MODULE bdyice !!====================================================================== !! *** MODULE bdyice *** !! Unstructured Open Boundary Cond. : Open boundary conditions for sea-ice (SI3) !!====================================================================== !! History : 3.3 ! 2010-09 (D. Storkey) Original code !! 3.4 ! 2012-01 (C. Rousset) add new sea ice model !! 4.0 ! 2018 (C. Rousset) SI3 compatibility !!---------------------------------------------------------------------- #if defined key_si3 !!---------------------------------------------------------------------- !! 'key_si3' SI3 sea ice model !!---------------------------------------------------------------------- !! bdy_ice : Application of open boundaries to ice !! bdy_ice_frs : Application of Flow Relaxation Scheme !!---------------------------------------------------------------------- USE oce ! ocean dynamics and tracers variables USE ice ! sea-ice: variables USE icevar ! sea-ice: operations USE icecor ! sea-ice: corrections USE icectl ! sea-ice: control prints USE phycst ! physical constant USE eosbn2 ! equation of state USE par_oce ! ocean parameters USE dom_oce ! ocean space and time domain variables USE sbc_oce ! Surface boundary condition: ocean fields USE bdy_oce ! ocean open boundary conditions ! USE lbclnk ! ocean lateral boundary conditions (or mpp link) USE in_out_manager ! write to numout file USE lib_mpp ! distributed memory computing USE lib_fortran ! to use key_nosignedzero USE timing ! Timing IMPLICIT NONE PRIVATE PUBLIC bdy_ice ! routine called in sbcmod PUBLIC bdy_ice_dyn ! routine called in icedyn_rhg_evp !!---------------------------------------------------------------------- !! NEMO/OCE 4.0 , NEMO Consortium (2018) !! $Id: bdyice.F90 8306 2017-07-10 10:18:03Z clem $ !! Software governed by the CeCILL licence (./LICENSE) !!---------------------------------------------------------------------- CONTAINS SUBROUTINE bdy_ice( kt ) !!---------------------------------------------------------------------- !! *** SUBROUTINE bdy_ice *** !! !! ** Purpose : - Apply open boundary conditions for ice (SI3) !! !!---------------------------------------------------------------------- INTEGER, INTENT(in) :: kt ! Main time step counter ! INTEGER :: ib_bdy ! Loop index !!---------------------------------------------------------------------- ! IF( ln_timing ) CALL timing_start('bdy_ice') ! CALL ice_var_glo2eqv ! DO ib_bdy = 1, nb_bdy ! SELECT CASE( cn_ice(ib_bdy) ) CASE('none') ; CYCLE CASE('frs' ) ; CALL bdy_ice_frs( idx_bdy(ib_bdy), dta_bdy(ib_bdy), kt, ib_bdy ) CASE DEFAULT CALL ctl_stop( 'bdy_ice : unrecognised option for open boundaries for ice fields' ) END SELECT ! END DO ! CALL ice_cor( kt , 0 ) ! -- In case categories are out of bounds, do a remapping ! ! i.e. inputs have not the same ice thickness distribution (set by rn_himean) ! ! than the regional simulation CALL ice_var_agg(1) ! IF( ln_icectl ) CALL ice_prt( kt, iiceprt, jiceprt, 1, ' - ice thermo bdy - ' ) IF( ln_timing ) CALL timing_stop('bdy_ice') ! END SUBROUTINE bdy_ice SUBROUTINE bdy_ice_frs( idx, dta, kt, ib_bdy ) !!------------------------------------------------------------------------------ !! *** SUBROUTINE bdy_ice_frs *** !! !! ** Purpose : Apply the Flow Relaxation Scheme for sea-ice fields in the case !! of unstructured open boundaries. !! !! Reference : Engedahl H., 1995: Use of the flow relaxation scheme in a three- !! dimensional baroclinic ocean model with realistic topography. Tellus, 365-382. !!------------------------------------------------------------------------------ TYPE(OBC_INDEX), INTENT(in) :: idx ! OBC indices TYPE(OBC_DATA), INTENT(in) :: dta ! OBC external data INTEGER, INTENT(in) :: kt ! main time-step counter INTEGER, INTENT(in) :: ib_bdy ! BDY set index ! INTEGER :: jpbound ! 0 = incoming ice ! ! 1 = outgoing ice INTEGER :: jb, jk, jgrd, jl ! dummy loop indices INTEGER :: ji, jj, ii, ij ! local scalar REAL(wp) :: zwgt, zwgt1 ! local scalar REAL(wp) :: ztmelts, zdh !!------------------------------------------------------------------------------ ! jgrd = 1 ! Everything is at T-points here ! DO jl = 1, jpl DO jb = 1, idx%nblenrim(jgrd) ji = idx%nbi(jb,jgrd) jj = idx%nbj(jb,jgrd) zwgt = idx%nbw(jb,jgrd) zwgt1 = 1.e0 - idx%nbw(jb,jgrd) a_i(ji,jj,jl) = ( a_i(ji,jj,jl) * zwgt1 + dta%a_i(jb,jl) * zwgt ) * tmask(ji,jj,1) ! Leads fraction h_i(ji,jj,jl) = ( h_i(ji,jj,jl) * zwgt1 + dta%h_i(jb,jl) * zwgt ) * tmask(ji,jj,1) ! Ice depth h_s(ji,jj,jl) = ( h_s(ji,jj,jl) * zwgt1 + dta%h_s(jb,jl) * zwgt ) * tmask(ji,jj,1) ! Snow depth ! ----------------- ! Pathological case ! ----------------- ! In case a) snow load would be in excess or b) ice is coming into a warmer environment that would lead to ! very large transformation from snow to ice (see icethd_dh.F90) ! Then, a) transfer the snow excess into the ice (different from icethd_dh) zdh = MAX( 0._wp, ( rhosn * h_s(ji,jj,jl) + ( rhoic - rau0 ) * h_i(ji,jj,jl) ) * r1_rau0 ) ! Or, b) transfer all the snow into ice (if incoming ice is likely to melt as it comes into a warmer environment) !zdh = MAX( 0._wp, h_s(ji,jj,jl) * rhosn / rhoic ) ! recompute h_i, h_s h_i(ji,jj,jl) = MIN( hi_max(jl), h_i(ji,jj,jl) + zdh ) h_s(ji,jj,jl) = MAX( 0._wp, h_s(ji,jj,jl) - zdh * rhoic / rhosn ) ENDDO CALL lbc_bdy_lnk( a_i(:,:,jl), 'T', 1., ib_bdy ) CALL lbc_bdy_lnk( h_i(:,:,jl), 'T', 1., ib_bdy ) CALL lbc_bdy_lnk( h_s(:,:,jl), 'T', 1., ib_bdy ) ENDDO DO jl = 1, jpl DO jb = 1, idx%nblenrim(jgrd) ji = idx%nbi(jb,jgrd) jj = idx%nbj(jb,jgrd) ! condition on ice thickness depends on the ice velocity ! if velocity is outward (strictly), then ice thickness, volume... must be equal to adjacent values jpbound = 0 ; ii = ji ; ij = jj ! IF( u_ice(ji+1,jj ) < 0. .AND. umask(ji-1,jj ,1) == 0. ) jpbound = 1; ii = ji+1; ij = jj IF( u_ice(ji-1,jj ) > 0. .AND. umask(ji+1,jj ,1) == 0. ) jpbound = 1; ii = ji-1; ij = jj IF( v_ice(ji ,jj+1) < 0. .AND. vmask(ji ,jj-1,1) == 0. ) jpbound = 1; ii = ji ; ij = jj+1 IF( v_ice(ji ,jj-1) > 0. .AND. vmask(ji ,jj+1,1) == 0. ) jpbound = 1; ii = ji ; ij = jj-1 ! IF( nn_ice_dta(ib_bdy) == 0 ) jpbound = 0; ii = ji; ij = jj ! case ice boundaries = initial conditions ! ! do not make state variables dependent on velocity ! IF( a_i(ii,ij,jl) > 0._wp ) THEN ! there is ice at the boundary ! a_i(ji,jj,jl) = a_i(ii,ij,jl) ! concentration h_i(ji,jj,jl) = h_i(ii,ij,jl) ! thickness ice h_s(ji,jj,jl) = h_s(ii,ij,jl) ! thickness snw ! SELECT CASE( jpbound ) ! CASE( 0 ) ! velocity is inward ! oa_i(ji,jj, jl) = rn_ice_age(ib_bdy) * a_i(ji,jj,jl) ! age a_ip(ji,jj, jl) = 0._wp ! pond concentration v_ip(ji,jj, jl) = 0._wp ! pond volume t_su(ji,jj, jl) = rn_ice_tem(ib_bdy) ! temperature surface t_s (ji,jj,:,jl) = rn_ice_tem(ib_bdy) ! temperature snw t_i (ji,jj,:,jl) = rn_ice_tem(ib_bdy) ! temperature ice s_i (ji,jj, jl) = rn_ice_sal(ib_bdy) ! salinity sz_i(ji,jj,:,jl) = rn_ice_sal(ib_bdy) ! salinity profile ! CASE( 1 ) ! velocity is outward ! oa_i(ji,jj, jl) = oa_i(ii,ij, jl) ! age a_ip(ji,jj, jl) = a_ip(ii,ij, jl) ! pond concentration v_ip(ji,jj, jl) = v_ip(ii,ij, jl) ! pond volume t_su(ji,jj, jl) = t_su(ii,ij, jl) ! temperature surface t_s (ji,jj,:,jl) = t_s (ii,ij,:,jl) ! temperature snw t_i (ji,jj,:,jl) = t_i (ii,ij,:,jl) ! temperature ice s_i (ji,jj, jl) = s_i (ii,ij, jl) ! salinity sz_i(ji,jj,:,jl) = sz_i(ii,ij,:,jl) ! salinity profile ! END SELECT ! IF( nn_icesal == 1 ) THEN ! if constant salinity s_i (ji,jj ,jl) = rn_icesal sz_i(ji,jj,:,jl) = rn_icesal ENDIF ! ! global fields v_i (ji,jj,jl) = h_i(ji,jj,jl) * a_i(ji,jj,jl) ! volume ice v_s (ji,jj,jl) = h_s(ji,jj,jl) * a_i(ji,jj,jl) ! volume snw sv_i(ji,jj,jl) = MIN( s_i(ji,jj,jl) , sss_m(ji,jj) ) * v_i(ji,jj,jl) ! salt content DO jk = 1, nlay_s e_s(ji,jj,jk,jl) = rhosn * ( cpic * ( rt0 - t_s(ji,jj,jk,jl) ) + lfus ) ! enthalpy in J/m3 e_s(ji,jj,jk,jl) = e_s(ji,jj,jk,jl) * v_s(ji,jj,jl) * r1_nlay_s ! enthalpy in J/m2 END DO DO jk = 1, nlay_i ztmelts = - tmut * sz_i(ji,jj,jk,jl) ! Melting temperature in C t_i(ji,jj,jk,jl) = MIN( t_i(ji,jj,jk,jl), ztmelts + rt0 ) ! Force t_i to be lower than melting point => likely conservation issue ! e_i(ji,jj,jk,jl) = rhoic * ( cpic * ( ztmelts - ( t_i(ji,jj,jk,jl) - rt0 ) ) & ! enthalpy in J/m3 & + lfus * ( 1._wp - ztmelts / ( t_i(ji,jj,jk,jl) - rt0 ) ) & & - rcp * ztmelts ) e_i(ji,jj,jk,jl) = e_i(ji,jj,jk,jl) * v_i(ji,jj,jl) * r1_nlay_i ! enthalpy in J/m2 END DO ! ELSE ! no ice at the boundary ! a_i (ji,jj, jl) = 0._wp h_i (ji,jj, jl) = 0._wp h_s (ji,jj, jl) = 0._wp oa_i(ji,jj, jl) = 0._wp a_ip(ji,jj, jl) = 0._wp v_ip(ji,jj, jl) = 0._wp t_su(ji,jj, jl) = rt0 t_s (ji,jj,:,jl) = rt0 t_i (ji,jj,:,jl) = rt0 IF( nn_icesal == 1 ) THEN ! if constant salinity s_i (ji,jj ,jl) = rn_icesal sz_i(ji,jj,:,jl) = rn_icesal ELSE ! if variable salinity s_i (ji,jj,jl) = rn_simin sz_i(ji,jj,:,jl) = rn_simin ENDIF ! ! global fields v_i (ji,jj, jl) = 0._wp v_s (ji,jj, jl) = 0._wp sv_i(ji,jj, jl) = 0._wp e_s (ji,jj,:,jl) = 0._wp e_i (ji,jj,:,jl) = 0._wp ENDIF END DO ! CALL lbc_bdy_lnk( a_i (:,:,jl), 'T', 1., ib_bdy ) CALL lbc_bdy_lnk( h_i (:,:,jl), 'T', 1., ib_bdy ) CALL lbc_bdy_lnk( h_s (:,:,jl), 'T', 1., ib_bdy ) CALL lbc_bdy_lnk( oa_i(:,:,jl), 'T', 1., ib_bdy ) CALL lbc_bdy_lnk( a_ip(:,:,jl), 'T', 1., ib_bdy ) CALL lbc_bdy_lnk( v_ip(:,:,jl), 'T', 1., ib_bdy ) CALL lbc_bdy_lnk( s_i (:,:,jl), 'T', 1., ib_bdy ) CALL lbc_bdy_lnk( t_su(:,:,jl), 'T', 1., ib_bdy ) CALL lbc_bdy_lnk( v_i (:,:,jl), 'T', 1., ib_bdy ) CALL lbc_bdy_lnk( v_s (:,:,jl), 'T', 1., ib_bdy ) CALL lbc_bdy_lnk( sv_i(:,:,jl), 'T', 1., ib_bdy ) DO jk = 1, nlay_s CALL lbc_bdy_lnk(t_s(:,:,jk,jl), 'T', 1., ib_bdy ) CALL lbc_bdy_lnk(e_s(:,:,jk,jl), 'T', 1., ib_bdy ) END DO DO jk = 1, nlay_i CALL lbc_bdy_lnk(t_i(:,:,jk,jl), 'T', 1., ib_bdy ) CALL lbc_bdy_lnk(e_i(:,:,jk,jl), 'T', 1., ib_bdy ) END DO ! END DO ! jl ! END SUBROUTINE bdy_ice_frs SUBROUTINE bdy_ice_dyn( cd_type ) !!------------------------------------------------------------------------------ !! *** SUBROUTINE bdy_ice_dyn *** !! !! ** Purpose : Apply dynamics boundary conditions for sea-ice in the cas of unstructured open boundaries. !! u_ice and v_ice are equal to the value of the adjacent grid point if this latter is not ice free !! if adjacent grid point is ice free, then u_ice and v_ice are equal to ocean velocities !! !! 2013-06 : C. Rousset !!------------------------------------------------------------------------------ CHARACTER(len=1), INTENT(in) :: cd_type ! nature of velocity grid-points ! INTEGER :: jb, jgrd ! dummy loop indices INTEGER :: ji, jj ! local scalar INTEGER :: ib_bdy ! Loop index REAL(wp) :: zmsk1, zmsk2, zflag !!------------------------------------------------------------------------------ ! DO ib_bdy=1, nb_bdy ! SELECT CASE( cn_ice(ib_bdy) ) ! CASE('none') CYCLE ! CASE('frs') ! IF( nn_ice_dta(ib_bdy) == 0 ) CYCLE ! case ice boundaries = initial conditions ! ! do not change ice velocity (it is only computed by rheology) SELECT CASE ( cd_type ) ! CASE ( 'U' ) jgrd = 2 ! u velocity DO jb = 1, idx_bdy(ib_bdy)%nblenrim(jgrd) ji = idx_bdy(ib_bdy)%nbi(jb,jgrd) jj = idx_bdy(ib_bdy)%nbj(jb,jgrd) zflag = idx_bdy(ib_bdy)%flagu(jb,jgrd) ! IF ( ABS( zflag ) == 1. ) THEN ! eastern and western boundaries ! one of the two zmsk is always 0 (because of zflag) zmsk1 = 1._wp - MAX( 0.0_wp, SIGN ( 1.0_wp , - vt_i(ji+1,jj) ) ) ! 0 if no ice zmsk2 = 1._wp - MAX( 0.0_wp, SIGN ( 1.0_wp , - vt_i(ji-1,jj) ) ) ! 0 if no ice ! ! u_ice = u_ice of the adjacent grid point except if this grid point is ice-free (then do not change u_ice) u_ice (ji,jj) = u_ice(ji+1,jj) * 0.5_wp * ABS( zflag + 1._wp ) * zmsk1 + & & u_ice(ji-1,jj) * 0.5_wp * ABS( zflag - 1._wp ) * zmsk2 + & & u_ice(ji ,jj) * ( 1._wp - MIN( 1._wp, zmsk1 + zmsk2 ) ) ELSE ! everywhere else u_ice(ji,jj) = 0._wp ENDIF ! END DO CALL lbc_bdy_lnk( u_ice(:,:), 'U', -1., ib_bdy ) ! CASE ( 'V' ) jgrd = 3 ! v velocity DO jb = 1, idx_bdy(ib_bdy)%nblenrim(jgrd) ji = idx_bdy(ib_bdy)%nbi(jb,jgrd) jj = idx_bdy(ib_bdy)%nbj(jb,jgrd) zflag = idx_bdy(ib_bdy)%flagv(jb,jgrd) ! IF ( ABS( zflag ) == 1. ) THEN ! northern and southern boundaries ! one of the two zmsk is always 0 (because of zflag) zmsk1 = 1._wp - MAX( 0.0_wp, SIGN ( 1.0_wp , - vt_i(ji,jj+1) ) ) ! 0 if no ice zmsk2 = 1._wp - MAX( 0.0_wp, SIGN ( 1.0_wp , - vt_i(ji,jj-1) ) ) ! 0 if no ice ! ! v_ice = v_ice of the adjacent grid point except if this grid point is ice-free (then do not change v_ice) v_ice (ji,jj) = v_ice(ji,jj+1) * 0.5_wp * ABS( zflag + 1._wp ) * zmsk1 + & & v_ice(ji,jj-1) * 0.5_wp * ABS( zflag - 1._wp ) * zmsk2 + & & v_ice(ji,jj ) * ( 1._wp - MIN( 1._wp, zmsk1 + zmsk2 ) ) ELSE ! everywhere else v_ice(ji,jj) = 0._wp ENDIF ! END DO CALL lbc_bdy_lnk( v_ice(:,:), 'V', -1., ib_bdy ) ! END SELECT ! CASE DEFAULT CALL ctl_stop( 'bdy_ice_dyn : unrecognised option for open boundaries for ice fields' ) END SELECT ! END DO ! END SUBROUTINE bdy_ice_dyn #else !!--------------------------------------------------------------------------------- !! Default option Empty module !!--------------------------------------------------------------------------------- CONTAINS SUBROUTINE bdy_ice( kt ) ! Empty routine WRITE(*,*) 'bdy_ice: You should not have seen this print! error?', kt END SUBROUTINE bdy_ice #endif !!================================================================================= END MODULE bdyice