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,hfacZ, |
I hDiv,vort3,tension,strain,KE,hFacZ, |
12 |
I myThid) |
I myThid) |
13 |
|
|
14 |
IMPLICIT NONE |
IMPLICIT NONE |
35 |
C |
C |
36 |
C LIMITERS -- limit min and max values of viscosities |
C LIMITERS -- limit min and max values of viscosities |
37 |
C viscAhRemax is min value for grid point harmonic Reynolds num |
C viscAhRemax is min value for grid point harmonic Reynolds num |
38 |
C harmonic viscosity>sqrt(2*KE)*L/2/viscAhRemax |
C harmonic viscosity>sqrt(2*KE)*L/viscAhRemax |
39 |
C |
C |
40 |
C viscA4Remax is min value for grid point biharmonic Reynolds num |
C viscA4Remax is min value for grid point biharmonic Reynolds num |
41 |
C biharmonic viscosity>sqrt(2*KE)*L**3/16/viscA4Remax |
C biharmonic viscosity>sqrt(2*KE)*L**3/8/viscA4Remax |
42 |
C |
C |
43 |
C viscAhgridmax is CFL stability limiter for harmonic viscosity |
C viscAhgridmax is CFL stability limiter for harmonic viscosity |
44 |
C harmonic viscosity<0.25*viscAhgridmax*L**2/deltaT |
C harmonic viscosity<0.25*viscAhgridmax*L**2/deltaT |
58 |
C viscC2smag=2.2-4 (Griffies and Hallberg,2000) |
C viscC2smag=2.2-4 (Griffies and Hallberg,2000) |
59 |
C 0.2-0.9 (Smagorinsky,1993) |
C 0.2-0.9 (Smagorinsky,1993) |
60 |
C viscC4smag=2.2-4 (Griffies and Hallberg,2000) |
C viscC4smag=2.2-4 (Griffies and Hallberg,2000) |
61 |
C viscAhRemax>=1 |
C viscAhRemax>=1, (<2 suppresses a computational mode) |
62 |
C viscA4Remax>=1 |
C viscA4Remax>=1, (<2 suppresses a computational mode) |
63 |
C viscAhgridmax=1 |
C viscAhgridmax=1 |
64 |
C viscA4gridmax=1 |
C viscA4gridmax=1 |
65 |
C viscAhgrid<1 |
C viscAhgrid<1 |
92 |
INTEGER I,J |
INTEGER I,J |
93 |
_RL smag2fac, smag4fac |
_RL smag2fac, smag4fac |
94 |
_RL viscAhRe_max, viscA4Re_max |
_RL viscAhRe_max, viscA4Re_max |
95 |
_RL Alin,Alinmin,grdVrt,grdDiv |
_RL Alin,grdVrt,grdDiv, keZpt |
96 |
_RL recip_dt,L2,L3,L4,L5,L2rdt,L4rdt |
_RL recip_dt,L2,L3,L4,L5,L2rdt,L4rdt |
97 |
_RL Uscl,U4scl |
_RL Uscl,U4scl |
98 |
_RL viscAh_ZMax(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
_RL viscAh_ZMax(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
136 |
& .OR.(viscC2leithD.NE.0.) |
& .OR.(viscC2leithD.NE.0.) |
137 |
& .OR.(viscC2smag.NE.0.) |
& .OR.(viscC2smag.NE.0.) |
138 |
|
|
139 |
IF (harmonic) viscAhre_max=viscAhremax |
IF ((harmonic).and.(viscAhremax.ne.0.)) THEN |
140 |
|
viscAhre_max=sqrt(2. _d 0)/viscAhRemax |
141 |
|
ELSE |
142 |
|
viscAhre_max=0. _d 0 |
143 |
|
ENDIF |
144 |
|
|
145 |
biharmonic= |
biharmonic= |
146 |
& (viscA4.NE.0.) |
& (viscA4.NE.0.) |
151 |
& .OR.(viscC4leithD.NE.0.) |
& .OR.(viscC4leithD.NE.0.) |
152 |
& .OR.(viscC4smag.NE.0.) |
& .OR.(viscC4smag.NE.0.) |
153 |
|
|
154 |
IF (biharmonic) viscA4re_max=viscA4remax |
IF ((biharmonic).and.(viscA4remax.ne.0.)) THEN |
155 |
|
viscA4re_max=0.125 _d 0*sqrt(2. _d 0)/viscA4Remax |
156 |
|
ELSE |
157 |
|
viscA4re_max=0. _d 0 |
158 |
|
ENDIF |
159 |
|
|
160 |
calcleith= |
calcleith= |
161 |
& (viscC2leith.NE.0.) |
& (viscC2leith.NE.0.) |
168 |
& .OR.(viscC4smag.NE.0.) |
& .OR.(viscC4smag.NE.0.) |
169 |
|
|
170 |
IF (deltaTmom.NE.0.) THEN |
IF (deltaTmom.NE.0.) THEN |
171 |
recip_dt=1./deltaTmom |
recip_dt=1. _d 0/deltaTmom |
172 |
ELSE |
ELSE |
173 |
recip_dt=0. |
recip_dt=0. _d 0 |
174 |
ENDIF |
ENDIF |
175 |
|
|
176 |
IF (calcsmag) THEN |
IF (calcsmag) THEN |
177 |
smag2fac=(viscC2smag/pi)**2 |
smag2fac=(viscC2smag/pi)**2 |
178 |
smag4fac=0.125*(viscC4smag/pi)**2 |
smag4fac=0.125 _d 0*(viscC4smag/pi)**2 |
179 |
|
ELSE |
180 |
|
smag2fac=0. _d 0 |
181 |
|
smag4fac=0. _d 0 |
182 |
ENDIF |
ENDIF |
183 |
|
|
184 |
C - Viscosity |
C - Viscosity |
188 |
CCCCCCCCCCCCCCC Divergence Point CalculationsCCCCCCCCCCCCCCCCCCCC |
CCCCCCCCCCCCCCC Divergence Point CalculationsCCCCCCCCCCCCCCCCCCCC |
189 |
|
|
190 |
C These are (powers of) length scales |
C These are (powers of) length scales |
191 |
L2=2./((recip_DXF(I,J,bi,bj)**2+recip_DYF(I,J,bi,bj)**2)) |
IF (useAreaViscLength) THEN |
192 |
|
L2=rA(i,j,bi,bj) |
193 |
|
ELSE |
194 |
|
L2=2. _d 0/((recip_DXF(I,J,bi,bj)**2+recip_DYF(I,J,bi,bj)**2)) |
195 |
|
ENDIF |
196 |
L3=(L2**1.5) |
L3=(L2**1.5) |
197 |
L4=(L2**2) |
L4=(L2**2) |
198 |
L5=(L2**2.5) |
L5=(L2**2.5) |
199 |
|
|
200 |
L2rdt=0.25*recip_dt*L2 |
L2rdt=0.25 _d 0*recip_dt*L2 |
201 |
|
|
202 |
L4rdt=recip_dt/( 6.*(recip_DXF(I,J,bi,bj)**4 |
IF (useAreaViscLength) THEN |
203 |
& +recip_DYF(I,J,bi,bj)**4) |
L4rdt=0.125 _d 0*recip_dt*rA(i,j,bi,bj)**2 |
204 |
& +8.*((recip_DXF(I,J,bi,bj) |
ELSE |
205 |
& *recip_DYF(I,J,bi,bj))**2) ) |
L4rdt=recip_dt/( 6. _d 0*(recip_DXF(I,J,bi,bj)**4 |
206 |
|
& +recip_DYF(I,J,bi,bj)**4) |
207 |
|
& +8. _d 0*((recip_DXF(I,J,bi,bj) |
208 |
|
& *recip_DYF(I,J,bi,bj))**2) ) |
209 |
|
ENDIF |
210 |
|
|
211 |
C Velocity Reynolds Scale |
C Velocity Reynolds Scale |
212 |
Uscl=sqrt(KE(i,j)*L2*0.5)/viscAhRe_max |
IF ( viscAhRe_max.GT.0. .AND. KE(i,j).GT.0. ) THEN |
213 |
U4scl=0.125*L2*Uscl/viscA4Re_max |
Uscl=sqrt(KE(i,j)*L2)*viscAhRe_max |
214 |
|
ELSE |
215 |
|
Uscl=0. |
216 |
|
ENDIF |
217 |
|
IF ( viscA4Re_max.GT.0. .AND. KE(i,j).GT.0. ) THEN |
218 |
|
U4scl=sqrt(KE(i,j))*L3*viscA4Re_max |
219 |
|
ELSE |
220 |
|
U4scl=0. |
221 |
|
ENDIF |
222 |
|
|
223 |
IF (useFullLeith.and.calcleith) THEN |
IF (useFullLeith.and.calcleith) THEN |
224 |
C This is the vector magnitude of the vorticity gradient squared |
C This is the vector magnitude of the vorticity gradient squared |
225 |
grdVrt=0.25*( |
grdVrt=0.25 _d 0*( |
226 |
& ((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 |
227 |
& +((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 |
228 |
& +((vort3(i+1,j+1)-vort3(i,j+1))*recip_DXG(i,j+1,bi,bj))**2 |
& +((vort3(i+1,j+1)-vort3(i,j+1)) |
229 |
& +((vort3(i+1,j+1)-vort3(i+1,j))*recip_DYG(i+1,j,bi,bj))**2) |
& *recip_DXG(i,j+1,bi,bj))**2 |
230 |
|
& +((vort3(i+1,j+1)-vort3(i+1,j)) |
231 |
|
& *recip_DYG(i+1,j,bi,bj))**2) |
232 |
|
|
233 |
C This is the vector magnitude of grad (div.v) squared |
C This is the vector magnitude of grad (div.v) squared |
234 |
C Using it in Leith serves to damp instabilities in w. |
C Using it in Leith serves to damp instabilities in w. |
235 |
grdDiv=0.25*( |
grdDiv=0.25 _d 0*( |
236 |
& ((hDiv(i+1,j)-hDiv(i,j))*recip_DXC(i+1,j,bi,bj))**2 |
& ((hDiv(i+1,j)-hDiv(i,j))*recip_DXC(i+1,j,bi,bj))**2 |
237 |
& +((hDiv(i,j+1)-hDiv(i,j))*recip_DYC(i,j+1,bi,bj))**2 |
& +((hDiv(i,j+1)-hDiv(i,j))*recip_DYC(i,j+1,bi,bj))**2 |
238 |
& +((hDiv(i,j)-hDiv(i-1,j))*recip_DXC(i,j,bi,bj))**2 |
& +((hDiv(i,j)-hDiv(i-1,j))*recip_DXC(i,j,bi,bj))**2 |
240 |
|
|
241 |
viscAh_DLth(i,j)= |
viscAh_DLth(i,j)= |
242 |
& sqrt(viscC2leith**2*grdVrt+viscC2leithD**2*grdDiv)*L3 |
& sqrt(viscC2leith**2*grdVrt+viscC2leithD**2*grdDiv)*L3 |
243 |
viscA4_DLth(i,j)= |
viscA4_DLth(i,j)=0.125 _d 0* |
244 |
& sqrt(viscC4leith**2*grdVrt+viscC4leithD**2*grdDiv)*L5 |
& sqrt(viscC4leith**2*grdVrt+viscC4leithD**2*grdDiv)*L5 |
245 |
viscAh_DLthd(i,j)= |
viscAh_DLthd(i,j)= |
246 |
& sqrt(viscC2leithD**2*grdDiv)*L3 |
& sqrt(viscC2leithD**2*grdDiv)*L3 |
247 |
viscA4_DLthd(i,j)= |
viscA4_DLthd(i,j)=0.125 _d 0* |
248 |
& sqrt(viscC4leithD**2*grdDiv)*L5 |
& sqrt(viscC4leithD**2*grdDiv)*L5 |
249 |
ELSEIF (calcleith) THEN |
ELSEIF (calcleith) THEN |
250 |
C but this approximation will work on cube |
C but this approximation will work on cube |
268 |
c This approximation is good to the same order as above... |
c This approximation is good to the same order as above... |
269 |
viscAh_Dlth(i,j)= |
viscAh_Dlth(i,j)= |
270 |
& (viscC2leith*grdVrt+(viscC2leithD*grdDiv))*L3 |
& (viscC2leith*grdVrt+(viscC2leithD*grdDiv))*L3 |
271 |
viscA4_Dlth(i,j)=0.125* |
viscA4_Dlth(i,j)=0.125 _d 0* |
272 |
& (viscC4leith*grdVrt+(viscC4leithD*grdDiv))*L5 |
& (viscC4leith*grdVrt+(viscC4leithD*grdDiv))*L5 |
273 |
viscAh_DlthD(i,j)= |
viscAh_DlthD(i,j)= |
274 |
& ((viscC2leithD*grdDiv))*L3 |
& ((viscC2leithD*grdDiv))*L3 |
275 |
viscA4_DlthD(i,j)=0.125* |
viscA4_DlthD(i,j)=0.125 _d 0* |
276 |
& ((viscC4leithD*grdDiv))*L5 |
& ((viscC4leithD*grdDiv))*L5 |
277 |
ELSE |
ELSE |
278 |
viscAh_Dlth(i,j)=0d0 |
viscAh_Dlth(i,j)=0. _d 0 |
279 |
viscA4_Dlth(i,j)=0d0 |
viscA4_Dlth(i,j)=0. _d 0 |
280 |
viscAh_DlthD(i,j)=0d0 |
viscAh_DlthD(i,j)=0. _d 0 |
281 |
viscA4_DlthD(i,j)=0d0 |
viscA4_DlthD(i,j)=0. _d 0 |
282 |
ENDIF |
ENDIF |
283 |
|
|
284 |
IF (calcsmag) THEN |
IF (calcsmag) THEN |
285 |
viscAh_DSmg(i,j)=L2 |
viscAh_DSmg(i,j)=L2 |
286 |
& *sqrt(tension(i,j)**2 |
& *sqrt(tension(i,j)**2 |
287 |
& +0.25*(strain(i+1, j )**2+strain( i ,j+1)**2 |
& +0.25 _d 0*(strain(i+1, j )**2+strain( i ,j+1)**2 |
288 |
& +strain(i , j )**2+strain(i+1,j+1)**2)) |
& +strain(i , j )**2+strain(i+1,j+1)**2)) |
289 |
viscA4_DSmg(i,j)=smag4fac*L2*viscAh_DSmg(i,j) |
viscA4_DSmg(i,j)=smag4fac*L2*viscAh_DSmg(i,j) |
290 |
viscAh_DSmg(i,j)=smag2fac*viscAh_DSmg(i,j) |
viscAh_DSmg(i,j)=smag2fac*viscAh_DSmg(i,j) |
291 |
ELSE |
ELSE |
292 |
viscAh_DSmg(i,j)=0d0 |
viscAh_DSmg(i,j)=0. _d 0 |
293 |
viscA4_DSmg(i,j)=0d0 |
viscA4_DSmg(i,j)=0. _d 0 |
294 |
ENDIF |
ENDIF |
295 |
|
|
296 |
C Harmonic on Div.u points |
C Harmonic on Div.u points |
311 |
|
|
312 |
CCCCCCCCCCCCC Vorticity Point CalculationsCCCCCCCCCCCCCCCCCC |
CCCCCCCCCCCCC Vorticity Point CalculationsCCCCCCCCCCCCCCCCCC |
313 |
C These are (powers of) length scales |
C These are (powers of) length scales |
314 |
L2=2./((recip_DXV(I,J,bi,bj)**2+recip_DYU(I,J,bi,bj)**2)) |
IF (useAreaViscLength) THEN |
315 |
|
L2=rAz(i,j,bi,bj) |
316 |
|
ELSE |
317 |
|
L2=2. _d 0/((recip_DXV(I,J,bi,bj)**2+recip_DYU(I,J,bi,bj)**2)) |
318 |
|
ENDIF |
319 |
|
|
320 |
L3=(L2**1.5) |
L3=(L2**1.5) |
321 |
L4=(L2**2) |
L4=(L2**2) |
322 |
L5=(L2**2.5) |
L5=(L2**2.5) |
323 |
|
|
324 |
L2rdt=0.25*recip_dt*L2 |
L2rdt=0.25 _d 0*recip_dt*L2 |
325 |
L4rdt=recip_dt/ |
IF (useAreaViscLength) THEN |
326 |
& ( 6.*(recip_DXF(I,J,bi,bj)**4+recip_DYF(I,J,bi,bj)**4) |
L4rdt=0.125 _d 0*recip_dt*rAz(i,j,bi,bj)**2 |
327 |
& +8.*((recip_DXF(I,J,bi,bj)*recip_DYF(I,J,bi,bj))**2)) |
ELSE |
328 |
|
L4rdt=recip_dt/ |
329 |
|
& ( 6. _d 0*(recip_DXV(I,J,bi,bj)**4+recip_DYU(I,J,bi,bj)**4) |
330 |
|
& +8. _d 0*((recip_DXV(I,J,bi,bj)*recip_DYU(I,J,bi,bj))**2)) |
331 |
|
ENDIF |
332 |
|
|
333 |
C Velocity Reynolds Scale |
C Velocity Reynolds Scale (Pb here at CS-grid corners !) |
334 |
Uscl=sqrt((KE(i,j)+KE(i,j+1)+KE(i+1,j)+KE(i+1,j+1))*L2*0.125)/ |
IF ( viscAhRe_max.GT.0. .OR. viscA4Re_max.GT.0. ) THEN |
335 |
& viscAhRe_max |
keZpt=0.25 _d 0*( (KE(i,j)+KE(i-1,j-1)) |
336 |
U4scl=0.125*L2*Uscl/viscA4Re_max |
& +(KE(i-1,j)+KE(i,j-1)) ) |
337 |
|
IF ( keZpt.GT.0. ) THEN |
338 |
|
Uscl = sqrt(keZpt*L2)*viscAhRe_max |
339 |
|
U4scl= sqrt(keZpt)*L3*viscA4Re_max |
340 |
|
ELSE |
341 |
|
Uscl =0. |
342 |
|
U4scl=0. |
343 |
|
ENDIF |
344 |
|
ELSE |
345 |
|
Uscl =0. |
346 |
|
U4scl=0. |
347 |
|
ENDIF |
348 |
|
|
349 |
C This is the vector magnitude of the vorticity gradient squared |
C This is the vector magnitude of the vorticity gradient squared |
350 |
IF (useFullLeith.and.calcleith) THEN |
IF (useFullLeith.and.calcleith) THEN |
351 |
grdVrt=0.25*( |
grdVrt=0.25 _d 0*( |
352 |
& ((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 |
353 |
& +((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 |
354 |
& +((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 |
355 |
& +((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) |
356 |
|
|
357 |
C This is the vector magnitude of grad(div.v) squared |
C This is the vector magnitude of grad(div.v) squared |
358 |
grdDiv=0.25*( |
grdDiv=0.25 _d 0*( |
359 |
& ((hDiv(i,j)-hDiv(i-1,j))*recip_DXC(i,j,bi,bj))**2 |
& ((hDiv(i,j)-hDiv(i-1,j))*recip_DXC(i,j,bi,bj))**2 |
360 |
& +((hDiv(i,j)-hDiv(i,j-1))*recip_DYC(i,j,bi,bj))**2 |
& +((hDiv(i,j)-hDiv(i,j-1))*recip_DYC(i,j,bi,bj))**2 |
361 |
& +((hDiv(i,j-1)-hDiv(i-1,j-1))*recip_DXC(i,j-1,bi,bj))**2 |
& +((hDiv(i,j-1)-hDiv(i-1,j-1))*recip_DXC(i,j-1,bi,bj))**2 |
363 |
|
|
364 |
viscAh_ZLth(i,j)= |
viscAh_ZLth(i,j)= |
365 |
& sqrt(viscC2leith**2*grdVrt+viscC2leithD**2*grdDiv)*L3 |
& sqrt(viscC2leith**2*grdVrt+viscC2leithD**2*grdDiv)*L3 |
366 |
viscA4_ZLth(i,j)= |
viscA4_ZLth(i,j)=0.125 _d 0* |
367 |
& sqrt(viscC4leith**2*grdVrt+viscC4leithD**2*grdDiv)*L5 |
& sqrt(viscC4leith**2*grdVrt+viscC4leithD**2*grdDiv)*L5 |
368 |
viscAh_ZLthD(i,j)= |
viscAh_ZLthD(i,j)= |
369 |
& sqrt(viscC2leithD**2*grdDiv)*L3 |
& sqrt(viscC2leithD**2*grdDiv)*L3 |
370 |
viscA4_ZLthD(i,j)= |
viscA4_ZLthD(i,j)=0.125 _d 0* |
371 |
& sqrt(viscC4leithD**2*grdDiv)*L5 |
& sqrt(viscC4leithD**2*grdDiv)*L5 |
372 |
|
|
373 |
ELSEIF (calcleith) THEN |
ELSEIF (calcleith) THEN |
384 |
grdDiv=max(grdDiv, |
grdDiv=max(grdDiv, |
385 |
& abs((hDiv(i,j)-hDiv(i,j-1))*recip_DYC(i,j,bi,bj))) |
& abs((hDiv(i,j)-hDiv(i,j-1))*recip_DYC(i,j,bi,bj))) |
386 |
grdDiv=max(grdDiv, |
grdDiv=max(grdDiv, |
387 |
& abs((hDiv(i,j-1)-hDiv(i-1,j-1))*recip_DXG(i,j-1,bi,bj))) |
& abs((hDiv(i,j-1)-hDiv(i-1,j-1))*recip_DXC(i,j-1,bi,bj))) |
388 |
grdDiv=max(grdDiv, |
grdDiv=max(grdDiv, |
389 |
& abs((hDiv(i-1,j)-hDiv(i-1,j-1))*recip_DYG(i-1,j,bi,bj))) |
& abs((hDiv(i-1,j)-hDiv(i-1,j-1))*recip_DYC(i-1,j,bi,bj))) |
390 |
|
|
391 |
viscAh_ZLth(i,j)=(viscC2leith*grdVrt |
viscAh_ZLth(i,j)=(viscC2leith*grdVrt |
392 |
& +(viscC2leithD*grdDiv))*L3 |
& +(viscC2leithD*grdDiv))*L3 |
393 |
viscA4_ZLth(i,j)=(viscC4leith*grdVrt |
viscA4_ZLth(i,j)=0.125 _d 0*(viscC4leith*grdVrt |
394 |
& +(viscC4leithD*grdDiv))*L5 |
& +(viscC4leithD*grdDiv))*L5 |
395 |
viscAh_ZLthD(i,j)=((viscC2leithD*grdDiv))*L3 |
viscAh_ZLthD(i,j)=((viscC2leithD*grdDiv))*L3 |
396 |
viscA4_ZLthD(i,j)=((viscC4leithD*grdDiv))*L5 |
viscA4_ZLthD(i,j)=0.125 _d 0*((viscC4leithD*grdDiv))*L5 |
397 |
ELSE |
ELSE |
398 |
viscAh_ZLth(i,j)=0d0 |
viscAh_ZLth(i,j)=0. _d 0 |
399 |
viscA4_ZLth(i,j)=0d0 |
viscA4_ZLth(i,j)=0. _d 0 |
400 |
viscAh_ZLthD(i,j)=0d0 |
viscAh_ZLthD(i,j)=0. _d 0 |
401 |
viscA4_ZLthD(i,j)=0d0 |
viscA4_ZLthD(i,j)=0. _d 0 |
402 |
ENDIF |
ENDIF |
403 |
|
|
404 |
IF (calcsmag) THEN |
IF (calcsmag) THEN |
405 |
viscAh_ZSmg(i,j)=L2 |
viscAh_ZSmg(i,j)=L2 |
406 |
& *sqrt(strain(i,j)**2 |
& *sqrt(strain(i,j)**2 |
407 |
& +0.25*(tension( i , j )**2+tension( i ,j-1)**2 |
& +0.25 _d 0*(tension( i , j )**2+tension( i ,j-1)**2 |
408 |
& +tension(i-1, j )**2+tension(i-1,j-1)**2)) |
& +tension(i-1, j )**2+tension(i-1,j-1)**2)) |
409 |
viscA4_ZSmg(i,j)=smag4fac*L2*viscAh_ZSmg(i,j) |
viscA4_ZSmg(i,j)=smag4fac*L2*viscAh_ZSmg(i,j) |
410 |
viscAh_ZSmg(i,j)=smag2fac*viscAh_ZSmg(i,j) |
viscAh_ZSmg(i,j)=smag2fac*viscAh_ZSmg(i,j) |
411 |
ENDIF |
ENDIF |
460 |
CALL DIAGNOSTICS_FILL(viscAh_ZLth,'VAHZLTH ',k,1,2,bi,bj,myThid) |
CALL DIAGNOSTICS_FILL(viscAh_ZLth,'VAHZLTH ',k,1,2,bi,bj,myThid) |
461 |
CALL DIAGNOSTICS_FILL(viscA4_ZLth,'VA4ZLTH ',k,1,2,bi,bj,myThid) |
CALL DIAGNOSTICS_FILL(viscA4_ZLth,'VA4ZLTH ',k,1,2,bi,bj,myThid) |
462 |
|
|
463 |
CALL DIAGNOSTICS_FILL(viscAh_DLthD,'VAHDLTHD',k,1,2,bi,bj,myThid) |
CALL DIAGNOSTICS_FILL(viscAh_DLthD,'VAHDLTHD' |
464 |
CALL DIAGNOSTICS_FILL(viscA4_DLthD,'VA4DLTHD',k,1,2,bi,bj,myThid) |
& ,k,1,2,bi,bj,myThid) |
465 |
CALL DIAGNOSTICS_FILL(viscAh_ZLthD,'VAHZLTHD',k,1,2,bi,bj,myThid) |
CALL DIAGNOSTICS_FILL(viscA4_DLthD,'VA4DLTHD' |
466 |
CALL DIAGNOSTICS_FILL(viscA4_ZLthD,'VA4ZLTHD',k,1,2,bi,bj,myThid) |
& ,k,1,2,bi,bj,myThid) |
467 |
|
CALL DIAGNOSTICS_FILL(viscAh_ZLthD,'VAHZLTHD' |
468 |
|
& ,k,1,2,bi,bj,myThid) |
469 |
|
CALL DIAGNOSTICS_FILL(viscA4_ZLthD,'VA4ZLTHD' |
470 |
|
& ,k,1,2,bi,bj,myThid) |
471 |
|
|
472 |
CALL DIAGNOSTICS_FILL(viscAh_DSmg,'VAHDSMAG',k,1,2,bi,bj,myThid) |
CALL DIAGNOSTICS_FILL(viscAh_DSmg,'VAHDSMAG',k,1,2,bi,bj,myThid) |
473 |
CALL DIAGNOSTICS_FILL(viscA4_DSmg,'VA4DSMAG',k,1,2,bi,bj,myThid) |
CALL DIAGNOSTICS_FILL(viscA4_DSmg,'VA4DSMAG',k,1,2,bi,bj,myThid) |