1 | MODULE improvedclouds_mod |
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2 | |
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3 | IMPLICIT NONE |
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4 | |
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5 | CONTAINS |
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6 | |
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7 | subroutine improvedclouds(microtimestep, |
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8 | & pplay,pt,pq, |
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9 | & subpdqcloud,subpdtcloud, |
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10 | & nq,tauscaling,mmean) |
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11 | USE updaterad, ONLY: updaterice_micro, updaterccn |
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12 | USE watersat_mod, ONLY: watersat |
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13 | use tracer_mod, only: rho_ice, nuice_sed, igcm_h2o_vap, |
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14 | & igcm_h2o_ice, igcm_dust_mass, |
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15 | & igcm_dust_number, igcm_ccn_mass, |
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16 | & igcm_ccn_number, |
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17 | & igcm_hdo_vap,igcm_hdo_ice, |
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18 | & qperemin |
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19 | use comcstfi_h, only: pi, cpp |
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20 | use write_output_mod, only: write_output |
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21 | implicit none |
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22 | |
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23 | |
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24 | c------------------------------------------------------------------ |
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25 | c This routine is used to form clouds when a parcel of the GCM is |
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26 | c saturated. It includes the ability to have supersaturation, a |
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27 | c computation of the nucleation rates, growthrates and the |
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28 | c scavenging of dust particles by clouds. |
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29 | c It is worth noting that the amount of dust is computed using the |
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30 | c dust optical depth computed in aeropacity.F. That's why |
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31 | c the variable called "tauscaling" is used to convert |
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32 | c pq(dust_mass) and pq(dust_number), which are relative |
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33 | c quantities, to absolute and realistic quantities stored in zq. |
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34 | c This has to be done to convert the inputs into absolute |
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35 | c values, but also to convert the outputs back into relative |
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36 | c values which are then used by the sedimentation and advection |
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37 | c schemes. |
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38 | |
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39 | c Authors: J.-B. Madeleine, based on the work by Franck Montmessin |
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40 | c (October 2011) |
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41 | c T. Navarro, debug,correction, new scheme (October-April 2011) |
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42 | c A. Spiga, optimization (February 2012) |
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43 | c J. Naar, from global to local (no more ngrid, nlay) to allow |
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44 | c different microphysical timesteps (May 2023) |
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45 | c------------------------------------------------------------------ |
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46 | #include "callkeys.h" |
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47 | #include "microphys.h" |
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48 | c------------------------------------------------------------------ |
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49 | c Inputs/outputs: |
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50 | |
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51 | INTEGER, INTENT(IN) :: nq ! nombre de traceurs |
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52 | REAL, INTENT(IN) :: microtimestep ! pas de temps physique (s) |
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53 | REAL, INTENT(IN) :: pplay ! pression au milieu des couches (Pa) |
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54 | REAL, INTENT(IN) :: pt ! temperature at the middle of the |
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55 | ! layers (K) |
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56 | ! param. |
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57 | REAL, INTENT(IN) :: pq(nq) ! traceur (kg/kg) |
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58 | ! (kg/kg.s-1) |
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59 | REAL, INTENT(IN) :: tauscaling ! Convertion factor for qdust and Ndust |
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60 | REAL, INTENT(IN) :: mmean ! Mean atmospheric mass |
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61 | |
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62 | REAL, INTENT(OUT) :: subpdqcloud(nq) ! tendance de la condensation |
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63 | ! H2O(kg/kg.s-1) |
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64 | REAL, INTENT(OUT) :: subpdtcloud ! tendance temperature due |
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65 | ! a la chaleur latente |
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66 | |
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67 | c------------------------------------------------------------------ |
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68 | c Local variables: |
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69 | |
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70 | LOGICAL firstcall |
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71 | DATA firstcall/.true./ |
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72 | SAVE firstcall |
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73 | |
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74 | !$OMP THREADPRIVATE(firstcall) |
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75 | |
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76 | REAL*8 derf ! Error function |
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77 | !external derf |
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78 | |
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79 | INTEGER ig,l,i |
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80 | |
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81 | REAL zq(nq) ! local value of tracers |
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82 | REAL zq0(nq) ! local initial value of tracers |
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83 | REAL zt ! local value of temperature |
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84 | REAL zqsat_tmp(1) ! saturation |
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85 | REAL zqsat ! saturation |
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86 | REAL lw !Latent heat of sublimation (J.kg-1) |
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87 | REAL cste |
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88 | REAL dMice ! mass of condensed ice |
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89 | REAL dMice_hdo ! mass of condensed HDO ice |
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90 | REAL alpha ! HDO equilibrium fractionation coefficient (Saturation=1) |
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91 | REAL alpha_c ! HDO real fractionation coefficient |
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92 | ! REAL sumcheck |
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93 | REAL*8 ph2o ! Water vapor partial pressure (Pa) |
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94 | REAL*8 satu ! Water vapor saturation ratio over ice |
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95 | REAL*8 Mo,No |
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96 | REAL*8 Rn, Rm, dev2, n_derf, m_derf |
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97 | REAL*8 n_aer(nbin_cld) ! number conc. of particle/each size bin |
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98 | REAL*8 m_aer(nbin_cld) ! mass mixing ratio of particle/each size bin |
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99 | |
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100 | REAL*8 sig ! Water-ice/air surface tension (N.m) |
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101 | EXTERNAL sig |
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102 | |
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103 | REAL dN,dM |
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104 | REAL rate(nbin_cld) ! nucleation rate |
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105 | REAL seq |
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106 | |
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107 | REAL rice ! Ice mass mean radius (m) |
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108 | ! (r_c in montmessin_2004) |
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109 | REAL rhocloud ! Cloud density (kg.m-3) |
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110 | REAL rdust ! Dust geometric mean radius (m) |
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111 | |
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112 | REAL res ! Resistance growth |
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113 | REAL Dv,Dv_hdo ! Water/HDO vapor diffusion coefficient |
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114 | |
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115 | |
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116 | c Parameters of the size discretization |
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117 | c used by the microphysical scheme |
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118 | DOUBLE PRECISION, PARAMETER :: rmin_cld = 0.1e-6 ! Minimum radius (m) |
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119 | DOUBLE PRECISION, PARAMETER :: rmax_cld = 10.e-6 ! Maximum radius (m) |
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120 | DOUBLE PRECISION, PARAMETER :: rbmin_cld = 0.0001e-6 |
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121 | ! Minimum boundary radius (m) |
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122 | DOUBLE PRECISION, PARAMETER :: rbmax_cld = 1.e-2 ! Maximum boundary radius (m) |
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123 | DOUBLE PRECISION vrat_cld ! Volume ratio |
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124 | DOUBLE PRECISION rb_cld(nbin_cld+1)! boundary values of each rad_cld bin (m) |
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125 | SAVE rb_cld |
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126 | DOUBLE PRECISION dr_cld(nbin_cld) ! width of each rad_cld bin (m) |
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127 | DOUBLE PRECISION vol_cld(nbin_cld) ! particle volume for each bin (m3) |
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128 | |
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129 | !$OMP THREADPRIVATE(rb_cld) |
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130 | |
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131 | |
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132 | REAL sigma_ice ! Variance of the ice and CCN distributions |
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133 | SAVE sigma_ice |
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134 | |
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135 | !$OMP THREADPRIVATE(sigma_ice) |
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136 | |
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137 | |
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138 | |
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139 | c---------------------------------- |
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140 | c TESTS |
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141 | |
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142 | INTEGER countcells |
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143 | |
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144 | LOGICAL test_flag ! flag for test/debuging outputs |
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145 | SAVE test_flag |
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146 | |
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147 | !$OMP THREADPRIVATE(test_flag) |
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148 | |
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149 | |
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150 | REAL satubf,satuaf |
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151 | REAL res_out |
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152 | |
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153 | |
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154 | c------------------------------------------------------------------ |
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155 | |
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156 | ! AS: firstcall OK absolute |
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157 | IF (firstcall) THEN |
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158 | !============================================================= |
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159 | ! 0. Definition of the size grid |
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160 | !============================================================= |
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161 | c rad_cld is the primary radius grid used for microphysics computation. |
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162 | c The grid spacing is computed assuming a constant volume ratio |
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163 | c between two consecutive bins; i.e. vrat_cld. |
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164 | c vrat_cld is determined from the boundary values of the size grid: |
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165 | c rmin_cld and rmax_cld. |
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166 | c The rb_cld array contains the boundary values of each rad_cld bin. |
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167 | c dr_cld is the width of each rad_cld bin. |
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168 | |
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169 | c Volume ratio between two adjacent bins |
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170 | ! vrat_cld = log(rmax_cld/rmin_cld) / float(nbin_cld-1) *3. |
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171 | ! vrat_cld = exp(vrat_cld) |
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172 | vrat_cld = log(rmax_cld/rmin_cld) / float(nbin_cld-1) *3. |
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173 | vrat_cld = exp(vrat_cld) |
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174 | write(*,*) "vrat_cld", vrat_cld |
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175 | |
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176 | rb_cld(1) = rbmin_cld |
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177 | rad_cld(1) = rmin_cld |
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178 | vol_cld(1) = 4./3. * dble(pi) * rmin_cld*rmin_cld*rmin_cld |
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179 | ! vol_cld(1) = 4./3. * pi * rmin_cld*rmin_cld*rmin_cld |
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180 | |
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181 | do i=1,nbin_cld-1 |
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182 | rad_cld(i+1) = rad_cld(i) * vrat_cld**(1./3.) |
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183 | vol_cld(i+1) = vol_cld(i) * vrat_cld |
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184 | enddo |
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185 | |
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186 | do i=1,nbin_cld |
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187 | rb_cld(i+1)= ( (2.*vrat_cld) / (vrat_cld+1.) )**(1./3.) * |
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188 | & rad_cld(i) |
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189 | dr_cld(i) = rb_cld(i+1) - rb_cld(i) |
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190 | enddo |
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191 | rb_cld(nbin_cld+1) = rbmax_cld |
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192 | dr_cld(nbin_cld) = rb_cld(nbin_cld+1) - rb_cld(nbin_cld) |
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193 | |
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194 | print*, ' ' |
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195 | print*,'Microphysics: size bin information:' |
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196 | print*,'i,rb_cld(i), rad_cld(i),dr_cld(i)' |
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197 | print*,'-----------------------------------' |
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198 | do i=1,nbin_cld |
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199 | write(*,'(i2,3x,3(e12.6,4x))') i,rb_cld(i), rad_cld(i), |
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200 | & dr_cld(i) |
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201 | enddo |
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202 | write(*,'(i2,3x,e12.6)') nbin_cld+1,rb_cld(nbin_cld+1) |
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203 | print*,'-----------------------------------' |
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204 | |
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205 | do i=1,nbin_cld+1 |
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206 | ! rb_cld(i) = log(rb_cld(i)) |
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207 | rb_cld(i) = log(rb_cld(i)) !! we save that so that it is not computed |
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208 | !! at each timestep and gridpoint |
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209 | enddo |
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210 | |
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211 | c Contact parameter of water ice on dust ( m=cos(theta) ) |
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212 | c ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ |
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213 | ! mteta = 0.95 |
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214 | write(*,*) 'water_param contact parameter:', mteta |
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215 | |
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216 | c Volume of a water molecule (m3) |
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217 | vo1 = mh2o / dble(rho_ice) |
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218 | c Variance of the ice and CCN distributions |
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219 | sigma_ice = sqrt(log(1.+nuice_sed)) |
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220 | |
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221 | |
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222 | write(*,*) 'Variance of ice & CCN distribs :', sigma_ice |
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223 | write(*,*) 'nuice for sedimentation:', nuice_sed |
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224 | write(*,*) 'Volume of a water molecule:', vo1 |
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225 | |
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226 | |
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227 | test_flag = .false. |
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228 | |
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229 | firstcall=.false. |
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230 | END IF |
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231 | |
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232 | |
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233 | !============================================================= |
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234 | ! 1. Initialisation |
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235 | !============================================================= |
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236 | cste = 4*pi*rho_ice*microtimestep |
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237 | |
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238 | res_out = 0 |
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239 | rice = 1.e-8 |
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240 | |
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241 | c Initialize the tendencies |
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242 | subpdqcloud(1:nq)=0 |
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243 | subpdtcloud=0 |
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244 | |
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245 | c temperature and tracers previously incremented here |
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246 | c now done outside, in watercloud_mod.F |
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247 | c zt = pteff + sum_subpdt * microtimestep |
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248 | c zq(1:nq) = pqeff(1:nq) + sum_subpdq(1:nq) * microtimestep |
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249 | |
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250 | zq(1:nq)=pq(1:nq) |
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251 | zt=pt |
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252 | |
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253 | WHERE( zq(1:nq) < 1.e-30 ) |
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254 | & zq(1:nq) = 1.e-30 |
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255 | |
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256 | zq0(1:nq) = zq(1:nq) |
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257 | |
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258 | !============================================================= |
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259 | ! 2. Compute saturation |
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260 | !============================================================= |
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261 | |
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262 | |
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263 | dev2 = 1. / ( sqrt(2.) * sigma_ice ) |
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264 | |
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265 | call watersat(1,(/zt/),(/pplay/),zqsat_tmp) |
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266 | zqsat=zqsat_tmp(1) |
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267 | countcells = 0 |
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268 | |
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269 | c Get the partial pressure of water vapor and its saturation ratio |
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270 | ph2o = zq(igcm_h2o_vap) * (mmean/18.) * pplay |
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271 | satu = zq(igcm_h2o_vap) / zqsat |
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272 | |
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273 | !============================================================= |
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274 | ! 3. Nucleation |
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275 | !============================================================= |
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276 | |
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277 | IF ( satu .ge. 1. ) THEN ! if there is condensation |
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278 | |
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279 | call updaterccn(zq(igcm_dust_mass), |
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280 | & zq(igcm_dust_number),rdust,tauscaling) |
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281 | |
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282 | |
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283 | c Expand the dust moments into a binned distribution |
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284 | Mo = zq(igcm_dust_mass)* tauscaling + 1.e-30 |
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285 | No = zq(igcm_dust_number)* tauscaling + 1.e-30 |
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286 | Rn = rdust |
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287 | Rn = -log(Rn) |
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288 | Rm = Rn - 3. * sigma_ice*sigma_ice |
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289 | n_derf = derf( (rb_cld(1)+Rn) *dev2) |
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290 | m_derf = derf( (rb_cld(1)+Rm) *dev2) |
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291 | do i = 1, nbin_cld |
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292 | n_aer(i) = -0.5 * No * n_derf !! this ith previously computed |
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293 | m_aer(i) = -0.5 * Mo * m_derf !! this ith previously computed |
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294 | n_derf = derf( (rb_cld(i+1)+Rn) *dev2) |
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295 | m_derf = derf( (rb_cld(i+1)+Rm) *dev2) |
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296 | n_aer(i) = n_aer(i) + 0.5 * No * n_derf |
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297 | m_aer(i) = m_aer(i) + 0.5 * Mo * m_derf |
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298 | enddo |
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299 | |
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300 | ! sumcheck = 0 |
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301 | ! do i = 1, nbin_cld |
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302 | ! sumcheck = sumcheck + n_aer(i) |
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303 | ! enddo |
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304 | ! sumcheck = abs(sumcheck/No - 1) |
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305 | ! if ((sumcheck .gt. 1e-5).and. (1./Rn .gt. rmin_cld)) then |
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306 | ! print*, "WARNING, No sumcheck PROBLEM" |
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307 | ! print*, "sumcheck, No",sumcheck, No |
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308 | ! print*, "min radius, Rn, ig, l", rmin_cld, 1./Rn, ig, l |
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309 | ! print*, "Dust binned distribution", n_aer |
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310 | ! endif |
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311 | ! |
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312 | ! sumcheck = 0 |
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313 | ! do i = 1, nbin_cld |
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314 | ! sumcheck = sumcheck + m_aer(i) |
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315 | ! enddo |
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316 | ! sumcheck = abs(sumcheck/Mo - 1) |
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317 | ! if ((sumcheck .gt. 1e-5) .and. (1./Rn .gt. rmin_cld)) then |
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318 | ! print*, "WARNING, Mo sumcheck PROBLEM" |
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319 | ! print*, "sumcheck, Mo",sumcheck, Mo |
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320 | ! print*, "min radius, Rm, ig, l", rmin_cld, 1./Rm, ig, l |
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321 | ! print*, "Dust binned distribution", m_aer |
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322 | ! endif |
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323 | |
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324 | |
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325 | c Get the rates of nucleation |
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326 | call nuclea(ph2o,zt,satu,n_aer,rate) |
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327 | |
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328 | dN = 0. |
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329 | dM = 0. |
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330 | do i = 1, nbin_cld |
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331 | dN = dN + n_aer(i)*(exp(-rate(i)*microtimestep)-1.) |
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332 | dM = dM + m_aer(i)*(exp(-rate(i)*microtimestep)-1.) |
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333 | enddo |
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334 | |
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335 | |
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336 | c Update Dust particles |
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337 | zq(igcm_dust_mass) = |
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338 | & zq(igcm_dust_mass) + dM/ tauscaling !max(tauscaling,1.e-10) |
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339 | zq(igcm_dust_number) = |
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340 | & zq(igcm_dust_number) + dN/ tauscaling !max(tauscaling,1.e-10) |
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341 | c Update CCNs |
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342 | zq(igcm_ccn_mass) = |
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343 | & zq(igcm_ccn_mass) - dM/ tauscaling !max(tauscaling,1.e-10) |
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344 | zq(igcm_ccn_number) = |
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345 | & zq(igcm_ccn_number) - dN/ tauscaling !max(tauscaling,1.e-10) |
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346 | |
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347 | ENDIF ! of is satu >1 |
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348 | |
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349 | !============================================================= |
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350 | ! 4. Ice growth: scheme for radius evolution |
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351 | !============================================================= |
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352 | |
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353 | c We trigger crystal growth if and only if there is at least one nuclei (N>1). |
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354 | c Indeed, if we are supersaturated and still don't have at least one nuclei, we should better wait |
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355 | c to avoid unrealistic value for nuclei radius and so on for cases that remain negligible. |
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356 | |
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357 | IF ( zq(igcm_ccn_number)*tauscaling.ge. 1.) THEN ! we trigger crystal growth |
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358 | |
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359 | |
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360 | call updaterice_micro(zq(igcm_h2o_ice), |
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361 | & zq(igcm_ccn_mass),zq(igcm_ccn_number), |
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362 | & tauscaling,rice,rhocloud) |
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363 | |
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364 | No = zq(igcm_ccn_number)* tauscaling + 1.e-30 |
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365 | |
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366 | c saturation at equilibrium |
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367 | c rice should not be too small, otherwise seq value is not valid |
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368 | seq = exp(2.*sig(zt)*mh2o / (rho_ice*rgp*zt* |
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369 | & max(rice,1.e-7))) |
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370 | |
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371 | c get resistance growth |
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372 | call growthrate(zt,pplay, |
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373 | & real(ph2o/satu),rice,res,Dv) |
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374 | |
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375 | res_out = res |
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376 | |
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377 | ccccccc implicit scheme of mass growth |
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378 | |
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379 | dMice = |
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380 | & (zq(igcm_h2o_vap)-seq*zqsat) |
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381 | & /(res*zqsat/(cste*No*rice) + 1.) |
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382 | |
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383 | |
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384 | ! With the above scheme, dMice cannot be bigger than vapor, |
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385 | ! but can be bigger than all available ice. |
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386 | dMice = max(dMice,-zq(igcm_h2o_ice)) |
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387 | dMice = min(dMice,zq(igcm_h2o_vap)) ! this should be useless... |
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388 | |
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389 | zq(igcm_h2o_ice) = zq(igcm_h2o_ice)+dMice |
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390 | zq(igcm_h2o_vap) = zq(igcm_h2o_vap)-dMice |
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391 | |
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392 | |
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393 | countcells = countcells + 1 |
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394 | |
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395 | ! latent heat release |
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396 | lw=(2834.3-0.28*(zt-To)- |
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397 | & 0.004*(zt-To)*(zt-To))*1.e+3 |
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398 | subpdtcloud= dMice*lw/cpp/microtimestep |
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399 | |
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400 | c Special case of the isotope of water HDO |
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401 | if (hdo) then |
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402 | !! condensation |
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403 | if (dMice.gt.0.0) then |
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404 | !! do we use fractionation? |
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405 | if (hdofrac) then |
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406 | !! Calculation of the HDO vapor coefficient |
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407 | Dv_hdo = 1./3. * sqrt( 8*kbz*zt/(pi*mhdo/nav) ) |
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408 | & * kbz * zt / |
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409 | & ( pi * pplay * (molco2+molhdo)*(molco2+molhdo) |
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410 | & * sqrt(1.+mhdo/mco2) ) |
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411 | !! Calculation of the fractionnation coefficient at equilibrium |
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412 | c alpha = exp(16288./zt**2.-9.34d-2) ! Merlivat and Nief et al. 1967 |
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413 | alpha = exp(13525./zt**2.-5.59d-2) ! Lamb et al. 2017 |
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414 | !! Calculation of the 'real' fractionnation coefficient |
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415 | alpha_c = (alpha*satu)/ |
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416 | & ( (alpha*(Dv/Dv_hdo)*(satu-1.)) + 1.) |
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417 | c alpha_c = alpha ! to test without the effect of cinetics |
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418 | else |
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419 | alpha_c = 1.d0 |
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420 | endif |
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421 | if (zq0(igcm_h2o_vap).gt.qperemin) then |
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422 | dMice_hdo= |
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423 | & dMice*alpha_c* |
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424 | & ( zq0(igcm_hdo_vap) |
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425 | & /zq0(igcm_h2o_vap) ) |
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426 | else |
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427 | dMice_hdo=0. |
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428 | endif |
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429 | !! sublimation |
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430 | else |
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431 | if (zq0(igcm_h2o_ice).gt.qperemin) then |
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432 | dMice_hdo= |
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433 | & dMice* |
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434 | & ( zq0(igcm_hdo_ice) |
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435 | & /zq0(igcm_h2o_ice) ) |
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436 | else |
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437 | dMice_hdo=0. |
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438 | endif |
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439 | endif !if (dMice.gt.0.0) |
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440 | |
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441 | dMice_hdo = max(dMice_hdo,-zq(igcm_hdo_ice)) |
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442 | dMice_hdo = min(dMice_hdo,zq(igcm_hdo_vap)) |
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443 | |
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444 | zq(igcm_hdo_ice) = zq(igcm_hdo_ice)+dMice_hdo |
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445 | zq(igcm_hdo_vap) = zq(igcm_hdo_vap)-dMice_hdo |
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446 | |
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447 | endif ! if (hdo) |
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448 | |
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449 | !============================================================= |
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450 | ! 5. Dust cores released, tendancies, latent heat, etc ... |
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451 | !============================================================= |
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452 | |
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453 | c If all the ice particles sublimate, all the condensation |
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454 | c nuclei are released: |
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455 | if (zq(igcm_h2o_ice).le.1.e-28) then |
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456 | |
---|
457 | c Water |
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458 | zq(igcm_h2o_vap) = zq(igcm_h2o_vap) |
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459 | & + zq(igcm_h2o_ice) |
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460 | zq(igcm_h2o_ice) = 0. |
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461 | if (hdo) then |
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462 | zq(igcm_hdo_vap) = zq(igcm_hdo_vap) |
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463 | & + zq(igcm_hdo_ice) |
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464 | zq(igcm_hdo_ice) = 0. |
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465 | endif |
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466 | c Dust particles |
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467 | zq(igcm_dust_mass) = zq(igcm_dust_mass) |
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468 | & + zq(igcm_ccn_mass) |
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469 | zq(igcm_dust_number) = zq(igcm_dust_number) |
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470 | & + zq(igcm_ccn_number) |
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471 | c CCNs |
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472 | zq(igcm_ccn_mass) = 0. |
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473 | zq(igcm_ccn_number) = 0. |
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474 | |
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475 | endif |
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476 | |
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477 | ENDIF !of if Nccn>1 |
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478 | |
---|
479 | |
---|
480 | ! Get cloud tendencies |
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481 | subpdqcloud(igcm_h2o_vap) = |
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482 | & (zq(igcm_h2o_vap) - |
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483 | & zq0(igcm_h2o_vap))/microtimestep |
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484 | subpdqcloud(igcm_h2o_ice) = |
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485 | & (zq(igcm_h2o_ice) - |
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486 | & zq0(igcm_h2o_ice))/microtimestep |
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487 | if (hdo) then |
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488 | subpdqcloud(igcm_hdo_vap) = |
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489 | & (zq(igcm_hdo_vap) - |
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490 | & zq0(igcm_hdo_vap))/microtimestep |
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491 | subpdqcloud(igcm_hdo_ice) = |
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492 | & (zq(igcm_hdo_ice) - |
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493 | & zq0(igcm_hdo_ice))/microtimestep |
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494 | endif |
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495 | subpdqcloud(igcm_ccn_mass) = |
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496 | & (zq(igcm_ccn_mass) - |
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497 | & zq0(igcm_ccn_mass))/microtimestep |
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498 | subpdqcloud(igcm_ccn_number) = |
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499 | & (zq(igcm_ccn_number) - |
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500 | & zq0(igcm_ccn_number))/microtimestep |
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501 | |
---|
502 | if (scavenging) then |
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503 | |
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504 | subpdqcloud(igcm_dust_mass) = |
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505 | & (zq(igcm_dust_mass) - |
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506 | & zq0(igcm_dust_mass))/microtimestep |
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507 | subpdqcloud(igcm_dust_number) = |
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508 | & (zq(igcm_dust_number) - |
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509 | & zq0(igcm_dust_number))/microtimestep |
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510 | |
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511 | endif |
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512 | |
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513 | |
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514 | |
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515 | !!!!!!!!!!!!!! TESTS OUTPUTS TESTS OUTPUTS TESTS OUTPUTS TESTS OUTPUTS |
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516 | !!!!!!!!!!!!!! TESTS OUTPUTS TESTS OUTPUTS TESTS OUTPUTS TESTS OUTPUTS |
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517 | !!!!!!!!!!!!!! TESTS OUTPUTS TESTS OUTPUTS TESTS OUTPUTS TESTS OUTPUTS |
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518 | IF (test_flag) then |
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519 | |
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520 | ! error2d(:) = 0. |
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521 | ! error2d(ig) = max(abs(error_out),error2d(ig)) |
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522 | satubf = zq0(igcm_h2o_vap)/zqsat |
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523 | satuaf = zq(igcm_h2o_vap)/zqsat |
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524 | |
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525 | c print*, 'count is ',countcells, ' i.e. ', |
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526 | c & countcells*100/(nlay*ngrid), '% for microphys computation' |
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527 | |
---|
528 | #ifndef MESOSCALE |
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529 | ! IF (ngrid.ne.1) THEN ! 3D |
---|
530 | ! call write_output("satu","ratio saturation","", |
---|
531 | ! & satu_out) |
---|
532 | ! call write_output("dM","ccn variation","kg/kg", |
---|
533 | ! & dM_out) |
---|
534 | ! call write_output("dN","ccn variation","#", |
---|
535 | ! & dN_out) |
---|
536 | ! call write_output("error","dichotomy max error","%", |
---|
537 | ! & error2d) |
---|
538 | ! call write_output("zqsat","zqsat","kg", |
---|
539 | ! & zqsat) |
---|
540 | ! ENDIF |
---|
541 | |
---|
542 | ! IF (ngrid.eq.1) THEN ! 1D |
---|
543 | ! call write_output("error","incertitude sur glace","%", |
---|
544 | ! & error_out) |
---|
545 | call write_output("resist","resistance","s/m2", |
---|
546 | & res_out) |
---|
547 | call write_output("satu_bf","satu before","kg/kg", |
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548 | & satubf) |
---|
549 | call write_output("satu_af","satu after","kg/kg", |
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550 | & satuaf) |
---|
551 | call write_output("vapbf","h2ovap before","kg/kg", |
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552 | & zq0(igcm_h2o_vap)) |
---|
553 | call write_output("vapaf","h2ovap after","kg/kg", |
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554 | & zq(igcm_h2o_vap)) |
---|
555 | call write_output("icebf","h2oice before","kg/kg", |
---|
556 | & zq0(igcm_h2o_ice)) |
---|
557 | call write_output("iceaf","h2oice after","kg/kg", |
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558 | & zq(igcm_h2o_ice)) |
---|
559 | call write_output("ccnbf","ccn before","/kg", |
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560 | & zq0(igcm_ccn_number)) |
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561 | call write_output("ccnaf","ccn after","/kg", |
---|
562 | & zq(igcm_ccn_number)) |
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563 | c call write_output("growthrate","growth rate","m^2/s", |
---|
564 | c & gr_out) |
---|
565 | c call write_output("nuclearate","nucleation rate","", |
---|
566 | c & rate_out) |
---|
567 | c call write_output("dM","ccn variation","kg", |
---|
568 | c & dM_out) |
---|
569 | c call write_output("dN","ccn variation","#", |
---|
570 | c & dN_out) |
---|
571 | call write_output("zqsat","p vap sat","kg/kg", |
---|
572 | & zqsat) |
---|
573 | ! call write_output("satu","ratio saturation","", |
---|
574 | ! & satu_out(:,:)) |
---|
575 | call write_output("rice","ice radius","m", |
---|
576 | & rice) |
---|
577 | ! call write_output("rdust_sca","rdust","m", |
---|
578 | ! & rdust) |
---|
579 | ! call write_output("rsedcloud","rsedcloud","m", |
---|
580 | ! & rsedcloud) |
---|
581 | ! call write_output("rhocloud","rhocloud","kg.m-3", |
---|
582 | ! & rhocloud) |
---|
583 | ! ENDIF |
---|
584 | #endif |
---|
585 | |
---|
586 | ENDIF ! endif test_flag |
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587 | !!!!!!!!!!!!!! TESTS OUTPUTS TESTS OUTPUTS TESTS OUTPUTS TESTS OUTPUTS |
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588 | !!!!!!!!!!!!!! TESTS OUTPUTS TESTS OUTPUTS TESTS OUTPUTS TESTS OUTPUTS |
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589 | !!!!!!!!!!!!!! TESTS OUTPUTS TESTS OUTPUTS TESTS OUTPUTS TESTS OUTPUTS |
---|
590 | |
---|
591 | return |
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592 | |
---|
593 | |
---|
594 | |
---|
595 | |
---|
596 | cccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccc |
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597 | cccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccc |
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598 | c The so -called "phi" function is such as phi(r) - phi(r0) = t - t0 |
---|
599 | c It is an analytical solution to the ice radius growth equation, |
---|
600 | c with the approximation of a constant 'reduced' cunningham correction factor |
---|
601 | c (lambda in growthrate.F) taken at radius req instead of rice |
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602 | cccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccc |
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603 | cccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccc |
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604 | |
---|
605 | c subroutine phi(rice,req,coeff1,coeff2,time) |
---|
606 | c |
---|
607 | c implicit none |
---|
608 | c |
---|
609 | c ! inputs |
---|
610 | c real rice ! ice radius |
---|
611 | c real req ! ice radius at equilibirum |
---|
612 | c real coeff1 ! coeff for the log |
---|
613 | c real coeff2 ! coeff for the arctan |
---|
614 | c |
---|
615 | c ! output |
---|
616 | c real time |
---|
617 | c |
---|
618 | c !local |
---|
619 | c real var |
---|
620 | c |
---|
621 | c ! 1.73205 is sqrt(3) |
---|
622 | c |
---|
623 | c var = max( |
---|
624 | c & abs(rice-req) / sqrt(rice*rice + rice*req + req*req),1e-30) |
---|
625 | c |
---|
626 | c time = |
---|
627 | c & coeff1 * |
---|
628 | c & log( var ) |
---|
629 | c & + coeff2 * 1.73205 * |
---|
630 | c & atan( (2*rice+req) / (1.73205*req) ) |
---|
631 | c |
---|
632 | c return |
---|
633 | c end |
---|
634 | |
---|
635 | |
---|
636 | |
---|
637 | END SUBROUTINE improvedclouds |
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638 | |
---|
639 | END MODULE improvedclouds_mod |
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