MODULE limthd_2 !!====================================================================== !! *** MODULE limthd_2 *** !! LIM thermo ice model : ice thermodynamic !!====================================================================== !! History : 1.0 ! 00-01 (LIM) !! 2.0 ! 02-07 (C. Ethe, G. Madec) F90 !! 2.0 ! 03-08 (C. Ethe) add lim_thd_init !!--------------------------------------------------------------------- #if defined key_lim2 !!---------------------------------------------------------------------- !! 'key_lim2' : LIM 2.0 sea-ice model !!---------------------------------------------------------------------- !! lim_thd_2 : thermodynamic of sea ice !! lim_thd_init_2 : initialisation of sea-ice thermodynamic !!---------------------------------------------------------------------- !! * Modules used USE phycst ! physical constants USE dom_oce ! ocean space and time domain variables USE lbclnk USE in_out_manager ! I/O manager USE ice_2 ! LIM sea-ice variables USE ice_oce ! sea-ice/ocean variables USE sbc_oce ! USE sbc_ice ! USE thd_ice_2 ! LIM thermodynamic sea-ice variables USE dom_ice_2 ! LIM sea-ice domain USE iceini_2 USE limthd_zdf_2 USE limthd_lac_2 USE limtab_2 USE prtctl ! Print control IMPLICIT NONE PRIVATE PUBLIC lim_thd_2 ! called by lim_step REAL(wp) :: epsi20 = 1.e-20 , & ! constant values & epsi16 = 1.e-16 , & & epsi04 = 1.e-04 , & & zzero = 0.e0 , & & zone = 1.e0 !! * Substitutions # include "domzgr_substitute.h90" # include "vectopt_loop_substitute.h90" !!-------- ------------------------------------------------------------- !! LIM 2.0, UCL-LOCEAN-IPSL (2005) !! $ Id: $ !! Software governed by the CeCILL licence (modipsl/doc/NEMO_CeCILL.txt) !!---------------------------------------------------------------------- CONTAINS SUBROUTINE lim_thd_2( kt ) !!------------------------------------------------------------------- !! *** ROUTINE lim_thd_2 *** !! !! ** Purpose : This routine manages the ice thermodynamic. !! !! ** Action : - Initialisation of some variables !! - Some preliminary computation (oceanic heat flux !! at the ice base, snow acc.,heat budget of the leads) !! - selection of the icy points and put them in an array !! - call lim_vert_ther for vert ice thermodynamic !! - back to the geographic grid !! - selection of points for lateral accretion !! - call lim_lat_acc for the ice accretion !! - back to the geographic grid !! !! References : Goosse et al. 1996, Bul. Soc. Roy. Sc. Liege, 65, 87-90 !!--------------------------------------------------------------------- INTEGER, INTENT(in) :: kt ! number of iteration !! INTEGER :: ji, jj, & ! dummy loop indices nbpb , & ! nb of icy pts for thermo. cal. nbpac ! nb of pts for lateral accretion CHARACTER (len=22) :: charout REAL(wp) :: & zfric_umin = 5e-03 , & ! lower bound for the friction velocity zfric_umax = 2e-02 ! upper bound for the friction velocity REAL(wp) :: & zinda , & ! switch for test. the val. of concen. zindb, zindg , & ! switches for test. the val of arg za , zh, zthsnice , & zfric_u , & ! friction velocity zfnsol , & ! total non solar heat zfontn , & ! heat flux from snow thickness zfntlat, zpareff ! test. the val. of lead heat budget REAL(wp), DIMENSION(jpi,jpj) :: zhicifp, & ! ice thickness for outputs & zqlbsbq ! link with lead energy budget qldif REAL(wp), DIMENSION(jpi,jpj,jpk) :: zmsk ! working array !!------------------------------------------------------------------- IF( kt == nit000 ) CALL lim_thd_init_2 ! Initialization (first time-step only) !-------------------------------------------! ! Initilization of diagnostic variables ! !-------------------------------------------! !i est-ce utile? oui au moins en partie rdvosif(:,:) = 0.e0 ! variation of ice volume at surface rdvobif(:,:) = 0.e0 ! variation of ice volume at bottom fdvolif(:,:) = 0.e0 ! total variation of ice volume rdvonif(:,:) = 0.e0 ! lateral variation of ice volume fstric (:,:) = 0.e0 ! part of solar radiation absorbing inside the ice fscmbq (:,:) = 0.e0 ! linked with fstric ffltbif(:,:) = 0.e0 ! linked with fstric qfvbq (:,:) = 0.e0 ! linked with fstric rdmsnif(:,:) = 0.e0 ! variation of snow mass per unit area rdmicif(:,:) = 0.e0 ! variation of ice mass per unit area hicifp (:,:) = 0.e0 ! daily thermodynamic ice production. zmsk (:,:,:) = 0.e0 DO jj = 1, jpj DO ji = 1, jpi hsnif(ji,jj) = hsnif(ji,jj) * MAX( zzero, SIGN( zone , hsnif(ji,jj) - epsi04 ) ) END DO END DO IF(ln_ctl) CALL prt_ctl(tab2d_1=hsnif , clinfo1=' lim_thd: hsnif : ') !-----------------------------------! ! Treatment of particular cases ! !-----------------------------------! DO jj = 1, jpj DO ji = 1, jpi ! snow is transformed into ice if the original ice cover disappears. zindg = tms(ji,jj) * MAX( zzero , SIGN( zone , -hicif(ji,jj) ) ) hicif(ji,jj) = hicif(ji,jj) + zindg * rhosn * hsnif(ji,jj) / rau0 hsnif(ji,jj) = ( zone - zindg ) * hsnif(ji,jj) + zindg * hicif(ji,jj) * ( rau0 - rhoic ) / rhosn dmgwi(ji,jj) = zindg * (1.0 - frld(ji,jj)) * rhoic * hicif(ji,jj) ! snow/ice mass ! the lead fraction, frld, must be little than or equal to amax (ice ridging). zthsnice = hsnif(ji,jj) + hicif(ji,jj) zindb = tms(ji,jj) * ( 1.0 - MAX( zzero , SIGN( zone , - zthsnice ) ) ) za = zindb * MIN( zone, ( 1.0 - frld(ji,jj) ) * uscomi ) hsnif (ji,jj) = hsnif(ji,jj) * za hicif (ji,jj) = hicif(ji,jj) * za qstoif(ji,jj) = qstoif(ji,jj) * za frld (ji,jj) = 1.0 - zindb * ( 1.0 - frld(ji,jj) ) / MAX( za , epsi20 ) ! the in situ ice thickness, hicif, must be equal to or greater than hiclim. zh = MAX( zone , zindb * hiclim / MAX( hicif(ji,jj) , epsi20 ) ) hsnif (ji,jj) = hsnif(ji,jj) * zh hicif (ji,jj) = hicif(ji,jj) * zh qstoif(ji,jj) = qstoif(ji,jj) * zh frld (ji,jj) = ( frld(ji,jj) + ( zh - 1.0 ) ) / zh END DO END DO IF(ln_ctl) THEN CALL prt_ctl(tab2d_1=hicif , clinfo1=' lim_thd: hicif : ') CALL prt_ctl(tab2d_1=hsnif , clinfo1=' lim_thd: hsnif : ') CALL prt_ctl(tab2d_1=dmgwi , clinfo1=' lim_thd: dmgwi : ') CALL prt_ctl(tab2d_1=qstoif , clinfo1=' lim_thd: qstoif : ') CALL prt_ctl(tab2d_1=frld , clinfo1=' lim_thd: frld : ') ENDIF !-------------------------------! ! Thermodynamics of sea ice ! !-------------------------------! ! Partial computation of forcing for the thermodynamic sea ice model. !-------------------------------------------------------------------------- sst_m(:,:) = sst_m(:,:) + rt0 !CDIR NOVERRCHK DO jj = 1, jpj !CDIR NOVERRCHK DO ji = 1, jpi zthsnice = hsnif(ji,jj) + hicif(ji,jj) zindb = tms(ji,jj) * ( 1.0 - MAX( zzero , SIGN( zone , - zthsnice ) ) ) pfrld(ji,jj) = frld(ji,jj) zinda = 1.0 - MAX( zzero , SIGN( zone , - ( 1.0 - pfrld(ji,jj) ) ) ) ! solar irradiance transmission at the mixed layer bottom and used in the lead heat budget thcm(ji,jj) = 0.e0 ! net downward heat flux from the ice to the ocean, expressed as a function of ocean ! temperature and turbulent mixing (McPhee, 1992) zfric_u = MAX ( MIN( SQRT( ust2s(ji,jj) ) , zfric_umax ) , zfric_umin ) ! friction velocity fdtcn(ji,jj) = zindb * rau0 * rcp * 0.006 * zfric_u * ( sst_m(ji,jj) - tfu(ji,jj) ) qdtcn(ji,jj) = zindb * fdtcn(ji,jj) * frld(ji,jj) * rdt_ice ! partial computation of the lead energy budget (qldif) zfontn = ( sprecip(ji,jj) / rhosn ) * xlsn ! energy for melting zfnsol = qns(ji,jj) ! total non solar flux over the ocean qldif(ji,jj) = tms(ji,jj) * ( qsr(ji,jj) * ( 1.0 - thcm(ji,jj) ) & & + zfnsol + fdtcn(ji,jj) - zfontn & & + ( 1.0 - zindb ) * fsbbq(ji,jj) ) & & * frld(ji,jj) * rdt_ice ! parlat : percentage of energy used for lateral ablation (0.0) zfntlat = 1.0 - MAX( zzero , SIGN( zone , - qldif(ji,jj) ) ) zpareff = 1.0 + ( parlat - 1.0 ) * zinda * zfntlat zqlbsbq(ji,jj) = qldif(ji,jj) * ( 1.0 - zpareff ) / MAX( (1.0 - frld(ji,jj)) * rdt_ice , epsi16 ) qldif (ji,jj) = zpareff * qldif(ji,jj) qdtcn (ji,jj) = zpareff * qdtcn(ji,jj) ! energy needed to bring ocean surface layer until its freezing qcmif (ji,jj) = rau0 * rcp * fse3t(ji,jj,1) * ( tfu(ji,jj) - sst_m(ji,jj) ) * ( 1 - zinda ) ! calculate oceanic heat flux. fbif (ji,jj) = zindb * ( fsbbq(ji,jj) / MAX( (1.0 - frld(ji,jj)) , epsi20 ) + fdtcn(ji,jj) ) ! computation of the daily thermodynamic ice production (only needed for output) zhicifp(ji,jj) = hicif(ji,jj) * ( 1.0 - frld(ji,jj) ) END DO END DO sst_m(:,:) = sst_m(:,:) - rt0 ! Select icy points and fulfill arrays for the vectorial grid. !---------------------------------------------------------------------- nbpb = 0 DO jj = 1, jpj DO ji = 1, jpi IF ( frld(ji,jj) < 1.0 ) THEN nbpb = nbpb + 1 npb(nbpb) = (jj - 1) * jpi + ji ENDIF END DO END DO IF(ln_ctl) THEN CALL prt_ctl(tab2d_1=pfrld, clinfo1=' lim_thd: pfrld : ', tab2d_2=thcm , clinfo2=' thcm : ') CALL prt_ctl(tab2d_1=fdtcn, clinfo1=' lim_thd: fdtcn : ', tab2d_2=qdtcn , clinfo2=' qdtcn : ') CALL prt_ctl(tab2d_1=qldif, clinfo1=' lim_thd: qldif : ', tab2d_2=zqlbsbq, clinfo2=' zqlbsbq : ') CALL prt_ctl(tab2d_1=qcmif, clinfo1=' lim_thd: qcmif : ', tab2d_2=fbif , clinfo2=' fbif : ') zmsk(:,:,1) = tms(:,:) CALL prt_ctl(tab2d_1=qcmif , clinfo1=' lim_thd: qcmif : ', mask1=zmsk) CALL prt_ctl(tab2d_1=zhicifp, clinfo1=' lim_thd: zhicifp : ') WRITE(charout, FMT="('lim_thd: nbpb = ',I4)") nbpb CALL prt_ctl_info(charout) ENDIF ! If there is no ice, do nothing. Otherwise, compute Top and Bottom accretion/ablation !------------------------------------------------------------------------------------ IF ( nbpb > 0) THEN ! put the variable in a 1-D array for thermodynamics process CALL tab_2d_1d_2( nbpb, frld_1d (1:nbpb) , frld , jpi, jpj, npb(1:nbpb) ) CALL tab_2d_1d_2( nbpb, h_ice_1d (1:nbpb) , hicif , jpi, jpj, npb(1:nbpb) ) CALL tab_2d_1d_2( nbpb, h_snow_1d (1:nbpb) , hsnif , jpi, jpj, npb(1:nbpb) ) CALL tab_2d_1d_2( nbpb, sist_1d (1:nbpb) , sist , jpi, jpj, npb(1:nbpb) ) CALL tab_2d_1d_2( nbpb, tbif_1d (1:nbpb , 1 ), tbif(:,:,1), jpi, jpj, npb(1:nbpb) ) CALL tab_2d_1d_2( nbpb, tbif_1d (1:nbpb , 2 ), tbif(:,:,2), jpi, jpj, npb(1:nbpb) ) CALL tab_2d_1d_2( nbpb, tbif_1d (1:nbpb , 3 ), tbif(:,:,3), jpi, jpj, npb(1:nbpb) ) CALL tab_2d_1d_2( nbpb, qsr_ice_1d (1:nbpb) , qsr_ice , jpi, jpj, npb(1:nbpb) ) CALL tab_2d_1d_2( nbpb, fr1_i0_1d (1:nbpb) , fr1_i0 , jpi, jpj, npb(1:nbpb) ) CALL tab_2d_1d_2( nbpb, fr2_i0_1d (1:nbpb) , fr2_i0 , jpi, jpj, npb(1:nbpb) ) CALL tab_2d_1d_2( nbpb, qns_ice_1d (1:nbpb) , qns_ice , jpi, jpj, npb(1:nbpb) ) #if ! defined key_coupled CALL tab_2d_1d_2( nbpb, qla_ice_1d (1:nbpb) , qla_ice , jpi, jpj, npb(1:nbpb) ) CALL tab_2d_1d_2( nbpb, dqla_ice_1d(1:nbpb) , dqla_ice , jpi, jpj, npb(1:nbpb) ) #endif CALL tab_2d_1d_2( nbpb, dqns_ice_1d(1:nbpb) , dqns_ice , jpi, jpj, npb(1:nbpb) ) CALL tab_2d_1d_2( nbpb, tfu_1d (1:nbpb) , tfu , jpi, jpj, npb(1:nbpb) ) CALL tab_2d_1d_2( nbpb, sprecip_1d (1:nbpb) , sprecip , jpi, jpj, npb(1:nbpb) ) CALL tab_2d_1d_2( nbpb, fbif_1d (1:nbpb) , fbif , jpi, jpj, npb(1:nbpb) ) CALL tab_2d_1d_2( nbpb, thcm_1d (1:nbpb) , thcm , jpi, jpj, npb(1:nbpb) ) CALL tab_2d_1d_2( nbpb, qldif_1d (1:nbpb) , qldif , jpi, jpj, npb(1:nbpb) ) CALL tab_2d_1d_2( nbpb, qstbif_1d (1:nbpb) , qstoif , jpi, jpj, npb(1:nbpb) ) CALL tab_2d_1d_2( nbpb, rdmicif_1d (1:nbpb) , rdmicif , jpi, jpj, npb(1:nbpb) ) CALL tab_2d_1d_2( nbpb, dmgwi_1d (1:nbpb) , dmgwi , jpi, jpj, npb(1:nbpb) ) CALL tab_2d_1d_2( nbpb, qlbbq_1d (1:nbpb) , zqlbsbq , jpi, jpj, npb(1:nbpb) ) CALL lim_thd_zdf_2( 1, nbpb ) ! compute ice growth ! back to the geographic grid. CALL tab_1d_2d_2( nbpb, frld , npb, frld_1d (1:nbpb) , jpi, jpj ) CALL tab_1d_2d_2( nbpb, hicif , npb, h_ice_1d (1:nbpb) , jpi, jpj ) CALL tab_1d_2d_2( nbpb, hsnif , npb, h_snow_1d (1:nbpb) , jpi, jpj ) CALL tab_1d_2d_2( nbpb, sist , npb, sist_1d (1:nbpb) , jpi, jpj ) CALL tab_1d_2d_2( nbpb, tbif(:,:,1), npb, tbif_1d (1:nbpb , 1 ), jpi, jpj ) CALL tab_1d_2d_2( nbpb, tbif(:,:,2), npb, tbif_1d (1:nbpb , 2 ), jpi, jpj ) CALL tab_1d_2d_2( nbpb, tbif(:,:,3), npb, tbif_1d (1:nbpb , 3 ), jpi, jpj ) CALL tab_1d_2d_2( nbpb, fscmbq , npb, fscbq_1d (1:nbpb) , jpi, jpj ) CALL tab_1d_2d_2( nbpb, ffltbif , npb, fltbif_1d (1:nbpb) , jpi, jpj ) CALL tab_1d_2d_2( nbpb, fstric , npb, fstbif_1d (1:nbpb) , jpi, jpj ) CALL tab_1d_2d_2( nbpb, qldif , npb, qldif_1d (1:nbpb) , jpi, jpj ) CALL tab_1d_2d_2( nbpb, qfvbq , npb, qfvbq_1d (1:nbpb) , jpi, jpj ) CALL tab_1d_2d_2( nbpb, qstoif , npb, qstbif_1d (1:nbpb) , jpi, jpj ) CALL tab_1d_2d_2( nbpb, rdmicif , npb, rdmicif_1d(1:nbpb) , jpi, jpj ) CALL tab_1d_2d_2( nbpb, dmgwi , npb, dmgwi_1d (1:nbpb) , jpi, jpj ) CALL tab_1d_2d_2( nbpb, rdmsnif , npb, rdmsnif_1d(1:nbpb) , jpi, jpj ) CALL tab_1d_2d_2( nbpb, rdvosif , npb, dvsbq_1d (1:nbpb) , jpi, jpj ) CALL tab_1d_2d_2( nbpb, rdvobif , npb, dvbbq_1d (1:nbpb) , jpi, jpj ) CALL tab_1d_2d_2( nbpb, fdvolif , npb, dvlbq_1d (1:nbpb) , jpi, jpj ) CALL tab_1d_2d_2( nbpb, rdvonif , npb, dvnbq_1d (1:nbpb) , jpi, jpj ) ENDIF ! Up-date sea ice thickness. !--------------------------------- DO jj = 1, jpj DO ji = 1, jpi phicif(ji,jj) = hicif(ji,jj) hicif(ji,jj) = hicif(ji,jj) * ( zone - MAX( zzero, SIGN( zone, - ( 1.0 - frld(ji,jj) ) ) ) ) END DO END DO ! Tricky trick : add 2 to frld in the Southern Hemisphere. !---------------------------------------------------------- IF( fcor(1,1) < 0.e0 ) THEN DO jj = 1, njeqm1 DO ji = 1, jpi frld(ji,jj) = frld(ji,jj) + 2.0 END DO END DO ENDIF ! Select points for lateral accretion (this occurs when heat exchange ! between ice and ocean is negative; ocean losing heat) !----------------------------------------------------------------- nbpac = 0 DO jj = 1, jpj DO ji = 1, jpi !i yes! IF ( ( qcmif(ji,jj) - qldif(ji,jj) ) > 0.e0 ) THEN IF ( tms(ji,jj) * ( qcmif(ji,jj) - qldif(ji,jj) ) > 0.e0 ) THEN nbpac = nbpac + 1 npac( nbpac ) = (jj - 1) * jpi + ji ENDIF END DO END DO IF(ln_ctl) THEN CALL prt_ctl(tab2d_1=phicif, clinfo1=' lim_thd: phicif : ', tab2d_2=hicif, clinfo2=' hicif : ') WRITE(charout, FMT="('lim_thd: nbpac = ',I4)") nbpac CALL prt_ctl_info(charout) ENDIF ! ! If ocean gains heat do nothing ; otherwise, one performs lateral accretion !-------------------------------------------------------------------------------- IF( nbpac > 0 ) THEN !...Put the variable in a 1-D array for lateral accretion CALL tab_2d_1d_2( nbpac, frld_1d (1:nbpac) , frld , jpi, jpj, npac(1:nbpac) ) CALL tab_2d_1d_2( nbpac, h_snow_1d (1:nbpac) , hsnif , jpi, jpj, npac(1:nbpac) ) CALL tab_2d_1d_2( nbpac, h_ice_1d (1:nbpac) , hicif , jpi, jpj, npac(1:nbpac) ) CALL tab_2d_1d_2( nbpac, tbif_1d (1:nbpac , 1 ), tbif(:,:,1), jpi, jpj, npac(1:nbpac) ) CALL tab_2d_1d_2( nbpac, tbif_1d (1:nbpac , 2 ), tbif(:,:,2), jpi, jpj, npac(1:nbpac) ) CALL tab_2d_1d_2( nbpac, tbif_1d (1:nbpac , 3 ), tbif(:,:,3), jpi, jpj, npac(1:nbpac) ) CALL tab_2d_1d_2( nbpac, qldif_1d (1:nbpac) , qldif , jpi, jpj, npac(1:nbpac) ) CALL tab_2d_1d_2( nbpac, qcmif_1d (1:nbpac) , qcmif , jpi, jpj, npac(1:nbpac) ) CALL tab_2d_1d_2( nbpac, qstbif_1d (1:nbpac) , qstoif , jpi, jpj, npac(1:nbpac) ) CALL tab_2d_1d_2( nbpac, rdmicif_1d(1:nbpac) , rdmicif , jpi, jpj, npac(1:nbpac) ) CALL tab_2d_1d_2( nbpac, dvlbq_1d (1:nbpac) , fdvolif , jpi, jpj, npac(1:nbpac) ) CALL tab_2d_1d_2( nbpac, tfu_1d (1:nbpac) , tfu , jpi, jpj, npac(1:nbpac) ) ! call lateral accretion routine. CALL lim_thd_lac_2( 1 , nbpac ) ! back to the geographic grid CALL tab_1d_2d_2( nbpac, frld , npac(1:nbpac), frld_1d (1:nbpac) , jpi, jpj ) CALL tab_1d_2d_2( nbpac, hsnif , npac(1:nbpac), h_snow_1d (1:nbpac) , jpi, jpj ) CALL tab_1d_2d_2( nbpac, hicif , npac(1:nbpac), h_ice_1d (1:nbpac) , jpi, jpj ) CALL tab_1d_2d_2( nbpac, tbif(:,:,1), npac(1:nbpac), tbif_1d (1:nbpac , 1 ), jpi, jpj ) CALL tab_1d_2d_2( nbpac, tbif(:,:,2), npac(1:nbpac), tbif_1d (1:nbpac , 2 ), jpi, jpj ) CALL tab_1d_2d_2( nbpac, tbif(:,:,3), npac(1:nbpac), tbif_1d (1:nbpac , 3 ), jpi, jpj ) CALL tab_1d_2d_2( nbpac, qstoif , npac(1:nbpac), qstbif_1d (1:nbpac) , jpi, jpj ) CALL tab_1d_2d_2( nbpac, rdmicif , npac(1:nbpac), rdmicif_1d(1:nbpac) , jpi, jpj ) CALL tab_1d_2d_2( nbpac, fdvolif , npac(1:nbpac), dvlbq_1d (1:nbpac) , jpi, jpj ) ENDIF ! Recover frld values between 0 and 1 in the Southern Hemisphere (tricky trick) ! Update daily thermodynamic ice production. !------------------------------------------------------------------------------ DO jj = 1, jpj DO ji = 1, jpi frld (ji,jj) = MIN( frld(ji,jj), ABS( frld(ji,jj) - 2.0 ) ) hicifp(ji,jj) = hicif(ji,jj) * ( 1.0 - frld(ji,jj) ) - zhicifp(ji,jj) + hicifp(ji,jj) END DO END DO IF(ln_ctl) THEN CALL prt_ctl_info(' lim_thd end ') CALL prt_ctl(tab2d_1=hicif , clinfo1=' lim_thd: hicif : ', tab2d_2=hsnif , clinfo2=' hsnif : ') CALL prt_ctl(tab2d_1=frld , clinfo1=' lim_thd: frld : ', tab2d_2=hicifp, clinfo2=' hicifp : ') CALL prt_ctl(tab2d_1=phicif, clinfo1=' lim_thd: phicif : ', tab2d_2=pfrld , clinfo2=' pfrld : ') CALL prt_ctl(tab2d_1=sist , clinfo1=' lim_thd: sist : ') CALL prt_ctl(tab2d_1=tbif(:,:,1), clinfo1=' lim_thd: tbif 1 : ') CALL prt_ctl(tab2d_1=tbif(:,:,2), clinfo1=' lim_thd: tbif 2 : ') CALL prt_ctl(tab2d_1=tbif(:,:,3), clinfo1=' lim_thd: tbif 3 : ') CALL prt_ctl(tab2d_1=fdtcn , clinfo1=' lim_thd: fdtcn : ', tab2d_2=qdtcn , clinfo2=' qdtcn : ') CALL prt_ctl(tab2d_1=qstoif, clinfo1=' lim_thd: qstoif : ', tab2d_2=fsbbq , clinfo2=' fsbbq : ') ENDIF ! END SUBROUTINE lim_thd_2 SUBROUTINE lim_thd_init_2 !!------------------------------------------------------------------- !! *** ROUTINE lim_thd_init_2 *** !! !! ** Purpose : Physical constants and parameters linked to the ice !! thermodynamics !! !! ** Method : Read the namicethd namelist and check the ice-thermo !! parameter values called at the first timestep (nit000) !! !! ** input : Namelist namicether !!------------------------------------------------------------------- NAMELIST/namicethd/ hmelt , hiccrit, hicmin, hiclim, amax , & & swiqst, sbeta , parlat, hakspl, hibspl, exld, & & hakdif, hnzst , thth , parsub, alphs !!------------------------------------------------------------------- ! Define the initial parameters ! ------------------------- REWIND( numnam_ice ) READ ( numnam_ice , namicethd ) IF(lwp) THEN WRITE(numout,*) WRITE(numout,*)'lim_thd_init_2: ice parameters for ice thermodynamic computation ' WRITE(numout,*)'~~~~~~~~~~~~~~' WRITE(numout,*)' maximum melting at the bottom hmelt = ', hmelt WRITE(numout,*)' ice thick. for lateral accretion in NH (SH) hiccrit(1/2) = ', hiccrit WRITE(numout,*)' ice thick. corr. to max. energy stored in brine pocket hicmin = ', hicmin WRITE(numout,*)' minimum ice thickness hiclim = ', hiclim WRITE(numout,*)' maximum lead fraction amax = ', amax WRITE(numout,*)' energy stored in brine pocket (=1) or not (=0) swiqst = ', swiqst WRITE(numout,*)' numerical carac. of the scheme for diffusion in ice ' WRITE(numout,*)' Cranck-Nicholson (=0.5), implicit (=1), explicit (=0) sbeta = ', sbeta WRITE(numout,*)' percentage of energy used for lateral ablation parlat = ', parlat WRITE(numout,*)' slope of distr. for Hakkinen-Mellor lateral melting hakspl = ', hakspl WRITE(numout,*)' slope of distribution for Hibler lateral melting hibspl = ', hibspl WRITE(numout,*)' exponent for leads-closure rate exld = ', exld WRITE(numout,*)' coefficient for diffusions of ice and snow hakdif = ', hakdif WRITE(numout,*)' threshold thick. for comp. of eq. thermal conductivity zhth = ', thth WRITE(numout,*)' thickness of the surf. layer in temp. computation hnzst = ', hnzst WRITE(numout,*)' switch for snow sublimation (=1) or not (=0) parsub = ', parsub WRITE(numout,*)' coefficient for snow density when snow ice formation alphs = ', alphs ENDIF uscomi = 1.0 / ( 1.0 - amax ) ! inverse of minimum lead fraction rcdsn = hakdif * rcdsn rcdic = hakdif * rcdic IF ( ( hsndif > 100.e0 ) .OR. ( hicdif > 100.e0 ) ) THEN cnscg = 0.e0 ELSE cnscg = rcpsn / rcpic ! ratio rcpsn/rcpic ENDIF END SUBROUTINE lim_thd_init_2 #else !!---------------------------------------------------------------------- !! Default option Dummy module NO LIM 2.0 sea-ice model !!---------------------------------------------------------------------- CONTAINS SUBROUTINE lim_thd_2 ! Dummy routine END SUBROUTINE lim_thd_2 #endif !!====================================================================== END MODULE limthd_2