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C $Header: /u/gcmpack/MITgcm/pkg/mom_vecinv/mom_vecinv.F,v 1.33 2004/12/18 02:18:55 edhill Exp $ |
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C $Name: $ |
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|
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#include "MOM_VECINV_OPTIONS.h" |
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|
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SUBROUTINE MOM_VECINV( |
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I bi,bj,iMin,iMax,jMin,jMax,k,kUp,kDown, |
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I dPhiHydX,dPhiHydY,KappaRU,KappaRV, |
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U fVerU, fVerV, |
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O guDiss, gvDiss, |
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I myTime, myIter, myThid) |
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C /==========================================================\ |
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C | S/R MOM_VECINV | |
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C | o Form the right hand-side of the momentum equation. | |
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C |==========================================================| |
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C | Terms are evaluated one layer at a time working from | |
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C | the bottom to the top. The vertically integrated | |
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C | barotropic flow tendency term is evluated by summing the | |
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C | tendencies. | |
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C | Notes: | |
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C | We have not sorted out an entirely satisfactory formula | |
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C | for the diffusion equation bc with lopping. The present | |
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C | form produces a diffusive flux that does not scale with | |
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C | open-area. Need to do something to solidfy this and to | |
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C | deal "properly" with thin walls. | |
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C \==========================================================/ |
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IMPLICIT NONE |
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|
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C == Global variables == |
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#include "SIZE.h" |
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#include "DYNVARS.h" |
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#include "EEPARAMS.h" |
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#include "PARAMS.h" |
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#ifdef ALLOW_MNC |
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#include "MNC_PARAMS.h" |
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#endif |
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#include "GRID.h" |
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#ifdef ALLOW_TIMEAVE |
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#include "TIMEAVE_STATV.h" |
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#endif |
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|
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C == Routine arguments == |
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C fVerU :: Flux of momentum in the vertical direction, out of the upper |
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C fVerV :: face of a cell K ( flux into the cell above ). |
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C dPhiHydX,Y :: Gradient (X & Y dir.) of Hydrostatic Potential |
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C guDiss :: dissipation tendency (all explicit terms), u component |
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C gvDiss :: dissipation tendency (all explicit terms), v component |
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C bi, bj, iMin, iMax, jMin, jMax - Range of points for which calculation |
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C results will be set. |
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C kUp, kDown - Index for upper and lower layers. |
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C myThid - Instance number for this innvocation of CALC_MOM_RHS |
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_RL dPhiHydX(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
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_RL dPhiHydY(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
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_RL KappaRU(1-OLx:sNx+OLx,1-OLy:sNy+OLy,Nr) |
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_RL KappaRV(1-OLx:sNx+OLx,1-OLy:sNy+OLy,Nr) |
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_RL fVerU(1-OLx:sNx+OLx,1-OLy:sNy+OLy,2) |
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_RL fVerV(1-OLx:sNx+OLx,1-OLy:sNy+OLy,2) |
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_RL guDiss(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL gvDiss(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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INTEGER kUp,kDown |
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_RL myTime |
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INTEGER myIter |
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INTEGER myThid |
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INTEGER bi,bj,iMin,iMax,jMin,jMax |
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|
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#ifdef ALLOW_MOM_VECINV |
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|
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C == Functions == |
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LOGICAL DIFFERENT_MULTIPLE |
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EXTERNAL DIFFERENT_MULTIPLE |
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|
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C == Local variables == |
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_RL vF (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL vrF (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL uCf (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL vCf (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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c _RL mT (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL del2u(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL del2v(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL tension(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL strain(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RS hFacZ(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RS r_hFacZ(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL uFld(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL vFld(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL dStar(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL zStar(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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C I,J,K - Loop counters |
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INTEGER i,j,k |
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C xxxFac - On-off tracer parameters used for switching terms off. |
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_RL ArDudrFac |
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_RL phxFac |
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c _RL mtFacU |
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_RL ArDvdrFac |
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_RL phyFac |
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c _RL mtFacV |
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LOGICAL bottomDragTerms |
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LOGICAL writeDiag |
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_RL KE(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL omega3(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL vort3(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL hDiv(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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|
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#ifdef ALLOW_MNC |
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INTEGER offsets(9) |
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#endif |
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|
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#ifdef ALLOW_AUTODIFF_TAMC |
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C-- only the kDown part of fverU/V is set in this subroutine |
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C-- the kUp is still required |
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C-- In the case of mom_fluxform Kup is set as well |
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C-- (at least in part) |
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fVerU(1,1,kUp) = fVerU(1,1,kUp) |
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fVerV(1,1,kUp) = fVerV(1,1,kUp) |
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#endif |
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|
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writeDiag = DIFFERENT_MULTIPLE(diagFreq, myTime, |
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& myTime-deltaTClock) |
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|
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#ifdef ALLOW_MNC |
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IF (useMNC .AND. snapshot_mnc .AND. writeDiag) THEN |
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IF ((bi .EQ. 1).AND.(bj .EQ. 1).AND.(k .EQ. 1)) THEN |
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CALL MNC_CW_SET_UDIM('mom_vi', -1, myThid) |
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CALL MNC_CW_I_W_S('I','mom_vi',0,0,'T',myIter,myThid) |
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CALL MNC_CW_SET_UDIM('mom_vi', 0, myThid) |
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ENDIF |
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DO i = 1,9 |
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offsets(i) = 0 |
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ENDDO |
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offsets(3) = k |
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C write(*,*) 'offsets = ',(offsets(i),i=1,9) |
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ENDIF |
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#endif /* ALLOW_MNC */ |
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|
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C Initialise intermediate terms |
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DO J=1-OLy,sNy+OLy |
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DO I=1-OLx,sNx+OLx |
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vF(i,j) = 0. |
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vrF(i,j) = 0. |
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uCf(i,j) = 0. |
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vCf(i,j) = 0. |
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c mT(i,j) = 0. |
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del2u(i,j) = 0. |
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del2v(i,j) = 0. |
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dStar(i,j) = 0. |
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zStar(i,j) = 0. |
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guDiss(i,j)= 0. |
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gvDiss(i,j)= 0. |
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vort3(i,j) = 0. |
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omega3(i,j)= 0. |
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ke(i,j) = 0. |
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#ifdef ALLOW_AUTODIFF_TAMC |
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strain(i,j) = 0. _d 0 |
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tension(i,j) = 0. _d 0 |
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#endif |
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ENDDO |
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ENDDO |
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|
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C-- Term by term tracer parmeters |
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C o U momentum equation |
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ArDudrFac = vfFacMom*1. |
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c mTFacU = mtFacMom*1. |
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phxFac = pfFacMom*1. |
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C o V momentum equation |
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ArDvdrFac = vfFacMom*1. |
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c mTFacV = mtFacMom*1. |
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phyFac = pfFacMom*1. |
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|
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IF ( no_slip_bottom |
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& .OR. bottomDragQuadratic.NE.0. |
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& .OR. bottomDragLinear.NE.0.) THEN |
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bottomDragTerms=.TRUE. |
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ELSE |
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bottomDragTerms=.FALSE. |
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ENDIF |
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|
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C-- with stagger time stepping, grad Phi_Hyp is directly incoporated in TIMESTEP |
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IF (staggerTimeStep) THEN |
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phxFac = 0. |
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phyFac = 0. |
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ENDIF |
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|
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C-- Calculate open water fraction at vorticity points |
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CALL MOM_CALC_HFACZ(bi,bj,k,hFacZ,r_hFacZ,myThid) |
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|
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C Make local copies of horizontal flow field |
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DO j=1-OLy,sNy+OLy |
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DO i=1-OLx,sNx+OLx |
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uFld(i,j) = uVel(i,j,k,bi,bj) |
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vFld(i,j) = vVel(i,j,k,bi,bj) |
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ENDDO |
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ENDDO |
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|
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C note (jmc) : Dissipation and Vort3 advection do not necesary |
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C use the same maskZ (and hFacZ) => needs 2 call(s) |
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c CALL MOM_VI_HFACZ_DISS(bi,bj,k,hFacZ,r_hFacZ,myThid) |
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|
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CALL MOM_CALC_KE(bi,bj,k,2,uFld,vFld,KE,myThid) |
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|
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CALL MOM_CALC_HDIV(bi,bj,k,2,uFld,vFld,hDiv,myThid) |
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|
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CALL MOM_CALC_RELVORT3(bi,bj,k,uFld,vFld,hFacZ,vort3,myThid) |
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|
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IF (useAbsVorticity) |
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& CALL MOM_CALC_ABSVORT3(bi,bj,k,vort3,omega3,myThid) |
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|
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IF (momViscosity) THEN |
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C Calculate del^2 u and del^2 v for bi-harmonic term |
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IF ( (viscA4.NE.0. .AND. no_slip_sides) |
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& .OR. viscA4D.NE.0. .OR. viscA4Z.NE.0. |
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& .OR. viscA4Grid.NE.0. |
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& .OR. viscC4leith.NE.0. |
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& .OR. viscC4leithD.NE.0. |
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& ) THEN |
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CALL MOM_VI_DEL2UV(bi,bj,k,hDiv,vort3,hFacZ, |
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O del2u,del2v, |
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& myThid) |
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CALL MOM_CALC_HDIV(bi,bj,k,2,del2u,del2v,dStar,myThid) |
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CALL MOM_CALC_RELVORT3( |
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& bi,bj,k,del2u,del2v,hFacZ,zStar,myThid) |
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ENDIF |
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C Calculate dissipation terms for U and V equations |
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C in terms of vorticity and divergence |
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IF ( viscAhD.NE.0. .OR. viscAhZ.NE.0. |
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& .OR. viscA4D.NE.0. .OR. viscA4Z.NE.0. |
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& .OR. viscAhGrid.NE.0. .OR. viscA4Grid.NE.0. |
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& .OR. viscC2leith.NE.0. .OR. viscC4leith.NE.0. |
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& .OR. viscC2leithD.NE.0. .OR. viscC4leithD.NE.0. |
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& ) THEN |
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CALL MOM_VI_HDISSIP(bi,bj,k,hDiv,vort3,hFacZ,dStar,zStar, |
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O guDiss,gvDiss, |
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& myThid) |
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ENDIF |
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C or in terms of tension and strain |
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IF (viscAstrain.NE.0. .OR. viscAtension.NE.0.) THEN |
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CALL MOM_CALC_TENSION(bi,bj,k,uFld,vFld, |
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O tension, |
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I myThid) |
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CALL MOM_CALC_STRAIN(bi,bj,k,uFld,vFld,hFacZ, |
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O strain, |
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I myThid) |
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CALL MOM_HDISSIP(bi,bj,k, |
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I tension,strain,hFacZ,viscAtension,viscAstrain, |
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O guDiss,gvDiss, |
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I myThid) |
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ENDIF |
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ENDIF |
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|
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C- Return to standard hfacZ (min-4) and mask vort3 accordingly: |
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c CALL MOM_VI_MASK_VORT3(bi,bj,k,hFacZ,r_hFacZ,vort3,myThid) |
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|
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C---- Zonal momentum equation starts here |
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|
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C-- Vertical flux (fVer is at upper face of "u" cell) |
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|
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C Eddy component of vertical flux (interior component only) -> vrF |
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IF (momViscosity.AND..NOT.implicitViscosity) THEN |
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CALL MOM_U_RVISCFLUX(bi,bj,k,uVel,KappaRU,vrF,myThid) |
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|
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C Combine fluxes |
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DO j=jMin,jMax |
| 262 |
DO i=iMin,iMax |
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fVerU(i,j,kDown) = ArDudrFac*vrF(i,j) |
| 264 |
ENDDO |
| 265 |
ENDDO |
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|
| 267 |
C-- Tendency is minus divergence of the fluxes |
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DO j=2-Oly,sNy+Oly-1 |
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DO i=2-Olx,sNx+Olx-1 |
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guDiss(i,j) = guDiss(i,j) |
| 271 |
& -_recip_hFacW(i,j,k,bi,bj)*recip_drF(k) |
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& *recip_rAw(i,j,bi,bj) |
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& *( |
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& +fVerU(i,j,kUp)*rkFac - fVerU(i,j,kDown)*rkFac |
| 275 |
& ) |
| 276 |
ENDDO |
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ENDDO |
| 278 |
ENDIF |
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|
| 280 |
C-- No-slip and drag BCs appear as body forces in cell abutting topography |
| 281 |
IF (momViscosity.AND.no_slip_sides) THEN |
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C- No-slip BCs impose a drag at walls... |
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CALL MOM_U_SIDEDRAG(bi,bj,k,uFld,del2u,hFacZ,vF,myThid) |
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DO j=jMin,jMax |
| 285 |
DO i=iMin,iMax |
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guDiss(i,j) = guDiss(i,j)+vF(i,j) |
| 287 |
ENDDO |
| 288 |
ENDDO |
| 289 |
ENDIF |
| 290 |
|
| 291 |
C- No-slip BCs impose a drag at bottom |
| 292 |
IF (momViscosity.AND.bottomDragTerms) THEN |
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CALL MOM_U_BOTTOMDRAG(bi,bj,k,uFld,KE,KappaRU,vF,myThid) |
| 294 |
DO j=jMin,jMax |
| 295 |
DO i=iMin,iMax |
| 296 |
guDiss(i,j) = guDiss(i,j)+vF(i,j) |
| 297 |
ENDDO |
| 298 |
ENDDO |
| 299 |
ENDIF |
| 300 |
|
| 301 |
C-- Metric terms for curvilinear grid systems |
| 302 |
c IF (usingSphericalPolarMTerms) THEN |
| 303 |
C o Spherical polar grid metric terms |
| 304 |
c CALL MOM_U_METRIC_NH(bi,bj,k,uFld,wVel,mT,myThid) |
| 305 |
c DO j=jMin,jMax |
| 306 |
c DO i=iMin,iMax |
| 307 |
c gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+mTFacU*mT(i,j) |
| 308 |
c ENDDO |
| 309 |
c ENDDO |
| 310 |
c ENDIF |
| 311 |
|
| 312 |
C---- Meridional momentum equation starts here |
| 313 |
|
| 314 |
C-- Vertical flux (fVer is at upper face of "v" cell) |
| 315 |
|
| 316 |
C Eddy component of vertical flux (interior component only) -> vrF |
| 317 |
IF (momViscosity.AND..NOT.implicitViscosity) THEN |
| 318 |
CALL MOM_V_RVISCFLUX(bi,bj,k,vVel,KappaRV,vrf,myThid) |
| 319 |
|
| 320 |
C Combine fluxes -> fVerV |
| 321 |
DO j=jMin,jMax |
| 322 |
DO i=iMin,iMax |
| 323 |
fVerV(i,j,kDown) = ArDvdrFac*vrF(i,j) |
| 324 |
ENDDO |
| 325 |
ENDDO |
| 326 |
|
| 327 |
C-- Tendency is minus divergence of the fluxes |
| 328 |
DO j=jMin,jMax |
| 329 |
DO i=iMin,iMax |
| 330 |
gvDiss(i,j) = gvDiss(i,j) |
| 331 |
& -_recip_hFacS(i,j,k,bi,bj)*recip_drF(k) |
| 332 |
& *recip_rAs(i,j,bi,bj) |
| 333 |
& *( |
| 334 |
& +fVerV(i,j,kUp)*rkFac - fVerV(i,j,kDown)*rkFac |
| 335 |
& ) |
| 336 |
ENDDO |
| 337 |
ENDDO |
| 338 |
ENDIF |
| 339 |
|
| 340 |
C-- No-slip and drag BCs appear as body forces in cell abutting topography |
| 341 |
IF (momViscosity.AND.no_slip_sides) THEN |
| 342 |
C- No-slip BCs impose a drag at walls... |
| 343 |
CALL MOM_V_SIDEDRAG(bi,bj,k,vFld,del2v,hFacZ,vF,myThid) |
| 344 |
DO j=jMin,jMax |
| 345 |
DO i=iMin,iMax |
| 346 |
gvDiss(i,j) = gvDiss(i,j)+vF(i,j) |
| 347 |
ENDDO |
| 348 |
ENDDO |
| 349 |
ENDIF |
| 350 |
C- No-slip BCs impose a drag at bottom |
| 351 |
IF (momViscosity.AND.bottomDragTerms) THEN |
| 352 |
CALL MOM_V_BOTTOMDRAG(bi,bj,k,vFld,KE,KappaRV,vF,myThid) |
| 353 |
DO j=jMin,jMax |
| 354 |
DO i=iMin,iMax |
| 355 |
gvDiss(i,j) = gvDiss(i,j)+vF(i,j) |
| 356 |
ENDDO |
| 357 |
ENDDO |
| 358 |
ENDIF |
| 359 |
|
| 360 |
C-- Metric terms for curvilinear grid systems |
| 361 |
c IF (usingSphericalPolarMTerms) THEN |
| 362 |
C o Spherical polar grid metric terms |
| 363 |
c CALL MOM_V_METRIC_NH(bi,bj,k,vFld,wVel,mT,myThid) |
| 364 |
c DO j=jMin,jMax |
| 365 |
c DO i=iMin,iMax |
| 366 |
c gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+mTFacV*mT(i,j) |
| 367 |
c ENDDO |
| 368 |
c ENDDO |
| 369 |
c ENDIF |
| 370 |
|
| 371 |
C-- Horizontal Coriolis terms |
| 372 |
IF (useCoriolis .AND. .NOT.useCDscheme |
| 373 |
& .AND. .NOT. useAbsVorticity) THEN |
| 374 |
CALL MOM_VI_CORIOLIS(bi,bj,k,uFld,vFld,hFacZ,r_hFacZ, |
| 375 |
& uCf,vCf,myThid) |
| 376 |
DO j=jMin,jMax |
| 377 |
DO i=iMin,iMax |
| 378 |
gU(i,j,k,bi,bj) = uCf(i,j) - phxFac*dPhiHydX(i,j) |
| 379 |
gV(i,j,k,bi,bj) = vCf(i,j) - phyFac*dPhiHydY(i,j) |
| 380 |
ENDDO |
| 381 |
ENDDO |
| 382 |
IF ( writeDiag ) THEN |
| 383 |
IF (snapshot_mdsio) THEN |
| 384 |
CALL WRITE_LOCAL_RL('fV','I10',1,uCf,bi,bj,k,myIter,myThid) |
| 385 |
CALL WRITE_LOCAL_RL('fU','I10',1,vCf,bi,bj,k,myIter,myThid) |
| 386 |
ENDIF |
| 387 |
#ifdef ALLOW_MNC |
| 388 |
IF (useMNC .AND. snapshot_mnc) THEN |
| 389 |
CALL MNC_CW_RL_W_OFFSET('D','mom_vi',bi,bj, 'fV', uCf, |
| 390 |
& offsets, myThid) |
| 391 |
CALL MNC_CW_RL_W_OFFSET('D','mom_vi',bi,bj, 'fU', vCf, |
| 392 |
& offsets, myThid) |
| 393 |
ENDIF |
| 394 |
#endif /* ALLOW_MNC */ |
| 395 |
ENDIF |
| 396 |
ELSE |
| 397 |
DO j=jMin,jMax |
| 398 |
DO i=iMin,iMax |
| 399 |
gU(i,j,k,bi,bj) = -phxFac*dPhiHydX(i,j) |
| 400 |
gV(i,j,k,bi,bj) = -phyFac*dPhiHydY(i,j) |
| 401 |
ENDDO |
| 402 |
ENDDO |
| 403 |
ENDIF |
| 404 |
|
| 405 |
IF (momAdvection) THEN |
| 406 |
C-- Horizontal advection of relative vorticity |
| 407 |
IF (useAbsVorticity) THEN |
| 408 |
CALL MOM_VI_U_CORIOLIS(bi,bj,K,vFld,omega3,hFacZ,r_hFacZ, |
| 409 |
& uCf,myThid) |
| 410 |
ELSE |
| 411 |
CALL MOM_VI_U_CORIOLIS(bi,bj,k,vFld,vort3,hFacZ,r_hFacZ, |
| 412 |
& uCf,myThid) |
| 413 |
ENDIF |
| 414 |
c CALL MOM_VI_U_CORIOLIS_C4(bi,bj,K,vFld,vort3,r_hFacZ,uCf,myThid) |
| 415 |
DO j=jMin,jMax |
| 416 |
DO i=iMin,iMax |
| 417 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+uCf(i,j) |
| 418 |
ENDDO |
| 419 |
ENDDO |
| 420 |
IF (useAbsVorticity) THEN |
| 421 |
CALL MOM_VI_V_CORIOLIS(bi,bj,K,uFld,omega3,hFacZ,r_hFacZ, |
| 422 |
& vCf,myThid) |
| 423 |
ELSE |
| 424 |
CALL MOM_VI_V_CORIOLIS(bi,bj,k,uFld,vort3,hFacZ,r_hFacZ, |
| 425 |
& vCf,myThid) |
| 426 |
ENDIF |
| 427 |
c CALL MOM_VI_V_CORIOLIS_C4(bi,bj,K,uFld,vort3,r_hFacZ,vCf,myThid) |
| 428 |
DO j=jMin,jMax |
| 429 |
DO i=iMin,iMax |
| 430 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vCf(i,j) |
| 431 |
ENDDO |
| 432 |
ENDDO |
| 433 |
|
| 434 |
IF ( writeDiag ) THEN |
| 435 |
IF (snapshot_mdsio) THEN |
| 436 |
CALL WRITE_LOCAL_RL('zV','I10',1,uCf,bi,bj,k,myIter,myThid) |
| 437 |
CALL WRITE_LOCAL_RL('zU','I10',1,vCf,bi,bj,k,myIter,myThid) |
| 438 |
ENDIF |
| 439 |
#ifdef ALLOW_MNC |
| 440 |
IF (useMNC .AND. snapshot_mnc) THEN |
| 441 |
CALL MNC_CW_RL_W_OFFSET('D','mom_vi',bi,bj, 'zV', uCf, |
| 442 |
& offsets, myThid) |
| 443 |
CALL MNC_CW_RL_W_OFFSET('D','mom_vi',bi,bj, 'zU', vCf, |
| 444 |
& offsets, myThid) |
| 445 |
ENDIF |
| 446 |
#endif /* ALLOW_MNC */ |
| 447 |
ENDIF |
| 448 |
|
| 449 |
#ifdef ALLOW_TIMEAVE |
| 450 |
#ifndef MINIMAL_TAVE_OUTPUT |
| 451 |
IF (taveFreq.GT.0.) THEN |
| 452 |
CALL TIMEAVE_CUMUL_1K1T(uZetatave,vCf,deltaTClock, |
| 453 |
& Nr, k, bi, bj, myThid) |
| 454 |
CALL TIMEAVE_CUMUL_1K1T(vZetatave,uCf,deltaTClock, |
| 455 |
& Nr, k, bi, bj, myThid) |
| 456 |
ENDIF |
| 457 |
#endif /* ndef MINIMAL_TAVE_OUTPUT */ |
| 458 |
#endif /* ALLOW_TIMEAVE */ |
| 459 |
|
| 460 |
C-- Vertical shear terms (-w*du/dr & -w*dv/dr) |
| 461 |
IF ( .NOT. momImplVertAdv ) THEN |
| 462 |
CALL MOM_VI_U_VERTSHEAR(bi,bj,K,uVel,wVel,uCf,myThid) |
| 463 |
DO j=jMin,jMax |
| 464 |
DO i=iMin,iMax |
| 465 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+uCf(i,j) |
| 466 |
ENDDO |
| 467 |
ENDDO |
| 468 |
CALL MOM_VI_V_VERTSHEAR(bi,bj,K,vVel,wVel,vCf,myThid) |
| 469 |
DO j=jMin,jMax |
| 470 |
DO i=iMin,iMax |
| 471 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vCf(i,j) |
| 472 |
ENDDO |
| 473 |
ENDDO |
| 474 |
ENDIF |
| 475 |
|
| 476 |
C-- Bernoulli term |
| 477 |
CALL MOM_VI_U_GRAD_KE(bi,bj,K,KE,uCf,myThid) |
| 478 |
DO j=jMin,jMax |
| 479 |
DO i=iMin,iMax |
| 480 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+uCf(i,j) |
| 481 |
ENDDO |
| 482 |
ENDDO |
| 483 |
CALL MOM_VI_V_GRAD_KE(bi,bj,K,KE,vCf,myThid) |
| 484 |
DO j=jMin,jMax |
| 485 |
DO i=iMin,iMax |
| 486 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vCf(i,j) |
| 487 |
ENDDO |
| 488 |
ENDDO |
| 489 |
IF ( writeDiag ) THEN |
| 490 |
IF (snapshot_mdsio) THEN |
| 491 |
CALL WRITE_LOCAL_RL('KEx','I10',1,uCf,bi,bj,k,myIter,myThid) |
| 492 |
CALL WRITE_LOCAL_RL('KEy','I10',1,vCf,bi,bj,k,myIter,myThid) |
| 493 |
ENDIF |
| 494 |
#ifdef ALLOW_MNC |
| 495 |
IF (useMNC .AND. snapshot_mnc) THEN |
| 496 |
CALL MNC_CW_RL_W_OFFSET('D','mom_vi',bi,bj, 'KEx', uCf, |
| 497 |
& offsets, myThid) |
| 498 |
CALL MNC_CW_RL_W_OFFSET('D','mom_vi',bi,bj, 'KEy', vCf, |
| 499 |
& offsets, myThid) |
| 500 |
ENDIF |
| 501 |
#endif /* ALLOW_MNC */ |
| 502 |
ENDIF |
| 503 |
|
| 504 |
C-- end if momAdvection |
| 505 |
ENDIF |
| 506 |
|
| 507 |
C-- Set du/dt & dv/dt on boundaries to zero |
| 508 |
DO j=jMin,jMax |
| 509 |
DO i=iMin,iMax |
| 510 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)*_maskW(i,j,k,bi,bj) |
| 511 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)*_maskS(i,j,k,bi,bj) |
| 512 |
ENDDO |
| 513 |
ENDDO |
| 514 |
|
| 515 |
#ifdef ALLOW_DEBUG |
| 516 |
IF ( debugLevel .GE. debLevB |
| 517 |
& .AND. k.EQ.4 .AND. myIter.EQ.nIter0 |
| 518 |
& .AND. nPx.EQ.1 .AND. nPy.EQ.1 |
| 519 |
& .AND. useCubedSphereExchange ) THEN |
| 520 |
CALL DEBUG_CS_CORNER_UV( ' uDiss,vDiss from MOM_VECINV', |
| 521 |
& guDiss,gvDiss, k, standardMessageUnit,bi,bj,myThid ) |
| 522 |
ENDIF |
| 523 |
#endif /* ALLOW_DEBUG */ |
| 524 |
|
| 525 |
IF ( writeDiag ) THEN |
| 526 |
IF (snapshot_mdsio) THEN |
| 527 |
CALL WRITE_LOCAL_RL('Ds','I10',1,strain,bi,bj,k,myIter,myThid) |
| 528 |
CALL WRITE_LOCAL_RL('Dt','I10',1,tension,bi,bj,k,myIter, |
| 529 |
& myThid) |
| 530 |
CALL WRITE_LOCAL_RL('Du','I10',1,guDiss,bi,bj,k,myIter,myThid) |
| 531 |
CALL WRITE_LOCAL_RL('Dv','I10',1,gvDiss,bi,bj,k,myIter,myThid) |
| 532 |
CALL WRITE_LOCAL_RL('Z3','I10',1,vort3,bi,bj,k,myIter,myThid) |
| 533 |
CALL WRITE_LOCAL_RL('W3','I10',1,omega3,bi,bj,k,myIter,myThid) |
| 534 |
CALL WRITE_LOCAL_RL('KE','I10',1,KE,bi,bj,k,myIter,myThid) |
| 535 |
CALL WRITE_LOCAL_RL('D','I10',1,hdiv,bi,bj,k,myIter,myThid) |
| 536 |
ENDIF |
| 537 |
#ifdef ALLOW_MNC |
| 538 |
IF (useMNC .AND. snapshot_mnc) THEN |
| 539 |
CALL MNC_CW_RL_W_OFFSET('D','mom_vi',bi,bj,'Ds',strain, |
| 540 |
& offsets, myThid) |
| 541 |
CALL MNC_CW_RL_W_OFFSET('D','mom_vi',bi,bj,'Dt',tension, |
| 542 |
& offsets, myThid) |
| 543 |
CALL MNC_CW_RL_W_OFFSET('D','mom_vi',bi,bj,'Du',guDiss, |
| 544 |
& offsets, myThid) |
| 545 |
CALL MNC_CW_RL_W_OFFSET('D','mom_vi',bi,bj,'Dv',gvDiss, |
| 546 |
& offsets, myThid) |
| 547 |
CALL MNC_CW_RL_W_OFFSET('D','mom_vi',bi,bj,'Z3',vort3, |
| 548 |
& offsets, myThid) |
| 549 |
CALL MNC_CW_RL_W_OFFSET('D','mom_vi',bi,bj,'W3',omega3, |
| 550 |
& offsets, myThid) |
| 551 |
CALL MNC_CW_RL_W_OFFSET('D','mom_vi',bi,bj,'KE',KE, |
| 552 |
& offsets, myThid) |
| 553 |
CALL MNC_CW_RL_W_OFFSET('D','mom_vi',bi,bj,'D', hdiv, |
| 554 |
& offsets, myThid) |
| 555 |
ENDIF |
| 556 |
#endif /* ALLOW_MNC */ |
| 557 |
ENDIF |
| 558 |
|
| 559 |
#endif /* ALLOW_MOM_VECINV */ |
| 560 |
|
| 561 |
RETURN |
| 562 |
END |
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