1 |
C $Header: /u/gcmpack/MITgcm/pkg/mom_vecinv/mom_vecinv.F,v 1.11 2003/11/04 19:51:54 edhill Exp $ |
2 |
C $Name: $ |
3 |
|
4 |
#include "PACKAGES_CONFIG.h" |
5 |
#include "CPP_OPTIONS.h" |
6 |
|
7 |
SUBROUTINE MOM_VECINV( |
8 |
I bi,bj,iMin,iMax,jMin,jMax,k,kUp,kDown, |
9 |
I dPhiHydX,dPhiHydY,KappaRU,KappaRV, |
10 |
U fVerU, fVerV, |
11 |
I myCurrentTime, myIter, myThid) |
12 |
C /==========================================================\ |
13 |
C | S/R MOM_VECINV | |
14 |
C | o Form the right hand-side of the momentum equation. | |
15 |
C |==========================================================| |
16 |
C | Terms are evaluated one layer at a time working from | |
17 |
C | the bottom to the top. The vertically integrated | |
18 |
C | barotropic flow tendency term is evluated by summing the | |
19 |
C | tendencies. | |
20 |
C | Notes: | |
21 |
C | We have not sorted out an entirely satisfactory formula | |
22 |
C | for the diffusion equation bc with lopping. The present | |
23 |
C | form produces a diffusive flux that does not scale with | |
24 |
C | open-area. Need to do something to solidfy this and to | |
25 |
C | deal "properly" with thin walls. | |
26 |
C \==========================================================/ |
27 |
IMPLICIT NONE |
28 |
|
29 |
C == Global variables == |
30 |
#include "SIZE.h" |
31 |
#include "DYNVARS.h" |
32 |
#include "EEPARAMS.h" |
33 |
#include "PARAMS.h" |
34 |
#include "GRID.h" |
35 |
#ifdef ALLOW_TIMEAVE |
36 |
#include "TIMEAVE_STATV.h" |
37 |
#endif |
38 |
|
39 |
C == Routine arguments == |
40 |
C fVerU - Flux of momentum in the vertical |
41 |
C fVerV direction out of the upper face of a cell K |
42 |
C ( flux into the cell above ). |
43 |
C dPhiHydX,Y :: Gradient (X & Y dir.) of Hydrostatic Potential |
44 |
C bi, bj, iMin, iMax, jMin, jMax - Range of points for which calculation |
45 |
C results will be set. |
46 |
C kUp, kDown - Index for upper and lower layers. |
47 |
C myThid - Instance number for this innvocation of CALC_MOM_RHS |
48 |
_RL dPhiHydX(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
49 |
_RL dPhiHydY(1-Olx:sNx+Olx,1-Oly:sNy+Oly) |
50 |
_RL KappaRU(1-OLx:sNx+OLx,1-OLy:sNy+OLy,Nr) |
51 |
_RL KappaRV(1-OLx:sNx+OLx,1-OLy:sNy+OLy,Nr) |
52 |
_RL fVerU(1-OLx:sNx+OLx,1-OLy:sNy+OLy,2) |
53 |
_RL fVerV(1-OLx:sNx+OLx,1-OLy:sNy+OLy,2) |
54 |
INTEGER kUp,kDown |
55 |
_RL myCurrentTime |
56 |
INTEGER myIter |
57 |
INTEGER myThid |
58 |
INTEGER bi,bj,iMin,iMax,jMin,jMax |
59 |
|
60 |
#ifdef ALLOW_MOM_VECINV |
61 |
|
62 |
C == Functions == |
63 |
LOGICAL DIFFERENT_MULTIPLE |
64 |
EXTERNAL DIFFERENT_MULTIPLE |
65 |
|
66 |
C == Local variables == |
67 |
_RL aF (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
68 |
_RL vF (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
69 |
_RL vrF (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
70 |
_RL uCf (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
71 |
_RL vCf (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
72 |
_RL mT (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
73 |
_RL pF (1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
74 |
_RL del2u(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
75 |
_RL del2v(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
76 |
_RL tension(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
77 |
_RL strain(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
78 |
_RS hFacZ(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
79 |
_RS r_hFacZ(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
80 |
_RS xA(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
81 |
_RS yA(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
82 |
_RL uFld(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
83 |
_RL vFld(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
84 |
_RL dStar(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
85 |
_RL zStar(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
86 |
_RL uDiss(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
87 |
_RL vDiss(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
88 |
C I,J,K - Loop counters |
89 |
INTEGER i,j,k |
90 |
C rVelMaskOverride - Factor for imposing special surface boundary conditions |
91 |
C ( set according to free-surface condition ). |
92 |
C hFacROpen - Lopped cell factos used tohold fraction of open |
93 |
C hFacRClosed and closed cell wall. |
94 |
_RL rVelMaskOverride |
95 |
C xxxFac - On-off tracer parameters used for switching terms off. |
96 |
_RL uDudxFac |
97 |
_RL AhDudxFac |
98 |
_RL A4DuxxdxFac |
99 |
_RL vDudyFac |
100 |
_RL AhDudyFac |
101 |
_RL A4DuyydyFac |
102 |
_RL rVelDudrFac |
103 |
_RL ArDudrFac |
104 |
_RL fuFac |
105 |
_RL phxFac |
106 |
_RL mtFacU |
107 |
_RL uDvdxFac |
108 |
_RL AhDvdxFac |
109 |
_RL A4DvxxdxFac |
110 |
_RL vDvdyFac |
111 |
_RL AhDvdyFac |
112 |
_RL A4DvyydyFac |
113 |
_RL rVelDvdrFac |
114 |
_RL ArDvdrFac |
115 |
_RL fvFac |
116 |
_RL phyFac |
117 |
_RL vForcFac |
118 |
_RL mtFacV |
119 |
_RL wVelBottomOverride |
120 |
LOGICAL bottomDragTerms |
121 |
_RL KE(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
122 |
_RL omega3(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
123 |
_RL vort3(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
124 |
_RL hDiv(1-OLx:sNx+OLx,1-OLy:sNy+OLy) |
125 |
|
126 |
#ifdef ALLOW_AUTODIFF_TAMC |
127 |
C-- only the kDown part of fverU/V is set in this subroutine |
128 |
C-- the kUp is still required |
129 |
C-- In the case of mom_fluxform Kup is set as well |
130 |
C-- (at least in part) |
131 |
fVerU(1,1,kUp) = fVerU(1,1,kUp) |
132 |
fVerV(1,1,kUp) = fVerV(1,1,kUp) |
133 |
#endif |
134 |
|
135 |
rVelMaskOverride=1. |
136 |
IF ( k .EQ. 1 ) rVelMaskOverride=freeSurfFac |
137 |
wVelBottomOverride=1. |
138 |
IF (k.EQ.Nr) wVelBottomOverride=0. |
139 |
|
140 |
C Initialise intermediate terms |
141 |
DO J=1-OLy,sNy+OLy |
142 |
DO I=1-OLx,sNx+OLx |
143 |
aF(i,j) = 0. |
144 |
vF(i,j) = 0. |
145 |
vrF(i,j) = 0. |
146 |
uCf(i,j) = 0. |
147 |
vCf(i,j) = 0. |
148 |
mT(i,j) = 0. |
149 |
pF(i,j) = 0. |
150 |
del2u(i,j) = 0. |
151 |
del2v(i,j) = 0. |
152 |
dStar(i,j) = 0. |
153 |
zStar(i,j) = 0. |
154 |
uDiss(i,j) = 0. |
155 |
vDiss(i,j) = 0. |
156 |
vort3(i,j) = 0. |
157 |
omega3(i,j) = 0. |
158 |
ke(i,j) = 0. |
159 |
#ifdef ALLOW_AUTODIFF_TAMC |
160 |
strain(i,j) = 0. _d 0 |
161 |
tension(i,j) = 0. _d 0 |
162 |
#endif |
163 |
ENDDO |
164 |
ENDDO |
165 |
|
166 |
C-- Term by term tracer parmeters |
167 |
C o U momentum equation |
168 |
uDudxFac = afFacMom*1. |
169 |
AhDudxFac = vfFacMom*1. |
170 |
A4DuxxdxFac = vfFacMom*1. |
171 |
vDudyFac = afFacMom*1. |
172 |
AhDudyFac = vfFacMom*1. |
173 |
A4DuyydyFac = vfFacMom*1. |
174 |
rVelDudrFac = afFacMom*1. |
175 |
ArDudrFac = vfFacMom*1. |
176 |
mTFacU = mtFacMom*1. |
177 |
fuFac = cfFacMom*1. |
178 |
phxFac = pfFacMom*1. |
179 |
C o V momentum equation |
180 |
uDvdxFac = afFacMom*1. |
181 |
AhDvdxFac = vfFacMom*1. |
182 |
A4DvxxdxFac = vfFacMom*1. |
183 |
vDvdyFac = afFacMom*1. |
184 |
AhDvdyFac = vfFacMom*1. |
185 |
A4DvyydyFac = vfFacMom*1. |
186 |
rVelDvdrFac = afFacMom*1. |
187 |
ArDvdrFac = vfFacMom*1. |
188 |
mTFacV = mtFacMom*1. |
189 |
fvFac = cfFacMom*1. |
190 |
phyFac = pfFacMom*1. |
191 |
vForcFac = foFacMom*1. |
192 |
|
193 |
IF ( no_slip_bottom |
194 |
& .OR. bottomDragQuadratic.NE.0. |
195 |
& .OR. bottomDragLinear.NE.0.) THEN |
196 |
bottomDragTerms=.TRUE. |
197 |
ELSE |
198 |
bottomDragTerms=.FALSE. |
199 |
ENDIF |
200 |
|
201 |
C-- with stagger time stepping, grad Phi_Hyp is directly incoporated in TIMESTEP |
202 |
IF (staggerTimeStep) THEN |
203 |
phxFac = 0. |
204 |
phyFac = 0. |
205 |
ENDIF |
206 |
|
207 |
C-- Calculate open water fraction at vorticity points |
208 |
CALL MOM_CALC_HFACZ(bi,bj,k,hFacZ,r_hFacZ,myThid) |
209 |
|
210 |
C---- Calculate common quantities used in both U and V equations |
211 |
C Calculate tracer cell face open areas |
212 |
DO j=1-OLy,sNy+OLy |
213 |
DO i=1-OLx,sNx+OLx |
214 |
xA(i,j) = _dyG(i,j,bi,bj) |
215 |
& *drF(k)*_hFacW(i,j,k,bi,bj) |
216 |
yA(i,j) = _dxG(i,j,bi,bj) |
217 |
& *drF(k)*_hFacS(i,j,k,bi,bj) |
218 |
ENDDO |
219 |
ENDDO |
220 |
|
221 |
C Make local copies of horizontal flow field |
222 |
DO j=1-OLy,sNy+OLy |
223 |
DO i=1-OLx,sNx+OLx |
224 |
uFld(i,j) = uVel(i,j,k,bi,bj) |
225 |
vFld(i,j) = vVel(i,j,k,bi,bj) |
226 |
ENDDO |
227 |
ENDDO |
228 |
|
229 |
C note (jmc) : Dissipation and Vort3 advection do not necesary |
230 |
C use the same maskZ (and hFacZ) => needs 2 call(s) |
231 |
c CALL MOM_VI_HFACZ_DISS(bi,bj,k,hFacZ,r_hFacZ,myThid) |
232 |
|
233 |
CALL MOM_VI_CALC_KE(bi,bj,k,uFld,vFld,KE,myThid) |
234 |
|
235 |
CALL MOM_VI_CALC_HDIV(bi,bj,k,uFld,vFld,hDiv,myThid) |
236 |
|
237 |
CALL MOM_VI_CALC_RELVORT3(bi,bj,k,uFld,vFld,hFacZ,vort3,myThid) |
238 |
|
239 |
c CALL MOM_VI_CALC_ABSVORT3(bi,bj,k,vort3,omega3,myThid) |
240 |
|
241 |
IF (momViscosity) THEN |
242 |
C Calculate del^2 u and del^2 v for bi-harmonic term |
243 |
IF (viscA4.NE.0.) THEN |
244 |
CALL MOM_VI_DEL2UV(bi,bj,k,hDiv,vort3,hFacZ, |
245 |
O del2u,del2v, |
246 |
& myThid) |
247 |
CALL MOM_VI_CALC_HDIV(bi,bj,k,del2u,del2v,dStar,myThid) |
248 |
CALL MOM_VI_CALC_RELVORT3( |
249 |
& bi,bj,k,del2u,del2v,hFacZ,zStar,myThid) |
250 |
ENDIF |
251 |
C Calculate dissipation terms for U and V equations |
252 |
C in terms of vorticity and divergence |
253 |
IF (viscAh.NE.0. .OR. viscA4.NE.0.) THEN |
254 |
CALL MOM_VI_HDISSIP(bi,bj,k,hDiv,vort3,hFacZ,dStar,zStar, |
255 |
O uDiss,vDiss, |
256 |
& myThid) |
257 |
ENDIF |
258 |
C or in terms of tension and strain |
259 |
IF (viscAstrain.NE.0. .OR. viscAtension.NE.0.) THEN |
260 |
CALL MOM_CALC_TENSION(bi,bj,k,uFld,vFld, |
261 |
O tension, |
262 |
I myThid) |
263 |
CALL MOM_CALC_STRAIN(bi,bj,k,uFld,vFld,hFacZ, |
264 |
O strain, |
265 |
I myThid) |
266 |
CALL MOM_HDISSIP(bi,bj,k, |
267 |
I tension,strain,hFacZ,viscAtension,viscAstrain, |
268 |
O uDiss,vDiss, |
269 |
I myThid) |
270 |
ENDIF |
271 |
ENDIF |
272 |
|
273 |
C- Return to standard hfacZ (min-4) and mask vort3 accordingly: |
274 |
c CALL MOM_VI_MASK_VORT3(bi,bj,k,hFacZ,r_hFacZ,vort3,myThid) |
275 |
|
276 |
C---- Zonal momentum equation starts here |
277 |
|
278 |
C-- Vertical flux (fVer is at upper face of "u" cell) |
279 |
|
280 |
C Eddy component of vertical flux (interior component only) -> vrF |
281 |
IF (momViscosity.AND..NOT.implicitViscosity) |
282 |
& CALL MOM_U_RVISCFLUX(bi,bj,k,uVel,KappaRU,vrF,myThid) |
283 |
|
284 |
C Combine fluxes |
285 |
DO j=jMin,jMax |
286 |
DO i=iMin,iMax |
287 |
fVerU(i,j,kDown) = ArDudrFac*vrF(i,j) |
288 |
ENDDO |
289 |
ENDDO |
290 |
|
291 |
C-- Tendency is minus divergence of the fluxes + coriolis + pressure term |
292 |
DO j=2-Oly,sNy+Oly-1 |
293 |
DO i=2-Olx,sNx+Olx-1 |
294 |
gU(i,j,k,bi,bj) = uDiss(i,j) |
295 |
& -_recip_hFacW(i,j,k,bi,bj)*recip_drF(k) |
296 |
& *recip_rAw(i,j,bi,bj) |
297 |
& *( |
298 |
& +fVerU(i,j,kUp)*rkFac - fVerU(i,j,kDown)*rkFac |
299 |
& ) |
300 |
& - phxFac*dPhiHydX(i,j) |
301 |
ENDDO |
302 |
ENDDO |
303 |
|
304 |
C-- No-slip and drag BCs appear as body forces in cell abutting topography |
305 |
IF (momViscosity.AND.no_slip_sides) THEN |
306 |
C- No-slip BCs impose a drag at walls... |
307 |
CALL MOM_U_SIDEDRAG(bi,bj,k,uFld,del2u,hFacZ,vF,myThid) |
308 |
DO j=jMin,jMax |
309 |
DO i=iMin,iMax |
310 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+vF(i,j) |
311 |
ENDDO |
312 |
ENDDO |
313 |
ENDIF |
314 |
|
315 |
C- No-slip BCs impose a drag at bottom |
316 |
IF (momViscosity.AND.bottomDragTerms) THEN |
317 |
CALL MOM_U_BOTTOMDRAG(bi,bj,k,uFld,KE,KappaRU,vF,myThid) |
318 |
DO j=jMin,jMax |
319 |
DO i=iMin,iMax |
320 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+vF(i,j) |
321 |
ENDDO |
322 |
ENDDO |
323 |
ENDIF |
324 |
|
325 |
C-- Metric terms for curvilinear grid systems |
326 |
c IF (usingSphericalPolarMTerms) THEN |
327 |
C o Spherical polar grid metric terms |
328 |
c CALL MOM_U_METRIC_NH(bi,bj,k,uFld,wVel,mT,myThid) |
329 |
c DO j=jMin,jMax |
330 |
c DO i=iMin,iMax |
331 |
c gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+mTFacU*mT(i,j) |
332 |
c ENDDO |
333 |
c ENDDO |
334 |
c ENDIF |
335 |
|
336 |
C---- Meridional momentum equation starts here |
337 |
|
338 |
C-- Vertical flux (fVer is at upper face of "v" cell) |
339 |
|
340 |
C Eddy component of vertical flux (interior component only) -> vrF |
341 |
IF (momViscosity.AND..NOT.implicitViscosity) |
342 |
& CALL MOM_V_RVISCFLUX(bi,bj,k,vVel,KappaRV,vrf,myThid) |
343 |
|
344 |
C Combine fluxes -> fVerV |
345 |
DO j=jMin,jMax |
346 |
DO i=iMin,iMax |
347 |
fVerV(i,j,kDown) = ArDvdrFac*vrF(i,j) |
348 |
ENDDO |
349 |
ENDDO |
350 |
|
351 |
C-- Tendency is minus divergence of the fluxes + coriolis + pressure term |
352 |
DO j=jMin,jMax |
353 |
DO i=iMin,iMax |
354 |
gV(i,j,k,bi,bj) = vDiss(i,j) |
355 |
& -_recip_hFacS(i,j,k,bi,bj)*recip_drF(k) |
356 |
& *recip_rAs(i,j,bi,bj) |
357 |
& *( |
358 |
& +fVerV(i,j,kUp)*rkFac - fVerV(i,j,kDown)*rkFac |
359 |
& ) |
360 |
& - phyFac*dPhiHydY(i,j) |
361 |
ENDDO |
362 |
ENDDO |
363 |
|
364 |
C-- No-slip and drag BCs appear as body forces in cell abutting topography |
365 |
IF (momViscosity.AND.no_slip_sides) THEN |
366 |
C- No-slip BCs impose a drag at walls... |
367 |
CALL MOM_V_SIDEDRAG(bi,bj,k,vFld,del2v,hFacZ,vF,myThid) |
368 |
DO j=jMin,jMax |
369 |
DO i=iMin,iMax |
370 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vF(i,j) |
371 |
ENDDO |
372 |
ENDDO |
373 |
ENDIF |
374 |
C- No-slip BCs impose a drag at bottom |
375 |
IF (momViscosity.AND.bottomDragTerms) THEN |
376 |
CALL MOM_V_BOTTOMDRAG(bi,bj,k,vFld,KE,KappaRV,vF,myThid) |
377 |
DO j=jMin,jMax |
378 |
DO i=iMin,iMax |
379 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vF(i,j) |
380 |
ENDDO |
381 |
ENDDO |
382 |
ENDIF |
383 |
|
384 |
C-- Metric terms for curvilinear grid systems |
385 |
c IF (usingSphericalPolarMTerms) THEN |
386 |
C o Spherical polar grid metric terms |
387 |
c CALL MOM_V_METRIC_NH(bi,bj,k,vFld,wVel,mT,myThid) |
388 |
c DO j=jMin,jMax |
389 |
c DO i=iMin,iMax |
390 |
c gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+mTFacV*mT(i,j) |
391 |
c ENDDO |
392 |
c ENDDO |
393 |
c ENDIF |
394 |
|
395 |
C-- Horizontal Coriolis terms |
396 |
IF (useCoriolis .AND. .NOT.useCDscheme) THEN |
397 |
CALL MOM_VI_CORIOLIS(bi,bj,k,uFld,vFld,omega3,hFacZ,r_hFacZ, |
398 |
& uCf,vCf,myThid) |
399 |
DO j=jMin,jMax |
400 |
DO i=iMin,iMax |
401 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+uCf(i,j) |
402 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vCf(i,j) |
403 |
ENDDO |
404 |
ENDDO |
405 |
ENDIF |
406 |
|
407 |
IF (momAdvection) THEN |
408 |
C-- Horizontal advection of relative vorticity |
409 |
c CALL MOM_VI_U_CORIOLIS(bi,bj,K,vFld,omega3,r_hFacZ,uCf,myThid) |
410 |
CALL MOM_VI_U_CORIOLIS(bi,bj,k,vFld,vort3,hFacZ,r_hFacZ, |
411 |
& uCf,myThid) |
412 |
c CALL MOM_VI_U_CORIOLIS_C4(bi,bj,K,vFld,vort3,r_hFacZ,uCf,myThid) |
413 |
DO j=jMin,jMax |
414 |
DO i=iMin,iMax |
415 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+uCf(i,j) |
416 |
ENDDO |
417 |
ENDDO |
418 |
c CALL MOM_VI_V_CORIOLIS(bi,bj,K,uFld,omega3,r_hFacZ,vCf,myThid) |
419 |
CALL MOM_VI_V_CORIOLIS(bi,bj,k,uFld,vort3,hFacZ,r_hFacZ, |
420 |
& vCf,myThid) |
421 |
c CALL MOM_VI_V_CORIOLIS_C4(bi,bj,K,uFld,vort3,r_hFacZ,vCf,myThid) |
422 |
DO j=jMin,jMax |
423 |
DO i=iMin,iMax |
424 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vCf(i,j) |
425 |
ENDDO |
426 |
ENDDO |
427 |
|
428 |
#ifdef ALLOW_TIMEAVE |
429 |
IF (taveFreq.GT.0.) THEN |
430 |
CALL TIMEAVE_CUMUL_1K1T(uZetatave,vCf,deltaTClock, |
431 |
& Nr, k, bi, bj, myThid) |
432 |
CALL TIMEAVE_CUMUL_1K1T(vZetatave,uCf,deltaTClock, |
433 |
& Nr, k, bi, bj, myThid) |
434 |
ENDIF |
435 |
#endif |
436 |
|
437 |
C-- Vertical shear terms (-w*du/dr & -w*dv/dr) |
438 |
IF ( .NOT. momImplVertAdv ) THEN |
439 |
CALL MOM_VI_U_VERTSHEAR(bi,bj,K,uVel,wVel,uCf,myThid) |
440 |
DO j=jMin,jMax |
441 |
DO i=iMin,iMax |
442 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+uCf(i,j) |
443 |
ENDDO |
444 |
ENDDO |
445 |
CALL MOM_VI_V_VERTSHEAR(bi,bj,K,vVel,wVel,vCf,myThid) |
446 |
DO j=jMin,jMax |
447 |
DO i=iMin,iMax |
448 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vCf(i,j) |
449 |
ENDDO |
450 |
ENDDO |
451 |
ENDIF |
452 |
|
453 |
C-- Bernoulli term |
454 |
CALL MOM_VI_U_GRAD_KE(bi,bj,K,KE,uCf,myThid) |
455 |
DO j=jMin,jMax |
456 |
DO i=iMin,iMax |
457 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)+uCf(i,j) |
458 |
ENDDO |
459 |
ENDDO |
460 |
CALL MOM_VI_V_GRAD_KE(bi,bj,K,KE,vCf,myThid) |
461 |
DO j=jMin,jMax |
462 |
DO i=iMin,iMax |
463 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)+vCf(i,j) |
464 |
ENDDO |
465 |
ENDDO |
466 |
C-- end if momAdvection |
467 |
ENDIF |
468 |
|
469 |
C-- Set du/dt & dv/dt on boundaries to zero |
470 |
DO j=jMin,jMax |
471 |
DO i=iMin,iMax |
472 |
gU(i,j,k,bi,bj) = gU(i,j,k,bi,bj)*_maskW(i,j,k,bi,bj) |
473 |
gV(i,j,k,bi,bj) = gV(i,j,k,bi,bj)*_maskS(i,j,k,bi,bj) |
474 |
ENDDO |
475 |
ENDDO |
476 |
|
477 |
|
478 |
IF ( |
479 |
& DIFFERENT_MULTIPLE(diagFreq,myCurrentTime, |
480 |
& myCurrentTime-deltaTClock) |
481 |
& ) THEN |
482 |
CALL WRITE_LOCAL_RL('Ds','I10',1,strain,bi,bj,k,myIter,myThid) |
483 |
CALL WRITE_LOCAL_RL('Dt','I10',1,tension,bi,bj,k,myIter,myThid) |
484 |
CALL WRITE_LOCAL_RL('fV','I10',1,uCf,bi,bj,k,myIter,myThid) |
485 |
CALL WRITE_LOCAL_RL('fU','I10',1,vCf,bi,bj,k,myIter,myThid) |
486 |
CALL WRITE_LOCAL_RL('Du','I10',1,uDiss,bi,bj,k,myIter,myThid) |
487 |
CALL WRITE_LOCAL_RL('Dv','I10',1,vDiss,bi,bj,k,myIter,myThid) |
488 |
CALL WRITE_LOCAL_RL('Z3','I10',1,vort3,bi,bj,k,myIter,myThid) |
489 |
c CALL WRITE_LOCAL_RL('W3','I10',1,omega3,bi,bj,k,myIter,myThid) |
490 |
CALL WRITE_LOCAL_RL('KE','I10',1,KE,bi,bj,k,myIter,myThid) |
491 |
CALL WRITE_LOCAL_RL('D','I10',1,hdiv,bi,bj,k,myIter,myThid) |
492 |
ENDIF |
493 |
|
494 |
#endif /* ALLOW_MOM_VECINV */ |
495 |
|
496 |
RETURN |
497 |
END |