C $Header: /u/gcmpack/MITgcm/pkg/generic_advdiff/gad_dst3fl_adv_r.F,v 1.11 2014/04/04 20:29:08 jmc Exp $ C $Name: $ #include "GAD_OPTIONS.h" CBOP C !ROUTINE: GAD_DST3FL_ADV_R C !INTERFACE: ========================================================== SUBROUTINE GAD_DST3FL_ADV_R( I bi,bj,k,dTarg, I rTrans, wFld, I tracer, O wT, I myThid ) C !DESCRIPTION: C Calculates the area integrated vertical flux due to advection of a tracer C using 3rd Order DST Scheme with flux limiting C !USES: =============================================================== IMPLICIT NONE C == GLobal variables == #include "SIZE.h" #include "GRID.h" #include "GAD.h" C == Routine arguments == C !INPUT PARAMETERS: =================================================== C bi,bj :: tile indices C k :: vertical level C deltaTloc :: local time-step (s) C rTrans :: vertical volume transport C wFld :: vertical flow C tracer :: tracer field C myThid :: thread number INTEGER bi,bj,k _RL dTarg _RL rTrans(1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL wFld (1-OLx:sNx+OLx,1-OLy:sNy+OLy) _RL tracer(1-OLx:sNx+OLx,1-OLy:sNy+OLy,Nr) INTEGER myThid C !OUTPUT PARAMETERS: ================================================== C wT :: vertical advective flux _RL wT (1-OLx:sNx+OLx,1-OLy:sNy+OLy) C == Local variables == C !LOCAL VARIABLES: ==================================================== C i,j :: loop indices C km1 :: =max( k-1 , 1 ) C wLoc :: velocity, vertical component C wCFL :: Courant-Friedrich-Levy number INTEGER i,j,kp1,km1,km2 _RL Rjm,Rj,Rjp,wCFL,d0,d1 _RL psiP,psiM,thetaP,thetaM _RL wLoc _RL thetaMax PARAMETER( thetaMax = 1.D+20 ) km2=MAX(1,k-2) km1=MAX(1,k-1) kp1=MIN(Nr,k+1) DO j=1-OLy,sNy+OLy DO i=1-OLx,sNx+OLx #if (defined ALLOW_AUTODIFF defined TARGET_NEC_SX) C These lines make TAF create vectorizable code thetaP = 0. _d 0 thetaM = 0. _d 0 #endif Rjp=(tracer(i,j,k)-tracer(i,j,kp1)) & *maskC(i,j,kp1,bi,bj) Rj =(tracer(i,j,km1)-tracer(i,j,k)) & *maskC(i,j,k,bi,bj)*maskC(i,j,km1,bi,bj) Rjm=(tracer(i,j,km2)-tracer(i,j,km1)) & *maskC(i,j,km1,bi,bj) wLoc = wFld(i,j) wCFL = ABS(wLoc*dTarg*recip_drC(k)) d0=(2. _d 0 -wCFL)*(1. _d 0 -wCFL)*oneSixth d1=(1. _d 0 -wCFL*wCFL)*oneSixth C- the old version: can produce overflow, division by zero, C and is wrong for tracer with low concentration: c thetaP=Rjm/(1.D-20+Rj) c thetaM=Rjp/(1.D-20+Rj) C- the right expression, but not bounded: c thetaP=0.D0 c thetaM=0.D0 c IF (Rj.NE.0.D0) thetaP=Rjm/Rj c IF (Rj.NE.0.D0) thetaM=Rjp/Rj C- prevent |thetaP,M| to reach too big value: IF ( ABS(Rj)*thetaMax .LE. ABS(Rjm) ) THEN thetaP=SIGN(thetaMax,Rjm*Rj) ELSE thetaP=Rjm/Rj ENDIF IF ( ABS(Rj)*thetaMax .LE. ABS(Rjp) ) THEN thetaM=SIGN(thetaMax,Rjp*Rj) ELSE thetaM=Rjp/Rj ENDIF psiP=d0+d1*thetaP psiP=MAX(0. _d 0,MIN(MIN(1. _d 0,psiP), & thetaP*(1. _d 0 -wCFL)/(wCFL+1. _d -20) )) psiM=d0+d1*thetaM psiM=MAX(0. _d 0,MIN(MIN(1. _d 0,psiM), & thetaM*(1. _d 0 -wCFL)/(wCFL+1. _d -20) )) wT(i,j)= & 0.5*(rTrans(i,j)+ABS(rTrans(i,j))) & *( tracer(i,j, k ) + psiM*Rj ) & +0.5*(rTrans(i,j)-ABS(rTrans(i,j))) & *( tracer(i,j,km1) - psiP*Rj ) ENDDO ENDDO RETURN END