34 |
INTEGER i,j,k |
INTEGER i,j,k |
35 |
INTEGER ks, kp1 |
INTEGER ks, kp1 |
36 |
_RL numPnts,theVol,tmpVal, mskp1, msk_1 |
_RL numPnts,theVol,tmpVal, mskp1, msk_1 |
37 |
_RL weight0, weight1 |
_RL abFac1, abFac2, R_drK, cosLat |
38 |
_RL theMax,theMean,theVolMean,potEnMean |
_RL theMax,theMean,theVolMean,potEnMean |
39 |
_RL uBarC, vBarC, totAMu, totAMs |
_RL totAMu, totAMs |
40 |
_RL tileMean(nSx,nSy) |
_RL tileMean(nSx,nSy) |
41 |
_RL tileVlAv(nSx,nSy) |
_RL tileVlAv(nSx,nSy) |
42 |
_RL tilePEav(nSx,nSy) |
_RL tilePEav(nSx,nSy) |
43 |
_RL tileVol (nSx,nSy) |
_RL tileVol (nSx,nSy) |
44 |
_RL tileAMu (nSx,nSy) |
_RL tileAMu (nSx,nSy) |
45 |
_RL tileAMs (nSx,nSy) |
_RL tileAMs (nSx,nSy) |
46 |
_RL radDist(1:sNx,1:sNy) |
_RL tmpFld(1:sNx,1:sNy) |
47 |
|
_RS cos2LatG(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
48 |
#ifdef ALLOW_NONHYDROSTATIC |
#ifdef ALLOW_NONHYDROSTATIC |
49 |
_RL tmpWke |
_RL tmpWke |
50 |
#endif |
#endif |
51 |
|
#ifdef ALLOW_ADAMSBASHFORTH_3 |
52 |
|
INTEGER m1, m2 |
53 |
|
#endif |
54 |
|
|
55 |
C---+----1----+----2----+----3----+----4----+----5----+----6----+----7-|--+----| |
C---+----1----+----2----+----3----+----4----+----5----+----6----+----7-|--+----| |
56 |
|
|
169 |
IF ( mon_output_AM ) THEN |
IF ( mon_output_AM ) THEN |
170 |
DO bj=myByLo(myThid),myByHi(myThid) |
DO bj=myByLo(myThid),myByHi(myThid) |
171 |
DO bi=myBxLo(myThid),myBxHi(myThid) |
DO bi=myBxLo(myThid),myBxHi(myThid) |
172 |
C- calculate radial distance |
C- Calculate contribution from zonal velocity |
173 |
|
abFac1 = 0. _d 0 |
174 |
|
abFac2 = 0. _d 0 |
175 |
|
#ifdef ALLOW_ADAMSBASHFORTH_3 |
176 |
|
m1 = 1 + mod(myIter+1,2) |
177 |
|
m2 = 1 + mod( myIter ,2) |
178 |
|
IF ( myIter.GE.2 ) abFac2 = beta_AB |
179 |
|
IF ( myIter.GE.1 ) abFac1 = -( alph_AB + abFac2 ) |
180 |
|
#else |
181 |
|
IF ( myIter.GE.1 ) abFac1 = -( 0.5 _d 0 + abEps ) |
182 |
|
#endif |
183 |
|
C- contribution from uVel component: 1rst integrate vertically |
184 |
DO j=1,sNy |
DO j=1,sNy |
185 |
DO i=1,sNx |
DO i=1,sNx |
186 |
radDist(i,j) = rSphere*COS( deg2rad*yC(i,j,bi,bj) ) |
tmpFld(i,j) = 0. _d 0 |
|
& *maskInC(i,j,bi,bj) |
|
187 |
ENDDO |
ENDDO |
188 |
ENDDO |
ENDDO |
|
C- calculate contribution from zonal velocity |
|
|
tileAMu(bi,bj) = 0. _d 0 |
|
|
tileAMs(bi,bj) = 0. _d 0 |
|
189 |
DO k=1,Nr |
DO k=1,Nr |
190 |
|
R_drK = rSphere*deepFacC(k)*deepFac2C(k) |
191 |
|
& *rhoFacC(k)*drF(k) |
192 |
DO j=1,sNy |
DO j=1,sNy |
193 |
DO i=1,sNx |
DO i=1,sNx |
194 |
uBarC = (uVel(i,j,k,bi,bj)+uVel(i+1,j,k,bi,bj))*0.5 _d 0 |
#ifdef ALLOW_ADAMSBASHFORTH_3 |
195 |
vBarC = (vVel(i,j,k,bi,bj)+vVel(i,j+1,k,bi,bj))*0.5 _d 0 |
tmpVal = abFac1*guNm(i,j,k,bi,bj,m1) |
196 |
tmpVal = ( angleCosC(i,j,bi,bj)*uBarC |
& + abFac2*guNm(i,j,k,bi,bj,m2) |
197 |
& -angleSinC(i,j,bi,bj)*vBarC |
#else |
198 |
& )*radDist(i,j)*deepFacC(k) |
tmpVal = abFac1*guNm1(i,j,k,bi,bj) |
199 |
tileAMu(bi,bj) = tileAMu(bi,bj) |
#endif |
200 |
& + tmpVal*rA(i,j,bi,bj)*deepFac2C(k) |
tmpVal = tmpVal*deltaTMom + uVel(i,j,k,bi,bj) |
201 |
& *rhoFacC(k)*drF(k)*_hFacC(i,j,k,bi,bj) |
tmpFld(i,j) = tmpFld(i,j) |
202 |
|
& + R_drK*tmpVal*_hFacW(i,j,k,bi,bj) |
203 |
ENDDO |
ENDDO |
204 |
ENDDO |
ENDDO |
205 |
ENDDO |
ENDDO |
206 |
C- and contribution from mass distribution anomaly (i.e., free-surface) |
C- and then integrate horizontally over this tile |
207 |
c IF ( .FALSE. ) THEN |
DO j=1,sNy |
208 |
IF ( exactConserv ) THEN |
DO i=1,sNx |
209 |
C- To improve balance between zonal-wind (AMu) and mass (AMs) AM, need |
cosLat = COS( deg2rad* |
210 |
C a consistent time-stepping of meridional mass transport in Coriolis |
& ( yG(i,j,bi,bj) + yG(i,j+1,bi,bj) )*halfRL ) |
211 |
C (zonal momentum, go through AB) and mass transport divergence; |
tmpFld(i,j) = tmpFld(i,j)*u2zonDir(i,j,bi,bj) |
212 |
C try to account for AB-2 in AMs the same way it applies to f*v: |
& *cosLat*rAw(i,j,bi,bj) |
213 |
|
& *maskInW(i,j,bi,bj) |
214 |
|
ENDDO |
215 |
|
ENDDO |
216 |
|
tileAMu(bi,bj) = 0. _d 0 |
217 |
|
DO j=1,sNy |
218 |
|
DO i=1,sNx |
219 |
|
tileAMu(bi,bj) = tileAMu(bi,bj) + tmpFld(i,j) |
220 |
|
ENDDO |
221 |
|
ENDDO |
222 |
|
C- contribution from vVel component: 1rst integrate vertically |
223 |
|
DO j=1,sNy |
224 |
|
DO i=1,sNx |
225 |
|
tmpFld(i,j) = 0. _d 0 |
226 |
|
ENDDO |
227 |
|
ENDDO |
228 |
|
DO k=1,Nr |
229 |
|
R_drK = rSphere*deepFacC(k)*deepFac2C(k) |
230 |
|
& *rhoFacC(k)*drF(k) |
231 |
|
DO j=1,sNy |
232 |
|
DO i=1,sNx |
233 |
#ifdef ALLOW_ADAMSBASHFORTH_3 |
#ifdef ALLOW_ADAMSBASHFORTH_3 |
234 |
weight1 = alph_AB |
tmpVal = abFac1*gvNm(i,j,k,bi,bj,m1) |
235 |
|
& + abFac2*gvNm(i,j,k,bi,bj,m2) |
236 |
#else |
#else |
237 |
weight1 = 0.5 _d 0 + abEps |
tmpVal = abFac1*gvNm1(i,j,k,bi,bj) |
238 |
#endif |
#endif |
239 |
weight0 = 1.0 _d 0 - weight1 |
tmpVal = tmpVal*deltaTMom + vVel(i,j,k,bi,bj) |
240 |
|
tmpFld(i,j) = tmpFld(i,j) |
241 |
|
& + R_drK*tmpVal*_hFacS(i,j,k,bi,bj) |
242 |
|
ENDDO |
243 |
|
ENDDO |
244 |
|
ENDDO |
245 |
|
C- and then integrate horizontally over this tile |
246 |
|
DO j=1,sNy |
247 |
|
DO i=1,sNx |
248 |
|
cosLat = COS( deg2rad* |
249 |
|
& ( yG(i,j,bi,bj) + yG(i+1,j,bi,bj) )*halfRL ) |
250 |
|
tmpFld(i,j) = tmpFld(i,j)*v2zonDir(i,j,bi,bj) |
251 |
|
& *cosLat*rAs(i,j,bi,bj) |
252 |
|
& *maskInS(i,j,bi,bj) |
253 |
|
ENDDO |
254 |
|
ENDDO |
255 |
|
DO j=1,sNy |
256 |
|
DO i=1,sNx |
257 |
|
tileAMu(bi,bj) = tileAMu(bi,bj) + tmpFld(i,j) |
258 |
|
ENDDO |
259 |
|
ENDDO |
260 |
|
C- Calculate contribution from mass distribution anomaly (i.e., free-surface) |
261 |
|
IF ( exactConserv ) THEN |
262 |
DO j=1,sNy |
DO j=1,sNy |
263 |
DO i=1,sNx |
DO i=1,sNx |
|
ks = kSurfC(i,j,bi,bj) |
|
|
tmpVal = weight1*etaH(i,j,bi,bj) |
|
264 |
#ifdef EXACT_CONSERV |
#ifdef EXACT_CONSERV |
265 |
& + weight0*etaHnm1(i,j,bi,bj) |
tmpFld(i,j) = etaHnm1(i,j,bi,bj) |
266 |
|
#else |
267 |
|
tmpFld(i,j) = 0. |
268 |
#endif |
#endif |
|
tmpVal = omega*tmpVal |
|
|
& * radDist(i,j)*radDist(i,j)*deepFac2F(ks) |
|
|
tileAMs(bi,bj) = tileAMs(bi,bj) |
|
|
& + tmpVal*rA(i,j,bi,bj)*deepFac2F(ks)*rhoFacF(ks) |
|
269 |
ENDDO |
ENDDO |
270 |
ENDDO |
ENDDO |
271 |
ELSE |
ELSE |
272 |
DO j=1,sNy |
DO j=1,sNy |
273 |
DO i=1,sNx |
DO i=1,sNx |
274 |
ks = kSurfC(i,j,bi,bj) |
tmpFld(i,j) = etaN(i,j,bi,bj) |
|
tmpVal = omega*etaN(i,j,bi,bj) |
|
|
& * radDist(i,j)*radDist(i,j)*deepFac2F(ks) |
|
|
tileAMs(bi,bj) = tileAMs(bi,bj) |
|
|
& + tmpVal*rA(i,j,bi,bj)*deepFac2F(ks)*rhoFacF(ks) |
|
275 |
ENDDO |
ENDDO |
276 |
ENDDO |
ENDDO |
277 |
ENDIF |
ENDIF |
278 |
|
C- calculate angular momentum from mass-distribution anomaly |
279 |
|
C using square of radial distance (averaged @ center point) |
280 |
|
DO j=1-OLy,sNy+OLy |
281 |
|
DO i=1-OLx,sNx+OLx |
282 |
|
cosLat = COS( deg2rad*yG(i,j,bi,bj) ) |
283 |
|
cos2LatG(i,j) = cosLat*cosLat |
284 |
|
ENDDO |
285 |
|
ENDDO |
286 |
|
DO j=1,sNy |
287 |
|
DO i=1,sNx |
288 |
|
tmpFld(i,j) = tmpFld(i,j) |
289 |
|
& *omega*rSphere*rSphere |
290 |
|
& *( ( cos2LatG(i,j) + cos2LatG(i+1,j+1) ) |
291 |
|
& + ( cos2LatG(i+1,j) + cos2LatG(i,j+1) ) |
292 |
|
& )*0.25 _d 0 |
293 |
|
ENDDO |
294 |
|
ENDDO |
295 |
|
DO j=1,sNy |
296 |
|
DO i=1,sNx |
297 |
|
ks = kSurfC(i,j,bi,bj) |
298 |
|
tmpFld(i,j) = tmpFld(i,j) |
299 |
|
& *maskInC(i,j,bi,bj)*deepFac2F(ks) |
300 |
|
& *rA(i,j,bi,bj)*deepFac2F(ks)*rhoFacF(ks) |
301 |
|
ENDDO |
302 |
|
ENDDO |
303 |
|
tileAMs(bi,bj) = 0. _d 0 |
304 |
|
DO j=1,sNy |
305 |
|
DO i=1,sNx |
306 |
|
tileAMs(bi,bj) = tileAMs(bi,bj) + tmpFld(i,j) |
307 |
|
ENDDO |
308 |
|
ENDDO |
309 |
C- end bi,bj loops |
C- end bi,bj loops |
310 |
ENDDO |
ENDDO |
311 |
ENDDO |
ENDDO |
322 |
& '_eta_mean', myThid ) |
& '_eta_mean', myThid ) |
323 |
CALL MON_OUT_RL( mon_string_none, totAMu, |
CALL MON_OUT_RL( mon_string_none, totAMu, |
324 |
& '_uZo_mean', myThid ) |
& '_uZo_mean', myThid ) |
325 |
totAMu = totAMu + totAMs |
totAMu = totAMu + freeSurfFac*totAMs |
326 |
CALL MON_OUT_RL( mon_string_none, totAMu, |
CALL MON_OUT_RL( mon_string_none, totAMu, |
327 |
& '_tot_mean', myThid ) |
& '_tot_mean', myThid ) |
328 |
|
|