls
! First call:
!
! iappel = 1: ncesmp: calculation of the number of cells with
! mass source term
! Second call (if ncesmp>0):
! iappel = 2: icetsm: index number of cells with mass source terms
! WARNINGS
! ========
! Do not use smacel in this section (it is set on the third call, iappel=3)
! Do not use icetsm in this section on the first call (iappel=1)
! This section (iappel=1 or 2) is only accessed at the beginning of a
! calculation. Should the localization of the mass source terms evolve
! in time, the user must identify at the beginning all cells that can
! potentially becomea mass source term.
!===============================================================================
! 1.1 To be completed by the user: cell selection
! -----------------------------------------------
! Example 1: No mass source term (default)
ieltsm = 0
! Example 2 : Mass source term one in the cells that
! have a boundary face of color 3 and the cells
! with a coordinate X between 2.5 and 5.
!
! In this test in two parts, one mut pay attention not to count
! the cells twice (a cell with a boundary face of color 3 can
! also have a coordinate X between 2.5 and 5).
! One should also pay attention that, on the first call, the
! array icetsm doesn't exist yet. It mustn't be used outside
! of tests (iappel.eq.2).
! It is quite frequent to forget to remove this example when it is
! not needed. Therefore the following test is designed to prevent
! any bad surprise.
if (.false.) then
izone = 0
ieltsm = 0
! Cells with coordinate X between 2.5 and 5.
call getcel('X > 2.5 and X < 5.0',nlelt,lstelt)
izone = izone + 1
do ilelt = 1, nlelt
ii = lstelt(ilelt)
izctsm(ii) = izone
ieltsm = ieltsm + 1
if (iappel.eq.2) icetsm(ieltsm) = ii
enddo
! Cells with a boundary face of color 3
call getfbr('3',nlelt,lstelt)
izone = izone + 1
do ilelt = 1, nlelt
ifac = lstelt(ilelt)
ii = ifabor(ifac)
! The cells that have already been counted above are not
! counted again.
if (.not.(xyzcen(1,ii).lt.500.d0.and. &
xyzcen(1,ii).gt.250.d0) )then
ieltsm = ieltsm + 1
izctsm(ii) = izone
if (iappel.eq.2) icetsm(ieltsm) = ii
endif
enddo
endif
! 1.2 Generic subsection: do not modify
! -------------------------------------
! --- For iappel = 1,
! Specification of ncesmp. This block is valid for both examples.
if (iappel.eq.1) then
ncesmp = ieltsm
endif
!-------------------------------------------------------------------------------
elseif (iappel.eq.3) then
!===============================================================================
! 2. For ncesmp > 0 , third call
! iappel = 3 : itypsm : type of mass source term
! smacel : mass source term
! Remark
! ======
! If itypsm(ieltsm,ivar) is set to 1, smacel(ieltsm,ivar) must be set.
!===============================================================================
! 2.1 To be completed by the user: itypsm and smacel
! --------------------------------------------------
! Example 1: simulation of an inlet condition by mass source terms
! and printing of the total mass rate.
vent = 0.1d0
vent2 = vent**2
dh = 0.5d0
!
! Calculation of the inlet conditions for k and epsilon with standard
! laws in a circular pipe.
ustar2 = 0.d0
xkent = epzero
xeent = epzero
call keendb &
!==========
( vent2, dh, ro0, viscl0, cmu, xkappa, &
ustar2, xkent, xeent )
flucel = 0.d0
do ieltsm = 1, ncesmp
smacel(ieltsm,ipr) = 30000.d0
itypsm(ieltsm,iv) = 1
smacel(ieltsm,iv) = vent
if (itytur.eq.2) then
itypsm(ieltsm,ik) = 1
smacel(ieltsm,ik) = xkent
itypsm(ieltsm,iep) = 1
smacel(ieltsm,iep) = xeent
else if (itytur.eq.3) then
itypsm(ieltsm,ir11) = 1
itypsm(ieltsm,ir12) = 1
itypsm(ieltsm,ir13) = 1
itypsm(ieltsm,ir22) = 1
itypsm(ieltsm,ir23) = 1
itypsm(ieltsm,ir33) = 1
smacel(ieltsm,ir11) = 2.d0/3.d0*xkent
smacel(ieltsm,ir12) = 0.d0
smacel(ieltsm,ir13) = 0.d0
smacel(ieltsm,ir22) = 2.d0/3.d0*xkent
smacel(ieltsm,ir23) = 0.d0
smacel(ieltsm,ir33) = 2.d0/3.d0*xkent
itypsm(ieltsm,iep) = 1
smacel(ieltsm,iep) = xeent
else if (iturb.eq.50) then
itypsm(ieltsm,ik) = 1
smacel(ieltsm,ik) = xkent
itypsm(ieltsm,iep) = 1
smacel(ieltsm,iep) = xeent
itypsm(ieltsm,iphi) = 1
smacel(ieltsm,iphi) = 2.d0/3.d0
! There is no mass source term in the equation for f_bar
else if (iturb.eq.60) then
itypsm(ieltsm,ik) = 1
smacel(ieltsm,ik) = xkent
itypsm(ieltsm,iomg)= 1
smacel(ieltsm,iomg)= xeent/cmu/xkent
endif
if (nscal.gt.0) then
do ii = 1, nscal
itypsm(ieltsm,isca(ii)) = 1
smacel(ieltsm,isca(ii)) = 1.d0
enddo
endif
flucel = flucel+ &
volume(icetsm(ieltsm))*smacel(ieltsm,ipr)
enddo
if (irangp.ge.0) then
call parsom (flucel)
endif
if (iwarni(ipr).ge.1) then
write(nfecra,1000) flucel
endif
!-------------------------------------------------------------------------------
! Example 2 : simulation of a suction (by a pump for instance) with a
! total rate of 80 000 kg/s.
! The suction rate is supposed to be uniformly distributed
! on all the cells selected above.
! It is quite frequent to forget to remove this example when it is
! not needed. Therefore the following test is designed to prevent
! any bad surprise.
if (.false.) then
! Calculation of the total volume of the area where the mass source
! term is imposed (the case of parallel computing is taken into
! account with the call to parsom).
vtot = 0.d0
do ieltsm = 1, ncesmp
vtot = vtot + volume(icetsm(ieltsm))
enddo
if (irangp.ge.0) then
call parsom (vtot)
endif
! The mass suction rate is gamma = -80000/vtot (in kg/m3/s)
! It is set below, with a test for cases where vtot=0. The total
! mass rate is calculated for verification.
if (vtot.gt.0.d0) then
gamma = -80000.d0/vtot
else
write(nfecra,9000) vtot
call csexit (1)
endif
flucel = 0.d0
do ieltsm = 1, ncesmp
smacel(ieltsm,ipr) = gamma
flucel = flucel+ &
volume(icetsm(ieltsm))*smacel(ieltsm,ipr)
enddo
if (irangp.ge.0) then
call parsom (flucel)
endif
if (iwarni(ipr).ge.1) then
write(nfecra,2000) flucel, vtot
endif
endif
!-------------------------------------------------------------------------------
endif
!--------
! Formats
!--------
1000 format(/,'Mass rate generated in the domain: ',E14.5,/)
2000 format(/,'Mass flux rate generated in the domain: ',E14.5,/, &
' distributed on the volume: ',E14.5)
9000 format(/,'Error in ustsma ',/, &
' the volume of the mass suction area is = ',E14.5,/)
!----
! End
!----
! Deallocate the temporary array
deallocate(lstelt)
return
end subroutine ustsma
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