1 | module turbdiff_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 turbdiff(ngrid,nlay,nq,rnat, & |
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8 | ptimestep,pcapcal, & |
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9 | pplay,pplev,pzlay,pzlev,pz0, & |
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10 | pu,pv,pt,ppopsk,pq,ptsrf,pemis,pqsurf, & |
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11 | pdtfi,pdqfi,pfluxsrf, & |
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12 | Pdudif,pdvdif,pdtdif,pdtsrf,sensibFlux,pq2, & |
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13 | pdqdif,pdqevap,pdqsdif,flux_u,flux_v) |
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14 | |
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15 | use watercommon_h, only : RLVTT, T_h2O_ice_liq, RCPD, mx_eau_sol,Psat_water, Lcpdqsat_water |
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16 | use radcommon_h, only : sigma, glat |
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17 | use surfdat_h, only: dryness |
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18 | use tracer_h, only: igcm_h2o_vap, igcm_h2o_ice |
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19 | use comcstfi_mod, only: rcp, g, r, cpp |
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20 | use callkeys_mod, only: water,tracer,nosurf,kmixmin |
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21 | use turb_mod, only : ustar |
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22 | #ifdef MESOSCALE |
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23 | use comm_wrf, only : comm_LATENT_HF |
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24 | #endif |
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25 | implicit none |
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26 | |
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27 | !================================================================== |
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28 | ! |
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29 | ! Purpose |
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30 | ! ------- |
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31 | ! Turbulent diffusion (mixing) for pot. T, U, V and tracers |
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32 | ! |
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33 | ! Implicit scheme |
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34 | ! We start by adding to variables x the physical tendencies |
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35 | ! already computed. We resolve the equation: |
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36 | ! |
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37 | ! x(t+1) = x(t) + dt * (dx/dt)phys(t) + dt * (dx/dt)difv(t+1) |
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38 | ! |
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39 | ! Authors |
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40 | ! ------- |
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41 | ! F. Hourdin, F. Forget, R. Fournier (199X) |
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42 | ! R. Wordsworth, B. Charnay (2010) |
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43 | ! J. Leconte (2012): To f90 |
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44 | ! - Rewritten the diffusion scheme to conserve total enthalpy |
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45 | ! by accounting for dissipation of turbulent kinetic energy. |
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46 | ! - Accounting for lost mean flow kinetic energy should come soon. |
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47 | ! |
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48 | !================================================================== |
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49 | |
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50 | !----------------------------------------------------------------------- |
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51 | ! declarations |
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52 | ! ------------ |
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53 | |
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54 | ! arguments |
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55 | ! --------- |
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56 | INTEGER,INTENT(IN) :: ngrid |
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57 | INTEGER,INTENT(IN) :: nlay |
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58 | REAL,INTENT(IN) :: ptimestep |
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59 | REAL,INTENT(IN) :: pplay(ngrid,nlay),pplev(ngrid,nlay+1) |
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60 | REAL,INTENT(IN) :: pzlay(ngrid,nlay),pzlev(ngrid,nlay+1) |
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61 | REAL,INTENT(IN) :: pu(ngrid,nlay),pv(ngrid,nlay) |
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62 | REAL,INTENT(IN) :: pt(ngrid,nlay),ppopsk(ngrid,nlay) |
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63 | REAL,INTENT(IN) :: ptsrf(ngrid) ! surface temperature (K) |
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64 | REAL,INTENT(IN) :: pemis(ngrid) |
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65 | REAL,INTENT(IN) :: pdtfi(ngrid,nlay) |
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66 | REAL,INTENT(IN) :: pfluxsrf(ngrid) |
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67 | REAL,INTENT(OUT) :: pdudif(ngrid,nlay),pdvdif(ngrid,nlay) |
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68 | REAL,INTENT(OUT) :: pdtdif(ngrid,nlay) |
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69 | REAL,INTENT(OUT) :: pdtsrf(ngrid) ! tendency (K/s) on surface temperature |
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70 | REAL,INTENT(OUT) :: sensibFlux(ngrid) |
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71 | REAL,INTENT(IN) :: pcapcal(ngrid) |
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72 | REAL,INTENT(INOUT) :: pq2(ngrid,nlay+1) |
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73 | REAL,INTENT(OUT) :: flux_u(ngrid),flux_v(ngrid) |
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74 | REAL,INTENT(IN) :: rnat(ngrid) |
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75 | |
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76 | REAL,INTENT(IN) :: pz0 |
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77 | |
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78 | ! Tracers |
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79 | ! -------- |
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80 | integer,intent(in) :: nq |
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81 | real,intent(in) :: pqsurf(ngrid,nq) |
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82 | real,intent(in) :: pq(ngrid,nlay,nq), pdqfi(ngrid,nlay,nq) |
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83 | real,intent(out) :: pdqdif(ngrid,nlay,nq) |
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84 | real,intent(out) :: pdqsdif(ngrid,nq) |
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85 | |
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86 | ! local |
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87 | ! ----- |
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88 | integer ilev,ig,ilay,nlev |
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89 | |
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90 | REAL z4st,zdplanck(ngrid) |
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91 | REAL zkv(ngrid,nlay+1),zkh(ngrid,nlay+1) |
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92 | REAL zcdv(ngrid),zcdh(ngrid) |
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93 | REAL zcdv_true(ngrid),zcdh_true(ngrid) |
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94 | REAL zu(ngrid,nlay),zv(ngrid,nlay) |
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95 | REAL zh(ngrid,nlay),zt(ngrid,nlay) |
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96 | REAL ztsrf(ngrid) |
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97 | REAL z1(ngrid),z2(ngrid) |
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98 | REAL zmass(ngrid,nlay) |
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99 | REAL zfluxv(ngrid,nlay),zfluxt(ngrid,nlay),zfluxq(ngrid,nlay) |
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100 | REAL zb0(ngrid,nlay) |
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101 | REAL zExner(ngrid,nlay),zovExner(ngrid,nlay) |
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102 | REAL zcv(ngrid,nlay),zdv(ngrid,nlay) !inversion coefficient for winds |
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103 | REAL zct(ngrid,nlay),zdt(ngrid,nlay) !inversion coefficient for temperature |
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104 | REAL zcq(ngrid,nlay),zdq(ngrid,nlay) !inversion coefficient for tracers |
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105 | REAL zcst1 |
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106 | REAL zu2!, a |
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107 | REAL zcq0(ngrid),zdq0(ngrid) |
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108 | REAL zx_alf1(ngrid),zx_alf2(ngrid) |
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109 | ! 1D eddy diffusion coefficient |
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110 | REAL kzz_eddy(nlay) |
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111 | REAL pmin_kzz |
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112 | |
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113 | LOGICAL,SAVE :: firstcall=.true. |
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114 | !$OMP THREADPRIVATE(firstcall) |
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115 | |
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116 | ! Tracers |
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117 | ! ------- |
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118 | INTEGER iq |
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119 | REAL zq(ngrid,nlay,nq) |
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120 | REAL zqnoevap(ngrid,nlay) !special for water case to compute where evaporated water goes. |
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121 | REAL pdqevap(ngrid,nlay) !special for water case to compute where evaporated water goes. |
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122 | REAL zdmassevap(ngrid) |
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123 | REAL rho(ngrid) ! near-surface air density |
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124 | |
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125 | ! Variables added for implicit latent heat inclusion |
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126 | ! -------------------------------------------------- |
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127 | real dqsat(ngrid),psat_temp,qsat(ngrid),psat(ngrid) |
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128 | |
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129 | integer, save :: ivap, iliq, iliq_surf,iice_surf ! also make liq for clarity on surface... |
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130 | !$OMP THREADPRIVATE(ivap,iliq,iliq_surf,iice_surf) |
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131 | |
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132 | real, parameter :: karman=0.4 |
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133 | real cd0, roughratio |
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134 | |
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135 | real dqsdif_total(ngrid) |
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136 | real zq0(ngrid) |
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137 | |
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138 | |
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139 | ! Coherence test |
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140 | ! -------------- |
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141 | |
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142 | IF (firstcall) THEN |
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143 | |
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144 | if(water)then |
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145 | ivap=igcm_h2o_vap |
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146 | iliq=igcm_h2o_ice |
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147 | iliq_surf=igcm_h2o_vap |
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148 | iice_surf=igcm_h2o_ice ! simply to make the code legible |
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149 | ! to be generalised |
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150 | else |
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151 | ivap=0 |
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152 | iliq=0 |
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153 | iliq_surf=0 |
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154 | iice_surf=0 ! simply to make the code legible |
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155 | endif |
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156 | sensibFlux(:)=0. |
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157 | |
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158 | firstcall=.false. |
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159 | ENDIF |
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160 | |
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161 | !----------------------------------------------------------------------- |
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162 | ! 1. Initialisation |
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163 | ! ----------------- |
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164 | |
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165 | nlev=nlay+1 |
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166 | |
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167 | ! Calculate rho*dz, (P/Ps)**(R/cp) and dt*rho/dz=dt*rho**2 g/dp |
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168 | ! with rho=p/RT=p/ (R Theta) (p/ps)**kappa |
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169 | ! --------------------------------------------- |
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170 | |
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171 | DO ilay=1,nlay |
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172 | DO ig=1,ngrid |
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173 | zmass(ig,ilay)=(pplev(ig,ilay)-pplev(ig,ilay+1))/glat(ig) |
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174 | zExner(ig,ilay)=(pplev(ig,ilay)/pplev(ig,1))**rcp |
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175 | zovExner(ig,ilay)=1./ppopsk(ig,ilay) |
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176 | ENDDO |
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177 | ENDDO |
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178 | |
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179 | zcst1=4.*g*ptimestep/(R*R) |
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180 | DO ilev=2,nlev-1 |
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181 | DO ig=1,ngrid |
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182 | zb0(ig,ilev)=pplev(ig,ilev)/(pt(ig,ilev-1)+pt(ig,ilev)) |
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183 | zb0(ig,ilev)=zcst1*zb0(ig,ilev)*zb0(ig,ilev)/(pplay(ig,ilev-1)-pplay(ig,ilev)) |
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184 | ENDDO |
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185 | ENDDO |
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186 | DO ig=1,ngrid |
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187 | zb0(ig,1)=ptimestep*pplev(ig,1)/(R*ptsrf(ig)) |
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188 | ENDDO |
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189 | dqsdif_total(:)=0.0 |
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190 | |
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191 | !----------------------------------------------------------------------- |
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192 | ! 2. Add the physical tendencies computed so far |
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193 | ! ---------------------------------------------- |
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194 | |
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195 | DO ilev=1,nlay |
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196 | DO ig=1,ngrid |
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197 | zu(ig,ilev)=pu(ig,ilev) |
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198 | zv(ig,ilev)=pv(ig,ilev) |
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199 | zt(ig,ilev)=pt(ig,ilev)+pdtfi(ig,ilev)*ptimestep |
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200 | zh(ig,ilev)=pt(ig,ilev)*zovExner(ig,ilev) !for call vdif_kc, but could be moved and computed there |
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201 | ENDDO |
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202 | ENDDO |
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203 | if(tracer) then |
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204 | DO iq =1, nq |
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205 | DO ilev=1,nlay |
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206 | DO ig=1,ngrid |
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207 | zq(ig,ilev,iq)=pq(ig,ilev,iq) + pdqfi(ig,ilev,iq)*ptimestep |
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208 | ENDDO |
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209 | ENDDO |
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210 | ENDDO |
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211 | if (water) then |
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212 | DO ilev=1,nlay |
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213 | DO ig=1,ngrid |
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214 | zqnoevap(ig,ilev)=pq(ig,ilev,ivap) + pdqfi(ig,ilev,ivap)*ptimestep |
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215 | ENDDO |
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216 | ENDDO |
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217 | Endif |
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218 | end if |
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219 | |
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220 | !----------------------------------------------------------------------- |
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221 | ! 3. Turbulence scheme |
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222 | ! -------------------- |
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223 | ! |
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224 | ! Source of turbulent kinetic energy at the surface |
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225 | ! ------------------------------------------------- |
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226 | ! Formula is Cd_0 = (karman / log[1+z1/z0])^2 |
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227 | |
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228 | DO ig=1,ngrid |
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229 | roughratio = 1. + pzlay(ig,1)/pz0 |
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230 | cd0 = karman/log(roughratio) |
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231 | cd0 = cd0*cd0 |
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232 | zcdv_true(ig) = cd0 |
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233 | zcdh_true(ig) = cd0 |
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234 | if(nosurf)then |
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235 | zcdv_true(ig)=0.D+0 !JL12 disable atm/surface momentum flux |
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236 | zcdh_true(ig)=0.D+0 !JL12 disable sensible heat flux |
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237 | endif |
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238 | ENDDO |
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239 | |
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240 | DO ig=1,ngrid |
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241 | zu2=pu(ig,1)*pu(ig,1)+pv(ig,1)*pv(ig,1) |
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242 | zcdv(ig)=zcdv_true(ig)*sqrt(zu2) |
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243 | zcdh(ig)=zcdh_true(ig)*sqrt(zu2) |
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244 | ENDDO |
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245 | |
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246 | ! Turbulent diffusion coefficients in the boundary layer |
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247 | ! ------------------------------------------------------ |
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248 | |
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249 | call vdif_kc(ngrid,nlay,nq,ptimestep,g,pzlev,pzlay,pu,pv,pq,zh,zcdv_true,pq2,zkv,zkh) !JL12 why not call vdif_kc with updated winds and temperature |
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250 | |
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251 | ! Adding eddy mixing to mimic 3D general circulation in 1D |
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252 | ! R. Wordsworth & F. Forget (2010) |
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253 | if ((ngrid.eq.1)) then |
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254 | ! kmixmin minimum eddy mix coeff in 1D |
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255 | ! set up in inifis_mod.F90 - default value 1.0e-2 |
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256 | do ilev=1,nlay |
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257 | |
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258 | ! Here to code your specific eddy mix coeff in 1D |
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259 | ! Earth example that can be uncommented below |
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260 | ! ------------------------------------------------- |
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261 | ! *====== Earth kzz from Zahnle et al. 2006 ======* |
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262 | ! ------------------------------------------------- |
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263 | ! if(pzlev(1,ilev).le.11.0e3) then |
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264 | ! kzz_eddy(ilev)=10.0 |
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265 | ! pmin_kzz=pplev(1,ilev)*exp((pzlev(1,ilev)-11.0e3)*g/(r*zt(1,ilev))) |
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266 | ! else |
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267 | ! kzz_eddy(ilev)=0.1*(pplev(1,ilev)/pmin_kzz)**(-0.5) |
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268 | ! kzz_eddy(ilev)=min(kzz_eddy(ilev),100.0) |
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269 | ! endif |
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270 | ! do ig=1,ngrid |
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271 | ! zkh(ig,ilev) = max(kzz_eddy(ilev),zkh(ig,ilev)) |
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272 | ! zkv(ig,ilev) = max(kzz_eddy(ilev),zkv(ig,ilev)) |
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273 | ! end do |
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274 | |
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275 | do ig=1,ngrid |
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276 | zkh(ig,ilev) = max(kmixmin,zkh(ig,ilev)) |
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277 | zkv(ig,ilev) = max(kmixmin,zkv(ig,ilev)) |
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278 | end do |
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279 | end do |
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280 | end if |
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281 | |
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282 | !JL12 change zkv at the surface by zcdv to calculate the surface momentum flux properly |
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283 | DO ig=1,ngrid |
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284 | zkv(ig,1)=zcdv(ig) |
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285 | ENDDO |
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286 | !we treat only winds, energy and tracers coefficients will be computed with upadted winds |
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287 | !JL12 calculate the flux coefficients (tables multiplied elements by elements) |
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288 | zfluxv(1:ngrid,1:nlay)=zkv(1:ngrid,1:nlay)*zb0(1:ngrid,1:nlay) |
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289 | |
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290 | !----------------------------------------------------------------------- |
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291 | ! 4. Implicit inversion of u |
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292 | ! -------------------------- |
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293 | |
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294 | ! u(t+1) = u(t) + dt * {(du/dt)phys}(t) + dt * {(du/dt)difv}(t+1) |
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295 | ! avec |
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296 | ! /zu/ = u(t) + dt * {(du/dt)phys}(t) (voir paragraphe 2.) |
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297 | ! et |
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298 | ! dt * {(du/dt)difv}(t+1) = dt * {(d/dz)[ Ku (du/dz) ]}(t+1) |
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299 | ! donc les entrees sont /zcdv/ pour la condition a la limite sol |
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300 | ! et /zkv/ = Ku |
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301 | |
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302 | DO ig=1,ngrid |
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303 | z1(ig)=1./(zmass(ig,nlay)+zfluxv(ig,nlay)) |
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304 | zcv(ig,nlay)=zmass(ig,nlay)*zu(ig,nlay)*z1(ig) |
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305 | zdv(ig,nlay)=zfluxv(ig,nlay)*z1(ig) |
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306 | ENDDO |
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307 | |
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308 | DO ilay=nlay-1,1,-1 |
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309 | DO ig=1,ngrid |
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310 | z1(ig)=1./(zmass(ig,ilay)+zfluxv(ig,ilay) + zfluxv(ig,ilay+1)*(1.-zdv(ig,ilay+1))) |
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311 | zcv(ig,ilay)=(zmass(ig,ilay)*zu(ig,ilay)+zfluxv(ig,ilay+1)*zcv(ig,ilay+1))*z1(ig) |
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312 | zdv(ig,ilay)=zfluxv(ig,ilay)*z1(ig) |
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313 | ENDDO |
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314 | ENDDO |
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315 | |
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316 | DO ig=1,ngrid |
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317 | zu(ig,1)=zcv(ig,1) |
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318 | ENDDO |
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319 | DO ilay=2,nlay |
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320 | DO ig=1,ngrid |
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321 | zu(ig,ilay)=zcv(ig,ilay)+zdv(ig,ilay)*zu(ig,ilay-1) |
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322 | ENDDO |
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323 | ENDDO |
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324 | |
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325 | !----------------------------------------------------------------------- |
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326 | ! 5. Implicit inversion of v |
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327 | ! -------------------------- |
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328 | |
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329 | ! v(t+1) = v(t) + dt * {(dv/dt)phys}(t) + dt * {(dv/dt)difv}(t+1) |
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330 | ! avec |
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331 | ! /zv/ = v(t) + dt * {(dv/dt)phys}(t) (voir paragraphe 2.) |
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332 | ! et |
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333 | ! dt * {(dv/dt)difv}(t+1) = dt * {(d/dz)[ Kv (dv/dz) ]}(t+1) |
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334 | ! donc les entrees sont /zcdv/ pour la condition a la limite sol |
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335 | ! et /zkv/ = Kv |
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336 | |
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337 | DO ig=1,ngrid |
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338 | z1(ig)=1./(zmass(ig,nlay)+zfluxv(ig,nlay)) |
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339 | zcv(ig,nlay)=zmass(ig,nlay)*zv(ig,nlay)*z1(ig) |
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340 | zdv(ig,nlay)=zfluxv(ig,nlay)*z1(ig) |
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341 | ENDDO |
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342 | |
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343 | DO ilay=nlay-1,1,-1 |
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344 | DO ig=1,ngrid |
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345 | z1(ig)=1./(zmass(ig,ilay)+zfluxv(ig,ilay)+zfluxv(ig,ilay+1)*(1.-zdv(ig,ilay+1))) |
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346 | zcv(ig,ilay)=(zmass(ig,ilay)*zv(ig,ilay)+zfluxv(ig,ilay+1)*zcv(ig,ilay+1))*z1(ig) |
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347 | zdv(ig,ilay)=zfluxv(ig,ilay)*z1(ig) |
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348 | ENDDO |
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349 | ENDDO |
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350 | |
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351 | DO ig=1,ngrid |
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352 | zv(ig,1)=zcv(ig,1) |
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353 | ENDDO |
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354 | DO ilay=2,nlay |
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355 | DO ig=1,ngrid |
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356 | zv(ig,ilay)=zcv(ig,ilay)+zdv(ig,ilay)*zv(ig,ilay-1) |
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357 | ENDDO |
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358 | ENDDO |
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359 | |
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360 | ! Calcul of wind stress |
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361 | |
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362 | DO ig=1,ngrid |
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363 | flux_u(ig) = zfluxv(ig,1)/ptimestep*zu(ig,1) |
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364 | flux_v(ig) = zfluxv(ig,1)/ptimestep*zv(ig,1) |
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365 | ENDDO |
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366 | |
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367 | |
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368 | !---------------------------------------------------------------------------- |
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369 | ! 6. Implicit inversion of h, not forgetting the coupling with the ground |
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370 | |
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371 | ! h(t+1) = h(t) + dt * {(dh/dt)phys}(t) + dt * {(dh/dt)difv}(t+1) |
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372 | ! avec |
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373 | ! /zh/ = h(t) + dt * {(dh/dt)phys}(t) (voir paragraphe 2.) |
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374 | ! et |
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375 | ! dt * {(dh/dt)difv}(t+1) = dt * {(d/dz)[ Kh (dh/dz) ]}(t+1) |
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376 | ! donc les entrees sont /zcdh/ pour la condition de raccord au sol |
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377 | ! et /zkh/ = Kh |
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378 | |
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379 | ! Using the wind modified by friction for lifting and sublimation |
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380 | ! --------------------------------------------------------------- |
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381 | DO ig=1,ngrid |
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382 | zu2 = zu(ig,1)*zu(ig,1)+zv(ig,1)*zv(ig,1) |
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383 | zcdv(ig) = zcdv_true(ig)*sqrt(zu2) |
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384 | zcdh(ig) = zcdh_true(ig)*sqrt(zu2) |
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385 | zkh(ig,1)= zcdh(ig) |
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386 | ustar(ig)=sqrt(zcdv_true(ig))*sqrt(zu2) |
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387 | ENDDO |
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388 | |
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389 | |
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390 | ! JL12 calculate the flux coefficients (tables multiplied elements by elements) |
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391 | ! --------------------------------------------------------------- |
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392 | zfluxq(1:ngrid,1:nlay)=zkh(1:ngrid,1:nlay)*zb0(1:ngrid,1:nlay) !JL12 we save zfluxq which doesn't need the Exner factor |
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393 | zfluxt(1:ngrid,1:nlay)=zfluxq(1:ngrid,1:nlay)*zExner(1:ngrid,1:nlay) |
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394 | |
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395 | DO ig=1,ngrid |
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396 | z1(ig)=1./(zmass(ig,nlay)+zfluxt(ig,nlay)*zovExner(ig,nlay)) |
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397 | zct(ig,nlay)=zmass(ig,nlay)*zt(ig,nlay)*z1(ig) |
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398 | zdt(ig,nlay)=zfluxt(ig,nlay)*zovExner(ig,nlay-1)*z1(ig) |
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399 | ENDDO |
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400 | |
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401 | DO ilay=nlay-1,2,-1 |
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402 | DO ig=1,ngrid |
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403 | z1(ig)=1./(zmass(ig,ilay)+zfluxt(ig,ilay)*zovExner(ig,ilay)+ & |
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404 | zfluxt(ig,ilay+1)*(zovExner(ig,ilay)-zdt(ig,ilay+1)*zovExner(ig,ilay+1))) |
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405 | zct(ig,ilay)=(zmass(ig,ilay)*zt(ig,ilay)+zfluxt(ig,ilay+1)*zct(ig,ilay+1)*zovExner(ig,ilay+1))*z1(ig) |
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406 | zdt(ig,ilay)=zfluxt(ig,ilay)*z1(ig)*zovExner(ig,ilay-1) |
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407 | ENDDO |
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408 | ENDDO |
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409 | |
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410 | !JL12 we treat last point afterward because zovExner(ig,ilay-1) does not exist there |
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411 | DO ig=1,ngrid |
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412 | z1(ig)=1./(zmass(ig,1)+zfluxt(ig,1)*zovExner(ig,1)+ & |
---|
413 | zfluxt(ig,2)*(zovExner(ig,1)-zdt(ig,2)*zovExner(ig,2))) |
---|
414 | zct(ig,1)=(zmass(ig,1)*zt(ig,1)+zfluxt(ig,2)*zct(ig,2)*zovExner(ig,2))*z1(ig) |
---|
415 | zdt(ig,1)=zfluxt(ig,1)*z1(ig) |
---|
416 | ENDDO |
---|
417 | |
---|
418 | |
---|
419 | ! Calculate (d Planck / dT) at the interface temperature |
---|
420 | ! ------------------------------------------------------ |
---|
421 | |
---|
422 | z4st=4.0*sigma*ptimestep |
---|
423 | DO ig=1,ngrid |
---|
424 | zdplanck(ig)=z4st*pemis(ig)*ptsrf(ig)*ptsrf(ig)*ptsrf(ig) |
---|
425 | ENDDO |
---|
426 | |
---|
427 | ! Calculate temperature tendency at the interface (dry case) |
---|
428 | ! ---------------------------------------------------------- |
---|
429 | ! Sum of fluxes at interface at time t + \delta t gives change in T: |
---|
430 | ! radiative fluxes |
---|
431 | ! turbulent convective (sensible) heat flux |
---|
432 | ! flux (if any) from subsurface |
---|
433 | |
---|
434 | if(.not.water) then |
---|
435 | |
---|
436 | DO ig=1,ngrid |
---|
437 | z1(ig)=pcapcal(ig)*ptsrf(ig)+cpp*zfluxt(ig,1)*zct(ig,1)*zovExner(ig,1) & |
---|
438 | + pfluxsrf(ig)*ptimestep + zdplanck(ig)*ptsrf(ig) |
---|
439 | z2(ig) = pcapcal(ig)+zdplanck(ig)+cpp*zfluxt(ig,1)*(1.-zovExner(ig,1)*zdt(ig,1)) |
---|
440 | ztsrf(ig) = z1(ig) / z2(ig) |
---|
441 | pdtsrf(ig) = (ztsrf(ig) - ptsrf(ig))/ptimestep |
---|
442 | zt(ig,1) = zct(ig,1) + zdt(ig,1)*ztsrf(ig) |
---|
443 | ENDDO |
---|
444 | ! JL12 note that the black body radiative flux emitted by the surface has been updated by the implicit scheme |
---|
445 | |
---|
446 | |
---|
447 | ! Recalculate temperature to top of atmosphere, starting from ground |
---|
448 | ! ------------------------------------------------------------------ |
---|
449 | |
---|
450 | DO ilay=2,nlay |
---|
451 | DO ig=1,ngrid |
---|
452 | zt(ig,ilay)=zct(ig,ilay)+zdt(ig,ilay)*zt(ig,ilay-1) |
---|
453 | ENDDO |
---|
454 | ENDDO |
---|
455 | |
---|
456 | endif ! not water |
---|
457 | |
---|
458 | !----------------------------------------------------------------------- |
---|
459 | ! TRACERS (no vapour) |
---|
460 | ! ------- |
---|
461 | |
---|
462 | if(tracer) then |
---|
463 | |
---|
464 | ! Calculate vertical flux from the bottom to the first layer (dust) |
---|
465 | ! ----------------------------------------------------------------- |
---|
466 | do ig=1,ngrid |
---|
467 | rho(ig) = zb0(ig,1) /ptimestep |
---|
468 | end do |
---|
469 | |
---|
470 | pdqsdif(:,:)=0. |
---|
471 | |
---|
472 | ! Implicit inversion of q |
---|
473 | ! ----------------------- |
---|
474 | do iq=1,nq |
---|
475 | |
---|
476 | if (iq.ne.ivap) then |
---|
477 | |
---|
478 | DO ig=1,ngrid |
---|
479 | z1(ig)=1./(zmass(ig,nlay)+zfluxq(ig,nlay)) |
---|
480 | zcq(ig,nlay)=zmass(ig,nlay)*zq(ig,nlay,iq)*z1(ig) |
---|
481 | zdq(ig,nlay)=zfluxq(ig,nlay)*z1(ig) |
---|
482 | ENDDO |
---|
483 | |
---|
484 | DO ilay=nlay-1,2,-1 |
---|
485 | DO ig=1,ngrid |
---|
486 | z1(ig)=1./(zmass(ig,ilay)+zfluxq(ig,ilay)+zfluxq(ig,ilay+1)*(1.-zdq(ig,ilay+1))) |
---|
487 | zcq(ig,ilay)=(zmass(ig,ilay)*zq(ig,ilay,iq)+zfluxq(ig,ilay+1)*zcq(ig,ilay+1))*z1(ig) |
---|
488 | zdq(ig,ilay)=zfluxq(ig,ilay)*z1(ig) |
---|
489 | ENDDO |
---|
490 | ENDDO |
---|
491 | |
---|
492 | if ((water).and.(iq.eq.iliq)) then |
---|
493 | ! special case for condensed water tracer: do not include |
---|
494 | ! h2o ice tracer from surface (which is set when handling |
---|
495 | ! h2o vapour case (see further down). |
---|
496 | ! zb(ig,1)=0 if iq ne ivap |
---|
497 | DO ig=1,ngrid |
---|
498 | z1(ig)=1./(zmass(ig,1)+zfluxq(ig,2)*(1.-zdq(ig,2))) |
---|
499 | zcq(ig,1)=(zmass(ig,1)*zq(ig,1,iq)+zfluxq(ig,2)*zcq(ig,2))*z1(ig) |
---|
500 | ENDDO |
---|
501 | else ! general case |
---|
502 | do ig=1,ngrid |
---|
503 | z1(ig)=1./(zmass(ig,1)+zfluxq(ig,2)*(1.-zdq(ig,2))) |
---|
504 | zcq(ig,1)=(zmass(ig,1)*zq(ig,1,iq)+zfluxq(ig,2)*zcq(ig,2)+(-pdqsdif(ig,iq))*ptimestep)*z1(ig) |
---|
505 | ! tracer flux from surface |
---|
506 | ! currently pdqsdif always zero here, |
---|
507 | ! so last line is superfluous |
---|
508 | enddo |
---|
509 | endif ! of if (water.and.(iq.eq.igcm_h2o_ice)) |
---|
510 | |
---|
511 | |
---|
512 | ! Starting upward calculations for simple tracer mixing (e.g., dust) |
---|
513 | do ig=1,ngrid |
---|
514 | zq(ig,1,iq)=zcq(ig,1) |
---|
515 | end do |
---|
516 | |
---|
517 | do ilay=2,nlay |
---|
518 | do ig=1,ngrid |
---|
519 | zq(ig,ilay,iq)=zcq(ig,ilay)+zdq(ig,ilay)*zq(ig,ilay-1,iq) |
---|
520 | end do |
---|
521 | end do |
---|
522 | |
---|
523 | endif ! if (iq.ne.ivap) |
---|
524 | |
---|
525 | ! Calculate temperature tendency including latent heat term |
---|
526 | ! and assuming an infinite source of water on the ground |
---|
527 | ! ------------------------------------------------------------------ |
---|
528 | |
---|
529 | if (water.and.(iq.eq.ivap)) then |
---|
530 | |
---|
531 | ! compute evaporation efficiency |
---|
532 | do ig=1,ngrid |
---|
533 | if(nint(rnat(ig)).eq.1)then |
---|
534 | dryness(ig)=pqsurf(ig,iliq_surf)+pqsurf(ig,iice_surf) |
---|
535 | dryness(ig)=MIN(1.,2*dryness(ig)/mx_eau_sol) |
---|
536 | dryness(ig)=MAX(0.,dryness(ig)) |
---|
537 | endif |
---|
538 | enddo |
---|
539 | |
---|
540 | do ig=1,ngrid |
---|
541 | ! Calculate the value of qsat at the surface (water) |
---|
542 | call Psat_water(ptsrf(ig),pplev(ig,1),psat(ig),qsat(ig)) |
---|
543 | call Lcpdqsat_water(ptsrf(ig),pplev(ig,1),psat(ig),qsat(ig),dqsat(ig),psat_temp) |
---|
544 | dqsat(ig)=dqsat(ig)*RCPD/RLVTT |
---|
545 | enddo |
---|
546 | |
---|
547 | ! coefficients for q |
---|
548 | |
---|
549 | do ig=1,ngrid |
---|
550 | z1(ig)=1./(zmass(ig,nlay)+zfluxq(ig,nlay)) |
---|
551 | zcq(ig,nlay)=zmass(ig,nlay)*zq(ig,nlay,iq)*z1(ig) |
---|
552 | zdq(ig,nlay)=zfluxq(ig,nlay)*z1(ig) |
---|
553 | enddo |
---|
554 | |
---|
555 | do ilay=nlay-1,2,-1 |
---|
556 | do ig=1,ngrid |
---|
557 | z1(ig)=1./(zmass(ig,ilay)+zfluxq(ig,ilay)+zfluxq(ig,ilay+1)*(1.-zdq(ig,ilay+1))) |
---|
558 | zcq(ig,ilay)=(zmass(ig,ilay)*zq(ig,ilay,iq)+zfluxq(ig,ilay+1)*zcq(ig,ilay+1))*z1(ig) |
---|
559 | zdq(ig,ilay)=zfluxq(ig,ilay)*z1(ig) |
---|
560 | enddo |
---|
561 | enddo |
---|
562 | |
---|
563 | do ig=1,ngrid |
---|
564 | z1(ig)=1./(zmass(ig,1)+zfluxq(ig,1)*dryness(ig)+zfluxq(ig,2)*(1.-zdq(ig,2))) |
---|
565 | zcq(ig,1)=(zmass(ig,1)*zq(ig,1,iq)+zfluxq(ig,2)*zcq(ig,2))*z1(ig) |
---|
566 | zdq(ig,1)=dryness(ig)*zfluxq(ig,1)*z1(ig) |
---|
567 | enddo |
---|
568 | |
---|
569 | do ig=1,ngrid |
---|
570 | !calculation of surface temperature |
---|
571 | zdq0(ig) = dqsat(ig) |
---|
572 | zcq0(ig) = qsat(ig)-dqsat(ig)*ptsrf(ig) |
---|
573 | |
---|
574 | z1(ig) = pcapcal(ig)*ptsrf(ig) +cpp*zfluxt(ig,1)*zct(ig,1)*zovExner(ig,1) & |
---|
575 | + zdplanck(ig)*ptsrf(ig) + pfluxsrf(ig)*ptimestep & |
---|
576 | + zfluxq(ig,1)*dryness(ig)*RLVTT*((zdq(ig,1)-1.0)*zcq0(ig)+zcq(ig,1)) |
---|
577 | |
---|
578 | z2(ig) = pcapcal(ig) + cpp*zfluxt(ig,1)*(1.-zovExner(ig,1)*zdt(ig,1)) & |
---|
579 | + zdplanck(ig)+zfluxq(ig,1)*dryness(ig)*RLVTT*zdq0(ig)*(1.0-zdq(ig,1)) |
---|
580 | |
---|
581 | ztsrf(ig) = z1(ig) / z2(ig) |
---|
582 | |
---|
583 | ! calculation of qs and q1 |
---|
584 | zq0(ig) = zcq0(ig)+zdq0(ig)*ztsrf(ig) |
---|
585 | zq(ig,1,iq) = zcq(ig,1)+zdq(ig,1)*zq0(ig) |
---|
586 | |
---|
587 | ! calculation of evaporation |
---|
588 | dqsdif_total(ig)=zfluxq(ig,1)*dryness(ig)*(zq(ig,1,ivap)-zq0(ig)) |
---|
589 | |
---|
590 | ! -------------------------------------------------------- |
---|
591 | ! Now check if we've taken too much water from the surface |
---|
592 | ! This can only occur on the continent |
---|
593 | ! If we do, we recompute Tsurf, T1 and q1 accordingly |
---|
594 | if((-dqsdif_total(ig).gt.(pqsurf(ig,iice_surf)+pqsurf(ig,iliq_surf))).and.rnat(ig).eq.1)then |
---|
595 | !water flux * ptimestep |
---|
596 | dqsdif_total(ig)=-(pqsurf(ig,iice_surf)+pqsurf(ig,iliq_surf)) |
---|
597 | |
---|
598 | !recompute surface temperature |
---|
599 | z1(ig) = pcapcal(ig)*ptsrf(ig) +cpp*zfluxq(ig,1)*zct(ig,1)*zovExner(ig,1) & |
---|
600 | + zdplanck(ig)*ptsrf(ig) + pfluxsrf(ig)*ptimestep & |
---|
601 | + RLVTT*dqsdif_total(ig) |
---|
602 | z2(ig) = pcapcal(ig) + cpp*zfluxq(ig,1)*(1.-zovExner(ig,1)*zdt(ig,1)) & |
---|
603 | + zdplanck(ig) |
---|
604 | ztsrf(ig) = z1(ig) / z2(ig) |
---|
605 | |
---|
606 | !recompute q1 with new water flux from surface |
---|
607 | zq(ig,1,iq) = (zmass(ig,1)*(pq(ig,1,iq)+ptimestep*pdqfi(ig,1,iq)) & |
---|
608 | +zfluxq(ig,2)*zcq(ig,2)-dqsdif_total(ig)) & |
---|
609 | / (zmass(ig,1)+(1.-zdq(ig,2))*zfluxq(ig,2)) |
---|
610 | end if |
---|
611 | |
---|
612 | ! calculation surface T tendency and T(1) |
---|
613 | pdtsrf(ig) = (ztsrf(ig) - ptsrf(ig))/ptimestep |
---|
614 | zt(ig,1) = zct(ig,1) + zdt(ig,1)*ztsrf(ig) |
---|
615 | enddo |
---|
616 | |
---|
617 | |
---|
618 | ! recalculate temperature and q(vap) to top of atmosphere, starting from ground |
---|
619 | do ilay=2,nlay |
---|
620 | do ig=1,ngrid |
---|
621 | zq(ig,ilay,iq)=zcq(ig,ilay)+zdq(ig,ilay)*zq(ig,ilay-1,iq) |
---|
622 | zt(ig,ilay)=zct(ig,ilay)+zdt(ig,ilay)*zt(ig,ilay-1) |
---|
623 | end do |
---|
624 | end do |
---|
625 | |
---|
626 | |
---|
627 | do ig=1,ngrid |
---|
628 | ! -------------------------------------------------------------------------- |
---|
629 | ! On the ocean, if T > 0 C then the vapour tendency must replace the ice one |
---|
630 | ! The surface vapour tracer is actually liquid. To make things difficult. |
---|
631 | |
---|
632 | if (nint(rnat(ig)).eq.0) then ! unfrozen ocean |
---|
633 | |
---|
634 | pdqsdif(ig,iliq_surf)=dqsdif_total(ig)/ptimestep |
---|
635 | pdqsdif(ig,iice_surf)=0.0 |
---|
636 | |
---|
637 | elseif (nint(rnat(ig)).eq.1) then ! (continent) |
---|
638 | ! If water is evaporating / subliming, we take it from ice before liquid |
---|
639 | ! -- is this valid?? |
---|
640 | if(dqsdif_total(ig).lt.0)then |
---|
641 | if (-dqsdif_total(ig).gt.pqsurf(ig,iice_surf))then |
---|
642 | pdqsdif(ig,iice_surf) = -pqsurf(ig,iice_surf)/ptimestep ! removes all the ice! |
---|
643 | pdqsdif(ig,iliq_surf) = dqsdif_total(ig)/ptimestep- pdqsdif(ig,iice_surf) ! take the remainder from the liquid instead |
---|
644 | else |
---|
645 | pdqsdif(ig,iice_surf)=dqsdif_total(ig)/ptimestep |
---|
646 | pdqsdif(ig,iliq_surf)=0. |
---|
647 | end if |
---|
648 | else !dqsdif_total(ig).ge.0 |
---|
649 | !If water vapour is condensing, we must decide whether it forms ice or liquid. |
---|
650 | if(ztsrf(ig).gt.T_h2O_ice_liq)then |
---|
651 | pdqsdif(ig,iice_surf)=0.0 |
---|
652 | pdqsdif(ig,iliq_surf)=dqsdif_total(ig)/ptimestep |
---|
653 | else |
---|
654 | pdqsdif(ig,iice_surf)=dqsdif_total(ig)/ptimestep |
---|
655 | pdqsdif(ig,iliq_surf)=0.0 |
---|
656 | endif |
---|
657 | endif |
---|
658 | |
---|
659 | elseif (nint(rnat(ig)).eq.2) then ! (continental glaciers) |
---|
660 | pdqsdif(ig,iliq_surf)=0.0 |
---|
661 | pdqsdif(ig,iice_surf)=dqsdif_total(ig)/ptimestep |
---|
662 | |
---|
663 | endif !rnat |
---|
664 | end do ! of DO ig=1,ngrid |
---|
665 | |
---|
666 | endif ! if (water et iq=ivap) |
---|
667 | end do ! of do iq=1,nq |
---|
668 | |
---|
669 | if (water) then ! special case where we recompute water mixing without any evaporation. |
---|
670 | ! The difference with the first calculation then tells us where evaporated water has gone |
---|
671 | |
---|
672 | DO ig=1,ngrid |
---|
673 | z1(ig)=1./(zmass(ig,nlay)+zfluxq(ig,nlay)) |
---|
674 | zcq(ig,nlay)=zmass(ig,nlay)*zqnoevap(ig,nlay)*z1(ig) |
---|
675 | zdq(ig,nlay)=zfluxq(ig,nlay)*z1(ig) |
---|
676 | ENDDO |
---|
677 | |
---|
678 | DO ilay=nlay-1,2,-1 |
---|
679 | DO ig=1,ngrid |
---|
680 | z1(ig)=1./(zmass(ig,ilay)+zfluxq(ig,ilay)+zfluxq(ig,ilay+1)*(1.-zdq(ig,ilay+1))) |
---|
681 | zcq(ig,ilay)=(zmass(ig,ilay)*zqnoevap(ig,ilay)+zfluxq(ig,ilay+1)*zcq(ig,ilay+1))*z1(ig) |
---|
682 | zdq(ig,ilay)=zfluxq(ig,ilay)*z1(ig) |
---|
683 | ENDDO |
---|
684 | ENDDO |
---|
685 | |
---|
686 | do ig=1,ngrid |
---|
687 | z1(ig)=1./(zmass(ig,1)+zfluxq(ig,2)*(1.-zdq(ig,2))) |
---|
688 | zcq(ig,1)=(zmass(ig,1)*zqnoevap(ig,1)+zfluxq(ig,2)*zcq(ig,2))*z1(ig) |
---|
689 | enddo |
---|
690 | |
---|
691 | ! Starting upward calculations for simple tracer mixing (e.g., dust) |
---|
692 | do ig=1,ngrid |
---|
693 | zqnoevap(ig,1)=zcq(ig,1) |
---|
694 | end do |
---|
695 | |
---|
696 | do ilay=2,nlay |
---|
697 | do ig=1,ngrid |
---|
698 | zqnoevap(ig,ilay)=zcq(ig,ilay)+zdq(ig,ilay)*zqnoevap(ig,ilay-1) |
---|
699 | end do |
---|
700 | end do |
---|
701 | |
---|
702 | endif ! if water |
---|
703 | |
---|
704 | |
---|
705 | endif ! tracer |
---|
706 | |
---|
707 | |
---|
708 | !----------------------------------------------------------------------- |
---|
709 | ! 8. Final calculation of the vertical diffusion tendencies |
---|
710 | ! ----------------------------------------------------------------- |
---|
711 | |
---|
712 | do ilev = 1, nlay |
---|
713 | do ig=1,ngrid |
---|
714 | pdudif(ig,ilev)=(zu(ig,ilev)-(pu(ig,ilev)))/ptimestep |
---|
715 | pdvdif(ig,ilev)=(zv(ig,ilev)-(pv(ig,ilev)))/ptimestep |
---|
716 | pdtdif(ig,ilev)=( zt(ig,ilev)- pt(ig,ilev))/ptimestep-pdtfi(ig,ilev) |
---|
717 | enddo |
---|
718 | enddo |
---|
719 | |
---|
720 | DO ig=1,ngrid ! computing sensible heat flux (atm => surface) |
---|
721 | sensibFlux(ig)=cpp*zfluxt(ig,1)/ptimestep*(zt(ig,1)*zovExner(ig,1)-ztsrf(ig)) |
---|
722 | ENDDO |
---|
723 | |
---|
724 | if (tracer) then |
---|
725 | do iq = 1, nq |
---|
726 | do ilev = 1, nlay |
---|
727 | do ig=1,ngrid |
---|
728 | pdqdif(ig,ilev,iq)=(zq(ig,ilev,iq)-(pq(ig,ilev,iq)+pdqfi(ig,ilev,iq)*ptimestep))/ptimestep |
---|
729 | enddo |
---|
730 | enddo |
---|
731 | enddo |
---|
732 | if (water) then |
---|
733 | do ilev = 1, nlay |
---|
734 | do ig=1,ngrid |
---|
735 | pdqevap(ig,ilev)=(zq(ig,ilev,ivap)-zqnoevap(ig,ilev))/ptimestep |
---|
736 | enddo |
---|
737 | enddo |
---|
738 | do ig=1,ngrid |
---|
739 | zdmassevap(ig)=SUM(pdqevap(ig,:)*zmass(ig,:))*ptimestep |
---|
740 | end do |
---|
741 | endif |
---|
742 | endif |
---|
743 | |
---|
744 | if(water)then |
---|
745 | #ifndef MESOSCALE |
---|
746 | call writediagfi(ngrid,'beta','Dryness coefficient',' ',2,dryness) |
---|
747 | #endif |
---|
748 | if (tracer) then |
---|
749 | #ifndef MESOSCALE |
---|
750 | call writediagfi(ngrid,'evap_surf_flux','surface latent heat flux','W.m-2',2,RLVTT*dqsdif_total/ptimestep) |
---|
751 | call writediagfi(ngrid,'fluxsurf_rad','total IR and VIS surface flux','W.m-2',2,pfluxsrf) |
---|
752 | call writediagfi(ngrid,'dqevap','evaporated water vapor specific concentration','s-1',3,pdqevap) |
---|
753 | #else |
---|
754 | comm_LATENT_HF(:)=0.0 |
---|
755 | comm_LATENT_HF(1:ngrid)=RLVTT*dqsdif_total(1:ngrid)/ptimestep |
---|
756 | #endif |
---|
757 | endif |
---|
758 | endif |
---|
759 | |
---|
760 | end subroutine turbdiff |
---|
761 | |
---|
762 | end module turbdiff_mod |
---|