5 |
contains |
contains |
6 |
|
|
7 |
SUBROUTINE bilan_dyn(ps, masse, pk, flux_u, flux_v, teta, phi, ucov, vcov, & |
SUBROUTINE bilan_dyn(ps, masse, pk, flux_u, flux_v, teta, phi, ucov, vcov, & |
8 |
trac, dt_app, dt_cum) |
trac) |
9 |
|
|
10 |
! From LMDZ4/libf/dyn3d/bilan_dyn.F, version 1.5 2005/03/16 |
! From LMDZ4/libf/dyn3d/bilan_dyn.F, version 1.5 2005/03/16 10:12:17 |
|
! 10:12:17 fairhead |
|
11 |
|
|
12 |
! Sous-programme consacré à des diagnostics dynamiques de base |
! Sous-programme consacr\'e \`a des diagnostics dynamiques de |
13 |
! De façon générale, les moyennes des scalaires Q sont pondérées par |
! base. De fa\c{}con g\'en\'erale, les moyennes des scalaires Q |
14 |
! la masse. Les flux de masse sont, eux, simplement moyennés. |
! sont pond\'er\'ees par la masse. Les flux de masse sont, eux, |
15 |
|
! simplement moyenn\'es. |
16 |
|
|
17 |
USE histcom, ONLY: histbeg_totreg, histdef, histend, histvert |
USE comconst, ONLY: cpp |
18 |
USE calendar, ONLY: ymds2ju |
USE comgeom, ONLY: constang_2d, cu_2d, cv_2d |
19 |
USE histwrite_m, ONLY: histwrite |
use covcont_m, only: covcont |
20 |
USE dimens_m, ONLY: iim, jjm, llm |
USE dimens_m, ONLY: iim, jjm, llm |
21 |
|
use enercin_m, only: enercin |
22 |
|
USE histwrite_m, ONLY: histwrite |
23 |
|
use init_dynzon_m, only: ncum, fileid, znom, ntr, nq, nom |
24 |
|
use massbar_m, only: massbar |
25 |
USE paramet_m, ONLY: iip1, jjp1 |
USE paramet_m, ONLY: iip1, jjp1 |
26 |
USE comconst, ONLY: cpp |
|
27 |
USE comvert, ONLY: presnivs |
real, intent(in):: ps(iip1, jjp1) |
28 |
USE comgeom, ONLY: constang_2d, cu_2d, cv_2d, rlatv |
real, intent(in):: masse(iip1, jjp1, llm), pk(iip1, jjp1, llm) |
29 |
USE temps, ONLY: annee_ref, day_ref, itau_dyn |
real, intent(in):: flux_u(iip1, jjp1, llm) |
30 |
USE inigrads_m, ONLY: inigrads |
real, intent(in):: flux_v(iip1, jjm, llm) |
|
USE nr_util, ONLY: pi |
|
|
|
|
|
! Arguments: |
|
|
|
|
|
real, intent(in):: dt_app, dt_cum |
|
|
real ps(iip1, jjp1) |
|
|
real masse(iip1, jjp1, llm), pk(iip1, jjp1, llm) |
|
|
real flux_u(iip1, jjp1, llm) |
|
|
real flux_v(iip1, jjm, llm) |
|
31 |
real, intent(in):: teta(iip1, jjp1, llm) |
real, intent(in):: teta(iip1, jjp1, llm) |
32 |
real phi(iip1, jjp1, llm) |
real, intent(in):: phi(iip1, jjp1, llm) |
33 |
real ucov(iip1, jjp1, llm) |
real, intent(in):: ucov(:, :, :) ! (iip1, jjp1, llm) |
34 |
real vcov(iip1, jjm, llm) |
real, intent(in):: vcov(iip1, jjm, llm) |
35 |
real, intent(in):: trac(:, :, :) ! (iim + 1, jjm + 1, llm) |
real, intent(in):: trac(:, :, :) ! (iim + 1, jjm + 1, llm) |
36 |
|
|
37 |
! Local: |
! Local: |
38 |
|
|
39 |
integer:: icum = 0 |
integer:: icum = 0 |
|
integer, save:: ncum |
|
|
logical:: first = .true. |
|
|
real zz, zqy, zfactv(jjm, llm) |
|
|
|
|
|
integer, parameter:: nQ = 7 |
|
|
character(len=4), parameter:: nom(nQ) = (/'T ', 'gz ', 'K ', 'ang ', & |
|
|
'u ', 'ovap', 'un '/) |
|
|
character(len=5), parameter:: unites(nQ) = (/'K ', 'm2/s2', 'm2/s2', & |
|
|
'ang ', 'm/s ', 'kg/kg', 'un '/) |
|
|
|
|
|
real:: time = 0. |
|
40 |
integer:: itau = 0 |
integer:: itau = 0 |
41 |
real ww |
real qy, factv(jjm, llm) |
42 |
|
|
43 |
! Variables dynamiques intermédiaires |
! Variables dynamiques interm\'ediaires |
44 |
REAL vcont(iip1, jjm, llm), ucont(iip1, jjp1, llm) |
REAL vcont(iip1, jjm, llm), ucont(iip1, jjp1, llm) |
45 |
REAL ang(iip1, jjp1, llm), unat(iip1, jjp1, llm) |
REAL ang(iip1, jjp1, llm), unat(iip1, jjp1, llm) |
46 |
REAL massebx(iip1, jjp1, llm), masseby(iip1, jjm, llm) |
REAL massebx(iip1, jjp1, llm), masseby(iip1, jjm, llm) |
47 |
REAL w(iip1, jjp1, llm), ecin(iip1, jjp1, llm), convm(iip1, jjp1, llm) |
REAL ecin(iip1, jjp1, llm) |
48 |
|
|
49 |
! Champ contenant les scalaires advectés |
! Champ contenant les scalaires advect\'es |
50 |
real Q(iip1, jjp1, llm, nQ) |
real Q(iip1, jjp1, llm, nQ) |
51 |
|
|
52 |
! Champs cumulés |
! Champs cumul\'es |
53 |
real, save:: ps_cum(iip1, jjp1) |
real, save:: ps_cum(iip1, jjp1) |
54 |
real, save:: masse_cum(iip1, jjp1, llm) |
real, save:: masse_cum(iip1, jjp1, llm) |
55 |
real, save:: flux_u_cum(iip1, jjp1, llm) |
real, save:: flux_u_cum(iip1, jjp1, llm) |
57 |
real, save:: Q_cum(iip1, jjp1, llm, nQ) |
real, save:: Q_cum(iip1, jjp1, llm, nQ) |
58 |
real, save:: flux_uQ_cum(iip1, jjp1, llm, nQ) |
real, save:: flux_uQ_cum(iip1, jjp1, llm, nQ) |
59 |
real, save:: flux_vQ_cum(iip1, jjm, llm, nQ) |
real, save:: flux_vQ_cum(iip1, jjm, llm, nQ) |
|
real dQ(iip1, jjp1, llm, nQ) |
|
60 |
|
|
61 |
! champs de tansport en moyenne zonale |
! champs de tansport en moyenne zonale |
62 |
integer itr |
integer itr |
|
integer, parameter:: ntr = 5 |
|
|
|
|
|
character(len=10), save:: znom(ntr, nQ) |
|
|
character(len=26), save:: znoml(ntr, nQ) |
|
|
character(len=12), save:: zunites(ntr, nQ) |
|
|
|
|
63 |
integer, parameter:: iave = 1, itot = 2, immc = 3, itrs = 4, istn = 5 |
integer, parameter:: iave = 1, itot = 2, immc = 3, itrs = 4, istn = 5 |
|
character(len=3), parameter:: ctrs(ntr) = (/' ', 'TOT', 'MMC', 'TRS', & |
|
|
'STN'/) |
|
64 |
|
|
65 |
real zvQ(jjm, llm, ntr, nQ), zvQtmp(jjm, llm) |
real vq(jjm, llm, ntr, nQ), vqtmp(jjm, llm) |
66 |
real zavQ(jjm, 2: ntr, nQ), psiQ(jjm, llm + 1, nQ) |
real avq(jjm, 2: ntr, nQ), psiQ(jjm, llm + 1, nQ) |
67 |
real zmasse(jjm, llm) |
real zmasse(jjm, llm) |
68 |
|
real v(jjm, llm), psi(jjm, llm + 1) |
|
real zv(jjm, llm), psi(jjm, llm + 1) |
|
|
|
|
69 |
integer i, j, l, iQ |
integer i, j, l, iQ |
70 |
|
|
|
! Initialisation du fichier contenant les moyennes zonales. |
|
|
|
|
|
integer, save:: fileid |
|
|
integer thoriid, zvertiid |
|
|
|
|
|
real zjulian |
|
|
integer zan, dayref |
|
|
|
|
|
real rlong(jjm), rlatg(jjm) |
|
|
|
|
71 |
!----------------------------------------------------------------- |
!----------------------------------------------------------------- |
72 |
|
|
|
!!print *, "Call sequence information: bilan_dyn" |
|
|
|
|
|
! Initialisation |
|
|
|
|
|
time = time + dt_app |
|
|
itau = itau + 1 |
|
|
|
|
|
first_call: if (first) then |
|
|
! initialisation des fichiers |
|
|
first = .false. |
|
|
! ncum est la frequence de stokage en pas de temps |
|
|
ncum = dt_cum / dt_app |
|
|
if (abs(ncum * dt_app - dt_cum) > 1e-5 * dt_app) then |
|
|
print *, 'Problème : le pas de cumul doit être multiple du pas' |
|
|
print *, 'dt_app = ', dt_app |
|
|
print *, 'dt_cum = ', dt_cum |
|
|
stop 1 |
|
|
endif |
|
|
|
|
|
call inigrads(i_f=4, x=(/0./), fx=180./pi, xmin=0., xmax=0., y=rlatv, & |
|
|
ymin=-90., ymax=90., fy=180./pi, z=presnivs, fz=1., dt=dt_cum, & |
|
|
file='dynzon', titlel='dyn_zon ') |
|
|
|
|
|
! Initialisation du fichier contenant les moyennes zonales |
|
|
|
|
|
zan = annee_ref |
|
|
dayref = day_ref |
|
|
CALL ymds2ju(zan, 1, dayref, 0.0, zjulian) |
|
|
|
|
|
rlong = 0. |
|
|
rlatg = rlatv*180./pi |
|
|
|
|
|
call histbeg_totreg('dynzon', rlong(:1), rlatg, 1, 1, 1, jjm, itau_dyn, & |
|
|
zjulian, dt_cum, thoriid, fileid) |
|
|
|
|
|
! Appel à histvert pour la grille verticale |
|
|
|
|
|
call histvert(fileid, 'presnivs', 'Niveaux sigma', 'mb', llm, presnivs, & |
|
|
zvertiid) |
|
|
|
|
|
! Appels à histdef pour la définition des variables à sauvegarder |
|
|
do iQ = 1, nQ |
|
|
do itr = 1, ntr |
|
|
if (itr == 1) then |
|
|
znom(itr, iQ) = nom(iQ) |
|
|
znoml(itr, iQ) = nom(iQ) |
|
|
zunites(itr, iQ) = unites(iQ) |
|
|
else |
|
|
znom(itr, iQ) = ctrs(itr)//'v'//nom(iQ) |
|
|
znoml(itr, iQ) = 'transport : v * '//nom(iQ)//' '//ctrs(itr) |
|
|
zunites(itr, iQ) = 'm/s * '//unites(iQ) |
|
|
endif |
|
|
enddo |
|
|
enddo |
|
|
|
|
|
! Déclarations des champs avec dimension verticale |
|
|
do iQ = 1, nQ |
|
|
do itr = 1, ntr |
|
|
call histdef(fileid, znom(itr, iQ), znoml(itr, iQ), & |
|
|
zunites(itr, iQ), 1, jjm, thoriid, llm, 1, llm, zvertiid, & |
|
|
'ave(X)', dt_cum, dt_cum) |
|
|
enddo |
|
|
! Declarations pour les fonctions de courant |
|
|
call histdef(fileid, 'psi'//nom(iQ), 'stream fn. '//znoml(itot, iQ), & |
|
|
zunites(itot, iQ), 1, jjm, thoriid, llm, 1, llm, zvertiid, & |
|
|
'ave(X)', dt_cum, dt_cum) |
|
|
enddo |
|
|
|
|
|
! Declarations pour les champs de transport d'air |
|
|
call histdef(fileid, 'masse', 'masse', & |
|
|
'kg', 1, jjm, thoriid, llm, 1, llm, zvertiid, & |
|
|
'ave(X)', dt_cum, dt_cum) |
|
|
call histdef(fileid, 'v', 'v', & |
|
|
'm/s', 1, jjm, thoriid, llm, 1, llm, zvertiid, & |
|
|
'ave(X)', dt_cum, dt_cum) |
|
|
! Declarations pour les fonctions de courant |
|
|
call histdef(fileid, 'psi', 'stream fn. MMC ', 'mega t/s', & |
|
|
1, jjm, thoriid, llm, 1, llm, zvertiid, & |
|
|
'ave(X)', dt_cum, dt_cum) |
|
|
|
|
|
! Declaration des champs 1D de transport en latitude |
|
|
do iQ = 1, nQ |
|
|
do itr = 2, ntr |
|
|
call histdef(fileid, 'a'//znom(itr, iQ), znoml(itr, iQ), & |
|
|
zunites(itr, iQ), 1, jjm, thoriid, 1, 1, 1, -99, & |
|
|
'ave(X)', dt_cum, dt_cum) |
|
|
enddo |
|
|
enddo |
|
|
|
|
|
CALL histend(fileid) |
|
|
endif first_call |
|
|
|
|
73 |
! Calcul des champs dynamiques |
! Calcul des champs dynamiques |
74 |
|
|
75 |
! Énergie cinétique |
! \'Energie cin\'etique |
76 |
ucont = 0 |
ucont = 0 |
77 |
CALL covcont(llm, ucov, vcov, ucont, vcont) |
CALL covcont(llm, ucov, vcov, ucont, vcont) |
78 |
CALL enercin(vcov, ucov, vcont, ucont, ecin) |
CALL enercin(vcov, ucov, vcont, ucont, ecin) |
79 |
|
|
80 |
! moment cinétique |
! moment cin\'etique |
81 |
do l = 1, llm |
forall (l = 1: llm) |
82 |
ang(:, :, l) = ucov(:, :, l) + constang_2d |
ang(:, :, l) = ucov(:, :, l) + constang_2d |
83 |
unat(:, :, l) = ucont(:, :, l)*cu_2d |
unat(:, :, l) = ucont(:, :, l) * cu_2d |
84 |
enddo |
end forall |
85 |
|
|
86 |
Q(:, :, :, 1) = teta * pk / cpp |
Q(:, :, :, 1) = teta * pk / cpp |
87 |
Q(:, :, :, 2) = phi |
Q(:, :, :, 2) = phi |
103 |
flux_uQ_cum = 0. |
flux_uQ_cum = 0. |
104 |
endif |
endif |
105 |
|
|
106 |
|
itau = itau + 1 |
107 |
icum = icum + 1 |
icum = icum + 1 |
108 |
|
|
109 |
! Accumulation des flux de masse horizontaux |
! Accumulation des flux de masse horizontaux |
111 |
masse_cum = masse_cum + masse |
masse_cum = masse_cum + masse |
112 |
flux_u_cum = flux_u_cum + flux_u |
flux_u_cum = flux_u_cum + flux_u |
113 |
flux_v_cum = flux_v_cum + flux_v |
flux_v_cum = flux_v_cum + flux_v |
114 |
do iQ = 1, nQ |
forall (iQ = 1: nQ) Q_cum(:, :, :, iQ) = Q_cum(:, :, :, iQ) & |
115 |
Q_cum(:, :, :, iQ) = Q_cum(:, :, :, iQ) + Q(:, :, :, iQ)*masse |
+ Q(:, :, :, iQ) * masse |
|
enddo |
|
|
|
|
|
! FLUX ET TENDANCES |
|
116 |
|
|
117 |
! Flux longitudinal |
! Flux longitudinal |
118 |
forall (iQ = 1: nQ, i = 1: iim) flux_uQ_cum(i, :, :, iQ) & |
forall (iQ = 1: nQ, i = 1: iim) flux_uQ_cum(i, :, :, iQ) & |
120 |
+ flux_u(i, :, :) * 0.5 * (Q(i, :, :, iQ) + Q(i + 1, :, :, iQ)) |
+ flux_u(i, :, :) * 0.5 * (Q(i, :, :, iQ) + Q(i + 1, :, :, iQ)) |
121 |
flux_uQ_cum(iip1, :, :, :) = flux_uQ_cum(1, :, :, :) |
flux_uQ_cum(iip1, :, :, :) = flux_uQ_cum(1, :, :, :) |
122 |
|
|
123 |
! Flux méridien |
! Flux m\'eridien |
124 |
forall (iQ = 1: nQ, j = 1: jjm) flux_vQ_cum(:, j, :, iQ) & |
forall (iQ = 1: nQ, j = 1: jjm) flux_vQ_cum(:, j, :, iQ) & |
125 |
= flux_vQ_cum(:, j, :, iQ) & |
= flux_vQ_cum(:, j, :, iQ) & |
126 |
+ flux_v(:, j, :) * 0.5 * (Q(:, j, :, iQ) + Q(:, j + 1, :, iQ)) |
+ flux_v(:, j, :) * 0.5 * (Q(:, j, :, iQ) + Q(:, j + 1, :, iQ)) |
127 |
|
|
|
! tendances |
|
|
|
|
|
! convergence horizontale |
|
|
call convflu(flux_uQ_cum, flux_vQ_cum, llm*nQ, dQ) |
|
|
|
|
|
! calcul de la vitesse verticale |
|
|
call convmas(flux_u_cum, flux_v_cum, convm) |
|
|
CALL vitvert(convm, w) |
|
|
|
|
|
do iQ = 1, nQ |
|
|
do l = 1, llm-1 |
|
|
do j = 1, jjp1 |
|
|
do i = 1, iip1 |
|
|
ww = -0.5*w(i, j, l + 1)*(Q(i, j, l, iQ) + Q(i, j, l + 1, iQ)) |
|
|
dQ(i, j, l, iQ) = dQ(i, j, l, iQ)-ww |
|
|
dQ(i, j, l + 1, iQ) = dQ(i, j, l + 1, iQ) + ww |
|
|
enddo |
|
|
enddo |
|
|
enddo |
|
|
enddo |
|
|
|
|
|
! PAS DE TEMPS D'ECRITURE |
|
|
|
|
128 |
writing_step: if (icum == ncum) then |
writing_step: if (icum == ncum) then |
129 |
! Normalisation |
! Normalisation |
130 |
do iQ = 1, nQ |
forall (iQ = 1: nQ) Q_cum(:, :, :, iQ) = Q_cum(:, :, :, iQ) / masse_cum |
131 |
Q_cum(:, :, :, iQ) = Q_cum(:, :, :, iQ)/masse_cum |
ps_cum = ps_cum / ncum |
132 |
enddo |
masse_cum = masse_cum / ncum |
133 |
zz = 1. / real(ncum) |
flux_u_cum = flux_u_cum / ncum |
134 |
ps_cum = ps_cum*zz |
flux_v_cum = flux_v_cum / ncum |
135 |
masse_cum = masse_cum*zz |
flux_uQ_cum = flux_uQ_cum / ncum |
136 |
flux_u_cum = flux_u_cum*zz |
flux_vQ_cum = flux_vQ_cum / ncum |
|
flux_v_cum = flux_v_cum*zz |
|
|
flux_uQ_cum = flux_uQ_cum*zz |
|
|
flux_vQ_cum = flux_vQ_cum*zz |
|
|
dQ = dQ*zz |
|
|
|
|
|
! A retravailler eventuellement |
|
|
! division de dQ par la masse pour revenir aux bonnes grandeurs |
|
|
do iQ = 1, nQ |
|
|
dQ(:, :, :, iQ) = dQ(:, :, :, iQ)/masse_cum |
|
|
enddo |
|
137 |
|
|
138 |
! Transport méridien |
! Transport m\'eridien |
139 |
|
|
140 |
! cumul zonal des masses des mailles |
! Cumul zonal des masses des mailles |
141 |
|
|
142 |
zv = 0. |
v = 0. |
143 |
zmasse = 0. |
zmasse = 0. |
144 |
call massbar(masse_cum, massebx, masseby) |
call massbar(masse_cum, massebx, masseby) |
145 |
do l = 1, llm |
do l = 1, llm |
146 |
do j = 1, jjm |
do j = 1, jjm |
147 |
do i = 1, iim |
do i = 1, iim |
148 |
zmasse(j, l) = zmasse(j, l) + masseby(i, j, l) |
zmasse(j, l) = zmasse(j, l) + masseby(i, j, l) |
149 |
zv(j, l) = zv(j, l) + flux_v_cum(i, j, l) |
v(j, l) = v(j, l) + flux_v_cum(i, j, l) |
150 |
enddo |
enddo |
151 |
zfactv(j, l) = cv_2d(1, j)/zmasse(j, l) |
factv(j, l) = cv_2d(1, j) / zmasse(j, l) |
152 |
enddo |
enddo |
153 |
enddo |
enddo |
154 |
|
|
155 |
! Transport dans le plan latitude-altitude |
! Transport dans le plan latitude-altitude |
156 |
|
|
157 |
zvQ = 0. |
vq = 0. |
158 |
psiQ = 0. |
psiQ = 0. |
159 |
do iQ = 1, nQ |
do iQ = 1, nQ |
160 |
zvQtmp = 0. |
vqtmp = 0. |
161 |
do l = 1, llm |
do l = 1, llm |
162 |
do j = 1, jjm |
do j = 1, jjm |
163 |
! Calcul des moyennes zonales du transort total et de zvQtmp |
! Calcul des moyennes zonales du transport total et de vqtmp |
164 |
do i = 1, iim |
do i = 1, iim |
165 |
zvQ(j, l, itot, iQ) = zvQ(j, l, itot, iQ) & |
vq(j, l, itot, iQ) = vq(j, l, itot, iQ) & |
166 |
+ flux_vQ_cum(i, j, l, iQ) |
+ flux_vQ_cum(i, j, l, iQ) |
167 |
zqy = 0.5 * (Q_cum(i, j, l, iQ) * masse_cum(i, j, l) & |
qy = 0.5 * (Q_cum(i, j, l, iQ) * masse_cum(i, j, l) & |
168 |
+ Q_cum(i, j + 1, l, iQ) * masse_cum(i, j + 1, l)) |
+ Q_cum(i, j + 1, l, iQ) * masse_cum(i, j + 1, l)) |
169 |
zvQtmp(j, l) = zvQtmp(j, l) + flux_v_cum(i, j, l) * zqy & |
vqtmp(j, l) = vqtmp(j, l) + flux_v_cum(i, j, l) * qy & |
170 |
/ (0.5 * (masse_cum(i, j, l) + masse_cum(i, j + 1, l))) |
/ (0.5 * (masse_cum(i, j, l) + masse_cum(i, j + 1, l))) |
171 |
zvQ(j, l, iave, iQ) = zvQ(j, l, iave, iQ) + zqy |
vq(j, l, iave, iQ) = vq(j, l, iave, iQ) + qy |
172 |
enddo |
enddo |
173 |
! Decomposition |
! Decomposition |
174 |
zvQ(j, l, iave, iQ) = zvQ(j, l, iave, iQ)/zmasse(j, l) |
vq(j, l, iave, iQ) = vq(j, l, iave, iQ) / zmasse(j, l) |
175 |
zvQ(j, l, itot, iQ) = zvQ(j, l, itot, iQ)*zfactv(j, l) |
vq(j, l, itot, iQ) = vq(j, l, itot, iQ) * factv(j, l) |
176 |
zvQtmp(j, l) = zvQtmp(j, l)*zfactv(j, l) |
vqtmp(j, l) = vqtmp(j, l) * factv(j, l) |
177 |
zvQ(j, l, immc, iQ) = zv(j, l)*zvQ(j, l, iave, iQ)*zfactv(j, l) |
vq(j, l, immc, iQ) = v(j, l) * vq(j, l, iave, iQ) * factv(j, l) |
178 |
zvQ(j, l, itrs, iQ) = zvQ(j, l, itot, iQ)-zvQtmp(j, l) |
vq(j, l, itrs, iQ) = vq(j, l, itot, iQ) - vqtmp(j, l) |
179 |
zvQ(j, l, istn, iQ) = zvQtmp(j, l)-zvQ(j, l, immc, iQ) |
vq(j, l, istn, iQ) = vqtmp(j, l) - vq(j, l, immc, iQ) |
180 |
enddo |
enddo |
181 |
enddo |
enddo |
182 |
! fonction de courant meridienne pour la quantite Q |
! Fonction de courant m\'eridienne pour la quantit\'e Q |
183 |
do l = llm, 1, -1 |
do l = llm, 1, -1 |
184 |
do j = 1, jjm |
do j = 1, jjm |
185 |
psiQ(j, l, iQ) = psiQ(j, l + 1, iQ) + zvQ(j, l, itot, iQ) |
psiQ(j, l, iQ) = psiQ(j, l + 1, iQ) + vq(j, l, itot, iQ) |
186 |
enddo |
enddo |
187 |
enddo |
enddo |
188 |
enddo |
enddo |
189 |
|
|
190 |
! fonction de courant pour la circulation meridienne moyenne |
! Fonction de courant pour la circulation m\'eridienne moyenne |
191 |
psi = 0. |
psi = 0. |
192 |
do l = llm, 1, -1 |
do l = llm, 1, -1 |
193 |
do j = 1, jjm |
do j = 1, jjm |
194 |
psi(j, l) = psi(j, l + 1) + zv(j, l) |
psi(j, l) = psi(j, l + 1) + v(j, l) |
195 |
zv(j, l) = zv(j, l)*zfactv(j, l) |
v(j, l) = v(j, l) * factv(j, l) |
196 |
enddo |
enddo |
197 |
enddo |
enddo |
198 |
|
|
199 |
! sorties proprement dites |
! Sorties proprement dites |
200 |
do iQ = 1, nQ |
do iQ = 1, nQ |
201 |
do itr = 1, ntr |
do itr = 1, ntr |
202 |
call histwrite(fileid, znom(itr, iQ), itau, zvQ(:, :, itr, iQ)) |
call histwrite(fileid, znom(itr, iQ), itau, vq(:, :, itr, iQ)) |
203 |
enddo |
enddo |
204 |
call histwrite(fileid, 'psi'//nom(iQ), itau, psiQ(:, :llm, iQ)) |
call histwrite(fileid, 'psi' // nom(iQ), itau, psiQ(:, :llm, iQ)) |
205 |
enddo |
enddo |
206 |
|
|
207 |
call histwrite(fileid, 'masse', itau, zmasse) |
call histwrite(fileid, 'masse', itau, zmasse) |
208 |
call histwrite(fileid, 'v', itau, zv) |
call histwrite(fileid, 'v', itau, v) |
209 |
psi = psi*1.e-9 |
psi = psi * 1e-9 |
210 |
call histwrite(fileid, 'psi', itau, psi(:, :llm)) |
call histwrite(fileid, 'psi', itau, psi(:, :llm)) |
211 |
|
|
212 |
! Moyenne verticale |
! Int\'egrale verticale |
213 |
|
|
214 |
forall (iQ = 1: nQ, itr = 2: ntr) zavQ(:, itr, iQ) & |
forall (iQ = 1: nQ, itr = 2: ntr) avq(:, itr, iQ) & |
215 |
= sum(zvQ(:, :, itr, iQ) * zmasse, dim=2) / sum(zmasse, dim=2) |
= sum(vq(:, :, itr, iQ) * zmasse, dim=2) / cv_2d(1, :) |
216 |
|
|
217 |
do iQ = 1, nQ |
do iQ = 1, nQ |
218 |
do itr = 2, ntr |
do itr = 2, ntr |
219 |
call histwrite(fileid, 'a'//znom(itr, iQ), itau, zavQ(:, itr, iQ)) |
call histwrite(fileid, 'a' // znom(itr, iQ), itau, avq(:, itr, iQ)) |
220 |
enddo |
enddo |
221 |
enddo |
enddo |
222 |
|
|
|
! On doit pouvoir tracer systematiquement la fonction de courant. |
|
223 |
icum = 0 |
icum = 0 |
224 |
endif writing_step |
endif writing_step |
225 |
|
|