[4664] | 1 | MODULE lmdz_lscp |
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[3999] | 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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[4380] | 8 | SUBROUTINE lscp(klon,klev,dtime,missing_val, & |
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[4686] | 9 | paprs,pplay,temp,qt,ptconv,ratqs, & |
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[4380] | 10 | d_t, d_q, d_ql, d_qi, rneb, rneblsvol, rneb_seri, & |
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[4530] | 11 | pfraclr,pfracld, & |
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| 12 | radocond, radicefrac, rain, snow, & |
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[3999] | 13 | frac_impa, frac_nucl, beta, & |
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| 14 | prfl, psfl, rhcl, zqta, fraca, & |
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| 15 | ztv, zpspsk, ztla, zthl, iflag_cld_th, & |
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[4380] | 16 | iflag_ice_thermo, ok_ice_sursat, qsatl, qsats, & |
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[4639] | 17 | distcltop,temp_cltop, & |
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[4380] | 18 | qclr, qcld, qss, qvc, rnebclr, rnebss, gamma_ss, & |
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[4651] | 19 | Tcontr, qcontr, qcontr2, fcontrN, fcontrP, & |
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[4803] | 20 | cloudth_sth,cloudth_senv,cloudth_sigmath,cloudth_sigmaenv, & |
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| 21 | dqreva,dqssub,dqrauto,dqrcol,dqrmelt,dqrfreez,dqsauto, & |
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| 22 | dqsagg,dqsrim,dqsmelt,dqsfreez) |
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[3999] | 23 | |
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| 24 | !++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
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| 25 | ! Authors: Z.X. Li (LMD), J-L Dufresne (LMD), C. Rio (LMD), J-Y Grandpeix (LMD) |
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| 26 | ! A. JAM (LMD), J-B Madeleine (LMD), E. Vignon (LMD), L. Touzze-Peiffert (LMD) |
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| 27 | !-------------------------------------------------------------------------------- |
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| 28 | ! Date: 01/2021 |
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| 29 | !-------------------------------------------------------------------------------- |
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| 30 | ! Aim: Large Scale Clouds and Precipitation (LSCP) |
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[4226] | 31 | ! |
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[3999] | 32 | ! This code is a new version of the fisrtilp.F90 routine, which is itself a |
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[4072] | 33 | ! merge of 'first' (superrsaturation physics, P. LeVan K. Laval) |
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[3999] | 34 | ! and 'ilp' (il pleut, L. Li) |
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| 35 | ! |
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[4380] | 36 | ! Compared to the original fisrtilp code, lscp |
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[3999] | 37 | ! -> assumes thermcep = .TRUE. all the time (fisrtilp inconsistent when .FALSE.) |
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| 38 | ! -> consider always precipitation thermalisation (fl_cor_ebil>0) |
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| 39 | ! -> option iflag_fisrtilp_qsat<0 no longer possible (qsat does not evolve with T) |
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| 40 | ! -> option "oldbug" by JYG has been removed |
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| 41 | ! -> iflag_t_glace >0 always |
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| 42 | ! -> the 'all or nothing' cloud approach is no longer available (cpartiel=T always) |
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| 43 | ! -> rectangular distribution from L. Li no longer available |
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| 44 | ! -> We always account for the Wegener-Findeisen-Bergeron process (iflag_bergeron = 2 in fisrt) |
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| 45 | !-------------------------------------------------------------------------------- |
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| 46 | ! References: |
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| 47 | ! |
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[4412] | 48 | ! - Bony, S., & Emanuel, K. A. 2001, JAS, doi: 10.1175/1520-0469(2001)058<3158:APOTCA>2.0.CO;2 |
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[3999] | 49 | ! - Hourdin et al. 2013, Clim Dyn, doi:10.1007/s00382-012-1343-y |
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| 50 | ! - Jam et al. 2013, Boundary-Layer Meteorol, doi:10.1007/s10546-012-9789-3 |
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[4412] | 51 | ! - Jouhaud, et al. 2018. JAMES, doi:10.1029/2018MS001379 |
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[3999] | 52 | ! - Madeleine et al. 2020, JAMES, doi:10.1029/2020MS002046 |
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[4412] | 53 | ! - Touzze-Peifert Ludo, PhD thesis, p117-124 |
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[3999] | 54 | ! ------------------------------------------------------------------------------- |
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| 55 | ! Code structure: |
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| 56 | ! |
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[4226] | 57 | ! P0> Thermalization of the precipitation coming from the overlying layer |
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[3999] | 58 | ! P1> Evaporation of the precipitation (falling from the k+1 level) |
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| 59 | ! P2> Cloud formation (at the k level) |
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[4412] | 60 | ! P2.A.1> With the PDFs, calculation of cloud properties using the inital |
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[3999] | 61 | ! values of T and Q |
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| 62 | ! P2.A.2> Coupling between condensed water and temperature |
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| 63 | ! P2.A.3> Calculation of final quantities associated with cloud formation |
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[4412] | 64 | ! P2.B> Release of Latent heat after cloud formation |
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[3999] | 65 | ! P3> Autoconversion to precipitation (k-level) |
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| 66 | ! P4> Wet scavenging |
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| 67 | !------------------------------------------------------------------------------ |
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| 68 | ! Some preliminary comments (JBM) : |
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| 69 | ! |
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| 70 | ! The cloud water that the radiation scheme sees is not the same that the cloud |
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| 71 | ! water used in the physics and the dynamics |
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| 72 | ! |
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[4412] | 73 | ! During the autoconversion to precipitation (P3 step), radocond (cloud water used |
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[3999] | 74 | ! by the radiation scheme) is calculated as an average of the water that remains |
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| 75 | ! in the cloud during the precipitation and not the water remaining at the end |
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| 76 | ! of the time step. The latter is used in the rest of the physics and advected |
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| 77 | ! by the dynamics. |
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| 78 | ! |
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| 79 | ! In summary: |
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| 80 | ! |
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| 81 | ! Radiation: |
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| 82 | ! xflwc(newmicro)+xfiwc(newmicro) = |
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[4412] | 83 | ! radocond=lwcon(nc)+iwcon(nc) |
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[3999] | 84 | ! |
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| 85 | ! Notetheless, be aware of: |
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| 86 | ! |
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[4412] | 87 | ! radocond .NE. ocond(nc) |
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[3999] | 88 | ! i.e.: |
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| 89 | ! lwcon(nc)+iwcon(nc) .NE. ocond(nc) |
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[4412] | 90 | ! but oliq+(ocond-oliq) .EQ. ocond |
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[3999] | 91 | ! (which is not trivial) |
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| 92 | !++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
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[4226] | 93 | ! |
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[4654] | 94 | |
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| 95 | ! USE de modules contenant des fonctions. |
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[4651] | 96 | USE lmdz_cloudth, ONLY : cloudth, cloudth_v3, cloudth_v6, cloudth_mpc |
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[4664] | 97 | USE lmdz_lscp_tools, ONLY : calc_qsat_ecmwf, icefrac_lscp, calc_gammasat |
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| 98 | USE lmdz_lscp_tools, ONLY : fallice_velocity, distance_to_cloud_top |
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[4380] | 99 | USE ice_sursat_mod, ONLY : ice_sursat |
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[4803] | 100 | USE lmdz_lscp_poprecip, ONLY : poprecip_evapsub, poprecip_postcld |
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[3999] | 101 | |
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[4664] | 102 | ! Use du module lmdz_lscp_ini contenant les constantes |
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[4666] | 103 | USE lmdz_lscp_ini, ONLY : prt_level, lunout |
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[4664] | 104 | USE lmdz_lscp_ini, ONLY : seuil_neb, niter_lscp, iflag_evap_prec, t_coup, DDT0, ztfondue, rain_int_min |
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| 105 | USE lmdz_lscp_ini, ONLY : iflag_mpc_bl, ok_radocond_snow, a_tr_sca, cld_expo_con, cld_expo_lsc |
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| 106 | USE lmdz_lscp_ini, ONLY : iflag_cloudth_vert, iflag_rain_incloud_vol, iflag_t_glace, t_glace_min |
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| 107 | USE lmdz_lscp_ini, ONLY : coef_eva, coef_eva_i,cld_tau_lsc, cld_tau_con, cld_lc_lsc, cld_lc_con |
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| 108 | USE lmdz_lscp_ini, ONLY : iflag_bergeron, iflag_fisrtilp_qsat, iflag_vice, cice_velo, dice_velo |
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| 109 | USE lmdz_lscp_ini, ONLY : iflag_autoconversion, ffallv_con, ffallv_lsc |
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| 110 | USE lmdz_lscp_ini, ONLY : RCPD, RLSTT, RLVTT, RLMLT, RVTMP2, RTT, RD, RG |
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[4803] | 111 | USE lmdz_lscp_ini, ONLY : ok_poprecip |
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[4380] | 112 | |
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[3999] | 113 | IMPLICIT NONE |
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| 114 | |
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| 115 | !=============================================================================== |
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[4380] | 116 | ! VARIABLES DECLARATION |
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[3999] | 117 | !=============================================================================== |
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| 118 | |
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| 119 | ! INPUT VARIABLES: |
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| 120 | !----------------- |
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| 121 | |
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[4380] | 122 | INTEGER, INTENT(IN) :: klon,klev ! number of horizontal grid points and vertical levels |
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[3999] | 123 | REAL, INTENT(IN) :: dtime ! time step [s] |
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[4380] | 124 | REAL, INTENT(IN) :: missing_val ! missing value for output |
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[4059] | 125 | |
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[3999] | 126 | REAL, DIMENSION(klon,klev+1), INTENT(IN) :: paprs ! inter-layer pressure [Pa] |
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| 127 | REAL, DIMENSION(klon,klev), INTENT(IN) :: pplay ! mid-layer pressure [Pa] |
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[4654] | 128 | REAL, DIMENSION(klon,klev), INTENT(IN) :: temp ! temperature (K) |
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[4686] | 129 | REAL, DIMENSION(klon,klev), INTENT(IN) :: qt ! total specific humidity (in vapor phase in input) [kg/kg] |
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[3999] | 130 | INTEGER, INTENT(IN) :: iflag_cld_th ! flag that determines the distribution of convective clouds |
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| 131 | INTEGER, INTENT(IN) :: iflag_ice_thermo! flag to activate the ice thermodynamics |
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[4226] | 132 | ! CR: if iflag_ice_thermo=2, only convection is active |
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[4072] | 133 | LOGICAL, INTENT(IN) :: ok_ice_sursat ! flag to determine if ice sursaturation is activated |
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[4059] | 134 | |
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[3999] | 135 | LOGICAL, DIMENSION(klon,klev), INTENT(IN) :: ptconv ! grid points where deep convection scheme is active |
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| 136 | |
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| 137 | !Inputs associated with thermal plumes |
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[4226] | 138 | |
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[3999] | 139 | REAL, DIMENSION(klon,klev), INTENT(IN) :: ztv ! virtual potential temperature [K] |
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| 140 | REAL, DIMENSION(klon,klev), INTENT(IN) :: zqta ! specific humidity within thermals [kg/kg] |
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| 141 | REAL, DIMENSION(klon,klev), INTENT(IN) :: fraca ! fraction of thermals within the mesh [-] |
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| 142 | REAL, DIMENSION(klon,klev), INTENT(IN) :: zpspsk ! exner potential (p/100000)**(R/cp) |
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| 143 | REAL, DIMENSION(klon,klev), INTENT(IN) :: ztla ! liquid temperature within thermals [K] |
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| 144 | |
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| 145 | ! INPUT/OUTPUT variables |
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| 146 | !------------------------ |
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[4562] | 147 | |
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| 148 | REAL, DIMENSION(klon,klev), INTENT(INOUT) :: zthl ! liquid potential temperature [K] |
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[4686] | 149 | REAL, DIMENSION(klon,klev), INTENT(INOUT) :: ratqs ! function of pressure that sets the large-scale |
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[4059] | 150 | |
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[4380] | 151 | |
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[4059] | 152 | ! Input sursaturation en glace |
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| 153 | REAL, DIMENSION(klon,klev), INTENT(INOUT):: rneb_seri ! fraction nuageuse en memoire |
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[3999] | 154 | |
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| 155 | ! OUTPUT variables |
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| 156 | !----------------- |
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| 157 | |
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| 158 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: d_t ! temperature increment [K] |
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| 159 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: d_q ! specific humidity increment [kg/kg] |
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| 160 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: d_ql ! liquid water increment [kg/kg] |
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| 161 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: d_qi ! cloud ice mass increment [kg/kg] |
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| 162 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: rneb ! cloud fraction [-] |
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[4380] | 163 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: rneblsvol ! cloud fraction per unit volume [-] |
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[4530] | 164 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: pfraclr ! precip fraction clear-sky part [-] |
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| 165 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: pfracld ! precip fraction cloudy part [-] |
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[4412] | 166 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: radocond ! condensed water used in the radiation scheme [kg/kg] |
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[3999] | 167 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: radicefrac ! ice fraction of condensed water for radiation scheme |
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| 168 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: rhcl ! clear-sky relative humidity [-] |
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[4412] | 169 | REAL, DIMENSION(klon), INTENT(OUT) :: rain ! surface large-scale rainfall [kg/s/m2] |
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| 170 | REAL, DIMENSION(klon), INTENT(OUT) :: snow ! surface large-scale snowfall [kg/s/m2] |
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[4380] | 171 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qsatl ! saturation specific humidity wrt liquid [kg/kg] |
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| 172 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qsats ! saturation specific humidity wrt ice [kg/kg] |
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[3999] | 173 | REAL, DIMENSION(klon,klev+1), INTENT(OUT) :: prfl ! large-scale rainfall flux in the column [kg/s/m2] |
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| 174 | REAL, DIMENSION(klon,klev+1), INTENT(OUT) :: psfl ! large-scale snowfall flux in the column [kg/s/m2] |
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[4562] | 175 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: distcltop ! distance to cloud top [m] |
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[4639] | 176 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: temp_cltop ! temperature of cloud top [K] |
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[4686] | 177 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: beta ! conversion rate of condensed water |
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| 178 | |
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[3999] | 179 | ! fraction of aerosol scavenging through impaction and nucleation (for on-line) |
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| 180 | |
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| 181 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: frac_impa ! scavenging fraction due tu impaction [-] |
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| 182 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: frac_nucl ! scavenging fraction due tu nucleation [-] |
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| 183 | |
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[4380] | 184 | ! for supersaturation and contrails parameterisation |
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[3999] | 185 | |
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[4380] | 186 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qclr ! specific total water content in clear sky region [kg/kg] |
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| 187 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qcld ! specific total water content in cloudy region [kg/kg] |
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| 188 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qss ! specific total water content in supersat region [kg/kg] |
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| 189 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qvc ! specific vapor content in clouds [kg/kg] |
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| 190 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: rnebclr ! mesh fraction of clear sky [-] |
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| 191 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: rnebss ! mesh fraction of ISSR [-] |
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| 192 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: gamma_ss ! coefficient governing the ice nucleation RHi threshold [-] |
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[4425] | 193 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: Tcontr ! threshold temperature for contrail formation [K] |
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| 194 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qcontr ! threshold humidity for contrail formation [kg/kg] |
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| 195 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qcontr2 ! // (2nd expression more consistent with LMDZ expression of q) |
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| 196 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: fcontrN ! fraction of grid favourable to non-persistent contrails |
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| 197 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: fcontrP ! fraction of grid favourable to persistent contrails |
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[4686] | 198 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: cloudth_sth ! mean saturation deficit in thermals |
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| 199 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: cloudth_senv ! mean saturation deficit in environment |
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| 200 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: cloudth_sigmath ! std of saturation deficit in thermals |
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| 201 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: cloudth_sigmaenv ! std of saturation deficit in environment |
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[3999] | 202 | |
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[4803] | 203 | ! for POPRECIP |
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[4686] | 204 | |
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[4803] | 205 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqreva !-- rain tendendy due to evaporation [kg/kg/s] |
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| 206 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqssub !-- snow tendency due to sublimation [kg/kg/s] |
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| 207 | 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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| 208 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqsagg !-- snow tendency due to collection of lcoud ice by aggregation [kg/kg/s] |
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| 209 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqrauto !-- rain tendency due to autoconversion of cloud liquid [kg/kg/s] |
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| 210 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqsauto !-- snow tendency due to autoconversion of cloud ice [kg/kg/s] |
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| 211 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqsrim !-- snow tendency due to riming [kg/kg/s] |
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| 212 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqsmelt !-- snow tendency due to melting [kg/kg/s] |
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| 213 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqrmelt !-- rain tendency due to melting [kg/kg/s] |
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| 214 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqsfreez !-- snow tendency due to freezing [kg/kg/s] |
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| 215 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqrfreez !-- rain tendency due to freezing [kg/kg/s] |
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[4686] | 216 | |
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[4803] | 217 | |
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[3999] | 218 | ! LOCAL VARIABLES: |
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| 219 | !---------------- |
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| 220 | |
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[4654] | 221 | REAL,DIMENSION(klon) :: qsl, qsi |
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| 222 | REAL :: zct, zcl,zexpo |
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| 223 | REAL, DIMENSION(klon,klev) :: ctot |
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| 224 | REAL, DIMENSION(klon,klev) :: ctot_vol |
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| 225 | REAL, DIMENSION(klon) :: zqs, zdqs |
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| 226 | REAL :: zdelta, zcor, zcvm5 |
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| 227 | REAL, DIMENSION(klon) :: zdqsdT_raw |
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| 228 | REAL, DIMENSION(klon) :: gammasat,dgammasatdt ! coefficient to make cold condensation at the correct RH and derivative wrt T |
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| 229 | REAL, DIMENSION(klon) :: Tbef,qlbef,DT |
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| 230 | REAL :: num,denom |
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| 231 | REAL :: cste |
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| 232 | REAL, DIMENSION(klon) :: zpdf_sig,zpdf_k,zpdf_delta |
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| 233 | REAL, DIMENSION(klon) :: Zpdf_a,zpdf_b,zpdf_e1,zpdf_e2 |
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| 234 | REAL :: erf |
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| 235 | REAL, DIMENSION(klon,klev) :: icefrac_mpc |
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| 236 | REAL, DIMENSION(klon) :: qcloud, qincloud_mpc |
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| 237 | REAL, DIMENSION(klon) :: zrfl, zrfln |
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| 238 | REAL :: zqev, zqevt |
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| 239 | REAL, DIMENSION(klon) :: zifl, zifln, ziflprev |
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| 240 | REAL :: zqev0,zqevi, zqevti |
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| 241 | REAL, DIMENSION(klon) :: zoliq, zcond, zq, zqn |
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| 242 | REAL, DIMENSION(klon) :: zoliql, zoliqi |
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| 243 | REAL, DIMENSION(klon) :: zt |
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| 244 | REAL, DIMENSION(klon,klev) :: zrho |
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| 245 | REAL, DIMENSION(klon) :: zdz,iwc |
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| 246 | REAL :: zchau,zfroi |
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| 247 | REAL, DIMENSION(klon) :: zfice,zneb,znebprecip |
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| 248 | REAL :: zmelt,zrain,zsnow,zprecip |
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| 249 | REAL, DIMENSION(klon) :: dzfice |
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| 250 | REAL :: zsolid |
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| 251 | REAL, DIMENSION(klon) :: qtot, qzero |
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| 252 | REAL, DIMENSION(klon) :: dqsl,dqsi |
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| 253 | REAL :: smallestreal |
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[3999] | 254 | ! Variables for Bergeron process |
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[4654] | 255 | REAL :: zcp, coef1, DeltaT, Deltaq, Deltaqprecl |
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| 256 | REAL, DIMENSION(klon) :: zqpreci, zqprecl |
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[3999] | 257 | ! Variables precipitation energy conservation |
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[4654] | 258 | REAL, DIMENSION(klon) :: zmqc |
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| 259 | REAL :: zalpha_tr |
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| 260 | REAL :: zfrac_lessi |
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| 261 | REAL, DIMENSION(klon) :: zprec_cond |
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[4803] | 262 | REAL :: zmair |
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[4654] | 263 | REAL :: zcpair, zcpeau |
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| 264 | REAL, DIMENSION(klon) :: zlh_solid |
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[4803] | 265 | REAL, DIMENSION(klon) :: ztupnew |
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[4654] | 266 | REAL :: zm_solid ! for liquid -> solid conversion |
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| 267 | REAL, DIMENSION(klon) :: zrflclr, zrflcld |
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| 268 | REAL, DIMENSION(klon) :: d_zrfl_clr_cld, d_zifl_clr_cld |
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| 269 | REAL, DIMENSION(klon) :: d_zrfl_cld_clr, d_zifl_cld_clr |
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| 270 | REAL, DIMENSION(klon) :: ziflclr, ziflcld |
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| 271 | REAL, DIMENSION(klon) :: znebprecipclr, znebprecipcld |
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| 272 | REAL, DIMENSION(klon) :: tot_zneb, tot_znebn, d_tot_zneb |
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| 273 | REAL, DIMENSION(klon) :: d_znebprecip_clr_cld, d_znebprecip_cld_clr |
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| 274 | REAL, DIMENSION(klon,klev) :: velo |
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| 275 | REAL :: vr, ffallv |
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| 276 | REAL :: qlmpc, qimpc, rnebmpc |
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| 277 | REAL, DIMENSION(klon,klev) :: radocondi, radocondl |
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| 278 | REAL :: effective_zneb |
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| 279 | REAL, DIMENSION(klon) :: distcltop1D, temp_cltop1D |
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[3999] | 280 | |
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[4562] | 281 | |
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[4654] | 282 | INTEGER i, k, n, kk, iter |
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| 283 | INTEGER, DIMENSION(klon) :: n_i |
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[4226] | 284 | INTEGER ncoreczq |
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[4654] | 285 | INTEGER, DIMENSION(klon,klev) :: mpc_bl_points |
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[4803] | 286 | LOGICAL iftop |
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[3999] | 287 | |
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[4654] | 288 | LOGICAL, DIMENSION(klon) :: lognormale |
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| 289 | LOGICAL, DIMENSION(klon) :: keepgoing |
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[3999] | 290 | |
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| 291 | CHARACTER (len = 20) :: modname = 'lscp' |
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| 292 | CHARACTER (len = 80) :: abort_message |
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| 293 | |
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| 294 | |
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| 295 | !=============================================================================== |
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| 296 | ! INITIALISATION |
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| 297 | !=============================================================================== |
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| 298 | |
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[4226] | 299 | ! Few initial checks |
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[3999] | 300 | |
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[4654] | 301 | |
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[3999] | 302 | IF (iflag_fisrtilp_qsat .LT. 0) THEN |
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[4226] | 303 | abort_message = 'lscp cannot be used with iflag_fisrtilp<0' |
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| 304 | CALL abort_physic(modname,abort_message,1) |
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[3999] | 305 | ENDIF |
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| 306 | |
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| 307 | ! Few initialisations |
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| 308 | |
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[4226] | 309 | znebprecip(:)=0.0 |
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[3999] | 310 | ctot_vol(1:klon,1:klev)=0.0 |
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| 311 | rneblsvol(1:klon,1:klev)=0.0 |
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[4226] | 312 | smallestreal=1.e-9 |
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| 313 | znebprecipclr(:)=0.0 |
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| 314 | znebprecipcld(:)=0.0 |
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[3999] | 315 | mpc_bl_points(:,:)=0 |
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| 316 | |
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| 317 | IF (prt_level>9) WRITE(lunout,*) 'NUAGES4 A. JAM' |
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| 318 | |
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| 319 | ! AA for 'safety' reasons |
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| 320 | zalpha_tr = 0. |
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| 321 | zfrac_lessi = 0. |
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[4380] | 322 | beta(:,:)= 0. |
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[3999] | 323 | |
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[4380] | 324 | ! Initialisation of variables: |
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| 325 | |
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[3999] | 326 | prfl(:,:) = 0.0 |
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| 327 | psfl(:,:) = 0.0 |
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| 328 | d_t(:,:) = 0.0 |
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| 329 | d_q(:,:) = 0.0 |
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| 330 | d_ql(:,:) = 0.0 |
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| 331 | d_qi(:,:) = 0.0 |
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| 332 | rneb(:,:) = 0.0 |
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[4530] | 333 | pfraclr(:,:)=0.0 |
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| 334 | pfracld(:,:)=0.0 |
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[4412] | 335 | radocond(:,:) = 0.0 |
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[3999] | 336 | radicefrac(:,:) = 0.0 |
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[4226] | 337 | frac_nucl(:,:) = 1.0 |
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| 338 | frac_impa(:,:) = 1.0 |
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[3999] | 339 | rain(:) = 0.0 |
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| 340 | snow(:) = 0.0 |
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[4114] | 341 | zoliq(:)=0.0 |
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| 342 | zfice(:)=0.0 |
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| 343 | dzfice(:)=0.0 |
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| 344 | zqprecl(:)=0.0 |
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| 345 | zqpreci(:)=0.0 |
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[3999] | 346 | zrfl(:) = 0.0 |
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| 347 | zifl(:) = 0.0 |
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[4114] | 348 | ziflprev(:)=0.0 |
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[3999] | 349 | zneb(:) = seuil_neb |
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[4226] | 350 | zrflclr(:) = 0.0 |
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| 351 | ziflclr(:) = 0.0 |
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| 352 | zrflcld(:) = 0.0 |
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| 353 | ziflcld(:) = 0.0 |
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| 354 | tot_zneb(:) = 0.0 |
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| 355 | tot_znebn(:) = 0.0 |
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| 356 | d_tot_zneb(:) = 0.0 |
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| 357 | qzero(:) = 0.0 |
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[4562] | 358 | distcltop1D(:)=0.0 |
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[4639] | 359 | temp_cltop1D(:) = 0.0 |
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[4803] | 360 | ztupnew(:)=0.0 |
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[4380] | 361 | !--ice supersaturation |
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[4226] | 362 | gamma_ss(:,:) = 1.0 |
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| 363 | qss(:,:) = 0.0 |
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| 364 | rnebss(:,:) = 0.0 |
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[4059] | 365 | Tcontr(:,:) = missing_val |
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| 366 | qcontr(:,:) = missing_val |
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| 367 | qcontr2(:,:) = missing_val |
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| 368 | fcontrN(:,:) = 0.0 |
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| 369 | fcontrP(:,:) = 0.0 |
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[4654] | 370 | distcltop(:,:)=0. |
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| 371 | temp_cltop(:,:)=0. |
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[4803] | 372 | !-- poprecip |
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| 373 | dqreva(:,:)=0.0 |
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| 374 | dqrauto(:,:)=0.0 |
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| 375 | dqrmelt(:,:)=0.0 |
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| 376 | dqrfreez(:,:)=0.0 |
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| 377 | dqrcol(:,:)=0.0 |
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| 378 | dqssub(:,:)=0.0 |
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| 379 | dqsauto(:,:)=0.0 |
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| 380 | dqsrim(:,:)=0.0 |
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| 381 | dqsagg(:,:)=0.0 |
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| 382 | dqsfreez(:,:)=0.0 |
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| 383 | dqsmelt(:,:)=0.0 |
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[3999] | 384 | |
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[4803] | 385 | |
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| 386 | |
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| 387 | |
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[4392] | 388 | !c_iso: variable initialisation for iso |
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| 389 | |
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| 390 | |
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[3999] | 391 | !=============================================================================== |
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| 392 | ! BEGINNING OF VERTICAL LOOP FROM TOP TO BOTTOM |
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| 393 | !=============================================================================== |
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| 394 | |
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| 395 | ncoreczq=0 |
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| 396 | |
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| 397 | DO k = klev, 1, -1 |
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| 398 | |
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[4803] | 399 | IF (k.LE.klev-1) THEN |
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| 400 | iftop=.false. |
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| 401 | ELSE |
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| 402 | iftop=.true. |
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| 403 | ENDIF |
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| 404 | |
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[3999] | 405 | ! Initialisation temperature and specific humidity |
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| 406 | DO i = 1, klon |
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[4654] | 407 | zt(i)=temp(i,k) |
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[4686] | 408 | zq(i)=qt(i,k) |
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[4803] | 409 | IF (.not. iftop) THEN |
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| 410 | ztupnew(i)=temp(i,k+1)+d_t(i,k+1) |
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| 411 | ENDIF |
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[4392] | 412 | !c_iso init of iso |
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[3999] | 413 | ENDDO |
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[4803] | 414 | |
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| 415 | !================================================================ |
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| 416 | ! Flag for the new and more microphysical treatment of precipitation from Atelier Nuage (R) |
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| 417 | IF (ok_poprecip) THEN |
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| 418 | |
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| 419 | CALL poprecip_evapsub(klon, dtime, iftop, paprs(:,k), paprs(:,k+1), pplay(:,k), & |
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| 420 | zt, ztupnew, zq, zmqc, znebprecipclr, znebprecipcld, & |
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| 421 | zrfl, zrflclr, zrflcld, & |
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| 422 | zifl, ziflclr, ziflcld, & |
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| 423 | dqreva(:,k),dqssub(:,k) & |
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| 424 | ) |
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| 425 | |
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| 426 | !================================================================ |
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| 427 | ELSE |
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| 428 | |
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[3999] | 429 | ! -------------------------------------------------------------------- |
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[4803] | 430 | ! P1> Thermalization of precipitation falling from the overlying layer |
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[3999] | 431 | ! -------------------------------------------------------------------- |
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[4412] | 432 | ! Computes air temperature variation due to enthalpy transported by |
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[3999] | 433 | ! precipitation. Precipitation is then thermalized with the air in the |
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| 434 | ! layer. |
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| 435 | ! The precipitation should remain thermalized throughout the different |
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[4412] | 436 | ! thermodynamical transformations. |
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| 437 | ! The corresponding water mass should |
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[3999] | 438 | ! be added when calculating the layer's enthalpy change with |
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| 439 | ! temperature |
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[4412] | 440 | ! See lmdzpedia page todoan |
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| 441 | ! todoan: check consistency with ice phase |
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| 442 | ! todoan: understand why several steps |
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[3999] | 443 | ! --------------------------------------------------------------------- |
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| 444 | |
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[4803] | 445 | IF (iftop) THEN |
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[3999] | 446 | |
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| 447 | DO i = 1, klon |
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[4803] | 448 | zmqc(i) = 0. |
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| 449 | ENDDO |
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| 450 | |
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| 451 | ELSE |
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| 452 | |
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| 453 | DO i = 1, klon |
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[3999] | 454 | |
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[4803] | 455 | zmair=(paprs(i,k)-paprs(i,k+1))/RG |
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[3999] | 456 | ! no condensed water so cp=cp(vapor+dry air) |
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| 457 | ! RVTMP2=rcpv/rcpd-1 |
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| 458 | zcpair=RCPD*(1.0+RVTMP2*zq(i)) |
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[4226] | 459 | zcpeau=RCPD*RVTMP2 |
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| 460 | |
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[3999] | 461 | ! zmqc: precipitation mass that has to be thermalized with |
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| 462 | ! layer's air so that precipitation at the ground has the |
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| 463 | ! same temperature as the lowermost layer |
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[4803] | 464 | zmqc(i) = (zrfl(i)+zifl(i))*dtime/zmair |
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[3999] | 465 | ! t(i,k+1)+d_t(i,k+1): new temperature of the overlying layer |
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[4803] | 466 | zt(i) = ( ztupnew(i)*zmqc(i)*zcpeau + zcpair*zt(i) ) & |
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[3999] | 467 | / (zcpair + zmqc(i)*zcpeau) |
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[4226] | 468 | |
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[3999] | 469 | ENDDO |
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| 470 | |
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| 471 | ENDIF |
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| 472 | |
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| 473 | ! -------------------------------------------------------------------- |
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[4803] | 474 | ! P2> Precipitation evaporation/sublimation/melting |
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[3999] | 475 | ! -------------------------------------------------------------------- |
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[4803] | 476 | ! A part of the precipitation coming from above is evaporated/sublimated/melted. |
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[3999] | 477 | ! -------------------------------------------------------------------- |
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[4803] | 478 | |
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[4397] | 479 | IF (iflag_evap_prec.GE.1) THEN |
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[3999] | 480 | |
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[4072] | 481 | ! Calculation of saturation specific humidity |
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| 482 | ! depending on temperature: |
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[4380] | 483 | CALL calc_qsat_ecmwf(klon,zt(:),qzero(:),pplay(:,k),RTT,0,.false.,zqs(:),zdqs(:)) |
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[4072] | 484 | ! wrt liquid water |
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[4380] | 485 | CALL calc_qsat_ecmwf(klon,zt(:),qzero(:),pplay(:,k),RTT,1,.false.,qsl(:),dqsl(:)) |
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[4072] | 486 | ! wrt ice |
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[4380] | 487 | CALL calc_qsat_ecmwf(klon,zt(:),qzero(:),pplay(:,k),RTT,2,.false.,qsi(:),dqsi(:)) |
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[3999] | 488 | |
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| 489 | DO i = 1, klon |
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[4226] | 490 | |
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[3999] | 491 | ! if precipitation |
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| 492 | IF (zrfl(i)+zifl(i).GT.0.) THEN |
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[4226] | 493 | |
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[4563] | 494 | ! LudoTP: we only account for precipitation evaporation in the clear-sky (iflag_evap_prec>=4). |
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[4392] | 495 | ! c_iso: likely important to distinguish cs from neb isotope precipitation |
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| 496 | |
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[4563] | 497 | IF (iflag_evap_prec.GE.4) THEN |
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[4226] | 498 | zrfl(i) = zrflclr(i) |
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| 499 | zifl(i) = ziflclr(i) |
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| 500 | ENDIF |
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[3999] | 501 | |
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| 502 | IF (iflag_evap_prec.EQ.1) THEN |
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| 503 | znebprecip(i)=zneb(i) |
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| 504 | ELSE |
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| 505 | znebprecip(i)=MAX(zneb(i),znebprecip(i)) |
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| 506 | ENDIF |
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| 507 | |
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[4563] | 508 | IF (iflag_evap_prec.GT.4) THEN |
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| 509 | ! Max evaporation not to saturate the clear sky precip fraction |
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| 510 | ! i.e. the fraction where evaporation occurs |
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| 511 | zqev0 = MAX(0.0, (zqs(i)-zq(i))*znebprecipclr(i)) |
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| 512 | ELSEIF (iflag_evap_prec .EQ. 4) THEN |
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[4226] | 513 | ! Max evaporation not to saturate the whole mesh |
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[4563] | 514 | ! Pay attention -> lead to unrealistic and excessive evaporation |
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[4226] | 515 | zqev0 = MAX(0.0, zqs(i)-zq(i)) |
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| 516 | ELSE |
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| 517 | ! Max evap not to saturate the fraction below the cloud |
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| 518 | zqev0 = MAX(0.0, (zqs(i)-zq(i))*znebprecip(i)) |
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| 519 | ENDIF |
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[3999] | 520 | |
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| 521 | ! Evaporation of liquid precipitation coming from above |
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| 522 | ! dP/dz=beta*(1-q/qsat)*sqrt(P) |
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| 523 | ! formula from Sundquist 1988, Klemp & Wilhemson 1978 |
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[4563] | 524 | ! LTP: evaporation only in the clear sky part (iflag_evap_prec>=4) |
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[3999] | 525 | |
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| 526 | IF (iflag_evap_prec.EQ.3) THEN |
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[4072] | 527 | zqevt = znebprecip(i)*coef_eva*(1.0-zq(i)/qsl(i)) & |
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[3999] | 528 | *SQRT(zrfl(i)/max(1.e-4,znebprecip(i))) & |
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| 529 | *(paprs(i,k)-paprs(i,k+1))/pplay(i,k)*zt(i)*RD/RG |
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[4563] | 530 | ELSE IF (iflag_evap_prec.GE.4) THEN |
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[4072] | 531 | zqevt = znebprecipclr(i)*coef_eva*(1.0-zq(i)/qsl(i)) & |
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[3999] | 532 | *SQRT(zrfl(i)/max(1.e-8,znebprecipclr(i))) & |
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| 533 | *(paprs(i,k)-paprs(i,k+1))/pplay(i,k)*zt(i)*RD/RG |
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| 534 | ELSE |
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[4072] | 535 | zqevt = 1.*coef_eva*(1.0-zq(i)/qsl(i))*SQRT(zrfl(i)) & |
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[3999] | 536 | *(paprs(i,k)-paprs(i,k+1))/pplay(i,k)*zt(i)*RD/RG |
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| 537 | ENDIF |
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| 538 | |
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[4226] | 539 | zqevt = MAX(0.0,MIN(zqevt,zrfl(i))) & |
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| 540 | *RG*dtime/(paprs(i,k)-paprs(i,k+1)) |
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[3999] | 541 | |
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| 542 | ! sublimation of the solid precipitation coming from above |
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| 543 | IF (iflag_evap_prec.EQ.3) THEN |
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[4072] | 544 | zqevti = znebprecip(i)*coef_eva_i*(1.0-zq(i)/qsi(i)) & |
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[3999] | 545 | *SQRT(zifl(i)/max(1.e-4,znebprecip(i))) & |
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| 546 | *(paprs(i,k)-paprs(i,k+1))/pplay(i,k)*zt(i)*RD/RG |
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[4563] | 547 | ELSE IF (iflag_evap_prec.GE.4) THEN |
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[4072] | 548 | zqevti = znebprecipclr(i)*coef_eva_i*(1.0-zq(i)/qsi(i)) & |
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[3999] | 549 | *SQRT(zifl(i)/max(1.e-8,znebprecipclr(i))) & |
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| 550 | *(paprs(i,k)-paprs(i,k+1))/pplay(i,k)*zt(i)*RD/RG |
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| 551 | ELSE |
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[4072] | 552 | zqevti = 1.*coef_eva_i*(1.0-zq(i)/qsi(i))*SQRT(zifl(i)) & |
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[3999] | 553 | *(paprs(i,k)-paprs(i,k+1))/pplay(i,k)*zt(i)*RD/RG |
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| 554 | ENDIF |
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[4226] | 555 | |
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[3999] | 556 | zqevti = MAX(0.0,MIN(zqevti,zifl(i))) & |
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[4226] | 557 | *RG*dtime/(paprs(i,k)-paprs(i,k+1)) |
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[3999] | 558 | |
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| 559 | ! A. JAM |
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| 560 | ! Evaporation limit: we ensure that the layer's fraction below |
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| 561 | ! the cloud or the whole mesh (depending on iflag_evap_prec) |
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| 562 | ! does not reach saturation. In this case, we |
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| 563 | ! redistribute zqev0 conserving the ratio liquid/ice |
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[4226] | 564 | |
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[3999] | 565 | IF (zqevt+zqevti.GT.zqev0) THEN |
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| 566 | zqev=zqev0*zqevt/(zqevt+zqevti) |
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| 567 | zqevi=zqev0*zqevti/(zqevt+zqevti) |
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| 568 | ELSE |
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| 569 | zqev=zqevt |
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| 570 | zqevi=zqevti |
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| 571 | ENDIF |
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| 572 | |
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| 573 | |
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[4392] | 574 | ! New solid and liquid precipitation fluxes after evap and sublimation |
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[3999] | 575 | zrfln(i) = Max(0.,zrfl(i) - zqev*(paprs(i,k)-paprs(i,k+1)) & |
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| 576 | /RG/dtime) |
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| 577 | zifln(i) = Max(0.,zifl(i) - zqevi*(paprs(i,k)-paprs(i,k+1)) & |
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| 578 | /RG/dtime) |
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| 579 | |
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[4392] | 580 | |
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[3999] | 581 | ! vapor, temperature, precip fluxes update |
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[4803] | 582 | ! vapor is updated after evaporation/sublimation (it is increased) |
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[3999] | 583 | zq(i) = zq(i) - (zrfln(i)+zifln(i)-zrfl(i)-zifl(i)) & |
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| 584 | * (RG/(paprs(i,k)-paprs(i,k+1)))*dtime |
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[4803] | 585 | ! zmqc is the total condensed water in the precip flux (it is decreased) |
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[3999] | 586 | zmqc(i) = zmqc(i) + (zrfln(i)+zifln(i)-zrfl(i)-zifl(i)) & |
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| 587 | * (RG/(paprs(i,k)-paprs(i,k+1)))*dtime |
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[4803] | 588 | ! air and precip temperature (i.e., gridbox temperature) |
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| 589 | ! is updated due to latent heat cooling |
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[3999] | 590 | zt(i) = zt(i) + (zrfln(i)-zrfl(i)) & |
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| 591 | * (RG/(paprs(i,k)-paprs(i,k+1)))*dtime & |
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| 592 | * RLVTT/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i))) & |
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| 593 | + (zifln(i)-zifl(i)) & |
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| 594 | * (RG/(paprs(i,k)-paprs(i,k+1)))*dtime & |
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| 595 | * RLSTT/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i))) |
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| 596 | |
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| 597 | ! New values of liquid and solid precipitation |
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| 598 | zrfl(i) = zrfln(i) |
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| 599 | zifl(i) = zifln(i) |
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| 600 | |
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[4392] | 601 | ! c_iso here call_reevap that updates isotopic zrfl, zifl (in inout) |
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| 602 | ! due to evap + sublim |
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| 603 | |
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| 604 | |
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[4563] | 605 | IF (iflag_evap_prec.GE.4) THEN |
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[4226] | 606 | zrflclr(i) = zrfl(i) |
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| 607 | ziflclr(i) = zifl(i) |
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| 608 | IF(zrflclr(i) + ziflclr(i).LE.0) THEN |
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| 609 | znebprecipclr(i) = 0.0 |
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| 610 | ENDIF |
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| 611 | zrfl(i) = zrflclr(i) + zrflcld(i) |
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| 612 | zifl(i) = ziflclr(i) + ziflcld(i) |
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| 613 | ENDIF |
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[3999] | 614 | |
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[4392] | 615 | ! c_iso duplicate for isotopes or loop on isotopes |
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[3999] | 616 | |
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[4392] | 617 | ! Melting: |
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[4412] | 618 | zmelt = ((zt(i)-RTT)/(ztfondue-RTT)) ! JYG |
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[3999] | 619 | ! precip fraction that is melted |
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| 620 | zmelt = MIN(MAX(zmelt,0.),1.) |
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[4392] | 621 | |
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[4412] | 622 | ! update of rainfall and snowfall due to melting |
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[4563] | 623 | IF (iflag_evap_prec.GE.4) THEN |
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[4226] | 624 | zrflclr(i)=zrflclr(i)+zmelt*ziflclr(i) |
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| 625 | zrflcld(i)=zrflcld(i)+zmelt*ziflcld(i) |
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| 626 | zrfl(i)=zrflclr(i)+zrflcld(i) |
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[4412] | 627 | |
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| 628 | ziflclr(i)=ziflclr(i)*(1.-zmelt) |
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| 629 | ziflcld(i)=ziflcld(i)*(1.-zmelt) |
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| 630 | zifl(i)=ziflclr(i)+ziflcld(i) |
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| 631 | |
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[4226] | 632 | ELSE |
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| 633 | zrfl(i)=zrfl(i)+zmelt*zifl(i) |
---|
[4412] | 634 | |
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| 635 | zifl(i)=zifl(i)*(1.-zmelt) |
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[4226] | 636 | ENDIF |
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[4412] | 637 | |
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| 638 | |
---|
[4392] | 639 | ! c_iso: melting of isotopic precipi with zmelt (no fractionation) |
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[3999] | 640 | |
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[4803] | 641 | ! Latent heat of melting because of precipitation melting |
---|
| 642 | ! NB: the air + precip temperature is simultaneously updated |
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[3999] | 643 | zt(i)=zt(i)-zifl(i)*zmelt*(RG*dtime)/(paprs(i,k)-paprs(i,k+1)) & |
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| 644 | *RLMLT/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i))) |
---|
| 645 | |
---|
| 646 | |
---|
| 647 | ELSE |
---|
| 648 | ! if no precip, we reinitialize the cloud fraction used for the precip to 0 |
---|
| 649 | znebprecip(i)=0. |
---|
| 650 | |
---|
| 651 | ENDIF ! (zrfl(i)+zifl(i).GT.0.) |
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| 652 | |
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[4803] | 653 | ENDDO ! loop on klon |
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[4226] | 654 | |
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[3999] | 655 | ENDIF ! (iflag_evap_prec>=1) |
---|
| 656 | |
---|
[4803] | 657 | ENDIF ! (ok_poprecip) |
---|
| 658 | |
---|
[3999] | 659 | ! -------------------------------------------------------------------- |
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| 660 | ! End precip evaporation |
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| 661 | ! -------------------------------------------------------------------- |
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| 662 | |
---|
| 663 | ! Calculation of qsat, L/Cp*dqsat/dT and ncoreczq counter |
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| 664 | !------------------------------------------------------- |
---|
[4226] | 665 | |
---|
[4072] | 666 | qtot(:)=zq(:)+zmqc(:) |
---|
[4380] | 667 | CALL calc_qsat_ecmwf(klon,zt(:),qtot(:),pplay(:,k),RTT,0,.false.,zqs(:),zdqs(:)) |
---|
[4072] | 668 | DO i = 1, klon |
---|
[3999] | 669 | zdelta = MAX(0.,SIGN(1.,RTT-zt(i))) |
---|
[4059] | 670 | zdqsdT_raw(i) = zdqs(i)*RCPD*(1.0+RVTMP2*zq(i)) / (RLVTT*(1.-zdelta) + RLSTT*zdelta) |
---|
[3999] | 671 | IF (zq(i) .LT. 1.e-15) THEN |
---|
| 672 | ncoreczq=ncoreczq+1 |
---|
| 673 | zq(i)=1.e-15 |
---|
| 674 | ENDIF |
---|
[4392] | 675 | ! c_iso: do something similar for isotopes |
---|
[3999] | 676 | |
---|
[4072] | 677 | ENDDO |
---|
[3999] | 678 | |
---|
| 679 | ! -------------------------------------------------------------------- |
---|
| 680 | ! P2> Cloud formation |
---|
| 681 | !--------------------------------------------------------------------- |
---|
| 682 | ! |
---|
| 683 | ! Unlike fisrtilp, we always assume a 'fractional cloud' approach |
---|
| 684 | ! i.e. clouds occupy only a fraction of the mesh (the subgrid distribution |
---|
| 685 | ! is prescribed and depends on large scale variables and boundary layer |
---|
| 686 | ! properties) |
---|
| 687 | ! The decrease in condensed part due tu latent heating is taken into |
---|
| 688 | ! account |
---|
| 689 | ! ------------------------------------------------------------------- |
---|
| 690 | |
---|
| 691 | ! P2.1> With the PDFs (log-normal, bigaussian) |
---|
[4424] | 692 | ! cloud properties calculation with the initial values of t and q |
---|
[3999] | 693 | ! ---------------------------------------------------------------- |
---|
| 694 | |
---|
| 695 | ! initialise gammasat and qincloud_mpc |
---|
| 696 | gammasat(:)=1. |
---|
| 697 | qincloud_mpc(:)=0. |
---|
| 698 | |
---|
| 699 | IF (iflag_cld_th.GE.5) THEN |
---|
| 700 | |
---|
| 701 | IF (iflag_mpc_bl .LT. 1) THEN |
---|
| 702 | |
---|
| 703 | IF (iflag_cloudth_vert.LE.2) THEN |
---|
| 704 | |
---|
| 705 | CALL cloudth(klon,klev,k,ztv, & |
---|
| 706 | zq,zqta,fraca, & |
---|
| 707 | qcloud,ctot,zpspsk,paprs,pplay,ztla,zthl, & |
---|
[4654] | 708 | ratqs,zqs,temp, & |
---|
[4651] | 709 | cloudth_sth,cloudth_senv,cloudth_sigmath,cloudth_sigmaenv) |
---|
[3999] | 710 | |
---|
[4651] | 711 | |
---|
[3999] | 712 | ELSEIF (iflag_cloudth_vert.GE.3 .AND. iflag_cloudth_vert.LE.5) THEN |
---|
| 713 | |
---|
| 714 | CALL cloudth_v3(klon,klev,k,ztv, & |
---|
| 715 | zq,zqta,fraca, & |
---|
| 716 | qcloud,ctot,ctot_vol,zpspsk,paprs,pplay,ztla,zthl, & |
---|
[4654] | 717 | ratqs,zqs,temp, & |
---|
[4651] | 718 | cloudth_sth,cloudth_senv,cloudth_sigmath,cloudth_sigmaenv) |
---|
[3999] | 719 | |
---|
[4226] | 720 | !Jean Jouhaud's version, Decembre 2018 |
---|
| 721 | !------------------------------------- |
---|
[3999] | 722 | |
---|
| 723 | ELSEIF (iflag_cloudth_vert.EQ.6) THEN |
---|
| 724 | |
---|
| 725 | CALL cloudth_v6(klon,klev,k,ztv, & |
---|
| 726 | zq,zqta,fraca, & |
---|
| 727 | qcloud,ctot,ctot_vol,zpspsk,paprs,pplay,ztla,zthl, & |
---|
[4654] | 728 | ratqs,zqs,temp, & |
---|
[4651] | 729 | cloudth_sth,cloudth_senv,cloudth_sigmath,cloudth_sigmaenv) |
---|
[3999] | 730 | |
---|
| 731 | ENDIF |
---|
| 732 | |
---|
| 733 | ELSE |
---|
| 734 | ! cloudth_v3 + cold microphysical considerations |
---|
| 735 | ! + stationary mixed-phase cloud model |
---|
| 736 | |
---|
[4380] | 737 | CALL cloudth_mpc(klon,klev,k,iflag_mpc_bl,mpc_bl_points, & |
---|
[4654] | 738 | temp,ztv,zq,zqta,fraca, zpspsk, & |
---|
[3999] | 739 | paprs,pplay,ztla,zthl,ratqs,zqs,psfl, & |
---|
[4651] | 740 | qcloud,qincloud_mpc,icefrac_mpc,ctot,ctot_vol, & |
---|
| 741 | cloudth_sth,cloudth_senv,cloudth_sigmath,cloudth_sigmaenv) |
---|
[3999] | 742 | |
---|
| 743 | ENDIF ! iflag_mpc_bl |
---|
| 744 | |
---|
| 745 | DO i=1,klon |
---|
| 746 | rneb(i,k)=ctot(i,k) |
---|
| 747 | rneblsvol(i,k)=ctot_vol(i,k) |
---|
| 748 | zqn(i)=qcloud(i) |
---|
| 749 | ENDDO |
---|
| 750 | |
---|
| 751 | ENDIF |
---|
| 752 | |
---|
| 753 | IF (iflag_cld_th .LE. 4) THEN |
---|
| 754 | |
---|
| 755 | ! lognormal |
---|
| 756 | lognormale = .TRUE. |
---|
| 757 | |
---|
| 758 | ELSEIF (iflag_cld_th .GE. 6) THEN |
---|
| 759 | |
---|
| 760 | ! lognormal distribution when no thermals |
---|
| 761 | lognormale = fraca(:,k) < 1e-10 |
---|
| 762 | |
---|
| 763 | ELSE |
---|
[4226] | 764 | ! When iflag_cld_th=5, we always assume |
---|
[3999] | 765 | ! bi-gaussian distribution |
---|
| 766 | lognormale = .FALSE. |
---|
| 767 | |
---|
| 768 | ENDIF |
---|
| 769 | |
---|
| 770 | DT(:) = 0. |
---|
| 771 | n_i(:)=0 |
---|
| 772 | Tbef(:)=zt(:) |
---|
| 773 | qlbef(:)=0. |
---|
| 774 | |
---|
| 775 | ! Treatment of non-boundary layer clouds (lognormale) |
---|
| 776 | ! condensation with qsat(T) variation (adaptation) |
---|
[4424] | 777 | ! Iterative resolution to converge towards qsat |
---|
| 778 | ! with update of temperature, ice fraction and qsat at |
---|
| 779 | ! each iteration |
---|
[4226] | 780 | |
---|
[4424] | 781 | ! todoan -> sensitivity to iflag_fisrtilp_qsat |
---|
[3999] | 782 | DO iter=1,iflag_fisrtilp_qsat+1 |
---|
[4226] | 783 | |
---|
[3999] | 784 | DO i=1,klon |
---|
| 785 | |
---|
[4424] | 786 | ! keepgoing = .true. while convergence is not satisfied |
---|
| 787 | keepgoing(i)=ABS(DT(i)).GT.DDT0 |
---|
[4226] | 788 | |
---|
[4424] | 789 | IF ((keepgoing(i) .OR. (n_i(i) .EQ. 0)) .AND. lognormale(i)) THEN |
---|
[4226] | 790 | |
---|
[3999] | 791 | ! if not convergence: |
---|
| 792 | |
---|
| 793 | ! P2.2.1> cloud fraction and condensed water mass calculation |
---|
| 794 | ! Calculated variables: |
---|
| 795 | ! rneb : cloud fraction |
---|
| 796 | ! zqn : total water within the cloud |
---|
| 797 | ! zcond: mean condensed water within the mesh |
---|
| 798 | ! rhcl: clear-sky relative humidity |
---|
| 799 | !--------------------------------------------------------------- |
---|
| 800 | |
---|
[4424] | 801 | ! new temperature that only serves in the iteration process: |
---|
[3999] | 802 | Tbef(i)=Tbef(i)+DT(i) |
---|
| 803 | |
---|
| 804 | ! Rneb, qzn and zcond for lognormal PDFs |
---|
[4072] | 805 | qtot(i)=zq(i)+zmqc(i) |
---|
[4226] | 806 | |
---|
[4072] | 807 | ENDIF |
---|
[3999] | 808 | |
---|
[4072] | 809 | ENDDO |
---|
| 810 | |
---|
[4380] | 811 | ! Calculation of saturation specific humidity and ice fraction |
---|
[4226] | 812 | CALL calc_qsat_ecmwf(klon,Tbef(:),qtot(:),pplay(:,k),RTT,0,.false.,zqs(:),zdqs(:)) |
---|
| 813 | CALL calc_gammasat(klon,Tbef(:),qtot(:),pplay(:,k),gammasat(:),dgammasatdt(:)) |
---|
[4072] | 814 | ! saturation may occur at a humidity different from qsat (gamma qsat), so gamma correction for dqs |
---|
| 815 | zdqs(:) = gammasat(:)*zdqs(:)+zqs(:)*dgammasatdt(:) |
---|
[4562] | 816 | ! cloud phase determination |
---|
| 817 | IF (iflag_t_glace.GE.4) THEN |
---|
| 818 | ! For iflag_t_glace GE 4 the phase partition function dependends on temperature AND distance to cloud top |
---|
[4654] | 819 | CALL distance_to_cloud_top(klon,klev,k,temp,pplay,paprs,rneb,distcltop1D,temp_cltop1D) |
---|
[4562] | 820 | ENDIF |
---|
[4639] | 821 | CALL icefrac_lscp(klon, zt(:), iflag_ice_thermo, distcltop1D(:),temp_cltop1D(:),zfice(:),dzfice(:)) |
---|
[4072] | 822 | |
---|
[4424] | 823 | DO i=1,klon !todoan : check if loop in i is needed |
---|
[4072] | 824 | |
---|
[4424] | 825 | IF ((keepgoing(i) .OR. (n_i(i) .EQ. 0)) .AND. lognormale(i)) THEN |
---|
[4072] | 826 | |
---|
[3999] | 827 | zpdf_sig(i)=ratqs(i,k)*zq(i) |
---|
| 828 | zpdf_k(i)=-sqrt(log(1.+(zpdf_sig(i)/zq(i))**2)) |
---|
| 829 | zpdf_delta(i)=log(zq(i)/(gammasat(i)*zqs(i))) |
---|
| 830 | zpdf_a(i)=zpdf_delta(i)/(zpdf_k(i)*sqrt(2.)) |
---|
| 831 | zpdf_b(i)=zpdf_k(i)/(2.*sqrt(2.)) |
---|
| 832 | zpdf_e1(i)=zpdf_a(i)-zpdf_b(i) |
---|
| 833 | zpdf_e1(i)=sign(min(ABS(zpdf_e1(i)),5.),zpdf_e1(i)) |
---|
| 834 | zpdf_e1(i)=1.-erf(zpdf_e1(i)) |
---|
| 835 | zpdf_e2(i)=zpdf_a(i)+zpdf_b(i) |
---|
| 836 | zpdf_e2(i)=sign(min(ABS(zpdf_e2(i)),5.),zpdf_e2(i)) |
---|
| 837 | zpdf_e2(i)=1.-erf(zpdf_e2(i)) |
---|
[4226] | 838 | |
---|
[4062] | 839 | IF ((.NOT.ok_ice_sursat).OR.(Tbef(i).GT.t_glace_min)) THEN |
---|
[4059] | 840 | |
---|
| 841 | IF (zpdf_e1(i).LT.1.e-10) THEN |
---|
| 842 | rneb(i,k)=0. |
---|
| 843 | zqn(i)=gammasat(i)*zqs(i) |
---|
| 844 | ELSE |
---|
| 845 | rneb(i,k)=0.5*zpdf_e1(i) |
---|
| 846 | zqn(i)=zq(i)*zpdf_e2(i)/zpdf_e1(i) |
---|
| 847 | ENDIF |
---|
| 848 | |
---|
[4072] | 849 | rnebss(i,k)=0.0 !--added by OB (needed because of the convergence loop on time) |
---|
[4059] | 850 | fcontrN(i,k)=0.0 !--idem |
---|
| 851 | fcontrP(i,k)=0.0 !--idem |
---|
| 852 | qss(i,k)=0.0 !--idem |
---|
[4226] | 853 | |
---|
[4424] | 854 | ELSE ! in case of ice supersaturation by Audran |
---|
[4226] | 855 | |
---|
[4059] | 856 | !------------------------------------ |
---|
[4072] | 857 | ! ICE SUPERSATURATION |
---|
[4059] | 858 | !------------------------------------ |
---|
[3999] | 859 | |
---|
[4654] | 860 | CALL ice_sursat(pplay(i,k), paprs(i,k)-paprs(i,k+1), dtime, i, k, temp(i,k), zq(i), & |
---|
[4226] | 861 | gamma_ss(i,k), zqs(i), Tbef(i), rneb_seri(i,k), ratqs(i,k), & |
---|
| 862 | rneb(i,k), zqn(i), rnebss(i,k), qss(i,k), & |
---|
[4059] | 863 | Tcontr(i,k), qcontr(i,k), qcontr2(i,k), fcontrN(i,k), fcontrP(i,k) ) |
---|
| 864 | |
---|
| 865 | ENDIF ! ((flag_ice_sursat.eq.0).or.(Tbef(i).gt.t_glace_min)) |
---|
| 866 | |
---|
[3999] | 867 | ! If vertical heterogeneity, change fraction by volume as well |
---|
| 868 | IF (iflag_cloudth_vert.GE.3) THEN |
---|
| 869 | ctot_vol(i,k)=rneb(i,k) |
---|
| 870 | rneblsvol(i,k)=ctot_vol(i,k) |
---|
| 871 | ENDIF |
---|
| 872 | |
---|
| 873 | |
---|
[4072] | 874 | ! P2.2.2> Approximative calculation of temperature variation DT |
---|
| 875 | ! due to condensation. |
---|
| 876 | ! Calculated variables: |
---|
| 877 | ! dT : temperature change due to condensation |
---|
| 878 | !--------------------------------------------------------------- |
---|
[3999] | 879 | |
---|
| 880 | |
---|
| 881 | IF (zfice(i).LT.1) THEN |
---|
| 882 | cste=RLVTT |
---|
| 883 | ELSE |
---|
| 884 | cste=RLSTT |
---|
| 885 | ENDIF |
---|
| 886 | |
---|
| 887 | qlbef(i)=max(0.,zqn(i)-zqs(i)) |
---|
| 888 | num = -Tbef(i)+zt(i)+rneb(i,k)*((1-zfice(i))*RLVTT & |
---|
[4226] | 889 | +zfice(i)*RLSTT)/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i)))*qlbef(i) |
---|
[3999] | 890 | denom = 1.+rneb(i,k)*((1-zfice(i))*RLVTT+zfice(i)*RLSTT)/cste*zdqs(i) & |
---|
| 891 | -(RLSTT-RLVTT)/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i)))*rneb(i,k) & |
---|
[4226] | 892 | *qlbef(i)*dzfice(i) |
---|
[4424] | 893 | ! here we update a provisory temperature variable that only serves in the iteration |
---|
| 894 | ! process |
---|
[3999] | 895 | DT(i)=num/denom |
---|
| 896 | n_i(i)=n_i(i)+1 |
---|
| 897 | |
---|
[4424] | 898 | ENDIF ! end keepgoing |
---|
[3999] | 899 | |
---|
| 900 | ENDDO ! end loop on i |
---|
| 901 | |
---|
| 902 | ENDDO ! iter=1,iflag_fisrtilp_qsat+1 |
---|
| 903 | |
---|
| 904 | ! P2.3> Final quantities calculation |
---|
| 905 | ! Calculated variables: |
---|
| 906 | ! rneb : cloud fraction |
---|
| 907 | ! zcond: mean condensed water in the mesh |
---|
| 908 | ! zqn : mean water vapor in the mesh |
---|
[4562] | 909 | ! zfice: ice fraction in clouds |
---|
[3999] | 910 | ! zt : temperature |
---|
| 911 | ! rhcl : clear-sky relative humidity |
---|
| 912 | ! ---------------------------------------------------------------- |
---|
| 913 | |
---|
| 914 | |
---|
[4562] | 915 | ! For iflag_t_glace GE 4 the phase partition function dependends on temperature AND distance to cloud top |
---|
| 916 | IF (iflag_t_glace.GE.4) THEN |
---|
[4654] | 917 | CALL distance_to_cloud_top(klon,klev,k,temp,pplay,paprs,rneb,distcltop1D,temp_cltop1D) |
---|
[4562] | 918 | distcltop(:,k)=distcltop1D(:) |
---|
[4639] | 919 | temp_cltop(:,k)=temp_cltop1D(:) |
---|
[4562] | 920 | ENDIF |
---|
| 921 | |
---|
[3999] | 922 | ! Partition function in stratiform clouds (will be overwritten in boundary-layer MPCs) |
---|
[4803] | 923 | CALL icefrac_lscp(klon,zt,iflag_ice_thermo,distcltop1D,temp_cltop1D,zfice, dzfice) |
---|
[3999] | 924 | |
---|
[4562] | 925 | |
---|
| 926 | ! Water vapor update, Phase determination and subsequent latent heat exchange |
---|
[3999] | 927 | DO i=1, klon |
---|
| 928 | |
---|
| 929 | IF (mpc_bl_points(i,k) .GT. 0) THEN |
---|
| 930 | zcond(i) = MAX(0.0,qincloud_mpc(i))*rneb(i,k) |
---|
| 931 | ! following line is very strange and probably wrong |
---|
| 932 | rhcl(i,k)= (zqs(i)+zq(i))/2./zqs(i) |
---|
| 933 | ! water vapor update and partition function if thermals |
---|
| 934 | zq(i) = zq(i) - zcond(i) |
---|
| 935 | zfice(i)=icefrac_mpc(i,k) |
---|
| 936 | |
---|
| 937 | ELSE |
---|
| 938 | |
---|
| 939 | ! Checks on rneb, rhcl and zqn |
---|
| 940 | IF (rneb(i,k) .LE. 0.0) THEN |
---|
| 941 | zqn(i) = 0.0 |
---|
| 942 | rneb(i,k) = 0.0 |
---|
| 943 | zcond(i) = 0.0 |
---|
| 944 | rhcl(i,k)=zq(i)/zqs(i) |
---|
| 945 | ELSE IF (rneb(i,k) .GE. 1.0) THEN |
---|
| 946 | zqn(i) = zq(i) |
---|
| 947 | rneb(i,k) = 1.0 |
---|
| 948 | zcond(i) = MAX(0.0,zqn(i)-gammasat(i)*zqs(i)) |
---|
| 949 | rhcl(i,k)=1.0 |
---|
| 950 | ELSE |
---|
| 951 | zcond(i) = MAX(0.0,zqn(i)-gammasat(i)*zqs(i))*rneb(i,k) |
---|
| 952 | ! following line is very strange and probably wrong: |
---|
| 953 | rhcl(i,k)=(zqs(i)+zq(i))/2./zqs(i) |
---|
| 954 | ENDIF |
---|
| 955 | |
---|
[4226] | 956 | ! water vapor update |
---|
| 957 | zq(i) = zq(i) - zcond(i) |
---|
[3999] | 958 | |
---|
| 959 | ENDIF |
---|
| 960 | |
---|
[4392] | 961 | ! c_iso : routine that computes in-cloud supersaturation |
---|
| 962 | ! c_iso condensation of isotopes (zcond, zsursat, zfice, zq in input) |
---|
| 963 | |
---|
[3999] | 964 | ! temperature update due to phase change |
---|
| 965 | zt(i) = zt(i) + (1.-zfice(i))*zcond(i) & |
---|
| 966 | & * RLVTT/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i)+zcond(i))) & |
---|
| 967 | +zfice(i)*zcond(i) * RLSTT/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i)+zcond(i))) |
---|
| 968 | ENDDO |
---|
| 969 | |
---|
| 970 | ! If vertical heterogeneity, change volume fraction |
---|
| 971 | IF (iflag_cloudth_vert .GE. 3) THEN |
---|
| 972 | ctot_vol(1:klon,k)=min(max(ctot_vol(1:klon,k),0.),1.) |
---|
| 973 | rneblsvol(1:klon,k)=ctot_vol(1:klon,k) |
---|
| 974 | ENDIF |
---|
| 975 | |
---|
| 976 | ! ---------------------------------------------------------------- |
---|
[4114] | 977 | ! P3> Precipitation formation |
---|
[3999] | 978 | ! ---------------------------------------------------------------- |
---|
[4226] | 979 | |
---|
[4803] | 980 | !================================================================ |
---|
| 981 | IF (ok_poprecip) THEN |
---|
| 982 | |
---|
| 983 | DO i = 1, klon |
---|
| 984 | zoliql(i) = zcond(i) * ( 1. - zfice(i) ) |
---|
| 985 | zoliqi(i) = zcond(i) * zfice(i) |
---|
| 986 | ENDDO |
---|
| 987 | |
---|
| 988 | CALL poprecip_postcld(klon, dtime, paprs(:,k), paprs(:,k+1), pplay(:,k), & |
---|
| 989 | ctot_vol(:,k), ptconv(:,k), & |
---|
| 990 | zt, zq, zoliql, zoliqi, zfice, & |
---|
| 991 | rneb(:,k), znebprecipclr, znebprecipcld, & |
---|
| 992 | zrfl, zrflclr, zrflcld, & |
---|
| 993 | zifl, ziflclr, ziflcld, & |
---|
| 994 | dqrauto(:,k),dqrcol(:,k),dqrmelt(:,k),dqrfreez(:,k), & |
---|
| 995 | dqsauto(:,k),dqsagg(:,k),dqsrim(:,k),dqsmelt(:,k),dqsfreez(:,k) & |
---|
| 996 | ) |
---|
| 997 | |
---|
| 998 | DO i = 1, klon |
---|
| 999 | zoliq(i) = zoliql(i) + zoliqi(i) |
---|
| 1000 | IF ( zoliq(i) .GT. 0. ) THEN |
---|
| 1001 | zfice(i) = zoliqi(i)/zoliq(i) |
---|
| 1002 | ELSE |
---|
| 1003 | zfice(i) = 0.0 |
---|
| 1004 | ENDIF |
---|
| 1005 | ! when poprecip activated, radiation does not see any precipitation content |
---|
| 1006 | radocond(i,k) = zoliq(i) |
---|
| 1007 | radocondl(i,k)= radocond(i,k)*(1.-zfice(i)) |
---|
| 1008 | radocondi(i,k)= radocond(i,k)*zfice(i) |
---|
| 1009 | ENDDO |
---|
| 1010 | |
---|
| 1011 | !================================================================ |
---|
| 1012 | ELSE |
---|
| 1013 | |
---|
[3999] | 1014 | ! LTP: |
---|
[4563] | 1015 | IF (iflag_evap_prec .GE. 4) THEN |
---|
[3999] | 1016 | |
---|
| 1017 | !Partitionning between precipitation coming from clouds and that coming from CS |
---|
| 1018 | |
---|
| 1019 | !0) Calculate tot_zneb, total cloud fraction above the cloud |
---|
| 1020 | !assuming a maximum-random overlap (voir Jakob and Klein, 2000) |
---|
| 1021 | |
---|
| 1022 | DO i=1, klon |
---|
[4424] | 1023 | tot_znebn(i) = 1. - (1.-tot_zneb(i))*(1 - max(rneb(i,k),zneb(i))) & |
---|
| 1024 | /(1.-min(zneb(i),1.-smallestreal)) |
---|
[3999] | 1025 | d_tot_zneb(i) = tot_znebn(i) - tot_zneb(i) |
---|
| 1026 | tot_zneb(i) = tot_znebn(i) |
---|
| 1027 | |
---|
| 1028 | |
---|
| 1029 | !1) Cloudy to clear air |
---|
| 1030 | d_znebprecip_cld_clr(i) = znebprecipcld(i) - min(rneb(i,k),znebprecipcld(i)) |
---|
[4424] | 1031 | IF (znebprecipcld(i) .GT. 0.) THEN |
---|
[3999] | 1032 | d_zrfl_cld_clr(i) = d_znebprecip_cld_clr(i)/znebprecipcld(i)*zrflcld(i) |
---|
| 1033 | d_zifl_cld_clr(i) = d_znebprecip_cld_clr(i)/znebprecipcld(i)*ziflcld(i) |
---|
| 1034 | ELSE |
---|
| 1035 | d_zrfl_cld_clr(i) = 0. |
---|
| 1036 | d_zifl_cld_clr(i) = 0. |
---|
| 1037 | ENDIF |
---|
| 1038 | |
---|
| 1039 | !2) Clear to cloudy air |
---|
[4226] | 1040 | d_znebprecip_clr_cld(i) = max(0., min(znebprecipclr(i), rneb(i,k) - d_tot_zneb(i) - zneb(i))) |
---|
[3999] | 1041 | IF (znebprecipclr(i) .GT. 0) THEN |
---|
| 1042 | d_zrfl_clr_cld(i) = d_znebprecip_clr_cld(i)/znebprecipclr(i)*zrflclr(i) |
---|
| 1043 | d_zifl_clr_cld(i) = d_znebprecip_clr_cld(i)/znebprecipclr(i)*ziflclr(i) |
---|
| 1044 | ELSE |
---|
| 1045 | d_zrfl_clr_cld(i) = 0. |
---|
| 1046 | d_zifl_clr_cld(i) = 0. |
---|
| 1047 | ENDIF |
---|
| 1048 | |
---|
| 1049 | !Update variables |
---|
[4226] | 1050 | znebprecipcld(i) = znebprecipcld(i) + d_znebprecip_clr_cld(i) - d_znebprecip_cld_clr(i) |
---|
[3999] | 1051 | znebprecipclr(i) = znebprecipclr(i) + d_znebprecip_cld_clr(i) - d_znebprecip_clr_cld(i) |
---|
| 1052 | zrflcld(i) = zrflcld(i) + d_zrfl_clr_cld(i) - d_zrfl_cld_clr(i) |
---|
| 1053 | ziflcld(i) = ziflcld(i) + d_zifl_clr_cld(i) - d_zifl_cld_clr(i) |
---|
| 1054 | zrflclr(i) = zrflclr(i) + d_zrfl_cld_clr(i) - d_zrfl_clr_cld(i) |
---|
| 1055 | ziflclr(i) = ziflclr(i) + d_zifl_cld_clr(i) - d_zifl_clr_cld(i) |
---|
| 1056 | |
---|
[4392] | 1057 | ! c_iso do the same thing for isotopes precip |
---|
[3999] | 1058 | ENDDO |
---|
| 1059 | ENDIF |
---|
| 1060 | |
---|
[4559] | 1061 | |
---|
| 1062 | ! Autoconversion |
---|
| 1063 | ! ------------------------------------------------------------------------------- |
---|
| 1064 | |
---|
| 1065 | |
---|
[4412] | 1066 | ! Initialisation of zoliq and radocond variables |
---|
[3999] | 1067 | |
---|
| 1068 | DO i = 1, klon |
---|
| 1069 | zoliq(i) = zcond(i) |
---|
[4072] | 1070 | zoliqi(i)= zoliq(i)*zfice(i) |
---|
| 1071 | zoliql(i)= zoliq(i)*(1.-zfice(i)) |
---|
[4392] | 1072 | ! c_iso : initialisation of zoliq* also for isotopes |
---|
[4114] | 1073 | zrho(i,k) = pplay(i,k) / zt(i) / RD |
---|
| 1074 | zdz(i) = (paprs(i,k)-paprs(i,k+1)) / (zrho(i,k)*RG) |
---|
[4072] | 1075 | iwc(i) = 0. |
---|
| 1076 | zneb(i) = MAX(rneb(i,k),seuil_neb) |
---|
[4559] | 1077 | radocond(i,k) = zoliq(i)/REAL(niter_lscp+1) |
---|
| 1078 | radocondi(i,k)=zoliq(i)*zfice(i)/REAL(niter_lscp+1) |
---|
| 1079 | radocondl(i,k)=zoliq(i)*(1.-zfice(i))/REAL(niter_lscp+1) |
---|
[3999] | 1080 | ENDDO |
---|
| 1081 | |
---|
[4559] | 1082 | |
---|
| 1083 | DO n = 1, niter_lscp |
---|
[3999] | 1084 | |
---|
| 1085 | DO i=1,klon |
---|
| 1086 | IF (rneb(i,k).GT.0.0) THEN |
---|
[4114] | 1087 | iwc(i) = zrho(i,k) * zoliqi(i) / zneb(i) ! in-cloud ice condensate content |
---|
[3999] | 1088 | ENDIF |
---|
| 1089 | ENDDO |
---|
| 1090 | |
---|
[4226] | 1091 | CALL fallice_velocity(klon,iwc(:),zt(:),zrho(:,k),pplay(:,k),ptconv(:,k),velo(:,k)) |
---|
[3999] | 1092 | |
---|
| 1093 | DO i = 1, klon |
---|
| 1094 | |
---|
| 1095 | IF (rneb(i,k).GT.0.0) THEN |
---|
| 1096 | |
---|
[4072] | 1097 | ! Initialization of zrain, zsnow and zprecip: |
---|
| 1098 | zrain=0. |
---|
| 1099 | zsnow=0. |
---|
| 1100 | zprecip=0. |
---|
[4392] | 1101 | ! c_iso same init for isotopes. Externalisation? |
---|
[3999] | 1102 | |
---|
| 1103 | IF (zneb(i).EQ.seuil_neb) THEN |
---|
[4072] | 1104 | zprecip = 0.0 |
---|
| 1105 | zsnow = 0.0 |
---|
| 1106 | zrain= 0.0 |
---|
[3999] | 1107 | ELSE |
---|
[4420] | 1108 | |
---|
[3999] | 1109 | IF (ptconv(i,k)) THEN ! if convective point |
---|
| 1110 | zcl=cld_lc_con |
---|
| 1111 | zct=1./cld_tau_con |
---|
[4559] | 1112 | zexpo=cld_expo_con |
---|
| 1113 | ffallv=ffallv_con |
---|
[3999] | 1114 | ELSE |
---|
| 1115 | zcl=cld_lc_lsc |
---|
| 1116 | zct=1./cld_tau_lsc |
---|
[4559] | 1117 | zexpo=cld_expo_lsc |
---|
| 1118 | ffallv=ffallv_lsc |
---|
[3999] | 1119 | ENDIF |
---|
| 1120 | |
---|
[4559] | 1121 | |
---|
[3999] | 1122 | ! if vertical heterogeneity is taken into account, we use |
---|
| 1123 | ! the "true" volume fraction instead of a modified |
---|
| 1124 | ! surface fraction (which is larger and artificially |
---|
| 1125 | ! reduces the in-cloud water). |
---|
[4072] | 1126 | |
---|
[4559] | 1127 | ! Liquid water quantity to remove: zchau (Sundqvist, 1978) |
---|
| 1128 | ! dqliq/dt=-qliq/tau*(1-exp(-qcin/clw)**2) |
---|
| 1129 | !......................................................... |
---|
[3999] | 1130 | IF ((iflag_cloudth_vert.GE.3).AND.(iflag_rain_incloud_vol.EQ.1)) THEN |
---|
| 1131 | |
---|
[4420] | 1132 | ! if vertical heterogeneity is taken into account, we use |
---|
| 1133 | ! the "true" volume fraction instead of a modified |
---|
| 1134 | ! surface fraction (which is larger and artificially |
---|
| 1135 | ! reduces the in-cloud water). |
---|
[4559] | 1136 | effective_zneb=ctot_vol(i,k) |
---|
| 1137 | ELSE |
---|
| 1138 | effective_zneb=zneb(i) |
---|
| 1139 | ENDIF |
---|
[4420] | 1140 | |
---|
| 1141 | |
---|
[4559] | 1142 | IF (iflag_autoconversion .EQ. 2) THEN |
---|
| 1143 | ! two-steps resolution with niter_lscp=1 sufficient |
---|
| 1144 | ! we first treat the second term (with exponential) in an explicit way |
---|
| 1145 | ! and then treat the first term (-q/tau) in an exact way |
---|
| 1146 | zchau=zoliql(i)*(1.-exp(-dtime/REAL(niter_lscp)*zct & |
---|
| 1147 | *(1.-exp(-(zoliql(i)/effective_zneb/zcl)**zexpo)))) |
---|
[4420] | 1148 | ELSE |
---|
[4559] | 1149 | ! old explicit resolution with subtimesteps |
---|
| 1150 | zchau = zct*dtime/REAL(niter_lscp)*zoliql(i) & |
---|
| 1151 | *(1.0-EXP(-(zoliql(i)/effective_zneb/zcl)**zexpo)) |
---|
[4420] | 1152 | ENDIF |
---|
| 1153 | |
---|
| 1154 | |
---|
[4559] | 1155 | ! Ice water quantity to remove (Zender & Kiehl, 1997) |
---|
| 1156 | ! dqice/dt=1/rho*d(rho*wice*qice)/dz |
---|
| 1157 | !.................................... |
---|
| 1158 | IF (iflag_autoconversion .EQ. 2) THEN |
---|
| 1159 | ! exact resolution, niter_lscp=1 is sufficient but works only |
---|
| 1160 | ! with iflag_vice=0 |
---|
| 1161 | IF (zoliqi(i) .GT. 0.) THEN |
---|
| 1162 | zfroi=(zoliqi(i)-((zoliqi(i)**(-dice_velo)) & |
---|
| 1163 | +dice_velo*dtime/REAL(niter_lscp)*cice_velo/zdz(i)*ffallv)**(-1./dice_velo)) |
---|
| 1164 | ELSE |
---|
| 1165 | zfroi=0. |
---|
| 1166 | ENDIF |
---|
| 1167 | ELSE |
---|
| 1168 | ! old explicit resolution with subtimesteps |
---|
| 1169 | zfroi = dtime/REAL(niter_lscp)/zdz(i)*zoliqi(i)*velo(i,k) |
---|
| 1170 | ENDIF |
---|
| 1171 | |
---|
[4397] | 1172 | zrain = MIN(MAX(zchau,0.0),zoliql(i)) |
---|
| 1173 | zsnow = MIN(MAX(zfroi,0.0),zoliqi(i)) |
---|
[4072] | 1174 | zprecip = MAX(zrain + zsnow,0.0) |
---|
[3999] | 1175 | |
---|
| 1176 | ENDIF |
---|
[4226] | 1177 | |
---|
[4559] | 1178 | IF (iflag_autoconversion .GE. 1) THEN |
---|
| 1179 | ! debugged version with phase conservation through the autoconversion process |
---|
| 1180 | zoliql(i) = MAX(zoliql(i)-1.*zrain , 0.0) |
---|
| 1181 | zoliqi(i) = MAX(zoliqi(i)-1.*zsnow , 0.0) |
---|
| 1182 | zoliq(i) = MAX(zoliq(i)-zprecip , 0.0) |
---|
| 1183 | ELSE |
---|
| 1184 | ! bugged version with phase resetting |
---|
| 1185 | zoliql(i) = MAX(zoliq(i)*(1.-zfice(i))-1.*zrain , 0.0) |
---|
| 1186 | zoliqi(i) = MAX(zoliq(i)*zfice(i)-1.*zsnow , 0.0) |
---|
| 1187 | zoliq(i) = MAX(zoliq(i)-zprecip , 0.0) |
---|
| 1188 | ENDIF |
---|
[3999] | 1189 | |
---|
[4392] | 1190 | ! c_iso: call isotope_conversion (for readibility) or duplicate |
---|
| 1191 | |
---|
[4559] | 1192 | radocond(i,k) = radocond(i,k) + zoliq(i)/REAL(niter_lscp+1) |
---|
| 1193 | radocondl(i,k) = radocondl(i,k) + zoliql(i)/REAL(niter_lscp+1) |
---|
| 1194 | radocondi(i,k) = radocondi(i,k) + zoliqi(i)/REAL(niter_lscp+1) |
---|
[4226] | 1195 | |
---|
[4072] | 1196 | ENDIF ! rneb >0 |
---|
[3999] | 1197 | |
---|
| 1198 | ENDDO ! i = 1,klon |
---|
| 1199 | |
---|
| 1200 | ENDDO ! n = 1,niter |
---|
| 1201 | |
---|
[4072] | 1202 | ! Precipitation flux calculation |
---|
[3999] | 1203 | |
---|
| 1204 | DO i = 1, klon |
---|
[4380] | 1205 | |
---|
[4563] | 1206 | IF (iflag_evap_prec.GE.4) THEN |
---|
[4380] | 1207 | ziflprev(i)=ziflcld(i) |
---|
| 1208 | ELSE |
---|
| 1209 | ziflprev(i)=zifl(i)*zneb(i) |
---|
| 1210 | ENDIF |
---|
[3999] | 1211 | |
---|
| 1212 | IF (rneb(i,k) .GT. 0.0) THEN |
---|
| 1213 | |
---|
[4072] | 1214 | ! CR&JYG: We account for the Wegener-Findeisen-Bergeron process in the precipitation flux: |
---|
| 1215 | ! If T<0C, liquid precip are converted into ice, which leads to an increase in |
---|
| 1216 | ! temperature DeltaT. The effect of DeltaT on condensates and precipitation is roughly |
---|
| 1217 | ! taken into account through a linearization of the equations and by approximating |
---|
| 1218 | ! the liquid precipitation process with a "threshold" process. We assume that |
---|
| 1219 | ! condensates are not modified during this operation. Liquid precipitation is |
---|
| 1220 | ! removed (in the limit DeltaT<273.15-T). Solid precipitation increases. |
---|
| 1221 | ! Water vapor increases as well |
---|
| 1222 | ! Note that compared to fisrtilp, we always assume iflag_bergeron=2 |
---|
| 1223 | |
---|
| 1224 | zqpreci(i)=(zcond(i)-zoliq(i))*zfice(i) |
---|
| 1225 | zqprecl(i)=(zcond(i)-zoliq(i))*(1.-zfice(i)) |
---|
| 1226 | zcp=RCPD*(1.0+RVTMP2*(zq(i)+zmqc(i)+zcond(i))) |
---|
| 1227 | coef1 = rneb(i,k)*RLSTT/zcp*zdqsdT_raw(i) |
---|
| 1228 | ! Computation of DT if all the liquid precip freezes |
---|
| 1229 | DeltaT = RLMLT*zqprecl(i) / (zcp*(1.+coef1)) |
---|
| 1230 | ! T should not exceed the freezing point |
---|
| 1231 | ! that is Delta > RTT-zt(i) |
---|
| 1232 | DeltaT = max( min( RTT-zt(i), DeltaT) , 0. ) |
---|
| 1233 | zt(i) = zt(i) + DeltaT |
---|
| 1234 | ! water vaporization due to temp. increase |
---|
| 1235 | Deltaq = rneb(i,k)*zdqsdT_raw(i)*DeltaT |
---|
| 1236 | ! we add this vaporized water to the total vapor and we remove it from the precip |
---|
| 1237 | zq(i) = zq(i) + Deltaq |
---|
| 1238 | ! The three "max" lines herebelow protect from rounding errors |
---|
| 1239 | zcond(i) = max( zcond(i)- Deltaq, 0. ) |
---|
| 1240 | ! liquid precipitation converted to ice precip |
---|
| 1241 | Deltaqprecl = -zcp/RLMLT*(1.+coef1)*DeltaT |
---|
| 1242 | zqprecl(i) = max( zqprecl(i) + Deltaqprecl, 0. ) |
---|
| 1243 | ! iced water budget |
---|
| 1244 | zqpreci(i) = max (zqpreci(i) - Deltaqprecl - Deltaq, 0.) |
---|
[4226] | 1245 | |
---|
[4392] | 1246 | ! c_iso : mv here condensation of isotopes + redispatchage en precip |
---|
| 1247 | |
---|
[4563] | 1248 | IF (iflag_evap_prec.GE.4) THEN |
---|
[4226] | 1249 | zrflcld(i) = zrflcld(i)+zqprecl(i) & |
---|
| 1250 | *(paprs(i,k)-paprs(i,k+1))/(RG*dtime) |
---|
| 1251 | ziflcld(i) = ziflcld(i)+ zqpreci(i) & |
---|
| 1252 | *(paprs(i,k)-paprs(i,k+1))/(RG*dtime) |
---|
| 1253 | znebprecipcld(i) = rneb(i,k) |
---|
| 1254 | zrfl(i) = zrflcld(i) + zrflclr(i) |
---|
| 1255 | zifl(i) = ziflcld(i) + ziflclr(i) |
---|
| 1256 | ELSE |
---|
[3999] | 1257 | zrfl(i) = zrfl(i)+ zqprecl(i) & |
---|
| 1258 | *(paprs(i,k)-paprs(i,k+1))/(RG*dtime) |
---|
| 1259 | zifl(i) = zifl(i)+ zqpreci(i) & |
---|
[4226] | 1260 | *(paprs(i,k)-paprs(i,k+1))/(RG*dtime) |
---|
[3999] | 1261 | ENDIF |
---|
[4392] | 1262 | ! c_iso : same for isotopes |
---|
[3999] | 1263 | |
---|
| 1264 | ENDIF ! rneb>0 |
---|
| 1265 | |
---|
| 1266 | ENDDO |
---|
| 1267 | |
---|
[4226] | 1268 | ! LTP: limit of surface cloud fraction covered by precipitation when the local intensity of the flux is below rain_int_min |
---|
[4563] | 1269 | ! if iflag_evap_prec>=4 |
---|
| 1270 | IF (iflag_evap_prec.GE.4) THEN |
---|
[4114] | 1271 | |
---|
[4226] | 1272 | DO i=1,klon |
---|
[4114] | 1273 | |
---|
[4226] | 1274 | IF ((zrflclr(i) + ziflclr(i)) .GT. 0. ) THEN |
---|
[3999] | 1275 | znebprecipclr(i) = min(znebprecipclr(i),max(zrflclr(i)/ & |
---|
| 1276 | (MAX(znebprecipclr(i),seuil_neb)*rain_int_min), ziflclr(i)/(MAX(znebprecipclr(i),seuil_neb)*rain_int_min))) |
---|
| 1277 | ELSE |
---|
[4226] | 1278 | znebprecipclr(i)=0.0 |
---|
| 1279 | ENDIF |
---|
| 1280 | |
---|
| 1281 | IF ((zrflcld(i) + ziflcld(i)) .GT. 0.) THEN |
---|
[3999] | 1282 | znebprecipcld(i) = min(znebprecipcld(i), max(zrflcld(i)/ & |
---|
| 1283 | (MAX(znebprecipcld(i),seuil_neb)*rain_int_min), ziflcld(i)/(MAX(znebprecipcld(i),seuil_neb)*rain_int_min))) |
---|
[4226] | 1284 | ELSE |
---|
| 1285 | znebprecipcld(i)=0.0 |
---|
| 1286 | ENDIF |
---|
[3999] | 1287 | |
---|
[4226] | 1288 | ENDDO |
---|
[3999] | 1289 | |
---|
[4226] | 1290 | ENDIF |
---|
[3999] | 1291 | |
---|
[4803] | 1292 | ENDIF ! ok_poprecip |
---|
| 1293 | |
---|
[3999] | 1294 | ! End of precipitation formation |
---|
| 1295 | ! -------------------------------- |
---|
| 1296 | |
---|
| 1297 | |
---|
[4803] | 1298 | ! Calculation of cloud condensates amount seen by radiative scheme |
---|
| 1299 | !----------------------------------------------------------------- |
---|
| 1300 | |
---|
[4114] | 1301 | ! Calculation of the concentration of condensates seen by the radiation scheme |
---|
[4412] | 1302 | ! for liquid phase, we take radocondl |
---|
| 1303 | ! for ice phase, we take radocondi if we neglect snowfall, otherwise (ok_radocond_snow=true) |
---|
[4803] | 1304 | ! we recalculate radocondi to account for contributions from the precipitation flux |
---|
| 1305 | ! TODO: for the moment, we deactivate this option when ok_poprecip=.true. |
---|
[3999] | 1306 | |
---|
[4803] | 1307 | IF ((ok_radocond_snow) .AND. (k .LT. klev) .AND. (.NOT. ok_poprecip)) THEN |
---|
[4114] | 1308 | ! for the solid phase (crystals + snowflakes) |
---|
[4412] | 1309 | ! we recalculate radocondi by summing |
---|
[4114] | 1310 | ! the ice content calculated in the mesh |
---|
| 1311 | ! + the contribution of the non-evaporated snowfall |
---|
| 1312 | ! from the overlying layer |
---|
| 1313 | DO i=1,klon |
---|
| 1314 | IF (ziflprev(i) .NE. 0.0) THEN |
---|
[4412] | 1315 | radocondi(i,k)=zoliq(i)*zfice(i)+zqpreci(i)+ziflprev(i)/zrho(i,k+1)/velo(i,k+1) |
---|
[4114] | 1316 | ELSE |
---|
[4412] | 1317 | radocondi(i,k)=zoliq(i)*zfice(i)+zqpreci(i) |
---|
[4114] | 1318 | ENDIF |
---|
[4412] | 1319 | radocond(i,k)=radocondl(i,k)+radocondi(i,k) |
---|
[4114] | 1320 | ENDDO |
---|
| 1321 | ENDIF |
---|
| 1322 | |
---|
[4412] | 1323 | ! caculate the percentage of ice in "radocond" so cloud+precip seen by the radiation scheme |
---|
[4114] | 1324 | DO i=1,klon |
---|
[4412] | 1325 | IF (radocond(i,k) .GT. 0.) THEN |
---|
| 1326 | radicefrac(i,k)=MIN(MAX(radocondi(i,k)/radocond(i,k),0.),1.) |
---|
[4114] | 1327 | ENDIF |
---|
| 1328 | ENDDO |
---|
| 1329 | |
---|
[3999] | 1330 | ! ---------------------------------------------------------------- |
---|
| 1331 | ! P4> Wet scavenging |
---|
| 1332 | ! ---------------------------------------------------------------- |
---|
| 1333 | |
---|
| 1334 | !Scavenging through nucleation in the layer |
---|
| 1335 | |
---|
| 1336 | DO i = 1,klon |
---|
| 1337 | |
---|
| 1338 | IF(zcond(i).GT.zoliq(i)+1.e-10) THEN |
---|
| 1339 | beta(i,k) = (zcond(i)-zoliq(i))/zcond(i)/dtime |
---|
| 1340 | ELSE |
---|
| 1341 | beta(i,k) = 0. |
---|
| 1342 | ENDIF |
---|
| 1343 | |
---|
[4059] | 1344 | zprec_cond(i) = MAX(zcond(i)-zoliq(i),0.0)*(paprs(i,k)-paprs(i,k+1))/RG |
---|
[3999] | 1345 | |
---|
| 1346 | IF (rneb(i,k).GT.0.0.AND.zprec_cond(i).GT.0.) THEN |
---|
| 1347 | |
---|
[4654] | 1348 | IF (temp(i,k) .GE. t_glace_min) THEN |
---|
[3999] | 1349 | zalpha_tr = a_tr_sca(3) |
---|
| 1350 | ELSE |
---|
| 1351 | zalpha_tr = a_tr_sca(4) |
---|
| 1352 | ENDIF |
---|
| 1353 | |
---|
| 1354 | zfrac_lessi = 1. - EXP(zalpha_tr*zprec_cond(i)/zneb(i)) |
---|
| 1355 | frac_nucl(i,k)= 1.-zneb(i)*zfrac_lessi |
---|
[4226] | 1356 | |
---|
[3999] | 1357 | ! Nucleation with a factor of -1 instead of -0.5 |
---|
| 1358 | zfrac_lessi = 1. - EXP(-zprec_cond(i)/zneb(i)) |
---|
| 1359 | |
---|
| 1360 | ENDIF |
---|
| 1361 | |
---|
[4226] | 1362 | ENDDO |
---|
| 1363 | |
---|
[3999] | 1364 | ! Scavenging through impaction in the underlying layer |
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| 1365 | |
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| 1366 | DO kk = k-1, 1, -1 |
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| 1367 | |
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| 1368 | DO i = 1, klon |
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| 1369 | |
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| 1370 | IF (rneb(i,k).GT.0.0.AND.zprec_cond(i).GT.0.) THEN |
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| 1371 | |
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[4654] | 1372 | IF (temp(i,kk) .GE. t_glace_min) THEN |
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[3999] | 1373 | zalpha_tr = a_tr_sca(1) |
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| 1374 | ELSE |
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| 1375 | zalpha_tr = a_tr_sca(2) |
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| 1376 | ENDIF |
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| 1377 | |
---|
| 1378 | zfrac_lessi = 1. - EXP(zalpha_tr*zprec_cond(i)/zneb(i)) |
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| 1379 | frac_impa(i,kk)= 1.-zneb(i)*zfrac_lessi |
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| 1380 | |
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| 1381 | ENDIF |
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| 1382 | |
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| 1383 | ENDDO |
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| 1384 | |
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| 1385 | ENDDO |
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[4226] | 1386 | |
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[4072] | 1387 | !--save some variables for ice supersaturation |
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[4059] | 1388 | ! |
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| 1389 | DO i = 1, klon |
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[4072] | 1390 | ! for memory |
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[4059] | 1391 | rneb_seri(i,k) = rneb(i,k) |
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[3999] | 1392 | |
---|
[4072] | 1393 | ! for diagnostics |
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[4059] | 1394 | rnebclr(i,k) = 1.0 - rneb(i,k) - rnebss(i,k) |
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[3999] | 1395 | |
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[4059] | 1396 | qvc(i,k) = zqs(i) * rneb(i,k) |
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[4072] | 1397 | qclr(i,k) = MAX(1.e-10,zq(i) - qvc(i,k) - qss(i,k)) !--added by OB because of pathologic cases with the lognormal |
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[4059] | 1398 | qcld(i,k) = qvc(i,k) + zcond(i) |
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[4226] | 1399 | ENDDO |
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[4072] | 1400 | !q_sat |
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[4380] | 1401 | CALL calc_qsat_ecmwf(klon,Tbef(:),qzero(:),pplay(:,k),RTT,1,.false.,qsatl(:,k),zdqs(:)) |
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| 1402 | CALL calc_qsat_ecmwf(klon,Tbef(:),qzero(:),pplay(:,k),RTT,2,.false.,qsats(:,k),zdqs(:)) |
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[4059] | 1403 | |
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[4803] | 1404 | |
---|
| 1405 | |
---|
| 1406 | ! Outputs: |
---|
| 1407 | !------------------------------- |
---|
| 1408 | ! Precipitation fluxes at layer interfaces |
---|
| 1409 | ! + precipitation fractions + |
---|
| 1410 | ! temperature and water species tendencies |
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| 1411 | DO i = 1, klon |
---|
| 1412 | psfl(i,k)=zifl(i) |
---|
| 1413 | prfl(i,k)=zrfl(i) |
---|
| 1414 | pfraclr(i,k)=znebprecipclr(i) |
---|
| 1415 | pfracld(i,k)=znebprecipcld(i) |
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| 1416 | d_ql(i,k) = (1-zfice(i))*zoliq(i) |
---|
| 1417 | d_qi(i,k) = zfice(i)*zoliq(i) |
---|
| 1418 | d_q(i,k) = zq(i) - qt(i,k) |
---|
| 1419 | ! c_iso: same for isotopes |
---|
| 1420 | d_t(i,k) = zt(i) - temp(i,k) |
---|
| 1421 | ENDDO |
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| 1422 | |
---|
| 1423 | |
---|
[4226] | 1424 | ENDDO |
---|
[4059] | 1425 | |
---|
[3999] | 1426 | |
---|
| 1427 | ! Rain or snow at the surface (depending on the first layer temperature) |
---|
| 1428 | DO i = 1, klon |
---|
| 1429 | snow(i) = zifl(i) |
---|
| 1430 | rain(i) = zrfl(i) |
---|
[4392] | 1431 | ! c_iso final output |
---|
[3999] | 1432 | ENDDO |
---|
| 1433 | |
---|
| 1434 | IF (ncoreczq>0) THEN |
---|
| 1435 | WRITE(lunout,*)'WARNING : ZQ in LSCP ',ncoreczq,' val < 1.e-15.' |
---|
| 1436 | ENDIF |
---|
| 1437 | |
---|
[4654] | 1438 | |
---|
| 1439 | RETURN |
---|
| 1440 | |
---|
[4380] | 1441 | END SUBROUTINE lscp |
---|
[3999] | 1442 | !+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
---|
| 1443 | |
---|
[4664] | 1444 | END MODULE lmdz_lscp |
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