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jmc |
1.12 |
C $Header: /u/gcmpack/MITgcm/pkg/generic_advdiff/gad_dst3fl_adv_y.F,v 1.11 2006/06/19 14:40:43 jmc Exp $ |
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jmc |
1.5 |
C $Name: $ |
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adcroft |
1.1 |
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#include "GAD_OPTIONS.h" |
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jmc |
1.10 |
SUBROUTINE GAD_DST3FL_ADV_Y( |
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heimbach |
1.7 |
I bi,bj,k,deltaTloc, |
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jmc |
1.10 |
I vTrans, vFld, |
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jmc |
1.6 |
I maskLocS, tracer, |
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adcroft |
1.1 |
O vT, |
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I myThid ) |
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C /==========================================================\ |
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C | SUBROUTINE GAD_DST3FL_ADV_Y | |
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C | o Compute Meridional advective Flux of Tracer using | |
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C | 3rd Order DST Sceheme with flux limiting | |
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C |==========================================================| |
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IMPLICIT NONE |
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C == GLobal variables == |
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#include "SIZE.h" |
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#include "GRID.h" |
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#include "GAD.h" |
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C == Routine arguments == |
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INTEGER bi,bj,k |
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heimbach |
1.7 |
_RL deltaTloc |
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adcroft |
1.1 |
_RL vTrans(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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jmc |
1.10 |
_RL vFld (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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jmc |
1.6 |
_RS maskLocS(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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adcroft |
1.1 |
_RL tracer(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL vT (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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INTEGER myThid |
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C == Local variables == |
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jmc |
1.10 |
C vLoc :: velocity [m/s], meridional component |
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adcroft |
1.1 |
INTEGER i,j |
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jmc |
1.12 |
_RL Rjm,Rj,Rjp,vCFL,d0,d1,psiP,psiM,thetaP,thetaM |
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jmc |
1.10 |
_RL vLoc |
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jmc |
1.8 |
_RL thetaMax |
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PARAMETER( thetaMax = 1.D+20 ) |
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adcroft |
1.1 |
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DO i=1-Olx,sNx+Olx |
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jmc |
1.8 |
vT(i,1-Oly)=0. _d 0 |
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vT(i,2-Oly)=0. _d 0 |
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vT(i,sNy+Oly)=0. _d 0 |
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adcroft |
1.1 |
ENDDO |
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DO j=1-Oly+2,sNy+Oly-1 |
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DO i=1-Olx,sNx+Olx |
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jmc |
1.6 |
Rjp=(tracer(i,j+1)-tracer(i, j ))*maskLocS(i,j+1) |
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Rj =(tracer(i, j )-tracer(i,j-1))*maskLocS(i, j ) |
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Rjm=(tracer(i,j-1)-tracer(i,j-2))*maskLocS(i,j-1) |
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adcroft |
1.1 |
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jmc |
1.11 |
vLoc = vFld(i,j) |
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jmc |
1.12 |
vCFL = ABS( vLoc*deltaTloc |
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& *recip_dyC(i,j,bi,bj)*recip_deepFacC(k) ) |
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d0=(2. _d 0 -vCFL)*(1. _d 0 -vCFL)*oneSixth |
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d1=(1. _d 0 -vCFL*vCFL)*oneSixth |
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jmc |
1.8 |
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C- the old version: can produce overflow, division by zero, |
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c and is wrong for tracer with low concentration: |
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c thetaP=Rjm/(1.D-20+Rj) |
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c thetaM=Rjp/(1.D-20+Rj) |
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C- the right expression, but not bounded: |
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heimbach |
1.4 |
c thetaP=0.D0 |
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jmc |
1.8 |
c thetaM=0.D0 |
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heimbach |
1.4 |
c IF (Rj.NE.0.D0) thetaP=Rjm/Rj |
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jmc |
1.8 |
c IF (Rj.NE.0.D0) thetaM=Rjp/Rj |
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C- prevent |thetaP,M| to reach too big value: |
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IF ( ABS(Rj)*thetaMax .LE. ABS(Rjm) ) THEN |
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thetaP=SIGN(thetaMax,Rjm*Rj) |
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ELSE |
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thetaP=Rjm/Rj |
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ENDIF |
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IF ( ABS(Rj)*thetaMax .LE. ABS(Rjp) ) THEN |
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thetaM=SIGN(thetaMax,Rjp*Rj) |
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ELSE |
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thetaM=Rjp/Rj |
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ENDIF |
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adcroft |
1.1 |
psiP=d0+d1*thetaP |
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jmc |
1.12 |
psiP=MAX(0. _d 0,MIN(MIN(1. _d 0,psiP), |
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& thetaP*(1. _d 0 -vCFL)/(vCFL+1. _d -20) )) |
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adcroft |
1.1 |
psiM=d0+d1*thetaM |
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jmc |
1.12 |
psiM=MAX(0. _d 0,MIN(MIN(1. _d 0,psiM), |
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& thetaM*(1. _d 0 -vCFL)/(vCFL+1. _d -20) )) |
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jmc |
1.8 |
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adcroft |
1.1 |
vT(i,j)= |
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jmc |
1.12 |
& 0.5*(vTrans(i,j)+ABS(vTrans(i,j))) |
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heimbach |
1.2 |
& *( Tracer(i,j-1) + psiP*Rj ) |
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jmc |
1.12 |
& +0.5*(vTrans(i,j)-ABS(vTrans(i,j))) |
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heimbach |
1.2 |
& *( Tracer(i, j ) - psiM*Rj ) |
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adcroft |
1.1 |
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ENDDO |
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ENDDO |
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RETURN |
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END |
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