| 1 | MODULE bdyice |
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| 2 | !!====================================================================== |
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| 3 | !! *** MODULE bdyice *** |
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| 4 | !! Unstructured Open Boundary Cond. : Open boundary conditions for sea-ice (LIM3) |
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| 5 | !!====================================================================== |
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| 6 | !! History : 3.3 ! 2010-09 (D. Storkey) Original code |
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| 7 | !! 3.4 ! 2011 (D. Storkey) rewrite in preparation for OBC-BDY merge |
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| 8 | !! - ! 2012-01 (C. Rousset) add lim3 and remove useless jk loop |
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| 9 | !!---------------------------------------------------------------------- |
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| 10 | #if defined key_lim3 |
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| 11 | !!---------------------------------------------------------------------- |
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| 12 | !! 'key_lim3' LIM-3 sea ice model |
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| 13 | !!---------------------------------------------------------------------- |
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| 14 | !! bdy_ice : Application of open boundaries to ice |
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| 15 | !! bdy_ice_frs : Application of Flow Relaxation Scheme |
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| 16 | !!---------------------------------------------------------------------- |
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| 17 | USE timing ! Timing |
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| 18 | USE phycst ! physical constant |
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| 19 | USE eosbn2 ! equation of state |
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| 20 | USE oce ! ocean dynamics and tracers variables |
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| 21 | USE ice ! sea-ice: variables |
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| 22 | USE icevar ! sea-ice: operations |
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| 23 | USE iceitd ! sea-ice: rebining |
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| 24 | USE icectl ! sea-ice: control prints |
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| 25 | USE par_oce ! ocean parameters |
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| 26 | USE dom_oce ! ocean space and time domain variables |
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| 27 | USE sbc_oce ! Surface boundary condition: ocean fields |
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| 28 | USE bdy_oce ! ocean open boundary conditions |
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| 29 | USE lbclnk ! ocean lateral boundary conditions (or mpp link) |
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| 30 | USE in_out_manager ! write to numout file |
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| 31 | USE lib_mpp ! distributed memory computing |
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| 32 | USE lib_fortran ! to use key_nosignedzero |
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| 33 | |
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| 34 | IMPLICIT NONE |
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| 35 | PRIVATE |
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| 36 | |
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| 37 | PUBLIC bdy_ice ! routine called in sbcmod |
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| 38 | PUBLIC bdy_ice_dyn ! routine called in limrhg |
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| 39 | |
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| 40 | !!---------------------------------------------------------------------- |
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| 41 | !! NEMO/OPA 3.3 , NEMO Consortium (2010) |
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| 42 | !! $Id: bdyice.F90 8306 2017-07-10 10:18:03Z clem $ |
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| 43 | !! Software governed by the CeCILL licence (NEMOGCM/NEMO_CeCILL.txt) |
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| 44 | !!---------------------------------------------------------------------- |
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| 45 | CONTAINS |
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| 46 | |
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| 47 | SUBROUTINE bdy_ice( kt ) |
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| 48 | !!---------------------------------------------------------------------- |
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| 49 | !! *** SUBROUTINE bdy_ice *** |
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| 50 | !! |
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| 51 | !! ** Purpose : - Apply open boundary conditions for ice (LIM3) |
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| 52 | !! |
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| 53 | !!---------------------------------------------------------------------- |
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| 54 | INTEGER, INTENT( in ) :: kt ! Main time step counter |
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| 55 | ! |
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| 56 | INTEGER :: ib_bdy ! Loop index |
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| 57 | !!---------------------------------------------------------------------- |
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| 58 | ! |
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| 59 | CALL ice_var_glo2eqv |
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| 60 | ! |
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| 61 | DO ib_bdy=1, nb_bdy |
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| 62 | ! |
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| 63 | SELECT CASE( cn_ice_lim(ib_bdy) ) |
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| 64 | CASE('none') |
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| 65 | CYCLE |
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| 66 | CASE('frs') |
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| 67 | CALL bdy_ice_frs( idx_bdy(ib_bdy), dta_bdy(ib_bdy), kt, ib_bdy ) |
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| 68 | CASE DEFAULT |
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| 69 | CALL ctl_stop( 'bdy_ice : unrecognised option for open boundaries for ice fields' ) |
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| 70 | END SELECT |
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| 71 | ! |
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| 72 | END DO |
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| 73 | ! |
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| 74 | CALL ice_var_zapsmall |
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| 75 | CALL ice_var_agg(1) |
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| 76 | IF( ln_icectl ) CALL ice_prt( kt, iiceprt, jiceprt, 1, ' - ice thermo bdy - ' ) |
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| 77 | ! |
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| 78 | END SUBROUTINE bdy_ice |
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| 79 | |
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| 80 | |
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| 81 | SUBROUTINE bdy_ice_frs( idx, dta, kt, ib_bdy ) |
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| 82 | !!------------------------------------------------------------------------------ |
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| 83 | !! *** SUBROUTINE bdy_ice_frs *** |
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| 84 | !! |
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| 85 | !! ** Purpose : Apply the Flow Relaxation Scheme for sea-ice fields in the case |
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| 86 | !! of unstructured open boundaries. |
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| 87 | !! |
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| 88 | !! Reference : Engedahl H., 1995: Use of the flow relaxation scheme in a three- |
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| 89 | !! dimensional baroclinic ocean model with realistic topography. Tellus, 365-382. |
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| 90 | !!------------------------------------------------------------------------------ |
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| 91 | TYPE(OBC_INDEX), INTENT(in) :: idx ! OBC indices |
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| 92 | TYPE(OBC_DATA), INTENT(in) :: dta ! OBC external data |
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| 93 | INTEGER, INTENT(in) :: kt ! main time-step counter |
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| 94 | INTEGER, INTENT(in) :: ib_bdy ! BDY set index |
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| 95 | ! |
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| 96 | INTEGER :: jpbound ! 0 = incoming ice |
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| 97 | ! ! 1 = outgoing ice |
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| 98 | INTEGER :: jb, jk, jgrd, jl ! dummy loop indices |
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| 99 | INTEGER :: ji, jj, ii, ij ! local scalar |
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| 100 | REAL(wp) :: zwgt, zwgt1 ! local scalar |
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| 101 | REAL(wp) :: ztmelts, zdh |
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| 102 | !!------------------------------------------------------------------------------ |
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| 103 | ! |
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| 104 | IF( nn_timing == 1 ) CALL timing_start('bdy_ice_frs') |
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| 105 | ! |
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| 106 | jgrd = 1 ! Everything is at T-points here |
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| 107 | ! |
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| 108 | DO jl = 1, jpl |
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| 109 | DO jb = 1, idx%nblenrim(jgrd) |
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| 110 | ji = idx%nbi(jb,jgrd) |
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| 111 | jj = idx%nbj(jb,jgrd) |
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| 112 | zwgt = idx%nbw(jb,jgrd) |
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| 113 | zwgt1 = 1.e0 - idx%nbw(jb,jgrd) |
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| 114 | a_i(ji,jj,jl) = ( a_i(ji,jj,jl) * zwgt1 + dta%a_i(jb,jl) * zwgt ) * tmask(ji,jj,1) ! Leads fraction |
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| 115 | h_i(ji,jj,jl) = ( h_i(ji,jj,jl) * zwgt1 + dta%h_i(jb,jl) * zwgt ) * tmask(ji,jj,1) ! Ice depth |
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| 116 | h_s(ji,jj,jl) = ( h_s(ji,jj,jl) * zwgt1 + dta%h_s(jb,jl) * zwgt ) * tmask(ji,jj,1) ! Snow depth |
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| 117 | |
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| 118 | ! ----------------- |
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| 119 | ! Pathological case |
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| 120 | ! ----------------- |
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| 121 | ! In case a) snow load would be in excess or b) ice is coming into a warmer environment that would lead to |
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| 122 | ! very large transformation from snow to ice (see icethd_dh.F90) |
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| 123 | |
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| 124 | ! Then, a) transfer the snow excess into the ice (different from icethd_dh) |
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| 125 | zdh = MAX( 0._wp, ( rhosn * h_s(ji,jj,jl) + ( rhoic - rau0 ) * h_i(ji,jj,jl) ) * r1_rau0 ) |
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| 126 | ! Or, b) transfer all the snow into ice (if incoming ice is likely to melt as it comes into a warmer environment) |
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| 127 | !zdh = MAX( 0._wp, h_s(ji,jj,jl) * rhosn / rhoic ) |
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| 128 | |
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| 129 | ! recompute h_i, h_s |
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| 130 | h_i(ji,jj,jl) = MIN( hi_max(jl), h_i(ji,jj,jl) + zdh ) |
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| 131 | h_s(ji,jj,jl) = MAX( 0._wp, h_s(ji,jj,jl) - zdh * rhoic / rhosn ) |
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| 132 | |
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| 133 | ENDDO |
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| 134 | CALL lbc_bdy_lnk( a_i(:,:,jl), 'T', 1., ib_bdy ) |
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| 135 | CALL lbc_bdy_lnk( h_i(:,:,jl), 'T', 1., ib_bdy ) |
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| 136 | CALL lbc_bdy_lnk( h_s(:,:,jl), 'T', 1., ib_bdy ) |
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| 137 | ENDDO |
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| 138 | ! retrieve at_i |
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| 139 | at_i(:,:) = 0._wp |
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| 140 | DO jl = 1, jpl |
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| 141 | at_i(:,:) = a_i(:,:,jl) + at_i(:,:) |
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| 142 | END DO |
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| 143 | |
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| 144 | DO jl = 1, jpl |
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| 145 | DO jb = 1, idx%nblenrim(jgrd) |
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| 146 | ji = idx%nbi(jb,jgrd) |
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| 147 | jj = idx%nbj(jb,jgrd) |
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| 148 | |
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| 149 | ! condition on ice thickness depends on the ice velocity |
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| 150 | ! if velocity is outward (strictly), then ice thickness, volume... must be equal to adjacent values |
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| 151 | jpbound = 0 ; ii = ji ; ij = jj |
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| 152 | ! |
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| 153 | IF( u_ice(ji+1,jj ) < 0. .AND. umask(ji-1,jj ,1) == 0. ) jpbound = 1; ii = ji+1; ij = jj |
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| 154 | IF( u_ice(ji-1,jj ) > 0. .AND. umask(ji+1,jj ,1) == 0. ) jpbound = 1; ii = ji-1; ij = jj |
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| 155 | IF( v_ice(ji ,jj+1) < 0. .AND. vmask(ji ,jj-1,1) == 0. ) jpbound = 1; ii = ji ; ij = jj+1 |
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| 156 | IF( v_ice(ji ,jj-1) > 0. .AND. vmask(ji ,jj+1,1) == 0. ) jpbound = 1; ii = ji ; ij = jj-1 |
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| 157 | ! |
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| 158 | IF( nn_ice_lim_dta(ib_bdy) == 0 ) jpbound = 0; ii = ji; ij = jj ! case ice boundaries = initial conditions |
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| 159 | ! ! do not make state variables dependent on velocity |
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| 160 | ! |
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| 161 | rswitch = MAX( 0.0_wp , SIGN ( 1.0_wp , at_i(ii,ij) - 0.01 ) ) ! 0 if no ice |
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| 162 | ! |
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| 163 | ! concentration and thickness |
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| 164 | a_i(ji,jj,jl) = a_i(ii,ij,jl) * rswitch |
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| 165 | h_i(ji,jj,jl) = h_i(ii,ij,jl) * rswitch |
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| 166 | h_s(ji,jj,jl) = h_s(ii,ij,jl) * rswitch |
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| 167 | ! |
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| 168 | ! Ice and snow volumes |
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| 169 | v_i(ji,jj,jl) = h_i(ji,jj,jl) * a_i(ji,jj,jl) |
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| 170 | v_s(ji,jj,jl) = h_s(ji,jj,jl) * a_i(ji,jj,jl) |
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| 171 | ! |
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| 172 | SELECT CASE( jpbound ) |
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| 173 | ! |
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| 174 | CASE( 0 ) ! velocity is inward |
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| 175 | ! |
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| 176 | ! Ice salinity, age, temperature |
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| 177 | s_i (ji,jj,jl) = rswitch * rn_ice_sal(ib_bdy) + ( 1.0 - rswitch ) * rn_simin |
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| 178 | oa_i(ji,jj,jl) = rswitch * rn_ice_age(ib_bdy) * a_i(ji,jj,jl) |
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| 179 | t_su(ji,jj,jl) = rswitch * rn_ice_tem(ib_bdy) + ( 1.0 - rswitch ) * rn_ice_tem(ib_bdy) |
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| 180 | DO jk = 1, nlay_s |
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| 181 | t_s(ji,jj,jk,jl) = rswitch * rn_ice_tem(ib_bdy) + ( 1.0 - rswitch ) * rt0 |
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| 182 | END DO |
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| 183 | DO jk = 1, nlay_i |
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| 184 | t_i (ji,jj,jk,jl) = rswitch * rn_ice_tem(ib_bdy) + ( 1.0 - rswitch ) * rt0 |
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| 185 | sz_i(ji,jj,jk,jl) = rswitch * rn_ice_sal(ib_bdy) + ( 1.0 - rswitch ) * rn_simin |
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| 186 | END DO |
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| 187 | ! |
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| 188 | CASE( 1 ) ! velocity is outward |
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| 189 | ! |
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| 190 | ! Ice salinity, age, temperature |
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| 191 | s_i (ji,jj,jl) = rswitch * s_i (ii,ij,jl) + ( 1.0 - rswitch ) * rn_simin |
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| 192 | oa_i(ji,jj,jl) = rswitch * oa_i(ii,ij,jl) |
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| 193 | t_su(ji,jj,jl) = rswitch * t_su(ii,ij,jl) + ( 1.0 - rswitch ) * rt0 |
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| 194 | DO jk = 1, nlay_s |
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| 195 | t_s(ji,jj,jk,jl) = rswitch * t_s(ii,ij,jk,jl) + ( 1.0 - rswitch ) * rt0 |
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| 196 | END DO |
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| 197 | DO jk = 1, nlay_i |
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| 198 | t_i (ji,jj,jk,jl) = rswitch * t_i (ii,ij,jk,jl) + ( 1.0 - rswitch ) * rt0 |
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| 199 | sz_i(ji,jj,jk,jl) = rswitch * sz_i(ii,ij,jk,jl) + ( 1.0 - rswitch ) * rn_simin |
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| 200 | END DO |
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| 201 | ! |
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| 202 | END SELECT |
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| 203 | ! |
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| 204 | IF( nn_icesal == 1 ) THEN ! constant salinity : overwrite rn_icesal |
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| 205 | s_i (ji,jj ,jl) = rn_icesal |
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| 206 | sz_i(ji,jj,:,jl) = rn_icesal |
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| 207 | ENDIF |
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| 208 | ! |
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| 209 | ! contents |
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| 210 | sv_i(ji,jj,jl) = MIN( s_i(ji,jj,jl) , sss_m(ji,jj) ) * v_i(ji,jj,jl) |
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| 211 | DO jk = 1, nlay_s |
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| 212 | ! Snow energy of melting |
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| 213 | e_s(ji,jj,jk,jl) = rswitch * rhosn * ( cpic * ( rt0 - t_s(ji,jj,jk,jl) ) + lfus ) |
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| 214 | ! Multiply by volume, so that heat content in J/m2 |
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| 215 | e_s(ji,jj,jk,jl) = e_s(ji,jj,jk,jl) * v_s(ji,jj,jl) * r1_nlay_s |
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| 216 | END DO |
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| 217 | DO jk = 1, nlay_i |
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| 218 | ztmelts = - tmut * sz_i(ji,jj,jk,jl) + rt0 !Melting temperature in K |
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| 219 | ! heat content per unit volume |
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| 220 | e_i(ji,jj,jk,jl) = rswitch * rhoic * & |
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| 221 | ( cpic * ( ztmelts - t_i(ji,jj,jk,jl) ) & |
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| 222 | + lfus * ( 1.0 - (ztmelts-rt0) / MIN((t_i(ji,jj,jk,jl)-rt0),-epsi20) ) & |
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| 223 | - rcp * ( ztmelts - rt0 ) ) |
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| 224 | ! Mutliply by ice volume, and divide by number of layers to get heat content in J/m2 |
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| 225 | e_i(ji,jj,jk,jl) = e_i(ji,jj,jk,jl) * a_i(ji,jj,jl) * h_i(ji,jj,jl) * r1_nlay_i |
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| 226 | END DO |
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| 227 | ! |
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| 228 | END DO |
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| 229 | ! |
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| 230 | CALL lbc_bdy_lnk( a_i(:,:,jl), 'T', 1., ib_bdy ) |
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| 231 | CALL lbc_bdy_lnk( h_i(:,:,jl), 'T', 1., ib_bdy ) |
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| 232 | CALL lbc_bdy_lnk( h_s(:,:,jl), 'T', 1., ib_bdy ) |
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| 233 | CALL lbc_bdy_lnk( v_i(:,:,jl), 'T', 1., ib_bdy ) |
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| 234 | CALL lbc_bdy_lnk( v_s(:,:,jl), 'T', 1., ib_bdy ) |
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| 235 | ! |
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| 236 | CALL lbc_bdy_lnk( sv_i(:,:,jl), 'T', 1., ib_bdy ) |
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| 237 | CALL lbc_bdy_lnk( s_i(:,:,jl), 'T', 1., ib_bdy ) |
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| 238 | CALL lbc_bdy_lnk( oa_i(:,:,jl), 'T', 1., ib_bdy ) |
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| 239 | CALL lbc_bdy_lnk( t_su(:,:,jl), 'T', 1., ib_bdy ) |
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| 240 | DO jk = 1, nlay_s |
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| 241 | CALL lbc_bdy_lnk(t_s(:,:,jk,jl), 'T', 1., ib_bdy ) |
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| 242 | CALL lbc_bdy_lnk(e_s(:,:,jk,jl), 'T', 1., ib_bdy ) |
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| 243 | END DO |
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| 244 | DO jk = 1, nlay_i |
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| 245 | CALL lbc_bdy_lnk(t_i(:,:,jk,jl), 'T', 1., ib_bdy ) |
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| 246 | CALL lbc_bdy_lnk(e_i(:,:,jk,jl), 'T', 1., ib_bdy ) |
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| 247 | END DO |
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| 248 | ! |
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| 249 | END DO !jl |
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| 250 | ! |
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| 251 | ! --- In case categories are out of bounds, do a remapping --- ! |
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| 252 | ! i.e. inputs have not the same ice thickness distribution |
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| 253 | ! (set by rn_himean) than the regional simulation |
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| 254 | IF( jpl > 1 ) CALL ice_itd_reb( kt ) |
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| 255 | ! |
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| 256 | IF( nn_timing == 1 ) CALL timing_stop('bdy_ice_frs') |
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| 257 | ! |
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| 258 | END SUBROUTINE bdy_ice_frs |
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| 259 | |
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| 260 | |
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| 261 | SUBROUTINE bdy_ice_dyn( cd_type ) |
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| 262 | !!------------------------------------------------------------------------------ |
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| 263 | !! *** SUBROUTINE bdy_ice_dyn *** |
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| 264 | !! |
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| 265 | !! ** Purpose : Apply dynamics boundary conditions for sea-ice in the cas of unstructured open boundaries. |
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| 266 | !! u_ice and v_ice are equal to the value of the adjacent grid point if this latter is not ice free |
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| 267 | !! if adjacent grid point is ice free, then u_ice and v_ice are equal to ocean velocities |
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| 268 | !! |
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| 269 | !! 2013-06 : C. Rousset |
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| 270 | !!------------------------------------------------------------------------------ |
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| 271 | CHARACTER(len=1), INTENT(in) :: cd_type ! nature of velocity grid-points |
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| 272 | ! |
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| 273 | INTEGER :: jb, jgrd ! dummy loop indices |
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| 274 | INTEGER :: ji, jj ! local scalar |
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| 275 | INTEGER :: ib_bdy ! Loop index |
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| 276 | REAL(wp) :: zmsk1, zmsk2, zflag |
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| 277 | !!------------------------------------------------------------------------------ |
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| 278 | ! |
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| 279 | IF( nn_timing == 1 ) CALL timing_start('bdy_ice_dyn') |
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| 280 | ! |
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| 281 | DO ib_bdy=1, nb_bdy |
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| 282 | ! |
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| 283 | SELECT CASE( cn_ice_lim(ib_bdy) ) |
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| 284 | ! |
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| 285 | CASE('none') |
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| 286 | CYCLE |
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| 287 | ! |
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| 288 | CASE('frs') |
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| 289 | ! |
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| 290 | IF( nn_ice_lim_dta(ib_bdy) == 0 ) CYCLE ! case ice boundaries = initial conditions |
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| 291 | ! ! do not change ice velocity (it is only computed by rheology) |
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| 292 | SELECT CASE ( cd_type ) |
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| 293 | ! |
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| 294 | CASE ( 'U' ) |
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| 295 | jgrd = 2 ! u velocity |
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| 296 | DO jb = 1, idx_bdy(ib_bdy)%nblenrim(jgrd) |
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| 297 | ji = idx_bdy(ib_bdy)%nbi(jb,jgrd) |
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| 298 | jj = idx_bdy(ib_bdy)%nbj(jb,jgrd) |
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| 299 | zflag = idx_bdy(ib_bdy)%flagu(jb,jgrd) |
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| 300 | ! |
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| 301 | IF ( ABS( zflag ) == 1. ) THEN ! eastern and western boundaries |
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| 302 | ! one of the two zmsk is always 0 (because of zflag) |
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| 303 | zmsk1 = 1._wp - MAX( 0.0_wp, SIGN ( 1.0_wp , - vt_i(ji+1,jj) ) ) ! 0 if no ice |
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| 304 | zmsk2 = 1._wp - MAX( 0.0_wp, SIGN ( 1.0_wp , - vt_i(ji-1,jj) ) ) ! 0 if no ice |
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| 305 | ! |
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| 306 | ! u_ice = u_ice of the adjacent grid point except if this grid point is ice-free (then u_ice = u_oce) |
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| 307 | u_ice (ji,jj) = u_ice(ji+1,jj) * 0.5_wp * ABS( zflag + 1._wp ) * zmsk1 + & |
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| 308 | & u_ice(ji-1,jj) * 0.5_wp * ABS( zflag - 1._wp ) * zmsk2 + & |
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| 309 | & u_oce(ji ,jj) * ( 1._wp - MIN( 1._wp, zmsk1 + zmsk2 ) ) |
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| 310 | ELSE ! everywhere else |
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| 311 | !u_ice(ji,jj) = u_oce(ji,jj) |
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| 312 | u_ice(ji,jj) = 0._wp |
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| 313 | ENDIF |
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| 314 | ! mask ice velocities |
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| 315 | rswitch = MAX( 0.0_wp , SIGN ( 1.0_wp , at_i(ji,jj) - 0.01_wp ) ) ! 0 if no ice |
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| 316 | u_ice(ji,jj) = rswitch * u_ice(ji,jj) |
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| 317 | ! |
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| 318 | END DO |
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| 319 | CALL lbc_bdy_lnk( u_ice(:,:), 'U', -1., ib_bdy ) |
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| 320 | ! |
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| 321 | CASE ( 'V' ) |
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| 322 | jgrd = 3 ! v velocity |
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| 323 | DO jb = 1, idx_bdy(ib_bdy)%nblenrim(jgrd) |
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| 324 | ji = idx_bdy(ib_bdy)%nbi(jb,jgrd) |
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| 325 | jj = idx_bdy(ib_bdy)%nbj(jb,jgrd) |
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| 326 | zflag = idx_bdy(ib_bdy)%flagv(jb,jgrd) |
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| 327 | ! |
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| 328 | IF ( ABS( zflag ) == 1. ) THEN ! northern and southern boundaries |
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| 329 | ! one of the two zmsk is always 0 (because of zflag) |
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| 330 | zmsk1 = 1._wp - MAX( 0.0_wp, SIGN ( 1.0_wp , - vt_i(ji,jj+1) ) ) ! 0 if no ice |
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| 331 | zmsk2 = 1._wp - MAX( 0.0_wp, SIGN ( 1.0_wp , - vt_i(ji,jj-1) ) ) ! 0 if no ice |
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| 332 | ! |
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| 333 | ! u_ice = u_ice of the adjacent grid point except if this grid point is ice-free (then u_ice = u_oce) |
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| 334 | v_ice (ji,jj) = v_ice(ji,jj+1) * 0.5_wp * ABS( zflag + 1._wp ) * zmsk1 + & |
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| 335 | & v_ice(ji,jj-1) * 0.5_wp * ABS( zflag - 1._wp ) * zmsk2 + & |
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| 336 | & v_oce(ji,jj ) * ( 1._wp - MIN( 1._wp, zmsk1 + zmsk2 ) ) |
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| 337 | ELSE ! everywhere else |
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| 338 | !v_ice(ji,jj) = v_oce(ji,jj) |
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| 339 | v_ice(ji,jj) = 0._wp |
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| 340 | ENDIF |
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| 341 | ! mask ice velocities |
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| 342 | rswitch = MAX( 0.0_wp , SIGN ( 1.0_wp , at_i(ji,jj) - 0.01 ) ) ! 0 if no ice |
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| 343 | v_ice(ji,jj) = rswitch * v_ice(ji,jj) |
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| 344 | ! |
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| 345 | END DO |
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| 346 | CALL lbc_bdy_lnk( v_ice(:,:), 'V', -1., ib_bdy ) |
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| 347 | ! |
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| 348 | END SELECT |
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| 349 | ! |
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| 350 | CASE DEFAULT |
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| 351 | CALL ctl_stop( 'bdy_ice_dyn : unrecognised option for open boundaries for ice fields' ) |
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| 352 | END SELECT |
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| 353 | ! |
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| 354 | END DO |
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| 355 | ! |
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| 356 | IF( nn_timing == 1 ) CALL timing_stop('bdy_ice_dyn') |
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| 357 | ! |
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| 358 | END SUBROUTINE bdy_ice_dyn |
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| 359 | |
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| 360 | #else |
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| 361 | !!--------------------------------------------------------------------------------- |
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| 362 | !! Default option Empty module |
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| 363 | !!--------------------------------------------------------------------------------- |
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| 364 | CONTAINS |
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| 365 | SUBROUTINE bdy_ice( kt ) ! Empty routine |
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| 366 | WRITE(*,*) 'bdy_ice: You should not have seen this print! error?', kt |
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| 367 | END SUBROUTINE bdy_ice |
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| 368 | #endif |
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| 369 | |
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| 370 | !!================================================================================= |
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| 371 | END MODULE bdyice |
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