pkg/mom_vecinv/mom_vecinv.F

C $Header: /u/gcmpack/MITgcm/pkg/mom_vecinv/mom_vecinv.F,v 1.15 2004/02/25 00:56:47 jmc Exp $
C $Name:  $

#include "PACKAGES_CONFIG.h"
#include "CPP_OPTIONS.h"

      SUBROUTINE MOM_VECINV( 
     I        bi,bj,iMin,iMax,jMin,jMax,k,kUp,kDown,
     I        dPhiHydX,dPhiHydY,KappaRU,KappaRV,
     U        fVerU, fVerV,
     I        myTime, myIter, myThid)
C     /==========================================================\
C     | S/R MOM_VECINV                                           |
C     | o Form the right hand-side of the momentum equation.     |
C     |==========================================================|
C     | Terms are evaluated one layer at a time working from     |
C     | the bottom to the top. The vertically integrated         |
C     | barotropic flow tendency term is evluated by summing the |
C     | tendencies.                                              |
C     | Notes:                                                   |
C     | We have not sorted out an entirely satisfactory formula  |
C     | for the diffusion equation bc with lopping. The present  |
C     | form produces a diffusive flux that does not scale with  |
C     | open-area. Need to do something to solidfy this and to   |
C     | deal "properly" with thin walls.                         |
C     \==========================================================/
      IMPLICIT NONE

C     == Global variables ==
#include "SIZE.h"
#include "DYNVARS.h"
#include "EEPARAMS.h"
#include "PARAMS.h"
#include "GRID.h"
#ifdef ALLOW_TIMEAVE
#include "TIMEAVE_STATV.h"
#endif

C     == Routine arguments ==
C     fVerU   - Flux of momentum in the vertical
C     fVerV     direction out of the upper face of a cell K
C               ( flux into the cell above ).
C     dPhiHydX,Y :: Gradient (X & Y dir.) of Hydrostatic Potential
C     bi, bj, iMin, iMax, jMin, jMax - Range of points for which calculation
C                                      results will be set.
C     kUp, kDown                     - Index for upper and lower layers.
C     myThid - Instance number for this innvocation of CALC_MOM_RHS
      _RL dPhiHydX(1-Olx:sNx+Olx,1-Oly:sNy+Oly)
      _RL dPhiHydY(1-Olx:sNx+Olx,1-Oly:sNy+Oly)
      _RL KappaRU(1-OLx:sNx+OLx,1-OLy:sNy+OLy,Nr)
      _RL KappaRV(1-OLx:sNx+OLx,1-OLy:sNy+OLy,Nr)
      _RL fVerU(1-OLx:sNx+OLx,1-OLy:sNy+OLy,2)
      _RL fVerV(1-OLx:sNx+OLx,1-OLy:sNy+OLy,2)
      INTEGER kUp,kDown
      _RL     myTime
      INTEGER myIter
      INTEGER myThid
      INTEGER bi,bj,iMin,iMax,jMin,jMax

#ifdef ALLOW_MOM_VECINV

C     == Functions ==
      LOGICAL  DIFFERENT_MULTIPLE
      EXTERNAL DIFFERENT_MULTIPLE

C     == Local variables ==
      _RL      aF (1-OLx:sNx+OLx,1-OLy:sNy+OLy)
      _RL      vF (1-OLx:sNx+OLx,1-OLy:sNy+OLy)
      _RL      vrF (1-OLx:sNx+OLx,1-OLy:sNy+OLy)
      _RL      uCf (1-OLx:sNx+OLx,1-OLy:sNy+OLy)
      _RL      vCf (1-OLx:sNx+OLx,1-OLy:sNy+OLy)
      _RL      mT (1-OLx:sNx+OLx,1-OLy:sNy+OLy)
      _RL      pF (1-OLx:sNx+OLx,1-OLy:sNy+OLy)
      _RL del2u(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
      _RL del2v(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
      _RL tension(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
      _RL strain(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
      _RS hFacZ(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
      _RS r_hFacZ(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
      _RS xA(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
      _RS yA(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
      _RL uFld(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
      _RL vFld(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
      _RL dStar(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
      _RL zStar(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
      _RL uDiss(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
      _RL vDiss(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
C     I,J,K - Loop counters
      INTEGER i,j,k
C     rVelMaskOverride - Factor for imposing special surface boundary conditions
C                        ( set according to free-surface condition ).
C     hFacROpen        - Lopped cell factos used tohold fraction of open
C     hFacRClosed        and closed cell wall.
      _RL  rVelMaskOverride
C     xxxFac - On-off tracer parameters used for switching terms off.
      _RL  uDudxFac
      _RL  AhDudxFac
      _RL  A4DuxxdxFac
      _RL  vDudyFac
      _RL  AhDudyFac
      _RL  A4DuyydyFac
      _RL  rVelDudrFac
      _RL  ArDudrFac
      _RL  fuFac
      _RL  phxFac
      _RL  mtFacU
      _RL  uDvdxFac
      _RL  AhDvdxFac
      _RL  A4DvxxdxFac
      _RL  vDvdyFac
      _RL  AhDvdyFac
      _RL  A4DvyydyFac
      _RL  rVelDvdrFac
      _RL  ArDvdrFac
      _RL  fvFac
      _RL  phyFac
      _RL  vForcFac
      _RL  mtFacV
      _RL wVelBottomOverride
      LOGICAL bottomDragTerms
      LOGICAL writeDiag
      _RL KE(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
      _RL omega3(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
      _RL vort3(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
      _RL hDiv(1-OLx:sNx+OLx,1-OLy:sNy+OLy)

#ifdef ALLOW_AUTODIFF_TAMC
C--   only the kDown part of fverU/V is set in this subroutine
C--   the kUp is still required
C--   In the case of mom_fluxform Kup is set as well
C--   (at least in part)
      fVerU(1,1,kUp) = fVerU(1,1,kUp)
      fVerV(1,1,kUp) = fVerV(1,1,kUp)
#endif

      rVelMaskOverride=1.
      IF ( k .EQ. 1 ) rVelMaskOverride=freeSurfFac
      wVelBottomOverride=1.
      IF (k.EQ.Nr) wVelBottomOverride=0.
      writeDiag = DIFFERENT_MULTIPLE(diagFreq, myTime,
     &                                         myTime-deltaTClock)

C     Initialise intermediate terms
      DO J=1-OLy,sNy+OLy
       DO I=1-OLx,sNx+OLx
        aF(i,j)   = 0.
        vF(i,j)   = 0.
        vrF(i,j)  = 0.
        uCf(i,j)   = 0.
        vCf(i,j)   = 0.
        mT(i,j)   = 0.
        pF(i,j)   = 0.
        del2u(i,j) = 0.
        del2v(i,j) = 0.
        dStar(i,j) = 0.
        zStar(i,j) = 0.
        uDiss(i,j) = 0.
        vDiss(i,j) = 0.
        vort3(i,j) = 0.
        omega3(i,j) = 0.
        ke(i,j) = 0.
#ifdef ALLOW_AUTODIFF_TAMC
        strain(i,j)  = 0. _d 0
        tension(i,j) = 0. _d 0
#endif
       ENDDO
      ENDDO

C--   Term by term tracer parmeters
C     o U momentum equation
      uDudxFac     = afFacMom*1.
      AhDudxFac    = vfFacMom*1.
      A4DuxxdxFac  = vfFacMom*1.
      vDudyFac     = afFacMom*1.
      AhDudyFac    = vfFacMom*1.
      A4DuyydyFac  = vfFacMom*1.
      rVelDudrFac  = afFacMom*1.
      ArDudrFac    = vfFacMom*1.
      mTFacU       = mtFacMom*1.
      fuFac        = cfFacMom*1.
      phxFac       = pfFacMom*1.
C     o V momentum equation
      uDvdxFac     = afFacMom*1.
      AhDvdxFac    = vfFacMom*1.
      A4DvxxdxFac  = vfFacMom*1.
      vDvdyFac     = afFacMom*1.
      AhDvdyFac    = vfFacMom*1.
      A4DvyydyFac  = vfFacMom*1.
      rVelDvdrFac  = afFacMom*1.
      ArDvdrFac    = vfFacMom*1.
      mTFacV       = mtFacMom*1.
      fvFac        = cfFacMom*1.
      phyFac       = pfFacMom*1.
      vForcFac     = foFacMom*1.

      IF (     no_slip_bottom
     &    .OR. bottomDragQuadratic.NE.0.
     &    .OR. bottomDragLinear.NE.0.) THEN
       bottomDragTerms=.TRUE.
      ELSE
       bottomDragTerms=.FALSE.
      ENDIF

C-- with stagger time stepping, grad Phi_Hyp is directly incoporated in TIMESTEP
      IF (staggerTimeStep) THEN
        phxFac = 0.
        phyFac = 0.
      ENDIF

C--   Calculate open water fraction at vorticity points
      CALL MOM_CALC_HFACZ(bi,bj,k,hFacZ,r_hFacZ,myThid)

C---- Calculate common quantities used in both U and V equations
C     Calculate tracer cell face open areas
      DO j=1-OLy,sNy+OLy
       DO i=1-OLx,sNx+OLx
        xA(i,j) = _dyG(i,j,bi,bj)
     &   *drF(k)*_hFacW(i,j,k,bi,bj)
        yA(i,j) = _dxG(i,j,bi,bj)
     &   *drF(k)*_hFacS(i,j,k,bi,bj)
       ENDDO
      ENDDO

C     Make local copies of horizontal flow field
      DO j=1-OLy,sNy+OLy
       DO i=1-OLx,sNx+OLx
        uFld(i,j) = uVel(i,j,k,bi,bj)
        vFld(i,j) = vVel(i,j,k,bi,bj)
       ENDDO
      ENDDO

C note (jmc) : Dissipation and Vort3 advection do not necesary
C              use the same maskZ (and hFacZ)  => needs 2 call(s)
c     CALL MOM_VI_HFACZ_DISS(bi,bj,k,hFacZ,r_hFacZ,myThid)

      CALL MOM_CALC_KE(bi,bj,k,2,uFld,vFld,KE,myThid)

      CALL MOM_VI_CALC_HDIV(bi,bj,k,uFld,vFld,hDiv,myThid)

      CALL MOM_VI_CALC_RELVORT3(bi,bj,k,uFld,vFld,hFacZ,vort3,myThid)

c     CALL MOM_VI_CALC_ABSVORT3(bi,bj,k,vort3,omega3,myThid)

      IF (momViscosity) THEN
C      Calculate del^2 u and del^2 v for bi-harmonic term
       IF (viscA4.NE.0. .OR. viscA4Grid.NE.0.) THEN
         CALL MOM_VI_DEL2UV(bi,bj,k,hDiv,vort3,hFacZ,
     O                      del2u,del2v,
     &                      myThid)
         CALL MOM_VI_CALC_HDIV(bi,bj,k,del2u,del2v,dStar,myThid)
         CALL MOM_VI_CALC_RELVORT3(
     &                         bi,bj,k,del2u,del2v,hFacZ,zStar,myThid)
       ENDIF
C      Calculate dissipation terms for U and V equations
C      in terms of vorticity and divergence
       IF (viscAh.NE.0. .OR. viscA4.NE.0. .OR.
     &      viscAhGrid.NE.0. .OR. viscA4Grid.NE.0. ) THEN
         CALL MOM_VI_HDISSIP(bi,bj,k,hDiv,vort3,hFacZ,dStar,zStar,
     O                       uDiss,vDiss,
     &                       myThid)
       ENDIF
C      or in terms of tension and strain
       IF (viscAstrain.NE.0. .OR. viscAtension.NE.0.) THEN
         CALL MOM_CALC_TENSION(bi,bj,k,uFld,vFld,
     O                         tension,
     I                         myThid)
         CALL MOM_CALC_STRAIN(bi,bj,k,uFld,vFld,hFacZ,
     O                        strain,
     I                        myThid)
         CALL MOM_HDISSIP(bi,bj,k,
     I                    tension,strain,hFacZ,viscAtension,viscAstrain,
     O                    uDiss,vDiss,
     I                    myThid)
       ENDIF
      ENDIF

C-    Return to standard hfacZ (min-4) and mask vort3 accordingly:
c     CALL MOM_VI_MASK_VORT3(bi,bj,k,hFacZ,r_hFacZ,vort3,myThid)

C---- Zonal momentum equation starts here

C--   Vertical flux (fVer is at upper face of "u" cell)

C     Eddy component of vertical flux (interior component only) -> vrF
      IF (momViscosity.AND..NOT.implicitViscosity)
     & CALL MOM_U_RVISCFLUX(bi,bj,k,uVel,KappaRU,vrF,myThid)

C     Combine fluxes
      DO j=jMin,jMax
       DO i=iMin,iMax
        fVerU(i,j,kDown) = ArDudrFac*vrF(i,j)
       ENDDO
      ENDDO

C--   Tendency is minus divergence of the fluxes + coriolis + pressure term
      DO j=2-Oly,sNy+Oly-1
       DO i=2-Olx,sNx+Olx-1
        gU(i,j,k,bi,bj) = uDiss(i,j)
     &   -_recip_hFacW(i,j,k,bi,bj)*recip_drF(k)
     &   *recip_rAw(i,j,bi,bj)
     &  *(
     &   +fVerU(i,j,kUp)*rkFac - fVerU(i,j,kDown)*rkFac
     &   )
     &  - phxFac*dPhiHydX(i,j)
       ENDDO
      ENDDO

C-- No-slip and drag BCs appear as body forces in cell abutting topography 
      IF (momViscosity.AND.no_slip_sides) THEN
C-     No-slip BCs impose a drag at walls...
       CALL MOM_U_SIDEDRAG(bi,bj,k,uFld,del2u,hFacZ,vF,myThid)
       DO j=jMin,jMax
        DO i=iMin,iMax
         gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+vF(i,j)
        ENDDO
       ENDDO
      ENDIF

C-    No-slip BCs impose a drag at bottom
      IF (momViscosity.AND.bottomDragTerms) THEN
       CALL MOM_U_BOTTOMDRAG(bi,bj,k,uFld,KE,KappaRU,vF,myThid)
       DO j=jMin,jMax
        DO i=iMin,iMax
         gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+vF(i,j)
        ENDDO
       ENDDO
      ENDIF

C--   Metric terms for curvilinear grid systems
c     IF (usingSphericalPolarMTerms) THEN
C      o Spherical polar grid metric terms
c      CALL MOM_U_METRIC_NH(bi,bj,k,uFld,wVel,mT,myThid)
c      DO j=jMin,jMax
c       DO i=iMin,iMax
c        gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+mTFacU*mT(i,j)
c       ENDDO
c      ENDDO
c     ENDIF

C---- Meridional momentum equation starts here

C--   Vertical flux (fVer is at upper face of "v" cell)

C     Eddy component of vertical flux (interior component only) -> vrF
      IF (momViscosity.AND..NOT.implicitViscosity)
     & CALL MOM_V_RVISCFLUX(bi,bj,k,vVel,KappaRV,vrf,myThid)

C     Combine fluxes -> fVerV
      DO j=jMin,jMax
       DO i=iMin,iMax
        fVerV(i,j,kDown) = ArDvdrFac*vrF(i,j)
       ENDDO
      ENDDO

C--   Tendency is minus divergence of the fluxes + coriolis + pressure term
      DO j=jMin,jMax
       DO i=iMin,iMax
        gV(i,j,k,bi,bj) = vDiss(i,j)
     &   -_recip_hFacS(i,j,k,bi,bj)*recip_drF(k)
     &    *recip_rAs(i,j,bi,bj)
     &  *(
     &   +fVerV(i,j,kUp)*rkFac - fVerV(i,j,kDown)*rkFac
     &   )
     &  - phyFac*dPhiHydY(i,j)
       ENDDO
      ENDDO

C-- No-slip and drag BCs appear as body forces in cell abutting topography 
      IF (momViscosity.AND.no_slip_sides) THEN
C-     No-slip BCs impose a drag at walls...
       CALL MOM_V_SIDEDRAG(bi,bj,k,vFld,del2v,hFacZ,vF,myThid)
       DO j=jMin,jMax
        DO i=iMin,iMax
         gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vF(i,j)
        ENDDO
       ENDDO
      ENDIF
C-    No-slip BCs impose a drag at bottom
      IF (momViscosity.AND.bottomDragTerms) THEN
       CALL MOM_V_BOTTOMDRAG(bi,bj,k,vFld,KE,KappaRV,vF,myThid)
       DO j=jMin,jMax
        DO i=iMin,iMax
         gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vF(i,j)
        ENDDO
       ENDDO
      ENDIF

C--   Metric terms for curvilinear grid systems
c     IF (usingSphericalPolarMTerms) THEN
C      o Spherical polar grid metric terms
c      CALL MOM_V_METRIC_NH(bi,bj,k,vFld,wVel,mT,myThid)
c      DO j=jMin,jMax
c       DO i=iMin,iMax
c        gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+mTFacV*mT(i,j)
c       ENDDO
c      ENDDO
c     ENDIF

C--   Horizontal Coriolis terms
      IF (useCoriolis .AND. .NOT.useCDscheme) THEN
       CALL MOM_VI_CORIOLIS(bi,bj,k,uFld,vFld,omega3,hFacZ,r_hFacZ,
     &                      uCf,vCf,myThid)
       DO j=jMin,jMax
        DO i=iMin,iMax
         gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+uCf(i,j)
         gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vCf(i,j)
        ENDDO
       ENDDO
       IF ( writeDiag ) THEN
        CALL WRITE_LOCAL_RL('fV','I10',1,uCf,bi,bj,k,myIter,myThid)
        CALL WRITE_LOCAL_RL('fU','I10',1,vCf,bi,bj,k,myIter,myThid)
       ENDIF
      ENDIF

      IF (momAdvection) THEN
C--   Horizontal advection of relative vorticity
c      CALL MOM_VI_U_CORIOLIS(bi,bj,K,vFld,omega3,r_hFacZ,uCf,myThid)
       CALL MOM_VI_U_CORIOLIS(bi,bj,k,vFld,vort3,hFacZ,r_hFacZ,
     &                        uCf,myThid)
c      CALL MOM_VI_U_CORIOLIS_C4(bi,bj,K,vFld,vort3,r_hFacZ,uCf,myThid)
       DO j=jMin,jMax
        DO i=iMin,iMax
         gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+uCf(i,j)
        ENDDO
       ENDDO
c      CALL MOM_VI_V_CORIOLIS(bi,bj,K,uFld,omega3,r_hFacZ,vCf,myThid)
       CALL MOM_VI_V_CORIOLIS(bi,bj,k,uFld,vort3,hFacZ,r_hFacZ,
     &                        vCf,myThid)
c      CALL MOM_VI_V_CORIOLIS_C4(bi,bj,K,uFld,vort3,r_hFacZ,vCf,myThid)
       DO j=jMin,jMax
        DO i=iMin,iMax
         gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vCf(i,j)
        ENDDO
       ENDDO

       IF ( writeDiag ) THEN
        CALL WRITE_LOCAL_RL('zV','I10',1,uCf,bi,bj,k,myIter,myThid)
        CALL WRITE_LOCAL_RL('zU','I10',1,vCf,bi,bj,k,myIter,myThid)
       ENDIF
#ifdef ALLOW_TIMEAVE
#ifndef HRCUBE
       IF (taveFreq.GT.0.) THEN
         CALL TIMEAVE_CUMUL_1K1T(uZetatave,vCf,deltaTClock,
     &                           Nr, k, bi, bj, myThid)
         CALL TIMEAVE_CUMUL_1K1T(vZetatave,uCf,deltaTClock,
     &                           Nr, k, bi, bj, myThid)
       ENDIF
#endif /* ALLOW_TIMEAVE */
#endif /* ndef HRCUBE */

C--   Vertical shear terms (-w*du/dr & -w*dv/dr)
       IF ( .NOT. momImplVertAdv ) THEN
        CALL MOM_VI_U_VERTSHEAR(bi,bj,K,uVel,wVel,uCf,myThid)
        DO j=jMin,jMax
         DO i=iMin,iMax
          gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+uCf(i,j)
         ENDDO
        ENDDO
        CALL MOM_VI_V_VERTSHEAR(bi,bj,K,vVel,wVel,vCf,myThid)
        DO j=jMin,jMax
         DO i=iMin,iMax
          gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vCf(i,j)
         ENDDO
        ENDDO
       ENDIF

C--   Bernoulli term
       CALL MOM_VI_U_GRAD_KE(bi,bj,K,KE,uCf,myThid)
       DO j=jMin,jMax
        DO i=iMin,iMax
         gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+uCf(i,j)
        ENDDO
       ENDDO
       CALL MOM_VI_V_GRAD_KE(bi,bj,K,KE,vCf,myThid)
       DO j=jMin,jMax
        DO i=iMin,iMax
         gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vCf(i,j)
        ENDDO
       ENDDO
       IF ( writeDiag ) THEN
        CALL WRITE_LOCAL_RL('KEx','I10',1,uCf,bi,bj,k,myIter,myThid)
        CALL WRITE_LOCAL_RL('KEy','I10',1,vCf,bi,bj,k,myIter,myThid)
       ENDIF

C--   end if momAdvection
      ENDIF

C--   Set du/dt & dv/dt on boundaries to zero
      DO j=jMin,jMax
       DO i=iMin,iMax
        gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)*_maskW(i,j,k,bi,bj)
        gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)*_maskS(i,j,k,bi,bj)
       ENDDO
      ENDDO


      IF ( writeDiag ) THEN
       CALL WRITE_LOCAL_RL('Ds','I10',1,strain,bi,bj,k,myIter,myThid)
       CALL WRITE_LOCAL_RL('Dt','I10',1,tension,bi,bj,k,myIter,myThid)
       CALL WRITE_LOCAL_RL('Du','I10',1,uDiss,bi,bj,k,myIter,myThid)
       CALL WRITE_LOCAL_RL('Dv','I10',1,vDiss,bi,bj,k,myIter,myThid)
       CALL WRITE_LOCAL_RL('Z3','I10',1,vort3,bi,bj,k,myIter,myThid)
c      CALL WRITE_LOCAL_RL('W3','I10',1,omega3,bi,bj,k,myIter,myThid)
       CALL WRITE_LOCAL_RL('KE','I10',1,KE,bi,bj,k,myIter,myThid)
       CALL WRITE_LOCAL_RL('D','I10',1,hdiv,bi,bj,k,myIter,myThid)
      ENDIF

#endif /* ALLOW_MOM_VECINV */

      RETURN
      END
1	adcroft	1.16	C $Header: /u/gcmpack/MITgcm/pkg/mom_vecinv/mom_vecinv.F,v 1.15 2004/02/25 00:56:47 jmc Exp $
2	adcroft	1.2	C $Name: $
3	adcroft	1.1
4	edhill	1.10	#include "PACKAGES_CONFIG.h"
5	adcroft	1.1	#include "CPP_OPTIONS.h"
6
7			SUBROUTINE MOM_VECINV(
8			I bi,bj,iMin,iMax,jMin,jMax,k,kUp,kDown,
9	jmc	1.4	I dPhiHydX,dPhiHydY,KappaRU,KappaRV,
10	adcroft	1.1	U fVerU, fVerV,
11	jmc	1.15	I myTime, myIter, myThid)
12	adcroft	1.1	C /==========================================================\
13			C \| S/R MOM_VECINV \|
14			C \| o Form the right hand-side of the momentum equation. \|
15			C \|==========================================================\|
16			C \| Terms are evaluated one layer at a time working from \|
17			C \| the bottom to the top. The vertically integrated \|
18			C \| barotropic flow tendency term is evluated by summing the \|
19			C \| tendencies. \|
20			C \| Notes: \|
21			C \| We have not sorted out an entirely satisfactory formula \|
22			C \| for the diffusion equation bc with lopping. The present \|
23			C \| form produces a diffusive flux that does not scale with \|
24			C \| open-area. Need to do something to solidfy this and to \|
25			C \| deal "properly" with thin walls. \|
26			C \==========================================================/
27			IMPLICIT NONE
28
29			C == Global variables ==
30			#include "SIZE.h"
31			#include "DYNVARS.h"
32			#include "EEPARAMS.h"
33			#include "PARAMS.h"
34			#include "GRID.h"
35	jmc	1.7	#ifdef ALLOW_TIMEAVE
36			#include "TIMEAVE_STATV.h"
37			#endif
38	adcroft	1.1
39			C == Routine arguments ==
40			C fVerU - Flux of momentum in the vertical
41			C fVerV direction out of the upper face of a cell K
42			C ( flux into the cell above ).
43	jmc	1.4	C dPhiHydX,Y :: Gradient (X & Y dir.) of Hydrostatic Potential
44	adcroft	1.1	C bi, bj, iMin, iMax, jMin, jMax - Range of points for which calculation
45			C results will be set.
46			C kUp, kDown - Index for upper and lower layers.
47			C myThid - Instance number for this innvocation of CALC_MOM_RHS
48	jmc	1.4	_RL dPhiHydX(1-Olx:sNx+Olx,1-Oly:sNy+Oly)
49			_RL dPhiHydY(1-Olx:sNx+Olx,1-Oly:sNy+Oly)
50	adcroft	1.1	_RL KappaRU(1-OLx:sNx+OLx,1-OLy:sNy+OLy,Nr)
51			_RL KappaRV(1-OLx:sNx+OLx,1-OLy:sNy+OLy,Nr)
52			_RL fVerU(1-OLx:sNx+OLx,1-OLy:sNy+OLy,2)
53			_RL fVerV(1-OLx:sNx+OLx,1-OLy:sNy+OLy,2)
54			INTEGER kUp,kDown
55	jmc	1.15	_RL myTime
56	adcroft	1.2	INTEGER myIter
57	adcroft	1.1	INTEGER myThid
58			INTEGER bi,bj,iMin,iMax,jMin,jMax
59
60	edhill	1.11	#ifdef ALLOW_MOM_VECINV
61	jmc	1.7
62	adcroft	1.2	C == Functions ==
63			LOGICAL DIFFERENT_MULTIPLE
64			EXTERNAL DIFFERENT_MULTIPLE
65
66	adcroft	1.1	C == Local variables ==
67			_RL aF (1-OLx:sNx+OLx,1-OLy:sNy+OLy)
68			_RL vF (1-OLx:sNx+OLx,1-OLy:sNy+OLy)
69			_RL vrF (1-OLx:sNx+OLx,1-OLy:sNy+OLy)
70			_RL uCf (1-OLx:sNx+OLx,1-OLy:sNy+OLy)
71			_RL vCf (1-OLx:sNx+OLx,1-OLy:sNy+OLy)
72			_RL mT (1-OLx:sNx+OLx,1-OLy:sNy+OLy)
73			_RL pF (1-OLx:sNx+OLx,1-OLy:sNy+OLy)
74			_RL del2u(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
75			_RL del2v(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
76	adcroft	1.3	_RL tension(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
77			_RL strain(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
78	adcroft	1.1	_RS hFacZ(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
79			_RS r_hFacZ(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
80			_RS xA(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
81			_RS yA(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
82			_RL uFld(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
83			_RL vFld(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
84			_RL dStar(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
85			_RL zStar(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
86			_RL uDiss(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
87			_RL vDiss(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
88			C I,J,K - Loop counters
89			INTEGER i,j,k
90			C rVelMaskOverride - Factor for imposing special surface boundary conditions
91			C ( set according to free-surface condition ).
92			C hFacROpen - Lopped cell factos used tohold fraction of open
93			C hFacRClosed and closed cell wall.
94			_RL rVelMaskOverride
95			C xxxFac - On-off tracer parameters used for switching terms off.
96			_RL uDudxFac
97			_RL AhDudxFac
98			_RL A4DuxxdxFac
99			_RL vDudyFac
100			_RL AhDudyFac
101			_RL A4DuyydyFac
102			_RL rVelDudrFac
103			_RL ArDudrFac
104			_RL fuFac
105			_RL phxFac
106			_RL mtFacU
107			_RL uDvdxFac
108			_RL AhDvdxFac
109			_RL A4DvxxdxFac
110			_RL vDvdyFac
111			_RL AhDvdyFac
112			_RL A4DvyydyFac
113			_RL rVelDvdrFac
114			_RL ArDvdrFac
115			_RL fvFac
116			_RL phyFac
117			_RL vForcFac
118			_RL mtFacV
119			_RL wVelBottomOverride
120			LOGICAL bottomDragTerms
121	jmc	1.15	LOGICAL writeDiag
122	adcroft	1.1	_RL KE(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
123			_RL omega3(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
124			_RL vort3(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
125			_RL hDiv(1-OLx:sNx+OLx,1-OLy:sNy+OLy)
126
127	heimbach	1.9	#ifdef ALLOW_AUTODIFF_TAMC
128			C-- only the kDown part of fverU/V is set in this subroutine
129			C-- the kUp is still required
130			C-- In the case of mom_fluxform Kup is set as well
131			C-- (at least in part)
132			fVerU(1,1,kUp) = fVerU(1,1,kUp)
133			fVerV(1,1,kUp) = fVerV(1,1,kUp)
134			#endif
135
136	adcroft	1.1	rVelMaskOverride=1.
137			IF ( k .EQ. 1 ) rVelMaskOverride=freeSurfFac
138			wVelBottomOverride=1.
139			IF (k.EQ.Nr) wVelBottomOverride=0.
140	jmc	1.15	writeDiag = DIFFERENT_MULTIPLE(diagFreq, myTime,
141			& myTime-deltaTClock)
142	adcroft	1.1
143			C Initialise intermediate terms
144			DO J=1-OLy,sNy+OLy
145			DO I=1-OLx,sNx+OLx
146			aF(i,j) = 0.
147			vF(i,j) = 0.
148			vrF(i,j) = 0.
149			uCf(i,j) = 0.
150			vCf(i,j) = 0.
151			mT(i,j) = 0.
152			pF(i,j) = 0.
153			del2u(i,j) = 0.
154			del2v(i,j) = 0.
155			dStar(i,j) = 0.
156			zStar(i,j) = 0.
157			uDiss(i,j) = 0.
158			vDiss(i,j) = 0.
159			vort3(i,j) = 0.
160			omega3(i,j) = 0.
161			ke(i,j) = 0.
162	heimbach	1.8	#ifdef ALLOW_AUTODIFF_TAMC
163			strain(i,j) = 0. _d 0
164			tension(i,j) = 0. _d 0
165			#endif
166	adcroft	1.1	ENDDO
167			ENDDO
168
169			C-- Term by term tracer parmeters
170			C o U momentum equation
171			uDudxFac = afFacMom*1.
172			AhDudxFac = vfFacMom*1.
173			A4DuxxdxFac = vfFacMom*1.
174			vDudyFac = afFacMom*1.
175			AhDudyFac = vfFacMom*1.
176			A4DuyydyFac = vfFacMom*1.
177			rVelDudrFac = afFacMom*1.
178			ArDudrFac = vfFacMom*1.
179			mTFacU = mtFacMom*1.
180			fuFac = cfFacMom*1.
181			phxFac = pfFacMom*1.
182			C o V momentum equation
183			uDvdxFac = afFacMom*1.
184			AhDvdxFac = vfFacMom*1.
185			A4DvxxdxFac = vfFacMom*1.
186			vDvdyFac = afFacMom*1.
187			AhDvdyFac = vfFacMom*1.
188			A4DvyydyFac = vfFacMom*1.
189			rVelDvdrFac = afFacMom*1.
190			ArDvdrFac = vfFacMom*1.
191			mTFacV = mtFacMom*1.
192			fvFac = cfFacMom*1.
193			phyFac = pfFacMom*1.
194			vForcFac = foFacMom*1.
195
196			IF ( no_slip_bottom
197			& .OR. bottomDragQuadratic.NE.0.
198			& .OR. bottomDragLinear.NE.0.) THEN
199			bottomDragTerms=.TRUE.
200			ELSE
201			bottomDragTerms=.FALSE.
202			ENDIF
203
204			C-- with stagger time stepping, grad Phi_Hyp is directly incoporated in TIMESTEP
205			IF (staggerTimeStep) THEN
206			phxFac = 0.
207			phyFac = 0.
208			ENDIF
209
210			C-- Calculate open water fraction at vorticity points
211			CALL MOM_CALC_HFACZ(bi,bj,k,hFacZ,r_hFacZ,myThid)
212
213			C---- Calculate common quantities used in both U and V equations
214			C Calculate tracer cell face open areas
215			DO j=1-OLy,sNy+OLy
216			DO i=1-OLx,sNx+OLx
217			xA(i,j) = _dyG(i,j,bi,bj)
218			& drF(k)_hFacW(i,j,k,bi,bj)
219			yA(i,j) = _dxG(i,j,bi,bj)
220			& drF(k)_hFacS(i,j,k,bi,bj)
221			ENDDO
222			ENDDO
223
224			C Make local copies of horizontal flow field
225			DO j=1-OLy,sNy+OLy
226			DO i=1-OLx,sNx+OLx
227			uFld(i,j) = uVel(i,j,k,bi,bj)
228			vFld(i,j) = vVel(i,j,k,bi,bj)
229			ENDDO
230			ENDDO
231
232	jmc	1.7	C note (jmc) : Dissipation and Vort3 advection do not necesary
233			C use the same maskZ (and hFacZ) => needs 2 call(s)
234			c CALL MOM_VI_HFACZ_DISS(bi,bj,k,hFacZ,r_hFacZ,myThid)
235
236	adcroft	1.16	CALL MOM_CALC_KE(bi,bj,k,2,uFld,vFld,KE,myThid)
237	adcroft	1.1
238			CALL MOM_VI_CALC_HDIV(bi,bj,k,uFld,vFld,hDiv,myThid)
239
240			CALL MOM_VI_CALC_RELVORT3(bi,bj,k,uFld,vFld,hFacZ,vort3,myThid)
241
242	jmc	1.5	c CALL MOM_VI_CALC_ABSVORT3(bi,bj,k,vort3,omega3,myThid)
243	adcroft	1.1
244			IF (momViscosity) THEN
245			C Calculate del^2 u and del^2 v for bi-harmonic term
246	dimitri	1.14	IF (viscA4.NE.0. .OR. viscA4Grid.NE.0.) THEN
247	adcroft	1.2	CALL MOM_VI_DEL2UV(bi,bj,k,hDiv,vort3,hFacZ,
248			O del2u,del2v,
249			& myThid)
250			CALL MOM_VI_CALC_HDIV(bi,bj,k,del2u,del2v,dStar,myThid)
251			CALL MOM_VI_CALC_RELVORT3(
252			& bi,bj,k,del2u,del2v,hFacZ,zStar,myThid)
253			ENDIF
254	adcroft	1.1	C Calculate dissipation terms for U and V equations
255	adcroft	1.2	C in terms of vorticity and divergence
256	dimitri	1.14	IF (viscAh.NE.0. .OR. viscA4.NE.0. .OR.
257			& viscAhGrid.NE.0. .OR. viscA4Grid.NE.0. ) THEN
258	adcroft	1.2	CALL MOM_VI_HDISSIP(bi,bj,k,hDiv,vort3,hFacZ,dStar,zStar,
259			O uDiss,vDiss,
260			& myThid)
261			ENDIF
262	adcroft	1.3	C or in terms of tension and strain
263			IF (viscAstrain.NE.0. .OR. viscAtension.NE.0.) THEN
264			CALL MOM_CALC_TENSION(bi,bj,k,uFld,vFld,
265			O tension,
266			I myThid)
267			CALL MOM_CALC_STRAIN(bi,bj,k,uFld,vFld,hFacZ,
268			O strain,
269			I myThid)
270			CALL MOM_HDISSIP(bi,bj,k,
271			I tension,strain,hFacZ,viscAtension,viscAstrain,
272			O uDiss,vDiss,
273			I myThid)
274			ENDIF
275	adcroft	1.1	ENDIF
276
277	jmc	1.7	C- Return to standard hfacZ (min-4) and mask vort3 accordingly:
278			c CALL MOM_VI_MASK_VORT3(bi,bj,k,hFacZ,r_hFacZ,vort3,myThid)
279
280	adcroft	1.1	C---- Zonal momentum equation starts here
281
282			C-- Vertical flux (fVer is at upper face of "u" cell)
283
284			C Eddy component of vertical flux (interior component only) -> vrF
285			IF (momViscosity.AND..NOT.implicitViscosity)
286			& CALL MOM_U_RVISCFLUX(bi,bj,k,uVel,KappaRU,vrF,myThid)
287
288			C Combine fluxes
289			DO j=jMin,jMax
290			DO i=iMin,iMax
291			fVerU(i,j,kDown) = ArDudrFac*vrF(i,j)
292			ENDDO
293			ENDDO
294
295			C-- Tendency is minus divergence of the fluxes + coriolis + pressure term
296			DO j=2-Oly,sNy+Oly-1
297			DO i=2-Olx,sNx+Olx-1
298			gU(i,j,k,bi,bj) = uDiss(i,j)
299			& -_recip_hFacW(i,j,k,bi,bj)*recip_drF(k)
300			& *recip_rAw(i,j,bi,bj)
301			& *(
302			& +fVerU(i,j,kUp)rkFac - fVerU(i,j,kDown)rkFac
303			& )
304	jmc	1.4	& - phxFac*dPhiHydX(i,j)
305	adcroft	1.1	ENDDO
306			ENDDO
307
308			C-- No-slip and drag BCs appear as body forces in cell abutting topography
309			IF (momViscosity.AND.no_slip_sides) THEN
310			C- No-slip BCs impose a drag at walls...
311			CALL MOM_U_SIDEDRAG(bi,bj,k,uFld,del2u,hFacZ,vF,myThid)
312			DO j=jMin,jMax
313			DO i=iMin,iMax
314			gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+vF(i,j)
315			ENDDO
316			ENDDO
317			ENDIF
318	heimbach	1.8
319	adcroft	1.1	C- No-slip BCs impose a drag at bottom
320			IF (momViscosity.AND.bottomDragTerms) THEN
321			CALL MOM_U_BOTTOMDRAG(bi,bj,k,uFld,KE,KappaRU,vF,myThid)
322			DO j=jMin,jMax
323			DO i=iMin,iMax
324			gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+vF(i,j)
325			ENDDO
326			ENDDO
327			ENDIF
328
329			C-- Metric terms for curvilinear grid systems
330			c IF (usingSphericalPolarMTerms) THEN
331			C o Spherical polar grid metric terms
332			c CALL MOM_U_METRIC_NH(bi,bj,k,uFld,wVel,mT,myThid)
333			c DO j=jMin,jMax
334			c DO i=iMin,iMax
335			c gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+mTFacU*mT(i,j)
336			c ENDDO
337			c ENDDO
338			c ENDIF
339
340			C---- Meridional momentum equation starts here
341
342			C-- Vertical flux (fVer is at upper face of "v" cell)
343
344			C Eddy component of vertical flux (interior component only) -> vrF
345			IF (momViscosity.AND..NOT.implicitViscosity)
346			& CALL MOM_V_RVISCFLUX(bi,bj,k,vVel,KappaRV,vrf,myThid)
347
348			C Combine fluxes -> fVerV
349			DO j=jMin,jMax
350			DO i=iMin,iMax
351			fVerV(i,j,kDown) = ArDvdrFac*vrF(i,j)
352			ENDDO
353			ENDDO
354
355			C-- Tendency is minus divergence of the fluxes + coriolis + pressure term
356			DO j=jMin,jMax
357			DO i=iMin,iMax
358			gV(i,j,k,bi,bj) = vDiss(i,j)
359			& -_recip_hFacS(i,j,k,bi,bj)*recip_drF(k)
360			& *recip_rAs(i,j,bi,bj)
361			& *(
362			& +fVerV(i,j,kUp)rkFac - fVerV(i,j,kDown)rkFac
363			& )
364	jmc	1.4	& - phyFac*dPhiHydY(i,j)
365	adcroft	1.1	ENDDO
366			ENDDO
367
368			C-- No-slip and drag BCs appear as body forces in cell abutting topography
369			IF (momViscosity.AND.no_slip_sides) THEN
370			C- No-slip BCs impose a drag at walls...
371			CALL MOM_V_SIDEDRAG(bi,bj,k,vFld,del2v,hFacZ,vF,myThid)
372			DO j=jMin,jMax
373			DO i=iMin,iMax
374			gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vF(i,j)
375			ENDDO
376			ENDDO
377			ENDIF
378			C- No-slip BCs impose a drag at bottom
379			IF (momViscosity.AND.bottomDragTerms) THEN
380			CALL MOM_V_BOTTOMDRAG(bi,bj,k,vFld,KE,KappaRV,vF,myThid)
381			DO j=jMin,jMax
382			DO i=iMin,iMax
383			gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vF(i,j)
384			ENDDO
385			ENDDO
386			ENDIF
387
388			C-- Metric terms for curvilinear grid systems
389			c IF (usingSphericalPolarMTerms) THEN
390			C o Spherical polar grid metric terms
391			c CALL MOM_V_METRIC_NH(bi,bj,k,vFld,wVel,mT,myThid)
392			c DO j=jMin,jMax
393			c DO i=iMin,iMax
394			c gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+mTFacV*mT(i,j)
395			c ENDDO
396			c ENDDO
397			c ENDIF
398
399	jmc	1.5	C-- Horizontal Coriolis terms
400	jmc	1.6	IF (useCoriolis .AND. .NOT.useCDscheme) THEN
401	jmc	1.7	CALL MOM_VI_CORIOLIS(bi,bj,k,uFld,vFld,omega3,hFacZ,r_hFacZ,
402	jmc	1.5	& uCf,vCf,myThid)
403			DO j=jMin,jMax
404			DO i=iMin,iMax
405			gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+uCf(i,j)
406			gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vCf(i,j)
407			ENDDO
408	adcroft	1.1	ENDDO
409	jmc	1.15	IF ( writeDiag ) THEN
410			CALL WRITE_LOCAL_RL('fV','I10',1,uCf,bi,bj,k,myIter,myThid)
411			CALL WRITE_LOCAL_RL('fU','I10',1,vCf,bi,bj,k,myIter,myThid)
412			ENDIF
413	jmc	1.5	ENDIF
414	adcroft	1.1
415	jmc	1.5	IF (momAdvection) THEN
416			C-- Horizontal advection of relative vorticity
417			c CALL MOM_VI_U_CORIOLIS(bi,bj,K,vFld,omega3,r_hFacZ,uCf,myThid)
418	jmc	1.7	CALL MOM_VI_U_CORIOLIS(bi,bj,k,vFld,vort3,hFacZ,r_hFacZ,
419			& uCf,myThid)
420	jmc	1.5	c CALL MOM_VI_U_CORIOLIS_C4(bi,bj,K,vFld,vort3,r_hFacZ,uCf,myThid)
421			DO j=jMin,jMax
422			DO i=iMin,iMax
423			gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+uCf(i,j)
424			ENDDO
425	adcroft	1.1	ENDDO
426	jmc	1.5	c CALL MOM_VI_V_CORIOLIS(bi,bj,K,uFld,omega3,r_hFacZ,vCf,myThid)
427	jmc	1.7	CALL MOM_VI_V_CORIOLIS(bi,bj,k,uFld,vort3,hFacZ,r_hFacZ,
428			& vCf,myThid)
429	jmc	1.5	c CALL MOM_VI_V_CORIOLIS_C4(bi,bj,K,uFld,vort3,r_hFacZ,vCf,myThid)
430			DO j=jMin,jMax
431			DO i=iMin,iMax
432			gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vCf(i,j)
433			ENDDO
434	adcroft	1.1	ENDDO
435
436	jmc	1.15	IF ( writeDiag ) THEN
437			CALL WRITE_LOCAL_RL('zV','I10',1,uCf,bi,bj,k,myIter,myThid)
438			CALL WRITE_LOCAL_RL('zU','I10',1,vCf,bi,bj,k,myIter,myThid)
439			ENDIF
440	jmc	1.7	#ifdef ALLOW_TIMEAVE
441	dimitri	1.13	#ifndef HRCUBE
442	jmc	1.7	IF (taveFreq.GT.0.) THEN
443			CALL TIMEAVE_CUMUL_1K1T(uZetatave,vCf,deltaTClock,
444			& Nr, k, bi, bj, myThid)
445			CALL TIMEAVE_CUMUL_1K1T(vZetatave,uCf,deltaTClock,
446			& Nr, k, bi, bj, myThid)
447			ENDIF
448	dimitri	1.13	#endif /* ALLOW_TIMEAVE */
449			#endif /* ndef HRCUBE */
450	jmc	1.7
451	jmc	1.5	C-- Vertical shear terms (-wdu/dr & -wdv/dr)
452	jmc	1.12	IF ( .NOT. momImplVertAdv ) THEN
453			CALL MOM_VI_U_VERTSHEAR(bi,bj,K,uVel,wVel,uCf,myThid)
454			DO j=jMin,jMax
455			DO i=iMin,iMax
456			gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+uCf(i,j)
457			ENDDO
458	jmc	1.5	ENDDO
459	jmc	1.12	CALL MOM_VI_V_VERTSHEAR(bi,bj,K,vVel,wVel,vCf,myThid)
460			DO j=jMin,jMax
461			DO i=iMin,iMax
462			gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vCf(i,j)
463			ENDDO
464	jmc	1.5	ENDDO
465	jmc	1.12	ENDIF
466	adcroft	1.1
467			C-- Bernoulli term
468	jmc	1.5	CALL MOM_VI_U_GRAD_KE(bi,bj,K,KE,uCf,myThid)
469			DO j=jMin,jMax
470			DO i=iMin,iMax
471			gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+uCf(i,j)
472			ENDDO
473			ENDDO
474			CALL MOM_VI_V_GRAD_KE(bi,bj,K,KE,vCf,myThid)
475			DO j=jMin,jMax
476			DO i=iMin,iMax
477			gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vCf(i,j)
478			ENDDO
479	adcroft	1.1	ENDDO
480	jmc	1.15	IF ( writeDiag ) THEN
481			CALL WRITE_LOCAL_RL('KEx','I10',1,uCf,bi,bj,k,myIter,myThid)
482			CALL WRITE_LOCAL_RL('KEy','I10',1,vCf,bi,bj,k,myIter,myThid)
483			ENDIF
484
485	jmc	1.5	C-- end if momAdvection
486			ENDIF
487
488			C-- Set du/dt & dv/dt on boundaries to zero
489	adcroft	1.1	DO j=jMin,jMax
490			DO i=iMin,iMax
491	jmc	1.5	gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)*_maskW(i,j,k,bi,bj)
492			gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)*_maskS(i,j,k,bi,bj)
493	adcroft	1.1	ENDDO
494			ENDDO
495	jmc	1.5
496	adcroft	1.2
497	jmc	1.15	IF ( writeDiag ) THEN
498	adcroft	1.3	CALL WRITE_LOCAL_RL('Ds','I10',1,strain,bi,bj,k,myIter,myThid)
499			CALL WRITE_LOCAL_RL('Dt','I10',1,tension,bi,bj,k,myIter,myThid)
500	adcroft	1.2	CALL WRITE_LOCAL_RL('Du','I10',1,uDiss,bi,bj,k,myIter,myThid)
501			CALL WRITE_LOCAL_RL('Dv','I10',1,vDiss,bi,bj,k,myIter,myThid)
502	adcroft	1.3	CALL WRITE_LOCAL_RL('Z3','I10',1,vort3,bi,bj,k,myIter,myThid)
503	jmc	1.5	c CALL WRITE_LOCAL_RL('W3','I10',1,omega3,bi,bj,k,myIter,myThid)
504	adcroft	1.3	CALL WRITE_LOCAL_RL('KE','I10',1,KE,bi,bj,k,myIter,myThid)
505			CALL WRITE_LOCAL_RL('D','I10',1,hdiv,bi,bj,k,myIter,myThid)
506	adcroft	1.1	ENDIF
507	jmc	1.7
508	edhill	1.11	#endif /* ALLOW_MOM_VECINV */
509	adcroft	1.1
510			RETURN
511			END