1 | subroutine condense_n2(klon,klev,nq,ptimestep, & |
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2 | pcapcal,pplay,pplev,ptsrf,pt, & |
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3 | pphi,pdt,pdu,pdv,pdtsrf,pu,pv,pq,pdq, & |
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4 | picen2,psolaralb,pemisurf, & |
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5 | pdtc,pdtsrfc,pdpsrf,pduc,pdvc, & |
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6 | pdqc,pdicen2) |
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7 | |
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8 | use radinc_h, only : naerkind |
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9 | use comgeomfi_h |
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10 | use comcstfi_mod, only: g, r, cpp, pi |
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11 | USE surfdat_h, only: phisfi,kp,p00 |
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12 | USE tracer_h, only: noms, igcm_n2, lw_n2 |
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13 | USE callkeys_mod, only: fast,ch4lag,latlag,nbsub,no_n2frost,tsurfmax,kmixmin,source_haze,vmrlag |
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14 | USE comvert_mod, ONLY: ap,bp |
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15 | use geometry_mod, only: latitude |
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16 | |
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17 | |
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18 | implicit none |
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19 | |
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20 | !================================================================== |
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21 | ! Purpose |
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22 | ! ------- |
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23 | ! Condense and/or sublime N2 ice on the ground and in the |
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24 | ! atmosphere, and sediment the ice. |
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25 | ! |
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26 | ! Inputs |
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27 | ! ------ |
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28 | ! klon Number of vertical columns |
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29 | ! klev Number of layers |
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30 | ! pplay(klon,klev) Pressure layers |
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31 | ! pplev(klon,klev+1) Pressure levels |
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32 | ! pt(klon,klev) Temperature (in K) |
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33 | ! ptsrf(klon) Surface temperature |
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34 | ! |
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35 | ! pdt(klon,klev) Time derivative before condensation/sublimation of pt |
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36 | ! pdtsrf(klon) Time derivative before condensation/sublimation of ptsrf |
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37 | ! picen2(klon) n2 ice at the surface (kg/m2) |
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38 | ! |
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39 | ! Outputs |
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40 | ! ------- |
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41 | ! pdpsrf(klon) \ Contribution of condensation/sublimation |
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42 | ! pdtc(klon,klev) / to the time derivatives of Ps, pt, and ptsrf |
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43 | ! pdtsrfc(klon) / |
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44 | ! pdicen2(klon) Tendancy n2 ice at the surface (kg/m2) |
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45 | ! |
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46 | ! Both |
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47 | ! ---- |
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48 | ! psolaralb(klon) Albedo at the surface |
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49 | ! pemisurf(klon) Emissivity of the surface |
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50 | ! |
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51 | ! Authors |
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52 | ! ------- |
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53 | ! Francois Forget (1996,2013) |
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54 | ! Converted to Fortran 90 and slightly modified by R. Wordsworth (2009) |
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55 | ! |
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56 | ! |
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57 | !================================================================== |
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58 | |
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59 | !----------------------------------------------------------------------- |
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60 | ! Arguments |
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61 | |
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62 | INTEGER klon, klev, nq |
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63 | |
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64 | REAL ptimestep |
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65 | REAL pplay(klon,klev),pplev(klon,klev+1) |
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66 | REAL pcapcal(klon) |
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67 | REAL pt(klon,klev) |
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68 | REAL ptsrf(klon),flu1(klon),flu2(klon),flu3(klon) |
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69 | REAL pphi(klon,klev) |
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70 | REAL pdt(klon,klev),pdtsrf(klon),pdtc(klon,klev) |
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71 | REAL pdtsrfc(klon),pdpsrf(klon) |
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72 | REAL picen2(klon),psolaralb(klon),pemisurf(klon) |
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73 | |
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74 | |
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75 | REAL pu(klon,klev) , pv(klon,klev) |
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76 | REAL pdu(klon,klev) , pdv(klon,klev) |
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77 | REAL pduc(klon,klev) , pdvc(klon,klev) |
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78 | REAL pq(klon,klev,nq),pdq(klon,klev,nq) |
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79 | REAL pdqc(klon,klev,nq) |
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80 | |
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81 | !----------------------------------------------------------------------- |
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82 | ! Local variables |
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83 | |
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84 | INTEGER l,ig,ilay,it,iq,ich4_gas |
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85 | |
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86 | REAL*8 zt(klon,klev) |
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87 | REAL tcond_n2 |
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88 | REAL pcond_n2 |
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89 | REAL glob_average2d ! function |
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90 | REAL zqn2(klon,klev) ! N2 MMR used to compute Tcond/zqn2 |
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91 | REAL ztcond (klon,klev) |
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92 | REAL ztcondsol(klon),zfallheat |
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93 | REAL pdicen2(klon) |
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94 | REAL zcondicea(klon,klev), zcondices(klon) |
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95 | REAL zfallice(klon,klev+1) |
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96 | REAL zmflux(klev+1) |
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97 | REAL zu(klev),zv(klev) |
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98 | REAL zq(klev,nq),zq1(klev) |
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99 | REAL ztsrf(klon) |
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100 | REAL ztc(klev), ztm(klev+1) |
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101 | REAL zum(klev+1) , zvm(klev+1) |
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102 | REAL zqm(klev+1,nq),zqm1(klev+1) |
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103 | LOGICAL condsub(klon) |
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104 | REAL subptimestep |
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105 | Integer Ntime |
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106 | real masse (klev),w(klev+1) |
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107 | real wq(klon,klev+1) |
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108 | real vstokes,reff |
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109 | real dWtotsn2 |
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110 | real condnconsn2(klon) |
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111 | real nconsMAXn2 |
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112 | ! Special diagnostic variables |
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113 | real tconda1(klon,klev) |
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114 | real tconda2(klon,klev) |
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115 | real zdtsig (klon,klev) |
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116 | real zdtlatent (klon,klev) |
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117 | real zdt (klon,klev) |
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118 | REAL albediceF(klon) |
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119 | ! SAVE albediceF |
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120 | INTEGER nsubtimestep,itsub !number of subtimestep when calling vl1d |
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121 | REAL subtimestep !ptimestep/nsubtimestep |
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122 | REAL dtmax |
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123 | |
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124 | REAL zplevhist(klon) |
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125 | REAL zplevnew(klon) |
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126 | REAL zplev(klon) |
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127 | REAL zpicen2(klon) |
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128 | REAL ztsrfhist(klon) |
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129 | REAL zdtsrf(klon) |
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130 | REAL globzplevnew |
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131 | |
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132 | ! REAL vmrn2(klon) |
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133 | ! SAVE vmrn2 |
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134 | REAL stephan |
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135 | DATA stephan/5.67e-08/ ! Stephan Boltzman constant |
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136 | SAVE stephan |
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137 | !----------------------------------------------------------------------- |
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138 | ! Saved local variables |
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139 | |
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140 | ! REAL latcond |
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141 | REAL ccond |
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142 | REAL cpice ! for atm condensation |
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143 | SAVE cpice |
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144 | ! SAVE latcond,ccond |
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145 | SAVE ccond |
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146 | |
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147 | LOGICAL firstcall |
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148 | SAVE firstcall |
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149 | REAL SSUM |
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150 | EXTERNAL SSUM |
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151 | |
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152 | ! DATA latcond /2.5e5/ |
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153 | ! DATA latcond /1.98e5/ |
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154 | DATA cpice /1300./ |
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155 | DATA firstcall/.true./ |
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156 | |
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157 | INTEGER,SAVE :: i_n2ice=0 ! n2 ice |
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158 | CHARACTER(LEN=20) :: tracername ! to temporarily store text |
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159 | logical olkin ! option to prevent N2 ice effect in the south |
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160 | DATA olkin/.false./ |
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161 | save olkin |
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162 | |
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163 | CHARACTER(len=10) :: tname |
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164 | |
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165 | !----------------------------------------------------------------------- |
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166 | |
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167 | ! Initialisation |
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168 | IF (firstcall) THEN |
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169 | ccond=cpp/(g*lw_n2) |
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170 | print*,'In condense_n2cloud: ccond=',ccond,' latcond=',lw_n2 |
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171 | |
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172 | ! calculate global mean surface pressure for the fast mode |
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173 | IF (fast) THEN |
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174 | IF (.not. ALLOCATED(kp)) ALLOCATE(kp(klon)) |
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175 | DO ig=1,klon |
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176 | kp(ig) = exp(-phisfi(ig)/(r*38.)) |
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177 | ENDDO |
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178 | p00=glob_average2d(kp) ! mean pres at ref level |
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179 | ENDIF |
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180 | |
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181 | !vmrn2(:) = 1. |
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182 | !IF (ch4lag) then |
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183 | ! DO ig=1,klon |
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184 | ! if (latitude(ig)*180./pi.ge.latlag) then |
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185 | ! vmrn2(ig) = vmrlag |
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186 | ! endif |
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187 | ! ENDDO |
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188 | !ENDIF |
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189 | !IF (no_n2frost) then |
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190 | ! DO ig=1,klon |
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191 | ! if (picen2(ig).eq.0.) then |
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192 | ! vmrn2(ig) = 1.e-15 |
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193 | ! endif |
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194 | ! ENDDO |
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195 | !ENDIF |
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196 | firstcall=.false. |
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197 | ENDIF |
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198 | |
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199 | !----------------------------------------------------------------------- |
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200 | ! Calculation of n2 condensation / sublimation |
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201 | |
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202 | ! Variables used: |
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203 | ! picen2(klon) : amount of n2 ice on the ground (kg/m2) |
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204 | ! zcondicea(klon,klev): condensation rate in layer l (kg/m2/s) |
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205 | ! zcondices(klon) : condensation rate on the ground (kg/m2/s) |
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206 | ! zfallice(klon,klev) : amount of ice falling from layer l (kg/m2/s) |
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207 | ! zdtlatent(klon,klev): dT/dt due to phase changes (K/s) |
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208 | |
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209 | ! Tendencies initially set to 0 |
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210 | zcondices(1:klon) = 0. |
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211 | pdtsrfc(1:klon) = 0. |
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212 | pdpsrf(1:klon) = 0. |
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213 | ztsrfhist(1:klon) = 0. |
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214 | condsub(1:klon) = .false. |
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215 | pdicen2(1:klon) = 0. |
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216 | zfallheat=0 |
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217 | pdqc(1:klon,1:klev,1:nq)=0 |
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218 | pdtc(1:klon,1:klev)=0 |
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219 | pduc(1:klon,1:klev)=0 |
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220 | pdvc(1:klon,1:klev)=0 |
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221 | zfallice(1:klon,1:klev+1)=0 |
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222 | zcondicea(1:klon,1:klev)=0 |
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223 | zdtlatent(1:klon,1:klev)=0 |
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224 | zt(1:klon,1:klev)=0. |
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225 | |
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226 | !----------------------------------------------------------------------- |
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227 | ! Atmospheric condensation |
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228 | |
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229 | ! Condensation / sublimation in the atmosphere |
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230 | ! -------------------------------------------- |
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231 | ! (calcul of zcondicea , zfallice and pdtc) |
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232 | |
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233 | zt(1:klon,1:klev)=pt(1:klon,1:klev)+ pdt(1:klon,1:klev)*ptimestep |
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234 | if (igcm_n2.ne.0) then |
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235 | zqn2(1:klon,1:klev) = 1. ! & temporaire |
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236 | ! zqn2(1:klon,1:klev)= pq(1:klon,1:klev,igcm_n2) + pdq(1:klon,1:klev,igcm_n2)*ptimestep |
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237 | else |
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238 | zqn2(1:klon,1:klev) = 1. |
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239 | end if |
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240 | |
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241 | if (.not.fast) then |
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242 | ! Forecast the atmospheric frost temperature 'ztcond' with function tcond_n2 |
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243 | DO l=1,klev |
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244 | DO ig=1,klon |
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245 | ztcond (ig,l) = tcond_n2(pplay(ig,l),zqn2(ig,l)) |
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246 | ENDDO |
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247 | ENDDO |
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248 | |
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249 | DO l=klev,1,-1 |
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250 | DO ig=1,klon |
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251 | pdtc(ig,l)=0. ! final tendancy temperature set to 0 |
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252 | |
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253 | IF((zt(ig,l).LT.ztcond(ig,l)).or.(zfallice(ig,l+1).gt.0))THEN |
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254 | condsub(ig)=.true. !condensation at level l |
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255 | IF (zfallice(ig,l+1).gt.0) then |
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256 | zfallheat=zfallice(ig,l+1)*& |
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257 | (pphi(ig,l+1)-pphi(ig,l) +& |
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258 | cpice*(ztcond(ig,l+1)-ztcond(ig,l)))/lw_n2 |
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259 | ELSE |
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260 | zfallheat=0. |
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261 | ENDIF |
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262 | zdtlatent(ig,l)=(ztcond(ig,l) - zt(ig,l))/ptimestep |
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263 | zcondicea(ig,l)=(pplev(ig,l)-pplev(ig,l+1))& |
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264 | *ccond*zdtlatent(ig,l)- zfallheat |
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265 | ! Case when the ice from above sublimes entirely |
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266 | ! """"""""""""""""""""""""""""""""""""""""""""""" |
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267 | IF ((zfallice(ig,l+1).lt.-zcondicea(ig,l)) & |
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268 | .AND. (zfallice(ig,l+1).gt.0)) THEN |
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269 | |
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270 | zdtlatent(ig,l)=(-zfallice(ig,l+1)+zfallheat)/& |
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271 | (ccond*(pplev(ig,l)-pplev(ig,l+1))) |
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272 | zcondicea(ig,l)= -zfallice(ig,l+1) |
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273 | END IF |
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274 | |
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275 | zfallice(ig,l) = zcondicea(ig,l)+zfallice(ig,l+1) |
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276 | |
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277 | END IF |
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278 | |
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279 | ENDDO |
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280 | ENDDO |
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281 | endif ! not fast |
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282 | |
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283 | !----------------------------------------------------------------------- |
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284 | ! Condensation/sublimation on the ground |
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285 | ! (calculation of zcondices and pdtsrfc) |
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286 | |
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287 | ! Adding subtimesteps : in fast version, pressures too low lead to |
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288 | ! instabilities. |
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289 | IF (fast) THEN |
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290 | IF (pplev(1,1).gt.0.3) THEN |
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291 | nsubtimestep= 1 |
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292 | ELSE |
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293 | nsubtimestep= nbsub !max(nint(ptimestep/dtmax),1) |
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294 | ENDIF |
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295 | ELSE |
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296 | nsubtimestep= 1 ! if more then kp and p00 have to be calculated |
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297 | ! for nofast mode |
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298 | ENDIF |
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299 | subtimestep=ptimestep/float(nsubtimestep) |
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300 | |
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301 | do itsub=1,nsubtimestep |
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302 | ! first loop : getting zplev, ztsurf |
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303 | IF (itsub.eq.1) then |
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304 | DO ig=1,klon |
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305 | zplev(ig)=pplev(ig,1) |
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306 | ztsrfhist(ig)=ptsrf(ig) + pdtsrf(ig)*ptimestep |
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307 | ztsrf(ig)=ptsrf(ig) + pdtsrf(ig)*subtimestep !! |
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308 | zpicen2(ig)=picen2(ig) |
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309 | ENDDO |
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310 | ELSE |
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311 | ! additional loop : |
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312 | ! 1) pressure updated |
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313 | ! 2) direct redistribution of pressure over the globe |
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314 | ! 3) modification pressure for unstable cases |
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315 | ! 4) pressure update to conserve mass |
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316 | ! 5) temperature updated with radiative tendancies |
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317 | DO ig=1,klon |
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318 | zplevhist(ig)=zplev(ig) |
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319 | zplevnew(ig)=zplev(ig)+pdpsrf(ig)*subtimestep ! 1) |
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320 | !IF (zplevnew(ig).le.0.0001) then |
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321 | ! zplevnew(ig)=0.0001*kp(ig)/p00 |
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322 | !ENDIF |
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323 | ENDDO |
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324 | ! intermediaire de calcul: valeur moyenne de zplevnew (called twice in the code) |
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325 | globzplevnew=glob_average2d(zplevnew) |
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326 | DO ig=1,klon |
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327 | zplev(ig)=kp(ig)*globzplevnew/p00 ! 2) |
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328 | ENDDO |
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329 | DO ig=1,klon ! 3) unstable case condensation and sublimation: zplev=zplevhist |
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330 | IF (((pdpsrf(ig).lt.0.).and.(tcond_n2(zplev(ig),zqn2(ig,1)).le.ztsrf(ig))).or. & |
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331 | ((pdpsrf(ig).gt.0.).and.(tcond_n2(zplev(ig),zqn2(ig,1)).ge.ztsrf(ig)))) then |
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332 | zplev(ig)=zplevhist(ig) |
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333 | ENDIF |
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334 | zplevhist(ig)=zplev(ig) |
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335 | ENDDO |
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336 | zplev=zplev*globzplevnew/glob_average2d(zplevhist) ! 4) |
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337 | DO ig=1,klon ! 5) |
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338 | zdtsrf(ig)=pdtsrf(ig) + (stephan/pcapcal(ig))*(ptsrf(ig)**4-ztsrf(ig)**4) |
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339 | ztsrf(ig)=ztsrf(ig)+pdtsrfc(ig)*subtimestep+zdtsrf(ig)*subtimestep |
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340 | zpicen2(ig)=zpicen2(ig)+pdicen2(ig)*subtimestep |
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341 | ENDDO |
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342 | ENDIF ! (itsub=1) |
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343 | |
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344 | DO ig=1,klon |
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345 | ! forecast of frost temperature ztcondsol |
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346 | ztcondsol(ig) = tcond_n2(zplev(ig),zqn2(ig,1)) |
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347 | !ztcondsol(ig) = tcond_n2(zplev(ig),vmrn2(ig)) |
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348 | |
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349 | ! Loop over where we have condensation / sublimation |
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350 | IF ((ztsrf(ig) .LT. ztcondsol(ig)) .OR. & ! ground cond |
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351 | ((ztsrf(ig) .GT. ztcondsol(ig)) .AND. & ! ground sublim |
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352 | (zpicen2(ig) .GT. 0.))) THEN |
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353 | condsub(ig) = .true. ! condensation or sublimation |
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354 | |
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355 | ! Condensation or partial sublimation of N2 ice |
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356 | if (ztsrf(ig) .LT. ztcondsol(ig)) then ! condensation |
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357 | ! Include a correction to account for the cooling of air near |
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358 | ! the surface before condensing: |
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359 | zcondices(ig)=pcapcal(ig)*(ztcondsol(ig)-ztsrf(ig)) & |
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360 | /((lw_n2+cpp*(zt(ig,1)-ztcondsol(ig)))*subtimestep) |
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361 | else ! sublimation |
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362 | zcondices(ig)=pcapcal(ig)*(ztcondsol(ig)-ztsrf(ig)) & |
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363 | /(lw_n2*subtimestep) |
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364 | end if |
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365 | |
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366 | pdtsrfc(ig) = (ztcondsol(ig) - ztsrf(ig))/subtimestep |
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367 | |
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368 | ! partial sublimation of N2 ice |
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369 | ! If the entire N_2 ice layer sublimes |
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370 | ! (including what has just condensed in the atmosphere) |
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371 | IF((zpicen2(ig)/subtimestep).LE. & |
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372 | -zcondices(ig))THEN |
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373 | zcondices(ig) = -zpicen2(ig)/subtimestep |
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374 | pdtsrfc(ig)=(lw_n2/pcapcal(ig))* & |
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375 | (zcondices(ig)) |
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376 | END IF |
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377 | |
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378 | ! Changing N2 ice amount and pressure |
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379 | |
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380 | pdicen2(ig) = zcondices(ig) |
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381 | pdpsrf(ig) = -pdicen2(ig)*g |
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382 | ! pdpsrf(ig) = 0. ! OPTION to check impact N2 sub/cond |
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383 | IF (zplev(ig)+pdpsrf(ig)*subtimestep.le.0.0000001) then |
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384 | pdpsrf(ig)=(0.0000001*kp(ig)/p00-zplev(ig))/subtimestep |
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385 | pdicen2(ig)=-pdpsrf(ig)/g |
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386 | ENDIF |
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387 | |
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388 | ELSE ! no condsub |
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389 | pdpsrf(ig)=0. |
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390 | pdicen2(ig)=0. |
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391 | pdtsrfc(ig)=0. |
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392 | ENDIF |
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393 | ENDDO ! ig |
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394 | enddo ! subtimestep |
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395 | |
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396 | ! Updating pressure, temperature and ice reservoir |
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397 | DO ig=1,klon |
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398 | pdpsrf(ig)=(zplev(ig)+pdpsrf(ig)*subtimestep-pplev(ig,1))/ptimestep |
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399 | ! Two options here : 1 ok, 2 is wrong |
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400 | pdicen2(ig)=(zpicen2(ig)+pdicen2(ig)*subtimestep-picen2(ig))/ptimestep |
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401 | !pdicen2(ig)=-pdpsrf(ig)/g |
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402 | |
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403 | pdtsrfc(ig)=((ztsrf(ig)+pdtsrfc(ig)*subtimestep)-(ztsrfhist(ig)))/ptimestep |
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404 | |
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405 | ! security |
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406 | if (picen2(ig) + pdicen2(ig)*ptimestep.lt.0.) then |
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407 | write(*,*) 'WARNING in condense_n2:' |
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408 | write(*,*) picen2(ig),pdicen2(ig)*ptimestep |
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409 | pdicen2(ig)= -picen2(ig)/ptimestep |
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410 | pdpsrf(ig)=-pdicen2(ig)*g |
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411 | endif |
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412 | |
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413 | if(.not.picen2(ig).ge.0.) THEN |
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414 | ! if(picen2(ig) + pdicen2(ig)*ptimestep.le.-1.e-8) then |
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415 | print*, 'WARNING NEG RESERVOIR in condense_n2: picen2(',ig,')=', picen2(ig) + pdicen2(ig)*ptimestep |
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416 | ! pdicen2(ig)= -picen2(ig)/ptimestep |
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417 | ! else |
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418 | picen2(ig)=0.0 |
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419 | ! endif |
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420 | endif |
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421 | ENDDO |
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422 | |
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423 | ! *************************************************************** |
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424 | ! Correction to account for redistribution between sigma or hybrid |
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425 | ! layers when changing surface pressure (and warming/cooling |
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426 | ! of the n2 currently changing phase). |
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427 | ! ************************************************************* |
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428 | if (.not.fast) then |
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429 | DO ig=1,klon |
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430 | if (condsub(ig)) then |
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431 | |
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432 | ! Mass fluxes through the sigma levels (kg.m-2.s-1) (>0 when up) |
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433 | ! """""""""""""""""""""""""""""""""""""""""""""""""""""""""""""" |
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434 | zmflux(1) = -zcondices(ig) |
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435 | DO l=1,klev |
---|
436 | zmflux(l+1) = zmflux(l) -zcondicea(ig,l) & |
---|
437 | + (bp(l)-bp(l+1))*(zfallice(ig,1)-zmflux(1)) |
---|
438 | ! zmflux set to 0 if very low to avoid: top layer is disappearing in v1ld |
---|
439 | if (abs(zmflux(l+1)).lt.1E-13.OR.bp(l+1).eq.0.) zmflux(l+1)=0. |
---|
440 | END DO |
---|
441 | |
---|
442 | ! Mass of each layer |
---|
443 | ! ------------------ |
---|
444 | DO l=1,klev |
---|
445 | masse(l)=(pplev(ig,l) - pplev(ig,l+1))/g |
---|
446 | END DO |
---|
447 | |
---|
448 | |
---|
449 | ! Corresponding fluxes for T,U,V,Q |
---|
450 | ! """""""""""""""""""""""""""""""" |
---|
451 | ! averaging operator for TRANSPORT |
---|
452 | ! """""""""""""""""""""""""""""""" |
---|
453 | |
---|
454 | ! Subtimestep loop to perform the redistribution gently and simultaneously with |
---|
455 | ! the other tendencies |
---|
456 | ! Estimation of subtimestep (using only the first layer, the most critical) |
---|
457 | dtmax=ptimestep |
---|
458 | if (zmflux(1).gt.1.e-20) then |
---|
459 | dtmax=min(dtmax,masse(1)*zqn2(ig,1)/abs(zmflux(1))) |
---|
460 | endif |
---|
461 | nsubtimestep= max(nint(ptimestep/dtmax),nint(2.)) |
---|
462 | subtimestep=ptimestep/float(nsubtimestep) |
---|
463 | |
---|
464 | ! New flux for each subtimestep |
---|
465 | do l=1,klev+1 |
---|
466 | w(l)=-zmflux(l)*subtimestep |
---|
467 | enddo |
---|
468 | ! initializing variables that will vary during subtimestep: |
---|
469 | do l=1,klev |
---|
470 | ztc(l) =pt(ig,l) |
---|
471 | zu(l) =pu(ig,l) |
---|
472 | zv(l) =pv(ig,l) |
---|
473 | do iq=1,nq |
---|
474 | zq(l,iq) = pq(ig,l,iq) |
---|
475 | enddo |
---|
476 | end do |
---|
477 | |
---|
478 | ! loop over nsubtimestep |
---|
479 | ! """""""""""""""""""""" |
---|
480 | do itsub=1,nsubtimestep |
---|
481 | ! Progressively adding tendancies from other processes. |
---|
482 | do l=1,klev |
---|
483 | ztc(l) =ztc(l) +(pdt(ig,l) + zdtlatent(ig,l))*subtimestep |
---|
484 | zu(l) =zu(l) +pdu( ig,l) * subtimestep |
---|
485 | zv(l) =zv(l) +pdv( ig,l) * subtimestep |
---|
486 | do iq=1,nq |
---|
487 | zq(l,iq) = zq(l,iq) + pdq(ig,l,iq)* subtimestep |
---|
488 | enddo |
---|
489 | end do |
---|
490 | |
---|
491 | ! Change of mass in each layer |
---|
492 | do l=1,klev |
---|
493 | masse(l)=masse(l)+pdpsrf(ig)*subtimestep*(pplev(ig,l) - pplev(ig,l+1))& |
---|
494 | /(g*pplev(ig,1)) |
---|
495 | end do |
---|
496 | |
---|
497 | ! Value transfert at the surface interface when condensation sublimation: |
---|
498 | |
---|
499 | if (zmflux(1).lt.0) then |
---|
500 | ! Surface condensation |
---|
501 | zum(1)= zu(1) |
---|
502 | zvm(1)= zv(1) |
---|
503 | ztm(1) = ztc(1) |
---|
504 | else |
---|
505 | ! Surface sublimation: |
---|
506 | ztm(1) = ztsrf(ig) + pdtsrfc(ig)*ptimestep |
---|
507 | zum(1) = 0 |
---|
508 | zvm(1) = 0 |
---|
509 | end if |
---|
510 | do iq=1,nq |
---|
511 | zqm(1,iq)=0. ! most tracer do not condense ! |
---|
512 | enddo |
---|
513 | ! Special case if the tracer is n2 gas |
---|
514 | if (igcm_n2.ne.0) zqm(1,igcm_n2)=1. |
---|
515 | |
---|
516 | ztm(2:klev+1)=0. |
---|
517 | zum(2:klev+1)=0. |
---|
518 | zvm(2:klev+1)=0. |
---|
519 | zqm1(1:klev+1)=0. |
---|
520 | |
---|
521 | ! Van Leer scheme: |
---|
522 | call vl1d(klev,ztc,2.,masse,w,ztm) |
---|
523 | call vl1d(klev,zu ,2.,masse,w,zum) |
---|
524 | call vl1d(klev,zv ,2.,masse,w,zvm) |
---|
525 | do iq=1,nq |
---|
526 | do l=1,klev |
---|
527 | zq1(l)=zq(l,iq) |
---|
528 | enddo |
---|
529 | zqm1(1)=zqm(1,iq) |
---|
530 | call vl1d(klev,zq1,2.,masse,w,zqm1) |
---|
531 | do l=2,klev |
---|
532 | zqm(l,iq)=zqm1(l) |
---|
533 | enddo |
---|
534 | enddo |
---|
535 | |
---|
536 | ! Correction to prevent negative value for qn2 |
---|
537 | if (igcm_n2.ne.0) then |
---|
538 | zqm(1,igcm_n2)=1. |
---|
539 | do l=1,klev-1 |
---|
540 | if (w(l)*zqm(l,igcm_n2).gt.zq(l,igcm_n2)*masse(l)) then |
---|
541 | zqm(l+1,igcm_n2)=max(zqm(l+1,igcm_n2), & |
---|
542 | (zqm(l,igcm_n2)*w(l) -zq(l,igcm_n2)*masse(l))/w(l+1) ) |
---|
543 | else |
---|
544 | exit |
---|
545 | endif |
---|
546 | end do |
---|
547 | end if |
---|
548 | |
---|
549 | |
---|
550 | !!! Source haze: 0.02 pourcent when n2 sublimes |
---|
551 | IF (source_haze) THEN |
---|
552 | IF (pdicen2(ig).lt.0) THEN |
---|
553 | DO iq=1,nq |
---|
554 | tname=noms(iq) |
---|
555 | if (tname(1:4).eq."haze") then |
---|
556 | !zqm(1,iq)=0.02 |
---|
557 | !zqm(1,iq)=-pdicen2(ig)*0.02 |
---|
558 | zqm(1,iq)=-pdicen2(ig)*ptimestep*0.02 |
---|
559 | !zqm(10,iq)=-pdicen2(ig)*ptimestep*100. |
---|
560 | !zqm(1,iq)=-pdicen2(ig)*1000000. |
---|
561 | |
---|
562 | endif |
---|
563 | ENDDO |
---|
564 | ENDIF |
---|
565 | ENDIF |
---|
566 | ztm(klev+1)= ztc(klev) ! should not be used, but... |
---|
567 | zum(klev+1)= zu(klev) ! should not be used, but... |
---|
568 | zvm(klev+1)= zv(klev) ! should not be used, but... |
---|
569 | do iq=1,nq |
---|
570 | zqm(klev+1,iq)= zq(klev,iq) |
---|
571 | enddo |
---|
572 | |
---|
573 | ! Tendencies on T, U, V, Q |
---|
574 | ! """"""""""""""""""""""" |
---|
575 | DO l=1,klev |
---|
576 | |
---|
577 | ! Tendencies on T |
---|
578 | zdtsig(ig,l) = (1/masse(l)) * & |
---|
579 | ( zmflux(l)*(ztm(l) - ztc(l)) & |
---|
580 | - zmflux(l+1)*(ztm(l+1) - ztc(l)) & |
---|
581 | + zcondicea(ig,l)*(ztcond(ig,l)-ztc(l)) ) |
---|
582 | |
---|
583 | ! Tendencies on U |
---|
584 | pduc(ig,l) = (1/masse(l)) * & |
---|
585 | ( zmflux(l)*(zum(l) - zu(l))& |
---|
586 | - zmflux(l+1)*(zum(l+1) - zu(l)) ) |
---|
587 | |
---|
588 | ! Tendencies on V |
---|
589 | pdvc(ig,l) = (1/masse(l)) * & |
---|
590 | ( zmflux(l)*(zvm(l) - zv(l)) & |
---|
591 | - zmflux(l+1)*(zvm(l+1) - zv(l)) ) |
---|
592 | |
---|
593 | END DO |
---|
594 | |
---|
595 | ! Tendencies on Q |
---|
596 | do iq=1,nq |
---|
597 | if (iq.eq.igcm_n2) then |
---|
598 | ! SPECIAL Case when the tracer IS N2 : |
---|
599 | DO l=1,klev |
---|
600 | pdqc(ig,l,iq)= (1/masse(l)) * & |
---|
601 | ( zmflux(l)*(zqm(l,iq) - zq(l,iq)) & |
---|
602 | - zmflux(l+1)*(zqm(l+1,iq) - zq(l,iq))& |
---|
603 | + zcondicea(ig,l)*(zq(l,iq)-1.) ) |
---|
604 | END DO |
---|
605 | else |
---|
606 | DO l=1,klev |
---|
607 | pdqc(ig,l,iq)= (1/masse(l)) * & |
---|
608 | ( zmflux(l)*(zqm(l,iq) - zq(l,iq)) & |
---|
609 | - zmflux(l+1)*(zqm(l+1,iq) - zq(l,iq)) & |
---|
610 | + zcondicea(ig,l)*zq(l,iq) ) |
---|
611 | END DO |
---|
612 | end if |
---|
613 | enddo |
---|
614 | ! Update variables at the end of each subtimestep. |
---|
615 | do l=1,klev |
---|
616 | ztc(l) =ztc(l) + zdtsig(ig,l) *subtimestep |
---|
617 | zu(l) =zu(l) + pduc(ig,l) *subtimestep |
---|
618 | zv(l) =zv(l) + pdvc(ig,l) *subtimestep |
---|
619 | do iq=1,nq |
---|
620 | zq(l,iq) = zq(l,iq) + pdqc(ig,l,iq)*subtimestep |
---|
621 | enddo |
---|
622 | end do |
---|
623 | enddo ! loop on nsubtimestep |
---|
624 | ! Recomputing Total tendencies |
---|
625 | do l=1,klev |
---|
626 | pdtc(ig,l) = (ztc(l) - zt(ig,l) )/ptimestep |
---|
627 | pduc(ig,l) = (zu(l) - (pu(ig,l) + pdu(ig,l)*ptimestep))/ptimestep |
---|
628 | pdvc(ig,l) = (zv(l) - (pv(ig,l) + pdv(ig,l)*ptimestep))/ptimestep |
---|
629 | do iq=1,nq |
---|
630 | pdqc(ig,l,iq) = (zq(l,iq) - (pq(ig,l,iq) + pdq(ig,l,iq)*ptimestep))/ptimestep |
---|
631 | |
---|
632 | |
---|
633 | ! Correction temporaire |
---|
634 | if (iq.eq.igcm_n2) then |
---|
635 | if((pq(ig,l,iq) +(pdqc(ig,l,iq)+ pdq(ig,l,iq))*ptimestep) & |
---|
636 | .lt.0.01) then ! if n2 < 1 % ! |
---|
637 | write(*,*) 'Warning: n2 < 1%' |
---|
638 | pdqc(ig,l,iq)=(0.01-pq(ig,l,iq))/ptimestep-pdq(ig,l,iq) |
---|
639 | end if |
---|
640 | end if |
---|
641 | |
---|
642 | enddo |
---|
643 | end do |
---|
644 | ! *******************************TEMPORAIRE ****************** |
---|
645 | if (klon.eq.1) then |
---|
646 | write(*,*) 'nsubtimestep=' ,nsubtimestep |
---|
647 | write(*,*) 'masse avant' , (pplev(ig,1) - pplev(ig,2))/g |
---|
648 | write(*,*) 'masse apres' , masse(1) |
---|
649 | write(*,*) 'zmflux*DT, l=1' , zmflux(1)*ptimestep |
---|
650 | write(*,*) 'zmflux*DT, l=2' , zmflux(2)*ptimestep |
---|
651 | write(*,*) 'pq, l=1,2,3' , pq(1,1,1), pq(1,2,1),pq(1,3,1) |
---|
652 | write(*,*) 'zq, l=1,2,3' , zq(1,1), zq(2,1),zq(3,1) |
---|
653 | write(*,*) 'dq*Dt l=1' , pdq(1,1,1)*ptimestep |
---|
654 | write(*,*) 'dqcond*Dt l=1' , pdqc(1,1,1)*ptimestep |
---|
655 | end if |
---|
656 | |
---|
657 | ! *********************************************************** |
---|
658 | end if ! if (condsub) |
---|
659 | END DO ! loop on ig |
---|
660 | endif ! not fast |
---|
661 | |
---|
662 | ! ************ Option Olkin to prevent N2 effect in the south******** |
---|
663 | 112 continue |
---|
664 | if (olkin) then |
---|
665 | DO ig=1,klon |
---|
666 | if (latitude(ig).lt.0) then |
---|
667 | pdtsrfc(ig) = max(0.,pdtsrfc(ig)) |
---|
668 | pdpsrf(ig) = 0. |
---|
669 | pdicen2(ig) = 0. |
---|
670 | do l=1,klev |
---|
671 | pdtc(ig,l) = max(0.,zdtlatent(ig,l)) |
---|
672 | pduc(ig,l) = 0. |
---|
673 | pdvc(ig,l) = 0. |
---|
674 | do iq=1,nq |
---|
675 | pdqc(ig,l,iq) = 0 |
---|
676 | enddo |
---|
677 | end do |
---|
678 | end if |
---|
679 | END DO |
---|
680 | end if |
---|
681 | ! ******************************************************************* |
---|
682 | |
---|
683 | ! *************************************************************** |
---|
684 | ! Ecriture des diagnostiques |
---|
685 | ! *************************************************************** |
---|
686 | |
---|
687 | ! DO l=1,klev |
---|
688 | ! DO ig=1,klon |
---|
689 | ! Taux de cond en kg.m-2.pa-1.s-1 |
---|
690 | ! tconda1(ig,l)=zcondicea(ig,l)/(pplev(ig,l)-pplev(ig,l+1)) |
---|
691 | ! Taux de cond en kg.m-3.s-1 |
---|
692 | ! tconda2(ig,l)=tconda1(ig,l)*pplay(ig,l)*g/(r*pt(ig,l)) |
---|
693 | ! END DO |
---|
694 | ! END DO |
---|
695 | ! call WRITEDIAGFI(klon,'tconda1', & |
---|
696 | ! 'Taux de condensation N2 atmospherique /Pa', & |
---|
697 | ! 'kg.m-2.Pa-1.s-1',3,tconda1) |
---|
698 | ! call WRITEDIAGFI(klon,'tconda2', & |
---|
699 | ! 'Taux de condensation N2 atmospherique /m', & |
---|
700 | ! 'kg.m-3.s-1',3,tconda2) |
---|
701 | |
---|
702 | |
---|
703 | return |
---|
704 | end subroutine condense_n2 |
---|
705 | |
---|
706 | !------------------------------------------------------------------------- |
---|
707 | |
---|
708 | real function tcond_n2(p,vmr) |
---|
709 | ! Calculates the condensation temperature for N2 at pressure P and vmr |
---|
710 | implicit none |
---|
711 | real, intent(in):: p,vmr |
---|
712 | |
---|
713 | ! tcond_n2 = (1.)/(0.026315-0.0011877*log(.7143*p*vmr)) |
---|
714 | IF (p.ge.0.529995) then |
---|
715 | ! tcond Fray and Schmitt for N2 phase beta (T>35.6 K) FIT TB |
---|
716 | ! tcond_n2 = (1.)/(1./63.1470-296.925/(2.5e5*0.98)*log(1./(0.125570*1.e5)*p*vmr)) |
---|
717 | tcond_n2 = (1.)/(0.01583606505-1.211938776e-3*log(7.963685594e-5*p*vmr)) |
---|
718 | ELSE |
---|
719 | ! tcond Fray and Schmitt for N2 phase alpha(T<35.6 K) FIT BT |
---|
720 | ! tcond_n2 = (1.)/(1./35.6-296.925/(2.5e5*1.09)*log(1./(0.508059)*p*vmr)) |
---|
721 | tcond_n2 = (1.)/(1./35.6-1.089633028e-3*log(1.968275338*p*vmr)) |
---|
722 | ENDIF |
---|
723 | return |
---|
724 | end function tcond_n2 |
---|
725 | |
---|
726 | !------------------------------------------------------------------------- |
---|
727 | |
---|
728 | real function pcond_n2(t,vmr) |
---|
729 | ! Calculates the condensation pressure for N2 at temperature T and vmr |
---|
730 | implicit none |
---|
731 | real, intent(in):: t,vmr |
---|
732 | |
---|
733 | ! tcond_n2 = (1.)/(0.026315-0.0011877*log(.7143*p*vmr)) |
---|
734 | IF (t.ge.35.6) then |
---|
735 | ! tcond Fray and Schmitt for N2 phase beta (T>35.6 K) FIT TB |
---|
736 | ! pcond_n2 = 0.125570*1.e5/vmr*exp((2.5e5*0.98)/296.925*(1./63.1470-1./t)) |
---|
737 | pcond_n2 = 0.125570e5/vmr*exp(825.1241896*(1./63.147-1./t)) |
---|
738 | ELSE |
---|
739 | ! tcond Fray and Schmitt for N2 phase alpha(T<35.6 K) FIT TB |
---|
740 | ! pcond_n2 = 0.508059/vmr*exp((2.5e5*1.09)/296.925*(1./35.6-1./t)) |
---|
741 | pcond_n2 = 0.508059/vmr*exp(917.7401701*(1./35.6-1./t)) |
---|
742 | ENDIF |
---|
743 | return |
---|
744 | end function pcond_n2 |
---|
745 | |
---|
746 | !------------------------------------------------------------------------- |
---|
747 | |
---|
748 | real function glob_average2d(var) |
---|
749 | ! Calculates the global average of variable var |
---|
750 | use comgeomfi_h |
---|
751 | use dimphy, only: klon |
---|
752 | USE mod_grid_phy_lmdz, ONLY: nbp_lon, nbp_lat |
---|
753 | use geometry_mod, only: cell_area, latitude |
---|
754 | |
---|
755 | implicit none |
---|
756 | |
---|
757 | ! INTEGER klon |
---|
758 | REAL var(klon) |
---|
759 | INTEGER ig |
---|
760 | |
---|
761 | glob_average2d = 0. |
---|
762 | DO ig=2,klon-1 |
---|
763 | glob_average2d = glob_average2d + var(ig)*cell_area(ig) |
---|
764 | END DO |
---|
765 | glob_average2d = glob_average2d + var(1)*cell_area(1)*nbp_lon |
---|
766 | glob_average2d = glob_average2d + var(klon)*cell_area(klon)*nbp_lon |
---|
767 | glob_average2d = glob_average2d/(totarea+(cell_area(1)+cell_area(klon))*(nbp_lon-1)) |
---|
768 | |
---|
769 | end function glob_average2d |
---|
770 | |
---|
771 | ! ***************************************************************** |
---|
772 | |
---|
773 | subroutine vl1d(klev,q,pente_max,masse,w,qm) |
---|
774 | ! |
---|
775 | ! Operateur de moyenne inter-couche pour calcul de transport type |
---|
776 | ! Van-Leer " pseudo amont " dans la verticale |
---|
777 | ! q,w sont des arguments d'entree pour le s-pg .... |
---|
778 | ! masse : masse de la couche Dp/g |
---|
779 | ! w : masse d'atm ``transferee'' a chaque pas de temps (kg.m-2) |
---|
780 | ! pente_max = 2 conseillee |
---|
781 | ! -------------------------------------------------------------------- |
---|
782 | IMPLICIT NONE |
---|
783 | |
---|
784 | ! Arguments: |
---|
785 | ! ---------- |
---|
786 | integer klev |
---|
787 | real masse(klev),pente_max |
---|
788 | REAL q(klev),qm(klev+1) |
---|
789 | REAL w(klev+1) |
---|
790 | ! |
---|
791 | ! Local |
---|
792 | ! --------- |
---|
793 | ! |
---|
794 | INTEGER l |
---|
795 | ! |
---|
796 | real dzq(klev),dzqw(klev),adzqw(klev),dzqmax |
---|
797 | real sigw, Mtot, MQtot |
---|
798 | integer m |
---|
799 | |
---|
800 | |
---|
801 | ! On oriente tout dans le sens de la pression |
---|
802 | ! W > 0 WHEN DOWN !!!!!!!!!!!!! |
---|
803 | |
---|
804 | do l=2,klev |
---|
805 | dzqw(l)=q(l-1)-q(l) |
---|
806 | adzqw(l)=abs(dzqw(l)) |
---|
807 | enddo |
---|
808 | |
---|
809 | do l=2,klev-1 |
---|
810 | if(dzqw(l)*dzqw(l+1).gt.0.) then |
---|
811 | dzq(l)=0.5*(dzqw(l)+dzqw(l+1)) |
---|
812 | else |
---|
813 | dzq(l)=0. |
---|
814 | endif |
---|
815 | dzqmax=pente_max*min(adzqw(l),adzqw(l+1)) |
---|
816 | dzq(l)=sign(min(abs(dzq(l)),dzqmax),dzq(l)) |
---|
817 | enddo |
---|
818 | |
---|
819 | dzq(1)=0. |
---|
820 | dzq(klev)=0. |
---|
821 | |
---|
822 | do l = 1,klev-1 |
---|
823 | |
---|
824 | ! Regular scheme (transfered mass < layer mass) |
---|
825 | ! ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ |
---|
826 | if(w(l+1).gt.0. .and. w(l+1).le.masse(l+1)) then |
---|
827 | sigw=w(l+1)/masse(l+1) |
---|
828 | qm(l+1)=(q(l+1)+0.5*(1.-sigw)*dzq(l+1)) |
---|
829 | else if(w(l+1).le.0. .and. -w(l+1).le.masse(l)) then |
---|
830 | sigw=w(l+1)/masse(l) |
---|
831 | qm(l+1)=(q(l)-0.5*(1.+sigw)*dzq(l)) |
---|
832 | |
---|
833 | ! Extended scheme (transfered mass > layer mass) |
---|
834 | ! ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ |
---|
835 | else if(w(l+1).gt.0.) then |
---|
836 | m=l+1 |
---|
837 | Mtot = masse(m) |
---|
838 | MQtot = masse(m)*q(m) |
---|
839 | !if (m.lt.klev) then ! because some compilers will have problems |
---|
840 | ! ! evaluating masse(klev+1) |
---|
841 | do while ((m.lt.klev).and.(w(l+1).gt.(Mtot+masse(m+1)))) |
---|
842 | m=m+1 |
---|
843 | Mtot = Mtot + masse(m) |
---|
844 | MQtot = MQtot + masse(m)*q(m) |
---|
845 | ! if (m.eq.klev) exit |
---|
846 | end do |
---|
847 | !endif |
---|
848 | if (m.lt.klev) then |
---|
849 | sigw=(w(l+1)-Mtot)/masse(m+1) |
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850 | qm(l+1)= (1/w(l+1))*(MQtot + (w(l+1)-Mtot)* & |
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851 | (q(m+1)+0.5*(1.-sigw)*dzq(m+1)) ) |
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852 | else |
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853 | w(l+1) = Mtot |
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854 | qm(l+1) = Mqtot / Mtot |
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855 | write(*,*) 'top layer is disapearing !' |
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856 | stop |
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857 | end if |
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858 | else ! if(w(l+1).lt.0) |
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859 | m = l-1 |
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860 | Mtot = masse(m+1) |
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861 | MQtot = masse(m+1)*q(m+1) |
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862 | if (m.gt.0) then ! because some compilers will have problems |
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863 | ! evaluating masse(0) |
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864 | do while ((m.gt.0).and.(-w(l+1).gt.(Mtot+masse(m)))) |
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865 | m=m-1 |
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866 | Mtot = Mtot + masse(m+1) |
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867 | MQtot = MQtot + masse(m+1)*q(m+1) |
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868 | if (m.eq.0) exit |
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869 | end do |
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870 | endif |
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871 | if (m.gt.0) then |
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872 | sigw=(w(l+1)+Mtot)/masse(m) |
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873 | qm(l+1)= (-1/w(l+1))*(MQtot + (-w(l+1)-Mtot)* & |
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874 | (q(m)-0.5*(1.+sigw)*dzq(m)) ) |
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875 | else |
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876 | qm(l+1)= (-1/w(l+1))*(MQtot + (-w(l+1)-Mtot)*qm(1)) |
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877 | end if |
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878 | end if |
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879 | enddo |
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880 | |
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881 | return |
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882 | end subroutine vl1d |
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883 | |
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