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C $Header: $ |
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C $Name: $ |
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|
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#include "CPP_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 phi_hyd,KappaRU,KappaRV, |
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U fVerU, fVerV, |
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I myCurrentTime, 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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#include "GRID.h" |
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|
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C == Routine arguments == |
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C fVerU - Flux of momentum in the vertical |
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C fVerV direction out of the upper face of a cell K |
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C ( flux into the cell above ). |
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C phi_hyd - Hydrostatic pressure |
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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 phi_hyd(1-OLx:sNx+OLx,1-OLy:sNy+OLy,Nr) |
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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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INTEGER kUp,kDown |
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INTEGER myThid |
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_RL myCurrentTime |
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INTEGER bi,bj,iMin,iMax,jMin,jMax |
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|
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C == Local variables == |
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_RL aF (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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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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_RL mT (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL pF (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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_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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_RS xA(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RS yA(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL uTrans(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL vTrans(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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_RL uDiss(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL vDiss(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 rVelMaskOverride - Factor for imposing special surface boundary conditions |
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C ( set according to free-surface condition ). |
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C hFacROpen - Lopped cell factos used tohold fraction of open |
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C hFacRClosed and closed cell wall. |
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_RL rVelMaskOverride |
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C xxxFac - On-off tracer parameters used for switching terms off. |
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_RL uDudxFac |
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_RL AhDudxFac |
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_RL A4DuxxdxFac |
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_RL vDudyFac |
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_RL AhDudyFac |
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_RL A4DuyydyFac |
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_RL rVelDudrFac |
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_RL ArDudrFac |
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_RL fuFac |
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_RL phxFac |
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_RL mtFacU |
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_RL uDvdxFac |
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_RL AhDvdxFac |
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_RL A4DvxxdxFac |
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_RL vDvdyFac |
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_RL AhDvdyFac |
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_RL A4DvyydyFac |
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_RL rVelDvdrFac |
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_RL ArDvdrFac |
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_RL fvFac |
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_RL phyFac |
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_RL vForcFac |
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_RL mtFacV |
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INTEGER km1,kp1 |
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_RL wVelBottomOverride |
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LOGICAL bottomDragTerms |
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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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km1=MAX(1,k-1) |
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kp1=MIN(Nr,k+1) |
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rVelMaskOverride=1. |
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IF ( k .EQ. 1 ) rVelMaskOverride=freeSurfFac |
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wVelBottomOverride=1. |
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IF (k.EQ.Nr) wVelBottomOverride=0. |
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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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aF(i,j) = 0. |
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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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mT(i,j) = 0. |
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pF(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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uDiss(i,j) = 0. |
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vDiss(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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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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uDudxFac = afFacMom*1. |
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AhDudxFac = vfFacMom*1. |
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A4DuxxdxFac = vfFacMom*1. |
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vDudyFac = afFacMom*1. |
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AhDudyFac = vfFacMom*1. |
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A4DuyydyFac = vfFacMom*1. |
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rVelDudrFac = afFacMom*1. |
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ArDudrFac = vfFacMom*1. |
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mTFacU = mtFacMom*1. |
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fuFac = cfFacMom*1. |
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phxFac = pfFacMom*1. |
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C o V momentum equation |
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uDvdxFac = afFacMom*1. |
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AhDvdxFac = vfFacMom*1. |
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A4DvxxdxFac = vfFacMom*1. |
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vDvdyFac = afFacMom*1. |
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AhDvdyFac = vfFacMom*1. |
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A4DvyydyFac = vfFacMom*1. |
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rVelDvdrFac = afFacMom*1. |
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ArDvdrFac = vfFacMom*1. |
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mTFacV = mtFacMom*1. |
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fvFac = cfFacMom*1. |
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phyFac = pfFacMom*1. |
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vForcFac = foFacMom*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---- Calculate common quantities used in both U and V equations |
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C Calculate tracer cell face open areas |
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DO j=1-OLy,sNy+OLy |
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DO i=1-OLx,sNx+OLx |
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xA(i,j) = _dyG(i,j,bi,bj) |
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& *drF(k)*_hFacW(i,j,k,bi,bj) |
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yA(i,j) = _dxG(i,j,bi,bj) |
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& *drF(k)*_hFacS(i,j,k,bi,bj) |
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ENDDO |
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ENDDO |
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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 |
205 |
ENDDO |
206 |
|
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C Calculate velocity field "volume transports" through tracer cell faces. |
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DO j=1-OLy,sNy+OLy |
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DO i=1-OLx,sNx+OLx |
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uTrans(i,j) = uFld(i,j)*xA(i,j) |
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vTrans(i,j) = vFld(i,j)*yA(i,j) |
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ENDDO |
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ENDDO |
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|
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CALL MOM_VI_CALC_KE(bi,bj,k,uFld,vFld,KE,myThid) |
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|
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CALL MOM_VI_CALC_HDIV(bi,bj,k,uFld,vFld,hDiv,myThid) |
218 |
|
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CALL MOM_VI_CALC_RELVORT3(bi,bj,k,uFld,vFld,hFacZ,vort3,myThid) |
220 |
|
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CALL MOM_VI_CALC_ABSVORT3(bi,bj,k,vort3,omega3,myThid) |
222 |
|
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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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CALL MOM_VI_DEL2UV( |
226 |
I bi,bj,k,hDiv,vort3,hFacZ, |
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O del2u,del2v, |
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& myThid) |
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CALL MOM_VI_CALC_HDIV(bi,bj,k,del2u,del2v,dStar,myThid) |
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CALL MOM_VI_CALC_RELVORT3(bi,bj,k,del2u,del2v,hFacZ,zStar,myThid) |
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C Calculate dissipation terms for U and V equations |
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CALL MOM_VI_HDISSIP( |
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I bi,bj,k,hDiv,vort3,hFacZ,dStar,zStar, |
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O uDiss,vDiss, |
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& myThid) |
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ENDIF |
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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) |
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& CALL MOM_U_RVISCFLUX(bi,bj,k,uVel,KappaRU,vrF,myThid) |
245 |
|
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C Combine fluxes |
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DO j=jMin,jMax |
248 |
DO i=iMin,iMax |
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fVerU(i,j,kDown) = ArDudrFac*vrF(i,j) |
250 |
ENDDO |
251 |
ENDDO |
252 |
|
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C--- Hydrostatic term ( -1/rhoConst . dphi/dx ) |
254 |
IF (momPressureForcing) THEN |
255 |
DO j=1-Olx,sNy+Oly |
256 |
DO i=2-Olx,sNx+Olx |
257 |
pf(i,j) = - _recip_dxC(i,j,bi,bj) |
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& *(phi_hyd(i,j,k)-phi_hyd(i-1,j,k)) |
259 |
ENDDO |
260 |
ENDDO |
261 |
ENDIF |
262 |
|
263 |
C-- Tendency is minus divergence of the fluxes + coriolis + pressure term |
264 |
DO j=2-Oly,sNy+Oly-1 |
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DO i=2-Olx,sNx+Olx-1 |
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gU(i,j,k,bi,bj) = uDiss(i,j) |
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& -_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 |
271 |
& ) |
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& _PHM( +phxFac * pf(i,j) ) |
273 |
ENDDO |
274 |
ENDDO |
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|
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C-- No-slip and drag BCs appear as body forces in cell abutting topography |
277 |
IF (momViscosity.AND.no_slip_sides) THEN |
278 |
C- No-slip BCs impose a drag at walls... |
279 |
CALL MOM_U_SIDEDRAG(bi,bj,k,uFld,del2u,hFacZ,vF,myThid) |
280 |
DO j=jMin,jMax |
281 |
DO i=iMin,iMax |
282 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+vF(i,j) |
283 |
ENDDO |
284 |
ENDDO |
285 |
ENDIF |
286 |
C- No-slip BCs impose a drag at bottom |
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IF (momViscosity.AND.bottomDragTerms) THEN |
288 |
CALL MOM_U_BOTTOMDRAG(bi,bj,k,uFld,KE,KappaRU,vF,myThid) |
289 |
DO j=jMin,jMax |
290 |
DO i=iMin,iMax |
291 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+vF(i,j) |
292 |
ENDDO |
293 |
ENDDO |
294 |
ENDIF |
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|
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C-- Forcing term |
297 |
IF (momForcing) |
298 |
& CALL EXTERNAL_FORCING_U( |
299 |
I iMin,iMax,jMin,jMax,bi,bj,k, |
300 |
I myCurrentTime,myThid) |
301 |
|
302 |
C-- Metric terms for curvilinear grid systems |
303 |
c IF (usingSphericalPolarMTerms) THEN |
304 |
C o Spherical polar grid metric terms |
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c CALL MOM_U_METRIC_NH(bi,bj,k,uFld,wVel,mT,myThid) |
306 |
c DO j=jMin,jMax |
307 |
c DO i=iMin,iMax |
308 |
c gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+mTFacU*mT(i,j) |
309 |
c ENDDO |
310 |
c ENDDO |
311 |
c ENDIF |
312 |
|
313 |
C-- Set du/dt on boundaries to zero |
314 |
DO j=jMin,jMax |
315 |
DO i=iMin,iMax |
316 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)*_maskW(i,j,k,bi,bj) |
317 |
ENDDO |
318 |
ENDDO |
319 |
|
320 |
|
321 |
C---- Meridional momentum equation starts here |
322 |
|
323 |
C-- Vertical flux (fVer is at upper face of "v" cell) |
324 |
|
325 |
C Eddy component of vertical flux (interior component only) -> vrF |
326 |
IF (momViscosity.AND..NOT.implicitViscosity) |
327 |
& CALL MOM_V_RVISCFLUX(bi,bj,k,vVel,KappaRV,vrf,myThid) |
328 |
|
329 |
C Combine fluxes -> fVerV |
330 |
DO j=jMin,jMax |
331 |
DO i=iMin,iMax |
332 |
fVerV(i,j,kDown) = ArDvdrFac*vrF(i,j) |
333 |
ENDDO |
334 |
ENDDO |
335 |
|
336 |
C--- Hydorstatic term (-1/rhoConst . dphi/dy ) |
337 |
IF (momPressureForcing) THEN |
338 |
DO j=jMin,jMax |
339 |
DO i=iMin,iMax |
340 |
pF(i,j) = -_recip_dyC(i,j,bi,bj) |
341 |
& *(phi_hyd(i,j,k)-phi_hyd(i,j-1,k)) |
342 |
ENDDO |
343 |
ENDDO |
344 |
ENDIF |
345 |
|
346 |
C-- Tendency is minus divergence of the fluxes + coriolis + pressure term |
347 |
DO j=jMin,jMax |
348 |
DO i=iMin,iMax |
349 |
gV(i,j,k,bi,bj) = vDiss(i,j) |
350 |
& -_recip_hFacS(i,j,k,bi,bj)*recip_drF(k) |
351 |
& *recip_rAs(i,j,bi,bj) |
352 |
& *( |
353 |
& +fVerV(i,j,kUp)*rkFac - fVerV(i,j,kDown)*rkFac |
354 |
& ) |
355 |
& _PHM( +phyFac*pf(i,j) ) |
356 |
ENDDO |
357 |
ENDDO |
358 |
|
359 |
C-- No-slip and drag BCs appear as body forces in cell abutting topography |
360 |
IF (momViscosity.AND.no_slip_sides) THEN |
361 |
C- No-slip BCs impose a drag at walls... |
362 |
CALL MOM_V_SIDEDRAG(bi,bj,k,vFld,del2v,hFacZ,vF,myThid) |
363 |
DO j=jMin,jMax |
364 |
DO i=iMin,iMax |
365 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vF(i,j) |
366 |
ENDDO |
367 |
ENDDO |
368 |
ENDIF |
369 |
C- No-slip BCs impose a drag at bottom |
370 |
IF (momViscosity.AND.bottomDragTerms) THEN |
371 |
CALL MOM_V_BOTTOMDRAG(bi,bj,k,vFld,KE,KappaRV,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 |
|
379 |
C-- Forcing term |
380 |
IF (momForcing) |
381 |
& CALL EXTERNAL_FORCING_V( |
382 |
I iMin,iMax,jMin,jMax,bi,bj,k, |
383 |
I myCurrentTime,myThid) |
384 |
|
385 |
C-- Metric terms for curvilinear grid systems |
386 |
c IF (usingSphericalPolarMTerms) THEN |
387 |
C o Spherical polar grid metric terms |
388 |
c CALL MOM_V_METRIC_NH(bi,bj,k,vFld,wVel,mT,myThid) |
389 |
c DO j=jMin,jMax |
390 |
c DO i=iMin,iMax |
391 |
c gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+mTFacV*mT(i,j) |
392 |
c ENDDO |
393 |
c ENDDO |
394 |
c ENDIF |
395 |
|
396 |
C-- Set dv/dt on boundaries to zero |
397 |
DO j=jMin,jMax |
398 |
DO i=iMin,iMax |
399 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)*_maskS(i,j,k,bi,bj) |
400 |
ENDDO |
401 |
ENDDO |
402 |
|
403 |
C-- Horizontal Coriolis terms |
404 |
CALL MOM_VI_CORIOLIS(bi,bj,K,uFld,vFld,omega3,r_hFacZ, |
405 |
& uCf,vCf,myThid) |
406 |
DO j=jMin,jMax |
407 |
DO i=iMin,iMax |
408 |
gU(i,j,k,bi,bj) = (gU(i,j,k,bi,bj)+uCf(i,j)) |
409 |
& *_maskW(i,j,k,bi,bj) |
410 |
gV(i,j,k,bi,bj) = (gV(i,j,k,bi,bj)+vCf(i,j)) |
411 |
& *_maskS(i,j,k,bi,bj) |
412 |
ENDDO |
413 |
ENDDO |
414 |
c CALL MOM_VI_U_CORIOLIS(bi,bj,K,vFld,omega3,r_hFacZ,uCf,myThid) |
415 |
CALL MOM_VI_U_CORIOLIS(bi,bj,K,vFld,vort3,r_hFacZ,uCf,myThid) |
416 |
c CALL MOM_VI_U_CORIOLIS_C4(bi,bj,K,vFld,vort3,r_hFacZ,uCf,myThid) |
417 |
DO j=jMin,jMax |
418 |
DO i=iMin,iMax |
419 |
gU(i,j,k,bi,bj) = (gU(i,j,k,bi,bj)+uCf(i,j)) |
420 |
& *_maskW(i,j,k,bi,bj) |
421 |
ENDDO |
422 |
ENDDO |
423 |
c CALL MOM_VI_V_CORIOLIS(bi,bj,K,uFld,omega3,r_hFacZ,vCf,myThid) |
424 |
CALL MOM_VI_V_CORIOLIS(bi,bj,K,uFld,vort3,r_hFacZ,vCf,myThid) |
425 |
c CALL MOM_VI_V_CORIOLIS_C4(bi,bj,K,uFld,vort3,r_hFacZ,vCf,myThid) |
426 |
DO j=jMin,jMax |
427 |
DO i=iMin,iMax |
428 |
gV(i,j,k,bi,bj) = (gV(i,j,k,bi,bj)+vCf(i,j)) |
429 |
& *_maskS(i,j,k,bi,bj) |
430 |
ENDDO |
431 |
ENDDO |
432 |
|
433 |
IF (momAdvection) THEN |
434 |
C-- Vertical shear terms (Coriolis) |
435 |
CALL MOM_VI_U_VERTSHEAR(bi,bj,K,uVel,wVel,uCf,myThid) |
436 |
DO j=jMin,jMax |
437 |
DO i=iMin,iMax |
438 |
gU(i,j,k,bi,bj) = (gU(i,j,k,bi,bj)+uCf(i,j)) |
439 |
& *_maskW(i,j,k,bi,bj) |
440 |
ENDDO |
441 |
ENDDO |
442 |
CALL MOM_VI_V_VERTSHEAR(bi,bj,K,vVel,wVel,vCf,myThid) |
443 |
DO j=jMin,jMax |
444 |
DO i=iMin,iMax |
445 |
gV(i,j,k,bi,bj) = (gV(i,j,k,bi,bj)+vCf(i,j)) |
446 |
& *_maskS(i,j,k,bi,bj) |
447 |
ENDDO |
448 |
ENDDO |
449 |
|
450 |
C-- Bernoulli term |
451 |
CALL MOM_VI_U_GRAD_KE(bi,bj,K,KE,uCf,myThid) |
452 |
DO j=jMin,jMax |
453 |
DO i=iMin,iMax |
454 |
gU(i,j,k,bi,bj) = (gU(i,j,k,bi,bj)+uCf(i,j)) |
455 |
& *_maskW(i,j,k,bi,bj) |
456 |
ENDDO |
457 |
ENDDO |
458 |
CALL MOM_VI_V_GRAD_KE(bi,bj,K,KE,vCf,myThid) |
459 |
DO j=jMin,jMax |
460 |
DO i=iMin,iMax |
461 |
gV(i,j,k,bi,bj) = (gV(i,j,k,bi,bj)+vCf(i,j)) |
462 |
& *_maskS(i,j,k,bi,bj) |
463 |
ENDDO |
464 |
ENDDO |
465 |
ENDIF |
466 |
|
467 |
RETURN |
468 |
END |