[825] | 1 | MODULE limthd |
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| 2 | !!====================================================================== |
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| 3 | !! *** MODULE limthd *** |
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[1572] | 4 | !! LIM-3 : ice thermodynamic |
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[825] | 5 | !!====================================================================== |
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[1572] | 6 | !! History : LIM ! 2000-01 (M.A. Morales Maqueda, H. Goosse, T. Fichefet) LIM-1 |
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| 7 | !! 2.0 ! 2002-07 (C. Ethe, G. Madec) LIM-2 (F90 rewriting) |
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| 8 | !! 3.0 ! 2005-11 (M. Vancoppenolle) LIM-3 : Multi-layer thermodynamics + salinity variations |
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[2528] | 9 | !! - ! 2007-04 (M. Vancoppenolle) add lim_thd_glohec, lim_thd_con_dh and lim_thd_con_dif |
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[4688] | 10 | !! 3.2 ! 2009-07 (M. Vancoppenolle, Y. Aksenov, G. Madec) bug correction in wfx_snw |
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[2528] | 11 | !! 3.3 ! 2010-11 (G. Madec) corrected snow melting heat (due to factor betas) |
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[2715] | 12 | !! 4.0 ! 2011-02 (G. Madec) dynamical allocation |
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[4161] | 13 | !! - ! 2012-05 (C. Rousset) add penetration solar flux |
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[1572] | 14 | !!---------------------------------------------------------------------- |
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[825] | 15 | #if defined key_lim3 |
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| 16 | !!---------------------------------------------------------------------- |
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[834] | 17 | !! 'key_lim3' LIM3 sea-ice model |
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[825] | 18 | !!---------------------------------------------------------------------- |
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[3625] | 19 | !! lim_thd : thermodynamic of sea ice |
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| 20 | !! lim_thd_init : initialisation of sea-ice thermodynamic |
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[825] | 21 | !!---------------------------------------------------------------------- |
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[3625] | 22 | USE phycst ! physical constants |
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| 23 | USE dom_oce ! ocean space and time domain variables |
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[4205] | 24 | USE oce , ONLY : iatte, oatte |
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[3625] | 25 | USE ice ! LIM: sea-ice variables |
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| 26 | USE par_ice ! LIM: sea-ice parameters |
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| 27 | USE sbc_oce ! Surface boundary condition: ocean fields |
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| 28 | USE sbc_ice ! Surface boundary condition: ice fields |
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| 29 | USE thd_ice ! LIM thermodynamic sea-ice variables |
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| 30 | USE dom_ice ! LIM sea-ice domain |
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| 31 | USE domvvl ! domain: variable volume level |
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| 32 | USE limthd_dif ! LIM: thermodynamics, vertical diffusion |
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| 33 | USE limthd_dh ! LIM: thermodynamics, ice and snow thickness variation |
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| 34 | USE limthd_sal ! LIM: thermodynamics, ice salinity |
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| 35 | USE limthd_ent ! LIM: thermodynamics, ice enthalpy redistribution |
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| 36 | USE limtab ! LIM: 1D <==> 2D transformation |
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| 37 | USE limvar ! LIM: sea-ice variables |
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| 38 | USE lbclnk ! lateral boundary condition - MPP links |
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| 39 | USE lib_mpp ! MPP library |
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| 40 | USE wrk_nemo ! work arrays |
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| 41 | USE in_out_manager ! I/O manager |
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| 42 | USE prtctl ! Print control |
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| 43 | USE lib_fortran ! Fortran utilities (allows no signed zero when 'key_nosignedzero' defined) |
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[4161] | 44 | USE timing ! Timing |
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[4688] | 45 | USE cpl_oasis3, ONLY : lk_cpl |
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| 46 | USE limcons ! conservation tests |
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[825] | 47 | |
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| 48 | IMPLICIT NONE |
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| 49 | PRIVATE |
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| 50 | |
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[2528] | 51 | PUBLIC lim_thd ! called by limstp module |
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| 52 | PUBLIC lim_thd_init ! called by iceini module |
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[825] | 53 | |
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[4333] | 54 | REAL(wp) :: epsi10 = 1.e-10_wp ! |
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[825] | 55 | |
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| 56 | !! * Substitutions |
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| 57 | # include "domzgr_substitute.h90" |
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| 58 | # include "vectopt_loop_substitute.h90" |
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| 59 | !!---------------------------------------------------------------------- |
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[2528] | 60 | !! NEMO/LIM3 3.3 , UCL - NEMO Consortium (2010) |
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[1156] | 61 | !! $Id$ |
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[2528] | 62 | !! Software governed by the CeCILL licence (NEMOGCM/NEMO_CeCILL.txt) |
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[825] | 63 | !!---------------------------------------------------------------------- |
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| 64 | CONTAINS |
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| 65 | |
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[921] | 66 | SUBROUTINE lim_thd( kt ) |
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[825] | 67 | !!------------------------------------------------------------------- |
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| 68 | !! *** ROUTINE lim_thd *** |
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| 69 | !! |
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| 70 | !! ** Purpose : This routine manages the ice thermodynamic. |
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| 71 | !! |
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| 72 | !! ** Action : - Initialisation of some variables |
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| 73 | !! - Some preliminary computation (oceanic heat flux |
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| 74 | !! at the ice base, snow acc.,heat budget of the leads) |
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| 75 | !! - selection of the icy points and put them in an array |
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| 76 | !! - call lim_vert_ther for vert ice thermodynamic |
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| 77 | !! - back to the geographic grid |
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| 78 | !! - selection of points for lateral accretion |
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| 79 | !! - call lim_lat_acc for the ice accretion |
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| 80 | !! - back to the geographic grid |
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| 81 | !! |
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[1572] | 82 | !! ** References : H. Goosse et al. 1996, Bul. Soc. Roy. Sc. Liege, 65, 87-90 |
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| 83 | !!--------------------------------------------------------------------- |
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| 84 | INTEGER, INTENT(in) :: kt ! number of iteration |
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[825] | 85 | !! |
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[4688] | 86 | INTEGER :: ji, jj, jk, jl ! dummy loop indices |
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| 87 | INTEGER :: nbpb ! nb of icy pts for thermo. cal. |
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| 88 | INTEGER :: ii, ij ! temporary dummy loop index |
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| 89 | REAL(wp) :: zfric_umin = 0._wp ! lower bound for the friction velocity (cice value=5.e-04) |
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| 90 | REAL(wp) :: zch = 0.0057_wp ! heat transfer coefficient |
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| 91 | REAL(wp) :: zinda, zindb, zareamin |
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| 92 | REAL(wp) :: zfric_u, zqld, zqfr |
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| 93 | ! |
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| 94 | REAL(wp) :: zvi_b, zsmv_b, zei_b, zfs_b, zfw_b, zft_b |
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[825] | 95 | !!------------------------------------------------------------------- |
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[4161] | 96 | IF( nn_timing == 1 ) CALL timing_start('limthd') |
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[2715] | 97 | |
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[4688] | 98 | ! conservation test |
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| 99 | IF( ln_limdiahsb ) CALL lim_cons_hsm(0, 'limthd', zvi_b, zsmv_b, zei_b, zfw_b, zfs_b, zft_b) |
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[4161] | 100 | |
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[921] | 101 | !------------------------------------------------------------------------------! |
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| 102 | ! 1) Initialization of diagnostic variables ! |
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| 103 | !------------------------------------------------------------------------------! |
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[825] | 104 | |
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| 105 | !-------------------- |
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| 106 | ! 1.2) Heat content |
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| 107 | !-------------------- |
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[1572] | 108 | ! Change the units of heat content; from global units to J.m3 |
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[825] | 109 | DO jl = 1, jpl |
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[921] | 110 | DO jk = 1, nlay_i |
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| 111 | DO jj = 1, jpj |
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| 112 | DO ji = 1, jpi |
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| 113 | !0 if no ice and 1 if yes |
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[4333] | 114 | zindb = 1.0 - MAX( 0.0 , SIGN( 1.0 , - v_i(ji,jj,jl) + epsi10 ) ) |
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[4688] | 115 | !Energy of melting q(S,T) [J.m-3] |
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| 116 | e_i(ji,jj,jk,jl) = zindb * e_i(ji,jj,jk,jl) / ( area(ji,jj) * MAX( v_i(ji,jj,jl) , epsi10 ) ) * REAL( nlay_i ) |
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| 117 | !convert units ! very important that this line is here |
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| 118 | e_i(ji,jj,jk,jl) = e_i(ji,jj,jk,jl) * unit_fac |
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[921] | 119 | END DO |
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[825] | 120 | END DO |
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[921] | 121 | END DO |
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| 122 | DO jk = 1, nlay_s |
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| 123 | DO jj = 1, jpj |
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| 124 | DO ji = 1, jpi |
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| 125 | !0 if no ice and 1 if yes |
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[4333] | 126 | zindb = 1.0 - MAX( 0.0 , SIGN( 1.0 , - v_s(ji,jj,jl) + epsi10 ) ) |
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[4688] | 127 | !Energy of melting q(S,T) [J.m-3] |
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| 128 | e_s(ji,jj,jk,jl) = zindb * e_s(ji,jj,jk,jl) / ( area(ji,jj) * MAX( v_s(ji,jj,jl) , epsi10 ) ) * REAL( nlay_s ) |
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[921] | 129 | !convert units ! very important that this line is here |
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[4688] | 130 | e_s(ji,jj,jk,jl) = e_s(ji,jj,jk,jl) * unit_fac |
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[921] | 131 | END DO |
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[825] | 132 | END DO |
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[921] | 133 | END DO |
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[825] | 134 | END DO |
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| 135 | |
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[921] | 136 | ! 2) Partial computation of forcing for the thermodynamic sea ice model. ! |
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| 137 | !-----------------------------------------------------------------------------! |
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[825] | 138 | |
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[921] | 139 | !CDIR NOVERRCHK |
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| 140 | DO jj = 1, jpj |
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| 141 | !CDIR NOVERRCHK |
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| 142 | DO ji = 1, jpi |
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[4688] | 143 | zinda = tms(ji,jj) * ( 1._wp - MAX( 0._wp , SIGN( 1._wp , - at_i(ji,jj) + epsi10 ) ) ) ! 0 if no ice |
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[2528] | 144 | ! |
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[921] | 145 | ! ! solar irradiance transmission at the mixed layer bottom and used in the lead heat budget |
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| 146 | ! ! practically no "direct lateral ablation" |
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| 147 | ! |
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| 148 | ! ! net downward heat flux from the ice to the ocean, expressed as a function of ocean |
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| 149 | ! ! temperature and turbulent mixing (McPhee, 1992) |
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[4688] | 150 | ! |
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| 151 | ! --- Energy received in the lead, zqld is defined everywhere (J.m-2) --- ! |
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| 152 | zqld = tms(ji,jj) * rdt_ice * & |
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| 153 | & ( pfrld(ji,jj) * ( qsr(ji,jj) * oatte(ji,jj) & ! solar heat + clem modif |
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| 154 | & + qns(ji,jj) ) & ! non solar heat |
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| 155 | ! latent heat of precip (note that precip is included in qns but not in qns_ice) |
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| 156 | & + ( pfrld(ji,jj)**betas - pfrld(ji,jj) ) * sprecip(ji,jj) * ( cpic * ( MIN( tatm_ice(ji,jj), rt0_snow ) - rtt ) - lfus ) & |
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| 157 | & + ( 1._wp - pfrld(ji,jj) ) * ( tprecip(ji,jj) - sprecip(ji,jj) ) * rcp * ( tatm_ice(ji,jj) - rtt ) ) |
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[825] | 158 | |
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[4688] | 159 | !-- Energy needed to bring ocean surface layer until its freezing (<0, J.m-2) --- ! |
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| 160 | zqfr = tms(ji,jj) * rau0 * rcp * fse3t_m(ji,jj) * ( t_bo(ji,jj) - ( sst_m(ji,jj) + rt0 ) ) |
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| 161 | |
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| 162 | !-- Energy Budget of the leads (J.m-2). Must be < 0 to form ice |
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| 163 | qlead(ji,jj) = MIN( 0._wp , zqld - zqfr ) |
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| 164 | |
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| 165 | ! If there is ice and leads are warming, then transfer energy from the lead budget and use it for bottom melting |
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| 166 | IF( at_i(ji,jj) > epsi10 .AND. zqld > 0._wp ) THEN |
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| 167 | fhld (ji,jj) = zqld * r1_rdtice / at_i(ji,jj) ! divided by at_i since this is (re)multiplied by a_i in limthd_dh.F90 |
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| 168 | qlead(ji,jj) = 0._wp |
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| 169 | ENDIF |
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[2528] | 170 | ! |
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[4688] | 171 | !-- Energy from the turbulent oceanic heat flux --- ! |
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| 172 | !clem zfric_u = MAX ( MIN( SQRT( ust2s(ji,jj) ) , zfric_umax ) , zfric_umin ) |
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| 173 | zfric_u = MAX( SQRT( ust2s(ji,jj) ), zfric_umin ) |
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| 174 | fhtur(ji,jj) = MAX( 0._wp, zinda * rau0 * rcp * zch * zfric_u * ( ( sst_m(ji,jj) + rt0 ) - t_bo(ji,jj) ) ) ! W.m-2 |
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| 175 | ! upper bound for fhtur: we do not want SST to drop below Tfreeze. |
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| 176 | ! So we say that the heat retrieved from the ocean (fhtur+fhld) must be < to the heat necessary to reach Tfreeze (zqfr) |
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| 177 | ! This is not a clean budget, so that should be corrected at some point |
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| 178 | fhtur(ji,jj) = zinda * MIN( fhtur(ji,jj), - fhld(ji,jj) - zqfr * r1_rdtice / MAX( at_i(ji,jj), epsi10 ) ) |
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| 179 | |
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| 180 | ! ----------------------------------------- |
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| 181 | ! Net heat flux on top of ice-ocean [W.m-2] |
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| 182 | ! ----------------------------------------- |
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| 183 | ! First step here : heat flux at the ocean surface + precip |
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| 184 | ! Second step below : heat flux at the ice surface (after limthd_dif) |
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| 185 | hfx_in(ji,jj) = hfx_in(ji,jj) & |
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| 186 | ! heat flux above the ocean |
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| 187 | & + pfrld(ji,jj) * ( qns(ji,jj) + qsr(ji,jj) ) & |
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| 188 | ! latent heat of precip (note that precip is included in qns but not in qns_ice) |
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| 189 | & + ( 1._wp - pfrld(ji,jj) ) * sprecip(ji,jj) * ( cpic * ( MIN( tatm_ice(ji,jj), rt0_snow ) - rtt ) - lfus ) & |
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| 190 | & + ( 1._wp - pfrld(ji,jj) ) * ( tprecip(ji,jj) - sprecip(ji,jj) ) * rcp * ( tatm_ice(ji,jj) - rtt ) |
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| 191 | |
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| 192 | ! ----------------------------------------------------------------------------- |
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| 193 | ! Net heat flux that is retroceded to the ocean or taken from the ocean [W.m-2] |
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| 194 | ! ----------------------------------------------------------------------------- |
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| 195 | ! First step here : non solar + precip - qlead - qturb |
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| 196 | ! Second step in limthd_dh : heat remaining if total melt (zq_rema) |
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| 197 | ! Third step in limsbc : heat from ice-ocean mass exchange (zf_mass) + solar |
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| 198 | hfx_out(ji,jj) = hfx_out(ji,jj) & |
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| 199 | ! Non solar heat flux received by the ocean |
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| 200 | & + pfrld(ji,jj) * qns(ji,jj) & |
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| 201 | ! latent heat of precip (note that precip is included in qns but not in qns_ice) |
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| 202 | & + ( pfrld(ji,jj)**betas - pfrld(ji,jj) ) * sprecip(ji,jj) * ( cpic * ( MIN( tatm_ice(ji,jj), rt0_snow ) - rtt ) - lfus ) & |
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| 203 | & + ( 1._wp - pfrld(ji,jj) ) * ( tprecip(ji,jj) - sprecip(ji,jj) ) * rcp * ( tatm_ice(ji,jj) - rtt ) & |
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| 204 | ! heat flux taken from the ocean where there is open water ice formation |
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| 205 | & - qlead(ji,jj) * r1_rdtice & |
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| 206 | ! heat flux taken from the ocean during bottom growth/melt (fhld should be 0 while bott growth) |
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| 207 | & - at_i(ji,jj) * fhtur(ji,jj) & |
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| 208 | & - at_i(ji,jj) * fhld(ji,jj) |
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| 209 | |
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[825] | 210 | END DO |
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| 211 | END DO |
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| 212 | |
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[921] | 213 | !------------------------------------------------------------------------------! |
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| 214 | ! 3) Select icy points and fulfill arrays for the vectorial grid. |
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| 215 | !------------------------------------------------------------------------------! |
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[825] | 216 | |
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| 217 | DO jl = 1, jpl !loop over ice categories |
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| 218 | |
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[921] | 219 | IF( kt == nit000 .AND. lwp ) THEN |
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| 220 | WRITE(numout,*) ' lim_thd : transfer to 1D vectors. Category no : ', jl |
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| 221 | WRITE(numout,*) ' ~~~~~~~~' |
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| 222 | ENDIF |
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[825] | 223 | |
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[4333] | 224 | zareamin = epsi10 |
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[825] | 225 | nbpb = 0 |
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| 226 | DO jj = 1, jpj |
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| 227 | DO ji = 1, jpi |
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| 228 | IF ( a_i(ji,jj,jl) .gt. zareamin ) THEN |
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| 229 | nbpb = nbpb + 1 |
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| 230 | npb(nbpb) = (jj - 1) * jpi + ji |
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| 231 | ENDIF |
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| 232 | END DO |
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| 233 | END DO |
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| 234 | |
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[4333] | 235 | ! debug point to follow |
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| 236 | jiindex_1d = 0 |
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| 237 | IF( ln_nicep ) THEN |
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| 238 | DO ji = mi0(jiindx), mi1(jiindx) |
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| 239 | DO jj = mj0(jjindx), mj1(jjindx) |
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| 240 | jiindex_1d = (jj - 1) * jpi + ji |
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[4688] | 241 | WRITE(numout,*) ' lim_thd : Category no : ', jl |
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[4333] | 242 | END DO |
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| 243 | END DO |
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| 244 | ENDIF |
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| 245 | |
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[921] | 246 | !------------------------------------------------------------------------------! |
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| 247 | ! 4) Thermodynamic computation |
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| 248 | !------------------------------------------------------------------------------! |
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[825] | 249 | |
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[2715] | 250 | IF( lk_mpp ) CALL mpp_ini_ice( nbpb , numout ) |
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[869] | 251 | |
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[1572] | 252 | IF( nbpb > 0 ) THEN ! If there is no ice, do nothing. |
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[825] | 253 | |
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[921] | 254 | !------------------------- |
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| 255 | ! 4.1 Move to 1D arrays |
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| 256 | !------------------------- |
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[825] | 257 | |
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[1572] | 258 | CALL tab_2d_1d( nbpb, at_i_b (1:nbpb), at_i , jpi, jpj, npb(1:nbpb) ) |
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| 259 | CALL tab_2d_1d( nbpb, a_i_b (1:nbpb), a_i(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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| 260 | CALL tab_2d_1d( nbpb, ht_i_b (1:nbpb), ht_i(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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| 261 | CALL tab_2d_1d( nbpb, ht_s_b (1:nbpb), ht_s(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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[825] | 262 | |
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[1572] | 263 | CALL tab_2d_1d( nbpb, t_su_b (1:nbpb), t_su(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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| 264 | CALL tab_2d_1d( nbpb, sm_i_b (1:nbpb), sm_i(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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[825] | 265 | DO jk = 1, nlay_s |
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[1572] | 266 | CALL tab_2d_1d( nbpb, t_s_b(1:nbpb,jk), t_s(:,:,jk,jl) , jpi, jpj, npb(1:nbpb) ) |
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| 267 | CALL tab_2d_1d( nbpb, q_s_b(1:nbpb,jk), e_s(:,:,jk,jl) , jpi, jpj, npb(1:nbpb) ) |
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[825] | 268 | END DO |
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| 269 | DO jk = 1, nlay_i |
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[1572] | 270 | CALL tab_2d_1d( nbpb, t_i_b(1:nbpb,jk), t_i(:,:,jk,jl) , jpi, jpj, npb(1:nbpb) ) |
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| 271 | CALL tab_2d_1d( nbpb, q_i_b(1:nbpb,jk), e_i(:,:,jk,jl) , jpi, jpj, npb(1:nbpb) ) |
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| 272 | CALL tab_2d_1d( nbpb, s_i_b(1:nbpb,jk), s_i(:,:,jk,jl) , jpi, jpj, npb(1:nbpb) ) |
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[825] | 273 | END DO |
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| 274 | |
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[1572] | 275 | CALL tab_2d_1d( nbpb, tatm_ice_1d(1:nbpb), tatm_ice(:,:) , jpi, jpj, npb(1:nbpb) ) |
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| 276 | CALL tab_2d_1d( nbpb, qsr_ice_1d (1:nbpb), qsr_ice(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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| 277 | CALL tab_2d_1d( nbpb, fr1_i0_1d (1:nbpb), fr1_i0 , jpi, jpj, npb(1:nbpb) ) |
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| 278 | CALL tab_2d_1d( nbpb, fr2_i0_1d (1:nbpb), fr2_i0 , jpi, jpj, npb(1:nbpb) ) |
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[4688] | 279 | CALL tab_2d_1d( nbpb, qns_ice_1d (1:nbpb), qns_ice(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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| 280 | CALL tab_2d_1d( nbpb, ftr_ice_1d (1:nbpb), ftr_ice(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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| 281 | IF( .NOT. lk_cpl ) THEN |
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| 282 | CALL tab_2d_1d( nbpb, qla_ice_1d (1:nbpb), qla_ice(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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| 283 | CALL tab_2d_1d( nbpb, dqla_ice_1d(1:nbpb), dqla_ice(:,:,jl), jpi, jpj, npb(1:nbpb) ) |
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| 284 | ENDIF |
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[3625] | 285 | CALL tab_2d_1d( nbpb, dqns_ice_1d(1:nbpb), dqns_ice(:,:,jl), jpi, jpj, npb(1:nbpb) ) |
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| 286 | CALL tab_2d_1d( nbpb, t_bo_b (1:nbpb), t_bo , jpi, jpj, npb(1:nbpb) ) |
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| 287 | CALL tab_2d_1d( nbpb, sprecip_1d (1:nbpb), sprecip , jpi, jpj, npb(1:nbpb) ) |
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[4688] | 288 | CALL tab_2d_1d( nbpb, fhtur_1d (1:nbpb), fhtur , jpi, jpj, npb(1:nbpb) ) |
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| 289 | CALL tab_2d_1d( nbpb, qlead_1d (1:nbpb), qlead , jpi, jpj, npb(1:nbpb) ) |
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| 290 | CALL tab_2d_1d( nbpb, fhld_1d (1:nbpb), fhld , jpi, jpj, npb(1:nbpb) ) |
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[825] | 291 | |
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[4688] | 292 | CALL tab_2d_1d( nbpb, wfx_snw_1d (1:nbpb), wfx_snw , jpi, jpj, npb(1:nbpb) ) |
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| 293 | CALL tab_2d_1d( nbpb, wfx_sub_1d (1:nbpb), wfx_sub , jpi, jpj, npb(1:nbpb) ) |
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| 294 | |
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| 295 | CALL tab_2d_1d( nbpb, wfx_bog_1d (1:nbpb), wfx_bog , jpi, jpj, npb(1:nbpb) ) |
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| 296 | CALL tab_2d_1d( nbpb, wfx_bom_1d (1:nbpb), wfx_bom , jpi, jpj, npb(1:nbpb) ) |
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| 297 | CALL tab_2d_1d( nbpb, wfx_sum_1d (1:nbpb), wfx_sum , jpi, jpj, npb(1:nbpb) ) |
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| 298 | CALL tab_2d_1d( nbpb, wfx_sni_1d (1:nbpb), wfx_sni , jpi, jpj, npb(1:nbpb) ) |
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| 299 | CALL tab_2d_1d( nbpb, wfx_res_1d (1:nbpb), wfx_res , jpi, jpj, npb(1:nbpb) ) |
---|
| 300 | CALL tab_2d_1d( nbpb, wfx_spr_1d (1:nbpb), wfx_spr , jpi, jpj, npb(1:nbpb) ) |
---|
| 301 | |
---|
| 302 | CALL tab_2d_1d( nbpb, sfx_bog_1d (1:nbpb), sfx_bog , jpi, jpj, npb(1:nbpb) ) |
---|
| 303 | CALL tab_2d_1d( nbpb, sfx_bom_1d (1:nbpb), sfx_bom , jpi, jpj, npb(1:nbpb) ) |
---|
| 304 | CALL tab_2d_1d( nbpb, sfx_sum_1d (1:nbpb), sfx_sum , jpi, jpj, npb(1:nbpb) ) |
---|
| 305 | CALL tab_2d_1d( nbpb, sfx_sni_1d (1:nbpb), sfx_sni , jpi, jpj, npb(1:nbpb) ) |
---|
[3625] | 306 | CALL tab_2d_1d( nbpb, sfx_bri_1d (1:nbpb), sfx_bri , jpi, jpj, npb(1:nbpb) ) |
---|
[4688] | 307 | CALL tab_2d_1d( nbpb, sfx_res_1d (1:nbpb), sfx_res , jpi, jpj, npb(1:nbpb) ) |
---|
[825] | 308 | |
---|
[4688] | 309 | CALL tab_2d_1d( nbpb, iatte_1d (1:nbpb), iatte , jpi, jpj, npb(1:nbpb) ) |
---|
| 310 | CALL tab_2d_1d( nbpb, oatte_1d (1:nbpb), oatte , jpi, jpj, npb(1:nbpb) ) |
---|
| 311 | |
---|
| 312 | CALL tab_2d_1d( nbpb, hfx_thd_1d (1:nbpb), hfx_thd , jpi, jpj, npb(1:nbpb) ) |
---|
| 313 | CALL tab_2d_1d( nbpb, hfx_spr_1d (1:nbpb), hfx_spr , jpi, jpj, npb(1:nbpb) ) |
---|
| 314 | CALL tab_2d_1d( nbpb, hfx_sum_1d (1:nbpb), hfx_sum , jpi, jpj, npb(1:nbpb) ) |
---|
| 315 | CALL tab_2d_1d( nbpb, hfx_bom_1d (1:nbpb), hfx_bom , jpi, jpj, npb(1:nbpb) ) |
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| 316 | CALL tab_2d_1d( nbpb, hfx_bog_1d (1:nbpb), hfx_bog , jpi, jpj, npb(1:nbpb) ) |
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| 317 | CALL tab_2d_1d( nbpb, hfx_dif_1d (1:nbpb), hfx_dif , jpi, jpj, npb(1:nbpb) ) |
---|
| 318 | CALL tab_2d_1d( nbpb, hfx_opw_1d (1:nbpb), hfx_opw , jpi, jpj, npb(1:nbpb) ) |
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| 319 | CALL tab_2d_1d( nbpb, hfx_snw_1d (1:nbpb), hfx_snw , jpi, jpj, npb(1:nbpb) ) |
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| 320 | CALL tab_2d_1d( nbpb, hfx_sub_1d (1:nbpb), hfx_sub , jpi, jpj, npb(1:nbpb) ) |
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| 321 | CALL tab_2d_1d( nbpb, hfx_err_1d (1:nbpb), hfx_err , jpi, jpj, npb(1:nbpb) ) |
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| 322 | CALL tab_2d_1d( nbpb, hfx_res_1d (1:nbpb), hfx_res , jpi, jpj, npb(1:nbpb) ) |
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| 323 | CALL tab_2d_1d( nbpb, hfx_err_rem_1d (1:nbpb), hfx_err_rem , jpi, jpj, npb(1:nbpb) ) |
---|
| 324 | |
---|
[921] | 325 | !-------------------------------- |
---|
| 326 | ! 4.3) Thermodynamic processes |
---|
| 327 | !-------------------------------- |
---|
| 328 | |
---|
[4688] | 329 | !---------------------------------! |
---|
| 330 | ! Ice/Snow Temperature profile ! |
---|
| 331 | !---------------------------------! |
---|
| 332 | CALL lim_thd_dif( 1, nbpb ) |
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[921] | 333 | |
---|
[4688] | 334 | !---------------------------------! |
---|
| 335 | ! Ice/Snow thicnkess ! |
---|
| 336 | !---------------------------------! |
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| 337 | CALL lim_thd_dh( 1, nbpb ) |
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[825] | 338 | |
---|
[4688] | 339 | ! --- Ice enthalpy remapping --- ! |
---|
| 340 | CALL lim_thd_ent( 1, nbpb, q_i_b(1:nbpb,:) ) |
---|
| 341 | |
---|
| 342 | !---------------------------------! |
---|
| 343 | ! --- Ice salinity --- ! |
---|
| 344 | !---------------------------------! |
---|
| 345 | CALL lim_thd_sal( 1, nbpb ) |
---|
[825] | 346 | |
---|
[4688] | 347 | !---------------------------------! |
---|
| 348 | ! --- temperature update --- ! |
---|
| 349 | !---------------------------------! |
---|
| 350 | CALL lim_thd_temp( 1, nbpb ) |
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[825] | 351 | |
---|
[921] | 352 | !-------------------------------- |
---|
| 353 | ! 4.4) Move 1D to 2D vectors |
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| 354 | !-------------------------------- |
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[825] | 355 | |
---|
[3625] | 356 | CALL tab_1d_2d( nbpb, at_i , npb, at_i_b (1:nbpb) , jpi, jpj ) |
---|
| 357 | CALL tab_1d_2d( nbpb, ht_i(:,:,jl) , npb, ht_i_b (1:nbpb) , jpi, jpj ) |
---|
| 358 | CALL tab_1d_2d( nbpb, ht_s(:,:,jl) , npb, ht_s_b (1:nbpb) , jpi, jpj ) |
---|
| 359 | CALL tab_1d_2d( nbpb, a_i (:,:,jl) , npb, a_i_b (1:nbpb) , jpi, jpj ) |
---|
| 360 | CALL tab_1d_2d( nbpb, t_su(:,:,jl) , npb, t_su_b (1:nbpb) , jpi, jpj ) |
---|
| 361 | CALL tab_1d_2d( nbpb, sm_i(:,:,jl) , npb, sm_i_b (1:nbpb) , jpi, jpj ) |
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[825] | 362 | DO jk = 1, nlay_s |
---|
[3625] | 363 | CALL tab_1d_2d( nbpb, t_s(:,:,jk,jl), npb, t_s_b (1:nbpb,jk), jpi, jpj) |
---|
| 364 | CALL tab_1d_2d( nbpb, e_s(:,:,jk,jl), npb, q_s_b (1:nbpb,jk), jpi, jpj) |
---|
[825] | 365 | END DO |
---|
| 366 | DO jk = 1, nlay_i |
---|
[3625] | 367 | CALL tab_1d_2d( nbpb, t_i(:,:,jk,jl), npb, t_i_b (1:nbpb,jk), jpi, jpj) |
---|
| 368 | CALL tab_1d_2d( nbpb, e_i(:,:,jk,jl), npb, q_i_b (1:nbpb,jk), jpi, jpj) |
---|
| 369 | CALL tab_1d_2d( nbpb, s_i(:,:,jk,jl), npb, s_i_b (1:nbpb,jk), jpi, jpj) |
---|
[825] | 370 | END DO |
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[4688] | 371 | CALL tab_1d_2d( nbpb, qlead , npb, qlead_1d (1:nbpb) , jpi, jpj ) |
---|
| 372 | |
---|
| 373 | CALL tab_1d_2d( nbpb, wfx_snw , npb, wfx_snw_1d(1:nbpb) , jpi, jpj ) |
---|
| 374 | CALL tab_1d_2d( nbpb, wfx_sub , npb, wfx_sub_1d(1:nbpb) , jpi, jpj ) |
---|
| 375 | |
---|
| 376 | CALL tab_1d_2d( nbpb, wfx_bog , npb, wfx_bog_1d(1:nbpb) , jpi, jpj ) |
---|
| 377 | CALL tab_1d_2d( nbpb, wfx_bom , npb, wfx_bom_1d(1:nbpb) , jpi, jpj ) |
---|
| 378 | CALL tab_1d_2d( nbpb, wfx_sum , npb, wfx_sum_1d(1:nbpb) , jpi, jpj ) |
---|
| 379 | CALL tab_1d_2d( nbpb, wfx_sni , npb, wfx_sni_1d(1:nbpb) , jpi, jpj ) |
---|
| 380 | CALL tab_1d_2d( nbpb, wfx_res , npb, wfx_res_1d(1:nbpb) , jpi, jpj ) |
---|
| 381 | CALL tab_1d_2d( nbpb, wfx_spr , npb, wfx_spr_1d(1:nbpb) , jpi, jpj ) |
---|
| 382 | |
---|
| 383 | CALL tab_1d_2d( nbpb, sfx_bog , npb, sfx_bog_1d(1:nbpb) , jpi, jpj ) |
---|
| 384 | CALL tab_1d_2d( nbpb, sfx_bom , npb, sfx_bom_1d(1:nbpb) , jpi, jpj ) |
---|
| 385 | CALL tab_1d_2d( nbpb, sfx_sum , npb, sfx_sum_1d(1:nbpb) , jpi, jpj ) |
---|
| 386 | CALL tab_1d_2d( nbpb, sfx_sni , npb, sfx_sni_1d(1:nbpb) , jpi, jpj ) |
---|
| 387 | CALL tab_1d_2d( nbpb, sfx_res , npb, sfx_res_1d(1:nbpb) , jpi, jpj ) |
---|
[2528] | 388 | ! |
---|
[1572] | 389 | IF( num_sal == 2 ) THEN |
---|
[3625] | 390 | CALL tab_1d_2d( nbpb, sfx_bri , npb, sfx_bri_1d(1:nbpb) , jpi, jpj ) |
---|
[825] | 391 | ENDIF |
---|
[4688] | 392 | |
---|
| 393 | CALL tab_1d_2d( nbpb, hfx_thd , npb, hfx_thd_1d(1:nbpb) , jpi, jpj ) |
---|
| 394 | CALL tab_1d_2d( nbpb, hfx_spr , npb, hfx_spr_1d(1:nbpb) , jpi, jpj ) |
---|
| 395 | CALL tab_1d_2d( nbpb, hfx_sum , npb, hfx_sum_1d(1:nbpb) , jpi, jpj ) |
---|
| 396 | CALL tab_1d_2d( nbpb, hfx_bom , npb, hfx_bom_1d(1:nbpb) , jpi, jpj ) |
---|
| 397 | CALL tab_1d_2d( nbpb, hfx_bog , npb, hfx_bog_1d(1:nbpb) , jpi, jpj ) |
---|
| 398 | CALL tab_1d_2d( nbpb, hfx_dif , npb, hfx_dif_1d(1:nbpb) , jpi, jpj ) |
---|
| 399 | CALL tab_1d_2d( nbpb, hfx_opw , npb, hfx_opw_1d(1:nbpb) , jpi, jpj ) |
---|
| 400 | CALL tab_1d_2d( nbpb, hfx_snw , npb, hfx_snw_1d(1:nbpb) , jpi, jpj ) |
---|
| 401 | CALL tab_1d_2d( nbpb, hfx_sub , npb, hfx_sub_1d(1:nbpb) , jpi, jpj ) |
---|
| 402 | CALL tab_1d_2d( nbpb, hfx_err , npb, hfx_err_1d(1:nbpb) , jpi, jpj ) |
---|
| 403 | CALL tab_1d_2d( nbpb, hfx_res , npb, hfx_res_1d(1:nbpb) , jpi, jpj ) |
---|
| 404 | CALL tab_1d_2d( nbpb, hfx_err_rem , npb, hfx_err_rem_1d(1:nbpb) , jpi, jpj ) |
---|
[2528] | 405 | ! |
---|
[3625] | 406 | !+++++ temporary stuff for a dummy version |
---|
[4688] | 407 | CALL tab_1d_2d( nbpb, dh_i_surf2D, npb, dh_i_surf(1:nbpb) , jpi, jpj ) |
---|
| 408 | CALL tab_1d_2d( nbpb, dh_i_bott2D, npb, dh_i_bott(1:nbpb) , jpi, jpj ) |
---|
| 409 | CALL tab_1d_2d( nbpb, s_i_newice , npb, s_i_new (1:nbpb) , jpi, jpj ) |
---|
| 410 | CALL tab_1d_2d( nbpb, izero(:,:,jl) , npb, i0 (1:nbpb) , jpi, jpj ) |
---|
[825] | 411 | !+++++ |
---|
[4688] | 412 | CALL tab_1d_2d( nbpb, qns_ice(:,:,jl), npb, qns_ice_1d(1:nbpb) , jpi, jpj) |
---|
| 413 | CALL tab_1d_2d( nbpb, ftr_ice(:,:,jl), npb, ftr_ice_1d(1:nbpb) , jpi, jpj ) |
---|
[2528] | 414 | ! |
---|
[1572] | 415 | IF( lk_mpp ) CALL mpp_comm_free( ncomm_ice ) !RB necessary ?? |
---|
| 416 | ENDIF |
---|
| 417 | ! |
---|
| 418 | END DO |
---|
[825] | 419 | |
---|
[921] | 420 | !------------------------------------------------------------------------------! |
---|
| 421 | ! 5) Global variables, diagnostics |
---|
| 422 | !------------------------------------------------------------------------------! |
---|
[825] | 423 | |
---|
| 424 | !------------------------ |
---|
| 425 | ! 5.1) Ice heat content |
---|
| 426 | !------------------------ |
---|
[4688] | 427 | ! Enthalpies are global variables we have to readjust the units (heat content in Joules) |
---|
[825] | 428 | DO jl = 1, jpl |
---|
[921] | 429 | DO jk = 1, nlay_i |
---|
[4688] | 430 | e_i(:,:,jk,jl) = e_i(:,:,jk,jl) * area(:,:) * a_i(:,:,jl) * ht_i(:,:,jl) / ( unit_fac * REAL( nlay_i ) ) |
---|
[1572] | 431 | END DO |
---|
| 432 | END DO |
---|
[825] | 433 | |
---|
| 434 | !------------------------ |
---|
| 435 | ! 5.2) Snow heat content |
---|
| 436 | !------------------------ |
---|
[4688] | 437 | ! Enthalpies are global variables we have to readjust the units (heat content in Joules) |
---|
[825] | 438 | DO jl = 1, jpl |
---|
| 439 | DO jk = 1, nlay_s |
---|
[4688] | 440 | e_s(:,:,jk,jl) = e_s(:,:,jk,jl) * area(:,:) * a_i(:,:,jl) * ht_s(:,:,jl) / ( unit_fac * REAL( nlay_s ) ) |
---|
[1572] | 441 | END DO |
---|
| 442 | END DO |
---|
[825] | 443 | |
---|
| 444 | !---------------------------------- |
---|
| 445 | ! 5.3) Change thickness to volume |
---|
| 446 | !---------------------------------- |
---|
| 447 | CALL lim_var_eqv2glo |
---|
| 448 | |
---|
| 449 | !-------------------------------------------- |
---|
| 450 | ! 5.4) Diagnostic thermodynamic growth rates |
---|
| 451 | !-------------------------------------------- |
---|
[2528] | 452 | IF(ln_ctl) THEN ! Control print |
---|
[867] | 453 | CALL prt_ctl_info(' ') |
---|
| 454 | CALL prt_ctl_info(' - Cell values : ') |
---|
| 455 | CALL prt_ctl_info(' ~~~~~~~~~~~~~ ') |
---|
[863] | 456 | CALL prt_ctl(tab2d_1=area , clinfo1=' lim_thd : cell area :') |
---|
| 457 | CALL prt_ctl(tab2d_1=at_i , clinfo1=' lim_thd : at_i :') |
---|
| 458 | CALL prt_ctl(tab2d_1=vt_i , clinfo1=' lim_thd : vt_i :') |
---|
| 459 | CALL prt_ctl(tab2d_1=vt_s , clinfo1=' lim_thd : vt_s :') |
---|
| 460 | DO jl = 1, jpl |
---|
[867] | 461 | CALL prt_ctl_info(' ') |
---|
[863] | 462 | CALL prt_ctl_info(' - Category : ', ivar1=jl) |
---|
| 463 | CALL prt_ctl_info(' ~~~~~~~~~~') |
---|
| 464 | CALL prt_ctl(tab2d_1=a_i (:,:,jl) , clinfo1= ' lim_thd : a_i : ') |
---|
| 465 | CALL prt_ctl(tab2d_1=ht_i (:,:,jl) , clinfo1= ' lim_thd : ht_i : ') |
---|
| 466 | CALL prt_ctl(tab2d_1=ht_s (:,:,jl) , clinfo1= ' lim_thd : ht_s : ') |
---|
| 467 | CALL prt_ctl(tab2d_1=v_i (:,:,jl) , clinfo1= ' lim_thd : v_i : ') |
---|
| 468 | CALL prt_ctl(tab2d_1=v_s (:,:,jl) , clinfo1= ' lim_thd : v_s : ') |
---|
| 469 | CALL prt_ctl(tab2d_1=e_s (:,:,1,jl) , clinfo1= ' lim_thd : e_s : ') |
---|
| 470 | CALL prt_ctl(tab2d_1=t_su (:,:,jl) , clinfo1= ' lim_thd : t_su : ') |
---|
| 471 | CALL prt_ctl(tab2d_1=t_s (:,:,1,jl) , clinfo1= ' lim_thd : t_snow : ') |
---|
| 472 | CALL prt_ctl(tab2d_1=sm_i (:,:,jl) , clinfo1= ' lim_thd : sm_i : ') |
---|
| 473 | CALL prt_ctl(tab2d_1=smv_i (:,:,jl) , clinfo1= ' lim_thd : smv_i : ') |
---|
| 474 | DO jk = 1, nlay_i |
---|
[867] | 475 | CALL prt_ctl_info(' ') |
---|
[863] | 476 | CALL prt_ctl_info(' - Layer : ', ivar1=jk) |
---|
| 477 | CALL prt_ctl_info(' ~~~~~~~') |
---|
| 478 | CALL prt_ctl(tab2d_1=t_i(:,:,jk,jl) , clinfo1= ' lim_thd : t_i : ') |
---|
| 479 | CALL prt_ctl(tab2d_1=e_i(:,:,jk,jl) , clinfo1= ' lim_thd : e_i : ') |
---|
| 480 | END DO |
---|
| 481 | END DO |
---|
| 482 | ENDIF |
---|
[2528] | 483 | ! |
---|
[4688] | 484 | ! conservation test |
---|
| 485 | IF( ln_limdiahsb ) CALL lim_cons_hsm(1, 'limthd', zvi_b, zsmv_b, zei_b, zfw_b, zfs_b, zft_b) |
---|
[4161] | 486 | ! |
---|
| 487 | IF( nn_timing == 1 ) CALL timing_stop('limthd') |
---|
[4688] | 488 | END SUBROUTINE lim_thd |
---|
[825] | 489 | |
---|
[4688] | 490 | SUBROUTINE lim_thd_temp( kideb, kiut ) |
---|
[825] | 491 | !!----------------------------------------------------------------------- |
---|
[4688] | 492 | !! *** ROUTINE lim_thd_temp *** |
---|
[825] | 493 | !! |
---|
[4688] | 494 | !! ** Purpose : Computes sea ice temperature (Kelvin) from enthalpy |
---|
[825] | 495 | !! |
---|
| 496 | !! ** Method : Formula (Bitz and Lipscomb, 1999) |
---|
| 497 | !!------------------------------------------------------------------- |
---|
[1572] | 498 | INTEGER, INTENT(in) :: kideb, kiut ! bounds for the spatial loop |
---|
| 499 | !! |
---|
[2715] | 500 | INTEGER :: ji, jk ! dummy loop indices |
---|
[4688] | 501 | REAL(wp) :: ztmelts, zswitch, zaaa, zbbb, zccc, zdiscrim ! local scalar |
---|
[825] | 502 | !!------------------------------------------------------------------- |
---|
[4688] | 503 | ! Recover ice temperature |
---|
| 504 | DO jk = 1, nlay_i |
---|
[825] | 505 | DO ji = kideb, kiut |
---|
[4688] | 506 | ztmelts = -tmut * s_i_b(ji,jk) + rtt |
---|
| 507 | ! Conversion q(S,T) -> T (second order equation) |
---|
| 508 | zaaa = cpic |
---|
| 509 | zbbb = ( rcp - cpic ) * ( ztmelts - rtt ) + q_i_b(ji,jk) / rhoic - lfus |
---|
| 510 | zccc = lfus * ( ztmelts - rtt ) |
---|
| 511 | zdiscrim = SQRT( MAX( zbbb * zbbb - 4._wp * zaaa * zccc, 0._wp ) ) |
---|
| 512 | t_i_b(ji,jk) = rtt - ( zbbb + zdiscrim ) / ( 2._wp * zaaa ) |
---|
| 513 | |
---|
| 514 | ! mask temperature |
---|
| 515 | zswitch = 1._wp - MAX( 0._wp , SIGN( 1._wp , - ht_i_b(ji) ) ) |
---|
| 516 | t_i_b(ji,jk) = zswitch * t_i_b(ji,jk) + ( 1._wp - zswitch ) * rtt |
---|
| 517 | END DO |
---|
| 518 | END DO |
---|
[825] | 519 | |
---|
[4688] | 520 | END SUBROUTINE lim_thd_temp |
---|
[825] | 521 | |
---|
| 522 | SUBROUTINE lim_thd_init |
---|
| 523 | !!----------------------------------------------------------------------- |
---|
| 524 | !! *** ROUTINE lim_thd_init *** |
---|
| 525 | !! |
---|
| 526 | !! ** Purpose : Physical constants and parameters linked to the ice |
---|
[1572] | 527 | !! thermodynamics |
---|
[825] | 528 | !! |
---|
| 529 | !! ** Method : Read the namicethd namelist and check the ice-thermo |
---|
[1572] | 530 | !! parameter values called at the first timestep (nit000) |
---|
[825] | 531 | !! |
---|
| 532 | !! ** input : Namelist namicether |
---|
[2528] | 533 | !!------------------------------------------------------------------- |
---|
[4147] | 534 | INTEGER :: ios ! Local integer output status for namelist read |
---|
[1572] | 535 | NAMELIST/namicethd/ hmelt , hiccrit, fraz_swi, maxfrazb, vfrazb, Cfrazb, & |
---|
[4688] | 536 | & hiclim, hnzst, parsub, betas, & |
---|
[825] | 537 | & kappa_i, nconv_i_thd, maxer_i_thd, thcon_i_swi |
---|
| 538 | !!------------------------------------------------------------------- |
---|
[2528] | 539 | ! |
---|
[1572] | 540 | IF(lwp) THEN |
---|
| 541 | WRITE(numout,*) |
---|
| 542 | WRITE(numout,*) 'lim_thd : Ice Thermodynamics' |
---|
| 543 | WRITE(numout,*) '~~~~~~~' |
---|
| 544 | ENDIF |
---|
[2528] | 545 | ! |
---|
[4147] | 546 | REWIND( numnam_ice_ref ) ! Namelist namicethd in reference namelist : Ice thermodynamics |
---|
| 547 | READ ( numnam_ice_ref, namicethd, IOSTAT = ios, ERR = 901) |
---|
| 548 | 901 IF( ios /= 0 ) CALL ctl_nam ( ios , 'namicethd in reference namelist', lwp ) |
---|
| 549 | |
---|
| 550 | REWIND( numnam_ice_cfg ) ! Namelist namicethd in configuration namelist : Ice thermodynamics |
---|
| 551 | READ ( numnam_ice_cfg, namicethd, IOSTAT = ios, ERR = 902 ) |
---|
| 552 | 902 IF( ios /= 0 ) CALL ctl_nam ( ios , 'namicethd in configuration namelist', lwp ) |
---|
[4624] | 553 | IF(lwm) WRITE ( numoni, namicethd ) |
---|
[2528] | 554 | ! |
---|
[1572] | 555 | IF(lwp) THEN ! control print |
---|
[825] | 556 | WRITE(numout,*) |
---|
[1572] | 557 | WRITE(numout,*)' Namelist of ice parameters for ice thermodynamic computation ' |
---|
| 558 | WRITE(numout,*)' maximum melting at the bottom hmelt = ', hmelt |
---|
[4688] | 559 | WRITE(numout,*)' ice thick. for lateral accretion hiccrit = ', hiccrit |
---|
[1572] | 560 | WRITE(numout,*)' Frazil ice thickness as a function of wind or not fraz_swi = ', fraz_swi |
---|
| 561 | WRITE(numout,*)' Maximum proportion of frazil ice collecting at bottom maxfrazb = ', maxfrazb |
---|
| 562 | WRITE(numout,*)' Thresold relative drift speed for collection of frazil vfrazb = ', vfrazb |
---|
| 563 | WRITE(numout,*)' Squeezing coefficient for collection of frazil Cfrazb = ', Cfrazb |
---|
| 564 | WRITE(numout,*)' minimum ice thickness hiclim = ', hiclim |
---|
| 565 | WRITE(numout,*)' numerical carac. of the scheme for diffusion in ice ' |
---|
| 566 | WRITE(numout,*)' thickness of the surf. layer in temp. computation hnzst = ', hnzst |
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| 567 | WRITE(numout,*)' switch for snow sublimation (=1) or not (=0) parsub = ', parsub |
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| 568 | WRITE(numout,*)' coefficient for ice-lead partition of snowfall betas = ', betas |
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| 569 | WRITE(numout,*)' extinction radiation parameter in sea ice (1.0) kappa_i = ', kappa_i |
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| 570 | WRITE(numout,*)' maximal n. of iter. for heat diffusion computation nconv_i_thd = ', nconv_i_thd |
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| 571 | WRITE(numout,*)' maximal err. on T for heat diffusion computation maxer_i_thd = ', maxer_i_thd |
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| 572 | WRITE(numout,*)' switch for comp. of thermal conductivity in the ice thcon_i_swi = ', thcon_i_swi |
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[4688] | 573 | WRITE(numout,*)' check heat conservation in the ice/snow con_i = ', con_i |
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[825] | 574 | ENDIF |
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[1572] | 575 | ! |
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[825] | 576 | END SUBROUTINE lim_thd_init |
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| 577 | |
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| 578 | #else |
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[1572] | 579 | !!---------------------------------------------------------------------- |
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[2528] | 580 | !! Default option Dummy module NO LIM3 sea-ice model |
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[1572] | 581 | !!---------------------------------------------------------------------- |
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[825] | 582 | #endif |
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| 583 | |
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| 584 | !!====================================================================== |
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| 585 | END MODULE limthd |
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