1 | ! |
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2 | ! $Id: calltherm.F90 4089 2022-03-10 18:23:47Z emillour $ |
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3 | ! |
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4 | subroutine calltherm(dtime & |
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5 | & ,pplay,paprs,pphi,weak_inversion & |
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6 | & ,u_seri,v_seri,t_seri,q_seri,zqsat,debut & |
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7 | & ,d_u_ajs,d_v_ajs,d_t_ajs,d_q_ajs & |
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8 | & ,fm_therm,entr_therm,detr_therm,zqasc,clwcon0,lmax,ratqscth, & |
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9 | & ratqsdiff,zqsatth,ale_bl,alp_bl,lalim_conv,wght_th, & |
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10 | & zmax0,f0,zw2,fraca,ztv,zpspsk,ztla,zthl & |
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11 | !!! nrlmd le 10/04/2012 |
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12 | & ,pbl_tke,pctsrf,omega,airephy & |
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13 | & ,zlcl_th,fraca0,w0,w_conv,therm_tke_max0,env_tke_max0 & |
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14 | & ,n2,s2,ale_bl_stat & |
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15 | & ,therm_tke_max,env_tke_max & |
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16 | & ,alp_bl_det,alp_bl_fluct_m,alp_bl_fluct_tke & |
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17 | & ,alp_bl_conv,alp_bl_stat & |
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18 | !!! fin nrlmd le 10/04/2012 |
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19 | & ,zqla,ztva & |
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20 | #ifdef ISO |
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21 | & ,xt_seri,d_xt_ajs & |
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22 | #ifdef DIAGISO |
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23 | & ,q_the,xt_the & |
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24 | #endif |
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25 | #endif |
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26 | & ) |
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27 | |
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28 | USE dimphy |
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29 | USE indice_sol_mod |
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30 | USE print_control_mod, ONLY: prt_level,lunout |
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31 | #ifdef ISO |
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32 | use infotrac_phy, ONLY: ntraciso |
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33 | #ifdef ISOVERIF |
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34 | USE isotopes_mod, ONLY: iso_eau,iso_HDO |
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35 | USE isotopes_verif_mod, ONLY: iso_verif_aberrant_enc_vect2D, & |
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36 | iso_verif_egalite_vect2D |
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37 | #endif |
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38 | #endif |
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39 | |
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40 | implicit none |
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41 | include "clesphys.h" |
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42 | include "thermcell_old.h" |
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43 | |
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44 | |
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45 | !IM 140508 |
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46 | INTEGER, SAVE :: itap |
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47 | !$OMP THREADPRIVATE(itap) |
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48 | REAL dtime |
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49 | LOGICAL debut |
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50 | LOGICAL logexpr0, logexpr2(klon,klev), logexpr1(klon) |
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51 | REAL fact(klon) |
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52 | INTEGER nbptspb |
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53 | |
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54 | REAL u_seri(klon,klev),v_seri(klon,klev) |
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55 | REAL t_seri(klon,klev),q_seri(klon,klev),qmemoire(klon,klev) |
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56 | REAL weak_inversion(klon) |
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57 | REAL paprs(klon,klev+1) |
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58 | REAL pplay(klon,klev) |
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59 | REAL pphi(klon,klev) |
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60 | real zlev(klon,klev+1) |
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61 | !test: on sort lentr et a* pour alimenter KE |
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62 | REAL wght_th(klon,klev) |
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63 | INTEGER lalim_conv(klon) |
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64 | REAL zw2(klon,klev+1),fraca(klon,klev+1) |
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65 | |
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66 | !FH Update Thermiques |
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67 | REAL d_t_ajs(klon,klev), d_q_ajs(klon,klev) |
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68 | REAL d_u_ajs(klon,klev),d_v_ajs(klon,klev) |
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69 | real fm_therm(klon,klev+1) |
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70 | real entr_therm(klon,klev),detr_therm(klon,klev) |
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71 | |
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72 | !******************************************************** |
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73 | ! declarations |
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74 | LOGICAL flag_bidouille_stratocu |
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75 | real fmc_therm(klon,klev+1),zqasc(klon,klev) |
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76 | real zqla(klon,klev) |
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77 | real zqta(klon,klev) |
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78 | real ztv(klon,klev),ztva(klon,klev) |
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79 | real zpspsk(klon,klev) |
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80 | real ztla(klon,klev) |
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81 | real zthl(klon,klev) |
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82 | real wmax_sec(klon) |
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83 | real zmax_sec(klon) |
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84 | real f_sec(klon) |
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85 | real detrc_therm(klon,klev) |
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86 | ! FH WARNING : il semble que ces save ne servent a rien |
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87 | ! save fmc_therm, detrc_therm |
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88 | real clwcon0(klon,klev) |
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89 | real zqsat(klon,klev) |
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90 | real zw_sec(klon,klev+1) |
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91 | integer lmix_sec(klon) |
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92 | integer lmax(klon) |
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93 | real ratqscth(klon,klev) |
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94 | real ratqsdiff(klon,klev) |
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95 | real zqsatth(klon,klev) |
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96 | !nouvelles variables pour la convection |
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97 | real ale_bl(klon) |
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98 | real alp_bl(klon) |
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99 | real ale(klon) |
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100 | real alp(klon) |
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101 | !RC |
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102 | !on garde le zmax du pas de temps precedent |
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103 | real zmax0(klon), f0(klon) |
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104 | |
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105 | !!! nrlmd le 10/04/2012 |
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106 | real pbl_tke(klon,klev+1,nbsrf) |
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107 | real pctsrf(klon,nbsrf) |
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108 | real omega(klon,klev) |
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109 | real airephy(klon) |
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110 | real zlcl_th(klon),fraca0(klon),w0(klon),w_conv(klon) |
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111 | real therm_tke_max0(klon),env_tke_max0(klon) |
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112 | real n2(klon),s2(klon) |
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113 | real ale_bl_stat(klon) |
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114 | real therm_tke_max(klon,klev),env_tke_max(klon,klev) |
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115 | real alp_bl_det(klon),alp_bl_fluct_m(klon),alp_bl_fluct_tke(klon),alp_bl_conv(klon),alp_bl_stat(klon) |
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116 | !!! fin nrlmd le 10/04/2012 |
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117 | |
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118 | !******************************************************** |
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119 | |
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120 | real, dimension(klon) :: pcon |
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121 | real, dimension(klon,klev) :: rhobarz,wth3 |
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122 | integer,dimension(klon) :: lalim |
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123 | real, dimension(klon,klev+1) :: fm |
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124 | real, dimension(klon,klev) :: alim_star |
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125 | real, dimension(klon) :: zmax |
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126 | |
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127 | |
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128 | |
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129 | |
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130 | ! variables locales |
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131 | REAL d_t_the(klon,klev), d_q_the(klon,klev) |
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132 | REAL d_u_the(klon,klev),d_v_the(klon,klev) |
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133 | ! |
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134 | real zfm_therm(klon,klev+1),zdt |
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135 | real zentr_therm(klon,klev),zdetr_therm(klon,klev) |
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136 | ! FH A VERIFIER : SAVE INUTILES |
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137 | ! save zentr_therm,zfm_therm |
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138 | |
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139 | character (len=20) :: modname='calltherm' |
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140 | character (len=80) :: abort_message |
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141 | |
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142 | integer i,k,isplit |
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143 | logical, save :: first=.true. |
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144 | logical :: new_thermcell |
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145 | |
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146 | #ifdef ISO |
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147 | REAL xt_seri(ntraciso,klon,klev),xtmemoire(ntraciso,klon,klev) |
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148 | REAL d_xt_ajs(ntraciso,klon,klev) |
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149 | real d_xt_the(ntraciso,klon,klev) |
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150 | #ifdef DIAGISO |
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151 | real q_the(klon,klev) |
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152 | real xt_the(ntraciso,klon,klev) |
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153 | #endif |
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154 | real qprec(klon,klev) |
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155 | integer ixt |
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156 | #endif |
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157 | |
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158 | |
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159 | !$OMP THREADPRIVATE(first) |
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160 | !******************************************************** |
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161 | if (first) then |
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162 | itap=0 |
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163 | first=.false. |
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164 | endif |
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165 | |
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166 | ! Incrementer le compteur de la physique |
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167 | itap = itap + 1 |
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168 | |
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169 | ! Modele du thermique |
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170 | ! =================== |
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171 | ! print*,'thermiques: WARNING on passe t au lieu de t_seri' |
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172 | |
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173 | |
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174 | ! On prend comme valeur initiale des thermiques la valeur du pas |
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175 | ! de temps precedent |
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176 | zfm_therm(:,:)=fm_therm(:,:) |
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177 | zdetr_therm(:,:)=detr_therm(:,:) |
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178 | zentr_therm(:,:)=entr_therm(:,:) |
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179 | |
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180 | ! On reinitialise les flux de masse a zero pour le cumul en |
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181 | ! cas de splitting |
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182 | fm_therm(:,:)=0. |
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183 | entr_therm(:,:)=0. |
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184 | detr_therm(:,:)=0. |
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185 | |
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186 | ale_bl(:)=0. |
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187 | alp_bl(:)=0. |
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188 | if (prt_level.ge.10) then |
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189 | print*,'thermV4 nsplit: ',nsplit_thermals,' weak_inversion' |
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190 | endif |
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191 | |
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192 | ! tests sur les valeurs negatives de l'eau |
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193 | logexpr0=prt_level.ge.10 |
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194 | nbptspb=0 |
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195 | do k=1,klev |
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196 | do i=1,klon |
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197 | ! Attention teste abderr 19-03-09 |
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198 | ! logexpr2(i,k)=.not.q_seri(i,k).ge.0. |
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199 | logexpr2(i,k)=.not.q_seri(i,k).ge.1.e-15 |
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200 | if (logexpr2(i,k)) then |
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201 | #ifdef ISO |
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202 | qprec(i,k)=q_seri(i,k) |
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203 | #endif |
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204 | q_seri(i,k)=1.e-15 |
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205 | nbptspb=nbptspb+1 |
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206 | #ifdef ISO |
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207 | do ixt=1,ntraciso |
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208 | xt_seri(ixt,i,k)=1.e-15*(xt_seri(ixt,i,k)/qprec(i,k)) |
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209 | ! xt_seri(ixt,i,k)=1.e-15*(Rdefault(index_iso(ixt))) |
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210 | enddo |
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211 | #endif |
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212 | endif |
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213 | ! if (logexpr0) & |
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214 | ! & print*,'WARN eau<0 avant therm i=',i,' k=',k & |
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215 | ! & ,' dq,q',d_q_the(i,k),q_seri(i,k) |
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216 | enddo |
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217 | enddo |
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218 | if(nbptspb.GT.0) print*,'Number of points with q_seri(i,k)<=0 ',nbptspb |
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219 | |
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220 | |
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221 | new_thermcell=iflag_thermals>=15.and.iflag_thermals<=18 |
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222 | #ifdef ISO |
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223 | if (.not.new_thermcell) then |
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224 | CALL abort_gcm('calltherm 234','isos pas prevus ici',1) |
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225 | endif |
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226 | #ifdef ISOVERIF |
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227 | if (iso_eau.gt.0) then |
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228 | call iso_verif_egalite_vect2D( & |
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229 | & xt_seri,q_seri, & |
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230 | & 'calltherm 174',ntraciso,klon,klev) |
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231 | endif !if (iso_eau.gt.0) then |
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232 | #endif |
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233 | #endif |
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234 | zdt=dtime/REAL(nsplit_thermals) |
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235 | |
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236 | |
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237 | do isplit=1,nsplit_thermals |
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238 | |
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239 | if (iflag_thermals>=1000) then |
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240 | CALL thermcell_2002(klon,klev,zdt,iflag_thermals & |
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241 | & ,pplay,paprs,pphi & |
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242 | & ,u_seri,v_seri,t_seri,q_seri & |
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243 | & ,d_u_the,d_v_the,d_t_the,d_q_the & |
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244 | & ,zfm_therm,zentr_therm,fraca,zw2 & |
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245 | & ,r_aspect_thermals,30.,w2di_thermals & |
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246 | & ,tau_thermals) |
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247 | else if (iflag_thermals.eq.2) then |
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248 | CALL thermcell_sec(klon,klev,zdt & |
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249 | & ,pplay,paprs,pphi,zlev & |
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250 | & ,u_seri,v_seri,t_seri,q_seri & |
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251 | & ,d_u_the,d_v_the,d_t_the,d_q_the & |
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252 | & ,zfm_therm,zentr_therm & |
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253 | & ,r_aspect_thermals,30.,w2di_thermals & |
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254 | & ,tau_thermals) |
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255 | else if (iflag_thermals.eq.3) then |
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256 | CALL thermcell(klon,klev,zdt & |
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257 | & ,pplay,paprs,pphi & |
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258 | & ,u_seri,v_seri,t_seri,q_seri & |
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259 | & ,d_u_the,d_v_the,d_t_the,d_q_the & |
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260 | & ,zfm_therm,zentr_therm & |
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261 | & ,r_aspect_thermals,l_mix_thermals,w2di_thermals & |
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262 | & ,tau_thermals) |
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263 | else if (iflag_thermals.eq.10) then |
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264 | CALL thermcell_eau(klon,klev,zdt & |
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265 | & ,pplay,paprs,pphi & |
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266 | & ,u_seri,v_seri,t_seri,q_seri & |
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267 | & ,d_u_the,d_v_the,d_t_the,d_q_the & |
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268 | & ,zfm_therm,zentr_therm & |
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269 | & ,r_aspect_thermals,l_mix_thermals,w2di_thermals & |
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270 | & ,tau_thermals) |
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271 | else if (iflag_thermals.eq.11) then |
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272 | abort_message = 'cas non prevu dans calltherm' |
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273 | CALL abort_physic (modname,abort_message,1) |
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274 | else if (iflag_thermals.eq.12) then |
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275 | CALL calcul_sec(klon,klev,zdt & |
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276 | & ,pplay,paprs,pphi,zlev & |
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277 | & ,u_seri,v_seri,t_seri,q_seri & |
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278 | & ,zmax_sec,wmax_sec,zw_sec,lmix_sec & |
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279 | & ,r_aspect_thermals,l_mix_thermals,w2di_thermals & |
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280 | & ,tau_thermals) |
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281 | else if (iflag_thermals==13.or.iflag_thermals==14) then |
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282 | abort_message = 'thermcellV0_main enleve svn>2084' |
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283 | CALL abort_physic (modname,abort_message,1) |
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284 | else if (new_thermcell) then |
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285 | CALL thermcell_main(itap,klon,klev,zdt & |
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286 | & ,pplay,paprs,pphi,debut & |
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287 | & ,u_seri,v_seri,t_seri,q_seri & |
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288 | & ,d_u_the,d_v_the,d_t_the,d_q_the & |
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289 | & ,zfm_therm,zentr_therm,zdetr_therm,zqasc,zqla,lmax & |
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290 | & ,ratqscth,ratqsdiff,zqsatth & |
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291 | & ,zmax0,f0,zw2,fraca,ztv,zpspsk & |
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292 | & ,ztla,zthl,ztva & |
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293 | & ,pcon,rhobarz,wth3,wmax_sec,lalim,fm,alim_star,zmax & |
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294 | #ifdef ISO |
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295 | & ,xt_seri,d_xt_the & |
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296 | #endif |
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297 | & ) |
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298 | |
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299 | CALL thermcell_alp(klon,klev,zdt & ! in |
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300 | & ,pplay,paprs & ! in |
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301 | & ,zfm_therm,zentr_therm,lmax & ! in |
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302 | & ,pbl_tke,pctsrf,omega,airephy & ! in |
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303 | & ,zw2,fraca & ! in |
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304 | & ,pcon,rhobarz,wth3,wmax_sec,lalim,fm,alim_star,zmax & ! in |
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305 | & ,ale,alp,lalim_conv,wght_th & ! out |
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306 | & ,zlcl_th,fraca0,w0,w_conv,therm_tke_max0,env_tke_max0 &! out |
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307 | & ,n2,s2,ale_bl_stat & ! out |
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308 | & ,therm_tke_max,env_tke_max & ! out |
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309 | & ,alp_bl_det,alp_bl_fluct_m,alp_bl_fluct_tke & ! out |
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310 | & ,alp_bl_conv,alp_bl_stat & ! out |
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311 | & ) |
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312 | |
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313 | if (prt_level.gt.10) write(lunout,*)'Apres thermcell_main OK' |
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314 | else |
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315 | abort_message = 'Cas des thermiques non prevu' |
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316 | CALL abort_physic (modname,abort_message,1) |
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317 | endif |
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318 | |
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319 | ! Attention : les noms sont contre intuitif. |
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320 | ! flag_bidouille_stratocu est .true. si on ne fait pas de bidouille. |
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321 | ! Il aurait mieux valu avoir un nobidouille_stratocu |
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322 | ! Et pour simplifier : |
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323 | ! nobidouille_stratocu=.not.(iflag_thermals==13.or.iflag_thermals=15) |
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324 | ! Ce serait bien de changer, mai en prenant le temps de vérifier que ca |
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325 | ! fait bien ce qu'on croit. |
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326 | |
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327 | flag_bidouille_stratocu=iflag_thermals<=12.or.iflag_thermals==14.or.iflag_thermals==16.or.iflag_thermals==18 |
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328 | |
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329 | ! Calcul a posteriori du niveau max des thermiques pour les schémas qui |
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330 | ! ne la sortent pas. |
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331 | if (iflag_thermals<=12.or.iflag_thermals>=1000) then |
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332 | lmax(:)=1 |
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333 | do k=1,klev-1 |
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334 | zdetr_therm(:,k)=zentr_therm(:,k)+zfm_therm(:,k)-zfm_therm(:,k+1) |
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335 | enddo |
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336 | do k=1,klev-1 |
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337 | do i=1,klon |
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338 | if (zfm_therm(i,k+1)>0.) lmax(i)=k |
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339 | enddo |
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340 | enddo |
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341 | endif |
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342 | |
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343 | fact(:)=0. |
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344 | DO i=1,klon |
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345 | logexpr1(i)=flag_bidouille_stratocu.or.weak_inversion(i).gt.0.5 |
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346 | IF(logexpr1(i)) fact(i)=1./REAL(nsplit_thermals) |
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347 | ENDDO |
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348 | |
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349 | DO k=1,klev |
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350 | ! transformation de la derivee en tendance |
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351 | d_t_the(:,k)=d_t_the(:,k)*dtime*fact(:) |
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352 | d_u_the(:,k)=d_u_the(:,k)*dtime*fact(:) |
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353 | d_v_the(:,k)=d_v_the(:,k)*dtime*fact(:) |
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354 | d_q_the(:,k)=d_q_the(:,k)*dtime*fact(:) |
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355 | fm_therm(:,k)=fm_therm(:,k) & |
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356 | & +zfm_therm(:,k)*fact(:) |
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357 | entr_therm(:,k)=entr_therm(:,k) & |
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358 | & +zentr_therm(:,k)*fact(:) |
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359 | detr_therm(:,k)=detr_therm(:,k) & |
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360 | & +zdetr_therm(:,k)*fact(:) |
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361 | #ifdef ISO |
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362 | do ixt=1,ntraciso |
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363 | d_xt_the(ixt,:,k)=d_xt_the(ixt,:,k)*dtime*fact(:) |
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364 | enddo |
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365 | #endif |
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366 | ENDDO |
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367 | fm_therm(:,klev+1)=0. |
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368 | |
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369 | |
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370 | |
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371 | ! accumulation de la tendance |
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372 | d_t_ajs(:,:)=d_t_ajs(:,:)+d_t_the(:,:) |
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373 | d_u_ajs(:,:)=d_u_ajs(:,:)+d_u_the(:,:) |
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374 | d_v_ajs(:,:)=d_v_ajs(:,:)+d_v_the(:,:) |
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375 | d_q_ajs(:,:)=d_q_ajs(:,:)+d_q_the(:,:) |
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376 | #ifdef ISO |
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377 | d_xt_ajs(:,:,:)=d_xt_ajs(:,:,:)+d_xt_the(:,:,:) |
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378 | #endif |
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379 | |
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380 | ! incrementation des variables meteo |
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381 | t_seri(:,:) = t_seri(:,:) + d_t_the(:,:) |
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382 | u_seri(:,:) = u_seri(:,:) + d_u_the(:,:) |
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383 | v_seri(:,:) = v_seri(:,:) + d_v_the(:,:) |
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384 | qmemoire(:,:)=q_seri(:,:) |
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385 | q_seri(:,:) = q_seri(:,:) + d_q_the(:,:) |
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386 | #ifdef ISO |
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387 | xtmemoire(:,:,:)=xt_seri(:,:,:) |
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388 | xt_seri(:,:,:) = xt_seri(:,:,:) + d_xt_the(:,:,:) |
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389 | #ifdef ISOVERIF |
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390 | ! write(*,*) 'calltherm 350 tmp: ajout d_xt_the' |
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391 | if (iso_HDO.gt.0) then |
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392 | ! i=479 |
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393 | ! k=4 |
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394 | ! write(*,*) 'xt_seri(iso_hdo,i,k),q_seri(i,k)=', & |
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395 | ! & xt_seri(iso_hdo,i,k),q_seri(i,k) |
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396 | ! write(*,*) 'd_xt_the(iso_hdo,i,k),d_q_the(i,k)=', & |
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397 | ! & d_xt_the(iso_hdo,i,k),d_q_the(i,k) |
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398 | call iso_verif_aberrant_enc_vect2D( & |
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399 | & xt_seri,q_seri, & |
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400 | & 'calltherm 353, apres ajout d_xt_the',ntraciso,klon,klev) |
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401 | endif |
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402 | #endif |
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403 | #endif |
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404 | if (prt_level.gt.10) write(lunout,*)'Apres apres thermcell_main OK' |
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405 | |
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406 | DO i=1,klon |
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407 | fm_therm(i,klev+1)=0. |
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408 | ale_bl(i)=ale_bl(i)+ale(i)/REAL(nsplit_thermals) |
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409 | ! write(22,*)'ALE CALLTHERM',ale_bl(i),ale(i) |
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410 | alp_bl(i)=alp_bl(i)+alp(i)/REAL(nsplit_thermals) |
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411 | ! write(23,*)'ALP CALLTHERM',alp_bl(i),alp(i) |
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412 | if(prt_level.GE.10) print*,'calltherm i alp_bl alp ale_bl ale',i,alp_bl(i),alp(i),ale_bl(i),ale(i) |
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413 | ENDDO |
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414 | |
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415 | !IM 060508 marche pas comme cela !!! enddo ! isplit |
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416 | |
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417 | ! tests sur les valeurs negatives de l'eau |
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418 | nbptspb=0 |
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419 | DO k = 1, klev |
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420 | DO i = 1, klon |
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421 | logexpr2(i,k)=.not.q_seri(i,k).ge.0. |
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422 | if (logexpr2(i,k)) then |
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423 | q_seri(i,k)=1.e-15 |
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424 | nbptspb=nbptspb+1 |
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425 | #ifdef ISO |
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426 | do ixt=1,ntraciso |
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427 | xt_seri(ixt,i,k)=1.e-15*(xtmemoire(ixt,i,k)/qmemoire(i,k)) |
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428 | enddo |
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429 | #endif |
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430 | ! if (prt_level.ge.10) then |
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431 | ! print*,'WARN eau<0 apres therm i=',i,' k=',k & |
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432 | ! & ,' dq,q',d_q_the(i,k),q_seri(i,k), & |
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433 | ! & 'fm=',zfm_therm(i,k),'entr=',entr_therm(i,k) |
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434 | endif |
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435 | ENDDO |
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436 | ENDDO |
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437 | #ifdef ISO |
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438 | #ifdef ISOVERIF |
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439 | if (iso_HDO.gt.0) then |
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440 | call iso_verif_aberrant_enc_vect2D( & |
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441 | & xt_seri,q_seri, & |
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442 | & 'calltherm 393, apres bidouille q<0',ntraciso,klon,klev) |
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443 | endif |
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444 | #endif |
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445 | #endif |
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446 | |
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447 | IF(nbptspb.GT.0) print*,'Number of points with q_seri(i,k)<=0 ',nbptspb |
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448 | ! tests sur les valeurs de la temperature |
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449 | nbptspb=0 |
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450 | DO k = 1, klev |
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451 | DO i = 1, klon |
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452 | logexpr2(i,k)=t_seri(i,k).lt.50..or.t_seri(i,k).gt.370. |
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453 | if (logexpr2(i,k)) nbptspb=nbptspb+1 |
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454 | ! if ((t_seri(i,k).lt.50.) .or. & |
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455 | ! & (t_seri(i,k).gt.370.)) then |
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456 | ! print*,'WARN temp apres therm i=',i,' k=',k & |
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457 | ! & ,' t_seri',t_seri(i,k) |
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458 | ! CALL abort |
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459 | ! endif |
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460 | ENDDO |
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461 | ENDDO |
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462 | IF(nbptspb.GT.0) print*,'Number of points with q_seri(i,k)<=0 ',nbptspb |
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463 | enddo ! isplit |
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464 | |
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465 | ! |
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466 | !*************************************************************** |
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467 | ! calcul du flux ascencant conservatif |
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468 | ! print*,'<<<<calcul flux ascendant conservatif' |
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469 | |
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470 | fmc_therm=0. |
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471 | do k=1,klev |
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472 | do i=1,klon |
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473 | if (entr_therm(i,k).gt.0.) then |
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474 | fmc_therm(i,k+1)=fmc_therm(i,k)+entr_therm(i,k) |
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475 | else |
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476 | fmc_therm(i,k+1)=fmc_therm(i,k) |
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477 | endif |
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478 | detrc_therm(i,k)=(fmc_therm(i,k+1)-fm_therm(i,k+1)) & |
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479 | & -(fmc_therm(i,k)-fm_therm(i,k)) |
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480 | enddo |
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481 | enddo |
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482 | |
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483 | |
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484 | !**************************************************************** |
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485 | ! calcul de l'humidite dans l'ascendance |
---|
486 | ! print*,'<<<<calcul de lhumidite dans thermique' |
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487 | !CR:on ne le calcule que pour le cas sec |
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488 | if (iflag_thermals.le.11) then |
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489 | do i=1,klon |
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490 | zqasc(i,1)=q_seri(i,1) |
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491 | do k=2,klev |
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492 | if (fmc_therm(i,k+1).gt.1.e-6) then |
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493 | zqasc(i,k)=(fmc_therm(i,k)*zqasc(i,k-1) & |
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494 | & +entr_therm(i,k)*q_seri(i,k))/fmc_therm(i,k+1) |
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495 | !CR:test on asseche le thermique |
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496 | ! zqasc(i,k)=zqasc(i,k)/2. |
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497 | ! else |
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498 | ! zqasc(i,k)=q_seri(i,k) |
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499 | endif |
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500 | enddo |
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501 | enddo |
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502 | |
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503 | |
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504 | ! calcul de l'eau condensee dans l'ascendance |
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505 | ! print*,'<<<<calcul de leau condensee dans thermique' |
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506 | do i=1,klon |
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507 | do k=1,klev |
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508 | clwcon0(i,k)=zqasc(i,k)-zqsat(i,k) |
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509 | if (clwcon0(i,k).lt.0. .or. & |
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510 | & (fm_therm(i,k+1)+detrc_therm(i,k)).lt.1.e-6) then |
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511 | clwcon0(i,k)=0. |
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512 | endif |
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513 | enddo |
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514 | enddo |
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515 | else |
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516 | do i=1,klon |
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517 | do k=1,klev |
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518 | clwcon0(i,k)=zqla(i,k) |
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519 | if (clwcon0(i,k).lt.0. .or. & |
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520 | & (fm_therm(i,k+1)+detrc_therm(i,k)).lt.1.e-6) then |
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521 | clwcon0(i,k)=0. |
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522 | endif |
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523 | enddo |
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524 | enddo |
---|
525 | endif |
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526 | !******************************************************************* |
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527 | |
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528 | |
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529 | !jyg Protection contre les temperatures nulles |
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530 | do i=1,klon |
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531 | do k=1,klev |
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532 | if (ztla(i,k) .lt. 1.e-10) fraca(i,k) =0. |
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533 | enddo |
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534 | enddo |
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535 | |
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536 | |
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537 | return |
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538 | |
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539 | end |
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