[8586] | 1 | MODULE icethd |
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| 2 | !!====================================================================== |
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| 3 | !! *** MODULE icethd *** |
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| 4 | !! sea-ice : master routine for thermodynamics |
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| 5 | !!====================================================================== |
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[9656] | 6 | !! History : 1.0 ! 2000-01 (M.A. Morales Maqueda, H. Goosse, T. Fichefet) original code 1D |
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[9604] | 7 | !! 4.0 ! 2018 (many people) SI3 [aka Sea Ice cube] |
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[8586] | 8 | !!---------------------------------------------------------------------- |
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[9570] | 9 | #if defined key_si3 |
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[8586] | 10 | !!---------------------------------------------------------------------- |
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[9570] | 11 | !! 'key_si3' SI3 sea-ice model |
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[8586] | 12 | !!---------------------------------------------------------------------- |
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| 13 | !! ice_thd : thermodynamics of sea ice |
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| 14 | !! ice_thd_init : initialisation of sea-ice thermodynamics |
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| 15 | !!---------------------------------------------------------------------- |
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| 16 | USE phycst ! physical constants |
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| 17 | USE dom_oce ! ocean space and time domain variables |
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| 18 | USE ice ! sea-ice: variables |
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| 19 | !!gm list trop longue ==>>> why not passage en argument d'appel ? |
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[13589] | 20 | USE sbc_oce , ONLY : sss_m, sst_m, e3t_m, utau, vtau, ssu_m, ssv_m, frq_m, sprecip, ln_cpl |
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[8586] | 21 | USE sbc_ice , ONLY : qsr_oce, qns_oce, qemp_oce, qsr_ice, qns_ice, dqns_ice, evap_ice, qprec_ice, qevap_ice, & |
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[9910] | 22 | & qml_ice, qcn_ice, qtr_ice_top |
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[8586] | 23 | USE ice1D ! sea-ice: thermodynamics variables |
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| 24 | USE icethd_zdf ! sea-ice: vertical heat diffusion |
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| 25 | USE icethd_dh ! sea-ice: ice-snow growth and melt |
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| 26 | USE icethd_da ! sea-ice: lateral melting |
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| 27 | USE icethd_sal ! sea-ice: salinity |
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| 28 | USE icethd_ent ! sea-ice: enthalpy redistribution |
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| 29 | USE icethd_do ! sea-ice: growth in open water |
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[8637] | 30 | USE icethd_pnd ! sea-ice: melt ponds |
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[8586] | 31 | USE iceitd ! sea-ice: remapping thickness distribution |
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[13640] | 32 | USE icecor ! sea-ice: corrections |
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[8586] | 33 | USE icetab ! sea-ice: 1D <==> 2D transformation |
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| 34 | USE icevar ! sea-ice: operations |
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| 35 | USE icectl ! sea-ice: control print |
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| 36 | ! |
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| 37 | USE in_out_manager ! I/O manager |
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[13284] | 38 | USE iom ! I/O manager library |
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[8586] | 39 | USE lib_mpp ! MPP library |
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| 40 | USE lib_fortran ! fortran utilities (glob_sum + no signed zero) |
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| 41 | USE lbclnk ! lateral boundary conditions (or mpp links) |
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| 42 | USE timing ! Timing |
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| 43 | |
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| 44 | IMPLICIT NONE |
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| 45 | PRIVATE |
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| 46 | |
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| 47 | PUBLIC ice_thd ! called by limstp module |
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| 48 | PUBLIC ice_thd_init ! called by ice_init |
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| 49 | |
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| 50 | !!** namelist (namthd) ** |
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| 51 | LOGICAL :: ln_icedH ! activate ice thickness change from growing/melting (T) or not (F) |
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| 52 | LOGICAL :: ln_icedA ! activate lateral melting param. (T) or not (F) |
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| 53 | LOGICAL :: ln_icedO ! activate ice growth in open-water (T) or not (F) |
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| 54 | LOGICAL :: ln_icedS ! activate gravity drainage and flushing (T) or not (F) |
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[13589] | 55 | LOGICAL :: ln_leadhfx ! heat in the leads is used to melt sea-ice before warming the ocean |
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[8586] | 56 | |
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[13284] | 57 | !! for convergence tests |
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| 58 | REAL(wp), ALLOCATABLE, DIMENSION(:,:,:) :: ztice_cvgerr, ztice_cvgstp |
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| 59 | |
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[8586] | 60 | !! * Substitutions |
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| 61 | # include "vectopt_loop_substitute.h90" |
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| 62 | !!---------------------------------------------------------------------- |
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[9598] | 63 | !! NEMO/ICE 4.0 , NEMO Consortium (2018) |
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[10069] | 64 | !! $Id$ |
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[10068] | 65 | !! Software governed by the CeCILL license (see ./LICENSE) |
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[8586] | 66 | !!---------------------------------------------------------------------- |
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| 67 | CONTAINS |
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| 68 | |
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| 69 | SUBROUTINE ice_thd( kt ) |
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| 70 | !!------------------------------------------------------------------- |
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| 71 | !! *** ROUTINE ice_thd *** |
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| 72 | !! |
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| 73 | !! ** Purpose : This routine manages ice thermodynamics |
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| 74 | !! |
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[9604] | 75 | !! ** Action : - computation of oceanic sensible heat flux at the ice base |
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| 76 | !! energy budget in the leads |
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| 77 | !! net fluxes on top of ice and of ocean |
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| 78 | !! - selection of grid cells with ice |
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| 79 | !! - call ice_thd_zdf for vertical heat diffusion |
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| 80 | !! - call ice_thd_dh for vertical ice growth and melt |
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| 81 | !! - call ice_thd_pnd for melt ponds |
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| 82 | !! - call ice_thd_ent for enthalpy remapping |
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| 83 | !! - call ice_thd_sal for ice desalination |
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| 84 | !! - call ice_thd_temp to retrieve temperature from ice enthalpy |
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[9750] | 85 | !! - call ice_thd_mono for extra lateral ice melt if active virtual thickness distribution |
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[9604] | 86 | !! - call ice_thd_da for lateral ice melt |
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[8586] | 87 | !! - back to the geographic grid |
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[9604] | 88 | !! - call ice_thd_rem for remapping thickness distribution |
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| 89 | !! - call ice_thd_do for ice growth in leads |
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[8637] | 90 | !!------------------------------------------------------------------- |
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[8586] | 91 | INTEGER, INTENT(in) :: kt ! number of iteration |
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| 92 | ! |
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| 93 | INTEGER :: ji, jj, jk, jl ! dummy loop indices |
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[13589] | 94 | REAL(wp) :: zfric_u, zqld, zqfr, zqfr_neg, zqfr_pos |
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| 95 | REAL(wp), PARAMETER :: zfric_umin = 0._wp ! lower bound for the friction velocity (cice value=5.e-04) |
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| 96 | REAL(wp), PARAMETER :: zch = 0.0057_wp ! heat transfer coefficient |
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| 97 | REAL(wp), DIMENSION(jpi,jpj) :: zu_io, zv_io, zfric, zvel ! ice-ocean velocity (m/s) and frictional velocity (m2/s2) |
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[8586] | 98 | ! |
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| 99 | !!------------------------------------------------------------------- |
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| 100 | ! controls |
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[9124] | 101 | IF( ln_timing ) CALL timing_start('icethd') ! timing |
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| 102 | IF( ln_icediachk ) CALL ice_cons_hsm(0, 'icethd', rdiag_v, rdiag_s, rdiag_t, rdiag_fv, rdiag_fs, rdiag_ft) ! conservation |
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[11536] | 103 | IF( ln_icediachk ) CALL ice_cons2D (0, 'icethd', diag_v, diag_s, diag_t, diag_fv, diag_fs, diag_ft) ! conservation |
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[8586] | 104 | |
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| 105 | IF( kt == nit000 .AND. lwp ) THEN |
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| 106 | WRITE(numout,*) |
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| 107 | WRITE(numout,*) 'ice_thd: sea-ice thermodynamics' |
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| 108 | WRITE(numout,*) '~~~~~~~' |
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| 109 | ENDIF |
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[13284] | 110 | |
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| 111 | ! convergence tests |
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| 112 | IF( ln_zdf_chkcvg ) THEN |
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| 113 | ALLOCATE( ztice_cvgerr(jpi,jpj,jpl) , ztice_cvgstp(jpi,jpj,jpl) ) |
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| 114 | ztice_cvgerr = 0._wp ; ztice_cvgstp = 0._wp |
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| 115 | ENDIF |
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[8586] | 116 | |
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| 117 | !---------------------------------------------! |
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| 118 | ! computation of friction velocity at T points |
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| 119 | !---------------------------------------------! |
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| 120 | IF( ln_icedyn ) THEN |
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| 121 | zu_io(:,:) = u_ice(:,:) - ssu_m(:,:) |
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| 122 | zv_io(:,:) = v_ice(:,:) - ssv_m(:,:) |
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| 123 | DO jj = 2, jpjm1 |
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| 124 | DO ji = fs_2, fs_jpim1 |
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| 125 | zfric(ji,jj) = rn_cio * ( 0.5_wp * & |
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| 126 | & ( zu_io(ji,jj) * zu_io(ji,jj) + zu_io(ji-1,jj) * zu_io(ji-1,jj) & |
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| 127 | & + zv_io(ji,jj) * zv_io(ji,jj) + zv_io(ji,jj-1) * zv_io(ji,jj-1) ) ) * tmask(ji,jj,1) |
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[13589] | 128 | zvel(ji,jj) = 0.5_wp * SQRT( ( u_ice(ji-1,jj) + u_ice(ji,jj) ) * ( u_ice(ji-1,jj) + u_ice(ji,jj) ) + & |
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| 129 | & ( v_ice(ji,jj-1) + v_ice(ji,jj) ) * ( v_ice(ji,jj-1) + v_ice(ji,jj) ) ) |
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[8586] | 130 | END DO |
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| 131 | END DO |
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[13589] | 132 | ELSE ! if no ice dynamics => transfer directly the atmospheric stress to the ocean |
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[8586] | 133 | DO jj = 2, jpjm1 |
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| 134 | DO ji = fs_2, fs_jpim1 |
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| 135 | zfric(ji,jj) = r1_rau0 * SQRT( 0.5_wp * & |
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| 136 | & ( utau(ji,jj) * utau(ji,jj) + utau(ji-1,jj) * utau(ji-1,jj) & |
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| 137 | & + vtau(ji,jj) * vtau(ji,jj) + vtau(ji,jj-1) * vtau(ji,jj-1) ) ) * tmask(ji,jj,1) |
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[13589] | 138 | zvel(ji,jj) = 0._wp |
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[8586] | 139 | END DO |
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| 140 | END DO |
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| 141 | ENDIF |
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[13589] | 142 | CALL lbc_lnk_multi( 'icethd', zfric, 'T', 1._wp, zvel, 'T', 1._wp ) |
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[8586] | 143 | ! |
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| 144 | !--------------------------------------------------------------------! |
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| 145 | ! Partial computation of forcing for the thermodynamic sea ice model |
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| 146 | !--------------------------------------------------------------------! |
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| 147 | DO jj = 1, jpj |
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| 148 | DO ji = 1, jpi |
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| 149 | rswitch = tmask(ji,jj,1) * MAX( 0._wp , SIGN( 1._wp , at_i(ji,jj) - epsi10 ) ) ! 0 if no ice |
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| 150 | ! |
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[9922] | 151 | ! --- Energy received in the lead from atm-oce exchanges, zqld is defined everywhere (J.m-2) --- ! |
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[8586] | 152 | zqld = tmask(ji,jj,1) * rdt_ice * & |
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| 153 | & ( ( 1._wp - at_i_b(ji,jj) ) * qsr_oce(ji,jj) * frq_m(ji,jj) + & |
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| 154 | & ( 1._wp - at_i_b(ji,jj) ) * qns_oce(ji,jj) + qemp_oce(ji,jj) ) |
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| 155 | |
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[13589] | 156 | ! --- Energy needed to bring ocean surface layer until its freezing, zqfr is defined everywhere (J.m-2) --- ! |
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| 157 | ! (mostly<0 but >0 if supercooling) |
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[9922] | 158 | zqfr = rau0 * rcp * e3t_m(ji,jj) * ( t_bo(ji,jj) - ( sst_m(ji,jj) + rt0 ) ) * tmask(ji,jj,1) ! both < 0 (t_bo < sst) and > 0 (t_bo > sst) |
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| 159 | zqfr_neg = MIN( zqfr , 0._wp ) ! only < 0 |
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[13589] | 160 | zqfr_pos = MAX( zqfr , 0._wp ) ! only > 0 |
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[8586] | 161 | |
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[13589] | 162 | ! --- Sensible ocean-to-ice heat flux (W/m2) --- ! |
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| 163 | ! (mostly>0 but <0 if supercooling) |
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[9922] | 164 | zfric_u = MAX( SQRT( zfric(ji,jj) ), zfric_umin ) |
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[13589] | 165 | qsb_ice_bot(ji,jj) = rswitch * rau0 * rcp * zch * zfric_u * ( ( sst_m(ji,jj) + rt0 ) - t_bo(ji,jj) ) |
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[8586] | 166 | |
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[9913] | 167 | ! upper bound for qsb_ice_bot: the heat retrieved from the ocean must be smaller than the heat necessary to reach |
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| 168 | ! the freezing point, so that we do not have SST < T_freeze |
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[13589] | 169 | ! This implies: qsb_ice_bot(ji,jj) * at_i(ji,jj) * rtdice <= - zqfr_neg |
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| 170 | ! The following formulation is ok for both normal conditions and supercooling |
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| 171 | qsb_ice_bot(ji,jj) = rswitch * MIN( qsb_ice_bot(ji,jj), - zqfr_neg * r1_rdtice / MAX( at_i(ji,jj), epsi10 ) ) |
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[8586] | 172 | |
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[14026] | 173 | ! If conditions are always supercooled (such as at the mouth of ice-shelves), then ice grows continuously |
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| 174 | ! ==> stop ice formation by artificially setting up the turbulent fluxes to 0 when volume > 20m (arbitrary) |
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| 175 | IF( ( t_bo(ji,jj) - ( sst_m(ji,jj) + rt0 ) ) > 0._wp .AND. vt_i(ji,jj) >= 20._wp ) THEN |
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| 176 | zqfr = 0._wp |
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| 177 | zqfr_pos = 0._wp |
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| 178 | qsb_ice_bot(ji,jj) = 0._wp |
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| 179 | ENDIF |
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| 180 | ! |
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[13589] | 181 | ! --- Energy Budget of the leads (qlead, J.m-2) --- ! |
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| 182 | ! qlead is the energy received from the atm. in the leads. |
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| 183 | ! If warming (zqld >= 0), then the energy in the leads is used to melt ice (bottom melting) => fhld (W/m2) |
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| 184 | ! If cooling (zqld < 0), then the energy in the leads is used to grow ice in open water => qlead (J.m-2) |
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[15813] | 185 | IF( ( zqld - zqfr ) < 0._wp .OR. at_i(ji,jj) < epsi10 ) THEN |
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| 186 | fhld (ji,jj) = 0._wp |
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| 187 | ! upper bound for qlead: qlead should be equal to zqld |
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| 188 | ! but before using this heat for ice formation, we suppose that the ocean cools down till the freezing point. |
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| 189 | ! The energy for this cooling down is zqfr and freezing point is reached if zqfr = zqld |
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| 190 | ! so the max heat that can be pulled out of the ocean is zqld - zqfr |
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| 191 | ! The following formulation is ok for both normal conditions and supercooling |
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| 192 | qlead(ji,jj) = MIN( 0._wp , zqld - zqfr ) |
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| 193 | ELSE |
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[13589] | 194 | ! upper bound for fhld: fhld should be equal to zqld |
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| 195 | ! but we have to make sure that this heat will not make the sst drop below the freezing point |
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[15813] | 196 | ! so the max heat that can be pulled out of the ocean is zqld - zqfr_pos |
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[13589] | 197 | ! The following formulation is ok for both normal conditions and supercooling |
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[15813] | 198 | fhld (ji,jj) = rswitch * MAX( 0._wp, ( zqld - zqfr_pos ) * r1_rdtice / MAX( at_i(ji,jj), epsi10 ) ) ! divided by at_i since this is (re)multiplied by a_i in icethd_dh.F90 |
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[8586] | 199 | qlead(ji,jj) = 0._wp |
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| 200 | ENDIF |
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| 201 | ! |
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[13589] | 202 | ! If ice is landfast and ice concentration reaches its max |
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| 203 | ! => stop ice formation in open water |
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| 204 | IF( zvel(ji,jj) <= 5.e-04_wp .AND. at_i(ji,jj) >= rn_amax_2d(ji,jj)-epsi06 ) qlead(ji,jj) = 0._wp |
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| 205 | ! |
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| 206 | ! If the grid cell is almost fully covered by ice (no leads) |
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| 207 | ! => stop ice formation in open water |
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| 208 | IF( at_i(ji,jj) >= (1._wp - epsi10) ) qlead(ji,jj) = 0._wp |
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| 209 | ! |
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| 210 | ! If ln_leadhfx is false |
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| 211 | ! => do not use energy of the leads to melt sea-ice |
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| 212 | IF( .NOT.ln_leadhfx ) fhld(ji,jj) = 0._wp |
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| 213 | ! |
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[8586] | 214 | END DO |
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| 215 | END DO |
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| 216 | |
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| 217 | ! In case we bypass open-water ice formation |
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| 218 | IF( .NOT. ln_icedO ) qlead(:,:) = 0._wp |
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[10932] | 219 | ! In case we bypass growing/melting from top and bottom |
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[8586] | 220 | IF( .NOT. ln_icedH ) THEN |
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[9913] | 221 | qsb_ice_bot(:,:) = 0._wp |
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| 222 | fhld (:,:) = 0._wp |
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[8586] | 223 | ENDIF |
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| 224 | |
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| 225 | !-------------------------------------------------------------------------------------------! |
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| 226 | ! Thermodynamic computation (only on grid points covered by ice) => loop over ice categories |
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| 227 | !-------------------------------------------------------------------------------------------! |
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| 228 | DO jl = 1, jpl |
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| 229 | |
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| 230 | ! select ice covered grid points |
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| 231 | npti = 0 ; nptidx(:) = 0 |
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| 232 | DO jj = 1, jpj |
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| 233 | DO ji = 1, jpi |
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| 234 | IF ( a_i(ji,jj,jl) > epsi10 ) THEN |
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| 235 | npti = npti + 1 |
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| 236 | nptidx(npti) = (jj - 1) * jpi + ji |
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| 237 | ENDIF |
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| 238 | END DO |
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| 239 | END DO |
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| 240 | |
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| 241 | IF( npti > 0 ) THEN ! If there is no ice, do nothing. |
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| 242 | ! |
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| 243 | CALL ice_thd_1d2d( jl, 1 ) ! --- Move to 1D arrays --- ! |
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| 244 | ! ! --- & Change units of e_i, e_s from J/m2 to J/m3 --- ! |
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| 245 | ! |
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[13284] | 246 | s_i_new (1:npti) = 0._wp ; dh_s_tot(1:npti) = 0._wp ! --- some init --- ! (important to have them here) |
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[9750] | 247 | dh_i_sum (1:npti) = 0._wp ; dh_i_bom(1:npti) = 0._wp ; dh_i_itm (1:npti) = 0._wp |
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| 248 | dh_i_sub (1:npti) = 0._wp ; dh_i_bog(1:npti) = 0._wp |
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| 249 | dh_snowice(1:npti) = 0._wp ; dh_s_mlt(1:npti) = 0._wp |
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[10932] | 250 | ! |
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| 251 | CALL ice_thd_zdf ! --- Ice-Snow temperature --- ! |
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[8586] | 252 | ! |
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[10932] | 253 | IF( ln_icedH ) THEN ! --- Growing/Melting --- ! |
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| 254 | CALL ice_thd_dh ! Ice-Snow thickness |
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| 255 | CALL ice_thd_ent( e_i_1d(1:npti,:) ) ! Ice enthalpy remapping |
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[8586] | 256 | ENDIF |
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| 257 | CALL ice_thd_sal( ln_icedS ) ! --- Ice salinity --- ! |
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| 258 | ! |
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[10932] | 259 | CALL ice_thd_temp ! --- Temperature update --- ! |
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[8586] | 260 | ! |
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[10531] | 261 | IF( ln_icedH .AND. ln_virtual_itd ) & |
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[10932] | 262 | & CALL ice_thd_mono ! --- Extra lateral melting if virtual_itd --- ! |
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[8586] | 263 | ! |
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[10932] | 264 | IF( ln_icedA ) CALL ice_thd_da ! --- Lateral melting --- ! |
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[8586] | 265 | ! |
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[14026] | 266 | IF( ln_pnd .AND. ln_icedH ) & |
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| 267 | & CALL ice_thd_pnd ! --- Melt ponds formation --- ! |
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| 268 | ! |
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[8586] | 269 | CALL ice_thd_1d2d( jl, 2 ) ! --- Change units of e_i, e_s from J/m3 to J/m2 --- ! |
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| 270 | ! ! --- & Move to 2D arrays --- ! |
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| 271 | ENDIF |
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| 272 | ! |
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| 273 | END DO |
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[10994] | 274 | ! |
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[8586] | 275 | IF( ln_icediachk ) CALL ice_cons_hsm(1, 'icethd', rdiag_v, rdiag_s, rdiag_t, rdiag_fv, rdiag_fs, rdiag_ft) |
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[11536] | 276 | IF( ln_icediachk ) CALL ice_cons2D (1, 'icethd', diag_v, diag_s, diag_t, diag_fv, diag_fs, diag_ft) |
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[8586] | 277 | ! |
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[10932] | 278 | IF( jpl > 1 ) CALL ice_itd_rem( kt ) ! --- Transport ice between thickness categories --- ! |
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[8586] | 279 | ! |
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[10932] | 280 | IF( ln_icedO ) CALL ice_thd_do ! --- Frazil ice growth in leads --- ! |
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[8586] | 281 | ! |
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[13640] | 282 | CALL ice_cor( kt , 2 ) ! --- Corrections --- ! |
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| 283 | ! |
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| 284 | oa_i(:,:,:) = oa_i(:,:,:) + a_i(:,:,:) * rdt_ice ! ice natural aging incrementation |
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| 285 | ! |
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[13284] | 286 | ! convergence tests |
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| 287 | IF( ln_zdf_chkcvg ) THEN |
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| 288 | CALL iom_put( 'tice_cvgerr', ztice_cvgerr ) ; DEALLOCATE( ztice_cvgerr ) |
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| 289 | CALL iom_put( 'tice_cvgstp', ztice_cvgstp ) ; DEALLOCATE( ztice_cvgstp ) |
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| 290 | ENDIF |
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| 291 | ! |
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[8586] | 292 | ! controls |
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[9124] | 293 | IF( ln_icectl ) CALL ice_prt (kt, iiceprt, jiceprt, 1, ' - ice thermodyn. - ') ! prints |
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| 294 | IF( ln_ctl ) CALL ice_prt3D ('icethd') ! prints |
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| 295 | IF( ln_timing ) CALL timing_stop('icethd') ! timing |
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[8586] | 296 | ! |
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| 297 | END SUBROUTINE ice_thd |
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| 298 | |
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| 299 | |
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| 300 | SUBROUTINE ice_thd_temp |
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| 301 | !!----------------------------------------------------------------------- |
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| 302 | !! *** ROUTINE ice_thd_temp *** |
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| 303 | !! |
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| 304 | !! ** Purpose : Computes sea ice temperature (Kelvin) from enthalpy |
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| 305 | !! |
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| 306 | !! ** Method : Formula (Bitz and Lipscomb, 1999) |
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| 307 | !!------------------------------------------------------------------- |
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| 308 | INTEGER :: ji, jk ! dummy loop indices |
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| 309 | REAL(wp) :: ztmelts, zbbb, zccc ! local scalar |
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| 310 | !!------------------------------------------------------------------- |
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| 311 | ! Recover ice temperature |
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| 312 | DO jk = 1, nlay_i |
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| 313 | DO ji = 1, npti |
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[9935] | 314 | ztmelts = -rTmlt * sz_i_1d(ji,jk) |
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[8586] | 315 | ! Conversion q(S,T) -> T (second order equation) |
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[9935] | 316 | zbbb = ( rcp - rcpi ) * ztmelts + e_i_1d(ji,jk) * r1_rhoi - rLfus |
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| 317 | zccc = SQRT( MAX( zbbb * zbbb - 4._wp * rcpi * rLfus * ztmelts, 0._wp ) ) |
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| 318 | t_i_1d(ji,jk) = rt0 - ( zbbb + zccc ) * 0.5_wp * r1_rcpi |
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[8586] | 319 | |
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| 320 | ! mask temperature |
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| 321 | rswitch = 1._wp - MAX( 0._wp , SIGN( 1._wp , - h_i_1d(ji) ) ) |
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| 322 | t_i_1d(ji,jk) = rswitch * t_i_1d(ji,jk) + ( 1._wp - rswitch ) * rt0 |
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| 323 | END DO |
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| 324 | END DO |
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| 325 | ! |
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| 326 | END SUBROUTINE ice_thd_temp |
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| 327 | |
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| 328 | |
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[9750] | 329 | SUBROUTINE ice_thd_mono |
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[8586] | 330 | !!----------------------------------------------------------------------- |
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[9750] | 331 | !! *** ROUTINE ice_thd_mono *** |
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[8586] | 332 | !! |
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[9076] | 333 | !! ** Purpose : Lateral melting in case virtual_itd |
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[8586] | 334 | !! ( dA = A/2h dh ) |
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| 335 | !!----------------------------------------------------------------------- |
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| 336 | INTEGER :: ji ! dummy loop indices |
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| 337 | REAL(wp) :: zhi_bef ! ice thickness before thermo |
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| 338 | REAL(wp) :: zdh_mel, zda_mel ! net melting |
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| 339 | REAL(wp) :: zvi, zvs ! ice/snow volumes |
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| 340 | !!----------------------------------------------------------------------- |
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| 341 | ! |
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| 342 | DO ji = 1, npti |
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[9750] | 343 | zdh_mel = MIN( 0._wp, dh_i_itm(ji) + dh_i_sum(ji) + dh_i_bom(ji) + dh_snowice(ji) + dh_i_sub(ji) ) |
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[8586] | 344 | IF( zdh_mel < 0._wp .AND. a_i_1d(ji) > 0._wp ) THEN |
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| 345 | zvi = a_i_1d(ji) * h_i_1d(ji) |
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| 346 | zvs = a_i_1d(ji) * h_s_1d(ji) |
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| 347 | ! lateral melting = concentration change |
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| 348 | zhi_bef = h_i_1d(ji) - zdh_mel |
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| 349 | rswitch = MAX( 0._wp , SIGN( 1._wp , zhi_bef - epsi20 ) ) |
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| 350 | zda_mel = rswitch * a_i_1d(ji) * zdh_mel / ( 2._wp * MAX( zhi_bef, epsi20 ) ) |
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| 351 | a_i_1d(ji) = MAX( epsi20, a_i_1d(ji) + zda_mel ) |
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| 352 | ! adjust thickness |
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| 353 | h_i_1d(ji) = zvi / a_i_1d(ji) |
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| 354 | h_s_1d(ji) = zvs / a_i_1d(ji) |
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| 355 | ! retrieve total concentration |
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| 356 | at_i_1d(ji) = a_i_1d(ji) |
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| 357 | END IF |
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| 358 | END DO |
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| 359 | ! |
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[9750] | 360 | END SUBROUTINE ice_thd_mono |
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[8586] | 361 | |
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| 362 | |
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| 363 | SUBROUTINE ice_thd_1d2d( kl, kn ) |
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| 364 | !!----------------------------------------------------------------------- |
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| 365 | !! *** ROUTINE ice_thd_1d2d *** |
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| 366 | !! |
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| 367 | !! ** Purpose : move arrays from 1d to 2d and the reverse |
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| 368 | !!----------------------------------------------------------------------- |
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| 369 | INTEGER, INTENT(in) :: kl ! index of the ice category |
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| 370 | INTEGER, INTENT(in) :: kn ! 1= from 2D to 1D ; 2= from 1D to 2D |
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| 371 | ! |
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| 372 | INTEGER :: jk ! dummy loop indices |
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| 373 | !!----------------------------------------------------------------------- |
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| 374 | ! |
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| 375 | SELECT CASE( kn ) |
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| 376 | ! !---------------------! |
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| 377 | CASE( 1 ) !== from 2D to 1D ==! |
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| 378 | ! !---------------------! |
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| 379 | CALL tab_2d_1d( npti, nptidx(1:npti), at_i_1d(1:npti), at_i ) |
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| 380 | CALL tab_2d_1d( npti, nptidx(1:npti), a_i_1d (1:npti), a_i (:,:,kl) ) |
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[8637] | 381 | CALL tab_2d_1d( npti, nptidx(1:npti), h_i_1d (1:npti), h_i (:,:,kl) ) |
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| 382 | CALL tab_2d_1d( npti, nptidx(1:npti), h_s_1d (1:npti), h_s (:,:,kl) ) |
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[8586] | 383 | CALL tab_2d_1d( npti, nptidx(1:npti), t_su_1d(1:npti), t_su(:,:,kl) ) |
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[8637] | 384 | CALL tab_2d_1d( npti, nptidx(1:npti), s_i_1d (1:npti), s_i (:,:,kl) ) |
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[8586] | 385 | DO jk = 1, nlay_s |
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[8637] | 386 | CALL tab_2d_1d( npti, nptidx(1:npti), t_s_1d(1:npti,jk), t_s(:,:,jk,kl) ) |
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| 387 | CALL tab_2d_1d( npti, nptidx(1:npti), e_s_1d(1:npti,jk), e_s(:,:,jk,kl) ) |
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[8586] | 388 | END DO |
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| 389 | DO jk = 1, nlay_i |
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[8637] | 390 | CALL tab_2d_1d( npti, nptidx(1:npti), t_i_1d (1:npti,jk), t_i (:,:,jk,kl) ) |
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| 391 | CALL tab_2d_1d( npti, nptidx(1:npti), e_i_1d (1:npti,jk), e_i (:,:,jk,kl) ) |
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| 392 | CALL tab_2d_1d( npti, nptidx(1:npti), sz_i_1d(1:npti,jk), sz_i(:,:,jk,kl) ) |
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[8586] | 393 | END DO |
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[8637] | 394 | CALL tab_2d_1d( npti, nptidx(1:npti), a_ip_1d (1:npti), a_ip (:,:,kl) ) |
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| 395 | CALL tab_2d_1d( npti, nptidx(1:npti), h_ip_1d (1:npti), h_ip (:,:,kl) ) |
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[13284] | 396 | CALL tab_2d_1d( npti, nptidx(1:npti), h_il_1d (1:npti), h_il (:,:,kl) ) |
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[8586] | 397 | ! |
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[9910] | 398 | CALL tab_2d_1d( npti, nptidx(1:npti), qprec_ice_1d (1:npti), qprec_ice ) |
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| 399 | CALL tab_2d_1d( npti, nptidx(1:npti), qsr_ice_1d (1:npti), qsr_ice (:,:,kl) ) |
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| 400 | CALL tab_2d_1d( npti, nptidx(1:npti), qns_ice_1d (1:npti), qns_ice (:,:,kl) ) |
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| 401 | CALL tab_2d_1d( npti, nptidx(1:npti), evap_ice_1d (1:npti), evap_ice(:,:,kl) ) |
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| 402 | CALL tab_2d_1d( npti, nptidx(1:npti), dqns_ice_1d (1:npti), dqns_ice(:,:,kl) ) |
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| 403 | CALL tab_2d_1d( npti, nptidx(1:npti), t_bo_1d (1:npti), t_bo ) |
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| 404 | CALL tab_2d_1d( npti, nptidx(1:npti), sprecip_1d (1:npti), sprecip ) |
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[9913] | 405 | CALL tab_2d_1d( npti, nptidx(1:npti), qsb_ice_bot_1d(1:npti), qsb_ice_bot ) |
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[9910] | 406 | CALL tab_2d_1d( npti, nptidx(1:npti), fhld_1d (1:npti), fhld ) |
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[8813] | 407 | |
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[9910] | 408 | CALL tab_2d_1d( npti, nptidx(1:npti), qml_ice_1d (1:npti), qml_ice (:,:,kl) ) |
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| 409 | CALL tab_2d_1d( npti, nptidx(1:npti), qcn_ice_1d (1:npti), qcn_ice (:,:,kl) ) |
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| 410 | CALL tab_2d_1d( npti, nptidx(1:npti), qtr_ice_top_1d(1:npti), qtr_ice_top(:,:,kl) ) |
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[8586] | 411 | ! |
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| 412 | CALL tab_2d_1d( npti, nptidx(1:npti), wfx_snw_sni_1d(1:npti), wfx_snw_sni ) |
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| 413 | CALL tab_2d_1d( npti, nptidx(1:npti), wfx_snw_sum_1d(1:npti), wfx_snw_sum ) |
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| 414 | CALL tab_2d_1d( npti, nptidx(1:npti), wfx_sub_1d (1:npti), wfx_sub ) |
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| 415 | CALL tab_2d_1d( npti, nptidx(1:npti), wfx_snw_sub_1d(1:npti), wfx_snw_sub ) |
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| 416 | CALL tab_2d_1d( npti, nptidx(1:npti), wfx_ice_sub_1d(1:npti), wfx_ice_sub ) |
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| 417 | CALL tab_2d_1d( npti, nptidx(1:npti), wfx_err_sub_1d(1:npti), wfx_err_sub ) |
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| 418 | ! |
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| 419 | CALL tab_2d_1d( npti, nptidx(1:npti), wfx_bog_1d (1:npti), wfx_bog ) |
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| 420 | CALL tab_2d_1d( npti, nptidx(1:npti), wfx_bom_1d (1:npti), wfx_bom ) |
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| 421 | CALL tab_2d_1d( npti, nptidx(1:npti), wfx_sum_1d (1:npti), wfx_sum ) |
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| 422 | CALL tab_2d_1d( npti, nptidx(1:npti), wfx_sni_1d (1:npti), wfx_sni ) |
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| 423 | CALL tab_2d_1d( npti, nptidx(1:npti), wfx_res_1d (1:npti), wfx_res ) |
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| 424 | CALL tab_2d_1d( npti, nptidx(1:npti), wfx_spr_1d (1:npti), wfx_spr ) |
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| 425 | CALL tab_2d_1d( npti, nptidx(1:npti), wfx_lam_1d (1:npti), wfx_lam ) |
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[8637] | 426 | CALL tab_2d_1d( npti, nptidx(1:npti), wfx_pnd_1d (1:npti), wfx_pnd ) |
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[8586] | 427 | ! |
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| 428 | CALL tab_2d_1d( npti, nptidx(1:npti), sfx_bog_1d (1:npti), sfx_bog ) |
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| 429 | CALL tab_2d_1d( npti, nptidx(1:npti), sfx_bom_1d (1:npti), sfx_bom ) |
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| 430 | CALL tab_2d_1d( npti, nptidx(1:npti), sfx_sum_1d (1:npti), sfx_sum ) |
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| 431 | CALL tab_2d_1d( npti, nptidx(1:npti), sfx_sni_1d (1:npti), sfx_sni ) |
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| 432 | CALL tab_2d_1d( npti, nptidx(1:npti), sfx_bri_1d (1:npti), sfx_bri ) |
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| 433 | CALL tab_2d_1d( npti, nptidx(1:npti), sfx_res_1d (1:npti), sfx_res ) |
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| 434 | CALL tab_2d_1d( npti, nptidx(1:npti), sfx_sub_1d (1:npti), sfx_sub ) |
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| 435 | CALL tab_2d_1d( npti, nptidx(1:npti), sfx_lam_1d (1:npti), sfx_lam ) |
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| 436 | ! |
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[9910] | 437 | CALL tab_2d_1d( npti, nptidx(1:npti), hfx_thd_1d (1:npti), hfx_thd ) |
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| 438 | CALL tab_2d_1d( npti, nptidx(1:npti), hfx_spr_1d (1:npti), hfx_spr ) |
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| 439 | CALL tab_2d_1d( npti, nptidx(1:npti), hfx_sum_1d (1:npti), hfx_sum ) |
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| 440 | CALL tab_2d_1d( npti, nptidx(1:npti), hfx_bom_1d (1:npti), hfx_bom ) |
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| 441 | CALL tab_2d_1d( npti, nptidx(1:npti), hfx_bog_1d (1:npti), hfx_bog ) |
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| 442 | CALL tab_2d_1d( npti, nptidx(1:npti), hfx_dif_1d (1:npti), hfx_dif ) |
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| 443 | CALL tab_2d_1d( npti, nptidx(1:npti), hfx_opw_1d (1:npti), hfx_opw ) |
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| 444 | CALL tab_2d_1d( npti, nptidx(1:npti), hfx_snw_1d (1:npti), hfx_snw ) |
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| 445 | CALL tab_2d_1d( npti, nptidx(1:npti), hfx_sub_1d (1:npti), hfx_sub ) |
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| 446 | CALL tab_2d_1d( npti, nptidx(1:npti), hfx_res_1d (1:npti), hfx_res ) |
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[8586] | 447 | CALL tab_2d_1d( npti, nptidx(1:npti), hfx_err_dif_1d(1:npti), hfx_err_dif ) |
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| 448 | ! |
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| 449 | ! ocean surface fields |
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| 450 | CALL tab_2d_1d( npti, nptidx(1:npti), sst_1d(1:npti), sst_m ) |
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| 451 | CALL tab_2d_1d( npti, nptidx(1:npti), sss_1d(1:npti), sss_m ) |
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[13642] | 452 | CALL tab_2d_1d( npti, nptidx(1:npti), frq_m_1d(1:npti), frq_m ) |
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[10786] | 453 | ! |
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| 454 | ! to update ice age |
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| 455 | CALL tab_2d_1d( npti, nptidx(1:npti), o_i_1d (1:npti), o_i (:,:,kl) ) |
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| 456 | CALL tab_2d_1d( npti, nptidx(1:npti), oa_i_1d(1:npti), oa_i(:,:,kl) ) |
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| 457 | ! |
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[8586] | 458 | ! --- Change units of e_i, e_s from J/m2 to J/m3 --- ! |
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| 459 | DO jk = 1, nlay_i |
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| 460 | WHERE( h_i_1d(1:npti)>0._wp ) e_i_1d(1:npti,jk) = e_i_1d(1:npti,jk) / (h_i_1d(1:npti) * a_i_1d(1:npti)) * nlay_i |
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| 461 | END DO |
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| 462 | DO jk = 1, nlay_s |
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| 463 | WHERE( h_s_1d(1:npti)>0._wp ) e_s_1d(1:npti,jk) = e_s_1d(1:npti,jk) / (h_s_1d(1:npti) * a_i_1d(1:npti)) * nlay_s |
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| 464 | END DO |
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| 465 | ! |
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| 466 | ! !---------------------! |
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| 467 | CASE( 2 ) !== from 1D to 2D ==! |
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| 468 | ! !---------------------! |
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| 469 | ! --- Change units of e_i, e_s from J/m3 to J/m2 --- ! |
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| 470 | DO jk = 1, nlay_i |
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| 471 | e_i_1d(1:npti,jk) = e_i_1d(1:npti,jk) * h_i_1d(1:npti) * a_i_1d(1:npti) * r1_nlay_i |
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| 472 | END DO |
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| 473 | DO jk = 1, nlay_s |
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| 474 | e_s_1d(1:npti,jk) = e_s_1d(1:npti,jk) * h_s_1d(1:npti) * a_i_1d(1:npti) * r1_nlay_s |
---|
| 475 | END DO |
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| 476 | ! |
---|
| 477 | ! Change thickness to volume (replaces routine ice_var_eqv2glo) |
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[8637] | 478 | v_i_1d (1:npti) = h_i_1d (1:npti) * a_i_1d (1:npti) |
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| 479 | v_s_1d (1:npti) = h_s_1d (1:npti) * a_i_1d (1:npti) |
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| 480 | sv_i_1d(1:npti) = s_i_1d (1:npti) * v_i_1d (1:npti) |
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| 481 | v_ip_1d(1:npti) = h_ip_1d(1:npti) * a_ip_1d(1:npti) |
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[13284] | 482 | v_il_1d(1:npti) = h_il_1d(1:npti) * a_ip_1d(1:npti) |
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[10786] | 483 | oa_i_1d(1:npti) = o_i_1d (1:npti) * a_i_1d (1:npti) |
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[8586] | 484 | |
---|
| 485 | CALL tab_1d_2d( npti, nptidx(1:npti), at_i_1d(1:npti), at_i ) |
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| 486 | CALL tab_1d_2d( npti, nptidx(1:npti), a_i_1d (1:npti), a_i (:,:,kl) ) |
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[8637] | 487 | CALL tab_1d_2d( npti, nptidx(1:npti), h_i_1d (1:npti), h_i (:,:,kl) ) |
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| 488 | CALL tab_1d_2d( npti, nptidx(1:npti), h_s_1d (1:npti), h_s (:,:,kl) ) |
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[8586] | 489 | CALL tab_1d_2d( npti, nptidx(1:npti), t_su_1d(1:npti), t_su(:,:,kl) ) |
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[8637] | 490 | CALL tab_1d_2d( npti, nptidx(1:npti), s_i_1d (1:npti), s_i (:,:,kl) ) |
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[8586] | 491 | DO jk = 1, nlay_s |
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[8637] | 492 | CALL tab_1d_2d( npti, nptidx(1:npti), t_s_1d(1:npti,jk), t_s(:,:,jk,kl) ) |
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| 493 | CALL tab_1d_2d( npti, nptidx(1:npti), e_s_1d(1:npti,jk), e_s(:,:,jk,kl) ) |
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[8586] | 494 | END DO |
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| 495 | DO jk = 1, nlay_i |
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[8637] | 496 | CALL tab_1d_2d( npti, nptidx(1:npti), t_i_1d (1:npti,jk), t_i (:,:,jk,kl) ) |
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| 497 | CALL tab_1d_2d( npti, nptidx(1:npti), e_i_1d (1:npti,jk), e_i (:,:,jk,kl) ) |
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| 498 | CALL tab_1d_2d( npti, nptidx(1:npti), sz_i_1d(1:npti,jk), sz_i(:,:,jk,kl) ) |
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[8586] | 499 | END DO |
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[8637] | 500 | CALL tab_1d_2d( npti, nptidx(1:npti), a_ip_1d (1:npti), a_ip (:,:,kl) ) |
---|
| 501 | CALL tab_1d_2d( npti, nptidx(1:npti), h_ip_1d (1:npti), h_ip (:,:,kl) ) |
---|
[13284] | 502 | CALL tab_1d_2d( npti, nptidx(1:npti), h_il_1d (1:npti), h_il (:,:,kl) ) |
---|
[8586] | 503 | ! |
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| 504 | CALL tab_1d_2d( npti, nptidx(1:npti), wfx_snw_sni_1d(1:npti), wfx_snw_sni ) |
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| 505 | CALL tab_1d_2d( npti, nptidx(1:npti), wfx_snw_sum_1d(1:npti), wfx_snw_sum ) |
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| 506 | CALL tab_1d_2d( npti, nptidx(1:npti), wfx_sub_1d (1:npti), wfx_sub ) |
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| 507 | CALL tab_1d_2d( npti, nptidx(1:npti), wfx_snw_sub_1d(1:npti), wfx_snw_sub ) |
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| 508 | CALL tab_1d_2d( npti, nptidx(1:npti), wfx_ice_sub_1d(1:npti), wfx_ice_sub ) |
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| 509 | CALL tab_1d_2d( npti, nptidx(1:npti), wfx_err_sub_1d(1:npti), wfx_err_sub ) |
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| 510 | ! |
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| 511 | CALL tab_1d_2d( npti, nptidx(1:npti), wfx_bog_1d (1:npti), wfx_bog ) |
---|
| 512 | CALL tab_1d_2d( npti, nptidx(1:npti), wfx_bom_1d (1:npti), wfx_bom ) |
---|
| 513 | CALL tab_1d_2d( npti, nptidx(1:npti), wfx_sum_1d (1:npti), wfx_sum ) |
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| 514 | CALL tab_1d_2d( npti, nptidx(1:npti), wfx_sni_1d (1:npti), wfx_sni ) |
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| 515 | CALL tab_1d_2d( npti, nptidx(1:npti), wfx_res_1d (1:npti), wfx_res ) |
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| 516 | CALL tab_1d_2d( npti, nptidx(1:npti), wfx_spr_1d (1:npti), wfx_spr ) |
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| 517 | CALL tab_1d_2d( npti, nptidx(1:npti), wfx_lam_1d (1:npti), wfx_lam ) |
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[8813] | 518 | CALL tab_1d_2d( npti, nptidx(1:npti), wfx_pnd_1d (1:npti), wfx_pnd ) |
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[8586] | 519 | ! |
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| 520 | CALL tab_1d_2d( npti, nptidx(1:npti), sfx_bog_1d (1:npti), sfx_bog ) |
---|
| 521 | CALL tab_1d_2d( npti, nptidx(1:npti), sfx_bom_1d (1:npti), sfx_bom ) |
---|
| 522 | CALL tab_1d_2d( npti, nptidx(1:npti), sfx_sum_1d (1:npti), sfx_sum ) |
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| 523 | CALL tab_1d_2d( npti, nptidx(1:npti), sfx_sni_1d (1:npti), sfx_sni ) |
---|
| 524 | CALL tab_1d_2d( npti, nptidx(1:npti), sfx_bri_1d (1:npti), sfx_bri ) |
---|
| 525 | CALL tab_1d_2d( npti, nptidx(1:npti), sfx_res_1d (1:npti), sfx_res ) |
---|
| 526 | CALL tab_1d_2d( npti, nptidx(1:npti), sfx_sub_1d (1:npti), sfx_sub ) |
---|
| 527 | CALL tab_1d_2d( npti, nptidx(1:npti), sfx_lam_1d (1:npti), sfx_lam ) |
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| 528 | ! |
---|
[9912] | 529 | CALL tab_1d_2d( npti, nptidx(1:npti), hfx_thd_1d (1:npti), hfx_thd ) |
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| 530 | CALL tab_1d_2d( npti, nptidx(1:npti), hfx_spr_1d (1:npti), hfx_spr ) |
---|
| 531 | CALL tab_1d_2d( npti, nptidx(1:npti), hfx_sum_1d (1:npti), hfx_sum ) |
---|
| 532 | CALL tab_1d_2d( npti, nptidx(1:npti), hfx_bom_1d (1:npti), hfx_bom ) |
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| 533 | CALL tab_1d_2d( npti, nptidx(1:npti), hfx_bog_1d (1:npti), hfx_bog ) |
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| 534 | CALL tab_1d_2d( npti, nptidx(1:npti), hfx_dif_1d (1:npti), hfx_dif ) |
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| 535 | CALL tab_1d_2d( npti, nptidx(1:npti), hfx_opw_1d (1:npti), hfx_opw ) |
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| 536 | CALL tab_1d_2d( npti, nptidx(1:npti), hfx_snw_1d (1:npti), hfx_snw ) |
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| 537 | CALL tab_1d_2d( npti, nptidx(1:npti), hfx_sub_1d (1:npti), hfx_sub ) |
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| 538 | CALL tab_1d_2d( npti, nptidx(1:npti), hfx_res_1d (1:npti), hfx_res ) |
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[8586] | 539 | CALL tab_1d_2d( npti, nptidx(1:npti), hfx_err_dif_1d(1:npti), hfx_err_dif ) |
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| 540 | ! |
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[9910] | 541 | CALL tab_1d_2d( npti, nptidx(1:npti), qns_ice_1d (1:npti), qns_ice (:,:,kl) ) |
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| 542 | CALL tab_1d_2d( npti, nptidx(1:npti), qtr_ice_bot_1d(1:npti), qtr_ice_bot(:,:,kl) ) |
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[10534] | 543 | ! effective conductivity and 1st layer temperature (ln_cndflx=T) |
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[8933] | 544 | CALL tab_1d_2d( npti, nptidx(1:npti), cnd_ice_1d(1:npti), cnd_ice(:,:,kl) ) |
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| 545 | CALL tab_1d_2d( npti, nptidx(1:npti), t1_ice_1d (1:npti), t1_ice (:,:,kl) ) |
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[8586] | 546 | ! SIMIP diagnostics |
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[9916] | 547 | CALL tab_1d_2d( npti, nptidx(1:npti), t_si_1d (1:npti), t_si (:,:,kl) ) |
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| 548 | CALL tab_1d_2d( npti, nptidx(1:npti), qcn_ice_bot_1d(1:npti), qcn_ice_bot(:,:,kl) ) |
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| 549 | CALL tab_1d_2d( npti, nptidx(1:npti), qcn_ice_top_1d(1:npti), qcn_ice_top(:,:,kl) ) |
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[14885] | 550 | CALL tab_1d_2d( npti, nptidx(1:npti), qml_ice_1d (1:npti), qml_ice (:,:,kl) ) |
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[8586] | 551 | ! extensive variables |
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| 552 | CALL tab_1d_2d( npti, nptidx(1:npti), v_i_1d (1:npti), v_i (:,:,kl) ) |
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| 553 | CALL tab_1d_2d( npti, nptidx(1:npti), v_s_1d (1:npti), v_s (:,:,kl) ) |
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| 554 | CALL tab_1d_2d( npti, nptidx(1:npti), sv_i_1d(1:npti), sv_i(:,:,kl) ) |
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[8637] | 555 | CALL tab_1d_2d( npti, nptidx(1:npti), v_ip_1d(1:npti), v_ip(:,:,kl) ) |
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[13284] | 556 | CALL tab_1d_2d( npti, nptidx(1:npti), v_il_1d(1:npti), v_il(:,:,kl) ) |
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[10786] | 557 | CALL tab_1d_2d( npti, nptidx(1:npti), oa_i_1d(1:npti), oa_i(:,:,kl) ) |
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[13284] | 558 | ! check convergence of heat diffusion scheme |
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| 559 | IF( ln_zdf_chkcvg ) THEN |
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| 560 | CALL tab_1d_2d( npti, nptidx(1:npti), tice_cvgerr_1d(1:npti), ztice_cvgerr(:,:,kl) ) |
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| 561 | CALL tab_1d_2d( npti, nptidx(1:npti), tice_cvgstp_1d(1:npti), ztice_cvgstp(:,:,kl) ) |
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| 562 | ENDIF |
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[8586] | 563 | ! |
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| 564 | END SELECT |
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| 565 | ! |
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| 566 | END SUBROUTINE ice_thd_1d2d |
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| 567 | |
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| 568 | |
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| 569 | SUBROUTINE ice_thd_init |
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[8637] | 570 | !!------------------------------------------------------------------- |
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[8586] | 571 | !! *** ROUTINE ice_thd_init *** |
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| 572 | !! |
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| 573 | !! ** Purpose : Physical constants and parameters associated with |
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| 574 | !! ice thermodynamics |
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| 575 | !! |
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| 576 | !! ** Method : Read the namthd namelist and check the parameters |
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| 577 | !! called at the first timestep (nit000) |
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| 578 | !! |
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| 579 | !! ** input : Namelist namthd |
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| 580 | !!------------------------------------------------------------------- |
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| 581 | INTEGER :: ios ! Local integer output status for namelist read |
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| 582 | !! |
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[13284] | 583 | NAMELIST/namthd/ ln_icedH, ln_icedA, ln_icedO, ln_icedS, ln_leadhfx |
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[8586] | 584 | !!------------------------------------------------------------------- |
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| 585 | ! |
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| 586 | REWIND( numnam_ice_ref ) ! Namelist namthd in reference namelist : Ice thermodynamics |
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| 587 | READ ( numnam_ice_ref, namthd, IOSTAT = ios, ERR = 901) |
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[11536] | 588 | 901 IF( ios /= 0 ) CALL ctl_nam ( ios , 'namthd in reference namelist' ) |
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[8586] | 589 | REWIND( numnam_ice_cfg ) ! Namelist namthd in configuration namelist : Ice thermodynamics |
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| 590 | READ ( numnam_ice_cfg, namthd, IOSTAT = ios, ERR = 902 ) |
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[11536] | 591 | 902 IF( ios > 0 ) CALL ctl_nam ( ios , 'namthd in configuration namelist' ) |
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[9169] | 592 | IF(lwm) WRITE( numoni, namthd ) |
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[8586] | 593 | ! |
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| 594 | IF(lwp) THEN ! control print |
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[9169] | 595 | WRITE(numout,*) |
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[8586] | 596 | WRITE(numout,*) 'ice_thd_init: Ice Thermodynamics' |
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| 597 | WRITE(numout,*) '~~~~~~~~~~~~' |
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| 598 | WRITE(numout,*) ' Namelist namthd:' |
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[13284] | 599 | WRITE(numout,*) ' activate ice thick change from top/bot (T) or not (F) ln_icedH = ', ln_icedH |
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| 600 | WRITE(numout,*) ' activate lateral melting (T) or not (F) ln_icedA = ', ln_icedA |
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| 601 | WRITE(numout,*) ' activate ice growth in open-water (T) or not (F) ln_icedO = ', ln_icedO |
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| 602 | WRITE(numout,*) ' activate gravity drainage and flushing (T) or not (F) ln_icedS = ', ln_icedS |
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| 603 | WRITE(numout,*) ' heat in the leads is used to melt sea-ice before warming the ocean ln_leadhfx = ', ln_leadhfx |
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[8586] | 604 | ENDIF |
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| 605 | ! |
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| 606 | CALL ice_thd_zdf_init ! set ice heat diffusion parameters |
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| 607 | IF( ln_icedA ) CALL ice_thd_da_init ! set ice lateral melting parameters |
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| 608 | IF( ln_icedO ) CALL ice_thd_do_init ! set ice growth in open water parameters |
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| 609 | CALL ice_thd_sal_init ! set ice salinity parameters |
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[8637] | 610 | CALL ice_thd_pnd_init ! set melt ponds parameters |
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[8586] | 611 | ! |
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| 612 | END SUBROUTINE ice_thd_init |
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| 613 | |
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| 614 | #else |
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| 615 | !!---------------------------------------------------------------------- |
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[9570] | 616 | !! Default option Dummy module NO SI3 sea-ice model |
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[8586] | 617 | !!---------------------------------------------------------------------- |
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| 618 | #endif |
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| 619 | |
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| 620 | !!====================================================================== |
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| 621 | END MODULE icethd |
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