[825] | 1 | MODULE limthd_ent |
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| 2 | !!====================================================================== |
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| 3 | !! *** MODULE limthd_ent *** |
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| 4 | !! Redistribution of Enthalpy in the ice |
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| 5 | !! on the new vertical grid |
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| 6 | !! after vertical growth/decay |
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| 7 | !!====================================================================== |
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[2715] | 8 | !! History : LIM ! 2003-05 (M. Vancoppenolle) Original code in 1D |
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| 9 | !! ! 2005-07 (M. Vancoppenolle) 3D version |
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| 10 | !! ! 2006-11 (X. Fettweis) Vectorized |
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| 11 | !! 3.0 ! 2008-03 (M. Vancoppenolle) Energy conservation and clean code |
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[4688] | 12 | !! 3.4 ! 2011-02 (G. Madec) dynamical allocation |
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| 13 | !! - ! 2014-05 (C. Rousset) complete rewriting |
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[2715] | 14 | !!---------------------------------------------------------------------- |
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[2528] | 15 | #if defined key_lim3 |
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| 16 | !!---------------------------------------------------------------------- |
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| 17 | !! 'key_lim3' LIM3 sea-ice model |
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| 18 | !!---------------------------------------------------------------------- |
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[3625] | 19 | !! lim_thd_ent : ice redistribution of enthalpy |
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[2528] | 20 | !!---------------------------------------------------------------------- |
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[3625] | 21 | USE par_oce ! ocean parameters |
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| 22 | USE dom_oce ! domain variables |
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| 23 | USE domain ! |
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| 24 | USE phycst ! physical constants |
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[4688] | 25 | USE sbc_oce ! Surface boundary condition: ocean fields |
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[3625] | 26 | USE ice ! LIM variables |
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| 27 | USE par_ice ! LIM parameters |
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| 28 | USE thd_ice ! LIM thermodynamics |
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| 29 | USE limvar ! LIM variables |
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| 30 | USE in_out_manager ! I/O manager |
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| 31 | USE lib_mpp ! MPP library |
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| 32 | USE wrk_nemo ! work arrays |
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| 33 | USE lib_fortran ! Fortran utilities (allows no signed zero when 'key_nosignedzero' defined) |
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[825] | 34 | |
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| 35 | IMPLICIT NONE |
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| 36 | PRIVATE |
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| 37 | |
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[4688] | 38 | PUBLIC lim_thd_ent ! called by limthd and limthd_lac |
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[825] | 39 | |
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| 40 | !!---------------------------------------------------------------------- |
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[4161] | 41 | !! NEMO/LIM3 4.0 , UCL - NEMO Consortium (2011) |
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[5232] | 42 | !! $Id: limthd_ent.F90 4990 2014-12-15 16:42:49Z timgraham $ |
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[2528] | 43 | !! Software governed by the CeCILL licence (NEMOGCM/NEMO_CeCILL.txt) |
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[825] | 44 | !!---------------------------------------------------------------------- |
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| 45 | CONTAINS |
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[3294] | 46 | |
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[4688] | 47 | SUBROUTINE lim_thd_ent( kideb, kiut, qnew ) |
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[825] | 48 | !!------------------------------------------------------------------- |
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| 49 | !! *** ROUTINE lim_thd_ent *** |
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| 50 | !! |
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| 51 | !! ** Purpose : |
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[4688] | 52 | !! This routine computes new vertical grids in the ice, |
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| 53 | !! and consistently redistributes temperatures. |
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[825] | 54 | !! Redistribution is made so as to ensure to energy conservation |
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| 55 | !! |
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| 56 | !! |
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| 57 | !! ** Method : linear conservative remapping |
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| 58 | !! |
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[4688] | 59 | !! ** Steps : 1) cumulative integrals of old enthalpies/thicknesses |
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| 60 | !! 2) linear remapping on the new layers |
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[825] | 61 | !! |
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[4688] | 62 | !! ------------ cum0(0) ------------- cum1(0) |
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| 63 | !! NEW ------------- |
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| 64 | !! ------------ cum0(1) ==> ------------- |
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| 65 | !! ... ------------- |
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| 66 | !! ------------ ------------- |
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| 67 | !! ------------ cum0(nlay_i+2) ------------- cum1(nlay_i) |
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| 68 | !! |
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| 69 | !! |
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[2715] | 70 | !! References : Bitz & Lipscomb, JGR 99; Vancoppenolle et al., GRL, 2005 |
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| 71 | !!------------------------------------------------------------------- |
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| 72 | INTEGER , INTENT(in) :: kideb, kiut ! Start/End point on which the the computation is applied |
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[825] | 73 | |
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[4688] | 74 | REAL(wp), INTENT(inout), DIMENSION(:,:) :: qnew ! new enthlapies (J.m-3, remapped) |
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[825] | 75 | |
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[4688] | 76 | INTEGER :: ji ! dummy loop indices |
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| 77 | INTEGER :: jk0, jk1 ! old/new layer indices |
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[2715] | 78 | ! |
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[4688] | 79 | REAL(wp), POINTER, DIMENSION(:,:) :: zqh_cum0, zh_cum0 ! old cumulative enthlapies and layers interfaces |
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| 80 | REAL(wp), POINTER, DIMENSION(:,:) :: zqh_cum1, zh_cum1 ! new cumulative enthlapies and layers interfaces |
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| 81 | REAL(wp), POINTER, DIMENSION(:) :: zhnew ! new layers thicknesses |
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[2715] | 82 | !!------------------------------------------------------------------- |
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[825] | 83 | |
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[4688] | 84 | CALL wrk_alloc( jpij, nlay_i+3, zqh_cum0, zh_cum0, kjstart = 0 ) |
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| 85 | CALL wrk_alloc( jpij, nlay_i+1, zqh_cum1, zh_cum1, kjstart = 0 ) |
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| 86 | CALL wrk_alloc( jpij, zhnew ) |
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[825] | 87 | |
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[4688] | 88 | !-------------------------------------------------------------------------- |
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| 89 | ! 1) Cumulative integral of old enthalpy * thicnkess and layers interfaces |
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| 90 | !-------------------------------------------------------------------------- |
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| 91 | zqh_cum0(:,0:nlay_i+2) = 0._wp |
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| 92 | zh_cum0 (:,0:nlay_i+2) = 0._wp |
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| 93 | DO jk0 = 1, nlay_i+2 |
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[921] | 94 | DO ji = kideb, kiut |
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[4688] | 95 | zqh_cum0(ji,jk0) = zqh_cum0(ji,jk0-1) + qh_i_old(ji,jk0-1) |
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| 96 | zh_cum0 (ji,jk0) = zh_cum0 (ji,jk0-1) + h_i_old (ji,jk0-1) |
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| 97 | ENDDO |
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[825] | 98 | ENDDO |
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| 99 | |
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[4688] | 100 | !------------------------------------ |
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| 101 | ! 2) Interpolation on the new layers |
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| 102 | !------------------------------------ |
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| 103 | ! new layer thickesses |
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[825] | 104 | DO ji = kideb, kiut |
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[4688] | 105 | zhnew(ji) = SUM( h_i_old(ji,0:nlay_i+1) ) / REAL( nlay_i ) |
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[825] | 106 | ENDDO |
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| 107 | |
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[4688] | 108 | ! new layers interfaces |
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| 109 | zh_cum1(:,0:nlay_i) = 0._wp |
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| 110 | DO jk1 = 1, nlay_i |
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[921] | 111 | DO ji = kideb, kiut |
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[4688] | 112 | zh_cum1(ji,jk1) = zh_cum1(ji,jk1-1) + zhnew(ji) |
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| 113 | ENDDO |
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[825] | 114 | ENDDO |
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| 115 | |
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[4688] | 116 | zqh_cum1(:,0:nlay_i) = 0._wp |
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| 117 | ! new cumulative q*h => linear interpolation |
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| 118 | DO jk0 = 1, nlay_i+1 |
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| 119 | DO jk1 = 1, nlay_i-1 |
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[921] | 120 | DO ji = kideb, kiut |
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[4688] | 121 | IF( zh_cum1(ji,jk1) <= zh_cum0(ji,jk0) .AND. zh_cum1(ji,jk1) > zh_cum0(ji,jk0-1) ) THEN |
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| 122 | zqh_cum1(ji,jk1) = ( zqh_cum0(ji,jk0-1) * ( zh_cum0(ji,jk0) - zh_cum1(ji,jk1 ) ) + & |
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| 123 | & zqh_cum0(ji,jk0 ) * ( zh_cum1(ji,jk1) - zh_cum0(ji,jk0-1) ) ) & |
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| 124 | & / ( zh_cum0(ji,jk0) - zh_cum0(ji,jk0-1) ) |
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| 125 | ENDIF |
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| 126 | ENDDO |
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| 127 | ENDDO |
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| 128 | ENDDO |
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| 129 | ! to ensure that total heat content is strictly conserved, set: |
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| 130 | zqh_cum1(:,nlay_i) = zqh_cum0(:,nlay_i+2) |
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[825] | 131 | |
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[4688] | 132 | ! new enthalpies |
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| 133 | DO jk1 = 1, nlay_i |
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[825] | 134 | DO ji = kideb, kiut |
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[4990] | 135 | rswitch = 1._wp - MAX( 0._wp , SIGN( 1._wp , - zhnew(ji) + epsi10 ) ) |
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| 136 | qnew(ji,jk1) = rswitch * ( zqh_cum1(ji,jk1) - zqh_cum1(ji,jk1-1) ) / MAX( zhnew(ji), epsi10 ) |
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[4688] | 137 | ENDDO |
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| 138 | ENDDO |
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[825] | 139 | |
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[4688] | 140 | ! --- diag error on heat remapping --- ! |
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| 141 | ! comment: if input h_i_old and qh_i_old are already multiplied by a_i (as in limthd_lac), |
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| 142 | ! then we should not (* a_i) again but not important since this is just to check that remap error is ~0 |
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[825] | 143 | DO ji = kideb, kiut |
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[4872] | 144 | hfx_err_rem_1d(ji) = hfx_err_rem_1d(ji) + a_i_1d(ji) * r1_rdtice * & |
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[4688] | 145 | & ( SUM( qnew(ji,1:nlay_i) ) * zhnew(ji) - SUM( qh_i_old(ji,0:nlay_i+1) ) ) |
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[2715] | 146 | END DO |
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[4688] | 147 | |
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[921] | 148 | ! |
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[4688] | 149 | CALL wrk_dealloc( jpij, nlay_i+3, zqh_cum0, zh_cum0, kjstart = 0 ) |
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| 150 | CALL wrk_dealloc( jpij, nlay_i+1, zqh_cum1, zh_cum1, kjstart = 0 ) |
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| 151 | CALL wrk_dealloc( jpij, zhnew ) |
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[921] | 152 | ! |
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| 153 | END SUBROUTINE lim_thd_ent |
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[825] | 154 | |
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| 155 | #else |
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[2715] | 156 | !!---------------------------------------------------------------------- |
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| 157 | !! Default option NO LIM3 sea-ice model |
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| 158 | !!---------------------------------------------------------------------- |
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[825] | 159 | CONTAINS |
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| 160 | SUBROUTINE lim_thd_ent ! Empty routine |
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| 161 | END SUBROUTINE lim_thd_ent |
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| 162 | #endif |
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[2715] | 163 | |
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| 164 | !!====================================================================== |
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[921] | 165 | END MODULE limthd_ent |
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