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(ngrid,nlay,ptimestep, |
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8 | & pplay,pt,pdt,pq,pdq,nq,tauscaling, |
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9 | & imicro,zt,zq) |
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10 | USE updaterad, ONLY: updaterice_micro, updaterccn |
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11 | USE watersat_mod, ONLY: watersat |
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12 | use tracer_mod, only: rho_ice, nuice_sed, igcm_h2o_vap, |
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13 | & igcm_h2o_ice, igcm_dust_mass, |
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14 | & igcm_dust_number, igcm_ccn_mass, |
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15 | & igcm_ccn_number, |
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16 | & igcm_hdo_vap,igcm_hdo_ice, |
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17 | & qperemin |
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18 | use conc_mod, only: mmean |
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19 | use comcstfi_h, only: pi, cpp |
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20 | use microphys_h, only: nbin_cld, rad_cld, mteta, kbz, nav, rgp |
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21 | use microphys_h, only: mco2, vo1, mh2o, mhdo, molco2, molhdo, To |
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22 | use nuclea_mod, only: nuclea |
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23 | use growthrate_mod, only: growthrate |
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24 | use write_output_mod, only: write_output |
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25 | implicit none |
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26 | |
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27 | |
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28 | c------------------------------------------------------------------ |
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29 | c This routine is used to form clouds when a parcel of the GCM is |
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30 | c saturated. It includes the ability to have supersaturation, a |
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31 | c computation of the nucleation rates, growthrates and the |
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32 | c scavenging of dust particles by clouds. |
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33 | c It is worth noting that the amount of dust is computed using the |
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34 | c dust optical depth computed in aeropacity.F. That's why |
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35 | c the variable called "tauscaling" is used to convert |
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36 | c pq(dust_mass) and pq(dust_number), which are relative |
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37 | c quantities, to absolute and realistic quantities stored in zq. |
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38 | c This has to be done to convert the inputs into absolute |
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39 | c values, but also to convert the outputs back into relative |
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40 | c values which are then used by the sedimentation and advection |
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41 | c schemes. |
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42 | |
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43 | c Authors: J.-B. Madeleine, based on the work by Franck Montmessin |
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44 | c (October 2011) |
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45 | c T. Navarro, debug,correction, new scheme (October-April 2011) |
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46 | c A. Spiga, optimization (February 2012) |
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47 | c J. Naar, adaptative subtimestep now done here (June 2023) |
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48 | c------------------------------------------------------------------ |
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49 | include "callkeys.h" |
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50 | c------------------------------------------------------------------ |
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51 | c Inputs/outputs: |
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52 | |
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53 | INTEGER, INTENT(IN) :: ngrid,nlay |
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54 | INTEGER, INTENT(IN) :: nq ! nombre de traceurs |
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55 | REAL, INTENT(IN) :: ptimestep ! pas de temps physique (s) |
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56 | REAL, INTENT(IN) :: pplay(ngrid,nlay) ! pression au milieu des couches (Pa) |
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57 | REAL, INTENT(IN) :: pt(ngrid,nlay) ! temperature at the middle of the |
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58 | ! layers (K) |
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59 | REAL, INTENT(IN) :: pdt(ngrid,nlay) ! temperature tendency (K/s) |
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60 | REAL, INTENT(IN) :: pq(ngrid,nlay,nq) ! tracer (kg/kg) |
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61 | REAL, INTENT(IN) :: pdq(ngrid,nlay,nq) ! tracer tendency (kg/kg/s) |
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62 | REAL, INTENT(IN) :: tauscaling(ngrid) ! Convertion factor for qdust and Ndust |
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63 | INTEGER, INTENT(IN) :: imicro ! nb. microphy calls(retrocompatibility) |
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64 | |
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65 | REAL, INTENT(OUT) :: zq(ngrid,nlay,nq) ! tracers post microphy (kg/kg) |
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66 | REAL, INTENT(OUT) :: zt(ngrid,nlay) ! temperature post microphy (K) |
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67 | |
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68 | c------------------------------------------------------------------ |
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69 | c Local variables: |
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70 | |
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71 | LOGICAL, SAVE :: firstcall = .true. |
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72 | !$OMP THREADPRIVATE(firstcall) |
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73 | |
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74 | REAL*8 derf ! Error function |
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75 | !external derf |
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76 | |
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77 | INTEGER ig,l,i |
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78 | |
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79 | REAL zqsat(ngrid,nlay) ! saturation |
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80 | REAL lw !Latent heat of sublimation (J.kg-1) |
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81 | REAL cste |
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82 | REAL dMice ! mass of condensed ice |
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83 | REAL dMice_hdo ! mass of condensed HDO ice |
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84 | REAL alpha(ngrid,nlay) ! HDO equilibrium fractionation coefficient (Saturation=1) |
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85 | REAL alpha_c(ngrid,nlay) ! HDO real fractionation coefficient |
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86 | ! REAL sumcheck |
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87 | REAL*8 ph2o ! Water vapor partial pressure (Pa) |
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88 | REAL*8 satu ! Water vapor saturation ratio over ice |
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89 | REAL*8 Mo,No |
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90 | REAL*8 Rn, Rm, dev2, n_derf, m_derf |
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91 | REAL*8 n_aer(nbin_cld) ! number conc. of particle/each size bin |
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92 | REAL*8 m_aer(nbin_cld) ! mass mixing ratio of particle/each size bin |
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93 | |
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94 | REAL*8 sig ! Water-ice/air surface tension (N.m) |
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95 | EXTERNAL sig |
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96 | |
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97 | REAL dN,dM |
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98 | REAL rate(nbin_cld) ! nucleation rate |
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99 | REAL seq |
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100 | |
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101 | REAL rice(ngrid,nlay) ! Ice mass mean radius (m) |
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102 | ! (r_c in montmessin_2004) |
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103 | REAL rhocloud(ngrid,nlay) ! Cloud density (kg.m-3) |
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104 | REAL rdust(ngrid,nlay) ! Dust geometric mean radius (m) |
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105 | |
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106 | REAL res ! Resistance growth |
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107 | REAL Dv,Dv_hdo ! Water/HDO vapor diffusion coefficient |
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108 | |
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109 | |
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110 | c Parameters of the size discretization |
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111 | c used by the microphysical scheme |
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112 | DOUBLE PRECISION, PARAMETER :: rmin_cld = 0.1e-6 ! Minimum radius (m) |
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113 | DOUBLE PRECISION, PARAMETER :: rmax_cld = 10.e-6 ! Maximum radius (m) |
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114 | DOUBLE PRECISION, PARAMETER :: rbmin_cld = 0.0001e-6 |
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115 | ! Minimum boundary radius (m) |
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116 | DOUBLE PRECISION, PARAMETER :: rbmax_cld = 1.e-2 ! Maximum boundary radius (m) |
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117 | DOUBLE PRECISION vrat_cld ! Volume ratio |
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118 | DOUBLE PRECISION, SAVE :: rb_cld(nbin_cld+1)! boundary values of each rad_cld bin (m) |
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119 | !$OMP THREADPRIVATE(rb_cld) |
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120 | |
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121 | DOUBLE PRECISION dr_cld(nbin_cld) ! width of each rad_cld bin (m) |
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122 | DOUBLE PRECISION vol_cld(nbin_cld) ! particle volume for each bin (m3) |
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123 | |
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124 | REAL, SAVE :: sigma_ice ! Variance of the ice and CCN distributions |
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125 | !$OMP THREADPRIVATE(sigma_ice) |
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126 | |
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127 | |
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128 | c---------------------------------- |
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129 | c JN : used in subtimestep |
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130 | REAL :: microtimestep! subdivision of ptimestep (s) |
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131 | REAL :: subpdtcloud(ngrid,nlay) ! Temperature variation due to latent heat |
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132 | REAL :: zq0(ngrid,nlay,nq) ! local initial value of tracers |
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133 | c REAL zt0(ngrid,nlay,nq) ! local initial value of temperature |
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134 | INTEGER :: zimicro(ngrid,nlay) ! Subdivision of ptimestep |
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135 | INTEGER :: count_micro(ngrid,nlay) ! Number of microphys calls |
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136 | REAL :: zpotcond_inst(ngrid,nlay) ! condensable water at the beginning of physics (kg/kg) |
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137 | REAL :: zpotcond_full(ngrid,nlay) ! condensable water with integrated tendancies (kg/kg) |
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138 | REAL :: zpotcond(ngrid,nlay) ! maximal condensable water (previous two) |
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139 | REAL :: zqsat_tmp(1) ! maximal condensable water (previous two) |
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140 | REAL :: spenttime ! time spent in while loop |
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141 | REAL :: zdq ! used to compute adaptative timestep |
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142 | LOGICAL :: ending_ts ! Condition to end while loop |
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143 | |
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144 | |
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145 | c---------------------------------- |
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146 | c TESTS |
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147 | |
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148 | INTEGER countcells |
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149 | |
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150 | LOGICAL, SAVE :: test_flag ! flag for test/debuging outputs |
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151 | !$OMP THREADPRIVATE(test_flag) |
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152 | |
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153 | |
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154 | REAL satubf(ngrid,nlay),satuaf(ngrid,nlay) |
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155 | REAL res_out(ngrid,nlay) |
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156 | |
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157 | |
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158 | c------------------------------------------------------------------ |
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159 | |
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160 | ! AS: firstcall OK absolute |
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161 | IF (firstcall) THEN |
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162 | !============================================================= |
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163 | ! 0. Definition of the size grid |
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164 | !============================================================= |
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165 | c rad_cld is the primary radius grid used for microphysics computation. |
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166 | c The grid spacing is computed assuming a constant volume ratio |
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167 | c between two consecutive bins; i.e. vrat_cld. |
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168 | c vrat_cld is determined from the boundary values of the size grid: |
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169 | c rmin_cld and rmax_cld. |
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170 | c The rb_cld array contains the boundary values of each rad_cld bin. |
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171 | c dr_cld is the width of each rad_cld bin. |
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172 | |
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173 | c Volume ratio between two adjacent bins |
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174 | ! vrat_cld = log(rmax_cld/rmin_cld) / float(nbin_cld-1) *3. |
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175 | ! vrat_cld = exp(vrat_cld) |
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176 | vrat_cld = log(rmax_cld/rmin_cld) / float(nbin_cld-1) *3. |
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177 | vrat_cld = exp(vrat_cld) |
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178 | write(*,*) "vrat_cld", vrat_cld |
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179 | |
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180 | rb_cld(1) = rbmin_cld |
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181 | rad_cld(1) = rmin_cld |
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182 | vol_cld(1) = 4./3. * dble(pi) * rmin_cld*rmin_cld*rmin_cld |
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183 | ! vol_cld(1) = 4./3. * pi * rmin_cld*rmin_cld*rmin_cld |
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184 | |
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185 | do i=1,nbin_cld-1 |
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186 | rad_cld(i+1) = rad_cld(i) * vrat_cld**(1./3.) |
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187 | vol_cld(i+1) = vol_cld(i) * vrat_cld |
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188 | enddo |
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189 | |
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190 | do i=1,nbin_cld |
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191 | rb_cld(i+1)= ( (2.*vrat_cld) / (vrat_cld+1.) )**(1./3.) * |
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192 | & rad_cld(i) |
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193 | dr_cld(i) = rb_cld(i+1) - rb_cld(i) |
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194 | enddo |
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195 | rb_cld(nbin_cld+1) = rbmax_cld |
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196 | dr_cld(nbin_cld) = rb_cld(nbin_cld+1) - rb_cld(nbin_cld) |
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197 | |
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198 | print*, ' ' |
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199 | print*,'Microphysics: size bin information:' |
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200 | print*,'i,rb_cld(i), rad_cld(i),dr_cld(i)' |
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201 | print*,'-----------------------------------' |
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202 | do i=1,nbin_cld |
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203 | write(*,'(i2,3x,3(e12.6,4x))') i,rb_cld(i), rad_cld(i), |
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204 | & dr_cld(i) |
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205 | enddo |
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206 | write(*,'(i2,3x,e12.6)') nbin_cld+1,rb_cld(nbin_cld+1) |
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207 | print*,'-----------------------------------' |
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208 | |
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209 | do i=1,nbin_cld+1 |
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210 | ! rb_cld(i) = log(rb_cld(i)) |
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211 | rb_cld(i) = log(rb_cld(i)) !! we save that so that it is not computed |
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212 | !! at each timestep and gridpoint |
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213 | enddo |
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214 | |
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215 | c Contact parameter of water ice on dust ( m=cos(theta) ) |
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216 | c ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ |
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217 | ! mteta is initialized in conf_phys |
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218 | write(*,*) 'water_param contact parameter:', mteta |
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219 | |
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220 | c Volume of a water molecule (m3) |
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221 | vo1 = mh2o / dble(rho_ice) |
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222 | c Variance of the ice and CCN distributions |
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223 | sigma_ice = sqrt(log(1.+nuice_sed)) |
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224 | |
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225 | |
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226 | write(*,*) 'Variance of ice & CCN distribs :', sigma_ice |
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227 | write(*,*) 'nuice for sedimentation:', nuice_sed |
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228 | write(*,*) 'Volume of a water molecule:', vo1 |
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229 | |
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230 | |
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231 | test_flag = .false. |
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232 | |
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233 | firstcall=.false. |
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234 | END IF |
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235 | |
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236 | |
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237 | !============================================================= |
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238 | ! 1. Initialisation |
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239 | !============================================================= |
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240 | |
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241 | res_out(:,:) = 0 |
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242 | rice(:,:) = 1.e-8 |
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243 | |
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244 | c Initialize the temperature, tracers |
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245 | zt(1:ngrid,1:nlay)=pt(1:ngrid,1:nlay) |
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246 | zq(1:ngrid,1:nlay,1:nq)=pq(1:ngrid,1:nlay,1:nq) |
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247 | subpdtcloud(1:ngrid,1:nlay)=0 |
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248 | |
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249 | WHERE( zq(1:ngrid,1:nlay,1:nq) < 1.e-30 ) |
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250 | & zq(1:ngrid,1:nlay,1:nq) = 1.e-30 |
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251 | |
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252 | |
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253 | !============================================================= |
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254 | ! 2. Compute saturation |
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255 | !============================================================= |
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256 | |
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257 | |
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258 | dev2 = 1. / ( sqrt(2.) * sigma_ice ) |
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259 | |
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260 | c Compute the condensable amount of water vapor |
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261 | c or the sublimable water ice (if negative) |
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262 | call watersat(ngrid*nlay,zt+pdt*ptimestep,pplay,zqsat) |
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263 | zpotcond_full=(zq(:,:,igcm_h2o_vap)+ |
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264 | & pdq(:,:,igcm_h2o_vap)*ptimestep) - zqsat |
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265 | zpotcond_full=max(zpotcond_full,-zq(:,:,igcm_h2o_ice)) |
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266 | call watersat(ngrid*nlay,zt,pplay,zqsat) |
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267 | zpotcond_inst=zq(:,:,igcm_h2o_vap) - zqsat |
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268 | zpotcond_inst=max(zpotcond_inst,-zq(:,:,igcm_h2o_ice)) |
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269 | c zpotcond is the most strict criterion between the two |
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270 | DO l=1,nlay |
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271 | DO ig=1,ngrid |
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272 | if (zpotcond_full(ig,l).gt.0.) then |
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273 | zpotcond(ig,l)=max(zpotcond_inst(ig,l),zpotcond_full(ig,l)) |
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274 | else if (zpotcond_full(ig,l).le.0.) then |
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275 | zpotcond(ig,l)=min(zpotcond_inst(ig,l),zpotcond_full(ig,l)) |
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276 | endif! (zpotcond_full.gt.0.) then |
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277 | ENDDO !ig=1,ngrid |
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278 | ENDDO !l=1,nlay |
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279 | |
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280 | countcells = 0 |
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281 | zimicro(1:ngrid,1:nlay)=imicro |
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282 | count_micro(1:ngrid,1:nlay)=0 |
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283 | |
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284 | c Main loop over the GCM's grid |
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285 | DO l=1,nlay |
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286 | DO ig=1,ngrid |
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287 | c Subtimestep : here we go |
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288 | IF (cloud_adapt_ts) then |
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289 | call adapt_imicro(ptimestep,zpotcond(ig,l), |
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290 | & zimicro(ig,l)) |
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291 | ENDIF! (cloud_adapt_ts) then |
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292 | spenttime = 0. |
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293 | ending_ts=.false. |
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294 | DO while (.not.ending_ts) |
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295 | microtimestep=ptimestep/real(zimicro(ig,l)) |
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296 | c Initialize tracers for scavenging + hdo computations (JN) |
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297 | DO i=1,nq |
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298 | zq0(ig,l,i)=zq(ig,l,i) |
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299 | ENDDO !i=1,nq |
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300 | |
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301 | ! Check if we are integrating over ptimestep |
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302 | if (spenttime+microtimestep.ge.ptimestep) then |
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303 | microtimestep=ptimestep-spenttime |
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304 | ! If so : last call ! |
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305 | ending_ts=.true. |
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306 | endif! (spenttime+microtimestep.ge.ptimestep) then |
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307 | call watersat(1,(/zt(ig,l)/),(/pplay(ig,l)/),zqsat_tmp) |
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308 | zqsat(ig,l)=zqsat_tmp(1) |
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309 | c Get the partial pressure of water vapor and its saturation ratio |
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310 | ph2o = zq(ig,l,igcm_h2o_vap) * (mmean(ig,l)/18.) * pplay(ig,l) |
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311 | satu = zq(ig,l,igcm_h2o_vap) / zqsat(ig,l) |
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312 | |
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313 | !============================================================= |
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314 | ! 3. Nucleation |
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315 | !============================================================= |
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316 | |
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317 | IF ( satu .ge. 1. ) THEN ! if there is condensation |
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318 | |
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319 | call updaterccn(zq(ig,l,igcm_dust_mass), |
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320 | & zq(ig,l,igcm_dust_number),rdust(ig,l),tauscaling(ig)) |
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321 | |
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322 | |
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323 | c Expand the dust moments into a binned distribution |
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324 | Mo = zq(ig,l,igcm_dust_mass)* tauscaling(ig) + 1.e-30 |
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325 | No = zq(ig,l,igcm_dust_number)* tauscaling(ig) + 1.e-30 |
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326 | Rn = rdust(ig,l) |
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327 | Rn = -log(Rn) |
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328 | Rm = Rn - 3. * sigma_ice*sigma_ice |
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329 | n_derf = derf( (rb_cld(1)+Rn) *dev2) |
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330 | m_derf = derf( (rb_cld(1)+Rm) *dev2) |
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331 | do i = 1, nbin_cld |
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332 | n_aer(i) = -0.5 * No * n_derf !! this ith previously computed |
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333 | m_aer(i) = -0.5 * Mo * m_derf !! this ith previously computed |
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334 | n_derf = derf( (rb_cld(i+1)+Rn) *dev2) |
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335 | m_derf = derf( (rb_cld(i+1)+Rm) *dev2) |
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336 | n_aer(i) = n_aer(i) + 0.5 * No * n_derf |
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337 | m_aer(i) = m_aer(i) + 0.5 * Mo * m_derf |
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338 | enddo |
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339 | |
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340 | ! sumcheck = 0 |
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341 | ! do i = 1, nbin_cld |
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342 | ! sumcheck = sumcheck + n_aer(i) |
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343 | ! enddo |
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344 | ! sumcheck = abs(sumcheck/No - 1) |
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345 | ! if ((sumcheck .gt. 1e-5).and. (1./Rn .gt. rmin_cld)) then |
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346 | ! print*, "WARNING, No sumcheck PROBLEM" |
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347 | ! print*, "sumcheck, No",sumcheck, No |
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348 | ! print*, "min radius, Rn, ig, l", rmin_cld, 1./Rn, ig, l |
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349 | ! print*, "Dust binned distribution", n_aer |
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350 | ! endif |
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351 | ! |
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352 | ! sumcheck = 0 |
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353 | ! do i = 1, nbin_cld |
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354 | ! sumcheck = sumcheck + m_aer(i) |
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355 | ! enddo |
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356 | ! sumcheck = abs(sumcheck/Mo - 1) |
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357 | ! if ((sumcheck .gt. 1e-5) .and. (1./Rn .gt. rmin_cld)) then |
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358 | ! print*, "WARNING, Mo sumcheck PROBLEM" |
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359 | ! print*, "sumcheck, Mo",sumcheck, Mo |
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360 | ! print*, "min radius, Rm, ig, l", rmin_cld, 1./Rm, ig, l |
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361 | ! print*, "Dust binned distribution", m_aer |
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362 | ! endif |
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363 | |
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364 | |
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365 | c Get the rates of nucleation |
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366 | call nuclea(ph2o,zt(ig,l),satu,n_aer,rate) |
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367 | |
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368 | dN = 0. |
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369 | dM = 0. |
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370 | do i = 1, nbin_cld |
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371 | dN = dN + n_aer(i)*(exp(-rate(i)*microtimestep)-1.) |
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372 | dM = dM + m_aer(i)*(exp(-rate(i)*microtimestep)-1.) |
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373 | enddo |
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374 | |
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375 | |
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376 | c Update Dust particles |
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377 | zq(ig,l,igcm_dust_mass) = |
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378 | & zq(ig,l,igcm_dust_mass) + dM/ tauscaling(ig) !max(tauscaling(ig),1.e-10) |
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379 | zq(ig,l,igcm_dust_number) = |
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380 | & zq(ig,l,igcm_dust_number) + dN/ tauscaling(ig) !max(tauscaling(ig),1.e-10) |
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381 | c Update CCNs |
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382 | zq(ig,l,igcm_ccn_mass) = |
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383 | & zq(ig,l,igcm_ccn_mass) - dM/ tauscaling(ig) !max(tauscaling(ig),1.e-10) |
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384 | zq(ig,l,igcm_ccn_number) = |
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385 | & zq(ig,l,igcm_ccn_number) - dN/ tauscaling(ig) !max(tauscaling(ig),1.e-10) |
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386 | |
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387 | ENDIF ! of is satu >1 |
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388 | |
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389 | !============================================================= |
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390 | ! 4. Ice growth: scheme for radius evolution |
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391 | !============================================================= |
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392 | |
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393 | c We trigger crystal growth if and only if there is at least one nuclei (N>1). |
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394 | c Indeed, if we are supersaturated and still don't have at least one nuclei, we should better wait |
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395 | c to avoid unrealistic value for nuclei radius and so on for cases that remain negligible. |
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396 | |
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397 | IF ( zq(ig,l,igcm_ccn_number)*tauscaling(ig).ge. 1.) THEN ! we trigger crystal growth |
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398 | |
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399 | call updaterice_micro(zq(ig,l,igcm_h2o_ice), |
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400 | & zq(ig,l,igcm_ccn_mass),zq(ig,l,igcm_ccn_number), |
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401 | & tauscaling(ig),rice(ig,l),rhocloud(ig,l)) |
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402 | |
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403 | No = zq(ig,l,igcm_ccn_number)* tauscaling(ig) + 1.e-30 |
---|
404 | |
---|
405 | c saturation at equilibrium |
---|
406 | c rice should not be too small, otherwise seq value is not valid |
---|
407 | seq = exp(2.*sig(zt(ig,l))*mh2o / (rho_ice*rgp*zt(ig,l)* |
---|
408 | & max(rice(ig,l),1.e-7))) |
---|
409 | |
---|
410 | c get resistance growth |
---|
411 | call growthrate(zt(ig,l),pplay(ig,l), |
---|
412 | & real(ph2o/satu),rice(ig,l),res,Dv) |
---|
413 | |
---|
414 | res_out(ig,l) = res |
---|
415 | |
---|
416 | ccccccc implicit scheme of mass growth |
---|
417 | c cste here must be computed at each step |
---|
418 | cste = 4*pi*rho_ice*microtimestep |
---|
419 | |
---|
420 | dMice = |
---|
421 | & (zq(ig,l,igcm_h2o_vap)-seq*zqsat(ig,l)) |
---|
422 | & /(res*zqsat(ig,l)/(cste*No*rice(ig,l)) + 1.) |
---|
423 | |
---|
424 | |
---|
425 | ! With the above scheme, dMice cannot be bigger than vapor, |
---|
426 | ! but can be bigger than all available ice. |
---|
427 | dMice = max(dMice,-zq(ig,l,igcm_h2o_ice)) |
---|
428 | dMice = min(dMice,zq(ig,l,igcm_h2o_vap)) ! this should be useless... |
---|
429 | |
---|
430 | zq(ig,l,igcm_h2o_ice) = zq(ig,l,igcm_h2o_ice)+dMice |
---|
431 | zq(ig,l,igcm_h2o_vap) = zq(ig,l,igcm_h2o_vap)-dMice |
---|
432 | |
---|
433 | |
---|
434 | countcells = countcells + 1 |
---|
435 | |
---|
436 | ! latent heat release |
---|
437 | lw=(2834.3-0.28*(zt(ig,l)-To)- |
---|
438 | & 0.004*(zt(ig,l)-To)*(zt(ig,l)-To))*1.e+3 |
---|
439 | subpdtcloud(ig,l)= dMice*lw/cpp/microtimestep |
---|
440 | |
---|
441 | c Special case of the isotope of water HDO |
---|
442 | if (hdo) then |
---|
443 | !! condensation |
---|
444 | if (dMice.gt.0.0) then |
---|
445 | !! do we use fractionation? |
---|
446 | if (hdofrac) then |
---|
447 | !! Calculation of the HDO vapor coefficient |
---|
448 | Dv_hdo = 1./3. * sqrt( 8*kbz*zt(ig,l)/(pi*mhdo/nav) ) |
---|
449 | & * kbz * zt(ig,l) / |
---|
450 | & ( pi * pplay(ig,l) * (molco2+molhdo)*(molco2+molhdo) |
---|
451 | & * sqrt(1.+mhdo/mco2) ) |
---|
452 | !! Calculation of the fractionnation coefficient at equilibrium |
---|
453 | alpha(ig,l) = exp(16288./zt(ig,l)**2.-9.34d-2) |
---|
454 | c alpha = exp(13525./zt(ig,l)**2.-5.59d-2) !Lamb |
---|
455 | !! Calculation of the 'real' fractionnation coefficient |
---|
456 | alpha_c(ig,l) = (alpha(ig,l)*satu)/ |
---|
457 | & ( (alpha(ig,l)*(Dv/Dv_hdo)*(satu-1.)) + 1.) |
---|
458 | c alpha_c(ig,l) = alpha(ig,l) ! to test without the effect of cinetics |
---|
459 | else |
---|
460 | alpha_c(ig,l) = 1.d0 |
---|
461 | endif |
---|
462 | if (zq0(ig,l,igcm_h2o_vap).gt.qperemin) then |
---|
463 | dMice_hdo= |
---|
464 | & dMice*alpha_c(ig,l)* |
---|
465 | & ( zq0(ig,l,igcm_hdo_vap) |
---|
466 | & /zq0(ig,l,igcm_h2o_vap) ) |
---|
467 | else |
---|
468 | dMice_hdo=0. |
---|
469 | endif |
---|
470 | !! sublimation |
---|
471 | else |
---|
472 | if (zq0(ig,l,igcm_h2o_ice).gt.qperemin) then |
---|
473 | dMice_hdo= |
---|
474 | & dMice* |
---|
475 | & ( zq0(ig,l,igcm_hdo_ice) |
---|
476 | & /zq0(ig,l,igcm_h2o_ice) ) |
---|
477 | else |
---|
478 | dMice_hdo=0. |
---|
479 | endif |
---|
480 | endif !if (dMice.gt.0.0) |
---|
481 | |
---|
482 | dMice_hdo = max(dMice_hdo,-zq(ig,l,igcm_hdo_ice)) |
---|
483 | dMice_hdo = min(dMice_hdo,zq(ig,l,igcm_hdo_vap)) |
---|
484 | |
---|
485 | zq(ig,l,igcm_hdo_ice) = zq(ig,l,igcm_hdo_ice)+dMice_hdo |
---|
486 | zq(ig,l,igcm_hdo_vap) = zq(ig,l,igcm_hdo_vap)-dMice_hdo |
---|
487 | |
---|
488 | endif ! if (hdo) |
---|
489 | |
---|
490 | !============================================================= |
---|
491 | ! 5. Dust cores released, tendancies, latent heat, etc ... |
---|
492 | !============================================================= |
---|
493 | |
---|
494 | c If all the ice particles sublimate, all the condensation |
---|
495 | c nuclei are released: |
---|
496 | if (zq(ig,l,igcm_h2o_ice).le.1.e-28) then |
---|
497 | |
---|
498 | c Water |
---|
499 | zq(ig,l,igcm_h2o_vap) = zq(ig,l,igcm_h2o_vap) |
---|
500 | & + zq(ig,l,igcm_h2o_ice) |
---|
501 | zq(ig,l,igcm_h2o_ice) = 0. |
---|
502 | if (hdo) then |
---|
503 | zq(ig,l,igcm_hdo_vap) = zq(ig,l,igcm_hdo_vap) |
---|
504 | & + zq(ig,l,igcm_hdo_ice) |
---|
505 | zq(ig,l,igcm_hdo_ice) = 0. |
---|
506 | endif |
---|
507 | c Dust particles |
---|
508 | zq(ig,l,igcm_dust_mass) = zq(ig,l,igcm_dust_mass) |
---|
509 | & + zq(ig,l,igcm_ccn_mass) |
---|
510 | zq(ig,l,igcm_dust_number) = zq(ig,l,igcm_dust_number) |
---|
511 | & + zq(ig,l,igcm_ccn_number) |
---|
512 | c CCNs |
---|
513 | zq(ig,l,igcm_ccn_mass) = 0. |
---|
514 | zq(ig,l,igcm_ccn_number) = 0. |
---|
515 | |
---|
516 | endif |
---|
517 | |
---|
518 | ENDIF !of if Nccn>1 |
---|
519 | |
---|
520 | |
---|
521 | ! No more getting tendency : we increment tracers & temp directly |
---|
522 | |
---|
523 | ! Increment tracers & temp for following microtimestep |
---|
524 | ! Dust : |
---|
525 | ! Special treatment of dust_mass / number for scavenging ? |
---|
526 | IF (scavenging) THEN |
---|
527 | zq(ig,l,igcm_dust_mass) =zq(ig,l,igcm_dust_mass)+ |
---|
528 | & pdq(ig,l,igcm_dust_mass)*microtimestep |
---|
529 | zq(ig,l,igcm_dust_number) =zq(ig,l,igcm_dust_number)+ |
---|
530 | & pdq(ig,l,igcm_dust_number)*microtimestep |
---|
531 | ELSE |
---|
532 | zq(ig,l,igcm_dust_mass) =zq0(ig,l,igcm_dust_mass) |
---|
533 | zq(ig,l,igcm_dust_number) =zq0(ig,l,igcm_dust_number) |
---|
534 | ENDIF !(scavenging) THEN |
---|
535 | zq(ig,l,igcm_ccn_mass) = zq(ig,l,igcm_ccn_mass) + |
---|
536 | & pdq(ig,l,igcm_ccn_mass)*microtimestep |
---|
537 | zq(ig,l,igcm_ccn_number) = zq(ig,l,igcm_ccn_number) + |
---|
538 | & pdq(ig,l,igcm_ccn_number)*microtimestep |
---|
539 | |
---|
540 | ! Water : |
---|
541 | zq(ig,l,igcm_h2o_ice) = zq(ig,l,igcm_h2o_ice)+ |
---|
542 | & pdq(ig,l,igcm_h2o_ice)*microtimestep |
---|
543 | zq(ig,l,igcm_h2o_vap) = zq(ig,l,igcm_h2o_vap)+ |
---|
544 | & pdq(ig,l,igcm_h2o_vap)*microtimestep |
---|
545 | |
---|
546 | ! HDO (if computed) : |
---|
547 | IF (hdo) THEN |
---|
548 | zq(ig,l,igcm_hdo_ice) = |
---|
549 | & zq(ig,l,igcm_hdo_ice)+ |
---|
550 | & pdq(ig,l,igcm_hdo_ice)*microtimestep |
---|
551 | zq(ig,l,igcm_hdo_vap) = |
---|
552 | & zq(ig,l,igcm_hdo_vap)+ |
---|
553 | & pdq(ig,l,igcm_hdo_vap)*microtimestep |
---|
554 | ENDIF ! hdo |
---|
555 | |
---|
556 | c Could also set subpdtcloud to 0 if not activice to make it simpler |
---|
557 | c or change name of the flag |
---|
558 | IF (.not.activice) THEN |
---|
559 | subpdtcloud(ig,l)=0. |
---|
560 | ENDIF |
---|
561 | ! Temperature : |
---|
562 | zt(ig,l) = zt(ig,l)+(pdt(ig,l)+ |
---|
563 | & subpdtcloud(ig,l))*microtimestep |
---|
564 | |
---|
565 | c Prevent negative tracers ! JN |
---|
566 | DO i=1,nq |
---|
567 | IF(zq(ig,l,i).lt.1.e-30) zq(ig,l,i)=1.e-30 |
---|
568 | ENDDO !i=1,nq |
---|
569 | |
---|
570 | IF (cloud_adapt_ts) then |
---|
571 | c Estimation of how much is actually condensing/subliming |
---|
572 | zdq=(dMice/spenttime)*(ptimestep-spenttime) |
---|
573 | c Threshold with powerlaw (sanity check) |
---|
574 | zdq=min(abs(zdq), |
---|
575 | & abs(zpotcond(ig,l)*((ptimestep-spenttime)/ptimestep))) |
---|
576 | call adapt_imicro(ptimestep,zdq, |
---|
577 | & zimicro(ig,l)) |
---|
578 | ENDIF! (cloud_adapt_ts) then |
---|
579 | c Increment time spent in here |
---|
580 | spenttime=spenttime+microtimestep |
---|
581 | count_micro(ig,l)=count_micro(ig,l)+1 |
---|
582 | ENDDO ! while (.not. ending_ts) |
---|
583 | ENDDO ! of ig loop |
---|
584 | ENDDO ! of nlayer loop |
---|
585 | |
---|
586 | |
---|
587 | c------ Useful outputs to check how it went |
---|
588 | call write_output("zpotcond_inst","zpotcond_inst "// |
---|
589 | & "microphysics","(kg/kg)",zpotcond_inst(:,:)) |
---|
590 | call write_output("zpotcond_full","zpotcond_full "// |
---|
591 | & "microphysics","(kg/kg)",zpotcond_full(:,:)) |
---|
592 | call write_output("zpotcond","zpotcond "// |
---|
593 | & "microphysics","(kg/kg)",zpotcond(:,:)) |
---|
594 | call write_output("count_micro","count_micro "// |
---|
595 | & "after microphysics","integer",count_micro(:,:)) |
---|
596 | |
---|
597 | |
---|
598 | |
---|
599 | !!!!!!!!!!!!!! TESTS OUTPUTS TESTS OUTPUTS TESTS OUTPUTS TESTS OUTPUTS |
---|
600 | !!!!!!!!!!!!!! TESTS OUTPUTS TESTS OUTPUTS TESTS OUTPUTS TESTS OUTPUTS |
---|
601 | !!!!!!!!!!!!!! TESTS OUTPUTS TESTS OUTPUTS TESTS OUTPUTS TESTS OUTPUTS |
---|
602 | IF (test_flag) then |
---|
603 | |
---|
604 | ! error2d(:) = 0. |
---|
605 | DO l=1,nlay |
---|
606 | DO ig=1,ngrid |
---|
607 | ! error2d(ig) = max(abs(error_out(ig,l)),error2d(ig)) |
---|
608 | satubf(ig,l) = zq0(ig,l,igcm_h2o_vap)/zqsat(ig,l) |
---|
609 | satuaf(ig,l) = zq(ig,l,igcm_h2o_vap)/zqsat(ig,l) |
---|
610 | ENDDO |
---|
611 | ENDDO |
---|
612 | |
---|
613 | print*, 'count is ',countcells, ' i.e. ', |
---|
614 | & countcells*100/(nlay*ngrid), '% for microphys computation' |
---|
615 | |
---|
616 | #ifndef MESOSCALE |
---|
617 | ! IF (ngrid.ne.1) THEN ! 3D |
---|
618 | ! call WRITEDIAGFI(ngrid,"satu","ratio saturation","",3, |
---|
619 | ! & satu_out) |
---|
620 | ! call WRITEDIAGFI(ngrid,"dM","ccn variation","kg/kg",3, |
---|
621 | ! & dM_out) |
---|
622 | ! call WRITEDIAGFI(ngrid,"dN","ccn variation","#",3, |
---|
623 | ! & dN_out) |
---|
624 | ! call WRITEDIAGFI(ngrid,"error","dichotomy max error","%",2, |
---|
625 | ! & error2d) |
---|
626 | ! call WRITEDIAGFI(ngrid,"zqsat","zqsat","kg",3, |
---|
627 | ! & zqsat) |
---|
628 | ! ENDIF |
---|
629 | |
---|
630 | ! IF (ngrid.eq.1) THEN ! 1D |
---|
631 | ! call WRITEDIAGFI(ngrid,"error","incertitude sur glace","%",1, |
---|
632 | ! & error_out) |
---|
633 | call WRITEdiagfi(ngrid,"resist","resistance","s/m2",1, |
---|
634 | & res_out) |
---|
635 | call WRITEdiagfi(ngrid,"satu_bf","satu before","kg/kg",1, |
---|
636 | & satubf) |
---|
637 | call WRITEdiagfi(ngrid,"satu_af","satu after","kg/kg",1, |
---|
638 | & satuaf) |
---|
639 | call WRITEdiagfi(ngrid,"vapbf","h2ovap before","kg/kg",1, |
---|
640 | & zq0(1,1,igcm_h2o_vap)) |
---|
641 | call WRITEdiagfi(ngrid,"vapaf","h2ovap after","kg/kg",1, |
---|
642 | & zq(1,1,igcm_h2o_vap)) |
---|
643 | call WRITEdiagfi(ngrid,"icebf","h2oice before","kg/kg",1, |
---|
644 | & zq0(1,1,igcm_h2o_ice)) |
---|
645 | call WRITEdiagfi(ngrid,"iceaf","h2oice after","kg/kg",1, |
---|
646 | & zq(1,1,igcm_h2o_ice)) |
---|
647 | call WRITEdiagfi(ngrid,"ccnbf","ccn before","/kg",1, |
---|
648 | & zq0(1,1,igcm_ccn_number)) |
---|
649 | call WRITEdiagfi(ngrid,"ccnaf","ccn after","/kg",1, |
---|
650 | & zq(1,1,igcm_ccn_number)) |
---|
651 | c call WRITEDIAGFI(ngrid,"growthrate","growth rate","m^2/s",1, |
---|
652 | c & gr_out) |
---|
653 | c call WRITEDIAGFI(ngrid,"nuclearate","nucleation rate","",1, |
---|
654 | c & rate_out) |
---|
655 | c call WRITEDIAGFI(ngrid,"dM","ccn variation","kg",1, |
---|
656 | c & dM_out) |
---|
657 | c call WRITEDIAGFI(ngrid,"dN","ccn variation","#",1, |
---|
658 | c & dN_out) |
---|
659 | call WRITEdiagfi(ngrid,"zqsat","p vap sat","kg/kg",1, |
---|
660 | & zqsat) |
---|
661 | ! call WRITEDIAGFI(ngrid,"satu","ratio saturation","",1, |
---|
662 | ! & satu_out) |
---|
663 | call WRITEdiagfi(ngrid,"rice","ice radius","m",1, |
---|
664 | & rice) |
---|
665 | ! call WRITEDIAGFI(ngrid,"rdust_sca","rdust","m",1, |
---|
666 | ! & rdust) |
---|
667 | ! call WRITEDIAGFI(ngrid,"rsedcloud","rsedcloud","m",1, |
---|
668 | ! & rsedcloud) |
---|
669 | ! call WRITEDIAGFI(ngrid,"rhocloud","rhocloud","kg.m-3",1, |
---|
670 | ! & rhocloud) |
---|
671 | ! ENDIF |
---|
672 | #endif |
---|
673 | |
---|
674 | ENDIF ! endif test_flag |
---|
675 | !!!!!!!!!!!!!! TESTS OUTPUTS TESTS OUTPUTS TESTS OUTPUTS TESTS OUTPUTS |
---|
676 | !!!!!!!!!!!!!! TESTS OUTPUTS TESTS OUTPUTS TESTS OUTPUTS TESTS OUTPUTS |
---|
677 | !!!!!!!!!!!!!! TESTS OUTPUTS TESTS OUTPUTS TESTS OUTPUTS TESTS OUTPUTS |
---|
678 | |
---|
679 | return |
---|
680 | |
---|
681 | |
---|
682 | |
---|
683 | |
---|
684 | cccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccc |
---|
685 | cccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccc |
---|
686 | c The so -called "phi" function is such as phi(r) - phi(r0) = t - t0 |
---|
687 | c It is an analytical solution to the ice radius growth equation, |
---|
688 | c with the approximation of a constant 'reduced' cunningham correction factor |
---|
689 | c (lambda in growthrate.F) taken at radius req instead of rice |
---|
690 | cccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccc |
---|
691 | cccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccccc |
---|
692 | |
---|
693 | c subroutine phi(rice,req,coeff1,coeff2,time) |
---|
694 | c |
---|
695 | c implicit none |
---|
696 | c |
---|
697 | c ! inputs |
---|
698 | c real rice ! ice radius |
---|
699 | c real req ! ice radius at equilibirum |
---|
700 | c real coeff1 ! coeff for the log |
---|
701 | c real coeff2 ! coeff for the arctan |
---|
702 | c |
---|
703 | c ! output |
---|
704 | c real time |
---|
705 | c |
---|
706 | c !local |
---|
707 | c real var |
---|
708 | c |
---|
709 | c ! 1.73205 is sqrt(3) |
---|
710 | c |
---|
711 | c var = max( |
---|
712 | c & abs(rice-req) / sqrt(rice*rice + rice*req + req*req),1e-30) |
---|
713 | c |
---|
714 | c time = |
---|
715 | c & coeff1 * |
---|
716 | c & log( var ) |
---|
717 | c & + coeff2 * 1.73205 * |
---|
718 | c & atan( (2*rice+req) / (1.73205*req) ) |
---|
719 | c |
---|
720 | c return |
---|
721 | c end |
---|
722 | |
---|
723 | |
---|
724 | |
---|
725 | END SUBROUTINE improvedclouds |
---|
726 | |
---|
727 | SUBROUTINE adapt_imicro(ptimestep,potcond, |
---|
728 | $ zimicro) |
---|
729 | |
---|
730 | c Adaptative timestep for water ice clouds. |
---|
731 | c Works using a powerlaw to compute the minimal duration of subtimestep |
---|
732 | c (in s) should all the avalaible vapor (resp. ice) condenses (resp.sublimates) |
---|
733 | c Then, we use the instantaneous vap (ice) gradient extrapolated to the |
---|
734 | c rest of duration to increase subtimestep duration, for computing |
---|
735 | c efficiency. |
---|
736 | |
---|
737 | real,intent(in) :: ptimestep ! total duration of physics (sec) |
---|
738 | real,intent(in) :: potcond ! condensible vapor / sublimable ice(kg/kg) |
---|
739 | real :: alpha, beta ! Coefficients for power law |
---|
740 | integer,intent(out) :: zimicro ! number of ptimestep division |
---|
741 | |
---|
742 | c zimicro = 30 |
---|
743 | c Coefficients good enough for present-day Mars : |
---|
744 | c alpha = 1.87485684e+09 |
---|
745 | c beta = 1.45655856e+00 |
---|
746 | c Coefficients covering high obliquity scenarios : |
---|
747 | alpha=3.36711332e+15 |
---|
748 | beta=1.98636414e+00 |
---|
749 | c nimicro=min(max(alpha*abs(potcond)**beta,5.),7000.) |
---|
750 | c zimicro=ceiling((ptimestep/timeleft)*nimicro) |
---|
751 | c zimicro=ceiling((timeleft/ptimestep)*nimicro) |
---|
752 | zimicro=ceiling(min(max(alpha*abs(potcond)**beta,5.),7000.)) |
---|
753 | |
---|
754 | END SUBROUTINE adapt_imicro |
---|
755 | |
---|
756 | END MODULE improvedclouds_mod |
---|