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guez |
47 |
SUBROUTINE thermcell(ngrid, nlay, ptimestep, pplay, pplev, pphi, pu, pv, pt, & |
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po, pduadj, pdvadj, pdtadj, pdoadj, fm0, entr0, r_aspect, l_mix, w2di, tho) |
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guez |
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guez |
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use dimens_m |
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use dimphy |
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use SUPHEC_M |
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IMPLICIT NONE |
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|
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! Calcul du transport verticale dans la couche limite en presence |
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! de "thermiques" explicitement representes |
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guez |
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|
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guez |
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! Réécriture à partir d'un listing papier à Habas, le 14/02/00 |
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guez |
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|
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guez |
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! le thermique est supposé homogène et dissipé par mélange avec |
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! son environnement. la longueur l_mix contrôle l'efficacité du |
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! mélange |
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|
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guez |
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! Le calcul du transport des différentes espèces se fait en prenant |
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! en compte: |
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! 1. un flux de masse montant |
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! 2. un flux de masse descendant |
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! 3. un entrainement |
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! 4. un detrainement |
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guez |
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guez |
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! arguments: |
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guez |
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guez |
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INTEGER ngrid, nlay, w2di, tho |
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real ptimestep, l_mix, r_aspect |
30 |
guez |
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REAL, intent(in):: pt(ngrid, nlay) |
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real pdtadj(ngrid, nlay) |
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guez |
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REAL pu(ngrid, nlay), pduadj(ngrid, nlay) |
33 |
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REAL pv(ngrid, nlay), pdvadj(ngrid, nlay) |
34 |
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REAL po(ngrid, nlay), pdoadj(ngrid, nlay) |
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REAL, intent(in):: pplay(ngrid, nlay) |
36 |
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real, intent(in):: pplev(ngrid, nlay+1) |
37 |
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real, intent(in):: pphi(ngrid, nlay) |
38 |
guez |
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39 |
guez |
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integer idetr |
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save idetr |
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data idetr/3/ |
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guez |
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43 |
guez |
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! local: |
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guez |
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|
45 |
guez |
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INTEGER ig, k, l, lmaxa(klon), lmix(klon) |
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real zsortie1d(klon) |
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! CR: on remplace lmax(klon, klev+1) |
48 |
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INTEGER lmax(klon), lmin(klon), lentr(klon) |
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real linter(klon) |
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real zmix(klon), fracazmix(klon) |
51 |
guez |
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52 |
guez |
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real zmax(klon), zw, zz, zw2(klon, klev+1), ztva(klon, klev), zzz |
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guez |
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|
54 |
guez |
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real zlev(klon, klev+1), zlay(klon, klev) |
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REAL zh(klon, klev), zdhadj(klon, klev) |
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REAL ztv(klon, klev) |
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real zu(klon, klev), zv(klon, klev), zo(klon, klev) |
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REAL wh(klon, klev+1) |
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real wu(klon, klev+1), wv(klon, klev+1), wo(klon, klev+1) |
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real zla(klon, klev+1) |
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real zwa(klon, klev+1) |
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real zld(klon, klev+1) |
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real zwd(klon, klev+1) |
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real zsortie(klon, klev) |
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real zva(klon, klev) |
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real zua(klon, klev) |
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real zoa(klon, klev) |
68 |
guez |
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|
69 |
guez |
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real zha(klon, klev) |
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real wa_moy(klon, klev+1) |
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real fraca(klon, klev+1) |
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real fracc(klon, klev+1) |
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real zf, zf2 |
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real thetath2(klon, klev), wth2(klon, klev) |
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common/comtherm/thetath2, wth2 |
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guez |
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77 |
guez |
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real count_time |
78 |
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integer isplit, nsplit, ialt |
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parameter (nsplit=10) |
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data isplit/0/ |
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save isplit |
82 |
guez |
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83 |
guez |
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logical sorties |
84 |
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real rho(klon, klev), rhobarz(klon, klev+1), masse(klon, klev) |
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real zpspsk(klon, klev) |
86 |
guez |
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87 |
guez |
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real wmax(klon), wmaxa(klon) |
88 |
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real wa(klon, klev, klev+1) |
89 |
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real wd(klon, klev+1) |
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real larg_part(klon, klev, klev+1) |
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real fracd(klon, klev+1) |
92 |
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real xxx(klon, klev+1) |
93 |
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real larg_cons(klon, klev+1) |
94 |
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real larg_detr(klon, klev+1) |
95 |
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real fm0(klon, klev+1), entr0(klon, klev), detr(klon, klev) |
96 |
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real pu_therm(klon, klev), pv_therm(klon, klev) |
97 |
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real fm(klon, klev+1), entr(klon, klev) |
98 |
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real fmc(klon, klev+1) |
99 |
guez |
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100 |
guez |
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!CR:nouvelles variables |
101 |
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real f_star(klon, klev+1), entr_star(klon, klev) |
102 |
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real entr_star_tot(klon), entr_star2(klon) |
103 |
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real f(klon), f0(klon) |
104 |
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real zlevinter(klon) |
105 |
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logical first |
106 |
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data first /.false./ |
107 |
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save first |
108 |
guez |
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109 |
guez |
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character*2 str2 |
110 |
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character*10 str10 |
111 |
guez |
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|
112 |
guez |
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LOGICAL vtest(klon), down |
113 |
guez |
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|
114 |
guez |
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EXTERNAL SCOPY |
115 |
guez |
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116 |
guez |
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integer ncorrec, ll |
117 |
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save ncorrec |
118 |
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data ncorrec/0/ |
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guez |
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|
120 |
guez |
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!----------------------------------------------------------------------- |
121 |
guez |
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|
122 |
guez |
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! initialisation: |
123 |
guez |
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|
124 |
guez |
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sorties=.true. |
125 |
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IF(ngrid.NE.klon) THEN |
126 |
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PRINT * |
127 |
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PRINT *, 'STOP dans convadj' |
128 |
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PRINT *, 'ngrid =', ngrid |
129 |
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PRINT *, 'klon =', klon |
130 |
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ENDIF |
131 |
guez |
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|
132 |
guez |
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! incrementation eventuelle de tendances precedentes: |
133 |
guez |
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|
134 |
guez |
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print *, '0 OK convect8' |
135 |
guez |
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|
136 |
guez |
47 |
DO l=1, nlay |
137 |
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DO ig=1, ngrid |
138 |
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zpspsk(ig, l)=(pplay(ig, l)/pplev(ig, 1))**RKAPPA |
139 |
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zh(ig, l)=pt(ig, l)/zpspsk(ig, l) |
140 |
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zu(ig, l)=pu(ig, l) |
141 |
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zv(ig, l)=pv(ig, l) |
142 |
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zo(ig, l)=po(ig, l) |
143 |
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ztv(ig, l)=zh(ig, l)*(1.+0.61*zo(ig, l)) |
144 |
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end DO |
145 |
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end DO |
146 |
guez |
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|
147 |
guez |
47 |
print *, '1 OK convect8' |
148 |
guez |
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|
149 |
guez |
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! + + + + + + + + + + + |
150 |
guez |
3 |
|
151 |
guez |
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! wa, fraca, wd, fracd -------------------- zlev(2), rhobarz |
152 |
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! wh, wt, wo ... |
153 |
guez |
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|
154 |
guez |
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! + + + + + + + + + + + zh, zu, zv, zo, rho |
155 |
guez |
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|
156 |
guez |
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! -------------------- zlev(1) |
157 |
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! \\\\\\\\\\\\\\\\\\\\ |
158 |
guez |
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|
159 |
guez |
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! Calcul des altitudes des couches |
160 |
guez |
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|
161 |
guez |
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do l=2, nlay |
162 |
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do ig=1, ngrid |
163 |
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zlev(ig, l)=0.5*(pphi(ig, l)+pphi(ig, l-1))/RG |
164 |
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enddo |
165 |
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enddo |
166 |
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do ig=1, ngrid |
167 |
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zlev(ig, 1)=0. |
168 |
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zlev(ig, nlay+1)=(2.*pphi(ig, klev)-pphi(ig, klev-1))/RG |
169 |
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enddo |
170 |
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do l=1, nlay |
171 |
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do ig=1, ngrid |
172 |
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zlay(ig, l)=pphi(ig, l)/RG |
173 |
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enddo |
174 |
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enddo |
175 |
guez |
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|
176 |
guez |
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! Calcul des densites |
177 |
guez |
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|
178 |
guez |
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do l=1, nlay |
179 |
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do ig=1, ngrid |
180 |
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rho(ig, l)=pplay(ig, l)/(zpspsk(ig, l)*RD*zh(ig, l)) |
181 |
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enddo |
182 |
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enddo |
183 |
guez |
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184 |
guez |
47 |
do l=2, nlay |
185 |
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do ig=1, ngrid |
186 |
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rhobarz(ig, l)=0.5*(rho(ig, l)+rho(ig, l-1)) |
187 |
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enddo |
188 |
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enddo |
189 |
guez |
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190 |
guez |
47 |
do k=1, nlay |
191 |
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do l=1, nlay+1 |
192 |
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do ig=1, ngrid |
193 |
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wa(ig, k, l)=0. |
194 |
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enddo |
195 |
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enddo |
196 |
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enddo |
197 |
guez |
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|
198 |
guez |
47 |
! Calcul de w2, quarre de w a partir de la cape |
199 |
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! a partir de w2, on calcule wa, vitesse de l'ascendance |
200 |
guez |
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|
201 |
guez |
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! ATTENTION: Dans cette version, pour cause d'economie de memoire, |
202 |
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! w2 est stoke dans wa |
203 |
guez |
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|
204 |
guez |
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! ATTENTION: dans convect8, on n'utilise le calcule des wa |
205 |
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! independants par couches que pour calculer l'entrainement |
206 |
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! a la base et la hauteur max de l'ascendance. |
207 |
guez |
3 |
|
208 |
guez |
47 |
! Indicages: |
209 |
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! l'ascendance provenant du niveau k traverse l'interface l avec |
210 |
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! une vitesse wa(k, l). |
211 |
guez |
3 |
|
212 |
guez |
47 |
! -------------------- |
213 |
guez |
3 |
|
214 |
guez |
47 |
! + + + + + + + + + + |
215 |
guez |
3 |
|
216 |
guez |
47 |
! wa(k, l) ---- -------------------- l |
217 |
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! /\ |
218 |
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! /||\ + + + + + + + + + + |
219 |
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! || |
220 |
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! || -------------------- |
221 |
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! || |
222 |
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! || + + + + + + + + + + |
223 |
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! || |
224 |
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! || -------------------- |
225 |
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! ||__ |
226 |
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! |___ + + + + + + + + + + k |
227 |
guez |
3 |
|
228 |
guez |
47 |
! -------------------- |
229 |
guez |
3 |
|
230 |
guez |
47 |
!CR: ponderation entrainement des couches instables |
231 |
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!def des entr_star tels que entr=f*entr_star |
232 |
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do l=1, klev |
233 |
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do ig=1, ngrid |
234 |
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entr_star(ig, l)=0. |
235 |
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enddo |
236 |
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enddo |
237 |
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! determination de la longueur de la couche d entrainement |
238 |
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do ig=1, ngrid |
239 |
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lentr(ig)=1 |
240 |
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enddo |
241 |
guez |
3 |
|
242 |
guez |
47 |
!on ne considere que les premieres couches instables |
243 |
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do k=nlay-2, 1, -1 |
244 |
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do ig=1, ngrid |
245 |
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if (ztv(ig, k).gt.ztv(ig, k+1).and. & |
246 |
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ztv(ig, k+1).le.ztv(ig, k+2)) then |
247 |
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lentr(ig)=k |
248 |
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endif |
249 |
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enddo |
250 |
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enddo |
251 |
guez |
3 |
|
252 |
guez |
47 |
! determination du lmin: couche d ou provient le thermique |
253 |
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do ig=1, ngrid |
254 |
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lmin(ig)=1 |
255 |
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enddo |
256 |
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do ig=1, ngrid |
257 |
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do l=nlay, 2, -1 |
258 |
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if (ztv(ig, l-1).gt.ztv(ig, l)) then |
259 |
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lmin(ig)=l-1 |
260 |
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endif |
261 |
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enddo |
262 |
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enddo |
263 |
guez |
3 |
|
264 |
guez |
47 |
! definition de l'entrainement des couches |
265 |
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do l=1, klev-1 |
266 |
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do ig=1, ngrid |
267 |
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if (ztv(ig, l).gt.ztv(ig, l+1).and. & |
268 |
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l.ge.lmin(ig).and.l.le.lentr(ig)) then |
269 |
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entr_star(ig, l)=(ztv(ig, l)-ztv(ig, l+1))* & |
270 |
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(zlev(ig, l+1)-zlev(ig, l)) |
271 |
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endif |
272 |
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enddo |
273 |
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enddo |
274 |
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! pas de thermique si couches 1->5 stables |
275 |
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do ig=1, ngrid |
276 |
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if (lmin(ig).gt.5) then |
277 |
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do l=1, klev |
278 |
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entr_star(ig, l)=0. |
279 |
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enddo |
280 |
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endif |
281 |
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enddo |
282 |
|
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! calcul de l entrainement total |
283 |
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do ig=1, ngrid |
284 |
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entr_star_tot(ig)=0. |
285 |
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enddo |
286 |
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do ig=1, ngrid |
287 |
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do k=1, klev |
288 |
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entr_star_tot(ig)=entr_star_tot(ig)+entr_star(ig, k) |
289 |
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enddo |
290 |
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enddo |
291 |
guez |
3 |
|
292 |
guez |
47 |
print *, 'fin calcul entr_star' |
293 |
|
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do k=1, klev |
294 |
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do ig=1, ngrid |
295 |
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ztva(ig, k)=ztv(ig, k) |
296 |
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enddo |
297 |
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enddo |
298 |
guez |
3 |
|
299 |
guez |
47 |
do k=1, klev+1 |
300 |
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do ig=1, ngrid |
301 |
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zw2(ig, k)=0. |
302 |
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fmc(ig, k)=0. |
303 |
guez |
3 |
|
304 |
guez |
47 |
f_star(ig, k)=0. |
305 |
guez |
3 |
|
306 |
guez |
47 |
larg_cons(ig, k)=0. |
307 |
|
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larg_detr(ig, k)=0. |
308 |
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wa_moy(ig, k)=0. |
309 |
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enddo |
310 |
|
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enddo |
311 |
guez |
3 |
|
312 |
guez |
47 |
do ig=1, ngrid |
313 |
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linter(ig)=1. |
314 |
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lmaxa(ig)=1 |
315 |
|
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lmix(ig)=1 |
316 |
|
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wmaxa(ig)=0. |
317 |
|
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enddo |
318 |
guez |
3 |
|
319 |
guez |
47 |
do l=1, nlay-2 |
320 |
|
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do ig=1, ngrid |
321 |
|
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if (ztv(ig, l).gt.ztv(ig, l+1) & |
322 |
|
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.and.entr_star(ig, l).gt.1.e-10 & |
323 |
|
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.and.zw2(ig, l).lt.1e-10) then |
324 |
|
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f_star(ig, l+1)=entr_star(ig, l) |
325 |
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!test:calcul de dteta |
326 |
|
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zw2(ig, l+1)=2.*RG*(ztv(ig, l)-ztv(ig, l+1))/ztv(ig, l+1) & |
327 |
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*(zlev(ig, l+1)-zlev(ig, l)) & |
328 |
|
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*0.4*pphi(ig, l)/(pphi(ig, l+1)-pphi(ig, l)) |
329 |
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larg_detr(ig, l)=0. |
330 |
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else if ((zw2(ig, l).ge.1e-10).and. & |
331 |
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(f_star(ig, l)+entr_star(ig, l).gt.1.e-10)) then |
332 |
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f_star(ig, l+1)=f_star(ig, l)+entr_star(ig, l) |
333 |
|
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ztva(ig, l)=(f_star(ig, l)*ztva(ig, l-1)+entr_star(ig, l) & |
334 |
|
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*ztv(ig, l))/f_star(ig, l+1) |
335 |
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zw2(ig, l+1)=zw2(ig, l)*(f_star(ig, l)/f_star(ig, l+1))**2+ & |
336 |
|
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2.*RG*(ztva(ig, l)-ztv(ig, l))/ztv(ig, l) & |
337 |
|
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*(zlev(ig, l+1)-zlev(ig, l)) |
338 |
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endif |
339 |
|
|
! determination de zmax continu par interpolation lineaire |
340 |
|
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if (zw2(ig, l+1).lt.0.) then |
341 |
|
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if (abs(zw2(ig, l+1)-zw2(ig, l)).lt.1e-10) then |
342 |
|
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print *, 'pb linter' |
343 |
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endif |
344 |
|
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linter(ig)=(l*(zw2(ig, l+1)-zw2(ig, l)) & |
345 |
|
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-zw2(ig, l))/(zw2(ig, l+1)-zw2(ig, l)) |
346 |
|
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zw2(ig, l+1)=0. |
347 |
|
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lmaxa(ig)=l |
348 |
|
|
else |
349 |
|
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if (zw2(ig, l+1).lt.0.) then |
350 |
|
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print *, 'pb1 zw2<0' |
351 |
|
|
endif |
352 |
|
|
wa_moy(ig, l+1)=sqrt(zw2(ig, l+1)) |
353 |
|
|
endif |
354 |
|
|
if (wa_moy(ig, l+1).gt.wmaxa(ig)) then |
355 |
|
|
! lmix est le niveau de la couche ou w (wa_moy) est maximum |
356 |
|
|
lmix(ig)=l+1 |
357 |
|
|
wmaxa(ig)=wa_moy(ig, l+1) |
358 |
|
|
endif |
359 |
|
|
enddo |
360 |
|
|
enddo |
361 |
|
|
print *, 'fin calcul zw2' |
362 |
guez |
3 |
|
363 |
guez |
47 |
! Calcul de la couche correspondant a la hauteur du thermique |
364 |
|
|
do ig=1, ngrid |
365 |
|
|
lmax(ig)=lentr(ig) |
366 |
|
|
enddo |
367 |
|
|
do ig=1, ngrid |
368 |
|
|
do l=nlay, lentr(ig)+1, -1 |
369 |
|
|
if (zw2(ig, l).le.1.e-10) then |
370 |
|
|
lmax(ig)=l-1 |
371 |
|
|
endif |
372 |
|
|
enddo |
373 |
|
|
enddo |
374 |
|
|
! pas de thermique si couches 1->5 stables |
375 |
|
|
do ig=1, ngrid |
376 |
|
|
if (lmin(ig).gt.5) then |
377 |
|
|
lmax(ig)=1 |
378 |
|
|
lmin(ig)=1 |
379 |
|
|
endif |
380 |
|
|
enddo |
381 |
guez |
3 |
|
382 |
guez |
47 |
! Determination de zw2 max |
383 |
|
|
do ig=1, ngrid |
384 |
|
|
wmax(ig)=0. |
385 |
|
|
enddo |
386 |
guez |
3 |
|
387 |
guez |
47 |
do l=1, nlay |
388 |
|
|
do ig=1, ngrid |
389 |
|
|
if (l.le.lmax(ig)) then |
390 |
|
|
if (zw2(ig, l).lt.0.)then |
391 |
|
|
print *, 'pb2 zw2<0' |
392 |
|
|
endif |
393 |
|
|
zw2(ig, l)=sqrt(zw2(ig, l)) |
394 |
|
|
wmax(ig)=max(wmax(ig), zw2(ig, l)) |
395 |
|
|
else |
396 |
|
|
zw2(ig, l)=0. |
397 |
|
|
endif |
398 |
|
|
enddo |
399 |
|
|
enddo |
400 |
guez |
3 |
|
401 |
guez |
47 |
! Longueur caracteristique correspondant a la hauteur des thermiques. |
402 |
|
|
do ig=1, ngrid |
403 |
|
|
zmax(ig)=0. |
404 |
|
|
zlevinter(ig)=zlev(ig, 1) |
405 |
|
|
enddo |
406 |
|
|
do ig=1, ngrid |
407 |
|
|
! calcul de zlevinter |
408 |
|
|
zlevinter(ig)=(zlev(ig, lmax(ig)+1)-zlev(ig, lmax(ig)))* & |
409 |
|
|
linter(ig)+zlev(ig, lmax(ig))-lmax(ig)*(zlev(ig, lmax(ig)+1) & |
410 |
|
|
-zlev(ig, lmax(ig))) |
411 |
|
|
zmax(ig)=max(zmax(ig), zlevinter(ig)-zlev(ig, lmin(ig))) |
412 |
|
|
enddo |
413 |
guez |
3 |
|
414 |
guez |
47 |
print *, 'avant fermeture' |
415 |
|
|
! Fermeture, determination de f |
416 |
|
|
do ig=1, ngrid |
417 |
|
|
entr_star2(ig)=0. |
418 |
|
|
enddo |
419 |
|
|
do ig=1, ngrid |
420 |
|
|
if (entr_star_tot(ig).LT.1.e-10) then |
421 |
|
|
f(ig)=0. |
422 |
|
|
else |
423 |
|
|
do k=lmin(ig), lentr(ig) |
424 |
|
|
entr_star2(ig)=entr_star2(ig)+entr_star(ig, k)**2 & |
425 |
|
|
/(rho(ig, k)*(zlev(ig, k+1)-zlev(ig, k))) |
426 |
|
|
enddo |
427 |
|
|
! Nouvelle fermeture |
428 |
|
|
f(ig)=wmax(ig)/(max(500., zmax(ig))*r_aspect & |
429 |
|
|
*entr_star2(ig))*entr_star_tot(ig) |
430 |
|
|
endif |
431 |
|
|
enddo |
432 |
|
|
print *, 'apres fermeture' |
433 |
guez |
3 |
|
434 |
guez |
47 |
! Calcul de l'entrainement |
435 |
|
|
do k=1, klev |
436 |
|
|
do ig=1, ngrid |
437 |
|
|
entr(ig, k)=f(ig)*entr_star(ig, k) |
438 |
|
|
enddo |
439 |
|
|
enddo |
440 |
|
|
! Calcul des flux |
441 |
|
|
do ig=1, ngrid |
442 |
|
|
do l=1, lmax(ig)-1 |
443 |
|
|
fmc(ig, l+1)=fmc(ig, l)+entr(ig, l) |
444 |
|
|
enddo |
445 |
|
|
enddo |
446 |
guez |
3 |
|
447 |
guez |
47 |
! determination de l'indice du debut de la mixed layer ou w decroit |
448 |
guez |
3 |
|
449 |
guez |
47 |
! calcul de la largeur de chaque ascendance dans le cas conservatif. |
450 |
|
|
! dans ce cas simple, on suppose que la largeur de l'ascendance provenant |
451 |
|
|
! d'une couche est égale à la hauteur de la couche alimentante. |
452 |
|
|
! La vitesse maximale dans l'ascendance est aussi prise comme estimation |
453 |
|
|
! de la vitesse d'entrainement horizontal dans la couche alimentante. |
454 |
guez |
3 |
|
455 |
guez |
47 |
do l=2, nlay |
456 |
|
|
do ig=1, ngrid |
457 |
|
|
if (l.le.lmaxa(ig)) then |
458 |
|
|
zw=max(wa_moy(ig, l), 1.e-10) |
459 |
|
|
larg_cons(ig, l)=zmax(ig)*r_aspect & |
460 |
|
|
*fmc(ig, l)/(rhobarz(ig, l)*zw) |
461 |
|
|
endif |
462 |
|
|
enddo |
463 |
|
|
enddo |
464 |
guez |
3 |
|
465 |
guez |
47 |
do l=2, nlay |
466 |
|
|
do ig=1, ngrid |
467 |
|
|
if (l.le.lmaxa(ig)) then |
468 |
|
|
if ((l_mix*zlev(ig, l)).lt.0.)then |
469 |
|
|
print *, 'pb l_mix*zlev<0' |
470 |
|
|
endif |
471 |
|
|
larg_detr(ig, l)=sqrt(l_mix*zlev(ig, l)) |
472 |
|
|
endif |
473 |
|
|
enddo |
474 |
|
|
enddo |
475 |
guez |
3 |
|
476 |
guez |
47 |
! calcul de la fraction de la maille concernée par l'ascendance en tenant |
477 |
|
|
! compte de l'epluchage du thermique. |
478 |
guez |
3 |
|
479 |
guez |
47 |
!CR def de zmix continu (profil parabolique des vitesses) |
480 |
|
|
do ig=1, ngrid |
481 |
|
|
if (lmix(ig).gt.1.) then |
482 |
|
|
if (((zw2(ig, lmix(ig)-1)-zw2(ig, lmix(ig))) & |
483 |
|
|
*((zlev(ig, lmix(ig)))-(zlev(ig, lmix(ig)+1))) & |
484 |
|
|
-(zw2(ig, lmix(ig))-zw2(ig, lmix(ig)+1)) & |
485 |
|
|
*((zlev(ig, lmix(ig)-1))-(zlev(ig, lmix(ig))))).gt.1e-10) & |
486 |
|
|
then |
487 |
guez |
3 |
|
488 |
guez |
47 |
zmix(ig)=((zw2(ig, lmix(ig)-1)-zw2(ig, lmix(ig))) & |
489 |
|
|
*((zlev(ig, lmix(ig)))**2-(zlev(ig, lmix(ig)+1))**2) & |
490 |
|
|
-(zw2(ig, lmix(ig))-zw2(ig, lmix(ig)+1)) & |
491 |
|
|
*((zlev(ig, lmix(ig)-1))**2-(zlev(ig, lmix(ig)))**2)) & |
492 |
|
|
/(2.*((zw2(ig, lmix(ig)-1)-zw2(ig, lmix(ig))) & |
493 |
|
|
*((zlev(ig, lmix(ig)))-(zlev(ig, lmix(ig)+1))) & |
494 |
|
|
-(zw2(ig, lmix(ig))-zw2(ig, lmix(ig)+1)) & |
495 |
|
|
*((zlev(ig, lmix(ig)-1))-(zlev(ig, lmix(ig)))))) |
496 |
|
|
else |
497 |
|
|
zmix(ig)=zlev(ig, lmix(ig)) |
498 |
|
|
print *, 'pb zmix' |
499 |
|
|
endif |
500 |
|
|
else |
501 |
|
|
zmix(ig)=0. |
502 |
|
|
endif |
503 |
guez |
3 |
|
504 |
guez |
47 |
if ((zmax(ig)-zmix(ig)).lt.0.) then |
505 |
|
|
zmix(ig)=0.99*zmax(ig) |
506 |
|
|
endif |
507 |
|
|
enddo |
508 |
guez |
3 |
|
509 |
guez |
47 |
! calcul du nouveau lmix correspondant |
510 |
|
|
do ig=1, ngrid |
511 |
|
|
do l=1, klev |
512 |
|
|
if (zmix(ig).ge.zlev(ig, l).and. & |
513 |
|
|
zmix(ig).lt.zlev(ig, l+1)) then |
514 |
|
|
lmix(ig)=l |
515 |
|
|
endif |
516 |
|
|
enddo |
517 |
|
|
enddo |
518 |
guez |
3 |
|
519 |
guez |
47 |
do l=2, nlay |
520 |
|
|
do ig=1, ngrid |
521 |
|
|
if(larg_cons(ig, l).gt.1.) then |
522 |
|
|
fraca(ig, l)=(larg_cons(ig, l)-larg_detr(ig, l)) & |
523 |
|
|
/(r_aspect*zmax(ig)) |
524 |
|
|
fraca(ig, l)=max(fraca(ig, l), 0.) |
525 |
|
|
fraca(ig, l)=min(fraca(ig, l), 0.5) |
526 |
|
|
fracd(ig, l)=1.-fraca(ig, l) |
527 |
|
|
fracc(ig, l)=larg_cons(ig, l)/(r_aspect*zmax(ig)) |
528 |
|
|
else |
529 |
|
|
fraca(ig, l)=0. |
530 |
|
|
fracc(ig, l)=0. |
531 |
|
|
fracd(ig, l)=1. |
532 |
|
|
endif |
533 |
|
|
enddo |
534 |
|
|
enddo |
535 |
|
|
!CR: calcul de fracazmix |
536 |
|
|
do ig=1, ngrid |
537 |
|
|
fracazmix(ig)=(fraca(ig, lmix(ig)+1)-fraca(ig, lmix(ig)))/ & |
538 |
|
|
(zlev(ig, lmix(ig)+1)-zlev(ig, lmix(ig)))*zmix(ig) & |
539 |
|
|
+fraca(ig, lmix(ig))-zlev(ig, lmix(ig))*(fraca(ig, lmix(ig)+1) & |
540 |
|
|
-fraca(ig, lmix(ig)))/(zlev(ig, lmix(ig)+1)-zlev(ig, lmix(ig))) |
541 |
|
|
enddo |
542 |
guez |
3 |
|
543 |
guez |
47 |
do l=2, nlay |
544 |
|
|
do ig=1, ngrid |
545 |
|
|
if(larg_cons(ig, l).gt.1.) then |
546 |
|
|
if (l.gt.lmix(ig)) then |
547 |
|
|
if (zmax(ig)-zmix(ig).lt.1.e-10) then |
548 |
|
|
xxx(ig, l)=(lmaxa(ig)+1.-l)/(lmaxa(ig)+1.-lmix(ig)) |
549 |
|
|
else |
550 |
|
|
xxx(ig, l)=(zmax(ig)-zlev(ig, l))/(zmax(ig)-zmix(ig)) |
551 |
|
|
endif |
552 |
|
|
if (idetr.eq.0) then |
553 |
|
|
fraca(ig, l)=fracazmix(ig) |
554 |
|
|
else if (idetr.eq.1) then |
555 |
|
|
fraca(ig, l)=fracazmix(ig)*xxx(ig, l) |
556 |
|
|
else if (idetr.eq.2) then |
557 |
|
|
fraca(ig, l)=fracazmix(ig)*(1.-(1.-xxx(ig, l))**2) |
558 |
|
|
else |
559 |
|
|
fraca(ig, l)=fracazmix(ig)*xxx(ig, l)**2 |
560 |
|
|
endif |
561 |
|
|
fraca(ig, l)=max(fraca(ig, l), 0.) |
562 |
|
|
fraca(ig, l)=min(fraca(ig, l), 0.5) |
563 |
|
|
fracd(ig, l)=1.-fraca(ig, l) |
564 |
|
|
fracc(ig, l)=larg_cons(ig, l)/(r_aspect*zmax(ig)) |
565 |
|
|
endif |
566 |
|
|
endif |
567 |
|
|
enddo |
568 |
|
|
enddo |
569 |
guez |
3 |
|
570 |
guez |
47 |
print *, 'fin calcul fraca' |
571 |
guez |
3 |
|
572 |
guez |
47 |
! Calcul de fracd, wd |
573 |
|
|
! somme wa - wd = 0 |
574 |
guez |
3 |
|
575 |
guez |
47 |
do ig=1, ngrid |
576 |
|
|
fm(ig, 1)=0. |
577 |
|
|
fm(ig, nlay+1)=0. |
578 |
|
|
enddo |
579 |
guez |
3 |
|
580 |
guez |
47 |
do l=2, nlay |
581 |
|
|
do ig=1, ngrid |
582 |
|
|
fm(ig, l)=fraca(ig, l)*wa_moy(ig, l)*rhobarz(ig, l) |
583 |
|
|
if (entr(ig, l-1).lt.1e-10.and.fm(ig, l).gt.fm(ig, l-1) & |
584 |
|
|
.and.l.gt.lmix(ig)) then |
585 |
|
|
fm(ig, l)=fm(ig, l-1) |
586 |
|
|
endif |
587 |
|
|
enddo |
588 |
|
|
do ig=1, ngrid |
589 |
|
|
if(fracd(ig, l).lt.0.1) then |
590 |
|
|
stop'fracd trop petit' |
591 |
|
|
else |
592 |
|
|
! vitesse descendante "diagnostique" |
593 |
|
|
wd(ig, l)=fm(ig, l)/(fracd(ig, l)*rhobarz(ig, l)) |
594 |
|
|
endif |
595 |
|
|
enddo |
596 |
|
|
enddo |
597 |
guez |
3 |
|
598 |
guez |
47 |
do l=1, nlay |
599 |
|
|
do ig=1, ngrid |
600 |
|
|
masse(ig, l)=(pplev(ig, l)-pplev(ig, l+1))/RG |
601 |
|
|
enddo |
602 |
|
|
enddo |
603 |
guez |
3 |
|
604 |
guez |
47 |
print *, '12 OK convect8' |
605 |
guez |
3 |
|
606 |
guez |
47 |
! calcul du transport vertical |
607 |
guez |
3 |
|
608 |
guez |
47 |
!CR:redefinition du entr |
609 |
|
|
do l=1, nlay |
610 |
|
|
do ig=1, ngrid |
611 |
|
|
detr(ig, l)=fm(ig, l)+entr(ig, l)-fm(ig, l+1) |
612 |
|
|
if (detr(ig, l).lt.0.) then |
613 |
|
|
entr(ig, l)=entr(ig, l)-detr(ig, l) |
614 |
|
|
detr(ig, l)=0. |
615 |
|
|
endif |
616 |
|
|
enddo |
617 |
|
|
enddo |
618 |
guez |
3 |
|
619 |
guez |
47 |
if (w2di.eq.1) then |
620 |
|
|
fm0=fm0+ptimestep*(fm-fm0)/float(tho) |
621 |
|
|
entr0=entr0+ptimestep*(entr-entr0)/float(tho) |
622 |
|
|
else |
623 |
|
|
fm0=fm |
624 |
|
|
entr0=entr |
625 |
|
|
endif |
626 |
guez |
3 |
|
627 |
guez |
47 |
if (1.eq.1) then |
628 |
|
|
call dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse & |
629 |
|
|
, zh, zdhadj, zha) |
630 |
|
|
call dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse & |
631 |
|
|
, zo, pdoadj, zoa) |
632 |
|
|
else |
633 |
|
|
call dqthermcell2(ngrid, nlay, ptimestep, fm0, entr0, masse, fraca & |
634 |
|
|
, zh, zdhadj, zha) |
635 |
|
|
call dqthermcell2(ngrid, nlay, ptimestep, fm0, entr0, masse, fraca & |
636 |
|
|
, zo, pdoadj, zoa) |
637 |
|
|
endif |
638 |
guez |
3 |
|
639 |
guez |
47 |
if (1.eq.0) then |
640 |
|
|
call dvthermcell2(ngrid, nlay, ptimestep, fm0, entr0, masse & |
641 |
|
|
, fraca, zmax & |
642 |
|
|
, zu, zv, pduadj, pdvadj, zua, zva) |
643 |
|
|
else |
644 |
|
|
call dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse & |
645 |
|
|
, zu, pduadj, zua) |
646 |
|
|
call dqthermcell(ngrid, nlay, ptimestep, fm0, entr0, masse & |
647 |
|
|
, zv, pdvadj, zva) |
648 |
|
|
endif |
649 |
guez |
3 |
|
650 |
guez |
47 |
do l=1, nlay |
651 |
|
|
do ig=1, ngrid |
652 |
|
|
zf=0.5*(fracc(ig, l)+fracc(ig, l+1)) |
653 |
|
|
zf2=zf/(1.-zf) |
654 |
|
|
thetath2(ig, l)=zf2*(zha(ig, l)-zh(ig, l))**2 |
655 |
|
|
wth2(ig, l)=zf2*(0.5*(wa_moy(ig, l)+wa_moy(ig, l+1)))**2 |
656 |
|
|
enddo |
657 |
|
|
enddo |
658 |
guez |
3 |
|
659 |
guez |
47 |
do l=1, nlay |
660 |
|
|
do ig=1, ngrid |
661 |
|
|
pdtadj(ig, l)=zdhadj(ig, l)*zpspsk(ig, l) |
662 |
|
|
enddo |
663 |
|
|
enddo |
664 |
guez |
3 |
|
665 |
guez |
47 |
print *, '14 OK convect8' |
666 |
guez |
3 |
|
667 |
guez |
47 |
! Calculs pour les sorties |
668 |
guez |
3 |
|
669 |
guez |
47 |
if(sorties) then |
670 |
|
|
do l=1, nlay |
671 |
|
|
do ig=1, ngrid |
672 |
|
|
zla(ig, l)=(1.-fracd(ig, l))*zmax(ig) |
673 |
|
|
zld(ig, l)=fracd(ig, l)*zmax(ig) |
674 |
|
|
if(1.-fracd(ig, l).gt.1.e-10) & |
675 |
|
|
zwa(ig, l)=wd(ig, l)*fracd(ig, l)/(1.-fracd(ig, l)) |
676 |
|
|
enddo |
677 |
|
|
enddo |
678 |
guez |
3 |
|
679 |
guez |
47 |
isplit=isplit+1 |
680 |
|
|
endif |
681 |
guez |
3 |
|
682 |
guez |
47 |
print *, '19 OK convect8' |
683 |
guez |
3 |
|
684 |
guez |
47 |
end SUBROUTINE thermcell |