1 | MODULE lmdz_thermcell_main |
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2 | ! $Id: lmdz_thermcell_main.F90 5158 2024-08-02 12:12:03Z abarral $ |
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3 | |
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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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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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7 | CONTAINS |
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8 | |
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9 | SUBROUTINE thermcell_main(itap, ngrid, nlay, ptimestep & |
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10 | , pplay,pplev, pphi, debut & |
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11 | , puwind, pvwind,ptemp, p_o, ptemp_env, po_env & |
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12 | , pduadj,pdvadj, pdtadj, pdoadj & |
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13 | , fm0, entr0,detr0, zqta, zqla, lmax & |
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14 | , ratqscth,ratqsdiff, zqsatth & |
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15 | , zmax0, f0, zw2,fraca, ztv & |
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16 | , zpspsk, ztla, zthl,ztva & |
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17 | , pcon, rhobarz, wth3, wmax_sec,lalim, fm, alim_star, zmax, zcong & |
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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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22 | |
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23 | |
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24 | |
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25 | ! USE necessaires pour les lignes importees de thermcell_env |
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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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29 | USE lmdz_thermcell_ini, ONLY: iflag_thermals_tenv |
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30 | USE lmdz_thermcell_ini, ONLY: RD, RG |
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31 | |
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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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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 | USE lmdz_abort_physic, ONLY: abort_physic |
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47 | |
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48 | |
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49 | #ifdef ISO |
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50 | USE infotrac_phy, ONLY: ntiso |
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51 | #ifdef ISOVERIF |
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52 | USE isotopes_mod, ONLY: iso_eau,iso_HDO |
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53 | USE isotopes_verif_mod, ONLY: iso_verif_egalite, & |
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54 | iso_verif_aberrant_encadre |
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55 | #endif |
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56 | #endif |
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57 | |
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58 | |
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59 | IMPLICIT NONE |
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60 | |
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61 | !======================================================================= |
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62 | ! Auteurs: Frederic Hourdin, Catherine Rio, Anne Mathieu |
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63 | ! Version du 09.02.07 |
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64 | ! Calcul du transport vertical dans la couche limite en presence |
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65 | ! de "thermiques" explicitement representes avec processus nuageux |
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66 | |
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67 | ! Reecriture a partir d'un listing papier a Habas, le 14/02/00 |
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68 | |
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69 | ! le thermique est suppose homogene et dissipe par melange avec |
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70 | ! son environnement. la longueur l_mix controle l'efficacite du |
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71 | ! melange |
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72 | |
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73 | ! Le calcul du transport des differentes especes se fait en prenant |
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74 | ! en compte: |
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75 | ! 1. un flux de masse montant |
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76 | ! 2. un flux de masse descendant |
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77 | ! 3. un entrainement |
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78 | ! 4. un detrainement |
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79 | |
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80 | ! Modif 2013/01/04 (FH hourdin@lmd.jussieu.fr) |
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81 | ! Introduction of an implicit computation of vertical advection in |
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82 | ! the environment of thermal plumes in thermcell_dq |
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83 | ! impl = 0 : explicit, 1 : implicit, -1 : old version |
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84 | ! controled by iflag_thermals = |
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85 | ! 15, 16 run with impl=-1 : numerical convergence with NPv3 |
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86 | ! 17, 18 run with impl=1 : more stable |
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87 | ! 15 and 17 correspond to the activation of the stratocumulus "bidouille" |
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88 | |
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89 | ! Using |
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90 | ! abort_physic |
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91 | ! iso_verif_aberrant_encadre |
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92 | ! iso_verif_egalite |
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93 | ! test_ltherm |
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94 | ! thermcell_closure |
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95 | ! thermcell_dq |
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96 | ! thermcell_dry |
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97 | ! thermcell_dv2 |
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98 | ! thermcell_env |
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99 | ! thermcell_flux2 |
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100 | ! thermcell_height |
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101 | ! thermcell_plume |
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102 | ! thermcell_plume_5B |
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103 | ! thermcell_plume_6A |
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104 | |
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105 | !======================================================================= |
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106 | |
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107 | |
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108 | !----------------------------------------------------------------------- |
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109 | ! declarations: |
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110 | ! ------------- |
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111 | |
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112 | |
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113 | ! arguments: |
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114 | ! ---------- |
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115 | INTEGER, INTENT(IN) :: itap, ngrid, nlay |
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116 | REAL, INTENT(IN) :: ptimestep |
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117 | REAL, INTENT(IN), DIMENSION(ngrid, nlay) :: ptemp, puwind, pvwind, pplay, pphi, ptemp_env, po_env |
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118 | ! ATTENTION : zpspsk est inout et out mais c'est pas forcement pour de bonnes raisons (FH, 2023) |
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119 | REAL, INTENT(IN), DIMENSION(ngrid, nlay) :: p_o |
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120 | REAL, INTENT(OUT), DIMENSION(ngrid, nlay) :: zpspsk |
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121 | REAL, INTENT(IN), DIMENSION(ngrid, nlay + 1) :: pplev |
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122 | INTEGER, INTENT(OUT), DIMENSION(ngrid) :: lmax |
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123 | REAL, INTENT(OUT), DIMENSION(ngrid, nlay) :: pdtadj, pduadj, pdvadj, pdoadj, entr0, detr0 |
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124 | REAL, INTENT(OUT), DIMENSION(ngrid, nlay) :: ztla, zqla, zqta, zqsatth, zthl |
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125 | REAL, INTENT(OUT), DIMENSION(ngrid, nlay + 1) :: fm0, zw2, fraca |
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126 | REAL, INTENT(INOUT), DIMENSION(ngrid) :: zmax0, f0 |
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127 | REAL, INTENT(OUT), DIMENSION(ngrid, nlay) :: ztva, ztv |
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128 | logical, INTENT(IN) :: debut |
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129 | REAL, INTENT(OUT), DIMENSION(ngrid, nlay) :: ratqscth, ratqsdiff |
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130 | |
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131 | REAL, INTENT(OUT), DIMENSION(ngrid) :: pcon |
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132 | REAL, INTENT(OUT), DIMENSION(ngrid, nlay) :: rhobarz, wth3 |
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133 | REAL, INTENT(OUT), DIMENSION(ngrid) :: wmax_sec |
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134 | INTEGER, INTENT(OUT), DIMENSION(ngrid) :: lalim |
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135 | REAL, INTENT(OUT), DIMENSION(ngrid, nlay + 1) :: fm |
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136 | REAL, INTENT(OUT), DIMENSION(ngrid, nlay) :: alim_star |
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137 | REAL, INTENT(OUT), DIMENSION(ngrid) :: zmax, zcong |
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138 | |
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139 | ! local: |
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140 | ! ------ |
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141 | |
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142 | INTEGER, save :: igout = 1 |
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143 | !$OMP THREADPRIVATE(igout) |
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144 | INTEGER, save :: lunout1 = 6 |
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145 | !$OMP THREADPRIVATE(lunout1) |
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146 | INTEGER, save :: lev_out = 10 |
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147 | !$OMP THREADPRIVATE(lev_out) |
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148 | |
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149 | REAL lambda, zf, zf2, var, vardiff, CHI |
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150 | INTEGER ig, k, l, ierr, ll |
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151 | LOGICAL sorties |
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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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154 | REAL, DIMENSION(ngrid, nlay) :: ztva_est |
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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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157 | REAL, DIMENSION(ngrid, nlay) :: zta, zha, q2, wq, wthl, wthv, thetath2, wth2 |
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158 | REAL, DIMENSION(ngrid, nlay) :: rho, masse |
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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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165 | REAL, DIMENSION(ngrid, nlay) :: entrdn, detrdn |
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166 | logical, DIMENSION(ngrid, nlay) :: mask |
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167 | |
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168 | CHARACTER (LEN = 20) :: modname = 'thermcell_main' |
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169 | CHARACTER (LEN = 80) :: abort_message |
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170 | |
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171 | |
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172 | #ifdef ISO |
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173 | REAL xtpo(ntiso,ngrid,nlay),xtpdoadj(ntiso,ngrid,nlay) |
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174 | REAL xtzo(ntiso,ngrid,nlay) |
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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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180 | |
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181 | !----------------------------------------------------------------------- |
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182 | ! initialisation: |
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183 | ! --------------- |
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184 | |
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185 | fm = 0. ; entr = 0. ; detr = 0. |
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186 | |
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187 | IF (prt_level>=1) PRINT*, 'thermcell_main V4' |
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188 | |
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189 | sorties = .TRUE. |
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190 | IF(ngrid/=ngrid) THEN |
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191 | PRINT* |
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192 | PRINT*, 'STOP dans convadj' |
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193 | PRINT*, 'ngrid =', ngrid |
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194 | PRINT*, 'ngrid =', ngrid |
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195 | ENDIF |
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196 | |
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197 | !PRINT*,'thermcell_main debut' |
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198 | ! WRITE(lunout,*)'WARNING thermcell_main f0=max(f0,1.e-2)' |
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199 | DO ig = 1, ngrid |
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200 | f0(ig) = max(f0(ig), 1.e-2) |
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201 | zmax0(ig) = max(zmax0(ig), 40.) |
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202 | !IMmarche pas ?! if (f0(ig)<1.e-2) f0(ig)=1.e-2 |
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203 | enddo |
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204 | |
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205 | IF (prt_level>=20) THEN |
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206 | DO ig = 1, ngrid |
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207 | PRINT*, 'th_main ig f0', ig, f0(ig) |
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208 | enddo |
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209 | endif |
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210 | |
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211 | !----------------------------------------------------------------------- |
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212 | ! Calcul de T,q,ql a partir de Tl et qT dans l environnement |
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213 | ! -------------------------------------------------------------------- |
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214 | |
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215 | ! On condense l'eau liquide si besoin. |
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216 | ! En fait on arrive ici d'habitude (jusque 6A) après réévaporation |
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217 | ! Dans une nouvelle mouture, on passe les profiles |
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218 | ! avant la couche limite : iflag_thermals_tenv=1 |
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219 | ! dés le début de la physique : iflag_thermals_tenv=2 |
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220 | ! Mais même pour 2) on ne veut sans doute pas réévaporer. |
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221 | ! On veut comparer thetav dans le thermique, après condensation, |
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222 | ! avec le theta_v effectif de l'environnement. |
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223 | |
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224 | IF (iflag_thermals_tenv - 10 * (iflag_thermals_tenv / 10) == 0) THEN |
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225 | CALL thermcell_env(ngrid, nlay, p_o, ptemp_env, puwind, pvwind, pplay, & |
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226 | pplev, z_o, ztemp_env, zl, ztv, zthl, zu, zv, zpspsk, zqsat, lcong, lintercong, lev_out) |
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227 | |
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228 | else |
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229 | |
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230 | ! Chantier en cours : ne pas effacer (Fredho). 15 septembre 2023 |
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231 | ! Dans la version originale de thermcell_env, on condense l'eau de l'environnement |
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232 | ! pour calculer une temperature potentielle liquide. |
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233 | ! On en déduit un Theta v. |
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234 | |
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235 | ! ... |
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236 | ! contenu de thermcell_env |
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237 | ! SUBROUTINE thermcell_env(ngrid,nlay,po,pt,pu,pv,pplay, & |
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238 | ! & pplev,zo,zh,zl,ztv,zthl,zu,zv,zpspsk,pqsat,lev_out) |
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239 | ! contenu thermcell_env : CALL thermcell_qsat(ngrid*nlay,mask,pplev,pt,po,pqsat) |
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240 | ! contenu thermcell_env : do ll=1,nlay |
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241 | ! contenu thermcell_env : do ig=1,ngrid |
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242 | ! contenu thermcell_env : zl(ig,ll) = max(0.,po(ig,ll)-pqsat(ig,ll)) |
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243 | ! contenu thermcell_env : zh(ig,ll) = pt(ig,ll)+RLvCp*zl(ig,ll) ! T = Tl + Lv/Cp ql |
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244 | ! contenu thermcell_env : zo(ig,ll) = po(ig,ll)-zl(ig,ll) |
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245 | ! contenu thermcell_env : enddo |
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246 | ! contenu thermcell_env : enddo |
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247 | ! contenu thermcell_env : do ll=1,nlay |
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248 | ! contenu thermcell_env : do ig=1,ngrid |
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249 | ! contenu thermcell_env : zpspsk(ig,ll)=(pplay(ig,ll)/100000.)**RKAPPA |
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250 | ! contenu thermcell_env : zu(ig,ll)=pu(ig,ll) |
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251 | ! contenu thermcell_env : zv(ig,ll)=pv(ig,ll) |
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252 | ! contenu thermcell_env : ztv(ig,ll)=zh(ig,ll)/zpspsk(ig,ll) |
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253 | ! contenu thermcell_env : ztv(ig,ll)=ztv(ig,ll)*(1.+RETV*(zo(ig,ll))-zl(ig,ll)) |
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254 | ! contenu thermcell_env : zthl(ig,ll)=pt(ig,ll)/zpspsk(ig,ll) |
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255 | ! contenu thermcell_env : enddo |
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256 | ! contenu thermcell_env : enddo |
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257 | |
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258 | DO l = 1, nlay |
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259 | DO ig = 1, ngrid |
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260 | zl(ig, l) = 0. |
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261 | zu(ig, l) = puwind(ig, l) |
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262 | zv(ig, l) = pvwind(ig, l) |
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263 | ztemp_env(ig, l) = ptemp_env(ig, l) |
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264 | zpspsk(ig, l) = (pplay(ig, l) / 100000.)**RKAPPA |
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265 | ztv(ig, l) = ztemp_env(ig, l) / zpspsk(ig, l) |
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266 | ztv(ig, l) = ztv(ig, l) * (1. + RETV * po_env(ig, l)) |
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267 | zthl(ig, l) = ptemp(ig, l) / zpspsk(ig, l) |
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268 | mask(ig, l) = .TRUE. |
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269 | enddo |
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270 | enddo |
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271 | CALL thermcell_qsat(ngrid * nlay, mask, pplev, ptemp_env, p_o, zqsat) |
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272 | |
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273 | endif |
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274 | |
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275 | IF (prt_level>=1) PRINT*, 'thermcell_main apres thermcell_env' |
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276 | |
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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 | ! wa, fraca, wd, fracd -------------------- zlev(2), rhobarz |
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285 | ! wh,wt,wo ... |
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286 | |
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287 | ! + + + + + + + + + + + zh,zu,zv,z_o,rho |
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288 | |
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289 | |
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290 | ! -------------------- zlev(1) |
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291 | ! \\\\\\\\\\\\\\\\\\\\ |
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292 | |
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293 | |
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294 | !----------------------------------------------------------------------- |
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295 | ! Calcul des altitudes des couches |
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296 | !----------------------------------------------------------------------- |
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297 | |
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298 | DO l = 2, nlay |
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299 | zlev(:, l) = 0.5 * (pphi(:, l) + pphi(:, l - 1)) / RG |
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300 | enddo |
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301 | zlev(:, 1) = 0. |
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302 | zlev(:, nlay + 1) = (2. * pphi(:, nlay) - pphi(:, nlay - 1)) / RG |
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303 | DO l = 1, nlay |
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304 | zlay(:, l) = pphi(:, l) / RG |
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305 | enddo |
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306 | DO l = 1, nlay |
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307 | deltaz(:, l) = zlev(:, l + 1) - zlev(:, l) |
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308 | enddo |
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309 | |
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310 | !----------------------------------------------------------------------- |
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311 | ! Calcul des densites et masses |
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312 | !----------------------------------------------------------------------- |
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313 | |
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314 | rho(:, :) = pplay(:, :) / (zpspsk(:, :) * RD * ztv(:, :)) |
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315 | IF (prt_level>=10) WRITE(lunout, *) 'WARNING thermcell_main rhobarz(:,1)=rho(:,1)' |
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316 | rhobarz(:, 1) = rho(:, 1) |
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317 | DO l = 2, nlay |
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318 | rhobarz(:, l) = 0.5 * (rho(:, l) + rho(:, l - 1)) |
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319 | enddo |
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320 | DO l = 1, nlay |
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321 | masse(:, l) = (pplev(:, l) - pplev(:, l + 1)) / RG |
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322 | enddo |
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323 | IF (prt_level>=1) PRINT*, 'thermcell_main apres initialisation' |
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324 | |
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325 | !------------------------------------------------------------------ |
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326 | |
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327 | ! /|\ |
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328 | ! -------- | F_k+1 ------- |
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329 | ! ----> D_k |
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330 | ! /|\ <---- E_k , A_k |
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331 | ! -------- | F_k --------- |
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332 | ! ----> D_k-1 |
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333 | ! <---- E_k-1 , A_k-1 |
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334 | |
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335 | |
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336 | |
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337 | |
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338 | |
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339 | ! --------------------------- |
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340 | |
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341 | ! ----- F_lmax+1=0 ---------- \ |
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342 | ! lmax (zmax) | |
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343 | ! --------------------------- | |
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344 | ! | |
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345 | ! --------------------------- | |
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346 | ! | |
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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 | ! | E |
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353 | ! --------------------------- | D |
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354 | ! | |
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355 | ! --------------------------- | |
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356 | ! | |
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357 | ! --------------------------- \ | |
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358 | ! lalim | | |
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359 | ! --------------------------- | | |
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360 | ! | | |
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361 | ! --------------------------- | | |
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362 | ! | A | |
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363 | ! --------------------------- | | |
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364 | ! | | |
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365 | ! --------------------------- | | |
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366 | ! lmin (=1 pour le moment) | | |
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367 | ! ----- F_lmin=0 ------------ / / |
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368 | |
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369 | ! --------------------------- |
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370 | ! ////////////////////////// |
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371 | |
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372 | |
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373 | !============================================================================= |
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374 | ! Calculs initiaux ne faisant pas intervenir les changements de phase |
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375 | !============================================================================= |
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376 | |
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377 | !------------------------------------------------------------------ |
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378 | ! 1. alim_star est le profil vertical de l'alimentation a la base du |
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379 | ! panache thermique, calcule a partir de la flotabilite de l'air sec |
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380 | ! 2. lmin et lalim sont les indices inferieurs et superieurs de alim_star |
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381 | !------------------------------------------------------------------ |
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382 | |
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383 | entr_star = 0. ; detr_star = 0. ; alim_star = 0. ; alim_star_tot = 0. |
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384 | lmin = 1 |
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385 | |
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386 | !----------------------------------------------------------------------------- |
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387 | ! 3. wmax_sec et zmax_sec sont les vitesses et altitudes maximum d'un |
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388 | ! panache sec conservatif (e=d=0) alimente selon alim_star |
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389 | ! Il s'agit d'un calcul de type CAPE |
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390 | ! zmax_sec est utilise pour determiner la geometrie du thermique. |
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391 | !------------------------------------------------------------------------------ |
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392 | !--------------------------------------------------------------------------------- |
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393 | !calcul du melange et des variables dans le thermique |
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394 | !-------------------------------------------------------------------------------- |
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395 | |
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396 | IF (prt_level>=1) PRINT*, 'avant thermcell_plume ', lev_out |
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397 | |
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398 | !===================================================================== |
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399 | ! Old version of thermcell_plume in thermcell_plume_6A.F90 |
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400 | ! It includes both thermcell_plume_6A and thermcell_plume_5B corresponding |
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401 | ! to the 5B and 6A versions used for CMIP5 and CMIP6. |
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402 | ! The latest was previously named thermcellV1_plume. |
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403 | ! The new thermcell_plume is a clean version (removing obsolete |
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404 | ! options) of thermcell_plume_6A. |
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405 | ! The 3 versions are controled by |
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406 | ! flag_thermals_ed <= 9 thermcell_plume_6A |
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407 | ! <= 19 thermcell_plume_5B |
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408 | ! else thermcell_plume (default 20 for convergence with 6A) |
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409 | ! Fredho |
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410 | !===================================================================== |
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411 | |
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412 | IF (iflag_thermals_ed<=9) THEN |
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413 | ! PRINT*,'THERM NOUVELLE/NOUVELLE Arnaud' |
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414 | CALL thermcell_plume_6A(itap, ngrid, nlay, ptimestep, ztv, zthl, p_o, zl, rhobarz, & |
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415 | zlev, pplev, pphi, zpspsk, alim_star, alim_star_tot, & |
---|
416 | lalim, f0, detr_star, entr_star, f_star, csc, ztva, & |
---|
417 | ztla, zqla, zqta, zha, zw2, zw_est, ztva_est, zqsatth, lmix, lmix_bis, linter & |
---|
418 | , lev_out, lunout1, igout) |
---|
419 | |
---|
420 | elseif (iflag_thermals_ed<=19) THEN |
---|
421 | ! PRINT*,'THERM RIO et al 2010, version d Arnaud' |
---|
422 | CALL thermcell_plume_5B(itap, ngrid, nlay, ptimestep, ztv, zthl, p_o, zl, rhobarz, & |
---|
423 | zlev, pplev, pphi, zpspsk, alim_star, alim_star_tot, & |
---|
424 | lalim, f0, detr_star, entr_star, f_star, csc, ztva, & |
---|
425 | ztla, zqla, zqta, zha, zw2, zw_est, ztva_est, zqsatth, lmix, lmix_bis, linter & |
---|
426 | , lev_out, lunout1, igout) |
---|
427 | else |
---|
428 | CALL thermcell_plume(itap, ngrid, nlay, ptimestep, ztv, zthl, p_o, zl, rhobarz, & |
---|
429 | zlev, pplev, pphi, zpspsk, alim_star, alim_star_tot, & |
---|
430 | lalim, f0, detr_star, entr_star, f_star, csc, ztva, & |
---|
431 | ztla, zqla, zqta, zha, zw2, zw_est, ztva_est, zqsatth, lmix, lmix_bis, linter & |
---|
432 | , lev_out, lunout1, igout) |
---|
433 | endif |
---|
434 | |
---|
435 | IF (prt_level>=1) PRINT*, 'apres thermcell_plume ', lev_out |
---|
436 | |
---|
437 | CALL test_ltherm(ngrid, nlay, pplay, lalim, ztv, p_o, ztva, zqla, f_star, zw2, 'thermcell_plum lalim ') |
---|
438 | CALL test_ltherm(ngrid, nlay, pplay, lmix, ztv, p_o, ztva, zqla, f_star, zw2, 'thermcell_plum lmix ') |
---|
439 | |
---|
440 | IF (prt_level>=1) PRINT*, 'thermcell_main apres thermcell_plume' |
---|
441 | IF (prt_level>=10) THEN |
---|
442 | WRITE(lunout1, *) 'Dans thermcell_main 2' |
---|
443 | WRITE(lunout1, *) 'lmin ', lmin(igout) |
---|
444 | WRITE(lunout1, *) 'lalim ', lalim(igout) |
---|
445 | WRITE(lunout1, *) ' ig l alim_star entr_star detr_star f_star ' |
---|
446 | WRITE(lunout1, '(i6,i4,4e15.5)') (igout, l, alim_star(igout, l), entr_star(igout, l), detr_star(igout, l) & |
---|
447 | , f_star(igout, l + 1), l = 1, nint(linter(igout)) + 5) |
---|
448 | endif |
---|
449 | |
---|
450 | !------------------------------------------------------------------------------- |
---|
451 | ! Calcul des caracteristiques du thermique:zmax,zmix,wmax |
---|
452 | !------------------------------------------------------------------------------- |
---|
453 | |
---|
454 | CALL thermcell_height(ngrid, nlay, lalim, lmin, linter, lcong, lintercong, lmix, zw2, & |
---|
455 | zlev, lmax, zmax, zmax0, zmix, wmax, zcong) |
---|
456 | ! Attention, w2 est transforme en sa racine carree dans cette routine |
---|
457 | ! Le probleme vient du fait que linter et lmix sont souvent egaux a 1. |
---|
458 | wmax_tmp = 0. |
---|
459 | DO l = 1, nlay |
---|
460 | wmax_tmp(:) = max(wmax_tmp(:), zw2(:, l)) |
---|
461 | enddo |
---|
462 | ! PRINT*,"ZMAX ",lalim,lmin,linter,lmix,lmax,zmax,zmax0,zmix,wmax |
---|
463 | |
---|
464 | CALL test_ltherm(ngrid, nlay, pplay, lalim, ztv, p_o, ztva, zqla, f_star, zw2, 'thermcell_heig lalim ') |
---|
465 | CALL test_ltherm(ngrid, nlay, pplay, lmin, ztv, p_o, ztva, zqla, f_star, zw2, 'thermcell_heig lmin ') |
---|
466 | CALL test_ltherm(ngrid, nlay, pplay, lmix, ztv, p_o, ztva, zqla, f_star, zw2, 'thermcell_heig lmix ') |
---|
467 | CALL test_ltherm(ngrid, nlay, pplay, lmax, ztv, p_o, ztva, zqla, f_star, zw2, 'thermcell_heig lmax ') |
---|
468 | |
---|
469 | IF (prt_level>=1) PRINT*, 'thermcell_main apres thermcell_height' |
---|
470 | |
---|
471 | !------------------------------------------------------------------------------- |
---|
472 | ! Fermeture,determination de f |
---|
473 | !------------------------------------------------------------------------------- |
---|
474 | |
---|
475 | CALL thermcell_dry(ngrid, nlay, zlev, pphi, ztv, alim_star, & |
---|
476 | lalim, lmin, zmax_sec, wmax_sec) |
---|
477 | |
---|
478 | CALL test_ltherm(ngrid, nlay, pplay, lmin, ztv, p_o, ztva, zqla, f_star, zw2, 'thermcell_dry lmin ') |
---|
479 | CALL test_ltherm(ngrid, nlay, pplay, lalim, ztv, p_o, ztva, zqla, f_star, zw2, 'thermcell_dry lalim ') |
---|
480 | |
---|
481 | IF (prt_level>=1) PRINT*, 'thermcell_main apres thermcell_dry' |
---|
482 | IF (prt_level>=10) THEN |
---|
483 | WRITE(lunout1, *) 'Dans thermcell_main 1b' |
---|
484 | WRITE(lunout1, *) 'lmin ', lmin(igout) |
---|
485 | WRITE(lunout1, *) 'lalim ', lalim(igout) |
---|
486 | WRITE(lunout1, *) ' ig l alim_star entr_star detr_star f_star ' |
---|
487 | WRITE(lunout1, '(i6,i4,e15.5)') (igout, l, alim_star(igout, l) & |
---|
488 | , l = 1, lalim(igout) + 4) |
---|
489 | endif |
---|
490 | |
---|
491 | |
---|
492 | |
---|
493 | |
---|
494 | ! Choix de la fonction d'alimentation utilisee pour la fermeture. |
---|
495 | ! Apparemment sans importance |
---|
496 | alim_star_clos(:, :) = alim_star(:, :) |
---|
497 | alim_star_clos(:, :) = entr_star(:, :) + alim_star(:, :) |
---|
498 | |
---|
499 | !CR Appel de la fermeture seche |
---|
500 | IF (iflag_thermals_closure==1) THEN |
---|
501 | CALL thermcell_closure(ngrid, nlay, r_aspect_thermals, ptimestep, rho, & |
---|
502 | zlev, lalim, alim_star_clos, zmax_sec, wmax_sec, f) |
---|
503 | |
---|
504 | !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! |
---|
505 | ! Appel avec les zmax et wmax tenant compte de la condensation |
---|
506 | ! Semble moins bien marcher |
---|
507 | ELSE IF (iflag_thermals_closure==2) THEN |
---|
508 | CALL thermcell_closure(ngrid, nlay, r_aspect_thermals, ptimestep, rho, & |
---|
509 | zlev, lalim, alim_star, zmax, wmax, f) |
---|
510 | |
---|
511 | endif |
---|
512 | |
---|
513 | !!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!! |
---|
514 | |
---|
515 | IF(prt_level>=1)PRINT*, 'thermcell_closure apres thermcell_closure' |
---|
516 | |
---|
517 | IF (tau_thermals>1.) THEN |
---|
518 | lambda = exp(-ptimestep / tau_thermals) |
---|
519 | f0 = (1. - lambda) * f + lambda * f0 |
---|
520 | else |
---|
521 | f0 = f |
---|
522 | endif |
---|
523 | |
---|
524 | ! Test valable seulement en 1D mais pas genant |
---|
525 | IF (.NOT. (f0(1)>=0.)) THEN |
---|
526 | abort_message = '.NOT. (f0(1).ge.0.)' |
---|
527 | CALL abort_physic (modname, abort_message, 1) |
---|
528 | endif |
---|
529 | |
---|
530 | !------------------------------------------------------------------------------- |
---|
531 | !deduction des flux |
---|
532 | |
---|
533 | CALL thermcell_flux2(ngrid, nlay, ptimestep, masse, & |
---|
534 | lalim, lmax, alim_star, & |
---|
535 | entr_star, detr_star, f, rhobarz, zlev, zw2, fm, entr, & |
---|
536 | detr, zqla, lev_out, lunout1, igout) |
---|
537 | |
---|
538 | !IM 060508 & detr,zqla,zmax,lev_out,lunout,igout) |
---|
539 | |
---|
540 | IF (prt_level>=1) PRINT*, 'thermcell_main apres thermcell_flux' |
---|
541 | CALL test_ltherm(ngrid, nlay, pplay, lalim, ztv, p_o, ztva, zqla, f_star, zw2, 'thermcell_flux lalim ') |
---|
542 | CALL test_ltherm(ngrid, nlay, pplay, lmax, ztv, p_o, ztva, zqla, f_star, zw2, 'thermcell_flux lmax ') |
---|
543 | |
---|
544 | !------------------------------------------------------------------ |
---|
545 | ! On ne prend pas directement les profils issus des calculs precedents |
---|
546 | ! mais on s'autorise genereusement une relaxation vers ceci avec |
---|
547 | ! une constante de temps tau_thermals (typiquement 1800s). |
---|
548 | !------------------------------------------------------------------ |
---|
549 | |
---|
550 | IF (tau_thermals>1.) THEN |
---|
551 | lambda = exp(-ptimestep / tau_thermals) |
---|
552 | fm0 = (1. - lambda) * fm + lambda * fm0 |
---|
553 | entr0 = (1. - lambda) * entr + lambda * entr0 |
---|
554 | detr0 = (1. - lambda) * detr + lambda * detr0 |
---|
555 | else |
---|
556 | fm0 = fm |
---|
557 | entr0 = entr |
---|
558 | detr0 = detr |
---|
559 | endif |
---|
560 | |
---|
561 | !------------------------------------------------------------------ |
---|
562 | ! Calcul de la fraction de l'ascendance |
---|
563 | !------------------------------------------------------------------ |
---|
564 | DO ig = 1, ngrid |
---|
565 | fraca(ig, 1) = 0. |
---|
566 | fraca(ig, nlay + 1) = 0. |
---|
567 | enddo |
---|
568 | DO l = 2, nlay |
---|
569 | DO ig = 1, ngrid |
---|
570 | IF (zw2(ig, l)>1.e-10) THEN |
---|
571 | fraca(ig, l) = fm(ig, l) / (rhobarz(ig, l) * zw2(ig, l)) |
---|
572 | else |
---|
573 | fraca(ig, l) = 0. |
---|
574 | endif |
---|
575 | enddo |
---|
576 | enddo |
---|
577 | |
---|
578 | !c------------------------------------------------------------------ |
---|
579 | ! calcul du transport vertical |
---|
580 | !------------------------------------------------------------------ |
---|
581 | IF (iflag_thermals_down > 0) THEN |
---|
582 | IF (debut) PRINT*, 'WARNING !!! routine thermcell_down en cours de developpement' |
---|
583 | entrdn = fact_thermals_down * detr0 |
---|
584 | detrdn = fact_thermals_down * entr0 |
---|
585 | ! we want to transport potential temperature, total water and momentum |
---|
586 | CALL thermcell_updown_dq(ngrid, nlay, ptimestep, lmax, entr0, detr0, entrdn, detrdn, masse, zthl, zdthladj) |
---|
587 | CALL thermcell_updown_dq(ngrid, nlay, ptimestep, lmax, entr0, detr0, entrdn, detrdn, masse, p_o, pdoadj) |
---|
588 | CALL thermcell_updown_dq(ngrid, nlay, ptimestep, lmax, entr0, detr0, entrdn, detrdn, masse, zu, pduadj) |
---|
589 | CALL thermcell_updown_dq(ngrid, nlay, ptimestep, lmax, entr0, detr0, entrdn, detrdn, masse, zv, pdvadj) |
---|
590 | ELSE |
---|
591 | !-------------------------------------------------------------- |
---|
592 | |
---|
593 | ! Temperature potentielle liquide effectivement mélangée par les thermiques |
---|
594 | DO ll = 1, nlay |
---|
595 | DO ig = 1, ngrid |
---|
596 | zthl(ig, ll) = ptemp(ig, ll) / zpspsk(ig, ll) |
---|
597 | enddo |
---|
598 | enddo |
---|
599 | CALL thermcell_dq(ngrid, nlay, dqimpl, ptimestep, fm0, entr0, masse, & |
---|
600 | zthl, zdthladj, zta, lev_out) |
---|
601 | |
---|
602 | DO ll = 1, nlay |
---|
603 | DO ig = 1, ngrid |
---|
604 | z_o(ig, ll) = p_o(ig, ll) |
---|
605 | enddo |
---|
606 | enddo |
---|
607 | CALL thermcell_dq(ngrid, nlay, dqimpl, ptimestep, fm0, entr0, masse, & |
---|
608 | z_o, pdoadj, z_oa, lev_out) |
---|
609 | |
---|
610 | #ifdef ISO |
---|
611 | ! C Risi: on utilise directement la meme routine |
---|
612 | DO ixt=1,ntiso |
---|
613 | DO ll=1,nlay |
---|
614 | DO ig=1,ngrid |
---|
615 | xtpo_tmp(ig,ll)=xtpo(ixt,ig,ll) |
---|
616 | xtzo_tmp(ig,ll)=xtzo(ixt,ig,ll) |
---|
617 | enddo |
---|
618 | enddo |
---|
619 | CALL thermcell_dq(ngrid,nlay,dqimpl,ptimestep,fm0,entr0,masse, & |
---|
620 | xtpo_tmp,xtpdoadj_tmp,xtzo_tmp,lev_out) |
---|
621 | DO ll=1,nlay |
---|
622 | DO ig=1,ngrid |
---|
623 | xtpdoadj(ixt,ig,ll)=xtpdoadj_tmp(ig,ll) |
---|
624 | enddo |
---|
625 | enddo |
---|
626 | enddo |
---|
627 | #endif |
---|
628 | |
---|
629 | #ifdef ISO |
---|
630 | #ifdef ISOVERIF |
---|
631 | DO ll=1,nlay |
---|
632 | DO ig=1,ngrid |
---|
633 | IF (iso_eau.gt.0) THEN |
---|
634 | CALL iso_verif_egalite(xtpo(iso_eau,ig,ll), & |
---|
635 | p_o(ig,ll),'thermcell_main 594') |
---|
636 | CALL iso_verif_egalite(xtpdoadj(iso_eau,ig,ll), & |
---|
637 | pdoadj(ig,ll),'thermcell_main 596') |
---|
638 | endif |
---|
639 | IF (iso_HDO.gt.0) THEN |
---|
640 | CALL iso_verif_aberrant_encadre(xtpo(iso_hdo,ig,ll) & |
---|
641 | /p_o(ig,ll),'thermcell_main 610') |
---|
642 | endif |
---|
643 | enddo |
---|
644 | enddo !DO ll=1,nlay |
---|
645 | WRITE(*,*) 'thermcell_main 600 tmp: apres thermcell_dq' |
---|
646 | #endif |
---|
647 | #endif |
---|
648 | |
---|
649 | |
---|
650 | !------------------------------------------------------------------ |
---|
651 | ! calcul du transport vertical du moment horizontal |
---|
652 | !------------------------------------------------------------------ |
---|
653 | |
---|
654 | !IM 090508 |
---|
655 | IF (dvdq == 0) THEN |
---|
656 | ! Calcul du transport de V tenant compte d'echange par gradient |
---|
657 | ! de pression horizontal avec l'environnement |
---|
658 | |
---|
659 | CALL thermcell_dv2(ngrid, nlay, ptimestep, fm0, entr0, masse & |
---|
660 | ! & ,fraca*dvdq,zmax & |
---|
661 | , fraca, zmax & |
---|
662 | , zu, zv, pduadj, pdvadj, zua, zva, lev_out) |
---|
663 | |
---|
664 | else |
---|
665 | |
---|
666 | ! calcul purement conservatif pour le transport de V |
---|
667 | CALL thermcell_dq(ngrid, nlay, dqimpl, ptimestep, fm0, entr0, masse & |
---|
668 | , zu, pduadj, zua, lev_out) |
---|
669 | CALL thermcell_dq(ngrid, nlay, dqimpl, ptimestep, fm0, entr0, masse & |
---|
670 | , zv, pdvadj, zva, lev_out) |
---|
671 | |
---|
672 | endif |
---|
673 | ENDIF |
---|
674 | |
---|
675 | ! PRINT*,'13 OK convect8' |
---|
676 | DO l = 1, nlay |
---|
677 | DO ig = 1, ngrid |
---|
678 | pdtadj(ig, l) = zdthladj(ig, l) * zpspsk(ig, l) |
---|
679 | enddo |
---|
680 | enddo |
---|
681 | |
---|
682 | IF (prt_level>=1) PRINT*, '14 OK convect8' |
---|
683 | !------------------------------------------------------------------ |
---|
684 | ! Calculs de diagnostiques pour les sorties |
---|
685 | !------------------------------------------------------------------ |
---|
686 | !calcul de fraca pour les sorties |
---|
687 | |
---|
688 | IF (sorties) THEN |
---|
689 | IF (prt_level>=1) PRINT*, '14a OK convect8' |
---|
690 | ! calcul du niveau de condensation |
---|
691 | ! initialisation |
---|
692 | DO ig = 1, ngrid |
---|
693 | nivcon(ig) = 0 |
---|
694 | zcon(ig) = 0. |
---|
695 | enddo |
---|
696 | !nouveau calcul |
---|
697 | DO ig = 1, ngrid |
---|
698 | ! WARNING !!! verifier que c'est bien ztemp_env qu'on veut là |
---|
699 | CHI = ztemp_env(ig, 1) / (1669.0 - 122.0 * z_o(ig, 1) / zqsat(ig, 1) - ztemp_env(ig, 1)) |
---|
700 | pcon(ig) = pplay(ig, 1) * (z_o(ig, 1) / zqsat(ig, 1))**CHI |
---|
701 | enddo |
---|
702 | !IM do k=1,nlay |
---|
703 | DO k = 1, nlay - 1 |
---|
704 | DO ig = 1, ngrid |
---|
705 | IF ((pcon(ig)<=pplay(ig, k)) & |
---|
706 | .AND.(pcon(ig)>pplay(ig, k + 1))) THEN |
---|
707 | zcon2(ig) = zlay(ig, k) - (pcon(ig) - pplay(ig, k)) / (RG * rho(ig, k)) / 100. |
---|
708 | endif |
---|
709 | enddo |
---|
710 | enddo |
---|
711 | !IM |
---|
712 | ierr = 0 |
---|
713 | DO ig = 1, ngrid |
---|
714 | IF (pcon(ig)<=pplay(ig, nlay)) THEN |
---|
715 | zcon2(ig) = zlay(ig, nlay) - (pcon(ig) - pplay(ig, nlay)) / (RG * rho(ig, nlay)) / 100. |
---|
716 | ierr = 1 |
---|
717 | endif |
---|
718 | enddo |
---|
719 | ! if (ierr==1) THEN |
---|
720 | ! abort_message = 'thermcellV0_main: les thermiques vont trop haut ' |
---|
721 | ! CALL abort_physic (modname,abort_message,1) |
---|
722 | ! endif |
---|
723 | |
---|
724 | IF (prt_level>=1) PRINT*, '14b OK convect8' |
---|
725 | DO k = nlay, 1, -1 |
---|
726 | DO ig = 1, ngrid |
---|
727 | IF (zqla(ig, k)>1e-10) THEN |
---|
728 | nivcon(ig) = k |
---|
729 | zcon(ig) = zlev(ig, k) |
---|
730 | endif |
---|
731 | enddo |
---|
732 | enddo |
---|
733 | IF (prt_level>=1) PRINT*, '14c OK convect8' |
---|
734 | !calcul des moments |
---|
735 | !initialisation |
---|
736 | DO l = 1, nlay |
---|
737 | DO ig = 1, ngrid |
---|
738 | q2(ig, l) = 0. |
---|
739 | wth2(ig, l) = 0. |
---|
740 | wth3(ig, l) = 0. |
---|
741 | ratqscth(ig, l) = 0. |
---|
742 | ratqsdiff(ig, l) = 0. |
---|
743 | enddo |
---|
744 | enddo |
---|
745 | IF (prt_level>=1) PRINT*, '14d OK convect8' |
---|
746 | IF (prt_level>=10)WRITE(lunout, *) & |
---|
747 | 'WARNING thermcell_main wth2=0. si zw2 > 1.e-10' |
---|
748 | DO l = 1, nlay |
---|
749 | DO ig = 1, ngrid |
---|
750 | zf = fraca(ig, l) |
---|
751 | zf2 = zf / (1. - zf) |
---|
752 | |
---|
753 | thetath2(ig, l) = zf2 * (ztla(ig, l) - zthl(ig, l))**2 |
---|
754 | IF(zw2(ig, l)>1.e-10) THEN |
---|
755 | wth2(ig, l) = zf2 * (zw2(ig, l))**2 |
---|
756 | else |
---|
757 | wth2(ig, l) = 0. |
---|
758 | endif |
---|
759 | wth3(ig, l) = zf2 * (1 - 2. * fraca(ig, l)) / (1 - fraca(ig, l)) & |
---|
760 | * zw2(ig, l) * zw2(ig, l) * zw2(ig, l) |
---|
761 | q2(ig, l) = zf2 * (zqta(ig, l) * 1000. - p_o(ig, l) * 1000.)**2 |
---|
762 | !test: on calcul q2/p_o=ratqsc |
---|
763 | ratqscth(ig, l) = sqrt(max(q2(ig, l), 1.e-6) / (p_o(ig, l) * 1000.)) |
---|
764 | enddo |
---|
765 | enddo |
---|
766 | !calcul des flux: q, thetal et thetav |
---|
767 | DO l = 1, nlay |
---|
768 | DO ig = 1, ngrid |
---|
769 | wq(ig, l) = fraca(ig, l) * zw2(ig, l) * (zqta(ig, l) * 1000. - p_o(ig, l) * 1000.) |
---|
770 | wthl(ig, l) = fraca(ig, l) * zw2(ig, l) * (ztla(ig, l) - zthl(ig, l)) |
---|
771 | wthv(ig, l) = fraca(ig, l) * zw2(ig, l) * (ztva(ig, l) - ztv(ig, l)) |
---|
772 | enddo |
---|
773 | enddo |
---|
774 | |
---|
775 | !calcul du ratqscdiff |
---|
776 | IF (prt_level>=1) PRINT*, '14e OK convect8' |
---|
777 | var = 0. |
---|
778 | vardiff = 0. |
---|
779 | ratqsdiff(:, :) = 0. |
---|
780 | |
---|
781 | DO l = 1, nlay |
---|
782 | DO ig = 1, ngrid |
---|
783 | IF (l<=lalim(ig)) THEN |
---|
784 | var = var + alim_star(ig, l) * zqta(ig, l) * 1000. |
---|
785 | endif |
---|
786 | enddo |
---|
787 | enddo |
---|
788 | |
---|
789 | IF (prt_level>=1) PRINT*, '14f OK convect8' |
---|
790 | |
---|
791 | DO l = 1, nlay |
---|
792 | DO ig = 1, ngrid |
---|
793 | IF (l<=lalim(ig)) THEN |
---|
794 | zf = fraca(ig, l) |
---|
795 | zf2 = zf / (1. - zf) |
---|
796 | vardiff = vardiff + alim_star(ig, l) * (zqta(ig, l) * 1000. - var)**2 |
---|
797 | endif |
---|
798 | enddo |
---|
799 | enddo |
---|
800 | |
---|
801 | IF (prt_level>=1) PRINT*, '14g OK convect8' |
---|
802 | DO l = 1, nlay |
---|
803 | DO ig = 1, ngrid |
---|
804 | ratqsdiff(ig, l) = sqrt(vardiff) / (p_o(ig, l) * 1000.) |
---|
805 | enddo |
---|
806 | enddo |
---|
807 | endif |
---|
808 | |
---|
809 | IF (prt_level>=1) PRINT*, 'thermcell_main FIN OK' |
---|
810 | |
---|
811 | !PRINT*,'thermcell_main fin' |
---|
812 | |
---|
813 | END SUBROUTINE thermcell_main |
---|
814 | |
---|
815 | !============================================================================= |
---|
816 | !///////////////////////////////////////////////////////////////////////////// |
---|
817 | !============================================================================= |
---|
818 | SUBROUTINE test_ltherm(ngrid, nlay, pplay, long, ztv, p_o, ztva, & ! in |
---|
819 | zqla, f_star, zw2, comment) ! in |
---|
820 | !============================================================================= |
---|
821 | USE lmdz_thermcell_ini, ONLY: prt_level |
---|
822 | IMPLICIT NONE |
---|
823 | |
---|
824 | INTEGER i, k, ngrid, nlay |
---|
825 | REAL, INTENT(IN), DIMENSION(ngrid, nlay) :: pplay, ztv, p_o, ztva, zqla |
---|
826 | REAL, INTENT(IN), DIMENSION(ngrid, nlay) :: f_star, zw2 |
---|
827 | INTEGER, INTENT(IN), DIMENSION(ngrid) :: long |
---|
828 | REAL seuil |
---|
829 | CHARACTER*21 comment |
---|
830 | |
---|
831 | seuil = 0.25 |
---|
832 | |
---|
833 | IF (prt_level>=1) THEN |
---|
834 | PRINT*, 'WARNING !!! TEST ', comment |
---|
835 | endif |
---|
836 | return |
---|
837 | |
---|
838 | ! test sur la hauteur des thermiques ... |
---|
839 | DO i = 1, ngrid |
---|
840 | !IMtemp if (pplay(i,long(i)).lt.seuil*pplev(i,1)) THEN |
---|
841 | IF (prt_level>=10) THEN |
---|
842 | PRINT*, 'WARNING ', comment, ' au point ', i, ' K= ', long(i) |
---|
843 | PRINT*, ' K P(MB) THV(K) Qenv(g/kg)THVA QLA(g/kg) F* W2' |
---|
844 | DO k = 1, nlay |
---|
845 | 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) |
---|
846 | enddo |
---|
847 | endif |
---|
848 | enddo |
---|
849 | |
---|
850 | RETURN |
---|
851 | end |
---|
852 | |
---|
853 | ! nrlmd le 10/04/2012 Transport de la TKE par le thermique moyen pour la fermeture en ALP |
---|
854 | ! On transporte pbl_tke pour donner therm_tke |
---|
855 | ! Copie conforme de la SUBROUTINE DTKE dans physiq.F ecrite par Frederic Hourdin |
---|
856 | |
---|
857 | !======================================================================= |
---|
858 | !/////////////////////////////////////////////////////////////////////// |
---|
859 | !======================================================================= |
---|
860 | |
---|
861 | SUBROUTINE thermcell_tke_transport(& |
---|
862 | ngrid, nlay, ptimestep, fm0, entr0, rg, pplev, & ! in |
---|
863 | therm_tke_max) ! out |
---|
864 | USE lmdz_thermcell_ini, ONLY: prt_level |
---|
865 | IMPLICIT NONE |
---|
866 | |
---|
867 | !======================================================================= |
---|
868 | |
---|
869 | ! Calcul du transport verticale dans la couche limite en presence |
---|
870 | ! de "thermiques" explicitement representes |
---|
871 | ! calcul du dq/dt une fois qu'on connait les ascendances |
---|
872 | |
---|
873 | !======================================================================= |
---|
874 | |
---|
875 | INTEGER ngrid, nlay |
---|
876 | |
---|
877 | REAL, INTENT(IN) :: ptimestep |
---|
878 | REAL, INTENT(IN), DIMENSION(ngrid, nlay + 1) :: fm0, pplev |
---|
879 | REAL, INTENT(IN), DIMENSION(ngrid, nlay) :: entr0 |
---|
880 | REAL, INTENT(IN) :: rg |
---|
881 | REAL, INTENT(OUT), DIMENSION(ngrid, nlay) :: therm_tke_max |
---|
882 | |
---|
883 | REAL detr0(ngrid, nlay) |
---|
884 | REAL masse0(ngrid, nlay) |
---|
885 | REAL masse(ngrid, nlay), fm(ngrid, nlay + 1) |
---|
886 | REAL entr(ngrid, nlay) |
---|
887 | REAL q(ngrid, nlay) |
---|
888 | INTEGER lev_out ! niveau pour les print |
---|
889 | |
---|
890 | REAL qa(ngrid, nlay), detr(ngrid, nlay), wqd(ngrid, nlay + 1) |
---|
891 | INTEGER ig, k |
---|
892 | |
---|
893 | lev_out = 0 |
---|
894 | |
---|
895 | IF (prt_level>=1) PRINT*, 'Q2 THERMCEL_DQ 0' |
---|
896 | |
---|
897 | ! calcul du detrainement |
---|
898 | DO k = 1, nlay |
---|
899 | detr0(:, k) = fm0(:, k) - fm0(:, k + 1) + entr0(:, k) |
---|
900 | masse0(:, k) = (pplev(:, k) - pplev(:, k + 1)) / RG |
---|
901 | enddo |
---|
902 | |
---|
903 | |
---|
904 | ! Decalage vertical des entrainements et detrainements. |
---|
905 | masse(:, 1) = 0.5 * masse0(:, 1) |
---|
906 | entr(:, 1) = 0.5 * entr0(:, 1) |
---|
907 | detr(:, 1) = 0.5 * detr0(:, 1) |
---|
908 | fm(:, 1) = 0. |
---|
909 | DO k = 1, nlay - 1 |
---|
910 | masse(:, k + 1) = 0.5 * (masse0(:, k) + masse0(:, k + 1)) |
---|
911 | entr(:, k + 1) = 0.5 * (entr0(:, k) + entr0(:, k + 1)) |
---|
912 | detr(:, k + 1) = 0.5 * (detr0(:, k) + detr0(:, k + 1)) |
---|
913 | fm(:, k + 1) = fm(:, k) + entr(:, k) - detr(:, k) |
---|
914 | enddo |
---|
915 | fm(:, nlay + 1) = 0. |
---|
916 | |
---|
917 | q(:, :) = therm_tke_max(:, :) |
---|
918 | !!! nrlmd le 16/09/2010 |
---|
919 | DO ig = 1, ngrid |
---|
920 | qa(ig, 1) = q(ig, 1) |
---|
921 | enddo |
---|
922 | !!! |
---|
923 | |
---|
924 | IF (1==1) THEN |
---|
925 | DO k = 2, nlay |
---|
926 | DO ig = 1, ngrid |
---|
927 | IF ((fm(ig, k + 1) + detr(ig, k)) * ptimestep> & |
---|
928 | 1.e-5 * masse(ig, k)) THEN |
---|
929 | qa(ig, k) = (fm(ig, k) * qa(ig, k - 1) + entr(ig, k) * q(ig, k)) & |
---|
930 | / (fm(ig, k + 1) + detr(ig, k)) |
---|
931 | else |
---|
932 | qa(ig, k) = q(ig, k) |
---|
933 | endif |
---|
934 | IF (qa(ig, k)<0.) THEN |
---|
935 | ! PRINT*,'qa<0!!!' |
---|
936 | endif |
---|
937 | IF (q(ig, k)<0.) THEN |
---|
938 | ! PRINT*,'q<0!!!' |
---|
939 | endif |
---|
940 | enddo |
---|
941 | enddo |
---|
942 | |
---|
943 | ! Calcul du flux subsident |
---|
944 | |
---|
945 | DO k = 2, nlay |
---|
946 | DO ig = 1, ngrid |
---|
947 | wqd(ig, k) = fm(ig, k) * q(ig, k) |
---|
948 | IF (wqd(ig, k)<0.) THEN |
---|
949 | ! PRINT*,'wqd<0!!!' |
---|
950 | endif |
---|
951 | enddo |
---|
952 | enddo |
---|
953 | DO ig = 1, ngrid |
---|
954 | wqd(ig, 1) = 0. |
---|
955 | wqd(ig, nlay + 1) = 0. |
---|
956 | enddo |
---|
957 | |
---|
958 | ! Calcul des tendances |
---|
959 | DO k = 1, nlay |
---|
960 | DO ig = 1, ngrid |
---|
961 | q(ig, k) = q(ig, k) + (detr(ig, k) * qa(ig, k) - entr(ig, k) * q(ig, k) & |
---|
962 | - wqd(ig, k) + wqd(ig, k + 1)) & |
---|
963 | * ptimestep / masse(ig, k) |
---|
964 | enddo |
---|
965 | enddo |
---|
966 | |
---|
967 | endif |
---|
968 | |
---|
969 | therm_tke_max(:, :) = q(:, :) |
---|
970 | |
---|
971 | RETURN |
---|
972 | !!! fin nrlmd le 10/04/2012 |
---|
973 | end |
---|
974 | |
---|
975 | END MODULE lmdz_thermcell_main |
---|