34 |
C for roughly similar results with biharmonic and harmonic |
C for roughly similar results with biharmonic and harmonic |
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/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**3/8/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 |
47 |
C biharmonic viscosity<viscA4gridmax*L**4/32/deltaT (approx) |
C biharmonic viscosity<viscA4gridmax*L**4/32/deltaT (approx) |
48 |
C |
C |
49 |
C viscAhgridmin and viscA4gridmin are lower limits for viscosity: |
C viscAhgridmin and viscA4gridmin are lower limits for viscosity: |
50 |
C harmonic viscosity>0.25*viscAhgridmax*L**2/deltaT |
C harmonic viscosity>0.25*viscAhgridmin*L**2/deltaT |
51 |
C biharmonic viscosity>viscA4gridmax*L**4/32/deltaT (approx) |
C biharmonic viscosity>viscA4gridmin*L**4/32/deltaT (approx) |
52 |
|
|
53 |
|
|
54 |
C |
C |
55 |
C RECOMMENDED VALUES |
C RECOMMENDED VALUES |
56 |
C viscC2Leith=1-3 |
C viscC2Leith=1-3 |
57 |
C viscC2LeithD=1-3 |
C viscC2LeithD=1-3 |
58 |
C viscC4Leith=1-3 |
C viscC4Leith=1-3 |
59 |
C viscC4LeithD=1.5-3 |
C viscC4LeithD=1.5-3 |
60 |
C viscC2smag=2.2-4 (Griffies and Hallberg,2000) |
C viscC2smag=2.2-4 (Griffies and Hallberg,2000) |
61 |
C 0.2-0.9 (Smagorinsky,1993) |
C 0.2-0.9 (Smagorinsky,1993) |
62 |
C viscC4smag=2.2-4 (Griffies and Hallberg,2000) |
C viscC4smag=2.2-4 (Griffies and Hallberg,2000) |
63 |
C viscAhRemax>=1, (<2 suppresses a computational mode) |
C viscAhReMax>=1, (<2 suppresses a computational mode) |
64 |
C viscA4Remax>=1, (<2 suppresses a computational mode) |
C viscA4ReMax>=1, (<2 suppresses a computational mode) |
65 |
C viscAhgridmax=1 |
C viscAhgridmax=1 |
66 |
C viscA4gridmax=1 |
C viscA4gridmax=1 |
67 |
C viscAhgrid<1 |
C viscAhgrid<1 |
74 |
#include "GRID.h" |
#include "GRID.h" |
75 |
#include "EEPARAMS.h" |
#include "EEPARAMS.h" |
76 |
#include "PARAMS.h" |
#include "PARAMS.h" |
77 |
|
#ifdef ALLOW_NONHYDROSTATIC |
78 |
|
#include "NH_VARS.h" |
79 |
|
#endif |
80 |
|
#ifdef ALLOW_AUTODIFF_TAMC |
81 |
|
#include "tamc.h" |
82 |
|
#include "tamc_keys.h" |
83 |
|
#endif /* ALLOW_AUTODIFF_TAMC */ |
84 |
|
#include "MOM_VISC.h" |
85 |
|
|
86 |
C == Routine arguments == |
C == Routine arguments == |
87 |
INTEGER bi,bj,k |
INTEGER bi,bj,k |
100 |
|
|
101 |
C == Local variables == |
C == Local variables == |
102 |
INTEGER I,J |
INTEGER I,J |
103 |
|
#ifdef ALLOW_NONHYDROSTATIC |
104 |
|
INTEGER kp1 |
105 |
|
#endif |
106 |
|
#ifdef ALLOW_AUTODIFF_TAMC |
107 |
|
INTEGER lockey_1, lockey_2 |
108 |
|
#endif |
109 |
_RL smag2fac, smag4fac |
_RL smag2fac, smag4fac |
110 |
_RL leith2fac, leith4fac |
_RL leith2fac, leith4fac |
111 |
_RL leithD2fac, leithD4fac |
_RL leithD2fac, leithD4fac |
112 |
_RL viscAhRe_max, viscA4Re_max |
_RL viscAhRe_max, viscA4Re_max |
113 |
_RL Alin,grdVrt,grdDiv, keZpt |
_RL Alin,grdVrt,grdDiv, keZpt |
114 |
_RL recip_dt,L2,L3,L4,L5,L2rdt,L4rdt |
_RL L2,L3,L5,L2rdt,L4rdt |
115 |
_RL Uscl,U4scl |
_RL Uscl,U4scl |
116 |
_RL divDx(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
_RL divDx(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
117 |
_RL divDy(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
_RL divDy(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
118 |
|
_RL vrtDx(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
119 |
|
_RL vrtDy(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
120 |
_RL viscAh_ZMax(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
_RL viscAh_ZMax(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
121 |
_RL viscAh_DMax(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
_RL viscAh_DMax(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
122 |
_RL viscA4_ZMax(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
_RL viscA4_ZMax(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
137 |
_RL viscAh_DSmg(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
_RL viscAh_DSmg(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
138 |
_RL viscA4_ZSmg(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
_RL viscA4_ZSmg(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
139 |
_RL viscA4_DSmg(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
_RL viscA4_DSmg(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
140 |
LOGICAL calcLeith,calcSmag |
LOGICAL calcLeith, calcSmag |
141 |
|
|
142 |
|
#ifdef ALLOW_AUTODIFF_TAMC |
143 |
|
act1 = bi - myBxLo(myThid) |
144 |
|
max1 = myBxHi(myThid) - myBxLo(myThid) + 1 |
145 |
|
act2 = bj - myByLo(myThid) |
146 |
|
max2 = myByHi(myThid) - myByLo(myThid) + 1 |
147 |
|
act3 = myThid - 1 |
148 |
|
max3 = nTx*nTy |
149 |
|
act4 = ikey_dynamics - 1 |
150 |
|
ikey = (act1 + 1) + act2*max1 |
151 |
|
& + act3*max1*max2 |
152 |
|
& + act4*max1*max2*max3 |
153 |
|
lockey_1 = (ikey-1)*Nr + k |
154 |
|
#endif /* ALLOW_AUTODIFF_TAMC */ |
155 |
|
|
156 |
|
C-- Set flags which are used in this S/R and elsewhere : |
157 |
useVariableViscosity= |
useVariableViscosity= |
158 |
& (viscAhGrid.NE.0.) |
& (viscAhGrid.NE.0.) |
159 |
& .OR.(viscA4Grid.NE.0.) |
& .OR.(viscA4Grid.NE.0.) |
173 |
& .OR.(viscC2leithD.NE.0.) |
& .OR.(viscC2leithD.NE.0.) |
174 |
& .OR.(viscC2smag.NE.0.) |
& .OR.(viscC2smag.NE.0.) |
175 |
|
|
|
IF ((harmonic).and.(viscAhremax.ne.0.)) THEN |
|
|
viscAhre_max=sqrt(2. _d 0)/viscAhRemax |
|
|
ELSE |
|
|
viscAhre_max=0. _d 0 |
|
|
ENDIF |
|
|
|
|
176 |
biharmonic= |
biharmonic= |
177 |
& (viscA4.NE.0.) |
& (viscA4.NE.0.) |
178 |
& .OR.(viscA4D.NE.0.) |
& .OR.(viscA4D.NE.0.) |
182 |
& .OR.(viscC4leithD.NE.0.) |
& .OR.(viscC4leithD.NE.0.) |
183 |
& .OR.(viscC4smag.NE.0.) |
& .OR.(viscC4smag.NE.0.) |
184 |
|
|
185 |
IF ((biharmonic).and.(viscA4remax.ne.0.)) THEN |
IF (useVariableViscosity) THEN |
186 |
viscA4re_max=0.125 _d 0*sqrt(2. _d 0)/viscA4Remax |
C---- variable viscosity : |
187 |
ELSE |
|
188 |
viscA4re_max=0. _d 0 |
IF ((harmonic).AND.(viscAhReMax.NE.0.)) THEN |
189 |
ENDIF |
viscAhRe_max=SQRT(2. _d 0)/viscAhReMax |
190 |
|
ELSE |
191 |
|
viscAhRe_max=0. _d 0 |
192 |
|
ENDIF |
193 |
|
|
194 |
|
IF ((biharmonic).AND.(viscA4ReMax.NE.0.)) THEN |
195 |
|
viscA4Re_max=0.125 _d 0*SQRT(2. _d 0)/viscA4ReMax |
196 |
|
ELSE |
197 |
|
viscA4Re_max=0. _d 0 |
198 |
|
ENDIF |
199 |
|
|
200 |
calcleith= |
calcLeith= |
201 |
& (viscC2leith.NE.0.) |
& (viscC2leith.NE.0.) |
202 |
& .OR.(viscC2leithD.NE.0.) |
& .OR.(viscC2leithD.NE.0.) |
203 |
& .OR.(viscC4leith.NE.0.) |
& .OR.(viscC4leith.NE.0.) |
204 |
& .OR.(viscC4leithD.NE.0.) |
& .OR.(viscC4leithD.NE.0.) |
205 |
|
|
206 |
calcsmag= |
calcSmag= |
207 |
& (viscC2smag.NE.0.) |
& (viscC2smag.NE.0.) |
208 |
& .OR.(viscC4smag.NE.0.) |
& .OR.(viscC4smag.NE.0.) |
209 |
|
|
210 |
IF (deltaTmom.NE.0.) THEN |
IF (calcSmag) THEN |
|
recip_dt=1. _d 0/deltaTmom |
|
|
ELSE |
|
|
recip_dt=0. _d 0 |
|
|
ENDIF |
|
|
|
|
|
IF (calcsmag) THEN |
|
211 |
smag2fac=(viscC2smag/pi)**2 |
smag2fac=(viscC2smag/pi)**2 |
212 |
smag4fac=0.125 _d 0*(viscC4smag/pi)**2 |
smag4fac=0.125 _d 0*(viscC4smag/pi)**2 |
213 |
ELSE |
ELSE |
214 |
smag2fac=0. _d 0 |
smag2fac=0. _d 0 |
215 |
smag4fac=0. _d 0 |
smag4fac=0. _d 0 |
216 |
ENDIF |
ENDIF |
217 |
|
|
218 |
IF (calcleith) THEN |
IF (calcLeith) THEN |
219 |
IF (useFullLeith) THEN |
IF (useFullLeith) THEN |
220 |
leith2fac =(viscC2leith /pi)**6 |
leith2fac =(viscC2leith /pi)**6 |
221 |
leithD2fac=(viscC2leithD/pi)**6 |
leithD2fac=(viscC2leithD/pi)**6 |
227 |
leith4fac =0.125 _d 0*(viscC4leith /pi)**3 |
leith4fac =0.125 _d 0*(viscC4leith /pi)**3 |
228 |
leithD4fac=0.125 _d 0*(viscC4leithD/pi)**3 |
leithD4fac=0.125 _d 0*(viscC4leithD/pi)**3 |
229 |
ENDIF |
ENDIF |
230 |
ELSE |
ELSE |
231 |
leith2fac=0. _d 0 |
leith2fac=0. _d 0 |
232 |
leith4fac=0. _d 0 |
leith4fac=0. _d 0 |
233 |
leithD2fac=0. _d 0 |
leithD2fac=0. _d 0 |
234 |
leithD4fac=0. _d 0 |
leithD4fac=0. _d 0 |
235 |
ENDIF |
ENDIF |
236 |
|
|
237 |
C - Viscosity |
#ifdef ALLOW_AUTODIFF_TAMC |
238 |
IF (useVariableViscosity) THEN |
cphtest IF ( calcLeith .OR. calcSmag ) THEN |
239 |
|
cphtest STOP 'calcLeith or calcSmag not implemented for ADJOINT' |
240 |
|
cphtest ENDIF |
241 |
|
#endif |
242 |
|
DO j=1-Oly,sNy+Oly |
243 |
|
DO i=1-Olx,sNx+Olx |
244 |
|
viscAh_D(i,j)=viscAhD |
245 |
|
viscAh_Z(i,j)=viscAhZ |
246 |
|
viscA4_D(i,j)=viscA4D |
247 |
|
viscA4_Z(i,j)=viscA4Z |
248 |
|
c |
249 |
|
visca4_zsmg(i,j) = 0. _d 0 |
250 |
|
viscah_zsmg(i,j) = 0. _d 0 |
251 |
|
c |
252 |
|
viscAh_Dlth(i,j) = 0. _d 0 |
253 |
|
viscA4_Dlth(i,j) = 0. _d 0 |
254 |
|
viscAh_DlthD(i,j)= 0. _d 0 |
255 |
|
viscA4_DlthD(i,j)= 0. _d 0 |
256 |
|
c |
257 |
|
viscAh_DSmg(i,j) = 0. _d 0 |
258 |
|
viscA4_DSmg(i,j) = 0. _d 0 |
259 |
|
c |
260 |
|
viscAh_ZLth(i,j) = 0. _d 0 |
261 |
|
viscA4_ZLth(i,j) = 0. _d 0 |
262 |
|
viscAh_ZLthD(i,j)= 0. _d 0 |
263 |
|
viscA4_ZLthD(i,j)= 0. _d 0 |
264 |
|
ENDDO |
265 |
|
ENDDO |
266 |
|
|
267 |
C horizontal gradient of horizontal divergence: |
C- Initialise to zero gradient of vorticity & divergence: |
268 |
DO j=1-Oly,sNy+Oly |
DO j=1-Oly,sNy+Oly |
269 |
DO i=1-Olx,sNx+Olx |
DO i=1-Olx,sNx+Olx |
270 |
divDx(i,j) = 0. |
divDx(i,j) = 0. |
271 |
divDy(i,j) = 0. |
divDy(i,j) = 0. |
272 |
|
vrtDx(i,j) = 0. |
273 |
|
vrtDy(i,j) = 0. |
274 |
ENDDO |
ENDDO |
275 |
ENDDO |
ENDDO |
276 |
IF (calcleith) THEN |
|
277 |
|
IF (calcLeith) THEN |
278 |
|
C horizontal gradient of horizontal divergence: |
279 |
|
|
280 |
C- gradient in x direction: |
C- gradient in x direction: |
281 |
#ifndef ALLOW_AUTODIFF_TAMC |
cph-exch2#ifndef ALLOW_AUTODIFF_TAMC |
282 |
IF (useCubedSphereExchange) THEN |
IF (useCubedSphereExchange) THEN |
283 |
C to compute d/dx(hDiv), fill corners with appropriate values: |
C to compute d/dx(hDiv), fill corners with appropriate values: |
284 |
CALL FILL_CS_CORNER_TR_RL( .TRUE., hDiv, bi,bj, myThid ) |
CALL FILL_CS_CORNER_TR_RL( 1, .FALSE., |
285 |
|
& hDiv, bi,bj, myThid ) |
286 |
ENDIF |
ENDIF |
287 |
#endif |
cph-exch2#endif |
288 |
DO j=2-Oly,sNy+Oly-1 |
DO j=2-Oly,sNy+Oly-1 |
289 |
DO i=2-Olx,sNx+Olx-1 |
DO i=2-Olx,sNx+Olx-1 |
290 |
divDx(i,j) = (hDiv(i,j)-hDiv(i-1,j))*recip_DXC(i,j,bi,bj) |
divDx(i,j) = (hDiv(i,j)-hDiv(i-1,j))*recip_DXC(i,j,bi,bj) |
292 |
ENDDO |
ENDDO |
293 |
|
|
294 |
C- gradient in y direction: |
C- gradient in y direction: |
295 |
#ifndef ALLOW_AUTODIFF_TAMC |
cph-exch2#ifndef ALLOW_AUTODIFF_TAMC |
296 |
IF (useCubedSphereExchange) THEN |
IF (useCubedSphereExchange) THEN |
297 |
C to compute d/dy(hDiv), fill corners with appropriate values: |
C to compute d/dy(hDiv), fill corners with appropriate values: |
298 |
CALL FILL_CS_CORNER_TR_RL(.FALSE., hDiv, bi,bj, myThid ) |
CALL FILL_CS_CORNER_TR_RL( 2, .FALSE., |
299 |
|
& hDiv, bi,bj, myThid ) |
300 |
ENDIF |
ENDIF |
301 |
#endif |
cph-exch2#endif |
302 |
DO j=2-Oly,sNy+Oly-1 |
DO j=2-Oly,sNy+Oly-1 |
303 |
DO i=2-Olx,sNx+Olx-1 |
DO i=2-Olx,sNx+Olx-1 |
304 |
divDy(i,j) = (hDiv(i,j)-hDiv(i,j-1))*recip_DYC(i,j,bi,bj) |
divDy(i,j) = (hDiv(i,j)-hDiv(i,j-1))*recip_DYC(i,j,bi,bj) |
305 |
ENDDO |
ENDDO |
306 |
ENDDO |
ENDDO |
307 |
|
|
308 |
|
C horizontal gradient of vertical vorticity: |
309 |
|
C- gradient in x direction: |
310 |
|
DO j=2-Oly,sNy+Oly |
311 |
|
DO i=2-Olx,sNx+Olx-1 |
312 |
|
vrtDx(i,j) = (vort3(i+1,j)-vort3(i,j)) |
313 |
|
& *recip_DXG(i,j,bi,bj) |
314 |
|
& *maskS(i,j,k,bi,bj) |
315 |
|
ENDDO |
316 |
|
ENDDO |
317 |
|
C- gradient in y direction: |
318 |
|
DO j=2-Oly,sNy+Oly-1 |
319 |
|
DO i=2-Olx,sNx+Olx |
320 |
|
vrtDy(i,j) = (vort3(i,j+1)-vort3(i,j)) |
321 |
|
& *recip_DYG(i,j,bi,bj) |
322 |
|
& *maskW(i,j,k,bi,bj) |
323 |
|
ENDDO |
324 |
|
ENDDO |
325 |
|
|
326 |
ENDIF |
ENDIF |
327 |
|
|
328 |
DO j=2-Oly,sNy+Oly-1 |
DO j=2-Oly,sNy+Oly-1 |
329 |
DO i=2-Olx,sNx+Olx-1 |
DO i=2-Olx,sNx+Olx-1 |
330 |
CCCCCCCCCCCCCCC Divergence Point CalculationsCCCCCCCCCCCCCCCCCCCC |
CCCCCCCCCCCCCCC Divergence Point CalculationsCCCCCCCCCCCCCCCCCCCC |
331 |
|
|
332 |
C These are (powers of) length scales |
#ifdef ALLOW_AUTODIFF_TAMC |
333 |
IF (useAreaViscLength) THEN |
# ifndef AUTODIFF_DISABLE_LEITH |
334 |
L2=rA(i,j,bi,bj) |
lockey_2 = i+olx + (sNx+2*olx)*(j+oly-1) |
335 |
ELSE |
& + (sNx+2*olx)*(sNy+2*oly)*(lockey_1-1) |
336 |
L2=2. _d 0/((recip_DXF(I,J,bi,bj)**2+recip_DYF(I,J,bi,bj)**2)) |
CADJ STORE viscA4_ZSmg(i,j) |
337 |
ENDIF |
CADJ & = comlev1_mom_ijk_loop , key=lockey_2, byte=isbyte |
338 |
L3=(L2**1.5) |
CADJ STORE viscAh_ZSmg(i,j) |
339 |
L4=(L2**2) |
CADJ & = comlev1_mom_ijk_loop , key=lockey_2, byte=isbyte |
340 |
L5=(L2**2.5) |
# endif |
341 |
|
#endif /* ALLOW_AUTODIFF_TAMC */ |
342 |
L2rdt=0.25 _d 0*recip_dt*L2 |
|
343 |
|
C These are (powers of) length scales |
344 |
IF (useAreaViscLength) THEN |
L2 = L2_D(i,j,bi,bj) |
345 |
L4rdt=0.125 _d 0*recip_dt*rA(i,j,bi,bj)**2 |
L2rdt = 0.25 _d 0*recip_dt*L2 |
346 |
ELSE |
L3 = L3_D(i,j,bi,bj) |
347 |
L4rdt=recip_dt/( 6. _d 0*(recip_DXF(I,J,bi,bj)**4 |
L4rdt = L4rdt_D(i,j,bi,bj) |
348 |
& +recip_DYF(I,J,bi,bj)**4) |
L5 = (L2*L3) |
|
& +8. _d 0*((recip_DXF(I,J,bi,bj) |
|
|
& *recip_DYF(I,J,bi,bj))**2) ) |
|
|
ENDIF |
|
349 |
|
|
350 |
|
#ifndef AUTODIFF_DISABLE_REYNOLDS_SCALE |
351 |
C Velocity Reynolds Scale |
C Velocity Reynolds Scale |
352 |
IF ( viscAhRe_max.GT.0. .AND. KE(i,j).GT.0. ) THEN |
IF ( viscAhRe_max.GT.0. .AND. KE(i,j).GT.0. ) THEN |
353 |
Uscl=sqrt(KE(i,j)*L2)*viscAhRe_max |
Uscl=SQRT(KE(i,j)*L2)*viscAhRe_max |
354 |
ELSE |
ELSE |
355 |
Uscl=0. |
Uscl=0. |
356 |
ENDIF |
ENDIF |
357 |
IF ( viscA4Re_max.GT.0. .AND. KE(i,j).GT.0. ) THEN |
IF ( viscA4Re_max.GT.0. .AND. KE(i,j).GT.0. ) THEN |
358 |
U4scl=sqrt(KE(i,j))*L3*viscA4Re_max |
U4scl=SQRT(KE(i,j))*L3*viscA4Re_max |
359 |
ELSE |
ELSE |
360 |
U4scl=0. |
U4scl=0. |
361 |
ENDIF |
ENDIF |
362 |
|
#endif /* ndef AUTODIFF_DISABLE_REYNOLDS_SCALE */ |
363 |
|
|
364 |
IF (useFullLeith.and.calcleith) THEN |
cph-leith#ifndef ALLOW_AUTODIFF_TAMC |
365 |
|
#ifndef AUTODIFF_DISABLE_LEITH |
366 |
|
IF (useFullLeith.AND.calcLeith) THEN |
367 |
C This is the vector magnitude of the vorticity gradient squared |
C This is the vector magnitude of the vorticity gradient squared |
368 |
grdVrt=0.25 _d 0*( |
grdVrt=0.25 _d 0*( (vrtDx(i,j+1)*vrtDx(i,j+1) |
369 |
& ((vort3(i+1,j)-vort3(i,j))*recip_DXG(i,j,bi,bj))**2 |
& + vrtDx(i,j)*vrtDx(i,j) ) |
370 |
& +((vort3(i,j+1)-vort3(i,j))*recip_DYG(i,j,bi,bj))**2 |
& + (vrtDy(i+1,j)*vrtDy(i+1,j) |
371 |
& +((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) |
|
372 |
|
|
373 |
C This is the vector magnitude of grad (div.v) squared |
C This is the vector magnitude of grad (div.v) squared |
374 |
C Using it in Leith serves to damp instabilities in w. |
C Using it in Leith serves to damp instabilities in w. |
378 |
& + divDy(i,j)*divDy(i,j) ) ) |
& + divDy(i,j)*divDy(i,j) ) ) |
379 |
|
|
380 |
viscAh_DLth(i,j)= |
viscAh_DLth(i,j)= |
381 |
& sqrt(leith2fac*grdVrt+leithD2fac*grdDiv)*L3 |
& SQRT(leith2fac*grdVrt+leithD2fac*grdDiv)*L3 |
382 |
viscA4_DLth(i,j)= |
viscA4_DLth(i,j)= |
383 |
& sqrt(leith4fac*grdVrt+leithD4fac*grdDiv)*L5 |
& SQRT(leith4fac*grdVrt+leithD4fac*grdDiv)*L5 |
384 |
viscAh_DLthd(i,j)= |
viscAh_DLthd(i,j)= |
385 |
& sqrt(leithD2fac*grdDiv)*L3 |
& SQRT(leithD2fac*grdDiv)*L3 |
386 |
viscA4_DLthd(i,j)= |
viscA4_DLthd(i,j)= |
387 |
& sqrt(leithD4fac*grdDiv)*L5 |
& SQRT(leithD4fac*grdDiv)*L5 |
388 |
ELSEIF (calcleith) THEN |
ELSEIF (calcLeith) THEN |
389 |
C but this approximation will work on cube |
C but this approximation will work on cube |
390 |
c (and differs by as much as 4X) |
c (and differs by as much as 4X) |
391 |
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)) ) |
392 |
grdVrt=max(grdVrt, |
grdVrt=MAX( grdVrt, ABS(vrtDy(i+1,j)) ) |
393 |
& 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=max( abs(divDx(i+1,j)), abs(divDx(i,j)) ) |
|
|
grdDiv=max( grdDiv, abs(divDy(i,j+1)) ) |
|
|
grdDiv=max( grdDiv, abs(divDy(i,j)) ) |
|
394 |
|
|
395 |
c This approximation is good to the same order as above... |
c This approximation is good to the same order as above... |
396 |
|
grdDiv=MAX( ABS(divDx(i+1,j)), ABS(divDx(i,j)) ) |
397 |
|
grdDiv=MAX( grdDiv, ABS(divDy(i,j+1)) ) |
398 |
|
grdDiv=MAX( grdDiv, ABS(divDy(i,j)) ) |
399 |
|
|
400 |
viscAh_Dlth(i,j)=(leith2fac*grdVrt+(leithD2fac*grdDiv))*L3 |
viscAh_Dlth(i,j)=(leith2fac*grdVrt+(leithD2fac*grdDiv))*L3 |
401 |
viscA4_Dlth(i,j)=(leith4fac*grdVrt+(leithD4fac*grdDiv))*L5 |
viscA4_Dlth(i,j)=(leith4fac*grdVrt+(leithD4fac*grdDiv))*L5 |
402 |
viscAh_DlthD(i,j)=((leithD2fac*grdDiv))*L3 |
viscAh_DlthD(i,j)=((leithD2fac*grdDiv))*L3 |
408 |
viscA4_DlthD(i,j)=0. _d 0 |
viscA4_DlthD(i,j)=0. _d 0 |
409 |
ENDIF |
ENDIF |
410 |
|
|
411 |
IF (calcsmag) THEN |
IF (calcSmag) THEN |
412 |
viscAh_DSmg(i,j)=L2 |
viscAh_DSmg(i,j)=L2 |
413 |
& *sqrt(tension(i,j)**2 |
& *SQRT(tension(i,j)**2 |
414 |
& +0.25 _d 0*(strain(i+1, j )**2+strain( i ,j+1)**2 |
& +0.25 _d 0*(strain(i+1, j )**2+strain( i ,j+1)**2 |
415 |
& +strain(i , j )**2+strain(i+1,j+1)**2)) |
& +strain(i , j )**2+strain(i+1,j+1)**2)) |
416 |
viscA4_DSmg(i,j)=smag4fac*L2*viscAh_DSmg(i,j) |
viscA4_DSmg(i,j)=smag4fac*L2*viscAh_DSmg(i,j) |
419 |
viscAh_DSmg(i,j)=0. _d 0 |
viscAh_DSmg(i,j)=0. _d 0 |
420 |
viscA4_DSmg(i,j)=0. _d 0 |
viscA4_DSmg(i,j)=0. _d 0 |
421 |
ENDIF |
ENDIF |
422 |
|
#endif /* AUTODIFF_DISABLE_LEITH */ |
423 |
|
|
424 |
C Harmonic on Div.u points |
C Harmonic on Div.u points |
425 |
Alin=viscAhD+viscAhGrid*L2rdt |
Alin=viscAhD+viscAhGrid*L2rdt |
426 |
& +viscAh_DLth(i,j)+viscAh_DSmg(i,j) |
& +viscAh_DLth(i,j)+viscAh_DSmg(i,j) |
427 |
viscAh_DMin(i,j)=max(viscAhGridMin*L2rdt,Uscl) |
viscAh_DMin(i,j)=MAX(viscAhGridMin*L2rdt,Uscl) |
428 |
viscAh_D(i,j)=max(viscAh_DMin(i,j),Alin) |
viscAh_D(i,j)=MAX(viscAh_DMin(i,j),Alin) |
429 |
viscAh_DMax(i,j)=min(viscAhGridMax*L2rdt,viscAhMax) |
viscAh_DMax(i,j)=MIN(viscAhGridMax*L2rdt,viscAhMax) |
430 |
viscAh_D(i,j)=min(viscAh_DMax(i,j),viscAh_D(i,j)) |
viscAh_D(i,j)=MIN(viscAh_DMax(i,j),viscAh_D(i,j)) |
431 |
|
|
432 |
C BiHarmonic on Div.u points |
C BiHarmonic on Div.u points |
433 |
Alin=viscA4D+viscA4Grid*L4rdt |
Alin=viscA4D+viscA4Grid*L4rdt |
434 |
& +viscA4_DLth(i,j)+viscA4_DSmg(i,j) |
& +viscA4_DLth(i,j)+viscA4_DSmg(i,j) |
435 |
viscA4_DMin(i,j)=max(viscA4GridMin*L4rdt,U4scl) |
viscA4_DMin(i,j)=MAX(viscA4GridMin*L4rdt,U4scl) |
436 |
viscA4_D(i,j)=max(viscA4_DMin(i,j),Alin) |
viscA4_D(i,j)=MAX(viscA4_DMin(i,j),Alin) |
437 |
viscA4_DMax(i,j)=min(viscA4GridMax*L4rdt,viscA4Max) |
viscA4_DMax(i,j)=MIN(viscA4GridMax*L4rdt,viscA4Max) |
438 |
viscA4_D(i,j)=min(viscA4_DMax(i,j),viscA4_D(i,j)) |
viscA4_D(i,j)=MIN(viscA4_DMax(i,j),viscA4_D(i,j)) |
439 |
|
|
440 |
|
#ifdef ALLOW_NONHYDROSTATIC |
441 |
|
C-- Pass Viscosities to calc_gw, if constant, not necessary |
442 |
|
|
443 |
|
kp1 = MIN(k+1,Nr) |
444 |
|
|
445 |
|
IF ( k.EQ.1 ) THEN |
446 |
|
C Prepare for next level (next call) |
447 |
|
viscAh_W(i,j,kp1,bi,bj)=0.5*viscAh_D(i,j) |
448 |
|
viscA4_W(i,j,kp1,bi,bj)=0.5*viscA4_D(i,j) |
449 |
|
|
450 |
|
C These values dont get used |
451 |
|
viscAh_W(i,j,k,bi,bj)=viscAh_D(i,j) |
452 |
|
viscA4_W(i,j,k,bi,bj)=viscA4_D(i,j) |
453 |
|
|
454 |
|
ELSEIF ( k.EQ.Nr ) THEN |
455 |
|
viscAh_W(i,j,k,bi,bj)=viscAh_W(i,j,k,bi,bj)+0.5*viscAh_D(i,j) |
456 |
|
viscA4_W(i,j,k,bi,bj)=viscA4_W(i,j,k,bi,bj)+0.5*viscA4_D(i,j) |
457 |
|
|
|
CCCCCCCCCCCCC Vorticity Point CalculationsCCCCCCCCCCCCCCCCCC |
|
|
C These are (powers of) length scales |
|
|
IF (useAreaViscLength) THEN |
|
|
L2=rAz(i,j,bi,bj) |
|
458 |
ELSE |
ELSE |
459 |
L2=2. _d 0/((recip_DXV(I,J,bi,bj)**2+recip_DYU(I,J,bi,bj)**2)) |
C Prepare for next level (next call) |
460 |
ENDIF |
viscAh_W(i,j,kp1,bi,bj)=0.5*viscAh_D(i,j) |
461 |
|
viscA4_W(i,j,kp1,bi,bj)=0.5*viscA4_D(i,j) |
462 |
|
|
463 |
|
C Note that previous call of this function has already added half. |
464 |
|
viscAh_W(i,j,k,bi,bj)=viscAh_W(i,j,k,bi,bj)+0.5*viscAh_D(i,j) |
465 |
|
viscA4_W(i,j,k,bi,bj)=viscA4_W(i,j,k,bi,bj)+0.5*viscA4_D(i,j) |
466 |
|
|
|
L3=(L2**1.5) |
|
|
L4=(L2**2) |
|
|
L5=(L2**2.5) |
|
|
|
|
|
L2rdt=0.25 _d 0*recip_dt*L2 |
|
|
IF (useAreaViscLength) THEN |
|
|
L4rdt=0.125 _d 0*recip_dt*rAz(i,j,bi,bj)**2 |
|
|
ELSE |
|
|
L4rdt=recip_dt/ |
|
|
& ( 6. _d 0*(recip_DXV(I,J,bi,bj)**4+recip_DYU(I,J,bi,bj)**4) |
|
|
& +8. _d 0*((recip_DXV(I,J,bi,bj)*recip_DYU(I,J,bi,bj))**2)) |
|
467 |
ENDIF |
ENDIF |
468 |
|
#endif /* ALLOW_NONHYDROSTATIC */ |
469 |
|
|
470 |
|
CCCCCCCCCCCCC Vorticity Point CalculationsCCCCCCCCCCCCCCCCCC |
471 |
|
C These are (powers of) length scales |
472 |
|
L2 = L2_Z(i,j,bi,bj) |
473 |
|
L2rdt = 0.25 _d 0*recip_dt*L2 |
474 |
|
L3 = L3_Z(i,j,bi,bj) |
475 |
|
L4rdt = L4rdt_Z(i,j,bi,bj) |
476 |
|
L5 = (L2*L3) |
477 |
|
|
478 |
|
#ifndef AUTODIFF_DISABLE_REYNOLDS_SCALE |
479 |
C Velocity Reynolds Scale (Pb here at CS-grid corners !) |
C Velocity Reynolds Scale (Pb here at CS-grid corners !) |
480 |
IF ( viscAhRe_max.GT.0. .OR. viscA4Re_max.GT.0. ) THEN |
IF ( viscAhRe_max.GT.0. .OR. viscA4Re_max.GT.0. ) THEN |
481 |
keZpt=0.25 _d 0*( (KE(i,j)+KE(i-1,j-1)) |
keZpt=0.25 _d 0*( (KE(i,j)+KE(i-1,j-1)) |
482 |
& +(KE(i-1,j)+KE(i,j-1)) ) |
& +(KE(i-1,j)+KE(i,j-1)) ) |
483 |
IF ( keZpt.GT.0. ) THEN |
IF ( keZpt.GT.0. ) THEN |
484 |
Uscl = sqrt(keZpt*L2)*viscAhRe_max |
Uscl = SQRT(keZpt*L2)*viscAhRe_max |
485 |
U4scl= sqrt(keZpt)*L3*viscA4Re_max |
U4scl= SQRT(keZpt)*L3*viscA4Re_max |
486 |
ELSE |
ELSE |
487 |
Uscl =0. |
Uscl =0. |
488 |
U4scl=0. |
U4scl=0. |
491 |
Uscl =0. |
Uscl =0. |
492 |
U4scl=0. |
U4scl=0. |
493 |
ENDIF |
ENDIF |
494 |
|
#endif /* ndef AUTODIFF_DISABLE_REYNOLDS_SCALE */ |
495 |
|
|
496 |
|
#ifndef AUTODIFF_DISABLE_LEITH |
497 |
C This is the vector magnitude of the vorticity gradient squared |
C This is the vector magnitude of the vorticity gradient squared |
498 |
IF (useFullLeith.and.calcleith) THEN |
IF (useFullLeith.AND.calcLeith) THEN |
499 |
grdVrt=0.25 _d 0*( |
grdVrt=0.25 _d 0*( (vrtDx(i-1,j)*vrtDx(i-1,j) |
500 |
& ((vort3(i+1,j)-vort3(i,j))*recip_DXG(i,j,bi,bj))**2 |
& + vrtDx(i,j)*vrtDx(i,j) ) |
501 |
& +((vort3(i,j+1)-vort3(i,j))*recip_DYG(i,j,bi,bj))**2 |
& + (vrtDy(i,j-1)*vrtDy(i,j-1) |
502 |
& +((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) |
|
503 |
|
|
504 |
C This is the vector magnitude of grad(div.v) squared |
C This is the vector magnitude of grad(div.v) squared |
505 |
grdDiv=0.25 _d 0*( (divDx(i,j-1)*divDx(i,j-1) |
grdDiv=0.25 _d 0*( (divDx(i,j-1)*divDx(i,j-1) |
508 |
& + divDy(i,j)*divDy(i,j) ) ) |
& + divDy(i,j)*divDy(i,j) ) ) |
509 |
|
|
510 |
viscAh_ZLth(i,j)= |
viscAh_ZLth(i,j)= |
511 |
& sqrt(leith2fac*grdVrt+leithD2fac*grdDiv)*L3 |
& SQRT(leith2fac*grdVrt+leithD2fac*grdDiv)*L3 |
512 |
viscA4_ZLth(i,j)= |
viscA4_ZLth(i,j)= |
513 |
& sqrt(leith4fac*grdVrt+leithD4fac*grdDiv)*L5 |
& SQRT(leith4fac*grdVrt+leithD4fac*grdDiv)*L5 |
514 |
viscAh_ZLthD(i,j)= |
viscAh_ZLthD(i,j)= |
515 |
& sqrt(leithD2fac*grdDiv)*L3 |
& SQRT(leithD2fac*grdDiv)*L3 |
516 |
viscA4_ZLthD(i,j)= |
viscA4_ZLthD(i,j)= |
517 |
& sqrt(leithD4fac*grdDiv)*L5 |
& SQRT(leithD4fac*grdDiv)*L5 |
518 |
|
|
519 |
ELSEIF (calcleith) THEN |
ELSEIF (calcLeith) THEN |
520 |
C but this approximation will work on cube (and differs by 4X) |
C but this approximation will work on cube (and differs by 4X) |
521 |
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)) ) |
522 |
grdVrt=max(grdVrt, |
grdVrt=MAX( grdVrt, ABS(vrtDy(i,j-1)) ) |
523 |
& abs((vort3(i,j+1)-vort3(i,j))*recip_DYG(i,j,bi,bj))) |
grdVrt=MAX( grdVrt, ABS(vrtDy(i,j)) ) |
524 |
grdVrt=max(grdVrt, |
|
525 |
& 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)) ) |
526 |
grdVrt=max(grdVrt, |
grdDiv=MAX( grdDiv, ABS(divDy(i,j)) ) |
527 |
& abs((vort3(i,j-1)-vort3(i,j))*recip_DYG(i,j-1,bi,bj))) |
grdDiv=MAX( grdDiv, ABS(divDy(i-1,j)) ) |
|
|
|
|
grdDiv=max( abs(divDx(i,j)), abs(divDx(i,j-1)) ) |
|
|
grdDiv=max( grdDiv, abs(divDy(i,j)) ) |
|
|
grdDiv=max( grdDiv, abs(divDy(i-1,j)) ) |
|
528 |
|
|
529 |
viscAh_ZLth(i,j)=(leith2fac*grdVrt+(leithD2fac*grdDiv))*L3 |
viscAh_ZLth(i,j)=(leith2fac*grdVrt+(leithD2fac*grdDiv))*L3 |
530 |
viscA4_ZLth(i,j)=(leith4fac*grdVrt+(leithD4fac*grdDiv))*L5 |
viscA4_ZLth(i,j)=(leith4fac*grdVrt+(leithD4fac*grdDiv))*L5 |
537 |
viscA4_ZLthD(i,j)=0. _d 0 |
viscA4_ZLthD(i,j)=0. _d 0 |
538 |
ENDIF |
ENDIF |
539 |
|
|
540 |
IF (calcsmag) THEN |
IF (calcSmag) THEN |
541 |
viscAh_ZSmg(i,j)=L2 |
viscAh_ZSmg(i,j)=L2 |
542 |
& *sqrt(strain(i,j)**2 |
& *SQRT(strain(i,j)**2 |
543 |
& +0.25 _d 0*(tension( i , j )**2+tension( i ,j-1)**2 |
& +0.25 _d 0*(tension( i , j )**2+tension( i ,j-1)**2 |
544 |
& +tension(i-1, j )**2+tension(i-1,j-1)**2)) |
& +tension(i-1, j )**2+tension(i-1,j-1)**2)) |
545 |
viscA4_ZSmg(i,j)=smag4fac*L2*viscAh_ZSmg(i,j) |
viscA4_ZSmg(i,j)=smag4fac*L2*viscAh_ZSmg(i,j) |
546 |
viscAh_ZSmg(i,j)=smag2fac*viscAh_ZSmg(i,j) |
viscAh_ZSmg(i,j)=smag2fac*viscAh_ZSmg(i,j) |
547 |
ENDIF |
ENDIF |
548 |
|
#endif /* AUTODIFF_DISABLE_LEITH */ |
549 |
|
|
550 |
C Harmonic on Zeta points |
C Harmonic on Zeta points |
551 |
Alin=viscAhZ+viscAhGrid*L2rdt |
Alin=viscAhZ+viscAhGrid*L2rdt |
552 |
& +viscAh_ZLth(i,j)+viscAh_ZSmg(i,j) |
& +viscAh_ZLth(i,j)+viscAh_ZSmg(i,j) |
553 |
viscAh_ZMin(i,j)=max(viscAhGridMin*L2rdt,Uscl) |
viscAh_ZMin(i,j)=MAX(viscAhGridMin*L2rdt,Uscl) |
554 |
viscAh_Z(i,j)=max(viscAh_ZMin(i,j),Alin) |
viscAh_Z(i,j)=MAX(viscAh_ZMin(i,j),Alin) |
555 |
viscAh_ZMax(i,j)=min(viscAhGridMax*L2rdt,viscAhMax) |
viscAh_ZMax(i,j)=MIN(viscAhGridMax*L2rdt,viscAhMax) |
556 |
viscAh_Z(i,j)=min(viscAh_ZMax(i,j),viscAh_Z(i,j)) |
viscAh_Z(i,j)=MIN(viscAh_ZMax(i,j),viscAh_Z(i,j)) |
557 |
|
|
558 |
C BiHarmonic on Zeta points |
C BiHarmonic on Zeta points |
559 |
Alin=viscA4Z+viscA4Grid*L4rdt |
Alin=viscA4Z+viscA4Grid*L4rdt |
560 |
& +viscA4_ZLth(i,j)+viscA4_ZSmg(i,j) |
& +viscA4_ZLth(i,j)+viscA4_ZSmg(i,j) |
561 |
viscA4_ZMin(i,j)=max(viscA4GridMin*L4rdt,U4scl) |
viscA4_ZMin(i,j)=MAX(viscA4GridMin*L4rdt,U4scl) |
562 |
viscA4_Z(i,j)=max(viscA4_ZMin(i,j),Alin) |
viscA4_Z(i,j)=MAX(viscA4_ZMin(i,j),Alin) |
563 |
viscA4_ZMax(i,j)=min(viscA4GridMax*L4rdt,viscA4Max) |
viscA4_ZMax(i,j)=MIN(viscA4GridMax*L4rdt,viscA4Max) |
564 |
viscA4_Z(i,j)=min(viscA4_ZMax(i,j),viscA4_Z(i,j)) |
viscA4_Z(i,j)=MIN(viscA4_ZMax(i,j),viscA4_Z(i,j)) |
565 |
ENDDO |
ENDDO |
566 |
ENDDO |
ENDDO |
567 |
|
|
568 |
ELSE |
ELSE |
569 |
|
C---- use constant viscosity (useVariableViscosity=F): |
570 |
|
|
571 |
DO j=1-Oly,sNy+Oly |
DO j=1-Oly,sNy+Oly |
572 |
DO i=1-Olx,sNx+Olx |
DO i=1-Olx,sNx+Olx |
573 |
viscAh_D(i,j)=viscAhD |
viscAh_D(i,j)=viscAhD |
576 |
viscA4_Z(i,j)=viscA4Z |
viscA4_Z(i,j)=viscA4Z |
577 |
ENDDO |
ENDDO |
578 |
ENDDO |
ENDDO |
579 |
|
|
580 |
|
C---- variable/constant viscosity : end if/else block |
581 |
ENDIF |
ENDIF |
582 |
|
|
583 |
#ifdef ALLOW_DIAGNOSTICS |
#ifdef ALLOW_DIAGNOSTICS |