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, omega, temp, qt, ql_seri, qi_seri, & |
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10 | ptconv, ratqs, sigma_qtherm, & |
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11 | d_t, d_q, d_ql, d_qi, rneb, rneblsvol, & |
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12 | pfraclr, pfracld, & |
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13 | cldfraliq, sigma2_icefracturb,mean_icefracturb, & |
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14 | radocond, radicefrac, rain, snow, & |
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15 | frac_impa, frac_nucl, beta, & |
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16 | prfl, psfl, rhcl, qta, fraca, & |
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17 | tv, pspsk, tla, thl, iflag_cld_th, & |
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18 | iflag_ice_thermo, distcltop, temp_cltop, & |
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19 | tke, tke_dissip, & |
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20 | cell_area, & |
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21 | cf_seri, rvc_seri, u_seri, v_seri, & |
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22 | qsub, qissr, qcld, subfra, issrfra, gamma_cond, & |
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23 | dcf_sub, dcf_con, dcf_mix, & |
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24 | dqi_adj, dqi_sub, dqi_con, dqi_mix, dqvc_adj, & |
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25 | dqvc_sub, dqvc_con, dqvc_mix, qsatl, qsati, & |
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26 | rcont_seri, flight_dist, flight_h2o, contfra, & |
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27 | Tcritcont, qcritcont, potcontfraP, potcontfraNP, & |
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28 | dcontfra_cir, dcf_avi, dqi_avi, dqvc_avi, & |
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29 | cloudth_sth,cloudth_senv,cloudth_sigmath,cloudth_sigmaenv, & |
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30 | qraindiag, qsnowdiag, dqreva, dqssub, dqrauto, & |
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31 | dqrcol, dqrmelt, dqrfreez, dqsauto, dqsagg, dqsrim,& |
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32 | dqsmelt, dqsfreez) |
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33 | |
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34 | !++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
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35 | ! Authors: Z.X. Li (LMD), J-L Dufresne (LMD), C. Rio (LMD), J-Y Grandpeix (LMD) |
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36 | ! A. JAM (LMD), J-B Madeleine (LMD), E. Vignon (LMD), L. Touzze-Peiffert (LMD) |
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37 | !-------------------------------------------------------------------------------- |
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38 | ! Date: 01/2021 |
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39 | !-------------------------------------------------------------------------------- |
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40 | ! Aim: Large Scale Clouds and Precipitation (LSCP) |
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41 | ! |
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42 | ! This code is a new version of the fisrtilp.F90 routine, which is itself a |
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43 | ! merge of 'first' (superrsaturation physics, P. LeVan K. Laval) |
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44 | ! and 'ilp' (il pleut, L. Li) |
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45 | ! |
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46 | ! Compared to the original fisrtilp code, lscp |
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47 | ! -> assumes thermcep = .TRUE. all the time (fisrtilp inconsistent when .FALSE.) |
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48 | ! -> consider always precipitation thermalisation (fl_cor_ebil>0) |
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49 | ! -> option iflag_fisrtilp_qsat<0 no longer possible (qsat does not evolve with T) |
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50 | ! -> option "oldbug" by JYG has been removed |
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51 | ! -> iflag_t_glace >0 always |
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52 | ! -> the 'all or nothing' cloud approach is no longer available (cpartiel=T always) |
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53 | ! -> rectangular distribution from L. Li no longer available |
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54 | ! -> We always account for the Wegener-Findeisen-Bergeron process (iflag_bergeron = 2 in fisrt) |
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55 | !-------------------------------------------------------------------------------- |
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56 | ! References: |
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57 | ! |
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58 | ! - Bony, S., & Emanuel, K. A. 2001, JAS, doi: 10.1175/1520-0469(2001)058<3158:APOTCA>2.0.CO;2 |
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59 | ! - Hourdin et al. 2013, Clim Dyn, doi:10.1007/s00382-012-1343-y |
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60 | ! - Jam et al. 2013, Boundary-Layer Meteorol, doi:10.1007/s10546-012-9789-3 |
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61 | ! - Jouhaud, et al. 2018. JAMES, doi:10.1029/2018MS001379 |
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62 | ! - Madeleine et al. 2020, JAMES, doi:10.1029/2020MS002046 |
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63 | ! - Touzze-Peifert Ludo, PhD thesis, p117-124 |
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64 | ! ------------------------------------------------------------------------------- |
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65 | ! Code structure: |
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66 | ! |
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67 | ! P0> Thermalization of the precipitation coming from the overlying layer |
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68 | ! P1> Evaporation of the precipitation (falling from the k+1 level) |
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69 | ! P2> Cloud formation (at the k level) |
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70 | ! P2.A.1> With the PDFs, calculation of cloud properties using the inital |
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71 | ! values of T and Q |
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72 | ! P2.A.2> Coupling between condensed water and temperature |
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73 | ! P2.A.3> Calculation of final quantities associated with cloud formation |
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74 | ! P2.B> Release of Latent heat after cloud formation |
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75 | ! P3> Autoconversion to precipitation (k-level) |
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76 | ! P4> Wet scavenging |
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77 | !------------------------------------------------------------------------------ |
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78 | ! Some preliminary comments (JBM) : |
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79 | ! |
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80 | ! The cloud water that the radiation scheme sees is not the same that the cloud |
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81 | ! water used in the physics and the dynamics |
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82 | ! |
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83 | ! During the autoconversion to precipitation (P3 step), radocond (cloud water used |
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84 | ! by the radiation scheme) is calculated as an average of the water that remains |
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85 | ! in the cloud during the precipitation and not the water remaining at the end |
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86 | ! of the time step. The latter is used in the rest of the physics and advected |
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87 | ! by the dynamics. |
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88 | ! |
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89 | ! In summary: |
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90 | ! |
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91 | ! Radiation: |
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92 | ! xflwc(newmicro)+xfiwc(newmicro) = |
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93 | ! radocond=lwcon(nc)+iwcon(nc) |
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94 | ! |
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95 | ! Notetheless, be aware of: |
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96 | ! |
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97 | ! radocond .NE. ocond(nc) |
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98 | ! i.e.: |
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99 | ! lwcon(nc)+iwcon(nc) .NE. ocond(nc) |
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100 | ! but oliq+(ocond-oliq) .EQ. ocond |
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101 | ! (which is not trivial) |
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102 | !++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
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103 | ! |
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104 | |
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105 | ! USE de modules contenant des fonctions. |
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106 | USE lmdz_cloudth, ONLY : cloudth, cloudth_v3, cloudth_v6, cloudth_mpc |
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107 | USE lmdz_lscp_tools, ONLY : calc_qsat_ecmwf, calc_gammasat |
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108 | USE lmdz_lscp_tools, ONLY : icefrac_lscp, icefrac_lscp_turb, distance_to_cloud_top |
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109 | USE lmdz_lscp_condensation, ONLY : condensation_lognormal, condensation_ice_supersat |
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110 | USE lmdz_lscp_precip, ONLY : histprecip_precld, histprecip_postcld |
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111 | USE lmdz_lscp_precip, ONLY : poprecip_precld, poprecip_postcld |
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112 | |
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113 | ! Use du module lmdz_lscp_ini contenant les constantes |
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114 | USE lmdz_lscp_ini, ONLY : prt_level, lunout, eps |
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115 | USE lmdz_lscp_ini, ONLY : seuil_neb, iflag_evap_prec, DDT0 |
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116 | USE lmdz_lscp_ini, ONLY : ok_radocond_snow, a_tr_sca |
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117 | USE lmdz_lscp_ini, ONLY : iflag_cloudth_vert, iflag_t_glace, iflag_fisrtilp_qsat |
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118 | USE lmdz_lscp_ini, ONLY : t_glace_min, min_frac_th_cld |
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119 | USE lmdz_lscp_ini, ONLY : RCPD, RLSTT, RLVTT, RVTMP2, RTT, RD, RG |
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120 | USE lmdz_lscp_ini, ONLY : ok_poprecip, ok_bug_phase_lscp |
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121 | USE lmdz_lscp_ini, ONLY : ok_ice_supersat, ok_unadjusted_clouds, iflag_icefrac |
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122 | USE lmdz_lscp_ini, ONLY : ok_plane_contrail |
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123 | |
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124 | IMPLICIT NONE |
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125 | |
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126 | !=============================================================================== |
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127 | ! VARIABLES DECLARATION |
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128 | !=============================================================================== |
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129 | |
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130 | ! INPUT VARIABLES: |
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131 | !----------------- |
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132 | |
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133 | INTEGER, INTENT(IN) :: klon,klev ! number of horizontal grid points and vertical levels |
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134 | REAL, INTENT(IN) :: dtime ! time step [s] |
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135 | REAL, INTENT(IN) :: missing_val ! missing value for output |
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136 | |
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137 | REAL, DIMENSION(klon,klev+1), INTENT(IN) :: paprs ! inter-layer pressure [Pa] |
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138 | REAL, DIMENSION(klon,klev), INTENT(IN) :: pplay ! mid-layer pressure [Pa] |
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139 | REAL, DIMENSION(klon,klev), INTENT(IN) :: temp ! temperature (K) |
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140 | REAL, DIMENSION(klon,klev), INTENT(IN) :: omega ! vertical velocity [Pa/s] |
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141 | REAL, DIMENSION(klon,klev), INTENT(IN) :: qt ! total specific humidity (in vapor phase in input) [kg/kg] |
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142 | REAL, DIMENSION(klon,klev), INTENT(IN) :: ql_seri ! liquid specific content [kg/kg] |
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143 | REAL, DIMENSION(klon,klev), INTENT(IN) :: qi_seri ! ice specific content [kg/kg] |
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144 | INTEGER, INTENT(IN) :: iflag_cld_th ! flag that determines the distribution of convective clouds |
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145 | INTEGER, INTENT(IN) :: iflag_ice_thermo! flag to activate the ice thermodynamics |
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146 | ! CR: if iflag_ice_thermo=2, only convection is active |
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147 | LOGICAL, DIMENSION(klon,klev), INTENT(IN) :: ptconv ! grid points where deep convection scheme is active |
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148 | |
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149 | !Inputs associated with thermal plumes |
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150 | |
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151 | REAL, DIMENSION(klon,klev), INTENT(IN) :: tv ! virtual potential temperature [K] |
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152 | REAL, DIMENSION(klon,klev), INTENT(IN) :: qta ! specific humidity within thermals [kg/kg] |
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153 | REAL, DIMENSION(klon,klev), INTENT(IN) :: fraca ! fraction of thermals within the mesh [-] |
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154 | REAL, DIMENSION(klon,klev), INTENT(IN) :: pspsk ! exner potential (p/100000)**(R/cp) |
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155 | REAL, DIMENSION(klon,klev), INTENT(IN) :: tla ! liquid temperature within thermals [K] |
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156 | REAL, DIMENSION(klon,klev+1), INTENT(IN) :: tke !--turbulent kinetic energy [m2/s2] |
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157 | REAL, DIMENSION(klon,klev+1), INTENT(IN) :: tke_dissip !--TKE dissipation [m2/s3] |
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158 | |
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159 | ! INPUT/OUTPUT variables |
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160 | !------------------------ |
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161 | |
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162 | REAL, DIMENSION(klon,klev), INTENT(INOUT) :: thl ! liquid potential temperature [K] |
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163 | REAL, DIMENSION(klon,klev), INTENT(INOUT) :: ratqs,sigma_qtherm ! function of pressure that sets the large-scale |
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164 | |
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165 | |
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166 | ! INPUT/OUTPUT condensation and ice supersaturation |
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167 | !-------------------------------------------------- |
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168 | REAL, DIMENSION(klon,klev), INTENT(INOUT):: cf_seri ! cloud fraction [-] |
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169 | REAL, DIMENSION(klon,klev), INTENT(INOUT):: rvc_seri ! cloudy water vapor to total water vapor ratio [-] |
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170 | REAL, DIMENSION(klon,klev), INTENT(IN) :: u_seri ! eastward wind [m/s] |
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171 | REAL, DIMENSION(klon,klev), INTENT(IN) :: v_seri ! northward wind [m/s] |
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172 | REAL, DIMENSION(klon), INTENT(IN) :: cell_area ! area of each cell [m2] |
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173 | |
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174 | ! INPUT/OUTPUT aviation |
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175 | !-------------------------------------------------- |
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176 | REAL, DIMENSION(klon,klev), INTENT(INOUT):: rcont_seri ! ratio of contrails fraction to total cloud fraction [-] |
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177 | REAL, DIMENSION(klon,klev), INTENT(IN) :: flight_dist ! aviation distance flown within the mesh [m/s/mesh] |
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178 | REAL, DIMENSION(klon,klev), INTENT(IN) :: flight_h2o ! aviation H2O emitted within the mesh [kgH2O/s/mesh] |
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179 | |
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180 | ! OUTPUT variables |
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181 | !----------------- |
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182 | |
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183 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: d_t ! temperature increment [K] |
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184 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: d_q ! specific humidity increment [kg/kg] |
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185 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: d_ql ! liquid water increment [kg/kg] |
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186 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: d_qi ! cloud ice mass increment [kg/kg] |
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187 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: rneb ! cloud fraction [-] |
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188 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: rneblsvol ! cloud fraction per unit volume [-] |
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189 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: pfraclr ! precip fraction clear-sky part [-] |
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190 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: pfracld ! precip fraction cloudy part [-] |
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191 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: cldfraliq ! liquid fraction of cloud [-] |
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192 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: sigma2_icefracturb ! Variance of the diagnostic supersaturation distribution (icefrac_turb) [-] |
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193 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: mean_icefracturb ! Mean of the diagnostic supersaturation distribution (icefrac_turb) [-] |
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194 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: radocond ! condensed water used in the radiation scheme [kg/kg] |
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195 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: radicefrac ! ice fraction of condensed water for radiation scheme |
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196 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: rhcl ! clear-sky relative humidity [-] |
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197 | REAL, DIMENSION(klon), INTENT(OUT) :: rain ! surface large-scale rainfall [kg/s/m2] |
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198 | REAL, DIMENSION(klon), INTENT(OUT) :: snow ! surface large-scale snowfall [kg/s/m2] |
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199 | REAL, DIMENSION(klon,klev+1), INTENT(OUT) :: prfl ! large-scale rainfall flux in the column [kg/s/m2] |
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200 | REAL, DIMENSION(klon,klev+1), INTENT(OUT) :: psfl ! large-scale snowfall flux in the column [kg/s/m2] |
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201 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: distcltop ! distance to cloud top [m] |
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202 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: temp_cltop ! temperature of cloud top [K] |
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203 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: beta ! conversion rate of condensed water |
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204 | |
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205 | ! fraction of aerosol scavenging through impaction and nucleation (for on-line) |
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206 | |
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207 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: frac_impa ! scavenging fraction due tu impaction [-] |
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208 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: frac_nucl ! scavenging fraction due tu nucleation [-] |
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209 | |
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210 | ! for condensation and ice supersaturation |
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211 | |
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212 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qsub !--specific total water content in sub-saturated clear sky region [kg/kg] |
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213 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qissr !--specific total water content in supersat region [kg/kg] |
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214 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qcld !--specific total water content in cloudy region [kg/kg] |
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215 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: subfra !--mesh fraction of subsaturated clear sky [-] |
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216 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: issrfra !--mesh fraction of ISSR [-] |
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217 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: gamma_cond !--coefficient governing the ice nucleation RHi threshold [-] |
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218 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dcf_sub !--cloud fraction tendency because of sublimation [s-1] |
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219 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dcf_con !--cloud fraction tendency because of condensation [s-1] |
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220 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dcf_mix !--cloud fraction tendency because of cloud mixing [s-1] |
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221 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqi_adj !--specific ice content tendency because of temperature adjustment [kg/kg/s] |
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222 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqi_sub !--specific ice content tendency because of sublimation [kg/kg/s] |
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223 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqi_con !--specific ice content tendency because of condensation [kg/kg/s] |
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224 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqi_mix !--specific ice content tendency because of cloud mixing [kg/kg/s] |
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225 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqvc_adj !--specific cloud water vapor tendency because of temperature adjustment [kg/kg/s] |
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226 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqvc_sub !--specific cloud water vapor tendency because of sublimation [kg/kg/s] |
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227 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqvc_con !--specific cloud water vapor tendency because of condensation [kg/kg/s] |
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228 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqvc_mix !--specific cloud water vapor tendency because of cloud mixing [kg/kg/s] |
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229 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qsatl !--saturation specific humidity wrt liquid [kg/kg] |
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230 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qsati !--saturation specific humidity wrt ice [kg/kg] |
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231 | |
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232 | ! for contrails and aviation |
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233 | |
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234 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: contfra !--linear contrail fraction [-] |
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235 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: Tcritcont !--critical temperature for contrail formation [K] |
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236 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qcritcont !--critical specific humidity for contrail formation [kg/kg] |
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237 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: potcontfraP !--potential persistent contrail fraction [-] |
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238 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: potcontfraNP !--potential non-persistent contrail fraction [-] |
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239 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dcontfra_cir !--linear contrail fraction to cirrus cloud fraction tendency [s-1] |
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240 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dcf_avi !--cloud fraction tendency because of aviation [s-1] |
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241 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqi_avi !--specific ice content tendency because of aviation [kg/kg/s] |
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242 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqvc_avi !--specific cloud water vapor tendency because of aviation [kg/kg/s] |
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243 | |
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244 | |
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245 | ! for POPRECIP |
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246 | |
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247 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qraindiag !--DIAGNOSTIC specific rain content [kg/kg] |
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248 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qsnowdiag !--DIAGNOSTIC specific snow content [kg/kg] |
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249 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqreva !--rain tendendy due to evaporation [kg/kg/s] |
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250 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqssub !--snow tendency due to sublimation [kg/kg/s] |
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251 | 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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252 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqsagg !--snow tendency due to collection of lcoud ice by aggregation [kg/kg/s] |
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253 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqrauto !--rain tendency due to autoconversion of cloud liquid [kg/kg/s] |
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254 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqsauto !--snow tendency due to autoconversion of cloud ice [kg/kg/s] |
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255 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqsrim !--snow tendency due to riming [kg/kg/s] |
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256 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqsmelt !--snow tendency due to melting [kg/kg/s] |
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257 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqrmelt !--rain tendency due to melting [kg/kg/s] |
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258 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqsfreez !--snow tendency due to freezing [kg/kg/s] |
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259 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqrfreez !--rain tendency due to freezing [kg/kg/s] |
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260 | |
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261 | ! for thermals |
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262 | |
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263 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: cloudth_sth !--mean saturation deficit in thermals |
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264 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: cloudth_senv !--mean saturation deficit in environment |
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265 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: cloudth_sigmath !--std of saturation deficit in thermals |
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266 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: cloudth_sigmaenv !--std of saturation deficit in environment |
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267 | |
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268 | |
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269 | ! LOCAL VARIABLES: |
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270 | !---------------- |
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271 | REAL,DIMENSION(klon) :: qice_ini |
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272 | REAL, DIMENSION(klon,klev) :: ctot |
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273 | REAL, DIMENSION(klon,klev) :: ctot_vol |
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274 | REAL, DIMENSION(klon) :: zqs, zdqs, zqsl, zdqsl, zqsi, zdqsi |
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275 | REAL :: zdelta |
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276 | REAL, DIMENSION(klon) :: zdqsdT_raw |
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277 | REAL, DIMENSION(klon) :: gammasat,dgammasatdt ! coefficient to make cold condensation at the correct RH and derivative wrt T |
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278 | REAL, DIMENSION(klon) :: Tbef,qlbef,DT ! temperature, humidity and temp. variation during lognormal iteration |
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279 | REAL :: num,denom |
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280 | REAL :: cste |
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281 | REAL, DIMENSION(klon) :: zfice_th |
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282 | REAL, DIMENSION(klon) :: qcloud, qincloud_mpc |
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283 | REAL, DIMENSION(klon) :: zrfl, zifl |
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284 | REAL, DIMENSION(klon) :: zoliq, zcond, zq, zqn, zqnl |
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285 | REAL, DIMENSION(klon) :: zoliql, zoliqi |
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286 | REAL, DIMENSION(klon) :: zt |
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287 | REAL, DIMENSION(klon) :: zfice,zneb, znebl |
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288 | REAL, DIMENSION(klon) :: dzfice |
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289 | REAL, DIMENSION(klon) :: zfice_turb, dzfice_turb |
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290 | REAL, DIMENSION(klon) :: qtot, qzero |
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291 | ! Variables precipitation energy conservation |
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292 | REAL, DIMENSION(klon) :: zmqc |
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293 | REAL :: zalpha_tr |
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294 | REAL :: zfrac_lessi |
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295 | REAL, DIMENSION(klon) :: zprec_cond |
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296 | REAL, DIMENSION(klon) :: zlh_solid |
---|
297 | REAL, DIMENSION(klon) :: ztupnew |
---|
298 | REAL, DIMENSION(klon) :: zqvapclr, zqupnew ! for poprecip evap / subl |
---|
299 | REAL, DIMENSION(klon) :: zrflclr, zrflcld |
---|
300 | REAL, DIMENSION(klon) :: ziflclr, ziflcld |
---|
301 | REAL, DIMENSION(klon) :: znebprecip, znebprecipclr, znebprecipcld |
---|
302 | REAL, DIMENSION(klon) :: tot_zneb |
---|
303 | REAL :: qlmpc, qimpc, rnebmpc |
---|
304 | REAL, DIMENSION(klon) :: zdistcltop, ztemp_cltop |
---|
305 | REAL, DIMENSION(klon) :: zqliq, zqice, zqvapcl ! for icefrac_lscp_turb |
---|
306 | |
---|
307 | ! for quantity of condensates seen by radiation |
---|
308 | REAL, DIMENSION(klon) :: zradocond, zradoice |
---|
309 | REAL, DIMENSION(klon) :: zrho_up, zvelo_up |
---|
310 | |
---|
311 | ! for condensation and ice supersaturation |
---|
312 | REAL, DIMENSION(klon) :: qvc, qvcl, shear |
---|
313 | REAL :: delta_z |
---|
314 | ! for contrails |
---|
315 | !--Added for ice supersaturation (ok_ice_supersat) and contrails (ok_plane_contrail) |
---|
316 | ! Constants used for calculating ratios that are advected (using a parent-child |
---|
317 | ! formalism). This is not done in the dynamical core because at this moment, |
---|
318 | ! only isotopes can use this parent-child formalism. Note that the two constants |
---|
319 | ! are the same as the one use in the dynamical core, being also defined in |
---|
320 | ! dyn3d_common/infotrac.F90 |
---|
321 | REAL :: min_qParent, min_ratio |
---|
322 | |
---|
323 | INTEGER i, k, kk, iter |
---|
324 | INTEGER, DIMENSION(klon) :: n_i |
---|
325 | INTEGER ncoreczq |
---|
326 | INTEGER, DIMENSION(klon,klev) :: mpc_bl_points |
---|
327 | LOGICAL iftop |
---|
328 | |
---|
329 | LOGICAL, DIMENSION(klon) :: lognormale |
---|
330 | LOGICAL, DIMENSION(klon) :: keepgoing |
---|
331 | |
---|
332 | CHARACTER (len = 20) :: modname = 'lscp' |
---|
333 | CHARACTER (len = 80) :: abort_message |
---|
334 | |
---|
335 | |
---|
336 | !=============================================================================== |
---|
337 | ! INITIALISATION |
---|
338 | !=============================================================================== |
---|
339 | |
---|
340 | ! Few initial checks |
---|
341 | |
---|
342 | |
---|
343 | IF (iflag_fisrtilp_qsat .LT. 0) THEN |
---|
344 | abort_message = 'lscp cannot be used with iflag_fisrtilp<0' |
---|
345 | CALL abort_physic(modname,abort_message,1) |
---|
346 | ENDIF |
---|
347 | |
---|
348 | ! Few initialisations |
---|
349 | |
---|
350 | ctot_vol(1:klon,1:klev)=0.0 |
---|
351 | rneblsvol(1:klon,1:klev)=0.0 |
---|
352 | znebprecip(:)=0.0 |
---|
353 | znebprecipclr(:)=0.0 |
---|
354 | znebprecipcld(:)=0.0 |
---|
355 | mpc_bl_points(:,:)=0 |
---|
356 | |
---|
357 | IF (prt_level>9) WRITE(lunout,*) 'NUAGES4 A. JAM' |
---|
358 | |
---|
359 | ! AA for 'safety' reasons |
---|
360 | zalpha_tr = 0. |
---|
361 | zfrac_lessi = 0. |
---|
362 | beta(:,:)= 0. |
---|
363 | |
---|
364 | ! Initialisation of variables: |
---|
365 | |
---|
366 | prfl(:,:) = 0.0 |
---|
367 | psfl(:,:) = 0.0 |
---|
368 | d_t(:,:) = 0.0 |
---|
369 | d_q(:,:) = 0.0 |
---|
370 | d_ql(:,:) = 0.0 |
---|
371 | d_qi(:,:) = 0.0 |
---|
372 | rneb(:,:) = 0.0 |
---|
373 | pfraclr(:,:)=0.0 |
---|
374 | pfracld(:,:)=0.0 |
---|
375 | cldfraliq(:,:)=0. |
---|
376 | sigma2_icefracturb(:,:)=0. |
---|
377 | mean_icefracturb(:,:)=0. |
---|
378 | radocond(:,:) = 0.0 |
---|
379 | radicefrac(:,:) = 0.0 |
---|
380 | frac_nucl(:,:) = 1.0 |
---|
381 | frac_impa(:,:) = 1.0 |
---|
382 | rain(:) = 0.0 |
---|
383 | snow(:) = 0.0 |
---|
384 | zfice(:)=1.0 ! initialized at 1 as by default we assume mpc to be at ice saturation |
---|
385 | dzfice(:)=0.0 |
---|
386 | zfice_turb(:)=0.0 |
---|
387 | dzfice_turb(:)=0.0 |
---|
388 | zrfl(:) = 0.0 |
---|
389 | zifl(:) = 0.0 |
---|
390 | zneb(:) = seuil_neb |
---|
391 | zrflclr(:) = 0.0 |
---|
392 | ziflclr(:) = 0.0 |
---|
393 | zrflcld(:) = 0.0 |
---|
394 | ziflcld(:) = 0.0 |
---|
395 | tot_zneb(:) = 0.0 |
---|
396 | qzero(:) = 0.0 |
---|
397 | zdistcltop(:)=0.0 |
---|
398 | ztemp_cltop(:) = 0.0 |
---|
399 | ztupnew(:)=0.0 |
---|
400 | |
---|
401 | distcltop(:,:)=0. |
---|
402 | temp_cltop(:,:)=0. |
---|
403 | |
---|
404 | !--Ice supersaturation |
---|
405 | gamma_cond(:,:) = 1. |
---|
406 | qissr(:,:) = 0. |
---|
407 | issrfra(:,:) = 0. |
---|
408 | dcf_sub(:,:) = 0. |
---|
409 | dcf_con(:,:) = 0. |
---|
410 | dcf_mix(:,:) = 0. |
---|
411 | dqi_adj(:,:) = 0. |
---|
412 | dqi_sub(:,:) = 0. |
---|
413 | dqi_con(:,:) = 0. |
---|
414 | dqi_mix(:,:) = 0. |
---|
415 | dqvc_adj(:,:) = 0. |
---|
416 | dqvc_sub(:,:) = 0. |
---|
417 | dqvc_con(:,:) = 0. |
---|
418 | dqvc_mix(:,:) = 0. |
---|
419 | contfra(:,:) = 0. |
---|
420 | Tcritcont(:,:) = missing_val |
---|
421 | qcritcont(:,:) = missing_val |
---|
422 | potcontfraP(:,:)= 0. |
---|
423 | potcontfraNP(:,:)= 0. |
---|
424 | dcontfra_cir(:,:)= 0. |
---|
425 | dcf_avi(:,:) = 0. |
---|
426 | dqi_avi(:,:) = 0. |
---|
427 | dqvc_avi(:,:) = 0. |
---|
428 | qvc(:) = 0. |
---|
429 | shear(:) = 0. |
---|
430 | min_qParent = 1.e-30 |
---|
431 | min_ratio = 1.e-16 |
---|
432 | |
---|
433 | !-- poprecip |
---|
434 | qraindiag(:,:)= 0. |
---|
435 | qsnowdiag(:,:)= 0. |
---|
436 | dqreva(:,:) = 0. |
---|
437 | dqrauto(:,:) = 0. |
---|
438 | dqrmelt(:,:) = 0. |
---|
439 | dqrfreez(:,:) = 0. |
---|
440 | dqrcol(:,:) = 0. |
---|
441 | dqssub(:,:) = 0. |
---|
442 | dqsauto(:,:) = 0. |
---|
443 | dqsrim(:,:) = 0. |
---|
444 | dqsagg(:,:) = 0. |
---|
445 | dqsfreez(:,:) = 0. |
---|
446 | dqsmelt(:,:) = 0. |
---|
447 | zqupnew(:) = 0. |
---|
448 | zqvapclr(:) = 0. |
---|
449 | |
---|
450 | |
---|
451 | |
---|
452 | !c_iso: variable initialisation for iso |
---|
453 | |
---|
454 | |
---|
455 | !=============================================================================== |
---|
456 | ! BEGINNING OF VERTICAL LOOP FROM TOP TO BOTTOM |
---|
457 | !=============================================================================== |
---|
458 | |
---|
459 | ncoreczq=0 |
---|
460 | |
---|
461 | DO k = klev, 1, -1 |
---|
462 | |
---|
463 | qice_ini = qi_seri(:,k) |
---|
464 | |
---|
465 | IF (k.LE.klev-1) THEN |
---|
466 | iftop=.false. |
---|
467 | ELSE |
---|
468 | iftop=.true. |
---|
469 | ENDIF |
---|
470 | |
---|
471 | ! Initialisation temperature and specific humidity |
---|
472 | ! temp(klon,klev) is not modified by the routine, instead all changes in temperature are made on zt |
---|
473 | ! at the end of the klon loop, a temperature incremtent d_t due to all processes |
---|
474 | ! (thermalization, evap/sub incoming precip, cloud formation, precipitation processes) is calculated |
---|
475 | ! d_t = temperature tendency due to lscp |
---|
476 | ! The temperature of the overlying layer is updated here because needed for thermalization |
---|
477 | DO i = 1, klon |
---|
478 | zt(i)=temp(i,k) |
---|
479 | zq(i)=qt(i,k) |
---|
480 | IF (.not. iftop) THEN |
---|
481 | ztupnew(i) = temp(i,k+1) + d_t(i,k+1) |
---|
482 | zqupnew(i) = qt(i,k+1) + d_q(i,k+1) + d_ql(i,k+1) + d_qi(i,k+1) |
---|
483 | !--zqs(i) is the saturation specific humidity in the layer above |
---|
484 | zqvapclr(i) = MAX(0., qt(i,k+1) + d_q(i,k+1) - rneb(i,k+1) * zqs(i)) |
---|
485 | ENDIF |
---|
486 | !c_iso init of iso |
---|
487 | ENDDO |
---|
488 | |
---|
489 | ! -------------------------------------------------------------------- |
---|
490 | ! P1> Precipitation processes, before cloud formation: |
---|
491 | ! Thermalization of precipitation falling from the overlying layer AND |
---|
492 | ! Precipitation evaporation/sublimation/melting |
---|
493 | !--------------------------------------------------------------------- |
---|
494 | |
---|
495 | !================================================================ |
---|
496 | ! Flag for the new and more microphysical treatment of precipitation from Atelier Nuage (R) |
---|
497 | IF ( ok_poprecip ) THEN |
---|
498 | |
---|
499 | CALL poprecip_precld(klon, dtime, iftop, paprs(:,k), paprs(:,k+1), pplay(:,k), & |
---|
500 | zt, ztupnew, zq, zmqc, znebprecipclr, znebprecipcld, & |
---|
501 | zqvapclr, zqupnew, & |
---|
502 | cf_seri(:,k), rvc_seri(:,k), ql_seri(:,k), qi_seri(:,k), & |
---|
503 | zrfl, zrflclr, zrflcld, & |
---|
504 | zifl, ziflclr, ziflcld, & |
---|
505 | dqreva(:,k), dqssub(:,k) & |
---|
506 | ) |
---|
507 | |
---|
508 | !================================================================ |
---|
509 | ELSE |
---|
510 | |
---|
511 | CALL histprecip_precld(klon, dtime, iftop, paprs(:,k), paprs(:,k+1), pplay(:,k), & |
---|
512 | zt, ztupnew, zq, zmqc, zneb, znebprecip, znebprecipclr, & |
---|
513 | zrfl, zrflclr, zrflcld, & |
---|
514 | zifl, ziflclr, ziflcld, & |
---|
515 | dqreva(:,k), dqssub(:,k) & |
---|
516 | ) |
---|
517 | |
---|
518 | ENDIF ! (ok_poprecip) |
---|
519 | |
---|
520 | ! Calculation of qsat, L/Cp*dqsat/dT and ncoreczq counter |
---|
521 | !------------------------------------------------------- |
---|
522 | |
---|
523 | qtot(:)=zq(:)+zmqc(:) |
---|
524 | CALL calc_qsat_ecmwf(klon,zt,qtot,pplay(:,k),RTT,0,.false.,zqs,zdqs) |
---|
525 | DO i = 1, klon |
---|
526 | zdelta = MAX(0.,SIGN(1.,RTT-zt(i))) |
---|
527 | zdqsdT_raw(i) = zdqs(i)*RCPD*(1.0+RVTMP2*zq(i)) / (RLVTT*(1.-zdelta) + RLSTT*zdelta) |
---|
528 | IF (zq(i) .LT. 1.e-15) THEN |
---|
529 | ncoreczq=ncoreczq+1 |
---|
530 | zq(i)=1.e-15 |
---|
531 | ENDIF |
---|
532 | ! c_iso: do something similar for isotopes |
---|
533 | |
---|
534 | ENDDO |
---|
535 | |
---|
536 | ! -------------------------------------------------------------------- |
---|
537 | ! P2> Cloud formation |
---|
538 | !--------------------------------------------------------------------- |
---|
539 | ! |
---|
540 | ! Unlike fisrtilp, we always assume a 'fractional cloud' approach |
---|
541 | ! i.e. clouds occupy only a fraction of the mesh (the subgrid distribution |
---|
542 | ! is prescribed and depends on large scale variables and boundary layer |
---|
543 | ! properties) |
---|
544 | ! The decrease in condensed part due tu latent heating is taken into |
---|
545 | ! account |
---|
546 | ! ------------------------------------------------------------------- |
---|
547 | |
---|
548 | ! P2.1> With the PDFs (log-normal, bigaussian) |
---|
549 | ! cloud properties calculation with the initial values of t and q |
---|
550 | ! ---------------------------------------------------------------- |
---|
551 | |
---|
552 | ! initialise gammasat and qincloud_mpc |
---|
553 | gammasat(:)=1. |
---|
554 | qincloud_mpc(:)=0. |
---|
555 | |
---|
556 | IF (iflag_cld_th.GE.5) THEN |
---|
557 | ! Cloud cover and content in meshes affected by shallow convection, |
---|
558 | ! are retrieved from a bi-gaussian distribution of the saturation deficit |
---|
559 | ! following Jam et al. 2013 |
---|
560 | |
---|
561 | IF (iflag_cloudth_vert.LE.2) THEN |
---|
562 | ! Old version of Arnaud Jam |
---|
563 | |
---|
564 | CALL cloudth(klon,klev,k,tv, & |
---|
565 | zq,qta,fraca, & |
---|
566 | qcloud,ctot,pspsk,paprs,pplay,tla,thl, & |
---|
567 | ratqs,zqs,temp, & |
---|
568 | cloudth_sth,cloudth_senv,cloudth_sigmath,cloudth_sigmaenv) |
---|
569 | |
---|
570 | |
---|
571 | ELSEIF (iflag_cloudth_vert.GE.3 .AND. iflag_cloudth_vert.LE.5) THEN |
---|
572 | ! Default version of Arnaud Jam |
---|
573 | |
---|
574 | CALL cloudth_v3(klon,klev,k,tv, & |
---|
575 | zq,qta,fraca, & |
---|
576 | qcloud,ctot,ctot_vol,pspsk,paprs,pplay,tla,thl, & |
---|
577 | ratqs,sigma_qtherm,zqs,temp, & |
---|
578 | cloudth_sth,cloudth_senv,cloudth_sigmath,cloudth_sigmaenv) |
---|
579 | |
---|
580 | |
---|
581 | ELSEIF (iflag_cloudth_vert.EQ.6) THEN |
---|
582 | ! Jean Jouhaud's version, with specific separation between surface and volume |
---|
583 | ! cloud fraction Decembre 2018 |
---|
584 | |
---|
585 | CALL cloudth_v6(klon,klev,k,tv, & |
---|
586 | zq,qta,fraca, & |
---|
587 | qcloud,ctot,ctot_vol,pspsk,paprs,pplay,tla,thl, & |
---|
588 | ratqs,zqs,temp, & |
---|
589 | cloudth_sth,cloudth_senv,cloudth_sigmath,cloudth_sigmaenv) |
---|
590 | |
---|
591 | ELSEIF (iflag_cloudth_vert .EQ. 7) THEN |
---|
592 | ! Updated version of Arnaud Jam (correction by E. Vignon) + adapted treatment |
---|
593 | ! for boundary-layer mixed phase clouds |
---|
594 | CALL cloudth_mpc(klon,klev,k,mpc_bl_points,zt,zq,qta(:,k),fraca(:,k), & |
---|
595 | pspsk(:,k),paprs(:,k+1),paprs(:,k),pplay(:,k), tla(:,k), & |
---|
596 | ratqs(:,k),qcloud,qincloud_mpc,zfice_th,ctot(:,k),ctot_vol(:,k), & |
---|
597 | cloudth_sth(:,k),cloudth_senv(:,k),cloudth_sigmath(:,k),cloudth_sigmaenv(:,k)) |
---|
598 | |
---|
599 | ENDIF |
---|
600 | |
---|
601 | |
---|
602 | DO i=1,klon |
---|
603 | rneb(i,k)=ctot(i,k) |
---|
604 | rneblsvol(i,k)=ctot_vol(i,k) |
---|
605 | zqn(i)=qcloud(i) |
---|
606 | !--AB grid-mean vapor in the cloud - we assume saturation adjustment |
---|
607 | qvc(i) = rneb(i,k) * zqs(i) |
---|
608 | ENDDO |
---|
609 | |
---|
610 | ENDIF |
---|
611 | |
---|
612 | IF (iflag_cld_th .LE. 4) THEN |
---|
613 | |
---|
614 | ! lognormal |
---|
615 | lognormale(:) = .TRUE. |
---|
616 | |
---|
617 | ELSEIF (iflag_cld_th .GE. 6) THEN |
---|
618 | |
---|
619 | ! lognormal distribution when no thermals |
---|
620 | lognormale(:) = fraca(:,k) < min_frac_th_cld |
---|
621 | |
---|
622 | ELSE |
---|
623 | ! When iflag_cld_th=5, we always assume |
---|
624 | ! bi-gaussian distribution |
---|
625 | lognormale(:) = .FALSE. |
---|
626 | |
---|
627 | ENDIF |
---|
628 | |
---|
629 | DT(:) = 0. |
---|
630 | n_i(:)=0 |
---|
631 | Tbef(:)=zt(:) |
---|
632 | qlbef(:)=0. |
---|
633 | |
---|
634 | ! Treatment of non-boundary layer clouds (lognormale) |
---|
635 | ! We iterate here to take into account the change in qsat(T) and ice fraction |
---|
636 | ! during the condensation process |
---|
637 | ! the increment in temperature is calculated using the first principle of |
---|
638 | ! thermodynamics (enthalpy conservation equation in a mesh composed of a cloud fraction |
---|
639 | ! and a clear sky fraction) |
---|
640 | ! note that we assume that the vapor in the cloud is at saturation for this calculation |
---|
641 | |
---|
642 | DO iter=1,iflag_fisrtilp_qsat+1 |
---|
643 | |
---|
644 | keepgoing(:) = .FALSE. |
---|
645 | |
---|
646 | DO i=1,klon |
---|
647 | |
---|
648 | ! keepgoing = .true. while convergence is not satisfied |
---|
649 | |
---|
650 | IF (((ABS(DT(i)).GT.DDT0) .OR. (n_i(i) .EQ. 0)) .AND. lognormale(i)) THEN |
---|
651 | |
---|
652 | ! if not convergence: |
---|
653 | ! we calculate a new iteration |
---|
654 | keepgoing(i) = .TRUE. |
---|
655 | |
---|
656 | ! P2.2.1> cloud fraction and condensed water mass calculation |
---|
657 | ! Calculated variables: |
---|
658 | ! rneb : cloud fraction |
---|
659 | ! zqn : total water within the cloud |
---|
660 | ! zcond: mean condensed water within the mesh |
---|
661 | ! rhcl: clear-sky relative humidity |
---|
662 | !--------------------------------------------------------------- |
---|
663 | |
---|
664 | ! new temperature that only serves in the iteration process: |
---|
665 | Tbef(i)=Tbef(i)+DT(i) |
---|
666 | |
---|
667 | ! Rneb, qzn and zcond for lognormal PDFs |
---|
668 | qtot(i)=zq(i)+zmqc(i) |
---|
669 | |
---|
670 | ENDIF |
---|
671 | |
---|
672 | ENDDO |
---|
673 | |
---|
674 | ! Calculation of saturation specific humidity and ice fraction |
---|
675 | CALL calc_qsat_ecmwf(klon,Tbef,qtot,pplay(:,k),RTT,0,.false.,zqs,zdqs) |
---|
676 | |
---|
677 | IF (iflag_icefrac .GE. 3) THEN |
---|
678 | ! consider a ice weighted qs to ensure that liquid clouds at T<0 have a consistent cloud fraction |
---|
679 | ! and cloud condensed water content. idea following Dietlitcher et al. 2018, GMD |
---|
680 | ! we make this option works only for the physically-based and tke-depdenent param (iflag_icefrac>=1) |
---|
681 | DO i=1,klon |
---|
682 | CALL calc_qsat_ecmwf(klon,Tbef,qtot,pplay(:,k),RTT,1,.false.,zqsl,zdqsl) |
---|
683 | CALL calc_qsat_ecmwf(klon,Tbef,qtot,pplay(:,k),RTT,2,.false.,zqsi,zdqsi) |
---|
684 | zqs(i)=zfice(i)*zqsi(i)+(1.-zfice(i))*zqsl(i) |
---|
685 | zdqs(i)=zfice(i)*zdqsi(i)+zqsi(i)*dzfice(i)+(1.-zfice(i))*zdqsl(i)-zqsl(i)*dzfice(i) |
---|
686 | ENDDO |
---|
687 | ENDIF |
---|
688 | |
---|
689 | CALL calc_gammasat(klon,Tbef,qtot,pplay(:,k),gammasat,dgammasatdt) |
---|
690 | ! saturation may occur at a humidity different from qsat (gamma qsat), so gamma correction for dqs |
---|
691 | zdqs(:) = gammasat(:)*zdqs(:)+zqs(:)*dgammasatdt(:) |
---|
692 | |
---|
693 | ! Cloud condensation based on subgrid pdf |
---|
694 | !--AB Activates a condensation scheme that allows for |
---|
695 | !--ice supersaturation and contrails evolution from aviation |
---|
696 | IF (ok_ice_supersat) THEN |
---|
697 | |
---|
698 | !--Calculate the shear value (input for condensation and ice supersat) |
---|
699 | DO i = 1, klon |
---|
700 | !--Cell thickness [m] |
---|
701 | delta_z = ( paprs(i,k) - paprs(i,k+1) ) / RG / pplay(i,k) * Tbef(i) * RD |
---|
702 | IF ( iftop ) THEN |
---|
703 | ! top |
---|
704 | shear(i) = SQRT( ( (u_seri(i,k) - u_seri(i,k-1)) / delta_z )**2. & |
---|
705 | + ( (v_seri(i,k) - v_seri(i,k-1)) / delta_z )**2. ) |
---|
706 | ELSEIF ( k .EQ. 1 ) THEN |
---|
707 | ! surface |
---|
708 | shear(i) = SQRT( ( (u_seri(i,k+1) - u_seri(i,k)) / delta_z )**2. & |
---|
709 | + ( (v_seri(i,k+1) - v_seri(i,k)) / delta_z )**2. ) |
---|
710 | ELSE |
---|
711 | ! other layers |
---|
712 | shear(i) = SQRT( ( ( (u_seri(i,k+1) + u_seri(i,k)) / 2. & |
---|
713 | - (u_seri(i,k) + u_seri(i,k-1)) / 2. ) / delta_z )**2. & |
---|
714 | + ( ( (v_seri(i,k+1) + v_seri(i,k)) / 2. & |
---|
715 | - (v_seri(i,k) + v_seri(i,k-1)) / 2. ) / delta_z )**2. ) |
---|
716 | ENDIF |
---|
717 | ENDDO |
---|
718 | |
---|
719 | !--------------------------------------------- |
---|
720 | !-- CONDENSATION AND ICE SUPERSATURATION -- |
---|
721 | !--------------------------------------------- |
---|
722 | |
---|
723 | CALL condensation_ice_supersat( & |
---|
724 | klon, dtime, missing_val, & |
---|
725 | pplay(:,k), paprs(:,k), paprs(:,k+1), & |
---|
726 | cf_seri(:,k), rvc_seri(:,k), ql_seri(:,k), qi_seri(:,k), & |
---|
727 | shear, tke_dissip(:,k), cell_area, & |
---|
728 | Tbef, zq, zqs, gammasat, ratqs(:,k), keepgoing, & |
---|
729 | rneb(:,k), zqn, qvc, issrfra(:,k), qissr(:,k), & |
---|
730 | dcf_sub(:,k), dcf_con(:,k), dcf_mix(:,k), & |
---|
731 | dqi_adj(:,k), dqi_sub(:,k), dqi_con(:,k), dqi_mix(:,k), & |
---|
732 | dqvc_adj(:,k), dqvc_sub(:,k), dqvc_con(:,k), dqvc_mix(:,k), & |
---|
733 | rcont_seri(:,k), flight_dist(:,k), flight_h2o(:,k), contfra(:,k), & |
---|
734 | Tcritcont(:,k), qcritcont(:,k), potcontfraP(:,k), potcontfraNP(:,k), & |
---|
735 | dcontfra_cir(:,k), dcf_avi(:,k), dqi_avi(:,k), dqvc_avi(:,k)) |
---|
736 | |
---|
737 | |
---|
738 | ELSE |
---|
739 | !--generalised lognormal condensation scheme (Bony and Emanuel 2001) |
---|
740 | |
---|
741 | CALL condensation_lognormal( & |
---|
742 | klon, Tbef, zq, zqs, gammasat, ratqs(:,k), & |
---|
743 | keepgoing, rneb(:,k), zqn, qvc) |
---|
744 | |
---|
745 | |
---|
746 | ENDIF ! .NOT. ok_ice_supersat |
---|
747 | |
---|
748 | ! cloud phase determination |
---|
749 | IF (iflag_icefrac .GE. 2) THEN |
---|
750 | ! phase partitioning depending on temperature. activates here in the iteration process if iflag_icefrac > 2 |
---|
751 | CALL icefrac_lscp_turb(klon, dtime, Tbef, pplay(:,k), paprs(:,k), paprs(:,k+1), omega(:,k), qice_ini, ziflcld, zqn, & |
---|
752 | rneb(:,k), tke(:,k), tke_dissip(:,k), zqliq, zqvapcl, zqice, zfice, dzfice, cldfraliq(:,k),sigma2_icefracturb(:,k), mean_icefracturb(:,k)) |
---|
753 | ELSE |
---|
754 | ! phase partitioning depending on temperature and eventually distance to cloud top |
---|
755 | IF (iflag_t_glace.GE.4) THEN |
---|
756 | ! For iflag_t_glace GE 4 the phase partition function dependends on temperature AND distance to cloud top |
---|
757 | CALL distance_to_cloud_top(klon,klev,k,temp,pplay,paprs,rneb,zdistcltop,ztemp_cltop) |
---|
758 | ENDIF |
---|
759 | CALL icefrac_lscp(klon, zt, iflag_ice_thermo, zdistcltop,ztemp_cltop,zfice,dzfice) |
---|
760 | ENDIF |
---|
761 | |
---|
762 | |
---|
763 | DO i=1,klon |
---|
764 | IF (keepgoing(i)) THEN |
---|
765 | |
---|
766 | ! If vertical heterogeneity, change fraction by volume as well |
---|
767 | IF (iflag_cloudth_vert.GE.3) THEN |
---|
768 | ctot_vol(i,k)=rneb(i,k) |
---|
769 | rneblsvol(i,k)=ctot_vol(i,k) |
---|
770 | ENDIF |
---|
771 | |
---|
772 | |
---|
773 | ! P2.2.2> Approximative calculation of temperature variation DT |
---|
774 | ! due to condensation. |
---|
775 | ! Calculated variables: |
---|
776 | ! dT : temperature change due to condensation |
---|
777 | !--------------------------------------------------------------- |
---|
778 | |
---|
779 | |
---|
780 | IF (zfice(i).LT.1) THEN |
---|
781 | cste=RLVTT |
---|
782 | ELSE |
---|
783 | cste=RLSTT |
---|
784 | ENDIF |
---|
785 | |
---|
786 | IF ( ok_unadjusted_clouds ) THEN |
---|
787 | !--AB We relax the saturation adjustment assumption |
---|
788 | !-- qvc (grid-mean vapor in cloud) is calculated by the condensation scheme |
---|
789 | IF ( rneb(i,k) .GT. eps ) THEN |
---|
790 | qlbef(i) = MAX(0., zqn(i) - qvc(i) / rneb(i,k)) |
---|
791 | ELSE |
---|
792 | qlbef(i) = 0. |
---|
793 | ENDIF |
---|
794 | ELSE |
---|
795 | qlbef(i)=max(0.,zqn(i)-zqs(i)) |
---|
796 | ENDIF |
---|
797 | |
---|
798 | num = -Tbef(i)+zt(i)+rneb(i,k)*((1-zfice(i))*RLVTT & |
---|
799 | +zfice(i)*RLSTT)/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i)))*qlbef(i) |
---|
800 | denom = 1.+rneb(i,k)*((1-zfice(i))*RLVTT+zfice(i)*RLSTT)/cste*zdqs(i) & |
---|
801 | -(RLSTT-RLVTT)/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i)))*rneb(i,k) & |
---|
802 | *qlbef(i)*dzfice(i) |
---|
803 | ! here we update a provisory temperature variable that only serves in the iteration |
---|
804 | ! process |
---|
805 | DT(i)=num/denom |
---|
806 | n_i(i)=n_i(i)+1 |
---|
807 | |
---|
808 | ENDIF ! end keepgoing |
---|
809 | |
---|
810 | ENDDO ! end loop on i |
---|
811 | |
---|
812 | ENDDO ! iter=1,iflag_fisrtilp_qsat+1 |
---|
813 | |
---|
814 | ! P2.2> Final quantities calculation |
---|
815 | ! Calculated variables: |
---|
816 | ! rneb : cloud fraction |
---|
817 | ! zcond: mean condensed water in the mesh |
---|
818 | ! zqn : mean water vapor in the mesh |
---|
819 | ! zfice: ice fraction in clouds |
---|
820 | ! zt : temperature |
---|
821 | ! rhcl : clear-sky relative humidity |
---|
822 | ! ---------------------------------------------------------------- |
---|
823 | |
---|
824 | |
---|
825 | ! Cloud phase final determination |
---|
826 | !-------------------------------- |
---|
827 | ! For iflag_t_glace GE 4 the phase partition function dependends on temperature AND distance to cloud top |
---|
828 | IF (iflag_t_glace.GE.4) THEN |
---|
829 | CALL distance_to_cloud_top(klon,klev,k,temp,pplay,paprs,rneb,zdistcltop,ztemp_cltop) |
---|
830 | distcltop(:,k)=zdistcltop(:) |
---|
831 | temp_cltop(:,k)=ztemp_cltop(:) |
---|
832 | ENDIF |
---|
833 | ! Partition function depending on temperature for all clouds (shallow convective and stratiform) |
---|
834 | CALL icefrac_lscp(klon, zt, iflag_ice_thermo, zdistcltop, ztemp_cltop, zfice, dzfice) |
---|
835 | |
---|
836 | ! Partition function depending on tke for non shallow-convective clouds, erase previous estimation |
---|
837 | IF (iflag_icefrac .GE. 1) THEN |
---|
838 | CALL icefrac_lscp_turb(klon, dtime, Tbef, pplay(:,k), paprs(:,k), paprs(:,k+1), omega(:,k), qice_ini, ziflcld, zqn, & |
---|
839 | rneb(:,k), tke(:,k), tke_dissip(:,k), zqliq, zqvapcl, zqice, zfice_turb, dzfice_turb, cldfraliq(:,k),sigma2_icefracturb(:,k), mean_icefracturb(:,k)) |
---|
840 | ENDIF |
---|
841 | |
---|
842 | ! Water vapor update, subsequent latent heat exchange for each cloud type |
---|
843 | !------------------------------------------------------------------------ |
---|
844 | DO i=1, klon |
---|
845 | ! Overwrite phase partitioning in boundary layer mixed phase clouds when the |
---|
846 | ! iflag_cloudth_vert=7 and specific param is activated |
---|
847 | IF (mpc_bl_points(i,k) .GT. 0) THEN |
---|
848 | zcond(i) = MAX(0.0,qincloud_mpc(i))*rneb(i,k) |
---|
849 | ! following line is very strange and probably wrong |
---|
850 | rhcl(i,k)= (zqs(i)+zq(i))/2./zqs(i) |
---|
851 | ! water vapor update and partition function if thermals |
---|
852 | zq(i) = zq(i) - zcond(i) |
---|
853 | zfice(i)=zfice_th(i) |
---|
854 | ELSE |
---|
855 | ! Checks on rneb, rhcl and zqn |
---|
856 | IF (rneb(i,k) .LE. 0.0) THEN |
---|
857 | zqn(i) = 0.0 |
---|
858 | rneb(i,k) = 0.0 |
---|
859 | zcond(i) = 0.0 |
---|
860 | rhcl(i,k)=zq(i)/zqs(i) |
---|
861 | ELSE IF (rneb(i,k) .GE. 1.0) THEN |
---|
862 | zqn(i) = zq(i) |
---|
863 | rneb(i,k) = 1.0 |
---|
864 | IF ( ok_unadjusted_clouds ) THEN |
---|
865 | !--AB We relax the saturation adjustment assumption |
---|
866 | !-- qvc (grid-mean vapor in cloud) is calculated by the condensation scheme |
---|
867 | zcond(i) = MAX(0., zqn(i) - qvc(i)) |
---|
868 | ELSE |
---|
869 | zcond(i) = MAX(0.0,zqn(i)-zqs(i)) |
---|
870 | ENDIF |
---|
871 | rhcl(i,k)=1.0 |
---|
872 | ELSE |
---|
873 | IF ( ok_unadjusted_clouds ) THEN |
---|
874 | !--AB We relax the saturation adjustment assumption |
---|
875 | !-- qvc (grid-mean vapor in cloud) is calculated by the condensation scheme |
---|
876 | zcond(i) = MAX(0., zqn(i) * rneb(i,k) - qvc(i)) |
---|
877 | ELSE |
---|
878 | zcond(i) = MAX(0.0,zqn(i)-zqs(i))*rneb(i,k) |
---|
879 | ENDIF |
---|
880 | ! following line is very strange and probably wrong: |
---|
881 | rhcl(i,k)=(zqs(i)+zq(i))/2./zqs(i) |
---|
882 | ! Overwrite partitioning for non shallow-convective clouds if iflag_icefrac>1 (icefrac turb param) |
---|
883 | IF (iflag_icefrac .GE. 1) THEN |
---|
884 | IF (lognormale(i)) THEN |
---|
885 | zcond(i) = zqliq(i) + zqice(i) |
---|
886 | zfice(i) = zfice_turb(i) |
---|
887 | rhcl(i,k) = zqvapcl(i) * rneb(i,k) + (zq(i) - zqn(i)) * (1.-rneb(i,k)) |
---|
888 | ENDIF |
---|
889 | ENDIF |
---|
890 | ENDIF |
---|
891 | |
---|
892 | ! water vapor update |
---|
893 | zq(i) = zq(i) - zcond(i) |
---|
894 | |
---|
895 | ENDIF |
---|
896 | |
---|
897 | |
---|
898 | ! temperature update due to phase change |
---|
899 | zt(i) = zt(i) + (1.-zfice(i))*zcond(i) & |
---|
900 | & * RLVTT/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i)+zcond(i))) & |
---|
901 | +zfice(i)*zcond(i) * RLSTT/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i)+zcond(i))) |
---|
902 | ENDDO |
---|
903 | |
---|
904 | ! If vertical heterogeneity, change volume fraction |
---|
905 | IF (iflag_cloudth_vert .GE. 3) THEN |
---|
906 | ctot_vol(1:klon,k)=min(max(ctot_vol(1:klon,k),0.),1.) |
---|
907 | rneblsvol(1:klon,k)=ctot_vol(1:klon,k) |
---|
908 | ENDIF |
---|
909 | |
---|
910 | |
---|
911 | ! ---------------------------------------------------------------- |
---|
912 | ! P3> Precipitation processes, after cloud formation |
---|
913 | ! - precipitation formation, melting/freezing |
---|
914 | ! ---------------------------------------------------------------- |
---|
915 | |
---|
916 | ! Initiate the quantity of liquid and solid condensates |
---|
917 | ! Note that in the following, zcond is the total amount of condensates |
---|
918 | ! including newly formed precipitations (i.e., condensates formed by the |
---|
919 | ! condensation process), while zoliq is the total amount of condensates in |
---|
920 | ! the cloud (i.e., on which precipitation processes have applied) |
---|
921 | DO i = 1, klon |
---|
922 | zoliq(i) = zcond(i) |
---|
923 | zoliql(i) = zcond(i) * ( 1. - zfice(i) ) |
---|
924 | zoliqi(i) = zcond(i) * zfice(i) |
---|
925 | ENDDO |
---|
926 | |
---|
927 | !================================================================ |
---|
928 | ! Flag for the new and more microphysical treatment of precipitation from Atelier Nuage (R) |
---|
929 | IF (ok_poprecip) THEN |
---|
930 | |
---|
931 | CALL poprecip_postcld(klon, dtime, paprs(:,k), paprs(:,k+1), pplay(:,k), & |
---|
932 | ctot_vol(:,k), ptconv(:,k), & |
---|
933 | zt, zq, zoliql, zoliqi, zfice, & |
---|
934 | rneb(:,k), znebprecipclr, znebprecipcld, & |
---|
935 | zrfl, zrflclr, zrflcld, & |
---|
936 | zifl, ziflclr, ziflcld, & |
---|
937 | qraindiag(:,k), qsnowdiag(:,k), dqrauto(:,k), & |
---|
938 | dqrcol(:,k), dqrmelt(:,k), dqrfreez(:,k), & |
---|
939 | dqsauto(:,k), dqsagg(:,k), dqsrim(:,k), & |
---|
940 | dqsmelt(:,k), dqsfreez(:,k) & |
---|
941 | ) |
---|
942 | DO i = 1, klon |
---|
943 | zoliq(i) = zoliql(i) + zoliqi(i) |
---|
944 | ENDDO |
---|
945 | |
---|
946 | !================================================================ |
---|
947 | ELSE |
---|
948 | |
---|
949 | CALL histprecip_postcld(klon, dtime, iftop, paprs(:,k), paprs(:,k+1), pplay(:,k), & |
---|
950 | ctot_vol(:,k), ptconv(:,k), zdqsdT_raw, & |
---|
951 | zt, zq, zoliq, zoliql, zoliqi, zcond, zfice, zmqc, & |
---|
952 | rneb(:,k), znebprecipclr, znebprecipcld, & |
---|
953 | zneb, tot_zneb, zrho_up, zvelo_up, & |
---|
954 | zrfl, zrflclr, zrflcld, zifl, ziflclr, ziflcld, & |
---|
955 | zradocond, zradoice, dqrauto(:,k), dqsauto(:,k) & |
---|
956 | ) |
---|
957 | |
---|
958 | ENDIF ! ok_poprecip |
---|
959 | |
---|
960 | ! End of precipitation processes after cloud formation |
---|
961 | ! ---------------------------------------------------- |
---|
962 | |
---|
963 | !---------------------------------------------------------------------- |
---|
964 | ! P4> Calculation of cloud condensates amount seen by radiative scheme |
---|
965 | !---------------------------------------------------------------------- |
---|
966 | |
---|
967 | DO i=1,klon |
---|
968 | |
---|
969 | IF (ok_poprecip) THEN |
---|
970 | IF (ok_radocond_snow) THEN |
---|
971 | radocond(i,k) = zoliq(i) |
---|
972 | zradoice(i) = zoliqi(i) + qsnowdiag(i,k) |
---|
973 | ELSE |
---|
974 | radocond(i,k) = zoliq(i) |
---|
975 | zradoice(i) = zoliqi(i) |
---|
976 | ENDIF |
---|
977 | ELSE |
---|
978 | radocond(i,k) = zradocond(i) |
---|
979 | ENDIF |
---|
980 | |
---|
981 | ! calculate the percentage of ice in "radocond" so cloud+precip seen |
---|
982 | ! by the radiation scheme |
---|
983 | IF (radocond(i,k) .GT. 0.) THEN |
---|
984 | radicefrac(i,k)=MIN(MAX(zradoice(i)/radocond(i,k),0.),1.) |
---|
985 | ENDIF |
---|
986 | ENDDO |
---|
987 | |
---|
988 | ! ---------------------------------------------------------------- |
---|
989 | ! P5> Wet scavenging |
---|
990 | ! ---------------------------------------------------------------- |
---|
991 | |
---|
992 | !Scavenging through nucleation in the layer |
---|
993 | |
---|
994 | DO i = 1,klon |
---|
995 | |
---|
996 | IF(zcond(i).GT.zoliq(i)+1.e-10) THEN |
---|
997 | beta(i,k) = (zcond(i)-zoliq(i))/zcond(i)/dtime |
---|
998 | ELSE |
---|
999 | beta(i,k) = 0. |
---|
1000 | ENDIF |
---|
1001 | |
---|
1002 | zprec_cond(i) = MAX(zcond(i)-zoliq(i),0.0)*(paprs(i,k)-paprs(i,k+1))/RG |
---|
1003 | |
---|
1004 | IF (rneb(i,k).GT.0.0.AND.zprec_cond(i).GT.0.) THEN |
---|
1005 | |
---|
1006 | IF (temp(i,k) .GE. t_glace_min) THEN |
---|
1007 | zalpha_tr = a_tr_sca(3) |
---|
1008 | ELSE |
---|
1009 | zalpha_tr = a_tr_sca(4) |
---|
1010 | ENDIF |
---|
1011 | |
---|
1012 | zfrac_lessi = 1. - EXP(zalpha_tr*zprec_cond(i)/MAX(rneb(i,k),seuil_neb)) |
---|
1013 | frac_nucl(i,k)= 1.-MAX(rneb(i,k),seuil_neb)*zfrac_lessi |
---|
1014 | |
---|
1015 | ! Nucleation with a factor of -1 instead of -0.5 |
---|
1016 | zfrac_lessi = 1. - EXP(-zprec_cond(i)/MAX(rneb(i,k),seuil_neb)) |
---|
1017 | |
---|
1018 | ENDIF |
---|
1019 | |
---|
1020 | ENDDO |
---|
1021 | |
---|
1022 | ! Scavenging through impaction in the underlying layer |
---|
1023 | |
---|
1024 | DO kk = k-1, 1, -1 |
---|
1025 | |
---|
1026 | DO i = 1, klon |
---|
1027 | |
---|
1028 | IF (rneb(i,k).GT.0.0.AND.zprec_cond(i).GT.0.) THEN |
---|
1029 | |
---|
1030 | IF (temp(i,kk) .GE. t_glace_min) THEN |
---|
1031 | zalpha_tr = a_tr_sca(1) |
---|
1032 | ELSE |
---|
1033 | zalpha_tr = a_tr_sca(2) |
---|
1034 | ENDIF |
---|
1035 | |
---|
1036 | zfrac_lessi = 1. - EXP(zalpha_tr*zprec_cond(i)/MAX(rneb(i,k),seuil_neb)) |
---|
1037 | frac_impa(i,kk)= 1.-MAX(rneb(i,k),seuil_neb)*zfrac_lessi |
---|
1038 | |
---|
1039 | ENDIF |
---|
1040 | |
---|
1041 | ENDDO |
---|
1042 | |
---|
1043 | ENDDO |
---|
1044 | |
---|
1045 | !------------------------------------------------------------ |
---|
1046 | ! P6 > write diagnostics and outputs |
---|
1047 | !------------------------------------------------------------ |
---|
1048 | |
---|
1049 | !--AB Write diagnostics and tracers for ice supersaturation |
---|
1050 | IF ( ok_ice_supersat ) THEN |
---|
1051 | CALL calc_qsat_ecmwf(klon,zt,qzero,pplay(:,k),RTT,1,.false.,qsatl(:,k),zdqs) |
---|
1052 | CALL calc_qsat_ecmwf(klon,zt,qzero,pplay(:,k),RTT,2,.false.,qsati(:,k),zdqs) |
---|
1053 | |
---|
1054 | DO i = 1, klon |
---|
1055 | |
---|
1056 | IF ( zoliq(i) .LE. 0. ) THEN |
---|
1057 | !--If everything was precipitated, the remaining empty cloud is dissipated |
---|
1058 | !--and everything is transfered to the subsaturated clear sky region |
---|
1059 | rneb(i,k) = 0. |
---|
1060 | qvc(i) = 0. |
---|
1061 | ENDIF |
---|
1062 | |
---|
1063 | cf_seri(i,k) = rneb(i,k) |
---|
1064 | |
---|
1065 | IF ( .NOT. ok_unadjusted_clouds ) THEN |
---|
1066 | qvc(i) = zqs(i) * rneb(i,k) |
---|
1067 | ENDIF |
---|
1068 | IF ( zq(i) .GT. min_qParent ) THEN |
---|
1069 | rvc_seri(i,k) = qvc(i) / zq(i) |
---|
1070 | ELSE |
---|
1071 | rvc_seri(i,k) = min_ratio |
---|
1072 | ENDIF |
---|
1073 | !--The MIN barrier is NEEDED because of: |
---|
1074 | !-- 1) very rare pathological cases of the lsc scheme (rvc = 1. + 1e-16 sometimes) |
---|
1075 | !-- 2) the thermal scheme does NOT guarantee that qvc <= qvap (or even qincld <= qtot) |
---|
1076 | !--The MAX barrier is a safeguard that should not be activated |
---|
1077 | rvc_seri(i,k) = MIN(MAX(rvc_seri(i,k), 0.), 1.) |
---|
1078 | IF ( ok_plane_contrail ) THEN |
---|
1079 | IF ( rneb(i,k) .GT. min_qParent ) THEN |
---|
1080 | rcont_seri(i,k) = contfra(i,k) / rneb(i,k) |
---|
1081 | ELSE |
---|
1082 | rcont_seri(i,k) = min_ratio |
---|
1083 | ENDIF |
---|
1084 | !--This barrier should never be activated |
---|
1085 | rcont_seri(i,k) = MIN(MAX(rcont_seri(i,k), 0.), 1.) |
---|
1086 | ENDIF |
---|
1087 | |
---|
1088 | !--Diagnostics |
---|
1089 | gamma_cond(i,k) = gammasat(i) |
---|
1090 | subfra(i,k) = 1. - cf_seri(i,k) - issrfra(i,k) |
---|
1091 | qsub(i,k) = zq(i) - qvc(i) - qissr(i,k) |
---|
1092 | qcld(i,k) = qvc(i) + zoliq(i) |
---|
1093 | ENDDO |
---|
1094 | ENDIF |
---|
1095 | |
---|
1096 | ! Outputs: |
---|
1097 | !------------------------------- |
---|
1098 | ! Precipitation fluxes at layer interfaces |
---|
1099 | ! + precipitation fractions + |
---|
1100 | ! temperature and water species tendencies |
---|
1101 | DO i = 1, klon |
---|
1102 | psfl(i,k)=zifl(i) |
---|
1103 | prfl(i,k)=zrfl(i) |
---|
1104 | pfraclr(i,k)=znebprecipclr(i) |
---|
1105 | pfracld(i,k)=znebprecipcld(i) |
---|
1106 | d_q(i,k) = zq(i) - qt(i,k) |
---|
1107 | d_t(i,k) = zt(i) - temp(i,k) |
---|
1108 | |
---|
1109 | IF (ok_bug_phase_lscp) THEN |
---|
1110 | d_ql(i,k) = (1-zfice(i))*zoliq(i) |
---|
1111 | d_qi(i,k) = zfice(i)*zoliq(i) |
---|
1112 | ELSE |
---|
1113 | d_ql(i,k) = zoliql(i) |
---|
1114 | d_qi(i,k) = zoliqi(i) |
---|
1115 | ENDIF |
---|
1116 | |
---|
1117 | ENDDO |
---|
1118 | |
---|
1119 | |
---|
1120 | ENDDO ! loop on k from top to bottom |
---|
1121 | |
---|
1122 | |
---|
1123 | ! Rain or snow at the surface (depending on the first layer temperature) |
---|
1124 | DO i = 1, klon |
---|
1125 | snow(i) = zifl(i) |
---|
1126 | rain(i) = zrfl(i) |
---|
1127 | ! c_iso final output |
---|
1128 | ENDDO |
---|
1129 | |
---|
1130 | IF (ncoreczq>0) THEN |
---|
1131 | WRITE(lunout,*)'WARNING : ZQ in LSCP ',ncoreczq,' val < 1.e-15.' |
---|
1132 | ENDIF |
---|
1133 | |
---|
1134 | |
---|
1135 | RETURN |
---|
1136 | |
---|
1137 | END SUBROUTINE lscp |
---|
1138 | !+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
---|
1139 | |
---|
1140 | END MODULE lmdz_lscp |
---|