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 | $ pdufi,pdvfi,pdhfi,pdqfi,pfluxsrf, |
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12 | $ pdudif,pdvdif,pdhdif,pdtsrf,pq2, |
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13 | $ pdqdif,pdqsdif,wstar,zcdv_true,zcdh_true, |
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14 | $ hfmax,pcondicea_co2microp,sensibFlux, |
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15 | $ dustliftday,local_time,watercap, dwatercap_dif) |
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16 | |
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17 | use tracer_mod, only: noms, igcm_dust_mass, igcm_dust_number, |
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18 | & igcm_dust_submicron, igcm_h2o_vap, |
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19 | & igcm_h2o_ice, alpha_lift, igcm_co2, |
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20 | & igcm_hdo_vap, igcm_hdo_ice, |
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21 | & igcm_stormdust_mass, igcm_stormdust_number |
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22 | use surfdat_h, only: watercaptag, frost_albedo_threshold, dryness, |
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23 | & old_wsublimation_scheme |
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24 | USE comcstfi_h, ONLY: cpp, r, rcp, g, pi |
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25 | use watersat_mod, only: watersat |
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26 | use turb_mod, only: turb_resolved, ustar, tstar |
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27 | use compute_dtau_mod, only: ti_injection_sol,tf_injection_sol |
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28 | use hdo_surfex_mod, only: hdo_surfex |
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29 | c use geometry_mod, only: longitude_deg,latitude_deg ! Joseph |
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30 | use dust_param_mod, only: doubleq, submicron, lifting |
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31 | use write_output_mod, only: write_output |
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32 | use comslope_mod, ONLY: nslope,def_slope,def_slope_mean, |
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33 | & subslope_dist,major_slope,iflat |
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34 | use microphys_h, only: To |
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35 | use paleoclimate_mod, only: d_coef,h2o_ice_depth,lag_layer |
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36 | use comsoil_h, only: layer, mlayer,adsorption_soil |
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37 | use vdif_cd_mod, only: vdif_cd |
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38 | use lmdz_call_atke, only: call_atke |
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39 | IMPLICIT NONE |
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40 | |
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41 | c======================================================================= |
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42 | c |
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43 | c subject: |
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44 | c -------- |
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45 | c Turbulent diffusion (mixing) for potential T, U, V and tracer |
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46 | c |
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47 | c Shema implicite |
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48 | c On commence par rajouter au variables x la tendance physique |
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49 | c et on resoult en fait: |
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50 | c x(t+1) = x(t) + dt * (dx/dt)phys(t) + dt * (dx/dt)difv(t+1) |
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51 | c |
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52 | c author: |
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53 | c ------ |
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54 | c Hourdin/Forget/Fournier |
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55 | c======================================================================= |
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56 | |
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57 | c----------------------------------------------------------------------- |
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58 | c declarations: |
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59 | c ------------- |
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60 | |
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61 | include "callkeys.h" |
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62 | |
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63 | c |
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64 | c arguments: |
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65 | c ---------- |
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66 | |
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67 | INTEGER,INTENT(IN) :: ngrid,nlay,nsoil,nqsoil |
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68 | REAL,INTENT(IN) :: ptimestep |
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69 | REAL,INTENT(IN) :: pplay(ngrid,nlay),pplev(ngrid,nlay+1) |
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70 | REAL,INTENT(IN) :: pzlay(ngrid,nlay),pzlev(ngrid,nlay+1) |
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71 | REAL,INTENT(IN) :: pu(ngrid,nlay),pv(ngrid,nlay) |
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72 | REAL,INTENT(IN) :: ph(ngrid,nlay) |
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73 | REAL,INTENT(IN) :: ptsrf(ngrid,nslope),pemis(ngrid,nslope) |
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74 | REAL,INTENT(IN) :: pdufi(ngrid,nlay),pdvfi(ngrid,nlay) |
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75 | REAL,INTENT(IN) :: pdhfi(ngrid,nlay) |
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76 | REAL,INTENT(IN) :: pfluxsrf(ngrid,nslope) |
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77 | REAL,INTENT(OUT) :: pdudif(ngrid,nlay),pdvdif(ngrid,nlay) |
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78 | REAL,INTENT(OUT) :: pdtsrf(ngrid,nslope),pdhdif(ngrid,nlay) |
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79 | REAL,INTENT(IN) :: pcapcal(ngrid,nslope) |
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80 | REAL,INTENT(INOUT) :: pq2(ngrid,nlay+1) |
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81 | REAL,INTENT(IN) :: ptsoil(ngrid,nsoil,nslope) |
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82 | |
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83 | c Argument added for condensation: |
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84 | REAL,INTENT(IN) :: ppopsk(ngrid,nlay) |
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85 | logical,INTENT(IN) :: lecrit |
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86 | REAL,INTENT(IN) :: pcondicea_co2microp(ngrid,nlay)! tendency due to CO2 condensation (kg/kg.s-1) |
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87 | |
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88 | REAL,INTENT(IN) :: pz0(ngrid) ! surface roughness length (m) |
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89 | |
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90 | c Argument added to account for subgrid gustiness : |
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91 | |
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92 | REAL,INTENT(IN) :: wstar(ngrid), hfmax(ngrid)!, zi(ngrid) |
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93 | |
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94 | c Traceurs : |
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95 | integer,intent(in) :: nq |
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96 | REAL,INTENT(IN) :: pqsurf(ngrid,nq,nslope) |
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97 | REAL :: zqsurf(ngrid) ! temporary water tracer |
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98 | real,intent(in) :: pq(ngrid,nlay,nq), pdqfi(ngrid,nlay,nq) |
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99 | real,intent(out) :: pdqdif(ngrid,nlay,nq) |
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100 | real,intent(out) :: pdqsdif(ngrid,nq,nslope) |
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101 | REAL,INTENT(in) :: dustliftday(ngrid) |
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102 | REAL,INTENT(inout) :: qsoil(ngrid,nsoil,nqsoil,nslope) !subsurface tracers |
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103 | REAL,INTENT(in) :: local_time(ngrid) |
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104 | |
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105 | c local: |
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106 | c ------ |
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107 | |
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108 | REAL :: pt(ngrid,nlay) |
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109 | |
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110 | INTEGER ilev,ig,ilay,nlev,islope,ik,lice |
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111 | |
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112 | REAL z4st,zdplanck(ngrid) |
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113 | REAL zkv(ngrid,nlay+1),zkh(ngrid,nlay+1) |
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114 | REAL zkq(ngrid,nlay+1) |
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115 | REAL zcdv(ngrid,nslope),zcdh(ngrid,nslope) |
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116 | REAL, INTENT(OUT) :: zcdv_true(ngrid,nslope) |
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117 | REAL, INTENT(OUT) :: zcdh_true(ngrid,nslope) ! drag coeff are used by the LES to recompute u* and hfx |
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118 | REAL :: zcdv_tmp(ngrid),zcdh_tmp(ngrid) ! drag coeffs for the major sub-grid surface |
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119 | 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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120 | REAL zu(ngrid,nlay),zv(ngrid,nlay) |
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121 | REAL zh(ngrid,nlay) |
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122 | REAL ztsrf2(ngrid) |
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123 | REAL z1(ngrid),z2(ngrid) |
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124 | REAL za(ngrid,nlay),zb(ngrid,nlay) |
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125 | REAL zb0(ngrid,nlay) |
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126 | REAL zc(ngrid,nlay),zd(ngrid,nlay) |
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127 | REAL zcst1 |
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128 | REAL zu2(ngrid) |
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129 | REAL Tice(ngrid,nslope) ! subsurface temperature where ice is located. |
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130 | REAL qeq(ngrid,nslope) ! saturation water vapor in the subsurface |
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131 | REAL dist_up(ngrid,nslope) !distance from ice to layer above |
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132 | REAL dist_down(ngrid,nslope) !distance from ice to layer down |
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133 | REAL dist_sum(ngrid,nslope) ! sum of distance |
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134 | REAL zdqsdif_ssi(ngrid,nslope) !SSI flux |
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135 | REAL zdqsdif_ssi_frost(ngrid,nslope) !SSI-frost interaction |
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136 | |
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137 | EXTERNAL SSUM,SCOPY |
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138 | REAL SSUM |
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139 | LOGICAL,SAVE :: firstcall=.true. |
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140 | |
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141 | !$OMP THREADPRIVATE(firstcall) |
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142 | |
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143 | c variable added for CO2 condensation: |
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144 | c ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ |
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145 | REAL hh , zhcond(ngrid,nlay) |
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146 | REAL,PARAMETER :: latcond=5.9e5 |
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147 | REAL,PARAMETER :: tcond1mb=136.27 |
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148 | REAL,SAVE :: acond,bcond |
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149 | |
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150 | !$OMP THREADPRIVATE(acond,bcond) |
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151 | |
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152 | c Subtimestep & implicit treatment of water vapor |
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153 | c ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ |
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154 | REAL zdqsdif_surf(ngrid) ! subtimestep pdqsdif for water ice |
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155 | REAL ztsrf(ngrid) ! temporary surface temperature in tsub |
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156 | REAL zdtsrf(ngrid,nslope) ! surface temperature tendancy in tsub |
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157 | REAL surf_h2o_lh(ngrid,nslope) ! Surface h2o latent heat flux |
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158 | REAL zsurf_h2o_lh(ngrid,nslope) ! Tsub surface h2o latent heat flux |
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159 | |
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160 | c For latent heat release from ground water ice sublimation |
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161 | c ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~ |
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162 | REAL tsrf_lh(ngrid) ! temporary surface temperature with lh effect |
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163 | REAL lh ! latent heat, formulation given in the Technical Document: |
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164 | ! "Modeling water ice sublimation under Phoenix-like conditions", Montmessin et al. 2004 |
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165 | |
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166 | c Tracers : |
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167 | c ~~~~~~~ |
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168 | INTEGER iq |
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169 | REAL zq(ngrid,nlay,nq) |
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170 | REAL zq1temp(ngrid) |
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171 | REAL rho(ngrid) ! near surface air density |
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172 | REAL qsat(ngrid) |
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173 | REAL qsat2(ngrid,nslope) |
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174 | REAL resist(ngrid,nslope) !subsurface ice flux reduction coef |
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175 | |
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176 | REAL hdoflux(ngrid,nslope) ! value of vapour flux of HDO |
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177 | REAL hdoflux_meshavg(ngrid) ! value of vapour flux of HDO |
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178 | ! REAL h2oflux(ngrid) ! value of vapour flux of H2O |
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179 | REAL old_h2o_vap(ngrid) ! traceur d'eau avant traitement |
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180 | REAL saved_h2o_vap(ngrid) ! traceur d'eau avant traitement |
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181 | |
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182 | REAL kmixmin |
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183 | |
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184 | c Argument added for surface water ice budget: |
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185 | REAL,INTENT(IN) :: watercap(ngrid,nslope) |
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186 | REAL,INTENT(OUT) :: dwatercap_dif(ngrid,nslope) |
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187 | |
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188 | c Subtimestep to compute h2o latent heat flux: |
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189 | REAL :: dtmax = 0.5 ! subtimestep temp criterion |
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190 | INTEGER tsub ! adaptative subtimestep (seconds) |
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191 | REAL subtimestep !ptimestep/nsubtimestep |
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192 | INTEGER nsubtimestep(ngrid) ! number of subtimestep (int) |
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193 | |
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194 | c Mass-variation scheme : |
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195 | c ~~~~~~~ |
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196 | |
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197 | INTEGER j,l |
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198 | REAL zcondicea(ngrid,nlay) |
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199 | REAL zt(ngrid,nlay),ztcond(ngrid,nlay+1) |
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200 | REAL betam(ngrid,nlay),dmice(ngrid,nlay) |
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201 | REAL pdtc(ngrid,nlay) |
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202 | REAL zhs(ngrid,nlay) |
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203 | REAL,SAVE :: ccond |
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204 | |
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205 | !$OMP THREADPRIVATE(ccond) |
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206 | |
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207 | c Theta_m formulation for mass-variation scheme : |
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208 | c ~~~~~~~ |
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209 | |
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210 | INTEGER,SAVE :: ico2 |
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211 | INTEGER llnt(ngrid) |
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212 | REAL,SAVE :: m_co2, m_noco2, A , B |
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213 | REAL vmr_co2(ngrid,nlay) |
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214 | REAL qco2,mmean(ngrid,nlay) |
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215 | |
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216 | !$OMP THREADPRIVATE(ico2,m_co2,m_noco2,A,B) |
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217 | |
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218 | REAL,INTENT(OUT) :: sensibFlux(ngrid) |
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219 | |
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220 | !!MARGAUX |
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221 | REAL DoH_vap(ngrid,nlay) |
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222 | !! Sub-grid scale slopes |
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223 | REAL :: pdqsdif_tmp(ngrid,nq) ! Temporary for dust lifting |
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224 | REAL :: watercap_tmp(ngrid) |
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225 | REAL :: zq_slope_vap(ngrid,nlay,nq,nslope) |
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226 | REAL :: zq_tmp_vap(ngrid,nlay,nq) |
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227 | REAL :: ptsrf_tmp(ngrid) |
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228 | REAL :: pqsurf_tmp(ngrid,nq) |
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229 | REAL :: pdqsdif_tmphdo(ngrid,nq) |
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230 | REAL :: qsat_tmp(ngrid) |
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231 | INTEGER :: indmax |
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232 | |
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233 | character*2 str2 |
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234 | |
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235 | !! Subsurface exchanges |
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236 | LOGICAL :: exchange ! boolean to check if exchange between the subsurface and the atmosphere can occurs |
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237 | REAL :: zdqsdif_regolith(ngrid,nslope) ! Flux from subsurface (positive pointing outwards) (kg/m^2/s) |
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238 | REAL zq1temp_regolith(ngrid) ! Temporary atmospheric mixing ratio after exchange with subsurface (kg / kg) |
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239 | REAL zdqsdif_tot(ngrid) ! subtimestep pdqsdif for water ice |
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240 | 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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241 | |
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242 | !! Water buyoncy |
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243 | LOGICAL :: virtual |
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244 | |
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245 | |
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246 | |
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247 | c ** un petit test de coherence |
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248 | c -------------------------- |
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249 | |
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250 | ! AS: OK firstcall absolute |
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251 | IF (firstcall) THEN |
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252 | c To compute: Tcond= 1./(bcond-acond*log(.0095*p)) (p in pascal) |
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253 | bcond=1./tcond1mb |
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254 | acond=r/latcond |
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255 | ccond=cpp/(g*latcond) |
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256 | PRINT*,'In vdifc: Tcond(P=1mb)=',tcond1mb,' Lcond=',latcond |
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257 | PRINT*,' acond,bcond,ccond',acond,bcond,ccond |
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258 | |
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259 | |
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260 | ico2=0 |
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261 | |
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262 | c Prepare Special treatment if one of the tracer is CO2 gas |
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263 | do iq=1,nq |
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264 | if (noms(iq).eq."co2") then |
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265 | ico2=iq |
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266 | m_co2 = 44.01E-3 ! CO2 molecular mass (kg/mol) |
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267 | m_noco2 = 33.37E-3 ! Non condensible mol mass (kg/mol) |
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268 | c Compute A and B coefficient use to compute |
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269 | c mean molecular mass Mair defined by |
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270 | c 1/Mair = q(ico2)/m_co2 + (1-q(ico2))/m_noco2 |
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271 | c 1/Mair = A*q(ico2) + B |
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272 | A =(1/m_co2 - 1/m_noco2) |
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273 | B=1/m_noco2 |
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274 | endif |
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275 | enddo |
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276 | |
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277 | firstcall=.false. |
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278 | ENDIF |
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279 | |
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280 | DO ig = 1,ngrid |
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281 | ptsrf_tmp(ig) = ptsrf(ig,major_slope(ig)) |
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282 | pqsurf_tmp(ig,:) = pqsurf(ig,:,major_slope(ig)) |
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283 | ENDDO |
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284 | |
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285 | c----------------------------------------------------------------------- |
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286 | c 1. initialisation |
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287 | c ----------------- |
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288 | |
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289 | nlev=nlay+1 |
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290 | |
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291 | ! initialize output tendencies to zero: |
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292 | pdudif(1:ngrid,1:nlay)=0 |
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293 | pdvdif(1:ngrid,1:nlay)=0 |
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294 | pdhdif(1:ngrid,1:nlay)=0 |
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295 | pdtsrf(1:ngrid,1:nslope)=0 |
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296 | zdtsrf(1:ngrid,1:nslope)=0 |
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297 | surf_h2o_lh(1:ngrid,1:nslope)=0 |
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298 | zsurf_h2o_lh(1:ngrid,1:nslope)=0 |
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299 | pdqdif(1:ngrid,1:nlay,1:nq)=0 |
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300 | pdqsdif(1:ngrid,1:nq,1:nslope)=0 |
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301 | pdqsdif_tmp(1:ngrid,1:nq)=0 |
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302 | zdqsdif_surf(1:ngrid)=0 |
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303 | dwatercap_dif(1:ngrid,1:nslope)=0 |
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304 | zdqsdif_regolith(1:ngrid,1:nslope)=0 |
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305 | zq1temp_regolith(1:ngrid)=0 |
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306 | zdqsdif_tot(1:ngrid)=0 |
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307 | h2o_ice_depth(1:ngrid,1:nslope)=1 |
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308 | virtual = .false. |
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309 | |
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310 | c ** calcul de rho*dz et dt*rho/dz=dt*rho**2 g/dp |
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311 | c avec rho=p/RT=p/ (R Theta) (p/ps)**kappa |
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312 | c ---------------------------------------- |
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313 | |
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314 | DO ilay=1,nlay |
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315 | DO ig=1,ngrid |
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316 | za(ig,ilay)=(pplev(ig,ilay)-pplev(ig,ilay+1))/g |
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317 | ! Mass variation scheme: |
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318 | betam(ig,ilay)=-za(ig,ilay)*latcond/(cpp*ppopsk(ig,ilay)) |
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319 | ENDDO |
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320 | ENDDO |
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321 | |
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322 | zcst1=4.*g*ptimestep/(r*r) |
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323 | DO ilev=2,nlev-1 |
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324 | DO ig=1,ngrid |
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325 | zb0(ig,ilev)=pplev(ig,ilev)* |
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326 | s (pplev(ig,1)/pplev(ig,ilev))**rcp / |
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327 | s (ph(ig,ilev-1)+ph(ig,ilev)) |
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328 | zb0(ig,ilev)=zcst1*zb0(ig,ilev)*zb0(ig,ilev)/ |
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329 | s (pplay(ig,ilev-1)-pplay(ig,ilev)) |
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330 | ENDDO |
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331 | ENDDO |
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332 | DO ig=1,ngrid |
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333 | zb0(ig,1)=ptimestep*pplev(ig,1)/(r*ptsrf_tmp(ig)) |
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334 | ENDDO |
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335 | |
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336 | c ** diagnostique pour l'initialisation |
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337 | c ---------------------------------- |
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338 | |
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339 | IF(lecrit) THEN |
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340 | ig=ngrid/2+1 |
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341 | PRINT*,'Pression (mbar) ,altitude (km),u,v,theta, rho dz' |
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342 | DO ilay=1,nlay |
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343 | WRITE(*,'(6f11.5)') |
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344 | s .01*pplay(ig,ilay),.001*pzlay(ig,ilay), |
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345 | s pu(ig,ilay),pv(ig,ilay),ph(ig,ilay),za(ig,ilay) |
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346 | ENDDO |
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347 | PRINT*,'Pression (mbar) ,altitude (km),zb' |
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348 | DO ilev=1,nlay |
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349 | WRITE(*,'(3f15.7)') |
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350 | s .01*pplev(ig,ilev),.001*pzlev(ig,ilev), |
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351 | s zb0(ig,ilev) |
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352 | ENDDO |
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353 | ENDIF |
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354 | |
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355 | c ----------------------------------- |
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356 | c Potential Condensation temperature: |
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357 | c ----------------------------------- |
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358 | |
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359 | c Compute CO2 Volume mixing ratio |
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360 | c ------------------------------- |
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361 | if (callcond.and.(ico2.ne.0)) then |
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362 | DO ilev=1,nlay |
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363 | DO ig=1,ngrid |
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364 | qco2=MAX(1.E-30 |
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365 | & ,pq(ig,ilev,ico2)+pdqfi(ig,ilev,ico2)*ptimestep) |
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366 | c Mean air molecular mass = 1/(q(ico2)/m_co2 + (1-q(ico2))/m_noco2) |
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367 | mmean(ig,ilev)=1/(A*qco2 +B) |
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368 | vmr_co2(ig,ilev) = qco2*mmean(ig,ilev)/m_co2 |
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369 | ENDDO |
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370 | ENDDO |
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371 | else |
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372 | DO ilev=1,nlay |
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373 | DO ig=1,ngrid |
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374 | vmr_co2(ig,ilev)=0.95 |
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375 | ENDDO |
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376 | ENDDO |
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377 | end if |
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378 | |
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379 | c forecast of atmospheric temperature zt and frost temperature ztcond |
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380 | c -------------------------------------------------------------------- |
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381 | |
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382 | if (callcond) then |
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383 | DO ilev=1,nlay |
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384 | DO ig=1,ngrid |
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385 | ztcond(ig,ilev)= |
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386 | & 1./(bcond-acond*log(.01*vmr_co2(ig,ilev)*pplay(ig,ilev))) |
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387 | if (pplay(ig,ilev).lt.1e-4) ztcond(ig,ilev)=0.0 !mars Monica |
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388 | ! zhcond(ig,ilev) = |
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389 | ! & (1./(bcond-acond*log(.0095*pplay(ig,ilev))))/ppopsk(ig,ilev) |
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390 | zhcond(ig,ilev) = ztcond(ig,ilev)/ppopsk(ig,ilev) |
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391 | END DO |
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392 | END DO |
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393 | ztcond(:,nlay+1)=ztcond(:,nlay) |
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394 | else |
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395 | zhcond(:,:) = 0 |
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396 | ztcond(:,:) = 0 |
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397 | end if |
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398 | |
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399 | |
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400 | c----------------------------------------------------------------------- |
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401 | c 2. ajout des tendances physiques |
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402 | c ----------------------------- |
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403 | |
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404 | DO ilev=1,nlay |
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405 | DO ig=1,ngrid |
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406 | zu(ig,ilev)=pu(ig,ilev)+pdufi(ig,ilev)*ptimestep |
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407 | zv(ig,ilev)=pv(ig,ilev)+pdvfi(ig,ilev)*ptimestep |
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408 | zh(ig,ilev)=ph(ig,ilev)+pdhfi(ig,ilev)*ptimestep |
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409 | ! zh(ig,ilev)=max(zh(ig,ilev),zhcond(ig,ilev)) |
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410 | ENDDO |
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411 | ENDDO |
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412 | |
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413 | zq(1:ngrid,1:nlay,1:nq)=pq(1:ngrid,1:nlay,1:nq)+ |
---|
414 | & pdqfi(1:ngrid,1:nlay,1:nq)*ptimestep |
---|
415 | |
---|
416 | c----------------------------------------------------------------------- |
---|
417 | c 3. schema de turbulence |
---|
418 | c -------------------- |
---|
419 | |
---|
420 | c ** source d'energie cinetique turbulente a la surface |
---|
421 | c (condition aux limites du schema de diffusion turbulente |
---|
422 | c dans la couche limite |
---|
423 | c --------------------- |
---|
424 | |
---|
425 | CALL vdif_cd(ngrid,nlay,nslope,pz0,g,pzlay,pplay,pu,pv,wstar, |
---|
426 | & ptsrf,ph,virtual,mmean(:,1),zq(:,:,igcm_h2o_vap), |
---|
427 | & pqsurf(:,igcm_h2o_ice,:), |
---|
428 | & zcdv_true,zcdh_true) |
---|
429 | |
---|
430 | zu2(:)=pu(:,1)*pu(:,1)+pv(:,1)*pv(:,1) |
---|
431 | |
---|
432 | DO islope = 1,nslope |
---|
433 | IF (callrichsl) THEN |
---|
434 | zcdv(:,islope)=zcdv_true(:,islope)*sqrt(zu2(:)+ |
---|
435 | & (log(1.+0.7*wstar(:) + 2.3*wstar(:)**2))**2) |
---|
436 | zcdh(:,islope)=zcdh_true(:,islope)*sqrt(zu2(:)+ |
---|
437 | & (log(1.+0.7*wstar(:) + 2.3*wstar(:)**2))**2) |
---|
438 | ELSE |
---|
439 | zcdv(:,islope)=zcdv_true(:,islope)*sqrt(zu2(:)) ! 1 / bulk aerodynamic momentum conductance |
---|
440 | zcdh(:,islope)=zcdh_true(:,islope)*sqrt(zu2(:)) ! 1 / bulk aerodynamic heat conductance |
---|
441 | ENDIF |
---|
442 | ENDDO |
---|
443 | ustar(:) = 0 |
---|
444 | tstar(:) = 0 |
---|
445 | DO ig = 1,ngrid |
---|
446 | zcdv_tmp(ig) = zcdv(ig,major_slope(ig)) |
---|
447 | zcdh_tmp(ig) = zcdh(ig,major_slope(ig)) |
---|
448 | zcdv_true_tmp(ig) = zcdv_true(ig,major_slope(ig)) |
---|
449 | zcdh_true_tmp(ig) = zcdh_true(ig,major_slope(ig)) |
---|
450 | IF (callrichsl) THEN |
---|
451 | ustar(ig)=sqrt(zcdv_true(ig,major_slope(ig))) |
---|
452 | & *sqrt(zu2(ig)+(log(1.+0.7*wstar(ig) + |
---|
453 | & 2.3*wstar(ig)**2))**2) |
---|
454 | IF (zcdh_true(ig,major_slope(ig)) .ne. 0.) THEN ! When Cd=Ch=0, u*=t*=0 |
---|
455 | tstar(ig)=(ph(ig,1)-ptsrf_tmp(ig)) |
---|
456 | & *zcdh_tmp(ig)/ustar(ig) |
---|
457 | ENDIF |
---|
458 | ELSE |
---|
459 | ustar(ig)=sqrt(zcdv_true(ig,major_slope(ig))) |
---|
460 | & *sqrt(zu2(ig)) |
---|
461 | tstar(ig)=(ph(ig,1)-ptsrf_tmp(ig)) |
---|
462 | & *zcdh_true(ig,major_slope(ig)) |
---|
463 | & /sqrt(zcdv_true(ig,major_slope(ig))) |
---|
464 | ENDIF |
---|
465 | ENDDO |
---|
466 | |
---|
467 | c ** schema de diffusion turbulente dans la couche limite |
---|
468 | c ---------------------------------------------------- |
---|
469 | pt(:,:)=ph(:,:)*ppopsk(:,:) |
---|
470 | if (callyamada4) then |
---|
471 | call yamada4(ngrid,nlay,nq,ptimestep,g,r,pplev,pt |
---|
472 | s ,pzlev,pzlay,pu,pv,ph,pq,zcdv_true_tmp,pq2,zkv,zkh,zkq,ustar |
---|
473 | s ,9) |
---|
474 | |
---|
475 | elseif (callatke) then |
---|
476 | call call_atke(ptimestep,ngrid,nlay,zcdv_true_tmp, |
---|
477 | s zcdh_true_tmp,pu(:,1),pv(:,1),ptsrf_tmp, |
---|
478 | s pu,pv,pt,zq(:,1,igcm_h2o_vap),pplay,pplev, |
---|
479 | s pzlay,pzlev,pq2,zkv(:,1:nlay),zkh(:,1:nlay)) |
---|
480 | |
---|
481 | zkv(:,nlay+1) = zkv(:,nlay) |
---|
482 | zkh(:,nlay+1) = zkh(:,nlay) |
---|
483 | else |
---|
484 | call vdif_kc(ngrid,nlay,nq,ptimestep,g,pzlev,pzlay |
---|
485 | s ,pu,pv,ph,zcdv_true_tmp |
---|
486 | s ,pq2,zkv,zkh,zq) |
---|
487 | |
---|
488 | endif |
---|
489 | if ((doubleq).and.(ngrid.eq.1)) then |
---|
490 | kmixmin = 80. !80.! minimum eddy mix coeff in 1D |
---|
491 | do ilev=2,nlay |
---|
492 | do ig=1,ngrid |
---|
493 | zkh(ig,ilev) = max(kmixmin,zkh(ig,ilev)) |
---|
494 | zkv(ig,ilev) = max(kmixmin,zkv(ig,ilev)) |
---|
495 | end do |
---|
496 | end do |
---|
497 | end if |
---|
498 | |
---|
499 | c ** diagnostique pour le schema de turbulence |
---|
500 | c ----------------------------------------- |
---|
501 | |
---|
502 | IF(lecrit) THEN |
---|
503 | PRINT* |
---|
504 | PRINT*,'Diagnostic for the vertical turbulent mixing' |
---|
505 | PRINT*,'Cd for momentum and potential temperature' |
---|
506 | |
---|
507 | PRINT*,zcdv_tmp(ngrid/2+1),zcdh_tmp(ngrid/2+1) |
---|
508 | PRINT*,'Mixing coefficient for momentum and pot.temp.' |
---|
509 | DO ilev=1,nlay |
---|
510 | PRINT*,zkv(ngrid/2+1,ilev),zkh(ngrid/2+1,ilev) |
---|
511 | ENDDO |
---|
512 | ENDIF |
---|
513 | |
---|
514 | c----------------------------------------------------------------------- |
---|
515 | c 4. inversion pour l'implicite sur u |
---|
516 | c -------------------------------- |
---|
517 | |
---|
518 | c ** l'equation est |
---|
519 | c u(t+1) = u(t) + dt * {(du/dt)phys}(t) + dt * {(du/dt)difv}(t+1) |
---|
520 | c avec |
---|
521 | c /zu/ = u(t) + dt * {(du/dt)phys}(t) (voir paragraphe 2.) |
---|
522 | c et |
---|
523 | c dt * {(du/dt)difv}(t+1) = dt * {(d/dz)[ Ku (du/dz) ]}(t+1) |
---|
524 | c donc les entrees sont /zcdv/ pour la condition a la limite sol |
---|
525 | c et /zkv/ = Ku |
---|
526 | |
---|
527 | zb(1:ngrid,2:nlay)=zkv(1:ngrid,2:nlay)*zb0(1:ngrid,2:nlay) |
---|
528 | zb(1:ngrid,1)=zcdv_tmp(1:ngrid)*zb0(1:ngrid,1) |
---|
529 | |
---|
530 | DO ig=1,ngrid |
---|
531 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
---|
532 | zc(ig,nlay)=za(ig,nlay)*zu(ig,nlay)*z1(ig) |
---|
533 | zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
---|
534 | ENDDO |
---|
535 | |
---|
536 | DO ilay=nlay-1,1,-1 |
---|
537 | DO ig=1,ngrid |
---|
538 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
---|
539 | $ zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
---|
540 | zc(ig,ilay)=(za(ig,ilay)*zu(ig,ilay)+ |
---|
541 | $ zb(ig,ilay+1)*zc(ig,ilay+1))*z1(ig) |
---|
542 | zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
---|
543 | ENDDO |
---|
544 | ENDDO |
---|
545 | |
---|
546 | DO ig=1,ngrid |
---|
547 | zu(ig,1)=zc(ig,1) |
---|
548 | ENDDO |
---|
549 | DO ilay=2,nlay |
---|
550 | DO ig=1,ngrid |
---|
551 | zu(ig,ilay)=zc(ig,ilay)+zd(ig,ilay)*zu(ig,ilay-1) |
---|
552 | ENDDO |
---|
553 | ENDDO |
---|
554 | |
---|
555 | c----------------------------------------------------------------------- |
---|
556 | c 5. inversion pour l'implicite sur v |
---|
557 | c -------------------------------- |
---|
558 | |
---|
559 | c ** l'equation est |
---|
560 | c v(t+1) = v(t) + dt * {(dv/dt)phys}(t) + dt * {(dv/dt)difv}(t+1) |
---|
561 | c avec |
---|
562 | c /zv/ = v(t) + dt * {(dv/dt)phys}(t) (voir paragraphe 2.) |
---|
563 | c et |
---|
564 | c dt * {(dv/dt)difv}(t+1) = dt * {(d/dz)[ Kv (dv/dz) ]}(t+1) |
---|
565 | c donc les entrees sont /zcdv/ pour la condition a la limite sol |
---|
566 | c et /zkv/ = Kv |
---|
567 | |
---|
568 | DO ig=1,ngrid |
---|
569 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
---|
570 | zc(ig,nlay)=za(ig,nlay)*zv(ig,nlay)*z1(ig) |
---|
571 | zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
---|
572 | ENDDO |
---|
573 | |
---|
574 | DO ilay=nlay-1,1,-1 |
---|
575 | DO ig=1,ngrid |
---|
576 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
---|
577 | $ zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
---|
578 | zc(ig,ilay)=(za(ig,ilay)*zv(ig,ilay)+ |
---|
579 | $ zb(ig,ilay+1)*zc(ig,ilay+1))*z1(ig) |
---|
580 | zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
---|
581 | ENDDO |
---|
582 | ENDDO |
---|
583 | |
---|
584 | DO ig=1,ngrid |
---|
585 | zv(ig,1)=zc(ig,1) |
---|
586 | ENDDO |
---|
587 | DO ilay=2,nlay |
---|
588 | DO ig=1,ngrid |
---|
589 | zv(ig,ilay)=zc(ig,ilay)+zd(ig,ilay)*zv(ig,ilay-1) |
---|
590 | ENDDO |
---|
591 | ENDDO |
---|
592 | |
---|
593 | c----------------------------------------------------------------------- |
---|
594 | c Using the wind modified by friction for lifting and sublimation |
---|
595 | c ---------------------------------------------------------------- |
---|
596 | |
---|
597 | ! This is computed above and takes into account surface-atmosphere flux |
---|
598 | ! enhancement by subgrid gustiness and atmospheric-stability related |
---|
599 | ! variations of transfer coefficients. |
---|
600 | ! Calculate Cd again with wind slowed by friction |
---|
601 | c ------------------------------------------- |
---|
602 | |
---|
603 | CALL vdif_cd(ngrid,nlay,nslope,pz0,g,pzlay,pplay,zu,zv,wstar, |
---|
604 | & ptsrf,ph,virtual,mmean(:,1),zq(:,:,igcm_h2o_vap), |
---|
605 | & pqsurf(:,igcm_h2o_ice,:), |
---|
606 | & zcdv_true,zcdh_true) |
---|
607 | |
---|
608 | zu2(:)=zu(:,1)*zu(:,1)+zv(:,1)*zv(:,1) |
---|
609 | |
---|
610 | DO islope = 1,nslope |
---|
611 | IF (callrichsl) THEN |
---|
612 | zcdv(:,islope)=zcdv_true(:,islope)*sqrt(zu2(:)+ |
---|
613 | & (log(1.+0.7*wstar(:) + 2.3*wstar(:)**2))**2) |
---|
614 | zcdh(:,islope)=zcdh_true(:,islope)*sqrt(zu2(:)+ |
---|
615 | & (log(1.+0.7*wstar(:) + 2.3*wstar(:)**2))**2) |
---|
616 | ELSE |
---|
617 | zcdv(:,islope)=zcdv_true(:,islope)*sqrt(zu2(:)) ! 1 / bulk aerodynamic momentum conductance |
---|
618 | zcdh(:,islope)=zcdh_true(:,islope)*sqrt(zu2(:)) ! 1 / bulk aerodynamic heat conductance |
---|
619 | ENDIF |
---|
620 | ENDDO |
---|
621 | ustar(:) = 0 |
---|
622 | tstar(:) = 0 |
---|
623 | DO ig = 1,ngrid |
---|
624 | zcdv_tmp(ig) = zcdv(ig,major_slope(ig)) |
---|
625 | zcdh_tmp(ig) = zcdh(ig,major_slope(ig)) |
---|
626 | zcdv_true_tmp(ig) = zcdv_true(ig,major_slope(ig)) |
---|
627 | zcdh_true_tmp(ig) = zcdh_true(ig,major_slope(ig)) |
---|
628 | IF (callrichsl) THEN |
---|
629 | ustar(ig)=sqrt(zcdv_true(ig,major_slope(ig))) |
---|
630 | & *sqrt(zu2(ig)+(log(1.+0.7*wstar(ig) + |
---|
631 | & 2.3*wstar(ig)**2))**2) |
---|
632 | IF (zcdh_true(ig,major_slope(ig)) .ne. 0.) THEN ! When Cd=Ch=0, u*=t*=0 |
---|
633 | tstar(ig)=(ph(ig,1)-ptsrf_tmp(ig)) |
---|
634 | & *zcdh_tmp(ig)/ustar(ig) |
---|
635 | ENDIF |
---|
636 | ELSE |
---|
637 | ustar(ig)=sqrt(zcdv_true(ig,major_slope(ig))) |
---|
638 | & *sqrt(zu2(ig)) |
---|
639 | tstar(ig)=(ph(ig,1)-ptsrf_tmp(ig)) |
---|
640 | & *zcdh_true(ig,major_slope(ig)) |
---|
641 | & /sqrt(zcdv_true(ig,major_slope(ig))) |
---|
642 | ENDIF |
---|
643 | ENDDO |
---|
644 | |
---|
645 | |
---|
646 | c----------------------------------------------------------------------- |
---|
647 | c 6. inversion pour l'implicite sur h sans oublier le couplage |
---|
648 | c avec le sol (conduction) |
---|
649 | c ------------------------ |
---|
650 | |
---|
651 | c ** l'equation est |
---|
652 | c h(t+1) = h(t) + dt * {(dh/dt)phys}(t) + dt * {(dh/dt)difv}(t+1) |
---|
653 | c avec |
---|
654 | c /zh/ = h(t) + dt * {(dh/dt)phys}(t) (voir paragraphe 2.) |
---|
655 | c et |
---|
656 | c dt * {(dh/dt)difv}(t+1) = dt * {(d/dz)[ Kh (dh/dz) ]}(t+1) |
---|
657 | c donc les entrees sont /zcdh/ pour la condition de raccord au sol |
---|
658 | c et /zkh/ = Kh |
---|
659 | c ------------- |
---|
660 | |
---|
661 | c Mass variation scheme: |
---|
662 | zb(1:ngrid,2:nlay)=zkh(1:ngrid,2:nlay)*zb0(1:ngrid,2:nlay) |
---|
663 | zb(1:ngrid,1)=zcdh_tmp(1:ngrid)*zb0(1:ngrid,1) |
---|
664 | |
---|
665 | c on initialise dm c |
---|
666 | |
---|
667 | pdtc(:,:)=0. |
---|
668 | zt(:,:)=0. |
---|
669 | dmice(:,:)=0. |
---|
670 | |
---|
671 | c ** calcul de (d Planck / dT) a la temperature d'interface |
---|
672 | c ------------------------------------------------------ |
---|
673 | |
---|
674 | z4st=4.*5.67e-8*ptimestep |
---|
675 | IF (tke_heat_flux .eq. 0.) THEN |
---|
676 | DO ig=1,ngrid |
---|
677 | indmax = major_slope(ig) |
---|
678 | zdplanck(ig)=z4st*pemis(ig,indmax)*ptsrf(ig,indmax)* |
---|
679 | & ptsrf(ig,indmax)*ptsrf(ig,indmax) |
---|
680 | ENDDO |
---|
681 | ELSE |
---|
682 | zdplanck(:)=0. |
---|
683 | ENDIF |
---|
684 | |
---|
685 | ! calcul de zc et zd pour la couche top en prenant en compte le terme |
---|
686 | ! de variation de masse (on fait une boucle pour que \E7a converge) |
---|
687 | |
---|
688 | ! Identification des points de grilles qui ont besoin de la correction |
---|
689 | |
---|
690 | llnt(:)=1 |
---|
691 | IF (.not.turb_resolved) THEN |
---|
692 | IF (callcond) THEN |
---|
693 | DO ig=1,ngrid |
---|
694 | DO l=1,nlay |
---|
695 | if(zh(ig,l) .lt. zhcond(ig,l)) then |
---|
696 | llnt(ig)=300 |
---|
697 | ! 200 and 100 do not go beyond month 9 with normal dissipation |
---|
698 | goto 5 |
---|
699 | endif |
---|
700 | ENDDO |
---|
701 | 5 continue |
---|
702 | ENDDO |
---|
703 | ENDIF |
---|
704 | |
---|
705 | ENDIF |
---|
706 | |
---|
707 | DO ig=1,ngrid |
---|
708 | indmax = major_slope(ig) |
---|
709 | ! Initialization of z1 and zd, which do not depend on dmice |
---|
710 | |
---|
711 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
---|
712 | zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
---|
713 | |
---|
714 | DO ilay=nlay-1,1,-1 |
---|
715 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
---|
716 | $ zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
---|
717 | zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
---|
718 | ENDDO |
---|
719 | |
---|
720 | ! Convergence loop |
---|
721 | |
---|
722 | DO j=1,llnt(ig) |
---|
723 | |
---|
724 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
---|
725 | zc(ig,nlay)=za(ig,nlay)*zh(ig,nlay) |
---|
726 | & -betam(ig,nlay)*dmice(ig,nlay) |
---|
727 | zc(ig,nlay)=zc(ig,nlay)*z1(ig) |
---|
728 | ! zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
---|
729 | |
---|
730 | ! calcul de zc et zd pour les couches du haut vers le bas |
---|
731 | |
---|
732 | DO ilay=nlay-1,1,-1 |
---|
733 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
---|
734 | $ zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
---|
735 | zc(ig,ilay)=(za(ig,ilay)*zh(ig,ilay)+ |
---|
736 | $ zb(ig,ilay+1)*zc(ig,ilay+1)- |
---|
737 | $ betam(ig,ilay)*dmice(ig,ilay))*z1(ig) |
---|
738 | ! zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
---|
739 | ENDDO |
---|
740 | |
---|
741 | c ** calcul de la temperature_d'interface et de sa tendance. |
---|
742 | c on ecrit que la somme des flux est nulle a l'interface |
---|
743 | c a t + \delta t, |
---|
744 | c c'est a dire le flux radiatif a {t + \delta t} |
---|
745 | c + le flux turbulent a {t + \delta t} |
---|
746 | c qui s'ecrit K (T1-Tsurf) avec T1 = d1 Tsurf + c1 |
---|
747 | c (notation K dt = /cpp*b/) |
---|
748 | c + le flux dans le sol a t |
---|
749 | c + l'evolution du flux dans le sol lorsque la temperature d'interface |
---|
750 | c passe de sa valeur a t a sa valeur a {t + \delta t}. |
---|
751 | c ---------------------------------------------------- |
---|
752 | |
---|
753 | z1(ig)=pcapcal(ig,indmax)*ptsrf(ig,indmax) |
---|
754 | s + cpp*zb(ig,1)*zc(ig,1) |
---|
755 | s + zdplanck(ig)*ptsrf(ig,indmax) |
---|
756 | s + pfluxsrf(ig,indmax)*ptimestep |
---|
757 | z2(ig)= pcapcal(ig,indmax)+cpp*zb(ig,1)*(1.-zd(ig,1)) |
---|
758 | s +zdplanck(ig) |
---|
759 | ztsrf2(ig)=z1(ig)/z2(ig) |
---|
760 | ! pdtsrf(ig)=(ztsrf2(ig)-ptsrf(ig))/ptimestep !incremented outside loop |
---|
761 | zhs(ig,1)=zc(ig,1)+zd(ig,1)*ztsrf2(ig) |
---|
762 | |
---|
763 | c ** et a partir de la temperature au sol on remonte |
---|
764 | c ----------------------------------------------- |
---|
765 | |
---|
766 | DO ilay=2,nlay |
---|
767 | zhs(ig,ilay)=zc(ig,ilay)+zd(ig,ilay)*zhs(ig,ilay-1) |
---|
768 | ENDDO |
---|
769 | DO ilay=1,nlay |
---|
770 | zt(ig,ilay)=zhs(ig,ilay)*ppopsk(ig,ilay) |
---|
771 | ENDDO |
---|
772 | |
---|
773 | c Condensation/sublimation in the atmosphere |
---|
774 | c ------------------------------------------ |
---|
775 | c (computation of zcondicea and dmice) |
---|
776 | |
---|
777 | IF (.NOT. co2clouds) then |
---|
778 | DO l=nlay , 1, -1 |
---|
779 | IF(zt(ig,l).LT.ztcond(ig,l)) THEN |
---|
780 | pdtc(ig,l)=(ztcond(ig,l) - zt(ig,l))/ptimestep |
---|
781 | zcondicea(ig,l)=(pplev(ig,l)-pplev(ig,l+1)) |
---|
782 | & *ccond*pdtc(ig,l) |
---|
783 | dmice(ig,l)= dmice(ig,l) + zcondicea(ig,l)*ptimestep |
---|
784 | END IF |
---|
785 | ENDDO |
---|
786 | ELSE |
---|
787 | DO l=nlay , 1, -1 |
---|
788 | zcondicea(ig,l)= 0.!pcondicea_co2microp(ig,l)* |
---|
789 | c & (pplev(ig,l) - pplev(ig,l+1))/g |
---|
790 | dmice(ig,l)= 0.!dmice(ig,l) + zcondicea(ig,l)*ptimestep |
---|
791 | pdtc(ig,l)=0. |
---|
792 | ENDDO |
---|
793 | ENDIF |
---|
794 | |
---|
795 | ENDDO!of Do j=1,XXX |
---|
796 | pdtsrf(ig,indmax)=(ztsrf2(ig)-ptsrf(ig,indmax))/ptimestep |
---|
797 | ENDDO !of Do ig=1,ngrid |
---|
798 | |
---|
799 | DO ig=1,ngrid ! computing sensible heat flux (atm => surface) |
---|
800 | sensibFlux(ig)=cpp*zb(ig,1)/ptimestep*(zhs(ig,1)-ztsrf2(ig)) |
---|
801 | ENDDO |
---|
802 | |
---|
803 | c Now implicit sheme on each sub-grid subslope: |
---|
804 | IF (nslope.ne.1) then |
---|
805 | DO islope=1,nslope |
---|
806 | DO ig=1,ngrid |
---|
807 | IF(islope.ne.major_slope(ig)) then |
---|
808 | IF (tke_heat_flux .eq. 0.) THEN |
---|
809 | zdplanck(ig)=z4st*pemis(ig,islope)*ptsrf(ig,islope)**3 |
---|
810 | ELSE |
---|
811 | zdplanck(ig) = 0. |
---|
812 | ENDIF |
---|
813 | zb(ig,1)=zcdh(ig,islope)*zb0(ig,1) |
---|
814 | z1(ig)=pcapcal(ig,islope)*ptsrf(ig,islope) |
---|
815 | s + cpp*zb(ig,1)*zc(ig,1) |
---|
816 | s + zdplanck(ig)*ptsrf(ig,islope) |
---|
817 | s + pfluxsrf(ig,islope)*ptimestep |
---|
818 | z2(ig)= pcapcal(ig,islope)+cpp*zb(ig,1)*(1.-zd(ig,1)) |
---|
819 | s +zdplanck(ig) |
---|
820 | ztsrf2(ig)=z1(ig)/z2(ig) |
---|
821 | pdtsrf(ig,islope)=(ztsrf2(ig)-ptsrf(ig,islope))/ptimestep |
---|
822 | ENDIF ! islope != indmax |
---|
823 | ENDDO ! ig |
---|
824 | ENDDO !islope |
---|
825 | ENDIF !nslope.ne.1 |
---|
826 | |
---|
827 | c----------------------------------------------------------------------- |
---|
828 | c TRACERS |
---|
829 | c ------- |
---|
830 | c Calcul du flux vertical au bas de la premiere couche (dust) : |
---|
831 | c ----------------------------------------------------------- |
---|
832 | do ig=1,ngrid |
---|
833 | rho(ig) = zb0(ig,1) /ptimestep |
---|
834 | c zb(ig,1) = 0. |
---|
835 | end do |
---|
836 | c Dust lifting: |
---|
837 | if (lifting) then |
---|
838 | #ifndef MESOSCALE |
---|
839 | if (doubleq.AND.submicron) then |
---|
840 | do ig=1,ngrid |
---|
841 | c if(qsurf(ig,igcm_co2).lt.1) then |
---|
842 | pdqsdif_tmp(ig,igcm_dust_mass) = |
---|
843 | & -alpha_lift(igcm_dust_mass) |
---|
844 | pdqsdif_tmp(ig,igcm_dust_number) = |
---|
845 | & -alpha_lift(igcm_dust_number) |
---|
846 | pdqsdif_tmp(ig,igcm_dust_submicron) = |
---|
847 | & -alpha_lift(igcm_dust_submicron) |
---|
848 | c end if |
---|
849 | end do |
---|
850 | else if (doubleq) then |
---|
851 | if (dustinjection.eq.0) then !injection scheme 0 (old) |
---|
852 | !or 2 (injection in CL) |
---|
853 | do ig=1,ngrid |
---|
854 | if(pqsurf_tmp(ig,igcm_co2).lt.1) then ! pas de soulevement si glace CO2 |
---|
855 | pdqsdif_tmp(ig,igcm_dust_mass) = |
---|
856 | & -alpha_lift(igcm_dust_mass) |
---|
857 | pdqsdif_tmp(ig,igcm_dust_number) = |
---|
858 | & -alpha_lift(igcm_dust_number) |
---|
859 | end if |
---|
860 | end do |
---|
861 | elseif(dustinjection.eq.1)then ! dust injection scheme = 1 injection from surface |
---|
862 | do ig=1,ngrid |
---|
863 | if(pqsurf_tmp(ig,igcm_co2).lt.1) then ! pas de soulevement si glace CO2 |
---|
864 | IF((ti_injection_sol.LE.local_time(ig)).and. |
---|
865 | & (local_time(ig).LE.tf_injection_sol)) THEN |
---|
866 | if (rdstorm) then !Rocket dust storm scheme |
---|
867 | pdqsdif_tmp(ig,igcm_stormdust_mass) = |
---|
868 | & -alpha_lift(igcm_stormdust_mass) |
---|
869 | & *dustliftday(ig) |
---|
870 | pdqsdif_tmp(ig,igcm_stormdust_number) = |
---|
871 | & -alpha_lift(igcm_stormdust_number) |
---|
872 | & *dustliftday(ig) |
---|
873 | pdqsdif_tmp(ig,igcm_dust_mass)= 0. |
---|
874 | pdqsdif_tmp(ig,igcm_dust_number)= 0. |
---|
875 | else |
---|
876 | pdqsdif_tmp(ig,igcm_dust_mass)= |
---|
877 | & -dustliftday(ig)* |
---|
878 | & alpha_lift(igcm_dust_mass) |
---|
879 | pdqsdif_tmp(ig,igcm_dust_number)= |
---|
880 | & -dustliftday(ig)* |
---|
881 | & alpha_lift(igcm_dust_number) |
---|
882 | endif |
---|
883 | if (submicron) then |
---|
884 | pdqsdif_tmp(ig,igcm_dust_submicron) = 0. |
---|
885 | endif ! if (submicron) |
---|
886 | ELSE ! outside dust injection time frame |
---|
887 | pdqsdif_tmp(ig,igcm_dust_mass)= 0. |
---|
888 | pdqsdif_tmp(ig,igcm_dust_number)= 0. |
---|
889 | if (rdstorm) then |
---|
890 | pdqsdif_tmp(ig,igcm_stormdust_mass)= 0. |
---|
891 | pdqsdif_tmp(ig,igcm_stormdust_number)= 0. |
---|
892 | end if |
---|
893 | ENDIF |
---|
894 | |
---|
895 | end if ! of if(qsurf(ig,igcm_co2).lt.1) |
---|
896 | end do |
---|
897 | endif ! end if dustinjection |
---|
898 | else if (submicron) then |
---|
899 | do ig=1,ngrid |
---|
900 | pdqsdif_tmp(ig,igcm_dust_submicron) = |
---|
901 | & -alpha_lift(igcm_dust_submicron) |
---|
902 | end do |
---|
903 | else |
---|
904 | #endif |
---|
905 | call dustlift(ngrid,nlay,nq,rho,zcdh_true_tmp,zcdh_tmp, |
---|
906 | & pqsurf_tmp(:,igcm_co2),pdqsdif_tmp) |
---|
907 | #ifndef MESOSCALE |
---|
908 | endif !doubleq.AND.submicron |
---|
909 | #endif |
---|
910 | else |
---|
911 | pdqsdif_tmp(1:ngrid,1:nq) = 0. |
---|
912 | end if |
---|
913 | |
---|
914 | c OU calcul de la valeur de q a la surface (water) : |
---|
915 | c ---------------------------------------- |
---|
916 | |
---|
917 | c Inversion pour l'implicite sur q |
---|
918 | c Cas des traceurs qui ne sont pas h2o_vap |
---|
919 | c h2o_vap est traite plus loin avec un sous pas de temps |
---|
920 | c hdo_vap est traite ensuite car dependant de h2o_vap |
---|
921 | c -------------------------------- |
---|
922 | |
---|
923 | do iq=1,nq !for all tracers except water vapor |
---|
924 | if ((.not. water).or.(.not. iq.eq.igcm_h2o_vap).or. |
---|
925 | & (.not. iq.eq.igcm_hdo_vap)) then |
---|
926 | |
---|
927 | |
---|
928 | zb(1:ngrid,2:nlay)=zkh(1:ngrid,2:nlay)*zb0(1:ngrid,2:nlay) |
---|
929 | zb(1:ngrid,1)=0 |
---|
930 | |
---|
931 | DO ig=1,ngrid |
---|
932 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
---|
933 | zc(ig,nlay)=za(ig,nlay)*zq(ig,nlay,iq)*z1(ig) |
---|
934 | zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
---|
935 | ENDDO |
---|
936 | |
---|
937 | DO ilay=nlay-1,2,-1 |
---|
938 | DO ig=1,ngrid |
---|
939 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
---|
940 | $ zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
---|
941 | zc(ig,ilay)=(za(ig,ilay)*zq(ig,ilay,iq)+ |
---|
942 | $ zb(ig,ilay+1)*zc(ig,ilay+1))*z1(ig) |
---|
943 | zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
---|
944 | ENDDO |
---|
945 | ENDDO |
---|
946 | |
---|
947 | if ((iq.eq.igcm_h2o_ice) |
---|
948 | $ .or. (hdo.and.(iq.eq.igcm_hdo_ice) )) then |
---|
949 | |
---|
950 | DO ig=1,ngrid |
---|
951 | z1(ig)=1./(za(ig,1)+zb(ig,1)+ |
---|
952 | $ zb(ig,2)*(1.-zd(ig,2))) |
---|
953 | zc(ig,1)=(za(ig,1)*zq(ig,1,iq)+ |
---|
954 | $ zb(ig,2)*zc(ig,2)) *z1(ig) !special case h2o_ice |
---|
955 | ENDDO |
---|
956 | else ! every other tracer |
---|
957 | DO ig=1,ngrid |
---|
958 | z1(ig)=1./(za(ig,1)+zb(ig,1)+ |
---|
959 | $ zb(ig,2)*(1.-zd(ig,2))) |
---|
960 | zc(ig,1)=(za(ig,1)*zq(ig,1,iq)+ |
---|
961 | $ zb(ig,2)*zc(ig,2) + |
---|
962 | $ (-pdqsdif_tmp(ig,iq)) *ptimestep) *z1(ig) !tracer flux from surface |
---|
963 | ENDDO |
---|
964 | endif !((iq.eq.igcm_h2o_ice) |
---|
965 | c Starting upward calculations for simple mixing of tracer (dust) |
---|
966 | DO ig=1,ngrid |
---|
967 | zq(ig,1,iq)=zc(ig,1) |
---|
968 | DO ilay=2,nlay |
---|
969 | zq(ig,ilay,iq)=zc(ig,ilay)+zd(ig,ilay)*zq(ig,ilay-1,iq) |
---|
970 | ENDDO |
---|
971 | ENDDO |
---|
972 | DO islope = 1,nslope |
---|
973 | DO ig = 1,ngrid |
---|
974 | pdqsdif(ig,iq,islope) = pdqsdif_tmp(ig,iq) |
---|
975 | & * cos(pi*def_slope_mean(islope)/180.) |
---|
976 | ENDDO |
---|
977 | ENDDO |
---|
978 | |
---|
979 | endif! ((.not. water).or.(.not. iq.eq.igcm_h2o_vap)) then |
---|
980 | enddo ! of do iq=1,nq |
---|
981 | |
---|
982 | c --------- h2o_vap -------------------------------- |
---|
983 | |
---|
984 | |
---|
985 | c Traitement de la vapeur d'eau h2o_vap |
---|
986 | c Utilisation d'un sous pas de temps afin |
---|
987 | c de decrire le flux de chaleur latente |
---|
988 | |
---|
989 | do iq=1,nq |
---|
990 | if ((water).and.(iq.eq.igcm_h2o_vap)) then |
---|
991 | |
---|
992 | DO islope = 1,nslope |
---|
993 | DO ig=1,ngrid |
---|
994 | |
---|
995 | |
---|
996 | |
---|
997 | zqsurf(ig)=pqsurf(ig,igcm_h2o_ice,islope)/ |
---|
998 | & cos(pi*def_slope_mean(islope)/180.) |
---|
999 | watercap_tmp(ig) = watercap(ig,islope)/ |
---|
1000 | & cos(pi*def_slope_mean(islope)/180.) |
---|
1001 | ENDDO ! ig=1,ngrid |
---|
1002 | |
---|
1003 | c make_tsub : sous pas de temps adaptatif |
---|
1004 | c la subroutine est a la fin du fichier |
---|
1005 | call make_tsub(ngrid,pdtsrf(:,islope),zqsurf, |
---|
1006 | & ptimestep,dtmax,watercaptag, |
---|
1007 | & nsubtimestep) |
---|
1008 | c Calculation for turbulent exchange with the surface (for ice) |
---|
1009 | c initialization of ztsrf, which is surface temperature in |
---|
1010 | c the subtimestep. |
---|
1011 | saved_h2o_vap(:)= zq(:,1,igcm_h2o_vap) |
---|
1012 | DO ig=1,ngrid |
---|
1013 | ! nsubtimestep(ig)=1 !for debug |
---|
1014 | subtimestep = ptimestep/nsubtimestep(ig) |
---|
1015 | call write_output('subtimestep', |
---|
1016 | & 'vdifc substimestep length','s',subtimestep) |
---|
1017 | ztsrf(ig)=ptsrf(ig,islope) ! +pdtsrf(ig)*subtimestep |
---|
1018 | zq_tmp_vap(ig,:,:) =zq(ig,:,:) |
---|
1019 | c Debut du sous pas de temps |
---|
1020 | DO tsub=1,nsubtimestep(ig) |
---|
1021 | if(tsub.eq.nsubtimestep(ig)) writeoutput = .true. |
---|
1022 | c C'est parti ! |
---|
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 | !!! Subsurface exchange |
---|
1063 | ! Check for subsurface exchanges |
---|
1064 | if(.not.watercaptag(ig)) then |
---|
1065 | if (((-(zdqsdif_surf(ig))* |
---|
1066 | & subtimestep).gt.zqsurf(ig)) |
---|
1067 | & .and.(pqsurf(ig,igcm_co2,islope).eq.0.)) then |
---|
1068 | exchange = .true. |
---|
1069 | else |
---|
1070 | exchange = .false. |
---|
1071 | endif |
---|
1072 | else |
---|
1073 | exchange = .false. |
---|
1074 | endif |
---|
1075 | zdqsdif_tot(ig) = zdqsdif_surf(ig) |
---|
1076 | |
---|
1077 | |
---|
1078 | if (adsorption_soil) then |
---|
1079 | call soilwater(1,nlay,nq,nsoil, nqsoil, |
---|
1080 | & ztsrf(ig),ptsoil(ig,:,islope),subtimestep, |
---|
1081 | & exchange,qsat(ig),zq_tmp_vap(ig,:,:), |
---|
1082 | & za(ig,:),zb(ig,:),zc(ig,:),zd(ig,:), |
---|
1083 | & zdqsdif_surf(ig), zqsurf(ig), |
---|
1084 | & qsoil(ig,:,:,islope), pplev(ig,1), rho(ig), |
---|
1085 | & writeoutput,zdqsdif_regolith(ig,islope), |
---|
1086 | & zq1temp_regolith(ig)) |
---|
1087 | |
---|
1088 | |
---|
1089 | |
---|
1090 | if(.not.watercaptag(ig)) then |
---|
1091 | if (exchange) then |
---|
1092 | zq1temp(ig) = zq1temp_regolith(ig) |
---|
1093 | zdqsdif_tot(ig)= |
---|
1094 | & -zqsurf(ig)/subtimestep |
---|
1095 | else |
---|
1096 | zdqsdif_tot(ig) = zdqsdif_surf(ig) + |
---|
1097 | & zdqsdif_regolith(ig,islope) ! boundary condition = qsat, but pdqsdif is calculated to update qsurf (including loss of surface ice to the subsurface) |
---|
1098 | endif ! of "if exchange = true" |
---|
1099 | endif ! of "if not.watercaptag" |
---|
1100 | endif ! adsorption |
---|
1101 | |
---|
1102 | if(.not.watercaptag(ig).and.(.not.adsorption_soil)) then |
---|
1103 | if ((-zdqsdif_tot(ig)*subtimestep) |
---|
1104 | & .gt.(zqsurf(ig))) then |
---|
1105 | |
---|
1106 | |
---|
1107 | !EV subsurface ice |
---|
1108 | IF(h2o_ice_depth(ig,islope) .gt. 0 .and. lag_layer) |
---|
1109 | & then |
---|
1110 | zdqsdif_tot(ig)= |
---|
1111 | & -zqsurf(ig)/subtimestep |
---|
1112 | zqsurf(ig)=0 |
---|
1113 | |
---|
1114 | DO ik=0,nsoil-2 ! go through all the layers to find the ice locations |
---|
1115 | IF((mlayer(ik).le.h2o_ice_depth(ig,islope)).and. |
---|
1116 | & (mlayer(ik+1).gt.h2o_ice_depth(ig,islope))) THEN |
---|
1117 | lice = ik+1 |
---|
1118 | EXIT |
---|
1119 | ENDIF |
---|
1120 | ENDDO !of subsurface loop |
---|
1121 | IF (lice .gt. 1) then !calculate the distance from the layers |
---|
1122 | dist_up(ig,islope)=(h2o_ice_depth(ig,islope) |
---|
1123 | & -mlayer(lice-1)) |
---|
1124 | dist_down(ig,islope)=(mlayer(lice) |
---|
1125 | & -h2o_ice_depth(ig,islope)) |
---|
1126 | dist_sum(ig,islope)=dist_up(ig,islope) |
---|
1127 | & +dist_down(ig,islope) |
---|
1128 | Tice(ig,islope)=(dist_up(ig,islope) ! Linear interp to calculate the temp |
---|
1129 | & *ptsoil(ig,lice-1,islope) |
---|
1130 | & /dist_sum(ig,islope))+ |
---|
1131 | & (dist_down(ig,islope)*ptsoil(ig,lice,islope) |
---|
1132 | & /dist_sum(ig,islope)) |
---|
1133 | ELSE |
---|
1134 | Tice(ig,islope)=ptsoil(ig,1,islope) |
---|
1135 | ENDIF |
---|
1136 | call watersat(1,Tice(ig,1),pplev(ig,1) |
---|
1137 | & ,qsat2(ig,1)) |
---|
1138 | qeq(ig,1)=(ztsrf(ig)/Tice(ig,1)) |
---|
1139 | & *qsat2(ig,1) |
---|
1140 | resist(ig,1)=(1+(h2o_ice_depth(ig,islope)*zcdh(ig,islope) |
---|
1141 | & /d_coef(ig,islope))) |
---|
1142 | !write(*,*)'R=',resist(ig,islope) |
---|
1143 | !write(*,*)'zice=',h2o_ice_depth(ig,islope) |
---|
1144 | !write(*,*)'D=',d_coef(ig,islope) |
---|
1145 | !write(*,*)'zcdh=',zcdh(ig) |
---|
1146 | zb(ig,1)=zb(ig,1)/resist(ig,1) ! change zb to account subsurface ice |
---|
1147 | !vdifc algorithem !!!!!needs to change reseist io to the mean |
---|
1148 | !beacuse of the slopes!!!!! |
---|
1149 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
---|
1150 | zc(ig,nlay)=za(ig,nlay)*zq_tmp_vap(ig,nlay,iq)*z1(ig) |
---|
1151 | zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
---|
1152 | DO ilay=nlay-1,2,-1 |
---|
1153 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
---|
1154 | $ zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
---|
1155 | zc(ig,ilay)=(za(ig,ilay)*zq_tmp_vap(ig,ilay,iq)+ |
---|
1156 | $ zb(ig,ilay+1)*zc(ig,ilay+1))*z1(ig) |
---|
1157 | zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
---|
1158 | ENDDO |
---|
1159 | z1(ig)=1./(za(ig,1)+zb(ig,1)+ |
---|
1160 | $ zb(ig,2)*(1.-zd(ig,2))) |
---|
1161 | zc(ig,1)=(za(ig,1)*zq_tmp_vap(ig,1,iq)+ |
---|
1162 | $ zb(ig,2)*zc(ig,2)) * z1(ig) |
---|
1163 | zd(ig,1)=zb(ig,1)*z1(ig) |
---|
1164 | zq1temp(ig)=zc(ig,1)+ zd(ig,1)*qsat(ig) |
---|
1165 | zdqsdif_ssi(ig,1)=rho(ig)*dryness(ig)*zcdv(ig,islope) |
---|
1166 | & *(zq1temp(ig)-qeq(ig,islope)) |
---|
1167 | call write_output('zdq_ssi', |
---|
1168 | & '','',zdqsdif_ssi(ig,1)) |
---|
1169 | call write_output('qeq', |
---|
1170 | & '','',qeq(ig,1)) |
---|
1171 | call write_output('q1', |
---|
1172 | & '','',zq1temp(ig)) |
---|
1173 | !write(*,*)'qeq=',qeq(ig,1) |
---|
1174 | !write(*,*)'q1=',zq1temp(ig) |
---|
1175 | !write(*,*)'zdqsdif_ssi=',zdqsdif_ssi(ig,1) |
---|
1176 | !I should some all the interactions with the SSI accoridng |
---|
1177 | !to the statistics and the evaluate |
---|
1178 | |
---|
1179 | !write(*,*) "zdq_ssi*t", zdqsdif_ssi(ig)*subtimestep |
---|
1180 | if (zdqsdif_ssi(ig,1)<0) then |
---|
1181 | !zdqsdif_surf(ig)=zdqsdif_ssi(ig,1)-(zqsurf(ig)/subtimestep) |
---|
1182 | zdqsdif_tot(ig)=zdqsdif_tot(ig)+zdqsdif_ssi(ig,1) |
---|
1183 | call write_output('zdq_zdqssi', |
---|
1184 | & '','',zdqsdif_tot(ig)+zdqsdif_ssi(ig,1)) |
---|
1185 | endif |
---|
1186 | ELSE |
---|
1187 | c pdqsdif > 0 : ice condensing |
---|
1188 | c pdqsdif < 0 : ice subliming |
---|
1189 | c write(*,*) "subliming more than available frost: qsurf!" |
---|
1190 | zdqsdif_tot(ig)= |
---|
1191 | & -zqsurf(ig)/subtimestep |
---|
1192 | c write(*,*)'flux vers le sol=',pdqsdif(ig,nq) |
---|
1193 | z1(ig)=1./(za(ig,1)+ zb(ig,2)*(1.-zd(ig,2))) |
---|
1194 | zc(ig,1)=(za(ig,1)*zq_tmp_vap(ig,1,igcm_h2o_vap)+ |
---|
1195 | $ zb(ig,2)*zc(ig,2) + |
---|
1196 | $ (-zdqsdif_tot(ig)) *subtimestep) *z1(ig) |
---|
1197 | zq1temp(ig)=zc(ig,1) |
---|
1198 | ENDIF !if h2o_ice_depth>0 and lag_layer |
---|
1199 | endif !if .not.watercaptag(ig) |
---|
1200 | endif ! if sublim more than surface |
---|
1201 | |
---|
1202 | ! subsurface ice <--> frost interaction !EV |
---|
1203 | IF(h2o_ice_depth(ig,islope) .gt. 4e-4 .and. lag_layer |
---|
1204 | & .and. zqsurf(ig) .gt. 0) then |
---|
1205 | DO ik=0,nsoil-2 ! go through all the layers to find the ice locations |
---|
1206 | IF((mlayer(ik).le.h2o_ice_depth(ig,islope)).and. |
---|
1207 | & (mlayer(ik+1).gt.h2o_ice_depth(ig,islope))) THEN |
---|
1208 | lice = ik+1 |
---|
1209 | EXIT |
---|
1210 | ENDIF |
---|
1211 | ENDDO !of subsurface loop |
---|
1212 | IF (lice .gt. 1) then !calculate the distance from the layers |
---|
1213 | dist_up(ig,islope)=(h2o_ice_depth(ig,islope) |
---|
1214 | & -mlayer(lice-1)) |
---|
1215 | dist_down(ig,islope)=(mlayer(lice) |
---|
1216 | & -h2o_ice_depth(ig,islope)) |
---|
1217 | dist_sum(ig,islope)=dist_up(ig,islope) |
---|
1218 | & +dist_down(ig,islope) |
---|
1219 | Tice(ig,islope)=(dist_up(ig,islope) ! Linear interp to calculate the temp |
---|
1220 | & *ptsoil(ig,lice-1,islope) |
---|
1221 | & /dist_sum(ig,islope))+ |
---|
1222 | & (dist_down(ig,islope)*ptsoil(ig,lice,islope) |
---|
1223 | & /dist_sum(ig,islope)) |
---|
1224 | ELSE |
---|
1225 | Tice(ig,islope)=ptsoil(ig,1,islope) |
---|
1226 | ENDIF |
---|
1227 | |
---|
1228 | call watersat(1,Tice(ig,1),pplev(ig,1) |
---|
1229 | & ,qsat2(ig,1)) |
---|
1230 | qeq(ig,1)=(ztsrf(ig)/Tice(ig,1)) |
---|
1231 | & *qsat2(ig,1) |
---|
1232 | ! write(*,*)'icedep=',h2o_ice_depth(ig,1) |
---|
1233 | ! write(*,*)'qeq=',qeq(ig,1) |
---|
1234 | ! write(*,*)'d=',d_coef(ig,1) |
---|
1235 | ! write(*,*)'qsat=',qsat(ig) |
---|
1236 | ! write(*,*)'dry=',dryness(ig) |
---|
1237 | ! write(*,*)'rho=',rho(ig) |
---|
1238 | zdqsdif_ssi_frost(ig,1)=(d_coef(ig,1) |
---|
1239 | & /h2o_ice_depth(ig,1)) |
---|
1240 | & *rho(ig)*dryness(ig)*(qsat(ig)-qeq(ig,1)) |
---|
1241 | !needs to change to the mean of eq |
---|
1242 | zdqsdif_tot(ig)=zdqsdif_tot(ig)-zdqsdif_ssi_frost(ig,1) |
---|
1243 | !!!!! zdsqdif_ssi_frosst need to be changed to an |
---|
1244 | !average |
---|
1245 | ELSEIF (h2o_ice_depth(ig,islope) .gt. 4e-4 .and. lag_layer |
---|
1246 | & .and. watercaptag(ig)) then |
---|
1247 | DO ik=0,nsoil-2 ! go through all the layers to find the ice locations |
---|
1248 | IF((mlayer(ik).le.h2o_ice_depth(ig,islope)).and. |
---|
1249 | & (mlayer(ik+1).gt.h2o_ice_depth(ig,islope))) THEN |
---|
1250 | lice = ik+1 |
---|
1251 | EXIT |
---|
1252 | ENDIF |
---|
1253 | ENDDO !of subsurface loop |
---|
1254 | IF (lice .gt. 1) then !calculate the distance from the layers |
---|
1255 | dist_up(ig,islope)=(h2o_ice_depth(ig,islope) |
---|
1256 | & -mlayer(lice-1)) |
---|
1257 | dist_down(ig,islope)=(mlayer(lice) |
---|
1258 | & -h2o_ice_depth(ig,islope)) |
---|
1259 | dist_sum(ig,islope)=dist_up(ig,islope) |
---|
1260 | & +dist_down(ig,islope) |
---|
1261 | Tice(ig,islope)=(dist_up(ig,islope) ! Linear interp to calculate the temp |
---|
1262 | & *ptsoil(ig,lice-1,islope) |
---|
1263 | & /dist_sum(ig,islope))+ |
---|
1264 | & (dist_down(ig,islope)*ptsoil(ig,lice,islope) |
---|
1265 | & /dist_sum(ig,islope)) |
---|
1266 | ELSE |
---|
1267 | Tice(ig,islope)=ptsoil(ig,1,islope) |
---|
1268 | ENDIF |
---|
1269 | |
---|
1270 | call watersat(1,Tice(ig,1),pplev(ig,1) |
---|
1271 | & ,qsat2(ig,1)) |
---|
1272 | qeq(ig,1)=(ztsrf(ig)/Tice(ig,1)) |
---|
1273 | & *qsat2(ig,1) |
---|
1274 | |
---|
1275 | zdqsdif_ssi_frost(ig,1)=(d_coef(ig,1) |
---|
1276 | & /h2o_ice_depth(ig,1)) |
---|
1277 | & *rho(ig)*dryness(ig)*(qsat(ig)-qeq(ig,1)) |
---|
1278 | zdqsdif_tot(ig)=zdqsdif_tot(ig)-zdqsdif_ssi_frost(ig,1) |
---|
1279 | !needs to change to the mean of eq |
---|
1280 | ENDIF |
---|
1281 | ! call write_output('subtimestep', |
---|
1282 | ! & 'vdifc substimestep length','s',subtimestep) |
---|
1283 | ! ENDDO !subsurface ice subslope |
---|
1284 | |
---|
1285 | |
---|
1286 | |
---|
1287 | c Starting upward calculations for water : |
---|
1288 | c Actualisation de h2o_vap dans le premier niveau |
---|
1289 | zq_tmp_vap(ig,1,igcm_h2o_vap)=zq1temp(ig) |
---|
1290 | c Take into account the H2O latent heat impact on the surface temperature |
---|
1291 | if (latentheat_surfwater) then |
---|
1292 | lh=(2834.3-0.28*(ztsrf(ig)-To)- |
---|
1293 | & 0.004*(ztsrf(ig)-To)*(ztsrf(ig)-To))*1.e+3 |
---|
1294 | zdtsrf(ig,islope)= zdqsdif_tot(ig)*lh |
---|
1295 | & /pcapcal(ig,islope) |
---|
1296 | endif ! (latentheat_surfwater) then |
---|
1297 | |
---|
1298 | DO ilay=2,nlay |
---|
1299 | zq_tmp_vap(ig,ilay,iq)=zc(ig,ilay)+zd(ig,ilay) |
---|
1300 | & *zq_tmp_vap(ig,ilay-1,iq) |
---|
1301 | ENDDO |
---|
1302 | c Subtimestep water budget : |
---|
1303 | ztsrf(ig) = ztsrf(ig)+(pdtsrf(ig,islope) |
---|
1304 | & + zdtsrf(ig,islope))*subtimestep |
---|
1305 | zqsurf(ig)= zqsurf(ig)+( |
---|
1306 | & zdqsdif_tot(ig))*subtimestep |
---|
1307 | if (zqsurf(ig)<0 .and. |
---|
1308 | & (.not.watercaptag(ig))) then |
---|
1309 | zqsurf(ig)=0 |
---|
1310 | endif |
---|
1311 | |
---|
1312 | c Monitoring instantaneous latent heat flux in W.m-2 : |
---|
1313 | zsurf_h2o_lh(ig,islope) = zsurf_h2o_lh(ig,islope)+ |
---|
1314 | & (zdtsrf(ig,islope)*pcapcal(ig,islope)) |
---|
1315 | & *subtimestep |
---|
1316 | |
---|
1317 | c We ensure that surface temperature can't rise above the solid domain if there |
---|
1318 | c is still ice on the surface (oldschool) |
---|
1319 | if(zqsurf(ig) |
---|
1320 | & +zdqsdif_tot(ig)*subtimestep |
---|
1321 | & .gt.frost_albedo_threshold) then ! if there is still ice, T cannot exceed To |
---|
1322 | zdtsrf(ig,islope) = min(zdtsrf(ig,islope), |
---|
1323 | & (To-ztsrf(ig))/subtimestep) ! ice melt case |
---|
1324 | endif |
---|
1325 | |
---|
1326 | c Fin du sous pas de temps |
---|
1327 | ENDDO ! tsub=1,nsubtimestep |
---|
1328 | |
---|
1329 | c Integration of subtimestep temp and water budget : |
---|
1330 | c (btw could also compute the post timestep temp and ice |
---|
1331 | c by simply adding the subtimestep trend instead of this) |
---|
1332 | surf_h2o_lh(ig,islope)= zsurf_h2o_lh(ig,islope)/ptimestep |
---|
1333 | pdtsrf(ig,islope)= (ztsrf(ig) - |
---|
1334 | & ptsrf(ig,islope))/ptimestep |
---|
1335 | pdqsdif(ig,igcm_h2o_ice,islope)= |
---|
1336 | & (zqsurf(ig)- pqsurf(ig,igcm_h2o_ice,islope)/ |
---|
1337 | & cos(pi*def_slope_mean(islope)/180.)) |
---|
1338 | & /ptimestep |
---|
1339 | c if subliming more than qsurf(ice) and on watercaptag, water |
---|
1340 | c sublimates from watercap reservoir (dwatercap_dif is <0) |
---|
1341 | if(watercaptag(ig)) then |
---|
1342 | if ((-pdqsdif(ig,igcm_h2o_ice,islope)*ptimestep) |
---|
1343 | & .gt.(pqsurf(ig,igcm_h2o_ice,islope) |
---|
1344 | & /cos(pi*def_slope_mean(islope)/180.))) then |
---|
1345 | dwatercap_dif(ig,islope)= |
---|
1346 | & pdqsdif(ig,igcm_h2o_ice,islope)+ |
---|
1347 | & (pqsurf(ig,igcm_h2o_ice,islope) / |
---|
1348 | & cos(pi*def_slope_mean(islope)/180.))/ptimestep |
---|
1349 | pdqsdif(ig,igcm_h2o_ice,islope)= |
---|
1350 | & - (pqsurf(ig,igcm_h2o_ice,islope)/ |
---|
1351 | & cos(pi*def_slope_mean(islope)/180.))/ptimestep |
---|
1352 | endif! ((-pdqsdif(ig)*ptimestep) |
---|
1353 | endif !(watercaptag(ig)) then |
---|
1354 | zq_slope_vap(ig,:,:,islope) = zq_tmp_vap(ig,:,:) |
---|
1355 | ENDDO ! of DO ig=1,ngrid |
---|
1356 | ENDDO ! islope |
---|
1357 | c Some grid box averages: interface with the atmosphere |
---|
1358 | DO ig = 1,ngrid |
---|
1359 | DO ilay = 1,nlay |
---|
1360 | zq(ig,ilay,iq) = 0. |
---|
1361 | DO islope = 1,nslope |
---|
1362 | zq(ig,ilay,iq) = zq(ig,ilay,iq) + |
---|
1363 | $ zq_slope_vap(ig,ilay,iq,islope) * |
---|
1364 | $ subslope_dist(ig,islope) |
---|
1365 | ENDDO |
---|
1366 | ENDDO |
---|
1367 | ENDDO |
---|
1368 | ! Recompute values in kg/m^2 slopped |
---|
1369 | DO ig = 1,ngrid |
---|
1370 | DO islope = 1,nslope |
---|
1371 | pdqsdif(ig,igcm_h2o_ice,islope) = |
---|
1372 | & pdqsdif(ig,igcm_h2o_ice,islope) |
---|
1373 | & * cos(pi*def_slope_mean(islope)/180.) |
---|
1374 | |
---|
1375 | dwatercap_dif(ig,islope) = |
---|
1376 | & dwatercap_dif(ig,islope) |
---|
1377 | & * cos(pi*def_slope_mean(islope)/180.) |
---|
1378 | ENDDO |
---|
1379 | ENDDO |
---|
1380 | |
---|
1381 | END IF ! of IF ((water).and.(iq.eq.igcm_h2o_vap)) |
---|
1382 | |
---|
1383 | c --------- end of h2o_vap ---------------------------- |
---|
1384 | |
---|
1385 | c --------- hdo_vap ----------------------------------- |
---|
1386 | |
---|
1387 | c hdo_ice has already been with along h2o_ice |
---|
1388 | c amongst "normal" tracers (ie not h2o_vap) |
---|
1389 | |
---|
1390 | if (hdo.and.(iq.eq.igcm_hdo_vap)) then |
---|
1391 | zb(1:ngrid,2:nlay)=zkh(1:ngrid,2:nlay)*zb0(1:ngrid,2:nlay) |
---|
1392 | zb(1:ngrid,1)=0 |
---|
1393 | |
---|
1394 | DO ig=1,ngrid |
---|
1395 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
---|
1396 | zc(ig,nlay)=za(ig,nlay)*zq(ig,nlay,iq)*z1(ig) |
---|
1397 | zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
---|
1398 | ENDDO |
---|
1399 | |
---|
1400 | DO ilay=nlay-1,2,-1 |
---|
1401 | DO ig=1,ngrid |
---|
1402 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
---|
1403 | $ zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
---|
1404 | zc(ig,ilay)=(za(ig,ilay)*zq(ig,ilay,iq)+ |
---|
1405 | $ zb(ig,ilay+1)*zc(ig,ilay+1))*z1(ig) |
---|
1406 | zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
---|
1407 | ENDDO |
---|
1408 | ENDDO |
---|
1409 | hdoflux_meshavg(:) = 0. |
---|
1410 | DO islope = 1,nslope |
---|
1411 | |
---|
1412 | pdqsdif_tmphdo(:,:) = pdqsdif(:,:,islope) |
---|
1413 | & /cos(pi*def_slope_mean(islope)/180.) |
---|
1414 | |
---|
1415 | call watersat(ngrid,pdtsrf(:,islope)*ptimestep + |
---|
1416 | & ptsrf(:,islope),pplev(:,1),qsat_tmp) |
---|
1417 | |
---|
1418 | CALL hdo_surfex(ngrid,nlay,nq,ptimestep, |
---|
1419 | & zt,pplay,zq,pqsurf(:,:,islope), |
---|
1420 | & saved_h2o_vap,qsat_tmp, |
---|
1421 | & pdqsdif_tmphdo, |
---|
1422 | & dwatercap_dif(:,islope)/cos(pi*def_slope_mean(islope)/180.), |
---|
1423 | & hdoflux(:,islope)) |
---|
1424 | |
---|
1425 | pdqsdif(:,:,islope) = pdqsdif_tmphdo(:,:) * |
---|
1426 | & cos(pi*def_slope_mean(islope)/180.) |
---|
1427 | DO ig = 1,ngrid |
---|
1428 | hdoflux_meshavg(ig) = hdoflux_meshavg(ig) + |
---|
1429 | & hdoflux(ig,islope)*subslope_dist(ig,islope) |
---|
1430 | |
---|
1431 | ENDDO !ig = 1,ngrid |
---|
1432 | ENDDO !islope = 1,nslope |
---|
1433 | |
---|
1434 | DO ig=1,ngrid |
---|
1435 | z1(ig)=1./(za(ig,1)+zb(ig,1)+ |
---|
1436 | $ zb(ig,2)*(1.-zd(ig,2))) |
---|
1437 | zc(ig,1)=(za(ig,1)*zq(ig,1,iq)+ |
---|
1438 | $ zb(ig,2)*zc(ig,2) + |
---|
1439 | $ (-hdoflux_meshavg(ig)) *ptimestep) *z1(ig) !tracer flux from surface |
---|
1440 | ENDDO |
---|
1441 | |
---|
1442 | DO ig=1,ngrid |
---|
1443 | zq(ig,1,iq)=zc(ig,1) |
---|
1444 | DO ilay=2,nlay |
---|
1445 | zq(ig,ilay,iq)=zc(ig,ilay)+zd(ig,ilay)*zq(ig,ilay-1,iq) |
---|
1446 | ENDDO |
---|
1447 | ENDDO |
---|
1448 | endif ! (hdo.and.(iq.eq.igcm_hdo_vap)) |
---|
1449 | |
---|
1450 | c --------- end of hdo ---------------------------- |
---|
1451 | |
---|
1452 | enddo ! of do iq=1,nq |
---|
1453 | |
---|
1454 | c --------- end of tracers ---------------------------- |
---|
1455 | |
---|
1456 | call write_output("surf_h2o_lh", |
---|
1457 | & "Ground ice latent heat flux", |
---|
1458 | & "W.m-2",surf_h2o_lh(:,iflat)) |
---|
1459 | ! call write_output('zdqsdif_ssi_frost', |
---|
1460 | ! & 'Flux between frost and subsurface','kg.m-2.s-1', |
---|
1461 | ! & zdqsdif_ssi_frost(:,1)) |
---|
1462 | |
---|
1463 | ! call write_output('zdq_subtimestep', |
---|
1464 | ! & 'Actual flux zdqsdif_surf*subtimestep', |
---|
1465 | ! & 'kg.m-2',zdqsdif_tot(:)*subtimestep) |
---|
1466 | ! call write_output('zdq_end', |
---|
1467 | ! & 'Flux after all contributions', |
---|
1468 | ! & 'kg.m-2.s-1',zdqsdif_tot(:)) |
---|
1469 | C Diagnostic output for HDO |
---|
1470 | ! if (hdo) then |
---|
1471 | ! CALL write_output('hdoflux', |
---|
1472 | ! & 'hdoflux', |
---|
1473 | ! & ' ',hdoflux_meshavg(:)) |
---|
1474 | ! CALL write_output('h2oflux', |
---|
1475 | ! & 'h2oflux', |
---|
1476 | ! & ' ',h2oflux(:)) |
---|
1477 | ! endif |
---|
1478 | |
---|
1479 | c----------------------------------------------------------------------- |
---|
1480 | c 8. calcul final des tendances de la diffusion verticale |
---|
1481 | c ---------------------------------------------------- |
---|
1482 | |
---|
1483 | DO ilev = 1, nlay |
---|
1484 | DO ig=1,ngrid |
---|
1485 | pdudif(ig,ilev)=( zu(ig,ilev)- |
---|
1486 | $ (pu(ig,ilev)+pdufi(ig,ilev)*ptimestep) )/ptimestep |
---|
1487 | pdvdif(ig,ilev)=( zv(ig,ilev)- |
---|
1488 | $ (pv(ig,ilev)+pdvfi(ig,ilev)*ptimestep) )/ptimestep |
---|
1489 | hh = ph(ig,ilev)+pdhfi(ig,ilev)*ptimestep |
---|
1490 | $ + (latcond*dmice(ig,ilev)/cpp)/ppopsk(ig,ilev) |
---|
1491 | pdhdif(ig,ilev)=( zhs(ig,ilev)- hh )/ptimestep |
---|
1492 | ENDDO |
---|
1493 | ENDDO |
---|
1494 | |
---|
1495 | pdqdif(1:ngrid,1:nlay,1:nq)=(zq(1:ngrid,1:nlay,1:nq)- |
---|
1496 | & (pq(1:ngrid,1:nlay,1:nq) |
---|
1497 | & +pdqfi(1:ngrid,1:nlay,1:nq) |
---|
1498 | & *ptimestep))/ptimestep |
---|
1499 | |
---|
1500 | c ** diagnostique final |
---|
1501 | c ------------------ |
---|
1502 | |
---|
1503 | IF(lecrit) THEN |
---|
1504 | PRINT*,'In vdif' |
---|
1505 | PRINT*,'Ts (t) and Ts (t+st)' |
---|
1506 | WRITE(*,'(a10,3a15)') |
---|
1507 | s 'theta(t)','theta(t+dt)','u(t)','u(t+dt)' |
---|
1508 | PRINT*,ptsrf(ngrid/2+1,:),ztsrf2(ngrid/2+1) |
---|
1509 | DO ilev=1,nlay |
---|
1510 | WRITE(*,'(4f15.7)') |
---|
1511 | s ph(ngrid/2+1,ilev),zhs(ngrid/2+1,ilev), |
---|
1512 | s pu(ngrid/2+1,ilev),zu(ngrid/2+1,ilev) |
---|
1513 | |
---|
1514 | ENDDO |
---|
1515 | ENDIF |
---|
1516 | |
---|
1517 | END SUBROUTINE vdifc |
---|
1518 | |
---|
1519 | c==================================== |
---|
1520 | |
---|
1521 | SUBROUTINE make_tsub(naersize,dtsurf,qsurf,ptimestep, |
---|
1522 | $ dtmax,watercaptag,ntsub) |
---|
1523 | |
---|
1524 | c Pas de temps adaptatif en estimant le taux de sublimation |
---|
1525 | c et en adaptant avec un critere "dtmax" du chauffage a accomoder |
---|
1526 | c dtmax est regle empiriquement (pour l'instant) a 0.5 K |
---|
1527 | |
---|
1528 | integer,intent(in) :: naersize |
---|
1529 | real,intent(in) :: dtsurf(naersize) |
---|
1530 | real,intent(in) :: qsurf(naersize) |
---|
1531 | logical,intent(in) :: watercaptag(naersize) |
---|
1532 | real,intent(in) :: ptimestep |
---|
1533 | real,intent(in) :: dtmax |
---|
1534 | real :: ztsub(naersize) |
---|
1535 | integer :: i |
---|
1536 | integer,intent(out) :: ntsub(naersize) |
---|
1537 | |
---|
1538 | do i=1,naersize |
---|
1539 | if ((qsurf(i).eq.0).and. |
---|
1540 | & (.not.watercaptag(i))) then |
---|
1541 | ntsub(i) = 1 |
---|
1542 | else |
---|
1543 | ztsub(i) = ptimestep * dtsurf(i) / dtmax |
---|
1544 | ntsub(i) = ceiling(abs(ztsub(i))) |
---|
1545 | endif ! (qsurf(i).eq.0) then |
---|
1546 | c |
---|
1547 | c write(78,*), dtsurf*ptimestep, dtsurf, ntsub |
---|
1548 | enddo! 1=1,ngrid |
---|
1549 | |
---|
1550 | |
---|
1551 | |
---|
1552 | END SUBROUTINE make_tsub |
---|
1553 | END MODULE vdifc_mod |
---|