MODULE ldftra !!====================================================================== !! *** MODULE ldftra *** !! Ocean physics: lateral diffusivity coefficients !!===================================================================== !! History : ! 1997-07 (G. Madec) from inimix.F split in 2 routines !! NEMO 1.0 ! 2002-09 (G. Madec) F90: Free form and module !! 2.0 ! 2005-11 (G. Madec) !! 3.7 ! 2013-12 (F. Lemarie, G. Madec) restructuration/simplification of aht/aeiv specification, !! ! add velocity dependent coefficient and optional read in file !!---------------------------------------------------------------------- !!---------------------------------------------------------------------- !! ldf_tra_init : initialization, namelist read, and parameters control !! ldf_tra : update lateral eddy diffusivity coefficients at each time step !! ldf_eiv_init : initialization of the eiv coeff. from namelist choices !! ldf_eiv : time evolution of the eiv coefficients (function of the growth rate of baroclinic instability) !! ldf_eiv_trp : add to the input ocean transport the contribution of the EIV parametrization !! ldf_eiv_dia : diagnose the eddy induced velocity from the eiv streamfunction !!---------------------------------------------------------------------- USE oce ! ocean dynamics and tracers USE dom_oce ! ocean space and time domain USE phycst ! physical constants USE ldfslp ! lateral diffusion: slope of iso-neutral surfaces USE ldfc1d_c2d ! lateral diffusion: 1D & 2D cases USE diaptr ! USE in_out_manager ! I/O manager USE iom ! I/O module for ehanced bottom friction file USE lib_mpp ! distribued memory computing library USE lbclnk ! ocean lateral boundary conditions (or mpp link) IMPLICIT NONE PRIVATE PUBLIC ldf_tra_init ! called by nemogcm.F90 PUBLIC ldf_tra ! called by step.F90 PUBLIC ldf_eiv_init ! called by nemogcm.F90 PUBLIC ldf_eiv ! called by step.F90 PUBLIC ldf_eiv_trp ! called by traadv.F90 PUBLIC ldf_eiv_dia ! called by traldf_iso and traldf_iso_triad.F90 ! !!* Namelist namtra_ldf : lateral mixing on tracers * ! != Operator type =! LOGICAL , PUBLIC :: ln_traldf_OFF !: no operator: No explicit diffusion LOGICAL , PUBLIC :: ln_traldf_lap !: laplacian operator LOGICAL , PUBLIC :: ln_traldf_blp !: bilaplacian operator ! != Direction of action =! LOGICAL , PUBLIC :: ln_traldf_lev !: iso-level direction LOGICAL , PUBLIC :: ln_traldf_hor !: horizontal (geopotential) direction ! LOGICAL , PUBLIC :: ln_traldf_iso !: iso-neutral direction (see ldfslp) ! != iso-neutral options =! ! LOGICAL , PUBLIC :: ln_traldf_triad !: griffies triad scheme (see ldfslp) LOGICAL , PUBLIC :: ln_traldf_msc !: Method of Stabilizing Correction ! LOGICAL , PUBLIC :: ln_triad_iso !: pure horizontal mixing in ML (see ldfslp) ! LOGICAL , PUBLIC :: ln_botmix_triad !: mixing on bottom (see ldfslp) ! REAL(wp), PUBLIC :: rn_sw_triad !: =1/0 switching triad / all 4 triads used (see ldfslp) ! REAL(wp), PUBLIC :: rn_slpmax !: slope limit (see ldfslp) ! != Coefficients =! INTEGER , PUBLIC :: nn_aht_ijk_t !: choice of time & space variations of the lateral eddy diffusivity coef. ! ! time invariant coefficients: aht_0 = 1/2 Ud*Ld (lap case) ! ! bht_0 = 1/12 Ud*Ld^3 (blp case) REAL(wp), PUBLIC :: rn_Ud !: lateral diffusive velocity [m/s] REAL(wp), PUBLIC :: rn_Ld !: lateral diffusive length [m] ! !!* Namelist namtra_eiv : eddy induced velocity param. * ! != Use/diagnose eiv =! LOGICAL , PUBLIC :: ln_ldfeiv !: eddy induced velocity flag LOGICAL , PUBLIC :: ln_ldfeiv_dia !: diagnose & output eiv streamfunction and velocity (IOM) ! != Coefficients =! INTEGER , PUBLIC :: nn_aei_ijk_t !: choice of time/space variation of the eiv coeff. REAL(wp), PUBLIC :: rn_Ue !: lateral diffusive velocity [m/s] REAL(wp), PUBLIC :: rn_Le !: lateral diffusive length [m] ! ! Flag to control the type of lateral diffusive operator INTEGER, PARAMETER, PUBLIC :: np_ERROR =-10 ! error in specification of lateral diffusion INTEGER, PARAMETER, PUBLIC :: np_no_ldf = 00 ! without operator (i.e. no lateral diffusive trend) ! !! laplacian ! bilaplacian ! INTEGER, PARAMETER, PUBLIC :: np_lap = 10 , np_blp = 20 ! iso-level operator INTEGER, PARAMETER, PUBLIC :: np_lap_i = 11 , np_blp_i = 21 ! standard iso-neutral or geopotential operator INTEGER, PARAMETER, PUBLIC :: np_lap_it = 12 , np_blp_it = 22 ! triad iso-neutral or geopotential operator INTEGER , PUBLIC :: nldf_tra = 0 !: type of lateral diffusion used defined from ln_traldf_... (namlist logicals) LOGICAL , PUBLIC :: l_ldftra_time = .FALSE. !: flag for time variation of the lateral eddy diffusivity coef. LOGICAL , PUBLIC :: l_ldfeiv_time = .FALSE. !: flag for time variation of the eiv coef. REAL(wp), PUBLIC, ALLOCATABLE, SAVE, DIMENSION(:,:,:) :: ahtu, ahtv !: eddy diffusivity coef. at U- and V-points [m2/s] REAL(wp), PUBLIC, ALLOCATABLE, SAVE, DIMENSION(:,:,:) :: aeiu, aeiv !: eddy induced velocity coeff. [m2/s] REAL(wp) :: aht0, aei0 ! constant eddy coefficients (deduced from namelist values) [m2/s] REAL(wp) :: r1_2 = 0.5_wp ! =1/2 REAL(wp) :: r1_4 = 0.25_wp ! =1/4 REAL(wp) :: r1_12 = 1._wp / 12._wp ! =1/12 !! * Substitutions # include "vectopt_loop_substitute.h90" !!---------------------------------------------------------------------- !! NEMO/OCE 4.0 , NEMO Consortium (2018) !! $Id$ !! Software governed by the CeCILL license (see ./LICENSE) !!---------------------------------------------------------------------- CONTAINS SUBROUTINE ldf_tra_init !!---------------------------------------------------------------------- !! *** ROUTINE ldf_tra_init *** !! !! ** Purpose : initializations of the tracer lateral mixing coeff. !! !! ** Method : * the eddy diffusivity coef. specification depends on: !! !! ln_traldf_lap = T laplacian operator !! ln_traldf_blp = T bilaplacian operator !! !! nn_aht_ijk_t = 0 => = constant !! ! !! = 10 => = F(z) : constant with a reduction of 1/4 with depth !! ! !! =-20 => = F(i,j) = shape read in 'eddy_diffusivity.nc' file !! = 20 = F(i,j) = F(e1,e2) or F(e1^3,e2^3) (lap or bilap case) !! = 21 = F(i,j,t) = F(growth rate of baroclinic instability) !! ! !! =-30 => = F(i,j,k) = shape read in 'eddy_diffusivity.nc' file !! = 30 = F(i,j,k) = 2D (case 20) + decrease with depth (case 10) !! = 31 = F(i,j,k,t) = F(local velocity) ( 1/2 |u|e laplacian operator !! or 1/12 |u|e^3 bilaplacian operator ) !! * initialisation of the eddy induced velocity coefficient by a call to ldf_eiv_init !! !! ** action : ahtu, ahtv initialized one for all or l_ldftra_time set to true !! aeiu, aeiv initialized one for all or l_ldfeiv_time set to true !!---------------------------------------------------------------------- INTEGER :: jk ! dummy loop indices INTEGER :: ioptio, ierr, inum, ios, inn ! local integer REAL(wp) :: zah_max, zUfac ! - - CHARACTER(len=5) :: cl_Units ! units (m2/s or m4/s) !! NAMELIST/namtra_ldf/ ln_traldf_OFF, ln_traldf_lap , ln_traldf_blp , & ! type of operator & ln_traldf_lev, ln_traldf_hor , ln_traldf_triad, & ! acting direction of the operator & ln_traldf_iso, ln_traldf_msc , rn_slpmax , & ! option for iso-neutral operator & ln_triad_iso , ln_botmix_triad, rn_sw_triad , & ! option for triad operator & nn_aht_ijk_t , rn_Ud , rn_Ld ! lateral eddy coefficient !!---------------------------------------------------------------------- ! IF(lwp) THEN ! control print WRITE(numout,*) WRITE(numout,*) 'ldf_tra_init : lateral tracer diffusion' WRITE(numout,*) '~~~~~~~~~~~~ ' ENDIF ! ! Choice of lateral tracer physics ! ================================= ! REWIND( numnam_ref ) ! Namelist namtra_ldf in reference namelist : Lateral physics on tracers READ ( numnam_ref, namtra_ldf, IOSTAT = ios, ERR = 901) 901 IF( ios /= 0 ) CALL ctl_nam ( ios , 'namtra_ldf in reference namelist' ) REWIND( numnam_cfg ) ! Namelist namtra_ldf in configuration namelist : Lateral physics on tracers READ ( numnam_cfg, namtra_ldf, IOSTAT = ios, ERR = 902 ) 902 IF( ios > 0 ) CALL ctl_nam ( ios , 'namtra_ldf in configuration namelist' ) IF(lwm) WRITE( numond, namtra_ldf ) ! IF(lwp) THEN ! control print WRITE(numout,*) ' Namelist : namtra_ldf --- lateral mixing parameters (type, direction, coefficients)' WRITE(numout,*) ' type :' WRITE(numout,*) ' no explicit diffusion ln_traldf_OFF = ', ln_traldf_OFF WRITE(numout,*) ' laplacian operator ln_traldf_lap = ', ln_traldf_lap WRITE(numout,*) ' bilaplacian operator ln_traldf_blp = ', ln_traldf_blp WRITE(numout,*) ' direction of action :' WRITE(numout,*) ' iso-level ln_traldf_lev = ', ln_traldf_lev WRITE(numout,*) ' horizontal (geopotential) ln_traldf_hor = ', ln_traldf_hor WRITE(numout,*) ' iso-neutral Madec operator ln_traldf_iso = ', ln_traldf_iso WRITE(numout,*) ' iso-neutral triad operator ln_traldf_triad = ', ln_traldf_triad WRITE(numout,*) ' use the Method of Stab. Correction ln_traldf_msc = ', ln_traldf_msc WRITE(numout,*) ' maximum isoppycnal slope rn_slpmax = ', rn_slpmax WRITE(numout,*) ' pure lateral mixing in ML ln_triad_iso = ', ln_triad_iso WRITE(numout,*) ' switching triad or not rn_sw_triad = ', rn_sw_triad WRITE(numout,*) ' lateral mixing on bottom ln_botmix_triad = ', ln_botmix_triad WRITE(numout,*) ' coefficients :' WRITE(numout,*) ' type of time-space variation nn_aht_ijk_t = ', nn_aht_ijk_t WRITE(numout,*) ' lateral diffusive velocity (if cst) rn_Ud = ', rn_Ud, ' m/s' WRITE(numout,*) ' lateral diffusive length (if cst) rn_Ld = ', rn_Ld, ' m' ENDIF ! ! ! Operator and its acting direction (set nldf_tra) ! ================================= ! nldf_tra = np_ERROR ioptio = 0 IF( ln_traldf_OFF ) THEN ; nldf_tra = np_no_ldf ; ioptio = ioptio + 1 ; ENDIF IF( ln_traldf_lap ) THEN ; ioptio = ioptio + 1 ; ENDIF IF( ln_traldf_blp ) THEN ; ioptio = ioptio + 1 ; ENDIF IF( ioptio /= 1 ) CALL ctl_stop( 'tra_ldf_init: use ONE of the 3 operator options (NONE/lap/blp)' ) ! IF( .NOT.ln_traldf_OFF ) THEN !== direction ==>> type of operator ==! ioptio = 0 IF( ln_traldf_lev ) ioptio = ioptio + 1 IF( ln_traldf_hor ) ioptio = ioptio + 1 IF( ln_traldf_iso ) ioptio = ioptio + 1 IF( ln_traldf_triad ) ioptio = ioptio + 1 IF( ioptio /= 1 ) CALL ctl_stop( 'tra_ldf_init: use ONE direction (level/hor/iso/triad)' ) ! ! ! defined the type of lateral diffusion from ln_traldf_... logicals ierr = 0 IF ( ln_traldf_lap ) THEN ! laplacian operator IF ( ln_zco ) THEN ! z-coordinate IF ( ln_traldf_lev ) nldf_tra = np_lap ! iso-level = horizontal (no rotation) IF ( ln_traldf_hor ) nldf_tra = np_lap ! iso-level = horizontal (no rotation) IF ( ln_traldf_iso ) nldf_tra = np_lap_i ! iso-neutral: standard ( rotation) IF ( ln_traldf_triad ) nldf_tra = np_lap_it ! iso-neutral: triad ( rotation) ENDIF IF ( ln_zps ) THEN ! z-coordinate with partial step IF ( ln_traldf_lev ) ierr = 1 ! iso-level not allowed IF ( ln_traldf_hor ) nldf_tra = np_lap ! horizontal (no rotation) IF ( ln_traldf_iso ) nldf_tra = np_lap_i ! iso-neutral: standard (rotation) IF ( ln_traldf_triad ) nldf_tra = np_lap_it ! iso-neutral: triad (rotation) ENDIF IF ( ln_sco ) THEN ! s-coordinate IF ( ln_traldf_lev ) nldf_tra = np_lap ! iso-level (no rotation) IF ( ln_traldf_hor ) nldf_tra = np_lap_i ! horizontal ( rotation) IF ( ln_traldf_iso ) nldf_tra = np_lap_i ! iso-neutral: standard ( rotation) IF ( ln_traldf_triad ) nldf_tra = np_lap_it ! iso-neutral: triad ( rotation) ENDIF ENDIF ! IF( ln_traldf_blp ) THEN ! bilaplacian operator IF ( ln_zco ) THEN ! z-coordinate IF ( ln_traldf_lev ) nldf_tra = np_blp ! iso-level = horizontal (no rotation) IF ( ln_traldf_hor ) nldf_tra = np_blp ! iso-level = horizontal (no rotation) IF ( ln_traldf_iso ) nldf_tra = np_blp_i ! iso-neutral: standard ( rotation) IF ( ln_traldf_triad ) nldf_tra = np_blp_it ! iso-neutral: triad ( rotation) ENDIF IF ( ln_zps ) THEN ! z-coordinate with partial step IF ( ln_traldf_lev ) ierr = 1 ! iso-level not allowed IF ( ln_traldf_hor ) nldf_tra = np_blp ! horizontal (no rotation) IF ( ln_traldf_iso ) nldf_tra = np_blp_i ! iso-neutral: standard ( rotation) IF ( ln_traldf_triad ) nldf_tra = np_blp_it ! iso-neutral: triad ( rotation) ENDIF IF ( ln_sco ) THEN ! s-coordinate IF ( ln_traldf_lev ) nldf_tra = np_blp ! iso-level (no rotation) IF ( ln_traldf_hor ) nldf_tra = np_blp_it ! horizontal ( rotation) IF ( ln_traldf_iso ) nldf_tra = np_blp_i ! iso-neutral: standard ( rotation) IF ( ln_traldf_triad ) nldf_tra = np_blp_it ! iso-neutral: triad ( rotation) ENDIF ENDIF IF ( ierr == 1 ) CALL ctl_stop( 'iso-level in z-partial step, not allowed' ) ENDIF ! IF( ln_ldfeiv .AND. .NOT.( ln_traldf_iso .OR. ln_traldf_triad ) ) & & CALL ctl_stop( 'ln_ldfeiv=T requires iso-neutral laplacian diffusion' ) IF( ln_isfcav .AND. ln_traldf_triad ) & & CALL ctl_stop( ' ice shelf cavity and traldf_triad not tested' ) ! IF( nldf_tra == np_lap_i .OR. nldf_tra == np_lap_it .OR. & & nldf_tra == np_blp_i .OR. nldf_tra == np_blp_it ) l_ldfslp = .TRUE. ! slope of neutral surfaces required ! IF( ln_traldf_blp .AND. ( ln_traldf_iso .OR. ln_traldf_triad) ) THEN ! iso-neutral bilaplacian need MSC IF( .NOT.ln_traldf_msc ) CALL ctl_stop( 'tra_ldf_init: iso-neutral bilaplacian requires ln_traldf_msc=.true.' ) ENDIF ! IF(lwp) THEN WRITE(numout,*) SELECT CASE( nldf_tra ) CASE( np_no_ldf ) ; WRITE(numout,*) ' ==>>> NO lateral diffusion' CASE( np_lap ) ; WRITE(numout,*) ' ==>>> laplacian iso-level operator' CASE( np_lap_i ) ; WRITE(numout,*) ' ==>>> Rotated laplacian operator (standard)' CASE( np_lap_it ) ; WRITE(numout,*) ' ==>>> Rotated laplacian operator (triad)' CASE( np_blp ) ; WRITE(numout,*) ' ==>>> bilaplacian iso-level operator' CASE( np_blp_i ) ; WRITE(numout,*) ' ==>>> Rotated bilaplacian operator (standard)' CASE( np_blp_it ) ; WRITE(numout,*) ' ==>>> Rotated bilaplacian operator (triad)' END SELECT WRITE(numout,*) ENDIF ! ! Space/time variation of eddy coefficients ! =========================================== ! l_ldftra_time = .FALSE. ! no time variation except in case defined below ! IF( ln_traldf_OFF ) THEN !== no explicit diffusive operator ==! ! IF(lwp) WRITE(numout,*) ' ==>>> No diffusive operator selected. ahtu and ahtv are not allocated' RETURN ! ELSE !== a lateral diffusion operator is used ==! ! ! ! allocate the aht arrays ALLOCATE( ahtu(jpi,jpj,jpk) , ahtv(jpi,jpj,jpk) , STAT=ierr ) IF( ierr /= 0 ) CALL ctl_stop( 'STOP', 'ldf_tra_init: failed to allocate arrays') ! ahtu(:,:,jpk) = 0._wp ! last level always 0 ahtv(:,:,jpk) = 0._wp !. ! ! value of lap/blp eddy mixing coef. IF( ln_traldf_lap ) THEN ; zUfac = r1_2 *rn_Ud ; inn = 1 ; cl_Units = ' m2/s' ! laplacian ELSEIF( ln_traldf_blp ) THEN ; zUfac = r1_12*rn_Ud ; inn = 3 ; cl_Units = ' m4/s' ! bilaplacian ENDIF aht0 = zUfac * rn_Ld**inn ! mixing coefficient zah_max = zUfac * (ra*rad)**inn ! maximum reachable coefficient (value at the Equator for e1=1 degree) ! ! SELECT CASE( nn_aht_ijk_t ) !* Specification of space-time variations of ahtu, ahtv ! CASE( 0 ) !== constant ==! IF(lwp) WRITE(numout,*) ' ==>>> eddy diffusivity = constant = ', aht0, cl_Units ahtu(:,:,1:jpkm1) = aht0 ahtv(:,:,1:jpkm1) = aht0 ! CASE( 10 ) !== fixed profile ==! IF(lwp) WRITE(numout,*) ' ==>>> eddy diffusivity = F( depth )' IF(lwp) WRITE(numout,*) ' surface eddy diffusivity = constant = ', aht0, cl_Units ahtu(:,:,1) = aht0 ! constant surface value ahtv(:,:,1) = aht0 CALL ldf_c1d( 'TRA', ahtu(:,:,1), ahtv(:,:,1), ahtu, ahtv ) ! CASE ( -20 ) !== fixed horizontal shape and magnitude read in file ==! IF(lwp) WRITE(numout,*) ' ==>>> eddy diffusivity = F(i,j) read in eddy_diffusivity.nc file' CALL iom_open( 'eddy_diffusivity_2D.nc', inum ) CALL iom_get ( inum, jpdom_data, 'ahtu_2D', ahtu(:,:,1) ) CALL iom_get ( inum, jpdom_data, 'ahtv_2D', ahtv(:,:,1) ) CALL iom_close( inum ) DO jk = 2, jpkm1 ahtu(:,:,jk) = ahtu(:,:,1) ahtv(:,:,jk) = ahtv(:,:,1) END DO ! CASE( 20 ) !== fixed horizontal shape ==! IF(lwp) WRITE(numout,*) ' ==>>> eddy diffusivity = F( e1, e2 ) or F( e1^3, e2^3 ) (lap or blp case)' IF(lwp) WRITE(numout,*) ' using a fixed diffusive velocity = ', rn_Ud,' m/s and Ld = Max(e1,e2)' IF(lwp) WRITE(numout,*) ' maximum reachable coefficient (at the Equator) = ', zah_max, cl_Units, ' for e1=1°)' CALL ldf_c2d( 'TRA', zUfac , inn , ahtu, ahtv ) ! value proportional to scale factor^inn ! CASE( 21 ) !== time varying 2D field ==! IF(lwp) WRITE(numout,*) ' ==>>> eddy diffusivity = F( latitude, longitude, time )' IF(lwp) WRITE(numout,*) ' = F( growth rate of baroclinic instability )' IF(lwp) WRITE(numout,*) ' min value = 0.2 * aht0 (with aht0= 1/2 rn_Ud*rn_Ld)' IF(lwp) WRITE(numout,*) ' max value = aei0 (with aei0=1/2 rn_Ue*Le increased to aht0 within 20N-20S' ! l_ldftra_time = .TRUE. ! will be calculated by call to ldf_tra routine in step.F90 ! IF( ln_traldf_blp ) CALL ctl_stop( 'ldf_tra_init: aht=F( growth rate of baroc. insta .)', & & ' incompatible with bilaplacian operator' ) ! CASE( -30 ) !== fixed 3D shape read in file ==! IF(lwp) WRITE(numout,*) ' ==>>> eddy diffusivity = F(i,j,k) read in eddy_diffusivity.nc file' CALL iom_open( 'eddy_diffusivity_3D.nc', inum ) CALL iom_get ( inum, jpdom_data, 'ahtu_3D', ahtu ) CALL iom_get ( inum, jpdom_data, 'ahtv_3D', ahtv ) CALL iom_close( inum ) ! CASE( 30 ) !== fixed 3D shape ==! IF(lwp) WRITE(numout,*) ' ==>>> eddy diffusivity = F( latitude, longitude, depth )' IF(lwp) WRITE(numout,*) ' using a fixed diffusive velocity = ', rn_Ud,' m/s and Ld = Max(e1,e2)' IF(lwp) WRITE(numout,*) ' maximum reachable coefficient (at the Equator) = ', zah_max, cl_Units, ' for e1=1°)' CALL ldf_c2d( 'TRA', zUfac , inn , ahtu, ahtv ) ! surface value proportional to scale factor^inn CALL ldf_c1d( 'TRA', ahtu(:,:,1), ahtv(:,:,1), ahtu, ahtv ) ! reduction with depth ! CASE( 31 ) !== time varying 3D field ==! IF(lwp) WRITE(numout,*) ' ==>>> eddy diffusivity = F( latitude, longitude, depth , time )' IF(lwp) WRITE(numout,*) ' proportional to the velocity : 1/2 |u|e or 1/12 |u|e^3' ! l_ldftra_time = .TRUE. ! will be calculated by call to ldf_tra routine in step.F90 ! CASE DEFAULT CALL ctl_stop('ldf_tra_init: wrong choice for nn_aht_ijk_t, the type of space-time variation of aht') END SELECT ! IF( .NOT.l_ldftra_time ) THEN !* No time variation IF( ln_traldf_lap ) THEN ! laplacian operator (mask only) ahtu(:,:,1:jpkm1) = ahtu(:,:,1:jpkm1) * umask(:,:,1:jpkm1) ahtv(:,:,1:jpkm1) = ahtv(:,:,1:jpkm1) * vmask(:,:,1:jpkm1) ELSEIF( ln_traldf_blp ) THEN ! bilaplacian operator (square root + mask) ahtu(:,:,1:jpkm1) = SQRT( ahtu(:,:,1:jpkm1) ) * umask(:,:,1:jpkm1) ahtv(:,:,1:jpkm1) = SQRT( ahtv(:,:,1:jpkm1) ) * vmask(:,:,1:jpkm1) ENDIF ENDIF ! ENDIF ! END SUBROUTINE ldf_tra_init SUBROUTINE ldf_tra( kt ) !!---------------------------------------------------------------------- !! *** ROUTINE ldf_tra *** !! !! ** Purpose : update at kt the tracer lateral mixing coeff. (aht and aeiv) !! !! ** Method : * time varying eddy diffusivity coefficients: !! !! nn_aei_ijk_t = 21 aeiu, aeiv = F(i,j, t) = F(growth rate of baroclinic instability) !! with a reduction to 0 in vicinity of the Equator !! nn_aht_ijk_t = 21 ahtu, ahtv = F(i,j, t) = F(growth rate of baroclinic instability) !! !! = 31 ahtu, ahtv = F(i,j,k,t) = F(local velocity) ( |u|e /12 laplacian operator !! or |u|e^3/12 bilaplacian operator ) !! !! * time varying EIV coefficients: call to ldf_eiv routine !! !! ** action : ahtu, ahtv update at each time step !! aeiu, aeiv - - - - (if ln_ldfeiv=T) !!---------------------------------------------------------------------- INTEGER, INTENT(in) :: kt ! time step ! INTEGER :: ji, jj, jk ! dummy loop indices REAL(wp) :: zaht, zahf, zaht_min, zDaht, z1_f20 ! local scalar !!---------------------------------------------------------------------- ! IF( ln_ldfeiv .AND. nn_aei_ijk_t == 21 ) THEN ! eddy induced velocity coefficients ! ! =F(growth rate of baroclinic instability) ! ! max value aeiv_0 ; decreased to 0 within 20N-20S CALL ldf_eiv( kt, aei0, aeiu, aeiv ) ENDIF ! SELECT CASE( nn_aht_ijk_t ) ! Eddy diffusivity coefficients ! CASE( 21 ) !== time varying 2D field ==! = F( growth rate of baroclinic instability ) ! ! min value 0.2*aht0 ! ! max value aht0 (aei0 if nn_aei_ijk_t=21) ! ! increase to aht0 within 20N-20S IF( ln_ldfeiv .AND. nn_aei_ijk_t == 21 ) THEN ! use the already computed aei. ahtu(:,:,1) = aeiu(:,:,1) ahtv(:,:,1) = aeiv(:,:,1) ELSE ! compute aht. CALL ldf_eiv( kt, aht0, ahtu, ahtv ) ENDIF ! z1_f20 = 1._wp / ( 2._wp * omega * SIN( rad * 20._wp ) ) ! 1 / ff(20 degrees) zaht_min = 0.2_wp * aht0 ! minimum value for aht zDaht = aht0 - zaht_min DO jj = 1, jpj DO ji = 1, jpi !!gm CAUTION : here we assume lat/lon grid in 20deg N/S band (like all ORCA cfg) !! ==>>> The Coriolis value is identical for t- & u_points, and for v- and f-points zaht = ( 1._wp - MIN( 1._wp , ABS( ff_t(ji,jj) * z1_f20 ) ) ) * zDaht zahf = ( 1._wp - MIN( 1._wp , ABS( ff_f(ji,jj) * z1_f20 ) ) ) * zDaht ahtu(ji,jj,1) = ( MAX( zaht_min, ahtu(ji,jj,1) ) + zaht ) ! min value zaht_min ahtv(ji,jj,1) = ( MAX( zaht_min, ahtv(ji,jj,1) ) + zahf ) ! increase within 20S-20N END DO END DO DO jk = 1, jpkm1 ! deeper value = surface value + mask for all levels ahtu(:,:,jk) = ahtu(:,:,1) * umask(:,:,jk) ahtv(:,:,jk) = ahtv(:,:,1) * vmask(:,:,jk) END DO ! CASE( 31 ) !== time varying 3D field ==! = F( local velocity ) IF( ln_traldf_lap ) THEN ! laplacian operator |u| e /12 DO jk = 1, jpkm1 ahtu(:,:,jk) = ABS( ub(:,:,jk) ) * e1u(:,:) * r1_12 ! n.b. ub,vb are masked ahtv(:,:,jk) = ABS( vb(:,:,jk) ) * e2v(:,:) * r1_12 END DO ELSEIF( ln_traldf_blp ) THEN ! bilaplacian operator sqrt( |u| e^3 /12 ) = sqrt( |u| e /12 ) * e DO jk = 1, jpkm1 ahtu(:,:,jk) = SQRT( ABS( ub(:,:,jk) ) * e1u(:,:) * r1_12 ) * e1u(:,:) ahtv(:,:,jk) = SQRT( ABS( vb(:,:,jk) ) * e2v(:,:) * r1_12 ) * e2v(:,:) END DO ENDIF ! END SELECT ! CALL iom_put( "ahtu_2d", ahtu(:,:,1) ) ! surface u-eddy diffusivity coeff. CALL iom_put( "ahtv_2d", ahtv(:,:,1) ) ! surface v-eddy diffusivity coeff. CALL iom_put( "ahtu_3d", ahtu(:,:,:) ) ! 3D u-eddy diffusivity coeff. CALL iom_put( "ahtv_3d", ahtv(:,:,:) ) ! 3D v-eddy diffusivity coeff. ! IF( ln_ldfeiv ) THEN CALL iom_put( "aeiu_2d", aeiu(:,:,1) ) ! surface u-EIV coeff. CALL iom_put( "aeiv_2d", aeiv(:,:,1) ) ! surface v-EIV coeff. CALL iom_put( "aeiu_3d", aeiu(:,:,:) ) ! 3D u-EIV coeff. CALL iom_put( "aeiv_3d", aeiv(:,:,:) ) ! 3D v-EIV coeff. ENDIF ! END SUBROUTINE ldf_tra SUBROUTINE ldf_eiv_init !!---------------------------------------------------------------------- !! *** ROUTINE ldf_eiv_init *** !! !! ** Purpose : initialization of the eiv coeff. from namelist choices. !! !! ** Method : the eiv diffusivity coef. specification depends on: !! nn_aei_ijk_t = 0 => = constant !! ! !! = 10 => = F(z) : constant with a reduction of 1/4 with depth !! ! !! =-20 => = F(i,j) = shape read in 'eddy_diffusivity.nc' file !! = 20 = F(i,j) = F(e1,e2) or F(e1^3,e2^3) (lap or bilap case) !! = 21 = F(i,j,t) = F(growth rate of baroclinic instability) !! ! !! =-30 => = F(i,j,k) = shape read in 'eddy_diffusivity.nc' file !! = 30 = F(i,j,k) = 2D (case 20) + decrease with depth (case 10) !! !! ** Action : aeiu , aeiv : initialized one for all or l_ldftra_time set to true !! l_ldfeiv_time : =T if EIV coefficients vary with time !!---------------------------------------------------------------------- INTEGER :: jk ! dummy loop indices INTEGER :: ierr, inum, ios, inn ! local integer REAL(wp) :: zah_max, zUfac ! - scalar !! NAMELIST/namtra_eiv/ ln_ldfeiv , ln_ldfeiv_dia, & ! eddy induced velocity (eiv) & nn_aei_ijk_t, rn_Ue, rn_Le ! eiv coefficient !!---------------------------------------------------------------------- ! IF(lwp) THEN ! control print WRITE(numout,*) WRITE(numout,*) 'ldf_eiv_init : eddy induced velocity parametrization' WRITE(numout,*) '~~~~~~~~~~~~ ' ENDIF ! REWIND( numnam_ref ) ! Namelist namtra_eiv in reference namelist : eddy induced velocity param. READ ( numnam_ref, namtra_eiv, IOSTAT = ios, ERR = 901) 901 IF( ios /= 0 ) CALL ctl_nam ( ios , 'namtra_eiv in reference namelist' ) ! REWIND( numnam_cfg ) ! Namelist namtra_eiv in configuration namelist : eddy induced velocity param. READ ( numnam_cfg, namtra_eiv, IOSTAT = ios, ERR = 902 ) 902 IF( ios > 0 ) CALL ctl_nam ( ios , 'namtra_eiv in configuration namelist' ) IF(lwm) WRITE ( numond, namtra_eiv ) IF(lwp) THEN ! control print WRITE(numout,*) ' Namelist namtra_eiv : ' WRITE(numout,*) ' Eddy Induced Velocity (eiv) param. ln_ldfeiv = ', ln_ldfeiv WRITE(numout,*) ' eiv streamfunction & velocity diag. ln_ldfeiv_dia = ', ln_ldfeiv_dia WRITE(numout,*) ' coefficients :' WRITE(numout,*) ' type of time-space variation nn_aei_ijk_t = ', nn_aht_ijk_t WRITE(numout,*) ' lateral diffusive velocity (if cst) rn_Ue = ', rn_Ue, ' m/s' WRITE(numout,*) ' lateral diffusive length (if cst) rn_Le = ', rn_Le, ' m' WRITE(numout,*) ENDIF ! l_ldfeiv_time = .FALSE. ! no time variation except in case defined below ! ! IF( .NOT.ln_ldfeiv ) THEN !== Parametrization not used ==! ! IF(lwp) WRITE(numout,*) ' ==>>> eddy induced velocity param is NOT used' ln_ldfeiv_dia = .FALSE. ! ELSE !== use the parametrization ==! ! IF(lwp) WRITE(numout,*) ' ==>>> use eddy induced velocity parametrization' IF(lwp) WRITE(numout,*) ! IF( ln_traldf_blp ) CALL ctl_stop( 'ldf_eiv_init: eddy induced velocity ONLY with laplacian diffusivity' ) ! ! != allocate the aei arrays ALLOCATE( aeiu(jpi,jpj,jpk), aeiv(jpi,jpj,jpk), STAT=ierr ) IF( ierr /= 0 ) CALL ctl_stop('STOP', 'ldf_eiv: failed to allocate arrays') ! ! != Specification of space-time variations of eaiu, aeiv ! aeiu(:,:,jpk) = 0._wp ! last level always 0 aeiv(:,:,jpk) = 0._wp ! ! value of EIV coef. (laplacian operator) zUfac = r1_2 *rn_Ue ! velocity factor inn = 1 ! L-exponent aei0 = zUfac * rn_Le**inn ! mixing coefficient zah_max = zUfac * (ra*rad)**inn ! maximum reachable coefficient (value at the Equator) SELECT CASE( nn_aei_ijk_t ) !* Specification of space-time variations ! CASE( 0 ) !-- constant --! IF(lwp) WRITE(numout,*) ' ==>>> eddy induced velocity coef. = constant = ', aei0, ' m2/s' aeiu(:,:,1:jpkm1) = aei0 aeiv(:,:,1:jpkm1) = aei0 ! CASE( 10 ) !-- fixed profile --! IF(lwp) WRITE(numout,*) ' ==>>> eddy induced velocity coef. = F( depth )' IF(lwp) WRITE(numout,*) ' surface eddy diffusivity = constant = ', aht0, ' m2/s' aeiu(:,:,1) = aei0 ! constant surface value aeiv(:,:,1) = aei0 CALL ldf_c1d( 'TRA', aeiu(:,:,1), aeiv(:,:,1), aeiu, aeiv ) ! CASE ( -20 ) !-- fixed horizontal shape read in file --! IF(lwp) WRITE(numout,*) ' ==>>> eddy induced velocity coef. = F(i,j) read in eddy_diffusivity_2D.nc file' CALL iom_open ( 'eddy_induced_velocity_2D.nc', inum ) CALL iom_get ( inum, jpdom_data, 'aeiu', aeiu(:,:,1) ) CALL iom_get ( inum, jpdom_data, 'aeiv', aeiv(:,:,1) ) CALL iom_close( inum ) DO jk = 2, jpkm1 aeiu(:,:,jk) = aeiu(:,:,1) aeiv(:,:,jk) = aeiv(:,:,1) END DO ! CASE( 20 ) !-- fixed horizontal shape --! IF(lwp) WRITE(numout,*) ' ==>>> eddy induced velocity coef. = F( e1, e2 )' IF(lwp) WRITE(numout,*) ' using a fixed diffusive velocity = ', rn_Ue, ' m/s and Le = Max(e1,e2)' IF(lwp) WRITE(numout,*) ' maximum reachable coefficient (at the Equator) = ', zah_max, ' m2/s for e1=1°)' CALL ldf_c2d( 'TRA', zUfac , inn , aeiu, aeiv ) ! value proportional to scale factor^inn ! CASE( 21 ) !-- time varying 2D field --! IF(lwp) WRITE(numout,*) ' ==>>> eddy induced velocity coef. = F( latitude, longitude, time )' IF(lwp) WRITE(numout,*) ' = F( growth rate of baroclinic instability )' IF(lwp) WRITE(numout,*) ' maximum allowed value: aei0 = ', aei0, ' m2/s' ! l_ldfeiv_time = .TRUE. ! will be calculated by call to ldf_tra routine in step.F90 ! CASE( -30 ) !-- fixed 3D shape read in file --! IF(lwp) WRITE(numout,*) ' ==>>> eddy induced velocity coef. = F(i,j,k) read in eddy_diffusivity_3D.nc file' CALL iom_open ( 'eddy_induced_velocity_3D.nc', inum ) CALL iom_get ( inum, jpdom_data, 'aeiu', aeiu ) CALL iom_get ( inum, jpdom_data, 'aeiv', aeiv ) CALL iom_close( inum ) ! CASE( 30 ) !-- fixed 3D shape --! IF(lwp) WRITE(numout,*) ' ==>>> eddy induced velocity coef. = F( latitude, longitude, depth )' CALL ldf_c2d( 'TRA', zUfac , inn , aeiu, aeiv ) ! surface value proportional to scale factor^inn CALL ldf_c1d( 'TRA', aeiu(:,:,1), aeiv(:,:,1), aeiu, aeiv ) ! reduction with depth ! CASE DEFAULT CALL ctl_stop('ldf_tra_init: wrong choice for nn_aei_ijk_t, the type of space-time variation of aei') END SELECT ! IF( .NOT.l_ldfeiv_time ) THEN !* mask if No time variation DO jk = 1, jpkm1 aeiu(:,:,jk) = aeiu(:,:,jk) * umask(:,:,jk) ahtv(:,:,jk) = ahtv(:,:,jk) * vmask(:,:,jk) END DO ENDIF ! ENDIF ! END SUBROUTINE ldf_eiv_init SUBROUTINE ldf_eiv( kt, paei0, paeiu, paeiv ) !!---------------------------------------------------------------------- !! *** ROUTINE ldf_eiv *** !! !! ** Purpose : Compute the eddy induced velocity coefficient from the !! growth rate of baroclinic instability. !! !! ** Method : coefficient function of the growth rate of baroclinic instability !! !! Reference : Treguier et al. JPO 1997 ; Held and Larichev JAS 1996 !!---------------------------------------------------------------------- INTEGER , INTENT(in ) :: kt ! ocean time-step index REAL(wp) , INTENT(inout) :: paei0 ! max value [m2/s] REAL(wp), DIMENSION(jpi,jpj,jpk), INTENT(inout) :: paeiu, paeiv ! eiv coefficient [m2/s] ! INTEGER :: ji, jj, jk ! dummy loop indices REAL(wp) :: zfw, ze3w, zn2, z1_f20, zaht, zaht_min, zzaei ! local scalars REAL(wp), DIMENSION(jpi,jpj) :: zn, zah, zhw, zRo, zaeiw ! 2D workspace !!---------------------------------------------------------------------- ! zn (:,:) = 0._wp ! Local initialization zhw(:,:) = 5._wp zah(:,:) = 0._wp zRo(:,:) = 0._wp ! ! Compute lateral diffusive coefficient at T-point IF( ln_traldf_triad ) THEN DO jk = 1, jpk DO jj = 2, jpjm1 DO ji = 2, jpim1 ! Take the max of N^2 and zero then take the vertical sum ! of the square root of the resulting N^2 ( required to compute ! internal Rossby radius Ro = .5 * sum_jpk(N) / f zn2 = MAX( rn2b(ji,jj,jk), 0._wp ) zn(ji,jj) = zn(ji,jj) + SQRT( zn2 ) * e3w_n(ji,jj,jk) ! Compute elements required for the inverse time scale of baroclinic ! eddies using the isopycnal slopes calculated in ldfslp.F : ! T^-1 = sqrt(m_jpk(N^2*(r1^2+r2^2)*e3w)) ze3w = e3w_n(ji,jj,jk) * tmask(ji,jj,jk) zah(ji,jj) = zah(ji,jj) + zn2 * wslp2(ji,jj,jk) * ze3w zhw(ji,jj) = zhw(ji,jj) + ze3w END DO END DO END DO ELSE DO jk = 1, jpk DO jj = 2, jpjm1 DO ji = 2, jpim1 ! Take the max of N^2 and zero then take the vertical sum ! of the square root of the resulting N^2 ( required to compute ! internal Rossby radius Ro = .5 * sum_jpk(N) / f zn2 = MAX( rn2b(ji,jj,jk), 0._wp ) zn(ji,jj) = zn(ji,jj) + SQRT( zn2 ) * e3w_n(ji,jj,jk) ! Compute elements required for the inverse time scale of baroclinic ! eddies using the isopycnal slopes calculated in ldfslp.F : ! T^-1 = sqrt(m_jpk(N^2*(r1^2+r2^2)*e3w)) ze3w = e3w_n(ji,jj,jk) * tmask(ji,jj,jk) zah(ji,jj) = zah(ji,jj) + zn2 * ( wslpi(ji,jj,jk) * wslpi(ji,jj,jk) & & + wslpj(ji,jj,jk) * wslpj(ji,jj,jk) ) * ze3w zhw(ji,jj) = zhw(ji,jj) + ze3w END DO END DO END DO ENDIF DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. zfw = MAX( ABS( 2. * omega * SIN( rad * gphit(ji,jj) ) ) , 1.e-10 ) ! Rossby radius at w-point taken betwenn 2 km and 40km zRo(ji,jj) = MAX( 2.e3 , MIN( .4 * zn(ji,jj) / zfw, 40.e3 ) ) ! Compute aeiw by multiplying Ro^2 and T^-1 zaeiw(ji,jj) = zRo(ji,jj) * zRo(ji,jj) * SQRT( zah(ji,jj) / zhw(ji,jj) ) * tmask(ji,jj,1) END DO END DO ! !== Bound on eiv coeff. ==! z1_f20 = 1._wp / ( 2._wp * omega * sin( rad * 20._wp ) ) DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. zzaei = MIN( 1._wp, ABS( ff_t(ji,jj) * z1_f20 ) ) * zaeiw(ji,jj) ! tropical decrease zaeiw(ji,jj) = MIN( zzaei , paei0 ) ! Max value = paei0 END DO END DO CALL lbc_lnk( 'ldftra', zaeiw(:,:), 'W', 1. ) ! lateral boundary condition ! DO jj = 2, jpjm1 !== aei at u- and v-points ==! DO ji = fs_2, fs_jpim1 ! vector opt. paeiu(ji,jj,1) = 0.5_wp * ( zaeiw(ji,jj) + zaeiw(ji+1,jj ) ) * umask(ji,jj,1) paeiv(ji,jj,1) = 0.5_wp * ( zaeiw(ji,jj) + zaeiw(ji ,jj+1) ) * vmask(ji,jj,1) END DO END DO CALL lbc_lnk_multi( 'ldftra', paeiu(:,:,1), 'U', 1. , paeiv(:,:,1), 'V', 1. ) ! lateral boundary condition DO jk = 2, jpkm1 !== deeper values equal the surface one ==! paeiu(:,:,jk) = paeiu(:,:,1) * umask(:,:,jk) paeiv(:,:,jk) = paeiv(:,:,1) * vmask(:,:,jk) END DO ! END SUBROUTINE ldf_eiv SUBROUTINE ldf_eiv_trp( kt, kit000, pun, pvn, pwn, cdtype ) !!---------------------------------------------------------------------- !! *** ROUTINE ldf_eiv_trp *** !! !! ** Purpose : add to the input ocean transport the contribution of !! the eddy induced velocity parametrization. !! !! ** Method : The eddy induced transport is computed from a flux stream- !! function which depends on the slope of iso-neutral surfaces !! (see ldf_slp). For example, in the i-k plan : !! psi_uw = mk(aeiu) e2u mi(wslpi) [in m3/s] !! Utr_eiv = - dk[psi_uw] !! Vtr_eiv = + di[psi_uw] !! ln_ldfeiv_dia = T : output the associated streamfunction, !! velocity and heat transport (call ldf_eiv_dia) !! !! ** Action : pun, pvn increased by the eiv transport !!---------------------------------------------------------------------- INTEGER , INTENT(in ) :: kt ! ocean time-step index INTEGER , INTENT(in ) :: kit000 ! first time step index CHARACTER(len=3) , INTENT(in ) :: cdtype ! =TRA or TRC (tracer indicator) REAL(wp), DIMENSION(jpi,jpj,jpk), INTENT(inout) :: pun ! in : 3 ocean transport components [m3/s] REAL(wp), DIMENSION(jpi,jpj,jpk), INTENT(inout) :: pvn ! out: 3 ocean transport components [m3/s] REAL(wp), DIMENSION(jpi,jpj,jpk), INTENT(inout) :: pwn ! increased by the eiv [m3/s] !! INTEGER :: ji, jj, jk ! dummy loop indices REAL(wp) :: zuwk, zuwk1, zuwi, zuwi1 ! local scalars REAL(wp) :: zvwk, zvwk1, zvwj, zvwj1 ! - - REAL(wp), DIMENSION(jpi,jpj,jpk) :: zpsi_uw, zpsi_vw !!---------------------------------------------------------------------- ! IF( kt == kit000 ) THEN IF(lwp) WRITE(numout,*) IF(lwp) WRITE(numout,*) 'ldf_eiv_trp : eddy induced advection on ', cdtype,' :' IF(lwp) WRITE(numout,*) '~~~~~~~~~~~ add to velocity fields the eiv component' ENDIF zpsi_uw(:,:, 1 ) = 0._wp ; zpsi_vw(:,:, 1 ) = 0._wp zpsi_uw(:,:,jpk) = 0._wp ; zpsi_vw(:,:,jpk) = 0._wp ! DO jk = 2, jpkm1 DO jj = 1, jpjm1 DO ji = 1, fs_jpim1 ! vector opt. zpsi_uw(ji,jj,jk) = - r1_4 * e2u(ji,jj) * ( wslpi(ji,jj,jk ) + wslpi(ji+1,jj,jk) ) & & * ( aeiu (ji,jj,jk-1) + aeiu (ji ,jj,jk) ) * umask(ji,jj,jk) zpsi_vw(ji,jj,jk) = - r1_4 * e1v(ji,jj) * ( wslpj(ji,jj,jk ) + wslpj(ji,jj+1,jk) ) & & * ( aeiv (ji,jj,jk-1) + aeiv (ji,jj ,jk) ) * vmask(ji,jj,jk) END DO END DO END DO ! DO jk = 1, jpkm1 DO jj = 1, jpjm1 DO ji = 1, fs_jpim1 ! vector opt. pun(ji,jj,jk) = pun(ji,jj,jk) - ( zpsi_uw(ji,jj,jk) - zpsi_uw(ji,jj,jk+1) ) pvn(ji,jj,jk) = pvn(ji,jj,jk) - ( zpsi_vw(ji,jj,jk) - zpsi_vw(ji,jj,jk+1) ) END DO END DO END DO DO jk = 1, jpkm1 DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. pwn(ji,jj,jk) = pwn(ji,jj,jk) + ( zpsi_uw(ji,jj,jk) - zpsi_uw(ji-1,jj ,jk) & & + zpsi_vw(ji,jj,jk) - zpsi_vw(ji ,jj-1,jk) ) END DO END DO END DO ! ! ! diagnose the eddy induced velocity and associated heat transport IF( ln_ldfeiv_dia .AND. cdtype == 'TRA' ) CALL ldf_eiv_dia( zpsi_uw, zpsi_vw ) ! END SUBROUTINE ldf_eiv_trp SUBROUTINE ldf_eiv_dia( psi_uw, psi_vw ) !!---------------------------------------------------------------------- !! *** ROUTINE ldf_eiv_dia *** !! !! ** Purpose : diagnose the eddy induced velocity and its associated !! vertically integrated heat transport. !! !! ** Method : !! !!---------------------------------------------------------------------- REAL(wp), DIMENSION(jpi,jpj,jpk), INTENT(inout) :: psi_uw, psi_vw ! streamfunction [m3/s] ! INTEGER :: ji, jj, jk ! dummy loop indices REAL(wp) :: zztmp ! local scalar REAL(wp), DIMENSION(jpi,jpj) :: zw2d ! 2D workspace REAL(wp), DIMENSION(jpi,jpj,jpk) :: zw3d ! 3D workspace !!---------------------------------------------------------------------- ! !!gm I don't like this routine.... Crazy way of doing things, not optimal at all... !!gm to be redesigned.... ! !== eiv stream function: output ==! CALL lbc_lnk_multi( 'ldftra', psi_uw, 'U', -1. , psi_vw, 'V', -1. ) ! !!gm CALL iom_put( "psi_eiv_uw", psi_uw ) ! output !!gm CALL iom_put( "psi_eiv_vw", psi_vw ) ! ! !== eiv velocities: calculate and output ==! ! zw3d(:,:,jpk) = 0._wp ! bottom value always 0 ! DO jk = 1, jpkm1 ! e2u e3u u_eiv = -dk[psi_uw] zw3d(:,:,jk) = ( psi_uw(:,:,jk+1) - psi_uw(:,:,jk) ) / ( e2u(:,:) * e3u_n(:,:,jk) ) END DO CALL iom_put( "uoce_eiv", zw3d ) ! DO jk = 1, jpkm1 ! e1v e3v v_eiv = -dk[psi_vw] zw3d(:,:,jk) = ( psi_vw(:,:,jk+1) - psi_vw(:,:,jk) ) / ( e1v(:,:) * e3v_n(:,:,jk) ) END DO CALL iom_put( "voce_eiv", zw3d ) ! DO jk = 1, jpkm1 ! e1 e2 w_eiv = dk[psix] + dk[psix] DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. zw3d(ji,jj,jk) = ( psi_vw(ji,jj,jk) - psi_vw(ji ,jj-1,jk) & & + psi_uw(ji,jj,jk) - psi_uw(ji-1,jj ,jk) ) / e1e2t(ji,jj) END DO END DO END DO CALL lbc_lnk( 'ldftra', zw3d, 'T', 1. ) ! lateral boundary condition CALL iom_put( "woce_eiv", zw3d ) ! ! zztmp = 0.5_wp * rau0 * rcp IF( iom_use('ueiv_heattr') .OR. iom_use('ueiv_heattr3d') ) THEN zw2d(:,:) = 0._wp zw3d(:,:,:) = 0._wp DO jk = 1, jpkm1 DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. zw3d(ji,jj,jk) = zw3d(ji,jj,jk) + ( psi_uw(ji,jj,jk+1) - psi_uw(ji,jj,jk) ) & & * ( tsn (ji,jj,jk,jp_tem) + tsn (ji+1,jj,jk,jp_tem) ) zw2d(ji,jj) = zw2d(ji,jj) + zw3d(ji,jj,jk) END DO END DO END DO CALL lbc_lnk( 'ldftra', zw2d, 'U', -1. ) CALL lbc_lnk( 'ldftra', zw3d, 'U', -1. ) CALL iom_put( "ueiv_heattr" , zztmp * zw2d ) ! heat transport in i-direction CALL iom_put( "ueiv_heattr3d", zztmp * zw3d ) ! heat transport in i-direction ENDIF zw2d(:,:) = 0._wp zw3d(:,:,:) = 0._wp DO jk = 1, jpkm1 DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. zw3d(ji,jj,jk) = zw3d(ji,jj,jk) + ( psi_vw(ji,jj,jk+1) - psi_vw(ji,jj,jk) ) & & * ( tsn (ji,jj,jk,jp_tem) + tsn (ji,jj+1,jk,jp_tem) ) zw2d(ji,jj) = zw2d(ji,jj) + zw3d(ji,jj,jk) END DO END DO END DO CALL lbc_lnk( 'ldftra', zw2d, 'V', -1. ) CALL iom_put( "veiv_heattr", zztmp * zw2d ) ! heat transport in j-direction CALL iom_put( "veiv_heattr", zztmp * zw3d ) ! heat transport in j-direction ! IF( ln_diaptr ) CALL dia_ptr_hst( jp_tem, 'eiv', 0.5 * zw3d ) ! zztmp = 0.5_wp * 0.5 IF( iom_use('ueiv_salttr') .OR. iom_use('ueiv_salttr3d')) THEN zw2d(:,:) = 0._wp zw3d(:,:,:) = 0._wp DO jk = 1, jpkm1 DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. zw3d(ji,jj,jk) = zw3d(ji,jj,jk) * ( psi_uw(ji,jj,jk+1) - psi_uw(ji,jj,jk) ) & & * ( tsn (ji,jj,jk,jp_sal) + tsn (ji+1,jj,jk,jp_sal) ) zw2d(ji,jj) = zw2d(ji,jj) + zw3d(ji,jj,jk) END DO END DO END DO CALL lbc_lnk( 'ldftra', zw2d, 'U', -1. ) CALL lbc_lnk( 'ldftra', zw3d, 'U', -1. ) CALL iom_put( "ueiv_salttr", zztmp * zw2d ) ! salt transport in i-direction CALL iom_put( "ueiv_salttr3d", zztmp * zw3d ) ! salt transport in i-direction ENDIF zw2d(:,:) = 0._wp zw3d(:,:,:) = 0._wp DO jk = 1, jpkm1 DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. zw3d(ji,jj,jk) = zw3d(ji,jj,jk) + ( psi_vw(ji,jj,jk+1) - psi_vw(ji,jj,jk) ) & & * ( tsn (ji,jj,jk,jp_sal) + tsn (ji,jj+1,jk,jp_sal) ) zw2d(ji,jj) = zw2d(ji,jj) + zw3d(ji,jj,jk) END DO END DO END DO CALL lbc_lnk( 'ldftra', zw2d, 'V', -1. ) CALL iom_put( "veiv_salttr", zztmp * zw2d ) ! salt transport in j-direction CALL iom_put( "veiv_salttr", zztmp * zw3d ) ! salt transport in j-direction ! IF( ln_diaptr ) CALL dia_ptr_hst( jp_sal, 'eiv', 0.5 * zw3d ) ! ! END SUBROUTINE ldf_eiv_dia !!====================================================================== END MODULE ldftra