[4590] | 1 | MODULE lmdz_thermcell_main |
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[1403] | 2 | ! $Id: lmdz_thermcell_main.F90 4843 2024-03-04 17:58:03Z evignon $ |
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[878] | 3 | ! |
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[4678] | 4 | ! A REGARDER !!!!!!!!!!!!!!!!! |
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| 5 | ! ATTENTION : zpspsk est inout et out mais c'est pas forcement pour de bonnes raisons (FH, 2023) |
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[4690] | 6 | ! ATTENTION : dans thermcell_env, on condense potentiellement de l'eau. Mais comme on ne mélange pas l'eau liquide supposant qu'il n'y en n'a pas, c'est potentiellement un souci |
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[4590] | 7 | CONTAINS |
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| 8 | |
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[4089] | 9 | subroutine thermcell_main(itap,ngrid,nlay,ptimestep & |
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[878] | 10 | & ,pplay,pplev,pphi,debut & |
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[4690] | 11 | & ,puwind,pvwind,ptemp,p_o,ptemp_env, po_env & |
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[878] | 12 | & ,pduadj,pdvadj,pdtadj,pdoadj & |
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[1026] | 13 | & ,fm0,entr0,detr0,zqta,zqla,lmax & |
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[878] | 14 | & ,ratqscth,ratqsdiff,zqsatth & |
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[1403] | 15 | & ,zmax0, f0,zw2,fraca,ztv & |
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[4089] | 16 | & ,zpspsk,ztla,zthl,ztva & |
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[4843] | 17 | & ,pcon,rhobarz,wth3,wmax_sec,lalim,fm,alim_star,zmax,zcong & |
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[4089] | 18 | #ifdef ISO |
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| 19 | & ,xtpo,xtpdoadj & |
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| 20 | #endif |
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| 21 | & ) |
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[878] | 22 | |
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[4089] | 23 | |
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[4690] | 24 | |
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| 25 | ! USE necessaires pour les lignes importees de thermcell_env |
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[4590] | 26 | USE lmdz_thermcell_ini, ONLY: thermcell_ini,dqimpl,dvdq,prt_level,lunout,prt_level |
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| 27 | USE lmdz_thermcell_ini, ONLY: iflag_thermals_closure,iflag_thermals_ed,tau_thermals,r_aspect_thermals |
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| 28 | USE lmdz_thermcell_ini, ONLY: iflag_thermals_down,fact_thermals_down |
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[4690] | 29 | USE lmdz_thermcell_ini, ONLY: iflag_thermals_tenv |
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[4590] | 30 | USE lmdz_thermcell_ini, ONLY: RD,RG |
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[4089] | 31 | |
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[4590] | 32 | USE lmdz_thermcell_down, ONLY: thermcell_updown_dq |
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| 33 | USE lmdz_thermcell_closure, ONLY: thermcell_closure |
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| 34 | USE lmdz_thermcell_dq, ONLY: thermcell_dq |
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| 35 | USE lmdz_thermcell_dry, ONLY: thermcell_dry |
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| 36 | USE lmdz_thermcell_dv2, ONLY: thermcell_dv2 |
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| 37 | USE lmdz_thermcell_env, ONLY: thermcell_env |
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| 38 | USE lmdz_thermcell_flux2, ONLY: thermcell_flux2 |
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| 39 | USE lmdz_thermcell_height, ONLY: thermcell_height |
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| 40 | USE lmdz_thermcell_plume, ONLY: thermcell_plume |
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| 41 | USE lmdz_thermcell_plume_6A, ONLY: thermcell_plume_6A,thermcell_plume_5B |
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| 42 | |
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[4690] | 43 | ! USE necessaires pour les lignes importees de thermcell_env |
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| 44 | USE lmdz_thermcell_ini, ONLY : RLvCp,RKAPPA,RETV |
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| 45 | USE lmdz_thermcell_qsat, ONLY : thermcell_qsat |
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| 46 | |
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| 47 | |
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[4089] | 48 | #ifdef ISO |
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[4143] | 49 | USE infotrac_phy, ONLY : ntiso |
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[4089] | 50 | #ifdef ISOVERIF |
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| 51 | USE isotopes_mod, ONLY : iso_eau,iso_HDO |
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| 52 | USE isotopes_verif_mod, ONLY: iso_verif_egalite, & |
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| 53 | iso_verif_aberrant_encadre |
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| 54 | #endif |
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| 55 | #endif |
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| 56 | |
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| 57 | |
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[878] | 58 | IMPLICIT NONE |
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| 59 | |
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| 60 | !======================================================================= |
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| 61 | ! Auteurs: Frederic Hourdin, Catherine Rio, Anne Mathieu |
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| 62 | ! Version du 09.02.07 |
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| 63 | ! Calcul du transport vertical dans la couche limite en presence |
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| 64 | ! de "thermiques" explicitement representes avec processus nuageux |
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| 65 | ! |
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[1403] | 66 | ! Reecriture a partir d'un listing papier a Habas, le 14/02/00 |
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[878] | 67 | ! |
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[1403] | 68 | ! le thermique est suppose homogene et dissipe par melange avec |
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| 69 | ! son environnement. la longueur l_mix controle l'efficacite du |
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| 70 | ! melange |
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[878] | 71 | ! |
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[1403] | 72 | ! Le calcul du transport des differentes especes se fait en prenant |
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[878] | 73 | ! en compte: |
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| 74 | ! 1. un flux de masse montant |
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| 75 | ! 2. un flux de masse descendant |
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| 76 | ! 3. un entrainement |
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| 77 | ! 4. un detrainement |
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| 78 | ! |
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[1738] | 79 | ! Modif 2013/01/04 (FH hourdin@lmd.jussieu.fr) |
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| 80 | ! Introduction of an implicit computation of vertical advection in |
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| 81 | ! the environment of thermal plumes in thermcell_dq |
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| 82 | ! impl = 0 : explicit, 1 : implicit, -1 : old version |
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| 83 | ! controled by iflag_thermals = |
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| 84 | ! 15, 16 run with impl=-1 : numerical convergence with NPv3 |
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| 85 | ! 17, 18 run with impl=1 : more stable |
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| 86 | ! 15 and 17 correspond to the activation of the stratocumulus "bidouille" |
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| 87 | ! |
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[4133] | 88 | ! Using |
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| 89 | ! abort_physic |
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| 90 | ! iso_verif_aberrant_encadre |
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| 91 | ! iso_verif_egalite |
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| 92 | ! test_ltherm |
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| 93 | ! thermcell_closure |
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| 94 | ! thermcell_dq |
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| 95 | ! thermcell_dry |
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| 96 | ! thermcell_dv2 |
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| 97 | ! thermcell_env |
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| 98 | ! thermcell_flux2 |
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| 99 | ! thermcell_height |
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| 100 | ! thermcell_plume |
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| 101 | ! thermcell_plume_5B |
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| 102 | ! thermcell_plume_6A |
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| 103 | ! |
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[878] | 104 | !======================================================================= |
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| 105 | |
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[1738] | 106 | |
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[878] | 107 | !----------------------------------------------------------------------- |
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| 108 | ! declarations: |
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| 109 | ! ------------- |
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| 110 | |
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| 111 | |
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| 112 | ! arguments: |
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| 113 | ! ---------- |
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[4089] | 114 | integer, intent(in) :: itap,ngrid,nlay |
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| 115 | real, intent(in) :: ptimestep |
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[4690] | 116 | real, intent(in), dimension(ngrid,nlay) :: ptemp,puwind,pvwind,pplay,pphi,ptemp_env,po_env |
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[4678] | 117 | ! ATTENTION : zpspsk est inout et out mais c'est pas forcement pour de bonnes raisons (FH, 2023) |
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| 118 | real, intent(in), dimension(ngrid,nlay) :: p_o |
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[4590] | 119 | real, intent(out), dimension(ngrid,nlay) :: zpspsk |
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[4089] | 120 | real, intent(in), dimension(ngrid,nlay+1) :: pplev |
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[4133] | 121 | integer, intent(out), dimension(ngrid) :: lmax |
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[4089] | 122 | real, intent(out), dimension(ngrid,nlay) :: pdtadj,pduadj,pdvadj,pdoadj,entr0,detr0 |
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| 123 | real, intent(out), dimension(ngrid,nlay) :: ztla,zqla,zqta,zqsatth,zthl |
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| 124 | real, intent(out), dimension(ngrid,nlay+1) :: fm0,zw2,fraca |
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[4133] | 125 | real, intent(inout), dimension(ngrid) :: zmax0,f0 |
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[4089] | 126 | real, intent(out), dimension(ngrid,nlay) :: ztva,ztv |
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| 127 | logical, intent(in) :: debut |
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[4133] | 128 | real,intent(out), dimension(ngrid,nlay) :: ratqscth,ratqsdiff |
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[878] | 129 | |
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[4089] | 130 | real, intent(out), dimension(ngrid) :: pcon |
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| 131 | real, intent(out), dimension(ngrid,nlay) :: rhobarz,wth3 |
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| 132 | real, intent(out), dimension(ngrid) :: wmax_sec |
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| 133 | integer,intent(out), dimension(ngrid) :: lalim |
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| 134 | real, intent(out), dimension(ngrid,nlay+1) :: fm |
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| 135 | real, intent(out), dimension(ngrid,nlay) :: alim_star |
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[4843] | 136 | real, intent(out), dimension(ngrid) :: zmax,zcong |
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[972] | 137 | |
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[878] | 138 | ! local: |
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| 139 | ! ------ |
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| 140 | |
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[1738] | 141 | |
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[883] | 142 | integer,save :: igout=1 |
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[987] | 143 | !$OMP THREADPRIVATE(igout) |
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[938] | 144 | integer,save :: lunout1=6 |
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[987] | 145 | !$OMP THREADPRIVATE(lunout1) |
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[883] | 146 | integer,save :: lev_out=10 |
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[987] | 147 | !$OMP THREADPRIVATE(lev_out) |
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[878] | 148 | |
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[4089] | 149 | real lambda, zf,zf2,var,vardiff,CHI |
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| 150 | integer ig,k,l,ierr,ll |
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[878] | 151 | logical sorties |
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[4843] | 152 | real, dimension(ngrid) :: linter,zmix, zmax_sec,lintercong |
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| 153 | integer,dimension(ngrid) :: lmin,lmix,lmix_bis,nivcon, lcong |
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[4089] | 154 | real, dimension(ngrid,nlay) :: ztva_est |
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[4690] | 155 | real, dimension(ngrid,nlay) :: deltaz,zlay,zdthladj,zu,zv,z_o,zl,zva,zua,z_oa |
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| 156 | real, dimension(ngrid,nlay) :: ztemp_env ! temperarure liquide de l'environnement |
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[4089] | 157 | real, dimension(ngrid,nlay) :: zta,zha,q2,wq,wthl,wthv,thetath2,wth2 |
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[4133] | 158 | real, dimension(ngrid,nlay) :: rho,masse |
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[4089] | 159 | real, dimension(ngrid,nlay+1) :: zw_est,zlev |
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| 160 | real, dimension(ngrid) :: wmax,wmax_tmp |
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| 161 | real, dimension(ngrid,nlay+1) :: f_star |
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| 162 | real, dimension(ngrid,nlay) :: entr,detr,entr_star,detr_star,alim_star_clos |
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| 163 | real, dimension(ngrid,nlay) :: zqsat,csc |
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| 164 | real, dimension(ngrid) :: zcon,zcon2,alim_star_tot,f |
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[4413] | 165 | real, dimension(ngrid,nlay) :: entrdn,detrdn |
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[4690] | 166 | logical, dimension(ngrid,nlay) :: mask |
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[878] | 167 | |
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[4089] | 168 | character (len=20) :: modname='thermcell_main' |
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| 169 | character (len=80) :: abort_message |
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[878] | 170 | |
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| 171 | |
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[4089] | 172 | #ifdef ISO |
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[4143] | 173 | REAL xtpo(ntiso,ngrid,nlay),xtpdoadj(ntiso,ngrid,nlay) |
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| 174 | REAL xtzo(ntiso,ngrid,nlay) |
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[4089] | 175 | REAL xtpdoadj_tmp(ngrid,nlay) |
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| 176 | REAL xtpo_tmp(ngrid,nlay) |
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| 177 | REAL xtzo_tmp(ngrid,nlay) |
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| 178 | integer ixt |
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| 179 | #endif |
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[878] | 180 | |
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| 181 | ! |
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| 182 | |
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| 183 | !----------------------------------------------------------------------- |
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| 184 | ! initialisation: |
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| 185 | ! --------------- |
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| 186 | ! |
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[1943] | 187 | fm=0. ; entr=0. ; detr=0. |
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[972] | 188 | |
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[938] | 189 | if (prt_level.ge.1) print*,'thermcell_main V4' |
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[878] | 190 | |
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| 191 | sorties=.true. |
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[4089] | 192 | IF(ngrid.NE.ngrid) THEN |
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[878] | 193 | PRINT* |
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| 194 | PRINT*,'STOP dans convadj' |
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| 195 | PRINT*,'ngrid =',ngrid |
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[4089] | 196 | PRINT*,'ngrid =',ngrid |
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[878] | 197 | ENDIF |
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| 198 | ! |
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[4692] | 199 | !print*,'thermcell_main debut' |
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[1403] | 200 | ! write(lunout,*)'WARNING thermcell_main f0=max(f0,1.e-2)' |
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[4089] | 201 | do ig=1,ngrid |
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[972] | 202 | f0(ig)=max(f0(ig),1.e-2) |
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[1403] | 203 | zmax0(ig)=max(zmax0(ig),40.) |
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[972] | 204 | !IMmarche pas ?! if (f0(ig)<1.e-2) f0(ig)=1.e-2 |
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| 205 | enddo |
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[878] | 206 | |
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[1494] | 207 | if (prt_level.ge.20) then |
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| 208 | do ig=1,ngrid |
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| 209 | print*,'th_main ig f0',ig,f0(ig) |
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| 210 | enddo |
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| 211 | endif |
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[4690] | 212 | |
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[878] | 213 | !----------------------------------------------------------------------- |
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| 214 | ! Calcul de T,q,ql a partir de Tl et qT dans l environnement |
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| 215 | ! -------------------------------------------------------------------- |
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| 216 | ! |
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[4690] | 217 | ! On condense l'eau liquide si besoin. |
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| 218 | ! En fait on arrive ici d'habitude (jusque 6A) après réévaporation |
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| 219 | ! Dans une nouvelle mouture, on passe les profiles |
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| 220 | ! avant la couche limite : iflag_thermals_tenv=1 |
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| 221 | ! dés le début de la physique : iflag_thermals_tenv=2 |
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| 222 | ! Mais même pour 2) on ne veut sans doute pas réévaporer. |
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| 223 | ! On veut comparer thetav dans le thermique, après condensation, |
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| 224 | ! avec le theta_v effectif de l'environnement. |
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| 225 | |
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| 226 | if (iflag_thermals_tenv - 10 * ( iflag_thermals_tenv / 10 ) == 0) then |
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| 227 | |
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| 228 | CALL thermcell_env(ngrid,nlay,p_o,ptemp_env,puwind,pvwind,pplay, & |
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[4843] | 229 | & pplev,z_o,ztemp_env,zl,ztv,zthl,zu,zv,zpspsk,zqsat,lcong,lintercong,lev_out) |
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[4690] | 230 | |
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| 231 | else |
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| 232 | |
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| 233 | ! Chantier en cours : ne pas effacer (Fredho). 15 septembre 2023 |
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| 234 | ! Dans la version originale de thermcell_env, on condense l'eau de l'environnement |
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| 235 | ! pour calculer une temperature potentielle liquide. |
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| 236 | ! On en déduit un Theta v. |
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| 237 | |
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| 238 | ! ... |
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| 239 | ! contenu de thermcell_env |
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| 240 | ! SUBROUTINE thermcell_env(ngrid,nlay,po,pt,pu,pv,pplay, & |
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| 241 | ! & pplev,zo,zh,zl,ztv,zthl,zu,zv,zpspsk,pqsat,lev_out) |
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| 242 | ! contenu thermcell_env : call thermcell_qsat(ngrid*nlay,mask,pplev,pt,po,pqsat) |
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| 243 | ! contenu thermcell_env : do ll=1,nlay |
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| 244 | ! contenu thermcell_env : do ig=1,ngrid |
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| 245 | ! contenu thermcell_env : zl(ig,ll) = max(0.,po(ig,ll)-pqsat(ig,ll)) |
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| 246 | ! contenu thermcell_env : zh(ig,ll) = pt(ig,ll)+RLvCp*zl(ig,ll) ! T = Tl + Lv/Cp ql |
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| 247 | ! contenu thermcell_env : zo(ig,ll) = po(ig,ll)-zl(ig,ll) |
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| 248 | ! contenu thermcell_env : enddo |
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| 249 | ! contenu thermcell_env : enddo |
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| 250 | ! contenu thermcell_env : do ll=1,nlay |
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| 251 | ! contenu thermcell_env : do ig=1,ngrid |
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| 252 | ! contenu thermcell_env : zpspsk(ig,ll)=(pplay(ig,ll)/100000.)**RKAPPA |
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| 253 | ! contenu thermcell_env : zu(ig,ll)=pu(ig,ll) |
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| 254 | ! contenu thermcell_env : zv(ig,ll)=pv(ig,ll) |
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| 255 | ! contenu thermcell_env : ztv(ig,ll)=zh(ig,ll)/zpspsk(ig,ll) |
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| 256 | ! contenu thermcell_env : ztv(ig,ll)=ztv(ig,ll)*(1.+RETV*(zo(ig,ll))-zl(ig,ll)) |
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| 257 | ! contenu thermcell_env : zthl(ig,ll)=pt(ig,ll)/zpspsk(ig,ll) |
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| 258 | ! contenu thermcell_env : enddo |
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| 259 | ! contenu thermcell_env : enddo |
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| 260 | |
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| 261 | do l=1,nlay |
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| 262 | do ig=1,ngrid |
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| 263 | zl(ig,l)=0. |
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| 264 | zu(ig,l)=puwind(ig,l) |
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| 265 | zv(ig,l)=pvwind(ig,l) |
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| 266 | ztemp_env(ig,l)=ptemp_env(ig,l) |
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| 267 | zpspsk(ig,l)=(pplay(ig,l)/100000.)**RKAPPA |
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| 268 | ztv(ig,l)=ztemp_env(ig,l)/zpspsk(ig,l) |
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| 269 | ztv(ig,l)=ztv(ig,l)*(1.+RETV*po_env(ig,l)) |
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| 270 | zthl(ig,l)=ptemp(ig,l)/zpspsk(ig,l) |
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| 271 | mask(ig,l)=.true. |
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| 272 | enddo |
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| 273 | enddo |
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| 274 | call thermcell_qsat(ngrid*nlay,mask,pplev,ptemp_env,p_o,zqsat) |
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| 275 | |
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| 276 | endif |
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[878] | 277 | |
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[938] | 278 | if (prt_level.ge.1) print*,'thermcell_main apres thermcell_env' |
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[878] | 279 | |
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| 280 | !------------------------------------------------------------------------ |
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| 281 | ! -------------------- |
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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 | ! wa, fraca, wd, fracd -------------------- zlev(2), rhobarz |
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| 288 | ! wh,wt,wo ... |
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| 289 | ! |
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[4678] | 290 | ! + + + + + + + + + + + zh,zu,zv,z_o,rho |
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[878] | 291 | ! |
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| 292 | ! |
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| 293 | ! -------------------- zlev(1) |
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| 294 | ! \\\\\\\\\\\\\\\\\\\\ |
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| 295 | ! |
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| 296 | ! |
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| 297 | |
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| 298 | !----------------------------------------------------------------------- |
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| 299 | ! Calcul des altitudes des couches |
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| 300 | !----------------------------------------------------------------------- |
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| 301 | |
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| 302 | do l=2,nlay |
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| 303 | zlev(:,l)=0.5*(pphi(:,l)+pphi(:,l-1))/RG |
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| 304 | enddo |
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[4089] | 305 | zlev(:,1)=0. |
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| 306 | zlev(:,nlay+1)=(2.*pphi(:,nlay)-pphi(:,nlay-1))/RG |
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[878] | 307 | do l=1,nlay |
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| 308 | zlay(:,l)=pphi(:,l)/RG |
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| 309 | enddo |
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| 310 | do l=1,nlay |
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| 311 | deltaz(:,l)=zlev(:,l+1)-zlev(:,l) |
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| 312 | enddo |
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| 313 | |
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| 314 | !----------------------------------------------------------------------- |
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[4089] | 315 | ! Calcul des densites et masses |
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[878] | 316 | !----------------------------------------------------------------------- |
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| 317 | |
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[4089] | 318 | rho(:,:)=pplay(:,:)/(zpspsk(:,:)*RD*ztv(:,:)) |
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| 319 | if (prt_level.ge.10) write(lunout,*) 'WARNING thermcell_main rhobarz(:,1)=rho(:,1)' |
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[972] | 320 | rhobarz(:,1)=rho(:,1) |
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[878] | 321 | do l=2,nlay |
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| 322 | rhobarz(:,l)=0.5*(rho(:,l)+rho(:,l-1)) |
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| 323 | enddo |
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| 324 | do l=1,nlay |
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| 325 | masse(:,l)=(pplev(:,l)-pplev(:,l+1))/RG |
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| 326 | enddo |
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[938] | 327 | if (prt_level.ge.1) print*,'thermcell_main apres initialisation' |
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[878] | 328 | |
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| 329 | !------------------------------------------------------------------ |
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| 330 | ! |
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| 331 | ! /|\ |
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| 332 | ! -------- | F_k+1 ------- |
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| 333 | ! ----> D_k |
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| 334 | ! /|\ <---- E_k , A_k |
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| 335 | ! -------- | F_k --------- |
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| 336 | ! ----> D_k-1 |
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| 337 | ! <---- E_k-1 , A_k-1 |
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| 338 | ! |
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| 339 | ! |
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| 340 | ! |
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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 | ! ----- F_lmax+1=0 ---------- \ |
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| 346 | ! lmax (zmax) | |
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| 347 | ! --------------------------- | |
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| 348 | ! | |
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| 349 | ! --------------------------- | |
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| 350 | ! | |
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| 351 | ! --------------------------- | |
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| 352 | ! | |
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| 353 | ! --------------------------- | |
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| 354 | ! | |
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| 355 | ! --------------------------- | |
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| 356 | ! | E |
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| 357 | ! --------------------------- | D |
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| 358 | ! | |
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| 359 | ! --------------------------- | |
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| 360 | ! | |
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| 361 | ! --------------------------- \ | |
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| 362 | ! lalim | | |
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| 363 | ! --------------------------- | | |
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| 364 | ! | | |
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| 365 | ! --------------------------- | | |
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| 366 | ! | A | |
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| 367 | ! --------------------------- | | |
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| 368 | ! | | |
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| 369 | ! --------------------------- | | |
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| 370 | ! lmin (=1 pour le moment) | | |
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| 371 | ! ----- F_lmin=0 ------------ / / |
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| 372 | ! |
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| 373 | ! --------------------------- |
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| 374 | ! ////////////////////////// |
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| 375 | ! |
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| 376 | ! |
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| 377 | !============================================================================= |
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| 378 | ! Calculs initiaux ne faisant pas intervenir les changements de phase |
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| 379 | !============================================================================= |
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| 380 | |
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| 381 | !------------------------------------------------------------------ |
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[1403] | 382 | ! 1. alim_star est le profil vertical de l'alimentation a la base du |
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| 383 | ! panache thermique, calcule a partir de la flotabilite de l'air sec |
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[878] | 384 | ! 2. lmin et lalim sont les indices inferieurs et superieurs de alim_star |
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| 385 | !------------------------------------------------------------------ |
---|
| 386 | ! |
---|
| 387 | entr_star=0. ; detr_star=0. ; alim_star=0. ; alim_star_tot=0. |
---|
[1403] | 388 | lmin=1 |
---|
[878] | 389 | |
---|
| 390 | !----------------------------------------------------------------------------- |
---|
| 391 | ! 3. wmax_sec et zmax_sec sont les vitesses et altitudes maximum d'un |
---|
| 392 | ! panache sec conservatif (e=d=0) alimente selon alim_star |
---|
| 393 | ! Il s'agit d'un calcul de type CAPE |
---|
[1403] | 394 | ! zmax_sec est utilise pour determiner la geometrie du thermique. |
---|
[878] | 395 | !------------------------------------------------------------------------------ |
---|
[1403] | 396 | !--------------------------------------------------------------------------------- |
---|
| 397 | !calcul du melange et des variables dans le thermique |
---|
| 398 | !-------------------------------------------------------------------------------- |
---|
[878] | 399 | ! |
---|
[1403] | 400 | if (prt_level.ge.1) print*,'avant thermcell_plume ',lev_out |
---|
[878] | 401 | |
---|
[3451] | 402 | !===================================================================== |
---|
| 403 | ! Old version of thermcell_plume in thermcell_plume_6A.F90 |
---|
| 404 | ! It includes both thermcell_plume_6A and thermcell_plume_5B corresponding |
---|
| 405 | ! to the 5B and 6A versions used for CMIP5 and CMIP6. |
---|
| 406 | ! The latest was previously named thermcellV1_plume. |
---|
| 407 | ! The new thermcell_plume is a clean version (removing obsolete |
---|
| 408 | ! options) of thermcell_plume_6A. |
---|
| 409 | ! The 3 versions are controled by |
---|
| 410 | ! flag_thermals_ed <= 9 thermcell_plume_6A |
---|
| 411 | ! <= 19 thermcell_plume_5B |
---|
| 412 | ! else thermcell_plume (default 20 for convergence with 6A) |
---|
| 413 | ! Fredho |
---|
| 414 | !===================================================================== |
---|
[878] | 415 | |
---|
[1403] | 416 | if (iflag_thermals_ed<=9) then |
---|
| 417 | ! print*,'THERM NOUVELLE/NOUVELLE Arnaud' |
---|
[4678] | 418 | CALL thermcell_plume_6A(itap,ngrid,nlay,ptimestep,ztv,zthl,p_o,zl,rhobarz,& |
---|
[1403] | 419 | & zlev,pplev,pphi,zpspsk,alim_star,alim_star_tot, & |
---|
| 420 | & lalim,f0,detr_star,entr_star,f_star,csc,ztva, & |
---|
| 421 | & ztla,zqla,zqta,zha,zw2,zw_est,ztva_est,zqsatth,lmix,lmix_bis,linter & |
---|
| 422 | & ,lev_out,lunout1,igout) |
---|
[878] | 423 | |
---|
[3451] | 424 | elseif (iflag_thermals_ed<=19) then |
---|
[1403] | 425 | ! print*,'THERM RIO et al 2010, version d Arnaud' |
---|
[4678] | 426 | CALL thermcell_plume_5B(itap,ngrid,nlay,ptimestep,ztv,zthl,p_o,zl,rhobarz,& |
---|
[1403] | 427 | & zlev,pplev,pphi,zpspsk,alim_star,alim_star_tot, & |
---|
| 428 | & lalim,f0,detr_star,entr_star,f_star,csc,ztva, & |
---|
| 429 | & ztla,zqla,zqta,zha,zw2,zw_est,ztva_est,zqsatth,lmix,lmix_bis,linter & |
---|
| 430 | & ,lev_out,lunout1,igout) |
---|
[3451] | 431 | else |
---|
[4678] | 432 | CALL thermcell_plume(itap,ngrid,nlay,ptimestep,ztv,zthl,p_o,zl,rhobarz,& |
---|
[3451] | 433 | & zlev,pplev,pphi,zpspsk,alim_star,alim_star_tot, & |
---|
| 434 | & lalim,f0,detr_star,entr_star,f_star,csc,ztva, & |
---|
| 435 | & ztla,zqla,zqta,zha,zw2,zw_est,ztva_est,zqsatth,lmix,lmix_bis,linter & |
---|
| 436 | & ,lev_out,lunout1,igout) |
---|
[1403] | 437 | endif |
---|
[878] | 438 | |
---|
[972] | 439 | if (prt_level.ge.1) print*,'apres thermcell_plume ',lev_out |
---|
| 440 | |
---|
[4678] | 441 | call test_ltherm(ngrid,nlay,pplay,lalim,ztv,p_o,ztva,zqla,f_star,zw2,'thermcell_plum lalim ') |
---|
| 442 | call test_ltherm(ngrid,nlay,pplay,lmix ,ztv,p_o,ztva,zqla,f_star,zw2,'thermcell_plum lmix ') |
---|
[878] | 443 | |
---|
[938] | 444 | if (prt_level.ge.1) print*,'thermcell_main apres thermcell_plume' |
---|
| 445 | if (prt_level.ge.10) then |
---|
[972] | 446 | write(lunout1,*) 'Dans thermcell_main 2' |
---|
| 447 | write(lunout1,*) 'lmin ',lmin(igout) |
---|
| 448 | write(lunout1,*) 'lalim ',lalim(igout) |
---|
| 449 | write(lunout1,*) ' ig l alim_star entr_star detr_star f_star ' |
---|
| 450 | write(lunout1,'(i6,i4,4e15.5)') (igout,l,alim_star(igout,l),entr_star(igout,l),detr_star(igout,l) & |
---|
[878] | 451 | & ,f_star(igout,l+1),l=1,nint(linter(igout))+5) |
---|
| 452 | endif |
---|
| 453 | |
---|
| 454 | !------------------------------------------------------------------------------- |
---|
| 455 | ! Calcul des caracteristiques du thermique:zmax,zmix,wmax |
---|
| 456 | !------------------------------------------------------------------------------- |
---|
| 457 | ! |
---|
[4843] | 458 | CALL thermcell_height(ngrid,nlay,lalim,lmin,linter,lcong,lintercong,lmix,zw2, & |
---|
| 459 | & zlev,lmax,zmax,zmax0,zmix,wmax,zcong) |
---|
[1403] | 460 | ! Attention, w2 est transforme en sa racine carree dans cette routine |
---|
[4143] | 461 | ! Le probleme vient du fait que linter et lmix sont souvent egaux a 1. |
---|
[1403] | 462 | wmax_tmp=0. |
---|
| 463 | do l=1,nlay |
---|
| 464 | wmax_tmp(:)=max(wmax_tmp(:),zw2(:,l)) |
---|
| 465 | enddo |
---|
| 466 | ! print*,"ZMAX ",lalim,lmin,linter,lmix,lmax,zmax,zmax0,zmix,wmax |
---|
[878] | 467 | |
---|
| 468 | |
---|
[1403] | 469 | |
---|
[4678] | 470 | call test_ltherm(ngrid,nlay,pplay,lalim,ztv,p_o,ztva,zqla,f_star,zw2,'thermcell_heig lalim ') |
---|
| 471 | call test_ltherm(ngrid,nlay,pplay,lmin ,ztv,p_o,ztva,zqla,f_star,zw2,'thermcell_heig lmin ') |
---|
| 472 | call test_ltherm(ngrid,nlay,pplay,lmix ,ztv,p_o,ztva,zqla,f_star,zw2,'thermcell_heig lmix ') |
---|
| 473 | call test_ltherm(ngrid,nlay,pplay,lmax ,ztv,p_o,ztva,zqla,f_star,zw2,'thermcell_heig lmax ') |
---|
[878] | 474 | |
---|
[938] | 475 | if (prt_level.ge.1) print*,'thermcell_main apres thermcell_height' |
---|
[878] | 476 | |
---|
| 477 | !------------------------------------------------------------------------------- |
---|
| 478 | ! Fermeture,determination de f |
---|
| 479 | !------------------------------------------------------------------------------- |
---|
[1026] | 480 | ! |
---|
[1403] | 481 | ! |
---|
| 482 | CALL thermcell_dry(ngrid,nlay,zlev,pphi,ztv,alim_star, & |
---|
[4094] | 483 | & lalim,lmin,zmax_sec,wmax_sec) |
---|
[878] | 484 | |
---|
[1998] | 485 | |
---|
[4678] | 486 | call test_ltherm(ngrid,nlay,pplay,lmin,ztv,p_o,ztva,zqla,f_star,zw2,'thermcell_dry lmin ') |
---|
| 487 | call test_ltherm(ngrid,nlay,pplay,lalim,ztv,p_o,ztva,zqla,f_star,zw2,'thermcell_dry lalim ') |
---|
[1403] | 488 | |
---|
| 489 | if (prt_level.ge.1) print*,'thermcell_main apres thermcell_dry' |
---|
| 490 | if (prt_level.ge.10) then |
---|
| 491 | write(lunout1,*) 'Dans thermcell_main 1b' |
---|
| 492 | write(lunout1,*) 'lmin ',lmin(igout) |
---|
| 493 | write(lunout1,*) 'lalim ',lalim(igout) |
---|
| 494 | write(lunout1,*) ' ig l alim_star entr_star detr_star f_star ' |
---|
| 495 | write(lunout1,'(i6,i4,e15.5)') (igout,l,alim_star(igout,l) & |
---|
| 496 | & ,l=1,lalim(igout)+4) |
---|
| 497 | endif |
---|
| 498 | |
---|
| 499 | |
---|
| 500 | |
---|
| 501 | |
---|
| 502 | ! Choix de la fonction d'alimentation utilisee pour la fermeture. |
---|
| 503 | ! Apparemment sans importance |
---|
| 504 | alim_star_clos(:,:)=alim_star(:,:) |
---|
| 505 | alim_star_clos(:,:)=entr_star(:,:)+alim_star(:,:) |
---|
[1998] | 506 | ! |
---|
| 507 | !CR Appel de la fermeture seche |
---|
| 508 | if (iflag_thermals_closure.eq.1) then |
---|
[1403] | 509 | |
---|
[4094] | 510 | CALL thermcell_closure(ngrid,nlay,r_aspect_thermals,ptimestep,rho, & |
---|
| 511 | & zlev,lalim,alim_star_clos,zmax_sec,wmax_sec,f) |
---|
[878] | 512 | |
---|
[1403] | 513 | !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! |
---|
| 514 | ! Appel avec les zmax et wmax tenant compte de la condensation |
---|
| 515 | ! Semble moins bien marcher |
---|
[1998] | 516 | else if (iflag_thermals_closure.eq.2) then |
---|
| 517 | |
---|
| 518 | CALL thermcell_closure(ngrid,nlay,r_aspect_thermals,ptimestep,rho, & |
---|
[4094] | 519 | & zlev,lalim,alim_star,zmax,wmax,f) |
---|
[1998] | 520 | |
---|
[4094] | 521 | |
---|
[1998] | 522 | endif |
---|
| 523 | |
---|
[1403] | 524 | !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! |
---|
| 525 | |
---|
[938] | 526 | if(prt_level.ge.1)print*,'thermcell_closure apres thermcell_closure' |
---|
[878] | 527 | |
---|
[972] | 528 | if (tau_thermals>1.) then |
---|
| 529 | lambda=exp(-ptimestep/tau_thermals) |
---|
| 530 | f0=(1.-lambda)*f+lambda*f0 |
---|
| 531 | else |
---|
| 532 | f0=f |
---|
| 533 | endif |
---|
| 534 | |
---|
| 535 | ! Test valable seulement en 1D mais pas genant |
---|
| 536 | if (.not. (f0(1).ge.0.) ) then |
---|
[1403] | 537 | abort_message = '.not. (f0(1).ge.0.)' |
---|
[2311] | 538 | CALL abort_physic (modname,abort_message,1) |
---|
[972] | 539 | endif |
---|
| 540 | |
---|
[878] | 541 | !------------------------------------------------------------------------------- |
---|
| 542 | !deduction des flux |
---|
| 543 | |
---|
[972] | 544 | CALL thermcell_flux2(ngrid,nlay,ptimestep,masse, & |
---|
[878] | 545 | & lalim,lmax,alim_star, & |
---|
| 546 | & entr_star,detr_star,f,rhobarz,zlev,zw2,fm,entr, & |
---|
[972] | 547 | & detr,zqla,lev_out,lunout1,igout) |
---|
[4318] | 548 | |
---|
[972] | 549 | !IM 060508 & detr,zqla,zmax,lev_out,lunout,igout) |
---|
[878] | 550 | |
---|
[938] | 551 | if (prt_level.ge.1) print*,'thermcell_main apres thermcell_flux' |
---|
[4678] | 552 | call test_ltherm(ngrid,nlay,pplay,lalim,ztv,p_o,ztva,zqla,f_star,zw2,'thermcell_flux lalim ') |
---|
| 553 | call test_ltherm(ngrid,nlay,pplay,lmax ,ztv,p_o,ztva,zqla,f_star,zw2,'thermcell_flux lmax ') |
---|
[878] | 554 | |
---|
| 555 | !------------------------------------------------------------------ |
---|
[972] | 556 | ! On ne prend pas directement les profils issus des calculs precedents |
---|
| 557 | ! mais on s'autorise genereusement une relaxation vers ceci avec |
---|
| 558 | ! une constante de temps tau_thermals (typiquement 1800s). |
---|
| 559 | !------------------------------------------------------------------ |
---|
[878] | 560 | |
---|
[972] | 561 | if (tau_thermals>1.) then |
---|
| 562 | lambda=exp(-ptimestep/tau_thermals) |
---|
| 563 | fm0=(1.-lambda)*fm+lambda*fm0 |
---|
| 564 | entr0=(1.-lambda)*entr+lambda*entr0 |
---|
[1403] | 565 | detr0=(1.-lambda)*detr+lambda*detr0 |
---|
[878] | 566 | else |
---|
| 567 | fm0=fm |
---|
| 568 | entr0=entr |
---|
| 569 | detr0=detr |
---|
| 570 | endif |
---|
| 571 | |
---|
[4396] | 572 | !------------------------------------------------------------------ |
---|
| 573 | ! Calcul de la fraction de l'ascendance |
---|
| 574 | !------------------------------------------------------------------ |
---|
| 575 | do ig=1,ngrid |
---|
| 576 | fraca(ig,1)=0. |
---|
| 577 | fraca(ig,nlay+1)=0. |
---|
| 578 | enddo |
---|
| 579 | do l=2,nlay |
---|
| 580 | do ig=1,ngrid |
---|
| 581 | if (zw2(ig,l).gt.1.e-10) then |
---|
| 582 | fraca(ig,l)=fm(ig,l)/(rhobarz(ig,l)*zw2(ig,l)) |
---|
| 583 | else |
---|
| 584 | fraca(ig,l)=0. |
---|
| 585 | endif |
---|
| 586 | enddo |
---|
| 587 | enddo |
---|
| 588 | |
---|
[972] | 589 | !c------------------------------------------------------------------ |
---|
| 590 | ! calcul du transport vertical |
---|
| 591 | !------------------------------------------------------------------ |
---|
[4381] | 592 | IF (iflag_thermals_down .GT. 0) THEN |
---|
[4438] | 593 | if (debut) print*,'WARNING !!! routine thermcell_down en cours de developpement' |
---|
[4441] | 594 | entrdn=fact_thermals_down*detr0 |
---|
| 595 | detrdn=fact_thermals_down*entr0 |
---|
[4413] | 596 | ! we want to transport potential temperature, total water and momentum |
---|
| 597 | CALL thermcell_updown_dq(ngrid,nlay,ptimestep,lmax,entr0,detr0,entrdn,detrdn,masse,zthl,zdthladj) |
---|
[4678] | 598 | CALL thermcell_updown_dq(ngrid,nlay,ptimestep,lmax,entr0,detr0,entrdn,detrdn,masse,p_o,pdoadj) |
---|
[4413] | 599 | CALL thermcell_updown_dq(ngrid,nlay,ptimestep,lmax,entr0,detr0,entrdn,detrdn,masse,zu,pduadj) |
---|
| 600 | CALL thermcell_updown_dq(ngrid,nlay,ptimestep,lmax,entr0,detr0,entrdn,detrdn,masse,zv,pdvadj) |
---|
[4396] | 601 | ELSE |
---|
[4381] | 602 | !-------------------------------------------------------------- |
---|
[972] | 603 | |
---|
[4690] | 604 | ! Temperature potentielle liquide effectivement mélangée par les thermiques |
---|
| 605 | do ll=1,nlay |
---|
| 606 | do ig=1,ngrid |
---|
| 607 | zthl(ig,ll)=ptemp(ig,ll)/zpspsk(ig,ll) |
---|
| 608 | enddo |
---|
| 609 | enddo |
---|
[4396] | 610 | call thermcell_dq(ngrid,nlay,dqimpl,ptimestep,fm0,entr0,masse, & |
---|
| 611 | & zthl,zdthladj,zta,lev_out) |
---|
[4678] | 612 | |
---|
| 613 | do ll=1,nlay |
---|
| 614 | do ig=1,ngrid |
---|
| 615 | z_o(ig,ll)=p_o(ig,ll) |
---|
| 616 | enddo |
---|
| 617 | enddo |
---|
[4396] | 618 | call thermcell_dq(ngrid,nlay,dqimpl,ptimestep,fm0,entr0,masse, & |
---|
[4678] | 619 | & z_o,pdoadj,z_oa,lev_out) |
---|
[878] | 620 | |
---|
[4089] | 621 | #ifdef ISO |
---|
[4143] | 622 | ! C Risi: on utilise directement la meme routine |
---|
| 623 | do ixt=1,ntiso |
---|
[4089] | 624 | do ll=1,nlay |
---|
| 625 | DO ig=1,ngrid |
---|
| 626 | xtpo_tmp(ig,ll)=xtpo(ixt,ig,ll) |
---|
| 627 | xtzo_tmp(ig,ll)=xtzo(ixt,ig,ll) |
---|
| 628 | enddo |
---|
| 629 | enddo |
---|
| 630 | call thermcell_dq(ngrid,nlay,dqimpl,ptimestep,fm0,entr0,masse, & |
---|
| 631 | & xtpo_tmp,xtpdoadj_tmp,xtzo_tmp,lev_out) |
---|
| 632 | do ll=1,nlay |
---|
| 633 | DO ig=1,ngrid |
---|
| 634 | xtpdoadj(ixt,ig,ll)=xtpdoadj_tmp(ig,ll) |
---|
| 635 | enddo |
---|
| 636 | enddo |
---|
[4143] | 637 | enddo |
---|
[4089] | 638 | #endif |
---|
| 639 | |
---|
| 640 | #ifdef ISO |
---|
| 641 | #ifdef ISOVERIF |
---|
| 642 | DO ll=1,nlay |
---|
| 643 | DO ig=1,ngrid |
---|
| 644 | if (iso_eau.gt.0) then |
---|
| 645 | call iso_verif_egalite(xtpo(iso_eau,ig,ll), & |
---|
[4680] | 646 | & p_o(ig,ll),'thermcell_main 594') |
---|
[4089] | 647 | call iso_verif_egalite(xtpdoadj(iso_eau,ig,ll), & |
---|
| 648 | & pdoadj(ig,ll),'thermcell_main 596') |
---|
| 649 | endif |
---|
| 650 | if (iso_HDO.gt.0) then |
---|
| 651 | call iso_verif_aberrant_encadre(xtpo(iso_hdo,ig,ll) & |
---|
[4678] | 652 | & /p_o(ig,ll),'thermcell_main 610') |
---|
[4089] | 653 | endif |
---|
| 654 | enddo |
---|
| 655 | enddo !DO ll=1,nlay |
---|
| 656 | write(*,*) 'thermcell_main 600 tmp: apres thermcell_dq' |
---|
| 657 | #endif |
---|
| 658 | #endif |
---|
| 659 | |
---|
| 660 | |
---|
[883] | 661 | !------------------------------------------------------------------ |
---|
| 662 | ! calcul du transport vertical du moment horizontal |
---|
| 663 | !------------------------------------------------------------------ |
---|
[878] | 664 | |
---|
[972] | 665 | !IM 090508 |
---|
[1738] | 666 | if (dvdq == 0 ) then |
---|
[883] | 667 | |
---|
[878] | 668 | ! Calcul du transport de V tenant compte d'echange par gradient |
---|
| 669 | ! de pression horizontal avec l'environnement |
---|
| 670 | |
---|
| 671 | call thermcell_dv2(ngrid,nlay,ptimestep,fm0,entr0,masse & |
---|
[1738] | 672 | ! & ,fraca*dvdq,zmax & |
---|
| 673 | & ,fraca,zmax & |
---|
[972] | 674 | & ,zu,zv,pduadj,pdvadj,zua,zva,lev_out) |
---|
[1403] | 675 | |
---|
[878] | 676 | else |
---|
| 677 | |
---|
| 678 | ! calcul purement conservatif pour le transport de V |
---|
[1738] | 679 | call thermcell_dq(ngrid,nlay,dqimpl,ptimestep,fm0,entr0,masse & |
---|
[878] | 680 | & ,zu,pduadj,zua,lev_out) |
---|
[1738] | 681 | call thermcell_dq(ngrid,nlay,dqimpl,ptimestep,fm0,entr0,masse & |
---|
[878] | 682 | & ,zv,pdvadj,zva,lev_out) |
---|
[1738] | 683 | |
---|
[878] | 684 | endif |
---|
[4396] | 685 | ENDIF |
---|
[878] | 686 | |
---|
| 687 | ! print*,'13 OK convect8' |
---|
| 688 | do l=1,nlay |
---|
| 689 | do ig=1,ngrid |
---|
| 690 | pdtadj(ig,l)=zdthladj(ig,l)*zpspsk(ig,l) |
---|
| 691 | enddo |
---|
| 692 | enddo |
---|
| 693 | |
---|
[972] | 694 | if (prt_level.ge.1) print*,'14 OK convect8' |
---|
[878] | 695 | !------------------------------------------------------------------ |
---|
| 696 | ! Calculs de diagnostiques pour les sorties |
---|
| 697 | !------------------------------------------------------------------ |
---|
| 698 | !calcul de fraca pour les sorties |
---|
| 699 | |
---|
| 700 | if (sorties) then |
---|
[972] | 701 | if (prt_level.ge.1) print*,'14a OK convect8' |
---|
[878] | 702 | ! calcul du niveau de condensation |
---|
| 703 | ! initialisation |
---|
| 704 | do ig=1,ngrid |
---|
[879] | 705 | nivcon(ig)=0 |
---|
[878] | 706 | zcon(ig)=0. |
---|
| 707 | enddo |
---|
| 708 | !nouveau calcul |
---|
| 709 | do ig=1,ngrid |
---|
[4690] | 710 | ! WARNING !!! verifier que c'est bien ztemp_env qu'on veut là |
---|
| 711 | CHI=ztemp_env(ig,1)/(1669.0-122.0*z_o(ig,1)/zqsat(ig,1)-ztemp_env(ig,1)) |
---|
[4678] | 712 | pcon(ig)=pplay(ig,1)*(z_o(ig,1)/zqsat(ig,1))**CHI |
---|
[878] | 713 | enddo |
---|
[1403] | 714 | !IM do k=1,nlay |
---|
| 715 | do k=1,nlay-1 |
---|
[878] | 716 | do ig=1,ngrid |
---|
| 717 | if ((pcon(ig).le.pplay(ig,k)) & |
---|
| 718 | & .and.(pcon(ig).gt.pplay(ig,k+1))) then |
---|
| 719 | zcon2(ig)=zlay(ig,k)-(pcon(ig)-pplay(ig,k))/(RG*rho(ig,k))/100. |
---|
| 720 | endif |
---|
| 721 | enddo |
---|
| 722 | enddo |
---|
[1403] | 723 | !IM |
---|
[1494] | 724 | ierr=0 |
---|
[1403] | 725 | do ig=1,ngrid |
---|
| 726 | if (pcon(ig).le.pplay(ig,nlay)) then |
---|
| 727 | zcon2(ig)=zlay(ig,nlay)-(pcon(ig)-pplay(ig,nlay))/(RG*rho(ig,nlay))/100. |
---|
[1494] | 728 | ierr=1 |
---|
| 729 | endif |
---|
| 730 | enddo |
---|
[4843] | 731 | ! if (ierr==1) then |
---|
| 732 | ! abort_message = 'thermcellV0_main: les thermiques vont trop haut ' |
---|
| 733 | ! CALL abort_physic (modname,abort_message,1) |
---|
| 734 | ! endif |
---|
[1494] | 735 | |
---|
[972] | 736 | if (prt_level.ge.1) print*,'14b OK convect8' |
---|
[878] | 737 | do k=nlay,1,-1 |
---|
| 738 | do ig=1,ngrid |
---|
| 739 | if (zqla(ig,k).gt.1e-10) then |
---|
| 740 | nivcon(ig)=k |
---|
| 741 | zcon(ig)=zlev(ig,k) |
---|
| 742 | endif |
---|
| 743 | enddo |
---|
| 744 | enddo |
---|
[972] | 745 | if (prt_level.ge.1) print*,'14c OK convect8' |
---|
[878] | 746 | !calcul des moments |
---|
| 747 | !initialisation |
---|
| 748 | do l=1,nlay |
---|
| 749 | do ig=1,ngrid |
---|
| 750 | q2(ig,l)=0. |
---|
| 751 | wth2(ig,l)=0. |
---|
| 752 | wth3(ig,l)=0. |
---|
| 753 | ratqscth(ig,l)=0. |
---|
| 754 | ratqsdiff(ig,l)=0. |
---|
| 755 | enddo |
---|
| 756 | enddo |
---|
[972] | 757 | if (prt_level.ge.1) print*,'14d OK convect8' |
---|
[1146] | 758 | if (prt_level.ge.10)write(lunout,*) & |
---|
| 759 | & 'WARNING thermcell_main wth2=0. si zw2 > 1.e-10' |
---|
[878] | 760 | do l=1,nlay |
---|
| 761 | do ig=1,ngrid |
---|
| 762 | zf=fraca(ig,l) |
---|
| 763 | zf2=zf/(1.-zf) |
---|
[972] | 764 | ! |
---|
[1403] | 765 | thetath2(ig,l)=zf2*(ztla(ig,l)-zthl(ig,l))**2 |
---|
[972] | 766 | if(zw2(ig,l).gt.1.e-10) then |
---|
| 767 | wth2(ig,l)=zf2*(zw2(ig,l))**2 |
---|
| 768 | else |
---|
| 769 | wth2(ig,l)=0. |
---|
| 770 | endif |
---|
[878] | 771 | wth3(ig,l)=zf2*(1-2.*fraca(ig,l))/(1-fraca(ig,l)) & |
---|
| 772 | & *zw2(ig,l)*zw2(ig,l)*zw2(ig,l) |
---|
[4678] | 773 | q2(ig,l)=zf2*(zqta(ig,l)*1000.-p_o(ig,l)*1000.)**2 |
---|
| 774 | !test: on calcul q2/p_o=ratqsc |
---|
| 775 | ratqscth(ig,l)=sqrt(max(q2(ig,l),1.e-6)/(p_o(ig,l)*1000.)) |
---|
[878] | 776 | enddo |
---|
| 777 | enddo |
---|
[1403] | 778 | !calcul des flux: q, thetal et thetav |
---|
| 779 | do l=1,nlay |
---|
| 780 | do ig=1,ngrid |
---|
[4678] | 781 | wq(ig,l)=fraca(ig,l)*zw2(ig,l)*(zqta(ig,l)*1000.-p_o(ig,l)*1000.) |
---|
[1403] | 782 | wthl(ig,l)=fraca(ig,l)*zw2(ig,l)*(ztla(ig,l)-zthl(ig,l)) |
---|
| 783 | wthv(ig,l)=fraca(ig,l)*zw2(ig,l)*(ztva(ig,l)-ztv(ig,l)) |
---|
| 784 | enddo |
---|
[879] | 785 | enddo |
---|
[1638] | 786 | |
---|
[878] | 787 | !calcul du ratqscdiff |
---|
[972] | 788 | if (prt_level.ge.1) print*,'14e OK convect8' |
---|
[878] | 789 | var=0. |
---|
| 790 | vardiff=0. |
---|
| 791 | ratqsdiff(:,:)=0. |
---|
[1494] | 792 | |
---|
[4089] | 793 | do l=1,nlay |
---|
[1494] | 794 | do ig=1,ngrid |
---|
| 795 | if (l<=lalim(ig)) then |
---|
[878] | 796 | var=var+alim_star(ig,l)*zqta(ig,l)*1000. |
---|
[1494] | 797 | endif |
---|
[878] | 798 | enddo |
---|
| 799 | enddo |
---|
[1494] | 800 | |
---|
[972] | 801 | if (prt_level.ge.1) print*,'14f OK convect8' |
---|
[1494] | 802 | |
---|
[4089] | 803 | do l=1,nlay |
---|
[1494] | 804 | do ig=1,ngrid |
---|
| 805 | if (l<=lalim(ig)) then |
---|
| 806 | zf=fraca(ig,l) |
---|
| 807 | zf2=zf/(1.-zf) |
---|
| 808 | vardiff=vardiff+alim_star(ig,l)*(zqta(ig,l)*1000.-var)**2 |
---|
| 809 | endif |
---|
| 810 | enddo |
---|
[878] | 811 | enddo |
---|
[1494] | 812 | |
---|
[972] | 813 | if (prt_level.ge.1) print*,'14g OK convect8' |
---|
[4089] | 814 | do l=1,nlay |
---|
| 815 | do ig=1,ngrid |
---|
[4678] | 816 | ratqsdiff(ig,l)=sqrt(vardiff)/(p_o(ig,l)*1000.) |
---|
[4089] | 817 | enddo |
---|
| 818 | enddo |
---|
[878] | 819 | endif |
---|
| 820 | |
---|
[938] | 821 | if (prt_level.ge.1) print*,'thermcell_main FIN OK' |
---|
[878] | 822 | |
---|
[4692] | 823 | !print*,'thermcell_main fin' |
---|
[4094] | 824 | RETURN |
---|
[4089] | 825 | end subroutine thermcell_main |
---|
[878] | 826 | |
---|
[4089] | 827 | !============================================================================= |
---|
| 828 | !///////////////////////////////////////////////////////////////////////////// |
---|
| 829 | !============================================================================= |
---|
[4678] | 830 | subroutine test_ltherm(ngrid,nlay,pplay,long,ztv,p_o,ztva, & ! in |
---|
[4089] | 831 | & zqla,f_star,zw2,comment) ! in |
---|
| 832 | !============================================================================= |
---|
[4590] | 833 | USE lmdz_thermcell_ini, ONLY: prt_level |
---|
[938] | 834 | IMPLICIT NONE |
---|
[878] | 835 | |
---|
[4089] | 836 | integer i, k, ngrid,nlay |
---|
[4678] | 837 | real, intent(in), dimension(ngrid,nlay) :: pplay,ztv,p_o,ztva,zqla |
---|
[4089] | 838 | real, intent(in), dimension(ngrid,nlay) :: f_star,zw2 |
---|
| 839 | integer, intent(in), dimension(ngrid) :: long |
---|
[878] | 840 | real seuil |
---|
| 841 | character*21 comment |
---|
[4133] | 842 | |
---|
[4089] | 843 | seuil=0.25 |
---|
[878] | 844 | |
---|
[938] | 845 | if (prt_level.ge.1) THEN |
---|
| 846 | print*,'WARNING !!! TEST ',comment |
---|
| 847 | endif |
---|
[879] | 848 | return |
---|
| 849 | |
---|
[878] | 850 | ! test sur la hauteur des thermiques ... |
---|
[4089] | 851 | do i=1,ngrid |
---|
[972] | 852 | !IMtemp if (pplay(i,long(i)).lt.seuil*pplev(i,1)) then |
---|
| 853 | if (prt_level.ge.10) then |
---|
[878] | 854 | print*,'WARNING ',comment,' au point ',i,' K= ',long(i) |
---|
| 855 | print*,' K P(MB) THV(K) Qenv(g/kg)THVA QLA(g/kg) F* W2' |
---|
[4089] | 856 | do k=1,nlay |
---|
[4678] | 857 | write(6,'(i3,7f10.3)') k,pplay(i,k),ztv(i,k),1000*p_o(i,k),ztva(i,k),1000*zqla(i,k),f_star(i,k),zw2(i,k) |
---|
[878] | 858 | enddo |
---|
[972] | 859 | endif |
---|
[878] | 860 | enddo |
---|
| 861 | |
---|
| 862 | |
---|
| 863 | return |
---|
| 864 | end |
---|
| 865 | |
---|
[4089] | 866 | ! nrlmd le 10/04/2012 Transport de la TKE par le thermique moyen pour la fermeture en ALP |
---|
| 867 | ! On transporte pbl_tke pour donner therm_tke |
---|
[4143] | 868 | ! Copie conforme de la subroutine DTKE dans physiq.F ecrite par Frederic Hourdin |
---|
[4089] | 869 | |
---|
| 870 | !======================================================================= |
---|
| 871 | !/////////////////////////////////////////////////////////////////////// |
---|
| 872 | !======================================================================= |
---|
| 873 | |
---|
| 874 | subroutine thermcell_tke_transport( & |
---|
| 875 | & ngrid,nlay,ptimestep,fm0,entr0,rg,pplev, & ! in |
---|
| 876 | & therm_tke_max) ! out |
---|
[4590] | 877 | USE lmdz_thermcell_ini, ONLY: prt_level |
---|
[1638] | 878 | implicit none |
---|
| 879 | |
---|
| 880 | !======================================================================= |
---|
| 881 | ! |
---|
| 882 | ! Calcul du transport verticale dans la couche limite en presence |
---|
| 883 | ! de "thermiques" explicitement representes |
---|
| 884 | ! calcul du dq/dt une fois qu'on connait les ascendances |
---|
| 885 | ! |
---|
| 886 | !======================================================================= |
---|
| 887 | |
---|
[4089] | 888 | integer ngrid,nlay |
---|
[1638] | 889 | |
---|
[4089] | 890 | real, intent(in) :: ptimestep |
---|
| 891 | real, intent(in), dimension(ngrid,nlay+1) :: fm0,pplev |
---|
| 892 | real, intent(in), dimension(ngrid,nlay) :: entr0 |
---|
| 893 | real, intent(in) :: rg |
---|
| 894 | real, intent(out), dimension(ngrid,nlay) :: therm_tke_max |
---|
| 895 | |
---|
[1638] | 896 | real detr0(ngrid,nlay) |
---|
[4089] | 897 | real masse0(ngrid,nlay) |
---|
[1638] | 898 | real masse(ngrid,nlay),fm(ngrid,nlay+1) |
---|
| 899 | real entr(ngrid,nlay) |
---|
| 900 | real q(ngrid,nlay) |
---|
| 901 | integer lev_out ! niveau pour les print |
---|
| 902 | |
---|
| 903 | real qa(ngrid,nlay),detr(ngrid,nlay),wqd(ngrid,nlay+1) |
---|
| 904 | integer ig,k |
---|
| 905 | |
---|
| 906 | |
---|
| 907 | lev_out=0 |
---|
| 908 | |
---|
| 909 | |
---|
| 910 | if (prt_level.ge.1) print*,'Q2 THERMCEL_DQ 0' |
---|
| 911 | |
---|
| 912 | ! calcul du detrainement |
---|
| 913 | do k=1,nlay |
---|
| 914 | detr0(:,k)=fm0(:,k)-fm0(:,k+1)+entr0(:,k) |
---|
| 915 | masse0(:,k)=(pplev(:,k)-pplev(:,k+1))/RG |
---|
| 916 | enddo |
---|
| 917 | |
---|
| 918 | |
---|
| 919 | ! Decalage vertical des entrainements et detrainements. |
---|
| 920 | masse(:,1)=0.5*masse0(:,1) |
---|
| 921 | entr(:,1)=0.5*entr0(:,1) |
---|
| 922 | detr(:,1)=0.5*detr0(:,1) |
---|
| 923 | fm(:,1)=0. |
---|
| 924 | do k=1,nlay-1 |
---|
| 925 | masse(:,k+1)=0.5*(masse0(:,k)+masse0(:,k+1)) |
---|
| 926 | entr(:,k+1)=0.5*(entr0(:,k)+entr0(:,k+1)) |
---|
| 927 | detr(:,k+1)=0.5*(detr0(:,k)+detr0(:,k+1)) |
---|
| 928 | fm(:,k+1)=fm(:,k)+entr(:,k)-detr(:,k) |
---|
| 929 | enddo |
---|
| 930 | fm(:,nlay+1)=0. |
---|
| 931 | |
---|
| 932 | |
---|
| 933 | q(:,:)=therm_tke_max(:,:) |
---|
| 934 | !!! nrlmd le 16/09/2010 |
---|
| 935 | do ig=1,ngrid |
---|
| 936 | qa(ig,1)=q(ig,1) |
---|
| 937 | enddo |
---|
| 938 | !!! |
---|
| 939 | |
---|
| 940 | if (1==1) then |
---|
| 941 | do k=2,nlay |
---|
| 942 | do ig=1,ngrid |
---|
| 943 | if ((fm(ig,k+1)+detr(ig,k))*ptimestep.gt. & |
---|
| 944 | & 1.e-5*masse(ig,k)) then |
---|
| 945 | qa(ig,k)=(fm(ig,k)*qa(ig,k-1)+entr(ig,k)*q(ig,k)) & |
---|
| 946 | & /(fm(ig,k+1)+detr(ig,k)) |
---|
| 947 | else |
---|
| 948 | qa(ig,k)=q(ig,k) |
---|
| 949 | endif |
---|
| 950 | if (qa(ig,k).lt.0.) then |
---|
| 951 | ! print*,'qa<0!!!' |
---|
| 952 | endif |
---|
| 953 | if (q(ig,k).lt.0.) then |
---|
| 954 | ! print*,'q<0!!!' |
---|
| 955 | endif |
---|
| 956 | enddo |
---|
| 957 | enddo |
---|
| 958 | |
---|
| 959 | ! Calcul du flux subsident |
---|
| 960 | |
---|
| 961 | do k=2,nlay |
---|
| 962 | do ig=1,ngrid |
---|
| 963 | wqd(ig,k)=fm(ig,k)*q(ig,k) |
---|
| 964 | if (wqd(ig,k).lt.0.) then |
---|
| 965 | ! print*,'wqd<0!!!' |
---|
| 966 | endif |
---|
| 967 | enddo |
---|
| 968 | enddo |
---|
| 969 | do ig=1,ngrid |
---|
| 970 | wqd(ig,1)=0. |
---|
| 971 | wqd(ig,nlay+1)=0. |
---|
| 972 | enddo |
---|
| 973 | |
---|
| 974 | ! Calcul des tendances |
---|
| 975 | do k=1,nlay |
---|
| 976 | do ig=1,ngrid |
---|
| 977 | q(ig,k)=q(ig,k)+(detr(ig,k)*qa(ig,k)-entr(ig,k)*q(ig,k) & |
---|
| 978 | & -wqd(ig,k)+wqd(ig,k+1)) & |
---|
| 979 | & *ptimestep/masse(ig,k) |
---|
| 980 | enddo |
---|
| 981 | enddo |
---|
| 982 | |
---|
| 983 | endif |
---|
| 984 | |
---|
| 985 | therm_tke_max(:,:)=q(:,:) |
---|
| 986 | |
---|
| 987 | return |
---|
| 988 | !!! fin nrlmd le 10/04/2012 |
---|
| 989 | end |
---|
| 990 | |
---|
[4590] | 991 | END MODULE lmdz_thermcell_main |
---|