3 |
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4 |
#include "MOM_COMMON_OPTIONS.h" |
#include "MOM_COMMON_OPTIONS.h" |
5 |
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6 |
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7 |
SUBROUTINE MOM_CALC_VISC( |
SUBROUTINE MOM_CALC_VISC( |
8 |
I bi,bj,k, |
I bi,bj,k, |
9 |
O viscAh_Z,viscAh_D,viscA4_Z,viscA4_D, |
O viscAh_Z,viscAh_D,viscA4_Z,viscA4_D, |
10 |
O harmonic,biharmonic,useVariableViscosity, |
O harmonic,biharmonic,useVariableViscosity, |
11 |
I hDiv,vort3,tension,strain,KE, |
I hDiv,vort3,tension,strain,KE,hfacZ, |
12 |
I myThid) |
I myThid) |
13 |
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14 |
IMPLICIT NONE |
IMPLICIT NONE |
15 |
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C |
16 |
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C Calculate horizontal viscosities (L is typical grid width) |
17 |
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C harmonic viscosity= |
18 |
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C viscAh (or viscAhD on div pts and viscAhZ on zeta pts) |
19 |
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C +0.25*L**2*viscAhGrid/deltaT |
20 |
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C +sqrt(viscC2leith**2*grad(Vort3)**2 |
21 |
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C +viscC2leithD**2*grad(hDiv)**2)*L**3 |
22 |
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C +(viscC2smag/pi)**2*L**2*sqrt(Tension**2+Strain**2) |
23 |
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C |
24 |
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C biharmonic viscosity= |
25 |
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C viscA4 (or viscA4D on div pts and viscA4Z on zeta pts) |
26 |
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C +0.25*0.125*L**4*viscA4Grid/deltaT (approx) |
27 |
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C +0.125*L**5*sqrt(viscC4leith**2*grad(Vort3)**2 |
28 |
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C +viscC4leithD**2*grad(hDiv)**2) |
29 |
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C +0.125*L**4*(viscC4smag/pi)**2*sqrt(Tension**2+Strain**2) |
30 |
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C |
31 |
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C Note that often 0.125*L**2 is the scale between harmonic and |
32 |
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C biharmonic (see Griffies and Hallberg (2000)) |
33 |
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C This allows the same value of the coefficient to be used |
34 |
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C for roughly similar results with biharmonic and harmonic |
35 |
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C |
36 |
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C LIMITERS -- limit min and max values of viscosities |
37 |
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C viscAhRemax is min value for grid point harmonic Reynolds num |
38 |
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C harmonic viscosity>sqrt(2*KE)*L/2/viscAhRemax |
39 |
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C |
40 |
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C viscA4Remax is min value for grid point biharmonic Reynolds num |
41 |
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C biharmonic viscosity>sqrt(2*KE)*L**3/16/viscA4Remax |
42 |
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C |
43 |
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C viscAhgridmax is CFL stability limiter for harmonic viscosity |
44 |
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C harmonic viscosity<0.25*viscAhgridmax*L**2/deltaT |
45 |
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C |
46 |
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C viscA4gridmax is CFL stability limiter for biharmonic viscosity |
47 |
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C biharmonic viscosity<viscA4gridmax*L**4/32/deltaT (approx) |
48 |
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C |
49 |
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C viscAhgridmin and viscA4gridmin are lower limits for viscosity: |
50 |
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C harmonic viscosity>0.25*viscAhgridmax*L**2/deltaT |
51 |
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C biharmonic viscosity>viscA4gridmax*L**4/32/deltaT (approx) |
52 |
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C |
53 |
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C RECOMMENDED VALUES |
54 |
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C viscC2Leith=? |
55 |
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C viscC2LeithD=? |
56 |
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C viscC4Leith=? |
57 |
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C viscC4LeithD=? |
58 |
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C viscC2smag=2.2-4 (Griffies and Hallberg,2000) |
59 |
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C 0.2-0.9 (Smagorinsky,1993) |
60 |
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C viscC4smag=2.2-4 (Griffies and Hallberg,2000) |
61 |
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C viscAhRemax>=1 |
62 |
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C viscA4Remax>=1 |
63 |
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C viscAhgridmax=1 |
64 |
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C viscA4gridmax=1 |
65 |
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C viscAhgrid<1 |
66 |
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C viscA4grid<1 |
67 |
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C viscAhgridmin<<1 |
68 |
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C viscA4gridmin<<1 |
69 |
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70 |
C == Global variables == |
C == Global variables == |
71 |
#include "SIZE.h" |
#include "SIZE.h" |
90 |
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91 |
C == Local variables == |
C == Local variables == |
92 |
INTEGER I,J |
INTEGER I,J |
93 |
_RL ASmag2, ASmag4, smag2fac, smag4fac |
_RL smag2fac, smag4fac |
94 |
_RL vg2Min, vg2Max, AlinMax, AlinMin |
_RL viscAhRe_max, viscA4Re_max |
95 |
_RL lenA2, lenAz2 |
_RL Alin,Alinmin,grdVrt,grdDiv |
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_RL Alin,Alth2,Alth4,grdVrt,grdDiv |
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_RL vg2,vg4,vg4Min,vg4Max |
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96 |
_RL recip_dt,L2,L3,L4,L5,L2rdt,L4rdt |
_RL recip_dt,L2,L3,L4,L5,L2rdt,L4rdt |
97 |
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_RL Uscl,U4scl |
98 |
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_RL viscAh_ZMax(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
99 |
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_RL viscAh_DMax(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
100 |
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_RL viscA4_ZMax(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
101 |
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_RL viscA4_DMax(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
102 |
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_RL viscAh_ZMin(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
103 |
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_RL viscAh_DMin(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
104 |
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_RL viscA4_ZMin(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
105 |
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_RL viscA4_DMin(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
106 |
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_RL viscAh_ZLth(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
107 |
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_RL viscAh_DLth(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
108 |
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_RL viscA4_ZLth(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
109 |
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_RL viscA4_DLth(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
110 |
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_RL viscAh_ZLthD(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
111 |
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_RL viscAh_DLthD(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
112 |
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_RL viscA4_ZLthD(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
113 |
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_RL viscA4_DLthD(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
114 |
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_RL viscAh_ZSmg(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
115 |
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_RL viscAh_DSmg(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
116 |
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_RL viscA4_ZSmg(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
117 |
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_RL viscA4_DSmg(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
118 |
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LOGICAL calcLeith,calcSmag |
119 |
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120 |
useVariableViscosity= |
useVariableViscosity= |
121 |
& (viscAhGrid.NE.0.) |
& (viscAhGrid.NE.0.) |
136 |
& .OR.(viscC2leithD.NE.0.) |
& .OR.(viscC2leithD.NE.0.) |
137 |
& .OR.(viscC2smag.NE.0.) |
& .OR.(viscC2smag.NE.0.) |
138 |
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139 |
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IF (harmonic) viscAhre_max=viscAhremax |
140 |
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141 |
biharmonic= |
biharmonic= |
142 |
& (viscA4.NE.0.) |
& (viscA4.NE.0.) |
143 |
& .OR.(viscA4D.NE.0.) |
& .OR.(viscA4D.NE.0.) |
147 |
& .OR.(viscC4leithD.NE.0.) |
& .OR.(viscC4leithD.NE.0.) |
148 |
& .OR.(viscC4smag.NE.0.) |
& .OR.(viscC4smag.NE.0.) |
149 |
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150 |
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IF (biharmonic) viscA4re_max=viscA4remax |
151 |
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152 |
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calcleith= |
153 |
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& (viscC2leith.NE.0.) |
154 |
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& .OR.(viscC2leithD.NE.0.) |
155 |
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& .OR.(viscC4leith.NE.0.) |
156 |
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& .OR.(viscC4leithD.NE.0.) |
157 |
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158 |
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calcsmag= |
159 |
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& (viscC2smag.NE.0.) |
160 |
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& .OR.(viscC4smag.NE.0.) |
161 |
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162 |
IF (deltaTmom.NE.0.) THEN |
IF (deltaTmom.NE.0.) THEN |
163 |
recip_dt=1./deltaTmom |
recip_dt=1./deltaTmom |
164 |
ELSE |
ELSE |
165 |
recip_dt=0. |
recip_dt=0. |
166 |
ENDIF |
ENDIF |
167 |
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|
168 |
vg2=viscAhGrid*recip_dt |
IF (calcsmag) THEN |
169 |
vg2Min=viscAhGridMin*recip_dt |
smag2fac=(viscC2smag/pi)**2 |
170 |
vg2Max=viscAhGridMax*recip_dt |
smag4fac=0.125*(viscC4smag/pi)**2 |
171 |
vg4=viscA4Grid*recip_dt |
ENDIF |
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vg4Min=viscA4GridMin*recip_dt |
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vg4Max=viscA4GridMax*recip_dt |
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smag2fac=(viscC2smag/pi)**2 |
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smag4fac=0.125*(viscC4smag/pi)**2 |
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172 |
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173 |
C - Viscosity |
C - Viscosity |
174 |
IF (useVariableViscosity) THEN |
IF (useVariableViscosity) THEN |
175 |
DO j=2-Oly,sNy+Oly-1 |
DO j=2-Oly,sNy+Oly-1 |
176 |
DO i=2-Olx,sNx+Olx-1 |
DO i=2-Olx,sNx+Olx-1 |
177 |
CCCCCCCCCCCCCCC Divergence Point CalculationsCCCCCCCCCCCCCCCCCCCC |
CCCCCCCCCCCCCCC Divergence Point CalculationsCCCCCCCCCCCCCCCCCCCC |
178 |
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|
179 |
C These are (powers of) length scales |
C These are (powers of) length scales |
180 |
L2=rA(i,j,bi,bj) |
L2=2./((recip_DXF(I,J,bi,bj)**2+recip_DYF(I,J,bi,bj)**2)) |
181 |
L3=(L2**1.5) |
L3=(L2**1.5) |
182 |
L4=(L2**2) |
L4=(L2**2) |
183 |
L5=0.125*(L2**2.5) |
L5=(L2**2.5) |
184 |
IF (useAnisotropicViscAGridMax) THEN |
|
185 |
L2rdt=recip_dt/( 2.*(recip_DXF(I,J,bi,bj)**2 |
L2rdt=0.25*recip_dt*L2 |
186 |
& +recip_DYF(I,J,bi,bj)**2) ) |
|
187 |
L4rdt=recip_dt/( 6.*(recip_DXF(I,J,bi,bj)**4 |
L4rdt=recip_dt/( 6.*(recip_DXF(I,J,bi,bj)**4 |
188 |
& +recip_DYF(I,J,bi,bj)**4) |
& +recip_DYF(I,J,bi,bj)**4) |
189 |
& +8.*((recip_DXF(I,J,bi,bj) |
& +8.*((recip_DXF(I,J,bi,bj) |
190 |
& *recip_DYF(I,J,bi,bj))**2) ) |
& *recip_DYF(I,J,bi,bj))**2) ) |
|
ENDIF |
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191 |
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192 |
IF (useFullLeith) THEN |
C Velocity Reynolds Scale |
193 |
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Uscl=sqrt(KE(i,j)*L2*0.5)/viscAhRe_max |
194 |
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U4scl=0.125*L2*Uscl/viscA4Re_max |
195 |
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196 |
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IF (useFullLeith.and.calcleith) THEN |
197 |
C This is the vector magnitude of the vorticity gradient squared |
C This is the vector magnitude of the vorticity gradient squared |
198 |
grdVrt=0.25*( |
grdVrt=0.25*( |
199 |
& ((vort3(i+1,j)-vort3(i,j))*recip_DXG(i,j,bi,bj))**2 |
& ((vort3(i+1,j)-vort3(i,j))*recip_DXG(i,j,bi,bj))**2 |
203 |
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|
204 |
C This is the vector magnitude of grad (div.v) squared |
C This is the vector magnitude of grad (div.v) squared |
205 |
C Using it in Leith serves to damp instabilities in w. |
C Using it in Leith serves to damp instabilities in w. |
206 |
grdDiv=0.25*( |
grdDiv=0.25*( |
207 |
& ((hDiv(i+1,j)-hDiv(i,j))*recip_DXG(i,j,bi,bj))**2 |
& ((hDiv(i+1,j)-hDiv(i,j))*recip_DXC(i+1,j,bi,bj))**2 |
208 |
& +((hDiv(i,j+1)-hDiv(i,j))*recip_DYG(i,j,bi,bj))**2 |
& +((hDiv(i,j+1)-hDiv(i,j))*recip_DYC(i,j+1,bi,bj))**2 |
209 |
& +((hDiv(i-1,j)-hDiv(i,j))*recip_DXG(i-1,j,bi,bj))**2 |
& +((hDiv(i,j)-hDiv(i-1,j))*recip_DXC(i,j,bi,bj))**2 |
210 |
& +((hDiv(i,j-1)-hDiv(i,j))*recip_DYG(i,j-1,bi,bj))**2) |
& +((hDiv(i,j)-hDiv(i,j-1))*recip_DYC(i,j,bi,bj))**2) |
211 |
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|
212 |
IF ( (viscC2leith**2*grdVrt+viscC2leithD**2*grdDiv) |
viscAh_DLth(i,j)= |
213 |
& .NE. 0. ) THEN |
& sqrt(viscC2leith**2*grdVrt+viscC2leithD**2*grdDiv)*L3 |
214 |
Alth2=sqrt(viscC2leith**2*grdVrt+viscC2leithD**2*grdDiv)*L3 |
viscA4_DLth(i,j)= |
215 |
ELSE |
& sqrt(viscC4leith**2*grdVrt+viscC4leithD**2*grdDiv)*L5 |
216 |
Alth2=0. _d 0 |
viscAh_DLthd(i,j)= |
217 |
ENDIF |
& sqrt(viscC2leithD**2*grdDiv)*L3 |
218 |
IF ( (viscC4leith**2*grdVrt+viscC4leithD**2*grdDiv) |
viscA4_DLthd(i,j)= |
219 |
& .NE. 0. ) THEN |
& sqrt(viscC4leithD**2*grdDiv)*L5 |
220 |
Alth4=sqrt(viscC4leith**2*grdVrt+viscC4leithD**2*grdDiv)*L5 |
ELSEIF (calcleith) THEN |
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ELSE |
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Alth4=0. _d 0 |
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ENDIF |
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ELSE |
|
221 |
C but this approximation will work on cube |
C but this approximation will work on cube |
222 |
c (and differs by as much as 4X) |
c (and differs by as much as 4X) |
223 |
grdVrt=abs((vort3(i+1,j)-vort3(i,j))*recip_DXG(i,j,bi,bj)) |
grdVrt=abs((vort3(i+1,j)-vort3(i,j))*recip_DXG(i,j,bi,bj)) |
224 |
grdVrt=max(grdVrt, |
grdVrt=max(grdVrt, |
225 |
& abs((vort3(i,j+1)-vort3(i,j))*recip_DYG(i,j,bi,bj))) |
& abs((vort3(i,j+1)-vort3(i,j))*recip_DYG(i,j,bi,bj))) |
226 |
grdVrt=max(grdVrt, |
grdVrt=max(grdVrt, |
227 |
& abs((vort3(i+1,j+1)-vort3(i,j+1))*recip_DXG(i,j+1,bi,bj))) |
& abs((vort3(i+1,j+1)-vort3(i,j+1))*recip_DXG(i,j+1,bi,bj))) |
228 |
grdVrt=max(grdVrt, |
grdVrt=max(grdVrt, |
229 |
& abs((vort3(i+1,j+1)-vort3(i+1,j))*recip_DYG(i+1,j,bi,bj))) |
& abs((vort3(i+1,j+1)-vort3(i+1,j))*recip_DYG(i+1,j,bi,bj))) |
230 |
|
|
231 |
grdDiv=abs((hDiv(i+1,j)-hDiv(i,j))*recip_DXG(i,j,bi,bj)) |
grdDiv=abs((hDiv(i+1,j)-hDiv(i,j))*recip_DXC(i+1,j,bi,bj)) |
232 |
grdDiv=max(grdDiv, |
grdDiv=max(grdDiv, |
233 |
& abs((hDiv(i,j+1)-hDiv(i,j))*recip_DYG(i,j,bi,bj))) |
& abs((hDiv(i,j+1)-hDiv(i,j))*recip_DYC(i,j+1,bi,bj))) |
234 |
grdDiv=max(grdDiv, |
grdDiv=max(grdDiv, |
235 |
& abs((hDiv(i-1,j)-hDiv(i,j))*recip_DXG(i-1,j,bi,bj))) |
& abs((hDiv(i,j)-hDiv(i-1,j))*recip_DXC(i,j,bi,bj))) |
236 |
grdDiv=max(grdDiv, |
grdDiv=max(grdDiv, |
237 |
& abs((hDiv(i,j-1)-hDiv(i,j))*recip_DYG(i,j-1,bi,bj))) |
& abs((hDiv(i,j)-hDiv(i,j-1))*recip_DYC(i,j,bi,bj))) |
238 |
|
|
239 |
c This approximation is good to the same order as above... |
c This approximation is good to the same order as above... |
240 |
Alth2=(viscC2leith*grdVrt+(viscC2leithD*grdDiv))*L3 |
viscAh_Dlth(i,j)= |
241 |
Alth4=(viscC4leith*grdVrt+(viscC4leithD*grdDiv))*L5 |
& (viscC2leith*grdVrt+(viscC2leithD*grdDiv))*L3 |
242 |
ENDIF |
viscA4_Dlth(i,j)=0.125* |
243 |
|
& (viscC4leith*grdVrt+(viscC4leithD*grdDiv))*L5 |
244 |
IF (smag2fac.NE.0.) THEN |
viscAh_DlthD(i,j)= |
245 |
Asmag2=smag2fac*L2 |
& ((viscC2leithD*grdDiv))*L3 |
246 |
& *sqrt(tension(i,j)**2 |
viscA4_DlthD(i,j)=0.125* |
247 |
& +0.25*(strain(i+1, j )**2+strain( i ,j+1)**2 |
& ((viscC4leithD*grdDiv))*L5 |
|
& +strain(i-1, j )**2+strain( i ,j-1)**2)) |
|
248 |
ELSE |
ELSE |
249 |
Asmag2=0d0 |
viscAh_Dlth(i,j)=0d0 |
250 |
|
viscA4_Dlth(i,j)=0d0 |
251 |
|
viscAh_DlthD(i,j)=0d0 |
252 |
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viscA4_DlthD(i,j)=0d0 |
253 |
ENDIF |
ENDIF |
254 |
|
|
255 |
IF (smag4fac.NE.0.) THEN |
IF (calcsmag) THEN |
256 |
Asmag4=smag4fac*L4 |
viscAh_DSmg(i,j)=L2 |
257 |
& *sqrt(tension(i,j)**2 |
& *sqrt(tension(i,j)**2 |
258 |
& +0.25*(strain(i+1, j )**2+strain( i ,j+1)**2 |
& +0.25*(strain(i+1, j )**2+strain( i ,j+1)**2 |
259 |
& +strain(i-1, j )**2+strain( i ,j-1)**2)) |
& +strain(i , j )**2+strain(i+1,j+1)**2)) |
260 |
|
viscA4_DSmg(i,j)=smag4fac*L2*viscAh_DSmg(i,j) |
261 |
|
viscAh_DSmg(i,j)=smag2fac*viscAh_DSmg(i,j) |
262 |
ELSE |
ELSE |
263 |
Asmag4=0d0 |
viscAh_DSmg(i,j)=0d0 |
264 |
|
viscA4_DSmg(i,j)=0d0 |
265 |
ENDIF |
ENDIF |
266 |
|
|
267 |
C Harmonic on Div.u points |
C Harmonic on Div.u points |
268 |
Alin=viscAhD+vg2*L2+Alth2+Asmag2 |
Alin=viscAhD+viscAhGrid*L2rdt |
269 |
viscAh_D(i,j)=min(viscAhMax,Alin) |
& +viscAh_DLth(i,j)+viscAh_DSmg(i,j) |
270 |
IF (useAnisotropicViscAGridMax) THEN |
viscAh_DMin(i,j)=max(viscAhGridMin*L2rdt,Uscl) |
271 |
AlinMax=viscAhGridMax*L2rdt |
viscAh_D(i,j)=max(viscAh_DMin(i,j),Alin) |
272 |
viscAh_D(i,j)=min(AlinMax,viscAh_D(i,j)) |
viscAh_DMax(i,j)=min(viscAhGridMax*L2rdt,viscAhMax) |
273 |
ELSE |
viscAh_D(i,j)=min(viscAh_DMax(i,j),viscAh_D(i,j)) |
|
IF (vg2Max.GT.0.) THEN |
|
|
AlinMax=vg2Max*L2 |
|
|
viscAh_D(i,j)=min(AlinMax,viscAh_D(i,j)) |
|
|
ENDIF |
|
|
ENDIF |
|
|
AlinMin=vg2Min*L2 |
|
|
viscAh_D(i,j)=max(AlinMin,viscAh_D(i,j)) |
|
274 |
|
|
275 |
C BiHarmonic on Div.u points |
C BiHarmonic on Div.u points |
276 |
Alin=viscA4D+vg4*L4+Alth4+Asmag4 |
Alin=viscA4D+viscA4Grid*L4rdt |
277 |
viscA4_D(i,j)=min(viscA4Max,Alin) |
& +viscA4_DLth(i,j)+viscA4_DSmg(i,j) |
278 |
IF (useAnisotropicViscAGridMax) THEN |
viscA4_DMin(i,j)=max(viscA4GridMin*L4rdt,U4scl) |
279 |
AlinMax=viscA4GridMax*L4rdt |
viscA4_D(i,j)=max(viscA4_DMin(i,j),Alin) |
280 |
viscA4_D(i,j)=min(AlinMax,viscA4_D(i,j)) |
viscA4_DMax(i,j)=min(viscA4GridMax*L4rdt,viscA4Max) |
281 |
ELSE |
viscA4_D(i,j)=min(viscA4_DMax(i,j),viscA4_D(i,j)) |
|
IF (vg4Max.GT.0.) THEN |
|
|
AlinMax=vg4Max*L4 |
|
|
viscA4_D(i,j)=min(AlinMax,viscA4_D(i,j)) |
|
|
ENDIF |
|
|
ENDIF |
|
|
AlinMin=vg4Min*L4 |
|
|
viscA4_D(i,j)=max(AlinMin,viscA4_D(i,j)) |
|
282 |
|
|
283 |
CCCCCCCCCCCCC Vorticity Point CalculationsCCCCCCCCCCCCCCCCCC |
CCCCCCCCCCCCC Vorticity Point CalculationsCCCCCCCCCCCCCCCCCC |
284 |
C These are (powers of) length scales |
C These are (powers of) length scales |
285 |
L2=rAz(i,j,bi,bj) |
L2=2./((recip_DXV(I,J,bi,bj)**2+recip_DYU(I,J,bi,bj)**2)) |
286 |
L3=(L2**1.5) |
L3=(L2**1.5) |
287 |
L4=(L2**2) |
L4=(L2**2) |
288 |
L5=0.125*(L2**2.5) |
L5=(L2**2.5) |
289 |
IF (useAnisotropicViscAGridMax) THEN |
|
290 |
L2rdt=recip_dt/( 2.*(recip_DXV(I,J,bi,bj)**2 |
L2rdt=0.25*recip_dt*L2 |
291 |
& +recip_DYU(I,J,bi,bj)**2) ) |
L4rdt=recip_dt/ |
292 |
L4rdt=recip_dt/( 6.*(recip_DXV(I,J,bi,bj)**4 |
& ( 6.*(recip_DXF(I,J,bi,bj)**4+recip_DYF(I,J,bi,bj)**4) |
293 |
& +recip_DYU(I,J,bi,bj)**4) |
& +8.*((recip_DXF(I,J,bi,bj)*recip_DYF(I,J,bi,bj))**2)) |
294 |
& +8.*((recip_DXV(I,J,bi,bj) |
|
295 |
& *recip_DYU(I,J,bi,bj))**2) ) |
C Velocity Reynolds Scale |
296 |
ENDIF |
Uscl=sqrt((KE(i,j)+KE(i,j+1)+KE(i+1,j)+KE(i+1,j+1))*L2*0.125)/ |
297 |
|
& viscAhRe_max |
298 |
|
U4scl=0.125*L2*Uscl/viscA4Re_max |
299 |
|
|
300 |
C This is the vector magnitude of the vorticity gradient squared |
C This is the vector magnitude of the vorticity gradient squared |
301 |
IF (useFullLeith) THEN |
IF (useFullLeith.and.calcleith) THEN |
302 |
grdVrt=0.25*( |
grdVrt=0.25*( |
303 |
& ((vort3(i+1,j)-vort3(i,j))*recip_DXG(i,j,bi,bj))**2 |
& ((vort3(i+1,j)-vort3(i,j))*recip_DXG(i,j,bi,bj))**2 |
304 |
& +((vort3(i,j+1)-vort3(i,j))*recip_DYG(i,j,bi,bj))**2 |
& +((vort3(i,j+1)-vort3(i,j))*recip_DYG(i,j,bi,bj))**2 |
305 |
& +((vort3(i-1,j)-vort3(i,j))*recip_DXG(i-1,j,bi,bj))**2 |
& +((vort3(i-1,j)-vort3(i,j))*recip_DXG(i-1,j,bi,bj))**2 |
306 |
& +((vort3(i,j-1)-vort3(i,j))*recip_DYG(i,j-1,bi,bj))**2) |
& +((vort3(i,j-1)-vort3(i,j))*recip_DYG(i,j-1,bi,bj))**2) |
307 |
|
|
308 |
C This is the vector magnitude of grad(div.v) squared |
C This is the vector magnitude of grad(div.v) squared |
309 |
grdDiv=0.25*( |
grdDiv=0.25*( |
310 |
& ((hDiv(i+1,j)-hDiv(i,j))*recip_DXG(i,j,bi,bj))**2 |
& ((hDiv(i,j)-hDiv(i-1,j))*recip_DXC(i,j,bi,bj))**2 |
311 |
& +((hDiv(i,j+1)-hDiv(i,j))*recip_DYG(i,j,bi,bj))**2 |
& +((hDiv(i,j)-hDiv(i,j-1))*recip_DYC(i,j,bi,bj))**2 |
312 |
& +((hDiv(i+1,j+1)-hDiv(i,j+1))*recip_DXG(i,j+1,bi,bj))**2 |
& +((hDiv(i,j-1)-hDiv(i-1,j-1))*recip_DXC(i,j-1,bi,bj))**2 |
313 |
& +((hDiv(i+1,j+1)-hDiv(i+1,j))*recip_DYG(i+1,j,bi,bj))**2) |
& +((hDiv(i-1,j)-hDiv(i-1,j-1))*recip_DYC(i-1,j,bi,bj))**2) |
314 |
|
|
315 |
IF ( (viscC2leith**2*grdVrt+viscC2leithD**2*grdDiv) |
viscAh_ZLth(i,j)= |
316 |
& .NE. 0. ) THEN |
& sqrt(viscC2leith**2*grdVrt+viscC2leithD**2*grdDiv)*L3 |
317 |
Alth2=sqrt(viscC2leith**2*grdVrt+viscC2leithD**2*grdDiv)*L3 |
viscA4_ZLth(i,j)= |
318 |
ELSE |
& sqrt(viscC4leith**2*grdVrt+viscC4leithD**2*grdDiv)*L5 |
319 |
Alth2=0. _d 0 |
viscAh_ZLthD(i,j)= |
320 |
ENDIF |
& sqrt(viscC2leithD**2*grdDiv)*L3 |
321 |
IF ( (viscC4leith**2*grdVrt+viscC4leithD**2*grdDiv) |
viscA4_ZLthD(i,j)= |
322 |
& .NE. 0. ) THEN |
& sqrt(viscC4leithD**2*grdDiv)*L5 |
|
Alth4=sqrt(viscC4leith**2*grdVrt+viscC4leithD**2*grdDiv)*L5 |
|
|
ELSE |
|
|
Alth4=0. _d 0 |
|
|
ENDIF |
|
|
ELSE |
|
|
C but this approximation will work on cube (and differs by 4X) |
|
|
grdVrt=abs((vort3(i+1,j)-vort3(i,j))*recip_DXG(i,j,bi,bj)) |
|
|
grdVrt=max(grdVrt, |
|
|
& abs((vort3(i,j+1)-vort3(i,j))*recip_DYG(i,j,bi,bj))) |
|
|
grdVrt=max(grdVrt, |
|
|
& abs((vort3(i-1,j)-vort3(i,j))*recip_DXG(i-1,j,bi,bj))) |
|
|
grdVrt=max(grdVrt, |
|
|
& abs((vort3(i,j-1)-vort3(i,j))*recip_DYG(i,j-1,bi,bj))) |
|
|
|
|
|
grdDiv=abs((hDiv(i+1,j)-hDiv(i,j))*recip_DXG(i,j,bi,bj)) |
|
|
grdDiv=max(grdDiv, |
|
|
& abs((hDiv(i,j+1)-hDiv(i,j))*recip_DYG(i,j,bi,bj))) |
|
|
grdDiv=max(grdDiv, |
|
|
& abs((hDiv(i+1,j+1)-hDiv(i,j+1))*recip_DXG(i-1,j,bi,bj))) |
|
|
grdDiv=max(grdDiv, |
|
|
& abs((hDiv(i+1,j+1)-hDiv(i+1,j))*recip_DYG(i,j-1,bi,bj))) |
|
|
|
|
|
C This if statement is just to prevent bitwise changes when leithd=0 |
|
|
Alth2=(viscC2leith*grdVrt+(viscC2leithD*grdDiv))*L3 |
|
|
Alth4=(viscC4leith*grdVrt+(viscC4leithD*grdDiv))*L5 |
|
|
ENDIF |
|
323 |
|
|
324 |
IF (smag2fac.NE.0.) THEN |
ELSEIF (calcleith) THEN |
325 |
Asmag2=smag2fac*L2 |
C but this approximation will work on cube (and differs by 4X) |
326 |
& *sqrt(strain(i,j)**2 |
grdVrt=abs((vort3(i+1,j)-vort3(i,j))*recip_DXG(i,j,bi,bj)) |
327 |
& +0.25*(tension( i , j )**2+tension( i ,j+1)**2 |
grdVrt=max(grdVrt, |
328 |
& +tension(i+1, j )**2+tension(i+1,j+1)**2)) |
& abs((vort3(i,j+1)-vort3(i,j))*recip_DYG(i,j,bi,bj))) |
329 |
|
grdVrt=max(grdVrt, |
330 |
|
& abs((vort3(i-1,j)-vort3(i,j))*recip_DXG(i-1,j,bi,bj))) |
331 |
|
grdVrt=max(grdVrt, |
332 |
|
& abs((vort3(i,j-1)-vort3(i,j))*recip_DYG(i,j-1,bi,bj))) |
333 |
|
|
334 |
|
grdDiv=abs((hDiv(i,j)-hDiv(i-1,j))*recip_DXC(i,j,bi,bj)) |
335 |
|
grdDiv=max(grdDiv, |
336 |
|
& abs((hDiv(i,j)-hDiv(i,j-1))*recip_DYC(i,j,bi,bj))) |
337 |
|
grdDiv=max(grdDiv, |
338 |
|
& abs((hDiv(i,j-1)-hDiv(i-1,j-1))*recip_DXG(i,j-1,bi,bj))) |
339 |
|
grdDiv=max(grdDiv, |
340 |
|
& abs((hDiv(i-1,j)-hDiv(i-1,j-1))*recip_DYG(i-1,j,bi,bj))) |
341 |
|
|
342 |
|
viscAh_ZLth(i,j)=(viscC2leith*grdVrt |
343 |
|
& +(viscC2leithD*grdDiv))*L3 |
344 |
|
viscA4_ZLth(i,j)=(viscC4leith*grdVrt |
345 |
|
& +(viscC4leithD*grdDiv))*L5 |
346 |
|
viscAh_ZLthD(i,j)=((viscC2leithD*grdDiv))*L3 |
347 |
|
viscA4_ZLthD(i,j)=((viscC4leithD*grdDiv))*L5 |
348 |
ELSE |
ELSE |
349 |
Asmag2=0d0 |
viscAh_ZLth(i,j)=0d0 |
350 |
|
viscA4_ZLth(i,j)=0d0 |
351 |
|
viscAh_ZLthD(i,j)=0d0 |
352 |
|
viscA4_ZLthD(i,j)=0d0 |
353 |
ENDIF |
ENDIF |
354 |
|
|
355 |
IF (smag4fac.NE.0.) THEN |
IF (calcsmag) THEN |
356 |
Asmag4=smag4fac*L4 |
viscAh_ZSmg(i,j)=L2 |
357 |
& *sqrt(strain(i,j)**2 |
& *sqrt(strain(i,j)**2 |
358 |
& +0.25*(tension( i , j )**2+tension( i ,j+1)**2 |
& +0.25*(tension( i , j )**2+tension( i ,j-1)**2 |
359 |
& +tension(i+1, j )**2+tension(i+1,j+1)**2)) |
& +tension(i-1, j )**2+tension(i-1,j-1)**2)) |
360 |
ELSE |
viscA4_ZSmg(i,j)=smag4fac*L2*viscAh_ZSmg(i,j) |
361 |
Asmag4=0d0 |
viscAh_ZSmg(i,j)=smag2fac*viscAh_ZSmg(i,j) |
362 |
ENDIF |
ENDIF |
363 |
|
|
364 |
C Harmonic on Zeta points |
C Harmonic on Zeta points |
365 |
Alin=viscAhZ+vg2*L2+Alth2+Asmag2 |
Alin=viscAhZ+viscAhGrid*L2rdt |
366 |
viscAh_Z(i,j)=min(viscAhMax,Alin) |
& +viscAh_ZLth(i,j)+viscAh_ZSmg(i,j) |
367 |
IF (useAnisotropicViscAGridMax) THEN |
viscAh_ZMin(i,j)=max(viscAhGridMin*L2rdt,Uscl) |
368 |
AlinMax=viscAhGridMax*L2rdt |
viscAh_Z(i,j)=max(viscAh_ZMin(i,j),Alin) |
369 |
viscAh_Z(i,j)=min(AlinMax,viscAh_Z(i,j)) |
viscAh_ZMax(i,j)=min(viscAhGridMax*L2rdt,viscAhMax) |
370 |
ELSE |
viscAh_Z(i,j)=min(viscAh_ZMax(i,j),viscAh_Z(i,j)) |
371 |
IF (vg2Max.GT.0.) THEN |
|
372 |
AlinMax=vg2Max*L2 |
C BiHarmonic on Zeta points |
373 |
viscAh_Z(i,j)=min(AlinMax,viscAh_Z(i,j)) |
Alin=viscA4Z+viscA4Grid*L4rdt |
374 |
ENDIF |
& +viscA4_ZLth(i,j)+viscA4_ZSmg(i,j) |
375 |
ENDIF |
viscA4_ZMin(i,j)=max(viscA4GridMin*L4rdt,U4scl) |
376 |
AlinMin=vg2Min*L2 |
viscA4_Z(i,j)=max(viscA4_ZMin(i,j),Alin) |
377 |
viscAh_Z(i,j)=max(AlinMin,viscAh_Z(i,j)) |
viscA4_ZMax(i,j)=min(viscA4GridMax*L4rdt,viscA4Max) |
378 |
|
viscA4_Z(i,j)=min(viscA4_ZMax(i,j),viscA4_Z(i,j)) |
|
C BiHarmonic on Zeta Points |
|
|
Alin=viscA4Z+vg4*L4+Alth4+Asmag4 |
|
|
viscA4_Z(i,j)=min(viscA4Max,Alin) |
|
|
IF (useAnisotropicViscAGridMax) THEN |
|
|
AlinMax=viscA4GridMax*L4rdt |
|
|
viscA4_Z(i,j)=min(AlinMax,viscA4_Z(i,j)) |
|
|
ELSE |
|
|
IF (vg4Max.GT.0.) THEN |
|
|
AlinMax=vg4Max*L4 |
|
|
viscA4_Z(i,j)=min(AlinMax,viscA4_Z(i,j)) |
|
|
ENDIF |
|
|
ENDIF |
|
|
AlinMin=vg4Min*L4 |
|
|
viscA4_Z(i,j)=max(AlinMin,viscA4_Z(i,j)) |
|
379 |
ENDDO |
ENDDO |
380 |
ENDDO |
ENDDO |
381 |
ELSE |
ELSE |
395 |
CALL DIAGNOSTICS_FILL(viscA4_D,'VISCA4D ',k,1,2,bi,bj,myThid) |
CALL DIAGNOSTICS_FILL(viscA4_D,'VISCA4D ',k,1,2,bi,bj,myThid) |
396 |
CALL DIAGNOSTICS_FILL(viscAh_Z,'VISCAHZ ',k,1,2,bi,bj,myThid) |
CALL DIAGNOSTICS_FILL(viscAh_Z,'VISCAHZ ',k,1,2,bi,bj,myThid) |
397 |
CALL DIAGNOSTICS_FILL(viscA4_Z,'VISCA4Z ',k,1,2,bi,bj,myThid) |
CALL DIAGNOSTICS_FILL(viscA4_Z,'VISCA4Z ',k,1,2,bi,bj,myThid) |
398 |
|
|
399 |
|
CALL DIAGNOSTICS_FILL(viscAh_DMax,'VAHDMAX ',k,1,2,bi,bj,myThid) |
400 |
|
CALL DIAGNOSTICS_FILL(viscA4_DMax,'VA4DMAX ',k,1,2,bi,bj,myThid) |
401 |
|
CALL DIAGNOSTICS_FILL(viscAh_ZMax,'VAHZMAX ',k,1,2,bi,bj,myThid) |
402 |
|
CALL DIAGNOSTICS_FILL(viscA4_ZMax,'VA4ZMAX ',k,1,2,bi,bj,myThid) |
403 |
|
|
404 |
|
CALL DIAGNOSTICS_FILL(viscAh_DMin,'VAHDMIN ',k,1,2,bi,bj,myThid) |
405 |
|
CALL DIAGNOSTICS_FILL(viscA4_DMin,'VA4DMIN ',k,1,2,bi,bj,myThid) |
406 |
|
CALL DIAGNOSTICS_FILL(viscAh_ZMin,'VAHZMIN ',k,1,2,bi,bj,myThid) |
407 |
|
CALL DIAGNOSTICS_FILL(viscA4_ZMin,'VA4ZMIN ',k,1,2,bi,bj,myThid) |
408 |
|
|
409 |
|
CALL DIAGNOSTICS_FILL(viscAh_DLth,'VAHDLTH ',k,1,2,bi,bj,myThid) |
410 |
|
CALL DIAGNOSTICS_FILL(viscA4_DLth,'VA4DLTH ',k,1,2,bi,bj,myThid) |
411 |
|
CALL DIAGNOSTICS_FILL(viscAh_ZLth,'VAHZLTH ',k,1,2,bi,bj,myThid) |
412 |
|
CALL DIAGNOSTICS_FILL(viscA4_ZLth,'VA4ZLTH ',k,1,2,bi,bj,myThid) |
413 |
|
|
414 |
|
CALL DIAGNOSTICS_FILL(viscAh_DLthD,'VAHDLTHD',k,1,2,bi,bj,myThid) |
415 |
|
CALL DIAGNOSTICS_FILL(viscA4_DLthD,'VA4DLTHD',k,1,2,bi,bj,myThid) |
416 |
|
CALL DIAGNOSTICS_FILL(viscAh_ZLthD,'VAHZLTHD',k,1,2,bi,bj,myThid) |
417 |
|
CALL DIAGNOSTICS_FILL(viscA4_ZLthD,'VA4ZLTHD',k,1,2,bi,bj,myThid) |
418 |
|
|
419 |
|
CALL DIAGNOSTICS_FILL(viscAh_DSmg,'VAHDSMAG',k,1,2,bi,bj,myThid) |
420 |
|
CALL DIAGNOSTICS_FILL(viscA4_DSmg,'VA4DSMAG',k,1,2,bi,bj,myThid) |
421 |
|
CALL DIAGNOSTICS_FILL(viscAh_ZSmg,'VAHZSMAG',k,1,2,bi,bj,myThid) |
422 |
|
CALL DIAGNOSTICS_FILL(viscA4_ZSmg,'VA4ZSMAG',k,1,2,bi,bj,myThid) |
423 |
ENDIF |
ENDIF |
424 |
#endif |
#endif |
425 |
|
|
426 |
RETURN |
RETURN |
427 |
END |
END |
428 |
|
|