| 1 | ! $Id: thermcell_main.F90 4441 2023-02-17 16:11:37Z acozic $ |
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| 2 | ! |
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| 3 | subroutine thermcell_main(itap,ngrid,nlay,ptimestep & |
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| 4 | & ,pplay,pplev,pphi,debut & |
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| 5 | & ,pu,pv,pt,po & |
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| 6 | & ,pduadj,pdvadj,pdtadj,pdoadj & |
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| 7 | & ,fm0,entr0,detr0,zqta,zqla,lmax & |
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| 8 | & ,ratqscth,ratqsdiff,zqsatth & |
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| 9 | & ,zmax0, f0,zw2,fraca,ztv & |
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| 10 | & ,zpspsk,ztla,zthl,ztva & |
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| 11 | & ,pcon,rhobarz,wth3,wmax_sec,lalim,fm,alim_star,zmax & |
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| 12 | #ifdef ISO |
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| 13 | & ,xtpo,xtpdoadj & |
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| 14 | #endif |
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| 15 | & ) |
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| 16 | |
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| 17 | |
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| 18 | USE thermcell_ini_mod, ONLY: thermcell_ini,dqimpl,dvdq,prt_level,lunout,prt_level |
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| 19 | USE thermcell_ini_mod, ONLY: iflag_thermals_closure,iflag_thermals_ed,tau_thermals,r_aspect_thermals |
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| 20 | USE thermcell_ini_mod, ONLY: iflag_thermals_down, fact_thermals_down |
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| 21 | USE thermcell_ini_mod, ONLY: RD,RG |
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| 22 | |
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| 23 | #ifdef ISO |
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| 24 | USE infotrac_phy, ONLY : ntiso |
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| 25 | #ifdef ISOVERIF |
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| 26 | USE isotopes_mod, ONLY : iso_eau,iso_HDO |
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| 27 | USE isotopes_verif_mod, ONLY: iso_verif_egalite, & |
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| 28 | iso_verif_aberrant_encadre |
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| 29 | #endif |
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| 30 | #endif |
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| 31 | |
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| 32 | |
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| 33 | IMPLICIT NONE |
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| 34 | |
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| 35 | !======================================================================= |
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| 36 | ! Auteurs: Frederic Hourdin, Catherine Rio, Anne Mathieu |
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| 37 | ! Version du 09.02.07 |
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| 38 | ! Calcul du transport vertical dans la couche limite en presence |
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| 39 | ! de "thermiques" explicitement representes avec processus nuageux |
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| 40 | ! |
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| 41 | ! Reecriture a partir d'un listing papier a Habas, le 14/02/00 |
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| 42 | ! |
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| 43 | ! le thermique est suppose homogene et dissipe par melange avec |
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| 44 | ! son environnement. la longueur l_mix controle l'efficacite du |
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| 45 | ! melange |
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| 46 | ! |
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| 47 | ! Le calcul du transport des differentes especes se fait en prenant |
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| 48 | ! en compte: |
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| 49 | ! 1. un flux de masse montant |
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| 50 | ! 2. un flux de masse descendant |
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| 51 | ! 3. un entrainement |
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| 52 | ! 4. un detrainement |
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| 53 | ! |
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| 54 | ! Modif 2013/01/04 (FH hourdin@lmd.jussieu.fr) |
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| 55 | ! Introduction of an implicit computation of vertical advection in |
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| 56 | ! the environment of thermal plumes in thermcell_dq |
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| 57 | ! impl = 0 : explicit, 1 : implicit, -1 : old version |
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| 58 | ! controled by iflag_thermals = |
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| 59 | ! 15, 16 run with impl=-1 : numerical convergence with NPv3 |
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| 60 | ! 17, 18 run with impl=1 : more stable |
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| 61 | ! 15 and 17 correspond to the activation of the stratocumulus "bidouille" |
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| 62 | ! |
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| 63 | ! Using |
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| 64 | ! abort_physic |
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| 65 | ! iso_verif_aberrant_encadre |
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| 66 | ! iso_verif_egalite |
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| 67 | ! test_ltherm |
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| 68 | ! thermcell_closure |
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| 69 | ! thermcell_dq |
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| 70 | ! thermcell_dry |
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| 71 | ! thermcell_dv2 |
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| 72 | ! thermcell_env |
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| 73 | ! thermcell_flux2 |
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| 74 | ! thermcell_height |
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| 75 | ! thermcell_plume |
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| 76 | ! thermcell_plume_5B |
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| 77 | ! thermcell_plume_6A |
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| 78 | ! |
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| 79 | !======================================================================= |
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| 80 | |
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| 81 | |
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| 82 | !----------------------------------------------------------------------- |
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| 83 | ! declarations: |
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| 84 | ! ------------- |
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| 85 | |
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| 86 | |
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| 87 | ! arguments: |
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| 88 | ! ---------- |
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| 89 | integer, intent(in) :: itap,ngrid,nlay |
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| 90 | real, intent(in) :: ptimestep |
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| 91 | real, intent(in), dimension(ngrid,nlay) :: pt,pu,pv,po,pplay,pphi,zpspsk |
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| 92 | real, intent(in), dimension(ngrid,nlay+1) :: pplev |
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| 93 | integer, intent(out), dimension(ngrid) :: lmax |
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| 94 | real, intent(out), dimension(ngrid,nlay) :: pdtadj,pduadj,pdvadj,pdoadj,entr0,detr0 |
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| 95 | real, intent(out), dimension(ngrid,nlay) :: ztla,zqla,zqta,zqsatth,zthl |
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| 96 | real, intent(out), dimension(ngrid,nlay+1) :: fm0,zw2,fraca |
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| 97 | real, intent(inout), dimension(ngrid) :: zmax0,f0 |
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| 98 | real, intent(out), dimension(ngrid,nlay) :: ztva,ztv |
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| 99 | logical, intent(in) :: debut |
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| 100 | real,intent(out), dimension(ngrid,nlay) :: ratqscth,ratqsdiff |
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| 101 | |
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| 102 | real, intent(out), dimension(ngrid) :: pcon |
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| 103 | real, intent(out), dimension(ngrid,nlay) :: rhobarz,wth3 |
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| 104 | real, intent(out), dimension(ngrid) :: wmax_sec |
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| 105 | integer,intent(out), dimension(ngrid) :: lalim |
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| 106 | real, intent(out), dimension(ngrid,nlay+1) :: fm |
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| 107 | real, intent(out), dimension(ngrid,nlay) :: alim_star |
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| 108 | real, intent(out), dimension(ngrid) :: zmax |
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| 109 | |
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| 110 | ! local: |
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| 111 | ! ------ |
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| 112 | |
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| 113 | |
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| 114 | integer,save :: igout=1 |
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| 115 | !$OMP THREADPRIVATE(igout) |
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| 116 | integer,save :: lunout1=6 |
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| 117 | !$OMP THREADPRIVATE(lunout1) |
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| 118 | integer,save :: lev_out=10 |
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| 119 | !$OMP THREADPRIVATE(lev_out) |
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| 120 | |
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| 121 | real lambda, zf,zf2,var,vardiff,CHI |
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| 122 | integer ig,k,l,ierr,ll |
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| 123 | logical sorties |
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| 124 | real, dimension(ngrid) :: linter,zmix, zmax_sec |
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| 125 | integer,dimension(ngrid) :: lmin,lmix,lmix_bis,nivcon |
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| 126 | real, dimension(ngrid,nlay) :: ztva_est |
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| 127 | real, dimension(ngrid,nlay) :: deltaz,zlay,zh,zdthladj,zu,zv,zo,zl,zva,zua,zoa |
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| 128 | real, dimension(ngrid,nlay) :: zta,zha,q2,wq,wthl,wthv,thetath2,wth2 |
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| 129 | real, dimension(ngrid,nlay) :: rho,masse |
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| 130 | real, dimension(ngrid,nlay+1) :: zw_est,zlev |
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| 131 | real, dimension(ngrid) :: wmax,wmax_tmp |
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| 132 | real, dimension(ngrid,nlay+1) :: f_star |
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| 133 | real, dimension(ngrid,nlay) :: entr,detr,entr_star,detr_star,alim_star_clos |
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| 134 | real, dimension(ngrid,nlay) :: zqsat,csc |
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| 135 | real, dimension(ngrid) :: zcon,zcon2,alim_star_tot,f |
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| 136 | real, dimension(ngrid,nlay) :: entrdn,detrdn |
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| 137 | |
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| 138 | character (len=20) :: modname='thermcell_main' |
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| 139 | character (len=80) :: abort_message |
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| 140 | |
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| 141 | |
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| 142 | #ifdef ISO |
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| 143 | REAL xtpo(ntiso,ngrid,nlay),xtpdoadj(ntiso,ngrid,nlay) |
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| 144 | REAL xtzo(ntiso,ngrid,nlay) |
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| 145 | REAL xtpdoadj_tmp(ngrid,nlay) |
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| 146 | REAL xtpo_tmp(ngrid,nlay) |
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| 147 | REAL xtzo_tmp(ngrid,nlay) |
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| 148 | integer ixt |
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| 149 | #endif |
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| 150 | |
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| 151 | ! |
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| 152 | |
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| 153 | !----------------------------------------------------------------------- |
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| 154 | ! initialisation: |
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| 155 | ! --------------- |
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| 156 | ! |
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| 157 | fm=0. ; entr=0. ; detr=0. |
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| 158 | |
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| 159 | if (prt_level.ge.1) print*,'thermcell_main V4' |
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| 160 | |
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| 161 | sorties=.true. |
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| 162 | IF(ngrid.NE.ngrid) THEN |
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| 163 | PRINT* |
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| 164 | PRINT*,'STOP dans convadj' |
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| 165 | PRINT*,'ngrid =',ngrid |
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| 166 | PRINT*,'ngrid =',ngrid |
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| 167 | ENDIF |
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| 168 | ! |
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| 169 | ! write(lunout,*)'WARNING thermcell_main f0=max(f0,1.e-2)' |
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| 170 | do ig=1,ngrid |
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| 171 | f0(ig)=max(f0(ig),1.e-2) |
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| 172 | zmax0(ig)=max(zmax0(ig),40.) |
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| 173 | !IMmarche pas ?! if (f0(ig)<1.e-2) f0(ig)=1.e-2 |
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| 174 | enddo |
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| 175 | |
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| 176 | if (prt_level.ge.20) then |
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| 177 | do ig=1,ngrid |
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| 178 | print*,'th_main ig f0',ig,f0(ig) |
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| 179 | enddo |
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| 180 | endif |
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| 181 | !----------------------------------------------------------------------- |
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| 182 | ! Calcul de T,q,ql a partir de Tl et qT dans l environnement |
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| 183 | ! -------------------------------------------------------------------- |
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| 184 | ! |
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| 185 | CALL thermcell_env(ngrid,nlay,po,pt,pu,pv,pplay, & |
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| 186 | & pplev,zo,zh,zl,ztv,zthl,zu,zv,zpspsk,zqsat,lev_out) |
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| 187 | |
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| 188 | if (prt_level.ge.1) print*,'thermcell_main apres thermcell_env' |
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| 189 | |
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| 190 | !------------------------------------------------------------------------ |
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| 191 | ! -------------------- |
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| 192 | ! |
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| 193 | ! |
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| 194 | ! + + + + + + + + + + + |
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| 195 | ! |
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| 196 | ! |
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| 197 | ! wa, fraca, wd, fracd -------------------- zlev(2), rhobarz |
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| 198 | ! wh,wt,wo ... |
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| 199 | ! |
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| 200 | ! + + + + + + + + + + + zh,zu,zv,zo,rho |
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| 201 | ! |
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| 202 | ! |
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| 203 | ! -------------------- zlev(1) |
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| 204 | ! \\\\\\\\\\\\\\\\\\\\ |
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| 205 | ! |
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| 206 | ! |
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| 207 | |
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| 208 | !----------------------------------------------------------------------- |
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| 209 | ! Calcul des altitudes des couches |
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| 210 | !----------------------------------------------------------------------- |
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| 211 | |
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| 212 | do l=2,nlay |
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| 213 | zlev(:,l)=0.5*(pphi(:,l)+pphi(:,l-1))/RG |
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| 214 | enddo |
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| 215 | zlev(:,1)=0. |
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| 216 | zlev(:,nlay+1)=(2.*pphi(:,nlay)-pphi(:,nlay-1))/RG |
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| 217 | do l=1,nlay |
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| 218 | zlay(:,l)=pphi(:,l)/RG |
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| 219 | enddo |
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| 220 | do l=1,nlay |
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| 221 | deltaz(:,l)=zlev(:,l+1)-zlev(:,l) |
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| 222 | enddo |
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| 223 | |
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| 224 | !----------------------------------------------------------------------- |
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| 225 | ! Calcul des densites et masses |
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| 226 | !----------------------------------------------------------------------- |
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| 227 | |
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| 228 | rho(:,:)=pplay(:,:)/(zpspsk(:,:)*RD*ztv(:,:)) |
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| 229 | if (prt_level.ge.10) write(lunout,*) 'WARNING thermcell_main rhobarz(:,1)=rho(:,1)' |
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| 230 | rhobarz(:,1)=rho(:,1) |
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| 231 | do l=2,nlay |
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| 232 | rhobarz(:,l)=0.5*(rho(:,l)+rho(:,l-1)) |
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| 233 | enddo |
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| 234 | do l=1,nlay |
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| 235 | masse(:,l)=(pplev(:,l)-pplev(:,l+1))/RG |
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| 236 | enddo |
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| 237 | if (prt_level.ge.1) print*,'thermcell_main apres initialisation' |
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| 238 | |
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| 239 | !------------------------------------------------------------------ |
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| 240 | ! |
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| 241 | ! /|\ |
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| 242 | ! -------- | F_k+1 ------- |
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| 243 | ! ----> D_k |
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| 244 | ! /|\ <---- E_k , A_k |
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| 245 | ! -------- | F_k --------- |
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| 246 | ! ----> D_k-1 |
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| 247 | ! <---- E_k-1 , A_k-1 |
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| 248 | ! |
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| 249 | ! |
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| 250 | ! |
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| 251 | ! |
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| 252 | ! |
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| 253 | ! --------------------------- |
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| 254 | ! |
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| 255 | ! ----- F_lmax+1=0 ---------- \ |
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| 256 | ! lmax (zmax) | |
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| 257 | ! --------------------------- | |
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| 258 | ! | |
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| 259 | ! --------------------------- | |
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| 260 | ! | |
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| 261 | ! --------------------------- | |
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| 262 | ! | |
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| 263 | ! --------------------------- | |
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| 264 | ! | |
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| 265 | ! --------------------------- | |
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| 266 | ! | E |
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| 267 | ! --------------------------- | D |
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| 268 | ! | |
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| 269 | ! --------------------------- | |
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| 270 | ! | |
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| 271 | ! --------------------------- \ | |
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| 272 | ! lalim | | |
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| 273 | ! --------------------------- | | |
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| 274 | ! | | |
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| 275 | ! --------------------------- | | |
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| 276 | ! | A | |
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| 277 | ! --------------------------- | | |
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| 278 | ! | | |
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| 279 | ! --------------------------- | | |
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| 280 | ! lmin (=1 pour le moment) | | |
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| 281 | ! ----- F_lmin=0 ------------ / / |
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| 282 | ! |
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| 283 | ! --------------------------- |
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| 284 | ! ////////////////////////// |
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| 285 | ! |
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| 286 | ! |
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| 287 | !============================================================================= |
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| 288 | ! Calculs initiaux ne faisant pas intervenir les changements de phase |
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| 289 | !============================================================================= |
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| 290 | |
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| 291 | !------------------------------------------------------------------ |
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| 292 | ! 1. alim_star est le profil vertical de l'alimentation a la base du |
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| 293 | ! panache thermique, calcule a partir de la flotabilite de l'air sec |
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| 294 | ! 2. lmin et lalim sont les indices inferieurs et superieurs de alim_star |
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| 295 | !------------------------------------------------------------------ |
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| 296 | ! |
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| 297 | entr_star=0. ; detr_star=0. ; alim_star=0. ; alim_star_tot=0. |
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| 298 | lmin=1 |
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| 299 | |
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| 300 | !----------------------------------------------------------------------------- |
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| 301 | ! 3. wmax_sec et zmax_sec sont les vitesses et altitudes maximum d'un |
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| 302 | ! panache sec conservatif (e=d=0) alimente selon alim_star |
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| 303 | ! Il s'agit d'un calcul de type CAPE |
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| 304 | ! zmax_sec est utilise pour determiner la geometrie du thermique. |
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| 305 | !------------------------------------------------------------------------------ |
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| 306 | !--------------------------------------------------------------------------------- |
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| 307 | !calcul du melange et des variables dans le thermique |
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| 308 | !-------------------------------------------------------------------------------- |
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| 309 | ! |
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| 310 | if (prt_level.ge.1) print*,'avant thermcell_plume ',lev_out |
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| 311 | |
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| 312 | !===================================================================== |
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| 313 | ! Old version of thermcell_plume in thermcell_plume_6A.F90 |
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| 314 | ! It includes both thermcell_plume_6A and thermcell_plume_5B corresponding |
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| 315 | ! to the 5B and 6A versions used for CMIP5 and CMIP6. |
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| 316 | ! The latest was previously named thermcellV1_plume. |
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| 317 | ! The new thermcell_plume is a clean version (removing obsolete |
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| 318 | ! options) of thermcell_plume_6A. |
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| 319 | ! The 3 versions are controled by |
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| 320 | ! flag_thermals_ed <= 9 thermcell_plume_6A |
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| 321 | ! <= 19 thermcell_plume_5B |
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| 322 | ! else thermcell_plume (default 20 for convergence with 6A) |
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| 323 | ! Fredho |
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| 324 | !===================================================================== |
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| 325 | |
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| 326 | if (iflag_thermals_ed<=9) then |
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| 327 | ! print*,'THERM NOUVELLE/NOUVELLE Arnaud' |
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| 328 | CALL thermcell_plume_6A(itap,ngrid,nlay,ptimestep,ztv,zthl,po,zl,rhobarz,& |
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| 329 | & zlev,pplev,pphi,zpspsk,alim_star,alim_star_tot, & |
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| 330 | & lalim,f0,detr_star,entr_star,f_star,csc,ztva, & |
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| 331 | & ztla,zqla,zqta,zha,zw2,zw_est,ztva_est,zqsatth,lmix,lmix_bis,linter & |
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| 332 | & ,lev_out,lunout1,igout) |
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| 333 | |
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| 334 | elseif (iflag_thermals_ed<=19) then |
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| 335 | ! print*,'THERM RIO et al 2010, version d Arnaud' |
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| 336 | CALL thermcell_plume_5B(itap,ngrid,nlay,ptimestep,ztv,zthl,po,zl,rhobarz,& |
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| 337 | & zlev,pplev,pphi,zpspsk,alim_star,alim_star_tot, & |
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| 338 | & lalim,f0,detr_star,entr_star,f_star,csc,ztva, & |
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| 339 | & ztla,zqla,zqta,zha,zw2,zw_est,ztva_est,zqsatth,lmix,lmix_bis,linter & |
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| 340 | & ,lev_out,lunout1,igout) |
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| 341 | else |
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| 342 | CALL thermcell_plume(itap,ngrid,nlay,ptimestep,ztv,zthl,po,zl,rhobarz,& |
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| 343 | & zlev,pplev,pphi,zpspsk,alim_star,alim_star_tot, & |
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| 344 | & lalim,f0,detr_star,entr_star,f_star,csc,ztva, & |
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| 345 | & ztla,zqla,zqta,zha,zw2,zw_est,ztva_est,zqsatth,lmix,lmix_bis,linter & |
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| 346 | & ,lev_out,lunout1,igout) |
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| 347 | endif |
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| 348 | |
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| 349 | if (prt_level.ge.1) print*,'apres thermcell_plume ',lev_out |
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| 350 | |
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| 351 | call test_ltherm(ngrid,nlay,pplay,lalim,ztv,po,ztva,zqla,f_star,zw2,'thermcell_plum lalim ') |
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| 352 | call test_ltherm(ngrid,nlay,pplay,lmix ,ztv,po,ztva,zqla,f_star,zw2,'thermcell_plum lmix ') |
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| 353 | |
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| 354 | if (prt_level.ge.1) print*,'thermcell_main apres thermcell_plume' |
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| 355 | if (prt_level.ge.10) then |
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| 356 | write(lunout1,*) 'Dans thermcell_main 2' |
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| 357 | write(lunout1,*) 'lmin ',lmin(igout) |
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| 358 | write(lunout1,*) 'lalim ',lalim(igout) |
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| 359 | write(lunout1,*) ' ig l alim_star entr_star detr_star f_star ' |
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| 360 | write(lunout1,'(i6,i4,4e15.5)') (igout,l,alim_star(igout,l),entr_star(igout,l),detr_star(igout,l) & |
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| 361 | & ,f_star(igout,l+1),l=1,nint(linter(igout))+5) |
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| 362 | endif |
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| 363 | |
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| 364 | !------------------------------------------------------------------------------- |
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| 365 | ! Calcul des caracteristiques du thermique:zmax,zmix,wmax |
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| 366 | !------------------------------------------------------------------------------- |
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| 367 | ! |
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| 368 | CALL thermcell_height(ngrid,nlay,lalim,lmin,linter,lmix,zw2, & |
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| 369 | & zlev,lmax,zmax,zmax0,zmix,wmax) |
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| 370 | ! Attention, w2 est transforme en sa racine carree dans cette routine |
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| 371 | ! Le probleme vient du fait que linter et lmix sont souvent egaux a 1. |
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| 372 | wmax_tmp=0. |
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| 373 | do l=1,nlay |
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| 374 | wmax_tmp(:)=max(wmax_tmp(:),zw2(:,l)) |
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| 375 | enddo |
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| 376 | ! print*,"ZMAX ",lalim,lmin,linter,lmix,lmax,zmax,zmax0,zmix,wmax |
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| 377 | |
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| 378 | |
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| 379 | |
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| 380 | call test_ltherm(ngrid,nlay,pplay,lalim,ztv,po,ztva,zqla,f_star,zw2,'thermcell_heig lalim ') |
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| 381 | call test_ltherm(ngrid,nlay,pplay,lmin ,ztv,po,ztva,zqla,f_star,zw2,'thermcell_heig lmin ') |
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| 382 | call test_ltherm(ngrid,nlay,pplay,lmix ,ztv,po,ztva,zqla,f_star,zw2,'thermcell_heig lmix ') |
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| 383 | call test_ltherm(ngrid,nlay,pplay,lmax ,ztv,po,ztva,zqla,f_star,zw2,'thermcell_heig lmax ') |
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| 384 | |
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| 385 | if (prt_level.ge.1) print*,'thermcell_main apres thermcell_height' |
|---|
| 386 | |
|---|
| 387 | !------------------------------------------------------------------------------- |
|---|
| 388 | ! Fermeture,determination de f |
|---|
| 389 | !------------------------------------------------------------------------------- |
|---|
| 390 | ! |
|---|
| 391 | ! |
|---|
| 392 | CALL thermcell_dry(ngrid,nlay,zlev,pphi,ztv,alim_star, & |
|---|
| 393 | & lalim,lmin,zmax_sec,wmax_sec) |
|---|
| 394 | |
|---|
| 395 | |
|---|
| 396 | call test_ltherm(ngrid,nlay,pplay,lmin,ztv,po,ztva,zqla,f_star,zw2,'thermcell_dry lmin ') |
|---|
| 397 | call test_ltherm(ngrid,nlay,pplay,lalim,ztv,po,ztva,zqla,f_star,zw2,'thermcell_dry lalim ') |
|---|
| 398 | |
|---|
| 399 | if (prt_level.ge.1) print*,'thermcell_main apres thermcell_dry' |
|---|
| 400 | if (prt_level.ge.10) then |
|---|
| 401 | write(lunout1,*) 'Dans thermcell_main 1b' |
|---|
| 402 | write(lunout1,*) 'lmin ',lmin(igout) |
|---|
| 403 | write(lunout1,*) 'lalim ',lalim(igout) |
|---|
| 404 | write(lunout1,*) ' ig l alim_star entr_star detr_star f_star ' |
|---|
| 405 | write(lunout1,'(i6,i4,e15.5)') (igout,l,alim_star(igout,l) & |
|---|
| 406 | & ,l=1,lalim(igout)+4) |
|---|
| 407 | endif |
|---|
| 408 | |
|---|
| 409 | |
|---|
| 410 | |
|---|
| 411 | |
|---|
| 412 | ! Choix de la fonction d'alimentation utilisee pour la fermeture. |
|---|
| 413 | ! Apparemment sans importance |
|---|
| 414 | alim_star_clos(:,:)=alim_star(:,:) |
|---|
| 415 | alim_star_clos(:,:)=entr_star(:,:)+alim_star(:,:) |
|---|
| 416 | ! |
|---|
| 417 | !CR Appel de la fermeture seche |
|---|
| 418 | if (iflag_thermals_closure.eq.1) then |
|---|
| 419 | |
|---|
| 420 | CALL thermcell_closure(ngrid,nlay,r_aspect_thermals,ptimestep,rho, & |
|---|
| 421 | & zlev,lalim,alim_star_clos,zmax_sec,wmax_sec,f) |
|---|
| 422 | |
|---|
| 423 | !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! |
|---|
| 424 | ! Appel avec les zmax et wmax tenant compte de la condensation |
|---|
| 425 | ! Semble moins bien marcher |
|---|
| 426 | else if (iflag_thermals_closure.eq.2) then |
|---|
| 427 | |
|---|
| 428 | CALL thermcell_closure(ngrid,nlay,r_aspect_thermals,ptimestep,rho, & |
|---|
| 429 | & zlev,lalim,alim_star,zmax,wmax,f) |
|---|
| 430 | |
|---|
| 431 | |
|---|
| 432 | endif |
|---|
| 433 | |
|---|
| 434 | !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! |
|---|
| 435 | |
|---|
| 436 | if(prt_level.ge.1)print*,'thermcell_closure apres thermcell_closure' |
|---|
| 437 | |
|---|
| 438 | if (tau_thermals>1.) then |
|---|
| 439 | lambda=exp(-ptimestep/tau_thermals) |
|---|
| 440 | f0=(1.-lambda)*f+lambda*f0 |
|---|
| 441 | else |
|---|
| 442 | f0=f |
|---|
| 443 | endif |
|---|
| 444 | |
|---|
| 445 | ! Test valable seulement en 1D mais pas genant |
|---|
| 446 | if (.not. (f0(1).ge.0.) ) then |
|---|
| 447 | abort_message = '.not. (f0(1).ge.0.)' |
|---|
| 448 | CALL abort_physic (modname,abort_message,1) |
|---|
| 449 | endif |
|---|
| 450 | |
|---|
| 451 | !------------------------------------------------------------------------------- |
|---|
| 452 | !deduction des flux |
|---|
| 453 | |
|---|
| 454 | CALL thermcell_flux2(ngrid,nlay,ptimestep,masse, & |
|---|
| 455 | & lalim,lmax,alim_star, & |
|---|
| 456 | & entr_star,detr_star,f,rhobarz,zlev,zw2,fm,entr, & |
|---|
| 457 | & detr,zqla,lev_out,lunout1,igout) |
|---|
| 458 | |
|---|
| 459 | !IM 060508 & detr,zqla,zmax,lev_out,lunout,igout) |
|---|
| 460 | |
|---|
| 461 | if (prt_level.ge.1) print*,'thermcell_main apres thermcell_flux' |
|---|
| 462 | call test_ltherm(ngrid,nlay,pplay,lalim,ztv,po,ztva,zqla,f_star,zw2,'thermcell_flux lalim ') |
|---|
| 463 | call test_ltherm(ngrid,nlay,pplay,lmax ,ztv,po,ztva,zqla,f_star,zw2,'thermcell_flux lmax ') |
|---|
| 464 | |
|---|
| 465 | !------------------------------------------------------------------ |
|---|
| 466 | ! On ne prend pas directement les profils issus des calculs precedents |
|---|
| 467 | ! mais on s'autorise genereusement une relaxation vers ceci avec |
|---|
| 468 | ! une constante de temps tau_thermals (typiquement 1800s). |
|---|
| 469 | !------------------------------------------------------------------ |
|---|
| 470 | |
|---|
| 471 | if (tau_thermals>1.) then |
|---|
| 472 | lambda=exp(-ptimestep/tau_thermals) |
|---|
| 473 | fm0=(1.-lambda)*fm+lambda*fm0 |
|---|
| 474 | entr0=(1.-lambda)*entr+lambda*entr0 |
|---|
| 475 | detr0=(1.-lambda)*detr+lambda*detr0 |
|---|
| 476 | else |
|---|
| 477 | fm0=fm |
|---|
| 478 | entr0=entr |
|---|
| 479 | detr0=detr |
|---|
| 480 | endif |
|---|
| 481 | |
|---|
| 482 | !------------------------------------------------------------------ |
|---|
| 483 | ! Calcul de la fraction de l'ascendance |
|---|
| 484 | !------------------------------------------------------------------ |
|---|
| 485 | do ig=1,ngrid |
|---|
| 486 | fraca(ig,1)=0. |
|---|
| 487 | fraca(ig,nlay+1)=0. |
|---|
| 488 | enddo |
|---|
| 489 | do l=2,nlay |
|---|
| 490 | do ig=1,ngrid |
|---|
| 491 | if (zw2(ig,l).gt.1.e-10) then |
|---|
| 492 | fraca(ig,l)=fm(ig,l)/(rhobarz(ig,l)*zw2(ig,l)) |
|---|
| 493 | else |
|---|
| 494 | fraca(ig,l)=0. |
|---|
| 495 | endif |
|---|
| 496 | enddo |
|---|
| 497 | enddo |
|---|
| 498 | |
|---|
| 499 | !c------------------------------------------------------------------ |
|---|
| 500 | ! calcul du transport vertical |
|---|
| 501 | !------------------------------------------------------------------ |
|---|
| 502 | IF (iflag_thermals_down .GT. 0) THEN |
|---|
| 503 | if (debut) print*,'WARNING !!! routine thermcell_down en cours de developpement' |
|---|
| 504 | entrdn=fact_thermals_down*detr0 |
|---|
| 505 | detrdn=fact_thermals_down*entr0 |
|---|
| 506 | ! we want to transport potential temperature, total water and momentum |
|---|
| 507 | CALL thermcell_updown_dq(ngrid,nlay,ptimestep,lmax,entr0,detr0,entrdn,detrdn,masse,zthl,zdthladj) |
|---|
| 508 | CALL thermcell_updown_dq(ngrid,nlay,ptimestep,lmax,entr0,detr0,entrdn,detrdn,masse,po,pdoadj) |
|---|
| 509 | CALL thermcell_updown_dq(ngrid,nlay,ptimestep,lmax,entr0,detr0,entrdn,detrdn,masse,zu,pduadj) |
|---|
| 510 | CALL thermcell_updown_dq(ngrid,nlay,ptimestep,lmax,entr0,detr0,entrdn,detrdn,masse,zv,pdvadj) |
|---|
| 511 | ELSE |
|---|
| 512 | !-------------------------------------------------------------- |
|---|
| 513 | |
|---|
| 514 | call thermcell_dq(ngrid,nlay,dqimpl,ptimestep,fm0,entr0,masse, & |
|---|
| 515 | & zthl,zdthladj,zta,lev_out) |
|---|
| 516 | call thermcell_dq(ngrid,nlay,dqimpl,ptimestep,fm0,entr0,masse, & |
|---|
| 517 | & po,pdoadj,zoa,lev_out) |
|---|
| 518 | |
|---|
| 519 | #ifdef ISO |
|---|
| 520 | ! C Risi: on utilise directement la meme routine |
|---|
| 521 | do ixt=1,ntiso |
|---|
| 522 | do ll=1,nlay |
|---|
| 523 | DO ig=1,ngrid |
|---|
| 524 | xtpo_tmp(ig,ll)=xtpo(ixt,ig,ll) |
|---|
| 525 | xtzo_tmp(ig,ll)=xtzo(ixt,ig,ll) |
|---|
| 526 | enddo |
|---|
| 527 | enddo |
|---|
| 528 | call thermcell_dq(ngrid,nlay,dqimpl,ptimestep,fm0,entr0,masse, & |
|---|
| 529 | & xtpo_tmp,xtpdoadj_tmp,xtzo_tmp,lev_out) |
|---|
| 530 | do ll=1,nlay |
|---|
| 531 | DO ig=1,ngrid |
|---|
| 532 | xtpdoadj(ixt,ig,ll)=xtpdoadj_tmp(ig,ll) |
|---|
| 533 | enddo |
|---|
| 534 | enddo |
|---|
| 535 | enddo |
|---|
| 536 | #endif |
|---|
| 537 | |
|---|
| 538 | #ifdef ISO |
|---|
| 539 | #ifdef ISOVERIF |
|---|
| 540 | DO ll=1,nlay |
|---|
| 541 | DO ig=1,ngrid |
|---|
| 542 | if (iso_eau.gt.0) then |
|---|
| 543 | call iso_verif_egalite(xtpo(iso_eau,ig,ll), & |
|---|
| 544 | & po(ig,ll),'thermcell_main 594') |
|---|
| 545 | call iso_verif_egalite(xtpdoadj(iso_eau,ig,ll), & |
|---|
| 546 | & pdoadj(ig,ll),'thermcell_main 596') |
|---|
| 547 | endif |
|---|
| 548 | if (iso_HDO.gt.0) then |
|---|
| 549 | call iso_verif_aberrant_encadre(xtpo(iso_hdo,ig,ll) & |
|---|
| 550 | & /po(ig,ll),'thermcell_main 610') |
|---|
| 551 | endif |
|---|
| 552 | enddo |
|---|
| 553 | enddo !DO ll=1,nlay |
|---|
| 554 | write(*,*) 'thermcell_main 600 tmp: apres thermcell_dq' |
|---|
| 555 | #endif |
|---|
| 556 | #endif |
|---|
| 557 | |
|---|
| 558 | |
|---|
| 559 | !------------------------------------------------------------------ |
|---|
| 560 | ! calcul du transport vertical du moment horizontal |
|---|
| 561 | !------------------------------------------------------------------ |
|---|
| 562 | |
|---|
| 563 | !IM 090508 |
|---|
| 564 | if (dvdq == 0 ) then |
|---|
| 565 | |
|---|
| 566 | ! Calcul du transport de V tenant compte d'echange par gradient |
|---|
| 567 | ! de pression horizontal avec l'environnement |
|---|
| 568 | |
|---|
| 569 | call thermcell_dv2(ngrid,nlay,ptimestep,fm0,entr0,masse & |
|---|
| 570 | ! & ,fraca*dvdq,zmax & |
|---|
| 571 | & ,fraca,zmax & |
|---|
| 572 | & ,zu,zv,pduadj,pdvadj,zua,zva,lev_out) |
|---|
| 573 | |
|---|
| 574 | else |
|---|
| 575 | |
|---|
| 576 | ! calcul purement conservatif pour le transport de V |
|---|
| 577 | call thermcell_dq(ngrid,nlay,dqimpl,ptimestep,fm0,entr0,masse & |
|---|
| 578 | & ,zu,pduadj,zua,lev_out) |
|---|
| 579 | call thermcell_dq(ngrid,nlay,dqimpl,ptimestep,fm0,entr0,masse & |
|---|
| 580 | & ,zv,pdvadj,zva,lev_out) |
|---|
| 581 | |
|---|
| 582 | endif |
|---|
| 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 | |
|---|
| 592 | if (prt_level.ge.1) print*,'14 OK convect8' |
|---|
| 593 | !------------------------------------------------------------------ |
|---|
| 594 | ! Calculs de diagnostiques pour les sorties |
|---|
| 595 | !------------------------------------------------------------------ |
|---|
| 596 | !calcul de fraca pour les sorties |
|---|
| 597 | |
|---|
| 598 | if (sorties) then |
|---|
| 599 | if (prt_level.ge.1) print*,'14a OK convect8' |
|---|
| 600 | ! calcul du niveau de condensation |
|---|
| 601 | ! initialisation |
|---|
| 602 | do ig=1,ngrid |
|---|
| 603 | nivcon(ig)=0 |
|---|
| 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 |
|---|
| 611 | !IM do k=1,nlay |
|---|
| 612 | do k=1,nlay-1 |
|---|
| 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 |
|---|
| 620 | !IM |
|---|
| 621 | ierr=0 |
|---|
| 622 | do ig=1,ngrid |
|---|
| 623 | if (pcon(ig).le.pplay(ig,nlay)) then |
|---|
| 624 | zcon2(ig)=zlay(ig,nlay)-(pcon(ig)-pplay(ig,nlay))/(RG*rho(ig,nlay))/100. |
|---|
| 625 | ierr=1 |
|---|
| 626 | endif |
|---|
| 627 | enddo |
|---|
| 628 | if (ierr==1) then |
|---|
| 629 | abort_message = 'thermcellV0_main: les thermiques vont trop haut ' |
|---|
| 630 | CALL abort_physic (modname,abort_message,1) |
|---|
| 631 | endif |
|---|
| 632 | |
|---|
| 633 | if (prt_level.ge.1) print*,'14b OK convect8' |
|---|
| 634 | do k=nlay,1,-1 |
|---|
| 635 | do ig=1,ngrid |
|---|
| 636 | if (zqla(ig,k).gt.1e-10) then |
|---|
| 637 | nivcon(ig)=k |
|---|
| 638 | zcon(ig)=zlev(ig,k) |
|---|
| 639 | endif |
|---|
| 640 | enddo |
|---|
| 641 | enddo |
|---|
| 642 | if (prt_level.ge.1) print*,'14c OK convect8' |
|---|
| 643 | !calcul des moments |
|---|
| 644 | !initialisation |
|---|
| 645 | do l=1,nlay |
|---|
| 646 | do ig=1,ngrid |
|---|
| 647 | q2(ig,l)=0. |
|---|
| 648 | wth2(ig,l)=0. |
|---|
| 649 | wth3(ig,l)=0. |
|---|
| 650 | ratqscth(ig,l)=0. |
|---|
| 651 | ratqsdiff(ig,l)=0. |
|---|
| 652 | enddo |
|---|
| 653 | enddo |
|---|
| 654 | if (prt_level.ge.1) print*,'14d OK convect8' |
|---|
| 655 | if (prt_level.ge.10)write(lunout,*) & |
|---|
| 656 | & 'WARNING thermcell_main wth2=0. si zw2 > 1.e-10' |
|---|
| 657 | do l=1,nlay |
|---|
| 658 | do ig=1,ngrid |
|---|
| 659 | zf=fraca(ig,l) |
|---|
| 660 | zf2=zf/(1.-zf) |
|---|
| 661 | ! |
|---|
| 662 | thetath2(ig,l)=zf2*(ztla(ig,l)-zthl(ig,l))**2 |
|---|
| 663 | if(zw2(ig,l).gt.1.e-10) then |
|---|
| 664 | wth2(ig,l)=zf2*(zw2(ig,l))**2 |
|---|
| 665 | else |
|---|
| 666 | wth2(ig,l)=0. |
|---|
| 667 | endif |
|---|
| 668 | wth3(ig,l)=zf2*(1-2.*fraca(ig,l))/(1-fraca(ig,l)) & |
|---|
| 669 | & *zw2(ig,l)*zw2(ig,l)*zw2(ig,l) |
|---|
| 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 |
|---|
| 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 |
|---|
| 682 | enddo |
|---|
| 683 | |
|---|
| 684 | !calcul du ratqscdiff |
|---|
| 685 | if (prt_level.ge.1) print*,'14e OK convect8' |
|---|
| 686 | var=0. |
|---|
| 687 | vardiff=0. |
|---|
| 688 | ratqsdiff(:,:)=0. |
|---|
| 689 | |
|---|
| 690 | do l=1,nlay |
|---|
| 691 | do ig=1,ngrid |
|---|
| 692 | if (l<=lalim(ig)) then |
|---|
| 693 | var=var+alim_star(ig,l)*zqta(ig,l)*1000. |
|---|
| 694 | endif |
|---|
| 695 | enddo |
|---|
| 696 | enddo |
|---|
| 697 | |
|---|
| 698 | if (prt_level.ge.1) print*,'14f OK convect8' |
|---|
| 699 | |
|---|
| 700 | do l=1,nlay |
|---|
| 701 | do ig=1,ngrid |
|---|
| 702 | if (l<=lalim(ig)) then |
|---|
| 703 | zf=fraca(ig,l) |
|---|
| 704 | zf2=zf/(1.-zf) |
|---|
| 705 | vardiff=vardiff+alim_star(ig,l)*(zqta(ig,l)*1000.-var)**2 |
|---|
| 706 | endif |
|---|
| 707 | enddo |
|---|
| 708 | enddo |
|---|
| 709 | |
|---|
| 710 | if (prt_level.ge.1) print*,'14g OK convect8' |
|---|
| 711 | do l=1,nlay |
|---|
| 712 | do ig=1,ngrid |
|---|
| 713 | ratqsdiff(ig,l)=sqrt(vardiff)/(po(ig,l)*1000.) |
|---|
| 714 | enddo |
|---|
| 715 | enddo |
|---|
| 716 | endif |
|---|
| 717 | |
|---|
| 718 | if (prt_level.ge.1) print*,'thermcell_main FIN OK' |
|---|
| 719 | |
|---|
| 720 | RETURN |
|---|
| 721 | end subroutine thermcell_main |
|---|
| 722 | |
|---|
| 723 | !============================================================================= |
|---|
| 724 | !///////////////////////////////////////////////////////////////////////////// |
|---|
| 725 | !============================================================================= |
|---|
| 726 | subroutine test_ltherm(ngrid,nlay,pplay,long,ztv,po,ztva, & ! in |
|---|
| 727 | & zqla,f_star,zw2,comment) ! in |
|---|
| 728 | !============================================================================= |
|---|
| 729 | USE thermcell_ini_mod, ONLY: prt_level |
|---|
| 730 | IMPLICIT NONE |
|---|
| 731 | |
|---|
| 732 | integer i, k, ngrid,nlay |
|---|
| 733 | real, intent(in), dimension(ngrid,nlay) :: pplay,ztv,po,ztva,zqla |
|---|
| 734 | real, intent(in), dimension(ngrid,nlay) :: f_star,zw2 |
|---|
| 735 | integer, intent(in), dimension(ngrid) :: long |
|---|
| 736 | real seuil |
|---|
| 737 | character*21 comment |
|---|
| 738 | |
|---|
| 739 | seuil=0.25 |
|---|
| 740 | |
|---|
| 741 | if (prt_level.ge.1) THEN |
|---|
| 742 | print*,'WARNING !!! TEST ',comment |
|---|
| 743 | endif |
|---|
| 744 | return |
|---|
| 745 | |
|---|
| 746 | ! test sur la hauteur des thermiques ... |
|---|
| 747 | do i=1,ngrid |
|---|
| 748 | !IMtemp if (pplay(i,long(i)).lt.seuil*pplev(i,1)) then |
|---|
| 749 | if (prt_level.ge.10) then |
|---|
| 750 | print*,'WARNING ',comment,' au point ',i,' K= ',long(i) |
|---|
| 751 | print*,' K P(MB) THV(K) Qenv(g/kg)THVA QLA(g/kg) F* W2' |
|---|
| 752 | do k=1,nlay |
|---|
| 753 | 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) |
|---|
| 754 | enddo |
|---|
| 755 | endif |
|---|
| 756 | enddo |
|---|
| 757 | |
|---|
| 758 | |
|---|
| 759 | return |
|---|
| 760 | end |
|---|
| 761 | |
|---|
| 762 | ! nrlmd le 10/04/2012 Transport de la TKE par le thermique moyen pour la fermeture en ALP |
|---|
| 763 | ! On transporte pbl_tke pour donner therm_tke |
|---|
| 764 | ! Copie conforme de la subroutine DTKE dans physiq.F ecrite par Frederic Hourdin |
|---|
| 765 | |
|---|
| 766 | !======================================================================= |
|---|
| 767 | !/////////////////////////////////////////////////////////////////////// |
|---|
| 768 | !======================================================================= |
|---|
| 769 | |
|---|
| 770 | subroutine thermcell_tke_transport( & |
|---|
| 771 | & ngrid,nlay,ptimestep,fm0,entr0,rg,pplev, & ! in |
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| 772 | & therm_tke_max) ! out |
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| 773 | USE thermcell_ini_mod, ONLY: prt_level |
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| 774 | implicit none |
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| 775 | |
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| 776 | !======================================================================= |
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| 777 | ! |
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| 778 | ! Calcul du transport verticale dans la couche limite en presence |
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| 779 | ! de "thermiques" explicitement representes |
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| 780 | ! calcul du dq/dt une fois qu'on connait les ascendances |
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| 781 | ! |
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| 782 | !======================================================================= |
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| 783 | |
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| 784 | integer ngrid,nlay |
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| 785 | |
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| 786 | real, intent(in) :: ptimestep |
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| 787 | real, intent(in), dimension(ngrid,nlay+1) :: fm0,pplev |
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| 788 | real, intent(in), dimension(ngrid,nlay) :: entr0 |
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| 789 | real, intent(in) :: rg |
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| 790 | real, intent(out), dimension(ngrid,nlay) :: therm_tke_max |
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| 791 | |
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| 792 | real detr0(ngrid,nlay) |
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| 793 | real masse0(ngrid,nlay) |
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| 794 | real masse(ngrid,nlay),fm(ngrid,nlay+1) |
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| 795 | real entr(ngrid,nlay) |
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| 796 | real q(ngrid,nlay) |
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| 797 | integer lev_out ! niveau pour les print |
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| 798 | |
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| 799 | real qa(ngrid,nlay),detr(ngrid,nlay),wqd(ngrid,nlay+1) |
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| 800 | integer ig,k |
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| 801 | |
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| 802 | |
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| 803 | lev_out=0 |
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| 804 | |
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| 805 | |
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| 806 | if (prt_level.ge.1) print*,'Q2 THERMCEL_DQ 0' |
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| 807 | |
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| 808 | ! calcul du detrainement |
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| 809 | do k=1,nlay |
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| 810 | detr0(:,k)=fm0(:,k)-fm0(:,k+1)+entr0(:,k) |
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| 811 | masse0(:,k)=(pplev(:,k)-pplev(:,k+1))/RG |
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| 812 | enddo |
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| 813 | |
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| 814 | |
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| 815 | ! Decalage vertical des entrainements et detrainements. |
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| 816 | masse(:,1)=0.5*masse0(:,1) |
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| 817 | entr(:,1)=0.5*entr0(:,1) |
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| 818 | detr(:,1)=0.5*detr0(:,1) |
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| 819 | fm(:,1)=0. |
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| 820 | do k=1,nlay-1 |
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| 821 | masse(:,k+1)=0.5*(masse0(:,k)+masse0(:,k+1)) |
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| 822 | entr(:,k+1)=0.5*(entr0(:,k)+entr0(:,k+1)) |
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| 823 | detr(:,k+1)=0.5*(detr0(:,k)+detr0(:,k+1)) |
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| 824 | fm(:,k+1)=fm(:,k)+entr(:,k)-detr(:,k) |
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| 825 | enddo |
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| 826 | fm(:,nlay+1)=0. |
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| 827 | |
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| 828 | |
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| 829 | q(:,:)=therm_tke_max(:,:) |
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| 830 | !!! nrlmd le 16/09/2010 |
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| 831 | do ig=1,ngrid |
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| 832 | qa(ig,1)=q(ig,1) |
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| 833 | enddo |
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| 834 | !!! |
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| 835 | |
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| 836 | if (1==1) then |
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| 837 | do k=2,nlay |
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| 838 | do ig=1,ngrid |
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| 839 | if ((fm(ig,k+1)+detr(ig,k))*ptimestep.gt. & |
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| 840 | & 1.e-5*masse(ig,k)) then |
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| 841 | qa(ig,k)=(fm(ig,k)*qa(ig,k-1)+entr(ig,k)*q(ig,k)) & |
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| 842 | & /(fm(ig,k+1)+detr(ig,k)) |
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| 843 | else |
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| 844 | qa(ig,k)=q(ig,k) |
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| 845 | endif |
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| 846 | if (qa(ig,k).lt.0.) then |
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| 847 | ! print*,'qa<0!!!' |
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| 848 | endif |
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| 849 | if (q(ig,k).lt.0.) then |
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| 850 | ! print*,'q<0!!!' |
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| 851 | endif |
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| 852 | enddo |
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| 853 | enddo |
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| 854 | |
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| 855 | ! Calcul du flux subsident |
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| 856 | |
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| 857 | do k=2,nlay |
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| 858 | do ig=1,ngrid |
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| 859 | wqd(ig,k)=fm(ig,k)*q(ig,k) |
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| 860 | if (wqd(ig,k).lt.0.) then |
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| 861 | ! print*,'wqd<0!!!' |
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| 862 | endif |
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| 863 | enddo |
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| 864 | enddo |
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| 865 | do ig=1,ngrid |
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| 866 | wqd(ig,1)=0. |
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| 867 | wqd(ig,nlay+1)=0. |
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| 868 | enddo |
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| 869 | |
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| 870 | ! Calcul des tendances |
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| 871 | do k=1,nlay |
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| 872 | do ig=1,ngrid |
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| 873 | q(ig,k)=q(ig,k)+(detr(ig,k)*qa(ig,k)-entr(ig,k)*q(ig,k) & |
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| 874 | & -wqd(ig,k)+wqd(ig,k+1)) & |
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| 875 | & *ptimestep/masse(ig,k) |
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| 876 | enddo |
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| 877 | enddo |
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| 878 | |
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| 879 | endif |
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| 880 | |
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| 881 | therm_tke_max(:,:)=q(:,:) |
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| 882 | |
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| 883 | return |
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| 884 | !!! fin nrlmd le 10/04/2012 |
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| 885 | end |
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| 886 | |
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