| 1 | MODULE lmdz_lscp |
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| 2 | |
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| 3 | IMPLICIT NONE |
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| 4 | |
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| 5 | CONTAINS |
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| 6 | |
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| 7 | !++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
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| 8 | SUBROUTINE lscp(klon,klev,dtime,missing_val, & |
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| 9 | paprs,pplay,temp,qt,ptconv,ratqs, & |
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| 10 | d_t, d_q, d_ql, d_qi, rneb, rneblsvol, & |
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| 11 | pfraclr,pfracld, & |
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| 12 | radocond, radicefrac, rain, snow, & |
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| 13 | frac_impa, frac_nucl, beta, & |
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| 14 | prfl, psfl, rhcl, qta, fraca, & |
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| 15 | tv, pspsk, tla, thl, iflag_cld_th, & |
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| 16 | iflag_ice_thermo, distcltop, temp_cltop, cell_area,& |
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| 17 | cf_seri, rvc_seri, u_seri, v_seri, pbl_eps, & |
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| 18 | qsub, qissr, qcld, subfra, issrfra, gamma_cond, & |
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| 19 | ratio_qi_qtot, dcf_sub, dcf_con, dcf_mix, & |
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| 20 | dqi_adj, dqi_sub, dqi_con, dqi_mix, dqvc_adj, & |
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| 21 | dqvc_sub, dqvc_con, dqvc_mix, qsatl, qsati, & |
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| 22 | Tcontr, qcontr, qcontr2, fcontrN, fcontrP, dcf_avi,& |
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| 23 | dqi_avi, dqvc_avi, flight_dist, flight_h2o, & |
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| 24 | cloudth_sth,cloudth_senv,cloudth_sigmath,cloudth_sigmaenv, & |
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| 25 | qraindiag, qsnowdiag, dqreva, dqssub, dqrauto, & |
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| 26 | dqrcol, dqrmelt, dqrfreez, dqsauto, dqsagg, dqsrim,& |
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| 27 | dqsmelt, dqsfreez) |
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| 28 | |
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| 29 | !++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
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| 30 | ! Authors: Z.X. Li (LMD), J-L Dufresne (LMD), C. Rio (LMD), J-Y Grandpeix (LMD) |
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| 31 | ! A. JAM (LMD), J-B Madeleine (LMD), E. Vignon (LMD), L. Touzze-Peiffert (LMD) |
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| 32 | !-------------------------------------------------------------------------------- |
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| 33 | ! Date: 01/2021 |
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| 34 | !-------------------------------------------------------------------------------- |
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| 35 | ! Aim: Large Scale Clouds and Precipitation (LSCP) |
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| 36 | ! |
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| 37 | ! This code is a new version of the fisrtilp.F90 routine, which is itself a |
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| 38 | ! merge of 'first' (superrsaturation physics, P. LeVan K. Laval) |
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| 39 | ! and 'ilp' (il pleut, L. Li) |
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| 40 | ! |
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| 41 | ! Compared to the original fisrtilp code, lscp |
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| 42 | ! -> assumes thermcep = .TRUE. all the time (fisrtilp inconsistent when .FALSE.) |
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| 43 | ! -> consider always precipitation thermalisation (fl_cor_ebil>0) |
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| 44 | ! -> option iflag_fisrtilp_qsat<0 no longer possible (qsat does not evolve with T) |
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| 45 | ! -> option "oldbug" by JYG has been removed |
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| 46 | ! -> iflag_t_glace >0 always |
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| 47 | ! -> the 'all or nothing' cloud approach is no longer available (cpartiel=T always) |
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| 48 | ! -> rectangular distribution from L. Li no longer available |
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| 49 | ! -> We always account for the Wegener-Findeisen-Bergeron process (iflag_bergeron = 2 in fisrt) |
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| 50 | !-------------------------------------------------------------------------------- |
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| 51 | ! References: |
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| 52 | ! |
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| 53 | ! - Bony, S., & Emanuel, K. A. 2001, JAS, doi: 10.1175/1520-0469(2001)058<3158:APOTCA>2.0.CO;2 |
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| 54 | ! - Hourdin et al. 2013, Clim Dyn, doi:10.1007/s00382-012-1343-y |
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| 55 | ! - Jam et al. 2013, Boundary-Layer Meteorol, doi:10.1007/s10546-012-9789-3 |
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| 56 | ! - Jouhaud, et al. 2018. JAMES, doi:10.1029/2018MS001379 |
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| 57 | ! - Madeleine et al. 2020, JAMES, doi:10.1029/2020MS002046 |
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| 58 | ! - Touzze-Peifert Ludo, PhD thesis, p117-124 |
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| 59 | ! ------------------------------------------------------------------------------- |
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| 60 | ! Code structure: |
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| 61 | ! |
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| 62 | ! P0> Thermalization of the precipitation coming from the overlying layer |
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| 63 | ! P1> Evaporation of the precipitation (falling from the k+1 level) |
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| 64 | ! P2> Cloud formation (at the k level) |
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| 65 | ! P2.A.1> With the PDFs, calculation of cloud properties using the inital |
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| 66 | ! values of T and Q |
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| 67 | ! P2.A.2> Coupling between condensed water and temperature |
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| 68 | ! P2.A.3> Calculation of final quantities associated with cloud formation |
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| 69 | ! P2.B> Release of Latent heat after cloud formation |
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| 70 | ! P3> Autoconversion to precipitation (k-level) |
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| 71 | ! P4> Wet scavenging |
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| 72 | !------------------------------------------------------------------------------ |
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| 73 | ! Some preliminary comments (JBM) : |
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| 74 | ! |
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| 75 | ! The cloud water that the radiation scheme sees is not the same that the cloud |
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| 76 | ! water used in the physics and the dynamics |
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| 77 | ! |
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| 78 | ! During the autoconversion to precipitation (P3 step), radocond (cloud water used |
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| 79 | ! by the radiation scheme) is calculated as an average of the water that remains |
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| 80 | ! in the cloud during the precipitation and not the water remaining at the end |
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| 81 | ! of the time step. The latter is used in the rest of the physics and advected |
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| 82 | ! by the dynamics. |
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| 83 | ! |
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| 84 | ! In summary: |
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| 85 | ! |
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| 86 | ! Radiation: |
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| 87 | ! xflwc(newmicro)+xfiwc(newmicro) = |
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| 88 | ! radocond=lwcon(nc)+iwcon(nc) |
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| 89 | ! |
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| 90 | ! Notetheless, be aware of: |
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| 91 | ! |
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| 92 | ! radocond .NE. ocond(nc) |
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| 93 | ! i.e.: |
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| 94 | ! lwcon(nc)+iwcon(nc) .NE. ocond(nc) |
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| 95 | ! but oliq+(ocond-oliq) .EQ. ocond |
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| 96 | ! (which is not trivial) |
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| 97 | !++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
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| 98 | ! |
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| 99 | |
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| 100 | ! USE de modules contenant des fonctions. |
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| 101 | USE lmdz_cloudth, ONLY : cloudth, cloudth_v3, cloudth_v6, cloudth_mpc |
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| 102 | USE lmdz_lscp_tools, ONLY : calc_qsat_ecmwf, icefrac_lscp, calc_gammasat |
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| 103 | USE lmdz_lscp_tools, ONLY : fallice_velocity, distance_to_cloud_top |
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| 104 | USE lmdz_lscp_condensation, ONLY : condensation_lognormal, condensation_ice_supersat |
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| 105 | USE lmdz_lscp_poprecip, ONLY : poprecip_precld, poprecip_postcld |
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| 106 | |
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| 107 | ! Use du module lmdz_lscp_ini contenant les constantes |
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| 108 | USE lmdz_lscp_ini, ONLY : prt_level, lunout, eps |
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| 109 | USE lmdz_lscp_ini, ONLY : seuil_neb, niter_lscp, iflag_evap_prec, t_coup, DDT0, ztfondue, rain_int_min |
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| 110 | USE lmdz_lscp_ini, ONLY : ok_radocond_snow, a_tr_sca, cld_expo_con, cld_expo_lsc |
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| 111 | USE lmdz_lscp_ini, ONLY : iflag_cloudth_vert, iflag_rain_incloud_vol, iflag_t_glace, t_glace_min |
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| 112 | USE lmdz_lscp_ini, ONLY : coef_eva, coef_sub,cld_tau_lsc, cld_tau_con, cld_lc_lsc, cld_lc_con |
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| 113 | USE lmdz_lscp_ini, ONLY : iflag_bergeron, iflag_fisrtilp_qsat, iflag_vice, cice_velo, dice_velo |
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| 114 | USE lmdz_lscp_ini, ONLY : iflag_autoconversion, ffallv_con, ffallv_lsc, min_frac_th_cld |
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| 115 | USE lmdz_lscp_ini, ONLY : RCPD, RLSTT, RLVTT, RLMLT, RVTMP2, RTT, RD, RG |
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| 116 | USE lmdz_lscp_ini, ONLY : ok_poprecip |
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| 117 | USE lmdz_lscp_ini, ONLY : ok_external_lognormal, ok_ice_supersat, ok_unadjusted_clouds |
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| 118 | |
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| 119 | IMPLICIT NONE |
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| 120 | |
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| 121 | !=============================================================================== |
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| 122 | ! VARIABLES DECLARATION |
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| 123 | !=============================================================================== |
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| 124 | |
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| 125 | ! INPUT VARIABLES: |
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| 126 | !----------------- |
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| 127 | |
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| 128 | INTEGER, INTENT(IN) :: klon,klev ! number of horizontal grid points and vertical levels |
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| 129 | REAL, INTENT(IN) :: dtime ! time step [s] |
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| 130 | REAL, INTENT(IN) :: missing_val ! missing value for output |
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| 131 | |
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| 132 | REAL, DIMENSION(klon,klev+1), INTENT(IN) :: paprs ! inter-layer pressure [Pa] |
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| 133 | REAL, DIMENSION(klon,klev), INTENT(IN) :: pplay ! mid-layer pressure [Pa] |
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| 134 | REAL, DIMENSION(klon,klev), INTENT(IN) :: temp ! temperature (K) |
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| 135 | REAL, DIMENSION(klon,klev), INTENT(IN) :: qt ! total specific humidity (in vapor phase in input) [kg/kg] |
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| 136 | INTEGER, INTENT(IN) :: iflag_cld_th ! flag that determines the distribution of convective clouds |
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| 137 | INTEGER, INTENT(IN) :: iflag_ice_thermo! flag to activate the ice thermodynamics |
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| 138 | ! CR: if iflag_ice_thermo=2, only convection is active |
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| 139 | LOGICAL, DIMENSION(klon,klev), INTENT(IN) :: ptconv ! grid points where deep convection scheme is active |
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| 140 | |
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| 141 | !Inputs associated with thermal plumes |
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| 142 | |
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| 143 | REAL, DIMENSION(klon,klev), INTENT(IN) :: tv ! virtual potential temperature [K] |
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| 144 | REAL, DIMENSION(klon,klev), INTENT(IN) :: qta ! specific humidity within thermals [kg/kg] |
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| 145 | REAL, DIMENSION(klon,klev), INTENT(IN) :: fraca ! fraction of thermals within the mesh [-] |
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| 146 | REAL, DIMENSION(klon,klev), INTENT(IN) :: pspsk ! exner potential (p/100000)**(R/cp) |
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| 147 | REAL, DIMENSION(klon,klev), INTENT(IN) :: tla ! liquid temperature within thermals [K] |
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| 148 | |
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| 149 | ! INPUT/OUTPUT variables |
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| 150 | !------------------------ |
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| 151 | |
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| 152 | REAL, DIMENSION(klon,klev), INTENT(INOUT) :: thl ! liquid potential temperature [K] |
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| 153 | REAL, DIMENSION(klon,klev), INTENT(INOUT) :: ratqs ! function of pressure that sets the large-scale |
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| 154 | |
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| 155 | ! INPUT/OUTPUT condensation and ice supersaturation |
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| 156 | !-------------------------------------------------- |
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| 157 | REAL, DIMENSION(klon,klev), INTENT(INOUT):: cf_seri ! cloud fraction [-] |
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| 158 | REAL, DIMENSION(klon,klev), INTENT(INOUT):: ratio_qi_qtot ! solid specific water to total specific water ratio [-] |
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| 159 | REAL, DIMENSION(klon,klev), INTENT(INOUT):: rvc_seri ! cloudy water vapor to total water vapor ratio [-] |
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| 160 | REAL, DIMENSION(klon,klev), INTENT(IN) :: u_seri ! eastward wind [m/s] |
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| 161 | REAL, DIMENSION(klon,klev), INTENT(IN) :: v_seri ! northward wind [m/s] |
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| 162 | REAL, DIMENSION(klon,klev+1), INTENT(IN) :: pbl_eps ! TKE dissipation [?] |
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| 163 | REAL, DIMENSION(klon), INTENT(IN) :: cell_area ! area of each cell [m2] |
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| 164 | |
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| 165 | ! INPUT/OUTPUT aviation |
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| 166 | !-------------------------------------------------- |
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| 167 | REAL, DIMENSION(klon,klev), INTENT(IN) :: flight_dist ! Aviation distance flown within the mesh [m/s/mesh] |
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| 168 | REAL, DIMENSION(klon,klev), INTENT(IN) :: flight_h2o ! Aviation H2O emitted within the mesh [kg H2O/s/mesh] |
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| 169 | |
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| 170 | ! OUTPUT variables |
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| 171 | !----------------- |
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| 172 | |
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| 173 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: d_t ! temperature increment [K] |
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| 174 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: d_q ! specific humidity increment [kg/kg] |
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| 175 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: d_ql ! liquid water increment [kg/kg] |
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| 176 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: d_qi ! cloud ice mass increment [kg/kg] |
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| 177 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: rneb ! cloud fraction [-] |
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| 178 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: rneblsvol ! cloud fraction per unit volume [-] |
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| 179 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: pfraclr ! precip fraction clear-sky part [-] |
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| 180 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: pfracld ! precip fraction cloudy part [-] |
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| 181 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: radocond ! condensed water used in the radiation scheme [kg/kg] |
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| 182 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: radicefrac ! ice fraction of condensed water for radiation scheme |
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| 183 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: rhcl ! clear-sky relative humidity [-] |
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| 184 | REAL, DIMENSION(klon), INTENT(OUT) :: rain ! surface large-scale rainfall [kg/s/m2] |
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| 185 | REAL, DIMENSION(klon), INTENT(OUT) :: snow ! surface large-scale snowfall [kg/s/m2] |
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| 186 | REAL, DIMENSION(klon,klev+1), INTENT(OUT) :: prfl ! large-scale rainfall flux in the column [kg/s/m2] |
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| 187 | REAL, DIMENSION(klon,klev+1), INTENT(OUT) :: psfl ! large-scale snowfall flux in the column [kg/s/m2] |
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| 188 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: distcltop ! distance to cloud top [m] |
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| 189 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: temp_cltop ! temperature of cloud top [K] |
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| 190 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: beta ! conversion rate of condensed water |
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| 191 | |
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| 192 | ! fraction of aerosol scavenging through impaction and nucleation (for on-line) |
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| 193 | |
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| 194 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: frac_impa ! scavenging fraction due tu impaction [-] |
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| 195 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: frac_nucl ! scavenging fraction due tu nucleation [-] |
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| 196 | |
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| 197 | ! for condensation and ice supersaturation |
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| 198 | |
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| 199 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qsub !--specific total water content in sub-saturated clear sky region [kg/kg] |
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| 200 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qissr !--specific total water content in supersat region [kg/kg] |
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| 201 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qcld !--specific total water content in cloudy region [kg/kg] |
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| 202 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: subfra !--mesh fraction of subsaturated clear sky [-] |
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| 203 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: issrfra !--mesh fraction of ISSR [-] |
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| 204 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: gamma_cond !--coefficient governing the ice nucleation RHi threshold [-] |
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| 205 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dcf_sub !--cloud fraction tendency because of sublimation [s-1] |
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| 206 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dcf_con !--cloud fraction tendency because of condensation [s-1] |
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| 207 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dcf_mix !--cloud fraction tendency because of cloud mixing [s-1] |
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| 208 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqi_adj !--specific ice content tendency because of temperature adjustment [kg/kg/s] |
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| 209 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqi_sub !--specific ice content tendency because of sublimation [kg/kg/s] |
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| 210 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqi_con !--specific ice content tendency because of condensation [kg/kg/s] |
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| 211 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqi_mix !--specific ice content tendency because of cloud mixing [kg/kg/s] |
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| 212 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqvc_adj !--specific cloud water vapor tendency because of temperature adjustment [kg/kg/s] |
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| 213 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqvc_sub !--specific cloud water vapor tendency because of sublimation [kg/kg/s] |
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| 214 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqvc_con !--specific cloud water vapor tendency because of condensation [kg/kg/s] |
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| 215 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqvc_mix !--specific cloud water vapor tendency because of cloud mixing [kg/kg/s] |
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| 216 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qsatl !--saturation specific humidity wrt liquid [kg/kg] |
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| 217 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qsati !--saturation specific humidity wrt ice [kg/kg] |
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| 218 | |
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| 219 | ! for contrails and aviation |
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| 220 | |
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| 221 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: Tcontr !--threshold temperature for contrail formation [K] |
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| 222 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qcontr !--threshold humidity for contrail formation [kg/kg] |
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| 223 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qcontr2 !--// (2nd expression more consistent with LMDZ expression of q) |
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| 224 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: fcontrN !--fraction of grid favourable to non-persistent contrails |
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| 225 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: fcontrP !--fraction of grid favourable to persistent contrails |
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| 226 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dcf_avi !--cloud fraction tendency because of aviation [s-1] |
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| 227 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqi_avi !--specific ice content tendency because of aviation [kg/kg/s] |
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| 228 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqvc_avi !--specific cloud water vapor tendency because of aviation [kg/kg/s] |
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| 229 | |
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| 230 | |
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| 231 | ! for POPRECIP |
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| 232 | |
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| 233 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qraindiag !--DIAGNOSTIC specific rain content [kg/kg] |
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| 234 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: qsnowdiag !--DIAGNOSTIC specific snow content [kg/kg] |
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| 235 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqreva !--rain tendendy due to evaporation [kg/kg/s] |
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| 236 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqssub !--snow tendency due to sublimation [kg/kg/s] |
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| 237 | 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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| 238 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqsagg !--snow tendency due to collection of lcoud ice by aggregation [kg/kg/s] |
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| 239 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqrauto !--rain tendency due to autoconversion of cloud liquid [kg/kg/s] |
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| 240 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqsauto !--snow tendency due to autoconversion of cloud ice [kg/kg/s] |
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| 241 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqsrim !--snow tendency due to riming [kg/kg/s] |
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| 242 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqsmelt !--snow tendency due to melting [kg/kg/s] |
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| 243 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqrmelt !--rain tendency due to melting [kg/kg/s] |
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| 244 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqsfreez !--snow tendency due to freezing [kg/kg/s] |
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| 245 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: dqrfreez !--rain tendency due to freezing [kg/kg/s] |
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| 246 | |
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| 247 | ! for thermals |
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| 248 | |
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| 249 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: cloudth_sth !--mean saturation deficit in thermals |
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| 250 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: cloudth_senv !--mean saturation deficit in environment |
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| 251 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: cloudth_sigmath !--std of saturation deficit in thermals |
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| 252 | REAL, DIMENSION(klon,klev), INTENT(OUT) :: cloudth_sigmaenv !--std of saturation deficit in environment |
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| 253 | |
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| 254 | |
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| 255 | ! LOCAL VARIABLES: |
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| 256 | !---------------- |
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| 257 | |
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| 258 | REAL,DIMENSION(klon) :: qsl, qsi |
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| 259 | REAL :: zct, zcl,zexpo |
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| 260 | REAL, DIMENSION(klon,klev) :: ctot |
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| 261 | REAL, DIMENSION(klon,klev) :: ctot_vol |
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| 262 | REAL, DIMENSION(klon) :: zqs, zdqs |
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| 263 | REAL :: zdelta, zcor, zcvm5 |
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| 264 | REAL, DIMENSION(klon) :: zdqsdT_raw |
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| 265 | REAL, DIMENSION(klon) :: gammasat,dgammasatdt ! coefficient to make cold condensation at the correct RH and derivative wrt T |
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| 266 | REAL, DIMENSION(klon) :: Tbef,qlbef,DT |
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| 267 | REAL :: num,denom |
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| 268 | REAL :: cste |
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| 269 | REAL, DIMENSION(klon) :: zpdf_sig,zpdf_k,zpdf_delta |
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| 270 | REAL, DIMENSION(klon) :: Zpdf_a,zpdf_b,zpdf_e1,zpdf_e2 |
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| 271 | REAL :: erf |
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| 272 | REAL, DIMENSION(klon) :: zfice_th |
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| 273 | REAL, DIMENSION(klon) :: qcloud, qincloud_mpc |
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| 274 | REAL, DIMENSION(klon) :: zrfl, zrfln |
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| 275 | REAL :: zqev, zqevt |
|---|
| 276 | REAL, DIMENSION(klon) :: zifl, zifln, ziflprev |
|---|
| 277 | REAL :: zqev0,zqevi, zqevti |
|---|
| 278 | REAL, DIMENSION(klon) :: zoliq, zcond, zq, zqn |
|---|
| 279 | REAL, DIMENSION(klon) :: zoliql, zoliqi |
|---|
| 280 | REAL, DIMENSION(klon) :: zt |
|---|
| 281 | REAL, DIMENSION(klon,klev) :: zrho |
|---|
| 282 | REAL, DIMENSION(klon) :: zdz,iwc |
|---|
| 283 | REAL :: zchau,zfroi |
|---|
| 284 | REAL, DIMENSION(klon) :: zfice,zneb,znebprecip |
|---|
| 285 | REAL :: zmelt,zrain,zsnow,zprecip |
|---|
| 286 | REAL, DIMENSION(klon) :: dzfice |
|---|
| 287 | REAL :: zsolid |
|---|
| 288 | REAL, DIMENSION(klon) :: qtot, qzero |
|---|
| 289 | REAL, DIMENSION(klon) :: dqsl,dqsi |
|---|
| 290 | REAL :: smallestreal |
|---|
| 291 | ! Variables for Bergeron process |
|---|
| 292 | REAL :: zcp, coef1, DeltaT, Deltaq, Deltaqprecl |
|---|
| 293 | REAL, DIMENSION(klon) :: zqpreci, zqprecl |
|---|
| 294 | ! Variables precipitation energy conservation |
|---|
| 295 | REAL, DIMENSION(klon) :: zmqc |
|---|
| 296 | REAL :: zalpha_tr |
|---|
| 297 | REAL :: zfrac_lessi |
|---|
| 298 | REAL, DIMENSION(klon) :: zprec_cond |
|---|
| 299 | REAL :: zmair |
|---|
| 300 | REAL :: zcpair, zcpeau |
|---|
| 301 | REAL, DIMENSION(klon) :: zlh_solid |
|---|
| 302 | REAL, DIMENSION(klon) :: ztupnew |
|---|
| 303 | REAL, DIMENSION(klon) :: zqvapclr, zqupnew ! for poprecip evap / subl |
|---|
| 304 | REAL :: zm_solid ! for liquid -> solid conversion |
|---|
| 305 | REAL, DIMENSION(klon) :: zrflclr, zrflcld |
|---|
| 306 | REAL, DIMENSION(klon) :: d_zrfl_clr_cld, d_zifl_clr_cld |
|---|
| 307 | REAL, DIMENSION(klon) :: d_zrfl_cld_clr, d_zifl_cld_clr |
|---|
| 308 | REAL, DIMENSION(klon) :: ziflclr, ziflcld |
|---|
| 309 | REAL, DIMENSION(klon) :: znebprecipclr, znebprecipcld |
|---|
| 310 | REAL, DIMENSION(klon) :: tot_zneb, tot_znebn, d_tot_zneb |
|---|
| 311 | REAL, DIMENSION(klon) :: d_znebprecip_clr_cld, d_znebprecip_cld_clr |
|---|
| 312 | REAL, DIMENSION(klon,klev) :: velo |
|---|
| 313 | REAL :: vr, ffallv |
|---|
| 314 | REAL :: qlmpc, qimpc, rnebmpc |
|---|
| 315 | REAL, DIMENSION(klon,klev) :: radocondi, radocondl |
|---|
| 316 | REAL :: effective_zneb |
|---|
| 317 | REAL, DIMENSION(klon) :: distcltop1D, temp_cltop1D |
|---|
| 318 | |
|---|
| 319 | ! for condensation and ice supersaturation |
|---|
| 320 | REAL, DIMENSION(klon) :: qvc, shear |
|---|
| 321 | REAL :: delta_z |
|---|
| 322 | !--Added for ice supersaturation (ok_ice_supersat) and contrails (ok_plane_contrails) |
|---|
| 323 | ! Constants used for calculating ratios that are advected (using a parent-child |
|---|
| 324 | ! formalism). This is not done in the dynamical core because at this moment, |
|---|
| 325 | ! only isotopes can use this parent-child formalism. Note that the two constants |
|---|
| 326 | ! are the same as the one use in the dynamical core, being also defined in |
|---|
| 327 | ! dyn3d_common/infotrac.F90 |
|---|
| 328 | REAL :: min_qParent, min_ratio |
|---|
| 329 | |
|---|
| 330 | |
|---|
| 331 | INTEGER i, k, n, kk, iter |
|---|
| 332 | INTEGER, DIMENSION(klon) :: n_i |
|---|
| 333 | INTEGER ncoreczq |
|---|
| 334 | INTEGER, DIMENSION(klon,klev) :: mpc_bl_points |
|---|
| 335 | LOGICAL iftop |
|---|
| 336 | |
|---|
| 337 | LOGICAL, DIMENSION(klon) :: lognormale |
|---|
| 338 | LOGICAL, DIMENSION(klon) :: keepgoing |
|---|
| 339 | |
|---|
| 340 | CHARACTER (len = 20) :: modname = 'lscp' |
|---|
| 341 | CHARACTER (len = 80) :: abort_message |
|---|
| 342 | |
|---|
| 343 | |
|---|
| 344 | !=============================================================================== |
|---|
| 345 | ! INITIALISATION |
|---|
| 346 | !=============================================================================== |
|---|
| 347 | |
|---|
| 348 | ! Few initial checks |
|---|
| 349 | |
|---|
| 350 | |
|---|
| 351 | IF (iflag_fisrtilp_qsat .LT. 0) THEN |
|---|
| 352 | abort_message = 'lscp cannot be used with iflag_fisrtilp<0' |
|---|
| 353 | CALL abort_physic(modname,abort_message,1) |
|---|
| 354 | ENDIF |
|---|
| 355 | |
|---|
| 356 | ! Few initialisations |
|---|
| 357 | |
|---|
| 358 | znebprecip(:)=0.0 |
|---|
| 359 | ctot_vol(1:klon,1:klev)=0.0 |
|---|
| 360 | rneblsvol(1:klon,1:klev)=0.0 |
|---|
| 361 | smallestreal=1.e-9 |
|---|
| 362 | znebprecipclr(:)=0.0 |
|---|
| 363 | znebprecipcld(:)=0.0 |
|---|
| 364 | mpc_bl_points(:,:)=0 |
|---|
| 365 | |
|---|
| 366 | IF (prt_level>9) WRITE(lunout,*) 'NUAGES4 A. JAM' |
|---|
| 367 | |
|---|
| 368 | ! AA for 'safety' reasons |
|---|
| 369 | zalpha_tr = 0. |
|---|
| 370 | zfrac_lessi = 0. |
|---|
| 371 | beta(:,:)= 0. |
|---|
| 372 | |
|---|
| 373 | ! Initialisation of variables: |
|---|
| 374 | |
|---|
| 375 | prfl(:,:) = 0.0 |
|---|
| 376 | psfl(:,:) = 0.0 |
|---|
| 377 | d_t(:,:) = 0.0 |
|---|
| 378 | d_q(:,:) = 0.0 |
|---|
| 379 | d_ql(:,:) = 0.0 |
|---|
| 380 | d_qi(:,:) = 0.0 |
|---|
| 381 | rneb(:,:) = 0.0 |
|---|
| 382 | pfraclr(:,:)=0.0 |
|---|
| 383 | pfracld(:,:)=0.0 |
|---|
| 384 | radocond(:,:) = 0.0 |
|---|
| 385 | radicefrac(:,:) = 0.0 |
|---|
| 386 | frac_nucl(:,:) = 1.0 |
|---|
| 387 | frac_impa(:,:) = 1.0 |
|---|
| 388 | rain(:) = 0.0 |
|---|
| 389 | snow(:) = 0.0 |
|---|
| 390 | zoliq(:)=0.0 |
|---|
| 391 | zfice(:)=0.0 |
|---|
| 392 | dzfice(:)=0.0 |
|---|
| 393 | zqprecl(:)=0.0 |
|---|
| 394 | zqpreci(:)=0.0 |
|---|
| 395 | zrfl(:) = 0.0 |
|---|
| 396 | zifl(:) = 0.0 |
|---|
| 397 | ziflprev(:)=0.0 |
|---|
| 398 | zneb(:) = seuil_neb |
|---|
| 399 | zrflclr(:) = 0.0 |
|---|
| 400 | ziflclr(:) = 0.0 |
|---|
| 401 | zrflcld(:) = 0.0 |
|---|
| 402 | ziflcld(:) = 0.0 |
|---|
| 403 | tot_zneb(:) = 0.0 |
|---|
| 404 | tot_znebn(:) = 0.0 |
|---|
| 405 | d_tot_zneb(:) = 0.0 |
|---|
| 406 | qzero(:) = 0.0 |
|---|
| 407 | distcltop1D(:)=0.0 |
|---|
| 408 | temp_cltop1D(:) = 0.0 |
|---|
| 409 | ztupnew(:)=0.0 |
|---|
| 410 | |
|---|
| 411 | distcltop(:,:)=0. |
|---|
| 412 | temp_cltop(:,:)=0. |
|---|
| 413 | |
|---|
| 414 | !--Ice supersaturation |
|---|
| 415 | gamma_cond(:,:) = 1. |
|---|
| 416 | qissr(:,:) = 0. |
|---|
| 417 | issrfra(:,:) = 0. |
|---|
| 418 | dcf_sub(:,:) = 0. |
|---|
| 419 | dcf_con(:,:) = 0. |
|---|
| 420 | dcf_mix(:,:) = 0. |
|---|
| 421 | dqi_adj(:,:) = 0. |
|---|
| 422 | dqi_sub(:,:) = 0. |
|---|
| 423 | dqi_con(:,:) = 0. |
|---|
| 424 | dqi_mix(:,:) = 0. |
|---|
| 425 | dqvc_adj(:,:) = 0. |
|---|
| 426 | dqvc_sub(:,:) = 0. |
|---|
| 427 | dqvc_con(:,:) = 0. |
|---|
| 428 | dqvc_mix(:,:) = 0. |
|---|
| 429 | fcontrN(:,:) = 0. |
|---|
| 430 | fcontrP(:,:) = 0. |
|---|
| 431 | Tcontr(:,:) = missing_val |
|---|
| 432 | qcontr(:,:) = missing_val |
|---|
| 433 | qcontr2(:,:) = missing_val |
|---|
| 434 | dcf_avi(:,:) = 0. |
|---|
| 435 | dqi_avi(:,:) = 0. |
|---|
| 436 | dqvc_avi(:,:) = 0. |
|---|
| 437 | qvc(:) = 0. |
|---|
| 438 | shear(:) = 0. |
|---|
| 439 | min_qParent = 1.e-30 |
|---|
| 440 | min_ratio = 1.e-16 |
|---|
| 441 | |
|---|
| 442 | !-- poprecip |
|---|
| 443 | qraindiag(:,:)= 0. |
|---|
| 444 | qsnowdiag(:,:)= 0. |
|---|
| 445 | dqreva(:,:) = 0. |
|---|
| 446 | dqrauto(:,:) = 0. |
|---|
| 447 | dqrmelt(:,:) = 0. |
|---|
| 448 | dqrfreez(:,:) = 0. |
|---|
| 449 | dqrcol(:,:) = 0. |
|---|
| 450 | dqssub(:,:) = 0. |
|---|
| 451 | dqsauto(:,:) = 0. |
|---|
| 452 | dqsrim(:,:) = 0. |
|---|
| 453 | dqsagg(:,:) = 0. |
|---|
| 454 | dqsfreez(:,:) = 0. |
|---|
| 455 | dqsmelt(:,:) = 0. |
|---|
| 456 | zqupnew(:) = 0. |
|---|
| 457 | zqvapclr(:) = 0. |
|---|
| 458 | |
|---|
| 459 | |
|---|
| 460 | |
|---|
| 461 | |
|---|
| 462 | !c_iso: variable initialisation for iso |
|---|
| 463 | |
|---|
| 464 | |
|---|
| 465 | !=============================================================================== |
|---|
| 466 | ! BEGINNING OF VERTICAL LOOP FROM TOP TO BOTTOM |
|---|
| 467 | !=============================================================================== |
|---|
| 468 | |
|---|
| 469 | ncoreczq=0 |
|---|
| 470 | |
|---|
| 471 | DO k = klev, 1, -1 |
|---|
| 472 | |
|---|
| 473 | IF (k.LE.klev-1) THEN |
|---|
| 474 | iftop=.false. |
|---|
| 475 | ELSE |
|---|
| 476 | iftop=.true. |
|---|
| 477 | ENDIF |
|---|
| 478 | |
|---|
| 479 | ! Initialisation temperature and specific humidity |
|---|
| 480 | DO i = 1, klon |
|---|
| 481 | zt(i)=temp(i,k) |
|---|
| 482 | zq(i)=qt(i,k) |
|---|
| 483 | IF (.not. iftop) THEN |
|---|
| 484 | ztupnew(i) = temp(i,k+1) + d_t(i,k+1) |
|---|
| 485 | zqupnew(i) = qt(i,k+1) + d_q(i,k+1) + d_ql(i,k+1) + d_qi(i,k+1) |
|---|
| 486 | !--zqs(i) is the saturation specific humidity in the layer above |
|---|
| 487 | zqvapclr(i) = MAX(0., qt(i,k+1) + d_q(i,k+1) - rneb(i,k+1) * zqs(i)) |
|---|
| 488 | ENDIF |
|---|
| 489 | !c_iso init of iso |
|---|
| 490 | ENDDO |
|---|
| 491 | |
|---|
| 492 | !================================================================ |
|---|
| 493 | ! Flag for the new and more microphysical treatment of precipitation from Atelier Nuage (R) |
|---|
| 494 | IF (ok_poprecip) THEN |
|---|
| 495 | |
|---|
| 496 | CALL poprecip_precld(klon, dtime, iftop, paprs(:,k), paprs(:,k+1), pplay(:,k), & |
|---|
| 497 | zt, ztupnew, zq, zmqc, znebprecipclr, znebprecipcld, & |
|---|
| 498 | zqvapclr, zqupnew, & |
|---|
| 499 | zrfl, zrflclr, zrflcld, & |
|---|
| 500 | zifl, ziflclr, ziflcld, & |
|---|
| 501 | dqreva(:,k),dqssub(:,k) & |
|---|
| 502 | ) |
|---|
| 503 | |
|---|
| 504 | !================================================================ |
|---|
| 505 | ELSE |
|---|
| 506 | |
|---|
| 507 | ! -------------------------------------------------------------------- |
|---|
| 508 | ! P1> Thermalization of precipitation falling from the overlying layer |
|---|
| 509 | ! -------------------------------------------------------------------- |
|---|
| 510 | ! Computes air temperature variation due to enthalpy transported by |
|---|
| 511 | ! precipitation. Precipitation is then thermalized with the air in the |
|---|
| 512 | ! layer. |
|---|
| 513 | ! The precipitation should remain thermalized throughout the different |
|---|
| 514 | ! thermodynamical transformations. |
|---|
| 515 | ! The corresponding water mass should |
|---|
| 516 | ! be added when calculating the layer's enthalpy change with |
|---|
| 517 | ! temperature |
|---|
| 518 | ! See lmdzpedia page todoan |
|---|
| 519 | ! todoan: check consistency with ice phase |
|---|
| 520 | ! todoan: understand why several steps |
|---|
| 521 | ! --------------------------------------------------------------------- |
|---|
| 522 | |
|---|
| 523 | IF (iftop) THEN |
|---|
| 524 | |
|---|
| 525 | DO i = 1, klon |
|---|
| 526 | zmqc(i) = 0. |
|---|
| 527 | ENDDO |
|---|
| 528 | |
|---|
| 529 | ELSE |
|---|
| 530 | |
|---|
| 531 | DO i = 1, klon |
|---|
| 532 | |
|---|
| 533 | zmair=(paprs(i,k)-paprs(i,k+1))/RG |
|---|
| 534 | ! no condensed water so cp=cp(vapor+dry air) |
|---|
| 535 | ! RVTMP2=rcpv/rcpd-1 |
|---|
| 536 | zcpair=RCPD*(1.0+RVTMP2*zq(i)) |
|---|
| 537 | zcpeau=RCPD*RVTMP2 |
|---|
| 538 | |
|---|
| 539 | ! zmqc: precipitation mass that has to be thermalized with |
|---|
| 540 | ! layer's air so that precipitation at the ground has the |
|---|
| 541 | ! same temperature as the lowermost layer |
|---|
| 542 | zmqc(i) = (zrfl(i)+zifl(i))*dtime/zmair |
|---|
| 543 | ! t(i,k+1)+d_t(i,k+1): new temperature of the overlying layer |
|---|
| 544 | zt(i) = ( ztupnew(i)*zmqc(i)*zcpeau + zcpair*zt(i) ) & |
|---|
| 545 | / (zcpair + zmqc(i)*zcpeau) |
|---|
| 546 | |
|---|
| 547 | ENDDO |
|---|
| 548 | |
|---|
| 549 | ENDIF |
|---|
| 550 | |
|---|
| 551 | ! -------------------------------------------------------------------- |
|---|
| 552 | ! P2> Precipitation evaporation/sublimation/melting |
|---|
| 553 | ! -------------------------------------------------------------------- |
|---|
| 554 | ! A part of the precipitation coming from above is evaporated/sublimated/melted. |
|---|
| 555 | ! -------------------------------------------------------------------- |
|---|
| 556 | |
|---|
| 557 | IF (iflag_evap_prec.GE.1) THEN |
|---|
| 558 | |
|---|
| 559 | ! Calculation of saturation specific humidity |
|---|
| 560 | ! depending on temperature: |
|---|
| 561 | CALL calc_qsat_ecmwf(klon,zt(:),qzero(:),pplay(:,k),RTT,0,.false.,zqs(:),zdqs(:)) |
|---|
| 562 | ! wrt liquid water |
|---|
| 563 | CALL calc_qsat_ecmwf(klon,zt(:),qzero(:),pplay(:,k),RTT,1,.false.,qsl(:),dqsl(:)) |
|---|
| 564 | ! wrt ice |
|---|
| 565 | CALL calc_qsat_ecmwf(klon,zt(:),qzero(:),pplay(:,k),RTT,2,.false.,qsi(:),dqsi(:)) |
|---|
| 566 | |
|---|
| 567 | DO i = 1, klon |
|---|
| 568 | |
|---|
| 569 | ! if precipitation |
|---|
| 570 | IF (zrfl(i)+zifl(i).GT.0.) THEN |
|---|
| 571 | |
|---|
| 572 | ! LudoTP: we only account for precipitation evaporation in the clear-sky (iflag_evap_prec>=4). |
|---|
| 573 | ! c_iso: likely important to distinguish cs from neb isotope precipitation |
|---|
| 574 | |
|---|
| 575 | IF (iflag_evap_prec.GE.4) THEN |
|---|
| 576 | zrfl(i) = zrflclr(i) |
|---|
| 577 | zifl(i) = ziflclr(i) |
|---|
| 578 | ENDIF |
|---|
| 579 | |
|---|
| 580 | IF (iflag_evap_prec.EQ.1) THEN |
|---|
| 581 | znebprecip(i)=zneb(i) |
|---|
| 582 | ELSE |
|---|
| 583 | znebprecip(i)=MAX(zneb(i),znebprecip(i)) |
|---|
| 584 | ENDIF |
|---|
| 585 | |
|---|
| 586 | IF (iflag_evap_prec.GT.4) THEN |
|---|
| 587 | ! Max evaporation not to saturate the clear sky precip fraction |
|---|
| 588 | ! i.e. the fraction where evaporation occurs |
|---|
| 589 | zqev0 = MAX(0.0, (zqs(i)-zq(i))*znebprecipclr(i)) |
|---|
| 590 | ELSEIF (iflag_evap_prec .EQ. 4) THEN |
|---|
| 591 | ! Max evaporation not to saturate the whole mesh |
|---|
| 592 | ! Pay attention -> lead to unrealistic and excessive evaporation |
|---|
| 593 | zqev0 = MAX(0.0, zqs(i)-zq(i)) |
|---|
| 594 | ELSE |
|---|
| 595 | ! Max evap not to saturate the fraction below the cloud |
|---|
| 596 | zqev0 = MAX(0.0, (zqs(i)-zq(i))*znebprecip(i)) |
|---|
| 597 | ENDIF |
|---|
| 598 | |
|---|
| 599 | ! Evaporation of liquid precipitation coming from above |
|---|
| 600 | ! dP/dz=beta*(1-q/qsat)*sqrt(P) |
|---|
| 601 | ! formula from Sundquist 1988, Klemp & Wilhemson 1978 |
|---|
| 602 | ! LTP: evaporation only in the clear sky part (iflag_evap_prec>=4) |
|---|
| 603 | |
|---|
| 604 | IF (iflag_evap_prec.EQ.3) THEN |
|---|
| 605 | zqevt = znebprecip(i)*coef_eva*(1.0-zq(i)/qsl(i)) & |
|---|
| 606 | *SQRT(zrfl(i)/max(1.e-4,znebprecip(i))) & |
|---|
| 607 | *(paprs(i,k)-paprs(i,k+1))/pplay(i,k)*zt(i)*RD/RG |
|---|
| 608 | ELSE IF (iflag_evap_prec.GE.4) THEN |
|---|
| 609 | zqevt = znebprecipclr(i)*coef_eva*(1.0-zq(i)/qsl(i)) & |
|---|
| 610 | *SQRT(zrfl(i)/max(1.e-8,znebprecipclr(i))) & |
|---|
| 611 | *(paprs(i,k)-paprs(i,k+1))/pplay(i,k)*zt(i)*RD/RG |
|---|
| 612 | ELSE |
|---|
| 613 | zqevt = 1.*coef_eva*(1.0-zq(i)/qsl(i))*SQRT(zrfl(i)) & |
|---|
| 614 | *(paprs(i,k)-paprs(i,k+1))/pplay(i,k)*zt(i)*RD/RG |
|---|
| 615 | ENDIF |
|---|
| 616 | |
|---|
| 617 | zqevt = MAX(0.0,MIN(zqevt,zrfl(i))) & |
|---|
| 618 | *RG*dtime/(paprs(i,k)-paprs(i,k+1)) |
|---|
| 619 | |
|---|
| 620 | ! sublimation of the solid precipitation coming from above |
|---|
| 621 | IF (iflag_evap_prec.EQ.3) THEN |
|---|
| 622 | zqevti = znebprecip(i)*coef_sub*(1.0-zq(i)/qsi(i)) & |
|---|
| 623 | *SQRT(zifl(i)/max(1.e-4,znebprecip(i))) & |
|---|
| 624 | *(paprs(i,k)-paprs(i,k+1))/pplay(i,k)*zt(i)*RD/RG |
|---|
| 625 | ELSE IF (iflag_evap_prec.GE.4) THEN |
|---|
| 626 | zqevti = znebprecipclr(i)*coef_sub*(1.0-zq(i)/qsi(i)) & |
|---|
| 627 | *SQRT(zifl(i)/max(1.e-8,znebprecipclr(i))) & |
|---|
| 628 | *(paprs(i,k)-paprs(i,k+1))/pplay(i,k)*zt(i)*RD/RG |
|---|
| 629 | ELSE |
|---|
| 630 | zqevti = 1.*coef_sub*(1.0-zq(i)/qsi(i))*SQRT(zifl(i)) & |
|---|
| 631 | *(paprs(i,k)-paprs(i,k+1))/pplay(i,k)*zt(i)*RD/RG |
|---|
| 632 | ENDIF |
|---|
| 633 | |
|---|
| 634 | zqevti = MAX(0.0,MIN(zqevti,zifl(i))) & |
|---|
| 635 | *RG*dtime/(paprs(i,k)-paprs(i,k+1)) |
|---|
| 636 | |
|---|
| 637 | ! A. JAM |
|---|
| 638 | ! Evaporation limit: we ensure that the layer's fraction below |
|---|
| 639 | ! the cloud or the whole mesh (depending on iflag_evap_prec) |
|---|
| 640 | ! does not reach saturation. In this case, we |
|---|
| 641 | ! redistribute zqev0 conserving the ratio liquid/ice |
|---|
| 642 | |
|---|
| 643 | IF (zqevt+zqevti.GT.zqev0) THEN |
|---|
| 644 | zqev=zqev0*zqevt/(zqevt+zqevti) |
|---|
| 645 | zqevi=zqev0*zqevti/(zqevt+zqevti) |
|---|
| 646 | ELSE |
|---|
| 647 | zqev=zqevt |
|---|
| 648 | zqevi=zqevti |
|---|
| 649 | ENDIF |
|---|
| 650 | |
|---|
| 651 | |
|---|
| 652 | ! New solid and liquid precipitation fluxes after evap and sublimation |
|---|
| 653 | zrfln(i) = Max(0.,zrfl(i) - zqev*(paprs(i,k)-paprs(i,k+1)) & |
|---|
| 654 | /RG/dtime) |
|---|
| 655 | zifln(i) = Max(0.,zifl(i) - zqevi*(paprs(i,k)-paprs(i,k+1)) & |
|---|
| 656 | /RG/dtime) |
|---|
| 657 | |
|---|
| 658 | |
|---|
| 659 | ! vapor, temperature, precip fluxes update |
|---|
| 660 | ! vapor is updated after evaporation/sublimation (it is increased) |
|---|
| 661 | zq(i) = zq(i) - (zrfln(i)+zifln(i)-zrfl(i)-zifl(i)) & |
|---|
| 662 | * (RG/(paprs(i,k)-paprs(i,k+1)))*dtime |
|---|
| 663 | ! zmqc is the total condensed water in the precip flux (it is decreased) |
|---|
| 664 | zmqc(i) = zmqc(i) + (zrfln(i)+zifln(i)-zrfl(i)-zifl(i)) & |
|---|
| 665 | * (RG/(paprs(i,k)-paprs(i,k+1)))*dtime |
|---|
| 666 | ! air and precip temperature (i.e., gridbox temperature) |
|---|
| 667 | ! is updated due to latent heat cooling |
|---|
| 668 | zt(i) = zt(i) + (zrfln(i)-zrfl(i)) & |
|---|
| 669 | * (RG/(paprs(i,k)-paprs(i,k+1)))*dtime & |
|---|
| 670 | * RLVTT/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i))) & |
|---|
| 671 | + (zifln(i)-zifl(i)) & |
|---|
| 672 | * (RG/(paprs(i,k)-paprs(i,k+1)))*dtime & |
|---|
| 673 | * RLSTT/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i))) |
|---|
| 674 | |
|---|
| 675 | ! New values of liquid and solid precipitation |
|---|
| 676 | zrfl(i) = zrfln(i) |
|---|
| 677 | zifl(i) = zifln(i) |
|---|
| 678 | |
|---|
| 679 | ! c_iso here call_reevap that updates isotopic zrfl, zifl (in inout) |
|---|
| 680 | ! due to evap + sublim |
|---|
| 681 | |
|---|
| 682 | |
|---|
| 683 | IF (iflag_evap_prec.GE.4) THEN |
|---|
| 684 | zrflclr(i) = zrfl(i) |
|---|
| 685 | ziflclr(i) = zifl(i) |
|---|
| 686 | IF(zrflclr(i) + ziflclr(i).LE.0) THEN |
|---|
| 687 | znebprecipclr(i) = 0.0 |
|---|
| 688 | ENDIF |
|---|
| 689 | zrfl(i) = zrflclr(i) + zrflcld(i) |
|---|
| 690 | zifl(i) = ziflclr(i) + ziflcld(i) |
|---|
| 691 | ENDIF |
|---|
| 692 | |
|---|
| 693 | ! c_iso duplicate for isotopes or loop on isotopes |
|---|
| 694 | |
|---|
| 695 | ! Melting: |
|---|
| 696 | zmelt = ((zt(i)-RTT)/(ztfondue-RTT)) ! JYG |
|---|
| 697 | ! precip fraction that is melted |
|---|
| 698 | zmelt = MIN(MAX(zmelt,0.),1.) |
|---|
| 699 | |
|---|
| 700 | ! update of rainfall and snowfall due to melting |
|---|
| 701 | IF (iflag_evap_prec.GE.4) THEN |
|---|
| 702 | zrflclr(i)=zrflclr(i)+zmelt*ziflclr(i) |
|---|
| 703 | zrflcld(i)=zrflcld(i)+zmelt*ziflcld(i) |
|---|
| 704 | zrfl(i)=zrflclr(i)+zrflcld(i) |
|---|
| 705 | ELSE |
|---|
| 706 | zrfl(i)=zrfl(i)+zmelt*zifl(i) |
|---|
| 707 | ENDIF |
|---|
| 708 | |
|---|
| 709 | |
|---|
| 710 | ! c_iso: melting of isotopic precipi with zmelt (no fractionation) |
|---|
| 711 | |
|---|
| 712 | ! Latent heat of melting because of precipitation melting |
|---|
| 713 | ! NB: the air + precip temperature is simultaneously updated |
|---|
| 714 | zt(i)=zt(i)-zifl(i)*zmelt*(RG*dtime)/(paprs(i,k)-paprs(i,k+1)) & |
|---|
| 715 | *RLMLT/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i))) |
|---|
| 716 | |
|---|
| 717 | IF (iflag_evap_prec.GE.4) THEN |
|---|
| 718 | ziflclr(i)=ziflclr(i)*(1.-zmelt) |
|---|
| 719 | ziflcld(i)=ziflcld(i)*(1.-zmelt) |
|---|
| 720 | zifl(i)=ziflclr(i)+ziflcld(i) |
|---|
| 721 | ELSE |
|---|
| 722 | zifl(i)=zifl(i)*(1.-zmelt) |
|---|
| 723 | ENDIF |
|---|
| 724 | |
|---|
| 725 | ELSE |
|---|
| 726 | ! if no precip, we reinitialize the cloud fraction used for the precip to 0 |
|---|
| 727 | znebprecip(i)=0. |
|---|
| 728 | |
|---|
| 729 | ENDIF ! (zrfl(i)+zifl(i).GT.0.) |
|---|
| 730 | |
|---|
| 731 | ENDDO ! loop on klon |
|---|
| 732 | |
|---|
| 733 | ENDIF ! (iflag_evap_prec>=1) |
|---|
| 734 | |
|---|
| 735 | ENDIF ! (ok_poprecip) |
|---|
| 736 | |
|---|
| 737 | ! -------------------------------------------------------------------- |
|---|
| 738 | ! End precip evaporation |
|---|
| 739 | ! -------------------------------------------------------------------- |
|---|
| 740 | |
|---|
| 741 | ! Calculation of qsat, L/Cp*dqsat/dT and ncoreczq counter |
|---|
| 742 | !------------------------------------------------------- |
|---|
| 743 | |
|---|
| 744 | qtot(:)=zq(:)+zmqc(:) |
|---|
| 745 | CALL calc_qsat_ecmwf(klon,zt(:),qtot(:),pplay(:,k),RTT,0,.false.,zqs(:),zdqs(:)) |
|---|
| 746 | DO i = 1, klon |
|---|
| 747 | zdelta = MAX(0.,SIGN(1.,RTT-zt(i))) |
|---|
| 748 | zdqsdT_raw(i) = zdqs(i)*RCPD*(1.0+RVTMP2*zq(i)) / (RLVTT*(1.-zdelta) + RLSTT*zdelta) |
|---|
| 749 | IF (zq(i) .LT. 1.e-15) THEN |
|---|
| 750 | ncoreczq=ncoreczq+1 |
|---|
| 751 | zq(i)=1.e-15 |
|---|
| 752 | ENDIF |
|---|
| 753 | ! c_iso: do something similar for isotopes |
|---|
| 754 | |
|---|
| 755 | ENDDO |
|---|
| 756 | |
|---|
| 757 | ! -------------------------------------------------------------------- |
|---|
| 758 | ! P2> Cloud formation |
|---|
| 759 | !--------------------------------------------------------------------- |
|---|
| 760 | ! |
|---|
| 761 | ! Unlike fisrtilp, we always assume a 'fractional cloud' approach |
|---|
| 762 | ! i.e. clouds occupy only a fraction of the mesh (the subgrid distribution |
|---|
| 763 | ! is prescribed and depends on large scale variables and boundary layer |
|---|
| 764 | ! properties) |
|---|
| 765 | ! The decrease in condensed part due tu latent heating is taken into |
|---|
| 766 | ! account |
|---|
| 767 | ! ------------------------------------------------------------------- |
|---|
| 768 | |
|---|
| 769 | ! P2.1> With the PDFs (log-normal, bigaussian) |
|---|
| 770 | ! cloud properties calculation with the initial values of t and q |
|---|
| 771 | ! ---------------------------------------------------------------- |
|---|
| 772 | |
|---|
| 773 | ! initialise gammasat and qincloud_mpc |
|---|
| 774 | gammasat(:)=1. |
|---|
| 775 | qincloud_mpc(:)=0. |
|---|
| 776 | |
|---|
| 777 | IF (iflag_cld_th.GE.5) THEN |
|---|
| 778 | ! Cloud cover and content in meshes affected by shallow convection, |
|---|
| 779 | ! are retrieved from a bi-gaussian distribution of the saturation deficit |
|---|
| 780 | ! following Jam et al. 2013 |
|---|
| 781 | |
|---|
| 782 | IF (iflag_cloudth_vert.LE.2) THEN |
|---|
| 783 | ! Old version of Arnaud Jam |
|---|
| 784 | |
|---|
| 785 | CALL cloudth(klon,klev,k,tv, & |
|---|
| 786 | zq,qta,fraca, & |
|---|
| 787 | qcloud,ctot,pspsk,paprs,pplay,tla,thl, & |
|---|
| 788 | ratqs,zqs,temp, & |
|---|
| 789 | cloudth_sth,cloudth_senv,cloudth_sigmath,cloudth_sigmaenv) |
|---|
| 790 | |
|---|
| 791 | |
|---|
| 792 | ELSEIF (iflag_cloudth_vert.GE.3 .AND. iflag_cloudth_vert.LE.5) THEN |
|---|
| 793 | ! Default version of Arnaud Jam |
|---|
| 794 | |
|---|
| 795 | CALL cloudth_v3(klon,klev,k,tv, & |
|---|
| 796 | zq,qta,fraca, & |
|---|
| 797 | qcloud,ctot,ctot_vol,pspsk,paprs,pplay,tla,thl, & |
|---|
| 798 | ratqs,zqs,temp, & |
|---|
| 799 | cloudth_sth,cloudth_senv,cloudth_sigmath,cloudth_sigmaenv) |
|---|
| 800 | |
|---|
| 801 | |
|---|
| 802 | ELSEIF (iflag_cloudth_vert.EQ.6) THEN |
|---|
| 803 | ! Jean Jouhaud's version, with specific separation between surface and volume |
|---|
| 804 | ! cloud fraction Decembre 2018 |
|---|
| 805 | |
|---|
| 806 | CALL cloudth_v6(klon,klev,k,tv, & |
|---|
| 807 | zq,qta,fraca, & |
|---|
| 808 | qcloud,ctot,ctot_vol,pspsk,paprs,pplay,tla,thl, & |
|---|
| 809 | ratqs,zqs,temp, & |
|---|
| 810 | cloudth_sth,cloudth_senv,cloudth_sigmath,cloudth_sigmaenv) |
|---|
| 811 | |
|---|
| 812 | ELSEIF (iflag_cloudth_vert .EQ. 7) THEN |
|---|
| 813 | ! Updated version of Arnaud Jam (correction by E. Vignon) + adapted treatment |
|---|
| 814 | ! for boundary-layer mixed phase clouds following Vignon et al. |
|---|
| 815 | CALL cloudth_mpc(klon,klev,k,mpc_bl_points,zt,zq,qta(:,k),fraca(:,k), & |
|---|
| 816 | pspsk(:,k),paprs(:,k+1),paprs(:,k),pplay(:,k), tla(:,k), & |
|---|
| 817 | ratqs(:,k),qcloud,qincloud_mpc,zfice_th,ctot(:,k),ctot_vol(:,k), & |
|---|
| 818 | cloudth_sth(:,k),cloudth_senv(:,k),cloudth_sigmath(:,k),cloudth_sigmaenv(:,k)) |
|---|
| 819 | |
|---|
| 820 | ENDIF |
|---|
| 821 | |
|---|
| 822 | |
|---|
| 823 | DO i=1,klon |
|---|
| 824 | rneb(i,k)=ctot(i,k) |
|---|
| 825 | rneblsvol(i,k)=ctot_vol(i,k) |
|---|
| 826 | zqn(i)=qcloud(i) |
|---|
| 827 | !--AB grid-mean vapor in the cloud - we assume saturation adjustment |
|---|
| 828 | qvc(i) = rneb(i,k) * zqs(i) |
|---|
| 829 | ENDDO |
|---|
| 830 | |
|---|
| 831 | ENDIF |
|---|
| 832 | |
|---|
| 833 | IF (iflag_cld_th .LE. 4) THEN |
|---|
| 834 | |
|---|
| 835 | ! lognormal |
|---|
| 836 | lognormale = .TRUE. |
|---|
| 837 | |
|---|
| 838 | ELSEIF (iflag_cld_th .GE. 6) THEN |
|---|
| 839 | |
|---|
| 840 | ! lognormal distribution when no thermals |
|---|
| 841 | lognormale = fraca(:,k) < min_frac_th_cld |
|---|
| 842 | |
|---|
| 843 | ELSE |
|---|
| 844 | ! When iflag_cld_th=5, we always assume |
|---|
| 845 | ! bi-gaussian distribution |
|---|
| 846 | lognormale = .FALSE. |
|---|
| 847 | |
|---|
| 848 | ENDIF |
|---|
| 849 | |
|---|
| 850 | DT(:) = 0. |
|---|
| 851 | n_i(:)=0 |
|---|
| 852 | Tbef(:)=zt(:) |
|---|
| 853 | qlbef(:)=0. |
|---|
| 854 | |
|---|
| 855 | ! Treatment of non-boundary layer clouds (lognormale) |
|---|
| 856 | ! condensation with qsat(T) variation (adaptation) |
|---|
| 857 | ! Iterative resolution to converge towards qsat |
|---|
| 858 | ! with update of temperature, ice fraction and qsat at |
|---|
| 859 | ! each iteration |
|---|
| 860 | |
|---|
| 861 | ! todoan -> sensitivity to iflag_fisrtilp_qsat |
|---|
| 862 | DO iter=1,iflag_fisrtilp_qsat+1 |
|---|
| 863 | |
|---|
| 864 | keepgoing(:) = .FALSE. |
|---|
| 865 | |
|---|
| 866 | DO i=1,klon |
|---|
| 867 | |
|---|
| 868 | ! keepgoing = .true. while convergence is not satisfied |
|---|
| 869 | |
|---|
| 870 | IF (((ABS(DT(i)).GT.DDT0) .OR. (n_i(i) .EQ. 0)) .AND. lognormale(i)) THEN |
|---|
| 871 | |
|---|
| 872 | ! if not convergence: |
|---|
| 873 | ! we calculate a new iteration |
|---|
| 874 | keepgoing(i) = .TRUE. |
|---|
| 875 | |
|---|
| 876 | ! P2.2.1> cloud fraction and condensed water mass calculation |
|---|
| 877 | ! Calculated variables: |
|---|
| 878 | ! rneb : cloud fraction |
|---|
| 879 | ! zqn : total water within the cloud |
|---|
| 880 | ! zcond: mean condensed water within the mesh |
|---|
| 881 | ! rhcl: clear-sky relative humidity |
|---|
| 882 | !--------------------------------------------------------------- |
|---|
| 883 | |
|---|
| 884 | ! new temperature that only serves in the iteration process: |
|---|
| 885 | Tbef(i)=Tbef(i)+DT(i) |
|---|
| 886 | |
|---|
| 887 | ! Rneb, qzn and zcond for lognormal PDFs |
|---|
| 888 | qtot(i)=zq(i)+zmqc(i) |
|---|
| 889 | |
|---|
| 890 | ENDIF |
|---|
| 891 | |
|---|
| 892 | ENDDO |
|---|
| 893 | |
|---|
| 894 | ! Calculation of saturation specific humidity and ice fraction |
|---|
| 895 | CALL calc_qsat_ecmwf(klon,Tbef(:),qtot(:),pplay(:,k),RTT,0,.false.,zqs(:),zdqs(:)) |
|---|
| 896 | CALL calc_gammasat(klon,Tbef(:),qtot(:),pplay(:,k),gammasat(:),dgammasatdt(:)) |
|---|
| 897 | ! saturation may occur at a humidity different from qsat (gamma qsat), so gamma correction for dqs |
|---|
| 898 | zdqs(:) = gammasat(:)*zdqs(:)+zqs(:)*dgammasatdt(:) |
|---|
| 899 | ! cloud phase determination |
|---|
| 900 | IF (iflag_t_glace.GE.4) THEN |
|---|
| 901 | ! For iflag_t_glace GE 4 the phase partition function dependends on temperature AND distance to cloud top |
|---|
| 902 | CALL distance_to_cloud_top(klon,klev,k,temp,pplay,paprs,rneb,distcltop1D,temp_cltop1D) |
|---|
| 903 | ENDIF |
|---|
| 904 | CALL icefrac_lscp(klon, zt(:), iflag_ice_thermo, distcltop1D(:),temp_cltop1D(:),zfice(:),dzfice(:)) |
|---|
| 905 | |
|---|
| 906 | |
|---|
| 907 | !--AB Activates a condensation scheme that allows for |
|---|
| 908 | !--ice supersaturation and contrails evolution from aviation |
|---|
| 909 | IF (ok_ice_supersat) THEN |
|---|
| 910 | |
|---|
| 911 | !--Calculate the shear value (input for condensation and ice supersat) |
|---|
| 912 | DO i = 1, klon |
|---|
| 913 | !--Cell thickness [m] |
|---|
| 914 | delta_z = ( paprs(i,k) - paprs(i,k+1) ) / RG / pplay(i,k) * Tbef(i) * RD |
|---|
| 915 | IF ( iftop ) THEN |
|---|
| 916 | ! top |
|---|
| 917 | shear(i) = SQRT( ( (u_seri(i,k) - u_seri(i,k-1)) / delta_z )**2. & |
|---|
| 918 | + ( (v_seri(i,k) - v_seri(i,k-1)) / delta_z )**2. ) |
|---|
| 919 | ELSEIF ( k .EQ. 1 ) THEN |
|---|
| 920 | ! surface |
|---|
| 921 | shear(i) = SQRT( ( (u_seri(i,k+1) - u_seri(i,k)) / delta_z )**2. & |
|---|
| 922 | + ( (v_seri(i,k+1) - v_seri(i,k)) / delta_z )**2. ) |
|---|
| 923 | ELSE |
|---|
| 924 | ! other layers |
|---|
| 925 | shear(i) = SQRT( ( ( (u_seri(i,k+1) + u_seri(i,k)) / 2. & |
|---|
| 926 | - (u_seri(i,k) + u_seri(i,k-1)) / 2. ) / delta_z )**2. & |
|---|
| 927 | + ( ( (v_seri(i,k+1) + v_seri(i,k)) / 2. & |
|---|
| 928 | - (v_seri(i,k) + v_seri(i,k-1)) / 2. ) / delta_z )**2. ) |
|---|
| 929 | ENDIF |
|---|
| 930 | ENDDO |
|---|
| 931 | |
|---|
| 932 | !--------------------------------------------- |
|---|
| 933 | !-- CONDENSATION AND ICE SUPERSATURATION -- |
|---|
| 934 | !--------------------------------------------- |
|---|
| 935 | |
|---|
| 936 | CALL condensation_ice_supersat( & |
|---|
| 937 | klon, dtime, missing_val, & |
|---|
| 938 | pplay(:,k), paprs(:,k), paprs(:,k+1), & |
|---|
| 939 | cf_seri(:,k), rvc_seri(:,k), ratio_qi_qtot(:,k), & |
|---|
| 940 | shear(:), pbl_eps(:,k), cell_area(:), & |
|---|
| 941 | Tbef(:), zq(:), zqs(:), gammasat(:), ratqs(:,k), keepgoing(:), & |
|---|
| 942 | rneb(:,k), zqn(:), qvc(:), issrfra(:,k), qissr(:,k), & |
|---|
| 943 | dcf_sub(:,k), dcf_con(:,k), dcf_mix(:,k), & |
|---|
| 944 | dqi_adj(:,k), dqi_sub(:,k), dqi_con(:,k), dqi_mix(:,k), & |
|---|
| 945 | dqvc_adj(:,k), dqvc_sub(:,k), dqvc_con(:,k), dqvc_mix(:,k), & |
|---|
| 946 | Tcontr(:,k), qcontr(:,k), qcontr2(:,k), fcontrN(:,k), fcontrP(:,k), & |
|---|
| 947 | flight_dist(:,k), flight_h2o(:,k), & |
|---|
| 948 | dcf_avi(:,k), dqi_avi(:,k), dqvc_avi(:,k)) |
|---|
| 949 | |
|---|
| 950 | |
|---|
| 951 | !--If .TRUE., calls an externalised version of the generalised |
|---|
| 952 | !--lognormal condensation scheme (Bony and Emanuel 2001) |
|---|
| 953 | !--Numerically, convergence is conserved with this option |
|---|
| 954 | !--The objective is to simplify LSCP |
|---|
| 955 | ELSEIF ( ok_external_lognormal ) THEN |
|---|
| 956 | |
|---|
| 957 | CALL condensation_lognormal( & |
|---|
| 958 | klon, Tbef(:), zq(:), zqs(:), gammasat(:), ratqs(:,k), & |
|---|
| 959 | keepgoing(:), rneb(:,k), zqn(:), qvc(:)) |
|---|
| 960 | |
|---|
| 961 | |
|---|
| 962 | ELSE !--Generalised lognormal (Bony and Emanuel 2001) |
|---|
| 963 | |
|---|
| 964 | DO i=1,klon !todoan : check if loop in i is needed |
|---|
| 965 | |
|---|
| 966 | IF (keepgoing(i)) THEN |
|---|
| 967 | |
|---|
| 968 | zpdf_sig(i)=ratqs(i,k)*zq(i) |
|---|
| 969 | zpdf_k(i)=-sqrt(log(1.+(zpdf_sig(i)/zq(i))**2)) |
|---|
| 970 | zpdf_delta(i)=log(zq(i)/(gammasat(i)*zqs(i))) |
|---|
| 971 | zpdf_a(i)=zpdf_delta(i)/(zpdf_k(i)*sqrt(2.)) |
|---|
| 972 | zpdf_b(i)=zpdf_k(i)/(2.*sqrt(2.)) |
|---|
| 973 | zpdf_e1(i)=zpdf_a(i)-zpdf_b(i) |
|---|
| 974 | zpdf_e1(i)=sign(min(ABS(zpdf_e1(i)),5.),zpdf_e1(i)) |
|---|
| 975 | zpdf_e1(i)=1.-erf(zpdf_e1(i)) |
|---|
| 976 | zpdf_e2(i)=zpdf_a(i)+zpdf_b(i) |
|---|
| 977 | zpdf_e2(i)=sign(min(ABS(zpdf_e2(i)),5.),zpdf_e2(i)) |
|---|
| 978 | zpdf_e2(i)=1.-erf(zpdf_e2(i)) |
|---|
| 979 | |
|---|
| 980 | IF (zpdf_e1(i).LT.1.e-10) THEN |
|---|
| 981 | rneb(i,k)=0. |
|---|
| 982 | zqn(i)=zqs(i) |
|---|
| 983 | !--AB grid-mean vapor in the cloud - we assume saturation adjustment |
|---|
| 984 | qvc(i) = 0. |
|---|
| 985 | ELSE |
|---|
| 986 | rneb(i,k)=0.5*zpdf_e1(i) |
|---|
| 987 | zqn(i)=zq(i)*zpdf_e2(i)/zpdf_e1(i) |
|---|
| 988 | !--AB grid-mean vapor in the cloud - we assume saturation adjustment |
|---|
| 989 | qvc(i) = rneb(i,k) * zqs(i) |
|---|
| 990 | ENDIF |
|---|
| 991 | |
|---|
| 992 | ENDIF ! keepgoing |
|---|
| 993 | ENDDO ! loop on klon |
|---|
| 994 | |
|---|
| 995 | ENDIF ! .NOT. ok_ice_supersat |
|---|
| 996 | |
|---|
| 997 | DO i=1,klon |
|---|
| 998 | IF (keepgoing(i)) THEN |
|---|
| 999 | |
|---|
| 1000 | ! If vertical heterogeneity, change fraction by volume as well |
|---|
| 1001 | IF (iflag_cloudth_vert.GE.3) THEN |
|---|
| 1002 | ctot_vol(i,k)=rneb(i,k) |
|---|
| 1003 | rneblsvol(i,k)=ctot_vol(i,k) |
|---|
| 1004 | ENDIF |
|---|
| 1005 | |
|---|
| 1006 | |
|---|
| 1007 | ! P2.2.2> Approximative calculation of temperature variation DT |
|---|
| 1008 | ! due to condensation. |
|---|
| 1009 | ! Calculated variables: |
|---|
| 1010 | ! dT : temperature change due to condensation |
|---|
| 1011 | !--------------------------------------------------------------- |
|---|
| 1012 | |
|---|
| 1013 | |
|---|
| 1014 | IF (zfice(i).LT.1) THEN |
|---|
| 1015 | cste=RLVTT |
|---|
| 1016 | ELSE |
|---|
| 1017 | cste=RLSTT |
|---|
| 1018 | ENDIF |
|---|
| 1019 | |
|---|
| 1020 | qlbef(i)=max(0.,zqn(i)-zqs(i)) |
|---|
| 1021 | num = -Tbef(i)+zt(i)+rneb(i,k)*((1-zfice(i))*RLVTT & |
|---|
| 1022 | +zfice(i)*RLSTT)/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i)))*qlbef(i) |
|---|
| 1023 | denom = 1.+rneb(i,k)*((1-zfice(i))*RLVTT+zfice(i)*RLSTT)/cste*zdqs(i) & |
|---|
| 1024 | -(RLSTT-RLVTT)/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i)))*rneb(i,k) & |
|---|
| 1025 | *qlbef(i)*dzfice(i) |
|---|
| 1026 | ! here we update a provisory temperature variable that only serves in the iteration |
|---|
| 1027 | ! process |
|---|
| 1028 | DT(i)=num/denom |
|---|
| 1029 | n_i(i)=n_i(i)+1 |
|---|
| 1030 | |
|---|
| 1031 | ENDIF ! end keepgoing |
|---|
| 1032 | |
|---|
| 1033 | ENDDO ! end loop on i |
|---|
| 1034 | |
|---|
| 1035 | ENDDO ! iter=1,iflag_fisrtilp_qsat+1 |
|---|
| 1036 | |
|---|
| 1037 | ! P2.3> Final quantities calculation |
|---|
| 1038 | ! Calculated variables: |
|---|
| 1039 | ! rneb : cloud fraction |
|---|
| 1040 | ! zcond: mean condensed water in the mesh |
|---|
| 1041 | ! zqn : mean water vapor in the mesh |
|---|
| 1042 | ! zfice: ice fraction in clouds |
|---|
| 1043 | ! zt : temperature |
|---|
| 1044 | ! rhcl : clear-sky relative humidity |
|---|
| 1045 | ! ---------------------------------------------------------------- |
|---|
| 1046 | |
|---|
| 1047 | |
|---|
| 1048 | ! For iflag_t_glace GE 4 the phase partition function dependends on temperature AND distance to cloud top |
|---|
| 1049 | IF (iflag_t_glace.GE.4) THEN |
|---|
| 1050 | CALL distance_to_cloud_top(klon,klev,k,temp,pplay,paprs,rneb,distcltop1D,temp_cltop1D) |
|---|
| 1051 | distcltop(:,k)=distcltop1D(:) |
|---|
| 1052 | temp_cltop(:,k)=temp_cltop1D(:) |
|---|
| 1053 | ENDIF |
|---|
| 1054 | ! Partition function in stratiform clouds (will be overwritten in boundary-layer MPCs) |
|---|
| 1055 | CALL icefrac_lscp(klon,zt,iflag_ice_thermo,distcltop1D,temp_cltop1D,zfice,dzfice) |
|---|
| 1056 | |
|---|
| 1057 | |
|---|
| 1058 | ! Water vapor update, Phase determination and subsequent latent heat exchange |
|---|
| 1059 | DO i=1, klon |
|---|
| 1060 | |
|---|
| 1061 | IF (mpc_bl_points(i,k) .GT. 0) THEN |
|---|
| 1062 | |
|---|
| 1063 | zcond(i) = MAX(0.0,qincloud_mpc(i))*rneb(i,k) |
|---|
| 1064 | ! following line is very strange and probably wrong |
|---|
| 1065 | rhcl(i,k)= (zqs(i)+zq(i))/2./zqs(i) |
|---|
| 1066 | ! water vapor update and partition function if thermals |
|---|
| 1067 | zq(i) = zq(i) - zcond(i) |
|---|
| 1068 | zfice(i)=zfice_th(i) |
|---|
| 1069 | |
|---|
| 1070 | ELSE |
|---|
| 1071 | |
|---|
| 1072 | ! Checks on rneb, rhcl and zqn |
|---|
| 1073 | IF (rneb(i,k) .LE. 0.0) THEN |
|---|
| 1074 | zqn(i) = 0.0 |
|---|
| 1075 | rneb(i,k) = 0.0 |
|---|
| 1076 | zcond(i) = 0.0 |
|---|
| 1077 | rhcl(i,k)=zq(i)/zqs(i) |
|---|
| 1078 | ELSE IF (rneb(i,k) .GE. 1.0) THEN |
|---|
| 1079 | zqn(i) = zq(i) |
|---|
| 1080 | rneb(i,k) = 1.0 |
|---|
| 1081 | IF ( ok_unadjusted_clouds ) THEN |
|---|
| 1082 | !--AB We relax the saturation adjustment assumption |
|---|
| 1083 | !-- qvc (grid-mean vapor in cloud) is calculated by the condensation scheme |
|---|
| 1084 | zcond(i) = MAX(0., zqn(i) - qvc(i)) |
|---|
| 1085 | ELSE |
|---|
| 1086 | zcond(i) = MAX(0.0,zqn(i)-zqs(i)) |
|---|
| 1087 | ENDIF |
|---|
| 1088 | rhcl(i,k)=1.0 |
|---|
| 1089 | ELSE |
|---|
| 1090 | IF ( ok_unadjusted_clouds ) THEN |
|---|
| 1091 | !--AB We relax the saturation adjustment assumption |
|---|
| 1092 | !-- qvc (grid-mean vapor in cloud) is calculated by the condensation scheme |
|---|
| 1093 | zcond(i) = MAX(0., zqn(i) * rneb(i,k) - qvc(i)) |
|---|
| 1094 | ELSE |
|---|
| 1095 | zcond(i) = MAX(0.0,zqn(i)-zqs(i))*rneb(i,k) |
|---|
| 1096 | ENDIF |
|---|
| 1097 | ! following line is very strange and probably wrong: |
|---|
| 1098 | rhcl(i,k)=(zqs(i)+zq(i))/2./zqs(i) |
|---|
| 1099 | ENDIF |
|---|
| 1100 | |
|---|
| 1101 | ! water vapor update |
|---|
| 1102 | zq(i) = zq(i) - zcond(i) |
|---|
| 1103 | |
|---|
| 1104 | ENDIF |
|---|
| 1105 | |
|---|
| 1106 | ! c_iso : routine that computes in-cloud supersaturation |
|---|
| 1107 | ! c_iso condensation of isotopes (zcond, zsursat, zfice, zq in input) |
|---|
| 1108 | |
|---|
| 1109 | ! temperature update due to phase change |
|---|
| 1110 | zt(i) = zt(i) + (1.-zfice(i))*zcond(i) & |
|---|
| 1111 | & * RLVTT/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i)+zcond(i))) & |
|---|
| 1112 | +zfice(i)*zcond(i) * RLSTT/RCPD/(1.0+RVTMP2*(zq(i)+zmqc(i)+zcond(i))) |
|---|
| 1113 | ENDDO |
|---|
| 1114 | |
|---|
| 1115 | ! If vertical heterogeneity, change volume fraction |
|---|
| 1116 | IF (iflag_cloudth_vert .GE. 3) THEN |
|---|
| 1117 | ctot_vol(1:klon,k)=min(max(ctot_vol(1:klon,k),0.),1.) |
|---|
| 1118 | rneblsvol(1:klon,k)=ctot_vol(1:klon,k) |
|---|
| 1119 | ENDIF |
|---|
| 1120 | |
|---|
| 1121 | !--AB Write diagnostics and tracers for ice supersaturation |
|---|
| 1122 | IF ( ok_ice_supersat ) THEN |
|---|
| 1123 | CALL calc_qsat_ecmwf(klon,zt,qzero,pplay(:,k),RTT,1,.false.,qsatl(:,k),zdqs) |
|---|
| 1124 | CALL calc_qsat_ecmwf(klon,zt,qzero,pplay(:,k),RTT,2,.false.,qsati(:,k),zdqs) |
|---|
| 1125 | |
|---|
| 1126 | DO i = 1, klon |
|---|
| 1127 | |
|---|
| 1128 | cf_seri(i,k) = rneb(i,k) |
|---|
| 1129 | |
|---|
| 1130 | IF ( .NOT. ok_unadjusted_clouds ) THEN |
|---|
| 1131 | qvc(i) = zqs(i) * rneb(i,k) |
|---|
| 1132 | ENDIF |
|---|
| 1133 | IF ( zq(i) .GT. min_qParent ) THEN |
|---|
| 1134 | rvc_seri(i,k) = qvc(i) / zq(i) |
|---|
| 1135 | ELSE |
|---|
| 1136 | rvc_seri(i,k) = min_ratio |
|---|
| 1137 | ENDIF |
|---|
| 1138 | !--The MIN barrier is NEEDED because of: |
|---|
| 1139 | !-- 1) very rare pathological cases of the lsc scheme (rvc = 1. + 1e-16 sometimes) |
|---|
| 1140 | !-- 2) the thermal scheme does NOT guarantee that qvc <= qvap (or even qincld <= qtot) |
|---|
| 1141 | !--The MAX barrier is a safeguard that should not be activated |
|---|
| 1142 | rvc_seri(i,k) = MIN(MAX(rvc_seri(i,k), 0.), 1.) |
|---|
| 1143 | |
|---|
| 1144 | !--Diagnostics |
|---|
| 1145 | gamma_cond(i,k) = gammasat(i) |
|---|
| 1146 | IF ( issrfra(i,k) .LT. eps ) THEN |
|---|
| 1147 | issrfra(i,k) = 0. |
|---|
| 1148 | qissr(i,k) = 0. |
|---|
| 1149 | ENDIF |
|---|
| 1150 | subfra(i,k) = 1. - cf_seri(i,k) - issrfra(i,k) |
|---|
| 1151 | qsub(i,k) = zq(i) - qvc(i) - qissr(i,k) |
|---|
| 1152 | IF ( subfra(i,k) .LT. eps ) THEN |
|---|
| 1153 | subfra(i,k) = 0. |
|---|
| 1154 | qsub(i,k) = 0. |
|---|
| 1155 | ENDIF |
|---|
| 1156 | qcld(i,k) = qvc(i) + zcond(i) |
|---|
| 1157 | IF ( cf_seri(i,k) .LT. eps ) THEN |
|---|
| 1158 | qcld(i,k) = 0. |
|---|
| 1159 | ENDIF |
|---|
| 1160 | ENDDO |
|---|
| 1161 | ENDIF |
|---|
| 1162 | |
|---|
| 1163 | |
|---|
| 1164 | ! ---------------------------------------------------------------- |
|---|
| 1165 | ! P3> Precipitation formation |
|---|
| 1166 | ! ---------------------------------------------------------------- |
|---|
| 1167 | |
|---|
| 1168 | !================================================================ |
|---|
| 1169 | IF (ok_poprecip) THEN |
|---|
| 1170 | |
|---|
| 1171 | DO i = 1, klon |
|---|
| 1172 | zoliql(i) = zcond(i) * ( 1. - zfice(i) ) |
|---|
| 1173 | zoliqi(i) = zcond(i) * zfice(i) |
|---|
| 1174 | ENDDO |
|---|
| 1175 | |
|---|
| 1176 | CALL poprecip_postcld(klon, dtime, paprs(:,k), paprs(:,k+1), pplay(:,k), & |
|---|
| 1177 | ctot_vol(:,k), ptconv(:,k), & |
|---|
| 1178 | zt, zq, zoliql, zoliqi, zfice, & |
|---|
| 1179 | rneb(:,k), znebprecipclr, znebprecipcld, & |
|---|
| 1180 | zrfl, zrflclr, zrflcld, & |
|---|
| 1181 | zifl, ziflclr, ziflcld, & |
|---|
| 1182 | qraindiag(:,k), qsnowdiag(:,k), dqrauto(:,k), & |
|---|
| 1183 | dqrcol(:,k), dqrmelt(:,k), dqrfreez(:,k), & |
|---|
| 1184 | dqsauto(:,k), dqsagg(:,k), dqsrim(:,k), & |
|---|
| 1185 | dqsmelt(:,k), dqsfreez(:,k) & |
|---|
| 1186 | ) |
|---|
| 1187 | |
|---|
| 1188 | DO i = 1, klon |
|---|
| 1189 | zoliq(i) = zoliql(i) + zoliqi(i) |
|---|
| 1190 | IF ( zoliq(i) .GT. 0. ) THEN |
|---|
| 1191 | zfice(i) = zoliqi(i)/zoliq(i) |
|---|
| 1192 | ELSE |
|---|
| 1193 | zfice(i) = 0.0 |
|---|
| 1194 | ENDIF |
|---|
| 1195 | |
|---|
| 1196 | ! calculation of specific content of condensates seen by radiative scheme |
|---|
| 1197 | IF (ok_radocond_snow) THEN |
|---|
| 1198 | radocond(i,k) = zoliq(i) |
|---|
| 1199 | radocondl(i,k)= radocond(i,k)*(1.-zfice(i)) |
|---|
| 1200 | radocondi(i,k)= radocond(i,k)*zfice(i)+qsnowdiag(i,k) |
|---|
| 1201 | ELSE |
|---|
| 1202 | radocond(i,k) = zoliq(i) |
|---|
| 1203 | radocondl(i,k)= radocond(i,k)*(1.-zfice(i)) |
|---|
| 1204 | radocondi(i,k)= radocond(i,k)*zfice(i) |
|---|
| 1205 | ENDIF |
|---|
| 1206 | ENDDO |
|---|
| 1207 | |
|---|
| 1208 | !================================================================ |
|---|
| 1209 | ELSE |
|---|
| 1210 | |
|---|
| 1211 | ! LTP: |
|---|
| 1212 | IF (iflag_evap_prec .GE. 4) THEN |
|---|
| 1213 | |
|---|
| 1214 | !Partitionning between precipitation coming from clouds and that coming from CS |
|---|
| 1215 | |
|---|
| 1216 | !0) Calculate tot_zneb, total cloud fraction above the cloud |
|---|
| 1217 | !assuming a maximum-random overlap (voir Jakob and Klein, 2000) |
|---|
| 1218 | |
|---|
| 1219 | DO i=1, klon |
|---|
| 1220 | tot_znebn(i) = 1. - (1.-tot_zneb(i))*(1 - max(rneb(i,k),zneb(i))) & |
|---|
| 1221 | /(1.-min(zneb(i),1.-smallestreal)) |
|---|
| 1222 | d_tot_zneb(i) = tot_znebn(i) - tot_zneb(i) |
|---|
| 1223 | tot_zneb(i) = tot_znebn(i) |
|---|
| 1224 | |
|---|
| 1225 | |
|---|
| 1226 | !1) Cloudy to clear air |
|---|
| 1227 | d_znebprecip_cld_clr(i) = znebprecipcld(i) - min(rneb(i,k),znebprecipcld(i)) |
|---|
| 1228 | IF (znebprecipcld(i) .GT. 0.) THEN |
|---|
| 1229 | d_zrfl_cld_clr(i) = d_znebprecip_cld_clr(i)/znebprecipcld(i)*zrflcld(i) |
|---|
| 1230 | d_zifl_cld_clr(i) = d_znebprecip_cld_clr(i)/znebprecipcld(i)*ziflcld(i) |
|---|
| 1231 | ELSE |
|---|
| 1232 | d_zrfl_cld_clr(i) = 0. |
|---|
| 1233 | d_zifl_cld_clr(i) = 0. |
|---|
| 1234 | ENDIF |
|---|
| 1235 | |
|---|
| 1236 | !2) Clear to cloudy air |
|---|
| 1237 | d_znebprecip_clr_cld(i) = max(0., min(znebprecipclr(i), rneb(i,k) - d_tot_zneb(i) - zneb(i))) |
|---|
| 1238 | IF (znebprecipclr(i) .GT. 0) THEN |
|---|
| 1239 | d_zrfl_clr_cld(i) = d_znebprecip_clr_cld(i)/znebprecipclr(i)*zrflclr(i) |
|---|
| 1240 | d_zifl_clr_cld(i) = d_znebprecip_clr_cld(i)/znebprecipclr(i)*ziflclr(i) |
|---|
| 1241 | ELSE |
|---|
| 1242 | d_zrfl_clr_cld(i) = 0. |
|---|
| 1243 | d_zifl_clr_cld(i) = 0. |
|---|
| 1244 | ENDIF |
|---|
| 1245 | |
|---|
| 1246 | !Update variables |
|---|
| 1247 | znebprecipcld(i) = znebprecipcld(i) + d_znebprecip_clr_cld(i) - d_znebprecip_cld_clr(i) |
|---|
| 1248 | znebprecipclr(i) = znebprecipclr(i) + d_znebprecip_cld_clr(i) - d_znebprecip_clr_cld(i) |
|---|
| 1249 | zrflcld(i) = zrflcld(i) + d_zrfl_clr_cld(i) - d_zrfl_cld_clr(i) |
|---|
| 1250 | ziflcld(i) = ziflcld(i) + d_zifl_clr_cld(i) - d_zifl_cld_clr(i) |
|---|
| 1251 | zrflclr(i) = zrflclr(i) + d_zrfl_cld_clr(i) - d_zrfl_clr_cld(i) |
|---|
| 1252 | ziflclr(i) = ziflclr(i) + d_zifl_cld_clr(i) - d_zifl_clr_cld(i) |
|---|
| 1253 | |
|---|
| 1254 | ! c_iso do the same thing for isotopes precip |
|---|
| 1255 | ENDDO |
|---|
| 1256 | ENDIF |
|---|
| 1257 | |
|---|
| 1258 | |
|---|
| 1259 | ! Autoconversion |
|---|
| 1260 | ! ------------------------------------------------------------------------------- |
|---|
| 1261 | |
|---|
| 1262 | |
|---|
| 1263 | ! Initialisation of zoliq and radocond variables |
|---|
| 1264 | |
|---|
| 1265 | DO i = 1, klon |
|---|
| 1266 | zoliq(i) = zcond(i) |
|---|
| 1267 | zoliqi(i)= zoliq(i)*zfice(i) |
|---|
| 1268 | zoliql(i)= zoliq(i)*(1.-zfice(i)) |
|---|
| 1269 | ! c_iso : initialisation of zoliq* also for isotopes |
|---|
| 1270 | zrho(i,k) = pplay(i,k) / zt(i) / RD |
|---|
| 1271 | zdz(i) = (paprs(i,k)-paprs(i,k+1)) / (zrho(i,k)*RG) |
|---|
| 1272 | iwc(i) = 0. |
|---|
| 1273 | zneb(i) = MAX(rneb(i,k),seuil_neb) |
|---|
| 1274 | radocond(i,k) = zoliq(i)/REAL(niter_lscp+1) |
|---|
| 1275 | radocondi(i,k)=zoliq(i)*zfice(i)/REAL(niter_lscp+1) |
|---|
| 1276 | radocondl(i,k)=zoliq(i)*(1.-zfice(i))/REAL(niter_lscp+1) |
|---|
| 1277 | ENDDO |
|---|
| 1278 | |
|---|
| 1279 | |
|---|
| 1280 | DO n = 1, niter_lscp |
|---|
| 1281 | |
|---|
| 1282 | DO i=1,klon |
|---|
| 1283 | IF (rneb(i,k).GT.0.0) THEN |
|---|
| 1284 | iwc(i) = zrho(i,k) * zoliqi(i) / zneb(i) ! in-cloud ice condensate content |
|---|
| 1285 | ENDIF |
|---|
| 1286 | ENDDO |
|---|
| 1287 | |
|---|
| 1288 | CALL fallice_velocity(klon,iwc(:),zt(:),zrho(:,k),pplay(:,k),ptconv(:,k),velo(:,k)) |
|---|
| 1289 | |
|---|
| 1290 | DO i = 1, klon |
|---|
| 1291 | |
|---|
| 1292 | IF (rneb(i,k).GT.0.0) THEN |
|---|
| 1293 | |
|---|
| 1294 | ! Initialization of zrain, zsnow and zprecip: |
|---|
| 1295 | zrain=0. |
|---|
| 1296 | zsnow=0. |
|---|
| 1297 | zprecip=0. |
|---|
| 1298 | ! c_iso same init for isotopes. Externalisation? |
|---|
| 1299 | |
|---|
| 1300 | IF (zneb(i).EQ.seuil_neb) THEN |
|---|
| 1301 | zprecip = 0.0 |
|---|
| 1302 | zsnow = 0.0 |
|---|
| 1303 | zrain= 0.0 |
|---|
| 1304 | ELSE |
|---|
| 1305 | |
|---|
| 1306 | IF (ptconv(i,k)) THEN ! if convective point |
|---|
| 1307 | zcl=cld_lc_con |
|---|
| 1308 | zct=1./cld_tau_con |
|---|
| 1309 | zexpo=cld_expo_con |
|---|
| 1310 | ffallv=ffallv_con |
|---|
| 1311 | ELSE |
|---|
| 1312 | zcl=cld_lc_lsc |
|---|
| 1313 | zct=1./cld_tau_lsc |
|---|
| 1314 | zexpo=cld_expo_lsc |
|---|
| 1315 | ffallv=ffallv_lsc |
|---|
| 1316 | ENDIF |
|---|
| 1317 | |
|---|
| 1318 | |
|---|
| 1319 | ! if vertical heterogeneity is taken into account, we use |
|---|
| 1320 | ! the "true" volume fraction instead of a modified |
|---|
| 1321 | ! surface fraction (which is larger and artificially |
|---|
| 1322 | ! reduces the in-cloud water). |
|---|
| 1323 | |
|---|
| 1324 | ! Liquid water quantity to remove: zchau (Sundqvist, 1978) |
|---|
| 1325 | ! dqliq/dt=-qliq/tau*(1-exp(-qcin/clw)**2) |
|---|
| 1326 | !......................................................... |
|---|
| 1327 | IF ((iflag_cloudth_vert.GE.3).AND.(iflag_rain_incloud_vol.EQ.1)) THEN |
|---|
| 1328 | |
|---|
| 1329 | ! if vertical heterogeneity is taken into account, we use |
|---|
| 1330 | ! the "true" volume fraction instead of a modified |
|---|
| 1331 | ! surface fraction (which is larger and artificially |
|---|
| 1332 | ! reduces the in-cloud water). |
|---|
| 1333 | effective_zneb=ctot_vol(i,k) |
|---|
| 1334 | ELSE |
|---|
| 1335 | effective_zneb=zneb(i) |
|---|
| 1336 | ENDIF |
|---|
| 1337 | |
|---|
| 1338 | |
|---|
| 1339 | IF (iflag_autoconversion .EQ. 2) THEN |
|---|
| 1340 | ! two-steps resolution with niter_lscp=1 sufficient |
|---|
| 1341 | ! we first treat the second term (with exponential) in an explicit way |
|---|
| 1342 | ! and then treat the first term (-q/tau) in an exact way |
|---|
| 1343 | zchau=zoliql(i)*(1.-exp(-dtime/REAL(niter_lscp)*zct & |
|---|
| 1344 | *(1.-exp(-(zoliql(i)/effective_zneb/zcl)**zexpo)))) |
|---|
| 1345 | ELSE |
|---|
| 1346 | ! old explicit resolution with subtimesteps |
|---|
| 1347 | zchau = zct*dtime/REAL(niter_lscp)*zoliql(i) & |
|---|
| 1348 | *(1.0-EXP(-(zoliql(i)/effective_zneb/zcl)**zexpo)) |
|---|
| 1349 | ENDIF |
|---|
| 1350 | |
|---|
| 1351 | |
|---|
| 1352 | ! Ice water quantity to remove (Zender & Kiehl, 1997) |
|---|
| 1353 | ! dqice/dt=1/rho*d(rho*wice*qice)/dz |
|---|
| 1354 | !.................................... |
|---|
| 1355 | IF (iflag_autoconversion .EQ. 2) THEN |
|---|
| 1356 | ! exact resolution, niter_lscp=1 is sufficient but works only |
|---|
| 1357 | ! with iflag_vice=0 |
|---|
| 1358 | IF (zoliqi(i) .GT. 0.) THEN |
|---|
| 1359 | zfroi=(zoliqi(i)-((zoliqi(i)**(-dice_velo)) & |
|---|
| 1360 | +dice_velo*dtime/REAL(niter_lscp)*cice_velo/zdz(i)*ffallv)**(-1./dice_velo)) |
|---|
| 1361 | ELSE |
|---|
| 1362 | zfroi=0. |
|---|
| 1363 | ENDIF |
|---|
| 1364 | ELSE |
|---|
| 1365 | ! old explicit resolution with subtimesteps |
|---|
| 1366 | zfroi = dtime/REAL(niter_lscp)/zdz(i)*zoliqi(i)*velo(i,k) |
|---|
| 1367 | ENDIF |
|---|
| 1368 | |
|---|
| 1369 | zrain = MIN(MAX(zchau,0.0),zoliql(i)) |
|---|
| 1370 | zsnow = MIN(MAX(zfroi,0.0),zoliqi(i)) |
|---|
| 1371 | zprecip = MAX(zrain + zsnow,0.0) |
|---|
| 1372 | |
|---|
| 1373 | ENDIF |
|---|
| 1374 | |
|---|
| 1375 | IF (iflag_autoconversion .GE. 1) THEN |
|---|
| 1376 | ! debugged version with phase conservation through the autoconversion process |
|---|
| 1377 | zoliql(i) = MAX(zoliql(i)-1.*zrain , 0.0) |
|---|
| 1378 | zoliqi(i) = MAX(zoliqi(i)-1.*zsnow , 0.0) |
|---|
| 1379 | zoliq(i) = MAX(zoliq(i)-zprecip , 0.0) |
|---|
| 1380 | ELSE |
|---|
| 1381 | ! bugged version with phase resetting |
|---|
| 1382 | zoliql(i) = MAX(zoliq(i)*(1.-zfice(i))-1.*zrain , 0.0) |
|---|
| 1383 | zoliqi(i) = MAX(zoliq(i)*zfice(i)-1.*zsnow , 0.0) |
|---|
| 1384 | zoliq(i) = MAX(zoliq(i)-zprecip , 0.0) |
|---|
| 1385 | ENDIF |
|---|
| 1386 | |
|---|
| 1387 | ! c_iso: call isotope_conversion (for readibility) or duplicate |
|---|
| 1388 | |
|---|
| 1389 | radocond(i,k) = radocond(i,k) + zoliq(i)/REAL(niter_lscp+1) |
|---|
| 1390 | radocondl(i,k) = radocondl(i,k) + zoliql(i)/REAL(niter_lscp+1) |
|---|
| 1391 | radocondi(i,k) = radocondi(i,k) + zoliqi(i)/REAL(niter_lscp+1) |
|---|
| 1392 | |
|---|
| 1393 | ENDIF ! rneb >0 |
|---|
| 1394 | |
|---|
| 1395 | ENDDO ! i = 1,klon |
|---|
| 1396 | |
|---|
| 1397 | ENDDO ! n = 1,niter |
|---|
| 1398 | |
|---|
| 1399 | ! Precipitation flux calculation |
|---|
| 1400 | |
|---|
| 1401 | DO i = 1, klon |
|---|
| 1402 | |
|---|
| 1403 | IF (iflag_evap_prec.GE.4) THEN |
|---|
| 1404 | ziflprev(i)=ziflcld(i) |
|---|
| 1405 | ELSE |
|---|
| 1406 | ziflprev(i)=zifl(i)*zneb(i) |
|---|
| 1407 | ENDIF |
|---|
| 1408 | |
|---|
| 1409 | IF (rneb(i,k) .GT. 0.0) THEN |
|---|
| 1410 | |
|---|
| 1411 | ! CR&JYG: We account for the Wegener-Findeisen-Bergeron process in the precipitation flux: |
|---|
| 1412 | ! If T<0C, liquid precip are converted into ice, which leads to an increase in |
|---|
| 1413 | ! temperature DeltaT. The effect of DeltaT on condensates and precipitation is roughly |
|---|
| 1414 | ! taken into account through a linearization of the equations and by approximating |
|---|
| 1415 | ! the liquid precipitation process with a "threshold" process. We assume that |
|---|
| 1416 | ! condensates are not modified during this operation. Liquid precipitation is |
|---|
| 1417 | ! removed (in the limit DeltaT<273.15-T). Solid precipitation increases. |
|---|
| 1418 | ! Water vapor increases as well |
|---|
| 1419 | ! Note that compared to fisrtilp, we always assume iflag_bergeron=2 |
|---|
| 1420 | |
|---|
| 1421 | zqpreci(i)=(zcond(i)-zoliq(i))*zfice(i) |
|---|
| 1422 | zqprecl(i)=(zcond(i)-zoliq(i))*(1.-zfice(i)) |
|---|
| 1423 | zcp=RCPD*(1.0+RVTMP2*(zq(i)+zmqc(i)+zcond(i))) |
|---|
| 1424 | coef1 = rneb(i,k)*RLSTT/zcp*zdqsdT_raw(i) |
|---|
| 1425 | ! Computation of DT if all the liquid precip freezes |
|---|
| 1426 | DeltaT = RLMLT*zqprecl(i) / (zcp*(1.+coef1)) |
|---|
| 1427 | ! T should not exceed the freezing point |
|---|
| 1428 | ! that is Delta > RTT-zt(i) |
|---|
| 1429 | DeltaT = max( min( RTT-zt(i), DeltaT) , 0. ) |
|---|
| 1430 | zt(i) = zt(i) + DeltaT |
|---|
| 1431 | ! water vaporization due to temp. increase |
|---|
| 1432 | Deltaq = rneb(i,k)*zdqsdT_raw(i)*DeltaT |
|---|
| 1433 | ! we add this vaporized water to the total vapor and we remove it from the precip |
|---|
| 1434 | zq(i) = zq(i) + Deltaq |
|---|
| 1435 | ! The three "max" lines herebelow protect from rounding errors |
|---|
| 1436 | zcond(i) = max( zcond(i)- Deltaq, 0. ) |
|---|
| 1437 | ! liquid precipitation converted to ice precip |
|---|
| 1438 | Deltaqprecl = -zcp/RLMLT*(1.+coef1)*DeltaT |
|---|
| 1439 | zqprecl(i) = max( zqprecl(i) + Deltaqprecl, 0. ) |
|---|
| 1440 | ! iced water budget |
|---|
| 1441 | zqpreci(i) = max (zqpreci(i) - Deltaqprecl - Deltaq, 0.) |
|---|
| 1442 | |
|---|
| 1443 | ! c_iso : mv here condensation of isotopes + redispatchage en precip |
|---|
| 1444 | |
|---|
| 1445 | IF (iflag_evap_prec.GE.4) THEN |
|---|
| 1446 | zrflcld(i) = zrflcld(i)+zqprecl(i) & |
|---|
| 1447 | *(paprs(i,k)-paprs(i,k+1))/(RG*dtime) |
|---|
| 1448 | ziflcld(i) = ziflcld(i)+ zqpreci(i) & |
|---|
| 1449 | *(paprs(i,k)-paprs(i,k+1))/(RG*dtime) |
|---|
| 1450 | znebprecipcld(i) = rneb(i,k) |
|---|
| 1451 | zrfl(i) = zrflcld(i) + zrflclr(i) |
|---|
| 1452 | zifl(i) = ziflcld(i) + ziflclr(i) |
|---|
| 1453 | ELSE |
|---|
| 1454 | zrfl(i) = zrfl(i)+ zqprecl(i) & |
|---|
| 1455 | *(paprs(i,k)-paprs(i,k+1))/(RG*dtime) |
|---|
| 1456 | zifl(i) = zifl(i)+ zqpreci(i) & |
|---|
| 1457 | *(paprs(i,k)-paprs(i,k+1))/(RG*dtime) |
|---|
| 1458 | ENDIF |
|---|
| 1459 | ! c_iso : same for isotopes |
|---|
| 1460 | |
|---|
| 1461 | ENDIF ! rneb>0 |
|---|
| 1462 | |
|---|
| 1463 | ENDDO |
|---|
| 1464 | |
|---|
| 1465 | ! LTP: limit of surface cloud fraction covered by precipitation when the local intensity of the flux is below rain_int_min |
|---|
| 1466 | ! if iflag_evap_prec>=4 |
|---|
| 1467 | IF (iflag_evap_prec.GE.4) THEN |
|---|
| 1468 | |
|---|
| 1469 | DO i=1,klon |
|---|
| 1470 | |
|---|
| 1471 | IF ((zrflclr(i) + ziflclr(i)) .GT. 0. ) THEN |
|---|
| 1472 | znebprecipclr(i) = min(znebprecipclr(i),max(zrflclr(i)/ & |
|---|
| 1473 | (MAX(znebprecipclr(i),seuil_neb)*rain_int_min), ziflclr(i)/(MAX(znebprecipclr(i),seuil_neb)*rain_int_min))) |
|---|
| 1474 | ELSE |
|---|
| 1475 | znebprecipclr(i)=0.0 |
|---|
| 1476 | ENDIF |
|---|
| 1477 | |
|---|
| 1478 | IF ((zrflcld(i) + ziflcld(i)) .GT. 0.) THEN |
|---|
| 1479 | znebprecipcld(i) = min(znebprecipcld(i), max(zrflcld(i)/ & |
|---|
| 1480 | (MAX(znebprecipcld(i),seuil_neb)*rain_int_min), ziflcld(i)/(MAX(znebprecipcld(i),seuil_neb)*rain_int_min))) |
|---|
| 1481 | ELSE |
|---|
| 1482 | znebprecipcld(i)=0.0 |
|---|
| 1483 | ENDIF |
|---|
| 1484 | |
|---|
| 1485 | ENDDO |
|---|
| 1486 | |
|---|
| 1487 | ENDIF |
|---|
| 1488 | |
|---|
| 1489 | |
|---|
| 1490 | ENDIF ! ok_poprecip |
|---|
| 1491 | |
|---|
| 1492 | ! End of precipitation formation |
|---|
| 1493 | ! -------------------------------- |
|---|
| 1494 | |
|---|
| 1495 | |
|---|
| 1496 | ! Calculation of cloud condensates amount seen by radiative scheme |
|---|
| 1497 | !----------------------------------------------------------------- |
|---|
| 1498 | |
|---|
| 1499 | ! Calculation of the concentration of condensates seen by the radiation scheme |
|---|
| 1500 | ! for liquid phase, we take radocondl |
|---|
| 1501 | ! for ice phase, we take radocondi if we neglect snowfall, otherwise (ok_radocond_snow=true) |
|---|
| 1502 | ! we recalculate radocondi to account for contributions from the precipitation flux |
|---|
| 1503 | ! TODO: for the moment, we deactivate this option when ok_poprecip=.true. |
|---|
| 1504 | |
|---|
| 1505 | IF ((ok_radocond_snow) .AND. (k .LT. klev) .AND. (.NOT. ok_poprecip)) THEN |
|---|
| 1506 | ! for the solid phase (crystals + snowflakes) |
|---|
| 1507 | ! we recalculate radocondi by summing |
|---|
| 1508 | ! the ice content calculated in the mesh |
|---|
| 1509 | ! + the contribution of the non-evaporated snowfall |
|---|
| 1510 | ! from the overlying layer |
|---|
| 1511 | DO i=1,klon |
|---|
| 1512 | IF (ziflprev(i) .NE. 0.0) THEN |
|---|
| 1513 | radocondi(i,k)=zoliq(i)*zfice(i)+zqpreci(i)+ziflprev(i)/zrho(i,k+1)/velo(i,k+1) |
|---|
| 1514 | ELSE |
|---|
| 1515 | radocondi(i,k)=zoliq(i)*zfice(i)+zqpreci(i) |
|---|
| 1516 | ENDIF |
|---|
| 1517 | radocond(i,k)=radocondl(i,k)+radocondi(i,k) |
|---|
| 1518 | ENDDO |
|---|
| 1519 | ENDIF |
|---|
| 1520 | |
|---|
| 1521 | ! caculate the percentage of ice in "radocond" so cloud+precip seen by the radiation scheme |
|---|
| 1522 | DO i=1,klon |
|---|
| 1523 | IF (radocond(i,k) .GT. 0.) THEN |
|---|
| 1524 | radicefrac(i,k)=MIN(MAX(radocondi(i,k)/radocond(i,k),0.),1.) |
|---|
| 1525 | ENDIF |
|---|
| 1526 | ENDDO |
|---|
| 1527 | |
|---|
| 1528 | ! ---------------------------------------------------------------- |
|---|
| 1529 | ! P4> Wet scavenging |
|---|
| 1530 | ! ---------------------------------------------------------------- |
|---|
| 1531 | |
|---|
| 1532 | !Scavenging through nucleation in the layer |
|---|
| 1533 | |
|---|
| 1534 | DO i = 1,klon |
|---|
| 1535 | |
|---|
| 1536 | IF(zcond(i).GT.zoliq(i)+1.e-10) THEN |
|---|
| 1537 | beta(i,k) = (zcond(i)-zoliq(i))/zcond(i)/dtime |
|---|
| 1538 | ELSE |
|---|
| 1539 | beta(i,k) = 0. |
|---|
| 1540 | ENDIF |
|---|
| 1541 | |
|---|
| 1542 | zprec_cond(i) = MAX(zcond(i)-zoliq(i),0.0)*(paprs(i,k)-paprs(i,k+1))/RG |
|---|
| 1543 | |
|---|
| 1544 | IF (rneb(i,k).GT.0.0.AND.zprec_cond(i).GT.0.) THEN |
|---|
| 1545 | |
|---|
| 1546 | IF (temp(i,k) .GE. t_glace_min) THEN |
|---|
| 1547 | zalpha_tr = a_tr_sca(3) |
|---|
| 1548 | ELSE |
|---|
| 1549 | zalpha_tr = a_tr_sca(4) |
|---|
| 1550 | ENDIF |
|---|
| 1551 | |
|---|
| 1552 | zfrac_lessi = 1. - EXP(zalpha_tr*zprec_cond(i)/zneb(i)) |
|---|
| 1553 | frac_nucl(i,k)= 1.-zneb(i)*zfrac_lessi |
|---|
| 1554 | |
|---|
| 1555 | ! Nucleation with a factor of -1 instead of -0.5 |
|---|
| 1556 | zfrac_lessi = 1. - EXP(-zprec_cond(i)/zneb(i)) |
|---|
| 1557 | |
|---|
| 1558 | ENDIF |
|---|
| 1559 | |
|---|
| 1560 | ENDDO |
|---|
| 1561 | |
|---|
| 1562 | ! Scavenging through impaction in the underlying layer |
|---|
| 1563 | |
|---|
| 1564 | DO kk = k-1, 1, -1 |
|---|
| 1565 | |
|---|
| 1566 | DO i = 1, klon |
|---|
| 1567 | |
|---|
| 1568 | IF (rneb(i,k).GT.0.0.AND.zprec_cond(i).GT.0.) THEN |
|---|
| 1569 | |
|---|
| 1570 | IF (temp(i,kk) .GE. t_glace_min) THEN |
|---|
| 1571 | zalpha_tr = a_tr_sca(1) |
|---|
| 1572 | ELSE |
|---|
| 1573 | zalpha_tr = a_tr_sca(2) |
|---|
| 1574 | ENDIF |
|---|
| 1575 | |
|---|
| 1576 | zfrac_lessi = 1. - EXP(zalpha_tr*zprec_cond(i)/zneb(i)) |
|---|
| 1577 | frac_impa(i,kk)= 1.-zneb(i)*zfrac_lessi |
|---|
| 1578 | |
|---|
| 1579 | ENDIF |
|---|
| 1580 | |
|---|
| 1581 | ENDDO |
|---|
| 1582 | |
|---|
| 1583 | ENDDO |
|---|
| 1584 | |
|---|
| 1585 | ! Outputs: |
|---|
| 1586 | !------------------------------- |
|---|
| 1587 | ! Precipitation fluxes at layer interfaces |
|---|
| 1588 | ! + precipitation fractions + |
|---|
| 1589 | ! temperature and water species tendencies |
|---|
| 1590 | DO i = 1, klon |
|---|
| 1591 | psfl(i,k)=zifl(i) |
|---|
| 1592 | prfl(i,k)=zrfl(i) |
|---|
| 1593 | pfraclr(i,k)=znebprecipclr(i) |
|---|
| 1594 | pfracld(i,k)=znebprecipcld(i) |
|---|
| 1595 | d_ql(i,k) = (1-zfice(i))*zoliq(i) |
|---|
| 1596 | d_qi(i,k) = zfice(i)*zoliq(i) |
|---|
| 1597 | d_q(i,k) = zq(i) - qt(i,k) |
|---|
| 1598 | ! c_iso: same for isotopes |
|---|
| 1599 | d_t(i,k) = zt(i) - temp(i,k) |
|---|
| 1600 | ENDDO |
|---|
| 1601 | |
|---|
| 1602 | |
|---|
| 1603 | ENDDO |
|---|
| 1604 | |
|---|
| 1605 | |
|---|
| 1606 | ! Rain or snow at the surface (depending on the first layer temperature) |
|---|
| 1607 | DO i = 1, klon |
|---|
| 1608 | snow(i) = zifl(i) |
|---|
| 1609 | rain(i) = zrfl(i) |
|---|
| 1610 | ! c_iso final output |
|---|
| 1611 | ENDDO |
|---|
| 1612 | |
|---|
| 1613 | IF (ncoreczq>0) THEN |
|---|
| 1614 | WRITE(lunout,*)'WARNING : ZQ in LSCP ',ncoreczq,' val < 1.e-15.' |
|---|
| 1615 | ENDIF |
|---|
| 1616 | |
|---|
| 1617 | |
|---|
| 1618 | RETURN |
|---|
| 1619 | |
|---|
| 1620 | END SUBROUTINE lscp |
|---|
| 1621 | !+++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++++ |
|---|
| 1622 | |
|---|
| 1623 | END MODULE lmdz_lscp |
|---|