1 | subroutine vdifc(ngrid,nlay,nq,rnat,ppopsk, |
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2 | & ptimestep,pcapcal,lecrit, |
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3 | & pplay,pplev,pzlay,pzlev,pz0, |
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4 | & pu,pv,ph,pq,ptsrf,pemis,pqsurf, |
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5 | & pdufi,pdvfi,pdhfi,pdqfi,pfluxsrf, |
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6 | & pdudif,pdvdif,pdhdif,pdtsrf,pq2, |
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7 | & pdqdif,pdqsdif,lastcall) |
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8 | |
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9 | use watercommon_h, only : RLVTT, To, RCPD, mx_eau_sol |
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10 | |
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11 | implicit none |
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12 | |
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13 | !================================================================== |
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14 | ! |
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15 | ! Purpose |
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16 | ! ------- |
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17 | ! Turbulent diffusion (mixing) for pot. T, U, V and tracers |
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18 | ! |
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19 | ! Implicit scheme |
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20 | ! We start by adding to variables x the physical tendencies |
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21 | ! already computed. We resolve the equation: |
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22 | ! |
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23 | ! x(t+1) = x(t) + dt * (dx/dt)phys(t) + dt * (dx/dt)difv(t+1) |
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24 | ! |
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25 | ! Authors |
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26 | ! ------- |
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27 | ! F. Hourdin, F. Forget, R. Fournier (199X) |
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28 | ! R. Wordsworth, B. Charnay (2010) |
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29 | ! |
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30 | !================================================================== |
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31 | |
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32 | !----------------------------------------------------------------------- |
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33 | ! declarations |
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34 | ! ------------ |
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35 | |
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36 | #include "dimensions.h" |
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37 | #include "dimphys.h" |
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38 | #include "comcstfi.h" |
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39 | #include "callkeys.h" |
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40 | #include "surfdat.h" |
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41 | #include "comgeomfi.h" |
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42 | #include "tracer.h" |
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43 | |
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44 | #include "watercap.h" |
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45 | |
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46 | ! arguments |
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47 | ! --------- |
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48 | INTEGER ngrid,nlay |
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49 | REAL ptimestep |
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50 | REAL pplay(ngrid,nlay),pplev(ngrid,nlay+1) |
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51 | REAL pzlay(ngrid,nlay),pzlev(ngrid,nlay+1) |
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52 | REAL pu(ngrid,nlay),pv(ngrid,nlay),ph(ngrid,nlay) |
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53 | REAL ptsrf(ngrid),pemis(ngrid) |
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54 | REAL pdufi(ngrid,nlay),pdvfi(ngrid,nlay),pdhfi(ngrid,nlay) |
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55 | REAL pfluxsrf(ngrid) |
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56 | REAL pdudif(ngrid,nlay),pdvdif(ngrid,nlay),pdhdif(ngrid,nlay) |
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57 | REAL pdtsrf(ngrid),pcapcal(ngrid) |
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58 | REAL pq2(ngrid,nlay+1) |
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59 | |
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60 | integer rnat(ngrid) |
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61 | |
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62 | ! Arguments added for condensation |
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63 | REAL ppopsk(ngrid,nlay) |
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64 | logical lecrit |
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65 | REAL pz0 |
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66 | |
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67 | ! Tracers |
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68 | ! -------- |
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69 | integer nq |
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70 | real pqsurf(ngrid,nq) |
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71 | real pq(ngrid,nlay,nq), pdqfi(ngrid,nlay,nq) |
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72 | real pdqdif(ngrid,nlay,nq) |
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73 | real pdqsdif(ngrid,nq) |
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74 | |
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75 | ! local |
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76 | ! ----- |
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77 | integer ilev,ig,ilay,nlev |
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78 | |
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79 | REAL z4st,zdplanck(ngridmx) |
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80 | REAL zkv(ngridmx,nlayermx+1),zkh(ngridmx,nlayermx+1) |
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81 | REAL zcdv(ngridmx),zcdh(ngridmx) |
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82 | REAL zcdv_true(ngridmx),zcdh_true(ngridmx) |
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83 | REAL zu(ngridmx,nlayermx),zv(ngridmx,nlayermx) |
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84 | REAL zh(ngridmx,nlayermx) |
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85 | REAL ztsrf2(ngridmx) |
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86 | REAL z1(ngridmx),z2(ngridmx) |
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87 | REAL za(ngridmx,nlayermx),zb(ngridmx,nlayermx) |
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88 | REAL zb0(ngridmx,nlayermx) |
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89 | REAL zc(ngridmx,nlayermx),zd(ngridmx,nlayermx) |
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90 | REAL zcst1 |
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91 | REAL zu2!, a |
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92 | REAL zcq(ngridmx,nlayermx),zdq(ngridmx,nlayermx) |
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93 | REAL evap(ngridmx) |
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94 | REAL zcq0(ngridmx),zdq0(ngridmx) |
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95 | REAL zx_alf1(ngridmx),zx_alf2(ngridmx) |
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96 | |
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97 | LOGICAL firstcall |
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98 | SAVE firstcall |
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99 | |
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100 | LOGICAL lastcall |
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101 | |
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102 | ! variables added for CO2 condensation |
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103 | ! ------------------------------------ |
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104 | REAL hh !, zhcond(ngridmx,nlayermx) |
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105 | ! REAL latcond,tcond1mb |
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106 | ! REAL acond,bcond |
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107 | ! SAVE acond,bcond |
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108 | ! DATA latcond,tcond1mb/5.9e5,136.27/ |
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109 | |
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110 | ! Tracers |
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111 | ! ------- |
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112 | INTEGER iq |
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113 | REAL zq(ngridmx,nlayermx,nqmx) |
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114 | REAL zq1temp(ngridmx) |
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115 | REAL rho(ngridmx) ! near-surface air density |
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116 | REAL qsat(ngridmx) |
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117 | DATA firstcall/.true./ |
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118 | REAL kmixmin |
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119 | |
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120 | ! Variables added for implicit latent heat inclusion |
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121 | ! -------------------------------------------------- |
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122 | real latconst, dqsat(ngridmx), qsat_temp1, qsat_temp2 |
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123 | real z1_Tdry(ngridmx), z2_Tdry(ngridmx) |
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124 | real z1_T(ngridmx), z2_T(ngridmx) |
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125 | real zb_T(ngridmx) |
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126 | real zc_T(ngridmx,nlayermx) |
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127 | real zd_T(ngridmx,nlayermx) |
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128 | real lat1(ngridmx), lat2(ngridmx) |
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129 | real surfh2otot |
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130 | logical surffluxdiag |
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131 | integer isub ! sub-loop for precision |
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132 | |
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133 | integer ivap, iice ! also make liq for clarity on surface... |
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134 | save ivap, iice |
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135 | |
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136 | real, parameter :: sigma=5.67e-8 |
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137 | real, parameter :: karman=0.4 |
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138 | real cd0, roughratio |
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139 | |
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140 | logical forceWC |
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141 | real masse, Wtot, Wdiff |
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142 | |
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143 | real dqsdif_total(ngrid) |
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144 | real zq0(ngrid) |
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145 | |
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146 | forceWC=.true. |
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147 | ! forceWC=.false. |
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148 | |
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149 | |
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150 | ! Coherence test |
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151 | ! -------------- |
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152 | |
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153 | IF (firstcall) THEN |
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154 | ! IF(ngrid.NE.ngridmx) THEN |
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155 | ! PRINT*,'STOP dans vdifc' |
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156 | ! PRINT*,'probleme de dimensions :' |
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157 | ! PRINT*,'ngrid =',ngrid |
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158 | ! PRINT*,'ngridmx =',ngridmx |
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159 | ! STOP |
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160 | ! ENDIF |
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161 | ! To compute: Tcond= 1./(bcond-acond*log(.0095*p)) (p in pascal) |
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162 | ! bcond=1./tcond1mb |
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163 | ! acond=r/latcond |
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164 | ! PRINT*,'In vdifc: Tcond(P=1mb)=',tcond1mb,' Lcond=',latcond |
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165 | ! PRINT*,' acond,bcond',acond,bcond |
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166 | |
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167 | if(water)then |
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168 | ! iliq=igcm_h2o_vap |
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169 | ivap=igcm_h2o_vap |
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170 | iice=igcm_h2o_ice ! simply to make the code legible |
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171 | ! to be generalised later |
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172 | endif |
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173 | |
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174 | if(ngridmx.ne.1)then |
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175 | if(nonideal)then |
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176 | print*,'Nonideal doesnt work yet in 3D!!!' |
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177 | call abort |
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178 | endif |
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179 | endif |
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180 | |
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181 | firstcall=.false. |
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182 | ENDIF |
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183 | |
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184 | !----------------------------------------------------------------------- |
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185 | ! 1. Initialisation |
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186 | ! ----------------- |
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187 | |
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188 | nlev=nlay+1 |
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189 | |
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190 | ! Calculate rho*dz and dt*rho/dz=dt*rho**2 g/dp |
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191 | ! with rho=p/RT=p/ (R Theta) (p/ps)**kappa |
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192 | ! --------------------------------------------- |
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193 | |
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194 | DO ilay=1,nlay |
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195 | DO ig=1,ngrid |
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196 | za(ig,ilay)=(pplev(ig,ilay)-pplev(ig,ilay+1))/g |
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197 | ENDDO |
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198 | ENDDO |
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199 | |
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200 | zcst1=4.*g*ptimestep/(R*R) |
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201 | DO ilev=2,nlev-1 |
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202 | DO ig=1,ngrid |
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203 | zb0(ig,ilev)=pplev(ig,ilev)* |
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204 | s (pplev(ig,1)/pplev(ig,ilev))**rcp / |
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205 | s (ph(ig,ilev-1)+ph(ig,ilev)) |
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206 | zb0(ig,ilev)=zcst1*zb0(ig,ilev)*zb0(ig,ilev)/ |
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207 | s (pplay(ig,ilev-1)-pplay(ig,ilev)) |
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208 | ENDDO |
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209 | ENDDO |
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210 | DO ig=1,ngrid |
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211 | zb0(ig,1)=ptimestep*pplev(ig,1)/(R*ptsrf(ig)) |
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212 | ENDDO |
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213 | |
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214 | dqsdif_total(:)=0.0 |
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215 | |
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216 | !----------------------------------------------------------------------- |
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217 | ! 2. Add the physical tendencies computed so far |
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218 | ! ---------------------------------------------- |
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219 | |
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220 | DO ilev=1,nlay |
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221 | DO ig=1,ngrid |
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222 | zu(ig,ilev)=pu(ig,ilev)+pdufi(ig,ilev)*ptimestep |
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223 | zv(ig,ilev)=pv(ig,ilev)+pdvfi(ig,ilev)*ptimestep |
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224 | zh(ig,ilev)=ph(ig,ilev)+pdhfi(ig,ilev)*ptimestep |
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225 | ENDDO |
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226 | ENDDO |
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227 | if(tracer) then |
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228 | DO iq =1, nq |
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229 | DO ilev=1,nlay |
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230 | DO ig=1,ngrid |
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231 | zq(ig,ilev,iq)=pq(ig,ilev,iq) + |
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232 | & pdqfi(ig,ilev,iq)*ptimestep |
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233 | ENDDO |
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234 | ENDDO |
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235 | ENDDO |
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236 | end if |
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237 | |
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238 | !----------------------------------------------------------------------- |
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239 | ! 3. Turbulence scheme |
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240 | ! -------------------- |
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241 | ! |
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242 | ! Source of turbulent kinetic energy at the surface |
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243 | ! ------------------------------------------------- |
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244 | ! Formula is Cd_0 = (karman / log[1+z1/z0])^2 |
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245 | |
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246 | DO ig=1,ngrid |
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247 | roughratio = 1.E+0 + pzlay(ig,1)/pz0 |
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248 | cd0 = karman/log(roughratio) |
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249 | cd0 = cd0*cd0 |
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250 | zcdv_true(ig) = cd0 |
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251 | zcdh_true(ig) = cd0 |
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252 | ENDDO |
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253 | |
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254 | DO ig=1,ngrid |
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255 | zu2=pu(ig,1)*pu(ig,1)+pv(ig,1)*pv(ig,1) |
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256 | zcdv(ig)=zcdv_true(ig)*sqrt(zu2) |
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257 | zcdh(ig)=zcdh_true(ig)*sqrt(zu2) |
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258 | ENDDO |
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259 | |
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260 | ! Turbulent diffusion coefficients in the boundary layer |
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261 | ! ------------------------------------------------------ |
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262 | |
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263 | call vdif_kc(ptimestep,g,pzlev,pzlay |
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264 | & ,pu,pv,ph,zcdv_true |
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265 | & ,pq2,zkv,zkh) |
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266 | |
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267 | ! Adding eddy mixing to mimic 3D general circulation in 1D |
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268 | ! R. Wordsworth & F. Forget (2010) |
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269 | if ((ngrid.eq.1)) then |
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270 | kmixmin = 1.0e-2 ! minimum eddy mix coeff in 1D |
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271 | do ilev=1,nlay |
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272 | do ig=1,ngrid |
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273 | !zkh(ig,ilev) = 1.0 |
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274 | zkh(ig,ilev) = max(kmixmin,zkh(ig,ilev)) |
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275 | zkv(ig,ilev) = max(kmixmin,zkv(ig,ilev)) |
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276 | end do |
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277 | end do |
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278 | end if |
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279 | |
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280 | !----------------------------------------------------------------------- |
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281 | ! 4. Implicit inversion of u |
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282 | ! -------------------------- |
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283 | |
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284 | ! u(t+1) = u(t) + dt * {(du/dt)phys}(t) + dt * {(du/dt)difv}(t+1) |
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285 | ! avec |
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286 | ! /zu/ = u(t) + dt * {(du/dt)phys}(t) (voir paragraphe 2.) |
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287 | ! et |
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288 | ! dt * {(du/dt)difv}(t+1) = dt * {(d/dz)[ Ku (du/dz) ]}(t+1) |
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289 | ! donc les entrees sont /zcdv/ pour la condition a la limite sol |
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290 | ! et /zkv/ = Ku |
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291 | |
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292 | CALL multipl((nlay-1)*ngrid,zkv(1,2),zb0(1,2),zb(1,2)) |
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293 | CALL multipl(ngrid,zcdv,zb0,zb) |
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294 | |
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295 | DO ig=1,ngrid |
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296 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
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297 | zc(ig,nlay)=za(ig,nlay)*zu(ig,nlay)*z1(ig) |
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298 | zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
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299 | ENDDO |
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300 | |
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301 | DO ilay=nlay-1,1,-1 |
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302 | DO ig=1,ngrid |
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303 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
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304 | $ zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
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305 | zc(ig,ilay)=(za(ig,ilay)*zu(ig,ilay)+ |
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306 | $ zb(ig,ilay+1)*zc(ig,ilay+1))*z1(ig) |
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307 | zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
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308 | ENDDO |
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309 | ENDDO |
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310 | |
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311 | DO ig=1,ngrid |
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312 | zu(ig,1)=zc(ig,1) |
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313 | ENDDO |
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314 | DO ilay=2,nlay |
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315 | DO ig=1,ngrid |
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316 | zu(ig,ilay)=zc(ig,ilay)+zd(ig,ilay)*zu(ig,ilay-1) |
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317 | ENDDO |
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318 | ENDDO |
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319 | |
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320 | !----------------------------------------------------------------------- |
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321 | ! 5. Implicit inversion of v |
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322 | ! -------------------------- |
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323 | |
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324 | ! v(t+1) = v(t) + dt * {(dv/dt)phys}(t) + dt * {(dv/dt)difv}(t+1) |
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325 | ! avec |
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326 | ! /zv/ = v(t) + dt * {(dv/dt)phys}(t) (voir paragraphe 2.) |
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327 | ! et |
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328 | ! dt * {(dv/dt)difv}(t+1) = dt * {(d/dz)[ Kv (dv/dz) ]}(t+1) |
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329 | ! donc les entrees sont /zcdv/ pour la condition a la limite sol |
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330 | ! et /zkv/ = Kv |
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331 | |
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332 | DO ig=1,ngrid |
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333 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
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334 | zc(ig,nlay)=za(ig,nlay)*zv(ig,nlay)*z1(ig) |
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335 | zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
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336 | ENDDO |
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337 | |
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338 | DO ilay=nlay-1,1,-1 |
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339 | DO ig=1,ngrid |
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340 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
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341 | $ zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
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342 | zc(ig,ilay)=(za(ig,ilay)*zv(ig,ilay)+ |
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343 | $ zb(ig,ilay+1)*zc(ig,ilay+1))*z1(ig) |
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344 | zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
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345 | ENDDO |
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346 | ENDDO |
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347 | |
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348 | DO ig=1,ngrid |
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349 | zv(ig,1)=zc(ig,1) |
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350 | ENDDO |
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351 | DO ilay=2,nlay |
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352 | DO ig=1,ngrid |
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353 | zv(ig,ilay)=zc(ig,ilay)+zd(ig,ilay)*zv(ig,ilay-1) |
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354 | ENDDO |
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355 | ENDDO |
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356 | |
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357 | !---------------------------------------------------------------------------- |
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358 | ! 6. Implicit inversion of h, not forgetting the coupling with the ground |
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359 | |
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360 | ! h(t+1) = h(t) + dt * {(dh/dt)phys}(t) + dt * {(dh/dt)difv}(t+1) |
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361 | ! avec |
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362 | ! /zh/ = h(t) + dt * {(dh/dt)phys}(t) (voir paragraphe 2.) |
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363 | ! et |
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364 | ! dt * {(dh/dt)difv}(t+1) = dt * {(d/dz)[ Kh (dh/dz) ]}(t+1) |
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365 | ! donc les entrees sont /zcdh/ pour la condition de raccord au sol |
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366 | ! et /zkh/ = Kh |
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367 | |
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368 | ! Using the wind modified by friction for lifting and sublimation |
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369 | ! --------------------------------------------------------------- |
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370 | DO ig=1,ngrid |
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371 | zu2 = zu(ig,1)*zu(ig,1)+zv(ig,1)*zv(ig,1) |
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372 | zcdv(ig) = zcdv_true(ig)*sqrt(zu2) |
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373 | zcdh(ig) = zcdh_true(ig)*sqrt(zu2) |
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374 | ENDDO |
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375 | |
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376 | CALL multipl((nlay-1)*ngrid,zkh(1,2),zb0(1,2),zb(1,2)) |
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377 | CALL multipl(ngrid,zcdh,zb0,zb) |
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378 | |
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379 | DO ig=1,ngrid |
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380 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
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381 | zc(ig,nlay)=za(ig,nlay)*zh(ig,nlay)*z1(ig) |
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382 | zd(ig,nlay)=zb(ig,nlay)*z1(ig) |
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383 | ENDDO |
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384 | |
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385 | DO ilay=nlay-1,2,-1 |
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386 | DO ig=1,ngrid |
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387 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
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388 | & zb(ig,ilay+1)*(1.-zd(ig,ilay+1))) |
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389 | zc(ig,ilay)=(za(ig,ilay)*zh(ig,ilay)+ |
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390 | & zb(ig,ilay+1)*zc(ig,ilay+1))*z1(ig) |
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391 | zd(ig,ilay)=zb(ig,ilay)*z1(ig) |
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392 | ENDDO |
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393 | ENDDO |
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394 | |
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395 | DO ig=1,ngrid |
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396 | z1(ig)=1./(za(ig,1)+zb(ig,1)+ |
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397 | & zb(ig,2)*(1.-zd(ig,2))) |
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398 | zc(ig,1)=(za(ig,1)*zh(ig,1)+ |
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399 | & zb(ig,2)*zc(ig,2))*z1(ig) |
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400 | zd(ig,1)=zb(ig,1)*z1(ig) |
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401 | ENDDO |
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402 | |
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403 | ! Calculate (d Planck / dT) at the interface temperature |
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404 | ! ------------------------------------------------------ |
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405 | |
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406 | z4st=4.0*sigma*ptimestep |
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407 | DO ig=1,ngrid |
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408 | zdplanck(ig)=z4st*pemis(ig)*ptsrf(ig)*ptsrf(ig)*ptsrf(ig) |
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409 | ENDDO |
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410 | |
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411 | ! Calculate temperature tendency at the interface (dry case) |
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412 | ! ---------------------------------------------------------- |
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413 | ! Sum of fluxes at interface at time t + \delta t gives change in T: |
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414 | ! radiative fluxes |
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415 | ! turbulent convective (sensible) heat flux |
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416 | ! flux (if any) from subsurface |
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417 | |
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418 | if(.not.water) then |
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419 | |
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420 | DO ig=1,ngrid |
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421 | |
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422 | z1(ig) = pcapcal(ig)*ptsrf(ig) + cpp*zb(ig,1)*zc(ig,1) |
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423 | & + zdplanck(ig)*ptsrf(ig) + pfluxsrf(ig)*ptimestep |
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424 | z2(ig) = pcapcal(ig) + cpp*zb(ig,1)*(1.-zd(ig,1)) |
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425 | & +zdplanck(ig) |
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426 | ztsrf2(ig) = z1(ig) / z2(ig) |
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427 | pdtsrf(ig) = (ztsrf2(ig) - ptsrf(ig))/ptimestep |
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428 | zh(ig,1) = zc(ig,1) + zd(ig,1)*ztsrf2(ig) |
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429 | ENDDO |
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430 | |
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431 | ! Recalculate temperature to top of atmosphere, starting from ground |
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432 | ! ------------------------------------------------------------------ |
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433 | |
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434 | DO ilay=2,nlay |
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435 | DO ig=1,ngrid |
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436 | hh = zh(ig,ilay-1) |
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437 | zh(ig,ilay)=zc(ig,ilay)+zd(ig,ilay)*hh |
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438 | ENDDO |
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439 | ENDDO |
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440 | |
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441 | endif ! not water |
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442 | |
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443 | !----------------------------------------------------------------------- |
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444 | ! TRACERS (no vapour) |
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445 | ! ------- |
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446 | |
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447 | if(tracer) then |
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448 | |
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449 | ! Calculate vertical flux from the bottom to the first layer (dust) |
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450 | ! ----------------------------------------------------------------- |
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451 | do ig=1,ngridmx |
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452 | rho(ig) = zb0(ig,1) /ptimestep |
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453 | end do |
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454 | |
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455 | call zerophys(ngrid*nq,pdqsdif) |
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456 | |
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457 | ! Implicit inversion of q |
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458 | ! ----------------------- |
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459 | do iq=1,nq |
---|
460 | |
---|
461 | if (iq.ne.igcm_h2o_vap) then |
---|
462 | |
---|
463 | DO ig=1,ngrid |
---|
464 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
---|
465 | zcq(ig,nlay)=za(ig,nlay)*zq(ig,nlay,iq)*z1(ig) |
---|
466 | zdq(ig,nlay)=zb(ig,nlay)*z1(ig) |
---|
467 | ENDDO |
---|
468 | |
---|
469 | DO ilay=nlay-1,2,-1 |
---|
470 | DO ig=1,ngrid |
---|
471 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
---|
472 | & zb(ig,ilay+1)*(1.-zdq(ig,ilay+1))) |
---|
473 | zcq(ig,ilay)=(za(ig,ilay)*zq(ig,ilay,iq)+ |
---|
474 | & zb(ig,ilay+1)*zcq(ig,ilay+1))*z1(ig) |
---|
475 | zdq(ig,ilay)=zb(ig,ilay)*z1(ig) |
---|
476 | ENDDO |
---|
477 | ENDDO |
---|
478 | |
---|
479 | if ((water).and.(iq.eq.iice)) then |
---|
480 | ! special case for water ice tracer: do not include |
---|
481 | ! h2o ice tracer from surface (which is set when handling |
---|
482 | ! h2o vapour case (see further down). |
---|
483 | ! zb(ig,1)=0 if iq ne ivap |
---|
484 | DO ig=1,ngrid |
---|
485 | z1(ig)=1./(za(ig,1)+ |
---|
486 | & zb(ig,2)*(1.-zdq(ig,2))) |
---|
487 | zcq(ig,1)=(za(ig,1)*zq(ig,1,iq)+ |
---|
488 | & zb(ig,2)*zcq(ig,2))*z1(ig) |
---|
489 | ENDDO |
---|
490 | else ! general case |
---|
491 | DO ig=1,ngrid |
---|
492 | z1(ig)=1./(za(ig,1)+ |
---|
493 | & zb(ig,2)*(1.-zdq(ig,2))) |
---|
494 | zcq(ig,1)=(za(ig,1)*zq(ig,1,iq)+ |
---|
495 | & zb(ig,2)*zcq(ig,2) |
---|
496 | & +(-pdqsdif(ig,iq))*ptimestep)*z1(ig) |
---|
497 | ! tracer flux from surface |
---|
498 | ! currently pdqsdif always zero here, |
---|
499 | ! so last line is superfluous |
---|
500 | enddo |
---|
501 | endif ! of if (water.and.(iq.eq.igcm_h2o_ice)) |
---|
502 | |
---|
503 | |
---|
504 | ! Starting upward calculations for simple tracer mixing (e.g., dust) |
---|
505 | do ig=1,ngrid |
---|
506 | zq(ig,1,iq)=zcq(ig,1) |
---|
507 | end do |
---|
508 | |
---|
509 | do ilay=2,nlay |
---|
510 | do ig=1,ngrid |
---|
511 | zq(ig,ilay,iq)=zcq(ig,ilay)+ |
---|
512 | $ zdq(ig,ilay)*zq(ig,ilay-1,iq) |
---|
513 | end do |
---|
514 | end do |
---|
515 | |
---|
516 | endif ! if (iq.ne.igcm_h2o_vap) |
---|
517 | |
---|
518 | ! Calculate temperature tendency including latent heat term |
---|
519 | ! and assuming an infinite source of water on the ground |
---|
520 | ! ------------------------------------------------------------------ |
---|
521 | |
---|
522 | if (water.and.(iq.eq.igcm_h2o_vap)) then |
---|
523 | |
---|
524 | ! compute evaporation efficiency |
---|
525 | do ig = 1, ngrid |
---|
526 | if(rnat(ig).eq.1)then |
---|
527 | dryness(ig)=pqsurf(ig,ivap)+pqsurf(ig,iice) |
---|
528 | dryness(ig)=MIN(1.,2*dryness(ig)/mx_eau_sol) |
---|
529 | dryness(ig)=MAX(0.,dryness(ig)) |
---|
530 | endif |
---|
531 | enddo |
---|
532 | |
---|
533 | do ig=1,ngrid |
---|
534 | |
---|
535 | ! Calculate the value of qsat at the surface (water) |
---|
536 | call watersat(ptsrf(ig),pplev(ig,1),qsat(ig)) |
---|
537 | call watersat(ptsrf(ig)-0.0001,pplev(ig,1),qsat_temp1) |
---|
538 | call watersat(ptsrf(ig)+0.0001,pplev(ig,1),qsat_temp2) |
---|
539 | dqsat(ig)=(qsat_temp2-qsat_temp1)/0.0002 |
---|
540 | ! calculate dQsat / dT by finite differences |
---|
541 | ! we cannot use the updated temperature value yet... |
---|
542 | |
---|
543 | enddo |
---|
544 | |
---|
545 | ! coefficients for q |
---|
546 | |
---|
547 | do ig=1,ngrid |
---|
548 | z1(ig)=1./(za(ig,nlay)+zb(ig,nlay)) |
---|
549 | zcq(ig,nlay)=za(ig,nlay)*zq(ig,nlay,iq)*z1(ig) |
---|
550 | zdq(ig,nlay)=zb(ig,nlay)*z1(ig) |
---|
551 | enddo |
---|
552 | |
---|
553 | do ilay=nlay-1,2,-1 |
---|
554 | do ig=1,ngrid |
---|
555 | z1(ig)=1./(za(ig,ilay)+zb(ig,ilay)+ |
---|
556 | $ zb(ig,ilay+1)*(1.-zdq(ig,ilay+1))) |
---|
557 | zcq(ig,ilay)=(za(ig,ilay)*zq(ig,ilay,iq)+ |
---|
558 | $ zb(ig,ilay+1)*zcq(ig,ilay+1))*z1(ig) |
---|
559 | zdq(ig,ilay)=zb(ig,ilay)*z1(ig) |
---|
560 | enddo |
---|
561 | enddo |
---|
562 | |
---|
563 | do ig=1,ngrid |
---|
564 | z1(ig)=1./(za(ig,1)+zb(ig,1)*dryness(ig)+ |
---|
565 | $ zb(ig,2)*(1.-zdq(ig,2))) |
---|
566 | zcq(ig,1)=(za(ig,1)*zq(ig,1,iq)+ |
---|
567 | $ zb(ig,2)*zcq(ig,2))*z1(ig) |
---|
568 | zdq(ig,1)=dryness(ig)*zb(ig,1)*z1(ig) |
---|
569 | enddo |
---|
570 | |
---|
571 | ! calculation of h0 and h1 |
---|
572 | do ig=1,ngrid |
---|
573 | zdq0(ig) = dqsat(ig) |
---|
574 | zcq0(ig) = qsat(ig)-dqsat(ig)*ptsrf(ig) |
---|
575 | |
---|
576 | z1(ig) = pcapcal(ig)*ptsrf(ig) +cpp*zb(ig,1)*zc(ig,1) |
---|
577 | & + zdplanck(ig)*ptsrf(ig) + pfluxsrf(ig)*ptimestep |
---|
578 | & + zb(ig,1)*dryness(ig)*RLVTT* |
---|
579 | & ((zdq(ig,1)-1.0)*zcq0(ig)+zcq(ig,1)) |
---|
580 | |
---|
581 | z2(ig) = pcapcal(ig) + cpp*zb(ig,1)*(1.-zd(ig,1)) |
---|
582 | & +zdplanck(ig) |
---|
583 | & +zb(ig,1)*dryness(ig)*RLVTT*zdq0(ig)* |
---|
584 | & (1.0-zdq(ig,1)) |
---|
585 | |
---|
586 | ztsrf2(ig) = z1(ig) / z2(ig) |
---|
587 | pdtsrf(ig) = (ztsrf2(ig) - ptsrf(ig))/ptimestep |
---|
588 | zh(ig,1) = zc(ig,1) + zd(ig,1)*ztsrf2(ig) |
---|
589 | enddo |
---|
590 | |
---|
591 | ! calculation of qs and q1 |
---|
592 | do ig=1,ngrid |
---|
593 | zq0(ig) = zcq0(ig)+zdq0(ig)*ztsrf2(ig) |
---|
594 | zq(ig,1,iq) = zcq(ig,1)+zdq(ig,1)*zq0(ig) |
---|
595 | enddo |
---|
596 | |
---|
597 | ! calculation of evaporation |
---|
598 | do ig=1,ngrid |
---|
599 | evap(ig)= zb(ig,1)*dryness(ig)*(zq(ig,1,ivap)-zq0(ig)) |
---|
600 | dqsdif_total(ig)=evap(ig) |
---|
601 | enddo |
---|
602 | |
---|
603 | ! recalculate temperature and q(vap) to top of atmosphere, starting from ground |
---|
604 | do ilay=2,nlay |
---|
605 | do ig=1,ngrid |
---|
606 | zq(ig,ilay,iq)=zcq(ig,ilay) |
---|
607 | & +zdq(ig,ilay)*zq(ig,ilay-1,iq) |
---|
608 | zh(ig,ilay)=zc(ig,ilay)+zd(ig,ilay)*zh(ig,ilay-1) |
---|
609 | end do |
---|
610 | end do |
---|
611 | |
---|
612 | do ig=1,ngrid |
---|
613 | |
---|
614 | ! -------------------------------------------------------------------------- |
---|
615 | ! On the ocean, if T > 0 C then the vapour tendency must replace the ice one |
---|
616 | ! The surface vapour tracer is actually liquid. To make things difficult. |
---|
617 | |
---|
618 | if (rnat(ig).eq.0) then ! unfrozen ocean |
---|
619 | |
---|
620 | pdqsdif(ig,ivap)=dqsdif_total(ig)/ptimestep |
---|
621 | pdqsdif(ig,iice)=0.0 |
---|
622 | |
---|
623 | |
---|
624 | elseif (rnat(ig).eq.1) then ! (continent) |
---|
625 | |
---|
626 | ! -------------------------------------------------------- |
---|
627 | ! Now check if we've taken too much water from the surface |
---|
628 | ! This can only occur on the continent |
---|
629 | |
---|
630 | ! If water is evaporating / subliming, we take it from ice before liquid |
---|
631 | ! -- is this valid?? |
---|
632 | if(dqsdif_total(ig).lt.0)then |
---|
633 | pdqsdif(ig,iice)=dqsdif_total(ig)/ptimestep |
---|
634 | pdqsdif(ig,iice)=max(-pqsurf(ig,iice)/ptimestep |
---|
635 | & ,pdqsdif(ig,iice)) |
---|
636 | endif |
---|
637 | ! sublimation only greater than qsurf(ice) |
---|
638 | ! ---------------------------------------- |
---|
639 | ! we just convert some liquid to vapour too |
---|
640 | ! if latent heats are the same, no big deal |
---|
641 | if (-dqsdif_total(ig).gt.pqsurf(ig,iice))then |
---|
642 | pdqsdif(ig,iice) = -pqsurf(ig,iice)/ptimestep ! removes all the ice! |
---|
643 | pdqsdif(ig,ivap) = dqsdif_total(ig)/ptimestep |
---|
644 | & - pdqsdif(ig,iice) ! take the remainder from the liquid instead |
---|
645 | pdqsdif(ig,ivap) = max(-pqsurf(ig,ivap)/ptimestep |
---|
646 | & ,pdqsdif(ig,ivap)) |
---|
647 | endif |
---|
648 | |
---|
649 | endif ! if (rnat.ne.1) |
---|
650 | |
---|
651 | ! If water vapour is condensing, we must decide whether it forms ice or liquid. |
---|
652 | if(dqsdif_total(ig).gt.0)then ! a bug was here! |
---|
653 | if(ztsrf2(ig).gt.To)then |
---|
654 | pdqsdif(ig,iice)=0.0 |
---|
655 | pdqsdif(ig,ivap)=dqsdif_total(ig)/ptimestep |
---|
656 | else |
---|
657 | pdqsdif(ig,iice)=dqsdif_total(ig)/ptimestep |
---|
658 | pdqsdif(ig,ivap)=0.0 |
---|
659 | endif |
---|
660 | endif |
---|
661 | |
---|
662 | end do ! of DO ig=1,ngrid |
---|
663 | endif ! if (water et iq=ivap) |
---|
664 | end do ! of do iq=1,nq |
---|
665 | endif ! traceur |
---|
666 | |
---|
667 | |
---|
668 | !----------------------------------------------------------------------- |
---|
669 | ! 8. Final calculation of the vertical diffusion tendencies |
---|
670 | ! ----------------------------------------------------------------- |
---|
671 | |
---|
672 | do ilev = 1, nlay |
---|
673 | do ig=1,ngrid |
---|
674 | pdudif(ig,ilev)=(zu(ig,ilev)- |
---|
675 | & (pu(ig,ilev)+pdufi(ig,ilev)*ptimestep))/ptimestep |
---|
676 | pdvdif(ig,ilev)=(zv(ig,ilev)- |
---|
677 | & (pv(ig,ilev)+pdvfi(ig,ilev)*ptimestep))/ptimestep |
---|
678 | hh = ph(ig,ilev)+pdhfi(ig,ilev)*ptimestep |
---|
679 | |
---|
680 | pdhdif(ig,ilev)=( zh(ig,ilev)- hh )/ptimestep |
---|
681 | enddo |
---|
682 | enddo |
---|
683 | |
---|
684 | if (tracer) then |
---|
685 | do iq = 1, nq |
---|
686 | do ilev = 1, nlay |
---|
687 | do ig=1,ngrid |
---|
688 | pdqdif(ig,ilev,iq)=(zq(ig,ilev,iq)- |
---|
689 | & (pq(ig,ilev,iq)+pdqfi(ig,ilev,iq)*ptimestep))/ |
---|
690 | & ptimestep |
---|
691 | enddo |
---|
692 | enddo |
---|
693 | enddo |
---|
694 | |
---|
695 | if(water.and.forceWC)then ! force water conservation in model |
---|
696 | ! we calculate the difference and add it to the ground |
---|
697 | ! this is ugly and should be improved in the future |
---|
698 | do ig=1,ngrid |
---|
699 | Wtot=0.0 |
---|
700 | do ilay=1,nlay |
---|
701 | masse = (pplev(ig,ilay) - pplev(ig,ilay+1))/g |
---|
702 | ! Wtot=Wtot+masse*(zq(ig,ilay,iice)- |
---|
703 | ! & (pq(ig,ilay,iice)+pdqfi(ig,ilay,iice)*ptimestep)) |
---|
704 | Wtot=Wtot+masse*(zq(ig,ilay,ivap)- |
---|
705 | & (pq(ig,ilay,ivap)+pdqfi(ig,ilay,ivap)*ptimestep)) |
---|
706 | enddo |
---|
707 | Wdiff=Wtot/ptimestep+pdqsdif(ig,ivap)+pdqsdif(ig,iice) |
---|
708 | |
---|
709 | if(ztsrf2(ig).gt.To)then |
---|
710 | pdqsdif(ig,ivap)=pdqsdif(ig,ivap)-Wdiff |
---|
711 | else |
---|
712 | pdqsdif(ig,iice)=pdqsdif(ig,iice)-Wdiff |
---|
713 | endif |
---|
714 | enddo |
---|
715 | |
---|
716 | endif |
---|
717 | |
---|
718 | endif |
---|
719 | |
---|
720 | if(water)then |
---|
721 | call writediagfi(ngrid,'beta','Dryness coefficient',' ',2,dryness) |
---|
722 | endif |
---|
723 | |
---|
724 | ! if(lastcall)then |
---|
725 | ! if(ngrid.eq.1)then |
---|
726 | ! print*,'Saving k.out...' |
---|
727 | ! OPEN(12,file='k.out',form='formatted') |
---|
728 | ! DO ilay=1,nlay |
---|
729 | ! write(12,*) zkh(1,ilay), pplay(1,ilay) |
---|
730 | ! ENDDO |
---|
731 | ! CLOSE(12) |
---|
732 | ! endif |
---|
733 | ! endif |
---|
734 | |
---|
735 | |
---|
736 | return |
---|
737 | end |
---|