1 | MODULE lmdz_lscp |
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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,qt,qice_save,ptconv,ratqs, & |
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10 | d_t, d_q, d_ql, d_qi, rneb, rneblsvol, & |
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11 | pfraclr, pfracld, & |
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12 | cldfraliq, sigma2_icefracturb,mean_icefracturb, & |
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13 | radocond, radicefrac, rain, snow, & |
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14 | frac_impa, frac_nucl, beta, & |
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15 | prfl, psfl, rhcl, qta, fraca, & |
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16 | tv, pspsk, tla, thl, iflag_cld_th, & |
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17 | iflag_ice_thermo, distcltop, temp_cltop, & |
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18 | tke, tke_dissip, & |
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19 | cell_area, & |
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20 | cf_seri, rvc_seri, u_seri, v_seri, & |
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21 | qsub, qissr, qcld, subfra, issrfra, gamma_cond, & |
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22 | ratio_qi_qtot, dcf_sub, dcf_con, dcf_mix, & |
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23 | dqi_adj, dqi_sub, dqi_con, dqi_mix, dqvc_adj, & |
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24 | dqvc_sub, dqvc_con, dqvc_mix, qsatl, qsati, & |
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25 | Tcontr, qcontr, qcontr2, fcontrN, fcontrP, dcf_avi,& |
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26 | dqi_avi, dqvc_avi, flight_dist, flight_h2o, & |
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27 | cloudth_sth,cloudth_senv,cloudth_sigmath,cloudth_sigmaenv, & |
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28 | qraindiag, qsnowdiag, dqreva, dqssub, dqrauto, & |
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29 | dqrcol, dqrmelt, dqrfreez, dqsauto, dqsagg, dqsrim,& |
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30 | dqsmelt, dqsfreez) |
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31 | |
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32 | !++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
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33 | ! Authors: Z.X. Li (LMD), J-L Dufresne (LMD), C. Rio (LMD), J-Y Grandpeix (LMD) |
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34 | ! A. JAM (LMD), J-B Madeleine (LMD), E. Vignon (LMD), L. Touzze-Peiffert (LMD) |
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35 | !-------------------------------------------------------------------------------- |
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36 | ! Date: 01/2021 |
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37 | !-------------------------------------------------------------------------------- |
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38 | ! Aim: Large Scale Clouds and Precipitation (LSCP) |
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39 | ! |
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40 | ! This code is a new version of the fisrtilp.F90 routine, which is itself a |
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41 | ! merge of 'first' (superrsaturation physics, P. LeVan K. Laval) |
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42 | ! and 'ilp' (il pleut, L. Li) |
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43 | ! |
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44 | ! Compared to the original fisrtilp code, lscp |
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45 | ! -> assumes thermcep = .TRUE. all the time (fisrtilp inconsistent when .FALSE.) |
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46 | ! -> consider always precipitation thermalisation (fl_cor_ebil>0) |
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47 | ! -> option iflag_fisrtilp_qsat<0 no longer possible (qsat does not evolve with T) |
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48 | ! -> option "oldbug" by JYG has been removed |
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49 | ! -> iflag_t_glace >0 always |
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50 | ! -> the 'all or nothing' cloud approach is no longer available (cpartiel=T always) |
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51 | ! -> rectangular distribution from L. Li no longer available |
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52 | ! -> We always account for the Wegener-Findeisen-Bergeron process (iflag_bergeron = 2 in fisrt) |
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53 | !-------------------------------------------------------------------------------- |
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54 | ! References: |
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55 | ! |
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56 | ! - Bony, S., & Emanuel, K. A. 2001, JAS, doi: 10.1175/1520-0469(2001)058<3158:APOTCA>2.0.CO;2 |
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57 | ! - Hourdin et al. 2013, Clim Dyn, doi:10.1007/s00382-012-1343-y |
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58 | ! - Jam et al. 2013, Boundary-Layer Meteorol, doi:10.1007/s10546-012-9789-3 |
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59 | ! - Jouhaud, et al. 2018. JAMES, doi:10.1029/2018MS001379 |
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60 | ! - Madeleine et al. 2020, JAMES, doi:10.1029/2020MS002046 |
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61 | ! - Touzze-Peifert Ludo, PhD thesis, p117-124 |
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62 | ! ------------------------------------------------------------------------------- |
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63 | ! Code structure: |
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64 | ! |
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65 | ! P0> Thermalization of the precipitation coming from the overlying layer |
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66 | ! P1> Evaporation of the precipitation (falling from the k+1 level) |
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67 | ! P2> Cloud formation (at the k level) |
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68 | ! P2.A.1> With the PDFs, calculation of cloud properties using the inital |
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69 | ! values of T and Q |
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70 | ! P2.A.2> Coupling between condensed water and temperature |
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71 | ! P2.A.3> Calculation of final quantities associated with cloud formation |
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72 | ! P2.B> Release of Latent heat after cloud formation |
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73 | ! P3> Autoconversion to precipitation (k-level) |
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74 | ! P4> Wet scavenging |
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75 | !------------------------------------------------------------------------------ |
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76 | ! Some preliminary comments (JBM) : |
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77 | ! |
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78 | ! The cloud water that the radiation scheme sees is not the same that the cloud |
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79 | ! water used in the physics and the dynamics |
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80 | ! |
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81 | ! During the autoconversion to precipitation (P3 step), radocond (cloud water used |
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82 | ! by the radiation scheme) is calculated as an average of the water that remains |
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83 | ! in the cloud during the precipitation and not the water remaining at the end |
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84 | ! of the time step. The latter is used in the rest of the physics and advected |
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85 | ! by the dynamics. |
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86 | ! |
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87 | ! In summary: |
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88 | ! |
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89 | ! Radiation: |
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90 | ! xflwc(newmicro)+xfiwc(newmicro) = |
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91 | ! radocond=lwcon(nc)+iwcon(nc) |
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92 | ! |
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93 | ! Notetheless, be aware of: |
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94 | ! |
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95 | ! radocond .NE. ocond(nc) |
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96 | ! i.e.: |
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97 | ! lwcon(nc)+iwcon(nc) .NE. ocond(nc) |
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98 | ! but oliq+(ocond-oliq) .EQ. ocond |
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99 | ! (which is not trivial) |
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100 | !++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
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101 | ! |
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102 | |
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103 | ! USE de modules contenant des fonctions. |
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104 | USE lmdz_cloudth, ONLY : cloudth, cloudth_v3, cloudth_v6, cloudth_mpc |
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105 | USE lmdz_lscp_tools, ONLY : calc_qsat_ecmwf, calc_gammasat |
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106 | USE lmdz_lscp_tools, ONLY : icefrac_lscp, icefrac_lscp_turb |
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107 | USE lmdz_lscp_tools, ONLY : fallice_velocity, distance_to_cloud_top |
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108 | USE lmdz_lscp_condensation, ONLY : condensation_lognormal, condensation_ice_supersat |
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109 | USE lmdz_lscp_poprecip, ONLY : poprecip_precld, poprecip_postcld |
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110 | |
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111 | ! Use du module lmdz_lscp_ini contenant les constantes |
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112 | USE lmdz_lscp_ini, ONLY : prt_level, lunout, eps |
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113 | USE lmdz_lscp_ini, ONLY : seuil_neb, niter_lscp, iflag_evap_prec, t_coup, DDT0, ztfondue, rain_int_min |
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114 | USE lmdz_lscp_ini, ONLY : ok_radocond_snow, a_tr_sca, cld_expo_con, cld_expo_lsc |
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115 | USE lmdz_lscp_ini, ONLY : iflag_cloudth_vert, iflag_rain_incloud_vol, iflag_t_glace, t_glace_min |
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116 | USE lmdz_lscp_ini, ONLY : coef_eva, coef_sub,cld_tau_lsc, cld_tau_con, cld_lc_lsc, cld_lc_con |
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117 | USE lmdz_lscp_ini, ONLY : iflag_bergeron, iflag_fisrtilp_qsat, iflag_vice, cice_velo, dice_velo |
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118 | USE lmdz_lscp_ini, ONLY : iflag_autoconversion, ffallv_con, ffallv_lsc, min_frac_th_cld |
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119 | USE lmdz_lscp_ini, ONLY : RCPD, RLSTT, RLVTT, RLMLT, RVTMP2, RTT, RD, RG |
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120 | USE lmdz_lscp_ini, ONLY : ok_poprecip |
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121 | USE lmdz_lscp_ini, ONLY : ok_external_lognormal, ok_ice_supersat, ok_unadjusted_clouds, iflag_icefrac |
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122 | |
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123 | IMPLICIT NONE |
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124 | |
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125 | !=============================================================================== |
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126 | ! VARIABLES DECLARATION |
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127 | !=============================================================================== |
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128 | |
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129 | ! INPUT VARIABLES: |
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130 | !----------------- |
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131 | |
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132 | INTEGER, INTENT(IN) :: klon,klev ! number of horizontal grid points and vertical levels |
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133 | REAL, INTENT(IN) :: dtime ! time step [s] |
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134 | REAL, INTENT(IN) :: missing_val ! missing value for output |
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135 | |
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136 | REAL, DIMENSION(klon,klev+1), INTENT(IN) :: paprs ! inter-layer pressure [Pa] |
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137 | REAL, DIMENSION(klon,klev), INTENT(IN) :: pplay ! mid-layer pressure [Pa] |
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138 | REAL, DIMENSION(klon,klev), INTENT(IN) :: temp ! temperature (K) |
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139 | REAL, DIMENSION(klon,klev), INTENT(IN) :: qt ! total specific humidity (in vapor phase in input) [kg/kg] |
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140 | REAL, DIMENSION(klon,klev), INTENT(IN) :: qice_save ! ice specific from previous time step [kg/kg] |
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141 | INTEGER, INTENT(IN) :: iflag_cld_th ! flag that determines the distribution of convective clouds |
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142 | INTEGER, INTENT(IN) :: iflag_ice_thermo! flag to activate the ice thermodynamics |
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143 | ! CR: if iflag_ice_thermo=2, only convection is active |
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144 | LOGICAL, DIMENSION(klon,klev), INTENT(IN) :: ptconv ! grid points where deep convection scheme is active |
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145 | |
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146 | !Inputs associated with thermal plumes |
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147 | |
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148 | REAL, DIMENSION(klon,klev), INTENT(IN) :: tv ! virtual potential temperature [K] |
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149 | REAL, DIMENSION(klon,klev), INTENT(IN) :: qta ! specific humidity within thermals [kg/kg] |
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150 | REAL, DIMENSION(klon,klev), INTENT(IN) :: fraca ! fraction of thermals within the mesh [-] |
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151 | REAL, DIMENSION(klon,klev), INTENT(IN) :: pspsk ! exner potential (p/100000)**(R/cp) |
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152 | REAL, DIMENSION(klon,klev), INTENT(IN) :: tla ! liquid temperature within thermals [K] |
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153 | REAL, DIMENSION(klon,klev+1), INTENT(IN) :: tke !--turbulent kinetic energy [m2/s2] |
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154 | REAL, DIMENSION(klon,klev+1), INTENT(IN) :: tke_dissip !--TKE dissipation [m2/s3] |
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155 | |
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156 | ! INPUT/OUTPUT variables |
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157 | !------------------------ |
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158 | |
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159 | REAL, DIMENSION(klon,klev), INTENT(INOUT) :: thl ! liquid potential temperature [K] |
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160 | REAL, DIMENSION(klon,klev), INTENT(INOUT) :: ratqs ! function of pressure that sets the large-scale |
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161 | |
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162 | ! INPUT/OUTPUT condensation and ice supersaturation |
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163 | !-------------------------------------------------- |
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164 | REAL, DIMENSION(klon,klev), INTENT(INOUT):: cf_seri ! cloud fraction [-] |
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165 | REAL, DIMENSION(klon,klev), INTENT(INOUT):: ratio_qi_qtot ! solid specific water to total specific water ratio [-] |
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166 | REAL, DIMENSION(klon,klev), INTENT(INOUT):: rvc_seri ! cloudy water vapor to total water vapor ratio [-] |
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167 | REAL, DIMENSION(klon,klev), INTENT(IN) :: u_seri ! eastward wind [m/s] |
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168 | REAL, DIMENSION(klon,klev), INTENT(IN) :: v_seri ! northward wind [m/s] |
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169 | REAL, DIMENSION(klon), INTENT(IN) :: cell_area ! area of each cell [m2] |
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170 | |
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171 | ! INPUT/OUTPUT aviation |
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172 | !-------------------------------------------------- |
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173 | REAL, DIMENSION(klon,klev), INTENT(IN) :: flight_dist ! Aviation distance flown within the mesh [m/s/mesh] |
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174 | REAL, DIMENSION(klon,klev), INTENT(IN) :: flight_h2o ! Aviation H2O emitted within the mesh [kg H2O/s/mesh] |
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175 | |
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176 | ! OUTPUT variables |
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177 | !----------------- |
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178 | |
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179 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: d_t ! temperature increment [K] |
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180 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: d_q ! specific humidity increment [kg/kg] |
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181 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: d_ql ! liquid water increment [kg/kg] |
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182 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: d_qi ! cloud ice mass increment [kg/kg] |
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183 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: rneb ! cloud fraction [-] |
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184 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: rneblsvol ! cloud fraction per unit volume [-] |
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185 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: pfraclr ! precip fraction clear-sky part [-] |
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186 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: pfracld ! precip fraction cloudy part [-] |
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187 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: cldfraliq ! liquid fraction of cloud [-] |
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188 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: sigma2_icefracturb ! Variance of the diagnostic supersaturation distribution (icefrac_turb) [-] |
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189 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: mean_icefracturb ! Mean of the diagnostic supersaturation distribution (icefrac_turb) [-] |
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190 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: radocond ! condensed water used in the radiation scheme [kg/kg] |
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191 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: radicefrac ! ice fraction of condensed water for radiation scheme |
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192 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: rhcl ! clear-sky relative humidity [-] |
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193 | REAL, DIMENSION(klon), INTENT(OUT) :: rain ! surface large-scale rainfall [kg/s/m2] |
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194 | REAL, DIMENSION(klon), INTENT(OUT) :: snow ! surface large-scale snowfall [kg/s/m2] |
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195 | REAL, DIMENSION(klon,klev+1), INTENT(OUT) :: prfl ! large-scale rainfall flux in the column [kg/s/m2] |
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196 | REAL, DIMENSION(klon,klev+1), INTENT(OUT) :: psfl ! large-scale snowfall flux in the column [kg/s/m2] |
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197 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: distcltop ! distance to cloud top [m] |
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198 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: temp_cltop ! temperature of cloud top [K] |
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199 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: beta ! conversion rate of condensed water |
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200 | |
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201 | ! fraction of aerosol scavenging through impaction and nucleation (for on-line) |
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202 | |
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203 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: frac_impa ! scavenging fraction due tu impaction [-] |
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204 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: frac_nucl ! scavenging fraction due tu nucleation [-] |
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205 | |
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206 | ! for condensation and ice supersaturation |
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207 | |
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208 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qsub !--specific total water content in sub-saturated clear sky region [kg/kg] |
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209 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qissr !--specific total water content in supersat region [kg/kg] |
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210 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qcld !--specific total water content in cloudy region [kg/kg] |
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211 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: subfra !--mesh fraction of subsaturated clear sky [-] |
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212 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: issrfra !--mesh fraction of ISSR [-] |
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213 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: gamma_cond !--coefficient governing the ice nucleation RHi threshold [-] |
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214 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dcf_sub !--cloud fraction tendency because of sublimation [s-1] |
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215 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dcf_con !--cloud fraction tendency because of condensation [s-1] |
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216 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dcf_mix !--cloud fraction tendency because of cloud mixing [s-1] |
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217 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqi_adj !--specific ice content tendency because of temperature adjustment [kg/kg/s] |
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218 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqi_sub !--specific ice content tendency because of sublimation [kg/kg/s] |
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219 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqi_con !--specific ice content tendency because of condensation [kg/kg/s] |
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220 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqi_mix !--specific ice content tendency because of cloud mixing [kg/kg/s] |
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221 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqvc_adj !--specific cloud water vapor tendency because of temperature adjustment [kg/kg/s] |
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222 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqvc_sub !--specific cloud water vapor tendency because of sublimation [kg/kg/s] |
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223 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqvc_con !--specific cloud water vapor tendency because of condensation [kg/kg/s] |
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224 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqvc_mix !--specific cloud water vapor tendency because of cloud mixing [kg/kg/s] |
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225 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qsatl !--saturation specific humidity wrt liquid [kg/kg] |
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226 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qsati !--saturation specific humidity wrt ice [kg/kg] |
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227 | |
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228 | ! for contrails and aviation |
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229 | |
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230 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: Tcontr !--threshold temperature for contrail formation [K] |
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231 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qcontr !--threshold humidity for contrail formation [kg/kg] |
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232 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qcontr2 !--// (2nd expression more consistent with LMDZ expression of q) |
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233 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: fcontrN !--fraction of grid favourable to non-persistent contrails |
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234 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: fcontrP !--fraction of grid favourable to persistent contrails |
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235 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dcf_avi !--cloud fraction tendency because of aviation [s-1] |
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236 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqi_avi !--specific ice content tendency because of aviation [kg/kg/s] |
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237 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqvc_avi !--specific cloud water vapor tendency because of aviation [kg/kg/s] |
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238 | |
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239 | |
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240 | ! for POPRECIP |
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241 | |
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242 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qraindiag !--DIAGNOSTIC specific rain content [kg/kg] |
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243 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qsnowdiag !--DIAGNOSTIC specific snow content [kg/kg] |
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244 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqreva !--rain tendendy due to evaporation [kg/kg/s] |
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245 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqssub !--snow tendency due to sublimation [kg/kg/s] |
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246 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqrcol !--rain tendendy due to collection by rain of liquid cloud droplets [kg/kg/s] |
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247 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqsagg !--snow tendency due to collection of lcoud ice by aggregation [kg/kg/s] |
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248 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqrauto !--rain tendency due to autoconversion of cloud liquid [kg/kg/s] |
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249 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqsauto !--snow tendency due to autoconversion of cloud ice [kg/kg/s] |
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250 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqsrim !--snow tendency due to riming [kg/kg/s] |
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251 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqsmelt !--snow tendency due to melting [kg/kg/s] |
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252 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqrmelt !--rain tendency due to melting [kg/kg/s] |
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253 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqsfreez !--snow tendency due to freezing [kg/kg/s] |
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254 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqrfreez !--rain tendency due to freezing [kg/kg/s] |
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255 | |
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256 | ! for thermals |
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257 | |
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258 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: cloudth_sth !--mean saturation deficit in thermals |
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259 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: cloudth_senv !--mean saturation deficit in environment |
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260 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: cloudth_sigmath !--std of saturation deficit in thermals |
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261 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: cloudth_sigmaenv !--std of saturation deficit in environment |
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262 | |
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263 | |
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264 | ! LOCAL VARIABLES: |
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265 | !---------------- |
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266 | REAL,DIMENSION(klon) :: qsl, qsi ! saturation threshold at current vertical level |
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267 | REAL :: zct, zcl,zexpo |
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268 | REAL, DIMENSION(klon,klev) :: ctot |
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269 | REAL, DIMENSION(klon,klev) :: ctot_vol |
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270 | REAL, DIMENSION(klon) :: zqs, zdqs |
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271 | REAL :: zdelta, zcor, zcvm5 |
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272 | REAL, DIMENSION(klon) :: zdqsdT_raw |
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273 | REAL, DIMENSION(klon) :: gammasat,dgammasatdt ! coefficient to make cold condensation at the correct RH and derivative wrt T |
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274 | REAL, DIMENSION(klon) :: Tbef,qlbef,DT ! temperature, humidity and temp. variation during lognormal iteration |
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275 | REAL :: num,denom |
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276 | REAL :: cste |
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277 | REAL, DIMENSION(klon) :: zpdf_sig,zpdf_k,zpdf_delta ! lognormal parameters |
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278 | REAL, DIMENSION(klon) :: Zpdf_a,zpdf_b,zpdf_e1,zpdf_e2 ! lognormal intermediate variables |
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279 | REAL :: erf |
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280 | REAL, DIMENSION(klon) :: zfice_th |
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281 | REAL, DIMENSION(klon) :: qcloud, qincloud_mpc |
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282 | REAL, DIMENSION(klon) :: zrfl, zrfln |
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283 | REAL :: zqev, zqevt |
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284 | REAL, DIMENSION(klon) :: zifl, zifln, ziflprev |
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285 | REAL :: zqev0,zqevi, zqevti |
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286 | REAL, DIMENSION(klon) :: zoliq, zcond, zq, zqn |
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287 | REAL, DIMENSION(klon) :: zoliql, zoliqi |
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288 | REAL, DIMENSION(klon) :: zt |
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289 | REAL, DIMENSION(klon,klev) :: zrho |
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290 | REAL, DIMENSION(klon) :: zdz,iwc |
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291 | REAL :: zchau,zfroi |
---|
292 | REAL, DIMENSION(klon) :: zfice,zneb,znebprecip |
---|
293 | REAL :: zmelt,zrain,zsnow,zprecip |
---|
294 | REAL, DIMENSION(klon) :: dzfice |
---|
295 | REAL, DIMENSION(klon) :: zfice_turb, dzfice_turb |
---|
296 | REAL :: zsolid |
---|
297 | REAL, DIMENSION(klon) :: qtot, qzero |
---|
298 | REAL, DIMENSION(klon) :: dqsl,dqsi |
---|
299 | REAL :: smallestreal |
---|
300 | ! Variables for Bergeron process |
---|
301 | REAL :: zcp, coef1, DeltaT, Deltaq, Deltaqprecl |
---|
302 | REAL, DIMENSION(klon) :: zqpreci, zqprecl |
---|
303 | ! Variables precipitation energy conservation |
---|
304 | REAL, DIMENSION(klon) :: zmqc |
---|
305 | REAL :: zalpha_tr |
---|
306 | REAL :: zfrac_lessi |
---|
307 | REAL, DIMENSION(klon) :: zprec_cond |
---|
308 | REAL :: zmair |
---|
309 | REAL :: zcpair, zcpeau |
---|
310 | REAL, DIMENSION(klon) :: zlh_solid |
---|
311 | REAL, DIMENSION(klon) :: ztupnew |
---|
312 | REAL, DIMENSION(klon) :: zqvapclr, zqupnew ! for poprecip evap / subl |
---|
313 | REAL :: zm_solid ! for liquid -> solid conversion |
---|
314 | REAL, DIMENSION(klon) :: zrflclr, zrflcld |
---|
315 | REAL, DIMENSION(klon) :: d_zrfl_clr_cld, d_zifl_clr_cld |
---|
316 | REAL, DIMENSION(klon) :: d_zrfl_cld_clr, d_zifl_cld_clr |
---|
317 | REAL, DIMENSION(klon) :: ziflclr, ziflcld |
---|
318 | REAL, DIMENSION(klon) :: znebprecipclr, znebprecipcld |
---|
319 | REAL, DIMENSION(klon) :: tot_zneb, tot_znebn, d_tot_zneb |
---|
320 | REAL, DIMENSION(klon) :: d_znebprecip_clr_cld, d_znebprecip_cld_clr |
---|
321 | REAL, DIMENSION(klon,klev) :: velo |
---|
322 | REAL :: vr, ffallv |
---|
323 | REAL :: qlmpc, qimpc, rnebmpc |
---|
324 | REAL, DIMENSION(klon,klev) :: radocondi, radocondl |
---|
325 | REAL :: effective_zneb |
---|
326 | REAL, DIMENSION(klon) :: zdistcltop, ztemp_cltop |
---|
327 | REAL, DIMENSION(klon) :: zqliq, zqice, zqvapcl ! for icefrac_lscp_turb |
---|
328 | |
---|
329 | ! for condensation and ice supersaturation |
---|
330 | REAL, DIMENSION(klon) :: qvc, shear |
---|
331 | REAL :: delta_z |
---|
332 | !--Added for ice supersaturation (ok_ice_supersat) and contrails (ok_plane_contrails) |
---|
333 | ! Constants used for calculating ratios that are advected (using a parent-child |
---|
334 | ! formalism). This is not done in the dynamical core because at this moment, |
---|
335 | ! only isotopes can use this parent-child formalism. Note that the two constants |
---|
336 | ! are the same as the one use in the dynamical core, being also defined in |
---|
337 | ! dyn3d_common/infotrac.F90 |
---|
338 | REAL :: min_qParent, min_ratio |
---|
339 | |
---|
340 | INTEGER i, k, n, kk, iter |
---|
341 | INTEGER, DIMENSION(klon) :: n_i |
---|
342 | INTEGER ncoreczq |
---|
343 | INTEGER, DIMENSION(klon,klev) :: mpc_bl_points |
---|
344 | LOGICAL iftop |
---|
345 | |
---|
346 | LOGICAL, DIMENSION(klon) :: lognormale |
---|
347 | LOGICAL, DIMENSION(klon) :: keepgoing |
---|
348 | |
---|
349 | CHARACTER (len = 20) :: modname = 'lscp' |
---|
350 | CHARACTER (len = 80) :: abort_message |
---|
351 | |
---|
352 | |
---|
353 | !=============================================================================== |
---|
354 | ! INITIALISATION |
---|
355 | !=============================================================================== |
---|
356 | |
---|
357 | ! Few initial checks |
---|
358 | |
---|
359 | |
---|
360 | IF (iflag_fisrtilp_qsat .LT. 0) THEN |
---|
361 | abort_message = 'lscp cannot be used with iflag_fisrtilp<0' |
---|
362 | CALL abort_physic(modname,abort_message,1) |
---|
363 | ENDIF |
---|
364 | |
---|
365 | ! Few initialisations |
---|
366 | |
---|
367 | znebprecip(:)=0.0 |
---|
368 | ctot_vol(1:klon,1:klev)=0.0 |
---|
369 | rneblsvol(1:klon,1:klev)=0.0 |
---|
370 | smallestreal=1.e-9 |
---|
371 | znebprecipclr(:)=0.0 |
---|
372 | znebprecipcld(:)=0.0 |
---|
373 | mpc_bl_points(:,:)=0 |
---|
374 | |
---|
375 | IF (prt_level>9) WRITE(lunout,*) 'NUAGES4 A. JAM' |
---|
376 | |
---|
377 | ! AA for 'safety' reasons |
---|
378 | zalpha_tr = 0. |
---|
379 | zfrac_lessi = 0. |
---|
380 | beta(:,:)= 0. |
---|
381 | |
---|
382 | ! Initialisation of variables: |
---|
383 | |
---|
384 | prfl(:,:) = 0.0 |
---|
385 | psfl(:,:) = 0.0 |
---|
386 | d_t(:,:) = 0.0 |
---|
387 | d_q(:,:) = 0.0 |
---|
388 | d_ql(:,:) = 0.0 |
---|
389 | d_qi(:,:) = 0.0 |
---|
390 | rneb(:,:) = 0.0 |
---|
391 | pfraclr(:,:)=0.0 |
---|
392 | pfracld(:,:)=0.0 |
---|
393 | cldfraliq(:,:)=0. |
---|
394 | sigma2_icefracturb(:,:)=0. |
---|
395 | mean_icefracturb(:,:)=0. |
---|
396 | radocond(:,:) = 0.0 |
---|
397 | radicefrac(:,:) = 0.0 |
---|
398 | frac_nucl(:,:) = 1.0 |
---|
399 | frac_impa(:,:) = 1.0 |
---|
400 | rain(:) = 0.0 |
---|
401 | snow(:) = 0.0 |
---|
402 | zoliq(:)=0.0 |
---|
403 | zfice(:)=0.0 |
---|
404 | dzfice(:)=0.0 |
---|
405 | zfice_turb(:)=0.0 |
---|
406 | dzfice_turb(:)=0.0 |
---|
407 | zqprecl(:)=0.0 |
---|
408 | zqpreci(:)=0.0 |
---|
409 | zrfl(:) = 0.0 |
---|
410 | zifl(:) = 0.0 |
---|
411 | ziflprev(:)=0.0 |
---|
412 | zneb(:) = seuil_neb |
---|
413 | zrflclr(:) = 0.0 |
---|
414 | ziflclr(:) = 0.0 |
---|
415 | zrflcld(:) = 0.0 |
---|
416 | ziflcld(:) = 0.0 |
---|
417 | tot_zneb(:) = 0.0 |
---|
418 | tot_znebn(:) = 0.0 |
---|
419 | d_tot_zneb(:) = 0.0 |
---|
420 | qzero(:) = 0.0 |
---|
421 | zdistcltop(:)=0.0 |
---|
422 | ztemp_cltop(:) = 0.0 |
---|
423 | ztupnew(:)=0.0 |
---|
424 | |
---|
425 | distcltop(:,:)=0. |
---|
426 | temp_cltop(:,:)=0. |
---|
427 | |
---|
428 | !--Ice supersaturation |
---|
429 | gamma_cond(:,:) = 1. |
---|
430 | qissr(:,:) = 0. |
---|
431 | issrfra(:,:) = 0. |
---|
432 | dcf_sub(:,:) = 0. |
---|
433 | dcf_con(:,:) = 0. |
---|
434 | dcf_mix(:,:) = 0. |
---|
435 | dqi_adj(:,:) = 0. |
---|
436 | dqi_sub(:,:) = 0. |
---|
437 | dqi_con(:,:) = 0. |
---|
438 | dqi_mix(:,:) = 0. |
---|
439 | dqvc_adj(:,:) = 0. |
---|
440 | dqvc_sub(:,:) = 0. |
---|
441 | dqvc_con(:,:) = 0. |
---|
442 | dqvc_mix(:,:) = 0. |
---|
443 | fcontrN(:,:) = 0. |
---|
444 | fcontrP(:,:) = 0. |
---|
445 | Tcontr(:,:) = missing_val |
---|
446 | qcontr(:,:) = missing_val |
---|
447 | qcontr2(:,:) = missing_val |
---|
448 | dcf_avi(:,:) = 0. |
---|
449 | dqi_avi(:,:) = 0. |
---|
450 | dqvc_avi(:,:) = 0. |
---|
451 | qvc(:) = 0. |
---|
452 | shear(:) = 0. |
---|
453 | min_qParent = 1.e-30 |
---|
454 | min_ratio = 1.e-16 |
---|
455 | |
---|
456 | !-- poprecip |
---|
457 | qraindiag(:,:)= 0. |
---|
458 | qsnowdiag(:,:)= 0. |
---|
459 | dqreva(:,:) = 0. |
---|
460 | dqrauto(:,:) = 0. |
---|
461 | dqrmelt(:,:) = 0. |
---|
462 | dqrfreez(:,:) = 0. |
---|
463 | dqrcol(:,:) = 0. |
---|
464 | dqssub(:,:) = 0. |
---|
465 | dqsauto(:,:) = 0. |
---|
466 | dqsrim(:,:) = 0. |
---|
467 | dqsagg(:,:) = 0. |
---|
468 | dqsfreez(:,:) = 0. |
---|
469 | dqsmelt(:,:) = 0. |
---|
470 | zqupnew(:) = 0. |
---|
471 | zqvapclr(:) = 0. |
---|
472 | |
---|
473 | |
---|
474 | |
---|
475 | !c_iso: variable initialisation for iso |
---|
476 | |
---|
477 | |
---|
478 | !=============================================================================== |
---|
479 | ! BEGINNING OF VERTICAL LOOP FROM TOP TO BOTTOM |
---|
480 | !=============================================================================== |
---|
481 | |
---|
482 | ncoreczq=0 |
---|
483 | |
---|
484 | DO k = klev, 1, -1 |
---|
485 | |
---|
486 | IF (k.LE.klev-1) THEN |
---|
487 | iftop=.false. |
---|
488 | ELSE |
---|
489 | iftop=.true. |
---|
490 | ENDIF |
---|
491 | |
---|
492 | ! Initialisation temperature and specific humidity |
---|
493 | ! temp(klon,klev) is not modified by the routine, instead all changes in temperature are made on zt |
---|
494 | ! at the end of the klon loop, a temperature incremtent d_t due to all processes |
---|
495 | ! (thermalization, evap/sub incoming precip, cloud formation, precipitation processes) is calculated |
---|
496 | ! d_t = temperature tendency due to lscp |
---|
497 | ! The temperature of the overlying layer is updated here because needed for thermalization |
---|
498 | DO i = 1, klon |
---|
499 | zt(i)=temp(i,k) |
---|
500 | zq(i)=qt(i,k) |
---|
501 | IF (.not. iftop) THEN |
---|
502 | ztupnew(i) = temp(i,k+1) + d_t(i,k+1) |
---|
503 | zqupnew(i) = qt(i,k+1) + d_q(i,k+1) + d_ql(i,k+1) + d_qi(i,k+1) |
---|
504 | !--zqs(i) is the saturation specific humidity in the layer above |
---|
505 | zqvapclr(i) = MAX(0., qt(i,k+1) + d_q(i,k+1) - rneb(i,k+1) * zqs(i)) |
---|
506 | ENDIF |
---|
507 | !c_iso init of iso |
---|
508 | ENDDO |
---|
509 | |
---|
510 | !================================================================ |
---|
511 | ! Flag for the new and more microphysical treatment of precipitation from Atelier Nuage (R) |
---|
512 | IF (ok_poprecip) THEN |
---|
513 | |
---|
514 | CALL poprecip_precld(klon, dtime, iftop, paprs(:,k), paprs(:,k+1), pplay(:,k), & |
---|
515 | zt, ztupnew, zq, zmqc, znebprecipclr, znebprecipcld, & |
---|
516 | zqvapclr, zqupnew, & |
---|
517 | zrfl, zrflclr, zrflcld, & |
---|
518 | zifl, ziflclr, ziflcld, & |
---|
519 | dqreva(:,k),dqssub(:,k) & |
---|
520 | ) |
---|
521 | |
---|
522 | !================================================================ |
---|
523 | ELSE |
---|
524 | |
---|
525 | ! -------------------------------------------------------------------- |
---|
526 | ! P1> Thermalization of precipitation falling from the overlying layer |
---|
527 | ! -------------------------------------------------------------------- |
---|
528 | ! Computes air temperature variation due to enthalpy transported by |
---|
529 | ! precipitation. Precipitation is then thermalized with the air in the |
---|
530 | ! layer. |
---|
531 | ! The precipitation should remain thermalized throughout the different |
---|
532 | ! thermodynamical transformations. |
---|
533 | ! The corresponding water mass should |
---|
534 | ! be added when calculating the layer's enthalpy change with |
---|
535 | ! temperature |
---|
536 | ! See lmdzpedia page todoan |
---|
537 | ! todoan: check consistency with ice phase |
---|
538 | ! todoan: understand why several steps |
---|
539 | ! --------------------------------------------------------------------- |
---|
540 | |
---|
541 | IF (iftop) THEN |
---|
542 | |
---|
543 | DO i = 1, klon |
---|
544 | zmqc(i) = 0. |
---|
545 | ENDDO |
---|
546 | |
---|
547 | ELSE |
---|
548 | |
---|
549 | DO i = 1, klon |
---|
550 | |
---|
551 | zmair=(paprs(i,k)-paprs(i,k+1))/RG |
---|
552 | ! no condensed water so cp=cp(vapor+dry air) |
---|
553 | ! RVTMP2=rcpv/rcpd-1 |
---|
554 | zcpair=RCPD*(1.0+RVTMP2*zq(i)) |
---|
555 | zcpeau=RCPD*RVTMP2 |
---|
556 | |
---|
557 | ! zmqc: precipitation mass that has to be thermalized with |
---|
558 | ! layer's air so that precipitation at the ground has the |
---|
559 | ! same temperature as the lowermost layer |
---|
560 | zmqc(i) = (zrfl(i)+zifl(i))*dtime/zmair |
---|
561 | ! t(i,k+1)+d_t(i,k+1): new temperature of the overlying layer |
---|
562 | zt(i) = ( ztupnew(i)*zmqc(i)*zcpeau + zcpair*zt(i) ) & |
---|
563 | / (zcpair + zmqc(i)*zcpeau) |
---|
564 | |
---|
565 | ENDDO |
---|
566 | |
---|
567 | ENDIF |
---|
568 | |
---|
569 | ! -------------------------------------------------------------------- |
---|
570 | ! P2> Precipitation evaporation/sublimation/melting |
---|
571 | ! -------------------------------------------------------------------- |
---|
572 | ! A part of the precipitation coming from above is evaporated/sublimated/melted. |
---|
573 | ! -------------------------------------------------------------------- |
---|
574 | |
---|
575 | IF (iflag_evap_prec.GE.1) THEN |
---|
576 | |
---|
577 | ! Calculation of saturation specific humidity |
---|
578 | ! depending on temperature: |
---|
579 | CALL calc_qsat_ecmwf(klon,zt(:),qzero(:),pplay(:,k),RTT,0,.false.,zqs(:),zdqs(:)) |
---|
580 | ! wrt liquid water |
---|
581 | CALL calc_qsat_ecmwf(klon,zt(:),qzero(:),pplay(:,k),RTT,1,.false.,qsl(:),dqsl(:)) |
---|
582 | ! wrt ice |
---|
583 | CALL calc_qsat_ecmwf(klon,zt(:),qzero(:),pplay(:,k),RTT,2,.false.,qsi(:),dqsi(:)) |
---|
584 | |
---|
585 | DO i = 1, klon |
---|
586 | |
---|
587 | ! if precipitation |
---|
588 | IF (zrfl(i)+zifl(i).GT.0.) THEN |
---|
589 | |
---|
590 | ! LudoTP: we only account for precipitation evaporation in the clear-sky (iflag_evap_prec>=4). |
---|
591 | ! c_iso: likely important to distinguish cs from neb isotope precipitation |
---|
592 | |
---|
593 | IF (iflag_evap_prec.GE.4) THEN |
---|
594 | zrfl(i) = zrflclr(i) |
---|
595 | zifl(i) = ziflclr(i) |
---|
596 | ENDIF |
---|
597 | |
---|
598 | IF (iflag_evap_prec.EQ.1) THEN |
---|
599 | znebprecip(i)=zneb(i) |
---|
600 | ELSE |
---|
601 | znebprecip(i)=MAX(zneb(i),znebprecip(i)) |
---|
602 | ENDIF |
---|
603 | |
---|
604 | IF (iflag_evap_prec.GT.4) THEN |
---|
605 | ! Max evaporation not to saturate the clear sky precip fraction |
---|
606 | ! i.e. the fraction where evaporation occurs |
---|
607 | zqev0 = MAX(0.0, (zqs(i)-zq(i))*znebprecipclr(i)) |
---|
608 | ELSEIF (iflag_evap_prec .EQ. 4) THEN |
---|
609 | ! Max evaporation not to saturate the whole mesh |
---|
610 | ! Pay attention -> lead to unrealistic and excessive evaporation |
---|
611 | zqev0 = MAX(0.0, zqs(i)-zq(i)) |
---|
612 | ELSE |
---|
613 | ! Max evap not to saturate the fraction below the cloud |
---|
614 | zqev0 = MAX(0.0, (zqs(i)-zq(i))*znebprecip(i)) |
---|
615 | ENDIF |
---|
616 | |
---|
617 | ! Evaporation of liquid precipitation coming from above |
---|
618 | ! dP/dz=beta*(1-q/qsat)*sqrt(P) |
---|
619 | ! formula from Sundquist 1988, Klemp & Wilhemson 1978 |
---|
620 | ! LTP: evaporation only in the clear sky part (iflag_evap_prec>=4) |
---|
621 | |
---|
622 | IF (iflag_evap_prec.EQ.3) THEN |
---|
623 | zqevt = znebprecip(i)*coef_eva*(1.0-zq(i)/qsl(i)) & |
---|
624 | *SQRT(zrfl(i)/max(1.e-4,znebprecip(i))) & |
---|
625 | *(paprs(i,k)-paprs(i,k+1))/pplay(i,k)*zt(i)*RD/RG |
---|
626 | ELSE IF (iflag_evap_prec.GE.4) THEN |
---|
627 | zqevt = znebprecipclr(i)*coef_eva*(1.0-zq(i)/qsl(i)) & |
---|
628 | *SQRT(zrfl(i)/max(1.e-8,znebprecipclr(i))) & |
---|
629 | *(paprs(i,k)-paprs(i,k+1))/pplay(i,k)*zt(i)*RD/RG |
---|
630 | ELSE |
---|
631 | zqevt = 1.*coef_eva*(1.0-zq(i)/qsl(i))*SQRT(zrfl(i)) & |
---|
632 | *(paprs(i,k)-paprs(i,k+1))/pplay(i,k)*zt(i)*RD/RG |
---|
633 | ENDIF |
---|
634 | |
---|
635 | zqevt = MAX(0.0,MIN(zqevt,zrfl(i))) & |
---|
636 | *RG*dtime/(paprs(i,k)-paprs(i,k+1)) |
---|
637 | |
---|
638 | ! sublimation of the solid precipitation coming from above |
---|
639 | IF (iflag_evap_prec.EQ.3) THEN |
---|
640 | zqevti = znebprecip(i)*coef_sub*(1.0-zq(i)/qsi(i)) & |
---|
641 | *SQRT(zifl(i)/max(1.e-4,znebprecip(i))) & |
---|
642 | *(paprs(i,k)-paprs(i,k+1))/pplay(i,k)*zt(i)*RD/RG |
---|
643 | ELSE IF (iflag_evap_prec.GE.4) THEN |
---|
644 | zqevti = znebprecipclr(i)*coef_sub*(1.0-zq(i)/qsi(i)) & |
---|
645 | *SQRT(zifl(i)/max(1.e-8,znebprecipclr(i))) & |
---|
646 | *(paprs(i,k)-paprs(i,k+1))/pplay(i,k)*zt(i)*RD/RG |
---|
647 | ELSE |
---|
648 | zqevti = 1.*coef_sub*(1.0-zq(i)/qsi(i))*SQRT(zifl(i)) & |
---|
649 | *(paprs(i,k)-paprs(i,k+1))/pplay(i,k)*zt(i)*RD/RG |
---|
650 | ENDIF |
---|
651 | |
---|
652 | zqevti = MAX(0.0,MIN(zqevti,zifl(i))) & |
---|
653 | *RG*dtime/(paprs(i,k)-paprs(i,k+1)) |
---|
654 | |
---|
655 | ! A. JAM |
---|
656 | ! Evaporation limit: we ensure that the layer's fraction below |
---|
657 | ! the cloud or the whole mesh (depending on iflag_evap_prec) |
---|
658 | ! does not reach saturation. In this case, we |
---|
659 | ! redistribute zqev0 conserving the ratio liquid/ice |
---|
660 | |
---|
661 | IF (zqevt+zqevti.GT.zqev0) THEN |
---|
662 | zqev=zqev0*zqevt/(zqevt+zqevti) |
---|
663 | zqevi=zqev0*zqevti/(zqevt+zqevti) |
---|
664 | ELSE |
---|
665 | zqev=zqevt |
---|
666 | zqevi=zqevti |
---|
667 | ENDIF |
---|
668 | |
---|
669 | |
---|
670 | ! New solid and liquid precipitation fluxes after evap and sublimation |
---|
671 | zrfln(i) = Max(0.,zrfl(i) - zqev*(paprs(i,k)-paprs(i,k+1)) & |
---|
672 | /RG/dtime) |
---|
673 | zifln(i) = Max(0.,zifl(i) - zqevi*(paprs(i,k)-paprs(i,k+1)) & |
---|
674 | /RG/dtime) |
---|
675 | |
---|
676 | |
---|
677 | ! vapor, temperature, precip fluxes update |
---|
678 | ! vapor is updated after evaporation/sublimation (it is increased) |
---|
679 | zq(i) = zq(i) - (zrfln(i)+zifln(i)-zrfl(i)-zifl(i)) & |
---|
680 | * (RG/(paprs(i,k)-paprs(i,k+1)))*dtime |
---|
681 | ! zmqc is the total condensed water in the precip flux (it is decreased) |
---|
682 | zmqc(i) = zmqc(i) + (zrfln(i)+zifln(i)-zrfl(i)-zifl(i)) & |
---|
683 | * (RG/(paprs(i,k)-paprs(i,k+1)))*dtime |
---|
684 | ! air and precip temperature (i.e., gridbox temperature) |
---|
685 | ! is updated due to latent heat cooling |
---|
686 | zt(i) = zt(i) + (zrfln(i)-zrfl(i)) & |
---|
687 | * (RG/(paprs(i,k)-paprs(i,k+1)))*dtime & |
---|
688 | * RLVTT/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i))) & |
---|
689 | + (zifln(i)-zifl(i)) & |
---|
690 | * (RG/(paprs(i,k)-paprs(i,k+1)))*dtime & |
---|
691 | * RLSTT/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i))) |
---|
692 | |
---|
693 | ! New values of liquid and solid precipitation |
---|
694 | zrfl(i) = zrfln(i) |
---|
695 | zifl(i) = zifln(i) |
---|
696 | |
---|
697 | ! c_iso here call_reevap that updates isotopic zrfl, zifl (in inout) |
---|
698 | ! due to evap + sublim |
---|
699 | |
---|
700 | |
---|
701 | IF (iflag_evap_prec.GE.4) THEN |
---|
702 | zrflclr(i) = zrfl(i) |
---|
703 | ziflclr(i) = zifl(i) |
---|
704 | IF(zrflclr(i) + ziflclr(i).LE.0) THEN |
---|
705 | znebprecipclr(i) = 0.0 |
---|
706 | ENDIF |
---|
707 | zrfl(i) = zrflclr(i) + zrflcld(i) |
---|
708 | zifl(i) = ziflclr(i) + ziflcld(i) |
---|
709 | ENDIF |
---|
710 | |
---|
711 | ! c_iso duplicate for isotopes or loop on isotopes |
---|
712 | |
---|
713 | ! Melting: |
---|
714 | zmelt = ((zt(i)-RTT)/(ztfondue-RTT)) ! JYG |
---|
715 | ! precip fraction that is melted |
---|
716 | zmelt = MIN(MAX(zmelt,0.),1.) |
---|
717 | |
---|
718 | ! update of rainfall and snowfall due to melting |
---|
719 | IF (iflag_evap_prec.GE.4) THEN |
---|
720 | zrflclr(i)=zrflclr(i)+zmelt*ziflclr(i) |
---|
721 | zrflcld(i)=zrflcld(i)+zmelt*ziflcld(i) |
---|
722 | zrfl(i)=zrflclr(i)+zrflcld(i) |
---|
723 | ELSE |
---|
724 | zrfl(i)=zrfl(i)+zmelt*zifl(i) |
---|
725 | ENDIF |
---|
726 | |
---|
727 | |
---|
728 | ! c_iso: melting of isotopic precipi with zmelt (no fractionation) |
---|
729 | |
---|
730 | ! Latent heat of melting because of precipitation melting |
---|
731 | ! NB: the air + precip temperature is simultaneously updated |
---|
732 | zt(i)=zt(i)-zifl(i)*zmelt*(RG*dtime)/(paprs(i,k)-paprs(i,k+1)) & |
---|
733 | *RLMLT/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i))) |
---|
734 | |
---|
735 | IF (iflag_evap_prec.GE.4) THEN |
---|
736 | ziflclr(i)=ziflclr(i)*(1.-zmelt) |
---|
737 | ziflcld(i)=ziflcld(i)*(1.-zmelt) |
---|
738 | zifl(i)=ziflclr(i)+ziflcld(i) |
---|
739 | ELSE |
---|
740 | zifl(i)=zifl(i)*(1.-zmelt) |
---|
741 | ENDIF |
---|
742 | |
---|
743 | ELSE |
---|
744 | ! if no precip, we reinitialize the cloud fraction used for the precip to 0 |
---|
745 | znebprecip(i)=0. |
---|
746 | |
---|
747 | ENDIF ! (zrfl(i)+zifl(i).GT.0.) |
---|
748 | |
---|
749 | ENDDO ! loop on klon |
---|
750 | |
---|
751 | ENDIF ! (iflag_evap_prec>=1) |
---|
752 | |
---|
753 | ENDIF ! (ok_poprecip) |
---|
754 | |
---|
755 | ! -------------------------------------------------------------------- |
---|
756 | ! End precip evaporation |
---|
757 | ! -------------------------------------------------------------------- |
---|
758 | |
---|
759 | ! Calculation of qsat, L/Cp*dqsat/dT and ncoreczq counter |
---|
760 | !------------------------------------------------------- |
---|
761 | |
---|
762 | qtot(:)=zq(:)+zmqc(:) |
---|
763 | CALL calc_qsat_ecmwf(klon,zt(:),qtot(:),pplay(:,k),RTT,0,.false.,zqs(:),zdqs(:)) |
---|
764 | DO i = 1, klon |
---|
765 | zdelta = MAX(0.,SIGN(1.,RTT-zt(i))) |
---|
766 | zdqsdT_raw(i) = zdqs(i)*RCPD*(1.0+RVTMP2*zq(i)) / (RLVTT*(1.-zdelta) + RLSTT*zdelta) |
---|
767 | IF (zq(i) .LT. 1.e-15) THEN |
---|
768 | ncoreczq=ncoreczq+1 |
---|
769 | zq(i)=1.e-15 |
---|
770 | ENDIF |
---|
771 | ! c_iso: do something similar for isotopes |
---|
772 | |
---|
773 | ENDDO |
---|
774 | |
---|
775 | ! -------------------------------------------------------------------- |
---|
776 | ! P2> Cloud formation |
---|
777 | !--------------------------------------------------------------------- |
---|
778 | ! |
---|
779 | ! Unlike fisrtilp, we always assume a 'fractional cloud' approach |
---|
780 | ! i.e. clouds occupy only a fraction of the mesh (the subgrid distribution |
---|
781 | ! is prescribed and depends on large scale variables and boundary layer |
---|
782 | ! properties) |
---|
783 | ! The decrease in condensed part due tu latent heating is taken into |
---|
784 | ! account |
---|
785 | ! ------------------------------------------------------------------- |
---|
786 | |
---|
787 | ! P2.1> With the PDFs (log-normal, bigaussian) |
---|
788 | ! cloud properties calculation with the initial values of t and q |
---|
789 | ! ---------------------------------------------------------------- |
---|
790 | |
---|
791 | ! initialise gammasat and qincloud_mpc |
---|
792 | gammasat(:)=1. |
---|
793 | qincloud_mpc(:)=0. |
---|
794 | |
---|
795 | IF (iflag_cld_th.GE.5) THEN |
---|
796 | ! Cloud cover and content in meshes affected by shallow convection, |
---|
797 | ! are retrieved from a bi-gaussian distribution of the saturation deficit |
---|
798 | ! following Jam et al. 2013 |
---|
799 | |
---|
800 | IF (iflag_cloudth_vert.LE.2) THEN |
---|
801 | ! Old version of Arnaud Jam |
---|
802 | |
---|
803 | CALL cloudth(klon,klev,k,tv, & |
---|
804 | zq,qta,fraca, & |
---|
805 | qcloud,ctot,pspsk,paprs,pplay,tla,thl, & |
---|
806 | ratqs,zqs,temp, & |
---|
807 | cloudth_sth,cloudth_senv,cloudth_sigmath,cloudth_sigmaenv) |
---|
808 | |
---|
809 | |
---|
810 | ELSEIF (iflag_cloudth_vert.GE.3 .AND. iflag_cloudth_vert.LE.5) THEN |
---|
811 | ! Default version of Arnaud Jam |
---|
812 | |
---|
813 | CALL cloudth_v3(klon,klev,k,tv, & |
---|
814 | zq,qta,fraca, & |
---|
815 | qcloud,ctot,ctot_vol,pspsk,paprs,pplay,tla,thl, & |
---|
816 | ratqs,zqs,temp, & |
---|
817 | cloudth_sth,cloudth_senv,cloudth_sigmath,cloudth_sigmaenv) |
---|
818 | |
---|
819 | |
---|
820 | ELSEIF (iflag_cloudth_vert.EQ.6) THEN |
---|
821 | ! Jean Jouhaud's version, with specific separation between surface and volume |
---|
822 | ! cloud fraction Decembre 2018 |
---|
823 | |
---|
824 | CALL cloudth_v6(klon,klev,k,tv, & |
---|
825 | zq,qta,fraca, & |
---|
826 | qcloud,ctot,ctot_vol,pspsk,paprs,pplay,tla,thl, & |
---|
827 | ratqs,zqs,temp, & |
---|
828 | cloudth_sth,cloudth_senv,cloudth_sigmath,cloudth_sigmaenv) |
---|
829 | |
---|
830 | ELSEIF (iflag_cloudth_vert .EQ. 7) THEN |
---|
831 | ! Updated version of Arnaud Jam (correction by E. Vignon) + adapted treatment |
---|
832 | ! for boundary-layer mixed phase clouds |
---|
833 | CALL cloudth_mpc(klon,klev,k,mpc_bl_points,zt,zq,qta(:,k),fraca(:,k), & |
---|
834 | pspsk(:,k),paprs(:,k+1),paprs(:,k),pplay(:,k), tla(:,k), & |
---|
835 | ratqs(:,k),qcloud,qincloud_mpc,zfice_th,ctot(:,k),ctot_vol(:,k), & |
---|
836 | cloudth_sth(:,k),cloudth_senv(:,k),cloudth_sigmath(:,k),cloudth_sigmaenv(:,k)) |
---|
837 | |
---|
838 | ENDIF |
---|
839 | |
---|
840 | |
---|
841 | DO i=1,klon |
---|
842 | rneb(i,k)=ctot(i,k) |
---|
843 | rneblsvol(i,k)=ctot_vol(i,k) |
---|
844 | zqn(i)=qcloud(i) |
---|
845 | !--AB grid-mean vapor in the cloud - we assume saturation adjustment |
---|
846 | qvc(i) = rneb(i,k) * zqs(i) |
---|
847 | ENDDO |
---|
848 | |
---|
849 | ENDIF |
---|
850 | |
---|
851 | IF (iflag_cld_th .LE. 4) THEN |
---|
852 | |
---|
853 | ! lognormal |
---|
854 | lognormale(:) = .TRUE. |
---|
855 | |
---|
856 | ELSEIF (iflag_cld_th .GE. 6) THEN |
---|
857 | |
---|
858 | ! lognormal distribution when no thermals |
---|
859 | lognormale(:) = fraca(:,k) < min_frac_th_cld |
---|
860 | |
---|
861 | ELSE |
---|
862 | ! When iflag_cld_th=5, we always assume |
---|
863 | ! bi-gaussian distribution |
---|
864 | lognormale(:) = .FALSE. |
---|
865 | |
---|
866 | ENDIF |
---|
867 | |
---|
868 | DT(:) = 0. |
---|
869 | n_i(:)=0 |
---|
870 | Tbef(:)=zt(:) |
---|
871 | qlbef(:)=0. |
---|
872 | |
---|
873 | ! Treatment of non-boundary layer clouds (lognormale) |
---|
874 | ! condensation with qsat(T) variation (adaptation) |
---|
875 | ! Iterative resolution to converge towards qsat |
---|
876 | ! with update of temperature, ice fraction and qsat at |
---|
877 | ! each iteration |
---|
878 | |
---|
879 | ! todoan -> sensitivity to iflag_fisrtilp_qsat |
---|
880 | DO iter=1,iflag_fisrtilp_qsat+1 |
---|
881 | |
---|
882 | keepgoing(:) = .FALSE. |
---|
883 | |
---|
884 | DO i=1,klon |
---|
885 | |
---|
886 | ! keepgoing = .true. while convergence is not satisfied |
---|
887 | |
---|
888 | IF (((ABS(DT(i)).GT.DDT0) .OR. (n_i(i) .EQ. 0)) .AND. lognormale(i)) THEN |
---|
889 | |
---|
890 | ! if not convergence: |
---|
891 | ! we calculate a new iteration |
---|
892 | keepgoing(i) = .TRUE. |
---|
893 | |
---|
894 | ! P2.2.1> cloud fraction and condensed water mass calculation |
---|
895 | ! Calculated variables: |
---|
896 | ! rneb : cloud fraction |
---|
897 | ! zqn : total water within the cloud |
---|
898 | ! zcond: mean condensed water within the mesh |
---|
899 | ! rhcl: clear-sky relative humidity |
---|
900 | !--------------------------------------------------------------- |
---|
901 | |
---|
902 | ! new temperature that only serves in the iteration process: |
---|
903 | Tbef(i)=Tbef(i)+DT(i) |
---|
904 | |
---|
905 | ! Rneb, qzn and zcond for lognormal PDFs |
---|
906 | qtot(i)=zq(i)+zmqc(i) |
---|
907 | |
---|
908 | ENDIF |
---|
909 | |
---|
910 | ENDDO |
---|
911 | |
---|
912 | ! Calculation of saturation specific humidity and ice fraction |
---|
913 | CALL calc_qsat_ecmwf(klon,Tbef(:),qtot(:),pplay(:,k),RTT,0,.false.,zqs(:),zdqs(:)) |
---|
914 | CALL calc_gammasat(klon,Tbef(:),qtot(:),pplay(:,k),gammasat(:),dgammasatdt(:)) |
---|
915 | ! saturation may occur at a humidity different from qsat (gamma qsat), so gamma correction for dqs |
---|
916 | zdqs(:) = gammasat(:)*zdqs(:)+zqs(:)*dgammasatdt(:) |
---|
917 | ! cloud phase determination |
---|
918 | IF (iflag_t_glace.GE.4) THEN |
---|
919 | ! For iflag_t_glace GE 4 the phase partition function dependends on temperature AND distance to cloud top |
---|
920 | CALL distance_to_cloud_top(klon,klev,k,temp,pplay,paprs,rneb,zdistcltop,ztemp_cltop) |
---|
921 | ENDIF |
---|
922 | |
---|
923 | CALL icefrac_lscp(klon, zt(:), iflag_ice_thermo, zdistcltop(:),ztemp_cltop(:),zfice(:),dzfice(:)) |
---|
924 | |
---|
925 | !--AB Activates a condensation scheme that allows for |
---|
926 | !--ice supersaturation and contrails evolution from aviation |
---|
927 | IF (ok_ice_supersat) THEN |
---|
928 | |
---|
929 | !--Calculate the shear value (input for condensation and ice supersat) |
---|
930 | DO i = 1, klon |
---|
931 | !--Cell thickness [m] |
---|
932 | delta_z = ( paprs(i,k) - paprs(i,k+1) ) / RG / pplay(i,k) * Tbef(i) * RD |
---|
933 | IF ( iftop ) THEN |
---|
934 | ! top |
---|
935 | shear(i) = SQRT( ( (u_seri(i,k) - u_seri(i,k-1)) / delta_z )**2. & |
---|
936 | + ( (v_seri(i,k) - v_seri(i,k-1)) / delta_z )**2. ) |
---|
937 | ELSEIF ( k .EQ. 1 ) THEN |
---|
938 | ! surface |
---|
939 | shear(i) = SQRT( ( (u_seri(i,k+1) - u_seri(i,k)) / delta_z )**2. & |
---|
940 | + ( (v_seri(i,k+1) - v_seri(i,k)) / delta_z )**2. ) |
---|
941 | ELSE |
---|
942 | ! other layers |
---|
943 | shear(i) = SQRT( ( ( (u_seri(i,k+1) + u_seri(i,k)) / 2. & |
---|
944 | - (u_seri(i,k) + u_seri(i,k-1)) / 2. ) / delta_z )**2. & |
---|
945 | + ( ( (v_seri(i,k+1) + v_seri(i,k)) / 2. & |
---|
946 | - (v_seri(i,k) + v_seri(i,k-1)) / 2. ) / delta_z )**2. ) |
---|
947 | ENDIF |
---|
948 | ENDDO |
---|
949 | |
---|
950 | !--------------------------------------------- |
---|
951 | !-- CONDENSATION AND ICE SUPERSATURATION -- |
---|
952 | !--------------------------------------------- |
---|
953 | |
---|
954 | CALL condensation_ice_supersat( & |
---|
955 | klon, dtime, missing_val, & |
---|
956 | pplay(:,k), paprs(:,k), paprs(:,k+1), & |
---|
957 | cf_seri(:,k), rvc_seri(:,k), ratio_qi_qtot(:,k), & |
---|
958 | shear(:), tke_dissip(:,k), cell_area(:), & |
---|
959 | Tbef(:), zq(:), zqs(:), gammasat(:), ratqs(:,k), keepgoing(:), & |
---|
960 | rneb(:,k), zqn(:), qvc(:), issrfra(:,k), qissr(:,k), & |
---|
961 | dcf_sub(:,k), dcf_con(:,k), dcf_mix(:,k), & |
---|
962 | dqi_adj(:,k), dqi_sub(:,k), dqi_con(:,k), dqi_mix(:,k), & |
---|
963 | dqvc_adj(:,k), dqvc_sub(:,k), dqvc_con(:,k), dqvc_mix(:,k), & |
---|
964 | Tcontr(:,k), qcontr(:,k), qcontr2(:,k), fcontrN(:,k), fcontrP(:,k), & |
---|
965 | flight_dist(:,k), flight_h2o(:,k), & |
---|
966 | dcf_avi(:,k), dqi_avi(:,k), dqvc_avi(:,k)) |
---|
967 | |
---|
968 | |
---|
969 | !--If .TRUE., calls an externalised version of the generalised |
---|
970 | !--lognormal condensation scheme (Bony and Emanuel 2001) |
---|
971 | !--Numerically, convergence is conserved with this option |
---|
972 | !--The objective is to simplify LSCP |
---|
973 | ELSEIF ( ok_external_lognormal ) THEN |
---|
974 | |
---|
975 | CALL condensation_lognormal( & |
---|
976 | klon, Tbef(:), zq(:), zqs(:), gammasat(:), ratqs(:,k), & |
---|
977 | keepgoing(:), rneb(:,k), zqn(:), qvc(:)) |
---|
978 | |
---|
979 | |
---|
980 | ELSE !--Generalised lognormal (Bony and Emanuel 2001) |
---|
981 | |
---|
982 | DO i=1,klon !todoan : check if loop in i is needed |
---|
983 | |
---|
984 | IF (keepgoing(i)) THEN |
---|
985 | |
---|
986 | zpdf_sig(i)=ratqs(i,k)*zq(i) |
---|
987 | zpdf_k(i)=-sqrt(log(1.+(zpdf_sig(i)/zq(i))**2)) |
---|
988 | zpdf_delta(i)=log(zq(i)/(gammasat(i)*zqs(i))) |
---|
989 | zpdf_a(i)=zpdf_delta(i)/(zpdf_k(i)*sqrt(2.)) |
---|
990 | zpdf_b(i)=zpdf_k(i)/(2.*sqrt(2.)) |
---|
991 | zpdf_e1(i)=zpdf_a(i)-zpdf_b(i) |
---|
992 | zpdf_e1(i)=sign(min(ABS(zpdf_e1(i)),5.),zpdf_e1(i)) |
---|
993 | zpdf_e1(i)=1.-erf(zpdf_e1(i)) |
---|
994 | zpdf_e2(i)=zpdf_a(i)+zpdf_b(i) |
---|
995 | zpdf_e2(i)=sign(min(ABS(zpdf_e2(i)),5.),zpdf_e2(i)) |
---|
996 | zpdf_e2(i)=1.-erf(zpdf_e2(i)) |
---|
997 | |
---|
998 | IF (zpdf_e1(i).LT.1.e-10) THEN |
---|
999 | rneb(i,k)=0. |
---|
1000 | zqn(i)=zqs(i) |
---|
1001 | !--AB grid-mean vapor in the cloud - we assume saturation adjustment |
---|
1002 | qvc(i) = 0. |
---|
1003 | ELSE |
---|
1004 | rneb(i,k)=0.5*zpdf_e1(i) |
---|
1005 | zqn(i)=zq(i)*zpdf_e2(i)/zpdf_e1(i) |
---|
1006 | !--AB grid-mean vapor in the cloud - we assume saturation adjustment |
---|
1007 | qvc(i) = rneb(i,k) * zqs(i) |
---|
1008 | ENDIF |
---|
1009 | |
---|
1010 | ENDIF ! keepgoing |
---|
1011 | ENDDO ! loop on klon |
---|
1012 | |
---|
1013 | ENDIF ! .NOT. ok_ice_supersat |
---|
1014 | |
---|
1015 | DO i=1,klon |
---|
1016 | IF (keepgoing(i)) THEN |
---|
1017 | |
---|
1018 | ! If vertical heterogeneity, change fraction by volume as well |
---|
1019 | IF (iflag_cloudth_vert.GE.3) THEN |
---|
1020 | ctot_vol(i,k)=rneb(i,k) |
---|
1021 | rneblsvol(i,k)=ctot_vol(i,k) |
---|
1022 | ENDIF |
---|
1023 | |
---|
1024 | |
---|
1025 | ! P2.2.2> Approximative calculation of temperature variation DT |
---|
1026 | ! due to condensation. |
---|
1027 | ! Calculated variables: |
---|
1028 | ! dT : temperature change due to condensation |
---|
1029 | !--------------------------------------------------------------- |
---|
1030 | |
---|
1031 | |
---|
1032 | IF (zfice(i).LT.1) THEN |
---|
1033 | cste=RLVTT |
---|
1034 | ELSE |
---|
1035 | cste=RLSTT |
---|
1036 | ENDIF |
---|
1037 | |
---|
1038 | ! LEA_R : check formule |
---|
1039 | IF ( ok_unadjusted_clouds ) THEN |
---|
1040 | !--AB We relax the saturation adjustment assumption |
---|
1041 | !-- qvc (grid-mean vapor in cloud) is calculated by the condensation scheme |
---|
1042 | IF ( rneb(i,k) .GT. eps ) THEN |
---|
1043 | qlbef(i) = MAX(0., zqn(i) - qvc(i) / rneb(i,k)) |
---|
1044 | ELSE |
---|
1045 | qlbef(i) = 0. |
---|
1046 | ENDIF |
---|
1047 | ELSE |
---|
1048 | qlbef(i)=max(0.,zqn(i)-zqs(i)) |
---|
1049 | ENDIF |
---|
1050 | |
---|
1051 | num = -Tbef(i)+zt(i)+rneb(i,k)*((1-zfice(i))*RLVTT & |
---|
1052 | +zfice(i)*RLSTT)/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i)))*qlbef(i) |
---|
1053 | denom = 1.+rneb(i,k)*((1-zfice(i))*RLVTT+zfice(i)*RLSTT)/cste*zdqs(i) & |
---|
1054 | -(RLSTT-RLVTT)/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i)))*rneb(i,k) & |
---|
1055 | *qlbef(i)*dzfice(i) |
---|
1056 | ! here we update a provisory temperature variable that only serves in the iteration |
---|
1057 | ! process |
---|
1058 | DT(i)=num/denom |
---|
1059 | n_i(i)=n_i(i)+1 |
---|
1060 | |
---|
1061 | ENDIF ! end keepgoing |
---|
1062 | |
---|
1063 | ENDDO ! end loop on i |
---|
1064 | |
---|
1065 | ENDDO ! iter=1,iflag_fisrtilp_qsat+1 |
---|
1066 | |
---|
1067 | ! P2.3> Final quantities calculation |
---|
1068 | ! Calculated variables: |
---|
1069 | ! rneb : cloud fraction |
---|
1070 | ! zcond: mean condensed water in the mesh |
---|
1071 | ! zqn : mean water vapor in the mesh |
---|
1072 | ! zfice: ice fraction in clouds |
---|
1073 | ! zt : temperature |
---|
1074 | ! rhcl : clear-sky relative humidity |
---|
1075 | ! ---------------------------------------------------------------- |
---|
1076 | |
---|
1077 | |
---|
1078 | ! For iflag_t_glace GE 4 the phase partition function dependends on temperature AND distance to cloud top |
---|
1079 | IF (iflag_t_glace.GE.4) THEN |
---|
1080 | CALL distance_to_cloud_top(klon,klev,k,temp,pplay,paprs,rneb,zdistcltop,ztemp_cltop) |
---|
1081 | distcltop(:,k)=zdistcltop(:) |
---|
1082 | temp_cltop(:,k)=ztemp_cltop(:) |
---|
1083 | ENDIF |
---|
1084 | |
---|
1085 | ! Partition function depending on temperature |
---|
1086 | CALL icefrac_lscp(klon, zt, iflag_ice_thermo, zdistcltop, ztemp_cltop, zfice, dzfice) |
---|
1087 | |
---|
1088 | ! Partition function depending on tke for non shallow-convective clouds |
---|
1089 | IF (iflag_icefrac .GE. 1) THEN |
---|
1090 | |
---|
1091 | CALL icefrac_lscp_turb(klon, dtime, Tbef, pplay(:,k), paprs(:,k), paprs(:,k+1), qice_save(:,k), ziflcld, zqn, & |
---|
1092 | rneb(:,k), tke(:,k), tke_dissip(:,k), zqliq, zqvapcl, zqice, zfice_turb, dzfice_turb, cldfraliq(:,k),sigma2_icefracturb(:,k), mean_icefracturb(:,k)) |
---|
1093 | |
---|
1094 | ENDIF |
---|
1095 | |
---|
1096 | ! Water vapor update, Phase determination and subsequent latent heat exchange |
---|
1097 | DO i=1, klon |
---|
1098 | ! Overwrite phase partitioning in boundary layer mixed phase clouds when the |
---|
1099 | ! iflag_cloudth_vert=7 and specific param is activated |
---|
1100 | IF (mpc_bl_points(i,k) .GT. 0) THEN |
---|
1101 | zcond(i) = MAX(0.0,qincloud_mpc(i))*rneb(i,k) |
---|
1102 | ! following line is very strange and probably wrong |
---|
1103 | rhcl(i,k)= (zqs(i)+zq(i))/2./zqs(i) |
---|
1104 | ! water vapor update and partition function if thermals |
---|
1105 | zq(i) = zq(i) - zcond(i) |
---|
1106 | zfice(i)=zfice_th(i) |
---|
1107 | ELSE |
---|
1108 | ! Checks on rneb, rhcl and zqn |
---|
1109 | IF (rneb(i,k) .LE. 0.0) THEN |
---|
1110 | zqn(i) = 0.0 |
---|
1111 | rneb(i,k) = 0.0 |
---|
1112 | zcond(i) = 0.0 |
---|
1113 | rhcl(i,k)=zq(i)/zqs(i) |
---|
1114 | ELSE IF (rneb(i,k) .GE. 1.0) THEN |
---|
1115 | zqn(i) = zq(i) |
---|
1116 | rneb(i,k) = 1.0 |
---|
1117 | IF ( ok_unadjusted_clouds ) THEN |
---|
1118 | !--AB We relax the saturation adjustment assumption |
---|
1119 | !-- qvc (grid-mean vapor in cloud) is calculated by the condensation scheme |
---|
1120 | zcond(i) = MAX(0., zqn(i) - qvc(i)) |
---|
1121 | ELSE |
---|
1122 | zcond(i) = MAX(0.0,zqn(i)-zqs(i)) |
---|
1123 | ENDIF |
---|
1124 | rhcl(i,k)=1.0 |
---|
1125 | ELSE |
---|
1126 | IF ( ok_unadjusted_clouds ) THEN |
---|
1127 | !--AB We relax the saturation adjustment assumption |
---|
1128 | !-- qvc (grid-mean vapor in cloud) is calculated by the condensation scheme |
---|
1129 | zcond(i) = MAX(0., zqn(i) * rneb(i,k) - qvc(i)) |
---|
1130 | ELSE |
---|
1131 | zcond(i) = MAX(0.0,zqn(i)-zqs(i))*rneb(i,k) |
---|
1132 | ENDIF |
---|
1133 | ! following line is very strange and probably wrong: |
---|
1134 | rhcl(i,k)=(zqs(i)+zq(i))/2./zqs(i) |
---|
1135 | ! Overwrite partitioning for non shallow-convective clouds if iflag_icefrac>1 (icefrac turb param) |
---|
1136 | IF (iflag_icefrac .GE. 1) THEN |
---|
1137 | IF (lognormale(i)) THEN |
---|
1138 | zcond(i) = zqliq(i) + zqice(i) |
---|
1139 | zfice(i)=zfice_turb(i) |
---|
1140 | rhcl(i,k) = zqvapcl(i) * rneb(i,k) + (zq(i) - zqn(i)) * (1.-rneb(i,k)) |
---|
1141 | ENDIF |
---|
1142 | ENDIF |
---|
1143 | ENDIF |
---|
1144 | |
---|
1145 | ! water vapor update |
---|
1146 | zq(i) = zq(i) - zcond(i) |
---|
1147 | |
---|
1148 | ENDIF |
---|
1149 | |
---|
1150 | ! c_iso : routine that computes in-cloud supersaturation |
---|
1151 | ! c_iso condensation of isotopes (zcond, zsursat, zfice, zq in input) |
---|
1152 | |
---|
1153 | ! temperature update due to phase change |
---|
1154 | zt(i) = zt(i) + (1.-zfice(i))*zcond(i) & |
---|
1155 | & * RLVTT/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i)+zcond(i))) & |
---|
1156 | +zfice(i)*zcond(i) * RLSTT/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i)+zcond(i))) |
---|
1157 | ENDDO |
---|
1158 | |
---|
1159 | ! If vertical heterogeneity, change volume fraction |
---|
1160 | IF (iflag_cloudth_vert .GE. 3) THEN |
---|
1161 | ctot_vol(1:klon,k)=min(max(ctot_vol(1:klon,k),0.),1.) |
---|
1162 | rneblsvol(1:klon,k)=ctot_vol(1:klon,k) |
---|
1163 | ENDIF |
---|
1164 | |
---|
1165 | !--AB Write diagnostics and tracers for ice supersaturation |
---|
1166 | IF ( ok_ice_supersat ) THEN |
---|
1167 | CALL calc_qsat_ecmwf(klon,zt,qzero,pplay(:,k),RTT,1,.false.,qsatl(:,k),zdqs) |
---|
1168 | CALL calc_qsat_ecmwf(klon,zt,qzero,pplay(:,k),RTT,2,.false.,qsati(:,k),zdqs) |
---|
1169 | |
---|
1170 | DO i = 1, klon |
---|
1171 | |
---|
1172 | cf_seri(i,k) = rneb(i,k) |
---|
1173 | |
---|
1174 | IF ( .NOT. ok_unadjusted_clouds ) THEN |
---|
1175 | qvc(i) = zqs(i) * rneb(i,k) |
---|
1176 | ENDIF |
---|
1177 | IF ( zq(i) .GT. min_qParent ) THEN |
---|
1178 | rvc_seri(i,k) = qvc(i) / zq(i) |
---|
1179 | ELSE |
---|
1180 | rvc_seri(i,k) = min_ratio |
---|
1181 | ENDIF |
---|
1182 | !--The MIN barrier is NEEDED because of: |
---|
1183 | !-- 1) very rare pathological cases of the lsc scheme (rvc = 1. + 1e-16 sometimes) |
---|
1184 | !-- 2) the thermal scheme does NOT guarantee that qvc <= qvap (or even qincld <= qtot) |
---|
1185 | !--The MAX barrier is a safeguard that should not be activated |
---|
1186 | rvc_seri(i,k) = MIN(MAX(rvc_seri(i,k), 0.), 1.) |
---|
1187 | |
---|
1188 | !--Diagnostics |
---|
1189 | gamma_cond(i,k) = gammasat(i) |
---|
1190 | IF ( issrfra(i,k) .LT. eps ) THEN |
---|
1191 | issrfra(i,k) = 0. |
---|
1192 | qissr(i,k) = 0. |
---|
1193 | ENDIF |
---|
1194 | subfra(i,k) = 1. - cf_seri(i,k) - issrfra(i,k) |
---|
1195 | qsub(i,k) = zq(i) - qvc(i) - qissr(i,k) |
---|
1196 | IF ( subfra(i,k) .LT. eps ) THEN |
---|
1197 | subfra(i,k) = 0. |
---|
1198 | qsub(i,k) = 0. |
---|
1199 | ENDIF |
---|
1200 | qcld(i,k) = qvc(i) + zcond(i) |
---|
1201 | IF ( cf_seri(i,k) .LT. eps ) THEN |
---|
1202 | qcld(i,k) = 0. |
---|
1203 | ENDIF |
---|
1204 | ENDDO |
---|
1205 | ENDIF |
---|
1206 | |
---|
1207 | |
---|
1208 | ! ---------------------------------------------------------------- |
---|
1209 | ! P3> Precipitation formation |
---|
1210 | ! ---------------------------------------------------------------- |
---|
1211 | |
---|
1212 | !================================================================ |
---|
1213 | IF (ok_poprecip) THEN |
---|
1214 | |
---|
1215 | DO i = 1, klon |
---|
1216 | zoliql(i) = zcond(i) * ( 1. - zfice(i) ) |
---|
1217 | zoliqi(i) = zcond(i) * zfice(i) |
---|
1218 | ENDDO |
---|
1219 | |
---|
1220 | CALL poprecip_postcld(klon, dtime, paprs(:,k), paprs(:,k+1), pplay(:,k), & |
---|
1221 | ctot_vol(:,k), ptconv(:,k), & |
---|
1222 | zt, zq, zoliql, zoliqi, zfice, & |
---|
1223 | rneb(:,k), znebprecipclr, znebprecipcld, & |
---|
1224 | zrfl, zrflclr, zrflcld, & |
---|
1225 | zifl, ziflclr, ziflcld, & |
---|
1226 | qraindiag(:,k), qsnowdiag(:,k), dqrauto(:,k), & |
---|
1227 | dqrcol(:,k), dqrmelt(:,k), dqrfreez(:,k), & |
---|
1228 | dqsauto(:,k), dqsagg(:,k), dqsrim(:,k), & |
---|
1229 | dqsmelt(:,k), dqsfreez(:,k) & |
---|
1230 | ) |
---|
1231 | |
---|
1232 | DO i = 1, klon |
---|
1233 | zoliq(i) = zoliql(i) + zoliqi(i) |
---|
1234 | IF ( zoliq(i) .GT. 0. ) THEN |
---|
1235 | zfice(i) = zoliqi(i)/zoliq(i) |
---|
1236 | ELSE |
---|
1237 | zfice(i) = 0.0 |
---|
1238 | ENDIF |
---|
1239 | |
---|
1240 | ! calculation of specific content of condensates seen by radiative scheme |
---|
1241 | IF (ok_radocond_snow) THEN |
---|
1242 | radocond(i,k) = zoliq(i) |
---|
1243 | radocondl(i,k)= radocond(i,k)*(1.-zfice(i)) |
---|
1244 | radocondi(i,k)= radocond(i,k)*zfice(i)+qsnowdiag(i,k) |
---|
1245 | ELSE |
---|
1246 | radocond(i,k) = zoliq(i) |
---|
1247 | radocondl(i,k)= radocond(i,k)*(1.-zfice(i)) |
---|
1248 | radocondi(i,k)= radocond(i,k)*zfice(i) |
---|
1249 | ENDIF |
---|
1250 | ENDDO |
---|
1251 | |
---|
1252 | !================================================================ |
---|
1253 | ELSE |
---|
1254 | |
---|
1255 | ! LTP: |
---|
1256 | IF (iflag_evap_prec .GE. 4) THEN |
---|
1257 | |
---|
1258 | !Partitionning between precipitation coming from clouds and that coming from CS |
---|
1259 | |
---|
1260 | !0) Calculate tot_zneb, total cloud fraction above the cloud |
---|
1261 | !assuming a maximum-random overlap (voir Jakob and Klein, 2000) |
---|
1262 | |
---|
1263 | DO i=1, klon |
---|
1264 | tot_znebn(i) = 1. - (1.-tot_zneb(i))*(1 - max(rneb(i,k),zneb(i))) & |
---|
1265 | /(1.-min(zneb(i),1.-smallestreal)) |
---|
1266 | d_tot_zneb(i) = tot_znebn(i) - tot_zneb(i) |
---|
1267 | tot_zneb(i) = tot_znebn(i) |
---|
1268 | |
---|
1269 | |
---|
1270 | !1) Cloudy to clear air |
---|
1271 | d_znebprecip_cld_clr(i) = znebprecipcld(i) - min(rneb(i,k),znebprecipcld(i)) |
---|
1272 | IF (znebprecipcld(i) .GT. 0.) THEN |
---|
1273 | d_zrfl_cld_clr(i) = d_znebprecip_cld_clr(i)/znebprecipcld(i)*zrflcld(i) |
---|
1274 | d_zifl_cld_clr(i) = d_znebprecip_cld_clr(i)/znebprecipcld(i)*ziflcld(i) |
---|
1275 | ELSE |
---|
1276 | d_zrfl_cld_clr(i) = 0. |
---|
1277 | d_zifl_cld_clr(i) = 0. |
---|
1278 | ENDIF |
---|
1279 | |
---|
1280 | !2) Clear to cloudy air |
---|
1281 | d_znebprecip_clr_cld(i) = max(0., min(znebprecipclr(i), rneb(i,k) - d_tot_zneb(i) - zneb(i))) |
---|
1282 | IF (znebprecipclr(i) .GT. 0) THEN |
---|
1283 | d_zrfl_clr_cld(i) = d_znebprecip_clr_cld(i)/znebprecipclr(i)*zrflclr(i) |
---|
1284 | d_zifl_clr_cld(i) = d_znebprecip_clr_cld(i)/znebprecipclr(i)*ziflclr(i) |
---|
1285 | ELSE |
---|
1286 | d_zrfl_clr_cld(i) = 0. |
---|
1287 | d_zifl_clr_cld(i) = 0. |
---|
1288 | ENDIF |
---|
1289 | |
---|
1290 | !Update variables |
---|
1291 | znebprecipcld(i) = znebprecipcld(i) + d_znebprecip_clr_cld(i) - d_znebprecip_cld_clr(i) |
---|
1292 | znebprecipclr(i) = znebprecipclr(i) + d_znebprecip_cld_clr(i) - d_znebprecip_clr_cld(i) |
---|
1293 | zrflcld(i) = zrflcld(i) + d_zrfl_clr_cld(i) - d_zrfl_cld_clr(i) |
---|
1294 | ziflcld(i) = ziflcld(i) + d_zifl_clr_cld(i) - d_zifl_cld_clr(i) |
---|
1295 | zrflclr(i) = zrflclr(i) + d_zrfl_cld_clr(i) - d_zrfl_clr_cld(i) |
---|
1296 | ziflclr(i) = ziflclr(i) + d_zifl_cld_clr(i) - d_zifl_clr_cld(i) |
---|
1297 | |
---|
1298 | ! c_iso do the same thing for isotopes precip |
---|
1299 | ENDDO |
---|
1300 | ENDIF |
---|
1301 | |
---|
1302 | |
---|
1303 | ! Autoconversion |
---|
1304 | ! ------------------------------------------------------------------------------- |
---|
1305 | |
---|
1306 | |
---|
1307 | ! Initialisation of zoliq and radocond variables |
---|
1308 | |
---|
1309 | DO i = 1, klon |
---|
1310 | zoliq(i) = zcond(i) |
---|
1311 | zoliqi(i)= zoliq(i)*zfice(i) |
---|
1312 | zoliql(i)= zoliq(i)*(1.-zfice(i)) |
---|
1313 | ! c_iso : initialisation of zoliq* also for isotopes |
---|
1314 | zrho(i,k) = pplay(i,k) / zt(i) / RD |
---|
1315 | zdz(i) = (paprs(i,k)-paprs(i,k+1)) / (zrho(i,k)*RG) |
---|
1316 | iwc(i) = 0. |
---|
1317 | zneb(i) = MAX(rneb(i,k),seuil_neb) |
---|
1318 | radocond(i,k) = zoliq(i)/REAL(niter_lscp+1) |
---|
1319 | radocondi(i,k)=zoliq(i)*zfice(i)/REAL(niter_lscp+1) |
---|
1320 | radocondl(i,k)=zoliq(i)*(1.-zfice(i))/REAL(niter_lscp+1) |
---|
1321 | ENDDO |
---|
1322 | |
---|
1323 | |
---|
1324 | DO n = 1, niter_lscp |
---|
1325 | |
---|
1326 | DO i=1,klon |
---|
1327 | IF (rneb(i,k).GT.0.0) THEN |
---|
1328 | iwc(i) = zrho(i,k) * zoliqi(i) / zneb(i) ! in-cloud ice condensate content |
---|
1329 | ENDIF |
---|
1330 | ENDDO |
---|
1331 | |
---|
1332 | CALL fallice_velocity(klon,iwc(:),zt(:),zrho(:,k),pplay(:,k),ptconv(:,k),velo(:,k)) |
---|
1333 | |
---|
1334 | DO i = 1, klon |
---|
1335 | |
---|
1336 | IF (rneb(i,k).GT.0.0) THEN |
---|
1337 | |
---|
1338 | ! Initialization of zrain, zsnow and zprecip: |
---|
1339 | zrain=0. |
---|
1340 | zsnow=0. |
---|
1341 | zprecip=0. |
---|
1342 | ! c_iso same init for isotopes. Externalisation? |
---|
1343 | |
---|
1344 | IF (zneb(i).EQ.seuil_neb) THEN |
---|
1345 | zprecip = 0.0 |
---|
1346 | zsnow = 0.0 |
---|
1347 | zrain= 0.0 |
---|
1348 | ELSE |
---|
1349 | |
---|
1350 | IF (ptconv(i,k)) THEN ! if convective point |
---|
1351 | zcl=cld_lc_con |
---|
1352 | zct=1./cld_tau_con |
---|
1353 | zexpo=cld_expo_con |
---|
1354 | ffallv=ffallv_con |
---|
1355 | ELSE |
---|
1356 | zcl=cld_lc_lsc |
---|
1357 | zct=1./cld_tau_lsc |
---|
1358 | zexpo=cld_expo_lsc |
---|
1359 | ffallv=ffallv_lsc |
---|
1360 | ENDIF |
---|
1361 | |
---|
1362 | |
---|
1363 | ! if vertical heterogeneity is taken into account, we use |
---|
1364 | ! the "true" volume fraction instead of a modified |
---|
1365 | ! surface fraction (which is larger and artificially |
---|
1366 | ! reduces the in-cloud water). |
---|
1367 | |
---|
1368 | ! Liquid water quantity to remove: zchau (Sundqvist, 1978) |
---|
1369 | ! dqliq/dt=-qliq/tau*(1-exp(-qcin/clw)**2) |
---|
1370 | !......................................................... |
---|
1371 | IF ((iflag_cloudth_vert.GE.3).AND.(iflag_rain_incloud_vol.EQ.1)) THEN |
---|
1372 | |
---|
1373 | ! if vertical heterogeneity is taken into account, we use |
---|
1374 | ! the "true" volume fraction instead of a modified |
---|
1375 | ! surface fraction (which is larger and artificially |
---|
1376 | ! reduces the in-cloud water). |
---|
1377 | effective_zneb=ctot_vol(i,k) |
---|
1378 | ELSE |
---|
1379 | effective_zneb=zneb(i) |
---|
1380 | ENDIF |
---|
1381 | |
---|
1382 | |
---|
1383 | IF (iflag_autoconversion .EQ. 2) THEN |
---|
1384 | ! two-steps resolution with niter_lscp=1 sufficient |
---|
1385 | ! we first treat the second term (with exponential) in an explicit way |
---|
1386 | ! and then treat the first term (-q/tau) in an exact way |
---|
1387 | zchau=zoliql(i)*(1.-exp(-dtime/REAL(niter_lscp)*zct & |
---|
1388 | *(1.-exp(-(zoliql(i)/effective_zneb/zcl)**zexpo)))) |
---|
1389 | ELSE |
---|
1390 | ! old explicit resolution with subtimesteps |
---|
1391 | zchau = zct*dtime/REAL(niter_lscp)*zoliql(i) & |
---|
1392 | *(1.0-EXP(-(zoliql(i)/effective_zneb/zcl)**zexpo)) |
---|
1393 | ENDIF |
---|
1394 | |
---|
1395 | |
---|
1396 | ! Ice water quantity to remove (Zender & Kiehl, 1997) |
---|
1397 | ! dqice/dt=1/rho*d(rho*wice*qice)/dz |
---|
1398 | !.................................... |
---|
1399 | IF (iflag_autoconversion .EQ. 2) THEN |
---|
1400 | ! exact resolution, niter_lscp=1 is sufficient but works only |
---|
1401 | ! with iflag_vice=0 |
---|
1402 | IF (zoliqi(i) .GT. 0.) THEN |
---|
1403 | zfroi=(zoliqi(i)-((zoliqi(i)**(-dice_velo)) & |
---|
1404 | +dice_velo*dtime/REAL(niter_lscp)*cice_velo/zdz(i)*ffallv)**(-1./dice_velo)) |
---|
1405 | ELSE |
---|
1406 | zfroi=0. |
---|
1407 | ENDIF |
---|
1408 | ELSE |
---|
1409 | ! old explicit resolution with subtimesteps |
---|
1410 | zfroi = dtime/REAL(niter_lscp)/zdz(i)*zoliqi(i)*velo(i,k) |
---|
1411 | ENDIF |
---|
1412 | |
---|
1413 | zrain = MIN(MAX(zchau,0.0),zoliql(i)) |
---|
1414 | zsnow = MIN(MAX(zfroi,0.0),zoliqi(i)) |
---|
1415 | zprecip = MAX(zrain + zsnow,0.0) |
---|
1416 | |
---|
1417 | ENDIF |
---|
1418 | |
---|
1419 | IF (iflag_autoconversion .GE. 1) THEN |
---|
1420 | ! debugged version with phase conservation through the autoconversion process |
---|
1421 | zoliql(i) = MAX(zoliql(i)-1.*zrain , 0.0) |
---|
1422 | zoliqi(i) = MAX(zoliqi(i)-1.*zsnow , 0.0) |
---|
1423 | zoliq(i) = MAX(zoliq(i)-zprecip , 0.0) |
---|
1424 | ELSE |
---|
1425 | ! bugged version with phase resetting |
---|
1426 | zoliql(i) = MAX(zoliq(i)*(1.-zfice(i))-1.*zrain , 0.0) |
---|
1427 | zoliqi(i) = MAX(zoliq(i)*zfice(i)-1.*zsnow , 0.0) |
---|
1428 | zoliq(i) = MAX(zoliq(i)-zprecip , 0.0) |
---|
1429 | ENDIF |
---|
1430 | |
---|
1431 | ! c_iso: call isotope_conversion (for readibility) or duplicate |
---|
1432 | |
---|
1433 | radocond(i,k) = radocond(i,k) + zoliq(i)/REAL(niter_lscp+1) |
---|
1434 | radocondl(i,k) = radocondl(i,k) + zoliql(i)/REAL(niter_lscp+1) |
---|
1435 | radocondi(i,k) = radocondi(i,k) + zoliqi(i)/REAL(niter_lscp+1) |
---|
1436 | |
---|
1437 | ENDIF ! rneb >0 |
---|
1438 | |
---|
1439 | ENDDO ! i = 1,klon |
---|
1440 | |
---|
1441 | ENDDO ! n = 1,niter |
---|
1442 | |
---|
1443 | ! Precipitation flux calculation |
---|
1444 | |
---|
1445 | DO i = 1, klon |
---|
1446 | |
---|
1447 | IF (iflag_evap_prec.GE.4) THEN |
---|
1448 | ziflprev(i)=ziflcld(i) |
---|
1449 | ELSE |
---|
1450 | ziflprev(i)=zifl(i)*zneb(i) |
---|
1451 | ENDIF |
---|
1452 | |
---|
1453 | IF (rneb(i,k) .GT. 0.0) THEN |
---|
1454 | |
---|
1455 | ! CR&JYG: We account for the Wegener-Findeisen-Bergeron process in the precipitation flux: |
---|
1456 | ! If T<0C, liquid precip are converted into ice, which leads to an increase in |
---|
1457 | ! temperature DeltaT. The effect of DeltaT on condensates and precipitation is roughly |
---|
1458 | ! taken into account through a linearization of the equations and by approximating |
---|
1459 | ! the liquid precipitation process with a "threshold" process. We assume that |
---|
1460 | ! condensates are not modified during this operation. Liquid precipitation is |
---|
1461 | ! removed (in the limit DeltaT<273.15-T). Solid precipitation increases. |
---|
1462 | ! Water vapor increases as well |
---|
1463 | ! Note that compared to fisrtilp, we always assume iflag_bergeron=2 |
---|
1464 | |
---|
1465 | zqpreci(i)=(zcond(i)-zoliq(i))*zfice(i) |
---|
1466 | zqprecl(i)=(zcond(i)-zoliq(i))*(1.-zfice(i)) |
---|
1467 | zcp=RCPD*(1.0+RVTMP2*(zq(i)+zmqc(i)+zcond(i))) |
---|
1468 | coef1 = rneb(i,k)*RLSTT/zcp*zdqsdT_raw(i) |
---|
1469 | ! Computation of DT if all the liquid precip freezes |
---|
1470 | DeltaT = RLMLT*zqprecl(i) / (zcp*(1.+coef1)) |
---|
1471 | ! T should not exceed the freezing point |
---|
1472 | ! that is Delta > RTT-zt(i) |
---|
1473 | DeltaT = max( min( RTT-zt(i), DeltaT) , 0. ) |
---|
1474 | zt(i) = zt(i) + DeltaT |
---|
1475 | ! water vaporization due to temp. increase |
---|
1476 | Deltaq = rneb(i,k)*zdqsdT_raw(i)*DeltaT |
---|
1477 | ! we add this vaporized water to the total vapor and we remove it from the precip |
---|
1478 | zq(i) = zq(i) + Deltaq |
---|
1479 | ! The three "max" lines herebelow protect from rounding errors |
---|
1480 | zcond(i) = max( zcond(i)- Deltaq, 0. ) |
---|
1481 | ! liquid precipitation converted to ice precip |
---|
1482 | Deltaqprecl = -zcp/RLMLT*(1.+coef1)*DeltaT |
---|
1483 | zqprecl(i) = max( zqprecl(i) + Deltaqprecl, 0. ) |
---|
1484 | ! iced water budget |
---|
1485 | zqpreci(i) = max (zqpreci(i) - Deltaqprecl - Deltaq, 0.) |
---|
1486 | |
---|
1487 | ! c_iso : mv here condensation of isotopes + redispatchage en precip |
---|
1488 | |
---|
1489 | IF (iflag_evap_prec.GE.4) THEN |
---|
1490 | zrflcld(i) = zrflcld(i)+zqprecl(i) & |
---|
1491 | *(paprs(i,k)-paprs(i,k+1))/(RG*dtime) |
---|
1492 | ziflcld(i) = ziflcld(i)+ zqpreci(i) & |
---|
1493 | *(paprs(i,k)-paprs(i,k+1))/(RG*dtime) |
---|
1494 | znebprecipcld(i) = rneb(i,k) |
---|
1495 | zrfl(i) = zrflcld(i) + zrflclr(i) |
---|
1496 | zifl(i) = ziflcld(i) + ziflclr(i) |
---|
1497 | ELSE |
---|
1498 | zrfl(i) = zrfl(i)+ zqprecl(i) & |
---|
1499 | *(paprs(i,k)-paprs(i,k+1))/(RG*dtime) |
---|
1500 | zifl(i) = zifl(i)+ zqpreci(i) & |
---|
1501 | *(paprs(i,k)-paprs(i,k+1))/(RG*dtime) |
---|
1502 | ENDIF |
---|
1503 | ! c_iso : same for isotopes |
---|
1504 | |
---|
1505 | ENDIF ! rneb>0 |
---|
1506 | |
---|
1507 | ENDDO |
---|
1508 | |
---|
1509 | ! LTP: limit of surface cloud fraction covered by precipitation when the local intensity of the flux is below rain_int_min |
---|
1510 | ! if iflag_evap_prec>=4 |
---|
1511 | IF (iflag_evap_prec.GE.4) THEN |
---|
1512 | |
---|
1513 | DO i=1,klon |
---|
1514 | |
---|
1515 | IF ((zrflclr(i) + ziflclr(i)) .GT. 0. ) THEN |
---|
1516 | znebprecipclr(i) = min(znebprecipclr(i),max(zrflclr(i)/ & |
---|
1517 | (MAX(znebprecipclr(i),seuil_neb)*rain_int_min), ziflclr(i)/(MAX(znebprecipclr(i),seuil_neb)*rain_int_min))) |
---|
1518 | ELSE |
---|
1519 | znebprecipclr(i)=0.0 |
---|
1520 | ENDIF |
---|
1521 | |
---|
1522 | IF ((zrflcld(i) + ziflcld(i)) .GT. 0.) THEN |
---|
1523 | znebprecipcld(i) = min(znebprecipcld(i), max(zrflcld(i)/ & |
---|
1524 | (MAX(znebprecipcld(i),seuil_neb)*rain_int_min), ziflcld(i)/(MAX(znebprecipcld(i),seuil_neb)*rain_int_min))) |
---|
1525 | ELSE |
---|
1526 | znebprecipcld(i)=0.0 |
---|
1527 | ENDIF |
---|
1528 | !IF ( ((1-zfice(i))*zoliq(i) .GT. 0.) .AND. (zt(i) .LE. 233.15) ) THEN |
---|
1529 | !print*,'WARNING LEA OLIQ A <-40°C ' |
---|
1530 | !print*,'zt,Tbef,oliq,oice,cldfraliq,icefrac,rneb',zt(i),Tbef(i),(1-zfice(i))*zoliq(i),zfice(i)*zoliq(i),cldfraliq(i,k),zfice(i),rneb(i,k) |
---|
1531 | !ENDIF |
---|
1532 | ENDDO |
---|
1533 | |
---|
1534 | ENDIF |
---|
1535 | |
---|
1536 | |
---|
1537 | ENDIF ! ok_poprecip |
---|
1538 | |
---|
1539 | ! End of precipitation formation |
---|
1540 | ! -------------------------------- |
---|
1541 | |
---|
1542 | |
---|
1543 | ! Calculation of cloud condensates amount seen by radiative scheme |
---|
1544 | !----------------------------------------------------------------- |
---|
1545 | |
---|
1546 | ! Calculation of the concentration of condensates seen by the radiation scheme |
---|
1547 | ! for liquid phase, we take radocondl |
---|
1548 | ! for ice phase, we take radocondi if we neglect snowfall, otherwise (ok_radocond_snow=true) |
---|
1549 | ! we recalculate radocondi to account for contributions from the precipitation flux |
---|
1550 | ! TODO: for the moment, we deactivate this option when ok_poprecip=.true. |
---|
1551 | |
---|
1552 | IF ((ok_radocond_snow) .AND. (k .LT. klev) .AND. (.NOT. ok_poprecip)) THEN |
---|
1553 | ! for the solid phase (crystals + snowflakes) |
---|
1554 | ! we recalculate radocondi by summing |
---|
1555 | ! the ice content calculated in the mesh |
---|
1556 | ! + the contribution of the non-evaporated snowfall |
---|
1557 | ! from the overlying layer |
---|
1558 | DO i=1,klon |
---|
1559 | IF (ziflprev(i) .NE. 0.0) THEN |
---|
1560 | radocondi(i,k)=zoliq(i)*zfice(i)+zqpreci(i)+ziflprev(i)/zrho(i,k+1)/velo(i,k+1) |
---|
1561 | ELSE |
---|
1562 | radocondi(i,k)=zoliq(i)*zfice(i)+zqpreci(i) |
---|
1563 | ENDIF |
---|
1564 | radocond(i,k)=radocondl(i,k)+radocondi(i,k) |
---|
1565 | ENDDO |
---|
1566 | ENDIF |
---|
1567 | |
---|
1568 | ! caculate the percentage of ice in "radocond" so cloud+precip seen by the radiation scheme |
---|
1569 | DO i=1,klon |
---|
1570 | IF (radocond(i,k) .GT. 0.) THEN |
---|
1571 | radicefrac(i,k)=MIN(MAX(radocondi(i,k)/radocond(i,k),0.),1.) |
---|
1572 | ENDIF |
---|
1573 | ENDDO |
---|
1574 | |
---|
1575 | ! ---------------------------------------------------------------- |
---|
1576 | ! P4> Wet scavenging |
---|
1577 | ! ---------------------------------------------------------------- |
---|
1578 | |
---|
1579 | !Scavenging through nucleation in the layer |
---|
1580 | |
---|
1581 | DO i = 1,klon |
---|
1582 | |
---|
1583 | IF(zcond(i).GT.zoliq(i)+1.e-10) THEN |
---|
1584 | beta(i,k) = (zcond(i)-zoliq(i))/zcond(i)/dtime |
---|
1585 | ELSE |
---|
1586 | beta(i,k) = 0. |
---|
1587 | ENDIF |
---|
1588 | |
---|
1589 | zprec_cond(i) = MAX(zcond(i)-zoliq(i),0.0)*(paprs(i,k)-paprs(i,k+1))/RG |
---|
1590 | |
---|
1591 | IF (rneb(i,k).GT.0.0.AND.zprec_cond(i).GT.0.) THEN |
---|
1592 | |
---|
1593 | IF (temp(i,k) .GE. t_glace_min) THEN |
---|
1594 | zalpha_tr = a_tr_sca(3) |
---|
1595 | ELSE |
---|
1596 | zalpha_tr = a_tr_sca(4) |
---|
1597 | ENDIF |
---|
1598 | |
---|
1599 | zfrac_lessi = 1. - EXP(zalpha_tr*zprec_cond(i)/zneb(i)) |
---|
1600 | frac_nucl(i,k)= 1.-zneb(i)*zfrac_lessi |
---|
1601 | |
---|
1602 | ! Nucleation with a factor of -1 instead of -0.5 |
---|
1603 | zfrac_lessi = 1. - EXP(-zprec_cond(i)/zneb(i)) |
---|
1604 | |
---|
1605 | ENDIF |
---|
1606 | |
---|
1607 | ENDDO |
---|
1608 | |
---|
1609 | ! Scavenging through impaction in the underlying layer |
---|
1610 | |
---|
1611 | DO kk = k-1, 1, -1 |
---|
1612 | |
---|
1613 | DO i = 1, klon |
---|
1614 | |
---|
1615 | IF (rneb(i,k).GT.0.0.AND.zprec_cond(i).GT.0.) THEN |
---|
1616 | |
---|
1617 | IF (temp(i,kk) .GE. t_glace_min) THEN |
---|
1618 | zalpha_tr = a_tr_sca(1) |
---|
1619 | ELSE |
---|
1620 | zalpha_tr = a_tr_sca(2) |
---|
1621 | ENDIF |
---|
1622 | |
---|
1623 | zfrac_lessi = 1. - EXP(zalpha_tr*zprec_cond(i)/zneb(i)) |
---|
1624 | frac_impa(i,kk)= 1.-zneb(i)*zfrac_lessi |
---|
1625 | |
---|
1626 | ENDIF |
---|
1627 | |
---|
1628 | ENDDO |
---|
1629 | |
---|
1630 | ENDDO |
---|
1631 | |
---|
1632 | ! Outputs: |
---|
1633 | !------------------------------- |
---|
1634 | ! Precipitation fluxes at layer interfaces |
---|
1635 | ! + precipitation fractions + |
---|
1636 | ! temperature and water species tendencies |
---|
1637 | DO i = 1, klon |
---|
1638 | psfl(i,k)=zifl(i) |
---|
1639 | prfl(i,k)=zrfl(i) |
---|
1640 | pfraclr(i,k)=znebprecipclr(i) |
---|
1641 | pfracld(i,k)=znebprecipcld(i) |
---|
1642 | d_ql(i,k) = (1-zfice(i))*zoliq(i) |
---|
1643 | d_qi(i,k) = zfice(i)*zoliq(i) |
---|
1644 | d_q(i,k) = zq(i) - qt(i,k) |
---|
1645 | ! c_iso: same for isotopes |
---|
1646 | d_t(i,k) = zt(i) - temp(i,k) |
---|
1647 | ENDDO |
---|
1648 | |
---|
1649 | |
---|
1650 | ENDDO |
---|
1651 | |
---|
1652 | |
---|
1653 | ! Rain or snow at the surface (depending on the first layer temperature) |
---|
1654 | DO i = 1, klon |
---|
1655 | snow(i) = zifl(i) |
---|
1656 | rain(i) = zrfl(i) |
---|
1657 | ! c_iso final output |
---|
1658 | ENDDO |
---|
1659 | |
---|
1660 | IF (ncoreczq>0) THEN |
---|
1661 | WRITE(lunout,*)'WARNING : ZQ in LSCP ',ncoreczq,' val < 1.e-15.' |
---|
1662 | ENDIF |
---|
1663 | |
---|
1664 | |
---|
1665 | RETURN |
---|
1666 | |
---|
1667 | END SUBROUTINE lscp |
---|
1668 | !+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
---|
1669 | |
---|
1670 | END MODULE lmdz_lscp |
---|