[825] | 1 | MODULE limthd_dh |
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[1572] | 2 | !!====================================================================== |
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| 3 | !! *** MODULE limthd_dh *** |
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| 4 | !! LIM-3 : thermodynamic growth and decay of the ice |
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| 5 | !!====================================================================== |
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| 6 | !! History : LIM ! 2003-05 (M. Vancoppenolle) Original code in 1D |
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| 7 | !! ! 2005-06 (M. Vancoppenolle) 3D version |
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| 8 | !! 3.2 ! 2009-07 (M. Vancoppenolle, Y. Aksenov, G. Madec) bug correction in rdmsnif & rdmicif |
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[3625] | 9 | !! 3.4 ! 2011-02 (G. Madec) dynamical allocation |
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| 10 | !! 3.5 ! 2012-10 (G. Madec & co) salt flux + bug fixes |
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[1572] | 11 | !!---------------------------------------------------------------------- |
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[825] | 12 | #if defined key_lim3 |
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[834] | 13 | !!---------------------------------------------------------------------- |
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| 14 | !! 'key_lim3' LIM3 sea-ice model |
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| 15 | !!---------------------------------------------------------------------- |
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[3625] | 16 | !! lim_thd_dh : vertical accr./abl. and lateral ablation of sea ice |
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[825] | 17 | !!---------------------------------------------------------------------- |
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[3625] | 18 | USE par_oce ! ocean parameters |
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| 19 | USE phycst ! physical constants (OCE directory) |
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| 20 | USE sbc_oce ! Surface boundary condition: ocean fields |
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| 21 | USE ice ! LIM variables |
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| 22 | USE par_ice ! LIM parameters |
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| 23 | USE thd_ice ! LIM thermodynamics |
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| 24 | USE in_out_manager ! I/O manager |
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| 25 | USE lib_mpp ! MPP library |
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| 26 | USE wrk_nemo ! work arrays |
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| 27 | USE lib_fortran ! Fortran utilities (allows no signed zero when 'key_nosignedzero' defined) |
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[921] | 28 | |
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[825] | 29 | IMPLICIT NONE |
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| 30 | PRIVATE |
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| 31 | |
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[1572] | 32 | PUBLIC lim_thd_dh ! called by lim_thd |
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[825] | 33 | |
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[1572] | 34 | REAL(wp) :: epsi20 = 1e-20 ! constant values |
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| 35 | REAL(wp) :: epsi13 = 1e-13 ! |
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| 36 | REAL(wp) :: epsi16 = 1e-16 ! |
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| 37 | REAL(wp) :: zzero = 0.e0 ! |
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| 38 | REAL(wp) :: zone = 1.e0 ! |
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[825] | 39 | |
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| 40 | !!---------------------------------------------------------------------- |
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[3625] | 41 | !! NEMO/LIM3 3.4 , UCL - NEMO Consortium (2011) |
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[1156] | 42 | !! $Id$ |
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[2715] | 43 | !! Software governed by the CeCILL licence (NEMOGCM/NEMO_CeCILL.txt) |
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[825] | 44 | !!---------------------------------------------------------------------- |
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| 45 | CONTAINS |
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| 46 | |
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[2715] | 47 | SUBROUTINE lim_thd_dh( kideb, kiut, jl ) |
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[921] | 48 | !!------------------------------------------------------------------ |
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| 49 | !! *** ROUTINE lim_thd_dh *** |
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| 50 | !! |
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[1572] | 51 | !! ** Purpose : determines variations of ice and snow thicknesses. |
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[921] | 52 | !! |
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[1572] | 53 | !! ** Method : Ice/Snow surface melting arises from imbalance in surface fluxes |
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| 54 | !! Bottom accretion/ablation arises from flux budget |
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| 55 | !! Snow thickness can increase by precipitation and decrease by sublimation |
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| 56 | !! If snow load excesses Archmiede limit, snow-ice is formed by |
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| 57 | !! the flooding of sea-water in the snow |
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[921] | 58 | !! |
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[1572] | 59 | !! 1) Compute available flux of heat for surface ablation |
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| 60 | !! 2) Compute snow and sea ice enthalpies |
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| 61 | !! 3) Surface ablation and sublimation |
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| 62 | !! 4) Bottom accretion/ablation |
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| 63 | !! 5) Case of Total ablation |
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| 64 | !! 6) Snow ice formation |
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[921] | 65 | !! |
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[1572] | 66 | !! References : Bitz and Lipscomb, 1999, J. Geophys. Res. |
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| 67 | !! Fichefet T. and M. Maqueda 1997, J. Geophys. Res., 102(C6), 12609-12646 |
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| 68 | !! Vancoppenolle, Fichefet and Bitz, 2005, Geophys. Res. Let. |
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| 69 | !! Vancoppenolle et al.,2009, Ocean Modelling |
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[921] | 70 | !!------------------------------------------------------------------ |
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[1572] | 71 | INTEGER , INTENT(in) :: kideb, kiut ! Start/End point on which the the computation is applied |
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| 72 | INTEGER , INTENT(in) :: jl ! Thickness cateogry number |
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| 73 | !! |
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| 74 | INTEGER :: ji , jk ! dummy loop indices |
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[3625] | 75 | INTEGER :: ii, ij ! 2D corresponding indices to ji |
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[1572] | 76 | INTEGER :: isnow ! switch for presence (1) or absence (0) of snow |
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| 77 | INTEGER :: isnowic ! snow ice formation not |
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| 78 | INTEGER :: i_ice_switch ! ice thickness above a certain treshold or not |
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| 79 | INTEGER :: iter |
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[825] | 80 | |
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[2715] | 81 | REAL(wp) :: zzfmass_i, zihgnew ! local scalar |
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| 82 | REAL(wp) :: zzfmass_s, zhsnew, ztmelts ! local scalar |
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[1572] | 83 | REAL(wp) :: zhn, zdhcf, zdhbf, zhni, zhnfi, zihg ! |
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[2715] | 84 | REAL(wp) :: zdhnm, zhnnew, zhisn, zihic, zzc ! |
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[1572] | 85 | REAL(wp) :: zfracs ! fractionation coefficient for bottom salt entrapment |
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| 86 | REAL(wp) :: zds ! increment of bottom ice salinity |
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| 87 | REAL(wp) :: zcoeff ! dummy argument for snowfall partitioning over ice and leads |
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| 88 | REAL(wp) :: zsm_snowice ! snow-ice salinity |
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| 89 | REAL(wp) :: zswi1 ! switch for computation of bottom salinity |
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| 90 | REAL(wp) :: zswi12 ! switch for computation of bottom salinity |
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| 91 | REAL(wp) :: zswi2 ! switch for computation of bottom salinity |
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| 92 | REAL(wp) :: zgrr ! bottom growth rate |
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| 93 | REAL(wp) :: ztform ! bottom formation temperature |
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[2715] | 94 | ! |
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[3294] | 95 | REAL(wp), POINTER, DIMENSION(:) :: zh_i ! ice layer thickness |
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| 96 | REAL(wp), POINTER, DIMENSION(:) :: zh_s ! snow layer thickness |
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| 97 | REAL(wp), POINTER, DIMENSION(:) :: ztfs ! melting point |
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| 98 | REAL(wp), POINTER, DIMENSION(:) :: zhsold ! old snow thickness |
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| 99 | REAL(wp), POINTER, DIMENSION(:) :: zqprec ! energy of fallen snow |
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| 100 | REAL(wp), POINTER, DIMENSION(:) :: zqfont_su ! incoming, remaining surface energy |
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| 101 | REAL(wp), POINTER, DIMENSION(:) :: zqfont_bo ! incoming, bottom energy |
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| 102 | REAL(wp), POINTER, DIMENSION(:) :: z_f_surf ! surface heat for ablation |
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| 103 | REAL(wp), POINTER, DIMENSION(:) :: zhgnew ! new ice thickness |
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| 104 | REAL(wp), POINTER, DIMENSION(:) :: zfmass_i ! |
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| 105 | |
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[3625] | 106 | REAL(wp), POINTER, DIMENSION(:) :: zdh_s_mel ! snow melt |
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| 107 | REAL(wp), POINTER, DIMENSION(:) :: zdh_s_pre ! snow precipitation |
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| 108 | REAL(wp), POINTER, DIMENSION(:) :: zdh_s_sub ! snow sublimation |
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| 109 | REAL(wp), POINTER, DIMENSION(:) :: zsfx_melt ! salt flux due to ice melt |
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[3294] | 110 | |
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| 111 | REAL(wp), POINTER, DIMENSION(:,:) :: zdeltah |
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| 112 | |
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| 113 | ! Pathological cases |
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| 114 | REAL(wp), POINTER, DIMENSION(:) :: zfdt_init ! total incoming heat for ice melt |
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| 115 | REAL(wp), POINTER, DIMENSION(:) :: zfdt_final ! total remaing heat for ice melt |
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| 116 | REAL(wp), POINTER, DIMENSION(:) :: zqt_i ! total ice heat content |
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| 117 | REAL(wp), POINTER, DIMENSION(:) :: zqt_s ! total snow heat content |
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| 118 | REAL(wp), POINTER, DIMENSION(:) :: zqt_dummy ! dummy heat content |
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| 119 | |
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| 120 | REAL(wp), POINTER, DIMENSION(:,:) :: zqt_i_lay ! total ice heat content |
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| 121 | |
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| 122 | ! Heat conservation |
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| 123 | INTEGER :: num_iter_max, numce_dh |
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| 124 | REAL(wp) :: meance_dh |
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| 125 | REAL(wp), POINTER, DIMENSION(:) :: zinnermelt |
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| 126 | REAL(wp), POINTER, DIMENSION(:) :: zfbase, zdq_i |
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[1572] | 127 | !!------------------------------------------------------------------ |
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[825] | 128 | |
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[3294] | 129 | CALL wrk_alloc( jpij, zh_i, zh_s, ztfs, zhsold, zqprec, zqfont_su, zqfont_bo, z_f_surf, zhgnew, zfmass_i ) |
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[3625] | 130 | CALL wrk_alloc( jpij, zdh_s_mel, zdh_s_pre, zdh_s_sub, zsfx_melt, zfdt_init, zfdt_final, zqt_i, zqt_s, zqt_dummy ) |
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[3294] | 131 | CALL wrk_alloc( jpij, zinnermelt, zfbase, zdq_i ) |
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| 132 | CALL wrk_alloc( jpij, jkmax, zdeltah, zqt_i_lay ) |
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[825] | 133 | |
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[3625] | 134 | zsfx_melt (:) = 0._wp |
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| 135 | ftotal_fin(:) = 0._wp |
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| 136 | zfdt_init (:) = 0._wp |
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| 137 | zfdt_final(:) = 0._wp |
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[2715] | 138 | |
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[825] | 139 | DO ji = kideb, kiut |
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| 140 | old_ht_i_b(ji) = ht_i_b(ji) |
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| 141 | old_ht_s_b(ji) = ht_s_b(ji) |
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| 142 | END DO |
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[921] | 143 | ! |
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| 144 | !------------------------------------------------------------------------------! |
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| 145 | ! 1) Calculate available heat for surface ablation ! |
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| 146 | !------------------------------------------------------------------------------! |
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| 147 | ! |
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[2715] | 148 | DO ji = kideb, kiut |
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[3625] | 149 | isnow = INT( 1.0 - MAX( 0.0 , SIGN( 1.0 , - ht_s_b(ji) ) ) ) |
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| 150 | ztfs (ji) = isnow * rtt + ( 1.0 - isnow ) * rtt |
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| 151 | z_f_surf (ji) = qnsr_ice_1d(ji) + ( 1.0 - i0(ji) ) * qsr_ice_1d(ji) - fc_su(ji) |
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| 152 | z_f_surf (ji) = MAX( zzero , z_f_surf(ji) ) * MAX( zzero , SIGN( zone , t_su_b(ji) - ztfs(ji) ) ) |
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[1572] | 153 | zfdt_init(ji) = ( z_f_surf(ji) + MAX( fbif_1d(ji) + qlbbq_1d(ji) + fc_bo_i(ji),0.0 ) ) * rdt_ice |
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[825] | 154 | END DO ! ji |
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| 155 | |
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[2715] | 156 | zqfont_su (:) = 0._wp |
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| 157 | zqfont_bo (:) = 0._wp |
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| 158 | dsm_i_se_1d(:) = 0._wp |
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| 159 | dsm_i_si_1d(:) = 0._wp |
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[921] | 160 | ! |
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| 161 | !------------------------------------------------------------------------------! |
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| 162 | ! 2) Computing layer thicknesses and snow and sea-ice enthalpies. ! |
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| 163 | !------------------------------------------------------------------------------! |
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| 164 | ! |
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[2715] | 165 | DO ji = kideb, kiut ! Layer thickness |
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[825] | 166 | zh_i(ji) = ht_i_b(ji) / nlay_i |
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| 167 | zh_s(ji) = ht_s_b(ji) / nlay_s |
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| 168 | END DO |
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[2715] | 169 | ! |
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| 170 | zqt_s(:) = 0._wp ! Total enthalpy of the snow |
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[825] | 171 | DO jk = 1, nlay_s |
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[2715] | 172 | DO ji = kideb, kiut |
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[1572] | 173 | zqt_s(ji) = zqt_s(ji) + q_s_b(ji,jk) * ht_s_b(ji) / nlay_s |
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[825] | 174 | END DO |
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| 175 | END DO |
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[2715] | 176 | ! |
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| 177 | zqt_i(:) = 0._wp ! Total enthalpy of the ice |
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[825] | 178 | DO jk = 1, nlay_i |
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[2715] | 179 | DO ji = kideb, kiut |
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| 180 | zzc = q_i_b(ji,jk) * ht_i_b(ji) / nlay_i |
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| 181 | zqt_i(ji) = zqt_i(ji) + zzc |
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| 182 | zqt_i_lay(ji,jk) = zzc |
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[825] | 183 | END DO |
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| 184 | END DO |
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[921] | 185 | ! |
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| 186 | !------------------------------------------------------------------------------| |
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| 187 | ! 3) Surface ablation and sublimation | |
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| 188 | !------------------------------------------------------------------------------| |
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| 189 | ! |
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[834] | 190 | !------------------------- |
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| 191 | ! 3.1 Snow precips / melt |
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| 192 | !------------------------- |
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[825] | 193 | ! Snow accumulation in one thermodynamic time step |
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| 194 | ! snowfall is partitionned between leads and ice |
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| 195 | ! if snow fall was uniform, a fraction (1-at_i) would fall into leads |
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| 196 | ! but because of the winds, more snow falls on leads than on sea ice |
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| 197 | ! and a greater fraction (1-at_i)^beta of the total mass of snow |
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[834] | 198 | ! (beta < 1) falls in leads. |
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[825] | 199 | ! In reality, beta depends on wind speed, |
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| 200 | ! and should decrease with increasing wind speed but here, it is |
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[834] | 201 | ! considered as a constant. an average value is 0.66 |
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[825] | 202 | ! Martin Vancoppenolle, December 2006 |
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| 203 | |
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| 204 | ! Snow fall |
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| 205 | DO ji = kideb, kiut |
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| 206 | zcoeff = ( 1.0 - ( 1.0 - at_i_b(ji) )**betas ) / at_i_b(ji) |
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| 207 | zdh_s_pre(ji) = zcoeff * sprecip_1d(ji) * rdt_ice / rhosn |
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| 208 | END DO |
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[2715] | 209 | zdh_s_mel(:) = 0._wp |
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[825] | 210 | |
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| 211 | ! Melt of fallen snow |
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| 212 | DO ji = kideb, kiut |
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| 213 | ! tatm_ice is now in K |
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[1572] | 214 | zqprec (ji) = rhosn * ( cpic * ( rtt - tatm_ice_1d(ji) ) + lfus ) |
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| 215 | zqfont_su(ji) = z_f_surf(ji) * rdt_ice |
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| 216 | zdeltah (ji,1) = MIN( 0.e0 , - zqfont_su(ji) / MAX( zqprec(ji) , epsi13 ) ) |
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| 217 | zqfont_su(ji) = MAX( 0.e0 , - zdh_s_pre(ji) - zdeltah(ji,1) ) * zqprec(ji) |
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| 218 | zdeltah (ji,1) = MAX( - zdh_s_pre(ji) , zdeltah(ji,1) ) |
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| 219 | zdh_s_mel(ji) = zdh_s_mel(ji) + zdeltah(ji,1) |
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[825] | 220 | ! heat conservation |
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[1572] | 221 | qt_s_in(ji,jl) = qt_s_in(ji,jl) + zqprec(ji) * zdh_s_pre(ji) |
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| 222 | zqt_s (ji) = zqt_s (ji) + zqprec(ji) * zdh_s_pre(ji) |
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| 223 | zqt_s (ji) = MAX( zqt_s(ji) - zqfont_su(ji) , 0.e0 ) |
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[825] | 224 | END DO |
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| 225 | |
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| 226 | |
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| 227 | ! Snow melt due to surface heat imbalance |
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| 228 | DO jk = 1, nlay_s |
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| 229 | DO ji = kideb, kiut |
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[1572] | 230 | zdeltah (ji,jk) = - zqfont_su(ji) / q_s_b(ji,jk) |
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| 231 | zqfont_su(ji) = MAX( 0.0 , - zh_s(ji) - zdeltah(ji,jk) ) * q_s_b(ji,jk) |
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| 232 | zdeltah (ji,jk) = MAX( zdeltah(ji,jk) , - zh_s(ji) ) |
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| 233 | zdh_s_mel(ji) = zdh_s_mel(ji) + zdeltah(ji,jk) ! resulting melt of snow |
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[825] | 234 | END DO |
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| 235 | END DO |
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| 236 | |
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| 237 | ! Apply snow melt to snow depth |
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| 238 | DO ji = kideb, kiut |
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| 239 | dh_s_tot(ji) = zdh_s_mel(ji) + zdh_s_pre(ji) |
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| 240 | ! Old and new snow depths |
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| 241 | zhsold(ji) = ht_s_b(ji) |
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| 242 | zhsnew = ht_s_b(ji) + dh_s_tot(ji) |
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| 243 | ! If snow is still present zhn = 1, else zhn = 0 |
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[3625] | 244 | zhn = 1.0 - MAX( zzero , SIGN( zone , - zhsnew ) ) |
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[825] | 245 | ht_s_b(ji) = MAX( zzero , zhsnew ) |
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| 246 | ! Volume and mass variations of snow |
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[3625] | 247 | dvsbq_1d (ji) = a_i_b(ji) * ( ht_s_b(ji) - zhsold(ji) - zdh_s_pre(ji) ) |
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[1572] | 248 | dvsbq_1d (ji) = MIN( zzero, dvsbq_1d(ji) ) |
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[3625] | 249 | rdm_snw_1d(ji) = rdm_snw_1d(ji) + rhosn * dvsbq_1d(ji) |
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[825] | 250 | END DO ! ji |
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| 251 | |
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[834] | 252 | !-------------------------- |
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| 253 | ! 3.2 Surface ice ablation |
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| 254 | !-------------------------- |
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[825] | 255 | DO ji = kideb, kiut |
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[2715] | 256 | dh_i_surf(ji) = 0._wp |
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[3625] | 257 | z_f_surf (ji) = zqfont_su(ji) * r1_rdtice ! heat conservation test |
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[2715] | 258 | zdq_i (ji) = 0._wp |
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[825] | 259 | END DO ! ji |
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| 260 | |
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| 261 | DO jk = 1, nlay_i |
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| 262 | DO ji = kideb, kiut |
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[1572] | 263 | ! ! melt of layer jk |
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| 264 | zdeltah (ji,jk) = - zqfont_su(ji) / q_i_b(ji,jk) |
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| 265 | ! ! recompute heat available |
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[3625] | 266 | zqfont_su(ji ) = MAX( 0.0 , - zh_i(ji) - zdeltah(ji,jk) ) * q_i_b(ji,jk) |
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[1572] | 267 | ! ! melt of layer jk cannot be higher than its thickness |
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| 268 | zdeltah (ji,jk) = MAX( zdeltah(ji,jk) , - zh_i(ji) ) |
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| 269 | ! ! update surface melt |
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[3625] | 270 | dh_i_surf(ji ) = dh_i_surf(ji) + zdeltah(ji,jk) |
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[1572] | 271 | ! ! for energy conservation |
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[3625] | 272 | zdq_i (ji ) = zdq_i(ji) + zdeltah(ji,jk) * q_i_b(ji,jk) * r1_rdtice |
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[1572] | 273 | ! |
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[3625] | 274 | ! ! contribution to ice-ocean salt flux |
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| 275 | zsfx_melt(ji) = zsfx_melt(ji) - sm_i_b(ji) * a_i_b(ji) * MIN( zdeltah(ji,jk) , 0._wp ) * rhoic * r1_rdtice |
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[1572] | 276 | END DO |
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| 277 | END DO |
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[825] | 278 | |
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[1572] | 279 | ! !------------------- |
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| 280 | IF( con_i ) THEN ! Conservation test |
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| 281 | ! !------------------- |
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| 282 | numce_dh = 0 |
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[2715] | 283 | meance_dh = 0._wp |
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[921] | 284 | DO ji = kideb, kiut |
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| 285 | IF ( ( z_f_surf(ji) + zdq_i(ji) ) .GE. 1.0e-3 ) THEN |
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| 286 | numce_dh = numce_dh + 1 |
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| 287 | meance_dh = meance_dh + z_f_surf(ji) + zdq_i(ji) |
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| 288 | ENDIF |
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[1572] | 289 | IF( z_f_surf(ji) + zdq_i(ji) .GE. 1.0e-3 ) THEN! |
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[921] | 290 | WRITE(numout,*) ' ALERTE heat loss for surface melt ' |
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[3625] | 291 | WRITE(numout,*) ' ii, ij, jl :', ii, ij, jl |
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[2715] | 292 | WRITE(numout,*) ' ht_i_b : ', ht_i_b(ji) |
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| 293 | WRITE(numout,*) ' z_f_surf : ', z_f_surf(ji) |
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| 294 | WRITE(numout,*) ' zdq_i : ', zdq_i(ji) |
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| 295 | WRITE(numout,*) ' ht_i_b : ', ht_i_b(ji) |
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| 296 | WRITE(numout,*) ' fc_bo_i : ', fc_bo_i(ji) |
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| 297 | WRITE(numout,*) ' fbif_1d : ', fbif_1d(ji) |
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| 298 | WRITE(numout,*) ' qlbbq_1d : ', qlbbq_1d(ji) |
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| 299 | WRITE(numout,*) ' s_i_new : ', s_i_new(ji) |
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[3625] | 300 | WRITE(numout,*) ' sss_m : ', sss_m(ii,ij) |
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[921] | 301 | ENDIF |
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[1572] | 302 | END DO |
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| 303 | ! |
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| 304 | IF( numce_dh > 0 ) meance_dh = meance_dh / numce_dh |
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[921] | 305 | WRITE(numout,*) ' Error report - Category : ', jl |
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| 306 | WRITE(numout,*) ' ~~~~~~~~~~~~ ' |
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| 307 | WRITE(numout,*) ' Number of points where there is sur. me. error : ', numce_dh |
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| 308 | WRITE(numout,*) ' Mean basal growth error on error points : ', meance_dh |
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[1572] | 309 | ! |
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| 310 | ENDIF |
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[825] | 311 | |
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[834] | 312 | !---------------------- |
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| 313 | ! 3.3 Snow sublimation |
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| 314 | !---------------------- |
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[825] | 315 | |
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| 316 | DO ji = kideb, kiut |
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| 317 | ! if qla is positive (upwards), heat goes to the atmosphere, therefore |
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| 318 | ! snow sublimates, if qla is negative (downwards), snow condensates |
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[1572] | 319 | zdh_s_sub(ji) = - parsub * qla_ice_1d(ji) / ( rhosn * lsub ) * rdt_ice |
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| 320 | dh_s_tot (ji) = dh_s_tot(ji) + zdh_s_sub(ji) |
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| 321 | zdhcf = ht_s_b(ji) + zdh_s_sub(ji) |
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| 322 | ht_s_b (ji) = MAX( zzero , zdhcf ) |
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[825] | 323 | ! we recompute dh_s_tot |
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[1572] | 324 | dh_s_tot (ji) = ht_s_b(ji) - zhsold(ji) |
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| 325 | qt_s_in (ji,jl) = qt_s_in(ji,jl) + zdh_s_sub(ji)*q_s_b(ji,1) |
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| 326 | END DO |
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[825] | 327 | |
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[1572] | 328 | zqt_dummy(:) = 0.e0 |
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[825] | 329 | DO jk = 1, nlay_s |
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| 330 | DO ji = kideb,kiut |
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[1572] | 331 | q_s_b (ji,jk) = rhosn * ( cpic * ( rtt - t_s_b(ji,jk) ) + lfus ) |
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| 332 | zqt_dummy(ji) = zqt_dummy(ji) + q_s_b(ji,jk) * ht_s_b(ji) / nlay_s ! heat conservation |
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[825] | 333 | END DO |
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| 334 | END DO |
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| 335 | |
---|
[1572] | 336 | DO jk = 1, nlay_s |
---|
| 337 | DO ji = kideb, kiut |
---|
| 338 | ! In case of disparition of the snow, we have to update the snow temperatures |
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[3625] | 339 | zhisn = MAX( zzero , SIGN( zone, - ht_s_b(ji) ) ) |
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[825] | 340 | t_s_b(ji,jk) = ( 1.0 - zhisn ) * t_s_b(ji,jk) + zhisn * rtt |
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| 341 | q_s_b(ji,jk) = ( 1.0 - zhisn ) * q_s_b(ji,jk) |
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| 342 | END DO |
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[921] | 343 | END DO |
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[825] | 344 | |
---|
[921] | 345 | ! |
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| 346 | !------------------------------------------------------------------------------! |
---|
| 347 | ! 4) Basal growth / melt ! |
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| 348 | !------------------------------------------------------------------------------! |
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| 349 | ! |
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[825] | 350 | ! Ice basal growth / melt is given by the ratio of heat budget over basal |
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| 351 | ! ice heat content. Basal heat budget is given by the difference between |
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| 352 | ! the inner conductive flux (fc_bo_i), from the open water heat flux |
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| 353 | ! (qlbbqb) and the turbulent ocean flux (fbif). |
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[834] | 354 | ! fc_bo_i is positive downwards. fbif and qlbbq are positive to the ice |
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[825] | 355 | |
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[834] | 356 | !----------------------------------------------------- |
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| 357 | ! 4.1 Basal growth - (a) salinity not varying in time |
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| 358 | !----------------------------------------------------- |
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[3625] | 359 | IF( num_sal /= 2 ) THEN ! ice salinity constant in time |
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[825] | 360 | DO ji = kideb, kiut |
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[3625] | 361 | IF( ( fc_bo_i(ji) + fbif_1d(ji) + qlbbq_1d(ji) ) < 0._wp ) THEN |
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[825] | 362 | s_i_new(ji) = sm_i_b(ji) |
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| 363 | ! Melting point in K |
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| 364 | ztmelts = - tmut * s_i_new(ji) + rtt |
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| 365 | ! New ice heat content (Bitz and Lipscomb, 1999) |
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| 366 | ztform = t_i_b(ji,nlay_i) ! t_bo_b crashes in the |
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[921] | 367 | ! Baltic |
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[1572] | 368 | q_i_b(ji,nlay_i+1) = rhoic * ( cpic * ( ztmelts - ztform ) & |
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| 369 | & + lfus * ( 1.0 - ( ztmelts - rtt ) / ( ztform - rtt ) ) & |
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| 370 | & - rcp * ( ztmelts - rtt ) ) |
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[825] | 371 | ! Basal growth rate = - F*dt / q |
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[3625] | 372 | dh_i_bott(ji) = - rdt_ice * ( fc_bo_i(ji) + fbif_1d(ji) + qlbbq_1d(ji) ) / q_i_b(ji,nlay_i+1) |
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[1572] | 373 | ENDIF |
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| 374 | END DO |
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| 375 | ENDIF |
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[825] | 376 | |
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[834] | 377 | !------------------------------------------------- |
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| 378 | ! 4.1 Basal growth - (b) salinity varying in time |
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| 379 | !------------------------------------------------- |
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[3625] | 380 | IF( num_sal == 2 ) THEN |
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| 381 | ! the growth rate (dh_i_bott) is function of the new ice heat content (q_i_b(nlay_i+1)). |
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| 382 | ! q_i_b depends on the new ice salinity (snewice). |
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| 383 | ! snewice depends on dh_i_bott ; it converges quickly, so, no problem |
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[834] | 384 | ! See Vancoppenolle et al., OM08 for more info on this |
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[825] | 385 | |
---|
| 386 | ! Initial value (tested 1D, can be anything between 1 and 20) |
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| 387 | num_iter_max = 4 |
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[1572] | 388 | s_i_new(:) = 4.0 |
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[825] | 389 | |
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| 390 | ! Iterative procedure |
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| 391 | DO iter = 1, num_iter_max |
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| 392 | DO ji = kideb, kiut |
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[1572] | 393 | IF( fc_bo_i(ji) + fbif_1d(ji) + qlbbq_1d(ji) < 0.e0 ) THEN |
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[3625] | 394 | ii = MOD( npb(ji) - 1, jpi ) + 1 |
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| 395 | ij = ( npb(ji) - 1 ) / jpi + 1 |
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[825] | 396 | ! Melting point in K |
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| 397 | ztmelts = - tmut * s_i_new(ji) + rtt |
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| 398 | ! New ice heat content (Bitz and Lipscomb, 1999) |
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[1572] | 399 | q_i_b(ji,nlay_i+1) = rhoic * ( cpic * ( ztmelts - t_bo_b(ji) ) & |
---|
| 400 | & + lfus * ( 1.0 - ( ztmelts - rtt ) / ( t_bo_b(ji) - rtt ) ) & |
---|
| 401 | & - rcp * ( ztmelts-rtt ) ) |
---|
[825] | 402 | ! Bottom growth rate = - F*dt / q |
---|
[1572] | 403 | dh_i_bott(ji) = - rdt_ice * ( fc_bo_i(ji) + fbif_1d(ji) + qlbbq_1d(ji) ) / q_i_b(ji,nlay_i+1) |
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[825] | 404 | ! New ice salinity ( Cox and Weeks, JGR, 1988 ) |
---|
| 405 | ! zswi2 (1) if dh_i_bott/rdt .GT. 3.6e-7 |
---|
| 406 | ! zswi12 (1) if dh_i_bott/rdt .LT. 3.6e-7 and .GT. 2.0e-8 |
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| 407 | ! zswi1 (1) if dh_i_bott/rdt .LT. 2.0e-8 |
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[3625] | 408 | zgrr = MIN( 1.0e-3, MAX ( dh_i_bott(ji) * r1_rdtice , epsi13 ) ) |
---|
[825] | 409 | zswi2 = MAX( zzero , SIGN( zone , zgrr - 3.6e-7 ) ) |
---|
| 410 | zswi12 = MAX( zzero , SIGN( zone , zgrr - 2.0e-8 ) ) * ( 1.0 - zswi2 ) |
---|
| 411 | zswi1 = 1. - zswi2 * zswi12 |
---|
[1572] | 412 | zfracs = zswi1 * 0.12 + zswi12 * ( 0.8925 + 0.0568 * LOG( 100.0 * zgrr ) ) & |
---|
| 413 | & + zswi2 * 0.26 / ( 0.26 + 0.74 * EXP ( - 724300.0 * zgrr ) ) |
---|
[3625] | 414 | zds = zfracs * sss_m(ii,ij) - s_i_new(ji) |
---|
| 415 | s_i_new(ji) = zfracs * sss_m(ii,ij) |
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[825] | 416 | ENDIF ! fc_bo_i |
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| 417 | END DO ! ji |
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| 418 | END DO ! iter |
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| 419 | |
---|
| 420 | ! Final values |
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| 421 | DO ji = kideb, kiut |
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[1572] | 422 | IF( ( fc_bo_i(ji) + fbif_1d(ji) + qlbbq_1d(ji) ) .LT. 0.0 ) THEN |
---|
[825] | 423 | ! New ice salinity must not exceed 15 psu |
---|
| 424 | s_i_new(ji) = MIN( s_i_new(ji), s_i_max ) |
---|
| 425 | ! Metling point in K |
---|
| 426 | ztmelts = - tmut * s_i_new(ji) + rtt |
---|
| 427 | ! New ice heat content (Bitz and Lipscomb, 1999) |
---|
[1572] | 428 | q_i_b(ji,nlay_i+1) = rhoic * ( cpic * ( ztmelts - t_bo_b(ji) ) & |
---|
| 429 | & + lfus * ( 1.0 - ( ztmelts - rtt ) / ( t_bo_b(ji) - rtt ) ) & |
---|
| 430 | & - rcp * ( ztmelts - rtt ) ) |
---|
[825] | 431 | ! Basal growth rate = - F*dt / q |
---|
[3625] | 432 | dh_i_bott(ji) = - rdt_ice * ( fc_bo_i(ji) + fbif_1d(ji) + qlbbq_1d(ji) ) / q_i_b(ji,nlay_i+1) |
---|
[834] | 433 | ! Salinity update |
---|
[825] | 434 | ! entrapment during bottom growth |
---|
[1572] | 435 | dsm_i_se_1d(ji) = ( s_i_new(ji) * dh_i_bott(ji) + sm_i_b(ji) * ht_i_b(ji) ) & |
---|
| 436 | & / MAX( ht_i_b(ji) + dh_i_bott(ji) ,epsi13 ) - sm_i_b(ji) |
---|
[825] | 437 | ENDIF ! heat budget |
---|
[1572] | 438 | END DO |
---|
| 439 | ENDIF |
---|
[825] | 440 | |
---|
[834] | 441 | !---------------- |
---|
| 442 | ! 4.2 Basal melt |
---|
| 443 | !---------------- |
---|
[2715] | 444 | meance_dh = 0._wp |
---|
[1572] | 445 | numce_dh = 0 |
---|
[2715] | 446 | zinnermelt(:) = 0._wp |
---|
[825] | 447 | |
---|
| 448 | DO ji = kideb, kiut |
---|
| 449 | ! heat convergence at the surface > 0 |
---|
[2715] | 450 | IF( ( fc_bo_i(ji) + fbif_1d(ji) + qlbbq_1d(ji) ) >= 0._wp ) THEN |
---|
[825] | 451 | s_i_new(ji) = s_i_b(ji,nlay_i) |
---|
| 452 | zqfont_bo(ji) = rdt_ice * ( fc_bo_i(ji) + fbif_1d(ji) + qlbbq_1d(ji) ) |
---|
[3625] | 453 | zfbase(ji) = zqfont_bo(ji) * r1_rdtice ! heat conservation test |
---|
[2715] | 454 | zdq_i(ji) = 0._wp |
---|
| 455 | dh_i_bott(ji) = 0._wp |
---|
[825] | 456 | ENDIF |
---|
| 457 | END DO |
---|
| 458 | |
---|
| 459 | DO jk = nlay_i, 1, -1 |
---|
| 460 | DO ji = kideb, kiut |
---|
[3625] | 461 | IF( fc_bo_i(ji) + fbif_1d(ji) + qlbbq_1d(ji) >= 0._wp ) THEN |
---|
| 462 | ztmelts = - tmut * s_i_b(ji,jk) + rtt |
---|
| 463 | IF( t_i_b(ji,jk) >= ztmelts ) THEN !!gm : a comment is needed |
---|
| 464 | zdeltah (ji,jk) = - zh_i(ji) |
---|
| 465 | dh_i_bott (ji ) = dh_i_bott(ji) + zdeltah(ji,jk) |
---|
| 466 | zinnermelt(ji ) = 1._wp |
---|
| 467 | ELSE ! normal ablation |
---|
| 468 | zdeltah (ji,jk) = - zqfont_bo(ji) / q_i_b(ji,jk) |
---|
| 469 | zqfont_bo(ji ) = MAX( 0.0 , - zh_i(ji) - zdeltah(ji,jk) ) * q_i_b(ji,jk) |
---|
| 470 | zdeltah (ji,jk) = MAX(zdeltah(ji,jk), - zh_i(ji) ) |
---|
| 471 | dh_i_bott(ji ) = dh_i_bott(ji) + zdeltah(ji,jk) |
---|
| 472 | zdq_i (ji ) = zdq_i(ji) + zdeltah(ji,jk) * q_i_b(ji,jk) * r1_rdtice |
---|
[825] | 473 | ENDIF |
---|
[3625] | 474 | ! contribution to salt flux |
---|
| 475 | zsfx_melt(ji) = zsfx_melt(ji) - sm_i_b(ji) * a_i_b(ji) * MIN( zdeltah(ji,jk) , 0._wp ) * rhoic * r1_rdtice |
---|
[825] | 476 | ENDIF |
---|
| 477 | END DO ! ji |
---|
| 478 | END DO ! jk |
---|
| 479 | |
---|
[1572] | 480 | ! !------------------- |
---|
| 481 | IF( con_i ) THEN ! Conservation test |
---|
| 482 | ! !------------------- |
---|
[921] | 483 | DO ji = kideb, kiut |
---|
[1572] | 484 | IF( ( fc_bo_i(ji) + fbif_1d(ji) + qlbbq_1d(ji) ) >= 0.e0 ) THEN |
---|
| 485 | IF( ( zfbase(ji) + zdq_i(ji) ) >= 1.e-3 ) THEN |
---|
| 486 | numce_dh = numce_dh + 1 |
---|
[921] | 487 | meance_dh = meance_dh + zfbase(ji) + zdq_i(ji) |
---|
| 488 | ENDIF |
---|
| 489 | IF ( zfbase(ji) + zdq_i(ji) .GE. 1.0e-3 ) THEN |
---|
[3625] | 490 | WRITE(numout,*) ' ALERTE heat loss for basal melt : ii, ij, jl :', ii, ij, jl |
---|
[2715] | 491 | WRITE(numout,*) ' ht_i_b : ', ht_i_b(ji) |
---|
| 492 | WRITE(numout,*) ' zfbase : ', zfbase(ji) |
---|
| 493 | WRITE(numout,*) ' zdq_i : ', zdq_i(ji) |
---|
| 494 | WRITE(numout,*) ' ht_i_b : ', ht_i_b(ji) |
---|
| 495 | WRITE(numout,*) ' fc_bo_i : ', fc_bo_i(ji) |
---|
| 496 | WRITE(numout,*) ' fbif_1d : ', fbif_1d(ji) |
---|
| 497 | WRITE(numout,*) ' qlbbq_1d : ', qlbbq_1d(ji) |
---|
| 498 | WRITE(numout,*) ' s_i_new : ', s_i_new(ji) |
---|
[3625] | 499 | WRITE(numout,*) ' sss_m : ', sss_m(ii,ij) |
---|
[921] | 500 | WRITE(numout,*) ' dh_i_bott : ', dh_i_bott(ji) |
---|
[2715] | 501 | WRITE(numout,*) ' innermelt : ', INT( zinnermelt(ji) ) |
---|
[921] | 502 | ENDIF |
---|
[1572] | 503 | ENDIF |
---|
| 504 | END DO |
---|
| 505 | IF( numce_dh > 0 ) meance_dh = meance_dh / numce_dh |
---|
[921] | 506 | WRITE(numout,*) ' Number of points where there is bas. me. error : ', numce_dh |
---|
| 507 | WRITE(numout,*) ' Mean basal melt error on error points : ', meance_dh |
---|
| 508 | WRITE(numout,*) ' Remaining bottom heat : ', zqfont_bo(jiindex_1d) |
---|
[1572] | 509 | ! |
---|
| 510 | ENDIF |
---|
[825] | 511 | |
---|
[921] | 512 | ! |
---|
| 513 | !------------------------------------------------------------------------------! |
---|
| 514 | ! 5) Pathological cases ! |
---|
| 515 | !------------------------------------------------------------------------------! |
---|
| 516 | ! |
---|
[834] | 517 | !---------------------------------------------- |
---|
| 518 | ! 5.1 Excessive ablation in a 1-category model |
---|
| 519 | !---------------------------------------------- |
---|
[825] | 520 | |
---|
| 521 | DO ji = kideb, kiut |
---|
[1572] | 522 | ! ! in a 1-category sea ice model, bottom ablation must not exceed hmelt (-0.15) |
---|
| 523 | IF( jpl == 1 ) THEN ; zdhbf = MAX( hmelt , dh_i_bott(ji) ) |
---|
| 524 | ELSE ; zdhbf = dh_i_bott(ji) |
---|
| 525 | ENDIF |
---|
| 526 | ! ! excessive energy is sent to lateral ablation |
---|
| 527 | fsup (ji) = rhoic * lfus * at_i_b(ji) / MAX( 1.0 - at_i_b(ji) , epsi13 ) & |
---|
[3625] | 528 | & * ( zdhbf - dh_i_bott(ji) ) * r1_rdtice |
---|
[825] | 529 | dh_i_bott(ji) = zdhbf |
---|
[1572] | 530 | ! !since ice volume is only used for outputs, we keep it global for all categories |
---|
| 531 | dvbbq_1d (ji) = a_i_b(ji) * dh_i_bott(ji) |
---|
| 532 | ! !new ice thickness |
---|
| 533 | zhgnew (ji) = ht_i_b(ji) + dh_i_surf(ji) + dh_i_bott(ji) |
---|
| 534 | ! ! diagnostic ( bottom ice growth ) |
---|
[3625] | 535 | ii = MOD( npb(ji) - 1, jpi ) + 1 |
---|
| 536 | ij = ( npb(ji) - 1 ) / jpi + 1 |
---|
| 537 | diag_bot_gr(ii,ij) = diag_bot_gr(ii,ij) + MAX(dh_i_bott(ji),0.0)*a_i_b(ji) * r1_rdtice |
---|
| 538 | diag_sur_me(ii,ij) = diag_sur_me(ii,ij) + MIN(dh_i_surf(ji),0.0)*a_i_b(ji) * r1_rdtice |
---|
| 539 | diag_bot_me(ii,ij) = diag_bot_me(ii,ij) + MIN(dh_i_bott(ji),0.0)*a_i_b(ji) * r1_rdtice |
---|
[825] | 540 | END DO |
---|
| 541 | |
---|
[834] | 542 | !----------------------------------- |
---|
| 543 | ! 5.2 More than available ice melts |
---|
| 544 | !----------------------------------- |
---|
[3625] | 545 | ! then heat applied minus heat content at previous time step should equal heat remaining |
---|
[825] | 546 | ! |
---|
| 547 | DO ji = kideb, kiut |
---|
| 548 | ! Adapt the remaining energy if too much ice melts |
---|
| 549 | !-------------------------------------------------- |
---|
[3625] | 550 | zihgnew = 1.0 - MAX( zzero , SIGN( zone , - zhgnew(ji) ) ) ! =1 if ice |
---|
[825] | 551 | ! 0 if no more ice |
---|
[1572] | 552 | zhgnew (ji) = zihgnew * zhgnew(ji) ! ice thickness is put to 0 |
---|
[825] | 553 | ! remaining heat |
---|
[834] | 554 | zfdt_final(ji) = ( 1.0 - zihgnew ) * ( zqfont_su(ji) + zqfont_bo(ji) ) |
---|
[825] | 555 | |
---|
| 556 | ! If snow remains, energy is used to melt snow |
---|
[1572] | 557 | zhni = ht_s_b(ji) ! snow depth at previous time step |
---|
[3625] | 558 | zihg = MAX( zzero , SIGN ( zone , - ht_s_b(ji) ) ) ! =0 if snow |
---|
[825] | 559 | |
---|
| 560 | ! energy of melting of remaining snow |
---|
[1572] | 561 | zqt_s(ji) = ( 1. - zihg ) * zqt_s(ji) / MAX( zhni, epsi13 ) |
---|
| 562 | zdhnm = - ( 1. - zihg ) * ( 1. - zihgnew ) * zfdt_final(ji) / MAX( zqt_s(ji) , epsi13 ) |
---|
[3625] | 563 | zhnfi = zhni + zdhnm |
---|
[1572] | 564 | zfdt_final(ji) = MAX( zfdt_final(ji) + zqt_s(ji) * zdhnm , 0.0 ) |
---|
[825] | 565 | ht_s_b(ji) = MAX( zzero , zhnfi ) |
---|
| 566 | zqt_s(ji) = zqt_s(ji) * ht_s_b(ji) |
---|
| 567 | |
---|
| 568 | ! Mass variations of ice and snow |
---|
| 569 | !--------------------------------- |
---|
[1572] | 570 | ! ! mass variation of the jl category |
---|
[1571] | 571 | zzfmass_s = - a_i_b(ji) * ( zhni - ht_s_b(ji) ) * rhosn ! snow |
---|
| 572 | zzfmass_i = a_i_b(ji) * ( zhgnew(ji) - ht_i_b(ji) ) * rhoic ! ice |
---|
| 573 | ! |
---|
| 574 | zfmass_i(ji) = zzfmass_i ! ice variation saved to compute salt flux (see below) |
---|
| 575 | ! |
---|
| 576 | ! ! mass variation cumulated over category |
---|
[3625] | 577 | rdm_snw_1d(ji) = rdm_snw_1d(ji) + zzfmass_s ! snow |
---|
| 578 | rdm_ice_1d(ji) = rdm_ice_1d(ji) + zzfmass_i ! ice |
---|
[825] | 579 | |
---|
| 580 | ! Remaining heat to the ocean |
---|
| 581 | !--------------------------------- |
---|
[3625] | 582 | focea(ji) = - zfdt_final(ji) * r1_rdtice ! focea is in W.m-2 * dt |
---|
[825] | 583 | |
---|
| 584 | END DO |
---|
| 585 | |
---|
[3625] | 586 | ftotal_fin (:) = zfdt_final(:) * r1_rdtice |
---|
[825] | 587 | |
---|
| 588 | !--------------------------- |
---|
| 589 | ! Salt flux and heat fluxes |
---|
| 590 | !--------------------------- |
---|
| 591 | DO ji = kideb, kiut |
---|
[3625] | 592 | zihgnew = 1.0 - MAX( zzero , SIGN( zone , - zhgnew(ji) ) ) ! =1 if ice |
---|
| 593 | ! |
---|
[825] | 594 | ! Salt flux |
---|
[3625] | 595 | sfx_thd_1d(ji) = sfx_thd_1d(ji) + zihgnew * zsfx_melt(ji) & |
---|
| 596 | & - (1.0 - zihgnew) * zfmass_i (ji) * sm_i_b(ji) * r1_rdtice |
---|
| 597 | ! |
---|
[825] | 598 | ! Heat flux |
---|
| 599 | ! excessive bottom ablation energy (fsup) - 0 except if jpl = 1 |
---|
[3625] | 600 | ! excessive total ablation energy (focea) sent to the ocean |
---|
[1572] | 601 | qfvbq_1d(ji) = qfvbq_1d(ji) + fsup(ji) + ( 1.0 - zihgnew ) * focea(ji) * a_i_b(ji) * rdt_ice |
---|
[825] | 602 | |
---|
[3625] | 603 | zihic = 1.0 - MAX( zzero , SIGN( zone , -ht_i_b(ji) ) ) ! equals 0 if ht_i = 0, 1 if ht_i gt 0 |
---|
[825] | 604 | fscbq_1d(ji) = a_i_b(ji) * fstbif_1d(ji) |
---|
[3625] | 605 | qldif_1d(ji) = qldif_1d(ji) + fsup(ji) + ( 1.0 - zihgnew ) * focea (ji) * a_i_b(ji) * rdt_ice & |
---|
[1572] | 606 | & + ( 1.0 - zihic ) * fscbq_1d(ji) * rdt_ice |
---|
[825] | 607 | END DO ! ji |
---|
| 608 | |
---|
| 609 | !------------------------------------------- |
---|
| 610 | ! Correct temperature, energy and thickness |
---|
| 611 | !------------------------------------------- |
---|
| 612 | DO ji = kideb, kiut |
---|
[1572] | 613 | zihgnew = 1.0 - MAX( zzero , SIGN( zone , - zhgnew(ji) ) ) |
---|
| 614 | t_su_b(ji) = zihgnew * t_su_b(ji) + ( 1.0 - zihgnew ) * rtt |
---|
[825] | 615 | END DO ! ji |
---|
| 616 | |
---|
| 617 | DO jk = 1, nlay_i |
---|
| 618 | DO ji = kideb, kiut |
---|
[1572] | 619 | zihgnew = 1.0 - MAX( zzero , SIGN( zone , - zhgnew(ji) ) ) |
---|
| 620 | t_i_b(ji,jk) = zihgnew * t_i_b(ji,jk) + ( 1.0 - zihgnew ) * rtt |
---|
| 621 | q_i_b(ji,jk) = zihgnew * q_i_b(ji,jk) |
---|
[825] | 622 | END DO |
---|
| 623 | END DO ! ji |
---|
| 624 | |
---|
| 625 | DO ji = kideb, kiut |
---|
| 626 | ht_i_b(ji) = zhgnew(ji) |
---|
| 627 | END DO ! ji |
---|
[921] | 628 | ! |
---|
| 629 | !------------------------------------------------------------------------------| |
---|
| 630 | ! 6) Snow-Ice formation | |
---|
| 631 | !------------------------------------------------------------------------------| |
---|
[1572] | 632 | ! When snow load excesses Archimede's limit, snow-ice interface goes down under sea-level, |
---|
| 633 | ! flooding of seawater transforms snow into ice dh_snowice is positive for the ice |
---|
[825] | 634 | DO ji = kideb, kiut |
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[1572] | 635 | ! |
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| 636 | dh_snowice(ji) = MAX( zzero , ( rhosn * ht_s_b(ji) + (rhoic-rau0) * ht_i_b(ji) ) / ( rhosn+rau0-rhoic ) ) |
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| 637 | zhgnew(ji) = MAX( zhgnew(ji) , zhgnew(ji) + dh_snowice(ji) ) |
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| 638 | zhnnew = MIN( ht_s_b(ji) , ht_s_b(ji) - dh_snowice(ji) ) |
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[825] | 639 | |
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[921] | 640 | ! Changes in ice volume and ice mass. |
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[1572] | 641 | dvnbq_1d (ji) = a_i_b(ji) * ( zhgnew(ji)-ht_i_b(ji) ) |
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| 642 | dmgwi_1d (ji) = dmgwi_1d(ji) + a_i_b(ji) * ( ht_s_b(ji) - zhnnew ) * rhosn |
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[825] | 643 | |
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[3625] | 644 | ! All snow is thrown in the ocean, and seawater is taken to replace the volume |
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| 645 | rdm_ice_1d(ji) = rdm_ice_1d(ji) + a_i_b(ji) * ( zhgnew(ji) - ht_i_b(ji) ) * rhoic * ( 1. - rhosn / rhoic ) |
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| 646 | rdm_snw_1d(ji) = rdm_snw_1d(ji) + a_i_b(ji) * ( zhnnew - ht_s_b(ji) ) * rhosn |
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[825] | 647 | |
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[921] | 648 | ! Equivalent salt flux (1) Snow-ice formation component |
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| 649 | ! ----------------------------------------------------- |
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[3625] | 650 | ii = MOD( npb(ji) - 1, jpi ) + 1 |
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| 651 | ij = ( npb(ji) - 1 ) / jpi + 1 |
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[825] | 652 | |
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[3625] | 653 | IF( num_sal == 2 ) THEN ; zsm_snowice = sss_m(ii,ij) * ( rhoic - rhosn ) / rhoic |
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| 654 | ELSE ; zsm_snowice = sm_i_b(ji) |
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[1572] | 655 | ENDIF |
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[3625] | 656 | sfx_thd_1d(ji) = sfx_thd_1d(ji) - zsm_snowice * a_i_b(ji) * dh_snowice(ji) * rhoic * r1_rdtice |
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| 657 | ! |
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[825] | 658 | ! entrapment during snow ice formation |
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[1572] | 659 | i_ice_switch = 1.0 - MAX( 0.e0 , SIGN( 1.0 , - ht_i_b(ji) + 1.0e-6 ) ) |
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| 660 | isnowic = 1.0 - MAX( 0.e0 , SIGN( 1.0 , - dh_snowice(ji) ) ) * i_ice_switch |
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[3625] | 661 | IF( num_sal == 2 ) & |
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| 662 | dsm_i_si_1d(ji) = ( zsm_snowice * dh_snowice(ji) & |
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| 663 | & + sm_i_b(ji) * ht_i_b(ji) / MAX( ht_i_b(ji) + dh_snowice(ji), epsi13 ) & |
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| 664 | & - sm_i_b(ji) ) * isnowic |
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[825] | 665 | |
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[921] | 666 | ! Actualize new snow and ice thickness. |
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[825] | 667 | ht_s_b(ji) = zhnnew |
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| 668 | ht_i_b(ji) = zhgnew(ji) |
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| 669 | |
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| 670 | ! Total ablation ! new lines added to debug |
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[2715] | 671 | IF( ht_i_b(ji) <= 0._wp ) a_i_b(ji) = 0._wp |
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[825] | 672 | |
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| 673 | ! diagnostic ( snow ice growth ) |
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[3625] | 674 | ii = MOD( npb(ji) - 1, jpi ) + 1 |
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| 675 | ij = ( npb(ji) - 1 ) / jpi + 1 |
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| 676 | diag_sni_gr(ii,ij) = diag_sni_gr(ii,ij) + dh_snowice(ji)*a_i_b(ji) * r1_rdtice |
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[1572] | 677 | ! |
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[825] | 678 | END DO !ji |
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[2715] | 679 | ! |
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[3294] | 680 | CALL wrk_dealloc( jpij, zh_i, zh_s, ztfs, zhsold, zqprec, zqfont_su, zqfont_bo, z_f_surf, zhgnew, zfmass_i ) |
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[3625] | 681 | CALL wrk_dealloc( jpij, zdh_s_mel, zdh_s_pre, zdh_s_sub, zsfx_melt, zfdt_init, zfdt_final, zqt_i, zqt_s, zqt_dummy ) |
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[3294] | 682 | CALL wrk_dealloc( jpij, zinnermelt, zfbase, zdq_i ) |
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| 683 | CALL wrk_dealloc( jpij, jkmax, zdeltah, zqt_i_lay ) |
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[2715] | 684 | ! |
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[921] | 685 | END SUBROUTINE lim_thd_dh |
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[1572] | 686 | |
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[825] | 687 | #else |
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[1572] | 688 | !!---------------------------------------------------------------------- |
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| 689 | !! Default option NO LIM3 sea-ice model |
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| 690 | !!---------------------------------------------------------------------- |
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[825] | 691 | CONTAINS |
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| 692 | SUBROUTINE lim_thd_dh ! Empty routine |
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| 693 | END SUBROUTINE lim_thd_dh |
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| 694 | #endif |
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[1572] | 695 | |
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| 696 | !!====================================================================== |
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[921] | 697 | END MODULE limthd_dh |
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