1 | MODULE callradite_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 callradite(icount,ngrid,nlayer,nq,zday,ls,pq,albedo, |
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8 | $ emis,mu0,pplev,pplay,pt,tsurf,fract,dist_sol,igout, |
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9 | $ dtlw,dtsw,fluxsurf_lw,fluxsurf_dn_sw,fluxsurf_up_sw, |
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10 | $ fluxtop_lw,fluxtop_dn_sw,fluxtop_up_sw, |
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11 | & tau_pref_scenario,tau_pref_gcm, |
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12 | & tau,aerosol,dsodust,tauscaling,dust_rad_adjust,IRtoVIScoef, |
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13 | $ taucloudtes,rdust,rice,nuice,riceco2,nuiceco2,co2ice, |
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14 | $ rstormdust,rtopdust,totstormfract,clearatm,dsords,dsotop, |
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15 | $ nohmons,clearsky,totcloudfrac) |
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16 | |
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17 | use aeropacity_mod, only: aeropacity |
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18 | use updatereffrad_mod, only: updatereffrad |
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19 | use dimradmars_mod, only: ndomainsz, nflev, nsun, nir |
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20 | use dimradmars_mod, only: naerkind, name_iaer, |
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21 | & iaer_dust_conrath,iaer_dust_doubleq, |
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22 | & iaer_dust_submicron, iaer_h2o_ice, iaer_co2_ice, |
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23 | & iaer_stormdust_doubleq,iaer_topdust_doubleq,flux_1AU |
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24 | use yomlw_h, only: gcp, nlaylte |
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25 | use comcstfi_h, only: g,cpp |
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26 | use time_phylmdz_mod, only: daysec |
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27 | use lwmain_mod, only: lwmain |
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28 | use swmain_mod, only: swmain |
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29 | use dust_param_mod, only: doubleq, active, submicron |
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30 | IMPLICIT NONE |
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31 | c======================================================================= |
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32 | c subject: |
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33 | c -------- |
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34 | c Subroutine designed to call the main canonic |
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35 | c radiative transfer subroutine "lwmain" et "swmain" |
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36 | c to compute radiative heating and cooling rate and |
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37 | c radiative fluxes to the surface. |
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38 | c |
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39 | c These calculations are only valid on the part of the atmosphere |
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40 | c where Local Thermal Equilibrium (LTE) is verified. In practice |
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41 | c the calculations are only performed for the first "nlaylte" |
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42 | c parameters (nlaylte is calculated by subroutine "nlthermeq" |
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43 | c and stored in module "yomlw_h"). |
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44 | c |
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45 | c The purpose of this subroutine is to: |
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46 | c 1) Make some initial calculation at first call |
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47 | c 2) Split the calculation in several sub-grid |
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48 | c ("sub-domain") to save memory and |
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49 | c be able run on a workstation at high resolution |
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50 | c The sub-grid size is defined in dimradmars_mod |
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51 | c 3) Compute the 3D scattering parameters depending on the |
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52 | c size distribution of the different tracers (added by JBM) |
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53 | c 4) call "lwmain" and "swmain" |
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54 | c |
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55 | c |
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56 | c authors: |
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57 | c ------ |
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58 | c Francois Forget / Christophe Hourdin / J.-B. Madeleine (2009) |
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59 | c |
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60 | c |
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61 | c 3D scattering scheme user's guide (J.-B. Madeleine) |
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62 | c --------------------------------- |
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63 | c |
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64 | c This routine has been modified to take into account 3D, time |
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65 | c dependent scattering properties of the aerosols. |
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66 | c---- The look-up tables that contain the scattering parameters |
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67 | c of a given tracer, for different sizes, are read by SUAER.F90. |
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68 | c The names of the corresponding ASCII files have to be set in |
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69 | c this subroutine (file_id variable), and files must be in the |
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70 | c directory specified in datafile_mod. Please make sure that the |
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71 | c ASCII files are correctly written, and that the range |
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72 | c of particle sizes is consistent with what you would expect. |
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73 | c---- SUAER.F90 is in charge of reading the ASCII files and averaging |
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74 | c the scattering parameters in each GCM channel, using the three last |
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75 | c equations of Forget et al. 1998 (GRL 25, No.7, p.1105-1108). |
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76 | c---- These look-up tables, loaded during the firstcall, are then |
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77 | c constantly used by the subroutine "aeroptproperties.F" to compute, |
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78 | c online, the 3D scattering parameters, based on the size distribution |
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79 | c (reffrad and nueffrad) of the different tracers, in each grid box. |
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80 | c These 3D size distributions are loaded by the "updatereffrad.F" |
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81 | c subroutine. A log-normal distribution is then assumed in |
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82 | c "aeroptproperties.F", along with a Gauss-Legendre integration. |
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83 | c---- The optical depth at the visible reference wavelength (set in |
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84 | c SUAER.F90, after the file_id variable) is then computed by |
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85 | c the subroutine "aeropacity.F", by using the size and spatial |
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86 | c distribution of the corresponding tracer. This connection has to |
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87 | c be implemented in "aeropacity.F" when adding a new tracer. To do so, |
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88 | c one can use equation 2 of Forget et al. 1998 (Icarus 131, p.302-316). |
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89 | c---- The resulting variables "aerosol", "QVISsQREF3d", "omegaVIS3d" and |
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90 | c "gVIS3d" (same in the infrared) are finally used by lwmain.F and |
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91 | c swmain.F to solve the radiative transfer equation. |
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92 | c |
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93 | c changes: |
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94 | c ------- |
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95 | c |
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96 | c > SRL 7/2000 |
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97 | c |
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98 | c This version has been modified to only calculate radiative tendencies |
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99 | c over layers 1..NFLEV (set in dimradmars_mod). Returns zero for higher |
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100 | c layers, if any. |
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101 | c In other routines, nlayer -> nflev. |
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102 | c Routines affected: lwflux, lwi, lwmain, lwxb, lwxd, lwxn. |
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103 | c |
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104 | c > J.-B. Madeleine 10W12 |
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105 | c This version uses the variable's splitting, which can be usefull |
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106 | c when performing very high resolution simulation like LES. |
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107 | c |
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108 | c ---------- |
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109 | c Here, solar band#1 is spectral interval between "long1vis" and "long2vis" |
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110 | c set in dimradmars_mod |
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111 | c Here, solar band#2 is spectral interval between "long2vis" and "long3vis" |
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112 | c set in dimradmars_mod |
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113 | c |
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114 | c input: |
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115 | c ----- |
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116 | c icount counter of call to subroutine physic by gcm |
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117 | c ngrid number of gridpoint of horizontal grid |
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118 | c nlayer Number of layer |
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119 | c nq Number of tracer |
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120 | c ls Solar longitude (Ls) , radian |
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121 | c zday Date (time since Ls=0, in martian days) |
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122 | c pq(ngrid,nlayer,nq) Advected fields |
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123 | c |
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124 | c albedo (ngrid,2) hemispheric surface albedo |
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125 | c albedo (i,1) : mean albedo for solar band#1 |
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126 | c (see below) |
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127 | c albedo (i,2) : mean albedo for solar band#2 |
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128 | c (see below) |
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129 | c emis Thermal IR surface emissivity (no unit) |
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130 | c mu0(ngrid) cos of solar zenith angle |
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131 | c (=1 when sun at zenith) |
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132 | c pplay(ngrid,nlayer) pressure (Pa) in the middle of each layer |
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133 | c pplev(ngrid,nlayer+1) pressure (Pa) at boundaries of each layer |
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134 | c pt(ngrid,nlayer) atmospheric temperature in each layer (K) |
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135 | c tsurf(ngrid) surface temperature (K) |
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136 | c fract(ngrid) day fraction of the time interval |
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137 | c =1 during the full day ; =0 during the night |
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138 | c declin latitude of subsolar point |
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139 | c dist_sol sun-Mars distance (AU) |
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140 | c igout coordinate of analysed point for debugging |
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141 | c reffrad(ngrid,nlayer,naerkind) Aerosol effective radius |
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142 | c nueffrad(ngrid,nlayer,naerkind) Aerosol effective variance |
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143 | |
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144 | c======================================================================= |
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145 | c |
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146 | c Declarations : |
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147 | c ------------- |
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148 | c |
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149 | include "callkeys.h" |
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150 | |
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151 | c----------------------------------------------------------------------- |
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152 | c Input/Output |
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153 | c ------------ |
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154 | INTEGER,INTENT(IN) :: icount |
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155 | INTEGER,INTENT(IN) :: ngrid,nlayer,nq |
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156 | INTEGER,INTENT(IN) :: igout |
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157 | |
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158 | REAL,INTENT(IN) :: pq(ngrid,nlayer,nq) |
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159 | REAL,INTENT(INOUT) :: tauscaling(ngrid) ! Conversion factor for |
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160 | ! qdust and Ndust |
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161 | REAL,INTENT(INOUT) :: dust_rad_adjust(ngrid) ! Radiative adjustment |
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162 | ! factor for dust |
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163 | REAL,INTENT(INOUT) :: IRtoVIScoef(ngrid) ! conversion coefficient to apply on |
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164 | ! scenario absorption IR (9.3um) CDOD |
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165 | ! = tau_pref_gcm_VIS / tau_pref_gcm_IR |
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166 | REAL,INTENT(IN) :: albedo(ngrid,2),emis(ngrid) |
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167 | REAL,INTENT(IN) :: ls,zday |
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168 | |
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169 | REAL,INTENT(IN) :: pplev(ngrid,nlayer+1),pplay(ngrid,nlayer) |
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170 | REAL,INTENT(IN) :: pt(ngrid,nlayer) |
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171 | REAL,INTENT(IN) :: tsurf(ngrid) |
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172 | REAL,INTENT(IN) :: dist_sol,mu0(ngrid),fract(ngrid) |
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173 | REAL,INTENT(OUT) :: dtlw(ngrid,nlayer) ! longwave (IR) heating rate (K/s) |
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174 | REAL,INTENT(OUT) :: dtsw(ngrid,nlayer) ! shortwave (Solar) heating rate (K/s) |
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175 | REAL,INTENT(OUT) :: fluxsurf_lw(ngrid) ! total LW (thermal IR) downward flux |
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176 | ! (W.m-2) at the surface |
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177 | REAL,INTENT(OUT) :: fluxtop_lw(ngrid) ! outgoing total LW (thermal IR) |
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178 | ! upward flux (W.m-2) at the top of the atm. |
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179 | REAL,INTENT(OUT) :: fluxsurf_dn_sw(ngrid,2) ! surface downward SW flux for |
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180 | ! solar bands #1 and #2 (W.m-2) |
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181 | REAL,INTENT(OUT) :: fluxsurf_up_sw(ngrid,2) ! surface upward SW flux for |
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182 | ! solar bands #1 and #2 (W.m-2) |
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183 | REAL,INTENT(OUT) :: fluxtop_dn_sw(ngrid,2) ! incoming downward SW flux for |
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184 | ! solar bands #1 and #2 (W.m-2) at top of atm. |
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185 | REAL,INTENT(OUT) :: fluxtop_up_sw(ngrid,2) ! outgoing upward SW flux for |
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186 | ! solar bands #1 and #2 (W.m-2) at top of atm. |
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187 | REAL,INTENT(OUT) :: tau_pref_scenario(ngrid) ! prescribed dust column |
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188 | ! visible opacity at odpref from scenario |
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189 | REAL,INTENT(OUT) :: tau_pref_gcm(ngrid) ! computed dust column |
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190 | ! visible opacity at odpref in the GCM |
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191 | REAL,INTENT(OUT) :: tau(ngrid,naerkind) ! Column visible optical depth |
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192 | ! for each aerosol |
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193 | REAL,INTENT(OUT) :: taucloudtes(ngrid)! Cloud opacity at infrared |
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194 | ! reference wavelength using |
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195 | ! Qabs instead of Qext |
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196 | ! (direct comparison with TES) |
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197 | REAL,INTENT(OUT) :: aerosol(ngrid,nlayer,naerkind) ! aerosol extinction |
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198 | ! optical depth at reference wavelength "longrefvis", |
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199 | ! set in dimradmars_h, for each kind of aerosol |
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200 | REAL,INTENT(INOUT) :: dsodust(ngrid,nlayer) |
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201 | REAL,INTENT(OUT) :: rdust(ngrid,nlayer) ! Dust geometric mean radius (m) |
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202 | REAL,INTENT(OUT) :: rice(ngrid,nlayer) ! Ice geometric mean radius (m) |
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203 | REAL,INTENT(OUT) :: nuice(ngrid,nlayer) ! Estimated effective variance |
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204 | double precision,INTENT(OUT) :: riceco2(ngrid,nlayer) ! CO2 ice mean radius(m) |
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205 | REAL,INTENT(OUT) :: nuiceco2(ngrid,nlayer) ! Effective variance |
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206 | REAL,INTENT(IN) :: co2ice(ngrid) ! co2 ice surface layer (kg.m-2) |
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207 | |
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208 | c rocket dust storm |
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209 | LOGICAL,INTENT(IN) :: clearatm ! true for background dust |
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210 | REAL,INTENT(IN) :: totstormfract(ngrid) ! dust storm mesh fraction |
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211 | REAL,INTENT(OUT) :: rstormdust(ngrid,nlayer) ! Storm dust geometric mean radius (m) |
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212 | REAL,INTENT(OUT) :: dsords(ngrid,nlayer) ! density scaled opacity for rocket dust storm dust |
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213 | |
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214 | c entrainment by mountain top dust flows |
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215 | LOGICAL, INTENT(IN) :: nohmons ! true for background dust |
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216 | REAL,INTENT(OUT) :: rtopdust(ngrid,nlayer) ! Topdust geometric mean radius (m) |
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217 | REAL,INTENT(OUT) :: dsotop(ngrid,nlayer) ! density scaled opacity for topmons dust |
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218 | |
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219 | c sub-grid scale water ice clouds |
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220 | LOGICAL,INTENT(IN) :: clearsky |
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221 | REAL,INTENT(IN) :: totcloudfrac(ngrid) |
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222 | |
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223 | c |
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224 | c Local variables : |
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225 | c ----------------- |
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226 | |
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227 | INTEGER j,l,ig,n,ich |
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228 | INTEGER aer_count,iaer |
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229 | INTEGER jd,ig0,nd |
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230 | |
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231 | real cste_mars ! solar constant on Mars (Wm-2) |
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232 | REAL ptlev(ngrid,nlayer+1) |
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233 | |
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234 | INTEGER :: ndomain |
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235 | |
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236 | c Thermal IR net radiative budget (W m-2) |
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237 | |
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238 | real znetrad(ndomainsz,nflev) |
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239 | |
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240 | real zfluxd_sw(ndomainsz,nflev+1,2) |
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241 | real zfluxu_sw(ndomainsz,nflev+1,2) |
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242 | |
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243 | REAL zplev(ndomainsz,nflev+1) |
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244 | REAL zztlev(ndomainsz,nflev+1) |
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245 | REAL zplay(ndomainsz,nflev) |
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246 | REAL zt(ndomainsz,nflev) |
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247 | REAL zaerosol(ndomainsz,nflev,naerkind) |
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248 | REAL zalbedo(ndomainsz,2) |
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249 | REAL zdp(ndomainsz,nflev) |
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250 | REAL zdt0(ndomainsz) |
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251 | |
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252 | REAL zzdtlw(ndomainsz,nflev) |
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253 | REAL zzdtsw(ndomainsz,nflev) |
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254 | REAL zzflux(ndomainsz,6) |
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255 | real zrmuz |
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256 | |
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257 | REAL :: zQVISsQREF3d(ndomainsz,nflev,nsun,naerkind) |
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258 | REAL :: zomegaVIS3d(ndomainsz,nflev,nsun,naerkind) |
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259 | REAL :: zgVIS3d(ndomainsz,nflev,nsun,naerkind) |
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260 | |
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261 | REAL :: zQIRsQREF3d(ndomainsz,nflev,nir,naerkind) |
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262 | REAL :: zomegaIR3d(ndomainsz,nflev,nir,naerkind) |
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263 | REAL :: zgIR3d(ndomainsz,nflev,nir,naerkind) |
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264 | |
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265 | c Aerosol size distribution |
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266 | REAL :: reffrad(ngrid,nlayer,naerkind) |
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267 | REAL :: nueffrad(ngrid,nlayer,naerkind) |
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268 | c Aerosol optical properties |
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269 | REAL :: QVISsQREF3d(ngrid,nlayer,nsun,naerkind) |
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270 | REAL :: omegaVIS3d(ngrid,nlayer,nsun,naerkind) |
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271 | REAL :: gVIS3d(ngrid,nlayer,nsun,naerkind) |
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272 | |
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273 | REAL :: QIRsQREF3d(ngrid,nlayer,nir,naerkind) |
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274 | REAL :: omegaIR3d(ngrid,nlayer,nir,naerkind) |
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275 | REAL :: gIR3d(ngrid,nlayer,nir,naerkind) |
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276 | |
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277 | REAL :: QREFvis3d(ngrid,nlayer,naerkind) |
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278 | ! QREFvis3d : Extinction efficiency at the VISible reference wavelength |
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279 | REAL :: QREFir3d(ngrid,nlayer,naerkind) |
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280 | ! QREFir3d : Extinction efficiency at the InfraRed reference wavelength |
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281 | |
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282 | REAL :: omegaREFvis3d(ngrid,nlayer,naerkind) |
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283 | REAL :: omegaREFir3d(ngrid,nlayer,naerkind) |
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284 | |
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285 | c local saved variables |
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286 | c --------------------- |
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287 | |
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288 | real zco2 ! volume fraction of CO2 in Mars atmosphere |
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289 | !$OMP THREADPRIVATE(zco2) |
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290 | DATA zco2/0.95/ |
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291 | SAVE zco2 |
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292 | |
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293 | LOGICAL firstcall |
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294 | !$OMP THREADPRIVATE(firstcall) |
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295 | DATA firstcall/.true./ |
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296 | SAVE firstcall |
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297 | |
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298 | |
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299 | |
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300 | c---------------------------------------------------------------------- |
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301 | |
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302 | c Initialisation |
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303 | c -------------- |
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304 | |
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305 | ! compute ndomain |
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306 | ! AS: moved out of firstcall to allow nesting+evoluting domain |
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307 | ! ------------------------------------------------------------ |
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308 | ndomain= (ngrid-1) / ndomainsz + 1 |
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309 | |
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310 | IF (firstcall) THEN |
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311 | |
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312 | write(*,*) 'Splitting radiative calculations: ', |
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313 | $ ' ngrid,ndomainsz,ndomain', |
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314 | $ ngrid,ndomainsz,ndomain |
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315 | |
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316 | c Assign a number to the different scatterers |
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317 | c ------------------------------------------- |
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318 | |
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319 | iaer_dust_conrath=0 |
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320 | iaer_dust_doubleq=0 |
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321 | iaer_dust_submicron=0 |
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322 | iaer_h2o_ice=0 |
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323 | iaer_co2_ice=0 |
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324 | iaer_stormdust_doubleq=0 |
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325 | iaer_topdust_doubleq=0 |
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326 | |
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327 | aer_count=0 |
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328 | if (.NOT.active) then |
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329 | do iaer=1,naerkind |
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330 | if (name_iaer(iaer).eq."dust_conrath") then |
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331 | iaer_dust_conrath = iaer |
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332 | aer_count = aer_count + 1 |
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333 | endif |
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334 | enddo |
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335 | endif |
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336 | if (doubleq.AND.active) then |
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337 | do iaer=1,naerkind |
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338 | if (name_iaer(iaer).eq."dust_doubleq") then |
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339 | iaer_dust_doubleq = iaer |
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340 | aer_count = aer_count + 1 |
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341 | endif |
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342 | enddo |
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343 | endif |
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344 | if (submicron.AND.active) then |
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345 | do iaer=1,naerkind |
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346 | if (name_iaer(iaer).eq."dust_submicron") then |
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347 | iaer_dust_submicron = iaer |
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348 | aer_count = aer_count + 1 |
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349 | endif |
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350 | enddo |
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351 | endif |
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352 | if (water.AND.activice) then |
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353 | do iaer=1,naerkind |
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354 | if (name_iaer(iaer).eq."h2o_ice") then |
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355 | iaer_h2o_ice = iaer |
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356 | aer_count = aer_count + 1 |
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357 | endif |
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358 | enddo |
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359 | endif |
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360 | if (co2clouds.AND.activeco2ice) then |
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361 | do iaer=1,naerkind |
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362 | if (name_iaer(iaer).eq."co2_ice") then |
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363 | iaer_co2_ice = iaer |
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364 | aer_count = aer_count + 1 |
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365 | endif |
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366 | enddo |
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367 | endif |
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368 | if (rdstorm.AND.active) then |
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369 | do iaer=1,naerkind |
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370 | if (name_iaer(iaer).eq."stormdust_doubleq") then |
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371 | iaer_stormdust_doubleq = iaer |
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372 | aer_count = aer_count + 1 |
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373 | endif |
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374 | enddo |
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375 | end if |
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376 | if (topflows.AND.active) then |
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377 | do iaer=1,naerkind |
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378 | if (name_iaer(iaer).eq."topdust_doubleq") then |
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379 | iaer_topdust_doubleq = iaer |
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380 | aer_count = aer_count + 1 |
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381 | endif |
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382 | enddo |
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383 | end if |
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384 | |
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385 | c Check that we identified all tracers: |
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386 | if (aer_count.ne.naerkind) then |
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387 | write(*,*) "callradite: found only ",aer_count," scatterers" |
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388 | write(*,*) " expected ",naerkind |
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389 | write(*,*) "please make sure that the number of" |
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390 | write(*,*) "scatterers in scatterers.h, the names" |
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391 | write(*,*) "in callradite.F, and the flags in" |
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392 | write(*,*) "callphys.def are all consistent!" |
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393 | do iaer=1,naerkind |
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394 | write(*,*)' ',iaer,' ',trim(name_iaer(iaer)) |
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395 | enddo |
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396 | call abort_physic("callradite","incoherent scatterers",1) |
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397 | else |
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398 | write(*,*) "callradite: found all scatterers, namely:" |
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399 | do iaer=1,naerkind |
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400 | write(*,*)' ',iaer,' ',trim(name_iaer(iaer)) |
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401 | enddo |
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402 | endif |
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403 | c ------------------------------------------- |
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404 | |
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405 | gcp = g/cpp |
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406 | |
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407 | |
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408 | c Loading the optical properties in external look-up tables: |
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409 | |
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410 | CALL SUAER |
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411 | |
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412 | ! CALL SULW ! this step is now done in ini_yomlw_h |
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413 | |
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414 | if (ngrid .EQ. 1) then |
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415 | if (ndomainsz .NE. 1) then |
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416 | print* |
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417 | print*,'ATTENTION !!!' |
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418 | print*,'pour tourner en 1D, ' |
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419 | print*,'fixer ndomainsz=1 dans phymars/dimradmars_h' |
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420 | print* |
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421 | call exit(1) |
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422 | endif |
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423 | endif |
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424 | |
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425 | firstcall=.false. |
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426 | END IF |
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427 | |
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428 | c Computing aerosol optical properties and opacity |
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429 | c ------------------------------------------------ |
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430 | c Updating aerosol size distributions: |
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431 | CALL updatereffrad(ngrid,nlayer, |
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432 | & rdust,rstormdust,rtopdust,rice,nuice, |
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433 | & reffrad,nueffrad, riceco2, nuiceco2, |
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434 | & pq,tauscaling,tau,pplay, pt) |
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435 | c Computing 3D scattering parameters: |
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436 | gVIS3d(:,:,:,:) = 0. |
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437 | CALL aeroptproperties(ngrid,nlayer,reffrad,nueffrad, |
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438 | & QVISsQREF3d,omegaVIS3d,gVIS3d, |
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439 | & QIRsQREF3d,omegaIR3d,gIR3d, |
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440 | & QREFvis3d,QREFir3d, |
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441 | & omegaREFvis3d,omegaREFir3d) |
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442 | c Computing aerosol optical depth in each layer: |
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443 | CALL aeropacity(ngrid,nlayer,nq,zday,pplay,pplev,ls, |
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444 | & pq,pt,tauscaling,dust_rad_adjust,IRtoVIScoef, |
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445 | & tau_pref_scenario,tau_pref_gcm,tau,taucloudtes, |
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446 | & aerosol,dsodust,reffrad, |
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447 | & QREFvis3d,QREFir3d,omegaREFir3d, |
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448 | & totstormfract,clearatm,dsords,dsotop, |
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449 | & nohmons,clearsky,totcloudfrac) |
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450 | |
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451 | c Starting loop on sub-domain |
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452 | c ---------------------------- |
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453 | zgVIS3d(:,:,:,:) = 0. |
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454 | zfluxd_sw(:,:,:) = 0. |
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455 | zfluxu_sw(:,:,:) = 0. |
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456 | zQVISsQREF3d(:,:,:,:) = 0. |
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457 | zomegaVIS3d(:,:,:,:) = 0. |
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458 | DO jd=1,ndomain |
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459 | ig0=(jd-1)*ndomainsz |
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460 | if (jd.eq.ndomain) then |
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461 | nd=ngrid-ig0 |
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462 | else |
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463 | nd=ndomainsz |
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464 | endif |
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465 | |
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466 | c Spliting input variable in sub-domain input variables |
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467 | c --------------------------------------------------- |
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468 | |
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469 | do l=1,nlaylte |
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470 | do ig = 1,nd |
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471 | do iaer = 1, naerkind |
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472 | do ich = 1, nsun |
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473 | zQVISsQREF3d(ig,l,ich,iaer) = |
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474 | & QVISsQREF3d(ig0+ig,l,ich,iaer) |
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475 | zomegaVIS3d(ig,l,ich,iaer) = |
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476 | & omegaVIS3d(ig0+ig,l,ich,iaer) |
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477 | zgVIS3d(ig,l,ich,iaer) = |
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478 | & gVIS3d(ig0+ig,l,ich,iaer) |
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479 | enddo |
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480 | do ich = 1, nir |
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481 | zQIRsQREF3d(ig,l,ich,iaer) = |
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482 | & QIRsQREF3d(ig0+ig,l,ich,iaer) |
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483 | zomegaIR3d(ig,l,ich,iaer) = |
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484 | & omegaIR3d(ig0+ig,l,ich,iaer) |
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485 | zgIR3d(ig,l,ich,iaer) = |
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486 | & gIR3d(ig0+ig,l,ich,iaer) |
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487 | enddo |
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488 | enddo |
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489 | enddo |
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490 | enddo |
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491 | zplev(:,:) = 0. |
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492 | do l=1,nlaylte+1 |
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493 | do ig = 1,nd |
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494 | zplev(ig,l) = pplev(ig0+ig,l) |
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495 | enddo |
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496 | enddo |
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497 | zdp(:,:) = 0. |
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498 | |
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499 | do l=1,nlaylte |
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500 | do ig = 1,nd |
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501 | zplay(ig,l) = pplay(ig0+ig,l) |
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502 | zt(ig,l) = pt(ig0+ig,l) |
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503 | c Thickness of each layer (Pa) : |
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504 | zdp(ig,l)= pplev(ig0+ig,l) - pplev(ig0+ig,l+1) |
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505 | enddo |
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506 | enddo |
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507 | zaerosol(:,:,:) = 0. |
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508 | do n=1,naerkind |
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509 | do l=1,nlaylte |
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510 | do ig=1,nd |
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511 | zaerosol(ig,l,n) = aerosol(ig0+ig,l,n) |
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512 | enddo |
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513 | enddo |
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514 | enddo |
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515 | zalbedo(:,:) = 0. |
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516 | do j=1,2 |
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517 | do ig = 1,nd |
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518 | zalbedo(ig,j) = albedo(ig0+ig,j) |
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519 | enddo |
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520 | enddo |
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521 | |
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522 | c Intermediate levels: (computing tlev) |
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523 | c --------------------------------------- |
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524 | c Extrapolation for the air temperature above the surface |
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525 | DO ig=1,nd |
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526 | zztlev(ig,1)=zt(ig,1)+ |
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527 | s (zplev(ig,1)-zplay(ig,1))* |
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528 | s (zt(ig,1)-zt(ig,2))/(zplay(ig,1)-zplay(ig,2)) |
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529 | |
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530 | zdt0(ig) = tsurf(ig0+ig) - zztlev(ig,1) |
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531 | ENDDO |
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532 | |
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533 | DO l=2,nlaylte |
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534 | DO ig=1, nd |
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535 | zztlev(ig,l)=0.5*(zt(ig,l-1)+zt(ig,l)) |
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536 | ENDDO |
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537 | ENDDO |
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538 | |
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539 | DO ig=1, nd |
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540 | zztlev(ig,nlaylte+1)=zt(ig,nlaylte) |
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541 | ENDDO |
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542 | |
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543 | |
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544 | c Longwave ("lw") radiative transfer (= thermal infrared) |
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545 | c ------------------------------------------------------- |
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546 | call lwmain (ig0,icount,nd,nflev |
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547 | . ,zdp,zdt0,emis(ig0+1),zplev,zztlev,zt |
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548 | . ,zaerosol,zzdtlw |
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549 | . ,fluxsurf_lw(ig0+1),fluxtop_lw(ig0+1) |
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550 | . ,znetrad |
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551 | & ,zQIRsQREF3d,zomegaIR3d,zgIR3d |
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552 | & ,co2ice(ig0+1)) |
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553 | |
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554 | c Shortwave ("sw") radiative transfer (= solar radiation) |
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555 | c ------------------------------------------------------- |
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556 | c Mars solar constant (W m-2) |
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557 | c flux_1AU = 1370 W.m-2 is the solar constant at 1 AU. |
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558 | cste_mars=flux_1AU/(dist_sol*dist_sol) |
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559 | zzdtsw(:,:) = 0. |
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560 | call swmain ( nd, nflev, |
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561 | S cste_mars, zalbedo, |
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562 | S mu0(ig0+1), zdp, zplev, zaerosol, fract(ig0+1), |
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563 | S zzdtsw, zfluxd_sw, zfluxu_sw, |
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564 | & zQVISsQREF3d,zomegaVIS3d,zgVIS3d) |
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565 | c ------------------------------------------------------------ |
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566 | c Un-spliting output variable from sub-domain input variables |
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567 | c ------------------------------------------------------------ |
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568 | |
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569 | do l=1,nlaylte |
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570 | do ig = 1,nd |
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571 | dtlw(ig0+ig,l) = zzdtlw(ig,l) |
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572 | dtsw(ig0+ig,l) = zzdtsw(ig,l) |
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573 | enddo |
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574 | enddo |
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575 | |
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576 | ptlev(:, :) = 0. |
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577 | do l=1,nlaylte+1 |
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578 | do ig = 1,nd |
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579 | ptlev(ig0+ig,l) = zztlev(ig,l) |
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580 | enddo |
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581 | enddo |
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582 | |
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583 | ! copy SW fluxes at surface and TOA |
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584 | do ig = 1,nd |
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585 | ! surface downward SW flux |
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586 | fluxsurf_dn_sw(ig0+ig,1) = zfluxd_sw(ig,1,1) |
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587 | fluxsurf_dn_sw(ig0+ig,2) = zfluxd_sw(ig,1,2) |
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588 | ! surface upward SW flux |
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589 | fluxsurf_up_sw(ig0+ig,1) = zfluxu_sw(ig,1,1) |
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590 | fluxsurf_up_sw(ig0+ig,2) = zfluxu_sw(ig,1,2) |
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591 | ! downward SW flux at top of atmosphere |
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592 | fluxtop_dn_sw(ig0+ig,1) = zfluxd_sw(ig,nlaylte+1,1) |
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593 | fluxtop_dn_sw(ig0+ig,2) = zfluxd_sw(ig,nlaylte+1,2) |
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594 | ! upward SW flux at top of atmosphere |
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595 | fluxtop_up_sw(ig0+ig,1) = zfluxu_sw(ig,nlaylte+1,1) |
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596 | fluxtop_up_sw(ig0+ig,2) = zfluxu_sw(ig,nlaylte+1,2) |
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597 | enddo |
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598 | |
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599 | ENDDO ! (boucle jd=1, ndomain) |
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600 | |
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601 | c Zero tendencies for any remaining layers between nlaylte and nlayer |
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602 | if (nlayer.gt.nlaylte) then |
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603 | do l = nlaylte+1, nlayer |
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604 | do ig = 1, ngrid |
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605 | dtlw(ig, l) = 0. |
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606 | dtsw(ig, l) = 0. |
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607 | enddo |
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608 | enddo |
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609 | endif |
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610 | c Output for debugging |
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611 | c -------------------------------- |
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612 | c Write all nlayer layers, even though only nlaylte layers may have |
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613 | c non-zero tendencies. |
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614 | |
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615 | c PRINT*,'Diagnotique for the radiation' |
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616 | c PRINT*,'albedo, emissiv, mu0,fract,fluxsurf_lw,fluxsurf_sw' |
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617 | c PRINT*,albedo(igout,1),emis(igout),mu0(igout), |
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618 | c s fract(igout), fluxsurf_lw(igout), |
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619 | c $ fluxsurf_dn_sw(igout,1)+fluxsurf_dn_sw(igout,2) |
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620 | c PRINT*,'Tlay Tlev Play Plev dT/dt SW dT/dt LW (K/s)' |
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621 | c PRINT*,'daysec',daysec |
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622 | c DO l=1,nlayer |
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623 | c PRINT*,pt(igout,l),ptlev(igout,l), |
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624 | c s pplay(igout,l),pplev(igout,l), |
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625 | c s dtsw(igout,l),dtlw(igout,l) |
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626 | c ENDDO |
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627 | |
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628 | |
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629 | END SUBROUTINE callradite |
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630 | |
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631 | END MODULE callradite_mod |
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