1 | MODULE lmdz_lscp_poprecip |
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2 | !---------------------------------------------------------------- |
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3 | ! Module for the process-oriented treament of precipitation |
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4 | ! that are called in LSCP |
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5 | ! Authors: Atelier Nuage (G. Riviere, L. Raillard, M. Wimmer, |
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6 | ! N. Dutrievoz, E. Vignon, A. Borella, et al.) |
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7 | ! Jan. 2024 |
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8 | |
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9 | |
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10 | IMPLICIT NONE |
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11 | |
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12 | CONTAINS |
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13 | |
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14 | !---------------------------------------------------------------- |
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15 | ! Computes the processes-oriented precipitation formulations for |
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16 | ! evaporation and sublimation |
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17 | |
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18 | SUBROUTINE poprecip_precld( & |
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19 | klon, dtime, iftop, paprsdn, paprsup, pplay, temp, tempupnew, qvap, & |
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20 | qprecip, precipfracclr, precipfraccld, qvapclrup, qtotupnew, & |
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21 | rain, rainclr, raincld, snow, snowclr, snowcld, dqreva, dqssub & |
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22 | ) |
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23 | |
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24 | USE lmdz_lscp_ini, ONLY: prt_level, lunout |
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25 | USE lmdz_lscp_ini, ONLY: coef_eva, coef_sub, expo_eva, expo_sub, thresh_precip_frac |
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26 | USE lmdz_lscp_ini, ONLY: RCPD, RLSTT, RLVTT, RLMLT, RVTMP2, RTT, RD, RG |
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27 | USE lmdz_lscp_ini, ONLY: ok_corr_vap_evasub |
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28 | USE lmdz_lscp_tools, ONLY: calc_qsat_ecmwf |
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29 | |
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30 | IMPLICIT NONE |
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31 | |
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32 | |
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33 | INTEGER, INTENT(IN) :: klon !--number of horizontal grid points [-] |
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34 | REAL, INTENT(IN) :: dtime !--time step [s] |
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35 | LOGICAL, INTENT(IN) :: iftop !--if top of the column |
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36 | |
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37 | |
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38 | REAL, INTENT(IN), DIMENSION(klon) :: paprsdn !--pressure at the bottom interface of the layer [Pa] |
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39 | REAL, INTENT(IN), DIMENSION(klon) :: paprsup !--pressure at the top interface of the layer [Pa] |
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40 | REAL, INTENT(IN), DIMENSION(klon) :: pplay !--pressure in the middle of the layer [Pa] |
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41 | |
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42 | REAL, INTENT(INOUT), DIMENSION(klon) :: temp !--current temperature [K] |
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43 | REAL, INTENT(INOUT), DIMENSION(klon) :: tempupnew !--updated temperature of the overlying layer [K] |
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44 | |
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45 | REAL, INTENT(INOUT), DIMENSION(klon) :: qvap !--current water vapor specific humidity (includes evaporated qi and ql) [kg/kg] |
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46 | REAL, INTENT(INOUT), DIMENSION(klon) :: qprecip !--specific humidity in the precipitation falling from the upper layer [kg/kg] |
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47 | |
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48 | REAL, INTENT(INOUT), DIMENSION(klon) :: precipfracclr !--fraction of precipitation in the clear sky IN THE LAYER ABOVE [-] |
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49 | REAL, INTENT(INOUT), DIMENSION(klon) :: precipfraccld !--fraction of precipitation in the cloudy air IN THE LAYER ABOVE [-] |
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50 | |
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51 | REAL, INTENT(IN), DIMENSION(klon) :: qvapclrup !--clear-sky specific humidity IN THE LAYER ABOVE [kg/kg] |
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52 | REAL, INTENT(IN), DIMENSION(klon) :: qtotupnew !--total specific humidity IN THE LAYER ABOVE [kg/kg] |
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53 | |
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54 | REAL, INTENT(INOUT), DIMENSION(klon) :: rain !--flux of rain gridbox-mean coming from the layer above [kg/s/m2] |
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55 | REAL, INTENT(INOUT), DIMENSION(klon) :: rainclr !--flux of rain gridbox-mean in clear sky coming from the layer above [kg/s/m2] |
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56 | REAL, INTENT(IN), DIMENSION(klon) :: raincld !--flux of rain gridbox-mean in cloudy air coming from the layer above [kg/s/m2] |
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57 | REAL, INTENT(INOUT), DIMENSION(klon) :: snow !--flux of snow gridbox-mean coming from the layer above [kg/s/m2] |
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58 | REAL, INTENT(INOUT), DIMENSION(klon) :: snowclr !--flux of snow gridbox-mean in clear sky coming from the layer above [kg/s/m2] |
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59 | REAL, INTENT(IN), DIMENSION(klon) :: snowcld !--flux of snow gridbox-mean in cloudy air coming from the layer above [kg/s/m2] |
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60 | |
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61 | REAL, INTENT(OUT), DIMENSION(klon) :: dqreva !--rain tendency due to evaporation [kg/kg/s] |
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62 | REAL, INTENT(OUT), DIMENSION(klon) :: dqssub !--snow tendency due to sublimation [kg/kg/s] |
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63 | |
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64 | |
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65 | !--Integer for interating over klon |
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66 | INTEGER :: i |
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67 | !--dhum_to_dflux: coef to convert a specific quantity variation to a flux variation |
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68 | REAL, DIMENSION(klon) :: dhum_to_dflux |
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69 | !-- |
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70 | REAL, DIMENSION(klon) :: rho, dz |
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71 | |
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72 | !--Saturation values |
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73 | REAL, DIMENSION(klon) :: qzero, qsat, dqsat, qsatl, dqsatl, qsati, dqsati |
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74 | !--Vapor in the clear sky |
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75 | REAL :: qvapclr |
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76 | !--Fluxes tendencies because of evaporation and sublimation |
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77 | REAL :: dprecip_evasub_max, draineva, dsnowsub, dprecip_evasub_tot |
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78 | !--Specific humidity tendencies because of evaporation and sublimation |
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79 | REAL :: dqrevap, dqssubl |
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80 | !--Specific heat constant |
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81 | REAL :: cpair, cpw |
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82 | |
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83 | !--Initialisation |
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84 | qzero(:) = 0. |
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85 | dqreva(:) = 0. |
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86 | dqssub(:) = 0. |
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87 | dqrevap = 0. |
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88 | dqssubl = 0. |
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89 | |
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90 | !-- dhum_to_dflux = rho * dz/dt = 1 / g * dP/dt |
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91 | dhum_to_dflux(:) = ( paprsdn(:) - paprsup(:) ) / RG / dtime |
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92 | rho(:) = pplay(:) / temp(:) / RD |
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93 | dz(:) = ( paprsdn(:) - paprsup(:) ) / RG / rho(:) |
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94 | |
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95 | !--Calculation of saturation specific humidity |
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96 | !--depending on temperature: |
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97 | CALL calc_qsat_ecmwf(klon,temp(:),qzero(:),pplay(:),RTT,0,.FALSE.,qsat(:),dqsat(:)) |
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98 | !--wrt liquid water |
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99 | CALL calc_qsat_ecmwf(klon,temp(:),qzero(:),pplay(:),RTT,1,.FALSE.,qsatl(:),dqsatl(:)) |
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100 | !--wrt ice |
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101 | CALL calc_qsat_ecmwf(klon,temp(:),qzero(:),pplay(:),RTT,2,.FALSE.,qsati(:),dqsati(:)) |
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102 | |
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103 | |
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104 | |
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105 | !--First step consists in "thermalizing" the layer: |
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106 | !--as the flux of precip from layer above "advects" some heat (as the precip is at the temperature |
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107 | !--of the overlying layer) we recalculate a mean temperature that both the air and the precip in the |
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108 | !--layer have. |
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109 | |
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110 | IF (iftop) THEN |
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111 | |
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112 | DO i = 1, klon |
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113 | qprecip(i) = 0. |
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114 | ENDDO |
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115 | |
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116 | ELSE |
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117 | |
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118 | DO i = 1, klon |
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119 | !--No condensed water so cp=cp(vapor+dry air) |
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120 | !-- RVTMP2=rcpv/rcpd-1 |
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121 | cpair = RCPD * ( 1. + RVTMP2 * qvap(i) ) |
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122 | cpw = RCPD * RVTMP2 |
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123 | !--qprecip has to be thermalized with |
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124 | !--layer's air so that precipitation at the ground has the |
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125 | !--same temperature as the lowermost layer |
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126 | !--we convert the flux into a specific quantity qprecip |
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127 | qprecip(i) = ( rain(i) + snow(i) ) / dhum_to_dflux(i) |
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128 | !-- t(i,k+1) + d_t(i,k+1): new temperature of the overlying layer |
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129 | temp(i) = ( tempupnew(i) * qprecip(i) * cpw + cpair * temp(i) ) & |
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130 | / ( cpair + qprecip(i) * cpw ) |
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131 | ENDDO |
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132 | |
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133 | ENDIF |
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134 | |
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135 | ! TODO Probleme : on utilise qvap total dans la maille pour l'evap / sub |
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136 | ! alors qu'on n'evap / sub que dans le ciel clair |
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137 | ! deux options pour cette routine : |
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138 | ! - soit on diagnostique le nuage AVANT l'evap / sub et on estime donc |
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139 | ! la fraction precipitante ciel clair dans la maille, ce qui permet de travailler |
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140 | ! avec des fractions, des fluxs et surtout un qvap dans le ciel clair |
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141 | ! - soit on pousse la param de Ludo au bout, et on prend un qvap de k+1 |
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142 | ! dans le ciel clair, avec un truc comme : |
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143 | ! qvapclr(k) = qvapclr(k+1)/qtot(k+1) * qtot(k) |
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144 | ! UPDATE : on code la seconde version. A voir si on veut mettre la premiere version. |
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145 | |
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146 | |
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147 | DO i = 1, klon |
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148 | |
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149 | !--If there is precipitation from the layer above |
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150 | ! NOTE TODO here we could replace the condition on precipfracclr(i) by a condition |
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151 | ! such as eps or thresh_precip_frac, to remove the senseless barrier in the formulas |
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152 | ! of evap / sublim |
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153 | IF ( ( ( rain(i) + snow(i) ) > 0. ) .AND. ( precipfracclr(i) > 0. ) ) THEN |
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154 | |
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155 | IF ( ok_corr_vap_evasub ) THEN |
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156 | !--Corrected version - we use the same water ratio between |
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157 | !--the clear and the cloudy sky as in the layer above. This |
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158 | !--extends the assumption that the cloud fraction is the same |
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159 | !--as the layer above. This is assumed only for the evap / subl |
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160 | !--process |
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161 | !--Note that qvap(i) is the total water in the gridbox, and |
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162 | !--precipfraccld(i) is the cloud fraction in the layer above |
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163 | qvapclr = qvapclrup(i) / qtotupnew(i) * qvap(i) / ( 1. - precipfraccld(i) ) |
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164 | ELSE |
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165 | !--Legacy version from Ludo - we use the total specific humidity |
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166 | !--for the evap / subl process |
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167 | qvapclr = qvap(i) |
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168 | ENDIF |
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169 | |
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170 | !--Evaporation of liquid precipitation coming from above |
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171 | !--in the clear sky only |
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172 | !--dprecip/dz = -beta*(1-qvap/qsat)*(precip**expo_eva) |
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173 | !--formula from Sundqvist 1988, Klemp & Wilhemson 1978 |
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174 | !--Exact explicit formulation (rainclr is resolved exactly, qvap explicitly) |
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175 | !--which does not need a barrier on rainclr, because included in the formula |
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176 | draineva = precipfracclr(i) * ( MAX(0., & |
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177 | - coef_eva * ( 1. - expo_eva ) * (1. - qvapclr / qsatl(i)) * dz(i) & |
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178 | + ( rainclr(i) / MAX(thresh_precip_frac, precipfracclr(i)) )**( 1. - expo_eva ) & |
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179 | ) )**( 1. / ( 1. - expo_eva ) ) - rainclr(i) |
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180 | |
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181 | !--Evaporation is limited by 0 |
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182 | draineva = MIN(0., draineva) |
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183 | |
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184 | |
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185 | !--Sublimation of the solid precipitation coming from above |
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186 | !--(same formula as for liquid precip) |
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187 | !--Exact explicit formulation (snowclr is resolved exactly, qvap explicitly) |
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188 | !--which does not need a barrier on snowclr, because included in the formula |
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189 | dsnowsub = precipfracclr(i) * ( MAX(0., & |
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190 | - coef_sub * ( 1. - expo_sub ) * (1. - qvapclr / qsati(i)) * dz(i) & |
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191 | + ( snowclr(i) / MAX(thresh_precip_frac, precipfracclr(i)) )**( 1. - expo_sub ) & |
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192 | ) )**( 1. / ( 1. - expo_sub ) ) - snowclr(i) |
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193 | |
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194 | !--Sublimation is limited by 0 |
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195 | ! TODO: change max when we will allow for vapor deposition in supersaturated regions |
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196 | dsnowsub = MIN(0., dsnowsub) |
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197 | |
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198 | !--Evaporation limit: we ensure that the layer's fraction below |
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199 | !--the clear sky does not reach saturation. In this case, we |
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200 | !--redistribute the maximum flux dprecip_evasub_max conserving the ratio liquid/ice |
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201 | !--Max evaporation is computed not to saturate the clear sky precip fraction |
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202 | !--(i.e., the fraction where evaporation occurs) |
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203 | !--It is expressed as a max flux dprecip_evasub_max |
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204 | |
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205 | dprecip_evasub_max = MIN(0., ( qvapclr - qsat(i) ) * precipfracclr(i)) & |
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206 | * dhum_to_dflux(i) |
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207 | dprecip_evasub_tot = draineva + dsnowsub |
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208 | |
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209 | !--Barriers |
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210 | !--If activates if the total is LOWER than the max because |
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211 | !--everything is negative |
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212 | IF ( dprecip_evasub_tot < dprecip_evasub_max ) THEN |
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213 | draineva = dprecip_evasub_max * draineva / dprecip_evasub_tot |
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214 | dsnowsub = dprecip_evasub_max * dsnowsub / dprecip_evasub_tot |
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215 | ENDIF |
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216 | |
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217 | |
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218 | !--New solid and liquid precipitation fluxes after evap and sublimation |
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219 | dqrevap = draineva / dhum_to_dflux(i) |
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220 | dqssubl = dsnowsub / dhum_to_dflux(i) |
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221 | |
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222 | |
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223 | !--Vapor is updated after evaporation/sublimation (it is increased) |
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224 | qvap(i) = qvap(i) - dqrevap - dqssubl |
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225 | !--qprecip is the total condensed water in the precip flux (it is decreased) |
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226 | qprecip(i) = qprecip(i) + dqrevap + dqssubl |
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227 | !--Air and precip temperature (i.e., gridbox temperature) |
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228 | !--is updated due to latent heat cooling |
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229 | temp(i) = temp(i) & |
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230 | + dqrevap * RLVTT / RCPD & |
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231 | / ( 1. + RVTMP2 * ( qvap(i) + qprecip(i) ) ) & |
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232 | + dqssubl * RLSTT / RCPD & |
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233 | / ( 1. + RVTMP2 * ( qvap(i) + qprecip(i) ) ) |
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234 | |
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235 | !--Add tendencies |
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236 | !--The MAX is needed because in some cases, the flux can be slightly negative (numerical precision) |
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237 | rainclr(i) = MAX(0., rainclr(i) + draineva) |
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238 | snowclr(i) = MAX(0., snowclr(i) + dsnowsub) |
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239 | |
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240 | !--If there is no more precip fluxes, the precipitation fraction in clear |
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241 | !--sky is set to 0 |
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242 | IF ( ( rainclr(i) + snowclr(i) ) <= 0. ) precipfracclr(i) = 0. |
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243 | |
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244 | !--Calculation of the total fluxes |
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245 | rain(i) = rainclr(i) + raincld(i) |
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246 | snow(i) = snowclr(i) + snowcld(i) |
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247 | |
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248 | ELSEIF ( ( rain(i) + snow(i) ) <= 0. ) THEN |
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249 | !--If no precip, we reinitialize the cloud fraction used for the precip to 0 |
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250 | precipfraccld(i) = 0. |
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251 | precipfracclr(i) = 0. |
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252 | |
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253 | ENDIF ! ( ( rain(i) + snow(i) ) .GT. 0. ) |
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254 | |
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255 | !--Diagnostic tendencies |
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256 | dqssub(i) = dqssubl / dtime |
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257 | dqreva(i) = dqrevap / dtime |
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258 | |
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259 | ENDDO ! loop on klon |
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260 | |
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261 | |
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262 | END SUBROUTINE poprecip_precld |
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263 | |
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264 | !---------------------------------------------------------------- |
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265 | ! Computes the processes-oriented precipitation formulations for |
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266 | ! - autoconversion (auto) via a deposition process |
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267 | ! - aggregation (agg) |
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268 | ! - riming (rim) |
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269 | ! - collection (col) |
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270 | ! - melting (melt) |
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271 | ! - freezing (freez) |
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272 | |
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273 | SUBROUTINE poprecip_postcld( & |
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274 | klon, dtime, paprsdn, paprsup, pplay, ctot_vol, ptconv, & |
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275 | temp, qvap, qliq, qice, icefrac, cldfra, & |
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276 | precipfracclr, precipfraccld, & |
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277 | rain, rainclr, raincld, snow, snowclr, snowcld, & |
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278 | qraindiag, qsnowdiag, dqrauto, dqrcol, dqrmelt, dqrfreez, & |
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279 | dqsauto, dqsagg, dqsrim, dqsmelt, dqsfreez) |
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280 | |
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281 | USE lmdz_lscp_ini, ONLY: prt_level, lunout |
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282 | USE lmdz_lscp_ini, ONLY: RCPD, RLSTT, RLVTT, RLMLT, RVTMP2, RTT, RD, RG, RPI |
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283 | USE lmdz_lscp_tools, ONLY: calc_qsat_ecmwf |
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284 | |
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285 | USE lmdz_lscp_ini, ONLY: cld_lc_con, cld_tau_con, cld_expo_con, seuil_neb, & |
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286 | cld_lc_lsc, cld_tau_lsc, cld_expo_lsc, rain_int_min, & |
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287 | thresh_precip_frac, gamma_col, gamma_agg, gamma_rim, & |
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288 | rho_rain, r_rain, r_snow, rho_ice, & |
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289 | tau_auto_snow_min, tau_auto_snow_max, & |
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290 | thresh_precip_frac, eps, & |
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291 | gamma_melt, alpha_freez, beta_freez, temp_nowater, & |
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292 | iflag_cloudth_vert, iflag_rain_incloud_vol, & |
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293 | cld_lc_lsc_snow, cld_lc_con_snow, gamma_freez, & |
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294 | rain_fallspeed_clr, rain_fallspeed_cld, & |
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295 | snow_fallspeed_clr, snow_fallspeed_cld |
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296 | |
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297 | |
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298 | IMPLICIT NONE |
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299 | |
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300 | INTEGER, INTENT(IN) :: klon !--number of horizontal grid points [-] |
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301 | REAL, INTENT(IN) :: dtime !--time step [s] |
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302 | |
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303 | REAL, INTENT(IN), DIMENSION(klon) :: paprsdn !--pressure at the bottom interface of the layer [Pa] |
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304 | REAL, INTENT(IN), DIMENSION(klon) :: paprsup !--pressure at the top interface of the layer [Pa] |
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305 | REAL, INTENT(IN), DIMENSION(klon) :: pplay !--pressure in the middle of the layer [Pa] |
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306 | |
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307 | REAL, INTENT(IN), DIMENSION(klon) :: ctot_vol !--volumic cloud fraction [-] |
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308 | LOGICAL, INTENT(IN), DIMENSION(klon) :: ptconv !--true if we are in a convective point |
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309 | |
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310 | REAL, INTENT(INOUT), DIMENSION(klon) :: temp !--current temperature [K] |
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311 | REAL, INTENT(INOUT), DIMENSION(klon) :: qvap !--current water vapor specific humidity [kg/kg] |
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312 | REAL, INTENT(INOUT), DIMENSION(klon) :: qliq !--current liquid water specific humidity [kg/kg] |
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313 | REAL, INTENT(INOUT), DIMENSION(klon) :: qice !--current ice water specific humidity [kg/kg] |
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314 | REAL, INTENT(IN), DIMENSION(klon) :: icefrac !--ice fraction [-] |
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315 | REAL, INTENT(IN), DIMENSION(klon) :: cldfra !--cloud fraction [-] |
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316 | |
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317 | REAL, INTENT(INOUT), DIMENSION(klon) :: precipfracclr !--fraction of precipitation in the clear sky IN THE LAYER ABOVE [-] |
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318 | REAL, INTENT(INOUT), DIMENSION(klon) :: precipfraccld !--fraction of precipitation in the cloudy air IN THE LAYER ABOVE [-] |
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319 | !--NB. at the end of the routine, becomes the fraction of precip |
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320 | !--in the current layer |
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321 | |
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322 | REAL, INTENT(INOUT), DIMENSION(klon) :: rain !--flux of rain gridbox-mean coming from the layer above [kg/s/m2] |
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323 | REAL, INTENT(INOUT), DIMENSION(klon) :: rainclr !--flux of rain gridbox-mean in clear sky coming from the layer above [kg/s/m2] |
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324 | REAL, INTENT(INOUT), DIMENSION(klon) :: raincld !--flux of rain gridbox-mean in cloudy air coming from the layer above [kg/s/m2] |
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325 | REAL, INTENT(INOUT), DIMENSION(klon) :: snow !--flux of snow gridbox-mean coming from the layer above [kg/s/m2] |
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326 | REAL, INTENT(INOUT), DIMENSION(klon) :: snowclr !--flux of snow gridbox-mean in clear sky coming from the layer above [kg/s/m2] |
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327 | REAL, INTENT(INOUT), DIMENSION(klon) :: snowcld !--flux of snow gridbox-mean in cloudy air coming from the layer above [kg/s/m2] |
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328 | |
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329 | REAL, INTENT(OUT), DIMENSION(klon) :: qraindiag !--DIAGNOSTIC specific rain content [kg/kg] |
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330 | REAL, INTENT(OUT), DIMENSION(klon) :: qsnowdiag !--DIAGNOSTIC specific snow content [kg/kg] |
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331 | REAL, INTENT(OUT), DIMENSION(klon) :: dqrcol !--rain tendendy due to collection by rain of liquid cloud droplets [kg/kg/s] |
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332 | REAL, INTENT(OUT), DIMENSION(klon) :: dqsagg !--snow tendency due to collection of lcoud ice by aggregation [kg/kg/s] |
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333 | REAL, INTENT(OUT), DIMENSION(klon) :: dqrauto !--rain tendency due to autoconversion of cloud liquid [kg/kg/s] |
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334 | REAL, INTENT(OUT), DIMENSION(klon) :: dqsauto !--snow tendency due to autoconversion of cloud ice [kg/kg/s] |
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335 | REAL, INTENT(OUT), DIMENSION(klon) :: dqsrim !--snow tendency due to riming [kg/kg/s] |
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336 | REAL, INTENT(OUT), DIMENSION(klon) :: dqsmelt !--snow tendency due to melting [kg/kg/s] |
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337 | REAL, INTENT(OUT), DIMENSION(klon) :: dqrmelt !--rain tendency due to melting [kg/kg/s] |
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338 | REAL, INTENT(OUT), DIMENSION(klon) :: dqsfreez !--snow tendency due to freezing [kg/kg/s] |
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339 | REAL, INTENT(OUT), DIMENSION(klon) :: dqrfreez !--rain tendency due to freezing [kg/kg/s] |
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340 | |
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341 | |
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342 | |
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343 | !--Local variables |
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344 | |
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345 | INTEGER :: i |
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346 | !--dhum_to_dflux: coef to convert a specific quantity variation to a flux variation |
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347 | REAL, DIMENSION(klon) :: dhum_to_dflux |
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348 | REAL, DIMENSION(klon) :: qtot !--includes vap, liq, ice and precip |
---|
349 | |
---|
350 | !--Partition of the fluxes |
---|
351 | REAL :: dcldfra |
---|
352 | REAL :: precipfractot |
---|
353 | REAL :: dprecipfracclr, dprecipfraccld |
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354 | REAL :: drainclr, dsnowclr |
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355 | REAL :: draincld, dsnowcld |
---|
356 | |
---|
357 | !--Collection, aggregation and riming |
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358 | REAL :: eff_cldfra |
---|
359 | REAL :: coef_col, coef_agg, coef_rim, coef_tmp, qrain_tmp |
---|
360 | REAL :: Eff_rain_liq, Eff_snow_ice, Eff_snow_liq |
---|
361 | REAL :: rho_snow |
---|
362 | REAL :: dqlcol !--loss of liquid cloud content due to collection by rain [kg/kg/s] |
---|
363 | REAL :: dqiagg !--loss of ice cloud content due to collection by aggregation [kg/kg/s] |
---|
364 | REAL :: dqlrim !--loss of liquid cloud content due to riming on snow [kg/kg/s] |
---|
365 | |
---|
366 | !--Autoconversion |
---|
367 | REAL :: qthresh_auto_rain, tau_auto_rain, expo_auto_rain |
---|
368 | REAL :: qthresh_auto_snow, tau_auto_snow, expo_auto_snow |
---|
369 | REAL :: dqlauto !--loss of liquid cloud content due to autoconversion to rain [kg/kg/s] |
---|
370 | REAL :: dqiauto !--loss of ice cloud content due to autoconversion to snow [kg/kg/s] |
---|
371 | |
---|
372 | !--Melting |
---|
373 | REAL :: dqsmelt_max, air_thermal_conduct |
---|
374 | REAL :: nb_snowflake_clr, nb_snowflake_cld |
---|
375 | REAL :: capa_snowflake, temp_wetbulb |
---|
376 | REAL :: rho, r_ice |
---|
377 | REAL :: dqsclrmelt, dqscldmelt, dqstotmelt |
---|
378 | REAL, DIMENSION(klon) :: qzero, qsat, dqsat |
---|
379 | |
---|
380 | !--Freezing |
---|
381 | REAL :: dqrfreez_max |
---|
382 | REAL :: tau_freez |
---|
383 | REAL :: dqrclrfreez, dqrcldfreez, dqrtotfreez, dqrtotfreez_step1, dqrtotfreez_step2 |
---|
384 | REAL :: coef_freez |
---|
385 | REAL :: dqifreez !--loss of ice cloud content due to collection of ice from rain [kg/kg/s] |
---|
386 | REAL :: Eff_rain_ice |
---|
387 | |
---|
388 | |
---|
389 | !--Initialisation of variables |
---|
390 | |
---|
391 | |
---|
392 | qzero(:) = 0. |
---|
393 | |
---|
394 | dqrcol(:) = 0. |
---|
395 | dqsagg(:) = 0. |
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396 | dqsauto(:) = 0. |
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397 | dqrauto(:) = 0. |
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398 | dqsrim(:) = 0. |
---|
399 | dqrmelt(:) = 0. |
---|
400 | dqsmelt(:) = 0. |
---|
401 | dqrfreez(:) = 0. |
---|
402 | dqsfreez(:) = 0. |
---|
403 | |
---|
404 | |
---|
405 | DO i = 1, klon |
---|
406 | |
---|
407 | !--Variables initialisation |
---|
408 | dqlcol = 0. |
---|
409 | dqiagg = 0. |
---|
410 | dqiauto = 0. |
---|
411 | dqlauto = 0. |
---|
412 | dqlrim = 0. |
---|
413 | |
---|
414 | !-- dhum_to_dflux = rho * dz/dt = 1 / g * dP/dt |
---|
415 | dhum_to_dflux(i) = ( paprsdn(i) - paprsup(i) ) / RG / dtime |
---|
416 | qtot(i) = qvap(i) + qliq(i) + qice(i) & |
---|
417 | + ( raincld(i) + rainclr(i) + snowcld(i) + snowclr(i) ) / dhum_to_dflux(i) |
---|
418 | |
---|
419 | !------------------------------------------------------------ |
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420 | !-- PRECIPITATION FRACTIONS UPDATE |
---|
421 | !------------------------------------------------------------ |
---|
422 | !--The goal of this routine is to reattribute precipitation fractions |
---|
423 | !--and fluxes to clear or cloudy air, depending on the variation of |
---|
424 | !--the cloud fraction on the vertical dimension. We assume a |
---|
425 | !--maximum-random overlap of the cloud cover (see Jakob and Klein, 2000, |
---|
426 | !--and LTP thesis, 2021) |
---|
427 | !--NB. in fact, we assume a maximum-random overlap of the total precip. frac |
---|
428 | |
---|
429 | !--Initialisation |
---|
430 | precipfractot = precipfracclr(i) + precipfraccld(i) |
---|
431 | |
---|
432 | !--Instead of using the cloud cover which was use in LTP thesis, we use the |
---|
433 | !--total precip. fraction to compute the maximum-random overlap. This is |
---|
434 | !--because all the information of the cloud cover is embedded into |
---|
435 | !--precipfractot, and this allows for taking into account the potential |
---|
436 | !--reduction of the precipitation fraction because either the flux is too |
---|
437 | !--small (see barrier at the end of poprecip_postcld) or the flux is completely |
---|
438 | !--evaporated (see barrier at the end of poprecip_precld) |
---|
439 | !--NB. precipfraccld(i) is here the cloud fraction of the layer above |
---|
440 | !precipfractot = 1. - ( 1. - precipfractot ) * & |
---|
441 | ! ( 1. - MAX( cldfra(i), precipfraccld(i) ) ) & |
---|
442 | ! / ( 1. - MIN( precipfraccld(i), 1. - eps ) ) |
---|
443 | |
---|
444 | |
---|
445 | IF ( precipfraccld(i) > ( 1. - eps ) ) THEN |
---|
446 | precipfractot = 1. |
---|
447 | ELSE |
---|
448 | precipfractot = 1. - ( 1. - precipfractot ) * & |
---|
449 | ( 1. - MAX( cldfra(i), precipfraccld(i) ) ) & |
---|
450 | / ( 1. - precipfraccld(i) ) |
---|
451 | ENDIF |
---|
452 | |
---|
453 | !--precipfraccld(i) is here the cloud fraction of the layer above |
---|
454 | dcldfra = cldfra(i) - precipfraccld(i) |
---|
455 | !--Tendency of the clear-sky precipitation fraction. We add a MAX on the |
---|
456 | !--calculation of the current CS precip. frac. |
---|
457 | !dprecipfracclr = MAX( 0., ( precipfractot - cldfra(i) ) ) - precipfracclr(i) |
---|
458 | !--We remove it, because precipfractot is guaranteed to be > cldfra (the MAX is activated |
---|
459 | !--if precipfractot < cldfra) |
---|
460 | dprecipfracclr = ( precipfractot - cldfra(i) ) - precipfracclr(i) |
---|
461 | !--Tendency of the cloudy precipitation fraction. We add a MAX on the |
---|
462 | !--calculation of the current CS precip. frac. |
---|
463 | !dprecipfraccld = MAX( dcldfra , - precipfraccld(i) ) |
---|
464 | !--We remove it, because cldfra is guaranteed to be > 0 (the MAX is activated |
---|
465 | !--if cldfra < 0) |
---|
466 | dprecipfraccld = dcldfra |
---|
467 | |
---|
468 | |
---|
469 | !--If the cloud extends |
---|
470 | IF ( dprecipfraccld > 0. ) THEN |
---|
471 | !--If there is no CS precip, nothing happens. |
---|
472 | !--If there is, we reattribute some of the CS precip flux |
---|
473 | !--to the cloud precip flux, proportionnally to the |
---|
474 | !--decrease of the CS precip fraction |
---|
475 | IF ( precipfracclr(i) <= 0. ) THEN |
---|
476 | drainclr = 0. |
---|
477 | dsnowclr = 0. |
---|
478 | ELSE |
---|
479 | drainclr = dprecipfracclr / precipfracclr(i) * rainclr(i) |
---|
480 | dsnowclr = dprecipfracclr / precipfracclr(i) * snowclr(i) |
---|
481 | ENDIF |
---|
482 | !--If the cloud narrows |
---|
483 | ELSEIF ( dprecipfraccld < 0. ) THEN |
---|
484 | !--We reattribute some of the cloudy precip flux |
---|
485 | !--to the CS precip flux, proportionnally to the |
---|
486 | !--decrease of the cloud precip fraction |
---|
487 | draincld = dprecipfraccld / precipfraccld(i) * raincld(i) |
---|
488 | dsnowcld = dprecipfraccld / precipfraccld(i) * snowcld(i) |
---|
489 | drainclr = - draincld |
---|
490 | dsnowclr = - dsnowcld |
---|
491 | !--If the cloud stays the same or if there is no cloud above and |
---|
492 | !--in the current layer, nothing happens |
---|
493 | ELSE |
---|
494 | drainclr = 0. |
---|
495 | dsnowclr = 0. |
---|
496 | ENDIF |
---|
497 | |
---|
498 | !--We add the tendencies |
---|
499 | !--The MAX is needed because in some cases, the flux can be slightly negative (numerical precision) |
---|
500 | precipfraccld(i) = precipfraccld(i) + dprecipfraccld |
---|
501 | precipfracclr(i) = precipfracclr(i) + dprecipfracclr |
---|
502 | rainclr(i) = MAX(0., rainclr(i) + drainclr) |
---|
503 | snowclr(i) = MAX(0., snowclr(i) + dsnowclr) |
---|
504 | raincld(i) = MAX(0., raincld(i) - drainclr) |
---|
505 | snowcld(i) = MAX(0., snowcld(i) - dsnowclr) |
---|
506 | |
---|
507 | !--If vertical heterogeneity is taken into account, we use |
---|
508 | !--the "true" volume fraction instead of a modified |
---|
509 | !--surface fraction (which is larger and artificially |
---|
510 | !--reduces the in-cloud water). |
---|
511 | IF ( ( iflag_cloudth_vert >= 3 ) .AND. ( iflag_rain_incloud_vol == 1 ) ) THEN |
---|
512 | eff_cldfra = ctot_vol(i) |
---|
513 | ELSE |
---|
514 | eff_cldfra = cldfra(i) |
---|
515 | ENDIF |
---|
516 | |
---|
517 | |
---|
518 | !--Start precipitation growth processes |
---|
519 | |
---|
520 | !--If the cloud is big enough, the precipitation processes activate |
---|
521 | ! TODO met on seuil_neb ici ? |
---|
522 | IF ( cldfra(i) >= seuil_neb ) THEN |
---|
523 | |
---|
524 | !--------------------------------------------------------- |
---|
525 | !-- COLLECTION AND AGGREGATION |
---|
526 | !--------------------------------------------------------- |
---|
527 | !--Collection: processus through which rain collects small liquid droplets |
---|
528 | !--in suspension, and add it to the rain flux |
---|
529 | !--Aggregation: same for snow (precip flux) and ice crystals (in suspension) |
---|
530 | !--Those processes are treated before autoconversion because we do not |
---|
531 | !--want to collect/aggregate the newly formed fluxes, which already |
---|
532 | !--"saw" the cloud as they come from it |
---|
533 | !--The formulas come from Muench and Lohmann 2020 |
---|
534 | |
---|
535 | !--gamma_col: tuning coefficient [-] |
---|
536 | !--rho_rain: volumic mass of rain [kg/m3] |
---|
537 | !--r_rain: size of the rain droplets [m] |
---|
538 | !--Eff_rain_liq: efficiency of the collection process [-] (between 0 and 1) |
---|
539 | !--dqlcol is a gridbox-mean quantity, as is qliq and raincld. They are |
---|
540 | !--divided by respectively eff_cldfra, eff_cldfra and precipfraccld to |
---|
541 | !--get in-cloud mean quantities. The two divisions by eff_cldfra are |
---|
542 | !--then simplified. |
---|
543 | |
---|
544 | !--The collection efficiency is perfect. |
---|
545 | Eff_rain_liq = 1. |
---|
546 | coef_col = gamma_col * 3. / 4. / rho_rain / r_rain * Eff_rain_liq |
---|
547 | IF ( raincld(i) > 0. ) THEN |
---|
548 | !--Exact explicit version, which does not need a barrier because of |
---|
549 | !--the exponential decrease |
---|
550 | dqlcol = qliq(i) * ( EXP( - dtime * coef_col * raincld(i) / precipfraccld(i) ) - 1. ) |
---|
551 | |
---|
552 | !--Add tendencies |
---|
553 | qliq(i) = qliq(i) + dqlcol |
---|
554 | raincld(i) = raincld(i) - dqlcol * dhum_to_dflux(i) |
---|
555 | |
---|
556 | !--Diagnostic tendencies |
---|
557 | dqrcol(i) = - dqlcol / dtime |
---|
558 | ENDIF |
---|
559 | |
---|
560 | !--Same as for aggregation |
---|
561 | !--Eff_snow_liq formula: |
---|
562 | !--it s a product of a collection efficiency and a sticking efficiency |
---|
563 | ! Milbrandt and Yau formula that gives very low values: |
---|
564 | ! Eff_snow_ice = 0.05 * EXP( 0.1 * ( temp(i) - RTT ) ) |
---|
565 | ! Lin 1983's formula |
---|
566 | Eff_snow_ice = EXP( 0.025 * MIN( ( temp(i) - RTT ), 0.) ) |
---|
567 | !--rho_snow formula follows Brandes et al. 2007 (JAMC) |
---|
568 | rho_snow = 1.e3 * 0.178 * ( r_snow * 2. * 1000. )**(-0.922) |
---|
569 | coef_agg = gamma_agg * 3. / 4. / rho_snow / r_snow * Eff_snow_ice |
---|
570 | IF ( snowcld(i) > 0. ) THEN |
---|
571 | !--Exact explicit version, which does not need a barrier because of |
---|
572 | !--the exponential decrease |
---|
573 | dqiagg = qice(i) * ( EXP( - dtime * coef_agg * snowcld(i) / precipfraccld(i) ) - 1. ) |
---|
574 | |
---|
575 | !--Add tendencies |
---|
576 | qice(i) = qice(i) + dqiagg |
---|
577 | snowcld(i) = snowcld(i) - dqiagg * dhum_to_dflux(i) |
---|
578 | |
---|
579 | !--Diagnostic tendencies |
---|
580 | dqsagg(i) = - dqiagg / dtime |
---|
581 | ENDIF |
---|
582 | |
---|
583 | |
---|
584 | !--------------------------------------------------------- |
---|
585 | !-- AUTOCONVERSION |
---|
586 | !--------------------------------------------------------- |
---|
587 | !--Autoconversion converts liquid droplets/ice crystals into |
---|
588 | !--rain drops/snowflakes. It relies on the formulations by |
---|
589 | !--Sundqvist 1978. |
---|
590 | |
---|
591 | !--If we are in a convective point, we have different parameters |
---|
592 | !--for the autoconversion |
---|
593 | IF ( ptconv(i) ) THEN |
---|
594 | qthresh_auto_rain = cld_lc_con |
---|
595 | qthresh_auto_snow = cld_lc_con_snow |
---|
596 | |
---|
597 | tau_auto_rain = cld_tau_con |
---|
598 | !--tau for snow depends on the ice fraction in mixed-phase clouds |
---|
599 | tau_auto_snow = tau_auto_snow_max & |
---|
600 | + ( tau_auto_snow_min - tau_auto_snow_max ) * ( 1. - icefrac(i) ) |
---|
601 | |
---|
602 | expo_auto_rain = cld_expo_con |
---|
603 | expo_auto_snow = cld_expo_con |
---|
604 | ELSE |
---|
605 | qthresh_auto_rain = cld_lc_lsc |
---|
606 | qthresh_auto_snow = cld_lc_lsc_snow |
---|
607 | |
---|
608 | tau_auto_rain = cld_tau_lsc |
---|
609 | !--tau for snow depends on the ice fraction in mixed-phase clouds |
---|
610 | tau_auto_snow = tau_auto_snow_max & |
---|
611 | + ( tau_auto_snow_min - tau_auto_snow_max ) * ( 1. - icefrac(i) ) |
---|
612 | |
---|
613 | expo_auto_rain = cld_expo_lsc |
---|
614 | expo_auto_snow = cld_expo_lsc |
---|
615 | ENDIF |
---|
616 | |
---|
617 | |
---|
618 | ! Liquid water quantity to remove according to (Sundqvist, 1978) |
---|
619 | ! dqliq/dt = -qliq/tau * ( 1-exp(-(qliqincld/qthresh)**2) ) |
---|
620 | |
---|
621 | !--And same formula for ice |
---|
622 | |
---|
623 | !--We first treat the second term (with exponential) in an explicit way |
---|
624 | !--and then treat the first term (-q/tau) in an exact way |
---|
625 | |
---|
626 | dqlauto = - qliq(i) * ( 1. - exp( - dtime / tau_auto_rain * ( 1. - exp( & |
---|
627 | - ( qliq(i) / eff_cldfra / qthresh_auto_rain ) ** expo_auto_rain ) ) ) ) |
---|
628 | |
---|
629 | dqiauto = - qice(i) * ( 1. - exp( - dtime / tau_auto_snow * ( 1. - exp( & |
---|
630 | - ( qice(i) / eff_cldfra / qthresh_auto_snow ) ** expo_auto_snow ) ) ) ) |
---|
631 | |
---|
632 | |
---|
633 | !--Barriers so that we don't create more rain/snow |
---|
634 | !--than there is liquid/ice |
---|
635 | dqlauto = MAX( - qliq(i), dqlauto ) |
---|
636 | dqiauto = MAX( - qice(i), dqiauto ) |
---|
637 | |
---|
638 | !--Add tendencies |
---|
639 | qliq(i) = qliq(i) + dqlauto |
---|
640 | qice(i) = qice(i) + dqiauto |
---|
641 | raincld(i) = raincld(i) - dqlauto * dhum_to_dflux(i) |
---|
642 | snowcld(i) = snowcld(i) - dqiauto * dhum_to_dflux(i) |
---|
643 | |
---|
644 | !--Diagnostic tendencies |
---|
645 | dqsauto(i) = - dqiauto / dtime |
---|
646 | dqrauto(i) = - dqlauto / dtime |
---|
647 | |
---|
648 | |
---|
649 | !--------------------------------------------------------- |
---|
650 | !-- RIMING |
---|
651 | !--------------------------------------------------------- |
---|
652 | !--Process which converts liquid droplets in suspension into |
---|
653 | !--snow because of the collision between |
---|
654 | !--those and falling snowflakes. |
---|
655 | !--The formula comes from Muench and Lohmann 2020 |
---|
656 | !--NB.: this process needs a temperature adjustment |
---|
657 | |
---|
658 | !--Eff_snow_liq formula: following Ferrier 1994, |
---|
659 | !--assuming 1 |
---|
660 | Eff_snow_liq = 1.0 |
---|
661 | !--rho_snow formula follows Brandes et al. 2007 (JAMC) |
---|
662 | rho_snow = 1.e3 * 0.178 * ( r_snow * 2. * 1000. )**(-0.922) |
---|
663 | coef_rim = gamma_rim * 3. / 4. / rho_snow / r_snow * Eff_snow_liq |
---|
664 | IF ( snowcld(i) > 0. ) THEN |
---|
665 | !--Exact version, which does not need a barrier because of |
---|
666 | !--the exponential decrease |
---|
667 | dqlrim = qliq(i) * ( EXP( - dtime * coef_rim * snowcld(i) / precipfraccld(i) ) - 1. ) |
---|
668 | |
---|
669 | !--Add tendencies |
---|
670 | !--The MAX is needed because in some cases, the flux can be slightly negative (numerical precision) |
---|
671 | qliq(i) = qliq(i) + dqlrim |
---|
672 | snowcld(i) = snowcld(i) - dqlrim * dhum_to_dflux(i) |
---|
673 | |
---|
674 | !--Temperature adjustment with the release of latent |
---|
675 | !--heat because of solid condensation |
---|
676 | temp(i) = temp(i) - dqlrim * RLMLT / RCPD & |
---|
677 | / ( 1. + RVTMP2 * qtot(i) ) |
---|
678 | |
---|
679 | !--Diagnostic tendencies |
---|
680 | dqsrim(i) = - dqlrim / dtime |
---|
681 | ENDIF |
---|
682 | |
---|
683 | ENDIF ! cldfra .GE. seuil_neb |
---|
684 | |
---|
685 | ENDDO ! loop on klon |
---|
686 | |
---|
687 | |
---|
688 | !--Re-calculation of saturation specific humidity |
---|
689 | !--because riming changed temperature |
---|
690 | CALL calc_qsat_ecmwf(klon, temp, qzero, pplay, RTT, 0, .FALSE., qsat, dqsat) |
---|
691 | |
---|
692 | DO i = 1, klon |
---|
693 | |
---|
694 | !--------------------------------------------------------- |
---|
695 | !-- MELTING |
---|
696 | !--------------------------------------------------------- |
---|
697 | !--Process through which snow melts into rain. |
---|
698 | !--The formula is homemade. |
---|
699 | !--NB.: this process needs a temperature adjustment |
---|
700 | |
---|
701 | !--dqsmelt_max : maximum snow melting so that temperature |
---|
702 | !-- stays higher than 273 K [kg/kg] |
---|
703 | !--capa_snowflake : capacitance of a snowflake, equal to |
---|
704 | !-- the radius if the snowflake is a sphere [m] |
---|
705 | !--temp_wetbulb : wet-bulb temperature [K] |
---|
706 | !--snow_fallspeed : snow fall velocity (in clear/cloudy sky) [m/s] |
---|
707 | !--air_thermal_conduct : thermal conductivity of the air [J/m/K/s] |
---|
708 | !--gamma_melt : tuning parameter for melting [-] |
---|
709 | !--nb_snowflake : number of snowflakes (in clear/cloudy air) [-] |
---|
710 | |
---|
711 | IF ( ( snowclr(i) + snowcld(i) ) > 0. ) THEN |
---|
712 | !--Computed according to |
---|
713 | !--Cpdry * Delta T * (1 + (Cpvap/Cpdry - 1) * qtot) = Lfusion * Delta q |
---|
714 | dqsmelt_max = MIN(0., ( RTT - temp(i) ) / RLMLT * RCPD & |
---|
715 | * ( 1. + RVTMP2 * qtot(i) )) |
---|
716 | |
---|
717 | !--Initialisation |
---|
718 | dqsclrmelt = 0. |
---|
719 | dqscldmelt = 0. |
---|
720 | |
---|
721 | !--We assume that the snowflakes are spherical |
---|
722 | capa_snowflake = r_snow |
---|
723 | !--Thermal conductivity of the air, empirical formula from Beard and Pruppacher (1971) |
---|
724 | air_thermal_conduct = ( 5.69 + 0.017 * ( temp(i) - RTT ) ) * 1.e-3 * 4.184 |
---|
725 | !--rho_snow formula follows Brandes et al. 2007 (JAMC) |
---|
726 | rho_snow = 1.e3 * 0.178 * ( r_snow * 2. * 1000. )**(-0.922) |
---|
727 | |
---|
728 | !--In clear air |
---|
729 | IF ( ( snowclr(i) > 0. ) .AND. ( precipfracclr(i) > 0. ) ) THEN |
---|
730 | !--Formula for the wet-bulb temperature from ECMWF (IFS) |
---|
731 | !--The vapor used is the vapor in the clear sky |
---|
732 | temp_wetbulb = temp(i) & |
---|
733 | - ( qsat(i) - ( qvap(i) - cldfra(i) * qsat(i) ) / ( 1. - cldfra(i) ) ) & |
---|
734 | * ( 1329.31 + 0.0074615 * ( pplay(i) - 0.85e5 ) & |
---|
735 | - 40.637 * ( temp(i) - 275. ) ) |
---|
736 | !--Calculated according to |
---|
737 | !-- flux = velocity_snowflakes * nb_snowflakes * volume_snowflakes * rho_snow |
---|
738 | nb_snowflake_clr = snowclr(i) / precipfracclr(i) / snow_fallspeed_clr & |
---|
739 | / ( 4. / 3. * RPI * r_snow**3. * rho_snow ) |
---|
740 | dqsclrmelt = - nb_snowflake_clr * 4. * RPI * air_thermal_conduct & |
---|
741 | * capa_snowflake / RLMLT * gamma_melt & |
---|
742 | * MAX(0., temp_wetbulb - RTT) * dtime |
---|
743 | |
---|
744 | !--Barrier to limit the melting flux to the clr snow flux in the mesh |
---|
745 | dqsclrmelt = MAX( dqsclrmelt , -snowclr(i) / dhum_to_dflux(i)) |
---|
746 | ENDIF |
---|
747 | |
---|
748 | |
---|
749 | !--In cloudy air |
---|
750 | IF ( ( snowcld(i) > 0. ) .AND. ( precipfraccld(i) > 0. ) ) THEN |
---|
751 | !--As the air is saturated, the wet-bulb temperature is equal to the |
---|
752 | !--temperature |
---|
753 | temp_wetbulb = temp(i) |
---|
754 | !--Calculated according to |
---|
755 | !-- flux = velocity_snowflakes * nb_snowflakes * volume_snowflakes * rho_snow |
---|
756 | nb_snowflake_cld = snowcld(i) / precipfraccld(i) / snow_fallspeed_cld & |
---|
757 | / ( 4. / 3. * RPI * r_snow**3. * rho_snow ) |
---|
758 | dqscldmelt = - nb_snowflake_cld * 4. * RPI * air_thermal_conduct & |
---|
759 | * capa_snowflake / RLMLT * gamma_melt & |
---|
760 | * MAX(0., temp_wetbulb - RTT) * dtime |
---|
761 | |
---|
762 | !--Barrier to limit the melting flux to the cld snow flux in the mesh |
---|
763 | dqscldmelt = MAX(dqscldmelt , - snowcld(i) / dhum_to_dflux(i)) |
---|
764 | ENDIF |
---|
765 | |
---|
766 | |
---|
767 | !--Barrier on temperature. If the total melting flux leads to a |
---|
768 | !--positive temperature, it is limited to keep temperature above 0 degC. |
---|
769 | !--It is activated if the total is LOWER than the max |
---|
770 | !--because everything is negative |
---|
771 | dqstotmelt = dqsclrmelt + dqscldmelt |
---|
772 | IF ( dqstotmelt < dqsmelt_max ) THEN |
---|
773 | !--We redistribute the max melted snow keeping |
---|
774 | !--the clear/cloud partition of the melted snow |
---|
775 | dqsclrmelt = dqsmelt_max * dqsclrmelt / dqstotmelt |
---|
776 | dqscldmelt = dqsmelt_max * dqscldmelt / dqstotmelt |
---|
777 | dqstotmelt = dqsmelt_max |
---|
778 | |
---|
779 | ENDIF |
---|
780 | |
---|
781 | !--Add tendencies |
---|
782 | !--The MAX is needed because in some cases, the flux can be slightly negative (numerical precision) |
---|
783 | rainclr(i) = MAX(0., rainclr(i) - dqsclrmelt * dhum_to_dflux(i)) |
---|
784 | raincld(i) = MAX(0., raincld(i) - dqscldmelt * dhum_to_dflux(i)) |
---|
785 | snowclr(i) = MAX(0., snowclr(i) + dqsclrmelt * dhum_to_dflux(i)) |
---|
786 | snowcld(i) = MAX(0., snowcld(i) + dqscldmelt * dhum_to_dflux(i)) |
---|
787 | |
---|
788 | !--Temperature adjustment with the release of latent |
---|
789 | !--heat because of melting |
---|
790 | temp(i) = temp(i) + dqstotmelt * RLMLT / RCPD & |
---|
791 | / ( 1. + RVTMP2 * qtot(i) ) |
---|
792 | |
---|
793 | !--Diagnostic tendencies |
---|
794 | dqrmelt(i) = - dqstotmelt / dtime |
---|
795 | dqsmelt(i) = dqstotmelt / dtime |
---|
796 | |
---|
797 | ENDIF |
---|
798 | |
---|
799 | |
---|
800 | !--------------------------------------------------------- |
---|
801 | !-- FREEZING |
---|
802 | !--------------------------------------------------------- |
---|
803 | !--Process through which rain freezes into snow. |
---|
804 | !-- We parameterize it as a 2 step process: |
---|
805 | !--first: freezing following collision with ice crystals |
---|
806 | !--second: immersion freezing following (inspired by Bigg 1953) |
---|
807 | !--the latter is parameterized as an exponential decrease of the rain |
---|
808 | !--water content with a homemade formulya |
---|
809 | !--This is based on a caracteritic time of freezing, which |
---|
810 | !--exponentially depends on temperature so that it is |
---|
811 | !--equal to 1 for temp_nowater (see below) and is close to |
---|
812 | !--0 for RTT (=273.15 K). |
---|
813 | !--NB.: this process needs a temperature adjustment |
---|
814 | !--dqrfreez_max : maximum rain freezing so that temperature |
---|
815 | !-- stays lower than 273 K [kg/kg] |
---|
816 | !--tau_freez : caracteristic time of freezing [s] |
---|
817 | !--gamma_freez : tuning parameter [s-1] |
---|
818 | !--alpha_freez : tuning parameter for the shape of the exponential curve [-] |
---|
819 | !--temp_nowater : temperature below which no liquid water exists [K] (about -40 degC) |
---|
820 | |
---|
821 | IF ( ( rainclr(i) + raincld(i) ) > 0. ) THEN |
---|
822 | |
---|
823 | |
---|
824 | !--1st step: freezing following collision with ice crystals |
---|
825 | !--Sub-process of freezing which quantifies the collision between |
---|
826 | !--ice crystals in suspension and falling rain droplets. |
---|
827 | !--The rain droplets freeze, becoming graupel, and carrying |
---|
828 | !--the ice crystal (which acted as an ice nucleating particle). |
---|
829 | !--The formula is adapted from the riming formula. |
---|
830 | !--it works only in the cloudy part |
---|
831 | |
---|
832 | dqifreez = 0. |
---|
833 | dqrtotfreez_step1 = 0. |
---|
834 | |
---|
835 | IF ( ( qice(i) > 0. ) .AND. ( cldfra(i) > 0. ) .AND. & |
---|
836 | ( raincld(i) > 0. ) .AND. ( precipfraccld(i) > 0. ) ) THEN |
---|
837 | dqrclrfreez = 0. |
---|
838 | dqrcldfreez = 0. |
---|
839 | |
---|
840 | !--Computed according to |
---|
841 | !--Cpdry * Delta T * (1 + (Cpvap/Cpdry - 1) * qtot) = Lfusion * Delta q |
---|
842 | dqrfreez_max = MIN(0., ( temp(i) - RTT ) / RLMLT * RCPD & |
---|
843 | * ( 1. + RVTMP2 * qtot(i) )) |
---|
844 | |
---|
845 | |
---|
846 | !--The collision efficiency is assumed unity |
---|
847 | Eff_rain_ice = 1. |
---|
848 | coef_freez = gamma_freez * 3. / 4. / rho_rain / r_rain * Eff_rain_ice |
---|
849 | !--Exact version, which does not need a barrier because of |
---|
850 | !--the exponential decrease. |
---|
851 | dqifreez = qice(i) * ( EXP( - dtime * coef_freez * raincld(i) / precipfraccld(i) ) - 1. ) |
---|
852 | |
---|
853 | !--We add the part of rain water that freezes, limited by a temperature barrier |
---|
854 | !--This quantity is calculated assuming that the number of drop that freeze correspond to the number |
---|
855 | !--of crystals collected (and assuming uniform distributions of ice crystals and rain drops) |
---|
856 | !--The ice specific humidity that collide with rain is dqi = dNi 4/3 PI rho_ice r_ice**3 |
---|
857 | !--The rain that collide with ice is, similarly, dqr = dNr 4/3 PI rho_rain r_rain**3 |
---|
858 | !--The assumption above corresponds to dNi = dNr, i.e., |
---|
859 | !-- dqr = dqi * (4/3 PI rho_rain * r_rain**3) / (4/3 PI rho_ice * r_ice**3) |
---|
860 | !--Dry density [kg/m3] |
---|
861 | rho = pplay(i) / temp(i) / RD |
---|
862 | !--r_ice formula from Sun and Rikus (1999) |
---|
863 | r_ice = 1.e-6 * ( 45.8966 * ( qice(i) / cldfra(i) * rho * 1e3 )**0.2214 & |
---|
864 | + 0.7957 * ( qice(i) / cldfra(i) * rho * 1e3 )**0.2535 * ( temp(i) - RTT + 190. ) ) / 2. |
---|
865 | dqrcldfreez = dqifreez * rho_rain * r_rain**3. / ( rho_ice * r_ice**3. ) |
---|
866 | dqrcldfreez = MAX(dqrcldfreez, - raincld(i) / dhum_to_dflux(i)) |
---|
867 | dqrcldfreez = MAX(dqrcldfreez, dqrfreez_max) |
---|
868 | dqrtotfreez_step1 = dqrcldfreez |
---|
869 | |
---|
870 | !--Add tendencies |
---|
871 | !--The MAX is needed because in some cases, the flux can be slightly negative (numerical precision) |
---|
872 | qice(i) = qice(i) + dqifreez |
---|
873 | raincld(i) = MAX(0., raincld(i) + dqrcldfreez * dhum_to_dflux(i)) |
---|
874 | snowcld(i) = MAX(0., snowcld(i) - dqrcldfreez * dhum_to_dflux(i) - dqifreez * dhum_to_dflux(i)) |
---|
875 | temp(i) = temp(i) - dqrtotfreez_step1 * RLMLT / RCPD & |
---|
876 | / ( 1. + RVTMP2 * qtot(i) ) |
---|
877 | |
---|
878 | ENDIF |
---|
879 | |
---|
880 | !-- Second step immersion freezing of rain drops |
---|
881 | !-- with a homemade timeconstant depending on temperature |
---|
882 | |
---|
883 | dqrclrfreez = 0. |
---|
884 | dqrcldfreez = 0. |
---|
885 | dqrtotfreez_step2 = 0. |
---|
886 | !--Computed according to |
---|
887 | !--Cpdry * Delta T * (1 + (Cpvap/Cpdry - 1) * qtot) = Lfusion * Delta q |
---|
888 | |
---|
889 | dqrfreez_max = MIN(0., ( temp(i) - RTT ) / RLMLT * RCPD & |
---|
890 | * ( 1. + RVTMP2 * qtot(i) )) |
---|
891 | |
---|
892 | |
---|
893 | tau_freez = 1. / ( beta_freez & |
---|
894 | * EXP( - alpha_freez * ( temp(i) - temp_nowater ) / ( RTT - temp_nowater ) ) ) |
---|
895 | |
---|
896 | |
---|
897 | !--In clear air |
---|
898 | IF ( rainclr(i) > 0. ) THEN |
---|
899 | !--Exact solution of dqrain/dt = -qrain/tau_freez |
---|
900 | dqrclrfreez = rainclr(i) / dhum_to_dflux(i) * ( EXP( - dtime / tau_freez ) - 1. ) |
---|
901 | ENDIF |
---|
902 | |
---|
903 | !--In cloudy air |
---|
904 | IF ( raincld(i) > 0. ) THEN |
---|
905 | !--Exact solution of dqrain/dt = -qrain/tau_freez |
---|
906 | dqrcldfreez = raincld(i) / dhum_to_dflux(i) * ( EXP( - dtime / tau_freez ) - 1. ) |
---|
907 | ENDIF |
---|
908 | |
---|
909 | !--temperature barrier step 2 |
---|
910 | !--It is activated if the total is LOWER than the max |
---|
911 | !--because everything is negative |
---|
912 | dqrtotfreez_step2 = dqrclrfreez + dqrcldfreez |
---|
913 | |
---|
914 | IF ( dqrtotfreez_step2 < dqrfreez_max ) THEN |
---|
915 | !--We redistribute the max freezed rain keeping |
---|
916 | !--the clear/cloud partition of the freezing rain |
---|
917 | dqrclrfreez = dqrfreez_max * dqrclrfreez / dqrtotfreez_step2 |
---|
918 | dqrcldfreez = dqrfreez_max * dqrcldfreez / dqrtotfreez_step2 |
---|
919 | dqrtotfreez_step2 = dqrfreez_max |
---|
920 | ENDIF |
---|
921 | |
---|
922 | |
---|
923 | !--Add tendencies |
---|
924 | !--The MAX is needed because in some cases, the flux can be slightly negative (numerical precision) |
---|
925 | rainclr(i) = MAX(0., rainclr(i) + dqrclrfreez * dhum_to_dflux(i)) |
---|
926 | raincld(i) = MAX(0., raincld(i) + dqrcldfreez * dhum_to_dflux(i)) |
---|
927 | snowclr(i) = MAX(0., snowclr(i) - dqrclrfreez * dhum_to_dflux(i)) |
---|
928 | snowcld(i) = MAX(0., snowcld(i) - dqrcldfreez * dhum_to_dflux(i)) |
---|
929 | |
---|
930 | |
---|
931 | !--Temperature adjustment with the uptake of latent |
---|
932 | !--heat because of freezing |
---|
933 | temp(i) = temp(i) - dqrtotfreez_step2 * RLMLT / RCPD & |
---|
934 | / ( 1. + RVTMP2 * qtot(i) ) |
---|
935 | |
---|
936 | !--Diagnostic tendencies |
---|
937 | dqrtotfreez = dqrtotfreez_step1 + dqrtotfreez_step2 |
---|
938 | dqrfreez(i) = dqrtotfreez / dtime |
---|
939 | dqsfreez(i) = -(dqrtotfreez + dqifreez) / dtime |
---|
940 | |
---|
941 | ENDIF |
---|
942 | |
---|
943 | |
---|
944 | |
---|
945 | !--If the local flux of rain+snow in clear/cloudy air is lower than rain_int_min, |
---|
946 | !--we reduce the precipiration fraction in the clear/cloudy air so that the new |
---|
947 | !--local flux of rain+snow is equal to rain_int_min. |
---|
948 | !--Here, rain+snow is the gridbox-mean flux of precip. |
---|
949 | !--Therefore, (rain+snow)/precipfrac is the local flux of precip. |
---|
950 | !--If the local flux of precip is lower than rain_int_min, i.e., |
---|
951 | !-- (rain+snow)/precipfrac < rain_int_min , i.e., |
---|
952 | !-- (rain+snow)/rain_int_min < precipfrac , then we want to reduce |
---|
953 | !--the precip fraction to the equality, i.e., precipfrac = (rain+snow)/rain_int_min. |
---|
954 | !--Note that this is physically different than what is proposed in LTP thesis. |
---|
955 | precipfracclr(i) = MIN( precipfracclr(i), ( rainclr(i) + snowclr(i) ) / rain_int_min ) |
---|
956 | precipfraccld(i) = MIN( precipfraccld(i), ( raincld(i) + snowcld(i) ) / rain_int_min ) |
---|
957 | |
---|
958 | !--Calculate outputs |
---|
959 | rain(i) = rainclr(i) + raincld(i) |
---|
960 | snow(i) = snowclr(i) + snowcld(i) |
---|
961 | |
---|
962 | !--Diagnostics |
---|
963 | !--BEWARE this is indeed a diagnostic: this is an estimation from |
---|
964 | !--the value of the flux at the bottom interface of the mesh and |
---|
965 | !--and assuming an upstream numerical calculation |
---|
966 | !--If ok_radocond_snow is TRUE, then the diagnostic qsnowdiag is |
---|
967 | !--used for computing the total ice water content in the mesh |
---|
968 | !--for radiation only |
---|
969 | qraindiag(i) = ( rainclr(i) / ( pplay(i) / RD / temp(i) ) / rain_fallspeed_clr & |
---|
970 | + raincld(i) / ( pplay(i) / RD / temp(i) ) / rain_fallspeed_cld ) |
---|
971 | qsnowdiag(i) = ( snowclr(i) / ( pplay(i) / RD / temp(i) ) / snow_fallspeed_clr & |
---|
972 | + snowcld(i) / ( pplay(i) / RD / temp(i) ) / snow_fallspeed_cld ) |
---|
973 | |
---|
974 | |
---|
975 | ENDDO ! loop on klon |
---|
976 | |
---|
977 | |
---|
978 | END SUBROUTINE poprecip_postcld |
---|
979 | |
---|
980 | END MODULE lmdz_lscp_poprecip |
---|