1 | SUBROUTINE vdifc(ngrid,nlay,nq,co2ice,ppopsk, |
---|
2 | $ ptimestep,pcapcal,lecrit, |
---|
3 | $ pplay,pplev,pzlay,pzlev,pz0, |
---|
4 | $ pu,pv,ph,pq,ptsrf,pemis,pqsurf, |
---|
5 | $ pdufi,pdvfi,pdhfi,pdqfi,pfluxsrf, |
---|
6 | $ pdudif,pdvdif,pdhdif,pdtsrf,pq2, |
---|
7 | $ pdqdif,pdqsdif,wmax,zcdv_true,zcdh_true) |
---|
8 | IMPLICIT NONE |
---|
9 | |
---|
10 | c======================================================================= |
---|
11 | c |
---|
12 | c subject: |
---|
13 | c -------- |
---|
14 | c Turbulent diffusion (mixing) for potential T, U, V and tracer |
---|
15 | c |
---|
16 | c Shema implicite |
---|
17 | c On commence par rajouter au variables x la tendance physique |
---|
18 | c et on resoult en fait: |
---|
19 | c x(t+1) = x(t) + dt * (dx/dt)phys(t) + dt * (dx/dt)difv(t+1) |
---|
20 | c |
---|
21 | c author: |
---|
22 | c ------ |
---|
23 | c Hourdin/Forget/Fournier |
---|
24 | c======================================================================= |
---|
25 | |
---|
26 | c----------------------------------------------------------------------- |
---|
27 | c declarations: |
---|
28 | c ------------- |
---|
29 | |
---|
30 | #include "dimensions.h" |
---|
31 | #include "dimphys.h" |
---|
32 | #include "comcstfi.h" |
---|
33 | #include "callkeys.h" |
---|
34 | #include "surfdat.h" |
---|
35 | #include "comgeomfi.h" |
---|
36 | #include "tracer.h" |
---|
37 | |
---|
38 | c |
---|
39 | c arguments: |
---|
40 | c ---------- |
---|
41 | |
---|
42 | INTEGER ngrid,nlay |
---|
43 | REAL ptimestep |
---|
44 | REAL pplay(ngrid,nlay),pplev(ngrid,nlay+1) |
---|
45 | REAL pzlay(ngrid,nlay),pzlev(ngrid,nlay+1) |
---|
46 | REAL pu(ngrid,nlay),pv(ngrid,nlay),ph(ngrid,nlay) |
---|
47 | REAL ptsrf(ngrid),pemis(ngrid) |
---|
48 | REAL pdufi(ngrid,nlay),pdvfi(ngrid,nlay),pdhfi(ngrid,nlay) |
---|
49 | REAL pfluxsrf(ngrid) |
---|
50 | REAL pdudif(ngrid,nlay),pdvdif(ngrid,nlay),pdhdif(ngrid,nlay) |
---|
51 | REAL pdtsrf(ngrid),pcapcal(ngrid) |
---|
52 | REAL pq2(ngrid,nlay+1) |
---|
53 | |
---|
54 | c Argument added for condensation: |
---|
55 | REAL co2ice (ngrid), ppopsk(ngrid,nlay) |
---|
56 | logical lecrit |
---|
57 | |
---|
58 | REAL pz0(ngridmx) ! surface roughness length (m) |
---|
59 | |
---|
60 | c Argument added to account for subgrid gustiness : |
---|
61 | |
---|
62 | REAL wmax(ngridmx) |
---|
63 | |
---|
64 | c Traceurs : |
---|
65 | integer nq |
---|
66 | REAL pqsurf(ngrid,nq) |
---|
67 | real pq(ngrid,nlay,nq), pdqfi(ngrid,nlay,nq) |
---|
68 | real pdqdif(ngrid,nlay,nq) |
---|
69 | real pdqsdif(ngrid,nq) |
---|
70 | |
---|
71 | c local: |
---|
72 | c ------ |
---|
73 | |
---|
74 | INTEGER ilev,ig,ilay,nlev |
---|
75 | |
---|
76 | REAL z4st,zdplanck(ngridmx) |
---|
77 | REAL zkv(ngridmx,nlayermx+1),zkh(ngridmx,nlayermx+1) |
---|
78 | REAL zcdv(ngridmx),zcdh(ngridmx) |
---|
79 | REAL zcdv_true(ngridmx),zcdh_true(ngridmx) ! drag coeff are used by the LES to recompute u* and hfx |
---|
80 | REAL zu(ngridmx,nlayermx),zv(ngridmx,nlayermx) |
---|
81 | REAL zh(ngridmx,nlayermx) |
---|
82 | REAL ztsrf2(ngridmx) |
---|
83 | REAL z1(ngridmx),z2(ngridmx) |
---|
84 | REAL za(ngridmx,nlayermx),zb(ngridmx,nlayermx) |
---|
85 | REAL zb0(ngridmx,nlayermx) |
---|
86 | REAL zc(ngridmx,nlayermx),zd(ngridmx,nlayermx) |
---|
87 | REAL zcst1 |
---|
88 | REAL zu2(ngridmx) |
---|
89 | |
---|
90 | EXTERNAL SSUM,SCOPY |
---|
91 | REAL SSUM |
---|
92 | LOGICAL firstcall |
---|
93 | SAVE firstcall |
---|
94 | |
---|
95 | c variable added for CO2 condensation: |
---|
96 | c ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ |
---|
97 | REAL hh , zhcond(ngridmx,nlayermx) |
---|
98 | REAL latcond,tcond1mb |
---|
99 | REAL acond,bcond |
---|
100 | SAVE acond,bcond |
---|
101 | DATA latcond,tcond1mb/5.9e5,136.27/ |
---|
102 | |
---|
103 | c Tracers : |
---|
104 | c ~~~~~~~ |
---|
105 | INTEGER iq |
---|
106 | REAL zq(ngridmx,nlayermx,nqmx) |
---|
107 | REAL zq1temp(ngridmx) |
---|
108 | REAL rho(ngridmx) ! near surface air density |
---|
109 | REAL qsat(ngridmx) |
---|
110 | DATA firstcall/.true./ |
---|
111 | |
---|
112 | REAL kmixmin |
---|
113 | |
---|
114 | c ** un petit test de coherence |
---|
115 | c -------------------------- |
---|
116 | |
---|
117 | IF (firstcall) THEN |
---|
118 | IF(ngrid.NE.ngridmx) THEN |
---|
119 | PRINT*,'STOP dans vdifc' |
---|
120 | PRINT*,'probleme de dimensions :' |
---|
121 | PRINT*,'ngrid =',ngrid |
---|
122 | PRINT*,'ngridmx =',ngridmx |
---|
123 | STOP |
---|
124 | ENDIF |
---|
125 | c To compute: Tcond= 1./(bcond-acond*log(.0095*p)) (p in pascal) |
---|
126 | bcond=1./tcond1mb |
---|
127 | acond=r/latcond |
---|
128 | PRINT*,'In vdifc: Tcond(P=1mb)=',tcond1mb,' Lcond=',latcond |
---|
129 | PRINT*,' acond,bcond',acond,bcond |
---|
130 | |
---|
131 | firstcall=.false. |
---|
132 | ENDIF |
---|
133 | |
---|
134 | |
---|
135 | |
---|
136 | |
---|
137 | |
---|
138 | c----------------------------------------------------------------------- |
---|
139 | c 1. initialisation |
---|
140 | c ----------------- |
---|
141 | |
---|
142 | nlev=nlay+1 |
---|
143 | |
---|
144 | c ** calcul de rho*dz et dt*rho/dz=dt*rho**2 g/dp |
---|
145 | c avec rho=p/RT=p/ (R Theta) (p/ps)**kappa |
---|
146 | c ---------------------------------------- |
---|
147 | |
---|
148 | DO ilay=1,nlay |
---|
149 | DO ig=1,ngrid |
---|
150 | za(ig,ilay)=(pplev(ig,ilay)-pplev(ig,ilay+1))/g |
---|
151 | ENDDO |
---|
152 | ENDDO |
---|
153 | |
---|
154 | zcst1=4.*g*ptimestep/(r*r) |
---|
155 | DO ilev=2,nlev-1 |
---|
156 | DO ig=1,ngrid |
---|
157 | zb0(ig,ilev)=pplev(ig,ilev)* |
---|
158 | s (pplev(ig,1)/pplev(ig,ilev))**rcp / |
---|
159 | s (ph(ig,ilev-1)+ph(ig,ilev)) |
---|
160 | zb0(ig,ilev)=zcst1*zb0(ig,ilev)*zb0(ig,ilev)/ |
---|
161 | s (pplay(ig,ilev-1)-pplay(ig,ilev)) |
---|
162 | ENDDO |
---|
163 | ENDDO |
---|
164 | DO ig=1,ngrid |
---|
165 | zb0(ig,1)=ptimestep*pplev(ig,1)/(r*ptsrf(ig)) |
---|
166 | ENDDO |
---|
167 | |
---|
168 | c ** diagnostique pour l'initialisation |
---|
169 | c ---------------------------------- |
---|
170 | |
---|
171 | IF(lecrit) THEN |
---|
172 | ig=ngrid/2+1 |
---|
173 | PRINT*,'Pression (mbar) ,altitude (km),u,v,theta, rho dz' |
---|
174 | DO ilay=1,nlay |
---|
175 | WRITE(*,'(6f11.5)') |
---|
176 | s .01*pplay(ig,ilay),.001*pzlay(ig,ilay), |
---|
177 | s pu(ig,ilay),pv(ig,ilay),ph(ig,ilay),za(ig,ilay) |
---|
178 | ENDDO |
---|
179 | PRINT*,'Pression (mbar) ,altitude (km),zb' |
---|
180 | DO ilev=1,nlay |
---|
181 | WRITE(*,'(3f15.7)') |
---|
182 | s .01*pplev(ig,ilev),.001*pzlev(ig,ilev), |
---|
183 | s zb0(ig,ilev) |
---|
184 | ENDDO |
---|
185 | ENDIF |
---|
186 | |
---|
187 | c Potential Condensation temperature: |
---|
188 | c ----------------------------------- |
---|
189 | |
---|
190 | c if (callcond) then |
---|
191 | c DO ilev=1,nlay |
---|
192 | c DO ig=1,ngrid |
---|
193 | c zhcond(ig,ilev) = |
---|
194 | c & (1./(bcond-acond*log(.0095*pplay(ig,ilev))))/ppopsk(ig,ilev) |
---|
195 | c END DO |
---|
196 | c END DO |
---|
197 | c else |
---|
198 | call zerophys(ngrid*nlay,zhcond) |
---|
199 | c end if |
---|
200 | |
---|
201 | |
---|
202 | c----------------------------------------------------------------------- |
---|
203 | c 2. ajout des tendances physiques |
---|
204 | c ----------------------------- |
---|
205 | |
---|
206 | DO ilev=1,nlay |
---|
207 | DO ig=1,ngrid |
---|
208 | zu(ig,ilev)=pu(ig,ilev)+pdufi(ig,ilev)*ptimestep |
---|
209 | zv(ig,ilev)=pv(ig,ilev)+pdvfi(ig,ilev)*ptimestep |
---|
210 | zh(ig,ilev)=ph(ig,ilev)+pdhfi(ig,ilev)*ptimestep |
---|
211 | zh(ig,ilev)=max(zh(ig,ilev),zhcond(ig,ilev)) |
---|
212 | ENDDO |
---|
213 | ENDDO |
---|
214 | if(tracer) then |
---|
215 | DO iq =1, nq |
---|
216 | DO ilev=1,nlay |
---|
217 | DO ig=1,ngrid |
---|
218 | zq(ig,ilev,iq)=pq(ig,ilev,iq)+pdqfi(ig,ilev,iq)*ptimestep |
---|
219 | ENDDO |
---|
220 | ENDDO |
---|
221 | ENDDO |
---|
222 | end if |
---|
223 | |
---|
224 | c----------------------------------------------------------------------- |
---|
225 | c 3. schema de turbulence |
---|
226 | c -------------------- |
---|
227 | |
---|
228 | c ** source d'energie cinetique turbulente a la surface |
---|
229 | c (condition aux limites du schema de diffusion turbulente |
---|
230 | c dans la couche limite |
---|
231 | c --------------------- |
---|
232 | |
---|
233 | CALL vdif_cd(ngrid,nlay,pz0,g,pzlay,pu,pv,wmax,ptsrf,ph |
---|
234 | & ,zcdv_true,zcdh_true) |
---|
235 | |
---|
236 | |
---|
237 | IF (callrichsl .eq. .true.) then |
---|
238 | zu2(:)=pu(:,1)*pu(:,1)+pv(:,1)*pv(:,1) |
---|
239 | & +(1.*wmax(:))**2 ! subgrid gustiness added by quadratic interpolation with a coeff beta, here beta=1. (tuned from |
---|
240 | ! LES comparisons. This parameter is linked to the thermals settings) |
---|
241 | ELSE |
---|
242 | zu2(:)=pu(:,1)*pu(:,1)+pv(:,1)*pv(:,1) |
---|
243 | ENDIF |
---|
244 | |
---|
245 | zcdv(:)=zcdv_true(:)*sqrt(zu2(:)) ! 1 / bulk aerodynamic momentum conductance |
---|
246 | zcdh(:)=zcdh_true(:)*sqrt(zu2(:)) ! 1 / bulk aerodynamic heat conductance |
---|
247 | ! these are the quantities to be looked at when comparing surface layers of different models |
---|
248 | |
---|
249 | ! Some usefull diagnostics for the new surface layer parametrization : |
---|
250 | |
---|
251 | ! call WRITEDIAGFI(ngridmx,'pcdv', |
---|
252 | ! & 'momentum drag','no units', |
---|
253 | ! & 2,zcdv_true) |
---|
254 | ! call WRITEDIAGFI(ngridmx,'pcdh', |
---|
255 | ! & 'heat drag','no units', |
---|
256 | ! & 2,zcdh_true) |
---|
257 | ! call WRITEDIAGFI(ngridmx,'u*', |
---|
258 | ! & 'friction velocity','m/s', |
---|
259 | ! & 2,sqrt(zcdv_true(:))*sqrt(zu2(:))) |
---|
260 | ! call WRITEDIAGFI(ngridmx,'T*', |
---|
261 | ! & 'friction temperature','K', |
---|
262 | ! & 2,-zcdh_true(:)*(ptsrf(:)-ph(:,1))/sqrt(zcdv_true(:))) |
---|
263 | ! call WRITEDIAGFI(ngridmx,'rm-1', |
---|
264 | ! & 'aerodyn momentum conductance','m/s', |
---|
265 | ! & 2,zcdv) |
---|
266 | ! call WRITEDIAGFI(ngridmx,'rh-1', |
---|
267 | ! & 'aerodyn heat conductance','m/s', |
---|
268 | ! & 2,zcdh) |
---|
269 | |
---|
270 | c ** schema de diffusion turbulente dans la couche limite |
---|
271 | c ---------------------------------------------------- |
---|
272 | |
---|
273 | CALL vdif_kc(ptimestep,g,pzlev,pzlay |
---|
274 | & ,pu,pv,ph,zcdv_true |
---|
275 | & ,pq2,zkv,zkh) |
---|
276 | |
---|
277 | if ((doubleq).and.(ngrid.eq.1)) then |
---|
278 | kmixmin = 80. !80.! minimum eddy mix coeff in 1D |
---|
279 | do ilev=1,nlay |
---|
280 | do ig=1,ngrid |
---|
281 | zkh(ig,ilev) = max(kmixmin,zkh(ig,ilev)) |
---|
282 | zkv(ig,ilev) = max(kmixmin,zkv(ig,ilev)) |
---|
283 | end do |
---|
284 | end do |
---|
285 | end if |
---|
286 | |
---|
287 | c ** diagnostique pour le schema de turbulence |
---|
288 | c ----------------------------------------- |
---|
289 | |
---|
290 | IF(lecrit) THEN |
---|
291 | PRINT* |
---|
292 | PRINT*,'Diagnostic for the vertical turbulent mixing' |
---|
293 | PRINT*,'Cd for momentum and potential temperature' |
---|
294 | |
---|
295 | PRINT*,zcdv(ngrid/2+1),zcdh(ngrid/2+1) |
---|
296 | PRINT*,'Mixing coefficient for momentum and pot.temp.' |
---|
297 | DO ilev=1,nlay |
---|
298 | PRINT*,zkv(ngrid/2+1,ilev),zkh(ngrid/2+1,ilev) |
---|
299 | ENDDO |
---|
300 | ENDIF |
---|
301 | |
---|
302 | |
---|
303 | |
---|
304 | |
---|
305 | c----------------------------------------------------------------------- |
---|
306 | c 4. inversion pour l'implicite sur u |
---|
307 | c -------------------------------- |
---|
308 | |
---|
309 | c ** l'equation est |
---|
310 | c u(t+1) = u(t) + dt * {(du/dt)phys}(t) + dt * {(du/dt)difv}(t+1) |
---|
311 | c avec |
---|
312 | c /zu/ = u(t) + dt * {(du/dt)phys}(t) (voir paragraphe 2.) |
---|
313 | c et |
---|
314 | c dt * {(du/dt)difv}(t+1) = dt * {(d/dz)[ Ku (du/dz) ]}(t+1) |
---|
315 | c donc les entrees sont /zcdv/ pour la condition a la limite sol |
---|
316 | c et /zkv/ = Ku |
---|
317 | |
---|
318 | CALL multipl((nlay-1)*ngrid,zkv(1,2),zb0(1,2),zb(1,2)) |
---|
319 | CALL multipl(ngrid,zcdv,zb0,zb) |
---|
320 | |
---|
321 | DO ig=1,ngrid |
---|
322 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
---|
323 | zc(ig,nlay)=za(ig,nlay)*zu(ig,nlay)*z1(ig) |
---|
324 | zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
---|
325 | ENDDO |
---|
326 | |
---|
327 | DO ilay=nlay-1,1,-1 |
---|
328 | DO ig=1,ngrid |
---|
329 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
---|
330 | $ zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
---|
331 | zc(ig,ilay)=(za(ig,ilay)*zu(ig,ilay)+ |
---|
332 | $ zb(ig,ilay+1)*zc(ig,ilay+1))*z1(ig) |
---|
333 | zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
---|
334 | ENDDO |
---|
335 | ENDDO |
---|
336 | |
---|
337 | DO ig=1,ngrid |
---|
338 | zu(ig,1)=zc(ig,1) |
---|
339 | ENDDO |
---|
340 | DO ilay=2,nlay |
---|
341 | DO ig=1,ngrid |
---|
342 | zu(ig,ilay)=zc(ig,ilay)+zd(ig,ilay)*zu(ig,ilay-1) |
---|
343 | ENDDO |
---|
344 | ENDDO |
---|
345 | |
---|
346 | |
---|
347 | |
---|
348 | |
---|
349 | |
---|
350 | c----------------------------------------------------------------------- |
---|
351 | c 5. inversion pour l'implicite sur v |
---|
352 | c -------------------------------- |
---|
353 | |
---|
354 | c ** l'equation est |
---|
355 | c v(t+1) = v(t) + dt * {(dv/dt)phys}(t) + dt * {(dv/dt)difv}(t+1) |
---|
356 | c avec |
---|
357 | c /zv/ = v(t) + dt * {(dv/dt)phys}(t) (voir paragraphe 2.) |
---|
358 | c et |
---|
359 | c dt * {(dv/dt)difv}(t+1) = dt * {(d/dz)[ Kv (dv/dz) ]}(t+1) |
---|
360 | c donc les entrees sont /zcdv/ pour la condition a la limite sol |
---|
361 | c et /zkv/ = Kv |
---|
362 | |
---|
363 | DO ig=1,ngrid |
---|
364 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
---|
365 | zc(ig,nlay)=za(ig,nlay)*zv(ig,nlay)*z1(ig) |
---|
366 | zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
---|
367 | ENDDO |
---|
368 | |
---|
369 | DO ilay=nlay-1,1,-1 |
---|
370 | DO ig=1,ngrid |
---|
371 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
---|
372 | $ zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
---|
373 | zc(ig,ilay)=(za(ig,ilay)*zv(ig,ilay)+ |
---|
374 | $ zb(ig,ilay+1)*zc(ig,ilay+1))*z1(ig) |
---|
375 | zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
---|
376 | ENDDO |
---|
377 | ENDDO |
---|
378 | |
---|
379 | DO ig=1,ngrid |
---|
380 | zv(ig,1)=zc(ig,1) |
---|
381 | ENDDO |
---|
382 | DO ilay=2,nlay |
---|
383 | DO ig=1,ngrid |
---|
384 | zv(ig,ilay)=zc(ig,ilay)+zd(ig,ilay)*zv(ig,ilay-1) |
---|
385 | ENDDO |
---|
386 | ENDDO |
---|
387 | |
---|
388 | |
---|
389 | |
---|
390 | |
---|
391 | |
---|
392 | c----------------------------------------------------------------------- |
---|
393 | c 6. inversion pour l'implicite sur h sans oublier le couplage |
---|
394 | c avec le sol (conduction) |
---|
395 | c ------------------------ |
---|
396 | |
---|
397 | c ** l'equation est |
---|
398 | c h(t+1) = h(t) + dt * {(dh/dt)phys}(t) + dt * {(dh/dt)difv}(t+1) |
---|
399 | c avec |
---|
400 | c /zh/ = h(t) + dt * {(dh/dt)phys}(t) (voir paragraphe 2.) |
---|
401 | c et |
---|
402 | c dt * {(dh/dt)difv}(t+1) = dt * {(d/dz)[ Kh (dh/dz) ]}(t+1) |
---|
403 | c donc les entrees sont /zcdh/ pour la condition de raccord au sol |
---|
404 | c et /zkh/ = Kh |
---|
405 | c ------------- |
---|
406 | |
---|
407 | CALL multipl((nlay-1)*ngrid,zkh(1,2),zb0(1,2),zb(1,2)) |
---|
408 | CALL multipl(ngrid,zcdh,zb0,zb) |
---|
409 | |
---|
410 | DO ig=1,ngrid |
---|
411 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
---|
412 | zc(ig,nlay)=za(ig,nlay)*zh(ig,nlay)*z1(ig) |
---|
413 | zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
---|
414 | ENDDO |
---|
415 | |
---|
416 | DO ilay=nlay-1,1,-1 |
---|
417 | DO ig=1,ngrid |
---|
418 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
---|
419 | $ zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
---|
420 | zc(ig,ilay)=(za(ig,ilay)*zh(ig,ilay)+ |
---|
421 | $ zb(ig,ilay+1)*zc(ig,ilay+1))*z1(ig) |
---|
422 | zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
---|
423 | ENDDO |
---|
424 | ENDDO |
---|
425 | |
---|
426 | c ** calcul de (d Planck / dT) a la temperature d'interface |
---|
427 | c ------------------------------------------------------ |
---|
428 | |
---|
429 | z4st=4.*5.67e-8*ptimestep |
---|
430 | DO ig=1,ngrid |
---|
431 | zdplanck(ig)=z4st*pemis(ig)*ptsrf(ig)*ptsrf(ig)*ptsrf(ig) |
---|
432 | ENDDO |
---|
433 | |
---|
434 | c ** calcul de la temperature_d'interface et de sa tendance. |
---|
435 | c on ecrit que la somme des flux est nulle a l'interface |
---|
436 | c a t + \delta t, |
---|
437 | c c'est a dire le flux radiatif a {t + \delta t} |
---|
438 | c + le flux turbulent a {t + \delta t} |
---|
439 | c qui s'ecrit K (T1-Tsurf) avec T1 = d1 Tsurf + c1 |
---|
440 | c (notation K dt = /cpp*b/) |
---|
441 | c + le flux dans le sol a t |
---|
442 | c + l'evolution du flux dans le sol lorsque la temperature d'interface |
---|
443 | c passe de sa valeur a t a sa valeur a {t + \delta t}. |
---|
444 | c ---------------------------------------------------- |
---|
445 | |
---|
446 | DO ig=1,ngrid |
---|
447 | z1(ig)=pcapcal(ig)*ptsrf(ig)+cpp*zb(ig,1)*zc(ig,1) |
---|
448 | s +zdplanck(ig)*ptsrf(ig)+ pfluxsrf(ig)*ptimestep |
---|
449 | z2(ig)= pcapcal(ig)+cpp*zb(ig,1)*(1.-zd(ig,1))+zdplanck(ig) |
---|
450 | ztsrf2(ig)=z1(ig)/z2(ig) |
---|
451 | pdtsrf(ig)=(ztsrf2(ig)-ptsrf(ig))/ptimestep |
---|
452 | |
---|
453 | c Modif speciale CO2 condensation: |
---|
454 | c tconds = 1./(bcond-acond*log(.0095*pplev(ig,1))) |
---|
455 | c if ((callcond).and. |
---|
456 | c & ((co2ice(ig).ne.0).or.(ztsrf2(ig).lt.tconds)))then |
---|
457 | c zh(ig,1)=zc(ig,1)+zd(ig,1)*tconds |
---|
458 | c else |
---|
459 | zh(ig,1)=zc(ig,1)+zd(ig,1)*ztsrf2(ig) |
---|
460 | c end if |
---|
461 | ENDDO |
---|
462 | |
---|
463 | c ** et a partir de la temperature au sol on remonte |
---|
464 | c ----------------------------------------------- |
---|
465 | |
---|
466 | DO ilay=2,nlay |
---|
467 | DO ig=1,ngrid |
---|
468 | hh = max( zh(ig,ilay-1) , zhcond(ig,ilay-1) ) ! modif co2cond |
---|
469 | zh(ig,ilay)=zc(ig,ilay)+zd(ig,ilay)*hh |
---|
470 | ENDDO |
---|
471 | ENDDO |
---|
472 | |
---|
473 | |
---|
474 | c----------------------------------------------------------------------- |
---|
475 | c TRACERS |
---|
476 | c ------- |
---|
477 | |
---|
478 | if(tracer) then |
---|
479 | |
---|
480 | c Using the wind modified by friction for lifting and sublimation |
---|
481 | c ---------------------------------------------------------------- |
---|
482 | DO ig=1,ngrid |
---|
483 | zu2(ig)=zu(ig,1)*zu(ig,1)+zv(ig,1)*zv(ig,1) |
---|
484 | zcdv(ig)=zcdv_true(ig)*sqrt(zu2(ig)) |
---|
485 | zcdh(ig)=zcdh_true(ig)*sqrt(zu2(ig)) |
---|
486 | ENDDO |
---|
487 | |
---|
488 | c Calcul du flux vertical au bas de la premiere couche (dust) : |
---|
489 | c ----------------------------------------------------------- |
---|
490 | do ig=1,ngridmx |
---|
491 | rho(ig) = zb0(ig,1) /ptimestep |
---|
492 | c zb(ig,1) = 0. |
---|
493 | end do |
---|
494 | c Dust lifting: |
---|
495 | if (lifting) then |
---|
496 | if (doubleq.AND.submicron) then |
---|
497 | do ig=1,ngrid |
---|
498 | c if(co2ice(ig).lt.1) then |
---|
499 | pdqsdif(ig,igcm_dust_mass) = |
---|
500 | & -alpha_lift(igcm_dust_mass) |
---|
501 | pdqsdif(ig,igcm_dust_number) = |
---|
502 | & -alpha_lift(igcm_dust_number) |
---|
503 | pdqsdif(ig,igcm_dust_submicron) = |
---|
504 | & -alpha_lift(igcm_dust_submicron) |
---|
505 | c end if |
---|
506 | end do |
---|
507 | else if (doubleq) then |
---|
508 | do ig=1,ngrid |
---|
509 | !!! soulevement constant |
---|
510 | pdqsdif(ig,igcm_dust_mass) = |
---|
511 | & -alpha_lift(igcm_dust_mass) |
---|
512 | pdqsdif(ig,igcm_dust_number) = |
---|
513 | & -alpha_lift(igcm_dust_number) |
---|
514 | end do |
---|
515 | else if (submicron) then |
---|
516 | do ig=1,ngrid |
---|
517 | pdqsdif(ig,igcm_dust_submicron) = |
---|
518 | & -alpha_lift(igcm_dust_submicron) |
---|
519 | end do |
---|
520 | else |
---|
521 | call dustlift(ngrid,nlay,nq,rho,zcdh_true,zcdh,co2ice, |
---|
522 | & pdqsdif) |
---|
523 | endif !doubleq.AND.submicron |
---|
524 | else |
---|
525 | pdqsdif(1:ngrid,1:nq) = 0. |
---|
526 | end if |
---|
527 | |
---|
528 | c OU calcul de la valeur de q a la surface (water) : |
---|
529 | c ---------------------------------------- |
---|
530 | if (water) then |
---|
531 | call watersat(ngridmx,ptsrf,pplev(1,1),qsat) |
---|
532 | end if |
---|
533 | |
---|
534 | c Inversion pour l'implicite sur q |
---|
535 | c -------------------------------- |
---|
536 | do iq=1,nq |
---|
537 | CALL multipl((nlay-1)*ngrid,zkh(1,2),zb0(1,2),zb(1,2)) |
---|
538 | |
---|
539 | if ((water).and.(iq.eq.igcm_h2o_vap)) then |
---|
540 | c This line is required to account for turbulent transport |
---|
541 | c from surface (e.g. ice) to mid-layer of atmosphere: |
---|
542 | CALL multipl(ngrid,zcdv,zb0,zb(1,1)) |
---|
543 | CALL multipl(ngrid,dryness,zb(1,1),zb(1,1)) |
---|
544 | else ! (re)-initialize zb(:,1) |
---|
545 | zb(1:ngrid,1)=0 |
---|
546 | end if |
---|
547 | |
---|
548 | DO ig=1,ngrid |
---|
549 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
---|
550 | zc(ig,nlay)=za(ig,nlay)*zq(ig,nlay,iq)*z1(ig) |
---|
551 | zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
---|
552 | ENDDO |
---|
553 | |
---|
554 | DO ilay=nlay-1,2,-1 |
---|
555 | DO ig=1,ngrid |
---|
556 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
---|
557 | $ zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
---|
558 | zc(ig,ilay)=(za(ig,ilay)*zq(ig,ilay,iq)+ |
---|
559 | $ zb(ig,ilay+1)*zc(ig,ilay+1))*z1(ig) |
---|
560 | zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
---|
561 | ENDDO |
---|
562 | ENDDO |
---|
563 | |
---|
564 | if (water.and.(iq.eq.igcm_h2o_ice)) then |
---|
565 | ! special case for water ice tracer: do not include |
---|
566 | ! h2o ice tracer from surface (which is set when handling |
---|
567 | ! h2o vapour case (see further down). |
---|
568 | DO ig=1,ngrid |
---|
569 | z1(ig)=1./(za(ig,1)+zb(ig,1)+ |
---|
570 | $ zb(ig,2)*(1.-zd(ig,2))) |
---|
571 | zc(ig,1)=(za(ig,1)*zq(ig,1,iq)+ |
---|
572 | $ zb(ig,2)*zc(ig,2)) *z1(ig) |
---|
573 | ENDDO |
---|
574 | else ! general case |
---|
575 | DO ig=1,ngrid |
---|
576 | z1(ig)=1./(za(ig,1)+zb(ig,1)+ |
---|
577 | $ zb(ig,2)*(1.-zd(ig,2))) |
---|
578 | zc(ig,1)=(za(ig,1)*zq(ig,1,iq)+ |
---|
579 | $ zb(ig,2)*zc(ig,2) + |
---|
580 | $ (-pdqsdif(ig,iq)) *ptimestep) *z1(ig) !tracer flux from surface |
---|
581 | ENDDO |
---|
582 | endif ! of if (water.and.(iq.eq.igcm_h2o_ice)) |
---|
583 | |
---|
584 | IF ((water).and.(iq.eq.igcm_h2o_vap)) then |
---|
585 | c Calculation for turbulent exchange with the surface (for ice) |
---|
586 | DO ig=1,ngrid |
---|
587 | zd(ig,1)=zb(ig,1)*z1(ig) |
---|
588 | zq1temp(ig)=zc(ig,1)+ zd(ig,1)*qsat(ig) |
---|
589 | |
---|
590 | pdqsdif(ig,igcm_h2o_ice)=rho(ig)*dryness(ig)*zcdv(ig) |
---|
591 | & *(zq1temp(ig)-qsat(ig)) |
---|
592 | c write(*,*)'flux vers le sol=',pdqsdif(ig,nq) |
---|
593 | END DO |
---|
594 | |
---|
595 | DO ig=1,ngrid |
---|
596 | if(.not.watercaptag(ig)) then |
---|
597 | if ((-pdqsdif(ig,igcm_h2o_ice)*ptimestep) |
---|
598 | & .gt.pqsurf(ig,igcm_h2o_ice)) then |
---|
599 | c write(*,*)'on sublime plus que qsurf!' |
---|
600 | pdqsdif(ig,igcm_h2o_ice)= |
---|
601 | & -pqsurf(ig,igcm_h2o_ice)/ptimestep |
---|
602 | c write(*,*)'flux vers le sol=',pdqsdif(ig,nq) |
---|
603 | z1(ig)=1./(za(ig,1)+ zb(ig,2)*(1.-zd(ig,2))) |
---|
604 | zc(ig,1)=(za(ig,1)*zq(ig,1,igcm_h2o_vap)+ |
---|
605 | $ zb(ig,2)*zc(ig,2) + |
---|
606 | $ (-pdqsdif(ig,igcm_h2o_ice)) *ptimestep) *z1(ig) |
---|
607 | zq1temp(ig)=zc(ig,1) |
---|
608 | endif |
---|
609 | endif ! if (.not.watercaptag(ig)) |
---|
610 | c Starting upward calculations for water : |
---|
611 | zq(ig,1,igcm_h2o_vap)=zq1temp(ig) |
---|
612 | ENDDO ! of DO ig=1,ngrid |
---|
613 | ELSE |
---|
614 | c Starting upward calculations for simple mixing of tracer (dust) |
---|
615 | DO ig=1,ngrid |
---|
616 | zq(ig,1,iq)=zc(ig,1) |
---|
617 | ENDDO |
---|
618 | END IF ! of IF ((water).and.(iq.eq.igcm_h2o_vap)) |
---|
619 | |
---|
620 | DO ilay=2,nlay |
---|
621 | DO ig=1,ngrid |
---|
622 | zq(ig,ilay,iq)=zc(ig,ilay)+zd(ig,ilay)*zq(ig,ilay-1,iq) |
---|
623 | ENDDO |
---|
624 | ENDDO |
---|
625 | enddo ! of do iq=1,nq |
---|
626 | end if ! of if(tracer) |
---|
627 | |
---|
628 | c----------------------------------------------------------------------- |
---|
629 | c 8. calcul final des tendances de la diffusion verticale |
---|
630 | c ---------------------------------------------------- |
---|
631 | |
---|
632 | DO ilev = 1, nlay |
---|
633 | DO ig=1,ngrid |
---|
634 | pdudif(ig,ilev)=( zu(ig,ilev)- |
---|
635 | $ (pu(ig,ilev)+pdufi(ig,ilev)*ptimestep) )/ptimestep |
---|
636 | pdvdif(ig,ilev)=( zv(ig,ilev)- |
---|
637 | $ (pv(ig,ilev)+pdvfi(ig,ilev)*ptimestep) )/ptimestep |
---|
638 | hh = max(ph(ig,ilev)+pdhfi(ig,ilev)*ptimestep , |
---|
639 | $ zhcond(ig,ilev)) ! modif co2cond |
---|
640 | pdhdif(ig,ilev)=( zh(ig,ilev)- hh )/ptimestep |
---|
641 | ENDDO |
---|
642 | ENDDO |
---|
643 | |
---|
644 | |
---|
645 | if (tracer) then |
---|
646 | DO iq = 1, nq |
---|
647 | DO ilev = 1, nlay |
---|
648 | DO ig=1,ngrid |
---|
649 | pdqdif(ig,ilev,iq)=(zq(ig,ilev,iq)- |
---|
650 | $ (pq(ig,ilev,iq) + pdqfi(ig,ilev,iq)*ptimestep))/ptimestep |
---|
651 | ENDDO |
---|
652 | ENDDO |
---|
653 | ENDDO |
---|
654 | end if |
---|
655 | |
---|
656 | c ** diagnostique final |
---|
657 | c ------------------ |
---|
658 | |
---|
659 | IF(lecrit) THEN |
---|
660 | PRINT*,'In vdif' |
---|
661 | PRINT*,'Ts (t) and Ts (t+st)' |
---|
662 | WRITE(*,'(a10,3a15)') |
---|
663 | s 'theta(t)','theta(t+dt)','u(t)','u(t+dt)' |
---|
664 | PRINT*,ptsrf(ngrid/2+1),ztsrf2(ngrid/2+1) |
---|
665 | DO ilev=1,nlay |
---|
666 | WRITE(*,'(4f15.7)') |
---|
667 | s ph(ngrid/2+1,ilev),zh(ngrid/2+1,ilev), |
---|
668 | s pu(ngrid/2+1,ilev),zu(ngrid/2+1,ilev) |
---|
669 | |
---|
670 | ENDDO |
---|
671 | ENDIF |
---|
672 | |
---|
673 | if (calltherm .and. outptherm) then |
---|
674 | if (ngrid .eq. 1) then |
---|
675 | call WRITEDIAGFI(ngrid,'zh','zh inside vdifc', |
---|
676 | & 'SI',1,ph(:,:)+pdhfi(:,:)*ptimestep) |
---|
677 | call WRITEDIAGFI(ngrid,'zkh','zkh', |
---|
678 | & 'SI',1,zkh) |
---|
679 | endif |
---|
680 | endif |
---|
681 | |
---|
682 | RETURN |
---|
683 | END |
---|