1 | MODULE lscp_mod |
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2 | |
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3 | IMPLICIT NONE |
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4 | |
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5 | CONTAINS |
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6 | |
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7 | !++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
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8 | SUBROUTINE lscp(klon,klev,dtime,missing_val, & |
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9 | paprs,pplay,temp,q,ptconv,ratqs, & |
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10 | d_t, d_q, d_ql, d_qi, rneb, rneblsvol, rneb_seri, & |
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11 | pfraclr,pfracld, & |
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12 | radocond, radicefrac, rain, snow, & |
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13 | frac_impa, frac_nucl, beta, & |
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14 | prfl, psfl, rhcl, zqta, fraca, & |
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15 | ztv, zpspsk, ztla, zthl, iflag_cld_th, & |
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16 | iflag_ice_thermo, ok_ice_sursat, qsatl, qsats, & |
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17 | distcltop,temp_cltop, & |
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18 | qclr, qcld, qss, qvc, rnebclr, rnebss, gamma_ss, & |
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19 | Tcontr, qcontr, qcontr2, fcontrN, fcontrP, & |
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20 | cloudth_sth,cloudth_senv,cloudth_sigmath,cloudth_sigmaenv) |
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21 | |
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22 | !++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
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23 | ! Authors: Z.X. Li (LMD), J-L Dufresne (LMD), C. Rio (LMD), J-Y Grandpeix (LMD) |
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24 | ! A. JAM (LMD), J-B Madeleine (LMD), E. Vignon (LMD), L. Touzze-Peiffert (LMD) |
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25 | !-------------------------------------------------------------------------------- |
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26 | ! Date: 01/2021 |
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27 | !-------------------------------------------------------------------------------- |
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28 | ! Aim: Large Scale Clouds and Precipitation (LSCP) |
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29 | ! |
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30 | ! This code is a new version of the fisrtilp.F90 routine, which is itself a |
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31 | ! merge of 'first' (superrsaturation physics, P. LeVan K. Laval) |
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32 | ! and 'ilp' (il pleut, L. Li) |
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33 | ! |
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34 | ! Compared to the original fisrtilp code, lscp |
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35 | ! -> assumes thermcep = .TRUE. all the time (fisrtilp inconsistent when .FALSE.) |
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36 | ! -> consider always precipitation thermalisation (fl_cor_ebil>0) |
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37 | ! -> option iflag_fisrtilp_qsat<0 no longer possible (qsat does not evolve with T) |
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38 | ! -> option "oldbug" by JYG has been removed |
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39 | ! -> iflag_t_glace >0 always |
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40 | ! -> the 'all or nothing' cloud approach is no longer available (cpartiel=T always) |
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41 | ! -> rectangular distribution from L. Li no longer available |
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42 | ! -> We always account for the Wegener-Findeisen-Bergeron process (iflag_bergeron = 2 in fisrt) |
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43 | !-------------------------------------------------------------------------------- |
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44 | ! References: |
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45 | ! |
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46 | ! - Bony, S., & Emanuel, K. A. 2001, JAS, doi: 10.1175/1520-0469(2001)058<3158:APOTCA>2.0.CO;2 |
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47 | ! - Hourdin et al. 2013, Clim Dyn, doi:10.1007/s00382-012-1343-y |
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48 | ! - Jam et al. 2013, Boundary-Layer Meteorol, doi:10.1007/s10546-012-9789-3 |
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49 | ! - Jouhaud, et al. 2018. JAMES, doi:10.1029/2018MS001379 |
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50 | ! - Madeleine et al. 2020, JAMES, doi:10.1029/2020MS002046 |
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51 | ! - Touzze-Peifert Ludo, PhD thesis, p117-124 |
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52 | ! ------------------------------------------------------------------------------- |
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53 | ! Code structure: |
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54 | ! |
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55 | ! P0> Thermalization of the precipitation coming from the overlying layer |
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56 | ! P1> Evaporation of the precipitation (falling from the k+1 level) |
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57 | ! P2> Cloud formation (at the k level) |
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58 | ! P2.A.1> With the PDFs, calculation of cloud properties using the inital |
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59 | ! values of T and Q |
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60 | ! P2.A.2> Coupling between condensed water and temperature |
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61 | ! P2.A.3> Calculation of final quantities associated with cloud formation |
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62 | ! P2.B> Release of Latent heat after cloud formation |
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63 | ! P3> Autoconversion to precipitation (k-level) |
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64 | ! P4> Wet scavenging |
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65 | !------------------------------------------------------------------------------ |
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66 | ! Some preliminary comments (JBM) : |
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67 | ! |
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68 | ! The cloud water that the radiation scheme sees is not the same that the cloud |
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69 | ! water used in the physics and the dynamics |
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70 | ! |
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71 | ! During the autoconversion to precipitation (P3 step), radocond (cloud water used |
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72 | ! by the radiation scheme) is calculated as an average of the water that remains |
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73 | ! in the cloud during the precipitation and not the water remaining at the end |
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74 | ! of the time step. The latter is used in the rest of the physics and advected |
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75 | ! by the dynamics. |
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76 | ! |
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77 | ! In summary: |
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78 | ! |
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79 | ! Radiation: |
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80 | ! xflwc(newmicro)+xfiwc(newmicro) = |
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81 | ! radocond=lwcon(nc)+iwcon(nc) |
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82 | ! |
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83 | ! Notetheless, be aware of: |
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84 | ! |
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85 | ! radocond .NE. ocond(nc) |
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86 | ! i.e.: |
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87 | ! lwcon(nc)+iwcon(nc) .NE. ocond(nc) |
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88 | ! but oliq+(ocond-oliq) .EQ. ocond |
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89 | ! (which is not trivial) |
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90 | !++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
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91 | ! |
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92 | USE print_control_mod, ONLY: prt_level, lunout |
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93 | |
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94 | ! USE de modules contenant des fonctions. |
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95 | USE lmdz_cloudth, ONLY : cloudth, cloudth_v3, cloudth_v6, cloudth_mpc |
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96 | USE lscp_tools_mod, ONLY : calc_qsat_ecmwf, icefrac_lscp, calc_gammasat |
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97 | USE lscp_tools_mod, ONLY : fallice_velocity, distance_to_cloud_top |
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98 | USE ice_sursat_mod, ONLY : ice_sursat |
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99 | |
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100 | ! Use du module lscp_ini_mod contenant les constantes |
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101 | USE lscp_ini_mod, ONLY : seuil_neb, niter_lscp, iflag_evap_prec, t_coup, DDT0, ztfondue, rain_int_min |
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102 | USE lscp_ini_mod, ONLY : iflag_mpc_bl, ok_radocond_snow, a_tr_sca, cld_expo_con, cld_expo_lsc |
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103 | USE lscp_ini_mod, ONLY : iflag_cloudth_vert, iflag_rain_incloud_vol, iflag_t_glace, t_glace_min |
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104 | USE lscp_ini_mod, ONLY : coef_eva, coef_eva_i,cld_tau_lsc, cld_tau_con, cld_lc_lsc, cld_lc_con |
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105 | USE lscp_ini_mod, ONLY : iflag_bergeron, iflag_fisrtilp_qsat, iflag_vice, cice_velo, dice_velo |
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106 | USE lscp_ini_mod, ONLY : iflag_autoconversion, ffallv_con, ffallv_lsc |
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107 | USE lscp_ini_mod, ONLY : RCPD, RLSTT, RLVTT, RLMLT, RVTMP2, RTT, RD, RG |
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108 | |
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109 | IMPLICIT NONE |
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110 | |
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111 | !=============================================================================== |
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112 | ! VARIABLES DECLARATION |
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113 | !=============================================================================== |
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114 | |
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115 | ! INPUT VARIABLES: |
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116 | !----------------- |
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117 | |
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118 | INTEGER, INTENT(IN) :: klon,klev ! number of horizontal grid points and vertical levels |
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119 | REAL, INTENT(IN) :: dtime ! time step [s] |
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120 | REAL, INTENT(IN) :: missing_val ! missing value for output |
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121 | |
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122 | REAL, DIMENSION(klon,klev+1), INTENT(IN) :: paprs ! inter-layer pressure [Pa] |
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123 | REAL, DIMENSION(klon,klev), INTENT(IN) :: pplay ! mid-layer pressure [Pa] |
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124 | REAL, DIMENSION(klon,klev), INTENT(IN) :: temp ! temperature (K) |
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125 | REAL, DIMENSION(klon,klev), INTENT(IN) :: q ! total specific humidity (= vapor phase) [kg/kg] |
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126 | INTEGER, INTENT(IN) :: iflag_cld_th ! flag that determines the distribution of convective clouds |
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127 | INTEGER, INTENT(IN) :: iflag_ice_thermo! flag to activate the ice thermodynamics |
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128 | ! CR: if iflag_ice_thermo=2, only convection is active |
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129 | LOGICAL, INTENT(IN) :: ok_ice_sursat ! flag to determine if ice sursaturation is activated |
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130 | |
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131 | LOGICAL, DIMENSION(klon,klev), INTENT(IN) :: ptconv ! grid points where deep convection scheme is active |
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132 | |
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133 | !Inputs associated with thermal plumes |
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134 | |
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135 | REAL, DIMENSION(klon,klev), INTENT(IN) :: ztv ! virtual potential temperature [K] |
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136 | REAL, DIMENSION(klon,klev), INTENT(IN) :: zqta ! specific humidity within thermals [kg/kg] |
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137 | REAL, DIMENSION(klon,klev), INTENT(IN) :: fraca ! fraction of thermals within the mesh [-] |
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138 | REAL, DIMENSION(klon,klev), INTENT(IN) :: zpspsk ! exner potential (p/100000)**(R/cp) |
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139 | REAL, DIMENSION(klon,klev), INTENT(IN) :: ztla ! liquid temperature within thermals [K] |
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140 | |
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141 | ! INPUT/OUTPUT variables |
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142 | !------------------------ |
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143 | |
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144 | REAL, DIMENSION(klon,klev), INTENT(INOUT) :: zthl ! liquid potential temperature [K] |
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145 | REAL, DIMENSION(klon,klev), INTENT(INOUT):: ratqs ! function of pressure that sets the large-scale |
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146 | REAL, DIMENSION(klon,klev), INTENT(INOUT):: beta ! conversion rate of condensed water |
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147 | |
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148 | |
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149 | ! Input sursaturation en glace |
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150 | REAL, DIMENSION(klon,klev), INTENT(INOUT):: rneb_seri ! fraction nuageuse en memoire |
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151 | |
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152 | ! OUTPUT variables |
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153 | !----------------- |
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154 | |
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155 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: d_t ! temperature increment [K] |
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156 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: d_q ! specific humidity increment [kg/kg] |
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157 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: d_ql ! liquid water increment [kg/kg] |
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158 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: d_qi ! cloud ice mass increment [kg/kg] |
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159 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: rneb ! cloud fraction [-] |
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160 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: rneblsvol ! cloud fraction per unit volume [-] |
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161 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: pfraclr ! precip fraction clear-sky part [-] |
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162 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: pfracld ! precip fraction cloudy part [-] |
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163 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: radocond ! condensed water used in the radiation scheme [kg/kg] |
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164 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: radicefrac ! ice fraction of condensed water for radiation scheme |
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165 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: rhcl ! clear-sky relative humidity [-] |
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166 | REAL, DIMENSION(klon), INTENT(OUT) :: rain ! surface large-scale rainfall [kg/s/m2] |
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167 | REAL, DIMENSION(klon), INTENT(OUT) :: snow ! surface large-scale snowfall [kg/s/m2] |
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168 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qsatl ! saturation specific humidity wrt liquid [kg/kg] |
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169 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qsats ! saturation specific humidity wrt ice [kg/kg] |
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170 | REAL, DIMENSION(klon,klev+1), INTENT(OUT) :: prfl ! large-scale rainfall flux in the column [kg/s/m2] |
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171 | REAL, DIMENSION(klon,klev+1), INTENT(OUT) :: psfl ! large-scale snowfall flux in the column [kg/s/m2] |
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172 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: distcltop ! distance to cloud top [m] |
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173 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: temp_cltop ! temperature of cloud top [K] |
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174 | ! fraction of aerosol scavenging through impaction and nucleation (for on-line) |
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175 | |
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176 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: frac_impa ! scavenging fraction due tu impaction [-] |
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177 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: frac_nucl ! scavenging fraction due tu nucleation [-] |
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178 | |
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179 | ! for supersaturation and contrails parameterisation |
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180 | |
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181 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qclr ! specific total water content in clear sky region [kg/kg] |
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182 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qcld ! specific total water content in cloudy region [kg/kg] |
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183 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qss ! specific total water content in supersat region [kg/kg] |
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184 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qvc ! specific vapor content in clouds [kg/kg] |
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185 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: rnebclr ! mesh fraction of clear sky [-] |
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186 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: rnebss ! mesh fraction of ISSR [-] |
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187 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: gamma_ss ! coefficient governing the ice nucleation RHi threshold [-] |
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188 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: Tcontr ! threshold temperature for contrail formation [K] |
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189 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qcontr ! threshold humidity for contrail formation [kg/kg] |
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190 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qcontr2 ! // (2nd expression more consistent with LMDZ expression of q) |
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191 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: fcontrN ! fraction of grid favourable to non-persistent contrails |
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192 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: fcontrP ! fraction of grid favourable to persistent contrails |
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193 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: cloudth_sth,cloudth_senv,cloudth_sigmath,cloudth_sigmaenv |
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194 | |
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195 | |
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196 | ! LOCAL VARIABLES: |
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197 | !---------------- |
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198 | |
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199 | REAL,DIMENSION(klon) :: qsl, qsi |
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200 | REAL :: zct, zcl,zexpo |
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201 | REAL, DIMENSION(klon,klev) :: ctot |
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202 | REAL, DIMENSION(klon,klev) :: ctot_vol |
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203 | REAL, DIMENSION(klon) :: zqs, zdqs |
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204 | REAL :: zdelta, zcor, zcvm5 |
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205 | REAL, DIMENSION(klon) :: zdqsdT_raw |
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206 | REAL, DIMENSION(klon) :: gammasat,dgammasatdt ! coefficient to make cold condensation at the correct RH and derivative wrt T |
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207 | REAL, DIMENSION(klon) :: Tbef,qlbef,DT |
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208 | REAL :: num,denom |
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209 | REAL :: cste |
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210 | REAL, DIMENSION(klon) :: zpdf_sig,zpdf_k,zpdf_delta |
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211 | REAL, DIMENSION(klon) :: Zpdf_a,zpdf_b,zpdf_e1,zpdf_e2 |
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212 | REAL :: erf |
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213 | REAL, DIMENSION(klon,klev) :: icefrac_mpc |
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214 | REAL, DIMENSION(klon) :: qcloud, qincloud_mpc |
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215 | REAL, DIMENSION(klon) :: zrfl, zrfln |
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216 | REAL :: zqev, zqevt |
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217 | REAL, DIMENSION(klon) :: zifl, zifln, ziflprev |
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218 | REAL :: zqev0,zqevi, zqevti |
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219 | REAL, DIMENSION(klon) :: zoliq, zcond, zq, zqn |
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220 | REAL, DIMENSION(klon) :: zoliql, zoliqi |
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221 | REAL, DIMENSION(klon) :: zt |
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222 | REAL, DIMENSION(klon,klev) :: zrho |
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223 | REAL, DIMENSION(klon) :: zdz,iwc |
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224 | REAL :: zchau,zfroi |
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225 | REAL, DIMENSION(klon) :: zfice,zneb,znebprecip |
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226 | REAL :: zmelt,zrain,zsnow,zprecip |
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227 | REAL, DIMENSION(klon) :: dzfice |
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228 | REAL :: zsolid |
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229 | REAL, DIMENSION(klon) :: qtot, qzero |
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230 | REAL, DIMENSION(klon) :: dqsl,dqsi |
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231 | REAL :: smallestreal |
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232 | ! Variables for Bergeron process |
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233 | REAL :: zcp, coef1, DeltaT, Deltaq, Deltaqprecl |
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234 | REAL, DIMENSION(klon) :: zqpreci, zqprecl |
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235 | ! Variables precipitation energy conservation |
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236 | REAL, DIMENSION(klon) :: zmqc |
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237 | REAL :: zalpha_tr |
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238 | REAL :: zfrac_lessi |
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239 | REAL, DIMENSION(klon) :: zprec_cond |
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240 | REAL, DIMENSION(klon) :: zmair |
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241 | REAL :: zcpair, zcpeau |
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242 | REAL, DIMENSION(klon) :: zlh_solid |
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243 | REAL :: zm_solid ! for liquid -> solid conversion |
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244 | REAL, DIMENSION(klon) :: zrflclr, zrflcld |
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245 | REAL, DIMENSION(klon) :: d_zrfl_clr_cld, d_zifl_clr_cld |
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246 | REAL, DIMENSION(klon) :: d_zrfl_cld_clr, d_zifl_cld_clr |
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247 | REAL, DIMENSION(klon) :: ziflclr, ziflcld |
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248 | REAL, DIMENSION(klon) :: znebprecipclr, znebprecipcld |
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249 | REAL, DIMENSION(klon) :: tot_zneb, tot_znebn, d_tot_zneb |
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250 | REAL, DIMENSION(klon) :: d_znebprecip_clr_cld, d_znebprecip_cld_clr |
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251 | REAL, DIMENSION(klon,klev) :: velo |
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252 | REAL :: vr, ffallv |
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253 | REAL :: qlmpc, qimpc, rnebmpc |
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254 | REAL, DIMENSION(klon,klev) :: radocondi, radocondl |
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255 | REAL :: effective_zneb |
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256 | REAL, DIMENSION(klon) :: distcltop1D, temp_cltop1D |
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257 | |
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258 | |
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259 | INTEGER i, k, n, kk, iter |
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260 | INTEGER, DIMENSION(klon) :: n_i |
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261 | INTEGER ncoreczq |
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262 | INTEGER, DIMENSION(klon,klev) :: mpc_bl_points |
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263 | |
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264 | LOGICAL, DIMENSION(klon) :: lognormale |
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265 | LOGICAL, DIMENSION(klon) :: keepgoing |
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266 | |
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267 | CHARACTER (len = 20) :: modname = 'lscp' |
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268 | CHARACTER (len = 80) :: abort_message |
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269 | |
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270 | |
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271 | !=============================================================================== |
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272 | ! INITIALISATION |
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273 | !=============================================================================== |
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274 | |
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275 | ! Few initial checks |
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276 | |
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277 | |
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278 | IF (iflag_fisrtilp_qsat .LT. 0) THEN |
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279 | abort_message = 'lscp cannot be used with iflag_fisrtilp<0' |
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280 | CALL abort_physic(modname,abort_message,1) |
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281 | ENDIF |
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282 | |
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283 | ! Few initialisations |
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284 | |
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285 | znebprecip(:)=0.0 |
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286 | ctot_vol(1:klon,1:klev)=0.0 |
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287 | rneblsvol(1:klon,1:klev)=0.0 |
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288 | smallestreal=1.e-9 |
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289 | znebprecipclr(:)=0.0 |
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290 | znebprecipcld(:)=0.0 |
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291 | mpc_bl_points(:,:)=0 |
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292 | |
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293 | IF (prt_level>9) WRITE(lunout,*) 'NUAGES4 A. JAM' |
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294 | |
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295 | ! AA for 'safety' reasons |
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296 | zalpha_tr = 0. |
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297 | zfrac_lessi = 0. |
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298 | beta(:,:)= 0. |
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299 | |
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300 | ! Initialisation of variables: |
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301 | |
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302 | prfl(:,:) = 0.0 |
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303 | psfl(:,:) = 0.0 |
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304 | d_t(:,:) = 0.0 |
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305 | d_q(:,:) = 0.0 |
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306 | d_ql(:,:) = 0.0 |
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307 | d_qi(:,:) = 0.0 |
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308 | rneb(:,:) = 0.0 |
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309 | pfraclr(:,:)=0.0 |
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310 | pfracld(:,:)=0.0 |
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311 | radocond(:,:) = 0.0 |
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312 | radicefrac(:,:) = 0.0 |
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313 | frac_nucl(:,:) = 1.0 |
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314 | frac_impa(:,:) = 1.0 |
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315 | rain(:) = 0.0 |
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316 | snow(:) = 0.0 |
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317 | zoliq(:)=0.0 |
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318 | zfice(:)=0.0 |
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319 | dzfice(:)=0.0 |
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320 | zqprecl(:)=0.0 |
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321 | zqpreci(:)=0.0 |
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322 | zrfl(:) = 0.0 |
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323 | zifl(:) = 0.0 |
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324 | ziflprev(:)=0.0 |
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325 | zneb(:) = seuil_neb |
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326 | zrflclr(:) = 0.0 |
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327 | ziflclr(:) = 0.0 |
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328 | zrflcld(:) = 0.0 |
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329 | ziflcld(:) = 0.0 |
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330 | tot_zneb(:) = 0.0 |
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331 | tot_znebn(:) = 0.0 |
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332 | d_tot_zneb(:) = 0.0 |
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333 | qzero(:) = 0.0 |
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334 | distcltop1D(:)=0.0 |
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335 | temp_cltop1D(:) = 0.0 |
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336 | !--ice supersaturation |
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337 | gamma_ss(:,:) = 1.0 |
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338 | qss(:,:) = 0.0 |
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339 | rnebss(:,:) = 0.0 |
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340 | Tcontr(:,:) = missing_val |
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341 | qcontr(:,:) = missing_val |
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342 | qcontr2(:,:) = missing_val |
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343 | fcontrN(:,:) = 0.0 |
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344 | fcontrP(:,:) = 0.0 |
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345 | distcltop(:,:)=0. |
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346 | temp_cltop(:,:)=0. |
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347 | |
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348 | !c_iso: variable initialisation for iso |
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349 | |
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350 | |
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351 | !=============================================================================== |
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352 | ! BEGINNING OF VERTICAL LOOP FROM TOP TO BOTTOM |
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353 | !=============================================================================== |
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354 | |
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355 | ncoreczq=0 |
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356 | |
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357 | DO k = klev, 1, -1 |
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358 | |
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359 | ! Initialisation temperature and specific humidity |
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360 | DO i = 1, klon |
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361 | zt(i)=temp(i,k) |
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362 | zq(i)=q(i,k) |
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363 | !c_iso init of iso |
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364 | ENDDO |
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365 | |
---|
366 | ! -------------------------------------------------------------------- |
---|
367 | ! P0> Thermalization of precipitation falling from the overlying layer |
---|
368 | ! -------------------------------------------------------------------- |
---|
369 | ! Computes air temperature variation due to enthalpy transported by |
---|
370 | ! precipitation. Precipitation is then thermalized with the air in the |
---|
371 | ! layer. |
---|
372 | ! The precipitation should remain thermalized throughout the different |
---|
373 | ! thermodynamical transformations. |
---|
374 | ! The corresponding water mass should |
---|
375 | ! be added when calculating the layer's enthalpy change with |
---|
376 | ! temperature |
---|
377 | ! See lmdzpedia page todoan |
---|
378 | ! todoan: check consistency with ice phase |
---|
379 | ! todoan: understand why several steps |
---|
380 | ! --------------------------------------------------------------------- |
---|
381 | |
---|
382 | IF (k.LE.klev-1) THEN |
---|
383 | |
---|
384 | DO i = 1, klon |
---|
385 | |
---|
386 | zmair(i)=(paprs(i,k)-paprs(i,k+1))/RG |
---|
387 | ! no condensed water so cp=cp(vapor+dry air) |
---|
388 | ! RVTMP2=rcpv/rcpd-1 |
---|
389 | zcpair=RCPD*(1.0+RVTMP2*zq(i)) |
---|
390 | zcpeau=RCPD*RVTMP2 |
---|
391 | |
---|
392 | ! zmqc: precipitation mass that has to be thermalized with |
---|
393 | ! layer's air so that precipitation at the ground has the |
---|
394 | ! same temperature as the lowermost layer |
---|
395 | zmqc(i) = (zrfl(i)+zifl(i))*dtime/zmair(i) |
---|
396 | ! t(i,k+1)+d_t(i,k+1): new temperature of the overlying layer |
---|
397 | zt(i) = ( (temp(i,k+1)+d_t(i,k+1))*zmqc(i)*zcpeau + zcpair*zt(i) ) & |
---|
398 | / (zcpair + zmqc(i)*zcpeau) |
---|
399 | |
---|
400 | ENDDO |
---|
401 | |
---|
402 | ELSE |
---|
403 | |
---|
404 | DO i = 1, klon |
---|
405 | zmair(i)=(paprs(i,k)-paprs(i,k+1))/RG |
---|
406 | zmqc(i) = 0. |
---|
407 | ENDDO |
---|
408 | |
---|
409 | ENDIF |
---|
410 | |
---|
411 | ! -------------------------------------------------------------------- |
---|
412 | ! P1> Precipitation evaporation/sublimation |
---|
413 | ! -------------------------------------------------------------------- |
---|
414 | ! A part of the precipitation coming from above is evaporated/sublimated. |
---|
415 | ! -------------------------------------------------------------------- |
---|
416 | |
---|
417 | IF (iflag_evap_prec.GE.1) THEN |
---|
418 | |
---|
419 | ! Calculation of saturation specific humidity |
---|
420 | ! depending on temperature: |
---|
421 | CALL calc_qsat_ecmwf(klon,zt(:),qzero(:),pplay(:,k),RTT,0,.false.,zqs(:),zdqs(:)) |
---|
422 | ! wrt liquid water |
---|
423 | CALL calc_qsat_ecmwf(klon,zt(:),qzero(:),pplay(:,k),RTT,1,.false.,qsl(:),dqsl(:)) |
---|
424 | ! wrt ice |
---|
425 | CALL calc_qsat_ecmwf(klon,zt(:),qzero(:),pplay(:,k),RTT,2,.false.,qsi(:),dqsi(:)) |
---|
426 | |
---|
427 | DO i = 1, klon |
---|
428 | |
---|
429 | ! if precipitation |
---|
430 | IF (zrfl(i)+zifl(i).GT.0.) THEN |
---|
431 | |
---|
432 | ! LudoTP: we only account for precipitation evaporation in the clear-sky (iflag_evap_prec>=4). |
---|
433 | ! c_iso: likely important to distinguish cs from neb isotope precipitation |
---|
434 | |
---|
435 | IF (iflag_evap_prec.GE.4) THEN |
---|
436 | zrfl(i) = zrflclr(i) |
---|
437 | zifl(i) = ziflclr(i) |
---|
438 | ENDIF |
---|
439 | |
---|
440 | IF (iflag_evap_prec.EQ.1) THEN |
---|
441 | znebprecip(i)=zneb(i) |
---|
442 | ELSE |
---|
443 | znebprecip(i)=MAX(zneb(i),znebprecip(i)) |
---|
444 | ENDIF |
---|
445 | |
---|
446 | IF (iflag_evap_prec.GT.4) THEN |
---|
447 | ! Max evaporation not to saturate the clear sky precip fraction |
---|
448 | ! i.e. the fraction where evaporation occurs |
---|
449 | zqev0 = MAX(0.0, (zqs(i)-zq(i))*znebprecipclr(i)) |
---|
450 | ELSEIF (iflag_evap_prec .EQ. 4) THEN |
---|
451 | ! Max evaporation not to saturate the whole mesh |
---|
452 | ! Pay attention -> lead to unrealistic and excessive evaporation |
---|
453 | zqev0 = MAX(0.0, zqs(i)-zq(i)) |
---|
454 | ELSE |
---|
455 | ! Max evap not to saturate the fraction below the cloud |
---|
456 | zqev0 = MAX(0.0, (zqs(i)-zq(i))*znebprecip(i)) |
---|
457 | ENDIF |
---|
458 | |
---|
459 | ! Evaporation of liquid precipitation coming from above |
---|
460 | ! dP/dz=beta*(1-q/qsat)*sqrt(P) |
---|
461 | ! formula from Sundquist 1988, Klemp & Wilhemson 1978 |
---|
462 | ! LTP: evaporation only in the clear sky part (iflag_evap_prec>=4) |
---|
463 | |
---|
464 | IF (iflag_evap_prec.EQ.3) THEN |
---|
465 | zqevt = znebprecip(i)*coef_eva*(1.0-zq(i)/qsl(i)) & |
---|
466 | *SQRT(zrfl(i)/max(1.e-4,znebprecip(i))) & |
---|
467 | *(paprs(i,k)-paprs(i,k+1))/pplay(i,k)*zt(i)*RD/RG |
---|
468 | ELSE IF (iflag_evap_prec.GE.4) THEN |
---|
469 | zqevt = znebprecipclr(i)*coef_eva*(1.0-zq(i)/qsl(i)) & |
---|
470 | *SQRT(zrfl(i)/max(1.e-8,znebprecipclr(i))) & |
---|
471 | *(paprs(i,k)-paprs(i,k+1))/pplay(i,k)*zt(i)*RD/RG |
---|
472 | ELSE |
---|
473 | zqevt = 1.*coef_eva*(1.0-zq(i)/qsl(i))*SQRT(zrfl(i)) & |
---|
474 | *(paprs(i,k)-paprs(i,k+1))/pplay(i,k)*zt(i)*RD/RG |
---|
475 | ENDIF |
---|
476 | |
---|
477 | zqevt = MAX(0.0,MIN(zqevt,zrfl(i))) & |
---|
478 | *RG*dtime/(paprs(i,k)-paprs(i,k+1)) |
---|
479 | |
---|
480 | ! sublimation of the solid precipitation coming from above |
---|
481 | IF (iflag_evap_prec.EQ.3) THEN |
---|
482 | zqevti = znebprecip(i)*coef_eva_i*(1.0-zq(i)/qsi(i)) & |
---|
483 | *SQRT(zifl(i)/max(1.e-4,znebprecip(i))) & |
---|
484 | *(paprs(i,k)-paprs(i,k+1))/pplay(i,k)*zt(i)*RD/RG |
---|
485 | ELSE IF (iflag_evap_prec.GE.4) THEN |
---|
486 | zqevti = znebprecipclr(i)*coef_eva_i*(1.0-zq(i)/qsi(i)) & |
---|
487 | *SQRT(zifl(i)/max(1.e-8,znebprecipclr(i))) & |
---|
488 | *(paprs(i,k)-paprs(i,k+1))/pplay(i,k)*zt(i)*RD/RG |
---|
489 | ELSE |
---|
490 | zqevti = 1.*coef_eva_i*(1.0-zq(i)/qsi(i))*SQRT(zifl(i)) & |
---|
491 | *(paprs(i,k)-paprs(i,k+1))/pplay(i,k)*zt(i)*RD/RG |
---|
492 | ENDIF |
---|
493 | |
---|
494 | zqevti = MAX(0.0,MIN(zqevti,zifl(i))) & |
---|
495 | *RG*dtime/(paprs(i,k)-paprs(i,k+1)) |
---|
496 | |
---|
497 | ! A. JAM |
---|
498 | ! Evaporation limit: we ensure that the layer's fraction below |
---|
499 | ! the cloud or the whole mesh (depending on iflag_evap_prec) |
---|
500 | ! does not reach saturation. In this case, we |
---|
501 | ! redistribute zqev0 conserving the ratio liquid/ice |
---|
502 | |
---|
503 | ! todoan: check the consistency of this formula |
---|
504 | IF (zqevt+zqevti.GT.zqev0) THEN |
---|
505 | zqev=zqev0*zqevt/(zqevt+zqevti) |
---|
506 | zqevi=zqev0*zqevti/(zqevt+zqevti) |
---|
507 | ELSE |
---|
508 | zqev=zqevt |
---|
509 | zqevi=zqevti |
---|
510 | ENDIF |
---|
511 | |
---|
512 | |
---|
513 | ! New solid and liquid precipitation fluxes after evap and sublimation |
---|
514 | zrfln(i) = Max(0.,zrfl(i) - zqev*(paprs(i,k)-paprs(i,k+1)) & |
---|
515 | /RG/dtime) |
---|
516 | zifln(i) = Max(0.,zifl(i) - zqevi*(paprs(i,k)-paprs(i,k+1)) & |
---|
517 | /RG/dtime) |
---|
518 | |
---|
519 | |
---|
520 | ! vapor, temperature, precip fluxes update |
---|
521 | zq(i) = zq(i) - (zrfln(i)+zifln(i)-zrfl(i)-zifl(i)) & |
---|
522 | * (RG/(paprs(i,k)-paprs(i,k+1)))*dtime |
---|
523 | zmqc(i) = zmqc(i) + (zrfln(i)+zifln(i)-zrfl(i)-zifl(i)) & |
---|
524 | * (RG/(paprs(i,k)-paprs(i,k+1)))*dtime |
---|
525 | zt(i) = zt(i) + (zrfln(i)-zrfl(i)) & |
---|
526 | * (RG/(paprs(i,k)-paprs(i,k+1)))*dtime & |
---|
527 | * RLVTT/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i))) & |
---|
528 | + (zifln(i)-zifl(i)) & |
---|
529 | * (RG/(paprs(i,k)-paprs(i,k+1)))*dtime & |
---|
530 | * RLSTT/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i))) |
---|
531 | |
---|
532 | ! New values of liquid and solid precipitation |
---|
533 | zrfl(i) = zrfln(i) |
---|
534 | zifl(i) = zifln(i) |
---|
535 | |
---|
536 | ! c_iso here call_reevap that updates isotopic zrfl, zifl (in inout) |
---|
537 | ! due to evap + sublim |
---|
538 | |
---|
539 | |
---|
540 | IF (iflag_evap_prec.GE.4) THEN |
---|
541 | zrflclr(i) = zrfl(i) |
---|
542 | ziflclr(i) = zifl(i) |
---|
543 | IF(zrflclr(i) + ziflclr(i).LE.0) THEN |
---|
544 | znebprecipclr(i) = 0.0 |
---|
545 | ENDIF |
---|
546 | zrfl(i) = zrflclr(i) + zrflcld(i) |
---|
547 | zifl(i) = ziflclr(i) + ziflcld(i) |
---|
548 | ENDIF |
---|
549 | |
---|
550 | ! c_iso duplicate for isotopes or loop on isotopes |
---|
551 | |
---|
552 | ! Melting: |
---|
553 | zmelt = ((zt(i)-RTT)/(ztfondue-RTT)) ! JYG |
---|
554 | ! precip fraction that is melted |
---|
555 | zmelt = MIN(MAX(zmelt,0.),1.) |
---|
556 | |
---|
557 | ! update of rainfall and snowfall due to melting |
---|
558 | IF (iflag_evap_prec.GE.4) THEN |
---|
559 | zrflclr(i)=zrflclr(i)+zmelt*ziflclr(i) |
---|
560 | zrflcld(i)=zrflcld(i)+zmelt*ziflcld(i) |
---|
561 | zrfl(i)=zrflclr(i)+zrflcld(i) |
---|
562 | |
---|
563 | ziflclr(i)=ziflclr(i)*(1.-zmelt) |
---|
564 | ziflcld(i)=ziflcld(i)*(1.-zmelt) |
---|
565 | zifl(i)=ziflclr(i)+ziflcld(i) |
---|
566 | |
---|
567 | ELSE |
---|
568 | zrfl(i)=zrfl(i)+zmelt*zifl(i) |
---|
569 | |
---|
570 | zifl(i)=zifl(i)*(1.-zmelt) |
---|
571 | ENDIF |
---|
572 | |
---|
573 | |
---|
574 | ! c_iso: melting of isotopic precipi with zmelt (no fractionation) |
---|
575 | |
---|
576 | ! Latent heat of melting with precipitation thermalization |
---|
577 | zt(i)=zt(i)-zifl(i)*zmelt*(RG*dtime)/(paprs(i,k)-paprs(i,k+1)) & |
---|
578 | *RLMLT/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i))) |
---|
579 | |
---|
580 | |
---|
581 | ELSE |
---|
582 | ! if no precip, we reinitialize the cloud fraction used for the precip to 0 |
---|
583 | znebprecip(i)=0. |
---|
584 | |
---|
585 | ENDIF ! (zrfl(i)+zifl(i).GT.0.) |
---|
586 | |
---|
587 | ENDDO |
---|
588 | |
---|
589 | ENDIF ! (iflag_evap_prec>=1) |
---|
590 | |
---|
591 | ! -------------------------------------------------------------------- |
---|
592 | ! End precip evaporation |
---|
593 | ! -------------------------------------------------------------------- |
---|
594 | |
---|
595 | ! Calculation of qsat, L/Cp*dqsat/dT and ncoreczq counter |
---|
596 | !------------------------------------------------------- |
---|
597 | |
---|
598 | qtot(:)=zq(:)+zmqc(:) |
---|
599 | CALL calc_qsat_ecmwf(klon,zt(:),qtot(:),pplay(:,k),RTT,0,.false.,zqs(:),zdqs(:)) |
---|
600 | DO i = 1, klon |
---|
601 | zdelta = MAX(0.,SIGN(1.,RTT-zt(i))) |
---|
602 | zdqsdT_raw(i) = zdqs(i)*RCPD*(1.0+RVTMP2*zq(i)) / (RLVTT*(1.-zdelta) + RLSTT*zdelta) |
---|
603 | IF (zq(i) .LT. 1.e-15) THEN |
---|
604 | ncoreczq=ncoreczq+1 |
---|
605 | zq(i)=1.e-15 |
---|
606 | ENDIF |
---|
607 | ! c_iso: do something similar for isotopes |
---|
608 | |
---|
609 | ENDDO |
---|
610 | |
---|
611 | ! -------------------------------------------------------------------- |
---|
612 | ! P2> Cloud formation |
---|
613 | !--------------------------------------------------------------------- |
---|
614 | ! |
---|
615 | ! Unlike fisrtilp, we always assume a 'fractional cloud' approach |
---|
616 | ! i.e. clouds occupy only a fraction of the mesh (the subgrid distribution |
---|
617 | ! is prescribed and depends on large scale variables and boundary layer |
---|
618 | ! properties) |
---|
619 | ! The decrease in condensed part due tu latent heating is taken into |
---|
620 | ! account |
---|
621 | ! ------------------------------------------------------------------- |
---|
622 | |
---|
623 | ! P2.1> With the PDFs (log-normal, bigaussian) |
---|
624 | ! cloud properties calculation with the initial values of t and q |
---|
625 | ! ---------------------------------------------------------------- |
---|
626 | |
---|
627 | ! initialise gammasat and qincloud_mpc |
---|
628 | gammasat(:)=1. |
---|
629 | qincloud_mpc(:)=0. |
---|
630 | |
---|
631 | IF (iflag_cld_th.GE.5) THEN |
---|
632 | |
---|
633 | IF (iflag_mpc_bl .LT. 1) THEN |
---|
634 | |
---|
635 | IF (iflag_cloudth_vert.LE.2) THEN |
---|
636 | |
---|
637 | CALL cloudth(klon,klev,k,ztv, & |
---|
638 | zq,zqta,fraca, & |
---|
639 | qcloud,ctot,zpspsk,paprs,pplay,ztla,zthl, & |
---|
640 | ratqs,zqs,temp, & |
---|
641 | cloudth_sth,cloudth_senv,cloudth_sigmath,cloudth_sigmaenv) |
---|
642 | |
---|
643 | |
---|
644 | |
---|
645 | |
---|
646 | |
---|
647 | ELSEIF (iflag_cloudth_vert.GE.3 .AND. iflag_cloudth_vert.LE.5) THEN |
---|
648 | |
---|
649 | CALL cloudth_v3(klon,klev,k,ztv, & |
---|
650 | zq,zqta,fraca, & |
---|
651 | qcloud,ctot,ctot_vol,zpspsk,paprs,pplay,ztla,zthl, & |
---|
652 | ratqs,zqs,temp, & |
---|
653 | cloudth_sth,cloudth_senv,cloudth_sigmath,cloudth_sigmaenv) |
---|
654 | |
---|
655 | !Jean Jouhaud's version, Decembre 2018 |
---|
656 | !------------------------------------- |
---|
657 | |
---|
658 | ELSEIF (iflag_cloudth_vert.EQ.6) THEN |
---|
659 | |
---|
660 | CALL cloudth_v6(klon,klev,k,ztv, & |
---|
661 | zq,zqta,fraca, & |
---|
662 | qcloud,ctot,ctot_vol,zpspsk,paprs,pplay,ztla,zthl, & |
---|
663 | ratqs,zqs,temp, & |
---|
664 | cloudth_sth,cloudth_senv,cloudth_sigmath,cloudth_sigmaenv) |
---|
665 | |
---|
666 | ENDIF |
---|
667 | |
---|
668 | ELSE |
---|
669 | ! cloudth_v3 + cold microphysical considerations |
---|
670 | ! + stationary mixed-phase cloud model |
---|
671 | |
---|
672 | CALL cloudth_mpc(klon,klev,k,iflag_mpc_bl,mpc_bl_points, & |
---|
673 | temp,ztv,zq,zqta,fraca, zpspsk, & |
---|
674 | paprs,pplay,ztla,zthl,ratqs,zqs,psfl, & |
---|
675 | qcloud,qincloud_mpc,icefrac_mpc,ctot,ctot_vol, & |
---|
676 | cloudth_sth,cloudth_senv,cloudth_sigmath,cloudth_sigmaenv) |
---|
677 | |
---|
678 | ENDIF ! iflag_mpc_bl |
---|
679 | |
---|
680 | DO i=1,klon |
---|
681 | rneb(i,k)=ctot(i,k) |
---|
682 | rneblsvol(i,k)=ctot_vol(i,k) |
---|
683 | zqn(i)=qcloud(i) |
---|
684 | ENDDO |
---|
685 | |
---|
686 | ENDIF |
---|
687 | |
---|
688 | IF (iflag_cld_th .LE. 4) THEN |
---|
689 | |
---|
690 | ! lognormal |
---|
691 | lognormale = .TRUE. |
---|
692 | |
---|
693 | ELSEIF (iflag_cld_th .GE. 6) THEN |
---|
694 | |
---|
695 | ! lognormal distribution when no thermals |
---|
696 | lognormale = fraca(:,k) < 1e-10 |
---|
697 | |
---|
698 | ELSE |
---|
699 | ! When iflag_cld_th=5, we always assume |
---|
700 | ! bi-gaussian distribution |
---|
701 | lognormale = .FALSE. |
---|
702 | |
---|
703 | ENDIF |
---|
704 | |
---|
705 | DT(:) = 0. |
---|
706 | n_i(:)=0 |
---|
707 | Tbef(:)=zt(:) |
---|
708 | qlbef(:)=0. |
---|
709 | |
---|
710 | ! Treatment of non-boundary layer clouds (lognormale) |
---|
711 | ! condensation with qsat(T) variation (adaptation) |
---|
712 | ! Iterative resolution to converge towards qsat |
---|
713 | ! with update of temperature, ice fraction and qsat at |
---|
714 | ! each iteration |
---|
715 | |
---|
716 | ! todoan -> sensitivity to iflag_fisrtilp_qsat |
---|
717 | DO iter=1,iflag_fisrtilp_qsat+1 |
---|
718 | |
---|
719 | DO i=1,klon |
---|
720 | |
---|
721 | ! keepgoing = .true. while convergence is not satisfied |
---|
722 | keepgoing(i)=ABS(DT(i)).GT.DDT0 |
---|
723 | |
---|
724 | IF ((keepgoing(i) .OR. (n_i(i) .EQ. 0)) .AND. lognormale(i)) THEN |
---|
725 | |
---|
726 | ! if not convergence: |
---|
727 | |
---|
728 | ! P2.2.1> cloud fraction and condensed water mass calculation |
---|
729 | ! Calculated variables: |
---|
730 | ! rneb : cloud fraction |
---|
731 | ! zqn : total water within the cloud |
---|
732 | ! zcond: mean condensed water within the mesh |
---|
733 | ! rhcl: clear-sky relative humidity |
---|
734 | !--------------------------------------------------------------- |
---|
735 | |
---|
736 | ! new temperature that only serves in the iteration process: |
---|
737 | Tbef(i)=Tbef(i)+DT(i) |
---|
738 | |
---|
739 | ! Rneb, qzn and zcond for lognormal PDFs |
---|
740 | qtot(i)=zq(i)+zmqc(i) |
---|
741 | |
---|
742 | ENDIF |
---|
743 | |
---|
744 | ENDDO |
---|
745 | |
---|
746 | ! Calculation of saturation specific humidity and ice fraction |
---|
747 | CALL calc_qsat_ecmwf(klon,Tbef(:),qtot(:),pplay(:,k),RTT,0,.false.,zqs(:),zdqs(:)) |
---|
748 | CALL calc_gammasat(klon,Tbef(:),qtot(:),pplay(:,k),gammasat(:),dgammasatdt(:)) |
---|
749 | ! saturation may occur at a humidity different from qsat (gamma qsat), so gamma correction for dqs |
---|
750 | zdqs(:) = gammasat(:)*zdqs(:)+zqs(:)*dgammasatdt(:) |
---|
751 | ! cloud phase determination |
---|
752 | IF (iflag_t_glace.GE.4) THEN |
---|
753 | ! For iflag_t_glace GE 4 the phase partition function dependends on temperature AND distance to cloud top |
---|
754 | CALL distance_to_cloud_top(klon,klev,k,temp,pplay,paprs,rneb,distcltop1D,temp_cltop1D) |
---|
755 | ENDIF |
---|
756 | CALL icefrac_lscp(klon, zt(:), iflag_ice_thermo, distcltop1D(:),temp_cltop1D(:),zfice(:),dzfice(:)) |
---|
757 | |
---|
758 | DO i=1,klon !todoan : check if loop in i is needed |
---|
759 | |
---|
760 | IF ((keepgoing(i) .OR. (n_i(i) .EQ. 0)) .AND. lognormale(i)) THEN |
---|
761 | |
---|
762 | zpdf_sig(i)=ratqs(i,k)*zq(i) |
---|
763 | zpdf_k(i)=-sqrt(log(1.+(zpdf_sig(i)/zq(i))**2)) |
---|
764 | zpdf_delta(i)=log(zq(i)/(gammasat(i)*zqs(i))) |
---|
765 | zpdf_a(i)=zpdf_delta(i)/(zpdf_k(i)*sqrt(2.)) |
---|
766 | zpdf_b(i)=zpdf_k(i)/(2.*sqrt(2.)) |
---|
767 | zpdf_e1(i)=zpdf_a(i)-zpdf_b(i) |
---|
768 | zpdf_e1(i)=sign(min(ABS(zpdf_e1(i)),5.),zpdf_e1(i)) |
---|
769 | zpdf_e1(i)=1.-erf(zpdf_e1(i)) |
---|
770 | zpdf_e2(i)=zpdf_a(i)+zpdf_b(i) |
---|
771 | zpdf_e2(i)=sign(min(ABS(zpdf_e2(i)),5.),zpdf_e2(i)) |
---|
772 | zpdf_e2(i)=1.-erf(zpdf_e2(i)) |
---|
773 | |
---|
774 | IF ((.NOT.ok_ice_sursat).OR.(Tbef(i).GT.t_glace_min)) THEN |
---|
775 | |
---|
776 | IF (zpdf_e1(i).LT.1.e-10) THEN |
---|
777 | rneb(i,k)=0. |
---|
778 | zqn(i)=gammasat(i)*zqs(i) |
---|
779 | ELSE |
---|
780 | rneb(i,k)=0.5*zpdf_e1(i) |
---|
781 | zqn(i)=zq(i)*zpdf_e2(i)/zpdf_e1(i) |
---|
782 | ENDIF |
---|
783 | |
---|
784 | rnebss(i,k)=0.0 !--added by OB (needed because of the convergence loop on time) |
---|
785 | fcontrN(i,k)=0.0 !--idem |
---|
786 | fcontrP(i,k)=0.0 !--idem |
---|
787 | qss(i,k)=0.0 !--idem |
---|
788 | |
---|
789 | ELSE ! in case of ice supersaturation by Audran |
---|
790 | |
---|
791 | !------------------------------------ |
---|
792 | ! ICE SUPERSATURATION |
---|
793 | !------------------------------------ |
---|
794 | |
---|
795 | CALL ice_sursat(pplay(i,k), paprs(i,k)-paprs(i,k+1), dtime, i, k, temp(i,k), zq(i), & |
---|
796 | gamma_ss(i,k), zqs(i), Tbef(i), rneb_seri(i,k), ratqs(i,k), & |
---|
797 | rneb(i,k), zqn(i), rnebss(i,k), qss(i,k), & |
---|
798 | Tcontr(i,k), qcontr(i,k), qcontr2(i,k), fcontrN(i,k), fcontrP(i,k) ) |
---|
799 | |
---|
800 | ENDIF ! ((flag_ice_sursat.eq.0).or.(Tbef(i).gt.t_glace_min)) |
---|
801 | |
---|
802 | ! If vertical heterogeneity, change fraction by volume as well |
---|
803 | IF (iflag_cloudth_vert.GE.3) THEN |
---|
804 | ctot_vol(i,k)=rneb(i,k) |
---|
805 | rneblsvol(i,k)=ctot_vol(i,k) |
---|
806 | ENDIF |
---|
807 | |
---|
808 | |
---|
809 | ! P2.2.2> Approximative calculation of temperature variation DT |
---|
810 | ! due to condensation. |
---|
811 | ! Calculated variables: |
---|
812 | ! dT : temperature change due to condensation |
---|
813 | !--------------------------------------------------------------- |
---|
814 | |
---|
815 | |
---|
816 | IF (zfice(i).LT.1) THEN |
---|
817 | cste=RLVTT |
---|
818 | ELSE |
---|
819 | cste=RLSTT |
---|
820 | ENDIF |
---|
821 | |
---|
822 | qlbef(i)=max(0.,zqn(i)-zqs(i)) |
---|
823 | num = -Tbef(i)+zt(i)+rneb(i,k)*((1-zfice(i))*RLVTT & |
---|
824 | +zfice(i)*RLSTT)/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i)))*qlbef(i) |
---|
825 | denom = 1.+rneb(i,k)*((1-zfice(i))*RLVTT+zfice(i)*RLSTT)/cste*zdqs(i) & |
---|
826 | -(RLSTT-RLVTT)/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i)))*rneb(i,k) & |
---|
827 | *qlbef(i)*dzfice(i) |
---|
828 | ! here we update a provisory temperature variable that only serves in the iteration |
---|
829 | ! process |
---|
830 | DT(i)=num/denom |
---|
831 | n_i(i)=n_i(i)+1 |
---|
832 | |
---|
833 | ENDIF ! end keepgoing |
---|
834 | |
---|
835 | ENDDO ! end loop on i |
---|
836 | |
---|
837 | ENDDO ! iter=1,iflag_fisrtilp_qsat+1 |
---|
838 | |
---|
839 | ! P2.3> Final quantities calculation |
---|
840 | ! Calculated variables: |
---|
841 | ! rneb : cloud fraction |
---|
842 | ! zcond: mean condensed water in the mesh |
---|
843 | ! zqn : mean water vapor in the mesh |
---|
844 | ! zfice: ice fraction in clouds |
---|
845 | ! zt : temperature |
---|
846 | ! rhcl : clear-sky relative humidity |
---|
847 | ! ---------------------------------------------------------------- |
---|
848 | |
---|
849 | |
---|
850 | ! For iflag_t_glace GE 4 the phase partition function dependends on temperature AND distance to cloud top |
---|
851 | IF (iflag_t_glace.GE.4) THEN |
---|
852 | CALL distance_to_cloud_top(klon,klev,k,temp,pplay,paprs,rneb,distcltop1D,temp_cltop1D) |
---|
853 | distcltop(:,k)=distcltop1D(:) |
---|
854 | temp_cltop(:,k)=temp_cltop1D(:) |
---|
855 | ENDIF |
---|
856 | |
---|
857 | ! Partition function in stratiform clouds (will be overwritten in boundary-layer MPCs) |
---|
858 | CALL icefrac_lscp(klon,zt(:),iflag_ice_thermo,distcltop1D(:),temp_cltop1D(:),zfice(:), dzfice(:)) |
---|
859 | |
---|
860 | |
---|
861 | ! Water vapor update, Phase determination and subsequent latent heat exchange |
---|
862 | DO i=1, klon |
---|
863 | |
---|
864 | IF (mpc_bl_points(i,k) .GT. 0) THEN |
---|
865 | zcond(i) = MAX(0.0,qincloud_mpc(i))*rneb(i,k) |
---|
866 | ! following line is very strange and probably wrong |
---|
867 | rhcl(i,k)= (zqs(i)+zq(i))/2./zqs(i) |
---|
868 | ! water vapor update and partition function if thermals |
---|
869 | zq(i) = zq(i) - zcond(i) |
---|
870 | zfice(i)=icefrac_mpc(i,k) |
---|
871 | |
---|
872 | ELSE |
---|
873 | |
---|
874 | ! Checks on rneb, rhcl and zqn |
---|
875 | IF (rneb(i,k) .LE. 0.0) THEN |
---|
876 | zqn(i) = 0.0 |
---|
877 | rneb(i,k) = 0.0 |
---|
878 | zcond(i) = 0.0 |
---|
879 | rhcl(i,k)=zq(i)/zqs(i) |
---|
880 | ELSE IF (rneb(i,k) .GE. 1.0) THEN |
---|
881 | zqn(i) = zq(i) |
---|
882 | rneb(i,k) = 1.0 |
---|
883 | zcond(i) = MAX(0.0,zqn(i)-gammasat(i)*zqs(i)) |
---|
884 | rhcl(i,k)=1.0 |
---|
885 | ELSE |
---|
886 | zcond(i) = MAX(0.0,zqn(i)-gammasat(i)*zqs(i))*rneb(i,k) |
---|
887 | ! following line is very strange and probably wrong: |
---|
888 | rhcl(i,k)=(zqs(i)+zq(i))/2./zqs(i) |
---|
889 | ENDIF |
---|
890 | |
---|
891 | ! water vapor update |
---|
892 | zq(i) = zq(i) - zcond(i) |
---|
893 | |
---|
894 | ENDIF |
---|
895 | |
---|
896 | ! c_iso : routine that computes in-cloud supersaturation |
---|
897 | ! c_iso condensation of isotopes (zcond, zsursat, zfice, zq in input) |
---|
898 | |
---|
899 | ! temperature update due to phase change |
---|
900 | zt(i) = zt(i) + (1.-zfice(i))*zcond(i) & |
---|
901 | & * RLVTT/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i)+zcond(i))) & |
---|
902 | +zfice(i)*zcond(i) * RLSTT/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i)+zcond(i))) |
---|
903 | ENDDO |
---|
904 | |
---|
905 | ! If vertical heterogeneity, change volume fraction |
---|
906 | IF (iflag_cloudth_vert .GE. 3) THEN |
---|
907 | ctot_vol(1:klon,k)=min(max(ctot_vol(1:klon,k),0.),1.) |
---|
908 | rneblsvol(1:klon,k)=ctot_vol(1:klon,k) |
---|
909 | ENDIF |
---|
910 | |
---|
911 | ! ---------------------------------------------------------------- |
---|
912 | ! P3> Precipitation formation |
---|
913 | ! ---------------------------------------------------------------- |
---|
914 | |
---|
915 | ! LTP: |
---|
916 | IF (iflag_evap_prec .GE. 4) THEN |
---|
917 | |
---|
918 | !Partitionning between precipitation coming from clouds and that coming from CS |
---|
919 | |
---|
920 | !0) Calculate tot_zneb, total cloud fraction above the cloud |
---|
921 | !assuming a maximum-random overlap (voir Jakob and Klein, 2000) |
---|
922 | |
---|
923 | DO i=1, klon |
---|
924 | tot_znebn(i) = 1. - (1.-tot_zneb(i))*(1 - max(rneb(i,k),zneb(i))) & |
---|
925 | /(1.-min(zneb(i),1.-smallestreal)) |
---|
926 | d_tot_zneb(i) = tot_znebn(i) - tot_zneb(i) |
---|
927 | tot_zneb(i) = tot_znebn(i) |
---|
928 | |
---|
929 | |
---|
930 | !1) Cloudy to clear air |
---|
931 | d_znebprecip_cld_clr(i) = znebprecipcld(i) - min(rneb(i,k),znebprecipcld(i)) |
---|
932 | IF (znebprecipcld(i) .GT. 0.) THEN |
---|
933 | d_zrfl_cld_clr(i) = d_znebprecip_cld_clr(i)/znebprecipcld(i)*zrflcld(i) |
---|
934 | d_zifl_cld_clr(i) = d_znebprecip_cld_clr(i)/znebprecipcld(i)*ziflcld(i) |
---|
935 | ELSE |
---|
936 | d_zrfl_cld_clr(i) = 0. |
---|
937 | d_zifl_cld_clr(i) = 0. |
---|
938 | ENDIF |
---|
939 | |
---|
940 | !2) Clear to cloudy air |
---|
941 | d_znebprecip_clr_cld(i) = max(0., min(znebprecipclr(i), rneb(i,k) - d_tot_zneb(i) - zneb(i))) |
---|
942 | IF (znebprecipclr(i) .GT. 0) THEN |
---|
943 | d_zrfl_clr_cld(i) = d_znebprecip_clr_cld(i)/znebprecipclr(i)*zrflclr(i) |
---|
944 | d_zifl_clr_cld(i) = d_znebprecip_clr_cld(i)/znebprecipclr(i)*ziflclr(i) |
---|
945 | ELSE |
---|
946 | d_zrfl_clr_cld(i) = 0. |
---|
947 | d_zifl_clr_cld(i) = 0. |
---|
948 | ENDIF |
---|
949 | |
---|
950 | !Update variables |
---|
951 | znebprecipcld(i) = znebprecipcld(i) + d_znebprecip_clr_cld(i) - d_znebprecip_cld_clr(i) |
---|
952 | znebprecipclr(i) = znebprecipclr(i) + d_znebprecip_cld_clr(i) - d_znebprecip_clr_cld(i) |
---|
953 | zrflcld(i) = zrflcld(i) + d_zrfl_clr_cld(i) - d_zrfl_cld_clr(i) |
---|
954 | ziflcld(i) = ziflcld(i) + d_zifl_clr_cld(i) - d_zifl_cld_clr(i) |
---|
955 | zrflclr(i) = zrflclr(i) + d_zrfl_cld_clr(i) - d_zrfl_clr_cld(i) |
---|
956 | ziflclr(i) = ziflclr(i) + d_zifl_cld_clr(i) - d_zifl_clr_cld(i) |
---|
957 | |
---|
958 | ! c_iso do the same thing for isotopes precip |
---|
959 | ENDDO |
---|
960 | ENDIF |
---|
961 | |
---|
962 | |
---|
963 | ! Autoconversion |
---|
964 | ! ------------------------------------------------------------------------------- |
---|
965 | |
---|
966 | |
---|
967 | ! Initialisation of zoliq and radocond variables |
---|
968 | |
---|
969 | DO i = 1, klon |
---|
970 | zoliq(i) = zcond(i) |
---|
971 | zoliqi(i)= zoliq(i)*zfice(i) |
---|
972 | zoliql(i)= zoliq(i)*(1.-zfice(i)) |
---|
973 | ! c_iso : initialisation of zoliq* also for isotopes |
---|
974 | zrho(i,k) = pplay(i,k) / zt(i) / RD |
---|
975 | zdz(i) = (paprs(i,k)-paprs(i,k+1)) / (zrho(i,k)*RG) |
---|
976 | iwc(i) = 0. |
---|
977 | zneb(i) = MAX(rneb(i,k),seuil_neb) |
---|
978 | radocond(i,k) = zoliq(i)/REAL(niter_lscp+1) |
---|
979 | radicefrac(i,k) = zfice(i) |
---|
980 | radocondi(i,k)=zoliq(i)*zfice(i)/REAL(niter_lscp+1) |
---|
981 | radocondl(i,k)=zoliq(i)*(1.-zfice(i))/REAL(niter_lscp+1) |
---|
982 | ENDDO |
---|
983 | |
---|
984 | |
---|
985 | DO n = 1, niter_lscp |
---|
986 | |
---|
987 | DO i=1,klon |
---|
988 | IF (rneb(i,k).GT.0.0) THEN |
---|
989 | iwc(i) = zrho(i,k) * zoliqi(i) / zneb(i) ! in-cloud ice condensate content |
---|
990 | ENDIF |
---|
991 | ENDDO |
---|
992 | |
---|
993 | CALL fallice_velocity(klon,iwc(:),zt(:),zrho(:,k),pplay(:,k),ptconv(:,k),velo(:,k)) |
---|
994 | |
---|
995 | DO i = 1, klon |
---|
996 | |
---|
997 | IF (rneb(i,k).GT.0.0) THEN |
---|
998 | |
---|
999 | ! Initialization of zrain, zsnow and zprecip: |
---|
1000 | zrain=0. |
---|
1001 | zsnow=0. |
---|
1002 | zprecip=0. |
---|
1003 | ! c_iso same init for isotopes. Externalisation? |
---|
1004 | |
---|
1005 | IF (zneb(i).EQ.seuil_neb) THEN |
---|
1006 | zprecip = 0.0 |
---|
1007 | zsnow = 0.0 |
---|
1008 | zrain= 0.0 |
---|
1009 | ELSE |
---|
1010 | |
---|
1011 | IF (ptconv(i,k)) THEN ! if convective point |
---|
1012 | zcl=cld_lc_con |
---|
1013 | zct=1./cld_tau_con |
---|
1014 | zexpo=cld_expo_con |
---|
1015 | ffallv=ffallv_con |
---|
1016 | ELSE |
---|
1017 | zcl=cld_lc_lsc |
---|
1018 | zct=1./cld_tau_lsc |
---|
1019 | zexpo=cld_expo_lsc |
---|
1020 | ffallv=ffallv_lsc |
---|
1021 | ENDIF |
---|
1022 | |
---|
1023 | |
---|
1024 | ! if vertical heterogeneity is taken into account, we use |
---|
1025 | ! the "true" volume fraction instead of a modified |
---|
1026 | ! surface fraction (which is larger and artificially |
---|
1027 | ! reduces the in-cloud water). |
---|
1028 | |
---|
1029 | ! Liquid water quantity to remove: zchau (Sundqvist, 1978) |
---|
1030 | ! dqliq/dt=-qliq/tau*(1-exp(-qcin/clw)**2) |
---|
1031 | !......................................................... |
---|
1032 | IF ((iflag_cloudth_vert.GE.3).AND.(iflag_rain_incloud_vol.EQ.1)) THEN |
---|
1033 | |
---|
1034 | ! if vertical heterogeneity is taken into account, we use |
---|
1035 | ! the "true" volume fraction instead of a modified |
---|
1036 | ! surface fraction (which is larger and artificially |
---|
1037 | ! reduces the in-cloud water). |
---|
1038 | effective_zneb=ctot_vol(i,k) |
---|
1039 | ELSE |
---|
1040 | effective_zneb=zneb(i) |
---|
1041 | ENDIF |
---|
1042 | |
---|
1043 | |
---|
1044 | IF (iflag_autoconversion .EQ. 2) THEN |
---|
1045 | ! two-steps resolution with niter_lscp=1 sufficient |
---|
1046 | ! we first treat the second term (with exponential) in an explicit way |
---|
1047 | ! and then treat the first term (-q/tau) in an exact way |
---|
1048 | zchau=zoliql(i)*(1.-exp(-dtime/REAL(niter_lscp)*zct & |
---|
1049 | *(1.-exp(-(zoliql(i)/effective_zneb/zcl)**zexpo)))) |
---|
1050 | ELSE |
---|
1051 | ! old explicit resolution with subtimesteps |
---|
1052 | zchau = zct*dtime/REAL(niter_lscp)*zoliql(i) & |
---|
1053 | *(1.0-EXP(-(zoliql(i)/effective_zneb/zcl)**zexpo)) |
---|
1054 | ENDIF |
---|
1055 | |
---|
1056 | |
---|
1057 | ! Ice water quantity to remove (Zender & Kiehl, 1997) |
---|
1058 | ! dqice/dt=1/rho*d(rho*wice*qice)/dz |
---|
1059 | !.................................... |
---|
1060 | IF (iflag_autoconversion .EQ. 2) THEN |
---|
1061 | ! exact resolution, niter_lscp=1 is sufficient but works only |
---|
1062 | ! with iflag_vice=0 |
---|
1063 | IF (zoliqi(i) .GT. 0.) THEN |
---|
1064 | zfroi=(zoliqi(i)-((zoliqi(i)**(-dice_velo)) & |
---|
1065 | +dice_velo*dtime/REAL(niter_lscp)*cice_velo/zdz(i)*ffallv)**(-1./dice_velo)) |
---|
1066 | ELSE |
---|
1067 | zfroi=0. |
---|
1068 | ENDIF |
---|
1069 | ELSE |
---|
1070 | ! old explicit resolution with subtimesteps |
---|
1071 | zfroi = dtime/REAL(niter_lscp)/zdz(i)*zoliqi(i)*velo(i,k) |
---|
1072 | ENDIF |
---|
1073 | |
---|
1074 | zrain = MIN(MAX(zchau,0.0),zoliql(i)) |
---|
1075 | zsnow = MIN(MAX(zfroi,0.0),zoliqi(i)) |
---|
1076 | zprecip = MAX(zrain + zsnow,0.0) |
---|
1077 | |
---|
1078 | ENDIF |
---|
1079 | |
---|
1080 | IF (iflag_autoconversion .GE. 1) THEN |
---|
1081 | ! debugged version with phase conservation through the autoconversion process |
---|
1082 | zoliql(i) = MAX(zoliql(i)-1.*zrain , 0.0) |
---|
1083 | zoliqi(i) = MAX(zoliqi(i)-1.*zsnow , 0.0) |
---|
1084 | zoliq(i) = MAX(zoliq(i)-zprecip , 0.0) |
---|
1085 | ELSE |
---|
1086 | ! bugged version with phase resetting |
---|
1087 | zoliql(i) = MAX(zoliq(i)*(1.-zfice(i))-1.*zrain , 0.0) |
---|
1088 | zoliqi(i) = MAX(zoliq(i)*zfice(i)-1.*zsnow , 0.0) |
---|
1089 | zoliq(i) = MAX(zoliq(i)-zprecip , 0.0) |
---|
1090 | ENDIF |
---|
1091 | |
---|
1092 | ! c_iso: call isotope_conversion (for readibility) or duplicate |
---|
1093 | |
---|
1094 | radocond(i,k) = radocond(i,k) + zoliq(i)/REAL(niter_lscp+1) |
---|
1095 | radocondl(i,k) = radocondl(i,k) + zoliql(i)/REAL(niter_lscp+1) |
---|
1096 | radocondi(i,k) = radocondi(i,k) + zoliqi(i)/REAL(niter_lscp+1) |
---|
1097 | |
---|
1098 | ENDIF ! rneb >0 |
---|
1099 | |
---|
1100 | ENDDO ! i = 1,klon |
---|
1101 | |
---|
1102 | ENDDO ! n = 1,niter |
---|
1103 | |
---|
1104 | ! Precipitation flux calculation |
---|
1105 | |
---|
1106 | DO i = 1, klon |
---|
1107 | |
---|
1108 | IF (iflag_evap_prec.GE.4) THEN |
---|
1109 | ziflprev(i)=ziflcld(i) |
---|
1110 | ELSE |
---|
1111 | ziflprev(i)=zifl(i)*zneb(i) |
---|
1112 | ENDIF |
---|
1113 | |
---|
1114 | IF (rneb(i,k) .GT. 0.0) THEN |
---|
1115 | |
---|
1116 | ! CR&JYG: We account for the Wegener-Findeisen-Bergeron process in the precipitation flux: |
---|
1117 | ! If T<0C, liquid precip are converted into ice, which leads to an increase in |
---|
1118 | ! temperature DeltaT. The effect of DeltaT on condensates and precipitation is roughly |
---|
1119 | ! taken into account through a linearization of the equations and by approximating |
---|
1120 | ! the liquid precipitation process with a "threshold" process. We assume that |
---|
1121 | ! condensates are not modified during this operation. Liquid precipitation is |
---|
1122 | ! removed (in the limit DeltaT<273.15-T). Solid precipitation increases. |
---|
1123 | ! Water vapor increases as well |
---|
1124 | ! Note that compared to fisrtilp, we always assume iflag_bergeron=2 |
---|
1125 | |
---|
1126 | zqpreci(i)=(zcond(i)-zoliq(i))*zfice(i) |
---|
1127 | zqprecl(i)=(zcond(i)-zoliq(i))*(1.-zfice(i)) |
---|
1128 | zcp=RCPD*(1.0+RVTMP2*(zq(i)+zmqc(i)+zcond(i))) |
---|
1129 | coef1 = rneb(i,k)*RLSTT/zcp*zdqsdT_raw(i) |
---|
1130 | ! Computation of DT if all the liquid precip freezes |
---|
1131 | DeltaT = RLMLT*zqprecl(i) / (zcp*(1.+coef1)) |
---|
1132 | ! T should not exceed the freezing point |
---|
1133 | ! that is Delta > RTT-zt(i) |
---|
1134 | DeltaT = max( min( RTT-zt(i), DeltaT) , 0. ) |
---|
1135 | zt(i) = zt(i) + DeltaT |
---|
1136 | ! water vaporization due to temp. increase |
---|
1137 | Deltaq = rneb(i,k)*zdqsdT_raw(i)*DeltaT |
---|
1138 | ! we add this vaporized water to the total vapor and we remove it from the precip |
---|
1139 | zq(i) = zq(i) + Deltaq |
---|
1140 | ! The three "max" lines herebelow protect from rounding errors |
---|
1141 | zcond(i) = max( zcond(i)- Deltaq, 0. ) |
---|
1142 | ! liquid precipitation converted to ice precip |
---|
1143 | Deltaqprecl = -zcp/RLMLT*(1.+coef1)*DeltaT |
---|
1144 | zqprecl(i) = max( zqprecl(i) + Deltaqprecl, 0. ) |
---|
1145 | ! iced water budget |
---|
1146 | zqpreci(i) = max (zqpreci(i) - Deltaqprecl - Deltaq, 0.) |
---|
1147 | |
---|
1148 | ! c_iso : mv here condensation of isotopes + redispatchage en precip |
---|
1149 | |
---|
1150 | IF (iflag_evap_prec.GE.4) THEN |
---|
1151 | zrflcld(i) = zrflcld(i)+zqprecl(i) & |
---|
1152 | *(paprs(i,k)-paprs(i,k+1))/(RG*dtime) |
---|
1153 | ziflcld(i) = ziflcld(i)+ zqpreci(i) & |
---|
1154 | *(paprs(i,k)-paprs(i,k+1))/(RG*dtime) |
---|
1155 | znebprecipcld(i) = rneb(i,k) |
---|
1156 | zrfl(i) = zrflcld(i) + zrflclr(i) |
---|
1157 | zifl(i) = ziflcld(i) + ziflclr(i) |
---|
1158 | ELSE |
---|
1159 | zrfl(i) = zrfl(i)+ zqprecl(i) & |
---|
1160 | *(paprs(i,k)-paprs(i,k+1))/(RG*dtime) |
---|
1161 | zifl(i) = zifl(i)+ zqpreci(i) & |
---|
1162 | *(paprs(i,k)-paprs(i,k+1))/(RG*dtime) |
---|
1163 | ENDIF |
---|
1164 | ! c_iso : same for isotopes |
---|
1165 | |
---|
1166 | ENDIF ! rneb>0 |
---|
1167 | |
---|
1168 | ENDDO |
---|
1169 | |
---|
1170 | ! LTP: limit of surface cloud fraction covered by precipitation when the local intensity of the flux is below rain_int_min |
---|
1171 | ! if iflag_evap_prec>=4 |
---|
1172 | IF (iflag_evap_prec.GE.4) THEN |
---|
1173 | |
---|
1174 | DO i=1,klon |
---|
1175 | |
---|
1176 | IF ((zrflclr(i) + ziflclr(i)) .GT. 0. ) THEN |
---|
1177 | znebprecipclr(i) = min(znebprecipclr(i),max(zrflclr(i)/ & |
---|
1178 | (MAX(znebprecipclr(i),seuil_neb)*rain_int_min), ziflclr(i)/(MAX(znebprecipclr(i),seuil_neb)*rain_int_min))) |
---|
1179 | ELSE |
---|
1180 | znebprecipclr(i)=0.0 |
---|
1181 | ENDIF |
---|
1182 | |
---|
1183 | IF ((zrflcld(i) + ziflcld(i)) .GT. 0.) THEN |
---|
1184 | znebprecipcld(i) = min(znebprecipcld(i), max(zrflcld(i)/ & |
---|
1185 | (MAX(znebprecipcld(i),seuil_neb)*rain_int_min), ziflcld(i)/(MAX(znebprecipcld(i),seuil_neb)*rain_int_min))) |
---|
1186 | ELSE |
---|
1187 | znebprecipcld(i)=0.0 |
---|
1188 | ENDIF |
---|
1189 | |
---|
1190 | ENDDO |
---|
1191 | |
---|
1192 | |
---|
1193 | ENDIF |
---|
1194 | |
---|
1195 | ! End of precipitation formation |
---|
1196 | ! -------------------------------- |
---|
1197 | |
---|
1198 | ! Outputs: |
---|
1199 | ! Precipitation fluxes at layer interfaces |
---|
1200 | ! + precipitation fractions + |
---|
1201 | ! temperature and water species tendencies |
---|
1202 | DO i = 1, klon |
---|
1203 | psfl(i,k)=zifl(i) |
---|
1204 | prfl(i,k)=zrfl(i) |
---|
1205 | pfraclr(i,k)=znebprecipclr(i) |
---|
1206 | pfracld(i,k)=znebprecipcld(i) |
---|
1207 | d_ql(i,k) = (1-zfice(i))*zoliq(i) |
---|
1208 | d_qi(i,k) = zfice(i)*zoliq(i) |
---|
1209 | d_q(i,k) = zq(i) - q(i,k) |
---|
1210 | ! c_iso: same for isotopes |
---|
1211 | d_t(i,k) = zt(i) - temp(i,k) |
---|
1212 | ENDDO |
---|
1213 | |
---|
1214 | ! Calculation of the concentration of condensates seen by the radiation scheme |
---|
1215 | ! for liquid phase, we take radocondl |
---|
1216 | ! for ice phase, we take radocondi if we neglect snowfall, otherwise (ok_radocond_snow=true) |
---|
1217 | ! we recaulate radocondi to account for contributions from the precipitation flux |
---|
1218 | |
---|
1219 | IF ((ok_radocond_snow) .AND. (k .LT. klev)) THEN |
---|
1220 | ! for the solid phase (crystals + snowflakes) |
---|
1221 | ! we recalculate radocondi by summing |
---|
1222 | ! the ice content calculated in the mesh |
---|
1223 | ! + the contribution of the non-evaporated snowfall |
---|
1224 | ! from the overlying layer |
---|
1225 | DO i=1,klon |
---|
1226 | IF (ziflprev(i) .NE. 0.0) THEN |
---|
1227 | radocondi(i,k)=zoliq(i)*zfice(i)+zqpreci(i)+ziflprev(i)/zrho(i,k+1)/velo(i,k+1) |
---|
1228 | ELSE |
---|
1229 | radocondi(i,k)=zoliq(i)*zfice(i)+zqpreci(i) |
---|
1230 | ENDIF |
---|
1231 | radocond(i,k)=radocondl(i,k)+radocondi(i,k) |
---|
1232 | ENDDO |
---|
1233 | ENDIF |
---|
1234 | |
---|
1235 | ! caculate the percentage of ice in "radocond" so cloud+precip seen by the radiation scheme |
---|
1236 | DO i=1,klon |
---|
1237 | IF (radocond(i,k) .GT. 0.) THEN |
---|
1238 | radicefrac(i,k)=MIN(MAX(radocondi(i,k)/radocond(i,k),0.),1.) |
---|
1239 | ENDIF |
---|
1240 | ENDDO |
---|
1241 | |
---|
1242 | ! ---------------------------------------------------------------- |
---|
1243 | ! P4> Wet scavenging |
---|
1244 | ! ---------------------------------------------------------------- |
---|
1245 | |
---|
1246 | !Scavenging through nucleation in the layer |
---|
1247 | |
---|
1248 | DO i = 1,klon |
---|
1249 | |
---|
1250 | IF(zcond(i).GT.zoliq(i)+1.e-10) THEN |
---|
1251 | beta(i,k) = (zcond(i)-zoliq(i))/zcond(i)/dtime |
---|
1252 | ELSE |
---|
1253 | beta(i,k) = 0. |
---|
1254 | ENDIF |
---|
1255 | |
---|
1256 | zprec_cond(i) = MAX(zcond(i)-zoliq(i),0.0)*(paprs(i,k)-paprs(i,k+1))/RG |
---|
1257 | |
---|
1258 | IF (rneb(i,k).GT.0.0.AND.zprec_cond(i).GT.0.) THEN |
---|
1259 | |
---|
1260 | IF (temp(i,k) .GE. t_glace_min) THEN |
---|
1261 | zalpha_tr = a_tr_sca(3) |
---|
1262 | ELSE |
---|
1263 | zalpha_tr = a_tr_sca(4) |
---|
1264 | ENDIF |
---|
1265 | |
---|
1266 | zfrac_lessi = 1. - EXP(zalpha_tr*zprec_cond(i)/zneb(i)) |
---|
1267 | frac_nucl(i,k)= 1.-zneb(i)*zfrac_lessi |
---|
1268 | |
---|
1269 | ! Nucleation with a factor of -1 instead of -0.5 |
---|
1270 | zfrac_lessi = 1. - EXP(-zprec_cond(i)/zneb(i)) |
---|
1271 | |
---|
1272 | ENDIF |
---|
1273 | |
---|
1274 | ENDDO |
---|
1275 | |
---|
1276 | ! Scavenging through impaction in the underlying layer |
---|
1277 | |
---|
1278 | DO kk = k-1, 1, -1 |
---|
1279 | |
---|
1280 | DO i = 1, klon |
---|
1281 | |
---|
1282 | IF (rneb(i,k).GT.0.0.AND.zprec_cond(i).GT.0.) THEN |
---|
1283 | |
---|
1284 | IF (temp(i,kk) .GE. t_glace_min) THEN |
---|
1285 | zalpha_tr = a_tr_sca(1) |
---|
1286 | ELSE |
---|
1287 | zalpha_tr = a_tr_sca(2) |
---|
1288 | ENDIF |
---|
1289 | |
---|
1290 | zfrac_lessi = 1. - EXP(zalpha_tr*zprec_cond(i)/zneb(i)) |
---|
1291 | frac_impa(i,kk)= 1.-zneb(i)*zfrac_lessi |
---|
1292 | |
---|
1293 | ENDIF |
---|
1294 | |
---|
1295 | ENDDO |
---|
1296 | |
---|
1297 | ENDDO |
---|
1298 | |
---|
1299 | !--save some variables for ice supersaturation |
---|
1300 | ! |
---|
1301 | DO i = 1, klon |
---|
1302 | ! for memory |
---|
1303 | rneb_seri(i,k) = rneb(i,k) |
---|
1304 | |
---|
1305 | ! for diagnostics |
---|
1306 | rnebclr(i,k) = 1.0 - rneb(i,k) - rnebss(i,k) |
---|
1307 | |
---|
1308 | qvc(i,k) = zqs(i) * rneb(i,k) |
---|
1309 | qclr(i,k) = MAX(1.e-10,zq(i) - qvc(i,k) - qss(i,k)) !--added by OB because of pathologic cases with the lognormal |
---|
1310 | qcld(i,k) = qvc(i,k) + zcond(i) |
---|
1311 | ENDDO |
---|
1312 | !q_sat |
---|
1313 | CALL calc_qsat_ecmwf(klon,Tbef(:),qzero(:),pplay(:,k),RTT,1,.false.,qsatl(:,k),zdqs(:)) |
---|
1314 | CALL calc_qsat_ecmwf(klon,Tbef(:),qzero(:),pplay(:,k),RTT,2,.false.,qsats(:,k),zdqs(:)) |
---|
1315 | |
---|
1316 | ENDDO |
---|
1317 | |
---|
1318 | !====================================================================== |
---|
1319 | ! END OF VERTICAL LOOP |
---|
1320 | !====================================================================== |
---|
1321 | |
---|
1322 | ! Rain or snow at the surface (depending on the first layer temperature) |
---|
1323 | DO i = 1, klon |
---|
1324 | snow(i) = zifl(i) |
---|
1325 | rain(i) = zrfl(i) |
---|
1326 | ! c_iso final output |
---|
1327 | ENDDO |
---|
1328 | |
---|
1329 | IF (ncoreczq>0) THEN |
---|
1330 | WRITE(lunout,*)'WARNING : ZQ in LSCP ',ncoreczq,' val < 1.e-15.' |
---|
1331 | ENDIF |
---|
1332 | |
---|
1333 | |
---|
1334 | RETURN |
---|
1335 | |
---|
1336 | END SUBROUTINE lscp |
---|
1337 | !+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
---|
1338 | |
---|
1339 | END MODULE lscp_mod |
---|