1 | MODULE vdifc_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 vdifc(ngrid,nlay,nsoil,nq,nqsoil,ppopsk, |
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8 | $ ptimestep,pcapcal,lecrit, |
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9 | $ pplay,pplev,pzlay,pzlev,pz0, |
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10 | $ pu,pv,ph,pq,ptsrf,ptsoil,pemis,pqsurf,qsoil, |
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11 | $ pore_icefraction,pdufi,pdvfi,pdhfi, |
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12 | $ pdqfi,pfluxsrf, |
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13 | $ pdudif,pdvdif,pdhdif,pdtsrf,pq2, |
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14 | $ pdqdif,pdqsdif,wstar, |
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15 | $ hfmax,pcondicea_co2microp,sensibFlux, |
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16 | $ dustliftday,local_time,watercap, dwatercap_dif) |
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17 | |
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18 | use tracer_mod, only: noms, igcm_dust_mass, igcm_dust_number, |
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19 | & igcm_dust_submicron, igcm_h2o_vap, |
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20 | & igcm_h2o_ice, alpha_lift, igcm_co2, |
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21 | & igcm_hdo_vap, igcm_hdo_ice, |
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22 | & igcm_stormdust_mass, igcm_stormdust_number |
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23 | use surfdat_h, only: watercaptag, frost_albedo_threshold, dryness, |
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24 | & old_wsublimation_scheme |
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25 | USE comcstfi_h, ONLY: cpp, r, rcp, g, pi |
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26 | use watersat_mod, only: watersat |
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27 | use turb_mod, only: turb_resolved, ustar, tstar |
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28 | use compute_dtau_mod, only: ti_injection_sol,tf_injection_sol |
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29 | use hdo_surfex_mod, only: hdo_surfex |
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30 | c use geometry_mod, only: longitude_deg,latitude_deg ! Joseph |
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31 | use dust_param_mod, only: doubleq, submicron, lifting |
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32 | use write_output_mod, only: write_output |
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33 | use comslope_mod, ONLY: nslope,def_slope,def_slope_mean, |
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34 | & subslope_dist,major_slope,iflat |
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35 | use microphys_h, only: To |
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36 | use paleoclimate_mod, only: d_coef,h2o_ice_depth,lag_layer |
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37 | use comsoil_h, only: layer, mlayer,adsorption_soil |
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38 | use vdif_cd_mod, only: vdif_cd |
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39 | use lmdz_call_atke, only: call_atke |
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40 | use dust_windstress_lift_mod, only: dust_windstress_lift |
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41 | IMPLICIT NONE |
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42 | |
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43 | c======================================================================= |
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44 | c |
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45 | c subject: |
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46 | c -------- |
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47 | c Turbulent diffusion (mixing) for potential T, U, V and tracer |
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48 | c |
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49 | c Shema implicite |
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50 | c On commence par rajouter au variables x la tendance physique |
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51 | c et on resoult en fait: |
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52 | c x(t+1) = x(t) + dt * (dx/dt)phys(t) + dt * (dx/dt)difv(t+1) |
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53 | c |
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54 | c author: |
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55 | c ------ |
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56 | c Hourdin/Forget/Fournier |
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57 | c======================================================================= |
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58 | |
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59 | c----------------------------------------------------------------------- |
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60 | c declarations: |
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61 | c ------------- |
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62 | |
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63 | include "callkeys.h" |
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64 | |
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65 | c |
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66 | c arguments: |
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67 | c ---------- |
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68 | |
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69 | INTEGER,INTENT(IN) :: ngrid,nlay,nsoil,nqsoil |
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70 | REAL,INTENT(IN) :: ptimestep |
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71 | REAL,INTENT(IN) :: pplay(ngrid,nlay),pplev(ngrid,nlay+1) |
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72 | REAL,INTENT(IN) :: pzlay(ngrid,nlay),pzlev(ngrid,nlay+1) |
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73 | REAL,INTENT(IN) :: pu(ngrid,nlay),pv(ngrid,nlay) |
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74 | REAL,INTENT(IN) :: ph(ngrid,nlay) |
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75 | REAL,INTENT(IN) :: ptsrf(ngrid,nslope),pemis(ngrid,nslope) |
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76 | REAL,INTENT(IN) :: pdufi(ngrid,nlay),pdvfi(ngrid,nlay) |
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77 | REAL,INTENT(IN) :: pdhfi(ngrid,nlay) |
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78 | REAL,INTENT(IN) :: pfluxsrf(ngrid,nslope) |
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79 | REAL,INTENT(OUT) :: pdudif(ngrid,nlay),pdvdif(ngrid,nlay) |
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80 | REAL,INTENT(OUT) :: pdtsrf(ngrid,nslope),pdhdif(ngrid,nlay) |
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81 | REAL,INTENT(IN) :: pcapcal(ngrid,nslope) |
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82 | REAL,INTENT(INOUT) :: pq2(ngrid,nlay+1) |
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83 | REAL,INTENT(IN) :: ptsoil(ngrid,nsoil,nslope) |
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84 | |
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85 | c Argument added for condensation: |
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86 | REAL,INTENT(IN) :: ppopsk(ngrid,nlay) |
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87 | logical,INTENT(IN) :: lecrit |
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88 | REAL,INTENT(IN) :: pcondicea_co2microp(ngrid,nlay)! tendency due to CO2 condensation (kg/kg.s-1) |
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89 | |
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90 | REAL,INTENT(IN) :: pz0(ngrid) ! surface roughness length (m) |
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91 | |
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92 | c Argument added to account for subgrid gustiness : |
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93 | |
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94 | REAL,INTENT(IN) :: wstar(ngrid), hfmax(ngrid)!, zi(ngrid) |
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95 | |
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96 | c Traceurs : |
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97 | integer,intent(in) :: nq |
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98 | REAL,INTENT(IN) :: pqsurf(ngrid,nq,nslope) |
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99 | REAL :: zqsurf(ngrid) ! temporary water tracer |
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100 | real,intent(in) :: pq(ngrid,nlay,nq), pdqfi(ngrid,nlay,nq) |
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101 | real,intent(out) :: pdqdif(ngrid,nlay,nq) |
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102 | real,intent(out) :: pdqsdif(ngrid,nq,nslope) |
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103 | REAL,INTENT(in) :: dustliftday(ngrid) |
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104 | REAL,INTENT(inout) :: qsoil(ngrid,nsoil,nqsoil,nslope) !subsurface tracers |
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105 | REAL,INTENT(in) :: local_time(ngrid) |
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106 | |
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107 | c local: |
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108 | c ------ |
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109 | |
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110 | REAL :: pt(ngrid,nlay) |
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111 | |
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112 | INTEGER ilev,ig,ilay,nlev,islope,ik,lice |
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113 | |
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114 | REAL z4st,zdplanck(ngrid) |
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115 | REAL zkv(ngrid,nlay+1),zkh(ngrid,nlay+1) |
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116 | REAL zkq(ngrid,nlay+1) |
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117 | REAL zcdv(ngrid,nslope),zcdh(ngrid,nslope) |
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118 | REAL :: zcdv_true(ngrid,nslope) |
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119 | REAL :: zcdh_true(ngrid,nslope) ! drag coeff are used by the LES to recompute u* and hfx |
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120 | REAL :: zcdv_tmp(ngrid),zcdh_tmp(ngrid) ! drag coeffs for the major sub-grid surface |
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121 | REAL :: zcdv_true_tmp(ngrid),zcdh_true_tmp(ngrid) ! drag coeffs (computed with wind gustiness for the major sub-grid surface |
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122 | REAL zu(ngrid,nlay),zv(ngrid,nlay) |
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123 | REAL zh(ngrid,nlay) |
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124 | REAL ztsrf2(ngrid) |
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125 | REAL z1(ngrid),z2(ngrid) |
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126 | REAL za(ngrid,nlay),zb(ngrid,nlay) |
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127 | REAL zb0(ngrid,nlay) |
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128 | REAL zc(ngrid,nlay),zd(ngrid,nlay) |
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129 | REAL zcst1 |
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130 | REAL zu2(ngrid) |
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131 | |
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132 | |
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133 | EXTERNAL SSUM,SCOPY |
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134 | REAL SSUM |
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135 | LOGICAL,SAVE :: firstcall=.true. |
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136 | |
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137 | !$OMP THREADPRIVATE(firstcall) |
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138 | |
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139 | c variable added for CO2 condensation: |
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140 | c ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ |
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141 | REAL hh , zhcond(ngrid,nlay) |
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142 | REAL,PARAMETER :: latcond=5.9e5 |
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143 | REAL,PARAMETER :: tcond1mb=136.27 |
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144 | REAL,SAVE :: acond,bcond |
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145 | |
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146 | !$OMP THREADPRIVATE(acond,bcond) |
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147 | |
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148 | c Subtimestep & implicit treatment of water vapor |
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149 | c ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ |
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150 | REAL zdqsdif_surf(ngrid) ! subtimestep pdqsdif for water ice |
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151 | REAL ztsrf(ngrid) ! temporary surface temperature in tsub |
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152 | REAL zdtsrf(ngrid,nslope) ! surface temperature tendancy in tsub |
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153 | REAL surf_h2o_lh(ngrid,nslope) ! Surface h2o latent heat flux |
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154 | REAL zsurf_h2o_lh(ngrid,nslope) ! Tsub surface h2o latent heat flux |
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155 | |
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156 | c For latent heat release from ground water ice sublimation |
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157 | c ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ |
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158 | REAL tsrf_lh(ngrid) ! temporary surface temperature with lh effect |
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159 | REAL lh ! latent heat, formulation given in the Technical Document: |
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160 | ! "Modeling water ice sublimation under Phoenix-like conditions", Montmessin et al. 2004 |
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161 | |
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162 | c Tracers : |
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163 | c ~~~~~~~ |
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164 | INTEGER iq |
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165 | REAL zq(ngrid,nlay,nq) |
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166 | REAL zq1temp(ngrid) |
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167 | REAL rho(ngrid) ! near surface air density |
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168 | REAL qsat(ngrid) |
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169 | |
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170 | |
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171 | REAL hdoflux(ngrid,nslope) ! value of vapour flux of HDO |
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172 | REAL hdoflux_meshavg(ngrid) ! value of vapour flux of HDO |
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173 | ! REAL h2oflux(ngrid) ! value of vapour flux of H2O |
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174 | REAL old_h2o_vap(ngrid) ! traceur d'eau avant traitement |
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175 | REAL saved_h2o_vap(ngrid) ! traceur d'eau avant traitement |
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176 | |
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177 | REAL kmixmin |
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178 | |
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179 | c Argument added for surface water ice budget: |
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180 | REAL,INTENT(IN) :: watercap(ngrid,nslope) |
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181 | REAL,INTENT(OUT) :: dwatercap_dif(ngrid,nslope) |
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182 | |
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183 | c Subtimestep to compute h2o latent heat flux: |
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184 | REAL :: dtmax = 0.5 ! subtimestep temp criterion |
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185 | INTEGER tsub ! adaptative subtimestep (seconds) |
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186 | REAL subtimestep !ptimestep/nsubtimestep |
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187 | INTEGER nsubtimestep(ngrid) ! number of subtimestep (int) |
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188 | |
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189 | c Mass-variation scheme : |
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190 | c ~~~~~~~ |
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191 | |
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192 | INTEGER j,l |
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193 | REAL zcondicea(ngrid,nlay) |
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194 | REAL zt(ngrid,nlay),ztcond(ngrid,nlay+1) |
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195 | REAL betam(ngrid,nlay),dmice(ngrid,nlay) |
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196 | REAL pdtc(ngrid,nlay) |
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197 | REAL zhs(ngrid,nlay) |
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198 | REAL,SAVE :: ccond |
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199 | |
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200 | !$OMP THREADPRIVATE(ccond) |
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201 | |
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202 | c Theta_m formulation for mass-variation scheme : |
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203 | c ~~~~~~~ |
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204 | |
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205 | INTEGER,SAVE :: ico2 |
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206 | INTEGER llnt(ngrid) |
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207 | REAL,SAVE :: m_co2, m_noco2, A , B |
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208 | REAL vmr_co2(ngrid,nlay) |
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209 | REAL qco2,mmean(ngrid,nlay) |
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210 | |
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211 | !$OMP THREADPRIVATE(ico2,m_co2,m_noco2,A,B) |
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212 | |
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213 | REAL,INTENT(OUT) :: sensibFlux(ngrid) |
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214 | |
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215 | !!MARGAUX |
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216 | REAL DoH_vap(ngrid,nlay) |
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217 | !! Sub-grid scale slopes |
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218 | REAL :: pdqsdif_tmp(ngrid,nq) ! Temporary for dust lifting |
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219 | REAL :: watercap_tmp(ngrid) |
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220 | REAL :: zq_slope_vap(ngrid,nlay,nq,nslope) |
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221 | REAL :: zq_tmp_vap(ngrid,nlay,nq) |
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222 | REAL :: ptsrf_tmp(ngrid) |
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223 | REAL :: pqsurf_tmp(ngrid,nq) |
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224 | REAL :: pdqsdif_tmphdo(ngrid,nq) |
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225 | REAL :: qsat_tmp(ngrid) |
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226 | INTEGER :: indmax |
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227 | |
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228 | character*2 str2 |
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229 | |
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230 | !! Subsurface exchanges |
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231 | LOGICAL :: exchange ! boolean to check if exchange between the subsurface and the atmosphere can occurs |
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232 | REAL :: zdqsdif_regolith(ngrid,nslope) ! Flux from subsurface (positive pointing outwards) (kg/m^2/s) |
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233 | REAL zq1temp_regolith(ngrid) ! Temporary atmospheric mixing ratio after exchange with subsurface (kg / kg) |
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234 | REAL zdqsdif_tot(ngrid) ! subtimestep pdqsdif for water ice |
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235 | LOGICAL :: writeoutput ! boolean to say to soilexchange.F if we are at the last iteration and thus if he can write in the diagsoil |
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236 | REAL, INTENT(out) :: pore_icefraction(ngrid,nsoil,nslope) ! ice filling fraction in the pores |
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237 | |
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238 | !! Subsurface ice interactions |
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239 | REAL Tice(ngrid,nslope) ! subsurface temperature where ice is located (K) |
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240 | REAL qsat_ssi(ngrid,nslope) ! qsat(Tice) (kg/kg) |
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241 | REAL resist(ngrid,nslope) ! subsurface ice flux reduction coef (1) |
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242 | REAL zdqsdif_ssi_atm(ngrid,nslope) ! SSI - atmosphere flux (kg/m^2/s^-1) at a given subtimestep |
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243 | REAL zdqsdif_ssi_frost(ngrid,nslope) ! SSI - frost flux (kg/m^2/s^-1) at a given subtimestep |
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244 | REAL zdqsdif_ssi_atm_tot(ngrid,nslope) ! SSI - atmosphere flux (kg/m^2/s^-1) summed over all subtimestep |
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245 | REAL zdqsdif_ssi_frost_tot(ngrid,nslope) ! SSI - frost flux (kg/m^2/s^-1) summed over all subtimestep |
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246 | REAL zdqsdif_ssi_tot(ngrid,nslope) ! Total flux of the interactions with SSI kg/m^2/s^-1) |
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247 | |
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248 | REAL :: tol_frost = 2e-3 ! tolerence for frost thicnkess (kg/m^2) to avoid numerical noise effect |
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249 | c ** un petit test de coherence |
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250 | c -------------------------- |
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251 | |
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252 | ! AS: OK firstcall absolute |
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253 | IF (firstcall) THEN |
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254 | c To compute: Tcond= 1./(bcond-acond*log(.0095*p)) (p in pascal) |
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255 | bcond=1./tcond1mb |
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256 | acond=r/latcond |
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257 | ccond=cpp/(g*latcond) |
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258 | PRINT*,'In vdifc: Tcond(P=1mb)=',tcond1mb,' Lcond=',latcond |
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259 | PRINT*,' acond,bcond,ccond',acond,bcond,ccond |
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260 | |
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261 | |
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262 | ico2=0 |
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263 | |
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264 | c Prepare Special treatment if one of the tracer is CO2 gas |
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265 | do iq=1,nq |
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266 | if (noms(iq).eq."co2") then |
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267 | ico2=iq |
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268 | m_co2 = 44.01E-3 ! CO2 molecular mass (kg/mol) |
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269 | m_noco2 = 33.37E-3 ! Non condensible mol mass (kg/mol) |
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270 | c Compute A and B coefficient use to compute |
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271 | c mean molecular mass Mair defined by |
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272 | c 1/Mair = q(ico2)/m_co2 + (1-q(ico2))/m_noco2 |
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273 | c 1/Mair = A*q(ico2) + B |
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274 | A =(1/m_co2 - 1/m_noco2) |
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275 | B=1/m_noco2 |
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276 | endif |
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277 | enddo |
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278 | |
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279 | firstcall=.false. |
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280 | ENDIF |
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281 | |
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282 | DO ig = 1,ngrid |
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283 | ptsrf_tmp(ig) = ptsrf(ig,major_slope(ig)) |
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284 | pqsurf_tmp(ig,:) = pqsurf(ig,:,major_slope(ig)) |
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285 | ENDDO |
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286 | |
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287 | c----------------------------------------------------------------------- |
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288 | c 1. initialisation |
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289 | c ----------------- |
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290 | |
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291 | nlev=nlay+1 |
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292 | |
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293 | ! initialize output tendencies to zero: |
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294 | pdudif(1:ngrid,1:nlay)=0 |
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295 | pdvdif(1:ngrid,1:nlay)=0 |
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296 | pdhdif(1:ngrid,1:nlay)=0 |
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297 | pdtsrf(1:ngrid,1:nslope)=0 |
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298 | zdtsrf(1:ngrid,1:nslope)=0 |
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299 | surf_h2o_lh(1:ngrid,1:nslope)=0 |
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300 | zsurf_h2o_lh(1:ngrid,1:nslope)=0 |
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301 | pdqdif(1:ngrid,1:nlay,1:nq)=0 |
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302 | pdqsdif(1:ngrid,1:nq,1:nslope)=0 |
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303 | pdqsdif_tmp(1:ngrid,1:nq)=0 |
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304 | zdqsdif_surf(1:ngrid)=0 |
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305 | dwatercap_dif(1:ngrid,1:nslope)=0 |
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306 | zdqsdif_regolith(1:ngrid,1:nslope)=0 |
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307 | zq1temp_regolith(1:ngrid)=0 |
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308 | zdqsdif_tot(1:ngrid)=0 |
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309 | pore_icefraction(:,:,:) = 0. |
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310 | zdqsdif_ssi_atm(:,:) = 0. |
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311 | zdqsdif_ssi_frost(:,:) = 0. |
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312 | zdqsdif_ssi_tot(:,:) = 0. |
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313 | zdqsdif_ssi_atm_tot(:,:) = 0. |
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314 | zdqsdif_ssi_frost_tot(:,:) = 0. |
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315 | |
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316 | |
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317 | c ** calcul de rho*dz et dt*rho/dz=dt*rho**2 g/dp |
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318 | c avec rho=p/RT=p/ (R Theta) (p/ps)**kappa |
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319 | c ---------------------------------------- |
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320 | |
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321 | DO ilay=1,nlay |
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322 | DO ig=1,ngrid |
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323 | za(ig,ilay)=(pplev(ig,ilay)-pplev(ig,ilay+1))/g |
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324 | ! Mass variation scheme: |
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325 | betam(ig,ilay)=-za(ig,ilay)*latcond/(cpp*ppopsk(ig,ilay)) |
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326 | ENDDO |
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327 | ENDDO |
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328 | |
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329 | zcst1=4.*g*ptimestep/(r*r) |
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330 | DO ilev=2,nlev-1 |
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331 | DO ig=1,ngrid |
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332 | zb0(ig,ilev)=pplev(ig,ilev)* |
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333 | s (pplev(ig,1)/pplev(ig,ilev))**rcp / |
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334 | s (ph(ig,ilev-1)+ph(ig,ilev)) |
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335 | zb0(ig,ilev)=zcst1*zb0(ig,ilev)*zb0(ig,ilev)/ |
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336 | s (pplay(ig,ilev-1)-pplay(ig,ilev)) |
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337 | ENDDO |
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338 | ENDDO |
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339 | DO ig=1,ngrid |
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340 | zb0(ig,1)=ptimestep*pplev(ig,1)/(r*ptsrf_tmp(ig)) |
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341 | ENDDO |
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342 | |
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343 | c ** diagnostique pour l'initialisation |
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344 | c ---------------------------------- |
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345 | |
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346 | IF(lecrit) THEN |
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347 | ig=ngrid/2+1 |
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348 | PRINT*,'Pression (mbar) ,altitude (km),u,v,theta, rho dz' |
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349 | DO ilay=1,nlay |
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350 | WRITE(*,'(6f11.5)') |
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351 | s .01*pplay(ig,ilay),.001*pzlay(ig,ilay), |
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352 | s pu(ig,ilay),pv(ig,ilay),ph(ig,ilay),za(ig,ilay) |
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353 | ENDDO |
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354 | PRINT*,'Pression (mbar) ,altitude (km),zb' |
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355 | DO ilev=1,nlay |
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356 | WRITE(*,'(3f15.7)') |
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357 | s .01*pplev(ig,ilev),.001*pzlev(ig,ilev), |
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358 | s zb0(ig,ilev) |
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359 | ENDDO |
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360 | ENDIF |
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361 | |
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362 | c ----------------------------------- |
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363 | c Potential Condensation temperature: |
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364 | c ----------------------------------- |
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365 | |
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366 | c Compute CO2 Volume mixing ratio |
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367 | c ------------------------------- |
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368 | if (callcond.and.(ico2.ne.0)) then |
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369 | DO ilev=1,nlay |
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370 | DO ig=1,ngrid |
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371 | qco2=MAX(1.E-30 |
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372 | & ,pq(ig,ilev,ico2)+pdqfi(ig,ilev,ico2)*ptimestep) |
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373 | c Mean air molecular mass = 1/(q(ico2)/m_co2 + (1-q(ico2))/m_noco2) |
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374 | mmean(ig,ilev)=1/(A*qco2 +B) |
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375 | vmr_co2(ig,ilev) = qco2*mmean(ig,ilev)/m_co2 |
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376 | ENDDO |
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377 | ENDDO |
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378 | else |
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379 | DO ilev=1,nlay |
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380 | DO ig=1,ngrid |
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381 | vmr_co2(ig,ilev)=0.95 |
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382 | ENDDO |
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383 | ENDDO |
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384 | end if |
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385 | |
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386 | c forecast of atmospheric temperature zt and frost temperature ztcond |
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387 | c -------------------------------------------------------------------- |
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388 | |
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389 | if (callcond) then |
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390 | DO ilev=1,nlay |
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391 | DO ig=1,ngrid |
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392 | ztcond(ig,ilev)= |
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393 | & 1./(bcond-acond*log(.01*vmr_co2(ig,ilev)*pplay(ig,ilev))) |
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394 | if (pplay(ig,ilev).lt.1e-4) ztcond(ig,ilev)=0.0 !mars Monica |
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395 | ! zhcond(ig,ilev) = |
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396 | ! & (1./(bcond-acond*log(.0095*pplay(ig,ilev))))/ppopsk(ig,ilev) |
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397 | zhcond(ig,ilev) = ztcond(ig,ilev)/ppopsk(ig,ilev) |
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398 | END DO |
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399 | END DO |
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400 | ztcond(:,nlay+1)=ztcond(:,nlay) |
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401 | else |
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402 | zhcond(:,:) = 0 |
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403 | ztcond(:,:) = 0 |
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404 | end if |
---|
405 | |
---|
406 | |
---|
407 | c----------------------------------------------------------------------- |
---|
408 | c 2. ajout des tendances physiques |
---|
409 | c ----------------------------- |
---|
410 | |
---|
411 | DO ilev=1,nlay |
---|
412 | DO ig=1,ngrid |
---|
413 | zu(ig,ilev)=pu(ig,ilev)+pdufi(ig,ilev)*ptimestep |
---|
414 | zv(ig,ilev)=pv(ig,ilev)+pdvfi(ig,ilev)*ptimestep |
---|
415 | zh(ig,ilev)=ph(ig,ilev)+pdhfi(ig,ilev)*ptimestep |
---|
416 | ! zh(ig,ilev)=max(zh(ig,ilev),zhcond(ig,ilev)) |
---|
417 | ENDDO |
---|
418 | ENDDO |
---|
419 | |
---|
420 | zq(1:ngrid,1:nlay,1:nq)=pq(1:ngrid,1:nlay,1:nq)+ |
---|
421 | & pdqfi(1:ngrid,1:nlay,1:nq)*ptimestep |
---|
422 | |
---|
423 | c----------------------------------------------------------------------- |
---|
424 | c 3. schema de turbulence |
---|
425 | c -------------------- |
---|
426 | |
---|
427 | c ** source d'energie cinetique turbulente a la surface |
---|
428 | c (condition aux limites du schema de diffusion turbulente |
---|
429 | c dans la couche limite |
---|
430 | c --------------------- |
---|
431 | |
---|
432 | CALL vdif_cd(ngrid,nlay,nslope,pz0,g,pzlay,pplay,pu,pv,wstar, |
---|
433 | & ptsrf,ph,mmean(:,1),zq(:,:,igcm_h2o_vap), |
---|
434 | & pqsurf(:,igcm_h2o_ice,:), .false., |
---|
435 | & zcdv_true,zcdh_true) |
---|
436 | |
---|
437 | zu2(:)=pu(:,1)*pu(:,1)+pv(:,1)*pv(:,1) |
---|
438 | |
---|
439 | DO islope = 1,nslope |
---|
440 | IF (callrichsl) THEN |
---|
441 | zcdv(:,islope)=zcdv_true(:,islope)*sqrt(zu2(:)+ |
---|
442 | & (log(1.+0.7*wstar(:) + 2.3*wstar(:)**2))**2) |
---|
443 | zcdh(:,islope)=zcdh_true(:,islope)*sqrt(zu2(:)+ |
---|
444 | & (log(1.+0.7*wstar(:) + 2.3*wstar(:)**2))**2) |
---|
445 | ELSE |
---|
446 | zcdv(:,islope)=zcdv_true(:,islope)*sqrt(zu2(:)) ! 1 / bulk aerodynamic momentum conductance |
---|
447 | zcdh(:,islope)=zcdh_true(:,islope)*sqrt(zu2(:)) ! 1 / bulk aerodynamic heat conductance |
---|
448 | ENDIF |
---|
449 | ENDDO |
---|
450 | ustar(:) = 0 |
---|
451 | tstar(:) = 0 |
---|
452 | DO ig = 1,ngrid |
---|
453 | zcdv_tmp(ig) = zcdv(ig,major_slope(ig)) |
---|
454 | zcdh_tmp(ig) = zcdh(ig,major_slope(ig)) |
---|
455 | zcdv_true_tmp(ig) = zcdv_true(ig,major_slope(ig)) |
---|
456 | zcdh_true_tmp(ig) = zcdh_true(ig,major_slope(ig)) |
---|
457 | IF (callrichsl) THEN |
---|
458 | ustar(ig)=sqrt(zcdv_true(ig,major_slope(ig))) |
---|
459 | & *sqrt(zu2(ig)+(log(1.+0.7*wstar(ig) + |
---|
460 | & 2.3*wstar(ig)**2))**2) |
---|
461 | IF (zcdh_true(ig,major_slope(ig)) .ne. 0.) THEN ! When Cd=Ch=0, u*=t*=0 |
---|
462 | tstar(ig)=(ph(ig,1)-ptsrf_tmp(ig)) |
---|
463 | & *zcdh_tmp(ig)/ustar(ig) |
---|
464 | ENDIF |
---|
465 | ELSE |
---|
466 | ustar(ig)=sqrt(zcdv_true(ig,major_slope(ig))) |
---|
467 | & *sqrt(zu2(ig)) |
---|
468 | tstar(ig)=(ph(ig,1)-ptsrf_tmp(ig)) |
---|
469 | & *zcdh_true(ig,major_slope(ig)) |
---|
470 | & /sqrt(zcdv_true(ig,major_slope(ig))) |
---|
471 | ENDIF |
---|
472 | ENDDO |
---|
473 | |
---|
474 | c ** schema de diffusion turbulente dans la couche limite |
---|
475 | c ---------------------------------------------------- |
---|
476 | pt(:,:)=ph(:,:)*ppopsk(:,:) |
---|
477 | if (callyamada4) then |
---|
478 | call yamada4(ngrid,nlay,nq,ptimestep,g,r,pplev,pt |
---|
479 | s ,pzlev,pzlay,pu,pv,ph,pq,zcdv_true_tmp,pq2,zkv,zkh,zkq,ustar |
---|
480 | s ,9) |
---|
481 | |
---|
482 | elseif (callatke) then |
---|
483 | call call_atke(ptimestep,ngrid,nlay,zcdv_true_tmp, |
---|
484 | s zcdh_true_tmp,pu(:,1),pv(:,1),ptsrf_tmp, |
---|
485 | s pu,pv,pt,zq(:,1,igcm_h2o_vap),pplay,pplev, |
---|
486 | s pzlay,pzlev,pq2,zkv(:,1:nlay),zkh(:,1:nlay)) |
---|
487 | |
---|
488 | zkv(:,nlay+1) = zkv(:,nlay) |
---|
489 | zkh(:,nlay+1) = zkh(:,nlay) |
---|
490 | else |
---|
491 | call vdif_kc(ngrid,nlay,nq,ptimestep,g,pzlev,pzlay |
---|
492 | s ,pu,pv,ph,zcdv_true_tmp |
---|
493 | s ,pq2,zkv,zkh,zq) |
---|
494 | |
---|
495 | endif |
---|
496 | if ((doubleq).and.(ngrid.eq.1)) then |
---|
497 | kmixmin = 80. !80.! minimum eddy mix coeff in 1D |
---|
498 | do ilev=2,nlay |
---|
499 | do ig=1,ngrid |
---|
500 | zkh(ig,ilev) = max(kmixmin,zkh(ig,ilev)) |
---|
501 | zkv(ig,ilev) = max(kmixmin,zkv(ig,ilev)) |
---|
502 | end do |
---|
503 | end do |
---|
504 | end if |
---|
505 | |
---|
506 | c ** diagnostique pour le schema de turbulence |
---|
507 | c ----------------------------------------- |
---|
508 | |
---|
509 | IF(lecrit) THEN |
---|
510 | PRINT* |
---|
511 | PRINT*,'Diagnostic for the vertical turbulent mixing' |
---|
512 | PRINT*,'Cd for momentum and potential temperature' |
---|
513 | |
---|
514 | PRINT*,zcdv_tmp(ngrid/2+1),zcdh_tmp(ngrid/2+1) |
---|
515 | PRINT*,'Mixing coefficient for momentum and pot.temp.' |
---|
516 | DO ilev=1,nlay |
---|
517 | PRINT*,zkv(ngrid/2+1,ilev),zkh(ngrid/2+1,ilev) |
---|
518 | ENDDO |
---|
519 | ENDIF |
---|
520 | |
---|
521 | c----------------------------------------------------------------------- |
---|
522 | c 4. inversion pour l'implicite sur u |
---|
523 | c -------------------------------- |
---|
524 | |
---|
525 | c ** l'equation est |
---|
526 | c u(t+1) = u(t) + dt * {(du/dt)phys}(t) + dt * {(du/dt)difv}(t+1) |
---|
527 | c avec |
---|
528 | c /zu/ = u(t) + dt * {(du/dt)phys}(t) (voir paragraphe 2.) |
---|
529 | c et |
---|
530 | c dt * {(du/dt)difv}(t+1) = dt * {(d/dz)[ Ku (du/dz) ]}(t+1) |
---|
531 | c donc les entrees sont /zcdv/ pour la condition a la limite sol |
---|
532 | c et /zkv/ = Ku |
---|
533 | |
---|
534 | zb(1:ngrid,2:nlay)=zkv(1:ngrid,2:nlay)*zb0(1:ngrid,2:nlay) |
---|
535 | zb(1:ngrid,1)=zcdv_tmp(1:ngrid)*zb0(1:ngrid,1) |
---|
536 | |
---|
537 | DO ig=1,ngrid |
---|
538 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
---|
539 | zc(ig,nlay)=za(ig,nlay)*zu(ig,nlay)*z1(ig) |
---|
540 | zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
---|
541 | ENDDO |
---|
542 | |
---|
543 | DO ilay=nlay-1,1,-1 |
---|
544 | DO ig=1,ngrid |
---|
545 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
---|
546 | $ zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
---|
547 | zc(ig,ilay)=(za(ig,ilay)*zu(ig,ilay)+ |
---|
548 | $ zb(ig,ilay+1)*zc(ig,ilay+1))*z1(ig) |
---|
549 | zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
---|
550 | ENDDO |
---|
551 | ENDDO |
---|
552 | |
---|
553 | DO ig=1,ngrid |
---|
554 | zu(ig,1)=zc(ig,1) |
---|
555 | ENDDO |
---|
556 | DO ilay=2,nlay |
---|
557 | DO ig=1,ngrid |
---|
558 | zu(ig,ilay)=zc(ig,ilay)+zd(ig,ilay)*zu(ig,ilay-1) |
---|
559 | ENDDO |
---|
560 | ENDDO |
---|
561 | |
---|
562 | c----------------------------------------------------------------------- |
---|
563 | c 5. inversion pour l'implicite sur v |
---|
564 | c -------------------------------- |
---|
565 | |
---|
566 | c ** l'equation est |
---|
567 | c v(t+1) = v(t) + dt * {(dv/dt)phys}(t) + dt * {(dv/dt)difv}(t+1) |
---|
568 | c avec |
---|
569 | c /zv/ = v(t) + dt * {(dv/dt)phys}(t) (voir paragraphe 2.) |
---|
570 | c et |
---|
571 | c dt * {(dv/dt)difv}(t+1) = dt * {(d/dz)[ Kv (dv/dz) ]}(t+1) |
---|
572 | c donc les entrees sont /zcdv/ pour la condition a la limite sol |
---|
573 | c et /zkv/ = Kv |
---|
574 | |
---|
575 | DO ig=1,ngrid |
---|
576 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
---|
577 | zc(ig,nlay)=za(ig,nlay)*zv(ig,nlay)*z1(ig) |
---|
578 | zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
---|
579 | ENDDO |
---|
580 | |
---|
581 | DO ilay=nlay-1,1,-1 |
---|
582 | DO ig=1,ngrid |
---|
583 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
---|
584 | $ zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
---|
585 | zc(ig,ilay)=(za(ig,ilay)*zv(ig,ilay)+ |
---|
586 | $ zb(ig,ilay+1)*zc(ig,ilay+1))*z1(ig) |
---|
587 | zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
---|
588 | ENDDO |
---|
589 | ENDDO |
---|
590 | |
---|
591 | DO ig=1,ngrid |
---|
592 | zv(ig,1)=zc(ig,1) |
---|
593 | ENDDO |
---|
594 | DO ilay=2,nlay |
---|
595 | DO ig=1,ngrid |
---|
596 | zv(ig,ilay)=zc(ig,ilay)+zd(ig,ilay)*zv(ig,ilay-1) |
---|
597 | ENDDO |
---|
598 | ENDDO |
---|
599 | |
---|
600 | c----------------------------------------------------------------------- |
---|
601 | c Using the wind modified by friction for lifting and sublimation |
---|
602 | c ---------------------------------------------------------------- |
---|
603 | |
---|
604 | ! This is computed above and takes into account surface-atmosphere flux |
---|
605 | ! enhancement by subgrid gustiness and atmospheric-stability related |
---|
606 | ! variations of transfer coefficients. |
---|
607 | ! Calculate Cd again with wind slowed by friction |
---|
608 | c ------------------------------------------- |
---|
609 | |
---|
610 | CALL vdif_cd(ngrid,nlay,nslope,pz0,g,pzlay,pplay,zu,zv,wstar, |
---|
611 | & ptsrf,ph,mmean(:,1),zq(:,:,igcm_h2o_vap), |
---|
612 | & pqsurf(:,igcm_h2o_ice,:), .true., |
---|
613 | & zcdv_true,zcdh_true) |
---|
614 | |
---|
615 | zu2(:)=zu(:,1)*zu(:,1)+zv(:,1)*zv(:,1) |
---|
616 | |
---|
617 | DO islope = 1,nslope |
---|
618 | IF (callrichsl) THEN |
---|
619 | zcdv(:,islope)=zcdv_true(:,islope)*sqrt(zu2(:)+ |
---|
620 | & (log(1.+0.7*wstar(:) + 2.3*wstar(:)**2))**2) |
---|
621 | zcdh(:,islope)=zcdh_true(:,islope)*sqrt(zu2(:)+ |
---|
622 | & (log(1.+0.7*wstar(:) + 2.3*wstar(:)**2))**2) |
---|
623 | ELSE |
---|
624 | zcdv(:,islope)=zcdv_true(:,islope)*sqrt(zu2(:)) ! 1 / bulk aerodynamic momentum conductance |
---|
625 | zcdh(:,islope)=zcdh_true(:,islope)*sqrt(zu2(:)) ! 1 / bulk aerodynamic heat conductance |
---|
626 | ENDIF |
---|
627 | ENDDO |
---|
628 | ustar(:) = 0 |
---|
629 | tstar(:) = 0 |
---|
630 | DO ig = 1,ngrid |
---|
631 | zcdv_tmp(ig) = zcdv(ig,major_slope(ig)) |
---|
632 | zcdh_tmp(ig) = zcdh(ig,major_slope(ig)) |
---|
633 | zcdv_true_tmp(ig) = zcdv_true(ig,major_slope(ig)) |
---|
634 | zcdh_true_tmp(ig) = zcdh_true(ig,major_slope(ig)) |
---|
635 | IF (callrichsl) THEN |
---|
636 | ustar(ig)=sqrt(zcdv_true(ig,major_slope(ig))) |
---|
637 | & *sqrt(zu2(ig)+(log(1.+0.7*wstar(ig) + |
---|
638 | & 2.3*wstar(ig)**2))**2) |
---|
639 | IF (zcdh_true(ig,major_slope(ig)) .ne. 0.) THEN ! When Cd=Ch=0, u*=t*=0 |
---|
640 | tstar(ig)=(ph(ig,1)-ptsrf_tmp(ig)) |
---|
641 | & *zcdh_tmp(ig)/ustar(ig) |
---|
642 | ENDIF |
---|
643 | ELSE |
---|
644 | ustar(ig)=sqrt(zcdv_true(ig,major_slope(ig))) |
---|
645 | & *sqrt(zu2(ig)) |
---|
646 | tstar(ig)=(ph(ig,1)-ptsrf_tmp(ig)) |
---|
647 | & *zcdh_true(ig,major_slope(ig)) |
---|
648 | & /sqrt(zcdv_true(ig,major_slope(ig))) |
---|
649 | ENDIF |
---|
650 | ENDDO |
---|
651 | |
---|
652 | |
---|
653 | c----------------------------------------------------------------------- |
---|
654 | c 6. inversion pour l'implicite sur h sans oublier le couplage |
---|
655 | c avec le sol (conduction) |
---|
656 | c ------------------------ |
---|
657 | |
---|
658 | c ** l'equation est |
---|
659 | c h(t+1) = h(t) + dt * {(dh/dt)phys}(t) + dt * {(dh/dt)difv}(t+1) |
---|
660 | c avec |
---|
661 | c /zh/ = h(t) + dt * {(dh/dt)phys}(t) (voir paragraphe 2.) |
---|
662 | c et |
---|
663 | c dt * {(dh/dt)difv}(t+1) = dt * {(d/dz)[ Kh (dh/dz) ]}(t+1) |
---|
664 | c donc les entrees sont /zcdh/ pour la condition de raccord au sol |
---|
665 | c et /zkh/ = Kh |
---|
666 | c ------------- |
---|
667 | |
---|
668 | c Mass variation scheme: |
---|
669 | zb(1:ngrid,2:nlay)=zkh(1:ngrid,2:nlay)*zb0(1:ngrid,2:nlay) |
---|
670 | zb(1:ngrid,1)=zcdh_tmp(1:ngrid)*zb0(1:ngrid,1) |
---|
671 | |
---|
672 | c on initialise dm c |
---|
673 | |
---|
674 | pdtc(:,:)=0. |
---|
675 | zt(:,:)=0. |
---|
676 | dmice(:,:)=0. |
---|
677 | |
---|
678 | c ** calcul de (d Planck / dT) a la temperature d'interface |
---|
679 | c ------------------------------------------------------ |
---|
680 | |
---|
681 | z4st=4.*5.67e-8*ptimestep |
---|
682 | IF (tke_heat_flux .eq. 0.) THEN |
---|
683 | DO ig=1,ngrid |
---|
684 | indmax = major_slope(ig) |
---|
685 | zdplanck(ig)=z4st*pemis(ig,indmax)*ptsrf(ig,indmax)* |
---|
686 | & ptsrf(ig,indmax)*ptsrf(ig,indmax) |
---|
687 | ENDDO |
---|
688 | ELSE |
---|
689 | zdplanck(:)=0. |
---|
690 | ENDIF |
---|
691 | |
---|
692 | ! calcul de zc et zd pour la couche top en prenant en compte le terme |
---|
693 | ! de variation de masse (on fait une boucle pour que \E7a converge) |
---|
694 | |
---|
695 | ! Identification des points de grilles qui ont besoin de la correction |
---|
696 | |
---|
697 | llnt(:)=1 |
---|
698 | IF (.not.turb_resolved) THEN |
---|
699 | IF (callcond) THEN |
---|
700 | DO ig=1,ngrid |
---|
701 | DO l=1,nlay |
---|
702 | if(zh(ig,l) .lt. zhcond(ig,l)) then |
---|
703 | llnt(ig)=300 |
---|
704 | ! 200 and 100 do not go beyond month 9 with normal dissipation |
---|
705 | goto 5 |
---|
706 | endif |
---|
707 | ENDDO |
---|
708 | 5 continue |
---|
709 | ENDDO |
---|
710 | ENDIF |
---|
711 | |
---|
712 | ENDIF |
---|
713 | |
---|
714 | DO ig=1,ngrid |
---|
715 | indmax = major_slope(ig) |
---|
716 | ! Initialization of z1 and zd, which do not depend on dmice |
---|
717 | |
---|
718 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
---|
719 | zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
---|
720 | |
---|
721 | DO ilay=nlay-1,1,-1 |
---|
722 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
---|
723 | $ zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
---|
724 | zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
---|
725 | ENDDO |
---|
726 | |
---|
727 | ! Convergence loop |
---|
728 | |
---|
729 | DO j=1,llnt(ig) |
---|
730 | |
---|
731 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
---|
732 | zc(ig,nlay)=za(ig,nlay)*zh(ig,nlay) |
---|
733 | & -betam(ig,nlay)*dmice(ig,nlay) |
---|
734 | zc(ig,nlay)=zc(ig,nlay)*z1(ig) |
---|
735 | ! zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
---|
736 | |
---|
737 | ! calcul de zc et zd pour les couches du haut vers le bas |
---|
738 | |
---|
739 | DO ilay=nlay-1,1,-1 |
---|
740 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
---|
741 | $ zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
---|
742 | zc(ig,ilay)=(za(ig,ilay)*zh(ig,ilay)+ |
---|
743 | $ zb(ig,ilay+1)*zc(ig,ilay+1)- |
---|
744 | $ betam(ig,ilay)*dmice(ig,ilay))*z1(ig) |
---|
745 | ! zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
---|
746 | ENDDO |
---|
747 | |
---|
748 | c ** calcul de la temperature_d'interface et de sa tendance. |
---|
749 | c on ecrit que la somme des flux est nulle a l'interface |
---|
750 | c a t + \delta t, |
---|
751 | c c'est a dire le flux radiatif a {t + \delta t} |
---|
752 | c + le flux turbulent a {t + \delta t} |
---|
753 | c qui s'ecrit K (T1-Tsurf) avec T1 = d1 Tsurf + c1 |
---|
754 | c (notation K dt = /cpp*b/) |
---|
755 | c + le flux dans le sol a t |
---|
756 | c + l'evolution du flux dans le sol lorsque la temperature d'interface |
---|
757 | c passe de sa valeur a t a sa valeur a {t + \delta t}. |
---|
758 | c ---------------------------------------------------- |
---|
759 | |
---|
760 | z1(ig)=pcapcal(ig,indmax)*ptsrf(ig,indmax) |
---|
761 | s + cpp*zb(ig,1)*zc(ig,1) |
---|
762 | s + zdplanck(ig)*ptsrf(ig,indmax) |
---|
763 | s + pfluxsrf(ig,indmax)*ptimestep |
---|
764 | z2(ig)= pcapcal(ig,indmax)+cpp*zb(ig,1)*(1.-zd(ig,1)) |
---|
765 | s +zdplanck(ig) |
---|
766 | ztsrf2(ig)=z1(ig)/z2(ig) |
---|
767 | ! pdtsrf(ig)=(ztsrf2(ig)-ptsrf(ig))/ptimestep !incremented outside loop |
---|
768 | zhs(ig,1)=zc(ig,1)+zd(ig,1)*ztsrf2(ig) |
---|
769 | |
---|
770 | c ** et a partir de la temperature au sol on remonte |
---|
771 | c ----------------------------------------------- |
---|
772 | |
---|
773 | DO ilay=2,nlay |
---|
774 | zhs(ig,ilay)=zc(ig,ilay)+zd(ig,ilay)*zhs(ig,ilay-1) |
---|
775 | ENDDO |
---|
776 | DO ilay=1,nlay |
---|
777 | zt(ig,ilay)=zhs(ig,ilay)*ppopsk(ig,ilay) |
---|
778 | ENDDO |
---|
779 | |
---|
780 | c Condensation/sublimation in the atmosphere |
---|
781 | c ------------------------------------------ |
---|
782 | c (computation of zcondicea and dmice) |
---|
783 | |
---|
784 | IF (.NOT. co2clouds) then |
---|
785 | DO l=nlay , 1, -1 |
---|
786 | IF(zt(ig,l).LT.ztcond(ig,l)) THEN |
---|
787 | pdtc(ig,l)=(ztcond(ig,l) - zt(ig,l))/ptimestep |
---|
788 | zcondicea(ig,l)=(pplev(ig,l)-pplev(ig,l+1)) |
---|
789 | & *ccond*pdtc(ig,l) |
---|
790 | dmice(ig,l)= dmice(ig,l) + zcondicea(ig,l)*ptimestep |
---|
791 | END IF |
---|
792 | ENDDO |
---|
793 | ELSE |
---|
794 | DO l=nlay , 1, -1 |
---|
795 | zcondicea(ig,l)= 0.!pcondicea_co2microp(ig,l)* |
---|
796 | c & (pplev(ig,l) - pplev(ig,l+1))/g |
---|
797 | dmice(ig,l)= 0.!dmice(ig,l) + zcondicea(ig,l)*ptimestep |
---|
798 | pdtc(ig,l)=0. |
---|
799 | ENDDO |
---|
800 | ENDIF |
---|
801 | |
---|
802 | ENDDO!of Do j=1,XXX |
---|
803 | pdtsrf(ig,indmax)=(ztsrf2(ig)-ptsrf(ig,indmax))/ptimestep |
---|
804 | ENDDO !of Do ig=1,ngrid |
---|
805 | |
---|
806 | DO ig=1,ngrid ! computing sensible heat flux (atm => surface) |
---|
807 | sensibFlux(ig)=cpp*zb(ig,1)/ptimestep*(zhs(ig,1)-ztsrf2(ig)) |
---|
808 | ENDDO |
---|
809 | |
---|
810 | c Now implicit sheme on each sub-grid subslope: |
---|
811 | IF (nslope.ne.1) then |
---|
812 | DO islope=1,nslope |
---|
813 | DO ig=1,ngrid |
---|
814 | IF(islope.ne.major_slope(ig)) then |
---|
815 | IF (tke_heat_flux .eq. 0.) THEN |
---|
816 | zdplanck(ig)=z4st*pemis(ig,islope)*ptsrf(ig,islope)**3 |
---|
817 | ELSE |
---|
818 | zdplanck(ig) = 0. |
---|
819 | ENDIF |
---|
820 | zb(ig,1)=zcdh(ig,islope)*zb0(ig,1) |
---|
821 | z1(ig)=pcapcal(ig,islope)*ptsrf(ig,islope) |
---|
822 | s + cpp*zb(ig,1)*zc(ig,1) |
---|
823 | s + zdplanck(ig)*ptsrf(ig,islope) |
---|
824 | s + pfluxsrf(ig,islope)*ptimestep |
---|
825 | z2(ig)= pcapcal(ig,islope)+cpp*zb(ig,1)*(1.-zd(ig,1)) |
---|
826 | s +zdplanck(ig) |
---|
827 | ztsrf2(ig)=z1(ig)/z2(ig) |
---|
828 | pdtsrf(ig,islope)=(ztsrf2(ig)-ptsrf(ig,islope))/ptimestep |
---|
829 | ENDIF ! islope != indmax |
---|
830 | ENDDO ! ig |
---|
831 | ENDDO !islope |
---|
832 | ENDIF !nslope.ne.1 |
---|
833 | |
---|
834 | c----------------------------------------------------------------------- |
---|
835 | c TRACERS |
---|
836 | c ------- |
---|
837 | c Calcul du flux vertical au bas de la premiere couche (dust) : |
---|
838 | c ----------------------------------------------------------- |
---|
839 | do ig=1,ngrid |
---|
840 | rho(ig) = zb0(ig,1) /ptimestep |
---|
841 | c zb(ig,1) = 0. |
---|
842 | end do |
---|
843 | c Dust lifting: |
---|
844 | if (lifting) then |
---|
845 | #ifndef MESOSCALE |
---|
846 | if (doubleq.AND.submicron) then |
---|
847 | do ig=1,ngrid |
---|
848 | c if(qsurf(ig,igcm_co2).lt.1) then |
---|
849 | pdqsdif_tmp(ig,igcm_dust_mass) = |
---|
850 | & -alpha_lift(igcm_dust_mass) |
---|
851 | pdqsdif_tmp(ig,igcm_dust_number) = |
---|
852 | & -alpha_lift(igcm_dust_number) |
---|
853 | pdqsdif_tmp(ig,igcm_dust_submicron) = |
---|
854 | & -alpha_lift(igcm_dust_submicron) |
---|
855 | c end if |
---|
856 | end do |
---|
857 | else if (doubleq) then |
---|
858 | if (dustinjection.eq.0) then !injection scheme 0 (old) |
---|
859 | !or 2 (injection in CL) |
---|
860 | do ig=1,ngrid |
---|
861 | if(pqsurf_tmp(ig,igcm_co2).lt.1) then ! pas de soulevement si glace CO2 |
---|
862 | pdqsdif_tmp(ig,igcm_dust_mass) = |
---|
863 | & -alpha_lift(igcm_dust_mass) |
---|
864 | pdqsdif_tmp(ig,igcm_dust_number) = |
---|
865 | & -alpha_lift(igcm_dust_number) |
---|
866 | end if |
---|
867 | end do |
---|
868 | elseif(dustinjection.eq.1)then ! dust injection scheme = 1 injection from surface |
---|
869 | do ig=1,ngrid |
---|
870 | if(pqsurf_tmp(ig,igcm_co2).lt.1) then ! pas de soulevement si glace CO2 |
---|
871 | IF((ti_injection_sol.LE.local_time(ig)).and. |
---|
872 | & (local_time(ig).LE.tf_injection_sol)) THEN |
---|
873 | if (rdstorm) then !Rocket dust storm scheme |
---|
874 | pdqsdif_tmp(ig,igcm_stormdust_mass) = |
---|
875 | & -alpha_lift(igcm_stormdust_mass) |
---|
876 | & *dustliftday(ig) |
---|
877 | pdqsdif_tmp(ig,igcm_stormdust_number) = |
---|
878 | & -alpha_lift(igcm_stormdust_number) |
---|
879 | & *dustliftday(ig) |
---|
880 | pdqsdif_tmp(ig,igcm_dust_mass)= 0. |
---|
881 | pdqsdif_tmp(ig,igcm_dust_number)= 0. |
---|
882 | else |
---|
883 | pdqsdif_tmp(ig,igcm_dust_mass)= |
---|
884 | & -dustliftday(ig)* |
---|
885 | & alpha_lift(igcm_dust_mass) |
---|
886 | pdqsdif_tmp(ig,igcm_dust_number)= |
---|
887 | & -dustliftday(ig)* |
---|
888 | & alpha_lift(igcm_dust_number) |
---|
889 | endif |
---|
890 | if (submicron) then |
---|
891 | pdqsdif_tmp(ig,igcm_dust_submicron) = 0. |
---|
892 | endif ! if (submicron) |
---|
893 | ELSE ! outside dust injection time frame |
---|
894 | pdqsdif_tmp(ig,igcm_dust_mass)= 0. |
---|
895 | pdqsdif_tmp(ig,igcm_dust_number)= 0. |
---|
896 | if (rdstorm) then |
---|
897 | pdqsdif_tmp(ig,igcm_stormdust_mass)= 0. |
---|
898 | pdqsdif_tmp(ig,igcm_stormdust_number)= 0. |
---|
899 | end if |
---|
900 | ENDIF |
---|
901 | |
---|
902 | end if ! of if(qsurf(ig,igcm_co2).lt.1) |
---|
903 | end do |
---|
904 | endif ! end if dustinjection |
---|
905 | else if (submicron) then |
---|
906 | do ig=1,ngrid |
---|
907 | pdqsdif_tmp(ig,igcm_dust_submicron) = |
---|
908 | & -alpha_lift(igcm_dust_submicron) |
---|
909 | end do |
---|
910 | else |
---|
911 | #endif |
---|
912 | call dust_windstress_lift(ngrid,nlay,nq,rho, |
---|
913 | & zcdh_true_tmp,zcdh_tmp, |
---|
914 | & pqsurf_tmp(:,igcm_co2),pdqsdif_tmp) |
---|
915 | #ifndef MESOSCALE |
---|
916 | endif !doubleq.AND.submicron |
---|
917 | #endif |
---|
918 | else |
---|
919 | pdqsdif_tmp(1:ngrid,1:nq) = 0. |
---|
920 | end if |
---|
921 | |
---|
922 | c OU calcul de la valeur de q a la surface (water) : |
---|
923 | c ---------------------------------------- |
---|
924 | |
---|
925 | c Inversion pour l'implicite sur q |
---|
926 | c Cas des traceurs qui ne sont pas h2o_vap |
---|
927 | c h2o_vap est traite plus loin avec un sous pas de temps |
---|
928 | c hdo_vap est traite ensuite car dependant de h2o_vap |
---|
929 | c -------------------------------- |
---|
930 | |
---|
931 | do iq=1,nq !for all tracers except water vapor |
---|
932 | if ((.not. water).or.(.not. iq.eq.igcm_h2o_vap).or. |
---|
933 | & (.not. iq.eq.igcm_hdo_vap)) then |
---|
934 | |
---|
935 | |
---|
936 | zb(1:ngrid,2:nlay)=zkh(1:ngrid,2:nlay)*zb0(1:ngrid,2:nlay) |
---|
937 | zb(1:ngrid,1)=0 |
---|
938 | |
---|
939 | DO ig=1,ngrid |
---|
940 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
---|
941 | zc(ig,nlay)=za(ig,nlay)*zq(ig,nlay,iq)*z1(ig) |
---|
942 | zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
---|
943 | ENDDO |
---|
944 | |
---|
945 | DO ilay=nlay-1,2,-1 |
---|
946 | DO ig=1,ngrid |
---|
947 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
---|
948 | $ zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
---|
949 | zc(ig,ilay)=(za(ig,ilay)*zq(ig,ilay,iq)+ |
---|
950 | $ zb(ig,ilay+1)*zc(ig,ilay+1))*z1(ig) |
---|
951 | zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
---|
952 | ENDDO |
---|
953 | ENDDO |
---|
954 | |
---|
955 | if ((iq.eq.igcm_h2o_ice) |
---|
956 | $ .or. (hdo.and.(iq.eq.igcm_hdo_ice) )) then |
---|
957 | |
---|
958 | DO ig=1,ngrid |
---|
959 | z1(ig)=1./(za(ig,1)+zb(ig,1)+ |
---|
960 | $ zb(ig,2)*(1.-zd(ig,2))) |
---|
961 | zc(ig,1)=(za(ig,1)*zq(ig,1,iq)+ |
---|
962 | $ zb(ig,2)*zc(ig,2)) *z1(ig) !special case h2o_ice |
---|
963 | ENDDO |
---|
964 | else ! every other tracer |
---|
965 | DO ig=1,ngrid |
---|
966 | z1(ig)=1./(za(ig,1)+zb(ig,1)+ |
---|
967 | $ zb(ig,2)*(1.-zd(ig,2))) |
---|
968 | zc(ig,1)=(za(ig,1)*zq(ig,1,iq)+ |
---|
969 | $ zb(ig,2)*zc(ig,2) + |
---|
970 | $ (-pdqsdif_tmp(ig,iq)) *ptimestep) *z1(ig) !tracer flux from surface |
---|
971 | ENDDO |
---|
972 | endif !((iq.eq.igcm_h2o_ice) |
---|
973 | c Starting upward calculations for simple mixing of tracer (dust) |
---|
974 | DO ig=1,ngrid |
---|
975 | zq(ig,1,iq)=zc(ig,1) |
---|
976 | DO ilay=2,nlay |
---|
977 | zq(ig,ilay,iq)=zc(ig,ilay)+zd(ig,ilay)*zq(ig,ilay-1,iq) |
---|
978 | ENDDO |
---|
979 | ENDDO |
---|
980 | DO islope = 1,nslope |
---|
981 | DO ig = 1,ngrid |
---|
982 | pdqsdif(ig,iq,islope) = pdqsdif_tmp(ig,iq) |
---|
983 | & * cos(pi*def_slope_mean(islope)/180.) |
---|
984 | ENDDO |
---|
985 | ENDDO |
---|
986 | |
---|
987 | endif! ((.not. water).or.(.not. iq.eq.igcm_h2o_vap)) then |
---|
988 | enddo ! of do iq=1,nq |
---|
989 | |
---|
990 | c --------- h2o_vap -------------------------------- |
---|
991 | |
---|
992 | c Treatement of the water frost |
---|
993 | c We use a subtimestep to take into account the release of latent heat |
---|
994 | |
---|
995 | do iq=1,nq |
---|
996 | if ((water).and.(iq.eq.igcm_h2o_vap)) then |
---|
997 | |
---|
998 | DO islope = 1,nslope |
---|
999 | DO ig=1,ngrid |
---|
1000 | |
---|
1001 | zqsurf(ig)=pqsurf(ig,igcm_h2o_ice,islope)/ |
---|
1002 | & cos(pi*def_slope_mean(islope)/180.) |
---|
1003 | watercap_tmp(ig) = watercap(ig,islope)/ |
---|
1004 | & cos(pi*def_slope_mean(islope)/180.) |
---|
1005 | ENDDO ! ig=1,ngrid |
---|
1006 | |
---|
1007 | c Computation of the subtimestep |
---|
1008 | call make_tsub(ngrid,pdtsrf(:,islope),zqsurf, |
---|
1009 | & ptimestep,dtmax,watercaptag, |
---|
1010 | & nsubtimestep) |
---|
1011 | c Calculation for turbulent exchange (rho Cd,h U (qatm - qsat(Tsurf)) with the surface (for ice) |
---|
1012 | c initialization of ztsrf, which is surface temperature in |
---|
1013 | c the subtimestep. |
---|
1014 | saved_h2o_vap(:)= zq(:,1,igcm_h2o_vap) |
---|
1015 | DO ig=1,ngrid |
---|
1016 | c nsubtimestep(ig)=1 !for debug |
---|
1017 | subtimestep = ptimestep/nsubtimestep(ig) |
---|
1018 | ztsrf(ig)=ptsrf(ig,islope) ! +pdtsrf(ig)*subtimestep |
---|
1019 | zq_tmp_vap(ig,:,:) =zq(ig,:,:) |
---|
1020 | c Beginning of the subtimestep |
---|
1021 | DO tsub=1,nsubtimestep(ig) |
---|
1022 | if(tsub.eq.nsubtimestep(ig)) writeoutput = .true. |
---|
1023 | zb(1:ngrid,2:nlay)=zkh(1:ngrid,2:nlay)*zb0(1:ngrid,2:nlay) |
---|
1024 | & /float(nsubtimestep(ig)) |
---|
1025 | if(old_wsublimation_scheme) then |
---|
1026 | zb(1:ngrid,1)=zcdv(1:ngrid,islope)*zb0(1:ngrid,1) |
---|
1027 | & /float(nsubtimestep(ig)) |
---|
1028 | else |
---|
1029 | zb(1:ngrid,1)=zcdh(1:ngrid,islope)*zb0(1:ngrid,1) |
---|
1030 | & /float(nsubtimestep(ig)) |
---|
1031 | endif |
---|
1032 | zb(1:ngrid,1)=dryness(1:ngrid)*zb(1:ngrid,1) |
---|
1033 | |
---|
1034 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
---|
1035 | zc(ig,nlay)=za(ig,nlay)*zq_tmp_vap(ig,nlay,iq)*z1(ig) |
---|
1036 | zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
---|
1037 | DO ilay=nlay-1,2,-1 |
---|
1038 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
---|
1039 | $ zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
---|
1040 | zc(ig,ilay)=(za(ig,ilay)*zq_tmp_vap(ig,ilay,iq)+ |
---|
1041 | $ zb(ig,ilay+1)*zc(ig,ilay+1))*z1(ig) |
---|
1042 | zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
---|
1043 | ENDDO |
---|
1044 | z1(ig)=1./(za(ig,1)+zb(ig,1)+ |
---|
1045 | $ zb(ig,2)*(1.-zd(ig,2))) |
---|
1046 | zc(ig,1)=(za(ig,1)*zq_tmp_vap(ig,1,iq)+ |
---|
1047 | $ zb(ig,2)*zc(ig,2)) * z1(ig) |
---|
1048 | |
---|
1049 | call watersat(1,ztsrf(ig),pplev(ig,1),qsat(ig)) |
---|
1050 | old_h2o_vap(ig)=zq_tmp_vap(ig,1,igcm_h2o_vap) |
---|
1051 | zd(ig,1)=zb(ig,1)*z1(ig) |
---|
1052 | zq1temp(ig)=zc(ig,1)+ zd(ig,1)*qsat(ig) |
---|
1053 | if(old_wsublimation_scheme) then |
---|
1054 | zdqsdif_surf(ig)=rho(ig)*dryness(ig)*zcdv(ig,islope) |
---|
1055 | & *(zq1temp(ig)-qsat(ig)) |
---|
1056 | else |
---|
1057 | zdqsdif_surf(ig)=rho(ig)*dryness(ig)*zcdh(ig,islope) |
---|
1058 | & *(zq1temp(ig)-qsat(ig)) |
---|
1059 | endif |
---|
1060 | |
---|
1061 | zdqsdif_tot(ig) = zdqsdif_surf(ig) |
---|
1062 | ! -------------------------------------------------------------------------------------------------------------------------------- |
---|
1063 | ! We consider here the possible interactions between the subsurface and the atmosphere in the case of the surface is free of frost |
---|
1064 | ! when computing the complete adsorption/desorption model |
---|
1065 | ! -------------------------------------------------------------------------------------------------------------------------------- |
---|
1066 | if(.not.watercaptag(ig)) then |
---|
1067 | if (((-(zdqsdif_surf(ig))* |
---|
1068 | & subtimestep).gt.zqsurf(ig)) |
---|
1069 | & .and.(pqsurf(ig,igcm_co2,islope).eq.0.)) then |
---|
1070 | exchange = .true. |
---|
1071 | else |
---|
1072 | exchange = .false. |
---|
1073 | endif |
---|
1074 | else |
---|
1075 | exchange = .false. |
---|
1076 | endif |
---|
1077 | |
---|
1078 | ! -------------------------------------------------------------------------------------------------------------------------------- |
---|
1079 | ! If one consider adsorption, all the fluxes to/from the surface/subsurface/atmosphere are computed here |
---|
1080 | ! -------------------------------------------------------------------------------------------------------------------------------- |
---|
1081 | |
---|
1082 | if (adsorption_soil) then |
---|
1083 | call soilwater(1,nlay,nq,nsoil, nqsoil, |
---|
1084 | & ztsrf(ig),ptsoil(ig,:,islope),subtimestep, |
---|
1085 | & exchange,qsat(ig),zq_tmp_vap(ig,:,:), |
---|
1086 | & za(ig,:),zb(ig,:),zc(ig,:),zd(ig,:), |
---|
1087 | & zdqsdif_surf(ig), zqsurf(ig), |
---|
1088 | & qsoil(ig,:,:,islope), pplev(ig,1), rho(ig), |
---|
1089 | & writeoutput,zdqsdif_regolith(ig,islope), |
---|
1090 | & zq1temp_regolith(ig), |
---|
1091 | & pore_icefraction(ig,:,islope)) |
---|
1092 | |
---|
1093 | |
---|
1094 | if(.not.watercaptag(ig)) then |
---|
1095 | if (exchange) then |
---|
1096 | zq1temp(ig) = zq1temp_regolith(ig) |
---|
1097 | zdqsdif_tot(ig)= |
---|
1098 | & -zqsurf(ig)/subtimestep |
---|
1099 | else |
---|
1100 | zdqsdif_tot(ig) = zdqsdif_surf(ig) + |
---|
1101 | & zdqsdif_regolith(ig,islope) ! boundary condition = qsat, but pdqsdif is calculated to update qsurf (including loss of surface ice to the subsurface) |
---|
1102 | endif ! of "if exchange = true" |
---|
1103 | endif ! of "if not.watercaptag" |
---|
1104 | endif ! adsorption |
---|
1105 | ! -------------------------------------------------------------------------------------------------------------------------------------- |
---|
1106 | ! Here we do the same, but without computing the complete adsorpption/desorption. Note that it work only if one does not use adsorption |
---|
1107 | ! If no subsurface ice, then the models computes the surface flux/water vapor flux as usual |
---|
1108 | ! -------------------------------------------------------------------------------------------------------------------------------------- |
---|
1109 | |
---|
1110 | ! ------------------------------------------------------------------------------------------------------------------------------------------ |
---|
1111 | ! First, We consider here the possible interactions between the subsurface and the atmosphere in the case of the surface is free of frost |
---|
1112 | ! ------------------------------------------------------------------------------------------------------------------------------------------ |
---|
1113 | |
---|
1114 | if(.not.watercaptag(ig).and.(.not.adsorption_soil)) then |
---|
1115 | if ((((-zdqsdif_tot(ig)*subtimestep) |
---|
1116 | & .ge.(zqsurf(ig)))) |
---|
1117 | & .or. |
---|
1118 | & (((-zdqsdif_tot(ig)*subtimestep) |
---|
1119 | & .lt.(zqsurf(ig))) |
---|
1120 | & .and. ((zqsurf(ig).lt.tol_frost)) |
---|
1121 | & .and.lag_layer)) then |
---|
1122 | |
---|
1123 | if ((-zdqsdif_tot(ig)*subtimestep) |
---|
1124 | & .ge.(zqsurf(ig))) then |
---|
1125 | zdqsdif_tot(ig)=-zqsurf(ig)/subtimestep |
---|
1126 | endif |
---|
1127 | |
---|
1128 | if((h2o_ice_depth(ig,islope).gt.0) |
---|
1129 | & .and. (zqsurf(ig) .lt. tol_frost) |
---|
1130 | & .and.lag_layer) then |
---|
1131 | ! Atm <-> subsurface exchange, we need to update the exchange coefficient zb by a factor 1/1+R; R = zice*Cd,h*/D and add the flux from the subsurface |
---|
1132 | ! zqsurf(ig) = 0 |
---|
1133 | if(old_wsublimation_scheme) then |
---|
1134 | resist(ig,islope)=h2o_ice_depth(ig,islope) |
---|
1135 | & *zcdv(ig,islope)/d_coef(ig,islope) |
---|
1136 | else |
---|
1137 | resist(ig,islope)=h2o_ice_depth(ig,islope) |
---|
1138 | & *zcdh(ig,islope)/d_coef(ig,islope) |
---|
1139 | endif |
---|
1140 | |
---|
1141 | zb(ig,1)=zb(ig,1)*1/(1+resist(ig,islope)) ! change zb to account subsurface ice |
---|
1142 | ! Now we add the flux from the subsurface ice : rho Cd,h U*(1/1+R) * (q1-qsat_ssi(Tice)) |
---|
1143 | |
---|
1144 | call compute_Tice(nsoil, ptsoil(ig,:,islope), |
---|
1145 | & ztsrf(ig), |
---|
1146 | & h2o_ice_depth(ig,islope), |
---|
1147 | & Tice(ig,islope)) ! compute ice temperature |
---|
1148 | |
---|
1149 | call watersat(1,Tice(ig,islope),pplev(ig,1), |
---|
1150 | & qsat_ssi(ig,islope)) |
---|
1151 | |
---|
1152 | qsat_ssi(ig,islope)=ztsrf(ig)/Tice(ig,islope) |
---|
1153 | & *qsat_ssi(ig,islope) |
---|
1154 | |
---|
1155 | ! And now we solve correctly the system |
---|
1156 | z1(ig)=1./(za(ig,1)+zb(ig,1)+ |
---|
1157 | & zb(ig,2)*(1.-zd(ig,2))) |
---|
1158 | zc(ig,1)=(za(ig,1)*zq_tmp_vap(ig,1,iq)+ |
---|
1159 | & zb(ig,2)*zc(ig,2) + |
---|
1160 | & (-zdqsdif_tot(ig)) *subtimestep) |
---|
1161 | & * z1(ig) |
---|
1162 | zd(ig,1)=zb(ig,1)*z1(ig) |
---|
1163 | zq1temp(ig)=zc(ig,1)+ zd(ig,1) |
---|
1164 | & *qsat_ssi(ig,islope) |
---|
1165 | |
---|
1166 | ! Flux from the subsurface |
---|
1167 | if(old_wsublimation_scheme) then |
---|
1168 | zdqsdif_ssi_atm(ig,islope)=rho(ig) |
---|
1169 | & *dryness(ig)*zcdv(ig,islope) |
---|
1170 | & *1/(1+resist(ig,islope)) |
---|
1171 | & *(zq1temp(ig)-qsat_ssi(ig,islope)) |
---|
1172 | else |
---|
1173 | zdqsdif_ssi_atm(ig,islope)=rho(ig)* |
---|
1174 | & *dryness(ig) *zcdh(ig,islope) |
---|
1175 | & *1/(1+resist(ig,islope)) |
---|
1176 | & *(zq1temp(ig)-qsat_ssi(ig,islope)) |
---|
1177 | endif |
---|
1178 | |
---|
1179 | else |
---|
1180 | ! No atm <-> subsurface exchange, we do it the usual way |
---|
1181 | zdqsdif_tot(ig)=-zqsurf(ig)/subtimestep |
---|
1182 | z1(ig)=1./(za(ig,1)+ zb(ig,2)*(1.-zd(ig,2))) |
---|
1183 | zc(ig,1)=(za(ig,1)* |
---|
1184 | & zq_tmp_vap(ig,1,igcm_h2o_vap)+ |
---|
1185 | & zb(ig,2)*zc(ig,2) + |
---|
1186 | & (-zdqsdif_tot(ig)) *subtimestep) *z1(ig) |
---|
1187 | zq1temp(ig)=zc(ig,1) |
---|
1188 | endif ! Of subsurface <-> atmosphere exchange |
---|
1189 | endif ! sublimating more than available frost & surface - frost exchange |
---|
1190 | endif !if .not.watercaptag(ig) |
---|
1191 | |
---|
1192 | ! -------------------------------------------------------------------------------------------------------------------------------- |
---|
1193 | ! We check possible frost subsurface ice interaction: since there is no subsurface water ice mass reservoir represented (yet), |
---|
1194 | ! we do not include their effect on the mass of surface frost. |
---|
1195 | ! -------------------------------------------------------------------------------------------------------------------------------- |
---|
1196 | |
---|
1197 | if((h2o_ice_depth(ig,islope).gt.0).and.lag_layer |
---|
1198 | & .and.(.not.adsorption_soil)) then |
---|
1199 | ! First case: still frost at the surface but no watercaptag |
---|
1200 | if(((watercaptag(ig))).or. |
---|
1201 | & (((-zdqsdif_tot(ig)*subtimestep) |
---|
1202 | & .lt.(zqsurf(ig))) |
---|
1203 | & .and. (zqsurf(ig).gt.tol_frost))) then |
---|
1204 | ! Still frost at the surface: we consider the possibility to have subsurface <-> frost exchange |
---|
1205 | ! The flux between frost and ssi is D/zice *(qsat(Tsurf)-qsat_ssi(Tice)) |
---|
1206 | call compute_Tice(nsoil, ptsoil(ig,:,islope), |
---|
1207 | & ztsrf(ig), |
---|
1208 | & h2o_ice_depth(ig,islope), |
---|
1209 | & Tice(ig,islope)) ! compute ice temperature |
---|
1210 | |
---|
1211 | call watersat(1,Tice(ig,islope),pplev(ig,1), |
---|
1212 | & qsat_ssi(ig,islope)) |
---|
1213 | |
---|
1214 | qsat_ssi(ig,islope)=ztsrf(ig)/Tice(ig,islope) |
---|
1215 | & *qsat_ssi(ig,islope) |
---|
1216 | |
---|
1217 | zdqsdif_ssi_frost(ig,islope)= d_coef(ig,islope) |
---|
1218 | & /h2o_ice_depth(ig,islope) |
---|
1219 | & *rho(ig)*dryness(ig) |
---|
1220 | & *(qsat(ig)-qsat_ssi(ig,islope)) |
---|
1221 | |
---|
1222 | ! Line to comment for now since we don't have a mass of subsurface frost |
---|
1223 | ! in our computation (otherwise, we would not conserve the H2O mass in |
---|
1224 | ! the system) |
---|
1225 | if ((-zdqsdif_tot(ig)+zdqsdif_ssi_frost(ig,islope)) |
---|
1226 | & *subtimestep.ge.(zqsurf(ig))) then |
---|
1227 | zdqsdif_ssi_frost(ig,islope) = |
---|
1228 | & zqsurf(ig)/subtimestep |
---|
1229 | & + zdqsdif_tot(ig) |
---|
1230 | endif |
---|
1231 | |
---|
1232 | zdqsdif_tot(ig) = zdqsdif_tot(ig) - |
---|
1233 | & zdqsdif_ssi_frost(ig,islope) |
---|
1234 | endif ! watercaptag or frost at the surface |
---|
1235 | endif ! interaction frost <-> subsurface ice |
---|
1236 | |
---|
1237 | |
---|
1238 | c Starting upward calculations for water : |
---|
1239 | zq_tmp_vap(ig,1,igcm_h2o_vap)=zq1temp(ig) |
---|
1240 | c Take into account the H2O latent heat impact on the surface temperature |
---|
1241 | if (latentheat_surfwater) then |
---|
1242 | lh=(2834.3-0.28*(ztsrf(ig)-To)- |
---|
1243 | & 0.004*(ztsrf(ig)-To)*(ztsrf(ig)-To))*1.e+3 |
---|
1244 | zdtsrf(ig,islope)= zdqsdif_tot(ig)*lh |
---|
1245 | & /pcapcal(ig,islope) |
---|
1246 | endif ! (latentheat_surfwater) then |
---|
1247 | |
---|
1248 | DO ilay=2,nlay |
---|
1249 | zq_tmp_vap(ig,ilay,iq)=zc(ig,ilay)+zd(ig,ilay) |
---|
1250 | & *zq_tmp_vap(ig,ilay-1,iq) |
---|
1251 | ENDDO |
---|
1252 | c Subtimestep water budget : |
---|
1253 | ztsrf(ig) = ztsrf(ig)+(pdtsrf(ig,islope) |
---|
1254 | & + zdtsrf(ig,islope))*subtimestep |
---|
1255 | zqsurf(ig)= zqsurf(ig)+( |
---|
1256 | & zdqsdif_tot(ig))*subtimestep |
---|
1257 | |
---|
1258 | if (zqsurf(ig)<0 .and.(.not.watercaptag(ig))) then |
---|
1259 | zqsurf(ig)=0 |
---|
1260 | endif |
---|
1261 | zdqsdif_ssi_atm_tot(ig,islope) = |
---|
1262 | & zdqsdif_ssi_atm_tot(ig,islope) |
---|
1263 | & + zdqsdif_ssi_atm(ig,islope)*subtimestep |
---|
1264 | zdqsdif_ssi_frost_tot(ig,islope) = |
---|
1265 | & zdqsdif_ssi_frost_tot(ig,islope) |
---|
1266 | & +zdqsdif_ssi_frost(ig,islope)*subtimestep |
---|
1267 | c Monitoring instantaneous latent heat flux in W.m-2 : |
---|
1268 | zsurf_h2o_lh(ig,islope) = zsurf_h2o_lh(ig,islope)+ |
---|
1269 | & (zdtsrf(ig,islope)*pcapcal(ig,islope)) |
---|
1270 | & *subtimestep |
---|
1271 | |
---|
1272 | c We ensure that surface temperature can't rise above the solid domain if there |
---|
1273 | c is still ice on the surface (oldschool) |
---|
1274 | if(zqsurf(ig) |
---|
1275 | & +zdqsdif_tot(ig)*subtimestep |
---|
1276 | & .gt.frost_albedo_threshold) then ! if there is still ice, T cannot exceed To |
---|
1277 | zdtsrf(ig,islope) = min(zdtsrf(ig,islope), |
---|
1278 | & (To-ztsrf(ig))/subtimestep) ! ice melt case |
---|
1279 | endif |
---|
1280 | |
---|
1281 | c End of the subtimestep |
---|
1282 | ENDDO ! tsub=1,nsubtimestep |
---|
1283 | |
---|
1284 | c Integration of subtimestep temp and water budget : |
---|
1285 | c (btw could also compute the post timestep temp and ice |
---|
1286 | c by simply adding the subtimestep trend instead of this) |
---|
1287 | surf_h2o_lh(ig,islope)= zsurf_h2o_lh(ig,islope)/ptimestep |
---|
1288 | pdtsrf(ig,islope)= (ztsrf(ig) - |
---|
1289 | & ptsrf(ig,islope))/ptimestep |
---|
1290 | pdqsdif(ig,igcm_h2o_ice,islope)= |
---|
1291 | & (zqsurf(ig)- pqsurf(ig,igcm_h2o_ice,islope)/ |
---|
1292 | & cos(pi*def_slope_mean(islope)/180.)) |
---|
1293 | & /ptimestep |
---|
1294 | |
---|
1295 | zdqsdif_ssi_atm_tot(ig,islope)= |
---|
1296 | & zdqsdif_ssi_atm_tot(ig,islope)/ptimestep |
---|
1297 | zdqsdif_ssi_frost_tot(ig,islope)= |
---|
1298 | & zdqsdif_ssi_frost_tot(ig,islope)/ptimestep |
---|
1299 | zdqsdif_ssi_tot(ig,islope) = |
---|
1300 | & zdqsdif_ssi_atm_tot(ig,islope) |
---|
1301 | & + zdqsdif_ssi_frost_tot(ig,islope) |
---|
1302 | c if subliming more than qsurf(ice) and on watercaptag, water |
---|
1303 | c sublimates from watercap reservoir (dwatercap_dif is <0) |
---|
1304 | if(watercaptag(ig)) then |
---|
1305 | if ((-pdqsdif(ig,igcm_h2o_ice,islope)*ptimestep) |
---|
1306 | & .gt.(pqsurf(ig,igcm_h2o_ice,islope) |
---|
1307 | & /cos(pi*def_slope_mean(islope)/180.))) then |
---|
1308 | dwatercap_dif(ig,islope)= |
---|
1309 | & pdqsdif(ig,igcm_h2o_ice,islope)+ |
---|
1310 | & (pqsurf(ig,igcm_h2o_ice,islope) / |
---|
1311 | & cos(pi*def_slope_mean(islope)/180.))/ptimestep |
---|
1312 | pdqsdif(ig,igcm_h2o_ice,islope)= |
---|
1313 | & - (pqsurf(ig,igcm_h2o_ice,islope)/ |
---|
1314 | & cos(pi*def_slope_mean(islope)/180.))/ptimestep |
---|
1315 | endif! ((-pdqsdif(ig)*ptimestep) |
---|
1316 | endif !(watercaptag(ig)) then |
---|
1317 | zq_slope_vap(ig,:,:,islope) = zq_tmp_vap(ig,:,:) |
---|
1318 | ENDDO ! of DO ig=1,ngrid |
---|
1319 | ENDDO ! islope |
---|
1320 | c Some grid box averages: interface with the atmosphere |
---|
1321 | DO ig = 1,ngrid |
---|
1322 | DO ilay = 1,nlay |
---|
1323 | zq(ig,ilay,iq) = 0. |
---|
1324 | DO islope = 1,nslope |
---|
1325 | zq(ig,ilay,iq) = zq(ig,ilay,iq) + |
---|
1326 | $ zq_slope_vap(ig,ilay,iq,islope) * |
---|
1327 | $ subslope_dist(ig,islope) |
---|
1328 | ENDDO |
---|
1329 | ENDDO |
---|
1330 | ENDDO |
---|
1331 | ! Recompute values in kg/m^2 slopped |
---|
1332 | DO ig = 1,ngrid |
---|
1333 | DO islope = 1,nslope |
---|
1334 | pdqsdif(ig,igcm_h2o_ice,islope) = |
---|
1335 | & pdqsdif(ig,igcm_h2o_ice,islope) |
---|
1336 | & * cos(pi*def_slope_mean(islope)/180.) |
---|
1337 | |
---|
1338 | dwatercap_dif(ig,islope) = |
---|
1339 | & dwatercap_dif(ig,islope) |
---|
1340 | & * cos(pi*def_slope_mean(islope)/180.) |
---|
1341 | ENDDO |
---|
1342 | ENDDO |
---|
1343 | |
---|
1344 | END IF ! of IF ((water).and.(iq.eq.igcm_h2o_vap)) |
---|
1345 | |
---|
1346 | c --------- end of h2o_vap ---------------------------- |
---|
1347 | |
---|
1348 | c --------- hdo_vap ----------------------------------- |
---|
1349 | |
---|
1350 | c hdo_ice has already been with along h2o_ice |
---|
1351 | c amongst "normal" tracers (ie not h2o_vap) |
---|
1352 | |
---|
1353 | if (hdo.and.(iq.eq.igcm_hdo_vap)) then |
---|
1354 | zb(1:ngrid,2:nlay)=zkh(1:ngrid,2:nlay)*zb0(1:ngrid,2:nlay) |
---|
1355 | zb(1:ngrid,1)=0 |
---|
1356 | |
---|
1357 | DO ig=1,ngrid |
---|
1358 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
---|
1359 | zc(ig,nlay)=za(ig,nlay)*zq(ig,nlay,iq)*z1(ig) |
---|
1360 | zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
---|
1361 | ENDDO |
---|
1362 | |
---|
1363 | DO ilay=nlay-1,2,-1 |
---|
1364 | DO ig=1,ngrid |
---|
1365 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
---|
1366 | $ zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
---|
1367 | zc(ig,ilay)=(za(ig,ilay)*zq(ig,ilay,iq)+ |
---|
1368 | $ zb(ig,ilay+1)*zc(ig,ilay+1))*z1(ig) |
---|
1369 | zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
---|
1370 | ENDDO |
---|
1371 | ENDDO |
---|
1372 | hdoflux_meshavg(:) = 0. |
---|
1373 | DO islope = 1,nslope |
---|
1374 | |
---|
1375 | pdqsdif_tmphdo(:,:) = pdqsdif(:,:,islope) |
---|
1376 | & /cos(pi*def_slope_mean(islope)/180.) |
---|
1377 | |
---|
1378 | call watersat(ngrid,pdtsrf(:,islope)*ptimestep + |
---|
1379 | & ptsrf(:,islope),pplev(:,1),qsat_tmp) |
---|
1380 | |
---|
1381 | CALL hdo_surfex(ngrid,nlay,nq,ptimestep, |
---|
1382 | & zt,pplay,zq,pqsurf(:,:,islope), |
---|
1383 | & saved_h2o_vap,qsat_tmp, |
---|
1384 | & pdqsdif_tmphdo, |
---|
1385 | & dwatercap_dif(:,islope)/cos(pi*def_slope_mean(islope)/180.), |
---|
1386 | & hdoflux(:,islope)) |
---|
1387 | |
---|
1388 | pdqsdif(:,:,islope) = pdqsdif_tmphdo(:,:) * |
---|
1389 | & cos(pi*def_slope_mean(islope)/180.) |
---|
1390 | DO ig = 1,ngrid |
---|
1391 | hdoflux_meshavg(ig) = hdoflux_meshavg(ig) + |
---|
1392 | & hdoflux(ig,islope)*subslope_dist(ig,islope) |
---|
1393 | |
---|
1394 | ENDDO !ig = 1,ngrid |
---|
1395 | ENDDO !islope = 1,nslope |
---|
1396 | |
---|
1397 | DO ig=1,ngrid |
---|
1398 | z1(ig)=1./(za(ig,1)+zb(ig,1)+ |
---|
1399 | $ zb(ig,2)*(1.-zd(ig,2))) |
---|
1400 | zc(ig,1)=(za(ig,1)*zq(ig,1,iq)+ |
---|
1401 | $ zb(ig,2)*zc(ig,2) + |
---|
1402 | $ (-hdoflux_meshavg(ig)) *ptimestep) *z1(ig) !tracer flux from surface |
---|
1403 | ENDDO |
---|
1404 | |
---|
1405 | DO ig=1,ngrid |
---|
1406 | zq(ig,1,iq)=zc(ig,1) |
---|
1407 | DO ilay=2,nlay |
---|
1408 | zq(ig,ilay,iq)=zc(ig,ilay)+zd(ig,ilay)*zq(ig,ilay-1,iq) |
---|
1409 | ENDDO |
---|
1410 | ENDDO |
---|
1411 | endif ! (hdo.and.(iq.eq.igcm_hdo_vap)) |
---|
1412 | |
---|
1413 | c --------- end of hdo ---------------------------- |
---|
1414 | |
---|
1415 | enddo ! of do iq=1,nq |
---|
1416 | |
---|
1417 | c --------- end of tracers ---------------------------- |
---|
1418 | |
---|
1419 | call write_output("surf_h2o_lh", |
---|
1420 | & "Ground ice latent heat flux", |
---|
1421 | & "W.m-2",surf_h2o_lh(:,iflat)) |
---|
1422 | |
---|
1423 | call write_output('zdqsdif_ssi_frost_tot', |
---|
1424 | & 'Flux between frost and subsurface ice','kg.m-2.s-1', |
---|
1425 | & zdqsdif_ssi_frost_tot(:,iflat)) |
---|
1426 | |
---|
1427 | call write_output('zdqsdif_ssi_atm_tot', |
---|
1428 | & 'Flux between atmosphere and subsurface ice','kg.m-2.s-1', |
---|
1429 | & zdqsdif_ssi_atm_tot(:,iflat)) |
---|
1430 | |
---|
1431 | call write_output('zdqsdif_ssi_tot', |
---|
1432 | & 'Total flux echange with subsurface ice','kg.m-2.s-1', |
---|
1433 | & zdqsdif_ssi_tot(:,iflat)) |
---|
1434 | |
---|
1435 | |
---|
1436 | C Diagnostic output for HDO |
---|
1437 | ! if (hdo) then |
---|
1438 | ! CALL write_output('hdoflux', |
---|
1439 | ! & 'hdoflux', |
---|
1440 | ! & ' ',hdoflux_meshavg(:)) |
---|
1441 | ! CALL write_output('h2oflux', |
---|
1442 | ! & 'h2oflux', |
---|
1443 | ! & ' ',h2oflux(:)) |
---|
1444 | ! endif |
---|
1445 | |
---|
1446 | c----------------------------------------------------------------------- |
---|
1447 | c 8. calcul final des tendances de la diffusion verticale |
---|
1448 | c ---------------------------------------------------- |
---|
1449 | |
---|
1450 | DO ilev = 1, nlay |
---|
1451 | DO ig=1,ngrid |
---|
1452 | pdudif(ig,ilev)=( zu(ig,ilev)- |
---|
1453 | $ (pu(ig,ilev)+pdufi(ig,ilev)*ptimestep) )/ptimestep |
---|
1454 | pdvdif(ig,ilev)=( zv(ig,ilev)- |
---|
1455 | $ (pv(ig,ilev)+pdvfi(ig,ilev)*ptimestep) )/ptimestep |
---|
1456 | hh = ph(ig,ilev)+pdhfi(ig,ilev)*ptimestep |
---|
1457 | $ + (latcond*dmice(ig,ilev)/cpp)/ppopsk(ig,ilev) |
---|
1458 | pdhdif(ig,ilev)=( zhs(ig,ilev)- hh )/ptimestep |
---|
1459 | ENDDO |
---|
1460 | ENDDO |
---|
1461 | |
---|
1462 | pdqdif(1:ngrid,1:nlay,1:nq)=(zq(1:ngrid,1:nlay,1:nq)- |
---|
1463 | & (pq(1:ngrid,1:nlay,1:nq) |
---|
1464 | & +pdqfi(1:ngrid,1:nlay,1:nq) |
---|
1465 | & *ptimestep))/ptimestep |
---|
1466 | |
---|
1467 | c ** diagnostique final |
---|
1468 | c ------------------ |
---|
1469 | |
---|
1470 | IF(lecrit) THEN |
---|
1471 | PRINT*,'In vdif' |
---|
1472 | PRINT*,'Ts (t) and Ts (t+st)' |
---|
1473 | WRITE(*,'(a10,3a15)') |
---|
1474 | s 'theta(t)','theta(t+dt)','u(t)','u(t+dt)' |
---|
1475 | PRINT*,ptsrf(ngrid/2+1,:),ztsrf2(ngrid/2+1) |
---|
1476 | DO ilev=1,nlay |
---|
1477 | WRITE(*,'(4f15.7)') |
---|
1478 | s ph(ngrid/2+1,ilev),zhs(ngrid/2+1,ilev), |
---|
1479 | s pu(ngrid/2+1,ilev),zu(ngrid/2+1,ilev) |
---|
1480 | |
---|
1481 | ENDDO |
---|
1482 | ENDIF |
---|
1483 | |
---|
1484 | END SUBROUTINE vdifc |
---|
1485 | |
---|
1486 | c==================================== |
---|
1487 | |
---|
1488 | SUBROUTINE make_tsub(naersize,dtsurf,qsurf,ptimestep, |
---|
1489 | $ dtmax,watercaptag,ntsub) |
---|
1490 | |
---|
1491 | c Pas de temps adaptatif en estimant le taux de sublimation |
---|
1492 | c et en adaptant avec un critere "dtmax" du chauffage a accomoder |
---|
1493 | c dtmax est regle empiriquement (pour l'instant) a 0.5 K |
---|
1494 | use surfdat_h, only: frost_albedo_threshold |
---|
1495 | |
---|
1496 | integer,intent(in) :: naersize |
---|
1497 | real,intent(in) :: dtsurf(naersize) |
---|
1498 | real,intent(in) :: qsurf(naersize) |
---|
1499 | logical,intent(in) :: watercaptag(naersize) |
---|
1500 | real,intent(in) :: ptimestep |
---|
1501 | real,intent(in) :: dtmax |
---|
1502 | real :: ztsub(naersize) |
---|
1503 | integer :: i |
---|
1504 | integer,intent(out) :: ntsub(naersize) |
---|
1505 | |
---|
1506 | do i=1,naersize |
---|
1507 | c If not on permanent ice or thin frost layer : |
---|
1508 | c do not use a subtimestep (ntsub=1) |
---|
1509 | if ((qsurf(i).lt.frost_albedo_threshold).and. |
---|
1510 | & (.not.watercaptag(i))) then |
---|
1511 | ntsub(i) = 1 |
---|
1512 | else |
---|
1513 | ztsub(i) = ptimestep * dtsurf(i) / dtmax |
---|
1514 | ntsub(i) = ceiling(abs(ztsub(i))) |
---|
1515 | endif ! (qsurf(i).eq.0) then |
---|
1516 | c |
---|
1517 | c write(78,*), dtsurf*ptimestep, dtsurf, ntsub |
---|
1518 | enddo! 1=1,ngrid |
---|
1519 | |
---|
1520 | |
---|
1521 | |
---|
1522 | END SUBROUTINE make_tsub |
---|
1523 | |
---|
1524 | |
---|
1525 | c==================================== |
---|
1526 | |
---|
1527 | SUBROUTINE compute_Tice(nsoil, ptsoil, ptsurf, ice_depth, Tice) |
---|
1528 | |
---|
1529 | c Compute subsurface ice temperature by interpolating the temperatures between the two adjacent cells. |
---|
1530 | use comsoil_h, only: layer, mlayer |
---|
1531 | |
---|
1532 | implicit none |
---|
1533 | integer,intent(in) :: nsoil ! Number of soil layers |
---|
1534 | real,intent(in) :: ptsoil(nsoil) ! Soil temperature (K) |
---|
1535 | real,intent(in) :: ptsurf ! Soil temperature (K) |
---|
1536 | real,intent(in) :: ice_depth ! Ice depth (m) |
---|
1537 | real,intent(out) :: Tice ! Ice temperatures (K) |
---|
1538 | |
---|
1539 | c Local |
---|
1540 | integer :: ik ! Loop variables |
---|
1541 | integer :: indexice ! Index of the ice |
---|
1542 | |
---|
1543 | c Code: |
---|
1544 | indexice = -1 |
---|
1545 | if(ice_depth.lt.mlayer(0)) then |
---|
1546 | indexice = 0. |
---|
1547 | else |
---|
1548 | do ik = 0,nsoil-2 ! go through all the layers to find the ice locations |
---|
1549 | if((mlayer(ik).le.ice_depth).and. |
---|
1550 | & (mlayer(ik+1).gt.ice_depth)) then |
---|
1551 | indexice = ik+1 |
---|
1552 | exit |
---|
1553 | endif |
---|
1554 | enddo |
---|
1555 | endif |
---|
1556 | |
---|
1557 | if(indexice.lt.0) then |
---|
1558 | call abort_physic("vdifc - compute Tice", |
---|
1559 | & "subsurface ice is below the last soil layer",1) |
---|
1560 | else |
---|
1561 | if(indexice .ge. 1) then ! Linear inteprolation between soil temperature |
---|
1562 | Tice = (ptsoil(indexice)-ptsoil(indexice+1)) |
---|
1563 | & /(mlayer(indexice-1)-mlayer(indexice)) |
---|
1564 | & *(ice_depth-mlayer(indexice)) + ptsoil(indexice+1) |
---|
1565 | else ! Linear inteprolation between the 1st soil temperature and the surface temperature |
---|
1566 | Tice = (ptsoil(1) - ptsurf)/mlayer(0) |
---|
1567 | & *(ice_depth-mlayer(0)) + ptsoil(1) |
---|
1568 | endif ! index ice >=0 |
---|
1569 | endif !indexice <0 |
---|
1570 | |
---|
1571 | |
---|
1572 | END SUBROUTINE compute_Tice |
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1573 | END MODULE vdifc_mod |
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