1 | MODULE lmdz_lscp_tools |
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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 | !+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
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8 | SUBROUTINE FALLICE_VELOCITY(klon,iwc,temp,rho,pres,ptconv,velo) |
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9 | |
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10 | ! Ref: |
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11 | ! Stubenrauch, C. J., Bonazzola, M., |
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12 | ! Protopapadaki, S. E., & Musat, I. (2019). |
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13 | ! New cloud system metrics to assess bulk |
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14 | ! ice cloud schemes in a GCM. Journal of |
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15 | ! Advances in Modeling Earth Systems, 11, |
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16 | ! 3212–3234. https://doi.org/10.1029/2019MS001642 |
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17 | |
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18 | use lmdz_lscp_ini, only: iflag_vice, ffallv_con, ffallv_lsc |
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19 | use lmdz_lscp_ini, only: cice_velo, dice_velo |
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20 | |
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21 | IMPLICIT NONE |
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22 | |
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23 | INTEGER, INTENT(IN) :: klon |
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24 | REAL, INTENT(IN), DIMENSION(klon) :: iwc ! specific ice water content [kg/m3] |
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25 | REAL, INTENT(IN), DIMENSION(klon) :: temp ! temperature [K] |
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26 | REAL, INTENT(IN), DIMENSION(klon) :: rho ! dry air density [kg/m3] |
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27 | REAL, INTENT(IN), DIMENSION(klon) :: pres ! air pressure [Pa] |
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28 | LOGICAL, INTENT(IN), DIMENSION(klon) :: ptconv ! convective point [-] |
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29 | |
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30 | REAL, INTENT(OUT), DIMENSION(klon) :: velo ! fallspeed velocity of crystals [m/s] |
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31 | |
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32 | |
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33 | INTEGER i |
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34 | REAL logvm,iwcg,tempc,phpa,fallv_tun |
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35 | REAL m2ice, m2snow, vmice, vmsnow |
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36 | REAL aice, bice, asnow, bsnow |
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37 | |
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38 | |
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39 | DO i=1,klon |
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40 | |
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41 | IF (ptconv(i)) THEN |
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42 | fallv_tun=ffallv_con |
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43 | ELSE |
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44 | fallv_tun=ffallv_lsc |
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45 | ENDIF |
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46 | |
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47 | tempc=temp(i)-273.15 ! celcius temp |
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48 | iwcg=MAX(iwc(i)*1000.,1E-3) ! iwc in g/m3. We set a minimum value to prevent from division by 0 |
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49 | phpa=pres(i)/100. ! pressure in hPa |
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50 | |
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51 | IF (iflag_vice == 1) THEN |
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52 | ! so-called 'empirical parameterization' in Stubenrauch et al. 2019 |
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53 | if (tempc >= -60.0) then |
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54 | |
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55 | logvm= -0.0000414122*tempc*tempc*log(iwcg)-0.00538922*tempc*log(iwcg) & |
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56 | -0.0516344*log(iwcg)+0.00216078*tempc + 1.9714 |
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57 | velo(i)=exp(logvm) |
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58 | else |
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59 | velo(i)=65.0*(iwcg**0.2)*(150./phpa)**0.15 |
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60 | endif |
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61 | |
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62 | velo(i)=fallv_tun*velo(i)/100.0 ! from cm/s to m/s |
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63 | |
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64 | ELSE IF (iflag_vice == 2) THEN |
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65 | ! so called PSDM empirical coherent bulk ice scheme in Stubenrauch et al. 2019 |
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66 | aice=0.587 |
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67 | bice=2.45 |
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68 | asnow=0.0444 |
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69 | bsnow=2.1 |
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70 | |
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71 | m2ice=((iwcg*0.001/aice)/(exp(13.6-bice*7.76+0.479*bice**2)* & |
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72 | exp((-0.0361+bice*0.0151+0.00149*bice**2)*tempc))) & |
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73 | **(1./(0.807+bice*0.00581+0.0457*bice**2)) |
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74 | |
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75 | vmice=100.*1042.4*exp(13.6-(bice+1)*7.76+0.479*(bice+1.)**2)*exp((-0.0361+ & |
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76 | (bice+1.)*0.0151+0.00149*(bice+1.)**2)*tempc) & |
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77 | *(m2ice**(0.807+(bice+1.)*0.00581+0.0457*(bice+1.)**2))/(iwcg*0.001/aice) |
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78 | |
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79 | |
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80 | vmice=vmice*((1000./phpa)**0.2) |
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81 | |
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82 | m2snow=((iwcg*0.001/asnow)/(exp(13.6-bsnow*7.76+0.479*bsnow**2)* & |
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83 | exp((-0.0361+bsnow*0.0151+0.00149*bsnow**2)*tempc))) & |
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84 | **(1./(0.807+bsnow*0.00581+0.0457*bsnow**2)) |
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85 | |
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86 | |
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87 | vmsnow=100.*14.3*exp(13.6-(bsnow+.416)*7.76+0.479*(bsnow+.416)**2)& |
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88 | *exp((-0.0361+(bsnow+.416)*0.0151+0.00149*(bsnow+.416)**2)*tempc)& |
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89 | *(m2snow**(0.807+(bsnow+.416)*0.00581+0.0457*(bsnow+.416)**2))/(iwcg*0.001/asnow) |
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90 | |
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91 | vmsnow=vmsnow*((1000./phpa)**0.35) |
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92 | velo(i)=fallv_tun*min(vmsnow,vmice)/100. ! to m/s |
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93 | |
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94 | ELSE |
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95 | ! By default, fallspeed velocity of ice crystals according to Heymsfield & Donner 1990 |
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96 | velo(i) = fallv_tun*cice_velo*((iwcg/1000.)**dice_velo) |
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97 | ENDIF |
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98 | ENDDO |
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99 | |
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100 | END SUBROUTINE FALLICE_VELOCITY |
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101 | !+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
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102 | |
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103 | !+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
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104 | SUBROUTINE ICEFRAC_LSCP(klon, temp, iflag_ice_thermo, distcltop, temp_cltop, icefrac, dicefracdT) |
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105 | !+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
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106 | |
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107 | ! Compute the ice fraction 1-xliq (see e.g. |
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108 | ! Doutriaux-Boucher & Quaas 2004, section 2.2.) |
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109 | ! as a function of temperature |
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110 | ! see also Fig 3 of Madeleine et al. 2020, JAMES |
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111 | !+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
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112 | |
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113 | |
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114 | USE print_control_mod, ONLY: lunout, prt_level |
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115 | USE lmdz_lscp_ini, ONLY: t_glace_min, t_glace_max, exposant_glace, iflag_t_glace |
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116 | USE lmdz_lscp_ini, ONLY: RTT, dist_liq, temp_nowater |
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117 | USE lmdz_abort_physic, ONLY: abort_physic |
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118 | |
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119 | IMPLICIT NONE |
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120 | |
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121 | |
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122 | INTEGER, INTENT(IN) :: klon ! number of horizontal grid points |
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123 | REAL, INTENT(IN), DIMENSION(klon) :: temp ! temperature |
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124 | REAL, INTENT(IN), DIMENSION(klon) :: distcltop ! distance to cloud top |
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125 | REAL, INTENT(IN), DIMENSION(klon) :: temp_cltop ! temperature of cloud top |
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126 | INTEGER, INTENT(IN) :: iflag_ice_thermo |
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127 | REAL, INTENT(OUT), DIMENSION(klon) :: icefrac |
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128 | REAL, INTENT(OUT), DIMENSION(klon) :: dicefracdT |
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129 | |
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130 | |
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131 | INTEGER i |
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132 | REAL liqfrac_tmp, dicefrac_tmp |
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133 | REAL Dv, denomdep,beta,qsi,dqsidt |
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134 | LOGICAL ice_thermo |
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135 | |
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136 | CHARACTER (len = 20) :: modname = 'lscp_tools' |
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137 | CHARACTER (len = 80) :: abort_message |
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138 | |
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139 | IF ((iflag_t_glace<2)) THEN !.OR. (iflag_t_glace.GT.6)) THEN |
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140 | abort_message = 'lscp cannot be used if iflag_t_glace<2 or >6' |
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141 | CALL abort_physic(modname,abort_message,1) |
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142 | ENDIF |
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143 | |
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144 | IF (.NOT.((iflag_ice_thermo == 1).OR.(iflag_ice_thermo >= 3))) THEN |
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145 | abort_message = 'lscp cannot be used without ice thermodynamics' |
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146 | CALL abort_physic(modname,abort_message,1) |
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147 | ENDIF |
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148 | |
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149 | |
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150 | DO i=1,klon |
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151 | |
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152 | ! old function with sole dependence upon temperature |
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153 | IF (iflag_t_glace == 2) THEN |
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154 | liqfrac_tmp = (temp(i)-t_glace_min) / (t_glace_max-t_glace_min) |
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155 | liqfrac_tmp = MIN(MAX(liqfrac_tmp,0.0),1.0) |
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156 | icefrac(i) = (1.0-liqfrac_tmp)**exposant_glace |
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157 | IF (icefrac(i) >0.) THEN |
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158 | dicefracdT(i)= exposant_glace * (icefrac(i)**(exposant_glace-1.)) & |
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159 | / (t_glace_min - t_glace_max) |
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160 | ENDIF |
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161 | |
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162 | IF ((icefrac(i)==0).OR.(icefrac(i)==1)) THEN |
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163 | dicefracdT(i)=0. |
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164 | ENDIF |
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165 | |
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166 | ENDIF |
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167 | |
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168 | ! function of temperature used in CMIP6 physics |
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169 | IF (iflag_t_glace == 3) THEN |
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170 | liqfrac_tmp = (temp(i)-t_glace_min) / (t_glace_max-t_glace_min) |
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171 | liqfrac_tmp = MIN(MAX(liqfrac_tmp,0.0),1.0) |
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172 | icefrac(i) = 1.0-liqfrac_tmp**exposant_glace |
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173 | IF ((icefrac(i) >0.) .AND. (liqfrac_tmp > 0.)) THEN |
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174 | dicefracdT(i)= exposant_glace * ((liqfrac_tmp)**(exposant_glace-1.)) & |
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175 | / (t_glace_min - t_glace_max) |
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176 | ELSE |
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177 | dicefracdT(i)=0. |
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178 | ENDIF |
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179 | ENDIF |
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180 | |
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181 | ! for iflag_t_glace .GE. 4, the liquid fraction depends upon temperature at cloud top |
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182 | ! and then decreases with decreasing height |
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183 | |
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184 | !with linear function of temperature at cloud top |
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185 | IF (iflag_t_glace == 4) THEN |
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186 | liqfrac_tmp = (temp(i)-t_glace_min) / (t_glace_max-t_glace_min) |
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187 | liqfrac_tmp = MIN(MAX(liqfrac_tmp,0.0),1.0) |
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188 | icefrac(i) = MAX(MIN(1.,1.0 - liqfrac_tmp*exp(-distcltop(i)/dist_liq)),0.) |
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189 | dicefrac_tmp = - temp(i)/(t_glace_max-t_glace_min) |
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190 | dicefracdT(i) = dicefrac_tmp*exp(-distcltop(i)/dist_liq) |
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191 | IF ((liqfrac_tmp <=0) .OR. (liqfrac_tmp >= 1)) THEN |
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192 | dicefracdT(i) = 0. |
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193 | ENDIF |
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194 | ENDIF |
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195 | |
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196 | ! with CMIP6 function of temperature at cloud top |
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197 | IF ((iflag_t_glace == 5) .OR. (iflag_t_glace == 7)) THEN |
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198 | liqfrac_tmp = (temp(i)-t_glace_min) / (t_glace_max-t_glace_min) |
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199 | liqfrac_tmp = MIN(MAX(liqfrac_tmp,0.0),1.0) |
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200 | liqfrac_tmp = liqfrac_tmp**exposant_glace |
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201 | icefrac(i) = MAX(MIN(1.,1.0 - liqfrac_tmp*exp(-distcltop(i)/dist_liq)),0.) |
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202 | IF ((liqfrac_tmp <=0) .OR. (liqfrac_tmp >= 1)) THEN |
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203 | dicefracdT(i) = 0. |
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204 | ELSE |
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205 | dicefracdT(i) = exposant_glace*((liqfrac_tmp)**(exposant_glace-1.))/(t_glace_min- t_glace_max) & |
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206 | *exp(-distcltop(i)/dist_liq) |
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207 | ENDIF |
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208 | ENDIF |
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209 | |
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210 | ! with modified function of temperature at cloud top |
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211 | ! to get largere values around 260 K, works well with t_glace_min = 241K |
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212 | IF (iflag_t_glace == 6) THEN |
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213 | IF (temp(i) > t_glace_max) THEN |
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214 | liqfrac_tmp = 1. |
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215 | ELSE |
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216 | liqfrac_tmp = -((temp(i)-t_glace_max) / (t_glace_max-t_glace_min))**2+1. |
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217 | ENDIF |
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218 | liqfrac_tmp = MIN(MAX(liqfrac_tmp,0.0),1.0) |
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219 | icefrac(i) = MAX(MIN(1.,1.0 - liqfrac_tmp*exp(-distcltop(i)/dist_liq)),0.) |
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220 | IF ((liqfrac_tmp <=0) .OR. (liqfrac_tmp >= 1)) THEN |
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221 | dicefracdT(i) = 0. |
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222 | ELSE |
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223 | dicefracdT(i) = 2*((temp(i)-t_glace_max) / (t_glace_max-t_glace_min))/(t_glace_max-t_glace_min) & |
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224 | *exp(-distcltop(i)/dist_liq) |
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225 | ENDIF |
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226 | ENDIF |
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227 | |
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228 | ! if temperature of cloud top <-40°C, |
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229 | IF (iflag_t_glace >= 4) THEN |
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230 | IF ((temp_cltop(i) <= temp_nowater) .AND. (temp(i) <= t_glace_max)) THEN |
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231 | icefrac(i) = 1. |
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232 | dicefracdT(i) = 0. |
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233 | ENDIF |
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234 | ENDIF |
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235 | |
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236 | |
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237 | ENDDO ! klon |
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238 | |
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239 | |
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240 | END SUBROUTINE ICEFRAC_LSCP |
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241 | !+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
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242 | |
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243 | SUBROUTINE ICEFRAC_LSCP_TURB(klon, dtime, temp, pplay, paprsdn, paprsup, qice_ini, snowcld, qtot_incl, cldfra, tke, tke_dissip, qliq, qvap_cld, qice, icefrac, dicefracdT, cldfraliq, sigma2_icefracturb, mean_icefracturb) |
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244 | !+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
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245 | ! Compute the liquid, ice and vapour content (+ice fraction) based |
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246 | ! on turbulence (see Fields 2014, Furtado 2016) |
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247 | !+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
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248 | |
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249 | |
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250 | USE lmdz_lscp_ini, ONLY: prt_level, lunout |
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251 | USE lmdz_lscp_ini, ONLY: RCPD, RLSTT, RLVTT, RLMLT, RVTMP2, RTT, RD, RG, RV, RPI |
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252 | USE lmdz_lscp_ini, ONLY: seuil_neb, temp_nowater |
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253 | USE lmdz_lscp_ini, ONLY: tau_mixenv, lmix_mpc, naero5, gamma_snwretro, gamma_taud, capa_crystal |
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254 | USE lmdz_lscp_ini, ONLY: eps |
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255 | |
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256 | IMPLICIT NONE |
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257 | |
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258 | INTEGER, INTENT(IN) :: klon !--number of horizontal grid points |
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259 | REAL, INTENT(IN) :: dtime !--time step [s] |
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260 | |
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261 | REAL, INTENT(IN), DIMENSION(klon) :: temp !--temperature |
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262 | REAL, INTENT(IN), DIMENSION(klon) :: pplay !--pressure in the middle of the layer [Pa] |
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263 | REAL, INTENT(IN), DIMENSION(klon) :: paprsdn !--pressure at the bottom interface of the layer [Pa] |
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264 | REAL, INTENT(IN), DIMENSION(klon) :: paprsup !--pressure at the top interface of the layer [Pa] |
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265 | REAL, INTENT(IN), DIMENSION(klon) :: qtot_incl !--specific total cloud water content, in-cloud content [kg/kg] |
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266 | REAL, INTENT(IN), DIMENSION(klon) :: cldfra !--cloud fraction in gridbox [-] |
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267 | REAL, INTENT(IN), DIMENSION(klon) :: tke !--turbulent kinetic energy [m2/s2] |
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268 | REAL, INTENT(IN), DIMENSION(klon) :: tke_dissip !--TKE dissipation [m2/s3] |
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269 | |
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270 | REAL, INTENT(IN), DIMENSION(klon) :: qice_ini !--initial specific ice content gridbox-mean [kg/kg] |
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271 | REAL, INTENT(IN), DIMENSION(klon) :: snowcld |
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272 | REAL, INTENT(OUT), DIMENSION(klon) :: qliq !--specific liquid content gridbox-mean [kg/kg] |
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273 | REAL, INTENT(OUT), DIMENSION(klon) :: qvap_cld !--specific cloud vapor content, gridbox-mean [kg/kg] |
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274 | REAL, INTENT(OUT), DIMENSION(klon) :: qice !--specific ice content gridbox-mean [kg/kg] |
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275 | REAL, INTENT(OUT), DIMENSION(klon) :: icefrac !--fraction of ice in condensed water [-] |
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276 | REAL, INTENT(OUT), DIMENSION(klon) :: dicefracdT |
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277 | |
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278 | REAL, INTENT(OUT), DIMENSION(klon) :: cldfraliq !--fraction of cldfra which is liquid only |
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279 | REAL, INTENT(OUT), DIMENSION(klon) :: sigma2_icefracturb !--Temporary |
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280 | REAL, INTENT(OUT), DIMENSION(klon) :: mean_icefracturb !--Temporary |
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281 | |
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282 | REAL, DIMENSION(klon) :: qzero, qsatl, dqsatl, qsati, dqsati !--specific humidity saturation values |
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283 | INTEGER :: i |
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284 | |
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285 | REAL :: qvap_incl, qice_incl, qliq_incl, qiceini_incl !--In-cloud specific quantities [kg/kg] |
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286 | REAL :: qsnowcld_incl |
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287 | !REAL :: capa_crystal !--Capacitance of ice crystals [-] |
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288 | REAL :: water_vapor_diff !--Water-vapour diffusion coefficient in air [m2/s] (function of T&P) |
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289 | REAL :: air_thermal_conduct !--Thermal conductivity of air [J/m/K/s] (function of T) |
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290 | REAL :: C0 !--Lagrangian structure function [-] |
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291 | REAL :: tau_mixingenv |
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292 | REAL :: tau_dissipturb |
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293 | REAL :: invtau_phaserelax |
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294 | REAL :: sigma2_pdf, mean_pdf |
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295 | REAL :: ai, bi, B0 |
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296 | REAL :: sursat_iceliq |
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297 | REAL :: sursat_env |
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298 | REAL :: liqfra_max |
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299 | REAL :: sursat_iceext |
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300 | REAL :: nb_crystals !--number concentration of ice crystals [#/m3] |
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301 | REAL :: moment1_PSD !--1st moment of ice PSD |
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302 | REAL :: N0_PSD, lambda_PSD !--parameters of the exponential PSD |
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303 | |
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304 | REAL :: rho_ice !--ice density [kg/m3] |
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305 | REAL :: cldfra1D |
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306 | REAL :: deltaz, rho_air |
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307 | REAL :: psati !--saturation vapor pressure wrt i [Pa] |
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308 | |
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309 | C0 = 10. !--value assumed in Field2014 |
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310 | rho_ice = 950. |
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311 | sursat_iceext = -0.1 |
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312 | !capa_crystal = 1. !r_ice |
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313 | qzero(:) = 0. |
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314 | cldfraliq(:) = 0. |
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315 | icefrac(:) = 0. |
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316 | dicefracdT(:) = 0. |
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317 | |
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318 | sigma2_icefracturb(:) = 0. |
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319 | mean_icefracturb(:) = 0. |
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320 | |
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321 | !--wrt liquid water |
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322 | CALL calc_qsat_ecmwf(klon,temp(:),qzero(:),pplay(:),RTT,1,.FALSE.,qsatl(:),dqsatl(:)) |
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323 | !--wrt ice |
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324 | CALL calc_qsat_ecmwf(klon,temp(:),qzero(:),pplay(:),RTT,2,.FALSE.,qsati(:),dqsati(:)) |
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325 | |
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326 | |
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327 | DO i=1,klon |
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328 | |
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329 | |
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330 | rho_air = pplay(i) / temp(i) / RD |
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331 | !deltaz = ( paprsdn(i) - paprsup(i) ) / RG / rho_air(i) |
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332 | ! because cldfra is intent in, but can be locally modified due to test |
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333 | cldfra1D = cldfra(i) |
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334 | IF (cldfra(i) <= 0.) THEN |
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335 | qvap_cld(i) = 0. |
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336 | qliq(i) = 0. |
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337 | qice(i) = 0. |
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338 | cldfraliq(i) = 0. |
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339 | icefrac(i) = 0. |
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340 | dicefracdT(i) = 0. |
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341 | |
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342 | ! If there is a cloud |
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343 | ELSE |
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344 | IF (cldfra(i) >= 1.0) THEN |
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345 | cldfra1D = 1.0 |
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346 | END IF |
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347 | |
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348 | ! T>0°C, no ice allowed |
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349 | IF ( temp(i) >= RTT ) THEN |
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350 | qvap_cld(i) = qsatl(i) * cldfra1D |
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351 | qliq(i) = MAX(0.0,qtot_incl(i)-qsatl(i)) * cldfra1D |
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352 | qice(i) = 0. |
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353 | cldfraliq(i) = 1. |
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354 | icefrac(i) = 0. |
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355 | dicefracdT(i) = 0. |
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356 | |
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357 | ! T<-38°C, no liquid allowed |
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358 | ELSE IF ( temp(i) <= temp_nowater) THEN |
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359 | qvap_cld(i) = qsati(i) * cldfra1D |
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360 | qliq(i) = 0. |
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361 | qice(i) = MAX(0.0,qtot_incl(i)-qsati(i)) * cldfra1D |
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362 | cldfraliq(i) = 0. |
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363 | icefrac(i) = 1. |
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364 | dicefracdT(i) = 0. |
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365 | |
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366 | ! MPC temperature |
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367 | ELSE |
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368 | ! Not enough TKE |
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369 | IF ( tke_dissip(i) <= eps ) THEN |
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370 | qvap_cld(i) = qsati(i) * cldfra1D |
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371 | qliq(i) = 0. |
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372 | qice(i) = MAX(0.,qtot_incl(i)-qsati(i)) * cldfra1D |
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373 | cldfraliq(i) = 0. |
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374 | icefrac(i) = 1. |
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375 | dicefracdT(i) = 0. |
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376 | |
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377 | ! Enough TKE |
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378 | ELSE |
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379 | !--------------------------------------------------------- |
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380 | !-- ICE SUPERSATURATION PDF |
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381 | !--------------------------------------------------------- |
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382 | !--If -38°C< T <0°C and there is enough turbulence, |
---|
383 | !--we compute the cloud liquid properties with a Gaussian PDF |
---|
384 | !--of ice supersaturation F(Si) (Field2014, Furtado2016). |
---|
385 | !--Parameters of the PDF are function of turbulence and |
---|
386 | !--microphysics/existing ice. |
---|
387 | |
---|
388 | sursat_iceliq = qsatl(i)/qsati(i) - 1. |
---|
389 | psati = qsati(i) * pplay(i) / (RD/RV) |
---|
390 | |
---|
391 | !-------------- MICROPHYSICAL TERMS -------------- |
---|
392 | !--We assume an exponential ice PSD whose parameters |
---|
393 | !--are computed following Morrison&Gettelman 2008 |
---|
394 | !--Ice number density is assumed equals to INP density |
---|
395 | !--which is a function of temperature (DeMott 2010) |
---|
396 | !--bi and B0 are microphysical function characterizing |
---|
397 | !--vapor/ice interactions |
---|
398 | !--tau_phase_relax is the typical time of vapor deposition |
---|
399 | !--onto ice crystals |
---|
400 | |
---|
401 | qiceini_incl = qice_ini(i) / cldfra1D |
---|
402 | qsnowcld_incl = snowcld(i) * RG * dtime / ( paprsdn(i) - paprsup(i) ) / cldfra1D |
---|
403 | sursat_env = max(0., (qtot_incl(i) - qiceini_incl)/qsati(i) - 1.) |
---|
404 | IF ( qiceini_incl > eps ) THEN |
---|
405 | nb_crystals = 1.e3 * 5.94e-5 * ( RTT - temp(i) )**3.33 * naero5**(0.0264*(RTT-temp(i))+0.0033) |
---|
406 | lambda_PSD = ( (RPI*rho_ice*nb_crystals*24.) / (6.*(qiceini_incl + gamma_snwretro * qsnowcld_incl)) ) ** (1./3.) |
---|
407 | N0_PSD = nb_crystals * lambda_PSD |
---|
408 | moment1_PSD = N0_PSD/2./lambda_PSD**2 |
---|
409 | ELSE |
---|
410 | moment1_PSD = 0. |
---|
411 | ENDIF |
---|
412 | |
---|
413 | !--Formulae for air thermal conductivity and water vapor diffusivity |
---|
414 | !--comes respectively from Beard and Pruppacher (1971) |
---|
415 | !--and Hall and Pruppacher (1976) |
---|
416 | |
---|
417 | air_thermal_conduct = ( 5.69 + 0.017 * ( temp(i) - RTT ) ) * 1.e-3 * 4.184 |
---|
418 | water_vapor_diff = 2.11*1e-5 * ( temp(i) / RTT )**1.94 * ( 101325 / pplay(i) ) |
---|
419 | |
---|
420 | bi = 1./((qsati(i)+qsatl(i))/2.) + RLSTT**2 / RCPD / RV / temp(i)**2 |
---|
421 | B0 = 4. * RPI * capa_crystal * 1. / ( RLSTT**2 / air_thermal_conduct / RV / temp(i)**2 & |
---|
422 | + RV * temp(i) / psati / water_vapor_diff ) |
---|
423 | |
---|
424 | invtau_phaserelax = (bi * B0 * moment1_PSD ) |
---|
425 | |
---|
426 | ! Old way of estimating moment1 : spherical crystals + monodisperse PSD |
---|
427 | ! nb_crystals = rho_air * qiceini_incl / ( 4. / 3. * RPI * r_ice**3. * rho_ice ) |
---|
428 | ! moment1_PSD = nb_crystals * r_ice |
---|
429 | |
---|
430 | !----------------- TURBULENT SOURCE/SINK TERMS ----------------- |
---|
431 | !--Tau_mixingenv is the time needed to homogeneize the parcel |
---|
432 | !--with its environment by turbulent diffusion over the parcel |
---|
433 | !--length scale |
---|
434 | !--if lmix_mpc <0, tau_mixigenv value is prescribed |
---|
435 | !--else tau_mixigenv value is derived from tke_dissip and lmix_mpc |
---|
436 | !--Tau_dissipturb is the time needed turbulence to decay due to |
---|
437 | !--viscosity |
---|
438 | |
---|
439 | ai = RG / RD / temp(i) * ( RD * RLSTT / RCPD / RV / temp(i) - 1. ) |
---|
440 | IF ( lmix_mpc > 0 ) THEN |
---|
441 | tau_mixingenv = ( lmix_mpc**2. / tke_dissip(i) )**(1./3.) |
---|
442 | ELSE |
---|
443 | tau_mixingenv = tau_mixenv |
---|
444 | ENDIF |
---|
445 | |
---|
446 | tau_dissipturb = gamma_taud * 2. * 2./3. * tke(i) / tke_dissip(i) / C0 |
---|
447 | |
---|
448 | !--------------------- PDF COMPUTATIONS --------------------- |
---|
449 | !--Formulae for sigma2_pdf (variance), mean of PDF in Furtado2016 |
---|
450 | !--cloud liquid fraction and in-cloud liquid content are given |
---|
451 | !--by integrating resp. F(Si) and Si*F(Si) |
---|
452 | !--Liquid is limited by the available water vapor trough a |
---|
453 | !--maximal liquid fraction |
---|
454 | |
---|
455 | liqfra_max = MAX(0., (MIN (1.,( qtot_incl(i) - qiceini_incl - qsati(i) * (1 + sursat_iceext ) ) / ( qsatl(i) - qsati(i) ) ) ) ) |
---|
456 | sigma2_pdf = 1./2. * ( ai**2 ) * 2./3. * tke(i) * tau_dissipturb / ( invtau_phaserelax + 1./tau_mixingenv ) |
---|
457 | mean_pdf = sursat_env * 1./tau_mixingenv / ( invtau_phaserelax + 1./tau_mixingenv ) |
---|
458 | cldfraliq(i) = 0.5 * (1. - erf( ( sursat_iceliq - mean_pdf) / (SQRT(2.* sigma2_pdf) ) ) ) |
---|
459 | !IF (cldfraliq(i) .GT. liqfra_max) THEN |
---|
460 | ! cldfraliq(i) = liqfra_max |
---|
461 | !ENDIF |
---|
462 | |
---|
463 | qliq_incl = qsati(i) * SQRT(sigma2_pdf) / SQRT(2.*RPI) * EXP( -1.*(sursat_iceliq - mean_pdf)**2. / (2.*sigma2_pdf) ) & |
---|
464 | - qsati(i) * cldfraliq(i) * (sursat_iceliq - mean_pdf ) |
---|
465 | |
---|
466 | sigma2_icefracturb(i)= sigma2_pdf |
---|
467 | mean_icefracturb(i) = mean_pdf |
---|
468 | !------------ ICE AMOUNT AND WATER CONSERVATION ------------ |
---|
469 | |
---|
470 | IF ( (qliq_incl <= eps) .OR. (cldfraliq(i) <= eps) ) THEN |
---|
471 | qliq_incl = 0. |
---|
472 | cldfraliq(i) = 0. |
---|
473 | END IF |
---|
474 | |
---|
475 | !--Choice for in-cloud vapor : |
---|
476 | !--1.Weighted mean between qvap in MPC parts and in ice-only parts |
---|
477 | !--2.Always at ice saturation |
---|
478 | qvap_incl = MAX(qsati(i), ( 1. - cldfraliq(i) ) * (sursat_iceext + 1.) * qsati(i) + cldfraliq(i) * qsatl(i) ) |
---|
479 | |
---|
480 | IF ( qvap_incl >= qtot_incl(i) ) THEN |
---|
481 | qvap_incl = qsati(i) |
---|
482 | qliq_incl = qtot_incl(i) - qvap_incl |
---|
483 | qice_incl = 0. |
---|
484 | |
---|
485 | ELSEIF ( (qvap_incl + qliq_incl) >= qtot_incl(i) ) THEN |
---|
486 | qliq_incl = MAX(0.0,qtot_incl(i) - qvap_incl) |
---|
487 | qice_incl = 0. |
---|
488 | ELSE |
---|
489 | qice_incl = qtot_incl(i) - qvap_incl - qliq_incl |
---|
490 | END IF |
---|
491 | |
---|
492 | qvap_cld(i) = qvap_incl * cldfra1D |
---|
493 | qliq(i) = qliq_incl * cldfra1D |
---|
494 | qice(i) = qice_incl * cldfra1D |
---|
495 | icefrac(i) = qice(i) / ( qice(i) + qliq(i) ) |
---|
496 | dicefracdT(i) = 0. |
---|
497 | !PRINT*,'MPC turb' |
---|
498 | |
---|
499 | END IF ! Enough TKE |
---|
500 | |
---|
501 | END IF ! ! MPC temperature |
---|
502 | |
---|
503 | END IF ! cldfra |
---|
504 | |
---|
505 | ENDDO ! klon |
---|
506 | END SUBROUTINE ICEFRAC_LSCP_TURB |
---|
507 | !+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
---|
508 | |
---|
509 | |
---|
510 | SUBROUTINE CALC_QSAT_ECMWF(klon,temp,qtot,pressure,tref,phase,flagth,qs,dqs) |
---|
511 | !+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
---|
512 | ! Calculate qsat following ECMWF method |
---|
513 | !+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
---|
514 | |
---|
515 | |
---|
516 | IMPLICIT NONE |
---|
517 | |
---|
518 | include "YOMCST.h" |
---|
519 | include "YOETHF.h" |
---|
520 | include "FCTTRE.h" |
---|
521 | |
---|
522 | INTEGER, INTENT(IN) :: klon ! number of horizontal grid points |
---|
523 | REAL, INTENT(IN), DIMENSION(klon) :: temp ! temperature in K |
---|
524 | REAL, INTENT(IN), DIMENSION(klon) :: qtot ! total specific water in kg/kg |
---|
525 | REAL, INTENT(IN), DIMENSION(klon) :: pressure ! pressure in Pa |
---|
526 | REAL, INTENT(IN) :: tref ! reference temperature in K |
---|
527 | LOGICAL, INTENT(IN) :: flagth ! flag for qsat calculation for thermals |
---|
528 | INTEGER, INTENT(IN) :: phase |
---|
529 | ! phase: 0=depend on temperature sign (temp>tref -> liquid, temp<tref, solid) |
---|
530 | ! 1=liquid |
---|
531 | ! 2=solid |
---|
532 | |
---|
533 | REAL, INTENT(OUT), DIMENSION(klon) :: qs ! saturation specific humidity [kg/kg] |
---|
534 | REAL, INTENT(OUT), DIMENSION(klon) :: dqs ! derivation of saturation specific humidity wrt T |
---|
535 | |
---|
536 | REAL delta, cor, cvm5 |
---|
537 | INTEGER i |
---|
538 | |
---|
539 | DO i=1,klon |
---|
540 | |
---|
541 | IF (phase == 1) THEN |
---|
542 | delta=0. |
---|
543 | ELSEIF (phase == 2) THEN |
---|
544 | delta=1. |
---|
545 | ELSE |
---|
546 | delta=MAX(0.,SIGN(1.,tref-temp(i))) |
---|
547 | ENDIF |
---|
548 | |
---|
549 | IF (flagth) THEN |
---|
550 | cvm5=R5LES*(1.-delta) + R5IES*delta |
---|
551 | ELSE |
---|
552 | cvm5 = R5LES*RLVTT*(1.-delta) + R5IES*RLSTT*delta |
---|
553 | cvm5 = cvm5 /RCPD/(1.0+RVTMP2*(qtot(i))) |
---|
554 | ENDIF |
---|
555 | |
---|
556 | qs(i)= R2ES*FOEEW(temp(i),delta)/pressure(i) |
---|
557 | qs(i)=MIN(0.5,qs(i)) |
---|
558 | cor=1./(1.-RETV*qs(i)) |
---|
559 | qs(i)=qs(i)*cor |
---|
560 | dqs(i)= FOEDE(temp(i),delta,cvm5,qs(i),cor) |
---|
561 | |
---|
562 | END DO |
---|
563 | |
---|
564 | END SUBROUTINE CALC_QSAT_ECMWF |
---|
565 | !+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
---|
566 | |
---|
567 | |
---|
568 | !+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
---|
569 | SUBROUTINE CALC_GAMMASAT(klon,temp,qtot,pressure,gammasat,dgammasatdt) |
---|
570 | |
---|
571 | !+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
---|
572 | ! programme that calculates the gammasat parameter that determines the |
---|
573 | ! homogeneous condensation thresholds for cold (<0oC) clouds |
---|
574 | ! condensation at q>gammasat*qsat |
---|
575 | ! Etienne Vignon, March 2021 |
---|
576 | !+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
---|
577 | |
---|
578 | use lmdz_lscp_ini, only: iflag_gammasat, t_glace_min, RTT |
---|
579 | |
---|
580 | IMPLICIT NONE |
---|
581 | |
---|
582 | |
---|
583 | INTEGER, INTENT(IN) :: klon ! number of horizontal grid points |
---|
584 | REAL, INTENT(IN), DIMENSION(klon) :: temp ! temperature in K |
---|
585 | REAL, INTENT(IN), DIMENSION(klon) :: qtot ! total specific water in kg/kg |
---|
586 | |
---|
587 | REAL, INTENT(IN), DIMENSION(klon) :: pressure ! pressure in Pa |
---|
588 | |
---|
589 | REAL, INTENT(OUT), DIMENSION(klon) :: gammasat ! coefficient to multiply qsat with to calculate saturation |
---|
590 | REAL, INTENT(OUT), DIMENSION(klon) :: dgammasatdt ! derivative of gammasat wrt temperature |
---|
591 | |
---|
592 | REAL, DIMENSION(klon) :: qsi,qsl,dqsl,dqsi |
---|
593 | REAL fcirrus, fac |
---|
594 | REAL, PARAMETER :: acirrus=2.349 |
---|
595 | REAL, PARAMETER :: bcirrus=259.0 |
---|
596 | |
---|
597 | INTEGER i |
---|
598 | |
---|
599 | CALL CALC_QSAT_ECMWF(klon,temp,qtot,pressure,RTT,1,.FALSE.,qsl,dqsl) |
---|
600 | CALL CALC_QSAT_ECMWF(klon,temp,qtot,pressure,RTT,2,.FALSE.,qsi,dqsi) |
---|
601 | |
---|
602 | DO i=1,klon |
---|
603 | |
---|
604 | IF (temp(i) >= RTT) THEN |
---|
605 | ! warm clouds: condensation at saturation wrt liquid |
---|
606 | gammasat(i)=1. |
---|
607 | dgammasatdt(i)=0. |
---|
608 | |
---|
609 | ELSEIF ((temp(i) < RTT) .AND. (temp(i) > t_glace_min)) THEN |
---|
610 | |
---|
611 | IF (iflag_gammasat >= 2) THEN |
---|
612 | gammasat(i)=qsl(i)/qsi(i) |
---|
613 | dgammasatdt(i)=(dqsl(i)*qsi(i)-dqsi(i)*qsl(i))/qsi(i)/qsi(i) |
---|
614 | ELSE |
---|
615 | gammasat(i)=1. |
---|
616 | dgammasatdt(i)=0. |
---|
617 | ENDIF |
---|
618 | |
---|
619 | ELSE |
---|
620 | |
---|
621 | IF (iflag_gammasat >=1) THEN |
---|
622 | ! homogeneous freezing of aerosols, according to |
---|
623 | ! Koop, 2000 and Karcher 2008, QJRMS |
---|
624 | ! 'Cirrus regime' |
---|
625 | fcirrus=acirrus-temp(i)/bcirrus |
---|
626 | IF (fcirrus > qsl(i)/qsi(i)) THEN |
---|
627 | gammasat(i)=qsl(i)/qsi(i) |
---|
628 | dgammasatdt(i)=(dqsl(i)*qsi(i)-dqsi(i)*qsl(i))/qsi(i)/qsi(i) |
---|
629 | ELSE |
---|
630 | gammasat(i)=fcirrus |
---|
631 | dgammasatdt(i)=-1.0/bcirrus |
---|
632 | ENDIF |
---|
633 | |
---|
634 | ELSE |
---|
635 | |
---|
636 | gammasat(i)=1. |
---|
637 | dgammasatdt(i)=0. |
---|
638 | |
---|
639 | ENDIF |
---|
640 | |
---|
641 | ENDIF |
---|
642 | |
---|
643 | END DO |
---|
644 | |
---|
645 | |
---|
646 | END SUBROUTINE CALC_GAMMASAT |
---|
647 | !+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
---|
648 | |
---|
649 | |
---|
650 | !++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
---|
651 | SUBROUTINE DISTANCE_TO_CLOUD_TOP(klon,klev,k,temp,pplay,paprs,rneb,distcltop1D,temp_cltop) |
---|
652 | !++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
---|
653 | |
---|
654 | USE lmdz_lscp_ini, ONLY: rd,rg,tresh_cl |
---|
655 | |
---|
656 | IMPLICIT NONE |
---|
657 | |
---|
658 | INTEGER, INTENT(IN) :: klon,klev !number of horizontal and vertical grid points |
---|
659 | INTEGER, INTENT(IN) :: k ! vertical index |
---|
660 | REAL, INTENT(IN), DIMENSION(klon,klev) :: temp ! temperature in K |
---|
661 | REAL, INTENT(IN), DIMENSION(klon,klev) :: pplay ! pressure middle layer in Pa |
---|
662 | REAL, INTENT(IN), DIMENSION(klon,klev+1) :: paprs ! pressure interfaces in Pa |
---|
663 | REAL, INTENT(IN), DIMENSION(klon,klev) :: rneb ! cloud fraction |
---|
664 | |
---|
665 | REAL, INTENT(OUT), DIMENSION(klon) :: distcltop1D ! distance from cloud top |
---|
666 | REAL, INTENT(OUT), DIMENSION(klon) :: temp_cltop ! temperature of cloud top |
---|
667 | |
---|
668 | REAL dzlay(klon,klev) |
---|
669 | REAL zlay(klon,klev) |
---|
670 | REAL dzinterf |
---|
671 | INTEGER i,k_top, kvert |
---|
672 | LOGICAL bool_cl |
---|
673 | |
---|
674 | |
---|
675 | DO i=1,klon |
---|
676 | ! Initialization height middle of first layer |
---|
677 | dzlay(i,1) = Rd * temp(i,1) / rg * log(paprs(i,1)/paprs(i,2)) |
---|
678 | zlay(i,1) = dzlay(i,1)/2 |
---|
679 | |
---|
680 | DO kvert=2,klev |
---|
681 | IF (kvert==klev) THEN |
---|
682 | dzlay(i,kvert) = 2*(rd * temp(i,kvert) / rg * log(paprs(i,kvert)/pplay(i,kvert))) |
---|
683 | ELSE |
---|
684 | dzlay(i,kvert) = rd * temp(i,kvert) / rg * log(paprs(i,kvert)/paprs(i,kvert+1)) |
---|
685 | ENDIF |
---|
686 | dzinterf = rd * temp(i,kvert) / rg * log(pplay(i,kvert-1)/pplay(i,kvert)) |
---|
687 | zlay(i,kvert) = zlay(i,kvert-1) + dzinterf |
---|
688 | ENDDO |
---|
689 | ENDDO |
---|
690 | |
---|
691 | DO i=1,klon |
---|
692 | k_top = k |
---|
693 | IF (rneb(i,k) <= tresh_cl) THEN |
---|
694 | bool_cl = .FALSE. |
---|
695 | ELSE |
---|
696 | bool_cl = .TRUE. |
---|
697 | ENDIF |
---|
698 | |
---|
699 | DO WHILE ((bool_cl) .AND. (k_top <= klev)) |
---|
700 | ! find cloud top |
---|
701 | IF (rneb(i,k_top) > tresh_cl) THEN |
---|
702 | k_top = k_top + 1 |
---|
703 | ELSE |
---|
704 | bool_cl = .FALSE. |
---|
705 | k_top = k_top - 1 |
---|
706 | ENDIF |
---|
707 | ENDDO |
---|
708 | k_top=min(k_top,klev) |
---|
709 | |
---|
710 | !dist to top is dist between current layer and layer of cloud top (from middle to middle) + dist middle to |
---|
711 | !interf for layer of cloud top |
---|
712 | distcltop1D(i) = zlay(i,k_top) - zlay(i,k) + dzlay(i,k_top)/2 |
---|
713 | temp_cltop(i) = temp(i,k_top) |
---|
714 | ENDDO ! klon |
---|
715 | |
---|
716 | END SUBROUTINE DISTANCE_TO_CLOUD_TOP |
---|
717 | !++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
---|
718 | |
---|
719 | END MODULE lmdz_lscp_tools |
---|
720 | |
---|
721 | |
---|