[4590] | 1 | MODULE lmdz_thermcell_main |
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[1403] | 2 | ! $Id: lmdz_thermcell_main.F90 4684 2023-09-11 13:18:47Z 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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[4590] | 6 | CONTAINS |
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| 7 | |
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[4089] | 8 | subroutine thermcell_main(itap,ngrid,nlay,ptimestep & |
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[878] | 9 | & ,pplay,pplev,pphi,debut & |
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[4684] | 10 | & ,puwind,pvwind,ptemp,p_o & |
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[878] | 11 | & ,pduadj,pdvadj,pdtadj,pdoadj & |
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[1026] | 12 | & ,fm0,entr0,detr0,zqta,zqla,lmax & |
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[878] | 13 | & ,ratqscth,ratqsdiff,zqsatth & |
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[1403] | 14 | & ,zmax0, f0,zw2,fraca,ztv & |
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[4089] | 15 | & ,zpspsk,ztla,zthl,ztva & |
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| 16 | & ,pcon,rhobarz,wth3,wmax_sec,lalim,fm,alim_star,zmax & |
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| 17 | #ifdef ISO |
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| 18 | & ,xtpo,xtpdoadj & |
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| 19 | #endif |
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| 20 | & ) |
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[878] | 21 | |
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[4089] | 22 | |
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[4590] | 23 | USE lmdz_thermcell_ini, ONLY: thermcell_ini,dqimpl,dvdq,prt_level,lunout,prt_level |
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| 24 | USE lmdz_thermcell_ini, ONLY: iflag_thermals_closure,iflag_thermals_ed,tau_thermals,r_aspect_thermals |
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| 25 | USE lmdz_thermcell_ini, ONLY: iflag_thermals_down,fact_thermals_down |
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| 26 | USE lmdz_thermcell_ini, ONLY: RD,RG |
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[4089] | 27 | |
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[4590] | 28 | USE lmdz_thermcell_down, ONLY: thermcell_updown_dq |
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| 29 | USE lmdz_thermcell_closure, ONLY: thermcell_closure |
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| 30 | USE lmdz_thermcell_dq, ONLY: thermcell_dq |
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| 31 | USE lmdz_thermcell_dry, ONLY: thermcell_dry |
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| 32 | USE lmdz_thermcell_dv2, ONLY: thermcell_dv2 |
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| 33 | USE lmdz_thermcell_env, ONLY: thermcell_env |
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| 34 | USE lmdz_thermcell_flux2, ONLY: thermcell_flux2 |
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| 35 | USE lmdz_thermcell_height, ONLY: thermcell_height |
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| 36 | USE lmdz_thermcell_plume, ONLY: thermcell_plume |
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| 37 | USE lmdz_thermcell_plume_6A, ONLY: thermcell_plume_6A,thermcell_plume_5B |
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| 38 | |
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[4089] | 39 | #ifdef ISO |
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[4143] | 40 | USE infotrac_phy, ONLY : ntiso |
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[4089] | 41 | #ifdef ISOVERIF |
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| 42 | USE isotopes_mod, ONLY : iso_eau,iso_HDO |
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| 43 | USE isotopes_verif_mod, ONLY: iso_verif_egalite, & |
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| 44 | iso_verif_aberrant_encadre |
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| 45 | #endif |
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| 46 | #endif |
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| 47 | |
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| 48 | |
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[878] | 49 | IMPLICIT NONE |
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| 50 | |
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| 51 | !======================================================================= |
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| 52 | ! Auteurs: Frederic Hourdin, Catherine Rio, Anne Mathieu |
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| 53 | ! Version du 09.02.07 |
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| 54 | ! Calcul du transport vertical dans la couche limite en presence |
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| 55 | ! de "thermiques" explicitement representes avec processus nuageux |
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| 56 | ! |
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[1403] | 57 | ! Reecriture a partir d'un listing papier a Habas, le 14/02/00 |
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[878] | 58 | ! |
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[1403] | 59 | ! le thermique est suppose homogene et dissipe par melange avec |
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| 60 | ! son environnement. la longueur l_mix controle l'efficacite du |
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| 61 | ! melange |
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[878] | 62 | ! |
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[1403] | 63 | ! Le calcul du transport des differentes especes se fait en prenant |
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[878] | 64 | ! en compte: |
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| 65 | ! 1. un flux de masse montant |
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| 66 | ! 2. un flux de masse descendant |
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| 67 | ! 3. un entrainement |
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| 68 | ! 4. un detrainement |
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| 69 | ! |
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[1738] | 70 | ! Modif 2013/01/04 (FH hourdin@lmd.jussieu.fr) |
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| 71 | ! Introduction of an implicit computation of vertical advection in |
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| 72 | ! the environment of thermal plumes in thermcell_dq |
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| 73 | ! impl = 0 : explicit, 1 : implicit, -1 : old version |
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| 74 | ! controled by iflag_thermals = |
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| 75 | ! 15, 16 run with impl=-1 : numerical convergence with NPv3 |
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| 76 | ! 17, 18 run with impl=1 : more stable |
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| 77 | ! 15 and 17 correspond to the activation of the stratocumulus "bidouille" |
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| 78 | ! |
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[4133] | 79 | ! Using |
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| 80 | ! abort_physic |
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| 81 | ! iso_verif_aberrant_encadre |
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| 82 | ! iso_verif_egalite |
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| 83 | ! test_ltherm |
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| 84 | ! thermcell_closure |
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| 85 | ! thermcell_dq |
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| 86 | ! thermcell_dry |
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| 87 | ! thermcell_dv2 |
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| 88 | ! thermcell_env |
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| 89 | ! thermcell_flux2 |
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| 90 | ! thermcell_height |
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| 91 | ! thermcell_plume |
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| 92 | ! thermcell_plume_5B |
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| 93 | ! thermcell_plume_6A |
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| 94 | ! |
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[878] | 95 | !======================================================================= |
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| 96 | |
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[1738] | 97 | |
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[878] | 98 | !----------------------------------------------------------------------- |
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| 99 | ! declarations: |
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| 100 | ! ------------- |
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| 101 | |
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| 102 | |
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| 103 | ! arguments: |
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| 104 | ! ---------- |
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[4089] | 105 | integer, intent(in) :: itap,ngrid,nlay |
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| 106 | real, intent(in) :: ptimestep |
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[4684] | 107 | real, intent(in), dimension(ngrid,nlay) :: ptemp,puwind,pvwind,pplay,pphi |
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[4678] | 108 | ! ATTENTION : zpspsk est inout et out mais c'est pas forcement pour de bonnes raisons (FH, 2023) |
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| 109 | real, intent(in), dimension(ngrid,nlay) :: p_o |
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[4590] | 110 | real, intent(out), dimension(ngrid,nlay) :: zpspsk |
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[4089] | 111 | real, intent(in), dimension(ngrid,nlay+1) :: pplev |
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[4133] | 112 | integer, intent(out), dimension(ngrid) :: lmax |
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[4089] | 113 | real, intent(out), dimension(ngrid,nlay) :: pdtadj,pduadj,pdvadj,pdoadj,entr0,detr0 |
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| 114 | real, intent(out), dimension(ngrid,nlay) :: ztla,zqla,zqta,zqsatth,zthl |
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| 115 | real, intent(out), dimension(ngrid,nlay+1) :: fm0,zw2,fraca |
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[4133] | 116 | real, intent(inout), dimension(ngrid) :: zmax0,f0 |
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[4089] | 117 | real, intent(out), dimension(ngrid,nlay) :: ztva,ztv |
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| 118 | logical, intent(in) :: debut |
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[4133] | 119 | real,intent(out), dimension(ngrid,nlay) :: ratqscth,ratqsdiff |
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[878] | 120 | |
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[4089] | 121 | real, intent(out), dimension(ngrid) :: pcon |
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| 122 | real, intent(out), dimension(ngrid,nlay) :: rhobarz,wth3 |
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| 123 | real, intent(out), dimension(ngrid) :: wmax_sec |
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| 124 | integer,intent(out), dimension(ngrid) :: lalim |
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| 125 | real, intent(out), dimension(ngrid,nlay+1) :: fm |
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| 126 | real, intent(out), dimension(ngrid,nlay) :: alim_star |
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| 127 | real, intent(out), dimension(ngrid) :: zmax |
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[972] | 128 | |
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[878] | 129 | ! local: |
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| 130 | ! ------ |
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| 131 | |
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[1738] | 132 | |
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[883] | 133 | integer,save :: igout=1 |
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[987] | 134 | !$OMP THREADPRIVATE(igout) |
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[938] | 135 | integer,save :: lunout1=6 |
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[987] | 136 | !$OMP THREADPRIVATE(lunout1) |
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[883] | 137 | integer,save :: lev_out=10 |
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[987] | 138 | !$OMP THREADPRIVATE(lev_out) |
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[878] | 139 | |
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[4089] | 140 | real lambda, zf,zf2,var,vardiff,CHI |
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| 141 | integer ig,k,l,ierr,ll |
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[878] | 142 | logical sorties |
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[4089] | 143 | real, dimension(ngrid) :: linter,zmix, zmax_sec |
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[4133] | 144 | integer,dimension(ngrid) :: lmin,lmix,lmix_bis,nivcon |
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[4089] | 145 | real, dimension(ngrid,nlay) :: ztva_est |
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[4678] | 146 | real, dimension(ngrid,nlay) :: deltaz,zlay,zh,zdthladj,zu,zv,z_o,zl,zva,zua,z_oa |
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[4089] | 147 | real, dimension(ngrid,nlay) :: zta,zha,q2,wq,wthl,wthv,thetath2,wth2 |
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[4133] | 148 | real, dimension(ngrid,nlay) :: rho,masse |
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[4089] | 149 | real, dimension(ngrid,nlay+1) :: zw_est,zlev |
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| 150 | real, dimension(ngrid) :: wmax,wmax_tmp |
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| 151 | real, dimension(ngrid,nlay+1) :: f_star |
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| 152 | real, dimension(ngrid,nlay) :: entr,detr,entr_star,detr_star,alim_star_clos |
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| 153 | real, dimension(ngrid,nlay) :: zqsat,csc |
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| 154 | real, dimension(ngrid) :: zcon,zcon2,alim_star_tot,f |
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[4413] | 155 | real, dimension(ngrid,nlay) :: entrdn,detrdn |
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[878] | 156 | |
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[4089] | 157 | character (len=20) :: modname='thermcell_main' |
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| 158 | character (len=80) :: abort_message |
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[878] | 159 | |
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| 160 | |
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[4089] | 161 | #ifdef ISO |
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[4143] | 162 | REAL xtpo(ntiso,ngrid,nlay),xtpdoadj(ntiso,ngrid,nlay) |
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| 163 | REAL xtzo(ntiso,ngrid,nlay) |
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[4089] | 164 | REAL xtpdoadj_tmp(ngrid,nlay) |
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| 165 | REAL xtpo_tmp(ngrid,nlay) |
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| 166 | REAL xtzo_tmp(ngrid,nlay) |
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| 167 | integer ixt |
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| 168 | #endif |
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[878] | 169 | |
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| 170 | ! |
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| 171 | |
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| 172 | !----------------------------------------------------------------------- |
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| 173 | ! initialisation: |
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| 174 | ! --------------- |
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| 175 | ! |
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[1943] | 176 | fm=0. ; entr=0. ; detr=0. |
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[972] | 177 | |
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[938] | 178 | if (prt_level.ge.1) print*,'thermcell_main V4' |
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[878] | 179 | |
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| 180 | sorties=.true. |
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[4089] | 181 | IF(ngrid.NE.ngrid) THEN |
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[878] | 182 | PRINT* |
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| 183 | PRINT*,'STOP dans convadj' |
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| 184 | PRINT*,'ngrid =',ngrid |
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[4089] | 185 | PRINT*,'ngrid =',ngrid |
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[878] | 186 | ENDIF |
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| 187 | ! |
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[4684] | 188 | print*,'thermcell_main debut' |
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[1403] | 189 | ! write(lunout,*)'WARNING thermcell_main f0=max(f0,1.e-2)' |
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[4089] | 190 | do ig=1,ngrid |
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[972] | 191 | f0(ig)=max(f0(ig),1.e-2) |
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[1403] | 192 | zmax0(ig)=max(zmax0(ig),40.) |
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[972] | 193 | !IMmarche pas ?! if (f0(ig)<1.e-2) f0(ig)=1.e-2 |
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| 194 | enddo |
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[878] | 195 | |
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[1494] | 196 | if (prt_level.ge.20) then |
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| 197 | do ig=1,ngrid |
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| 198 | print*,'th_main ig f0',ig,f0(ig) |
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| 199 | enddo |
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| 200 | endif |
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[878] | 201 | !----------------------------------------------------------------------- |
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| 202 | ! Calcul de T,q,ql a partir de Tl et qT dans l environnement |
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| 203 | ! -------------------------------------------------------------------- |
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| 204 | ! |
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[4684] | 205 | CALL thermcell_env(ngrid,nlay,p_o,ptemp,puwind,pvwind,pplay, & |
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[4678] | 206 | & pplev,z_o,zh,zl,ztv,zthl,zu,zv,zpspsk,zqsat,lev_out) |
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[878] | 207 | |
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[938] | 208 | if (prt_level.ge.1) print*,'thermcell_main apres thermcell_env' |
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[878] | 209 | |
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| 210 | !------------------------------------------------------------------------ |
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| 211 | ! -------------------- |
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| 212 | ! |
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| 213 | ! |
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| 214 | ! + + + + + + + + + + + |
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| 215 | ! |
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| 216 | ! |
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| 217 | ! wa, fraca, wd, fracd -------------------- zlev(2), rhobarz |
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| 218 | ! wh,wt,wo ... |
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| 219 | ! |
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[4678] | 220 | ! + + + + + + + + + + + zh,zu,zv,z_o,rho |
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[878] | 221 | ! |
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| 222 | ! |
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| 223 | ! -------------------- zlev(1) |
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| 224 | ! \\\\\\\\\\\\\\\\\\\\ |
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| 225 | ! |
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| 226 | ! |
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| 227 | |
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| 228 | !----------------------------------------------------------------------- |
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| 229 | ! Calcul des altitudes des couches |
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| 230 | !----------------------------------------------------------------------- |
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| 231 | |
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| 232 | do l=2,nlay |
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| 233 | zlev(:,l)=0.5*(pphi(:,l)+pphi(:,l-1))/RG |
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| 234 | enddo |
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[4089] | 235 | zlev(:,1)=0. |
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| 236 | zlev(:,nlay+1)=(2.*pphi(:,nlay)-pphi(:,nlay-1))/RG |
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[878] | 237 | do l=1,nlay |
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| 238 | zlay(:,l)=pphi(:,l)/RG |
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| 239 | enddo |
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| 240 | do l=1,nlay |
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| 241 | deltaz(:,l)=zlev(:,l+1)-zlev(:,l) |
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| 242 | enddo |
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| 243 | |
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| 244 | !----------------------------------------------------------------------- |
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[4089] | 245 | ! Calcul des densites et masses |
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[878] | 246 | !----------------------------------------------------------------------- |
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| 247 | |
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[4089] | 248 | rho(:,:)=pplay(:,:)/(zpspsk(:,:)*RD*ztv(:,:)) |
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| 249 | if (prt_level.ge.10) write(lunout,*) 'WARNING thermcell_main rhobarz(:,1)=rho(:,1)' |
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[972] | 250 | rhobarz(:,1)=rho(:,1) |
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[878] | 251 | do l=2,nlay |
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| 252 | rhobarz(:,l)=0.5*(rho(:,l)+rho(:,l-1)) |
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| 253 | enddo |
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| 254 | do l=1,nlay |
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| 255 | masse(:,l)=(pplev(:,l)-pplev(:,l+1))/RG |
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| 256 | enddo |
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[938] | 257 | if (prt_level.ge.1) print*,'thermcell_main apres initialisation' |
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[878] | 258 | |
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| 259 | !------------------------------------------------------------------ |
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| 260 | ! |
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| 261 | ! /|\ |
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| 262 | ! -------- | F_k+1 ------- |
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| 263 | ! ----> D_k |
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| 264 | ! /|\ <---- E_k , A_k |
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| 265 | ! -------- | F_k --------- |
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| 266 | ! ----> D_k-1 |
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| 267 | ! <---- E_k-1 , A_k-1 |
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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 | ! |
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| 273 | ! --------------------------- |
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| 274 | ! |
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| 275 | ! ----- F_lmax+1=0 ---------- \ |
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| 276 | ! lmax (zmax) | |
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| 277 | ! --------------------------- | |
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| 278 | ! | |
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| 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 | ! | E |
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| 287 | ! --------------------------- | D |
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| 288 | ! | |
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| 289 | ! --------------------------- | |
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| 290 | ! | |
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| 291 | ! --------------------------- \ | |
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| 292 | ! lalim | | |
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| 293 | ! --------------------------- | | |
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| 294 | ! | | |
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| 295 | ! --------------------------- | | |
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| 296 | ! | A | |
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| 297 | ! --------------------------- | | |
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| 298 | ! | | |
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| 299 | ! --------------------------- | | |
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| 300 | ! lmin (=1 pour le moment) | | |
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| 301 | ! ----- F_lmin=0 ------------ / / |
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| 302 | ! |
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| 303 | ! --------------------------- |
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| 304 | ! ////////////////////////// |
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| 305 | ! |
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| 306 | ! |
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| 307 | !============================================================================= |
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| 308 | ! Calculs initiaux ne faisant pas intervenir les changements de phase |
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| 309 | !============================================================================= |
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| 310 | |
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| 311 | !------------------------------------------------------------------ |
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[1403] | 312 | ! 1. alim_star est le profil vertical de l'alimentation a la base du |
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| 313 | ! panache thermique, calcule a partir de la flotabilite de l'air sec |
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[878] | 314 | ! 2. lmin et lalim sont les indices inferieurs et superieurs de alim_star |
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| 315 | !------------------------------------------------------------------ |
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| 316 | ! |
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| 317 | entr_star=0. ; detr_star=0. ; alim_star=0. ; alim_star_tot=0. |
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[1403] | 318 | lmin=1 |
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[878] | 319 | |
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| 320 | !----------------------------------------------------------------------------- |
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| 321 | ! 3. wmax_sec et zmax_sec sont les vitesses et altitudes maximum d'un |
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| 322 | ! panache sec conservatif (e=d=0) alimente selon alim_star |
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| 323 | ! Il s'agit d'un calcul de type CAPE |
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[1403] | 324 | ! zmax_sec est utilise pour determiner la geometrie du thermique. |
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[878] | 325 | !------------------------------------------------------------------------------ |
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[1403] | 326 | !--------------------------------------------------------------------------------- |
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| 327 | !calcul du melange et des variables dans le thermique |
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| 328 | !-------------------------------------------------------------------------------- |
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[878] | 329 | ! |
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[1403] | 330 | if (prt_level.ge.1) print*,'avant thermcell_plume ',lev_out |
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[878] | 331 | |
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[3451] | 332 | !===================================================================== |
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| 333 | ! Old version of thermcell_plume in thermcell_plume_6A.F90 |
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| 334 | ! It includes both thermcell_plume_6A and thermcell_plume_5B corresponding |
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| 335 | ! to the 5B and 6A versions used for CMIP5 and CMIP6. |
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| 336 | ! The latest was previously named thermcellV1_plume. |
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| 337 | ! The new thermcell_plume is a clean version (removing obsolete |
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| 338 | ! options) of thermcell_plume_6A. |
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| 339 | ! The 3 versions are controled by |
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| 340 | ! flag_thermals_ed <= 9 thermcell_plume_6A |
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| 341 | ! <= 19 thermcell_plume_5B |
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| 342 | ! else thermcell_plume (default 20 for convergence with 6A) |
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| 343 | ! Fredho |
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| 344 | !===================================================================== |
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[878] | 345 | |
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[1403] | 346 | if (iflag_thermals_ed<=9) then |
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| 347 | ! print*,'THERM NOUVELLE/NOUVELLE Arnaud' |
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[4678] | 348 | CALL thermcell_plume_6A(itap,ngrid,nlay,ptimestep,ztv,zthl,p_o,zl,rhobarz,& |
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[1403] | 349 | & zlev,pplev,pphi,zpspsk,alim_star,alim_star_tot, & |
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| 350 | & lalim,f0,detr_star,entr_star,f_star,csc,ztva, & |
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| 351 | & ztla,zqla,zqta,zha,zw2,zw_est,ztva_est,zqsatth,lmix,lmix_bis,linter & |
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| 352 | & ,lev_out,lunout1,igout) |
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[878] | 353 | |
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[3451] | 354 | elseif (iflag_thermals_ed<=19) then |
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[1403] | 355 | ! print*,'THERM RIO et al 2010, version d Arnaud' |
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[4678] | 356 | CALL thermcell_plume_5B(itap,ngrid,nlay,ptimestep,ztv,zthl,p_o,zl,rhobarz,& |
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[1403] | 357 | & zlev,pplev,pphi,zpspsk,alim_star,alim_star_tot, & |
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| 358 | & lalim,f0,detr_star,entr_star,f_star,csc,ztva, & |
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| 359 | & ztla,zqla,zqta,zha,zw2,zw_est,ztva_est,zqsatth,lmix,lmix_bis,linter & |
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| 360 | & ,lev_out,lunout1,igout) |
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[3451] | 361 | else |
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[4678] | 362 | CALL thermcell_plume(itap,ngrid,nlay,ptimestep,ztv,zthl,p_o,zl,rhobarz,& |
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[3451] | 363 | & zlev,pplev,pphi,zpspsk,alim_star,alim_star_tot, & |
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| 364 | & lalim,f0,detr_star,entr_star,f_star,csc,ztva, & |
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| 365 | & ztla,zqla,zqta,zha,zw2,zw_est,ztva_est,zqsatth,lmix,lmix_bis,linter & |
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| 366 | & ,lev_out,lunout1,igout) |
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[1403] | 367 | endif |
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[878] | 368 | |
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[972] | 369 | if (prt_level.ge.1) print*,'apres thermcell_plume ',lev_out |
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| 370 | |
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[4678] | 371 | call test_ltherm(ngrid,nlay,pplay,lalim,ztv,p_o,ztva,zqla,f_star,zw2,'thermcell_plum lalim ') |
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| 372 | call test_ltherm(ngrid,nlay,pplay,lmix ,ztv,p_o,ztva,zqla,f_star,zw2,'thermcell_plum lmix ') |
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[878] | 373 | |
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[938] | 374 | if (prt_level.ge.1) print*,'thermcell_main apres thermcell_plume' |
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| 375 | if (prt_level.ge.10) then |
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[972] | 376 | write(lunout1,*) 'Dans thermcell_main 2' |
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| 377 | write(lunout1,*) 'lmin ',lmin(igout) |
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| 378 | write(lunout1,*) 'lalim ',lalim(igout) |
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| 379 | write(lunout1,*) ' ig l alim_star entr_star detr_star f_star ' |
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| 380 | write(lunout1,'(i6,i4,4e15.5)') (igout,l,alim_star(igout,l),entr_star(igout,l),detr_star(igout,l) & |
---|
[878] | 381 | & ,f_star(igout,l+1),l=1,nint(linter(igout))+5) |
---|
| 382 | endif |
---|
| 383 | |
---|
| 384 | !------------------------------------------------------------------------------- |
---|
| 385 | ! Calcul des caracteristiques du thermique:zmax,zmix,wmax |
---|
| 386 | !------------------------------------------------------------------------------- |
---|
| 387 | ! |
---|
| 388 | CALL thermcell_height(ngrid,nlay,lalim,lmin,linter,lmix,zw2, & |
---|
[4094] | 389 | & zlev,lmax,zmax,zmax0,zmix,wmax) |
---|
[1403] | 390 | ! Attention, w2 est transforme en sa racine carree dans cette routine |
---|
[4143] | 391 | ! Le probleme vient du fait que linter et lmix sont souvent egaux a 1. |
---|
[1403] | 392 | wmax_tmp=0. |
---|
| 393 | do l=1,nlay |
---|
| 394 | wmax_tmp(:)=max(wmax_tmp(:),zw2(:,l)) |
---|
| 395 | enddo |
---|
| 396 | ! print*,"ZMAX ",lalim,lmin,linter,lmix,lmax,zmax,zmax0,zmix,wmax |
---|
[878] | 397 | |
---|
| 398 | |
---|
[1403] | 399 | |
---|
[4678] | 400 | call test_ltherm(ngrid,nlay,pplay,lalim,ztv,p_o,ztva,zqla,f_star,zw2,'thermcell_heig lalim ') |
---|
| 401 | call test_ltherm(ngrid,nlay,pplay,lmin ,ztv,p_o,ztva,zqla,f_star,zw2,'thermcell_heig lmin ') |
---|
| 402 | call test_ltherm(ngrid,nlay,pplay,lmix ,ztv,p_o,ztva,zqla,f_star,zw2,'thermcell_heig lmix ') |
---|
| 403 | call test_ltherm(ngrid,nlay,pplay,lmax ,ztv,p_o,ztva,zqla,f_star,zw2,'thermcell_heig lmax ') |
---|
[878] | 404 | |
---|
[938] | 405 | if (prt_level.ge.1) print*,'thermcell_main apres thermcell_height' |
---|
[878] | 406 | |
---|
| 407 | !------------------------------------------------------------------------------- |
---|
| 408 | ! Fermeture,determination de f |
---|
| 409 | !------------------------------------------------------------------------------- |
---|
[1026] | 410 | ! |
---|
[1403] | 411 | ! |
---|
| 412 | CALL thermcell_dry(ngrid,nlay,zlev,pphi,ztv,alim_star, & |
---|
[4094] | 413 | & lalim,lmin,zmax_sec,wmax_sec) |
---|
[878] | 414 | |
---|
[1998] | 415 | |
---|
[4678] | 416 | call test_ltherm(ngrid,nlay,pplay,lmin,ztv,p_o,ztva,zqla,f_star,zw2,'thermcell_dry lmin ') |
---|
| 417 | call test_ltherm(ngrid,nlay,pplay,lalim,ztv,p_o,ztva,zqla,f_star,zw2,'thermcell_dry lalim ') |
---|
[1403] | 418 | |
---|
| 419 | if (prt_level.ge.1) print*,'thermcell_main apres thermcell_dry' |
---|
| 420 | if (prt_level.ge.10) then |
---|
| 421 | write(lunout1,*) 'Dans thermcell_main 1b' |
---|
| 422 | write(lunout1,*) 'lmin ',lmin(igout) |
---|
| 423 | write(lunout1,*) 'lalim ',lalim(igout) |
---|
| 424 | write(lunout1,*) ' ig l alim_star entr_star detr_star f_star ' |
---|
| 425 | write(lunout1,'(i6,i4,e15.5)') (igout,l,alim_star(igout,l) & |
---|
| 426 | & ,l=1,lalim(igout)+4) |
---|
| 427 | endif |
---|
| 428 | |
---|
| 429 | |
---|
| 430 | |
---|
| 431 | |
---|
| 432 | ! Choix de la fonction d'alimentation utilisee pour la fermeture. |
---|
| 433 | ! Apparemment sans importance |
---|
| 434 | alim_star_clos(:,:)=alim_star(:,:) |
---|
| 435 | alim_star_clos(:,:)=entr_star(:,:)+alim_star(:,:) |
---|
[1998] | 436 | ! |
---|
| 437 | !CR Appel de la fermeture seche |
---|
| 438 | if (iflag_thermals_closure.eq.1) then |
---|
[1403] | 439 | |
---|
[4094] | 440 | CALL thermcell_closure(ngrid,nlay,r_aspect_thermals,ptimestep,rho, & |
---|
| 441 | & zlev,lalim,alim_star_clos,zmax_sec,wmax_sec,f) |
---|
[878] | 442 | |
---|
[1403] | 443 | !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! |
---|
| 444 | ! Appel avec les zmax et wmax tenant compte de la condensation |
---|
| 445 | ! Semble moins bien marcher |
---|
[1998] | 446 | else if (iflag_thermals_closure.eq.2) then |
---|
| 447 | |
---|
| 448 | CALL thermcell_closure(ngrid,nlay,r_aspect_thermals,ptimestep,rho, & |
---|
[4094] | 449 | & zlev,lalim,alim_star,zmax,wmax,f) |
---|
[1998] | 450 | |
---|
[4094] | 451 | |
---|
[1998] | 452 | endif |
---|
| 453 | |
---|
[1403] | 454 | !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! |
---|
| 455 | |
---|
[938] | 456 | if(prt_level.ge.1)print*,'thermcell_closure apres thermcell_closure' |
---|
[878] | 457 | |
---|
[972] | 458 | if (tau_thermals>1.) then |
---|
| 459 | lambda=exp(-ptimestep/tau_thermals) |
---|
| 460 | f0=(1.-lambda)*f+lambda*f0 |
---|
| 461 | else |
---|
| 462 | f0=f |
---|
| 463 | endif |
---|
| 464 | |
---|
| 465 | ! Test valable seulement en 1D mais pas genant |
---|
| 466 | if (.not. (f0(1).ge.0.) ) then |
---|
[1403] | 467 | abort_message = '.not. (f0(1).ge.0.)' |
---|
[2311] | 468 | CALL abort_physic (modname,abort_message,1) |
---|
[972] | 469 | endif |
---|
| 470 | |
---|
[878] | 471 | !------------------------------------------------------------------------------- |
---|
| 472 | !deduction des flux |
---|
| 473 | |
---|
[972] | 474 | CALL thermcell_flux2(ngrid,nlay,ptimestep,masse, & |
---|
[878] | 475 | & lalim,lmax,alim_star, & |
---|
| 476 | & entr_star,detr_star,f,rhobarz,zlev,zw2,fm,entr, & |
---|
[972] | 477 | & detr,zqla,lev_out,lunout1,igout) |
---|
[4318] | 478 | |
---|
[972] | 479 | !IM 060508 & detr,zqla,zmax,lev_out,lunout,igout) |
---|
[878] | 480 | |
---|
[938] | 481 | if (prt_level.ge.1) print*,'thermcell_main apres thermcell_flux' |
---|
[4678] | 482 | call test_ltherm(ngrid,nlay,pplay,lalim,ztv,p_o,ztva,zqla,f_star,zw2,'thermcell_flux lalim ') |
---|
| 483 | call test_ltherm(ngrid,nlay,pplay,lmax ,ztv,p_o,ztva,zqla,f_star,zw2,'thermcell_flux lmax ') |
---|
[878] | 484 | |
---|
| 485 | !------------------------------------------------------------------ |
---|
[972] | 486 | ! On ne prend pas directement les profils issus des calculs precedents |
---|
| 487 | ! mais on s'autorise genereusement une relaxation vers ceci avec |
---|
| 488 | ! une constante de temps tau_thermals (typiquement 1800s). |
---|
| 489 | !------------------------------------------------------------------ |
---|
[878] | 490 | |
---|
[972] | 491 | if (tau_thermals>1.) then |
---|
| 492 | lambda=exp(-ptimestep/tau_thermals) |
---|
| 493 | fm0=(1.-lambda)*fm+lambda*fm0 |
---|
| 494 | entr0=(1.-lambda)*entr+lambda*entr0 |
---|
[1403] | 495 | detr0=(1.-lambda)*detr+lambda*detr0 |
---|
[878] | 496 | else |
---|
| 497 | fm0=fm |
---|
| 498 | entr0=entr |
---|
| 499 | detr0=detr |
---|
| 500 | endif |
---|
| 501 | |
---|
[4396] | 502 | !------------------------------------------------------------------ |
---|
| 503 | ! Calcul de la fraction de l'ascendance |
---|
| 504 | !------------------------------------------------------------------ |
---|
| 505 | do ig=1,ngrid |
---|
| 506 | fraca(ig,1)=0. |
---|
| 507 | fraca(ig,nlay+1)=0. |
---|
| 508 | enddo |
---|
| 509 | do l=2,nlay |
---|
| 510 | do ig=1,ngrid |
---|
| 511 | if (zw2(ig,l).gt.1.e-10) then |
---|
| 512 | fraca(ig,l)=fm(ig,l)/(rhobarz(ig,l)*zw2(ig,l)) |
---|
| 513 | else |
---|
| 514 | fraca(ig,l)=0. |
---|
| 515 | endif |
---|
| 516 | enddo |
---|
| 517 | enddo |
---|
| 518 | |
---|
[972] | 519 | !c------------------------------------------------------------------ |
---|
| 520 | ! calcul du transport vertical |
---|
| 521 | !------------------------------------------------------------------ |
---|
[4381] | 522 | IF (iflag_thermals_down .GT. 0) THEN |
---|
[4438] | 523 | if (debut) print*,'WARNING !!! routine thermcell_down en cours de developpement' |
---|
[4441] | 524 | entrdn=fact_thermals_down*detr0 |
---|
| 525 | detrdn=fact_thermals_down*entr0 |
---|
[4413] | 526 | ! we want to transport potential temperature, total water and momentum |
---|
| 527 | CALL thermcell_updown_dq(ngrid,nlay,ptimestep,lmax,entr0,detr0,entrdn,detrdn,masse,zthl,zdthladj) |
---|
[4678] | 528 | CALL thermcell_updown_dq(ngrid,nlay,ptimestep,lmax,entr0,detr0,entrdn,detrdn,masse,p_o,pdoadj) |
---|
[4413] | 529 | CALL thermcell_updown_dq(ngrid,nlay,ptimestep,lmax,entr0,detr0,entrdn,detrdn,masse,zu,pduadj) |
---|
| 530 | CALL thermcell_updown_dq(ngrid,nlay,ptimestep,lmax,entr0,detr0,entrdn,detrdn,masse,zv,pdvadj) |
---|
[4396] | 531 | ELSE |
---|
[4381] | 532 | !-------------------------------------------------------------- |
---|
[972] | 533 | |
---|
[4396] | 534 | call thermcell_dq(ngrid,nlay,dqimpl,ptimestep,fm0,entr0,masse, & |
---|
| 535 | & zthl,zdthladj,zta,lev_out) |
---|
[4678] | 536 | |
---|
| 537 | do ll=1,nlay |
---|
| 538 | do ig=1,ngrid |
---|
| 539 | z_o(ig,ll)=p_o(ig,ll) |
---|
| 540 | enddo |
---|
| 541 | enddo |
---|
[4396] | 542 | call thermcell_dq(ngrid,nlay,dqimpl,ptimestep,fm0,entr0,masse, & |
---|
[4678] | 543 | & z_o,pdoadj,z_oa,lev_out) |
---|
[878] | 544 | |
---|
[4089] | 545 | #ifdef ISO |
---|
[4143] | 546 | ! C Risi: on utilise directement la meme routine |
---|
| 547 | do ixt=1,ntiso |
---|
[4089] | 548 | do ll=1,nlay |
---|
| 549 | DO ig=1,ngrid |
---|
| 550 | xtpo_tmp(ig,ll)=xtpo(ixt,ig,ll) |
---|
| 551 | xtzo_tmp(ig,ll)=xtzo(ixt,ig,ll) |
---|
| 552 | enddo |
---|
| 553 | enddo |
---|
| 554 | call thermcell_dq(ngrid,nlay,dqimpl,ptimestep,fm0,entr0,masse, & |
---|
| 555 | & xtpo_tmp,xtpdoadj_tmp,xtzo_tmp,lev_out) |
---|
| 556 | do ll=1,nlay |
---|
| 557 | DO ig=1,ngrid |
---|
| 558 | xtpdoadj(ixt,ig,ll)=xtpdoadj_tmp(ig,ll) |
---|
| 559 | enddo |
---|
| 560 | enddo |
---|
[4143] | 561 | enddo |
---|
[4089] | 562 | #endif |
---|
| 563 | |
---|
| 564 | #ifdef ISO |
---|
| 565 | #ifdef ISOVERIF |
---|
| 566 | DO ll=1,nlay |
---|
| 567 | DO ig=1,ngrid |
---|
| 568 | if (iso_eau.gt.0) then |
---|
| 569 | call iso_verif_egalite(xtpo(iso_eau,ig,ll), & |
---|
[4680] | 570 | & p_o(ig,ll),'thermcell_main 594') |
---|
[4089] | 571 | call iso_verif_egalite(xtpdoadj(iso_eau,ig,ll), & |
---|
| 572 | & pdoadj(ig,ll),'thermcell_main 596') |
---|
| 573 | endif |
---|
| 574 | if (iso_HDO.gt.0) then |
---|
| 575 | call iso_verif_aberrant_encadre(xtpo(iso_hdo,ig,ll) & |
---|
[4678] | 576 | & /p_o(ig,ll),'thermcell_main 610') |
---|
[4089] | 577 | endif |
---|
| 578 | enddo |
---|
| 579 | enddo !DO ll=1,nlay |
---|
| 580 | write(*,*) 'thermcell_main 600 tmp: apres thermcell_dq' |
---|
| 581 | #endif |
---|
| 582 | #endif |
---|
| 583 | |
---|
| 584 | |
---|
[883] | 585 | !------------------------------------------------------------------ |
---|
| 586 | ! calcul du transport vertical du moment horizontal |
---|
| 587 | !------------------------------------------------------------------ |
---|
[878] | 588 | |
---|
[972] | 589 | !IM 090508 |
---|
[1738] | 590 | if (dvdq == 0 ) then |
---|
[883] | 591 | |
---|
[878] | 592 | ! Calcul du transport de V tenant compte d'echange par gradient |
---|
| 593 | ! de pression horizontal avec l'environnement |
---|
| 594 | |
---|
| 595 | call thermcell_dv2(ngrid,nlay,ptimestep,fm0,entr0,masse & |
---|
[1738] | 596 | ! & ,fraca*dvdq,zmax & |
---|
| 597 | & ,fraca,zmax & |
---|
[972] | 598 | & ,zu,zv,pduadj,pdvadj,zua,zva,lev_out) |
---|
[1403] | 599 | |
---|
[878] | 600 | else |
---|
| 601 | |
---|
| 602 | ! calcul purement conservatif pour le transport de V |
---|
[1738] | 603 | call thermcell_dq(ngrid,nlay,dqimpl,ptimestep,fm0,entr0,masse & |
---|
[878] | 604 | & ,zu,pduadj,zua,lev_out) |
---|
[1738] | 605 | call thermcell_dq(ngrid,nlay,dqimpl,ptimestep,fm0,entr0,masse & |
---|
[878] | 606 | & ,zv,pdvadj,zva,lev_out) |
---|
[1738] | 607 | |
---|
[878] | 608 | endif |
---|
[4396] | 609 | ENDIF |
---|
[878] | 610 | |
---|
| 611 | ! print*,'13 OK convect8' |
---|
| 612 | do l=1,nlay |
---|
| 613 | do ig=1,ngrid |
---|
| 614 | pdtadj(ig,l)=zdthladj(ig,l)*zpspsk(ig,l) |
---|
| 615 | enddo |
---|
| 616 | enddo |
---|
| 617 | |
---|
[972] | 618 | if (prt_level.ge.1) print*,'14 OK convect8' |
---|
[878] | 619 | !------------------------------------------------------------------ |
---|
| 620 | ! Calculs de diagnostiques pour les sorties |
---|
| 621 | !------------------------------------------------------------------ |
---|
| 622 | !calcul de fraca pour les sorties |
---|
| 623 | |
---|
| 624 | if (sorties) then |
---|
[972] | 625 | if (prt_level.ge.1) print*,'14a OK convect8' |
---|
[878] | 626 | ! calcul du niveau de condensation |
---|
| 627 | ! initialisation |
---|
| 628 | do ig=1,ngrid |
---|
[879] | 629 | nivcon(ig)=0 |
---|
[878] | 630 | zcon(ig)=0. |
---|
| 631 | enddo |
---|
| 632 | !nouveau calcul |
---|
| 633 | do ig=1,ngrid |
---|
[4678] | 634 | CHI=zh(ig,1)/(1669.0-122.0*z_o(ig,1)/zqsat(ig,1)-zh(ig,1)) |
---|
| 635 | pcon(ig)=pplay(ig,1)*(z_o(ig,1)/zqsat(ig,1))**CHI |
---|
[878] | 636 | enddo |
---|
[1403] | 637 | !IM do k=1,nlay |
---|
| 638 | do k=1,nlay-1 |
---|
[878] | 639 | do ig=1,ngrid |
---|
| 640 | if ((pcon(ig).le.pplay(ig,k)) & |
---|
| 641 | & .and.(pcon(ig).gt.pplay(ig,k+1))) then |
---|
| 642 | zcon2(ig)=zlay(ig,k)-(pcon(ig)-pplay(ig,k))/(RG*rho(ig,k))/100. |
---|
| 643 | endif |
---|
| 644 | enddo |
---|
| 645 | enddo |
---|
[1403] | 646 | !IM |
---|
[1494] | 647 | ierr=0 |
---|
[1403] | 648 | do ig=1,ngrid |
---|
| 649 | if (pcon(ig).le.pplay(ig,nlay)) then |
---|
| 650 | zcon2(ig)=zlay(ig,nlay)-(pcon(ig)-pplay(ig,nlay))/(RG*rho(ig,nlay))/100. |
---|
[1494] | 651 | ierr=1 |
---|
| 652 | endif |
---|
| 653 | enddo |
---|
| 654 | if (ierr==1) then |
---|
[1403] | 655 | abort_message = 'thermcellV0_main: les thermiques vont trop haut ' |
---|
[2311] | 656 | CALL abort_physic (modname,abort_message,1) |
---|
[1494] | 657 | endif |
---|
| 658 | |
---|
[972] | 659 | if (prt_level.ge.1) print*,'14b OK convect8' |
---|
[878] | 660 | do k=nlay,1,-1 |
---|
| 661 | do ig=1,ngrid |
---|
| 662 | if (zqla(ig,k).gt.1e-10) then |
---|
| 663 | nivcon(ig)=k |
---|
| 664 | zcon(ig)=zlev(ig,k) |
---|
| 665 | endif |
---|
| 666 | enddo |
---|
| 667 | enddo |
---|
[972] | 668 | if (prt_level.ge.1) print*,'14c OK convect8' |
---|
[878] | 669 | !calcul des moments |
---|
| 670 | !initialisation |
---|
| 671 | do l=1,nlay |
---|
| 672 | do ig=1,ngrid |
---|
| 673 | q2(ig,l)=0. |
---|
| 674 | wth2(ig,l)=0. |
---|
| 675 | wth3(ig,l)=0. |
---|
| 676 | ratqscth(ig,l)=0. |
---|
| 677 | ratqsdiff(ig,l)=0. |
---|
| 678 | enddo |
---|
| 679 | enddo |
---|
[972] | 680 | if (prt_level.ge.1) print*,'14d OK convect8' |
---|
[1146] | 681 | if (prt_level.ge.10)write(lunout,*) & |
---|
| 682 | & 'WARNING thermcell_main wth2=0. si zw2 > 1.e-10' |
---|
[878] | 683 | do l=1,nlay |
---|
| 684 | do ig=1,ngrid |
---|
| 685 | zf=fraca(ig,l) |
---|
| 686 | zf2=zf/(1.-zf) |
---|
[972] | 687 | ! |
---|
[1403] | 688 | thetath2(ig,l)=zf2*(ztla(ig,l)-zthl(ig,l))**2 |
---|
[972] | 689 | if(zw2(ig,l).gt.1.e-10) then |
---|
| 690 | wth2(ig,l)=zf2*(zw2(ig,l))**2 |
---|
| 691 | else |
---|
| 692 | wth2(ig,l)=0. |
---|
| 693 | endif |
---|
[878] | 694 | wth3(ig,l)=zf2*(1-2.*fraca(ig,l))/(1-fraca(ig,l)) & |
---|
| 695 | & *zw2(ig,l)*zw2(ig,l)*zw2(ig,l) |
---|
[4678] | 696 | q2(ig,l)=zf2*(zqta(ig,l)*1000.-p_o(ig,l)*1000.)**2 |
---|
| 697 | !test: on calcul q2/p_o=ratqsc |
---|
| 698 | ratqscth(ig,l)=sqrt(max(q2(ig,l),1.e-6)/(p_o(ig,l)*1000.)) |
---|
[878] | 699 | enddo |
---|
| 700 | enddo |
---|
[1403] | 701 | !calcul des flux: q, thetal et thetav |
---|
| 702 | do l=1,nlay |
---|
| 703 | do ig=1,ngrid |
---|
[4678] | 704 | wq(ig,l)=fraca(ig,l)*zw2(ig,l)*(zqta(ig,l)*1000.-p_o(ig,l)*1000.) |
---|
[1403] | 705 | wthl(ig,l)=fraca(ig,l)*zw2(ig,l)*(ztla(ig,l)-zthl(ig,l)) |
---|
| 706 | wthv(ig,l)=fraca(ig,l)*zw2(ig,l)*(ztva(ig,l)-ztv(ig,l)) |
---|
| 707 | enddo |
---|
[879] | 708 | enddo |
---|
[1638] | 709 | |
---|
[878] | 710 | !calcul du ratqscdiff |
---|
[972] | 711 | if (prt_level.ge.1) print*,'14e OK convect8' |
---|
[878] | 712 | var=0. |
---|
| 713 | vardiff=0. |
---|
| 714 | ratqsdiff(:,:)=0. |
---|
[1494] | 715 | |
---|
[4089] | 716 | do l=1,nlay |
---|
[1494] | 717 | do ig=1,ngrid |
---|
| 718 | if (l<=lalim(ig)) then |
---|
[878] | 719 | var=var+alim_star(ig,l)*zqta(ig,l)*1000. |
---|
[1494] | 720 | endif |
---|
[878] | 721 | enddo |
---|
| 722 | enddo |
---|
[1494] | 723 | |
---|
[972] | 724 | if (prt_level.ge.1) print*,'14f OK convect8' |
---|
[1494] | 725 | |
---|
[4089] | 726 | do l=1,nlay |
---|
[1494] | 727 | do ig=1,ngrid |
---|
| 728 | if (l<=lalim(ig)) then |
---|
| 729 | zf=fraca(ig,l) |
---|
| 730 | zf2=zf/(1.-zf) |
---|
| 731 | vardiff=vardiff+alim_star(ig,l)*(zqta(ig,l)*1000.-var)**2 |
---|
| 732 | endif |
---|
| 733 | enddo |
---|
[878] | 734 | enddo |
---|
[1494] | 735 | |
---|
[972] | 736 | if (prt_level.ge.1) print*,'14g OK convect8' |
---|
[4089] | 737 | do l=1,nlay |
---|
| 738 | do ig=1,ngrid |
---|
[4678] | 739 | ratqsdiff(ig,l)=sqrt(vardiff)/(p_o(ig,l)*1000.) |
---|
[4089] | 740 | enddo |
---|
| 741 | enddo |
---|
[878] | 742 | endif |
---|
| 743 | |
---|
[938] | 744 | if (prt_level.ge.1) print*,'thermcell_main FIN OK' |
---|
[878] | 745 | |
---|
[4684] | 746 | print*,'thermcell_main fin' |
---|
[4094] | 747 | RETURN |
---|
[4089] | 748 | end subroutine thermcell_main |
---|
[878] | 749 | |
---|
[4089] | 750 | !============================================================================= |
---|
| 751 | !///////////////////////////////////////////////////////////////////////////// |
---|
| 752 | !============================================================================= |
---|
[4678] | 753 | subroutine test_ltherm(ngrid,nlay,pplay,long,ztv,p_o,ztva, & ! in |
---|
[4089] | 754 | & zqla,f_star,zw2,comment) ! in |
---|
| 755 | !============================================================================= |
---|
[4590] | 756 | USE lmdz_thermcell_ini, ONLY: prt_level |
---|
[938] | 757 | IMPLICIT NONE |
---|
[878] | 758 | |
---|
[4089] | 759 | integer i, k, ngrid,nlay |
---|
[4678] | 760 | real, intent(in), dimension(ngrid,nlay) :: pplay,ztv,p_o,ztva,zqla |
---|
[4089] | 761 | real, intent(in), dimension(ngrid,nlay) :: f_star,zw2 |
---|
| 762 | integer, intent(in), dimension(ngrid) :: long |
---|
[878] | 763 | real seuil |
---|
| 764 | character*21 comment |
---|
[4133] | 765 | |
---|
[4089] | 766 | seuil=0.25 |
---|
[878] | 767 | |
---|
[938] | 768 | if (prt_level.ge.1) THEN |
---|
| 769 | print*,'WARNING !!! TEST ',comment |
---|
| 770 | endif |
---|
[879] | 771 | return |
---|
| 772 | |
---|
[878] | 773 | ! test sur la hauteur des thermiques ... |
---|
[4089] | 774 | do i=1,ngrid |
---|
[972] | 775 | !IMtemp if (pplay(i,long(i)).lt.seuil*pplev(i,1)) then |
---|
| 776 | if (prt_level.ge.10) then |
---|
[878] | 777 | print*,'WARNING ',comment,' au point ',i,' K= ',long(i) |
---|
| 778 | print*,' K P(MB) THV(K) Qenv(g/kg)THVA QLA(g/kg) F* W2' |
---|
[4089] | 779 | do k=1,nlay |
---|
[4678] | 780 | 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] | 781 | enddo |
---|
[972] | 782 | endif |
---|
[878] | 783 | enddo |
---|
| 784 | |
---|
| 785 | |
---|
| 786 | return |
---|
| 787 | end |
---|
| 788 | |
---|
[4089] | 789 | ! nrlmd le 10/04/2012 Transport de la TKE par le thermique moyen pour la fermeture en ALP |
---|
| 790 | ! On transporte pbl_tke pour donner therm_tke |
---|
[4143] | 791 | ! Copie conforme de la subroutine DTKE dans physiq.F ecrite par Frederic Hourdin |
---|
[4089] | 792 | |
---|
| 793 | !======================================================================= |
---|
| 794 | !/////////////////////////////////////////////////////////////////////// |
---|
| 795 | !======================================================================= |
---|
| 796 | |
---|
| 797 | subroutine thermcell_tke_transport( & |
---|
| 798 | & ngrid,nlay,ptimestep,fm0,entr0,rg,pplev, & ! in |
---|
| 799 | & therm_tke_max) ! out |
---|
[4590] | 800 | USE lmdz_thermcell_ini, ONLY: prt_level |
---|
[1638] | 801 | implicit none |
---|
| 802 | |
---|
| 803 | !======================================================================= |
---|
| 804 | ! |
---|
| 805 | ! Calcul du transport verticale dans la couche limite en presence |
---|
| 806 | ! de "thermiques" explicitement representes |
---|
| 807 | ! calcul du dq/dt une fois qu'on connait les ascendances |
---|
| 808 | ! |
---|
| 809 | !======================================================================= |
---|
| 810 | |
---|
[4089] | 811 | integer ngrid,nlay |
---|
[1638] | 812 | |
---|
[4089] | 813 | real, intent(in) :: ptimestep |
---|
| 814 | real, intent(in), dimension(ngrid,nlay+1) :: fm0,pplev |
---|
| 815 | real, intent(in), dimension(ngrid,nlay) :: entr0 |
---|
| 816 | real, intent(in) :: rg |
---|
| 817 | real, intent(out), dimension(ngrid,nlay) :: therm_tke_max |
---|
| 818 | |
---|
[1638] | 819 | real detr0(ngrid,nlay) |
---|
[4089] | 820 | real masse0(ngrid,nlay) |
---|
[1638] | 821 | real masse(ngrid,nlay),fm(ngrid,nlay+1) |
---|
| 822 | real entr(ngrid,nlay) |
---|
| 823 | real q(ngrid,nlay) |
---|
| 824 | integer lev_out ! niveau pour les print |
---|
| 825 | |
---|
| 826 | real qa(ngrid,nlay),detr(ngrid,nlay),wqd(ngrid,nlay+1) |
---|
| 827 | integer ig,k |
---|
| 828 | |
---|
| 829 | |
---|
| 830 | lev_out=0 |
---|
| 831 | |
---|
| 832 | |
---|
| 833 | if (prt_level.ge.1) print*,'Q2 THERMCEL_DQ 0' |
---|
| 834 | |
---|
| 835 | ! calcul du detrainement |
---|
| 836 | do k=1,nlay |
---|
| 837 | detr0(:,k)=fm0(:,k)-fm0(:,k+1)+entr0(:,k) |
---|
| 838 | masse0(:,k)=(pplev(:,k)-pplev(:,k+1))/RG |
---|
| 839 | enddo |
---|
| 840 | |
---|
| 841 | |
---|
| 842 | ! Decalage vertical des entrainements et detrainements. |
---|
| 843 | masse(:,1)=0.5*masse0(:,1) |
---|
| 844 | entr(:,1)=0.5*entr0(:,1) |
---|
| 845 | detr(:,1)=0.5*detr0(:,1) |
---|
| 846 | fm(:,1)=0. |
---|
| 847 | do k=1,nlay-1 |
---|
| 848 | masse(:,k+1)=0.5*(masse0(:,k)+masse0(:,k+1)) |
---|
| 849 | entr(:,k+1)=0.5*(entr0(:,k)+entr0(:,k+1)) |
---|
| 850 | detr(:,k+1)=0.5*(detr0(:,k)+detr0(:,k+1)) |
---|
| 851 | fm(:,k+1)=fm(:,k)+entr(:,k)-detr(:,k) |
---|
| 852 | enddo |
---|
| 853 | fm(:,nlay+1)=0. |
---|
| 854 | |
---|
| 855 | |
---|
| 856 | q(:,:)=therm_tke_max(:,:) |
---|
| 857 | !!! nrlmd le 16/09/2010 |
---|
| 858 | do ig=1,ngrid |
---|
| 859 | qa(ig,1)=q(ig,1) |
---|
| 860 | enddo |
---|
| 861 | !!! |
---|
| 862 | |
---|
| 863 | if (1==1) then |
---|
| 864 | do k=2,nlay |
---|
| 865 | do ig=1,ngrid |
---|
| 866 | if ((fm(ig,k+1)+detr(ig,k))*ptimestep.gt. & |
---|
| 867 | & 1.e-5*masse(ig,k)) then |
---|
| 868 | qa(ig,k)=(fm(ig,k)*qa(ig,k-1)+entr(ig,k)*q(ig,k)) & |
---|
| 869 | & /(fm(ig,k+1)+detr(ig,k)) |
---|
| 870 | else |
---|
| 871 | qa(ig,k)=q(ig,k) |
---|
| 872 | endif |
---|
| 873 | if (qa(ig,k).lt.0.) then |
---|
| 874 | ! print*,'qa<0!!!' |
---|
| 875 | endif |
---|
| 876 | if (q(ig,k).lt.0.) then |
---|
| 877 | ! print*,'q<0!!!' |
---|
| 878 | endif |
---|
| 879 | enddo |
---|
| 880 | enddo |
---|
| 881 | |
---|
| 882 | ! Calcul du flux subsident |
---|
| 883 | |
---|
| 884 | do k=2,nlay |
---|
| 885 | do ig=1,ngrid |
---|
| 886 | wqd(ig,k)=fm(ig,k)*q(ig,k) |
---|
| 887 | if (wqd(ig,k).lt.0.) then |
---|
| 888 | ! print*,'wqd<0!!!' |
---|
| 889 | endif |
---|
| 890 | enddo |
---|
| 891 | enddo |
---|
| 892 | do ig=1,ngrid |
---|
| 893 | wqd(ig,1)=0. |
---|
| 894 | wqd(ig,nlay+1)=0. |
---|
| 895 | enddo |
---|
| 896 | |
---|
| 897 | ! Calcul des tendances |
---|
| 898 | do k=1,nlay |
---|
| 899 | do ig=1,ngrid |
---|
| 900 | q(ig,k)=q(ig,k)+(detr(ig,k)*qa(ig,k)-entr(ig,k)*q(ig,k) & |
---|
| 901 | & -wqd(ig,k)+wqd(ig,k+1)) & |
---|
| 902 | & *ptimestep/masse(ig,k) |
---|
| 903 | enddo |
---|
| 904 | enddo |
---|
| 905 | |
---|
| 906 | endif |
---|
| 907 | |
---|
| 908 | therm_tke_max(:,:)=q(:,:) |
---|
| 909 | |
---|
| 910 | return |
---|
| 911 | !!! fin nrlmd le 10/04/2012 |
---|
| 912 | end |
---|
| 913 | |
---|
[4590] | 914 | END MODULE lmdz_thermcell_main |
---|