[878] | 1 | ! |
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[1403] | 2 | ! $Id: thermcell_main.F90 1403 2010-07-01 09:02:53Z lfalletti $ |
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[878] | 3 | ! |
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[972] | 4 | SUBROUTINE thermcell_main(itap,ngrid,nlay,ptimestep & |
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[878] | 5 | & ,pplay,pplev,pphi,debut & |
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| 6 | & ,pu,pv,pt,po & |
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| 7 | & ,pduadj,pdvadj,pdtadj,pdoadj & |
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[1026] | 8 | & ,fm0,entr0,detr0,zqta,zqla,lmax & |
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[878] | 9 | & ,ratqscth,ratqsdiff,zqsatth & |
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[1403] | 10 | & ,r_aspect,l_mix,tau_thermals,iflag_thermals_ed & |
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[927] | 11 | & ,Ale_bl,Alp_bl,lalim_conv,wght_th & |
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[1403] | 12 | & ,zmax0, f0,zw2,fraca,ztv & |
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| 13 | & ,zpspsk,ztla,zthl) |
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[878] | 14 | |
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[972] | 15 | USE dimphy |
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[1026] | 16 | USE comgeomphy , ONLY:rlond,rlatd |
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[878] | 17 | IMPLICIT NONE |
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| 18 | |
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| 19 | !======================================================================= |
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| 20 | ! Auteurs: Frederic Hourdin, Catherine Rio, Anne Mathieu |
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| 21 | ! Version du 09.02.07 |
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| 22 | ! Calcul du transport vertical dans la couche limite en presence |
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| 23 | ! de "thermiques" explicitement representes avec processus nuageux |
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| 24 | ! |
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[1403] | 25 | ! Reecriture a partir d'un listing papier a Habas, le 14/02/00 |
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[878] | 26 | ! |
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[1403] | 27 | ! le thermique est suppose homogene et dissipe par melange avec |
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| 28 | ! son environnement. la longueur l_mix controle l'efficacite du |
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| 29 | ! melange |
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[878] | 30 | ! |
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[1403] | 31 | ! Le calcul du transport des differentes especes se fait en prenant |
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[878] | 32 | ! en compte: |
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| 33 | ! 1. un flux de masse montant |
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| 34 | ! 2. un flux de masse descendant |
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| 35 | ! 3. un entrainement |
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| 36 | ! 4. un detrainement |
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| 37 | ! |
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| 38 | !======================================================================= |
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| 39 | |
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| 40 | !----------------------------------------------------------------------- |
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| 41 | ! declarations: |
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| 42 | ! ------------- |
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| 43 | |
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| 44 | #include "dimensions.h" |
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| 45 | #include "YOMCST.h" |
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| 46 | #include "YOETHF.h" |
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| 47 | #include "FCTTRE.h" |
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[938] | 48 | #include "iniprint.h" |
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[878] | 49 | |
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| 50 | ! arguments: |
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| 51 | ! ---------- |
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| 52 | |
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[972] | 53 | !IM 140508 |
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| 54 | INTEGER itap |
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| 55 | |
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| 56 | INTEGER ngrid,nlay,w2di |
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| 57 | real tau_thermals |
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[1403] | 58 | integer iflag_thermals_ed |
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[878] | 59 | real ptimestep,l_mix,r_aspect |
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| 60 | REAL pt(ngrid,nlay),pdtadj(ngrid,nlay) |
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| 61 | REAL pu(ngrid,nlay),pduadj(ngrid,nlay) |
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| 62 | REAL pv(ngrid,nlay),pdvadj(ngrid,nlay) |
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| 63 | REAL po(ngrid,nlay),pdoadj(ngrid,nlay) |
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| 64 | REAL pplay(ngrid,nlay),pplev(ngrid,nlay+1) |
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| 65 | real pphi(ngrid,nlay) |
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| 66 | |
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| 67 | ! local: |
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| 68 | ! ------ |
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| 69 | |
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[972] | 70 | integer icount |
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| 71 | data icount/0/ |
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| 72 | save icount |
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[987] | 73 | !$OMP THREADPRIVATE(icount) |
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[972] | 74 | |
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[883] | 75 | integer,save :: igout=1 |
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[987] | 76 | !$OMP THREADPRIVATE(igout) |
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[938] | 77 | integer,save :: lunout1=6 |
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[987] | 78 | !$OMP THREADPRIVATE(lunout1) |
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[883] | 79 | integer,save :: lev_out=10 |
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[987] | 80 | !$OMP THREADPRIVATE(lev_out) |
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[878] | 81 | |
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| 82 | INTEGER ig,k,l,ll |
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| 83 | real zsortie1d(klon) |
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| 84 | INTEGER lmax(klon),lmin(klon),lalim(klon) |
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| 85 | INTEGER lmix(klon) |
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[1026] | 86 | INTEGER lmix_bis(klon) |
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[878] | 87 | real linter(klon) |
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| 88 | real zmix(klon) |
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[1403] | 89 | real zmax(klon),zw2(klon,klev+1),ztva(klon,klev),zw_est(klon,klev+1),ztva_est(klon,klev) |
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[1026] | 90 | ! real fraca(klon,klev) |
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| 91 | |
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[878] | 92 | real zmax_sec(klon) |
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| 93 | !on garde le zmax du pas de temps precedent |
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| 94 | real zmax0(klon) |
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[927] | 95 | !FH/IM save zmax0 |
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[878] | 96 | |
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[972] | 97 | real lambda |
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| 98 | |
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[878] | 99 | real zlev(klon,klev+1),zlay(klon,klev) |
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| 100 | real deltaz(klon,klev) |
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[972] | 101 | REAL zh(klon,klev) |
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[878] | 102 | real zthl(klon,klev),zdthladj(klon,klev) |
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| 103 | REAL ztv(klon,klev) |
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| 104 | real zu(klon,klev),zv(klon,klev),zo(klon,klev) |
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| 105 | real zl(klon,klev) |
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| 106 | real zsortie(klon,klev) |
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| 107 | real zva(klon,klev) |
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| 108 | real zua(klon,klev) |
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| 109 | real zoa(klon,klev) |
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| 110 | |
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| 111 | real zta(klon,klev) |
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| 112 | real zha(klon,klev) |
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| 113 | real fraca(klon,klev+1) |
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| 114 | real zf,zf2 |
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| 115 | real thetath2(klon,klev),wth2(klon,klev),wth3(klon,klev) |
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| 116 | real q2(klon,klev) |
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[972] | 117 | ! FH probleme de dimensionnement avec l'allocation dynamique |
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| 118 | ! common/comtherm/thetath2,wth2 |
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[1403] | 119 | real wq(klon,klev) |
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| 120 | real wthl(klon,klev) |
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| 121 | real wthv(klon,klev) |
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[878] | 122 | |
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| 123 | real ratqscth(klon,klev) |
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| 124 | real var |
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| 125 | real vardiff |
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| 126 | real ratqsdiff(klon,klev) |
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| 127 | |
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| 128 | logical sorties |
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[972] | 129 | real rho(klon,klev),rhobarz(klon,klev),masse(klon,klev) |
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[878] | 130 | real zpspsk(klon,klev) |
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| 131 | |
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| 132 | real wmax(klon) |
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[1403] | 133 | real wmax_tmp(klon) |
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[878] | 134 | real wmax_sec(klon) |
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[972] | 135 | real fm0(klon,klev+1),entr0(klon,klev),detr0(klon,klev) |
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| 136 | real fm(klon,klev+1),entr(klon,klev),detr(klon,klev) |
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[878] | 137 | |
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| 138 | real ztla(klon,klev),zqla(klon,klev),zqta(klon,klev) |
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| 139 | !niveau de condensation |
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[879] | 140 | integer nivcon(klon) |
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[878] | 141 | real zcon(klon) |
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| 142 | REAL CHI |
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| 143 | real zcon2(klon) |
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| 144 | real pcon(klon) |
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| 145 | real zqsat(klon,klev) |
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| 146 | real zqsatth(klon,klev) |
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| 147 | |
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| 148 | real f_star(klon,klev+1),entr_star(klon,klev) |
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| 149 | real detr_star(klon,klev) |
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[1403] | 150 | real alim_star_tot(klon) |
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[878] | 151 | real alim_star(klon,klev) |
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[1403] | 152 | real alim_star_clos(klon,klev) |
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[878] | 153 | real f(klon), f0(klon) |
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[927] | 154 | !FH/IM save f0 |
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[878] | 155 | real zlevinter(klon) |
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| 156 | logical debut |
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| 157 | real seuil |
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[1403] | 158 | real csc(klon,klev) |
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[878] | 159 | |
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| 160 | ! |
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[879] | 161 | !nouvelles variables pour la convection |
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| 162 | real Ale_bl(klon) |
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| 163 | real Alp_bl(klon) |
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| 164 | real alp_int(klon) |
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| 165 | real ale_int(klon) |
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| 166 | integer n_int(klon) |
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| 167 | real fm_tot(klon) |
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| 168 | real wght_th(klon,klev) |
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| 169 | integer lalim_conv(klon) |
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[926] | 170 | !v1d logical therm |
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| 171 | !v1d save therm |
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[878] | 172 | |
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| 173 | character*2 str2 |
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| 174 | character*10 str10 |
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| 175 | |
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[1403] | 176 | character (len=20) :: modname='thermcell_main' |
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| 177 | character (len=80) :: abort_message |
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| 178 | |
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[878] | 179 | EXTERNAL SCOPY |
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| 180 | ! |
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| 181 | |
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| 182 | !----------------------------------------------------------------------- |
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| 183 | ! initialisation: |
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| 184 | ! --------------- |
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| 185 | ! |
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| 186 | |
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| 187 | seuil=0.25 |
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| 188 | |
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[972] | 189 | if (debut) then |
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| 190 | fm0=0. |
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| 191 | entr0=0. |
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| 192 | detr0=0. |
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[1026] | 193 | |
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| 194 | |
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| 195 | #undef wrgrads_thermcell |
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| 196 | #ifdef wrgrads_thermcell |
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| 197 | ! Initialisation des sorties grads pour les thermiques. |
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| 198 | ! Pour l'instant en 1D sur le point igout. |
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| 199 | ! Utilise par thermcell_out3d.h |
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| 200 | str10='therm' |
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| 201 | call inigrads(1,1,rlond(igout),1.,-180.,180.,jjm, & |
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| 202 | & rlatd(igout),-90.,90.,1.,llm,pplay(igout,:),1., & |
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| 203 | & ptimestep,str10,'therm ') |
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| 204 | #endif |
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| 205 | |
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| 206 | |
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| 207 | |
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[972] | 208 | endif |
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| 209 | |
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| 210 | fm=0. ; entr=0. ; detr=0. |
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| 211 | |
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[1403] | 212 | |
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[972] | 213 | icount=icount+1 |
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| 214 | |
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| 215 | !IM 090508 beg |
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| 216 | !print*,'=====================================================================' |
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| 217 | !print*,'=====================================================================' |
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| 218 | !print*,' PAS ',icount,' PAS ',icount,' PAS ',icount,' PAS ',icount |
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| 219 | !print*,'=====================================================================' |
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| 220 | !print*,'=====================================================================' |
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| 221 | !IM 090508 end |
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| 222 | |
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[938] | 223 | if (prt_level.ge.1) print*,'thermcell_main V4' |
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[878] | 224 | |
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| 225 | sorties=.true. |
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| 226 | IF(ngrid.NE.klon) THEN |
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| 227 | PRINT* |
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| 228 | PRINT*,'STOP dans convadj' |
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| 229 | PRINT*,'ngrid =',ngrid |
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| 230 | PRINT*,'klon =',klon |
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| 231 | ENDIF |
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| 232 | ! |
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[1403] | 233 | ! write(lunout,*)'WARNING thermcell_main f0=max(f0,1.e-2)' |
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[972] | 234 | do ig=1,klon |
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| 235 | if (prt_level.ge.20) then |
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| 236 | print*,'th_main ig f0',ig,f0(ig) |
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[878] | 237 | endif |
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[972] | 238 | f0(ig)=max(f0(ig),1.e-2) |
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[1403] | 239 | zmax0(ig)=max(zmax0(ig),40.) |
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[972] | 240 | !IMmarche pas ?! if (f0(ig)<1.e-2) f0(ig)=1.e-2 |
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| 241 | enddo |
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[878] | 242 | |
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| 243 | !----------------------------------------------------------------------- |
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| 244 | ! Calcul de T,q,ql a partir de Tl et qT dans l environnement |
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| 245 | ! -------------------------------------------------------------------- |
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| 246 | ! |
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| 247 | CALL thermcell_env(ngrid,nlay,po,pt,pu,pv,pplay, & |
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| 248 | & pplev,zo,zh,zl,ztv,zthl,zu,zv,zpspsk,zqsat,lev_out) |
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| 249 | |
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[938] | 250 | if (prt_level.ge.1) print*,'thermcell_main apres thermcell_env' |
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[878] | 251 | |
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| 252 | !------------------------------------------------------------------------ |
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| 253 | ! -------------------- |
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| 254 | ! |
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| 255 | ! |
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| 256 | ! + + + + + + + + + + + |
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| 257 | ! |
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| 258 | ! |
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| 259 | ! wa, fraca, wd, fracd -------------------- zlev(2), rhobarz |
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| 260 | ! wh,wt,wo ... |
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| 261 | ! |
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| 262 | ! + + + + + + + + + + + zh,zu,zv,zo,rho |
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| 263 | ! |
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| 264 | ! |
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| 265 | ! -------------------- zlev(1) |
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| 266 | ! \\\\\\\\\\\\\\\\\\\\ |
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| 267 | ! |
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| 268 | ! |
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| 269 | |
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| 270 | !----------------------------------------------------------------------- |
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| 271 | ! Calcul des altitudes des couches |
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| 272 | !----------------------------------------------------------------------- |
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| 273 | |
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| 274 | do l=2,nlay |
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| 275 | zlev(:,l)=0.5*(pphi(:,l)+pphi(:,l-1))/RG |
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| 276 | enddo |
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| 277 | zlev(:,1)=0. |
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| 278 | zlev(:,nlay+1)=(2.*pphi(:,klev)-pphi(:,klev-1))/RG |
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| 279 | do l=1,nlay |
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| 280 | zlay(:,l)=pphi(:,l)/RG |
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| 281 | enddo |
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| 282 | !calcul de l epaisseur des couches |
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| 283 | do l=1,nlay |
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| 284 | deltaz(:,l)=zlev(:,l+1)-zlev(:,l) |
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| 285 | enddo |
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| 286 | |
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| 287 | ! print*,'2 OK convect8' |
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| 288 | !----------------------------------------------------------------------- |
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| 289 | ! Calcul des densites |
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| 290 | !----------------------------------------------------------------------- |
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| 291 | |
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| 292 | do l=1,nlay |
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| 293 | rho(:,l)=pplay(:,l)/(zpspsk(:,l)*RD*ztv(:,l)) |
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| 294 | enddo |
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| 295 | |
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[972] | 296 | !IM |
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[1146] | 297 | if (prt_level.ge.10)write(lunout,*) & |
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| 298 | & 'WARNING thermcell_main rhobarz(:,1)=rho(:,1)' |
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[972] | 299 | rhobarz(:,1)=rho(:,1) |
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| 300 | |
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[878] | 301 | do l=2,nlay |
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| 302 | rhobarz(:,l)=0.5*(rho(:,l)+rho(:,l-1)) |
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| 303 | enddo |
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| 304 | |
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| 305 | !calcul de la masse |
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| 306 | do l=1,nlay |
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| 307 | masse(:,l)=(pplev(:,l)-pplev(:,l+1))/RG |
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| 308 | enddo |
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| 309 | |
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[938] | 310 | if (prt_level.ge.1) print*,'thermcell_main apres initialisation' |
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[878] | 311 | |
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| 312 | !------------------------------------------------------------------ |
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| 313 | ! |
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| 314 | ! /|\ |
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| 315 | ! -------- | F_k+1 ------- |
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| 316 | ! ----> D_k |
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| 317 | ! /|\ <---- E_k , A_k |
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| 318 | ! -------- | F_k --------- |
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| 319 | ! ----> D_k-1 |
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| 320 | ! <---- E_k-1 , A_k-1 |
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| 321 | ! |
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| 322 | ! |
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| 323 | ! |
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| 324 | ! |
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| 325 | ! |
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| 326 | ! --------------------------- |
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| 327 | ! |
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| 328 | ! ----- F_lmax+1=0 ---------- \ |
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| 329 | ! lmax (zmax) | |
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| 330 | ! --------------------------- | |
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| 331 | ! | |
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| 332 | ! --------------------------- | |
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| 333 | ! | |
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| 334 | ! --------------------------- | |
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| 335 | ! | |
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| 336 | ! --------------------------- | |
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| 337 | ! | |
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| 338 | ! --------------------------- | |
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| 339 | ! | E |
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| 340 | ! --------------------------- | D |
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| 341 | ! | |
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| 342 | ! --------------------------- | |
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| 343 | ! | |
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| 344 | ! --------------------------- \ | |
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| 345 | ! lalim | | |
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| 346 | ! --------------------------- | | |
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| 347 | ! | | |
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| 348 | ! --------------------------- | | |
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| 349 | ! | A | |
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| 350 | ! --------------------------- | | |
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| 351 | ! | | |
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| 352 | ! --------------------------- | | |
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| 353 | ! lmin (=1 pour le moment) | | |
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| 354 | ! ----- F_lmin=0 ------------ / / |
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| 355 | ! |
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| 356 | ! --------------------------- |
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| 357 | ! ////////////////////////// |
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| 358 | ! |
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| 359 | ! |
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| 360 | !============================================================================= |
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| 361 | ! Calculs initiaux ne faisant pas intervenir les changements de phase |
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| 362 | !============================================================================= |
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| 363 | |
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| 364 | !------------------------------------------------------------------ |
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[1403] | 365 | ! 1. alim_star est le profil vertical de l'alimentation a la base du |
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| 366 | ! panache thermique, calcule a partir de la flotabilite de l'air sec |
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[878] | 367 | ! 2. lmin et lalim sont les indices inferieurs et superieurs de alim_star |
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| 368 | !------------------------------------------------------------------ |
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| 369 | ! |
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| 370 | entr_star=0. ; detr_star=0. ; alim_star=0. ; alim_star_tot=0. |
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[1403] | 371 | lmin=1 |
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[878] | 372 | |
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| 373 | !----------------------------------------------------------------------------- |
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| 374 | ! 3. wmax_sec et zmax_sec sont les vitesses et altitudes maximum d'un |
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| 375 | ! panache sec conservatif (e=d=0) alimente selon alim_star |
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| 376 | ! Il s'agit d'un calcul de type CAPE |
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[1403] | 377 | ! zmax_sec est utilise pour determiner la geometrie du thermique. |
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[878] | 378 | !------------------------------------------------------------------------------ |
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[1403] | 379 | !--------------------------------------------------------------------------------- |
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| 380 | !calcul du melange et des variables dans le thermique |
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| 381 | !-------------------------------------------------------------------------------- |
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[878] | 382 | ! |
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[1403] | 383 | if (prt_level.ge.1) print*,'avant thermcell_plume ',lev_out |
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| 384 | !IM 140508 CALL thermcell_plume(ngrid,nlay,ptimestep,ztv,zthl,po,zl,rhobarz, & |
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[878] | 385 | |
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[1403] | 386 | ! Gestion temporaire de plusieurs appels à thermcell_plume au travers |
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| 387 | ! de la variable iflag_thermals |
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[878] | 388 | |
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[1403] | 389 | ! print*,'THERM thermcell_main iflag_thermals_ed=',iflag_thermals_ed |
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| 390 | if (iflag_thermals_ed<=9) then |
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| 391 | ! print*,'THERM NOUVELLE/NOUVELLE Arnaud' |
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| 392 | CALL thermcell_plume(itap,ngrid,nlay,ptimestep,ztv,zthl,po,zl,rhobarz,& |
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| 393 | & zlev,pplev,pphi,zpspsk,alim_star,alim_star_tot, & |
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| 394 | & lalim,f0,detr_star,entr_star,f_star,csc,ztva, & |
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| 395 | & ztla,zqla,zqta,zha,zw2,zw_est,ztva_est,zqsatth,lmix,lmix_bis,linter & |
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| 396 | & ,lev_out,lunout1,igout) |
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[878] | 397 | |
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[1403] | 398 | elseif (iflag_thermals_ed>9) then |
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| 399 | ! print*,'THERM RIO et al 2010, version d Arnaud' |
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| 400 | CALL thermcellV1_plume(itap,ngrid,nlay,ptimestep,ztv,zthl,po,zl,rhobarz,& |
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| 401 | & zlev,pplev,pphi,zpspsk,alim_star,alim_star_tot, & |
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| 402 | & lalim,f0,detr_star,entr_star,f_star,csc,ztva, & |
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| 403 | & ztla,zqla,zqta,zha,zw2,zw_est,ztva_est,zqsatth,lmix,lmix_bis,linter & |
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| 404 | & ,lev_out,lunout1,igout) |
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[878] | 405 | |
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[1403] | 406 | endif |
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[878] | 407 | |
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[972] | 408 | if (prt_level.ge.1) print*,'apres thermcell_plume ',lev_out |
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| 409 | |
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[878] | 410 | call test_ltherm(ngrid,nlay,pplev,pplay,lalim,seuil,ztv,po,ztva,zqla,f_star,zw2,'thermcell_plum lalim ') |
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| 411 | call test_ltherm(ngrid,nlay,pplev,pplay,lmix ,seuil,ztv,po,ztva,zqla,f_star,zw2,'thermcell_plum lmix ') |
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| 412 | |
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[938] | 413 | if (prt_level.ge.1) print*,'thermcell_main apres thermcell_plume' |
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| 414 | if (prt_level.ge.10) then |
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[972] | 415 | write(lunout1,*) 'Dans thermcell_main 2' |
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| 416 | write(lunout1,*) 'lmin ',lmin(igout) |
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| 417 | write(lunout1,*) 'lalim ',lalim(igout) |
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| 418 | write(lunout1,*) ' ig l alim_star entr_star detr_star f_star ' |
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| 419 | write(lunout1,'(i6,i4,4e15.5)') (igout,l,alim_star(igout,l),entr_star(igout,l),detr_star(igout,l) & |
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[878] | 420 | & ,f_star(igout,l+1),l=1,nint(linter(igout))+5) |
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| 421 | endif |
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| 422 | |
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| 423 | !------------------------------------------------------------------------------- |
---|
| 424 | ! Calcul des caracteristiques du thermique:zmax,zmix,wmax |
---|
| 425 | !------------------------------------------------------------------------------- |
---|
| 426 | ! |
---|
| 427 | CALL thermcell_height(ngrid,nlay,lalim,lmin,linter,lmix,zw2, & |
---|
| 428 | & zlev,lmax,zmax,zmax0,zmix,wmax,lev_out) |
---|
[1403] | 429 | ! Attention, w2 est transforme en sa racine carree dans cette routine |
---|
| 430 | ! Le probleme vient du fait que linter et lmix sont souvent égaux à 1. |
---|
| 431 | wmax_tmp=0. |
---|
| 432 | do l=1,nlay |
---|
| 433 | wmax_tmp(:)=max(wmax_tmp(:),zw2(:,l)) |
---|
| 434 | enddo |
---|
| 435 | ! print*,"ZMAX ",lalim,lmin,linter,lmix,lmax,zmax,zmax0,zmix,wmax |
---|
[878] | 436 | |
---|
| 437 | |
---|
[1403] | 438 | |
---|
[878] | 439 | call test_ltherm(ngrid,nlay,pplev,pplay,lalim,seuil,ztv,po,ztva,zqla,f_star,zw2,'thermcell_heig lalim ') |
---|
| 440 | call test_ltherm(ngrid,nlay,pplev,pplay,lmin ,seuil,ztv,po,ztva,zqla,f_star,zw2,'thermcell_heig lmin ') |
---|
| 441 | call test_ltherm(ngrid,nlay,pplev,pplay,lmix ,seuil,ztv,po,ztva,zqla,f_star,zw2,'thermcell_heig lmix ') |
---|
| 442 | call test_ltherm(ngrid,nlay,pplev,pplay,lmax ,seuil,ztv,po,ztva,zqla,f_star,zw2,'thermcell_heig lmax ') |
---|
| 443 | |
---|
[938] | 444 | if (prt_level.ge.1) print*,'thermcell_main apres thermcell_height' |
---|
[878] | 445 | |
---|
| 446 | !------------------------------------------------------------------------------- |
---|
| 447 | ! Fermeture,determination de f |
---|
| 448 | !------------------------------------------------------------------------------- |
---|
[1026] | 449 | ! |
---|
[1403] | 450 | ! |
---|
| 451 | !! write(lunout,*)'THERM NOUVEAU XXXXX' |
---|
| 452 | CALL thermcell_dry(ngrid,nlay,zlev,pphi,ztv,alim_star, & |
---|
| 453 | & lalim,lmin,zmax_sec,wmax_sec,lev_out) |
---|
[878] | 454 | |
---|
[1403] | 455 | call test_ltherm(ngrid,nlay,pplev,pplay,lmin,seuil,ztv,po,ztva,zqla,f_star,zw2,'thermcell_dry lmin ') |
---|
| 456 | call test_ltherm(ngrid,nlay,pplev,pplay,lalim,seuil,ztv,po,ztva,zqla,f_star,zw2,'thermcell_dry lalim ') |
---|
| 457 | |
---|
| 458 | if (prt_level.ge.1) print*,'thermcell_main apres thermcell_dry' |
---|
| 459 | if (prt_level.ge.10) then |
---|
| 460 | write(lunout1,*) 'Dans thermcell_main 1b' |
---|
| 461 | write(lunout1,*) 'lmin ',lmin(igout) |
---|
| 462 | write(lunout1,*) 'lalim ',lalim(igout) |
---|
| 463 | write(lunout1,*) ' ig l alim_star entr_star detr_star f_star ' |
---|
| 464 | write(lunout1,'(i6,i4,e15.5)') (igout,l,alim_star(igout,l) & |
---|
| 465 | & ,l=1,lalim(igout)+4) |
---|
| 466 | endif |
---|
| 467 | |
---|
| 468 | |
---|
| 469 | |
---|
| 470 | |
---|
| 471 | ! Choix de la fonction d'alimentation utilisee pour la fermeture. |
---|
| 472 | ! Apparemment sans importance |
---|
| 473 | alim_star_clos(:,:)=alim_star(:,:) |
---|
| 474 | alim_star_clos(:,:)=entr_star(:,:)+alim_star(:,:) |
---|
| 475 | |
---|
| 476 | ! Appel avec la version seche |
---|
[878] | 477 | CALL thermcell_closure(ngrid,nlay,r_aspect,ptimestep,rho, & |
---|
[1403] | 478 | & zlev,lalim,alim_star_clos,f_star,zmax_sec,wmax_sec,f,lev_out) |
---|
[878] | 479 | |
---|
[1403] | 480 | !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! |
---|
| 481 | ! Appel avec les zmax et wmax tenant compte de la condensation |
---|
| 482 | ! Semble moins bien marcher |
---|
| 483 | ! CALL thermcell_closure(ngrid,nlay,r_aspect,ptimestep,rho, & |
---|
| 484 | ! & zlev,lalim,alim_star,f_star,zmax,wmax,f,lev_out) |
---|
| 485 | !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! |
---|
| 486 | |
---|
[938] | 487 | if(prt_level.ge.1)print*,'thermcell_closure apres thermcell_closure' |
---|
[878] | 488 | |
---|
[972] | 489 | if (tau_thermals>1.) then |
---|
| 490 | lambda=exp(-ptimestep/tau_thermals) |
---|
| 491 | f0=(1.-lambda)*f+lambda*f0 |
---|
| 492 | else |
---|
| 493 | f0=f |
---|
| 494 | endif |
---|
| 495 | |
---|
| 496 | ! Test valable seulement en 1D mais pas genant |
---|
| 497 | if (.not. (f0(1).ge.0.) ) then |
---|
[1403] | 498 | abort_message = '.not. (f0(1).ge.0.)' |
---|
| 499 | CALL abort_gcm (modname,abort_message,1) |
---|
[972] | 500 | endif |
---|
| 501 | |
---|
[878] | 502 | !------------------------------------------------------------------------------- |
---|
| 503 | !deduction des flux |
---|
| 504 | !------------------------------------------------------------------------------- |
---|
| 505 | |
---|
[972] | 506 | CALL thermcell_flux2(ngrid,nlay,ptimestep,masse, & |
---|
[878] | 507 | & lalim,lmax,alim_star, & |
---|
| 508 | & entr_star,detr_star,f,rhobarz,zlev,zw2,fm,entr, & |
---|
[972] | 509 | & detr,zqla,lev_out,lunout1,igout) |
---|
| 510 | !IM 060508 & detr,zqla,zmax,lev_out,lunout,igout) |
---|
[878] | 511 | |
---|
[938] | 512 | if (prt_level.ge.1) print*,'thermcell_main apres thermcell_flux' |
---|
[878] | 513 | call test_ltherm(ngrid,nlay,pplev,pplay,lalim,seuil,ztv,po,ztva,zqla,f_star,zw2,'thermcell_flux lalim ') |
---|
| 514 | call test_ltherm(ngrid,nlay,pplev,pplay,lmax ,seuil,ztv,po,ztva,zqla,f_star,zw2,'thermcell_flux lmax ') |
---|
| 515 | |
---|
| 516 | !------------------------------------------------------------------ |
---|
[972] | 517 | ! On ne prend pas directement les profils issus des calculs precedents |
---|
| 518 | ! mais on s'autorise genereusement une relaxation vers ceci avec |
---|
| 519 | ! une constante de temps tau_thermals (typiquement 1800s). |
---|
| 520 | !------------------------------------------------------------------ |
---|
[878] | 521 | |
---|
[972] | 522 | if (tau_thermals>1.) then |
---|
| 523 | lambda=exp(-ptimestep/tau_thermals) |
---|
| 524 | fm0=(1.-lambda)*fm+lambda*fm0 |
---|
| 525 | entr0=(1.-lambda)*entr+lambda*entr0 |
---|
[1403] | 526 | detr0=(1.-lambda)*detr+lambda*detr0 |
---|
[878] | 527 | else |
---|
| 528 | fm0=fm |
---|
| 529 | entr0=entr |
---|
| 530 | detr0=detr |
---|
| 531 | endif |
---|
| 532 | |
---|
[972] | 533 | !c------------------------------------------------------------------ |
---|
| 534 | ! calcul du transport vertical |
---|
| 535 | !------------------------------------------------------------------ |
---|
| 536 | |
---|
[878] | 537 | call thermcell_dq(ngrid,nlay,ptimestep,fm0,entr0,masse, & |
---|
| 538 | & zthl,zdthladj,zta,lev_out) |
---|
| 539 | call thermcell_dq(ngrid,nlay,ptimestep,fm0,entr0,masse, & |
---|
| 540 | & po,pdoadj,zoa,lev_out) |
---|
| 541 | |
---|
[883] | 542 | !------------------------------------------------------------------ |
---|
| 543 | ! Calcul de la fraction de l'ascendance |
---|
| 544 | !------------------------------------------------------------------ |
---|
| 545 | do ig=1,klon |
---|
| 546 | fraca(ig,1)=0. |
---|
| 547 | fraca(ig,nlay+1)=0. |
---|
| 548 | enddo |
---|
| 549 | do l=2,nlay |
---|
| 550 | do ig=1,klon |
---|
| 551 | if (zw2(ig,l).gt.1.e-10) then |
---|
| 552 | fraca(ig,l)=fm(ig,l)/(rhobarz(ig,l)*zw2(ig,l)) |
---|
| 553 | else |
---|
| 554 | fraca(ig,l)=0. |
---|
| 555 | endif |
---|
| 556 | enddo |
---|
| 557 | enddo |
---|
| 558 | |
---|
| 559 | !------------------------------------------------------------------ |
---|
| 560 | ! calcul du transport vertical du moment horizontal |
---|
| 561 | !------------------------------------------------------------------ |
---|
[878] | 562 | |
---|
[972] | 563 | !IM 090508 |
---|
[883] | 564 | if (1.eq.1) then |
---|
[972] | 565 | !IM 070508 vers. _dq |
---|
| 566 | ! if (1.eq.0) then |
---|
[883] | 567 | |
---|
| 568 | |
---|
[878] | 569 | ! Calcul du transport de V tenant compte d'echange par gradient |
---|
| 570 | ! de pression horizontal avec l'environnement |
---|
| 571 | |
---|
| 572 | call thermcell_dv2(ngrid,nlay,ptimestep,fm0,entr0,masse & |
---|
| 573 | & ,fraca,zmax & |
---|
[972] | 574 | & ,zu,zv,pduadj,pdvadj,zua,zva,lev_out) |
---|
[1403] | 575 | |
---|
[878] | 576 | else |
---|
| 577 | |
---|
| 578 | ! calcul purement conservatif pour le transport de V |
---|
| 579 | call thermcell_dq(ngrid,nlay,ptimestep,fm0,entr0,masse & |
---|
| 580 | & ,zu,pduadj,zua,lev_out) |
---|
| 581 | call thermcell_dq(ngrid,nlay,ptimestep,fm0,entr0,masse & |
---|
| 582 | & ,zv,pdvadj,zva,lev_out) |
---|
| 583 | endif |
---|
| 584 | |
---|
| 585 | ! print*,'13 OK convect8' |
---|
| 586 | do l=1,nlay |
---|
| 587 | do ig=1,ngrid |
---|
| 588 | pdtadj(ig,l)=zdthladj(ig,l)*zpspsk(ig,l) |
---|
| 589 | enddo |
---|
| 590 | enddo |
---|
| 591 | |
---|
[972] | 592 | if (prt_level.ge.1) print*,'14 OK convect8' |
---|
[878] | 593 | !------------------------------------------------------------------ |
---|
| 594 | ! Calculs de diagnostiques pour les sorties |
---|
| 595 | !------------------------------------------------------------------ |
---|
| 596 | !calcul de fraca pour les sorties |
---|
| 597 | |
---|
| 598 | if (sorties) then |
---|
[972] | 599 | if (prt_level.ge.1) print*,'14a OK convect8' |
---|
[878] | 600 | ! calcul du niveau de condensation |
---|
| 601 | ! initialisation |
---|
| 602 | do ig=1,ngrid |
---|
[879] | 603 | nivcon(ig)=0 |
---|
[878] | 604 | zcon(ig)=0. |
---|
| 605 | enddo |
---|
| 606 | !nouveau calcul |
---|
| 607 | do ig=1,ngrid |
---|
| 608 | CHI=zh(ig,1)/(1669.0-122.0*zo(ig,1)/zqsat(ig,1)-zh(ig,1)) |
---|
| 609 | pcon(ig)=pplay(ig,1)*(zo(ig,1)/zqsat(ig,1))**CHI |
---|
| 610 | enddo |
---|
[1403] | 611 | !IM do k=1,nlay |
---|
| 612 | do k=1,nlay-1 |
---|
[878] | 613 | do ig=1,ngrid |
---|
| 614 | if ((pcon(ig).le.pplay(ig,k)) & |
---|
| 615 | & .and.(pcon(ig).gt.pplay(ig,k+1))) then |
---|
| 616 | zcon2(ig)=zlay(ig,k)-(pcon(ig)-pplay(ig,k))/(RG*rho(ig,k))/100. |
---|
| 617 | endif |
---|
| 618 | enddo |
---|
| 619 | enddo |
---|
[1403] | 620 | !IM |
---|
| 621 | do ig=1,ngrid |
---|
| 622 | if (pcon(ig).le.pplay(ig,nlay)) then |
---|
| 623 | zcon2(ig)=zlay(ig,nlay)-(pcon(ig)-pplay(ig,nlay))/(RG*rho(ig,nlay))/100. |
---|
| 624 | abort_message = 'thermcellV0_main: les thermiques vont trop haut ' |
---|
| 625 | CALL abort_gcm (modname,abort_message,1) |
---|
| 626 | endif |
---|
| 627 | enddo |
---|
[972] | 628 | if (prt_level.ge.1) print*,'14b OK convect8' |
---|
[878] | 629 | do k=nlay,1,-1 |
---|
| 630 | do ig=1,ngrid |
---|
| 631 | if (zqla(ig,k).gt.1e-10) then |
---|
| 632 | nivcon(ig)=k |
---|
| 633 | zcon(ig)=zlev(ig,k) |
---|
| 634 | endif |
---|
| 635 | enddo |
---|
| 636 | enddo |
---|
[972] | 637 | if (prt_level.ge.1) print*,'14c OK convect8' |
---|
[878] | 638 | !calcul des moments |
---|
| 639 | !initialisation |
---|
| 640 | do l=1,nlay |
---|
| 641 | do ig=1,ngrid |
---|
| 642 | q2(ig,l)=0. |
---|
| 643 | wth2(ig,l)=0. |
---|
| 644 | wth3(ig,l)=0. |
---|
| 645 | ratqscth(ig,l)=0. |
---|
| 646 | ratqsdiff(ig,l)=0. |
---|
| 647 | enddo |
---|
| 648 | enddo |
---|
[972] | 649 | if (prt_level.ge.1) print*,'14d OK convect8' |
---|
[1146] | 650 | if (prt_level.ge.10)write(lunout,*) & |
---|
| 651 | & 'WARNING thermcell_main wth2=0. si zw2 > 1.e-10' |
---|
[878] | 652 | do l=1,nlay |
---|
| 653 | do ig=1,ngrid |
---|
| 654 | zf=fraca(ig,l) |
---|
| 655 | zf2=zf/(1.-zf) |
---|
[972] | 656 | ! |
---|
| 657 | if (prt_level.ge.10) print*,'14e OK convect8 ig,l,zf,zf2',ig,l,zf,zf2 |
---|
| 658 | ! |
---|
| 659 | if (prt_level.ge.10) print*,'14f OK convect8 ig,l,zha zh zpspsk ',ig,l,zha(ig,l),zh(ig,l),zpspsk(ig,l) |
---|
[1403] | 660 | thetath2(ig,l)=zf2*(ztla(ig,l)-zthl(ig,l))**2 |
---|
[972] | 661 | if(zw2(ig,l).gt.1.e-10) then |
---|
| 662 | wth2(ig,l)=zf2*(zw2(ig,l))**2 |
---|
| 663 | else |
---|
| 664 | wth2(ig,l)=0. |
---|
| 665 | endif |
---|
[878] | 666 | ! print*,'wth2=',wth2(ig,l) |
---|
| 667 | wth3(ig,l)=zf2*(1-2.*fraca(ig,l))/(1-fraca(ig,l)) & |
---|
| 668 | & *zw2(ig,l)*zw2(ig,l)*zw2(ig,l) |
---|
[972] | 669 | if (prt_level.ge.10) print*,'14g OK convect8 ig,l,po',ig,l,po(ig,l) |
---|
[878] | 670 | q2(ig,l)=zf2*(zqta(ig,l)*1000.-po(ig,l)*1000.)**2 |
---|
| 671 | !test: on calcul q2/po=ratqsc |
---|
| 672 | ratqscth(ig,l)=sqrt(max(q2(ig,l),1.e-6)/(po(ig,l)*1000.)) |
---|
| 673 | enddo |
---|
| 674 | enddo |
---|
[1403] | 675 | !calcul des flux: q, thetal et thetav |
---|
| 676 | do l=1,nlay |
---|
| 677 | do ig=1,ngrid |
---|
| 678 | wq(ig,l)=fraca(ig,l)*zw2(ig,l)*(zqta(ig,l)*1000.-po(ig,l)*1000.) |
---|
| 679 | wthl(ig,l)=fraca(ig,l)*zw2(ig,l)*(ztla(ig,l)-zthl(ig,l)) |
---|
| 680 | wthv(ig,l)=fraca(ig,l)*zw2(ig,l)*(ztva(ig,l)-ztv(ig,l)) |
---|
| 681 | enddo |
---|
[879] | 682 | enddo |
---|
[972] | 683 | ! |
---|
[1403] | 684 | ! print*,'avant calcul ale et alp' |
---|
| 685 | !calcul de ALE et ALP pour la convection |
---|
| 686 | Alp_bl(:)=0. |
---|
| 687 | Ale_bl(:)=0. |
---|
| 688 | ! print*,'ALE,ALP ,l,zw2(ig,l),Ale_bl(ig),Alp_bl(ig)' |
---|
[972] | 689 | do l=1,nlay |
---|
[879] | 690 | do ig=1,ngrid |
---|
[1403] | 691 | Alp_bl(ig)=max(Alp_bl(ig),0.5*rhobarz(ig,l)*wth3(ig,l) ) |
---|
| 692 | Ale_bl(ig)=max(Ale_bl(ig),0.5*zw2(ig,l)**2) |
---|
| 693 | ! print*,'ALE,ALP',l,zw2(ig,l),Ale_bl(ig),Alp_bl(ig) |
---|
[879] | 694 | enddo |
---|
| 695 | enddo |
---|
[1403] | 696 | |
---|
| 697 | ! print*,'AAAAAAA ',Alp_bl,Ale_bl,lmix |
---|
| 698 | |
---|
| 699 | |
---|
| 700 | ! TEST. IL FAUT REECRIRE LES ALE et ALP |
---|
| 701 | ! Ale_bl(:)=0.5*wmax(:)*wmax(:) |
---|
| 702 | ! Alp_bl(:)=0.1*wmax(:)*wmax(:)*wmax(:) |
---|
| 703 | |
---|
[879] | 704 | !test:calcul de la ponderation des couches pour KE |
---|
| 705 | !initialisations |
---|
| 706 | ! print*,'ponderation' |
---|
| 707 | do ig=1,ngrid |
---|
| 708 | fm_tot(ig)=0. |
---|
| 709 | enddo |
---|
| 710 | do ig=1,ngrid |
---|
| 711 | do k=1,klev |
---|
| 712 | wght_th(ig,k)=1. |
---|
| 713 | enddo |
---|
| 714 | enddo |
---|
| 715 | do ig=1,ngrid |
---|
| 716 | ! lalim_conv(ig)=lmix_bis(ig) |
---|
| 717 | !la hauteur de la couche alim_conv = hauteur couche alim_therm |
---|
| 718 | lalim_conv(ig)=lalim(ig) |
---|
| 719 | ! zentr(ig)=zlev(ig,lalim(ig)) |
---|
| 720 | enddo |
---|
| 721 | do ig=1,ngrid |
---|
| 722 | do k=1,lalim_conv(ig) |
---|
| 723 | fm_tot(ig)=fm_tot(ig)+fm(ig,k) |
---|
| 724 | enddo |
---|
| 725 | enddo |
---|
| 726 | do ig=1,ngrid |
---|
| 727 | do k=1,lalim_conv(ig) |
---|
| 728 | if (fm_tot(ig).gt.1.e-10) then |
---|
| 729 | ! wght_th(ig,k)=fm(ig,k)/fm_tot(ig) |
---|
| 730 | endif |
---|
| 731 | !on pondere chaque couche par a* |
---|
| 732 | if (alim_star(ig,k).gt.1.e-10) then |
---|
| 733 | wght_th(ig,k)=alim_star(ig,k) |
---|
| 734 | else |
---|
| 735 | wght_th(ig,k)=1. |
---|
| 736 | endif |
---|
| 737 | enddo |
---|
| 738 | enddo |
---|
| 739 | ! print*,'apres wght_th' |
---|
| 740 | !test pour prolonger la convection |
---|
| 741 | do ig=1,ngrid |
---|
[926] | 742 | !v1d if ((alim_star(ig,1).lt.1.e-10).and.(therm)) then |
---|
| 743 | if ((alim_star(ig,1).lt.1.e-10)) then |
---|
[879] | 744 | lalim_conv(ig)=1 |
---|
| 745 | wght_th(ig,1)=1. |
---|
| 746 | ! print*,'lalim_conv ok',lalim_conv(ig),wght_th(ig,1) |
---|
| 747 | endif |
---|
| 748 | enddo |
---|
| 749 | |
---|
[878] | 750 | !calcul du ratqscdiff |
---|
[972] | 751 | if (prt_level.ge.1) print*,'14e OK convect8' |
---|
[878] | 752 | var=0. |
---|
| 753 | vardiff=0. |
---|
| 754 | ratqsdiff(:,:)=0. |
---|
| 755 | do ig=1,ngrid |
---|
| 756 | do l=1,lalim(ig) |
---|
| 757 | var=var+alim_star(ig,l)*zqta(ig,l)*1000. |
---|
| 758 | enddo |
---|
| 759 | enddo |
---|
[972] | 760 | if (prt_level.ge.1) print*,'14f OK convect8' |
---|
[878] | 761 | do ig=1,ngrid |
---|
| 762 | do l=1,lalim(ig) |
---|
| 763 | zf=fraca(ig,l) |
---|
| 764 | zf2=zf/(1.-zf) |
---|
| 765 | vardiff=vardiff+alim_star(ig,l) & |
---|
| 766 | & *(zqta(ig,l)*1000.-var)**2 |
---|
| 767 | ! ratqsdiff=ratqsdiff+alim_star(ig,l)* |
---|
| 768 | ! s (zqta(ig,l)*1000.-po(ig,l)*1000.)**2 |
---|
| 769 | enddo |
---|
| 770 | enddo |
---|
[972] | 771 | if (prt_level.ge.1) print*,'14g OK convect8' |
---|
[878] | 772 | do l=1,nlay |
---|
| 773 | do ig=1,ngrid |
---|
| 774 | ratqsdiff(ig,l)=sqrt(vardiff)/(po(ig,l)*1000.) |
---|
| 775 | ! write(11,*)'ratqsdiff=',ratqsdiff(ig,l) |
---|
| 776 | enddo |
---|
| 777 | enddo |
---|
| 778 | !-------------------------------------------------------------------- |
---|
| 779 | ! |
---|
| 780 | !ecriture des fichiers sortie |
---|
| 781 | ! print*,'15 OK convect8' |
---|
| 782 | |
---|
[1403] | 783 | #ifdef wrgrads_thermcell |
---|
[938] | 784 | if (prt_level.ge.1) print*,'thermcell_main sorties 3D' |
---|
[878] | 785 | #include "thermcell_out3d.h" |
---|
| 786 | #endif |
---|
| 787 | |
---|
| 788 | endif |
---|
| 789 | |
---|
[938] | 790 | if (prt_level.ge.1) print*,'thermcell_main FIN OK' |
---|
[878] | 791 | |
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| 792 | return |
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| 793 | end |
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| 794 | |
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| 795 | !----------------------------------------------------------------------------- |
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| 796 | |
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| 797 | subroutine test_ltherm(klon,klev,pplev,pplay,long,seuil,ztv,po,ztva,zqla,f_star,zw2,comment) |
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[938] | 798 | IMPLICIT NONE |
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| 799 | #include "iniprint.h" |
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[878] | 800 | |
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[938] | 801 | integer i, k, klon,klev |
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[878] | 802 | real pplev(klon,klev+1),pplay(klon,klev) |
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| 803 | real ztv(klon,klev) |
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| 804 | real po(klon,klev) |
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| 805 | real ztva(klon,klev) |
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| 806 | real zqla(klon,klev) |
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| 807 | real f_star(klon,klev) |
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| 808 | real zw2(klon,klev) |
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| 809 | integer long(klon) |
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| 810 | real seuil |
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| 811 | character*21 comment |
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| 812 | |
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[938] | 813 | if (prt_level.ge.1) THEN |
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| 814 | print*,'WARNING !!! TEST ',comment |
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| 815 | endif |
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[879] | 816 | return |
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| 817 | |
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[878] | 818 | ! test sur la hauteur des thermiques ... |
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| 819 | do i=1,klon |
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[972] | 820 | !IMtemp if (pplay(i,long(i)).lt.seuil*pplev(i,1)) then |
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| 821 | if (prt_level.ge.10) then |
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[878] | 822 | print*,'WARNING ',comment,' au point ',i,' K= ',long(i) |
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| 823 | print*,' K P(MB) THV(K) Qenv(g/kg)THVA QLA(g/kg) F* W2' |
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| 824 | do k=1,klev |
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| 825 | write(6,'(i3,7f10.3)') k,pplay(i,k),ztv(i,k),1000*po(i,k),ztva(i,k),1000*zqla(i,k),f_star(i,k),zw2(i,k) |
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| 826 | enddo |
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[972] | 827 | endif |
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[878] | 828 | enddo |
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| 829 | |
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| 830 | |
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| 831 | return |
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| 832 | end |
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| 833 | |
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