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baylor |
1.27 |
C $Header: /u/gcmpack/MITgcm/pkg/mom_vecinv/mom_vi_hdissip.F,v 1.26 2005/09/16 19:32:20 baylor Exp $ |
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jmc |
1.3 |
C $Name: $ |
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adcroft |
1.2 |
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adcroft |
1.8 |
#include "MOM_VECINV_OPTIONS.h" |
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adcroft |
1.2 |
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SUBROUTINE MOM_VI_HDISSIP( |
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I bi,bj,k, |
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baylor |
1.26 |
I hDiv,vort3,tension,strain,KE, |
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I hFacZ,dStar,zStar, |
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adcroft |
1.2 |
O uDissip,vDissip, |
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I myThid) |
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heimbach |
1.14 |
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cph( |
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jmc |
1.15 |
cph The following line was commented in the argument list |
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heimbach |
1.14 |
cph TAMC cannot digest commented lines within continuing lines |
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c I viscAh_Z,viscAh_D,viscA4_Z,viscA4_D, |
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cph) |
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adcroft |
1.2 |
IMPLICIT NONE |
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C |
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C Calculate horizontal dissipation terms |
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C [del^2 - del^4] (u,v) |
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C |
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C == Global variables == |
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#include "SIZE.h" |
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#include "GRID.h" |
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#include "EEPARAMS.h" |
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#include "PARAMS.h" |
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C == Routine arguments == |
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INTEGER bi,bj,k |
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_RL hDiv(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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baylor |
1.26 |
_RL tension(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL strain(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL KE(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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adcroft |
1.2 |
_RS hFacZ(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL dStar(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL zStar(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL uDissip(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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_RL vDissip(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
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INTEGER myThid |
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C == Local variables == |
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baylor |
1.26 |
INTEGER I,J |
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_RL Zip,Zij,Zpj,Dim,Dij,Dmj,uD2,vD2,uD4,vD4 |
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jmc |
1.18 |
_RL viscAh_Z(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 viscA4_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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baylor |
1.26 |
LOGICAL harmonic, biharmonic, useVariableViscosity |
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adcroft |
1.6 |
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baylor |
1.26 |
CALL MOM_CALC_VISC( |
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I bi,bj,k, |
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O viscAh_Z,viscAh_D,viscA4_Z,viscA4_D, |
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O harmonic,biharmonic,useVariableViscosity, |
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baylor |
1.27 |
I hDiv,vort3,tension,strain,KE,hfacZ, |
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baylor |
1.26 |
I myThid) |
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adcroft |
1.2 |
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jmc |
1.12 |
C - Laplacian terms |
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baylor |
1.26 |
IF (harmonic) THEN |
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jmc |
1.12 |
DO j=2-Oly,sNy+Oly-1 |
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DO i=2-Olx,sNx+Olx-1 |
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Dim=hDiv( i ,j-1) |
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Dij=hDiv( i , j ) |
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Dmj=hDiv(i-1, j ) |
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Zip=hFacZ( i ,j+1)*vort3( i ,j+1) |
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Zij=hFacZ( i , j )*vort3( i , j ) |
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Zpj=hFacZ(i+1, j )*vort3(i+1, j ) |
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adcroft |
1.2 |
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adcroft |
1.4 |
C This bit scales the harmonic dissipation operator to be proportional |
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C to the grid-cell area over the time-step. viscAh is then non-dimensional |
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C and should be less than 1/8, for example viscAh=0.01 |
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jmc |
1.12 |
IF (useVariableViscosity) THEN |
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adcroft |
1.6 |
Dij=Dij*viscAh_D(i,j) |
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Dim=Dim*viscAh_D(i,j-1) |
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Dmj=Dmj*viscAh_D(i-1,j) |
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Zij=Zij*viscAh_Z(i,j) |
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Zip=Zip*viscAh_Z(i,j+1) |
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Zpj=Zpj*viscAh_Z(i+1,j) |
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adcroft |
1.4 |
uD2 = ( |
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& cosFacU(j,bi,bj)*( Dij-Dmj )*recip_DXC(i,j,bi,bj) |
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& -recip_hFacW(i,j,k,bi,bj)*( Zip-Zij )*recip_DYG(i,j,bi,bj) ) |
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vD2 = ( |
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& recip_hFacS(i,j,k,bi,bj)*( Zpj-Zij )*recip_DXG(i,j,bi,bj) |
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& *cosFacV(j,bi,bj) |
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& +( Dij-Dim )*recip_DYC(i,j,bi,bj) ) |
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jmc |
1.12 |
ELSE |
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uD2 = viscAhD* |
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adcroft |
1.2 |
& cosFacU(j,bi,bj)*( Dij-Dmj )*recip_DXC(i,j,bi,bj) |
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jmc |
1.12 |
& - viscAhZ*recip_hFacW(i,j,k,bi,bj)* |
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& ( Zip-Zij )*recip_DYG(i,j,bi,bj) |
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vD2 = viscAhZ*recip_hFacS(i,j,k,bi,bj)* |
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& cosFacV(j,bi,bj)*( Zpj-Zij )*recip_DXG(i,j,bi,bj) |
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& + viscAhD* ( Dij-Dim )*recip_DYC(i,j,bi,bj) |
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ENDIF |
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uDissip(i,j) = uD2 |
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vDissip(i,j) = vD2 |
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ENDDO |
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ENDDO |
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ELSE |
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DO j=2-Oly,sNy+Oly-1 |
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DO i=2-Olx,sNx+Olx-1 |
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uDissip(i,j) = 0. |
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vDissip(i,j) = 0. |
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ENDDO |
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ENDDO |
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ENDIF |
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C - Bi-harmonic terms |
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baylor |
1.26 |
IF (biharmonic) THEN |
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jmc |
1.12 |
DO j=2-Oly,sNy+Oly-1 |
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DO i=2-Olx,sNx+Olx-1 |
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adcroft |
1.2 |
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jmc |
1.11 |
#ifdef MOM_VI_ORIGINAL_VISCA4 |
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jmc |
1.12 |
Dim=dyF( i ,j-1,bi,bj)*dStar( i ,j-1) |
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Dij=dyF( i , j ,bi,bj)*dStar( i , j ) |
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Dmj=dyF(i-1, j ,bi,bj)*dStar(i-1, j ) |
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Zip=dxV( i ,j+1,bi,bj)*hFacZ( i ,j+1)*zStar( i ,j+1) |
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Zij=dxV( i , j ,bi,bj)*hFacZ( i , j )*zStar( i , j ) |
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Zpj=dxV(i+1, j ,bi,bj)*hFacZ(i+1, j )*zStar(i+1, j ) |
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jmc |
1.11 |
#else |
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jmc |
1.12 |
Dim=dStar( i ,j-1) |
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Dij=dStar( i , j ) |
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Dmj=dStar(i-1, j ) |
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Zip=hFacZ( i ,j+1)*zStar( i ,j+1) |
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Zij=hFacZ( i , j )*zStar( i , j ) |
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Zpj=hFacZ(i+1, j )*zStar(i+1, j ) |
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jmc |
1.11 |
#endif |
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adcroft |
1.4 |
C This bit scales the harmonic dissipation operator to be proportional |
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C to the grid-cell area over the time-step. viscAh is then non-dimensional |
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C and should be less than 1/8, for example viscAh=0.01 |
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jmc |
1.12 |
IF (useVariableViscosity) THEN |
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adcroft |
1.6 |
Dij=Dij*viscA4_D(i,j) |
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Dim=Dim*viscA4_D(i,j-1) |
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Dmj=Dmj*viscA4_D(i-1,j) |
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Zij=Zij*viscA4_Z(i,j) |
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Zip=Zip*viscA4_Z(i,j+1) |
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Zpj=Zpj*viscA4_Z(i+1,j) |
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jmc |
1.11 |
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#ifdef MOM_VI_ORIGINAL_VISCA4 |
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adcroft |
1.4 |
uD4 = recip_rAw(i,j,bi,bj)*( |
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& ( (Dij-Dmj)*cosFacU(j,bi,bj) ) |
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& -recip_hFacW(i,j,k,bi,bj)*( Zip-Zij ) ) |
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vD4 = recip_rAs(i,j,bi,bj)*( |
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& recip_hFacS(i,j,k,bi,bj)*( (Zpj-Zij)*cosFacV(j,bi,bj) ) |
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& + ( Dij-Dim ) ) |
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jmc |
1.12 |
ELSE |
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adcroft |
1.4 |
uD4 = recip_rAw(i,j,bi,bj)*( |
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adcroft |
1.2 |
& viscA4*( (Dij-Dmj)*cosFacU(j,bi,bj) ) |
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& -recip_hFacW(i,j,k,bi,bj)*viscA4*( Zip-Zij ) ) |
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adcroft |
1.4 |
vD4 = recip_rAs(i,j,bi,bj)*( |
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adcroft |
1.2 |
& recip_hFacS(i,j,k,bi,bj)*viscA4*( (Zpj-Zij)*cosFacV(j,bi,bj) ) |
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& + viscA4*( Dij-Dim ) ) |
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jmc |
1.11 |
#else /* MOM_VI_ORIGINAL_VISCA4 */ |
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uD4 = ( |
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& cosFacU(j,bi,bj)*( Dij-Dmj )*recip_DXC(i,j,bi,bj) |
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& -recip_hFacW(i,j,k,bi,bj)*( Zip-Zij )*recip_DYG(i,j,bi,bj) ) |
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vD4 = ( |
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& recip_hFacS(i,j,k,bi,bj)*( Zpj-Zij )*recip_DXG(i,j,bi,bj) |
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& *cosFacV(j,bi,bj) |
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& +( Dij-Dim )*recip_DYC(i,j,bi,bj) ) |
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jmc |
1.12 |
ELSE |
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jmc |
1.18 |
uD4 = viscA4D* |
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jmc |
1.11 |
& cosFacU(j,bi,bj)*( Dij-Dmj )*recip_DXC(i,j,bi,bj) |
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jmc |
1.12 |
& - viscA4Z*recip_hFacW(i,j,k,bi,bj)* |
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& ( Zip-Zij )*recip_DYG(i,j,bi,bj) |
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vD4 = viscA4Z*recip_hFacS(i,j,k,bi,bj)* |
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& cosFacV(j,bi,bj)*( Zpj-Zij )*recip_DXG(i,j,bi,bj) |
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& + viscA4D* ( Dij-Dim )*recip_DYC(i,j,bi,bj) |
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jmc |
1.11 |
#endif /* MOM_VI_ORIGINAL_VISCA4 */ |
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jmc |
1.12 |
ENDIF |
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adcroft |
1.2 |
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jmc |
1.12 |
uDissip(i,j) = uDissip(i,j) - uD4 |
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vDissip(i,j) = vDissip(i,j) - vD4 |
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adcroft |
1.2 |
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jmc |
1.12 |
ENDDO |
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adcroft |
1.2 |
ENDDO |
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jmc |
1.12 |
ENDIF |
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molod |
1.7 |
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adcroft |
1.2 |
RETURN |
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END |
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