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C $Header: /u/gcmpack/MITgcm/pkg/mom_fluxform/mom_fluxform.F,v 1.21 2004/10/29 16:25:37 jmc Exp $ |
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C $Name: $ |
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|
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CBOI |
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C !TITLE: pkg/mom\_advdiff |
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C !AUTHORS: adcroft@mit.edu |
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C !INTRODUCTION: Flux-form Momentum Equations Package |
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C |
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C Package "mom\_fluxform" provides methods for calculating explicit terms |
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C in the momentum equation cast in flux-form: |
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C \begin{eqnarray*} |
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C G^u & = & -\frac{1}{\rho} \partial_x \phi_h |
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C -\nabla \cdot {\bf v} u |
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C -fv |
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C +\frac{1}{\rho} \nabla \cdot {\bf \tau}^x |
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C + \mbox{metrics} |
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C \\ |
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C G^v & = & -\frac{1}{\rho} \partial_y \phi_h |
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C -\nabla \cdot {\bf v} v |
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C +fu |
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C +\frac{1}{\rho} \nabla \cdot {\bf \tau}^y |
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C + \mbox{metrics} |
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C \end{eqnarray*} |
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C where ${\bf v}=(u,v,w)$ and $\tau$, the stress tensor, includes surface |
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C stresses as well as internal viscous stresses. |
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CEOI |
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|
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#include "MOM_FLUXFORM_OPTIONS.h" |
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|
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CBOP |
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C !ROUTINE: MOM_FLUXFORM |
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|
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C !INTERFACE: ========================================================== |
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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 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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|
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C !DESCRIPTION: |
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C Calculates all the horizontal accelerations except for the implicit surface |
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C pressure gradient and implciit vertical viscosity. |
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|
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C !USES: =============================================================== |
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C == Global variables == |
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IMPLICIT NONE |
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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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|
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C !INPUT PARAMETERS: =================================================== |
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C bi,bj :: tile indices |
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C iMin,iMax,jMin,jMAx :: loop ranges |
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C k :: vertical level |
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C kUp :: =1 or 2 for consecutive k |
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C kDown :: =2 or 1 for consecutive k |
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C KappaRU :: vertical viscosity |
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C KappaRV :: vertical viscosity |
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C fVerU :: vertical flux of U, 2 1/2 dim for pipe-lining |
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C fVerV :: vertical flux of V, 2 1/2 dim for pipe-lining |
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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 myTime :: current time |
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C myIter :: current time-step number |
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C myThid :: thread number |
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INTEGER bi,bj,iMin,iMax,jMin,jMax |
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INTEGER k,kUp,kDown |
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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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_RL myTime |
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INTEGER myIter |
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INTEGER myThid |
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|
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C !OUTPUT PARAMETERS: ================================================== |
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C None - updates gU() and gV() in common blocks |
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|
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C !LOCAL VARIABLES: ==================================================== |
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C i,j :: loop indices |
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C vF :: viscous flux |
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C v4F :: bi-harmonic viscous flux |
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C cF :: Coriolis acceleration |
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C mT :: Metric terms |
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C fZon :: zonal fluxes |
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C fMer :: meridional fluxes |
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C fVrUp,fVrDw :: vertical viscous fluxes at interface k-1 & k |
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INTEGER i,j |
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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 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 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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_RL fVrUp(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL fVrDw(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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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 uDudxFac, AhDudxFac, etc ... individual term parameters for switching terms off |
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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 rTransU(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL rTransV(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL KE(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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c _RL viscAh_D(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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c _RL viscAh_Z(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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c _RL viscA4_D(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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c _RL viscA4_Z(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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c _RL vort3(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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c _RL hDiv(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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_RL tension(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL uDudxFac |
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_RL AhDudxFac |
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_RL vDudyFac |
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_RL AhDudyFac |
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_RL rVelDudrFac |
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_RL ArDudrFac |
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_RL fuFac |
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_RL mtFacU |
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_RL uDvdxFac |
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_RL AhDvdxFac |
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_RL vDvdyFac |
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_RL AhDvdyFac |
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_RL rVelDvdrFac |
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_RL ArDvdrFac |
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_RL fvFac |
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_RL mtFacV |
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LOGICAL bottomDragTerms |
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CEOP |
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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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v4F(i,j) = 0. |
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cF(i,j) = 0. |
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mT(i,j) = 0. |
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fZon(i,j) = 0. |
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fMer(i,j) = 0. |
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fVrUp(i,j)= 0. |
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fVrDw(i,j)= 0. |
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rTransU(i,j)= 0. |
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rTransV(i,j)= 0. |
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strain(i,j) = 0. |
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tension(i,j)= 0. |
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guDiss(i,j) = 0. |
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gvDiss(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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vDudyFac = afFacMom*1. |
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AhDudyFac = 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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C o V momentum equation |
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uDvdxFac = afFacMom*1. |
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AhDvdxFac = vfFacMom*1. |
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vDvdyFac = afFacMom*1. |
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AhDvdyFac = 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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|
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IF (implicitViscosity) THEN |
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ArDudrFac = 0. |
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ArDvdrFac = 0. |
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ENDIF |
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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-- 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 |
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ENDDO |
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|
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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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IF (bottomDragTerms) THEN |
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CALL MOM_CALC_KE(bi,bj,k,3,uFld,vFld,KE,myThid) |
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ENDIF |
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|
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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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ENDIF |
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|
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C--- First call (k=1): compute vertical adv. flux fVerU(kUp) & fVerV(kUp) |
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IF (momAdvection.AND.k.EQ.1) THEN |
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|
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C- Calculate vertical transports above U & V points (West & South face): |
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CALL MOM_CALC_RTRANS( k, bi, bj, |
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O rTransU, rTransV, |
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I myTime, myIter, myThid) |
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|
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C- Free surface correction term (flux at k=1) |
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CALL MOM_U_ADV_WU( bi,bj,k,uVel,wVel,rTransU, |
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O fVerU(1-OLx,1-OLy,kUp), myThid ) |
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|
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CALL MOM_V_ADV_WV( bi,bj,k,vVel,wVel,rTransV, |
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O fVerV(1-OLx,1-OLy,kUp), myThid ) |
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|
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C--- endif momAdvection & k=1 |
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ENDIF |
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|
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|
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C--- Calculate vertical transports (at k+1) below U & V points : |
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IF (momAdvection) THEN |
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CALL MOM_CALC_RTRANS( k+1, bi, bj, |
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O rTransU, rTransV, |
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I myTime, myIter, myThid) |
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ENDIF |
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|
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c IF (momViscosity) THEN |
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c & CALL MOM_CALC_VISCOSITY(bi,bj,k, |
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c I uFld,vFld, |
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c O viscAh_D,viscAh_Z,myThid) |
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|
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C---+----1----+----2----+----3----+----4----+----5----+----6----+----7-|--+----| |
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|
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C---- Zonal momentum equation starts here |
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|
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IF (momAdvection) THEN |
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C--- Calculate mean fluxes (advection) between cells for zonal flow. |
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|
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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 -> fZon |
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CALL MOM_U_ADV_UU(bi,bj,k,uTrans,uFld,fZon,myThid) |
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|
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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 -> fMer |
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CALL MOM_U_ADV_VU(bi,bj,k,vTrans,uFld,fMer,myThid) |
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|
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C-- Vertical flux (fVer is at upper face of "u" cell) |
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C Mean flow component of vertical flux (at k+1) -> fVer |
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CALL MOM_U_ADV_WU( |
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I bi,bj,k+1,uVel,wVel,rTransU, |
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O fVerU(1-OLx,1-OLy,kDown), myThid ) |
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|
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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) |
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#endif |
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& *( ( fZon(i,j ) - fZon(i-1,j) )*uDudxFac |
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& +( fMer(i,j+1) - fMer(i, j) )*vDudyFac |
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& +(fVerU(i,j,kDown) - fVerU(i,j,kUp))*rkSign*rVelDudrFac |
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& ) |
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ENDDO |
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ENDDO |
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|
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#ifdef NONLIN_FRSURF |
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C-- account for 3.D divergence of the flow in rStar coordinate: |
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IF ( select_rStar.GT.0 ) THEN |
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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) = gU(i,j,k,bi,bj) |
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& - (rStarExpW(i,j,bi,bj) - 1. _d 0)/deltaTfreesurf |
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& *uVel(i,j,k,bi,bj) |
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ENDDO |
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ENDDO |
| 327 |
ENDIF |
| 328 |
IF ( select_rStar.LT.0 ) THEN |
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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) = gU(i,j,k,bi,bj) |
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& - rStarDhWDt(i,j,bi,bj)*uVel(i,j,k,bi,bj) |
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ENDDO |
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ENDDO |
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ENDIF |
| 336 |
#endif /* NONLIN_FRSURF */ |
| 337 |
|
| 338 |
ELSE |
| 339 |
C- if momAdvection / else |
| 340 |
DO j=1-OLy,sNy+OLy |
| 341 |
DO i=1-OLx,sNx+OLx |
| 342 |
gU(i,j,k,bi,bj) = 0. _d 0 |
| 343 |
ENDDO |
| 344 |
ENDDO |
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|
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C- endif momAdvection. |
| 347 |
ENDIF |
| 348 |
|
| 349 |
IF (momViscosity) THEN |
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C--- Calculate eddy fluxes (dissipation) between cells for zonal flow. |
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|
| 352 |
C Bi-harmonic term del^2 U -> v4F |
| 353 |
IF ( viscA4.NE.0. ) |
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& CALL MOM_U_DEL2U(bi,bj,k,uFld,hFacZ,v4f,myThid) |
| 355 |
|
| 356 |
C Laplacian and bi-harmonic terms, Zonal Fluxes -> fZon |
| 357 |
CALL MOM_U_XVISCFLUX(bi,bj,k,uFld,v4F,fZon,myThid) |
| 358 |
|
| 359 |
C Laplacian and bi-harmonic termis, Merid Fluxes -> fMer |
| 360 |
CALL MOM_U_YVISCFLUX(bi,bj,k,uFld,v4F,hFacZ,fMer,myThid) |
| 361 |
|
| 362 |
C Eddy component of vertical flux (interior component only) -> fVrUp & fVrDw |
| 363 |
IF (.NOT.implicitViscosity) THEN |
| 364 |
CALL MOM_U_RVISCFLUX(bi,bj, k, uVel,KappaRU,fVrUp,myThid) |
| 365 |
CALL MOM_U_RVISCFLUX(bi,bj,k+1,uVel,KappaRU,fVrDw,myThid) |
| 366 |
ENDIF |
| 367 |
|
| 368 |
C-- Tendency is minus divergence of the fluxes |
| 369 |
DO j=jMin,jMax |
| 370 |
DO i=iMin,iMax |
| 371 |
guDiss(i,j) = |
| 372 |
#ifdef OLD_UV_GEOM |
| 373 |
& -_recip_hFacW(i,j,k,bi,bj)*recip_drF(k)/ |
| 374 |
& ( 0.5 _d 0*(rA(i,j,bi,bj)+rA(i-1,j,bi,bj)) ) |
| 375 |
#else |
| 376 |
& -_recip_hFacW(i,j,k,bi,bj)*recip_drF(k) |
| 377 |
& *recip_rAw(i,j,bi,bj) |
| 378 |
#endif |
| 379 |
& *( ( fZon(i,j ) - fZon(i-1,j) )*AhDudxFac |
| 380 |
& +( fMer(i,j+1) - fMer(i, j) )*AhDudyFac |
| 381 |
& +( fVrDw(i,j) - fVrUp(i,j) )*rkSign*ArDudrFac |
| 382 |
& ) |
| 383 |
ENDDO |
| 384 |
ENDDO |
| 385 |
|
| 386 |
C-- No-slip and drag BCs appear as body forces in cell abutting topography |
| 387 |
IF (no_slip_sides) THEN |
| 388 |
C- No-slip BCs impose a drag at walls... |
| 389 |
CALL MOM_U_SIDEDRAG(bi,bj,k,uFld,v4F,hFacZ,vF,myThid) |
| 390 |
DO j=jMin,jMax |
| 391 |
DO i=iMin,iMax |
| 392 |
gUdiss(i,j) = gUdiss(i,j) + vF(i,j) |
| 393 |
ENDDO |
| 394 |
ENDDO |
| 395 |
ENDIF |
| 396 |
C- No-slip BCs impose a drag at bottom |
| 397 |
IF (bottomDragTerms) THEN |
| 398 |
CALL MOM_U_BOTTOMDRAG(bi,bj,k,uFld,KE,KappaRU,vF,myThid) |
| 399 |
DO j=jMin,jMax |
| 400 |
DO i=iMin,iMax |
| 401 |
gUdiss(i,j) = gUdiss(i,j) + vF(i,j) |
| 402 |
ENDDO |
| 403 |
ENDDO |
| 404 |
ENDIF |
| 405 |
|
| 406 |
C- endif momViscosity |
| 407 |
ENDIF |
| 408 |
|
| 409 |
C-- Forcing term (moved to timestep.F) |
| 410 |
c IF (momForcing) |
| 411 |
c & CALL EXTERNAL_FORCING_U( |
| 412 |
c I iMin,iMax,jMin,jMax,bi,bj,k, |
| 413 |
c I myTime,myThid) |
| 414 |
|
| 415 |
C-- Metric terms for curvilinear grid systems |
| 416 |
IF (useNHMTerms) THEN |
| 417 |
C o Non-hydrosatic metric terms |
| 418 |
CALL MOM_U_METRIC_NH(bi,bj,k,uFld,wVel,mT,myThid) |
| 419 |
DO j=jMin,jMax |
| 420 |
DO i=iMin,iMax |
| 421 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+mTFacU*mT(i,j) |
| 422 |
ENDDO |
| 423 |
ENDDO |
| 424 |
ENDIF |
| 425 |
IF (usingSphericalPolarMTerms) THEN |
| 426 |
CALL MOM_U_METRIC_SPHERE(bi,bj,k,uFld,vFld,mT,myThid) |
| 427 |
DO j=jMin,jMax |
| 428 |
DO i=iMin,iMax |
| 429 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+mTFacU*mT(i,j) |
| 430 |
ENDDO |
| 431 |
ENDDO |
| 432 |
ENDIF |
| 433 |
IF (usingCylindricalGrid) THEN |
| 434 |
CALL MOM_U_METRIC_CYLINDER(bi,bj,k,uFld,vFld,mT,myThid) |
| 435 |
DO j=jMin,jMax |
| 436 |
DO i=iMin,iMax |
| 437 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+mTFacU*mT(i,j) |
| 438 |
ENDDO |
| 439 |
ENDDO |
| 440 |
ENDIF |
| 441 |
|
| 442 |
C---+----1----+----2----+----3----+----4----+----5----+----6----+----7-|--+----| |
| 443 |
|
| 444 |
C---- Meridional momentum equation starts here |
| 445 |
|
| 446 |
IF (momAdvection) THEN |
| 447 |
C--- Calculate mean fluxes (advection) between cells for meridional flow. |
| 448 |
C Mean flow component of zonal flux -> fZon |
| 449 |
CALL MOM_V_ADV_UV(bi,bj,k,uTrans,vFld,fZon,myThid) |
| 450 |
|
| 451 |
C-- Meridional flux (fMer is at north face of "v" cell) |
| 452 |
C Mean flow component of meridional flux -> fMer |
| 453 |
CALL MOM_V_ADV_VV(bi,bj,k,vTrans,vFld,fMer,myThid) |
| 454 |
|
| 455 |
C-- Vertical flux (fVer is at upper face of "v" cell) |
| 456 |
C Mean flow component of vertical flux (at k+1) -> fVerV |
| 457 |
CALL MOM_V_ADV_WV( |
| 458 |
I bi,bj,k+1,vVel,wVel,rTransV, |
| 459 |
O fVerV(1-OLx,1-OLy,kDown), myThid ) |
| 460 |
|
| 461 |
C-- Tendency is minus divergence of the fluxes + coriolis + pressure term |
| 462 |
DO j=jMin,jMax |
| 463 |
DO i=iMin,iMax |
| 464 |
gV(i,j,k,bi,bj) = |
| 465 |
#ifdef OLD_UV_GEOM |
| 466 |
& -_recip_hFacS(i,j,k,bi,bj)*recip_drF(k)/ |
| 467 |
& ( 0.5 _d 0*(_rA(i,j,bi,bj)+_rA(i,j-1,bi,bj)) ) |
| 468 |
#else |
| 469 |
& -_recip_hFacS(i,j,k,bi,bj)*recip_drF(k) |
| 470 |
& *recip_rAs(i,j,bi,bj) |
| 471 |
#endif |
| 472 |
& *( ( fZon(i+1,j) - fZon(i,j ) )*uDvdxFac |
| 473 |
& +( fMer(i, j) - fMer(i,j-1) )*vDvdyFac |
| 474 |
& +(fVerV(i,j,kDown) - fVerV(i,j,kUp))*rkSign*rVelDvdrFac |
| 475 |
& ) |
| 476 |
ENDDO |
| 477 |
ENDDO |
| 478 |
|
| 479 |
#ifdef NONLIN_FRSURF |
| 480 |
C-- account for 3.D divergence of the flow in rStar coordinate: |
| 481 |
IF ( select_rStar.GT.0 ) THEN |
| 482 |
DO j=jMin,jMax |
| 483 |
DO i=iMin,iMax |
| 484 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj) |
| 485 |
& - (rStarExpS(i,j,bi,bj) - 1. _d 0)/deltaTfreesurf |
| 486 |
& *vVel(i,j,k,bi,bj) |
| 487 |
ENDDO |
| 488 |
ENDDO |
| 489 |
ENDIF |
| 490 |
IF ( select_rStar.LT.0 ) THEN |
| 491 |
DO j=jMin,jMax |
| 492 |
DO i=iMin,iMax |
| 493 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj) |
| 494 |
& - rStarDhSDt(i,j,bi,bj)*vVel(i,j,k,bi,bj) |
| 495 |
ENDDO |
| 496 |
ENDDO |
| 497 |
ENDIF |
| 498 |
#endif /* NONLIN_FRSURF */ |
| 499 |
|
| 500 |
ELSE |
| 501 |
C- if momAdvection / else |
| 502 |
DO j=1-OLy,sNy+OLy |
| 503 |
DO i=1-OLx,sNx+OLx |
| 504 |
gV(i,j,k,bi,bj) = 0. _d 0 |
| 505 |
ENDDO |
| 506 |
ENDDO |
| 507 |
|
| 508 |
C- endif momAdvection. |
| 509 |
ENDIF |
| 510 |
|
| 511 |
IF (momViscosity) THEN |
| 512 |
C--- Calculate eddy fluxes (dissipation) between cells for meridional flow. |
| 513 |
C Bi-harmonic term del^2 V -> v4F |
| 514 |
IF ( viscA4.NE.0. ) |
| 515 |
& CALL MOM_V_DEL2V(bi,bj,k,vFld,hFacZ,v4f,myThid) |
| 516 |
|
| 517 |
C Laplacian and bi-harmonic terms, Zonal Fluxes -> fZon |
| 518 |
CALL MOM_V_XVISCFLUX(bi,bj,k,vFld,v4f,hFacZ,fZon,myThid) |
| 519 |
|
| 520 |
C Laplacian and bi-harmonic termis, Merid Fluxes -> fMer |
| 521 |
CALL MOM_V_YVISCFLUX(bi,bj,k,vFld,v4f,fMer,myThid) |
| 522 |
|
| 523 |
C Eddy component of vertical flux (interior component only) -> fVrUp & fVrDw |
| 524 |
IF (.NOT.implicitViscosity) THEN |
| 525 |
CALL MOM_V_RVISCFLUX(bi,bj, k, vVel,KappaRV,fVrUp,myThid) |
| 526 |
CALL MOM_V_RVISCFLUX(bi,bj,k+1,vVel,KappaRV,fVrDw,myThid) |
| 527 |
ENDIF |
| 528 |
|
| 529 |
C-- Tendency is minus divergence of the fluxes + coriolis + pressure term |
| 530 |
DO j=jMin,jMax |
| 531 |
DO i=iMin,iMax |
| 532 |
gvDiss(i,j) = |
| 533 |
#ifdef OLD_UV_GEOM |
| 534 |
& -_recip_hFacS(i,j,k,bi,bj)*recip_drF(k)/ |
| 535 |
& ( 0.5 _d 0*(_rA(i,j,bi,bj)+_rA(i,j-1,bi,bj)) ) |
| 536 |
#else |
| 537 |
& -_recip_hFacS(i,j,k,bi,bj)*recip_drF(k) |
| 538 |
& *recip_rAs(i,j,bi,bj) |
| 539 |
#endif |
| 540 |
& *( ( fZon(i+1,j) - fZon(i,j ) )*AhDvdxFac |
| 541 |
& +( fMer(i, j) - fMer(i,j-1) )*AhDvdyFac |
| 542 |
& +( fVrDw(i,j) - fVrUp(i,j) )*rkSign*ArDvdrFac |
| 543 |
& ) |
| 544 |
ENDDO |
| 545 |
ENDDO |
| 546 |
|
| 547 |
C-- No-slip and drag BCs appear as body forces in cell abutting topography |
| 548 |
IF (no_slip_sides) THEN |
| 549 |
C- No-slip BCs impose a drag at walls... |
| 550 |
CALL MOM_V_SIDEDRAG(bi,bj,k,vFld,v4F,hFacZ,vF,myThid) |
| 551 |
DO j=jMin,jMax |
| 552 |
DO i=iMin,iMax |
| 553 |
gvDiss(i,j) = gvDiss(i,j) + vF(i,j) |
| 554 |
ENDDO |
| 555 |
ENDDO |
| 556 |
ENDIF |
| 557 |
C- No-slip BCs impose a drag at bottom |
| 558 |
IF (bottomDragTerms) THEN |
| 559 |
CALL MOM_V_BOTTOMDRAG(bi,bj,k,vFld,KE,KappaRV,vF,myThid) |
| 560 |
DO j=jMin,jMax |
| 561 |
DO i=iMin,iMax |
| 562 |
gvDiss(i,j) = gvDiss(i,j) + vF(i,j) |
| 563 |
ENDDO |
| 564 |
ENDDO |
| 565 |
ENDIF |
| 566 |
|
| 567 |
C- endif momViscosity |
| 568 |
ENDIF |
| 569 |
|
| 570 |
C-- Forcing term (moved to timestep.F) |
| 571 |
c IF (momForcing) |
| 572 |
c & CALL EXTERNAL_FORCING_V( |
| 573 |
c I iMin,iMax,jMin,jMax,bi,bj,k, |
| 574 |
c I myTime,myThid) |
| 575 |
|
| 576 |
C-- Metric terms for curvilinear grid systems |
| 577 |
IF (useNHMTerms) THEN |
| 578 |
C o Spherical polar grid metric terms |
| 579 |
CALL MOM_V_METRIC_NH(bi,bj,k,vFld,wVel,mT,myThid) |
| 580 |
DO j=jMin,jMax |
| 581 |
DO i=iMin,iMax |
| 582 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+mTFacV*mT(i,j) |
| 583 |
ENDDO |
| 584 |
ENDDO |
| 585 |
ENDIF |
| 586 |
IF (usingSphericalPolarMTerms) THEN |
| 587 |
CALL MOM_V_METRIC_SPHERE(bi,bj,k,uFld,mT,myThid) |
| 588 |
DO j=jMin,jMax |
| 589 |
DO i=iMin,iMax |
| 590 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+mTFacV*mT(i,j) |
| 591 |
ENDDO |
| 592 |
ENDDO |
| 593 |
ENDIF |
| 594 |
IF (usingCylindricalGrid) THEN |
| 595 |
CALL MOM_V_METRIC_CYLINDER(bi,bj,k,uFld,vFld,mT,myThid) |
| 596 |
DO j=jMin,jMax |
| 597 |
DO i=iMin,iMax |
| 598 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+mTFacV*mT(i,j) |
| 599 |
ENDDO |
| 600 |
ENDDO |
| 601 |
ENDIF |
| 602 |
|
| 603 |
C---+----1----+----2----+----3----+----4----+----5----+----6----+----7-|--+----| |
| 604 |
|
| 605 |
C-- Coriolis term |
| 606 |
C Note. As coded here, coriolis will not work with "thin walls" |
| 607 |
c IF (useCDscheme) THEN |
| 608 |
c CALL MOM_CDSCHEME(bi,bj,k,dPhiHydX,dPhiHydY,myThid) |
| 609 |
c ELSE |
| 610 |
IF (.NOT.useCDscheme) THEN |
| 611 |
CALL MOM_U_CORIOLIS(bi,bj,k,vFld,cf,myThid) |
| 612 |
DO j=jMin,jMax |
| 613 |
DO i=iMin,iMax |
| 614 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+fuFac*cf(i,j) |
| 615 |
ENDDO |
| 616 |
ENDDO |
| 617 |
CALL MOM_V_CORIOLIS(bi,bj,k,uFld,cf,myThid) |
| 618 |
DO j=jMin,jMax |
| 619 |
DO i=iMin,iMax |
| 620 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+fvFac*cf(i,j) |
| 621 |
ENDDO |
| 622 |
ENDDO |
| 623 |
ENDIF |
| 624 |
|
| 625 |
IF (nonHydrostatic.OR.quasiHydrostatic) THEN |
| 626 |
CALL MOM_U_CORIOLIS_NH(bi,bj,k,wVel,cf,myThid) |
| 627 |
DO j=jMin,jMax |
| 628 |
DO i=iMin,iMax |
| 629 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+fuFac*cf(i,j) |
| 630 |
ENDDO |
| 631 |
ENDDO |
| 632 |
ENDIF |
| 633 |
|
| 634 |
C-- Set du/dt & dv/dt on boundaries to zero |
| 635 |
DO j=jMin,jMax |
| 636 |
DO i=iMin,iMax |
| 637 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)*_maskW(i,j,k,bi,bj) |
| 638 |
guDiss(i,j) = guDiss(i,j) *_maskW(i,j,k,bi,bj) |
| 639 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)*_maskS(i,j,k,bi,bj) |
| 640 |
gvDiss(i,j) = gvDiss(i,j) *_maskS(i,j,k,bi,bj) |
| 641 |
ENDDO |
| 642 |
ENDDO |
| 643 |
|
| 644 |
RETURN |
| 645 |
END |
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