1 |
jmc |
1.18 |
C $Header: /u/gcmpack/MITgcm/pkg/mom_vecinv/mom_vi_hdissip.F,v 1.17 2005/03/10 02:39:56 baylor Exp $ |
2 |
jmc |
1.3 |
C $Name: $ |
3 |
adcroft |
1.2 |
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4 |
adcroft |
1.8 |
#include "MOM_VECINV_OPTIONS.h" |
5 |
adcroft |
1.2 |
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SUBROUTINE MOM_VI_HDISSIP( |
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I bi,bj,k, |
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I hDiv,vort3,hFacZ,dStar,zStar, |
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O uDissip,vDissip, |
10 |
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I myThid) |
11 |
heimbach |
1.14 |
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cph( |
13 |
jmc |
1.15 |
cph The following line was commented in the argument list |
14 |
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, |
16 |
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cph) |
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adcroft |
1.2 |
IMPLICIT NONE |
19 |
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C |
20 |
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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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24 |
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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 == |
31 |
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INTEGER bi,bj,k |
32 |
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_RL hDiv(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
33 |
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_RL vort3(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
34 |
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_RS hFacZ(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
35 |
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_RL dStar(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
36 |
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_RL zStar(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
37 |
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_RL uDissip(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
38 |
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_RL vDissip(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
39 |
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INTEGER myThid |
40 |
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41 |
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C == Local variables == |
42 |
jmc |
1.18 |
_RL viscAh_Z(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
43 |
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_RL viscAh_D(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
44 |
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_RL viscA4_Z(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
45 |
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_RL viscA4_D(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
46 |
adcroft |
1.2 |
INTEGER I,J |
47 |
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_RL Zip,Zij,Zpj,Dim,Dij,Dmj,uD2,vD2,uD4,vD4 |
48 |
jmc |
1.18 |
_RL Alin,AlinMin,AlinMax,Alth2,Alth4,grdVrt,grdDiv |
49 |
baylor |
1.17 |
_RL vg2,vg2Min,vg2Max,vg4,vg4Min,vg4Max |
50 |
adcroft |
1.6 |
LOGICAL useVariableViscosity |
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useVariableViscosity= |
53 |
jmc |
1.18 |
& (viscAhGrid.NE.0.) |
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& .OR.(viscA4Grid.NE.0.) |
55 |
adcroft |
1.6 |
& .OR.(viscC2leith.NE.0.) |
56 |
baylor |
1.17 |
& .OR.(viscC2leithD.NE.0.) |
57 |
adcroft |
1.6 |
& .OR.(viscC4leith.NE.0.) |
58 |
baylor |
1.17 |
& .OR.(viscC4leithD.NE.0.) |
59 |
adcroft |
1.6 |
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60 |
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IF (deltaTmom.NE.0.) THEN |
61 |
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vg2=viscAhGrid/deltaTmom |
62 |
baylor |
1.17 |
vg2Min=viscAhGridMin/deltaTmom |
63 |
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vg2Max=viscAhGridMax/deltaTmom |
64 |
adcroft |
1.6 |
vg4=viscA4Grid/deltaTmom |
65 |
dimitri |
1.13 |
vg4Min=viscA4GridMin/deltaTmom |
66 |
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vg4Max=viscA4GridMax/deltaTmom |
67 |
adcroft |
1.6 |
ELSE |
68 |
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vg2=0. |
69 |
baylor |
1.17 |
vg2Min=0. |
70 |
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vg2Max=0. |
71 |
adcroft |
1.6 |
vg4=0. |
72 |
dimitri |
1.13 |
vg4Min=0. |
73 |
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vg4Max=0. |
74 |
adcroft |
1.6 |
ENDIF |
75 |
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76 |
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C - Viscosity |
77 |
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IF (useVariableViscosity) THEN |
78 |
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DO j=2-Oly,sNy+Oly-1 |
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DO i=2-Olx,sNx+Olx-1 |
80 |
jmc |
1.18 |
IF (useFullLeith) THEN |
81 |
baylor |
1.17 |
C This is the vector magnitude of the vorticity gradient squared |
82 |
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grdVrt=0.25*( |
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& ((vort3(i+1,j)-vort3(i,j))*recip_DXG(i,j,bi,bj))**2 |
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& +((vort3(i,j+1)-vort3(i,j))*recip_DYG(i,j,bi,bj))**2 |
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& +((vort3(i+1,j+1)-vort3(i,j+1))*recip_DXG(i,j+1,bi,bj))**2 |
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& +((vort3(i+1,j+1)-vort3(i+1,j))*recip_DYG(i+1,j,bi,bj))**2) |
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88 |
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C This is the vector magnitude of grad (div.v) squared |
89 |
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C Using it in Leith serves to damp instabilities in w. |
90 |
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grdDiv=0.25*( |
91 |
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& ((hDiv(i+1,j)-hDiv(i,j))*recip_DXG(i,j,bi,bj))**2 |
92 |
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& +((hDiv(i,j+1)-hDiv(i,j))*recip_DYG(i,j,bi,bj))**2 |
93 |
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& +((hDiv(i-1,j)-hDiv(i,j))*recip_DXG(i-1,j,bi,bj))**2 |
94 |
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& +((hDiv(i,j-1)-hDiv(i,j))*recip_DYG(i,j-1,bi,bj))**2) |
95 |
jmc |
1.18 |
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96 |
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Alth2=sqrt(viscC2leith**2*grdVrt+viscC2leithD**2*grdDiv) |
97 |
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& *(rA(i,j,bi,bj)**1.5) |
98 |
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Alth4=sqrt(viscC4leith**2*grdVrt+viscC4leithD**2*grdDiv) |
99 |
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& *0.125*(rA(i,j,bi,bj)**2.5) |
100 |
baylor |
1.17 |
ELSE |
101 |
jmc |
1.18 |
C but this approximation will work on cube |
102 |
baylor |
1.17 |
c (and differs by as much as 4X) |
103 |
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grdVrt=abs((vort3(i+1,j)-vort3(i,j))*recip_DXG(i,j,bi,bj)) |
104 |
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grdVrt=max(grdVrt, |
105 |
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& abs((vort3(i,j+1)-vort3(i,j))*recip_DYG(i,j,bi,bj))) |
106 |
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grdVrt=max(grdVrt, |
107 |
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& abs((vort3(i+1,j+1)-vort3(i,j+1))*recip_DXG(i,j+1,bi,bj))) |
108 |
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grdVrt=max(grdVrt, |
109 |
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& abs((vort3(i+1,j+1)-vort3(i+1,j))*recip_DYG(i+1,j,bi,bj))) |
110 |
jmc |
1.18 |
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111 |
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Alth2=viscC2leith*grdVrt*(rA(i,j,bi,bj)**1.5) |
112 |
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Alth4=viscC4leith*grdVrt*0.125*(rA(i,j,bi,bj)**2.5) |
113 |
baylor |
1.17 |
ENDIF |
114 |
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115 |
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C Harmonic Modified Leith on Div.u points |
116 |
jmc |
1.12 |
Alin=viscAhD+vg2*rA ( i , j ,bi,bj) |
117 |
jmc |
1.18 |
viscAh_D(i,j)=min(viscAhMax,Alin+Alth2) |
118 |
baylor |
1.17 |
IF (vg2Max.GT.0.) THEN |
119 |
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AlinMax=vg2Max*(rA ( i , j ,bi,bj)) |
120 |
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viscAh_D(i,j)=min(AlinMax,viscAh_D(i,j)) |
121 |
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ENDIF |
122 |
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AlinMin=vg2Min*(rA ( i , j ,bi,bj)) |
123 |
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viscAh_D(i,j)=max(AlinMin,viscAh_D(i,j)) |
124 |
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125 |
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C BiHarmonic Modified Leith on Div.u points |
126 |
jmc |
1.12 |
Alin=viscA4D+vg4*(rA ( i , j ,bi,bj)**2) |
127 |
jmc |
1.18 |
viscA4_D(i,j)=min(viscA4Max,Alin+Alth4) |
128 |
dimitri |
1.13 |
IF (vg4Max.GT.0.) THEN |
129 |
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AlinMax=vg4Max*(rA ( i , j ,bi,bj)**2) |
130 |
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viscA4_D(i,j)=min(AlinMax,viscA4_D(i,j)) |
131 |
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ENDIF |
132 |
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AlinMin=vg4Min*(rA ( i , j ,bi,bj)**2) |
133 |
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viscA4_D(i,j)=max(AlinMin,viscA4_D(i,j)) |
134 |
adcroft |
1.6 |
|
135 |
baylor |
1.17 |
C This is the vector magnitude of the vorticity gradient squared |
136 |
jmc |
1.18 |
IF (useFullLeith) THEN |
137 |
baylor |
1.17 |
grdVrt=0.25*( |
138 |
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& ((vort3(i+1,j)-vort3(i,j))*recip_DXG(i,j,bi,bj))**2 |
139 |
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& +((vort3(i,j+1)-vort3(i,j))*recip_DYG(i,j,bi,bj))**2 |
140 |
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& +((vort3(i-1,j)-vort3(i,j))*recip_DXG(i-1,j,bi,bj))**2 |
141 |
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& +((vort3(i,j-1)-vort3(i,j))*recip_DYG(i,j-1,bi,bj))**2) |
142 |
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143 |
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C This is the vector magnitude of grad(div.v) squared |
144 |
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grdDiv=0.25*( |
145 |
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& ((hDiv(i+1,j)-hDiv(i,j))*recip_DXG(i,j,bi,bj))**2 |
146 |
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& +((hDiv(i,j+1)-hDiv(i,j))*recip_DYG(i,j,bi,bj))**2 |
147 |
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& +((hDiv(i+1,j+1)-hDiv(i,j+1))*recip_DXG(i,j+1,bi,bj))**2 |
148 |
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& +((hDiv(i+1,j+1)-hDiv(i+1,j))*recip_DYG(i+1,j,bi,bj))**2) |
149 |
jmc |
1.18 |
|
150 |
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Alth2=sqrt(viscC2leith**2*grdVrt+viscC2leithD**2*grdDiv) |
151 |
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& *(rAz(i,j,bi,bj)**1.5) |
152 |
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Alth4=sqrt(viscC4leith**2*grdVrt+viscC4leithD**2*grdDiv) |
153 |
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& *0.125*(rAz(i,j,bi,bj)**2.5) |
154 |
baylor |
1.17 |
ELSE |
155 |
adcroft |
1.6 |
C but this approximation will work on cube (and differs by as much as 4X) |
156 |
baylor |
1.17 |
grdVrt=abs((vort3(i+1,j)-vort3(i,j))*recip_DXG(i,j,bi,bj)) |
157 |
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grdVrt=max(grdVrt, |
158 |
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& abs((vort3(i,j+1)-vort3(i,j))*recip_DYG(i,j,bi,bj))) |
159 |
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grdVrt=max(grdVrt, |
160 |
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& abs((vort3(i-1,j)-vort3(i,j))*recip_DXG(i-1,j,bi,bj))) |
161 |
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grdVrt=max(grdVrt, |
162 |
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& abs((vort3(i,j-1)-vort3(i,j))*recip_DYG(i,j-1,bi,bj))) |
163 |
jmc |
1.18 |
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164 |
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Alth2=viscC2leith*grdVrt*(rAz(i,j,bi,bj)**1.5) |
165 |
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Alth4=viscC4leith*grdVrt*0.125*(rAz(i,j,bi,bj)**2.5) |
166 |
baylor |
1.17 |
ENDIF |
167 |
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168 |
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C Harmonic Modified Leith on Zeta points |
169 |
jmc |
1.12 |
Alin=viscAhZ+vg2*rAz( i , j ,bi,bj) |
170 |
jmc |
1.18 |
viscAh_Z(i,j)=min(viscAhMax,Alin+Alth2) |
171 |
baylor |
1.17 |
IF (vg2Max.GT.0.) THEN |
172 |
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AlinMax=vg2Max*(rAz( i , j ,bi,bj)) |
173 |
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viscAh_Z(i,j)=min(AlinMax,viscAh_Z(i,j)) |
174 |
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ENDIF |
175 |
jmc |
1.18 |
AlinMin=vg2Min*(rAz( i , j ,bi,bj)) |
176 |
baylor |
1.17 |
viscAh_Z(i,j)=max(AlinMin,viscAh_Z(i,j)) |
177 |
adcroft |
1.6 |
|
178 |
baylor |
1.17 |
C BiHarmonic Modified Leith on Zeta Points |
179 |
jmc |
1.12 |
Alin=viscA4Z+vg4*(rAz( i , j ,bi,bj)**2) |
180 |
jmc |
1.18 |
viscA4_Z(i,j)=min(viscA4Max,Alin+Alth4) |
181 |
dimitri |
1.13 |
IF (vg4Max.GT.0.) THEN |
182 |
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AlinMax=vg4Max*(rAz( i , j ,bi,bj)**2) |
183 |
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viscA4_Z(i,j)=min(AlinMax,viscA4_Z(i,j)) |
184 |
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ENDIF |
185 |
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AlinMin=vg4Min*(rAz( i , j ,bi,bj)**2) |
186 |
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viscA4_Z(i,j)=max(AlinMin,viscA4_Z(i,j)) |
187 |
adcroft |
1.6 |
ENDDO |
188 |
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ENDDO |
189 |
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ELSE |
190 |
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DO j=1-Oly,sNy+Oly |
191 |
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DO i=1-Olx,sNx+Olx |
192 |
jmc |
1.12 |
viscAh_D(i,j)=viscAhD |
193 |
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viscAh_Z(i,j)=viscAhZ |
194 |
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viscA4_D(i,j)=viscA4D |
195 |
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viscA4_Z(i,j)=viscA4Z |
196 |
adcroft |
1.6 |
ENDDO |
197 |
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ENDDO |
198 |
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ENDIF |
199 |
adcroft |
1.2 |
|
200 |
jmc |
1.12 |
C - Laplacian terms |
201 |
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IF ( viscC2leith.NE.0. .OR. viscAhGrid.NE.0. |
202 |
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& .OR. viscAhD.NE.0. .OR. viscAhZ.NE.0. ) THEN |
203 |
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DO j=2-Oly,sNy+Oly-1 |
204 |
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DO i=2-Olx,sNx+Olx-1 |
205 |
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206 |
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Dim=hDiv( i ,j-1) |
207 |
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Dij=hDiv( i , j ) |
208 |
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Dmj=hDiv(i-1, j ) |
209 |
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Zip=hFacZ( i ,j+1)*vort3( i ,j+1) |
210 |
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Zij=hFacZ( i , j )*vort3( i , j ) |
211 |
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Zpj=hFacZ(i+1, j )*vort3(i+1, j ) |
212 |
adcroft |
1.2 |
|
213 |
adcroft |
1.4 |
C This bit scales the harmonic dissipation operator to be proportional |
214 |
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C to the grid-cell area over the time-step. viscAh is then non-dimensional |
215 |
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C and should be less than 1/8, for example viscAh=0.01 |
216 |
jmc |
1.12 |
IF (useVariableViscosity) THEN |
217 |
adcroft |
1.6 |
Dij=Dij*viscAh_D(i,j) |
218 |
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Dim=Dim*viscAh_D(i,j-1) |
219 |
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Dmj=Dmj*viscAh_D(i-1,j) |
220 |
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Zij=Zij*viscAh_Z(i,j) |
221 |
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Zip=Zip*viscAh_Z(i,j+1) |
222 |
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Zpj=Zpj*viscAh_Z(i+1,j) |
223 |
adcroft |
1.4 |
uD2 = ( |
224 |
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& cosFacU(j,bi,bj)*( Dij-Dmj )*recip_DXC(i,j,bi,bj) |
225 |
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& -recip_hFacW(i,j,k,bi,bj)*( Zip-Zij )*recip_DYG(i,j,bi,bj) ) |
226 |
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vD2 = ( |
227 |
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& recip_hFacS(i,j,k,bi,bj)*( Zpj-Zij )*recip_DXG(i,j,bi,bj) |
228 |
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& *cosFacV(j,bi,bj) |
229 |
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& +( Dij-Dim )*recip_DYC(i,j,bi,bj) ) |
230 |
jmc |
1.12 |
ELSE |
231 |
|
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uD2 = viscAhD* |
232 |
adcroft |
1.2 |
& cosFacU(j,bi,bj)*( Dij-Dmj )*recip_DXC(i,j,bi,bj) |
233 |
jmc |
1.12 |
& - viscAhZ*recip_hFacW(i,j,k,bi,bj)* |
234 |
|
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& ( Zip-Zij )*recip_DYG(i,j,bi,bj) |
235 |
|
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vD2 = viscAhZ*recip_hFacS(i,j,k,bi,bj)* |
236 |
|
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& cosFacV(j,bi,bj)*( Zpj-Zij )*recip_DXG(i,j,bi,bj) |
237 |
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& + viscAhD* ( Dij-Dim )*recip_DYC(i,j,bi,bj) |
238 |
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ENDIF |
239 |
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240 |
|
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uDissip(i,j) = uD2 |
241 |
|
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vDissip(i,j) = vD2 |
242 |
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243 |
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ENDDO |
244 |
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ENDDO |
245 |
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ELSE |
246 |
|
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DO j=2-Oly,sNy+Oly-1 |
247 |
|
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DO i=2-Olx,sNx+Olx-1 |
248 |
|
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uDissip(i,j) = 0. |
249 |
|
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vDissip(i,j) = 0. |
250 |
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ENDDO |
251 |
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ENDDO |
252 |
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ENDIF |
253 |
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|
254 |
|
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C - Bi-harmonic terms |
255 |
|
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IF ( viscC4leith.NE.0. .OR. viscA4Grid.NE.0. |
256 |
|
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& .OR. viscA4D.NE.0. .OR. viscA4Z.NE.0. ) THEN |
257 |
|
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DO j=2-Oly,sNy+Oly-1 |
258 |
|
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DO i=2-Olx,sNx+Olx-1 |
259 |
adcroft |
1.2 |
|
260 |
jmc |
1.11 |
#ifdef MOM_VI_ORIGINAL_VISCA4 |
261 |
jmc |
1.12 |
Dim=dyF( i ,j-1,bi,bj)*dStar( i ,j-1) |
262 |
|
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Dij=dyF( i , j ,bi,bj)*dStar( i , j ) |
263 |
|
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Dmj=dyF(i-1, j ,bi,bj)*dStar(i-1, j ) |
264 |
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|
265 |
|
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Zip=dxV( i ,j+1,bi,bj)*hFacZ( i ,j+1)*zStar( i ,j+1) |
266 |
|
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Zij=dxV( i , j ,bi,bj)*hFacZ( i , j )*zStar( i , j ) |
267 |
|
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Zpj=dxV(i+1, j ,bi,bj)*hFacZ(i+1, j )*zStar(i+1, j ) |
268 |
jmc |
1.11 |
#else |
269 |
jmc |
1.12 |
Dim=dStar( i ,j-1) |
270 |
|
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Dij=dStar( i , j ) |
271 |
|
|
Dmj=dStar(i-1, j ) |
272 |
|
|
|
273 |
|
|
Zip=hFacZ( i ,j+1)*zStar( i ,j+1) |
274 |
|
|
Zij=hFacZ( i , j )*zStar( i , j ) |
275 |
|
|
Zpj=hFacZ(i+1, j )*zStar(i+1, j ) |
276 |
jmc |
1.11 |
#endif |
277 |
|
|
|
278 |
adcroft |
1.4 |
C This bit scales the harmonic dissipation operator to be proportional |
279 |
|
|
C to the grid-cell area over the time-step. viscAh is then non-dimensional |
280 |
|
|
C and should be less than 1/8, for example viscAh=0.01 |
281 |
jmc |
1.12 |
IF (useVariableViscosity) THEN |
282 |
adcroft |
1.6 |
Dij=Dij*viscA4_D(i,j) |
283 |
|
|
Dim=Dim*viscA4_D(i,j-1) |
284 |
|
|
Dmj=Dmj*viscA4_D(i-1,j) |
285 |
|
|
Zij=Zij*viscA4_Z(i,j) |
286 |
|
|
Zip=Zip*viscA4_Z(i,j+1) |
287 |
|
|
Zpj=Zpj*viscA4_Z(i+1,j) |
288 |
jmc |
1.11 |
|
289 |
|
|
#ifdef MOM_VI_ORIGINAL_VISCA4 |
290 |
adcroft |
1.4 |
uD4 = recip_rAw(i,j,bi,bj)*( |
291 |
|
|
& ( (Dij-Dmj)*cosFacU(j,bi,bj) ) |
292 |
|
|
& -recip_hFacW(i,j,k,bi,bj)*( Zip-Zij ) ) |
293 |
|
|
vD4 = recip_rAs(i,j,bi,bj)*( |
294 |
|
|
& recip_hFacS(i,j,k,bi,bj)*( (Zpj-Zij)*cosFacV(j,bi,bj) ) |
295 |
|
|
& + ( Dij-Dim ) ) |
296 |
jmc |
1.12 |
ELSE |
297 |
adcroft |
1.4 |
uD4 = recip_rAw(i,j,bi,bj)*( |
298 |
adcroft |
1.2 |
& viscA4*( (Dij-Dmj)*cosFacU(j,bi,bj) ) |
299 |
|
|
& -recip_hFacW(i,j,k,bi,bj)*viscA4*( Zip-Zij ) ) |
300 |
adcroft |
1.4 |
vD4 = recip_rAs(i,j,bi,bj)*( |
301 |
adcroft |
1.2 |
& recip_hFacS(i,j,k,bi,bj)*viscA4*( (Zpj-Zij)*cosFacV(j,bi,bj) ) |
302 |
|
|
& + viscA4*( Dij-Dim ) ) |
303 |
jmc |
1.11 |
#else /* MOM_VI_ORIGINAL_VISCA4 */ |
304 |
|
|
uD4 = ( |
305 |
|
|
& cosFacU(j,bi,bj)*( Dij-Dmj )*recip_DXC(i,j,bi,bj) |
306 |
|
|
& -recip_hFacW(i,j,k,bi,bj)*( Zip-Zij )*recip_DYG(i,j,bi,bj) ) |
307 |
|
|
vD4 = ( |
308 |
|
|
& recip_hFacS(i,j,k,bi,bj)*( Zpj-Zij )*recip_DXG(i,j,bi,bj) |
309 |
|
|
& *cosFacV(j,bi,bj) |
310 |
|
|
& +( Dij-Dim )*recip_DYC(i,j,bi,bj) ) |
311 |
jmc |
1.12 |
ELSE |
312 |
jmc |
1.18 |
uD4 = viscA4D* |
313 |
jmc |
1.11 |
& cosFacU(j,bi,bj)*( Dij-Dmj )*recip_DXC(i,j,bi,bj) |
314 |
jmc |
1.12 |
& - viscA4Z*recip_hFacW(i,j,k,bi,bj)* |
315 |
|
|
& ( Zip-Zij )*recip_DYG(i,j,bi,bj) |
316 |
|
|
vD4 = viscA4Z*recip_hFacS(i,j,k,bi,bj)* |
317 |
|
|
& cosFacV(j,bi,bj)*( Zpj-Zij )*recip_DXG(i,j,bi,bj) |
318 |
|
|
& + viscA4D* ( Dij-Dim )*recip_DYC(i,j,bi,bj) |
319 |
jmc |
1.11 |
#endif /* MOM_VI_ORIGINAL_VISCA4 */ |
320 |
jmc |
1.12 |
ENDIF |
321 |
adcroft |
1.2 |
|
322 |
jmc |
1.12 |
uDissip(i,j) = uDissip(i,j) - uD4 |
323 |
|
|
vDissip(i,j) = vDissip(i,j) - vD4 |
324 |
adcroft |
1.2 |
|
325 |
jmc |
1.12 |
ENDDO |
326 |
adcroft |
1.2 |
ENDDO |
327 |
jmc |
1.12 |
ENDIF |
328 |
molod |
1.7 |
|
329 |
|
|
#ifdef ALLOW_DIAGNOSTICS |
330 |
jmc |
1.15 |
IF (useDiagnostics) THEN |
331 |
jmc |
1.16 |
CALL DIAGNOSTICS_FILL(viscAh_D,'VISCAH ',k,1,2,bi,bj,myThid) |
332 |
|
|
CALL DIAGNOSTICS_FILL(viscA4_D,'VISCA4 ',k,1,2,bi,bj,myThid) |
333 |
jmc |
1.15 |
ENDIF |
334 |
molod |
1.7 |
#endif |
335 |
adcroft |
1.2 |
|
336 |
|
|
RETURN |
337 |
|
|
END |