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adcroft |
1.1 |
C $Header: $ |
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C $Name: $ |
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#include "CPP_OPTIONS.h" |
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SUBROUTINE MOM_FLUXFORM( |
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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_FLUXFORM | |
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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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C == Global variables == |
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#include "SIZE.h" |
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#include "DYNVARS.h" |
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#include "FFIELDS.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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#include "SURFACE.h" |
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C == Routine arguments == |
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C fZon - Work array for flux of momentum in the east-west |
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C direction at the west face of a cell. |
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C fMer - Work array for flux of momentum in the north-south |
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C direction at the south face of a cell. |
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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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C == Local variables == |
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C ab15, ab05 - Weights for Adams-Bashforth time stepping scheme. |
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C i,j,k - Loop counters |
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C wMaskOverride - Land sea flag override for top layer. |
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C afFacMom - Tracer parameters for turning terms |
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C vfFacMom on and off. |
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C pfFacMom afFacMom - Advective terms |
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C cfFacMom vfFacMom - Eddy viscosity terms |
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C mTFacMom pfFacMom - Pressure terms |
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C cfFacMom - Coriolis terms |
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C foFacMom - Forcing |
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C mTFacMom - Metric term |
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C vF - Temporary holding viscous term (Laplacian) |
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C v4F - Temporary holding viscous term (Biharmonic) |
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C cF - Temporary holding coriolis term. |
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C mT - Temporary holding metric terms(s). |
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C pF - Temporary holding pressure|potential gradient terms. |
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C uDudxFac, AhDudxFac, etc ... individual term tracer parameters |
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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 v4F(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 cF (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 fZon (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL fMer (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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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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C ab05, ab15 - Adams-Bashforth time-stepping weights. |
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_RL ab05, ab15 |
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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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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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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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v4F(i,j) = 0. |
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vrF(i,j) = 0. |
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cF(i,j) = 0. |
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mT(i,j) = 0. |
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pF(i,j) = 0. |
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fZon(i,j) = 0. |
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fMer(i,j) = 0. |
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ENDDO |
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ENDDO |
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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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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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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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C-- Adams-Bashforth weighting factors |
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ab15 = 1.5 _d 0 + abEps |
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ab05 = -0.5 _d 0 - abEps |
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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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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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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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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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CALL MOM_CALC_KE(bi,bj,k,uFld,vFld,KE,myThid) |
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C---- Zonal momentum equation starts here |
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C Bi-harmonic term del^2 U -> v4F |
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IF (momViscosity) |
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& CALL MOM_U_DEL2U(bi,bj,k,uFld,hFacZ,v4f,myThid) |
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C--- Calculate mean and eddy fluxes between cells for zonal flow. |
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C-- Zonal flux (fZon is at east face of "u" cell) |
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C Mean flow component of zonal flux -> aF |
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IF (momAdvection) |
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& CALL MOM_U_ADV_UU(bi,bj,k,uTrans,uFld,aF,myThid) |
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C Laplacian and bi-harmonic terms -> vF |
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IF (momViscosity) |
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& CALL MOM_U_XVISCFLUX(bi,bj,k,uFld,v4F,vF,myThid) |
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C Combine fluxes -> fZon |
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DO j=jMin,jMax |
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DO i=iMin,iMax |
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fZon(i,j) = uDudxFac*aF(i,j) + AhDudxFac*vF(i,j) |
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ENDDO |
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ENDDO |
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C-- Meridional flux (fMer is at south face of "u" cell) |
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C Mean flow component of meridional flux |
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IF (momAdvection) |
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& CALL MOM_U_ADV_VU(bi,bj,k,vTrans,uFld,aF,myThid) |
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C Laplacian and bi-harmonic term |
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IF (momViscosity) |
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& CALL MOM_U_YVISCFLUX(bi,bj,k,uFld,v4F,hFacZ,vF,myThid) |
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C Combine fluxes -> fMer |
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DO j=jMin,jMax |
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DO i=iMin,iMax |
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fMer(i,j) = vDudyFac*aF(i,j) + AhDudyFac*vF(i,j) |
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ENDDO |
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ENDDO |
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C-- Vertical flux (fVer is at upper face of "u" cell) |
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C-- Free surface correction term (flux at k=1) |
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IF (momAdvection.AND.k.EQ.1) THEN |
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CALL MOM_U_ADV_WU(bi,bj,k,uVel,wVel,af,myThid) |
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DO j=jMin,jMax |
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DO i=iMin,iMax |
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fVerU(i,j,kUp) = af(i,j) |
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ENDDO |
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ENDDO |
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ENDIF |
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C Mean flow component of vertical flux (at k+1) -> aF |
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IF (momAdvection) |
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& CALL MOM_U_ADV_WU(bi,bj,k+1,uVel,wVel,af,myThid) |
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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) |
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C Combine fluxes |
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DO j=jMin,jMax |
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DO i=iMin,iMax |
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fVerU(i,j,kDown) = rVelDudrFac*aF(i,j) + ArDudrFac*vrF(i,j) |
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ENDDO |
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ENDDO |
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C--- Hydrostatic term ( -1/rhoConst . dphi/dx ) |
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IF (momPressureForcing) THEN |
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DO j=jMin,jMax |
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DO i=iMin,iMax |
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pf(i,j) = - _recip_dxC(i,j,bi,bj) |
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& *(phi_hyd(i,j,k)-phi_hyd(i-1,j,k)) |
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ENDDO |
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ENDDO |
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ENDIF |
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C-- Tendency is minus divergence of the fluxes + coriolis + pressure term |
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DO j=jMin,jMax |
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DO i=iMin,iMax |
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gU(i,j,k,bi,bj) = |
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#ifdef OLD_UV_GEOM |
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& -_recip_hFacW(i,j,k,bi,bj)*recip_drF(k)/ |
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& ( 0.5 _d 0*(rA(i,j,bi,bj)+rA(i-1,j,bi,bj)) ) |
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#else |
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& -_recip_hFacW(i,j,k,bi,bj)*recip_drF(k) |
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& *recip_rAw(i,j,bi,bj) |
| 320 |
|
|
#endif |
| 321 |
|
|
& *(fZon(i,j ) - fZon(i-1,j) |
| 322 |
|
|
& +fMer(i,j+1) - fMer(i ,j) |
| 323 |
|
|
& +fVerU(i,j,kUp)*rkFac - fVerU(i,j,kDown)*rkFac |
| 324 |
|
|
& ) |
| 325 |
|
|
& _PHM( +phxFac * pf(i,j) ) |
| 326 |
|
|
ENDDO |
| 327 |
|
|
ENDDO |
| 328 |
|
|
|
| 329 |
|
|
C-- No-slip and drag BCs appear as body forces in cell abutting topography |
| 330 |
|
|
IF (momViscosity.AND.no_slip_sides) THEN |
| 331 |
|
|
C- No-slip BCs impose a drag at walls... |
| 332 |
|
|
CALL MOM_U_SIDEDRAG(bi,bj,k,uFld,v4F,hFacZ,vF,myThid) |
| 333 |
|
|
DO j=jMin,jMax |
| 334 |
|
|
DO i=iMin,iMax |
| 335 |
|
|
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+vF(i,j) |
| 336 |
|
|
ENDDO |
| 337 |
|
|
ENDDO |
| 338 |
|
|
ENDIF |
| 339 |
|
|
C- No-slip BCs impose a drag at bottom |
| 340 |
|
|
IF (momViscosity.AND.bottomDragTerms) THEN |
| 341 |
|
|
CALL MOM_U_BOTTOMDRAG(bi,bj,k,uFld,KE,KappaRU,vF,myThid) |
| 342 |
|
|
DO j=jMin,jMax |
| 343 |
|
|
DO i=iMin,iMax |
| 344 |
|
|
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+vF(i,j) |
| 345 |
|
|
ENDDO |
| 346 |
|
|
ENDDO |
| 347 |
|
|
ENDIF |
| 348 |
|
|
|
| 349 |
|
|
C-- Forcing term |
| 350 |
|
|
IF (momForcing) |
| 351 |
|
|
& CALL EXTERNAL_FORCING_U( |
| 352 |
|
|
I iMin,iMax,jMin,jMax,bi,bj,k, |
| 353 |
|
|
I myCurrentTime,myThid) |
| 354 |
|
|
|
| 355 |
|
|
C-- Metric terms for curvilinear grid systems |
| 356 |
|
|
IF (usingSphericalPolarMTerms) THEN |
| 357 |
|
|
C o Spherical polar grid metric terms |
| 358 |
|
|
CALL MOM_U_METRIC_NH(bi,bj,k,uFld,wVel,mT,myThid) |
| 359 |
|
|
DO j=jMin,jMax |
| 360 |
|
|
DO i=iMin,iMax |
| 361 |
|
|
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+mTFacU*mT(i,j) |
| 362 |
|
|
ENDDO |
| 363 |
|
|
ENDDO |
| 364 |
|
|
CALL MOM_U_METRIC_SPHERE(bi,bj,k,uFld,vFld,mT,myThid) |
| 365 |
|
|
DO j=jMin,jMax |
| 366 |
|
|
DO i=iMin,iMax |
| 367 |
|
|
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+mTFacU*mT(i,j) |
| 368 |
|
|
ENDDO |
| 369 |
|
|
ENDDO |
| 370 |
|
|
ENDIF |
| 371 |
|
|
|
| 372 |
|
|
C-- Set du/dt on boundaries to zero |
| 373 |
|
|
DO j=jMin,jMax |
| 374 |
|
|
DO i=iMin,iMax |
| 375 |
|
|
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)*_maskW(i,j,k,bi,bj) |
| 376 |
|
|
ENDDO |
| 377 |
|
|
ENDDO |
| 378 |
|
|
|
| 379 |
|
|
|
| 380 |
|
|
C---- Meridional momentum equation starts here |
| 381 |
|
|
|
| 382 |
|
|
C Bi-harmonic term del^2 V -> v4F |
| 383 |
|
|
IF (momViscosity) |
| 384 |
|
|
& CALL MOM_V_DEL2V(bi,bj,k,vFld,hFacZ,v4f,myThid) |
| 385 |
|
|
|
| 386 |
|
|
C--- Calculate mean and eddy fluxes between cells for meridional flow. |
| 387 |
|
|
|
| 388 |
|
|
C-- Zonal flux (fZon is at west face of "v" cell) |
| 389 |
|
|
|
| 390 |
|
|
C Mean flow component of zonal flux -> aF |
| 391 |
|
|
IF (momAdvection) |
| 392 |
|
|
& CALL MOM_V_ADV_UV(bi,bj,k,uTrans,vFld,af,myThid) |
| 393 |
|
|
|
| 394 |
|
|
C Laplacian and bi-harmonic terms -> vF |
| 395 |
|
|
IF (momViscosity) |
| 396 |
|
|
& CALL MOM_V_XVISCFLUX(bi,bj,k,vFld,v4f,hFacZ,vf,myThid) |
| 397 |
|
|
|
| 398 |
|
|
C Combine fluxes -> fZon |
| 399 |
|
|
DO j=jMin,jMax |
| 400 |
|
|
DO i=iMin,iMax |
| 401 |
|
|
fZon(i,j) = uDvdxFac*aF(i,j) + AhDvdxFac*vF(i,j) |
| 402 |
|
|
ENDDO |
| 403 |
|
|
ENDDO |
| 404 |
|
|
|
| 405 |
|
|
C-- Meridional flux (fMer is at north face of "v" cell) |
| 406 |
|
|
|
| 407 |
|
|
C Mean flow component of meridional flux |
| 408 |
|
|
IF (momAdvection) |
| 409 |
|
|
& CALL MOM_V_ADV_VV(bi,bj,k,vTrans,vFld,af,myThid) |
| 410 |
|
|
|
| 411 |
|
|
C Laplacian and bi-harmonic term |
| 412 |
|
|
IF (momViscosity) |
| 413 |
|
|
& CALL MOM_V_YVISCFLUX(bi,bj,k,vFld,v4f,vf,myThid) |
| 414 |
|
|
|
| 415 |
|
|
C Combine fluxes -> fMer |
| 416 |
|
|
DO j=jMin,jMax |
| 417 |
|
|
DO i=iMin,iMax |
| 418 |
|
|
fMer(i,j) = vDvdyFac*aF(i,j) + AhDvdyFac*vF(i,j) |
| 419 |
|
|
ENDDO |
| 420 |
|
|
ENDDO |
| 421 |
|
|
|
| 422 |
|
|
C-- Vertical flux (fVer is at upper face of "v" cell) |
| 423 |
|
|
|
| 424 |
|
|
C-- Free surface correction term (flux at k=1) |
| 425 |
|
|
IF (momAdvection.AND.k.EQ.1) THEN |
| 426 |
|
|
CALL MOM_V_ADV_WV(bi,bj,k,vVel,wVel,af,myThid) |
| 427 |
|
|
DO j=jMin,jMax |
| 428 |
|
|
DO i=iMin,iMax |
| 429 |
|
|
fVerV(i,j,kUp) = af(i,j) |
| 430 |
|
|
ENDDO |
| 431 |
|
|
ENDDO |
| 432 |
|
|
ENDIF |
| 433 |
|
|
C o Mean flow component of vertical flux |
| 434 |
|
|
IF (momAdvection) |
| 435 |
|
|
& CALL MOM_V_ADV_WV(bi,bj,k+1,vVel,wVel,af,myThid) |
| 436 |
|
|
|
| 437 |
|
|
C Eddy component of vertical flux (interior component only) -> vrF |
| 438 |
|
|
IF (momViscosity.AND..NOT.implicitViscosity) |
| 439 |
|
|
& CALL MOM_V_RVISCFLUX(bi,bj,k,vVel,KappaRV,vrf,myThid) |
| 440 |
|
|
|
| 441 |
|
|
C Combine fluxes -> fVerV |
| 442 |
|
|
DO j=jMin,jMax |
| 443 |
|
|
DO i=iMin,iMax |
| 444 |
|
|
fVerV(i,j,kDown) = rVelDvdrFac*aF(i,j) + ArDvdrFac*vrF(i,j) |
| 445 |
|
|
ENDDO |
| 446 |
|
|
ENDDO |
| 447 |
|
|
|
| 448 |
|
|
C--- Hydorstatic term (-1/rhoConst . dphi/dy ) |
| 449 |
|
|
IF (momPressureForcing) THEN |
| 450 |
|
|
DO j=jMin,jMax |
| 451 |
|
|
DO i=iMin,iMax |
| 452 |
|
|
pF(i,j) = -_recip_dyC(i,j,bi,bj) |
| 453 |
|
|
& *(phi_hyd(i,j,k)-phi_hyd(i,j-1,k)) |
| 454 |
|
|
ENDDO |
| 455 |
|
|
ENDDO |
| 456 |
|
|
ENDIF |
| 457 |
|
|
|
| 458 |
|
|
C-- Tendency is minus divergence of the fluxes + coriolis + pressure term |
| 459 |
|
|
DO j=jMin,jMax |
| 460 |
|
|
DO i=iMin,iMax |
| 461 |
|
|
gV(i,j,k,bi,bj) = |
| 462 |
|
|
#ifdef OLD_UV_GEOM |
| 463 |
|
|
& -_recip_hFacS(i,j,k,bi,bj)*recip_drF(k)/ |
| 464 |
|
|
& ( 0.5 _d 0*(_rA(i,j,bi,bj)+_rA(i,j-1,bi,bj)) ) |
| 465 |
|
|
#else |
| 466 |
|
|
& -_recip_hFacS(i,j,k,bi,bj)*recip_drF(k) |
| 467 |
|
|
& *recip_rAs(i,j,bi,bj) |
| 468 |
|
|
#endif |
| 469 |
|
|
& *(fZon(i+1,j) - fZon(i,j ) |
| 470 |
|
|
& +fMer(i,j ) - fMer(i,j-1) |
| 471 |
|
|
& +fVerV(i,j,kUp)*rkFac - fVerV(i,j,kDown)*rkFac |
| 472 |
|
|
& ) |
| 473 |
|
|
& _PHM( +phyFac*pf(i,j) ) |
| 474 |
|
|
ENDDO |
| 475 |
|
|
ENDDO |
| 476 |
|
|
|
| 477 |
|
|
C-- No-slip and drag BCs appear as body forces in cell abutting topography |
| 478 |
|
|
IF (momViscosity.AND.no_slip_sides) THEN |
| 479 |
|
|
C- No-slip BCs impose a drag at walls... |
| 480 |
|
|
CALL MOM_V_SIDEDRAG(bi,bj,k,vFld,v4F,hFacZ,vF,myThid) |
| 481 |
|
|
DO j=jMin,jMax |
| 482 |
|
|
DO i=iMin,iMax |
| 483 |
|
|
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vF(i,j) |
| 484 |
|
|
ENDDO |
| 485 |
|
|
ENDDO |
| 486 |
|
|
ENDIF |
| 487 |
|
|
C- No-slip BCs impose a drag at bottom |
| 488 |
|
|
IF (momViscosity.AND.bottomDragTerms) THEN |
| 489 |
|
|
CALL MOM_V_BOTTOMDRAG(bi,bj,k,vFld,KE,KappaRV,vF,myThid) |
| 490 |
|
|
DO j=jMin,jMax |
| 491 |
|
|
DO i=iMin,iMax |
| 492 |
|
|
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vF(i,j) |
| 493 |
|
|
ENDDO |
| 494 |
|
|
ENDDO |
| 495 |
|
|
ENDIF |
| 496 |
|
|
|
| 497 |
|
|
C-- Forcing term |
| 498 |
|
|
IF (momForcing) |
| 499 |
|
|
& CALL EXTERNAL_FORCING_V( |
| 500 |
|
|
I iMin,iMax,jMin,jMax,bi,bj,k, |
| 501 |
|
|
I myCurrentTime,myThid) |
| 502 |
|
|
|
| 503 |
|
|
C-- Metric terms for curvilinear grid systems |
| 504 |
|
|
IF (usingSphericalPolarMTerms) THEN |
| 505 |
|
|
C o Spherical polar grid metric terms |
| 506 |
|
|
CALL MOM_V_METRIC_NH(bi,bj,k,vFld,wVel,mT,myThid) |
| 507 |
|
|
DO j=jMin,jMax |
| 508 |
|
|
DO i=iMin,iMax |
| 509 |
|
|
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+mTFacV*mT(i,j) |
| 510 |
|
|
ENDDO |
| 511 |
|
|
ENDDO |
| 512 |
|
|
CALL MOM_V_METRIC_SPHERE(bi,bj,k,uFld,mT,myThid) |
| 513 |
|
|
DO j=jMin,jMax |
| 514 |
|
|
DO i=iMin,iMax |
| 515 |
|
|
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+mTFacV*mT(i,j) |
| 516 |
|
|
ENDDO |
| 517 |
|
|
ENDDO |
| 518 |
|
|
ENDIF |
| 519 |
|
|
|
| 520 |
|
|
C-- Set dv/dt on boundaries to zero |
| 521 |
|
|
DO j=jMin,jMax |
| 522 |
|
|
DO i=iMin,iMax |
| 523 |
|
|
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)*_maskS(i,j,k,bi,bj) |
| 524 |
|
|
ENDDO |
| 525 |
|
|
ENDDO |
| 526 |
|
|
|
| 527 |
|
|
C-- Coriolis term |
| 528 |
|
|
C Note. As coded here, coriolis will not work with "thin walls" |
| 529 |
|
|
#ifdef INCLUDE_CD_CODE |
| 530 |
|
|
CALL MOM_CDSCHEME(bi,bj,k,phi_hyd,myThid) |
| 531 |
|
|
#else |
| 532 |
|
|
CALL MOM_U_CORIOLIS(bi,bj,k,vFld,cf,myThid) |
| 533 |
|
|
DO j=jMin,jMax |
| 534 |
|
|
DO i=iMin,iMax |
| 535 |
|
|
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+fuFac*cf(i,j) |
| 536 |
|
|
ENDDO |
| 537 |
|
|
ENDDO |
| 538 |
|
|
CALL MOM_V_CORIOLIS(bi,bj,k,uFld,cf,myThid) |
| 539 |
|
|
DO j=jMin,jMax |
| 540 |
|
|
DO i=iMin,iMax |
| 541 |
|
|
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+fvFac*cf(i,j) |
| 542 |
|
|
ENDDO |
| 543 |
|
|
ENDDO |
| 544 |
|
|
#endif /* INCLUDE_CD_CODE */ |
| 545 |
|
|
|
| 546 |
|
|
RETURN |
| 547 |
|
|
END |
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