1 |
guez |
3 |
module calfis_m |
2 |
|
|
|
3 |
|
|
! Clean: no C preprocessor directive, no include line |
4 |
|
|
|
5 |
|
|
IMPLICIT NONE |
6 |
|
|
|
7 |
|
|
contains |
8 |
|
|
|
9 |
|
|
SUBROUTINE calfis(nq, lafin, rdayvrai, heure, pucov, pvcov, pteta, pq, & |
10 |
guez |
10 |
pmasse, pps, ppk, pphis, pphi, pducov, pdvcov, pdteta, pdq, pw, & |
11 |
guez |
13 |
pdufi, pdvfi, pdhfi, pdqfi, pdpsfi) |
12 |
guez |
3 |
|
13 |
|
|
! From dyn3d/calfis.F,v 1.3 2005/05/25 13:10:09 |
14 |
|
|
|
15 |
|
|
! Auteurs : P. Le Van, F. Hourdin |
16 |
|
|
|
17 |
|
|
! 1. rearrangement des tableaux et transformation |
18 |
|
|
! variables dynamiques > variables physiques |
19 |
|
|
! 2. calcul des termes physiques |
20 |
|
|
! 3. retransformation des tendances physiques en tendances dynamiques |
21 |
|
|
|
22 |
|
|
! remarques: |
23 |
|
|
! ---------- |
24 |
|
|
|
25 |
|
|
! - les vents sont donnes dans la physique par leurs composantes |
26 |
|
|
! naturelles. |
27 |
|
|
! - la variable thermodynamique de la physique est une variable |
28 |
|
|
! intensive : T |
29 |
|
|
! pour la dynamique on prend T * (preff / p(l)) **kappa |
30 |
|
|
! - les deux seules variables dependant de la geometrie necessaires |
31 |
|
|
! pour la physique sont la latitude pour le rayonnement et |
32 |
|
|
! l'aire de la maille quand on veut integrer une grandeur |
33 |
|
|
! horizontalement. |
34 |
|
|
|
35 |
|
|
! Input : |
36 |
|
|
! ------- |
37 |
|
|
! pucov covariant zonal velocity |
38 |
|
|
! pvcov covariant meridional velocity |
39 |
|
|
! pteta potential temperature |
40 |
|
|
! pps surface pressure |
41 |
|
|
! pmasse masse d'air dans chaque maille |
42 |
|
|
! pts surface temperature (K) |
43 |
|
|
! callrad clef d'appel au rayonnement |
44 |
|
|
|
45 |
|
|
! Output : |
46 |
|
|
! -------- |
47 |
|
|
! pdufi tendency for the natural zonal velocity (ms-1) |
48 |
|
|
! pdvfi tendency for the natural meridional velocity |
49 |
|
|
! pdhfi tendency for the potential temperature |
50 |
|
|
! pdtsfi tendency for the surface temperature |
51 |
|
|
|
52 |
|
|
! pdtrad radiative tendencies \ both input |
53 |
|
|
! pfluxrad radiative fluxes / and output |
54 |
|
|
|
55 |
|
|
use dimens_m, only: iim, jjm, llm, nqmx |
56 |
|
|
use dimphy, only: klon |
57 |
|
|
use comconst, only: kappa, cpp, dtphys, g, pi |
58 |
|
|
use comvert, only: preff, presnivs |
59 |
|
|
use comgeom, only: apoln, cu_2d, cv_2d, unsaire_2d, apols, rlonu, rlonv |
60 |
guez |
18 |
use iniadvtrac_m, only: niadv |
61 |
guez |
3 |
use grid_change, only: dyn_phy, gr_fi_dyn |
62 |
|
|
use physiq_m, only: physiq |
63 |
guez |
10 |
use pressure_var, only: p3d, pls |
64 |
guez |
3 |
|
65 |
|
|
! 0. Declarations : |
66 |
|
|
|
67 |
guez |
18 |
INTEGER, intent(in):: nq |
68 |
guez |
3 |
|
69 |
|
|
! Arguments : |
70 |
|
|
|
71 |
|
|
LOGICAL, intent(in):: lafin |
72 |
|
|
REAL, intent(in):: heure ! heure de la journée en fraction de jour |
73 |
|
|
|
74 |
|
|
REAL pvcov(iim + 1,jjm,llm) |
75 |
|
|
REAL pucov(iim + 1,jjm + 1,llm) |
76 |
|
|
REAL pteta(iim + 1,jjm + 1,llm) |
77 |
|
|
REAL pmasse(iim + 1,jjm + 1,llm) |
78 |
|
|
|
79 |
|
|
REAL, intent(in):: pq(iim + 1,jjm + 1,llm,nqmx) |
80 |
|
|
! (mass fractions of advected fields) |
81 |
|
|
|
82 |
|
|
REAL pphis(iim + 1,jjm + 1) |
83 |
|
|
REAL pphi(iim + 1,jjm + 1,llm) |
84 |
|
|
|
85 |
|
|
REAL pdvcov(iim + 1,jjm,llm) |
86 |
|
|
REAL pducov(iim + 1,jjm + 1,llm) |
87 |
|
|
REAL pdteta(iim + 1,jjm + 1,llm) |
88 |
|
|
REAL pdq(iim + 1,jjm + 1,llm,nqmx) |
89 |
|
|
|
90 |
|
|
REAL pw(iim + 1,jjm + 1,llm) |
91 |
|
|
|
92 |
|
|
REAL pps(iim + 1,jjm + 1) |
93 |
guez |
10 |
REAL, intent(in):: ppk(iim + 1,jjm + 1,llm) |
94 |
guez |
3 |
|
95 |
|
|
REAL pdvfi(iim + 1,jjm,llm) |
96 |
|
|
REAL pdufi(iim + 1,jjm + 1,llm) |
97 |
|
|
REAL pdhfi(iim + 1,jjm + 1,llm) |
98 |
|
|
REAL pdqfi(iim + 1,jjm + 1,llm,nqmx) |
99 |
|
|
REAL pdpsfi(iim + 1,jjm + 1) |
100 |
|
|
|
101 |
|
|
INTEGER, PARAMETER:: longcles = 20 |
102 |
|
|
|
103 |
|
|
! Local variables : |
104 |
|
|
|
105 |
|
|
INTEGER i,j,l,ig0,ig,iq,iiq |
106 |
|
|
REAL zpsrf(klon) |
107 |
|
|
REAL zplev(klon,llm+1),zplay(klon,llm) |
108 |
|
|
REAL zphi(klon,llm),zphis(klon) |
109 |
|
|
|
110 |
|
|
REAL zufi(klon,llm), zvfi(klon,llm) |
111 |
|
|
REAL ztfi(klon,llm) ! temperature |
112 |
|
|
real zqfi(klon,llm,nqmx) ! mass fractions of advected fields |
113 |
|
|
|
114 |
|
|
REAL pcvgu(klon,llm), pcvgv(klon,llm) |
115 |
|
|
REAL pcvgt(klon,llm), pcvgq(klon,llm,2) |
116 |
|
|
|
117 |
|
|
REAL pvervel(klon,llm) |
118 |
|
|
|
119 |
|
|
REAL zdufi(klon,llm),zdvfi(klon,llm) |
120 |
|
|
REAL zdtfi(klon,llm),zdqfi(klon,llm,nqmx) |
121 |
|
|
REAL zdpsrf(klon) |
122 |
|
|
|
123 |
|
|
REAL zsin(iim),zcos(iim),z1(iim) |
124 |
|
|
REAL zsinbis(iim),zcosbis(iim),z1bis(iim) |
125 |
guez |
10 |
REAL pksurcp(iim + 1,jjm + 1) |
126 |
guez |
3 |
|
127 |
|
|
! I. Musat: diagnostic PVteta, Amip2 |
128 |
|
|
INTEGER, PARAMETER:: ntetaSTD=3 |
129 |
|
|
REAL:: rtetaSTD(ntetaSTD) = (/350., 380., 405./) |
130 |
|
|
REAL PVteta(klon,ntetaSTD) |
131 |
|
|
|
132 |
|
|
REAL SSUM |
133 |
|
|
|
134 |
|
|
LOGICAL:: firstcal = .true. |
135 |
guez |
7 |
REAL, intent(in):: rdayvrai |
136 |
guez |
3 |
|
137 |
|
|
!----------------------------------------------------------------------- |
138 |
|
|
|
139 |
|
|
!!print *, "Call sequence information: calfis" |
140 |
|
|
|
141 |
|
|
! 1. Initialisations : |
142 |
|
|
! latitude, longitude et aires des mailles pour la physique: |
143 |
|
|
|
144 |
|
|
! 40. transformation des variables dynamiques en variables physiques: |
145 |
|
|
! 41. pressions au sol (en Pascals) |
146 |
|
|
|
147 |
|
|
zpsrf(1) = pps(1,1) |
148 |
|
|
|
149 |
|
|
ig0 = 2 |
150 |
|
|
DO j = 2,jjm |
151 |
|
|
CALL SCOPY(iim,pps(1,j),1,zpsrf(ig0), 1) |
152 |
|
|
ig0 = ig0+iim |
153 |
|
|
ENDDO |
154 |
|
|
|
155 |
|
|
zpsrf(klon) = pps(1,jjm + 1) |
156 |
|
|
|
157 |
|
|
! 42. pression intercouches : |
158 |
|
|
|
159 |
|
|
! .... zplev definis aux (llm +1) interfaces des couches .... |
160 |
|
|
! .... zplay definis aux (llm) milieux des couches .... |
161 |
|
|
|
162 |
|
|
! ... Exner = cp * (p(l) / preff) ** kappa .... |
163 |
|
|
|
164 |
guez |
10 |
forall (l = 1: llm+1) zplev(:, l) = pack(p3d(:, :, l), dyn_phy) |
165 |
guez |
3 |
|
166 |
|
|
! 43. temperature naturelle (en K) et pressions milieux couches . |
167 |
|
|
DO l=1,llm |
168 |
guez |
10 |
pksurcp = ppk(:, :, l) / cpp |
169 |
|
|
pls(:, :, l) = preff * pksurcp**(1./ kappa) |
170 |
|
|
zplay(:, l) = pack(pls(:, :, l), dyn_phy) |
171 |
|
|
ztfi(:, l) = pack(pteta(:, :, l) * pksurcp, dyn_phy) |
172 |
|
|
pcvgt(:, l) = pack(pdteta(:, :, l) * pksurcp / pmasse(:, :, l), dyn_phy) |
173 |
guez |
3 |
ENDDO |
174 |
|
|
|
175 |
|
|
! 43.bis traceurs |
176 |
|
|
|
177 |
|
|
DO iq=1,nq |
178 |
|
|
iiq=niadv(iq) |
179 |
|
|
DO l=1,llm |
180 |
|
|
zqfi(1,l,iq) = pq(1,1,l,iiq) |
181 |
|
|
ig0 = 2 |
182 |
|
|
DO j=2,jjm |
183 |
|
|
DO i = 1, iim |
184 |
|
|
zqfi(ig0,l,iq) = pq(i,j,l,iiq) |
185 |
|
|
ig0 = ig0 + 1 |
186 |
|
|
ENDDO |
187 |
|
|
ENDDO |
188 |
|
|
zqfi(ig0,l,iq) = pq(1,jjm + 1,l,iiq) |
189 |
|
|
ENDDO |
190 |
|
|
ENDDO |
191 |
|
|
|
192 |
|
|
! convergence dynamique pour les traceurs "EAU" |
193 |
|
|
|
194 |
|
|
DO iq=1,2 |
195 |
|
|
DO l=1,llm |
196 |
|
|
pcvgq(1,l,iq)= pdq(1,1,l,iq) / pmasse(1,1,l) |
197 |
|
|
ig0 = 2 |
198 |
|
|
DO j=2,jjm |
199 |
|
|
DO i = 1, iim |
200 |
|
|
pcvgq(ig0,l,iq) = pdq(i,j,l,iq) / pmasse(i,j,l) |
201 |
|
|
ig0 = ig0 + 1 |
202 |
|
|
ENDDO |
203 |
|
|
ENDDO |
204 |
|
|
pcvgq(ig0,l,iq)= pdq(1,jjm + 1,l,iq) / pmasse(1,jjm + 1,l) |
205 |
|
|
ENDDO |
206 |
|
|
ENDDO |
207 |
|
|
|
208 |
|
|
! Geopotentiel calcule par rapport a la surface locale: |
209 |
|
|
|
210 |
|
|
forall (l = 1:llm) zphi(:, l) = pack(pphi(:, :, l), dyn_phy) |
211 |
|
|
zphis = pack(pphis, dyn_phy) |
212 |
|
|
DO l=1,llm |
213 |
|
|
DO ig=1,klon |
214 |
|
|
zphi(ig,l)=zphi(ig,l)-zphis(ig) |
215 |
|
|
ENDDO |
216 |
|
|
ENDDO |
217 |
|
|
|
218 |
|
|
! .... Calcul de la vitesse verticale (en Pa*m*s ou Kg/s) .... |
219 |
|
|
|
220 |
|
|
DO l=1,llm |
221 |
|
|
pvervel(1,l)=pw(1,1,l) * g /apoln |
222 |
|
|
ig0=2 |
223 |
|
|
DO j=2,jjm |
224 |
|
|
DO i = 1, iim |
225 |
|
|
pvervel(ig0,l) = pw(i,j,l) * g * unsaire_2d(i,j) |
226 |
|
|
ig0 = ig0 + 1 |
227 |
|
|
ENDDO |
228 |
|
|
ENDDO |
229 |
|
|
pvervel(ig0,l)=pw(1,jjm + 1,l) * g /apols |
230 |
|
|
ENDDO |
231 |
|
|
|
232 |
|
|
! 45. champ u: |
233 |
|
|
|
234 |
|
|
DO l=1,llm |
235 |
|
|
|
236 |
|
|
DO j=2,jjm |
237 |
|
|
ig0 = 1+(j-2)*iim |
238 |
|
|
zufi(ig0+1,l)= 0.5 * & |
239 |
|
|
(pucov(iim,j,l)/cu_2d(iim,j) + pucov(1,j,l)/cu_2d(1,j)) |
240 |
|
|
pcvgu(ig0+1,l)= 0.5 * & |
241 |
|
|
(pducov(iim,j,l)/cu_2d(iim,j) + pducov(1,j,l)/cu_2d(1,j)) |
242 |
|
|
DO i=2,iim |
243 |
|
|
zufi(ig0+i,l)= 0.5 * & |
244 |
|
|
(pucov(i-1,j,l)/cu_2d(i-1,j) & |
245 |
|
|
+ pucov(i,j,l)/cu_2d(i,j)) |
246 |
|
|
pcvgu(ig0+i,l)= 0.5 * & |
247 |
|
|
(pducov(i-1,j,l)/cu_2d(i-1,j) & |
248 |
|
|
+ pducov(i,j,l)/cu_2d(i,j)) |
249 |
|
|
end DO |
250 |
|
|
end DO |
251 |
|
|
|
252 |
|
|
end DO |
253 |
|
|
|
254 |
|
|
! 46.champ v: |
255 |
|
|
|
256 |
|
|
DO l=1,llm |
257 |
|
|
DO j=2,jjm |
258 |
|
|
ig0=1+(j-2)*iim |
259 |
|
|
DO i=1,iim |
260 |
|
|
zvfi(ig0+i,l)= 0.5 * & |
261 |
|
|
(pvcov(i,j-1,l)/cv_2d(i,j-1) & |
262 |
|
|
+ pvcov(i,j,l)/cv_2d(i,j)) |
263 |
|
|
pcvgv(ig0+i,l)= 0.5 * & |
264 |
|
|
(pdvcov(i,j-1,l)/cv_2d(i,j-1) & |
265 |
|
|
+ pdvcov(i,j,l)/cv_2d(i,j)) |
266 |
|
|
ENDDO |
267 |
|
|
ENDDO |
268 |
|
|
ENDDO |
269 |
|
|
|
270 |
|
|
! 47. champs de vents aux pole nord |
271 |
|
|
! U = 1 / pi * integrale [ v * cos(long) * d long ] |
272 |
|
|
! V = 1 / pi * integrale [ v * sin(long) * d long ] |
273 |
|
|
|
274 |
|
|
DO l=1,llm |
275 |
|
|
|
276 |
|
|
z1(1) =(rlonu(1)-rlonu(iim)+2.*pi)*pvcov(1,1,l)/cv_2d(1,1) |
277 |
|
|
z1bis(1)=(rlonu(1)-rlonu(iim)+2.*pi)*pdvcov(1,1,l)/cv_2d(1,1) |
278 |
|
|
DO i=2,iim |
279 |
|
|
z1(i) =(rlonu(i)-rlonu(i-1))*pvcov(i,1,l)/cv_2d(i,1) |
280 |
|
|
z1bis(i)=(rlonu(i)-rlonu(i-1))*pdvcov(i,1,l)/cv_2d(i,1) |
281 |
|
|
ENDDO |
282 |
|
|
|
283 |
|
|
DO i=1,iim |
284 |
|
|
zcos(i) = COS(rlonv(i))*z1(i) |
285 |
|
|
zcosbis(i)= COS(rlonv(i))*z1bis(i) |
286 |
|
|
zsin(i) = SIN(rlonv(i))*z1(i) |
287 |
|
|
zsinbis(i)= SIN(rlonv(i))*z1bis(i) |
288 |
|
|
ENDDO |
289 |
|
|
|
290 |
|
|
zufi(1,l) = SSUM(iim,zcos,1)/pi |
291 |
|
|
pcvgu(1,l) = SSUM(iim,zcosbis,1)/pi |
292 |
|
|
zvfi(1,l) = SSUM(iim,zsin,1)/pi |
293 |
|
|
pcvgv(1,l) = SSUM(iim,zsinbis,1)/pi |
294 |
|
|
|
295 |
|
|
ENDDO |
296 |
|
|
|
297 |
|
|
! 48. champs de vents aux pole sud: |
298 |
|
|
! U = 1 / pi * integrale [ v * cos(long) * d long ] |
299 |
|
|
! V = 1 / pi * integrale [ v * sin(long) * d long ] |
300 |
|
|
|
301 |
|
|
DO l=1,llm |
302 |
|
|
|
303 |
|
|
z1(1) =(rlonu(1)-rlonu(iim)+2.*pi)*pvcov(1,jjm,l) & |
304 |
|
|
/cv_2d(1,jjm) |
305 |
|
|
z1bis(1)=(rlonu(1)-rlonu(iim)+2.*pi)*pdvcov(1,jjm,l) & |
306 |
|
|
/cv_2d(1,jjm) |
307 |
|
|
DO i=2,iim |
308 |
|
|
z1(i) =(rlonu(i)-rlonu(i-1))*pvcov(i,jjm,l)/cv_2d(i,jjm) |
309 |
|
|
z1bis(i)=(rlonu(i)-rlonu(i-1))*pdvcov(i,jjm,l)/cv_2d(i,jjm) |
310 |
|
|
ENDDO |
311 |
|
|
|
312 |
|
|
DO i=1,iim |
313 |
|
|
zcos(i) = COS(rlonv(i))*z1(i) |
314 |
|
|
zcosbis(i) = COS(rlonv(i))*z1bis(i) |
315 |
|
|
zsin(i) = SIN(rlonv(i))*z1(i) |
316 |
|
|
zsinbis(i) = SIN(rlonv(i))*z1bis(i) |
317 |
|
|
ENDDO |
318 |
|
|
|
319 |
|
|
zufi(klon,l) = SSUM(iim,zcos,1)/pi |
320 |
|
|
pcvgu(klon,l) = SSUM(iim,zcosbis,1)/pi |
321 |
|
|
zvfi(klon,l) = SSUM(iim,zsin,1)/pi |
322 |
|
|
pcvgv(klon,l) = SSUM(iim,zsinbis,1)/pi |
323 |
|
|
|
324 |
|
|
ENDDO |
325 |
|
|
|
326 |
|
|
!IM calcul PV a teta=350, 380, 405K |
327 |
|
|
CALL PVtheta(klon,llm,pucov,pvcov,pteta, & |
328 |
|
|
ztfi,zplay,zplev, & |
329 |
|
|
ntetaSTD,rtetaSTD,PVteta) |
330 |
|
|
|
331 |
|
|
! Appel de la physique: |
332 |
|
|
|
333 |
|
|
CALL physiq(nq, firstcal, lafin, rdayvrai, heure, dtphys, & |
334 |
guez |
13 |
zplev, zplay, zphi, zphis, presnivs, zufi, zvfi, & |
335 |
guez |
3 |
ztfi, zqfi, pvervel, zdufi, zdvfi, zdtfi, zdqfi, zdpsrf, pducov, & |
336 |
|
|
PVteta) ! IM diagnostique PVteta, Amip2 |
337 |
|
|
|
338 |
|
|
! transformation des tendances physiques en tendances dynamiques: |
339 |
|
|
|
340 |
|
|
! tendance sur la pression : |
341 |
|
|
|
342 |
|
|
pdpsfi = gr_fi_dyn(zdpsrf) |
343 |
|
|
|
344 |
|
|
! 62. enthalpie potentielle |
345 |
|
|
|
346 |
|
|
DO l=1,llm |
347 |
|
|
|
348 |
|
|
DO i=1,iim + 1 |
349 |
|
|
pdhfi(i,1,l) = cpp * zdtfi(1,l) / ppk(i, 1 ,l) |
350 |
|
|
pdhfi(i,jjm + 1,l) = cpp * zdtfi(klon,l)/ ppk(i,jjm + 1,l) |
351 |
|
|
ENDDO |
352 |
|
|
|
353 |
|
|
DO j=2,jjm |
354 |
|
|
ig0=1+(j-2)*iim |
355 |
|
|
DO i=1,iim |
356 |
|
|
pdhfi(i,j,l) = cpp * zdtfi(ig0+i,l) / ppk(i,j,l) |
357 |
|
|
ENDDO |
358 |
|
|
pdhfi(iim + 1,j,l) = pdhfi(1,j,l) |
359 |
|
|
ENDDO |
360 |
|
|
|
361 |
|
|
ENDDO |
362 |
|
|
|
363 |
|
|
! 62. humidite specifique |
364 |
|
|
|
365 |
|
|
DO iq=1,nqmx |
366 |
|
|
DO l=1,llm |
367 |
|
|
DO i=1,iim + 1 |
368 |
|
|
pdqfi(i,1,l,iq) = zdqfi(1,l,iq) |
369 |
|
|
pdqfi(i,jjm + 1,l,iq) = zdqfi(klon,l,iq) |
370 |
|
|
ENDDO |
371 |
|
|
DO j=2,jjm |
372 |
|
|
ig0=1+(j-2)*iim |
373 |
|
|
DO i=1,iim |
374 |
|
|
pdqfi(i,j,l,iq) = zdqfi(ig0+i,l,iq) |
375 |
|
|
ENDDO |
376 |
|
|
pdqfi(iim + 1,j,l,iq) = pdqfi(1,j,l,iq) |
377 |
|
|
ENDDO |
378 |
|
|
ENDDO |
379 |
|
|
ENDDO |
380 |
|
|
|
381 |
|
|
! 63. traceurs |
382 |
|
|
|
383 |
|
|
! initialisation des tendances |
384 |
|
|
pdqfi=0. |
385 |
|
|
|
386 |
|
|
DO iq=1,nq |
387 |
|
|
iiq=niadv(iq) |
388 |
|
|
DO l=1,llm |
389 |
|
|
DO i=1,iim + 1 |
390 |
|
|
pdqfi(i,1,l,iiq) = zdqfi(1,l,iq) |
391 |
|
|
pdqfi(i,jjm + 1,l,iiq) = zdqfi(klon,l,iq) |
392 |
|
|
ENDDO |
393 |
|
|
DO j=2,jjm |
394 |
|
|
ig0=1+(j-2)*iim |
395 |
|
|
DO i=1,iim |
396 |
|
|
pdqfi(i,j,l,iiq) = zdqfi(ig0+i,l,iq) |
397 |
|
|
ENDDO |
398 |
|
|
pdqfi(iim + 1,j,l,iiq) = pdqfi(1,j,l,iq) |
399 |
|
|
ENDDO |
400 |
|
|
ENDDO |
401 |
|
|
ENDDO |
402 |
|
|
|
403 |
|
|
! 65. champ u: |
404 |
|
|
|
405 |
|
|
DO l=1,llm |
406 |
|
|
|
407 |
|
|
DO i=1,iim + 1 |
408 |
|
|
pdufi(i,1,l) = 0. |
409 |
|
|
pdufi(i,jjm + 1,l) = 0. |
410 |
|
|
ENDDO |
411 |
|
|
|
412 |
|
|
DO j=2,jjm |
413 |
|
|
ig0=1+(j-2)*iim |
414 |
|
|
DO i=1,iim-1 |
415 |
|
|
pdufi(i,j,l)= & |
416 |
|
|
0.5*(zdufi(ig0+i,l)+zdufi(ig0+i+1,l))*cu_2d(i,j) |
417 |
|
|
ENDDO |
418 |
|
|
pdufi(iim,j,l)= & |
419 |
|
|
0.5*(zdufi(ig0+1,l)+zdufi(ig0+iim,l))*cu_2d(iim,j) |
420 |
|
|
pdufi(iim + 1,j,l)=pdufi(1,j,l) |
421 |
|
|
ENDDO |
422 |
|
|
|
423 |
|
|
ENDDO |
424 |
|
|
|
425 |
|
|
! 67. champ v: |
426 |
|
|
|
427 |
|
|
DO l=1,llm |
428 |
|
|
|
429 |
|
|
DO j=2,jjm-1 |
430 |
|
|
ig0=1+(j-2)*iim |
431 |
|
|
DO i=1,iim |
432 |
|
|
pdvfi(i,j,l)= & |
433 |
|
|
0.5*(zdvfi(ig0+i,l)+zdvfi(ig0+i+iim,l))*cv_2d(i,j) |
434 |
|
|
ENDDO |
435 |
|
|
pdvfi(iim + 1,j,l) = pdvfi(1,j,l) |
436 |
|
|
ENDDO |
437 |
|
|
ENDDO |
438 |
|
|
|
439 |
|
|
! 68. champ v pres des poles: |
440 |
|
|
! v = U * cos(long) + V * SIN(long) |
441 |
|
|
|
442 |
|
|
DO l=1,llm |
443 |
|
|
|
444 |
|
|
DO i=1,iim |
445 |
|
|
pdvfi(i,1,l)= & |
446 |
|
|
zdufi(1,l)*COS(rlonv(i))+zdvfi(1,l)*SIN(rlonv(i)) |
447 |
|
|
pdvfi(i,jjm,l)=zdufi(klon,l)*COS(rlonv(i)) & |
448 |
|
|
+zdvfi(klon,l)*SIN(rlonv(i)) |
449 |
|
|
pdvfi(i,1,l)= & |
450 |
|
|
0.5*(pdvfi(i,1,l)+zdvfi(i+1,l))*cv_2d(i,1) |
451 |
|
|
pdvfi(i,jjm,l)= & |
452 |
|
|
0.5*(pdvfi(i,jjm,l)+zdvfi(klon-iim-1+i,l))*cv_2d(i,jjm) |
453 |
|
|
ENDDO |
454 |
|
|
|
455 |
|
|
pdvfi(iim + 1,1,l) = pdvfi(1,1,l) |
456 |
|
|
pdvfi(iim + 1,jjm,l)= pdvfi(1,jjm,l) |
457 |
|
|
|
458 |
|
|
ENDDO |
459 |
|
|
|
460 |
|
|
firstcal = .FALSE. |
461 |
|
|
|
462 |
|
|
END SUBROUTINE calfis |
463 |
|
|
|
464 |
|
|
end module calfis_m |