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 |
17 |
C harmonic viscosity= |
C harmonic viscosity= |
18 |
C viscAh (or viscAhD on div pts and viscAhZ on zeta pts) |
C viscAh (or viscAhD on div pts and viscAhZ on zeta pts) |
19 |
C +0.25*L**2*viscAhGrid/deltaT |
C +0.25*L**2*viscAhGrid/deltaT |
20 |
C +sqrt(viscC2leith**2*grad(Vort3)**2 |
C +sqrt((viscC2leith/pi)**6*grad(Vort3)**2 |
21 |
C +viscC2leithD**2*grad(hDiv)**2)*L**3 |
C +(viscC2leithD/pi)**6*grad(hDiv)**2)*L**3 |
22 |
C +(viscC2smag/pi)**2*L**2*sqrt(Tension**2+Strain**2) |
C +(viscC2smag/pi)**2*L**2*sqrt(Tension**2+Strain**2) |
23 |
C |
C |
24 |
C biharmonic viscosity= |
C biharmonic viscosity= |
25 |
C viscA4 (or viscA4D on div pts and viscA4Z on zeta pts) |
C viscA4 (or viscA4D on div pts and viscA4Z on zeta pts) |
26 |
C +0.25*0.125*L**4*viscA4Grid/deltaT (approx) |
C +0.25*0.125*L**4*viscA4Grid/deltaT (approx) |
27 |
C +0.125*L**5*sqrt(viscC4leith**2*grad(Vort3)**2 |
C +0.125*L**5*sqrt((viscC4leith/pi)**6*grad(Vort3)**2 |
28 |
C +viscC4leithD**2*grad(hDiv)**2) |
C +(viscC4leithD/pi)**6*grad(hDiv)**2) |
29 |
C +0.125*L**4*(viscC4smag/pi)**2*sqrt(Tension**2+Strain**2) |
C +0.125*L**4*(viscC4smag/pi)**2*sqrt(Tension**2+Strain**2) |
30 |
C |
C |
31 |
C Note that often 0.125*L**2 is the scale between harmonic and |
C Note that often 0.125*L**2 is the scale between harmonic and |
51 |
C biharmonic viscosity>viscA4gridmax*L**4/32/deltaT (approx) |
C biharmonic viscosity>viscA4gridmax*L**4/32/deltaT (approx) |
52 |
C |
C |
53 |
C RECOMMENDED VALUES |
C RECOMMENDED VALUES |
54 |
C viscC2Leith=? |
C viscC2Leith=1-3 |
55 |
C viscC2LeithD=? |
C viscC2LeithD=1-3 |
56 |
C viscC4Leith=? |
C viscC4Leith=1-3 |
57 |
C viscC4LeithD=? |
C viscC4LeithD=1.5-3 |
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) |
91 |
C == Local variables == |
C == Local variables == |
92 |
INTEGER I,J |
INTEGER I,J |
93 |
_RL smag2fac, smag4fac |
_RL smag2fac, smag4fac |
94 |
|
_RL leith2fac, leith4fac |
95 |
|
_RL leithD2fac, leithD4fac |
96 |
_RL viscAhRe_max, viscA4Re_max |
_RL viscAhRe_max, viscA4Re_max |
97 |
_RL Alin,Alinmin,grdVrt,grdDiv |
_RL Alin,grdVrt,grdDiv, keZpt |
98 |
_RL recip_dt,L2,L3,L4,L5,L2rdt,L4rdt |
_RL recip_dt,L2,L3,L4,L5,L2rdt,L4rdt |
99 |
_RL Uscl,U4scl |
_RL Uscl,U4scl |
100 |
|
_RL divDx(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
101 |
|
_RL divDy(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
102 |
|
_RL vrtDx(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
103 |
|
_RL vrtDy(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
104 |
_RL viscAh_ZMax(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
_RL viscAh_ZMax(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
105 |
_RL viscAh_DMax(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
_RL viscAh_DMax(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
106 |
_RL viscA4_ZMax(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
_RL viscA4_ZMax(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
187 |
smag4fac=0. _d 0 |
smag4fac=0. _d 0 |
188 |
ENDIF |
ENDIF |
189 |
|
|
190 |
|
IF (calcleith) THEN |
191 |
|
IF (useFullLeith) THEN |
192 |
|
leith2fac =(viscC2leith /pi)**6 |
193 |
|
leithD2fac=(viscC2leithD/pi)**6 |
194 |
|
leith4fac =0.015625 _d 0*(viscC4leith /pi)**6 |
195 |
|
leithD4fac=0.015625 _d 0*(viscC4leithD/pi)**6 |
196 |
|
ELSE |
197 |
|
leith2fac =(viscC2leith /pi)**3 |
198 |
|
leithD2fac=(viscC2leithD/pi)**3 |
199 |
|
leith4fac =0.125 _d 0*(viscC4leith /pi)**3 |
200 |
|
leithD4fac=0.125 _d 0*(viscC4leithD/pi)**3 |
201 |
|
ENDIF |
202 |
|
ELSE |
203 |
|
leith2fac=0. _d 0 |
204 |
|
leith4fac=0. _d 0 |
205 |
|
leithD2fac=0. _d 0 |
206 |
|
leithD4fac=0. _d 0 |
207 |
|
ENDIF |
208 |
|
|
209 |
C - Viscosity |
C - Viscosity |
210 |
IF (useVariableViscosity) THEN |
IF (useVariableViscosity) THEN |
211 |
|
|
212 |
|
C- Initialise to zero gradient of vorticity & divergence: |
213 |
|
DO j=1-Oly,sNy+Oly |
214 |
|
DO i=1-Olx,sNx+Olx |
215 |
|
divDx(i,j) = 0. |
216 |
|
divDy(i,j) = 0. |
217 |
|
vrtDx(i,j) = 0. |
218 |
|
vrtDy(i,j) = 0. |
219 |
|
ENDDO |
220 |
|
ENDDO |
221 |
|
|
222 |
|
IF (calcleith) THEN |
223 |
|
C horizontal gradient of horizontal divergence: |
224 |
|
|
225 |
|
C- gradient in x direction: |
226 |
|
#ifndef ALLOW_AUTODIFF_TAMC |
227 |
|
IF (useCubedSphereExchange) THEN |
228 |
|
C to compute d/dx(hDiv), fill corners with appropriate values: |
229 |
|
CALL FILL_CS_CORNER_TR_RL( .TRUE., hDiv, bi,bj, myThid ) |
230 |
|
ENDIF |
231 |
|
#endif |
232 |
|
DO j=2-Oly,sNy+Oly-1 |
233 |
|
DO i=2-Olx,sNx+Olx-1 |
234 |
|
divDx(i,j) = (hDiv(i,j)-hDiv(i-1,j))*recip_DXC(i,j,bi,bj) |
235 |
|
ENDDO |
236 |
|
ENDDO |
237 |
|
|
238 |
|
C- gradient in y direction: |
239 |
|
#ifndef ALLOW_AUTODIFF_TAMC |
240 |
|
IF (useCubedSphereExchange) THEN |
241 |
|
C to compute d/dy(hDiv), fill corners with appropriate values: |
242 |
|
CALL FILL_CS_CORNER_TR_RL(.FALSE., hDiv, bi,bj, myThid ) |
243 |
|
ENDIF |
244 |
|
#endif |
245 |
|
DO j=2-Oly,sNy+Oly-1 |
246 |
|
DO i=2-Olx,sNx+Olx-1 |
247 |
|
divDy(i,j) = (hDiv(i,j)-hDiv(i,j-1))*recip_DYC(i,j,bi,bj) |
248 |
|
ENDDO |
249 |
|
ENDDO |
250 |
|
|
251 |
|
C horizontal gradient of vertical vorticity: |
252 |
|
C- gradient in x direction: |
253 |
|
DO j=2-Oly,sNy+Oly |
254 |
|
DO i=2-Olx,sNx+Olx-1 |
255 |
|
vrtDx(i,j) = (vort3(i+1,j)-vort3(i,j)) |
256 |
|
& *recip_DXG(i,j,bi,bj) |
257 |
|
& *maskS(i,j,k,bi,bj) |
258 |
|
ENDDO |
259 |
|
ENDDO |
260 |
|
C- gradient in y direction: |
261 |
|
DO j=2-Oly,sNy+Oly-1 |
262 |
|
DO i=2-Olx,sNx+Olx |
263 |
|
vrtDy(i,j) = (vort3(i,j+1)-vort3(i,j)) |
264 |
|
& *recip_DYG(i,j,bi,bj) |
265 |
|
& *maskW(i,j,k,bi,bj) |
266 |
|
ENDDO |
267 |
|
ENDDO |
268 |
|
|
269 |
|
ENDIF |
270 |
|
|
271 |
DO j=2-Oly,sNy+Oly-1 |
DO j=2-Oly,sNy+Oly-1 |
272 |
DO i=2-Olx,sNx+Olx-1 |
DO i=2-Olx,sNx+Olx-1 |
273 |
CCCCCCCCCCCCCCC Divergence Point CalculationsCCCCCCCCCCCCCCCCCCCC |
CCCCCCCCCCCCCCC Divergence Point CalculationsCCCCCCCCCCCCCCCCCCCC |
274 |
|
|
275 |
C These are (powers of) length scales |
C These are (powers of) length scales |
276 |
L2=2. _d 0/((recip_DXF(I,J,bi,bj)**2+recip_DYF(I,J,bi,bj)**2)) |
IF (useAreaViscLength) THEN |
277 |
|
L2=rA(i,j,bi,bj) |
278 |
|
ELSE |
279 |
|
L2=2. _d 0/((recip_DXF(I,J,bi,bj)**2+recip_DYF(I,J,bi,bj)**2)) |
280 |
|
ENDIF |
281 |
L3=(L2**1.5) |
L3=(L2**1.5) |
282 |
L4=(L2**2) |
L4=(L2**2) |
283 |
L5=(L2**2.5) |
L5=(L2**2.5) |
284 |
|
|
285 |
L2rdt=0.25 _d 0*recip_dt*L2 |
L2rdt=0.25 _d 0*recip_dt*L2 |
286 |
|
|
287 |
L4rdt=recip_dt/( 6. _d 0*(recip_DXF(I,J,bi,bj)**4 |
IF (useAreaViscLength) THEN |
288 |
|
L4rdt=0.125 _d 0*recip_dt*rA(i,j,bi,bj)**2 |
289 |
|
ELSE |
290 |
|
L4rdt=recip_dt/( 6. _d 0*(recip_DXF(I,J,bi,bj)**4 |
291 |
& +recip_DYF(I,J,bi,bj)**4) |
& +recip_DYF(I,J,bi,bj)**4) |
292 |
& +8. _d 0*((recip_DXF(I,J,bi,bj) |
& +8. _d 0*((recip_DXF(I,J,bi,bj) |
293 |
& *recip_DYF(I,J,bi,bj))**2) ) |
& *recip_DYF(I,J,bi,bj))**2) ) |
294 |
|
ENDIF |
295 |
|
|
296 |
C Velocity Reynolds Scale |
C Velocity Reynolds Scale |
297 |
Uscl=sqrt(KE(i,j)*L2)*viscAhRe_max |
IF ( viscAhRe_max.GT.0. .AND. KE(i,j).GT.0. ) THEN |
298 |
U4scl=sqrt(KE(i,j))*L3*viscA4Re_max |
Uscl=sqrt(KE(i,j)*L2)*viscAhRe_max |
299 |
|
ELSE |
300 |
|
Uscl=0. |
301 |
|
ENDIF |
302 |
|
IF ( viscA4Re_max.GT.0. .AND. KE(i,j).GT.0. ) THEN |
303 |
|
U4scl=sqrt(KE(i,j))*L3*viscA4Re_max |
304 |
|
ELSE |
305 |
|
U4scl=0. |
306 |
|
ENDIF |
307 |
|
|
308 |
IF (useFullLeith.and.calcleith) THEN |
IF (useFullLeith.and.calcleith) THEN |
309 |
C This is the vector magnitude of the vorticity gradient squared |
C This is the vector magnitude of the vorticity gradient squared |
310 |
grdVrt=0.25 _d 0*( |
grdVrt=0.25 _d 0*( (vrtDx(i,j+1)*vrtDx(i,j+1) |
311 |
& ((vort3(i+1,j)-vort3(i,j))*recip_DXG(i,j,bi,bj))**2 |
& + vrtDx(i,j)*vrtDx(i,j) ) |
312 |
& +((vort3(i,j+1)-vort3(i,j))*recip_DYG(i,j,bi,bj))**2 |
& + (vrtDy(i+1,j)*vrtDy(i+1,j) |
313 |
& +((vort3(i+1,j+1)-vort3(i,j+1)) |
& + vrtDy(i,j)*vrtDy(i,j) ) ) |
|
& *recip_DXG(i,j+1,bi,bj))**2 |
|
|
& +((vort3(i+1,j+1)-vort3(i+1,j)) |
|
|
& *recip_DYG(i+1,j,bi,bj))**2) |
|
314 |
|
|
315 |
C This is the vector magnitude of grad (div.v) squared |
C This is the vector magnitude of grad (div.v) squared |
316 |
C Using it in Leith serves to damp instabilities in w. |
C Using it in Leith serves to damp instabilities in w. |
317 |
grdDiv=0.25 _d 0*( |
grdDiv=0.25 _d 0*( (divDx(i+1,j)*divDx(i+1,j) |
318 |
& ((hDiv(i+1,j)-hDiv(i,j))*recip_DXC(i+1,j,bi,bj))**2 |
& + divDx(i,j)*divDx(i,j) ) |
319 |
& +((hDiv(i,j+1)-hDiv(i,j))*recip_DYC(i,j+1,bi,bj))**2 |
& + (divDy(i,j+1)*divDy(i,j+1) |
320 |
& +((hDiv(i,j)-hDiv(i-1,j))*recip_DXC(i,j,bi,bj))**2 |
& + divDy(i,j)*divDy(i,j) ) ) |
|
& +((hDiv(i,j)-hDiv(i,j-1))*recip_DYC(i,j,bi,bj))**2) |
|
321 |
|
|
322 |
viscAh_DLth(i,j)= |
viscAh_DLth(i,j)= |
323 |
& sqrt(viscC2leith**2*grdVrt+viscC2leithD**2*grdDiv)*L3 |
& sqrt(leith2fac*grdVrt+leithD2fac*grdDiv)*L3 |
324 |
viscA4_DLth(i,j)=0.125 _d 0* |
viscA4_DLth(i,j)= |
325 |
& sqrt(viscC4leith**2*grdVrt+viscC4leithD**2*grdDiv)*L5 |
& sqrt(leith4fac*grdVrt+leithD4fac*grdDiv)*L5 |
326 |
viscAh_DLthd(i,j)= |
viscAh_DLthd(i,j)= |
327 |
& sqrt(viscC2leithD**2*grdDiv)*L3 |
& sqrt(leithD2fac*grdDiv)*L3 |
328 |
viscA4_DLthd(i,j)=0.125 _d 0* |
viscA4_DLthd(i,j)= |
329 |
& sqrt(viscC4leithD**2*grdDiv)*L5 |
& sqrt(leithD4fac*grdDiv)*L5 |
330 |
ELSEIF (calcleith) THEN |
ELSEIF (calcleith) THEN |
331 |
C but this approximation will work on cube |
C but this approximation will work on cube |
332 |
c (and differs by as much as 4X) |
c (and differs by as much as 4X) |
333 |
grdVrt=abs((vort3(i+1,j)-vort3(i,j))*recip_DXG(i,j,bi,bj)) |
grdVrt=max( abs(vrtDx(i,j+1)), abs(vrtDx(i,j)) ) |
334 |
grdVrt=max(grdVrt, |
grdVrt=max( grdVrt, abs(vrtDy(i+1,j)) ) |
335 |
& abs((vort3(i,j+1)-vort3(i,j))*recip_DYG(i,j,bi,bj))) |
grdVrt=max( grdVrt, abs(vrtDy(i,j)) ) |
|
grdVrt=max(grdVrt, |
|
|
& abs((vort3(i+1,j+1)-vort3(i,j+1))*recip_DXG(i,j+1,bi,bj))) |
|
|
grdVrt=max(grdVrt, |
|
|
& abs((vort3(i+1,j+1)-vort3(i+1,j))*recip_DYG(i+1,j,bi,bj))) |
|
|
|
|
|
grdDiv=abs((hDiv(i+1,j)-hDiv(i,j))*recip_DXC(i+1,j,bi,bj)) |
|
|
grdDiv=max(grdDiv, |
|
|
& abs((hDiv(i,j+1)-hDiv(i,j))*recip_DYC(i,j+1,bi,bj))) |
|
|
grdDiv=max(grdDiv, |
|
|
& abs((hDiv(i,j)-hDiv(i-1,j))*recip_DXC(i,j,bi,bj))) |
|
|
grdDiv=max(grdDiv, |
|
|
& abs((hDiv(i,j)-hDiv(i,j-1))*recip_DYC(i,j,bi,bj))) |
|
336 |
|
|
337 |
c This approximation is good to the same order as above... |
c This approximation is good to the same order as above... |
338 |
viscAh_Dlth(i,j)= |
grdDiv=max( abs(divDx(i+1,j)), abs(divDx(i,j)) ) |
339 |
& (viscC2leith*grdVrt+(viscC2leithD*grdDiv))*L3 |
grdDiv=max( grdDiv, abs(divDy(i,j+1)) ) |
340 |
viscA4_Dlth(i,j)=0.125 _d 0* |
grdDiv=max( grdDiv, abs(divDy(i,j)) ) |
341 |
& (viscC4leith*grdVrt+(viscC4leithD*grdDiv))*L5 |
|
342 |
viscAh_DlthD(i,j)= |
viscAh_Dlth(i,j)=(leith2fac*grdVrt+(leithD2fac*grdDiv))*L3 |
343 |
& ((viscC2leithD*grdDiv))*L3 |
viscA4_Dlth(i,j)=(leith4fac*grdVrt+(leithD4fac*grdDiv))*L5 |
344 |
viscA4_DlthD(i,j)=0.125 _d 0* |
viscAh_DlthD(i,j)=((leithD2fac*grdDiv))*L3 |
345 |
& ((viscC4leithD*grdDiv))*L5 |
viscA4_DlthD(i,j)=((leithD4fac*grdDiv))*L5 |
346 |
ELSE |
ELSE |
347 |
viscAh_Dlth(i,j)=0. _d 0 |
viscAh_Dlth(i,j)=0. _d 0 |
348 |
viscA4_Dlth(i,j)=0. _d 0 |
viscA4_Dlth(i,j)=0. _d 0 |
380 |
|
|
381 |
CCCCCCCCCCCCC Vorticity Point CalculationsCCCCCCCCCCCCCCCCCC |
CCCCCCCCCCCCC Vorticity Point CalculationsCCCCCCCCCCCCCCCCCC |
382 |
C These are (powers of) length scales |
C These are (powers of) length scales |
383 |
L2=2. _d 0/((recip_DXV(I,J,bi,bj)**2+recip_DYU(I,J,bi,bj)**2)) |
IF (useAreaViscLength) THEN |
384 |
|
L2=rAz(i,j,bi,bj) |
385 |
|
ELSE |
386 |
|
L2=2. _d 0/((recip_DXV(I,J,bi,bj)**2+recip_DYU(I,J,bi,bj)**2)) |
387 |
|
ENDIF |
388 |
|
|
389 |
L3=(L2**1.5) |
L3=(L2**1.5) |
390 |
L4=(L2**2) |
L4=(L2**2) |
391 |
L5=(L2**2.5) |
L5=(L2**2.5) |
392 |
|
|
393 |
L2rdt=0.25 _d 0*recip_dt*L2 |
L2rdt=0.25 _d 0*recip_dt*L2 |
394 |
L4rdt=recip_dt/ |
IF (useAreaViscLength) THEN |
395 |
& ( 6. _d 0*(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 |
396 |
& +8. _d 0*((recip_DXF(I,J,bi,bj)*recip_DYF(I,J,bi,bj))**2)) |
ELSE |
397 |
|
L4rdt=recip_dt/ |
398 |
|
& ( 6. _d 0*(recip_DXV(I,J,bi,bj)**4+recip_DYU(I,J,bi,bj)**4) |
399 |
|
& +8. _d 0*((recip_DXV(I,J,bi,bj)*recip_DYU(I,J,bi,bj))**2)) |
400 |
|
ENDIF |
401 |
|
|
402 |
C Velocity Reynolds Scale |
C Velocity Reynolds Scale (Pb here at CS-grid corners !) |
403 |
Uscl=sqrt(0.25 _d 0*(KE(i,j)+KE(i,j+1)+KE(i+1,j)+KE(i+1,j+1)) |
IF ( viscAhRe_max.GT.0. .OR. viscA4Re_max.GT.0. ) THEN |
404 |
& *L2)*viscAhRe_max |
keZpt=0.25 _d 0*( (KE(i,j)+KE(i-1,j-1)) |
405 |
U4scl=sqrt(0.25 _d 0*(KE(i,j)+KE(i,j+1)+KE(i+1,j)+KE(i+1,j+1))) |
& +(KE(i-1,j)+KE(i,j-1)) ) |
406 |
& *L3*viscA4Re_max |
IF ( keZpt.GT.0. ) THEN |
407 |
|
Uscl = sqrt(keZpt*L2)*viscAhRe_max |
408 |
|
U4scl= sqrt(keZpt)*L3*viscA4Re_max |
409 |
|
ELSE |
410 |
|
Uscl =0. |
411 |
|
U4scl=0. |
412 |
|
ENDIF |
413 |
|
ELSE |
414 |
|
Uscl =0. |
415 |
|
U4scl=0. |
416 |
|
ENDIF |
417 |
|
|
418 |
C This is the vector magnitude of the vorticity gradient squared |
C This is the vector magnitude of the vorticity gradient squared |
419 |
IF (useFullLeith.and.calcleith) THEN |
IF (useFullLeith.and.calcleith) THEN |
420 |
grdVrt=0.25 _d 0*( |
grdVrt=0.25 _d 0*( (vrtDx(i-1,j)*vrtDx(i-1,j) |
421 |
& ((vort3(i+1,j)-vort3(i,j))*recip_DXG(i,j,bi,bj))**2 |
& + vrtDx(i,j)*vrtDx(i,j) ) |
422 |
& +((vort3(i,j+1)-vort3(i,j))*recip_DYG(i,j,bi,bj))**2 |
& + (vrtDy(i,j-1)*vrtDy(i,j-1) |
423 |
& +((vort3(i-1,j)-vort3(i,j))*recip_DXG(i-1,j,bi,bj))**2 |
& + vrtDy(i,j)*vrtDy(i,j) ) ) |
|
& +((vort3(i,j-1)-vort3(i,j))*recip_DYG(i,j-1,bi,bj))**2) |
|
424 |
|
|
425 |
C This is the vector magnitude of grad(div.v) squared |
C This is the vector magnitude of grad(div.v) squared |
426 |
grdDiv=0.25 _d 0*( |
grdDiv=0.25 _d 0*( (divDx(i,j-1)*divDx(i,j-1) |
427 |
& ((hDiv(i,j)-hDiv(i-1,j))*recip_DXC(i,j,bi,bj))**2 |
& + divDx(i,j)*divDx(i,j) ) |
428 |
& +((hDiv(i,j)-hDiv(i,j-1))*recip_DYC(i,j,bi,bj))**2 |
& + (divDy(i-1,j)*divDy(i-1,j) |
429 |
& +((hDiv(i,j-1)-hDiv(i-1,j-1))*recip_DXC(i,j-1,bi,bj))**2 |
& + divDy(i,j)*divDy(i,j) ) ) |
|
& +((hDiv(i-1,j)-hDiv(i-1,j-1))*recip_DYC(i-1,j,bi,bj))**2) |
|
430 |
|
|
431 |
viscAh_ZLth(i,j)= |
viscAh_ZLth(i,j)= |
432 |
& sqrt(viscC2leith**2*grdVrt+viscC2leithD**2*grdDiv)*L3 |
& sqrt(leith2fac*grdVrt+leithD2fac*grdDiv)*L3 |
433 |
viscA4_ZLth(i,j)=0.125 _d 0* |
viscA4_ZLth(i,j)= |
434 |
& sqrt(viscC4leith**2*grdVrt+viscC4leithD**2*grdDiv)*L5 |
& sqrt(leith4fac*grdVrt+leithD4fac*grdDiv)*L5 |
435 |
viscAh_ZLthD(i,j)= |
viscAh_ZLthD(i,j)= |
436 |
& sqrt(viscC2leithD**2*grdDiv)*L3 |
& sqrt(leithD2fac*grdDiv)*L3 |
437 |
viscA4_ZLthD(i,j)=0.125 _d 0* |
viscA4_ZLthD(i,j)= |
438 |
& sqrt(viscC4leithD**2*grdDiv)*L5 |
& sqrt(leithD4fac*grdDiv)*L5 |
439 |
|
|
440 |
ELSEIF (calcleith) THEN |
ELSEIF (calcleith) THEN |
441 |
C but this approximation will work on cube (and differs by 4X) |
C but this approximation will work on cube (and differs by 4X) |
442 |
grdVrt=abs((vort3(i+1,j)-vort3(i,j))*recip_DXG(i,j,bi,bj)) |
grdVrt=max( abs(vrtDx(i-1,j)), abs(vrtDx(i,j)) ) |
443 |
grdVrt=max(grdVrt, |
grdVrt=max( grdVrt, abs(vrtDy(i,j-1)) ) |
444 |
& abs((vort3(i,j+1)-vort3(i,j))*recip_DYG(i,j,bi,bj))) |
grdVrt=max( grdVrt, abs(vrtDy(i,j)) ) |
445 |
grdVrt=max(grdVrt, |
|
446 |
& abs((vort3(i-1,j)-vort3(i,j))*recip_DXG(i-1,j,bi,bj))) |
grdDiv=max( abs(divDx(i,j)), abs(divDx(i,j-1)) ) |
447 |
grdVrt=max(grdVrt, |
grdDiv=max( grdDiv, abs(divDy(i,j)) ) |
448 |
& abs((vort3(i,j-1)-vort3(i,j))*recip_DYG(i,j-1,bi,bj))) |
grdDiv=max( grdDiv, abs(divDy(i-1,j)) ) |
449 |
|
|
450 |
grdDiv=abs((hDiv(i,j)-hDiv(i-1,j))*recip_DXC(i,j,bi,bj)) |
viscAh_ZLth(i,j)=(leith2fac*grdVrt+(leithD2fac*grdDiv))*L3 |
451 |
grdDiv=max(grdDiv, |
viscA4_ZLth(i,j)=(leith4fac*grdVrt+(leithD4fac*grdDiv))*L5 |
452 |
& abs((hDiv(i,j)-hDiv(i,j-1))*recip_DYC(i,j,bi,bj))) |
viscAh_ZLthD(i,j)=(leithD2fac*grdDiv)*L3 |
453 |
grdDiv=max(grdDiv, |
viscA4_ZLthD(i,j)=(leithD4fac*grdDiv)*L5 |
|
& abs((hDiv(i,j-1)-hDiv(i-1,j-1))*recip_DXC(i,j-1,bi,bj))) |
|
|
grdDiv=max(grdDiv, |
|
|
& abs((hDiv(i-1,j)-hDiv(i-1,j-1))*recip_DYC(i-1,j,bi,bj))) |
|
|
|
|
|
viscAh_ZLth(i,j)=(viscC2leith*grdVrt |
|
|
& +(viscC2leithD*grdDiv))*L3 |
|
|
viscA4_ZLth(i,j)=0.125 _d 0*(viscC4leith*grdVrt |
|
|
& +(viscC4leithD*grdDiv))*L5 |
|
|
viscAh_ZLthD(i,j)=((viscC2leithD*grdDiv))*L3 |
|
|
viscA4_ZLthD(i,j)=0.125 _d 0*((viscC4leithD*grdDiv))*L5 |
|
454 |
ELSE |
ELSE |
455 |
viscAh_ZLth(i,j)=0. _d 0 |
viscAh_ZLth(i,j)=0. _d 0 |
456 |
viscA4_ZLth(i,j)=0. _d 0 |
viscA4_ZLth(i,j)=0. _d 0 |