[821] | 1 | MODULE limthd_2 |
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[3] | 2 | !!====================================================================== |
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[821] | 3 | !! *** MODULE limthd_2 *** |
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[3] | 4 | !! LIM thermo ice model : ice thermodynamic |
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| 5 | !!====================================================================== |
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[1559] | 6 | !! History : 1.0 ! 2000-01 (LIM) |
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| 7 | !! 2.0 ! 2002-07 (C. Ethe, G. Madec) F90 |
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| 8 | !! 2.0 ! 2003-08 (C. Ethe) add lim_thd_init |
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| 9 | !! - ! 2008-2008 (A. Caubel, G. Madec, E. Maisonnave, S. Masson ) generic coupled interface |
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[888] | 10 | !!--------------------------------------------------------------------- |
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[821] | 11 | #if defined key_lim2 |
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[3] | 12 | !!---------------------------------------------------------------------- |
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[821] | 13 | !! 'key_lim2' : LIM 2.0 sea-ice model |
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[3] | 14 | !!---------------------------------------------------------------------- |
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[821] | 15 | !! lim_thd_2 : thermodynamic of sea ice |
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| 16 | !! lim_thd_init_2 : initialisation of sea-ice thermodynamic |
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[3] | 17 | !!---------------------------------------------------------------------- |
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[717] | 18 | USE phycst ! physical constants |
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[3] | 19 | USE dom_oce ! ocean space and time domain variables |
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[1758] | 20 | USE domvvl |
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[717] | 21 | USE lbclnk |
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| 22 | USE in_out_manager ! I/O manager |
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[1756] | 23 | USE lib_mpp |
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[1482] | 24 | USE iom ! IOM library |
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[821] | 25 | USE ice_2 ! LIM sea-ice variables |
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[888] | 26 | USE sbc_oce ! |
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| 27 | USE sbc_ice ! |
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[821] | 28 | USE thd_ice_2 ! LIM thermodynamic sea-ice variables |
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| 29 | USE dom_ice_2 ! LIM sea-ice domain |
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| 30 | USE limthd_zdf_2 |
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| 31 | USE limthd_lac_2 |
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| 32 | USE limtab_2 |
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[258] | 33 | USE prtctl ! Print control |
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[1218] | 34 | USE cpl_oasis3, ONLY : lk_cpl |
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[1756] | 35 | USE diaar5, ONLY : lk_diaar5 |
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[3] | 36 | |
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| 37 | IMPLICIT NONE |
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| 38 | PRIVATE |
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| 39 | |
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[888] | 40 | PUBLIC lim_thd_2 ! called by lim_step |
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[3] | 41 | |
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[1218] | 42 | REAL(wp) :: epsi20 = 1.e-20 ! constant values |
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| 43 | REAL(wp) :: epsi16 = 1.e-16 ! |
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| 44 | REAL(wp) :: epsi04 = 1.e-04 ! |
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| 45 | REAL(wp) :: rzero = 0.e0 ! |
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| 46 | REAL(wp) :: rone = 1.e0 ! |
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[70] | 47 | |
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[3] | 48 | !! * Substitutions |
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[70] | 49 | # include "domzgr_substitute.h90" |
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[3] | 50 | # include "vectopt_loop_substitute.h90" |
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| 51 | !!-------- ------------------------------------------------------------- |
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[2528] | 52 | !! NEMO/LIM2 3.3 , UCL - NEMO Consortium (2010) |
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[1156] | 53 | !! $Id$ |
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[2528] | 54 | !! Software governed by the CeCILL licence (NEMOGCM/NEMO_CeCILL.txt) |
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[3] | 55 | !!---------------------------------------------------------------------- |
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| 56 | |
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| 57 | CONTAINS |
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| 58 | |
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[821] | 59 | SUBROUTINE lim_thd_2( kt ) |
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[3] | 60 | !!------------------------------------------------------------------- |
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[821] | 61 | !! *** ROUTINE lim_thd_2 *** |
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[3] | 62 | !! |
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| 63 | !! ** Purpose : This routine manages the ice thermodynamic. |
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| 64 | !! |
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| 65 | !! ** Action : - Initialisation of some variables |
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| 66 | !! - Some preliminary computation (oceanic heat flux |
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| 67 | !! at the ice base, snow acc.,heat budget of the leads) |
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| 68 | !! - selection of the icy points and put them in an array |
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| 69 | !! - call lim_vert_ther for vert ice thermodynamic |
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| 70 | !! - back to the geographic grid |
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| 71 | !! - selection of points for lateral accretion |
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| 72 | !! - call lim_lat_acc for the ice accretion |
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| 73 | !! - back to the geographic grid |
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| 74 | !! |
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[888] | 75 | !! References : Goosse et al. 1996, Bul. Soc. Roy. Sc. Liege, 65, 87-90 |
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[3] | 76 | !!--------------------------------------------------------------------- |
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[2715] | 77 | USE wrk_nemo, ONLY: wrk_in_use, wrk_not_released |
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| 78 | USE wrk_nemo, ONLY: ztmp => wrk_2d_1, & ! 2D workspace |
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| 79 | zqlbsbq => wrk_2d_2, & ! link with lead energy budget qldif |
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| 80 | zlicegr => wrk_2d_3 ! link with lateral ice growth |
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| 81 | USE wrk_nemo, ONLY: zmsk => wrk_3d_4 ! 3D workspace |
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| 82 | USE wrk_nemo, ONLY: zdvosif => wrk_2d_4, & !: Variation of volume at surface |
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| 83 | zdvobif => wrk_2d_5, & !: Variation of ice volume at the bottom ice (outputs only) |
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| 84 | zdvolif => wrk_2d_6, & !: Total variation of ice volume (outputs only) |
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| 85 | zdvonif => wrk_2d_7, & !: Surface accretion Snow to Ice transformation (outputs only) |
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| 86 | zdvomif => wrk_2d_8, & !: Bottom variation of ice volume due to melting (outputs only) |
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| 87 | zu_imasstr =>wrk_2d_9, & !: Sea-ice transport along i-axis at U-point (outputs only) |
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| 88 | zv_imasstr =>wrk_2d_10 !: Sea-ice transport along j-axis at V-point (outputs only) |
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| 89 | !! |
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[508] | 90 | INTEGER, INTENT(in) :: kt ! number of iteration |
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[888] | 91 | !! |
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[1218] | 92 | INTEGER :: ji, jj ! dummy loop indices |
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| 93 | INTEGER :: nbpb ! nb of icy pts for thermo. cal. |
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| 94 | INTEGER :: nbpac ! nb of pts for lateral accretion |
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[258] | 95 | CHARACTER (len=22) :: charout |
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[1218] | 96 | REAL(wp) :: zfric_umin = 5e-03 ! lower bound for the friction velocity |
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| 97 | REAL(wp) :: zfric_umax = 2e-02 ! upper bound for the friction velocity |
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| 98 | REAL(wp) :: zinda ! switch for test. the val. of concen. |
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| 99 | REAL(wp) :: zindb, zindg ! switches for test. the val of arg |
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[1559] | 100 | REAL(wp) :: zfricp ! temporary scalar |
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[1218] | 101 | REAL(wp) :: za , zh, zthsnice ! |
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| 102 | REAL(wp) :: zfric_u ! friction velocity |
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| 103 | REAL(wp) :: zfnsol ! total non solar heat |
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| 104 | REAL(wp) :: zfontn ! heat flux from snow thickness |
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| 105 | REAL(wp) :: zfntlat, zpareff ! test. the val. of lead heat budget |
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[2715] | 106 | |
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[1756] | 107 | REAL(wp) :: zuice_m, zvice_m ! Sea-ice velocities at U & V-points |
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| 108 | REAL(wp) :: zhice_u, zhice_v ! Sea-ice volume at U & V-points |
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| 109 | REAL(wp) :: ztr_fram ! Sea-ice transport through Fram strait |
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| 110 | REAL(wp) :: zrhoij, zrhoijm1 ! temporary scalars |
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| 111 | REAL(wp) :: zztmp ! temporary scalars within a loop |
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| 112 | !!$ REAL(wp), DIMENSION(jpi,jpj) :: firic !: IR flux over the ice (outputs only) |
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| 113 | !!$ REAL(wp), DIMENSION(jpi,jpj) :: fcsic !: Sensible heat flux over the ice (outputs only) |
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| 114 | !!$ REAL(wp), DIMENSION(jpi,jpj) :: fleic !: Latent heat flux over the ice (outputs only) |
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| 115 | !!$ REAL(wp), DIMENSION(jpi,jpj) :: qlatic !: latent flux (outputs only) |
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[3] | 116 | !!------------------------------------------------------------------- |
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| 117 | |
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[2715] | 118 | IF( wrk_in_use(2, 1,2,3,4,5,6,7,8,9,10) .OR. & |
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| 119 | wrk_in_use(3, 4) ) THEN |
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| 120 | CALL ctl_stop('lim_thd_2 : requested workspace arrays unavailable') ; RETURN |
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| 121 | ENDIF |
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| 122 | |
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[888] | 123 | IF( kt == nit000 ) CALL lim_thd_init_2 ! Initialization (first time-step only) |
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[3] | 124 | |
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| 125 | !-------------------------------------------! |
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| 126 | ! Initilization of diagnostic variables ! |
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| 127 | !-------------------------------------------! |
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| 128 | |
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[1218] | 129 | !!gm needed? yes at least for some of these arrays |
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[1756] | 130 | zdvosif(:,:) = 0.e0 ! variation of ice volume at surface |
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| 131 | zdvobif(:,:) = 0.e0 ! variation of ice volume at bottom |
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| 132 | zdvolif(:,:) = 0.e0 ! total variation of ice volume |
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| 133 | zdvonif(:,:) = 0.e0 ! transformation of snow to sea-ice volume |
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| 134 | ! zdvonif(:,:) = 0.e0 ! lateral variation of ice volume |
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| 135 | zlicegr(:,:) = 0.e0 ! lateral variation of ice volume |
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| 136 | zdvomif(:,:) = 0.e0 ! variation of ice volume at bottom due to melting only |
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| 137 | ztr_fram = 0.e0 ! sea-ice transport through Fram strait |
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[70] | 138 | fstric (:,:) = 0.e0 ! part of solar radiation absorbing inside the ice |
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| 139 | fscmbq (:,:) = 0.e0 ! linked with fstric |
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| 140 | ffltbif(:,:) = 0.e0 ! linked with fstric |
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| 141 | qfvbq (:,:) = 0.e0 ! linked with fstric |
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| 142 | rdmsnif(:,:) = 0.e0 ! variation of snow mass per unit area |
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| 143 | rdmicif(:,:) = 0.e0 ! variation of ice mass per unit area |
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[258] | 144 | zmsk (:,:,:) = 0.e0 |
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[3] | 145 | |
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[1218] | 146 | ! set to zero snow thickness smaller than epsi04 |
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[3] | 147 | DO jj = 1, jpj |
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| 148 | DO ji = 1, jpi |
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[1218] | 149 | hsnif(ji,jj) = hsnif(ji,jj) * MAX( rzero, SIGN( rone , hsnif(ji,jj) - epsi04 ) ) |
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[3] | 150 | END DO |
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| 151 | END DO |
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[1218] | 152 | !!gm better coded (do not use SIGN...) |
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| 153 | ! WHERE( hsnif(:,:) < epsi04 ) hsnif(:,:) = 0.e0 |
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| 154 | !!gm |
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[258] | 155 | |
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[1218] | 156 | IF(ln_ctl) CALL prt_ctl( tab2d_1=hsnif, clinfo1=' lim_thd: hsnif : ' ) |
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[3] | 157 | |
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| 158 | !-----------------------------------! |
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| 159 | ! Treatment of particular cases ! |
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| 160 | !-----------------------------------! |
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| 161 | |
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| 162 | DO jj = 1, jpj |
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| 163 | DO ji = 1, jpi |
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| 164 | ! snow is transformed into ice if the original ice cover disappears. |
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[1218] | 165 | zindg = tms(ji,jj) * MAX( rzero , SIGN( rone , -hicif(ji,jj) ) ) |
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[3] | 166 | hicif(ji,jj) = hicif(ji,jj) + zindg * rhosn * hsnif(ji,jj) / rau0 |
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[1218] | 167 | hsnif(ji,jj) = ( rone - zindg ) * hsnif(ji,jj) + zindg * hicif(ji,jj) * ( rau0 - rhoic ) / rhosn |
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[3] | 168 | dmgwi(ji,jj) = zindg * (1.0 - frld(ji,jj)) * rhoic * hicif(ji,jj) ! snow/ice mass |
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| 169 | |
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| 170 | ! the lead fraction, frld, must be little than or equal to amax (ice ridging). |
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| 171 | zthsnice = hsnif(ji,jj) + hicif(ji,jj) |
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[1218] | 172 | zindb = tms(ji,jj) * ( 1.0 - MAX( rzero , SIGN( rone , - zthsnice ) ) ) |
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| 173 | za = zindb * MIN( rone, ( 1.0 - frld(ji,jj) ) * uscomi ) |
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[3] | 174 | hsnif (ji,jj) = hsnif(ji,jj) * za |
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| 175 | hicif (ji,jj) = hicif(ji,jj) * za |
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| 176 | qstoif(ji,jj) = qstoif(ji,jj) * za |
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[1218] | 177 | frld (ji,jj) = 1.0 - zindb * ( 1.0 - frld(ji,jj) ) / MAX( za, epsi20 ) |
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[3] | 178 | |
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| 179 | ! the in situ ice thickness, hicif, must be equal to or greater than hiclim. |
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[1218] | 180 | zh = MAX( rone , zindb * hiclim / MAX( hicif(ji,jj), epsi20 ) ) |
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[3] | 181 | hsnif (ji,jj) = hsnif(ji,jj) * zh |
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| 182 | hicif (ji,jj) = hicif(ji,jj) * zh |
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| 183 | qstoif(ji,jj) = qstoif(ji,jj) * zh |
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| 184 | frld (ji,jj) = ( frld(ji,jj) + ( zh - 1.0 ) ) / zh |
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| 185 | END DO |
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| 186 | END DO |
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[258] | 187 | |
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| 188 | IF(ln_ctl) THEN |
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[1218] | 189 | CALL prt_ctl( tab2d_1=hicif , clinfo1=' lim_thd: hicif : ' ) |
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| 190 | CALL prt_ctl( tab2d_1=hsnif , clinfo1=' lim_thd: hsnif : ' ) |
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| 191 | CALL prt_ctl( tab2d_1=dmgwi , clinfo1=' lim_thd: dmgwi : ' ) |
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| 192 | CALL prt_ctl( tab2d_1=qstoif, clinfo1=' lim_thd: qstoif : ' ) |
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| 193 | CALL prt_ctl( tab2d_1=frld , clinfo1=' lim_thd: frld : ' ) |
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[3] | 194 | ENDIF |
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| 195 | |
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| 196 | |
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| 197 | !-------------------------------! |
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| 198 | ! Thermodynamics of sea ice ! |
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| 199 | !-------------------------------! |
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| 200 | |
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| 201 | ! Partial computation of forcing for the thermodynamic sea ice model. |
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| 202 | !-------------------------------------------------------------------------- |
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| 203 | |
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[888] | 204 | sst_m(:,:) = sst_m(:,:) + rt0 |
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| 205 | |
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[1697] | 206 | !CDIR NOVERRCHK |
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[3] | 207 | DO jj = 1, jpj |
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[1697] | 208 | !CDIR NOVERRCHK |
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[3] | 209 | DO ji = 1, jpi |
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| 210 | zthsnice = hsnif(ji,jj) + hicif(ji,jj) |
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[1218] | 211 | zindb = tms(ji,jj) * ( 1.0 - MAX( rzero , SIGN( rone , - zthsnice ) ) ) |
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[3] | 212 | pfrld(ji,jj) = frld(ji,jj) |
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[1559] | 213 | zfricp = 1.0 - frld(ji,jj) |
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| 214 | zinda = 1.0 - MAX( rzero , SIGN( rone , - zfricp ) ) |
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[3] | 215 | |
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| 216 | ! solar irradiance transmission at the mixed layer bottom and used in the lead heat budget |
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[70] | 217 | thcm(ji,jj) = 0.e0 |
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[3] | 218 | |
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| 219 | ! net downward heat flux from the ice to the ocean, expressed as a function of ocean |
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| 220 | ! temperature and turbulent mixing (McPhee, 1992) |
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| 221 | zfric_u = MAX ( MIN( SQRT( ust2s(ji,jj) ) , zfric_umax ) , zfric_umin ) ! friction velocity |
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[888] | 222 | fdtcn(ji,jj) = zindb * rau0 * rcp * 0.006 * zfric_u * ( sst_m(ji,jj) - tfu(ji,jj) ) |
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[3] | 223 | qdtcn(ji,jj) = zindb * fdtcn(ji,jj) * frld(ji,jj) * rdt_ice |
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| 224 | |
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| 225 | ! partial computation of the lead energy budget (qldif) |
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[1218] | 226 | #if defined key_coupled |
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| 227 | qldif(ji,jj) = tms(ji,jj) * rdt_ice & |
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[1559] | 228 | & * ( ( qsr_tot(ji,jj) - qsr_ice(ji,jj,1) * zfricp ) * ( 1.0 - thcm(ji,jj) ) & |
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| 229 | & + ( qns_tot(ji,jj) - qns_ice(ji,jj,1) * zfricp ) & |
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[1218] | 230 | & + frld(ji,jj) * ( fdtcn(ji,jj) + ( 1.0 - zindb ) * fsbbq(ji,jj) ) ) |
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| 231 | #else |
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| 232 | zfontn = ( sprecip(ji,jj) / rhosn ) * xlsn ! energy for melting solid precipitation |
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[888] | 233 | zfnsol = qns(ji,jj) ! total non solar flux over the ocean |
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| 234 | qldif(ji,jj) = tms(ji,jj) * ( qsr(ji,jj) * ( 1.0 - thcm(ji,jj) ) & |
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[3] | 235 | & + zfnsol + fdtcn(ji,jj) - zfontn & |
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| 236 | & + ( 1.0 - zindb ) * fsbbq(ji,jj) ) & |
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[1218] | 237 | & * frld(ji,jj) * rdt_ice |
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| 238 | !!$ qldif(ji,jj) = tms(ji,jj) * rdt_ice * frld(ji,jj) |
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| 239 | !!$ & * ( qsr(ji,jj) * ( 1.0 - thcm(ji,jj) ) & |
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| 240 | !!$ & + qns(ji,jj) + fdtcn(ji,jj) - zfontn & |
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| 241 | !!$ & + ( 1.0 - zindb ) * fsbbq(ji,jj) ) & |
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| 242 | #endif |
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[3] | 243 | ! parlat : percentage of energy used for lateral ablation (0.0) |
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[1218] | 244 | zfntlat = 1.0 - MAX( rzero , SIGN( rone , - qldif(ji,jj) ) ) |
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[3] | 245 | zpareff = 1.0 + ( parlat - 1.0 ) * zinda * zfntlat |
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| 246 | zqlbsbq(ji,jj) = qldif(ji,jj) * ( 1.0 - zpareff ) / MAX( (1.0 - frld(ji,jj)) * rdt_ice , epsi16 ) |
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| 247 | qldif (ji,jj) = zpareff * qldif(ji,jj) |
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| 248 | qdtcn (ji,jj) = zpareff * qdtcn(ji,jj) |
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| 249 | |
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| 250 | ! energy needed to bring ocean surface layer until its freezing |
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[1565] | 251 | qcmif (ji,jj) = rau0 * rcp * fse3t_m(ji,jj,1) & |
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| 252 | & * ( tfu(ji,jj) - sst_m(ji,jj) ) * ( 1 - zinda ) |
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[3] | 253 | |
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| 254 | ! calculate oceanic heat flux. |
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| 255 | fbif (ji,jj) = zindb * ( fsbbq(ji,jj) / MAX( (1.0 - frld(ji,jj)) , epsi20 ) + fdtcn(ji,jj) ) |
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| 256 | |
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[1482] | 257 | ! computation of the thermodynamic ice production (only needed for output) |
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| 258 | hicifp(ji,jj) = hicif(ji,jj) * ( 1.0 - frld(ji,jj) ) |
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[3] | 259 | END DO |
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| 260 | END DO |
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| 261 | |
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[888] | 262 | sst_m(:,:) = sst_m(:,:) - rt0 |
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[1482] | 263 | |
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[3] | 264 | ! Select icy points and fulfill arrays for the vectorial grid. |
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| 265 | !---------------------------------------------------------------------- |
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| 266 | nbpb = 0 |
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| 267 | DO jj = 1, jpj |
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| 268 | DO ji = 1, jpi |
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| 269 | IF ( frld(ji,jj) < 1.0 ) THEN |
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| 270 | nbpb = nbpb + 1 |
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| 271 | npb(nbpb) = (jj - 1) * jpi + ji |
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| 272 | ENDIF |
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| 273 | END DO |
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| 274 | END DO |
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[258] | 275 | |
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| 276 | IF(ln_ctl) THEN |
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| 277 | CALL prt_ctl(tab2d_1=pfrld, clinfo1=' lim_thd: pfrld : ', tab2d_2=thcm , clinfo2=' thcm : ') |
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| 278 | CALL prt_ctl(tab2d_1=fdtcn, clinfo1=' lim_thd: fdtcn : ', tab2d_2=qdtcn , clinfo2=' qdtcn : ') |
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| 279 | CALL prt_ctl(tab2d_1=qldif, clinfo1=' lim_thd: qldif : ', tab2d_2=zqlbsbq, clinfo2=' zqlbsbq : ') |
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| 280 | CALL prt_ctl(tab2d_1=qcmif, clinfo1=' lim_thd: qcmif : ', tab2d_2=fbif , clinfo2=' fbif : ') |
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| 281 | zmsk(:,:,1) = tms(:,:) |
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[1482] | 282 | CALL prt_ctl(tab2d_1=qcmif , clinfo1=' lim_thd: qcmif : ', mask1=zmsk) |
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| 283 | CALL prt_ctl(tab2d_1=hicifp, clinfo1=' lim_thd: hicifp : ') |
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[258] | 284 | WRITE(charout, FMT="('lim_thd: nbpb = ',I4)") nbpb |
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| 285 | CALL prt_ctl_info(charout) |
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[3] | 286 | ENDIF |
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| 287 | |
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| 288 | |
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| 289 | ! If there is no ice, do nothing. Otherwise, compute Top and Bottom accretion/ablation |
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| 290 | !------------------------------------------------------------------------------------ |
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| 291 | |
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[1218] | 292 | IF( nbpb > 0 ) THEN |
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| 293 | ! |
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[3] | 294 | ! put the variable in a 1-D array for thermodynamics process |
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[1463] | 295 | CALL tab_2d_1d_2( nbpb, frld_1d (1:nbpb) , frld , jpi, jpj, npb(1:nbpb) ) |
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| 296 | CALL tab_2d_1d_2( nbpb, h_ice_1d (1:nbpb) , hicif , jpi, jpj, npb(1:nbpb) ) |
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| 297 | CALL tab_2d_1d_2( nbpb, h_snow_1d (1:nbpb) , hsnif , jpi, jpj, npb(1:nbpb) ) |
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| 298 | CALL tab_2d_1d_2( nbpb, sist_1d (1:nbpb) , sist , jpi, jpj, npb(1:nbpb) ) |
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| 299 | CALL tab_2d_1d_2( nbpb, tbif_1d (1:nbpb , 1 ), tbif(:,:,1) , jpi, jpj, npb(1:nbpb) ) |
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| 300 | CALL tab_2d_1d_2( nbpb, tbif_1d (1:nbpb , 2 ), tbif(:,:,2) , jpi, jpj, npb(1:nbpb) ) |
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| 301 | CALL tab_2d_1d_2( nbpb, tbif_1d (1:nbpb , 3 ), tbif(:,:,3) , jpi, jpj, npb(1:nbpb) ) |
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| 302 | CALL tab_2d_1d_2( nbpb, qsr_ice_1d (1:nbpb) , qsr_ice(:,:,1) , jpi, jpj, npb(1:nbpb) ) |
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| 303 | CALL tab_2d_1d_2( nbpb, fr1_i0_1d (1:nbpb) , fr1_i0 , jpi, jpj, npb(1:nbpb) ) |
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| 304 | CALL tab_2d_1d_2( nbpb, fr2_i0_1d (1:nbpb) , fr2_i0 , jpi, jpj, npb(1:nbpb) ) |
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| 305 | CALL tab_2d_1d_2( nbpb, qns_ice_1d(1:nbpb) , qns_ice(:,:,1), jpi, jpj, npb(1:nbpb) ) |
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| 306 | CALL tab_2d_1d_2( nbpb, dqns_ice_1d(1:nbpb) , dqns_ice(:,:,1), jpi, jpj, npb(1:nbpb) ) |
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[1218] | 307 | IF( .NOT. lk_cpl ) THEN |
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[1463] | 308 | CALL tab_2d_1d_2( nbpb, qla_ice_1d (1:nbpb) , qla_ice(:,:,1), jpi, jpj, npb(1:nbpb) ) |
---|
| 309 | CALL tab_2d_1d_2( nbpb, dqla_ice_1d(1:nbpb) , dqla_ice(:,:,1), jpi, jpj, npb(1:nbpb) ) |
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[1218] | 310 | ENDIF |
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[821] | 311 | CALL tab_2d_1d_2( nbpb, tfu_1d (1:nbpb) , tfu , jpi, jpj, npb(1:nbpb) ) |
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| 312 | CALL tab_2d_1d_2( nbpb, sprecip_1d (1:nbpb) , sprecip , jpi, jpj, npb(1:nbpb) ) |
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| 313 | CALL tab_2d_1d_2( nbpb, fbif_1d (1:nbpb) , fbif , jpi, jpj, npb(1:nbpb) ) |
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| 314 | CALL tab_2d_1d_2( nbpb, thcm_1d (1:nbpb) , thcm , jpi, jpj, npb(1:nbpb) ) |
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| 315 | CALL tab_2d_1d_2( nbpb, qldif_1d (1:nbpb) , qldif , jpi, jpj, npb(1:nbpb) ) |
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| 316 | CALL tab_2d_1d_2( nbpb, qstbif_1d (1:nbpb) , qstoif , jpi, jpj, npb(1:nbpb) ) |
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| 317 | CALL tab_2d_1d_2( nbpb, rdmicif_1d (1:nbpb) , rdmicif , jpi, jpj, npb(1:nbpb) ) |
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| 318 | CALL tab_2d_1d_2( nbpb, dmgwi_1d (1:nbpb) , dmgwi , jpi, jpj, npb(1:nbpb) ) |
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| 319 | CALL tab_2d_1d_2( nbpb, qlbbq_1d (1:nbpb) , zqlbsbq , jpi, jpj, npb(1:nbpb) ) |
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[1218] | 320 | ! |
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[821] | 321 | CALL lim_thd_zdf_2( 1, nbpb ) ! compute ice growth |
---|
[1218] | 322 | ! |
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[3] | 323 | ! back to the geographic grid. |
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[821] | 324 | CALL tab_1d_2d_2( nbpb, frld , npb, frld_1d (1:nbpb) , jpi, jpj ) |
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| 325 | CALL tab_1d_2d_2( nbpb, hicif , npb, h_ice_1d (1:nbpb) , jpi, jpj ) |
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| 326 | CALL tab_1d_2d_2( nbpb, hsnif , npb, h_snow_1d (1:nbpb) , jpi, jpj ) |
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| 327 | CALL tab_1d_2d_2( nbpb, sist , npb, sist_1d (1:nbpb) , jpi, jpj ) |
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| 328 | CALL tab_1d_2d_2( nbpb, tbif(:,:,1), npb, tbif_1d (1:nbpb , 1 ), jpi, jpj ) |
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| 329 | CALL tab_1d_2d_2( nbpb, tbif(:,:,2), npb, tbif_1d (1:nbpb , 2 ), jpi, jpj ) |
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| 330 | CALL tab_1d_2d_2( nbpb, tbif(:,:,3), npb, tbif_1d (1:nbpb , 3 ), jpi, jpj ) |
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| 331 | CALL tab_1d_2d_2( nbpb, fscmbq , npb, fscbq_1d (1:nbpb) , jpi, jpj ) |
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| 332 | CALL tab_1d_2d_2( nbpb, ffltbif , npb, fltbif_1d (1:nbpb) , jpi, jpj ) |
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| 333 | CALL tab_1d_2d_2( nbpb, fstric , npb, fstbif_1d (1:nbpb) , jpi, jpj ) |
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| 334 | CALL tab_1d_2d_2( nbpb, qldif , npb, qldif_1d (1:nbpb) , jpi, jpj ) |
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| 335 | CALL tab_1d_2d_2( nbpb, qfvbq , npb, qfvbq_1d (1:nbpb) , jpi, jpj ) |
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| 336 | CALL tab_1d_2d_2( nbpb, qstoif , npb, qstbif_1d (1:nbpb) , jpi, jpj ) |
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| 337 | CALL tab_1d_2d_2( nbpb, rdmicif , npb, rdmicif_1d(1:nbpb) , jpi, jpj ) |
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| 338 | CALL tab_1d_2d_2( nbpb, dmgwi , npb, dmgwi_1d (1:nbpb) , jpi, jpj ) |
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| 339 | CALL tab_1d_2d_2( nbpb, rdmsnif , npb, rdmsnif_1d(1:nbpb) , jpi, jpj ) |
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[1756] | 340 | CALL tab_1d_2d_2( nbpb, zdvosif , npb, dvsbq_1d (1:nbpb) , jpi, jpj ) |
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| 341 | CALL tab_1d_2d_2( nbpb, zdvobif , npb, dvbbq_1d (1:nbpb) , jpi, jpj ) |
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| 342 | CALL tab_1d_2d_2( nbpb, zdvomif , npb, rdvomif_1d(1:nbpb) , jpi, jpj ) |
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| 343 | CALL tab_1d_2d_2( nbpb, zdvolif , npb, dvlbq_1d (1:nbpb) , jpi, jpj ) |
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| 344 | CALL tab_1d_2d_2( nbpb, zdvonif , npb, dvnbq_1d (1:nbpb) , jpi, jpj ) |
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[1482] | 345 | CALL tab_1d_2d_2( nbpb, qsr_ice(:,:,1), npb, qsr_ice_1d(1:nbpb) , jpi, jpj ) |
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| 346 | CALL tab_1d_2d_2( nbpb, qns_ice(:,:,1), npb, qns_ice_1d(1:nbpb) , jpi, jpj ) |
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| 347 | IF( .NOT. lk_cpl ) CALL tab_1d_2d_2( nbpb, qla_ice(:,:,1), npb, qla_ice_1d(1:nbpb) , jpi, jpj ) |
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[1218] | 348 | ! |
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[3] | 349 | ENDIF |
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| 350 | |
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[1218] | 351 | ! Up-date sea ice thickness |
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| 352 | !-------------------------- |
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[3] | 353 | DO jj = 1, jpj |
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| 354 | DO ji = 1, jpi |
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| 355 | phicif(ji,jj) = hicif(ji,jj) |
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[1218] | 356 | hicif(ji,jj) = hicif(ji,jj) * ( rone - MAX( rzero, SIGN( rone, - ( 1.0 - frld(ji,jj) ) ) ) ) |
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[3] | 357 | END DO |
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| 358 | END DO |
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| 359 | |
---|
| 360 | |
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[1218] | 361 | ! Tricky trick : add 2 to frld in the Southern Hemisphere |
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| 362 | !-------------------------------------------------------- |
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[192] | 363 | IF( fcor(1,1) < 0.e0 ) THEN |
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[421] | 364 | DO jj = 1, njeqm1 |
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[192] | 365 | DO ji = 1, jpi |
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| 366 | frld(ji,jj) = frld(ji,jj) + 2.0 |
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| 367 | END DO |
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[3] | 368 | END DO |
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[192] | 369 | ENDIF |
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[1924] | 370 | |
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| 371 | CALL lbc_lnk( frld , 'T', 1. ) |
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[3] | 372 | |
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[1218] | 373 | ! Select points for lateral accretion (this occurs when heat exchange |
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| 374 | ! between ice and ocean is negative; ocean losing heat) |
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[3] | 375 | !----------------------------------------------------------------- |
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| 376 | nbpac = 0 |
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| 377 | DO jj = 1, jpj |
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| 378 | DO ji = 1, jpi |
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[70] | 379 | !i yes! IF ( ( qcmif(ji,jj) - qldif(ji,jj) ) > 0.e0 ) THEN |
---|
| 380 | IF ( tms(ji,jj) * ( qcmif(ji,jj) - qldif(ji,jj) ) > 0.e0 ) THEN |
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[3] | 381 | nbpac = nbpac + 1 |
---|
| 382 | npac( nbpac ) = (jj - 1) * jpi + ji |
---|
| 383 | ENDIF |
---|
| 384 | END DO |
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| 385 | END DO |
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| 386 | |
---|
[258] | 387 | IF(ln_ctl) THEN |
---|
| 388 | CALL prt_ctl(tab2d_1=phicif, clinfo1=' lim_thd: phicif : ', tab2d_2=hicif, clinfo2=' hicif : ') |
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| 389 | WRITE(charout, FMT="('lim_thd: nbpac = ',I4)") nbpac |
---|
| 390 | CALL prt_ctl_info(charout) |
---|
[3] | 391 | ENDIF |
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| 392 | |
---|
[1218] | 393 | |
---|
| 394 | ! If ocean gains heat do nothing ; otherwise, one performs lateral accretion |
---|
[3] | 395 | !-------------------------------------------------------------------------------- |
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[70] | 396 | IF( nbpac > 0 ) THEN |
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[1218] | 397 | ! |
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[1756] | 398 | zlicegr(:,:) = rdmicif(:,:) ! to output the lateral sea-ice growth |
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[3] | 399 | !...Put the variable in a 1-D array for lateral accretion |
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[821] | 400 | CALL tab_2d_1d_2( nbpac, frld_1d (1:nbpac) , frld , jpi, jpj, npac(1:nbpac) ) |
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| 401 | CALL tab_2d_1d_2( nbpac, h_snow_1d (1:nbpac) , hsnif , jpi, jpj, npac(1:nbpac) ) |
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| 402 | CALL tab_2d_1d_2( nbpac, h_ice_1d (1:nbpac) , hicif , jpi, jpj, npac(1:nbpac) ) |
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| 403 | CALL tab_2d_1d_2( nbpac, tbif_1d (1:nbpac , 1 ), tbif(:,:,1), jpi, jpj, npac(1:nbpac) ) |
---|
| 404 | CALL tab_2d_1d_2( nbpac, tbif_1d (1:nbpac , 2 ), tbif(:,:,2), jpi, jpj, npac(1:nbpac) ) |
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| 405 | CALL tab_2d_1d_2( nbpac, tbif_1d (1:nbpac , 3 ), tbif(:,:,3), jpi, jpj, npac(1:nbpac) ) |
---|
| 406 | CALL tab_2d_1d_2( nbpac, qldif_1d (1:nbpac) , qldif , jpi, jpj, npac(1:nbpac) ) |
---|
| 407 | CALL tab_2d_1d_2( nbpac, qcmif_1d (1:nbpac) , qcmif , jpi, jpj, npac(1:nbpac) ) |
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| 408 | CALL tab_2d_1d_2( nbpac, qstbif_1d (1:nbpac) , qstoif , jpi, jpj, npac(1:nbpac) ) |
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| 409 | CALL tab_2d_1d_2( nbpac, rdmicif_1d(1:nbpac) , rdmicif , jpi, jpj, npac(1:nbpac) ) |
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[1756] | 410 | CALL tab_2d_1d_2( nbpac, dvlbq_1d (1:nbpac) , zdvolif , jpi, jpj, npac(1:nbpac) ) |
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[821] | 411 | CALL tab_2d_1d_2( nbpac, tfu_1d (1:nbpac) , tfu , jpi, jpj, npac(1:nbpac) ) |
---|
[1218] | 412 | ! |
---|
| 413 | CALL lim_thd_lac_2( 1 , nbpac ) ! lateral accretion routine. |
---|
| 414 | ! |
---|
[70] | 415 | ! back to the geographic grid |
---|
[821] | 416 | CALL tab_1d_2d_2( nbpac, frld , npac(1:nbpac), frld_1d (1:nbpac) , jpi, jpj ) |
---|
| 417 | CALL tab_1d_2d_2( nbpac, hsnif , npac(1:nbpac), h_snow_1d (1:nbpac) , jpi, jpj ) |
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| 418 | CALL tab_1d_2d_2( nbpac, hicif , npac(1:nbpac), h_ice_1d (1:nbpac) , jpi, jpj ) |
---|
| 419 | CALL tab_1d_2d_2( nbpac, tbif(:,:,1), npac(1:nbpac), tbif_1d (1:nbpac , 1 ), jpi, jpj ) |
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| 420 | CALL tab_1d_2d_2( nbpac, tbif(:,:,2), npac(1:nbpac), tbif_1d (1:nbpac , 2 ), jpi, jpj ) |
---|
| 421 | CALL tab_1d_2d_2( nbpac, tbif(:,:,3), npac(1:nbpac), tbif_1d (1:nbpac , 3 ), jpi, jpj ) |
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| 422 | CALL tab_1d_2d_2( nbpac, qstoif , npac(1:nbpac), qstbif_1d (1:nbpac) , jpi, jpj ) |
---|
| 423 | CALL tab_1d_2d_2( nbpac, rdmicif , npac(1:nbpac), rdmicif_1d(1:nbpac) , jpi, jpj ) |
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[1756] | 424 | CALL tab_1d_2d_2( nbpac, zdvolif , npac(1:nbpac), dvlbq_1d (1:nbpac) , jpi, jpj ) |
---|
[1218] | 425 | ! |
---|
[70] | 426 | ENDIF |
---|
[3] | 427 | |
---|
| 428 | |
---|
[1218] | 429 | ! Recover frld values between 0 and 1 in the Southern Hemisphere (tricky trick) |
---|
| 430 | ! Update daily thermodynamic ice production. |
---|
[70] | 431 | !------------------------------------------------------------------------------ |
---|
[3] | 432 | DO jj = 1, jpj |
---|
| 433 | DO ji = 1, jpi |
---|
| 434 | frld (ji,jj) = MIN( frld(ji,jj), ABS( frld(ji,jj) - 2.0 ) ) |
---|
[1482] | 435 | fr_i (ji,jj) = 1.0 - frld(ji,jj) |
---|
| 436 | hicifp(ji,jj) = hicif(ji,jj) * fr_i(ji,jj) - hicifp(ji,jj) |
---|
[3] | 437 | END DO |
---|
| 438 | END DO |
---|
| 439 | |
---|
[1482] | 440 | ! Outputs |
---|
| 441 | !-------------------------------------------------------------------------------- |
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[1756] | 442 | ztmp(:,:) = 1. - pfrld(:,:) ! fraction of ice after the dynamic, before the thermodynamic |
---|
| 443 | CALL iom_put( 'ioceflxb', fbif ) ! Oceanic flux at the ice base [W/m2 ???] |
---|
| 444 | CALL iom_put( 'ist_cea', (sist(:,:) - rt0) * ztmp(:,:) ) ! Ice surface temperature [Celius] |
---|
| 445 | CALL iom_put( 'qsr_ai_cea', qsr_ice(:,:,1) * ztmp(:,:) ) ! Solar flux over the ice [W/m2] |
---|
| 446 | CALL iom_put( 'qns_ai_cea', qns_ice(:,:,1) * ztmp(:,:) ) ! Non-solar flux over the ice [W/m2] |
---|
[1482] | 447 | IF( .NOT. lk_cpl ) CALL iom_put( 'qla_ai_cea', qla_ice(:,:,1) * ztmp(:,:) ) ! Latent flux over the ice [W/m2] |
---|
| 448 | ! |
---|
[1756] | 449 | CALL iom_put( 'snowthic_cea', hsnif (:,:) * fr_i(:,:) ) ! Snow thickness [m] |
---|
| 450 | CALL iom_put( 'icethic_cea' , hicif (:,:) * fr_i(:,:) ) ! Ice thickness [m] |
---|
| 451 | zztmp = 1.0 / rdt_ice |
---|
| 452 | CALL iom_put( 'iceprod_cea' , hicifp (:,:) * zztmp ) ! Ice produced [m/s] |
---|
| 453 | IF( lk_diaar5 ) THEN |
---|
| 454 | CALL iom_put( 'snowmel_cea' , rdmsnif(:,:) * zztmp ) ! Snow melt [kg/m2/s] |
---|
| 455 | zztmp = rhoic / rdt_ice |
---|
| 456 | CALL iom_put( 'sntoice_cea' , zdvonif(:,:) * zztmp ) ! Snow to Ice transformation [kg/m2/s] |
---|
| 457 | CALL iom_put( 'ticemel_cea' , zdvosif(:,:) * zztmp ) ! Melt at Sea Ice top [kg/m2/s] |
---|
| 458 | CALL iom_put( 'bicemel_cea' , zdvomif(:,:) * zztmp ) ! Melt at Sea Ice bottom [kg/m2/s] |
---|
| 459 | zlicegr(:,:) = MAX( 0.e0, rdmicif(:,:)-zlicegr(:,:) ) |
---|
| 460 | CALL iom_put( 'licepro_cea' , zlicegr(:,:) * zztmp ) ! Latereal sea ice growth [kg/m2/s] |
---|
| 461 | ENDIF |
---|
[1482] | 462 | ! |
---|
[1756] | 463 | ! Compute the Eastward & Northward sea-ice transport |
---|
| 464 | zztmp = 0.25 * rhoic |
---|
| 465 | DO jj = 1, jpjm1 |
---|
| 466 | DO ji = 1, jpim1 ! NO vector opt. |
---|
| 467 | ! Ice velocities, volume & transport at U & V-points |
---|
| 468 | zuice_m = u_ice(ji+1,jj+1) + u_ice(ji+1,jj ) |
---|
| 469 | zvice_m = v_ice(ji+1,jj+1) + v_ice(ji ,jj+1) |
---|
| 470 | zhice_u = hicif(ji,jj)*e2t(ji,jj)*fr_i(ji,jj) + hicif(ji+1,jj )*e2t(ji+1,jj )*fr_i(ji+1,jj ) |
---|
| 471 | zhice_v = hicif(ji,jj)*e1t(ji,jj)*fr_i(ji,jj) + hicif(ji ,jj+1)*e1t(ji ,jj+1)*fr_i(ji ,jj+1) |
---|
| 472 | zu_imasstr(ji,jj) = zztmp * zhice_u * zuice_m |
---|
| 473 | zv_imasstr(ji,jj) = zztmp * zhice_v * zvice_m |
---|
| 474 | END DO |
---|
| 475 | END DO |
---|
| 476 | CALL lbc_lnk( zu_imasstr, 'U', -1. ) ; CALL lbc_lnk( zv_imasstr, 'V', -1. ) |
---|
| 477 | CALL iom_put( 'u_imasstr', zu_imasstr(:,:) ) ! Ice transport along i-axis at U-point [kg/s] |
---|
| 478 | CALL iom_put( 'v_imasstr', zv_imasstr(:,:) ) ! Ice transport along j-axis at V-point [kg/s] |
---|
[1482] | 479 | |
---|
[1756] | 480 | !! Fram Strait sea-ice transport (sea-ice + snow) (in ORCA2 = 5 points) |
---|
| 481 | IF( cp_cfg == "orca" .AND. jp_cfg == 2 ) THEN ! ORCA R2 configuration |
---|
| 482 | DO jj = mj0(137), mj1(137) ! B grid |
---|
| 483 | IF( mj0(jj-1) >= nldj ) THEN |
---|
| 484 | DO ji = MAX(mi0(134),nldi), MIN(mi1(138),nlei) |
---|
| 485 | zrhoij = e1t(ji,jj ) * fr_i(ji,jj ) * ( rhoic*hicif(ji,jj ) + rhosn*hsnif(ji,jj ) ) |
---|
| 486 | zrhoijm1 = e1t(ji,jj-1) * fr_i(ji,jj-1) * ( rhoic*hicif(ji,jj-1) + rhosn*hsnif(ji,jj-1) ) |
---|
| 487 | ztr_fram = ztr_fram - 0.25 * ( v_ice(ji,jj)+ v_ice(ji+1,jj) ) * ( zrhoij + zrhoijm1 ) |
---|
| 488 | END DO |
---|
| 489 | ENDIF |
---|
| 490 | END DO |
---|
| 491 | IF( lk_mpp ) CALL mpp_sum( ztr_fram ) |
---|
| 492 | CALL iom_put( 'fram_trans', ztr_fram ) ! Ice transport through Fram strait [kg/s] |
---|
| 493 | ENDIF |
---|
| 494 | |
---|
[2411] | 495 | !! ce ztmp(:,:) = 1. - AINT( frld(:,:), wp ) ! return 1 as soon as there is ice |
---|
| 496 | !! ce A big warning because the model crashes on IDRIS/IBM SP6 with xlf 13.1.0.3, see ticket #761 |
---|
| 497 | !! ce We Unroll the loop and everything works fine |
---|
| 498 | DO jj = 1, jpj |
---|
| 499 | DO ji = 1, jpi |
---|
| 500 | ztmp(ji,jj) = 1. - AINT( frld(ji,jj), wp ) ! return 1 as soon as there is ice |
---|
| 501 | END DO |
---|
| 502 | END DO |
---|
| 503 | ! |
---|
[1756] | 504 | CALL iom_put( 'ice_pres' , ztmp ) ! Ice presence [-] |
---|
| 505 | CALL iom_put( 'ist_ipa' , ( sist(:,:) - rt0 ) * ztmp(:,:) ) ! Ice surface temperature [Celius] |
---|
| 506 | CALL iom_put( 'uice_ipa' , u_ice(:,:) * ztmp(:,:) ) ! Ice velocity along i-axis at I-point [m/s] |
---|
| 507 | CALL iom_put( 'vice_ipa' , v_ice(:,:) * ztmp(:,:) ) ! Ice velocity along j-axis at I-point [m/s] |
---|
| 508 | |
---|
[258] | 509 | IF(ln_ctl) THEN |
---|
| 510 | CALL prt_ctl_info(' lim_thd end ') |
---|
[1218] | 511 | CALL prt_ctl( tab2d_1=hicif , clinfo1=' lim_thd: hicif : ', tab2d_2=hsnif , clinfo2=' hsnif : ' ) |
---|
| 512 | CALL prt_ctl( tab2d_1=frld , clinfo1=' lim_thd: frld : ', tab2d_2=hicifp, clinfo2=' hicifp : ' ) |
---|
| 513 | CALL prt_ctl( tab2d_1=phicif , clinfo1=' lim_thd: phicif : ', tab2d_2=pfrld , clinfo2=' pfrld : ' ) |
---|
| 514 | CALL prt_ctl( tab2d_1=sist , clinfo1=' lim_thd: sist : ' ) |
---|
| 515 | CALL prt_ctl( tab2d_1=tbif(:,:,1), clinfo1=' lim_thd: tbif 1 : ' ) |
---|
| 516 | CALL prt_ctl( tab2d_1=tbif(:,:,2), clinfo1=' lim_thd: tbif 2 : ' ) |
---|
| 517 | CALL prt_ctl( tab2d_1=tbif(:,:,3), clinfo1=' lim_thd: tbif 3 : ' ) |
---|
| 518 | CALL prt_ctl( tab2d_1=fdtcn , clinfo1=' lim_thd: fdtcn : ', tab2d_2=qdtcn , clinfo2=' qdtcn : ' ) |
---|
| 519 | CALL prt_ctl( tab2d_1=qstoif , clinfo1=' lim_thd: qstoif : ', tab2d_2=fsbbq , clinfo2=' fsbbq : ' ) |
---|
[3] | 520 | ENDIF |
---|
[888] | 521 | ! |
---|
[2715] | 522 | IF( wrk_not_released(2, 1,2,3,4,5,6,7,8,9,10) .OR. & |
---|
| 523 | wrk_not_released(3, 4) ) THEN |
---|
| 524 | CALL ctl_stop('lim_thd_2 : failed to release workspace arrays') |
---|
| 525 | ENDIF |
---|
| 526 | ! |
---|
[821] | 527 | END SUBROUTINE lim_thd_2 |
---|
[3] | 528 | |
---|
[719] | 529 | |
---|
[821] | 530 | SUBROUTINE lim_thd_init_2 |
---|
[3] | 531 | !!------------------------------------------------------------------- |
---|
[821] | 532 | !! *** ROUTINE lim_thd_init_2 *** |
---|
[3] | 533 | !! |
---|
| 534 | !! ** Purpose : Physical constants and parameters linked to the ice |
---|
| 535 | !! thermodynamics |
---|
| 536 | !! |
---|
| 537 | !! ** Method : Read the namicethd namelist and check the ice-thermo |
---|
| 538 | !! parameter values called at the first timestep (nit000) |
---|
| 539 | !! |
---|
| 540 | !! ** input : Namelist namicether |
---|
| 541 | !!------------------------------------------------------------------- |
---|
| 542 | NAMELIST/namicethd/ hmelt , hiccrit, hicmin, hiclim, amax , & |
---|
| 543 | & swiqst, sbeta , parlat, hakspl, hibspl, exld, & |
---|
| 544 | & hakdif, hnzst , thth , parsub, alphs |
---|
| 545 | !!------------------------------------------------------------------- |
---|
[1218] | 546 | ! |
---|
| 547 | REWIND( numnam_ice ) ! read namelist |
---|
[3] | 548 | READ ( numnam_ice , namicethd ) |
---|
[1218] | 549 | IF( lk_cpl .AND. parsub /= 0.0 ) CALL ctl_stop( 'In coupled mode, use parsub = 0. or send dqla' ) |
---|
| 550 | ! |
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| 551 | IF(lwp) THEN ! control print |
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[3] | 552 | WRITE(numout,*) |
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[821] | 553 | WRITE(numout,*)'lim_thd_init_2: ice parameters for ice thermodynamic computation ' |
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| 554 | WRITE(numout,*)'~~~~~~~~~~~~~~' |
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[70] | 555 | WRITE(numout,*)' maximum melting at the bottom hmelt = ', hmelt |
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| 556 | WRITE(numout,*)' ice thick. for lateral accretion in NH (SH) hiccrit(1/2) = ', hiccrit |
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| 557 | WRITE(numout,*)' ice thick. corr. to max. energy stored in brine pocket hicmin = ', hicmin |
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| 558 | WRITE(numout,*)' minimum ice thickness hiclim = ', hiclim |
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| 559 | WRITE(numout,*)' maximum lead fraction amax = ', amax |
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[1218] | 560 | WRITE(numout,*)' energy stored in brine pocket (=1) or not (=0) swiqst = ', swiqst |
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[70] | 561 | WRITE(numout,*)' numerical carac. of the scheme for diffusion in ice ' |
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| 562 | WRITE(numout,*)' Cranck-Nicholson (=0.5), implicit (=1), explicit (=0) sbeta = ', sbeta |
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| 563 | WRITE(numout,*)' percentage of energy used for lateral ablation parlat = ', parlat |
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| 564 | WRITE(numout,*)' slope of distr. for Hakkinen-Mellor lateral melting hakspl = ', hakspl |
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| 565 | WRITE(numout,*)' slope of distribution for Hibler lateral melting hibspl = ', hibspl |
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| 566 | WRITE(numout,*)' exponent for leads-closure rate exld = ', exld |
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| 567 | WRITE(numout,*)' coefficient for diffusions of ice and snow hakdif = ', hakdif |
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| 568 | WRITE(numout,*)' threshold thick. for comp. of eq. thermal conductivity zhth = ', thth |
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| 569 | WRITE(numout,*)' thickness of the surf. layer in temp. computation hnzst = ', hnzst |
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| 570 | WRITE(numout,*)' switch for snow sublimation (=1) or not (=0) parsub = ', parsub |
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| 571 | WRITE(numout,*)' coefficient for snow density when snow ice formation alphs = ', alphs |
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[3] | 572 | ENDIF |
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[1218] | 573 | ! |
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[3] | 574 | uscomi = 1.0 / ( 1.0 - amax ) ! inverse of minimum lead fraction |
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| 575 | rcdsn = hakdif * rcdsn |
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| 576 | rcdic = hakdif * rcdic |
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[1218] | 577 | ! |
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| 578 | IF( hsndif > 100.e0 .OR. hicdif > 100.e0 ) THEN |
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[3] | 579 | cnscg = 0.e0 |
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| 580 | ELSE |
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| 581 | cnscg = rcpsn / rcpic ! ratio rcpsn/rcpic |
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| 582 | ENDIF |
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[1218] | 583 | ! |
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[821] | 584 | END SUBROUTINE lim_thd_init_2 |
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[3] | 585 | |
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| 586 | #else |
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[70] | 587 | !!---------------------------------------------------------------------- |
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[821] | 588 | !! Default option Dummy module NO LIM 2.0 sea-ice model |
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[70] | 589 | !!---------------------------------------------------------------------- |
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[3] | 590 | CONTAINS |
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[821] | 591 | SUBROUTINE lim_thd_2 ! Dummy routine |
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| 592 | END SUBROUTINE lim_thd_2 |
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[3] | 593 | #endif |
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| 594 | |
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| 595 | !!====================================================================== |
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[821] | 596 | END MODULE limthd_2 |
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