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C $Header: /u/gcmpack/MITgcm/pkg/mom_fluxform/mom_fluxform.F,v 1.54 2015/01/03 23:57:57 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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#ifdef ALLOW_AUTODIFF |
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# include "AUTODIFF_OPTIONS.h" |
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#endif |
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#ifdef ALLOW_MOM_COMMON |
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# include "MOM_COMMON_OPTIONS.h" |
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#endif |
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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,k,iMin,iMax,jMin,jMax, |
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I kappaRU, kappaRV, |
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U fVerUkm, fVerVkm, |
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O fVerUkp, fVerVkp, |
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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 implicit 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 "EEPARAMS.h" |
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#include "PARAMS.h" |
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#include "GRID.h" |
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#include "DYNVARS.h" |
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#include "FFIELDS.h" |
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#include "SURFACE.h" |
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#ifdef ALLOW_MOM_COMMON |
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# include "MOM_VISC.h" |
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#endif |
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#ifdef ALLOW_AUTODIFF |
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# include "tamc.h" |
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# include "tamc_keys.h" |
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# include "MOM_FLUXFORM.h" |
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#endif |
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|
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C !INPUT PARAMETERS: =================================================== |
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C bi,bj :: current tile indices |
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C k :: current vertical level |
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C iMin,iMax,jMin,jMax :: loop ranges |
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C kappaRU :: vertical viscosity |
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C kappaRV :: vertical viscosity |
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C fVerUkm :: vertical advective flux of U, interface above (k-1/2) |
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C fVerVkm :: vertical advective flux of V, interface above (k-1/2) |
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C fVerUkp :: vertical advective flux of U, interface below (k+1/2) |
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C fVerVkp :: vertical advective flux of V, interface below (k+1/2) |
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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 :: my Thread Id number |
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INTEGER bi,bj,k |
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INTEGER iMin,iMax,jMin,jMax |
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_RL kappaRU(1-OLx:sNx+OLx,1-OLy:sNy+OLy,Nr+1) |
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_RL kappaRV(1-OLx:sNx+OLx,1-OLy:sNy+OLy,Nr+1) |
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_RL fVerUkm(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL fVerVkm(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL fVerUkp(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL fVerVkp(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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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 & k+1 |
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INTEGER i,j |
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#ifdef ALLOW_AUTODIFF_TAMC |
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INTEGER imomkey |
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#endif |
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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 on and off. |
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C vfFacMom |
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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 h0FacZ(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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_RL viscAh_D(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL viscAh_Z(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL viscA4_D(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL viscA4_Z(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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_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 mtNHFacU |
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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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_RL mtNHFacV |
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_RL sideMaskFac |
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LOGICAL bottomDragTerms |
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CEOP |
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#ifdef MOM_BOUNDARY_CONSERVE |
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COMMON / MOM_FLUXFORM_LOCAL / uBnd, vBnd |
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_RL uBnd(1-OLx:sNx+OLx,1-OLy:sNy+OLy,Nr,nSx,nSy) |
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_RL vBnd(1-OLx:sNx+OLx,1-OLy:sNy+OLy,Nr,nSx,nSy) |
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#endif /* MOM_BOUNDARY_CONSERVE */ |
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|
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#ifdef ALLOW_AUTODIFF_TAMC |
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act0 = k - 1 |
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max0 = Nr |
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act1 = bi - myBxLo(myThid) |
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max1 = myBxHi(myThid) - myBxLo(myThid) + 1 |
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act2 = bj - myByLo(myThid) |
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max2 = myByHi(myThid) - myByLo(myThid) + 1 |
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act3 = myThid - 1 |
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max3 = nTx*nTy |
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act4 = ikey_dynamics - 1 |
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imomkey = (act0 + 1) |
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& + act1*max0 |
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& + act2*max0*max1 |
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& + act3*max0*max1*max2 |
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& + act4*max0*max1*max2*max3 |
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#endif /* ALLOW_AUTODIFF_TAMC */ |
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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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c KE(i,j) = 0. |
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hDiv(i,j) = 0. |
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vort3(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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mtNHFacU = 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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mtNHFacV = 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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C note: using standard stencil (no mask) results in under-estimating |
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C vorticity at a no-slip boundary by a factor of 2 = sideDragFactor |
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IF ( no_slip_sides ) THEN |
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sideMaskFac = sideDragFactor |
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ELSE |
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sideMaskFac = 0. _d 0 |
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ENDIF |
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|
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IF ( selectImplicitDrag.EQ.0 .AND. |
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& ( no_slip_bottom |
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& .OR. selectBotDragQuadr.GE.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)*deepFacC(k) |
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& *drF(k)*_hFacW(i,j,k,bi,bj) |
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yA(i,j) = _dxG(i,j,bi,bj)*deepFacC(k) |
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& *drF(k)*_hFacS(i,j,k,bi,bj) |
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h0FacZ(i,j) = hFacZ(i,j) |
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ENDDO |
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ENDDO |
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#ifdef NONLIN_FRSURF |
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IF ( momViscosity .AND. no_slip_sides |
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& .AND. nonlinFreeSurf.GT.0 ) THEN |
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DO j=2-OLy,sNy+OLy |
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DO i=2-OLx,sNx+OLx |
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h0FacZ(i,j) = MIN( |
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& MIN( h0FacW(i,j,k,bi,bj), h0FacW(i,j-1,k,bi,bj) ), |
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& MIN( h0FacS(i,j,k,bi,bj), h0FacS(i-1,j,k,bi,bj) ) ) |
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ENDDO |
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ENDDO |
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ENDIF |
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#endif /* NONLIN_FRSURF */ |
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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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C anelastic: transports are scaled by rhoFacC (~ mass transport) |
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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)*rhoFacC(k) |
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vTrans(i,j) = vFld(i,j)*yA(i,j)*rhoFacC(k) |
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ENDDO |
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ENDDO |
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|
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CALL MOM_CALC_KE( bi,bj,k,2,uFld,vFld,KE,myThid ) |
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IF ( useVariableVisc ) THEN |
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CALL MOM_CALC_HDIV( bi,bj,k,2,uFld,vFld,hDiv,myThid ) |
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CALL MOM_CALC_RELVORT3( bi,bj,k,uFld,vFld,hFacZ,vort3,myThid ) |
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CALL MOM_CALC_TENSION( bi,bj,k,uFld,vFld,tension,myThid ) |
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CALL MOM_CALC_STRAIN( bi,bj,k,uFld,vFld,hFacZ,strain,myThid ) |
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DO j=1-OLy,sNy+OLy |
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DO i=1-OLx,sNx+OLx |
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IF ( hFacZ(i,j).EQ.0. ) THEN |
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vort3(i,j) = sideMaskFac*vort3(i,j) |
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strain(i,j) = sideMaskFac*strain(i,j) |
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ENDIF |
320 |
ENDDO |
321 |
ENDDO |
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#ifdef ALLOW_DIAGNOSTICS |
323 |
IF ( useDiagnostics ) THEN |
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CALL DIAGNOSTICS_FILL(hDiv, 'momHDiv ',k,1,2,bi,bj,myThid) |
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CALL DIAGNOSTICS_FILL(vort3, 'momVort3',k,1,2,bi,bj,myThid) |
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CALL DIAGNOSTICS_FILL(tension,'Tension ',k,1,2,bi,bj,myThid) |
327 |
CALL DIAGNOSTICS_FILL(strain, 'Strain ',k,1,2,bi,bj,myThid) |
328 |
ENDIF |
329 |
#endif |
330 |
ENDIF |
331 |
|
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C--- First call (k=1): compute vertical adv. flux fVerUkm & fVerVkm |
333 |
IF (momAdvection.AND.k.EQ.1) THEN |
334 |
|
335 |
#ifdef MOM_BOUNDARY_CONSERVE |
336 |
CALL MOM_UV_BOUNDARY( bi, bj, k, |
337 |
I uVel, vVel, |
338 |
O uBnd(1-OLx,1-OLy,k,bi,bj), |
339 |
O vBnd(1-OLx,1-OLy,k,bi,bj), |
340 |
I myTime, myIter, myThid ) |
341 |
#endif /* MOM_BOUNDARY_CONSERVE */ |
342 |
|
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C- Calculate vertical transports above U & V points (West & South face): |
344 |
|
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#ifdef ALLOW_AUTODIFF_TAMC |
346 |
# ifdef NONLIN_FRSURF |
347 |
# ifndef DISABLE_RSTAR_CODE |
348 |
CADJ STORE dwtransc(:,:,bi,bj) = |
349 |
CADJ & comlev1_bibj_k, key = imomkey, byte = isbyte |
350 |
CADJ STORE dwtransu(:,:,bi,bj) = |
351 |
CADJ & comlev1_bibj_k, key = imomkey, byte = isbyte |
352 |
CADJ STORE dwtransv(:,:,bi,bj) = |
353 |
CADJ & comlev1_bibj_k, key = imomkey, byte = isbyte |
354 |
# endif |
355 |
# endif /* NONLIN_FRSURF */ |
356 |
#endif /* ALLOW_AUTODIFF_TAMC */ |
357 |
CALL MOM_CALC_RTRANS( k, bi, bj, |
358 |
O rTransU, rTransV, |
359 |
I myTime, myIter, myThid ) |
360 |
|
361 |
C- Free surface correction term (flux at k=1) |
362 |
CALL MOM_U_ADV_WU( bi,bj,k,uVel,wVel,rTransU, |
363 |
O fVerUkm, myThid ) |
364 |
|
365 |
CALL MOM_V_ADV_WV( bi,bj,k,vVel,wVel,rTransV, |
366 |
O fVerVkm, myThid ) |
367 |
|
368 |
C--- endif momAdvection & k=1 |
369 |
ENDIF |
370 |
|
371 |
C--- Calculate vertical transports (at k+1) below U & V points : |
372 |
IF (momAdvection) THEN |
373 |
CALL MOM_CALC_RTRANS( k+1, bi, bj, |
374 |
O rTransU, rTransV, |
375 |
I myTime, myIter, myThid ) |
376 |
ENDIF |
377 |
|
378 |
#ifdef MOM_BOUNDARY_CONSERVE |
379 |
IF ( momAdvection .AND. k.LT.Nr ) THEN |
380 |
CALL MOM_UV_BOUNDARY( bi, bj, k+1, |
381 |
I uVel, vVel, |
382 |
O uBnd(1-OLx,1-OLy,k+1,bi,bj), |
383 |
O vBnd(1-OLx,1-OLy,k+1,bi,bj), |
384 |
I myTime, myIter, myThid ) |
385 |
ENDIF |
386 |
#endif /* MOM_BOUNDARY_CONSERVE */ |
387 |
|
388 |
IF (momViscosity) THEN |
389 |
DO j=1-OLy,sNy+OLy |
390 |
DO i=1-OLx,sNx+OLx |
391 |
viscAh_D(i,j) = viscAhD |
392 |
viscAh_Z(i,j) = viscAhZ |
393 |
viscA4_D(i,j) = viscA4D |
394 |
viscA4_Z(i,j) = viscA4Z |
395 |
ENDDO |
396 |
ENDDO |
397 |
IF ( useVariableVisc ) THEN |
398 |
CALL MOM_CALC_VISC( bi, bj, k, |
399 |
O viscAh_Z, viscAh_D, viscA4_Z, viscA4_D, |
400 |
I hDiv, vort3, tension, strain, KE, hFacZ, |
401 |
I myThid ) |
402 |
ENDIF |
403 |
ENDIF |
404 |
|
405 |
C---+----1----+----2----+----3----+----4----+----5----+----6----+----7-|--+----| |
406 |
|
407 |
C---- Zonal momentum equation starts here |
408 |
|
409 |
IF (momAdvection) THEN |
410 |
C--- Calculate mean fluxes (advection) between cells for zonal flow. |
411 |
|
412 |
#ifdef MOM_BOUNDARY_CONSERVE |
413 |
CALL MOM_U_ADV_UU( bi,bj,k,uTrans,uBnd(1-OLx,1-OLy,k,bi,bj), |
414 |
O fZon,myThid ) |
415 |
CALL MOM_U_ADV_VU( bi,bj,k,vTrans,uBnd(1-OLx,1-OLy,k,bi,bj), |
416 |
O fMer,myThid ) |
417 |
CALL MOM_U_ADV_WU( |
418 |
I bi,bj,k+1,uBnd,wVel,rTransU, |
419 |
O fVerUkp, myThid ) |
420 |
#else /* MOM_BOUNDARY_CONSERVE */ |
421 |
C-- Zonal flux (fZon is at east face of "u" cell) |
422 |
C Mean flow component of zonal flux -> fZon |
423 |
CALL MOM_U_ADV_UU( bi,bj,k,uTrans,uFld,fZon,myThid ) |
424 |
|
425 |
C-- Meridional flux (fMer is at south face of "u" cell) |
426 |
C Mean flow component of meridional flux -> fMer |
427 |
CALL MOM_U_ADV_VU( bi,bj,k,vTrans,uFld,fMer,myThid ) |
428 |
|
429 |
C-- Vertical flux (fVer is at upper face of "u" cell) |
430 |
C Mean flow component of vertical flux (at k+1) -> fVer |
431 |
CALL MOM_U_ADV_WU( |
432 |
I bi,bj,k+1,uVel,wVel,rTransU, |
433 |
O fVerUkp, myThid ) |
434 |
#endif /* MOM_BOUNDARY_CONSERVE */ |
435 |
|
436 |
C-- Tendency is minus divergence of the fluxes + coriolis + pressure term |
437 |
DO j=jMin,jMax |
438 |
DO i=iMin,iMax |
439 |
gU(i,j,k,bi,bj) = |
440 |
#ifdef OLD_UV_GEOM |
441 |
& -_recip_hFacW(i,j,k,bi,bj)*recip_drF(k)/ |
442 |
& ( 0.5 _d 0*(rA(i,j,bi,bj)+rA(i-1,j,bi,bj)) ) |
443 |
#else |
444 |
& -_recip_hFacW(i,j,k,bi,bj)*recip_drF(k) |
445 |
& *recip_rAw(i,j,bi,bj)*recip_deepFac2C(k)*recip_rhoFacC(k) |
446 |
#endif |
447 |
& *( ( fZon(i,j ) - fZon(i-1,j) )*uDudxFac |
448 |
& +( fMer(i,j+1) - fMer(i, j) )*vDudyFac |
449 |
& +( fVerUkp(i,j) - fVerUkm(i,j) )*rkSign*rVelDudrFac |
450 |
& ) |
451 |
ENDDO |
452 |
ENDDO |
453 |
|
454 |
#ifdef ALLOW_DIAGNOSTICS |
455 |
IF ( useDiagnostics ) THEN |
456 |
CALL DIAGNOSTICS_FILL( fZon, 'ADVx_Um ',k,1,2,bi,bj,myThid) |
457 |
CALL DIAGNOSTICS_FILL( fMer, 'ADVy_Um ',k,1,2,bi,bj,myThid) |
458 |
CALL DIAGNOSTICS_FILL(fVerUkm,'ADVrE_Um',k,1,2,bi,bj,myThid) |
459 |
ENDIF |
460 |
#endif |
461 |
|
462 |
#ifdef NONLIN_FRSURF |
463 |
C-- account for 3.D divergence of the flow in rStar coordinate: |
464 |
# ifndef DISABLE_RSTAR_CODE |
465 |
IF ( select_rStar.GT.0 ) THEN |
466 |
DO j=jMin,jMax |
467 |
DO i=iMin,iMax |
468 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj) |
469 |
& - (rStarExpW(i,j,bi,bj) - 1. _d 0)/deltaTFreeSurf |
470 |
& *uVel(i,j,k,bi,bj) |
471 |
ENDDO |
472 |
ENDDO |
473 |
ENDIF |
474 |
IF ( select_rStar.LT.0 ) THEN |
475 |
DO j=jMin,jMax |
476 |
DO i=iMin,iMax |
477 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj) |
478 |
& - rStarDhWDt(i,j,bi,bj)*uVel(i,j,k,bi,bj) |
479 |
ENDDO |
480 |
ENDDO |
481 |
ENDIF |
482 |
# endif /* DISABLE_RSTAR_CODE */ |
483 |
#endif /* NONLIN_FRSURF */ |
484 |
|
485 |
#ifdef ALLOW_ADDFLUID |
486 |
IF ( selectAddFluid.GE.1 ) THEN |
487 |
DO j=jMin,jMax |
488 |
DO i=iMin,iMax |
489 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj) |
490 |
& + uVel(i,j,k,bi,bj)*mass2rUnit*0.5 _d 0 |
491 |
& *( addMass(i-1,j,k,bi,bj) + addMass(i,j,k,bi,bj) ) |
492 |
& *_recip_hFacW(i,j,k,bi,bj)*recip_drF(k)*recip_rhoFacC(k) |
493 |
& * recip_rAw(i,j,bi,bj)*recip_deepFac2C(k) |
494 |
ENDDO |
495 |
ENDDO |
496 |
ENDIF |
497 |
#endif /* ALLOW_ADDFLUID */ |
498 |
|
499 |
ELSE |
500 |
C- if momAdvection / else |
501 |
DO j=1-OLy,sNy+OLy |
502 |
DO i=1-OLx,sNx+OLx |
503 |
gU(i,j,k,bi,bj) = 0. _d 0 |
504 |
ENDDO |
505 |
ENDDO |
506 |
|
507 |
C- endif momAdvection. |
508 |
ENDIF |
509 |
|
510 |
IF (momViscosity) THEN |
511 |
C--- Calculate eddy fluxes (dissipation) between cells for zonal flow. |
512 |
|
513 |
C Bi-harmonic term del^2 U -> v4F |
514 |
IF ( useBiharmonicVisc ) |
515 |
& CALL MOM_U_DEL2U( bi, bj, k, uFld, hFacZ, h0FacZ, |
516 |
O v4f, myThid ) |
517 |
|
518 |
C Laplacian and bi-harmonic terms, Zonal Fluxes -> fZon |
519 |
CALL MOM_U_XVISCFLUX( bi,bj,k,uFld,v4F,fZon, |
520 |
I viscAh_D,viscA4_D,myThid ) |
521 |
|
522 |
C Laplacian and bi-harmonic termis, Merid Fluxes -> fMer |
523 |
CALL MOM_U_YVISCFLUX( bi,bj,k,uFld,v4F,hFacZ,fMer, |
524 |
I viscAh_Z,viscA4_Z,myThid ) |
525 |
|
526 |
C Eddy component of vertical flux (interior component only) -> fVrUp & fVrDw |
527 |
IF (.NOT.implicitViscosity) THEN |
528 |
CALL MOM_U_RVISCFLUX( bi,bj, k, uVel,kappaRU,fVrUp,myThid ) |
529 |
CALL MOM_U_RVISCFLUX( bi,bj,k+1,uVel,kappaRU,fVrDw,myThid ) |
530 |
ENDIF |
531 |
|
532 |
C-- Tendency is minus divergence of the fluxes |
533 |
C anelastic: hor.visc.fluxes are not scaled by rhoFac (by vert.visc.flx is) |
534 |
DO j=jMin,jMax |
535 |
DO i=iMin,iMax |
536 |
guDiss(i,j) = |
537 |
#ifdef OLD_UV_GEOM |
538 |
& -_recip_hFacW(i,j,k,bi,bj)*recip_drF(k)/ |
539 |
& ( 0.5 _d 0*(rA(i,j,bi,bj)+rA(i-1,j,bi,bj)) ) |
540 |
#else |
541 |
& -_recip_hFacW(i,j,k,bi,bj)*recip_drF(k) |
542 |
& *recip_rAw(i,j,bi,bj)*recip_deepFac2C(k) |
543 |
#endif |
544 |
& *( ( fZon(i,j ) - fZon(i-1,j) )*AhDudxFac |
545 |
& +( fMer(i,j+1) - fMer(i, j) )*AhDudyFac |
546 |
& +( fVrDw(i,j) - fVrUp(i,j) )*rkSign*ArDudrFac |
547 |
& *recip_rhoFacC(k) |
548 |
& ) |
549 |
ENDDO |
550 |
ENDDO |
551 |
|
552 |
#ifdef ALLOW_DIAGNOSTICS |
553 |
IF ( useDiagnostics ) THEN |
554 |
CALL DIAGNOSTICS_FILL(fZon, 'VISCx_Um',k,1,2,bi,bj,myThid) |
555 |
CALL DIAGNOSTICS_FILL(fMer, 'VISCy_Um',k,1,2,bi,bj,myThid) |
556 |
IF (.NOT.implicitViscosity) |
557 |
& CALL DIAGNOSTICS_FILL(fVrUp,'VISrE_Um',k,1,2,bi,bj,myThid) |
558 |
ENDIF |
559 |
#endif |
560 |
|
561 |
C-- No-slip and drag BCs appear as body forces in cell abutting topography |
562 |
IF (no_slip_sides) THEN |
563 |
C- No-slip BCs impose a drag at walls... |
564 |
CALL MOM_U_SIDEDRAG( bi, bj, k, |
565 |
I uFld, v4f, h0FacZ, |
566 |
I viscAh_Z, viscA4_Z, |
567 |
I useHarmonicVisc, useBiharmonicVisc, useVariableVisc, |
568 |
O vF, |
569 |
I myThid ) |
570 |
DO j=jMin,jMax |
571 |
DO i=iMin,iMax |
572 |
gUdiss(i,j) = gUdiss(i,j) + vF(i,j) |
573 |
ENDDO |
574 |
ENDDO |
575 |
ENDIF |
576 |
C- No-slip BCs impose a drag at bottom |
577 |
IF (bottomDragTerms) THEN |
578 |
CALL MOM_U_BOTTOMDRAG( bi, bj, k, |
579 |
I uFld, vFld, KE, kappaRU, |
580 |
O vF, |
581 |
I myThid ) |
582 |
DO j=jMin,jMax |
583 |
DO i=iMin,iMax |
584 |
gUdiss(i,j) = gUdiss(i,j) + vF(i,j) |
585 |
ENDDO |
586 |
ENDDO |
587 |
ENDIF |
588 |
|
589 |
#ifdef ALLOW_SHELFICE |
590 |
IF (useShelfIce) THEN |
591 |
CALL SHELFICE_U_DRAG( bi, bj, k, |
592 |
I uFld, vFld, KE, kappaRU, |
593 |
O vF, |
594 |
I myThid ) |
595 |
DO j=jMin,jMax |
596 |
DO i=iMin,iMax |
597 |
gUdiss(i,j) = gUdiss(i,j) + vF(i,j) |
598 |
ENDDO |
599 |
ENDDO |
600 |
ENDIF |
601 |
#endif /* ALLOW_SHELFICE */ |
602 |
|
603 |
C- endif momViscosity |
604 |
ENDIF |
605 |
|
606 |
C-- Forcing term (moved to timestep.F) |
607 |
c IF (momForcing) |
608 |
c & CALL EXTERNAL_FORCING_U( |
609 |
c I iMin,iMax,jMin,jMax,bi,bj,k, |
610 |
c I myTime,myThid) |
611 |
|
612 |
C-- Metric terms for curvilinear grid systems |
613 |
IF (useNHMTerms) THEN |
614 |
C o Non-Hydrostatic (spherical) metric terms |
615 |
CALL MOM_U_METRIC_NH( bi,bj,k,uFld,wVel,mT,myThid ) |
616 |
DO j=jMin,jMax |
617 |
DO i=iMin,iMax |
618 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+mtNHFacU*mT(i,j) |
619 |
ENDDO |
620 |
ENDDO |
621 |
ENDIF |
622 |
IF ( usingSphericalPolarGrid .AND. metricTerms ) THEN |
623 |
C o Spherical polar grid metric terms |
624 |
CALL MOM_U_METRIC_SPHERE( bi,bj,k,uFld,vFld,mT,myThid ) |
625 |
DO j=jMin,jMax |
626 |
DO i=iMin,iMax |
627 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+mtFacU*mT(i,j) |
628 |
ENDDO |
629 |
ENDDO |
630 |
ENDIF |
631 |
IF ( usingCylindricalGrid .AND. metricTerms ) THEN |
632 |
C o Cylindrical grid metric terms |
633 |
CALL MOM_U_METRIC_CYLINDER( bi,bj,k,uFld,vFld,mT,myThid ) |
634 |
DO j=jMin,jMax |
635 |
DO i=iMin,iMax |
636 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+mtFacU*mT(i,j) |
637 |
ENDDO |
638 |
ENDDO |
639 |
ENDIF |
640 |
|
641 |
C---+----1----+----2----+----3----+----4----+----5----+----6----+----7-|--+----| |
642 |
|
643 |
C---- Meridional momentum equation starts here |
644 |
|
645 |
IF (momAdvection) THEN |
646 |
|
647 |
#ifdef MOM_BOUNDARY_CONSERVE |
648 |
CALL MOM_V_ADV_UV( bi,bj,k,uTrans,vBnd(1-OLx,1-OLy,k,bi,bj), |
649 |
O fZon,myThid ) |
650 |
CALL MOM_V_ADV_VV( bi,bj,k,vTrans,vBnd(1-OLx,1-OLy,k,bi,bj), |
651 |
O fMer,myThid ) |
652 |
CALL MOM_V_ADV_WV( bi,bj,k+1,vBnd,wVel,rTransV, |
653 |
O fVerVkp, myThid ) |
654 |
#else /* MOM_BOUNDARY_CONSERVE */ |
655 |
C--- Calculate mean fluxes (advection) between cells for meridional flow. |
656 |
C Mean flow component of zonal flux -> fZon |
657 |
CALL MOM_V_ADV_UV( bi,bj,k,uTrans,vFld,fZon,myThid ) |
658 |
|
659 |
C-- Meridional flux (fMer is at north face of "v" cell) |
660 |
C Mean flow component of meridional flux -> fMer |
661 |
CALL MOM_V_ADV_VV( bi,bj,k,vTrans,vFld,fMer,myThid ) |
662 |
|
663 |
C-- Vertical flux (fVer is at upper face of "v" cell) |
664 |
C Mean flow component of vertical flux (at k+1) -> fVerV |
665 |
CALL MOM_V_ADV_WV( bi,bj,k+1,vVel,wVel,rTransV, |
666 |
O fVerVkp, myThid ) |
667 |
#endif /* MOM_BOUNDARY_CONSERVE */ |
668 |
|
669 |
C-- Tendency is minus divergence of the fluxes + coriolis + pressure term |
670 |
DO j=jMin,jMax |
671 |
DO i=iMin,iMax |
672 |
gV(i,j,k,bi,bj) = |
673 |
#ifdef OLD_UV_GEOM |
674 |
& -_recip_hFacS(i,j,k,bi,bj)*recip_drF(k)/ |
675 |
& ( 0.5 _d 0*(_rA(i,j,bi,bj)+_rA(i,j-1,bi,bj)) ) |
676 |
#else |
677 |
& -_recip_hFacS(i,j,k,bi,bj)*recip_drF(k) |
678 |
& *recip_rAs(i,j,bi,bj)*recip_deepFac2C(k)*recip_rhoFacC(k) |
679 |
#endif |
680 |
& *( ( fZon(i+1,j) - fZon(i,j ) )*uDvdxFac |
681 |
& +( fMer(i, j) - fMer(i,j-1) )*vDvdyFac |
682 |
& +( fVerVkp(i,j) - fVerVkm(i,j) )*rkSign*rVelDvdrFac |
683 |
& ) |
684 |
ENDDO |
685 |
ENDDO |
686 |
|
687 |
#ifdef ALLOW_DIAGNOSTICS |
688 |
IF ( useDiagnostics ) THEN |
689 |
CALL DIAGNOSTICS_FILL( fZon, 'ADVx_Vm ',k,1,2,bi,bj,myThid) |
690 |
CALL DIAGNOSTICS_FILL( fMer, 'ADVy_Vm ',k,1,2,bi,bj,myThid) |
691 |
CALL DIAGNOSTICS_FILL(fVerVkm,'ADVrE_Vm',k,1,2,bi,bj,myThid) |
692 |
ENDIF |
693 |
#endif |
694 |
|
695 |
#ifdef NONLIN_FRSURF |
696 |
C-- account for 3.D divergence of the flow in rStar coordinate: |
697 |
# ifndef DISABLE_RSTAR_CODE |
698 |
IF ( select_rStar.GT.0 ) THEN |
699 |
DO j=jMin,jMax |
700 |
DO i=iMin,iMax |
701 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj) |
702 |
& - (rStarExpS(i,j,bi,bj) - 1. _d 0)/deltaTFreeSurf |
703 |
& *vVel(i,j,k,bi,bj) |
704 |
ENDDO |
705 |
ENDDO |
706 |
ENDIF |
707 |
IF ( select_rStar.LT.0 ) THEN |
708 |
DO j=jMin,jMax |
709 |
DO i=iMin,iMax |
710 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj) |
711 |
& - rStarDhSDt(i,j,bi,bj)*vVel(i,j,k,bi,bj) |
712 |
ENDDO |
713 |
ENDDO |
714 |
ENDIF |
715 |
# endif /* DISABLE_RSTAR_CODE */ |
716 |
#endif /* NONLIN_FRSURF */ |
717 |
|
718 |
#ifdef ALLOW_ADDFLUID |
719 |
IF ( selectAddFluid.GE.1 ) THEN |
720 |
DO j=jMin,jMax |
721 |
DO i=iMin,iMax |
722 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj) |
723 |
& + vVel(i,j,k,bi,bj)*mass2rUnit*0.5 _d 0 |
724 |
& *( addMass(i,j-1,k,bi,bj) + addMass(i,j,k,bi,bj) ) |
725 |
& *_recip_hFacS(i,j,k,bi,bj)*recip_drF(k)*recip_rhoFacC(k) |
726 |
& * recip_rAs(i,j,bi,bj)*recip_deepFac2C(k) |
727 |
ENDDO |
728 |
ENDDO |
729 |
ENDIF |
730 |
#endif /* ALLOW_ADDFLUID */ |
731 |
|
732 |
ELSE |
733 |
C- if momAdvection / else |
734 |
DO j=1-OLy,sNy+OLy |
735 |
DO i=1-OLx,sNx+OLx |
736 |
gV(i,j,k,bi,bj) = 0. _d 0 |
737 |
ENDDO |
738 |
ENDDO |
739 |
|
740 |
C- endif momAdvection. |
741 |
ENDIF |
742 |
|
743 |
IF (momViscosity) THEN |
744 |
C--- Calculate eddy fluxes (dissipation) between cells for meridional flow. |
745 |
C Bi-harmonic term del^2 V -> v4F |
746 |
IF ( useBiharmonicVisc ) |
747 |
& CALL MOM_V_DEL2V( bi, bj, k, vFld, hFacZ, h0FacZ, |
748 |
O v4f, myThid ) |
749 |
|
750 |
C Laplacian and bi-harmonic terms, Zonal Fluxes -> fZon |
751 |
CALL MOM_V_XVISCFLUX( bi,bj,k,vFld,v4f,hFacZ,fZon, |
752 |
I viscAh_Z,viscA4_Z,myThid ) |
753 |
|
754 |
C Laplacian and bi-harmonic termis, Merid Fluxes -> fMer |
755 |
CALL MOM_V_YVISCFLUX( bi,bj,k,vFld,v4f,fMer, |
756 |
I viscAh_D,viscA4_D,myThid ) |
757 |
|
758 |
C Eddy component of vertical flux (interior component only) -> fVrUp & fVrDw |
759 |
IF (.NOT.implicitViscosity) THEN |
760 |
CALL MOM_V_RVISCFLUX( bi,bj, k, vVel,KappaRV,fVrUp,myThid ) |
761 |
CALL MOM_V_RVISCFLUX( bi,bj,k+1,vVel,KappaRV,fVrDw,myThid ) |
762 |
ENDIF |
763 |
|
764 |
C-- Tendency is minus divergence of the fluxes + coriolis + pressure term |
765 |
C anelastic: hor.visc.fluxes are not scaled by rhoFac (by vert.visc.flx is) |
766 |
DO j=jMin,jMax |
767 |
DO i=iMin,iMax |
768 |
gvDiss(i,j) = |
769 |
#ifdef OLD_UV_GEOM |
770 |
& -_recip_hFacS(i,j,k,bi,bj)*recip_drF(k)/ |
771 |
& ( 0.5 _d 0*(_rA(i,j,bi,bj)+_rA(i,j-1,bi,bj)) ) |
772 |
#else |
773 |
& -_recip_hFacS(i,j,k,bi,bj)*recip_drF(k) |
774 |
& *recip_rAs(i,j,bi,bj)*recip_deepFac2C(k) |
775 |
#endif |
776 |
& *( ( fZon(i+1,j) - fZon(i,j ) )*AhDvdxFac |
777 |
& +( fMer(i, j) - fMer(i,j-1) )*AhDvdyFac |
778 |
& +( fVrDw(i,j) - fVrUp(i,j) )*rkSign*ArDvdrFac |
779 |
& *recip_rhoFacC(k) |
780 |
& ) |
781 |
ENDDO |
782 |
ENDDO |
783 |
|
784 |
#ifdef ALLOW_DIAGNOSTICS |
785 |
IF ( useDiagnostics ) THEN |
786 |
CALL DIAGNOSTICS_FILL(fZon, 'VISCx_Vm',k,1,2,bi,bj,myThid) |
787 |
CALL DIAGNOSTICS_FILL(fMer, 'VISCy_Vm',k,1,2,bi,bj,myThid) |
788 |
IF (.NOT.implicitViscosity) |
789 |
& CALL DIAGNOSTICS_FILL(fVrUp,'VISrE_Vm',k,1,2,bi,bj,myThid) |
790 |
ENDIF |
791 |
#endif |
792 |
|
793 |
C-- No-slip and drag BCs appear as body forces in cell abutting topography |
794 |
IF (no_slip_sides) THEN |
795 |
C- No-slip BCs impose a drag at walls... |
796 |
CALL MOM_V_SIDEDRAG( bi, bj, k, |
797 |
I vFld, v4f, h0FacZ, |
798 |
I viscAh_Z, viscA4_Z, |
799 |
I useHarmonicVisc, useBiharmonicVisc, useVariableVisc, |
800 |
O vF, |
801 |
I myThid ) |
802 |
DO j=jMin,jMax |
803 |
DO i=iMin,iMax |
804 |
gvDiss(i,j) = gvDiss(i,j) + vF(i,j) |
805 |
ENDDO |
806 |
ENDDO |
807 |
ENDIF |
808 |
C- No-slip BCs impose a drag at bottom |
809 |
IF (bottomDragTerms) THEN |
810 |
CALL MOM_V_BOTTOMDRAG( bi, bj, k, |
811 |
I uFld, vFld, KE, kappaRV, |
812 |
O vF, |
813 |
I myThid ) |
814 |
DO j=jMin,jMax |
815 |
DO i=iMin,iMax |
816 |
gvDiss(i,j) = gvDiss(i,j) + vF(i,j) |
817 |
ENDDO |
818 |
ENDDO |
819 |
ENDIF |
820 |
|
821 |
#ifdef ALLOW_SHELFICE |
822 |
IF (useShelfIce) THEN |
823 |
CALL SHELFICE_V_DRAG( bi, bj, k, |
824 |
I uFld, vFld, KE, kappaRV, |
825 |
O vF, |
826 |
I myThid ) |
827 |
DO j=jMin,jMax |
828 |
DO i=iMin,iMax |
829 |
gvDiss(i,j) = gvDiss(i,j) + vF(i,j) |
830 |
ENDDO |
831 |
ENDDO |
832 |
ENDIF |
833 |
#endif /* ALLOW_SHELFICE */ |
834 |
|
835 |
C- endif momViscosity |
836 |
ENDIF |
837 |
|
838 |
C-- Forcing term (moved to timestep.F) |
839 |
c IF (momForcing) |
840 |
c & CALL EXTERNAL_FORCING_V( |
841 |
c I iMin,iMax,jMin,jMax,bi,bj,k, |
842 |
c I myTime,myThid) |
843 |
|
844 |
C-- Metric terms for curvilinear grid systems |
845 |
IF (useNHMTerms) THEN |
846 |
C o Non-Hydrostatic (spherical) metric terms |
847 |
CALL MOM_V_METRIC_NH( bi,bj,k,vFld,wVel,mT,myThid ) |
848 |
DO j=jMin,jMax |
849 |
DO i=iMin,iMax |
850 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+mtNHFacV*mT(i,j) |
851 |
ENDDO |
852 |
ENDDO |
853 |
ENDIF |
854 |
IF ( usingSphericalPolarGrid .AND. metricTerms ) THEN |
855 |
C o Spherical polar grid metric terms |
856 |
CALL MOM_V_METRIC_SPHERE( bi,bj,k,uFld,mT,myThid ) |
857 |
DO j=jMin,jMax |
858 |
DO i=iMin,iMax |
859 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+mtFacV*mT(i,j) |
860 |
ENDDO |
861 |
ENDDO |
862 |
ENDIF |
863 |
IF ( usingCylindricalGrid .AND. metricTerms ) THEN |
864 |
C o Cylindrical grid metric terms |
865 |
CALL MOM_V_METRIC_CYLINDER( bi,bj,k,uFld,vFld,mT,myThid ) |
866 |
DO j=jMin,jMax |
867 |
DO i=iMin,iMax |
868 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+mtFacV*mT(i,j) |
869 |
ENDDO |
870 |
ENDDO |
871 |
ENDIF |
872 |
|
873 |
C---+----1----+----2----+----3----+----4----+----5----+----6----+----7-|--+----| |
874 |
|
875 |
C-- Coriolis term (call to CD_CODE_SCHEME has been moved to timestep.F) |
876 |
IF (.NOT.useCDscheme) THEN |
877 |
CALL MOM_U_CORIOLIS( bi,bj,k,vFld,cf,myThid ) |
878 |
DO j=jMin,jMax |
879 |
DO i=iMin,iMax |
880 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+fuFac*cf(i,j) |
881 |
ENDDO |
882 |
ENDDO |
883 |
#ifdef ALLOW_DIAGNOSTICS |
884 |
IF ( useDiagnostics ) |
885 |
& CALL DIAGNOSTICS_FILL(cf,'Um_Cori ',k,1,2,bi,bj,myThid) |
886 |
#endif |
887 |
CALL MOM_V_CORIOLIS( bi,bj,k,uFld,cf,myThid ) |
888 |
DO j=jMin,jMax |
889 |
DO i=iMin,iMax |
890 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+fvFac*cf(i,j) |
891 |
ENDDO |
892 |
ENDDO |
893 |
#ifdef ALLOW_DIAGNOSTICS |
894 |
IF ( useDiagnostics ) |
895 |
& CALL DIAGNOSTICS_FILL(cf,'Vm_Cori ',k,1,2,bi,bj,myThid) |
896 |
#endif |
897 |
ENDIF |
898 |
|
899 |
C-- 3.D Coriolis term (horizontal momentum, Eastward component: -fprime*w) |
900 |
IF ( use3dCoriolis ) THEN |
901 |
CALL MOM_U_CORIOLIS_NH( bi,bj,k,wVel,cf,myThid ) |
902 |
DO j=jMin,jMax |
903 |
DO i=iMin,iMax |
904 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+fuFac*cf(i,j) |
905 |
ENDDO |
906 |
ENDDO |
907 |
IF ( usingCurvilinearGrid ) THEN |
908 |
C- presently, non zero angleSinC array only supported with Curvilinear-Grid |
909 |
CALL MOM_V_CORIOLIS_NH( bi,bj,k,wVel,cf,myThid ) |
910 |
DO j=jMin,jMax |
911 |
DO i=iMin,iMax |
912 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+fvFac*cf(i,j) |
913 |
ENDDO |
914 |
ENDDO |
915 |
ENDIF |
916 |
ENDIF |
917 |
|
918 |
C-- Set du/dt & dv/dt on boundaries to zero |
919 |
DO j=jMin,jMax |
920 |
DO i=iMin,iMax |
921 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)*_maskW(i,j,k,bi,bj) |
922 |
guDiss(i,j) = guDiss(i,j) *_maskW(i,j,k,bi,bj) |
923 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)*_maskS(i,j,k,bi,bj) |
924 |
gvDiss(i,j) = gvDiss(i,j) *_maskS(i,j,k,bi,bj) |
925 |
ENDDO |
926 |
ENDDO |
927 |
|
928 |
#ifdef ALLOW_DIAGNOSTICS |
929 |
IF ( useDiagnostics ) THEN |
930 |
CALL DIAGNOSTICS_FILL(KE, 'momKE ',k,1,2,bi,bj,myThid) |
931 |
CALL DIAGNOSTICS_FILL(gU(1-OLx,1-OLy,k,bi,bj), |
932 |
& 'Um_Advec',k,1,2,bi,bj,myThid) |
933 |
CALL DIAGNOSTICS_FILL(gV(1-OLx,1-OLy,k,bi,bj), |
934 |
& 'Vm_Advec',k,1,2,bi,bj,myThid) |
935 |
ENDIF |
936 |
#endif /* ALLOW_DIAGNOSTICS */ |
937 |
|
938 |
RETURN |
939 |
END |