MODULE dynzdf_imp !!============================================================================== !! *** MODULE dynzdf_imp *** !! Ocean dynamics: vertical component(s) of the momentum mixing trend !!============================================================================== !!---------------------------------------------------------------------- !! dyn_zdf_imp : update the momentum trend with the vertical diffu- !! sion using a implicit time-stepping. !!---------------------------------------------------------------------- !! OPA 9.0 , LODYC-IPSL (2003) !!---------------------------------------------------------------------- !! * Modules used USE oce ! ocean dynamics and tracers USE dom_oce ! ocean space and time domain USE phycst ! physical constants USE zdf_oce ! ocean vertical physics USE in_out_manager ! I/O manager USE taumod ! surface ocean stress USE trddyn_oce ! dynamics trends diagnostics variables IMPLICIT NONE PRIVATE !! * Routine accessibility PUBLIC dyn_zdf_imp ! called by step.F90 !! * Substitutions # include "domzgr_substitute.h90" # include "vectopt_loop_substitute.h90" !!---------------------------------------------------------------------- !! OPA 9.0 , LODYC-IPSL (2003) !!---------------------------------------------------------------------- CONTAINS SUBROUTINE dyn_zdf_imp( kt ) !!---------------------------------------------------------------------- !! *** ROUTINE dyn_zdf_imp *** !! !! ** Purpose : Compute the trend due to the vert. momentum diffusion !! and the surface forcing, and add it to the general trend of !! the momentum equations. !! !! ** Method : The vertical momentum mixing trend is given by : !! dz( avmu dz(u) ) = 1/e3u dk+1( avmu/e3uw dk(ua) ) !! backward time stepping !! Surface boundary conditions: wind stress input !! Bottom boundary conditions : bottom stress (cf zdfbfr.F) !! Add this trend to the general trend ua : !! ua = ua + dz( avmu dz(u) ) !! !! ** Action : - Update (ua,va) arrays with the after vertical diffusive !! mixing trend. !! - Save the trends in (utrd,vtrd) ('key_diatrends') !! !! History : !! ! 90-10 (B. Blanke) Original code !! ! 97-05 (G. Madec) vertical component of isopycnal !! 8.5 ! 02-08 (G. Madec) F90: Free form and module !!--------------------------------------------------------------------- !! * Modules used USE oce, ONLY : zwd => ta, & ! use ta as workspace zws => sa ! use sa as workspace !! * Arguments INTEGER, INTENT( in ) :: kt ! ocean time-step index !! * Local declarations INTEGER :: ji, jj, jk ! dummy loop indices REAL(wp) :: & zrau0r, z2dt, zua, zva, & ! temporary scalars z2dtf, zcoef, zzws, zrhs ! " " REAL(wp), DIMENSION(jpi,jpj,jpk) :: & zwi ! temporary workspace arrays #if defined key_trddyn || defined key_trd_vor INTEGER :: & ikbu, ikbum1, ikbv, ikbvm1 ! temporary integers #endif !!---------------------------------------------------------------------- IF( kt == nit000 ) THEN IF(lwp) WRITE(numout,*) IF(lwp) WRITE(numout,*) 'dyn_zdf_imp : vertical momentum diffusion implicit operator' IF(lwp) WRITE(numout,*) '~~~~~~~~~~~ ' ENDIF ! 0. Local constant initialization ! -------------------------------- zrau0r = 1. / rau0 ! inverse of the reference density z2dt = 2. * rdt ! Leap-frog environnement ! Euler time stepping when starting from rest IF( neuler == 0 .AND. kt == nit000 ) z2dt = rdt ! Normalization to obtain the general momentum trend ua #if defined key_trddyn || defined key_trd_vor ! Save the previously computed trend DO jk = 1, jpkm1 DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. utrd(ji,jj,jk,7) = ua(ji,jj,jk) vtrd(ji,jj,jk,7) = va(ji,jj,jk) END DO END DO END DO #endif ! 1. Vertical diffusion on u ! --------------------------- ! Matrix and second member construction ! bottom boundary condition: only zws must be masked as avmu can take ! non zero value at the ocean bottom depending on the bottom friction ! used (see zdfmix.F) DO jk = 1, jpkm1 DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. zcoef = - z2dt / fse3u(ji,jj,jk) zwi(ji,jj,jk) = zcoef * avmu(ji,jj,jk ) / fse3uw(ji,jj,jk ) zzws = zcoef * avmu(ji,jj,jk+1) / fse3uw(ji,jj,jk+1) zws(ji,jj,jk) = zzws * umask(ji,jj,jk+1) zwd(ji,jj,jk) = 1. - zwi(ji,jj,jk) - zzws END DO END DO END DO ! Surface boudary conditions DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. zwi(ji,jj,1) = 0. zwd(ji,jj,1) = 1. - zws(ji,jj,1) END DO END DO ! Matrix inversion starting from the first level !----------------------------------------------------------------------- ! solve m.x = y where m is a tri diagonal matrix ( jpk*jpk ) ! ! ( zwd1 zws1 0 0 0 )( zwx1 ) ( zwy1 ) ! ( zwi2 zwd2 zws2 0 0 )( zwx2 ) ( zwy2 ) ! ( 0 zwi3 zwd3 zws3 0 )( zwx3 )=( zwy3 ) ! ( ... )( ... ) ( ... ) ! ( 0 0 0 zwik zwdk )( zwxk ) ( zwyk ) ! ! m is decomposed in the product of an upper and a lower triangular matrix ! The 3 diagonal terms are in 2d arrays: zwd, zws, zwi ! The solution (the after velocity) is in ua !----------------------------------------------------------------------- ! First recurrence : Dk = Dk - Lk * Uk-1 / Dk-1 (increasing k) DO jk = 2, jpkm1 DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. zwd(ji,jj,jk) = zwd(ji,jj,jk) - zwi(ji,jj,jk) * zws(ji,jj,jk-1) / zwd(ji,jj,jk-1) END DO END DO END DO ! second recurrence: SOLk = RHSk - Lk / Dk-1 Lk-1 DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. !!! change les resultats (derniers digit, pas significativement + rapide 1* de moins) !!! ua(ji,jj,1) = ub(ji,jj,1) & !!! + z2dt * ( ua(ji,jj,1) + taux(ji,jj) / ( fse3u(ji,jj,1)*rau0 ) ) z2dtf = z2dt / ( fse3u(ji,jj,1)*rau0 ) ua(ji,jj,1) = ub(ji,jj,1) & + z2dt * ua(ji,jj,1) + z2dtf * taux(ji,jj) END DO END DO DO jk = 2, jpkm1 DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. zrhs = ub(ji,jj,jk) + z2dt * ua(ji,jj,jk) ! zrhs=right hand side ua(ji,jj,jk) = zrhs - zwi(ji,jj,jk) / zwd(ji,jj,jk-1) * ua(ji,jj,jk-1) END DO END DO END DO ! thrid recurrence : SOLk = ( Lk - Uk * Ek+1 ) / Dk DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. ua(ji,jj,jpkm1) = ua(ji,jj,jpkm1) / zwd(ji,jj,jpkm1) END DO END DO DO jk = jpk-2, 1, -1 DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. ua(ji,jj,jk) =( ua(ji,jj,jk) - zws(ji,jj,jk) * ua(ji,jj,jk+1) ) / zwd(ji,jj,jk) END DO END DO END DO #if defined key_trddyn || defined key_trd_vor ! diagnose surface and bottom momentum fluxes DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. ! save the surface forcing momentum fluxes tautrd(ji,jj,1) = taux(ji,jj) / ( fse3u(ji,jj,1)*rau0 ) ! save bottom friction momentum fluxes ikbu = MIN( mbathy(ji+1,jj), mbathy(ji,jj) ) ikbum1 = MAX( ikbu-1, 1 ) tautrd(ji,jj,3) = - avmu(ji,jj,ikbu) * ua(ji,jj,ikbum1) & / ( fse3u(ji,jj,ikbum1)*fse3uw(ji,jj,ikbu) ) ! subtract surface forcing and bottom friction trend from vertical ! diffusive momentum trend utrd(ji,jj,1 ,7) = utrd(ji,jj,1 ,7) + tautrd(ji,jj,1) utrd(ji,jj,ikbum1,7) = utrd(ji,jj,ikbum1,7) + tautrd(ji,jj,3) END DO END DO #endif ! Normalization to obtain the general momentum trend ua DO jk = 1, jpkm1 DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. zua = ( ua(ji,jj,jk) - ub(ji,jj,jk) ) / z2dt #if defined key_trddyn || defined key_trd_vor ! save the vertical diffusive momentum trend (general trend - previous one) utrd(ji,jj,jk,7) = zua - utrd(ji,jj,jk,7) #endif ua(ji,jj,jk) = zua END DO END DO END DO ! 2. Vertical diffusion on v ! --------------------------- ! Matrix and second member construction ! bottom boundary condition: only zws must be masked as avmv can take ! non zero value at the ocean bottom depending on the bottom friction ! used (see zdfmix.F) DO jk = 1, jpkm1 DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. zcoef = -z2dt / fse3v(ji,jj,jk) zwi(ji,jj,jk) = zcoef * avmv(ji,jj,jk ) / fse3vw(ji,jj,jk ) zzws = zcoef * avmv(ji,jj,jk+1) / fse3vw(ji,jj,jk+1) zws(ji,jj,jk) = zzws * vmask(ji,jj,jk+1) zwd(ji,jj,jk) = 1. - zwi(ji,jj,jk) - zzws END DO END DO END DO ! Surface boudary conditions DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. zwi(ji,jj,1) = 0.e0 zwd(ji,jj,1) = 1. - zws(ji,jj,1) END DO END DO ! Matrix inversion !----------------------------------------------------------------------- ! solve m.x = y where m is a tri diagonal matrix ( jpk*jpk ) ! ! ( zwd1 zws1 0 0 0 )( zwx1 ) ( zwy1 ) ! ( zwi2 zwd2 zws2 0 0 )( zwx2 ) ( zwy2 ) ! ( 0 zwi3 zwd3 zws3 0 )( zwx3 )=( zwy3 ) ! ( ... )( ... ) ( ... ) ! ( 0 0 0 zwik zwdk )( zwxk ) ( zwyk ) ! ! m is decomposed in the product of an upper and lower triangular ! matrix ! The 3 diagonal terms are in 2d arrays: zwd, zws, zwi ! The solution (after velocity) is in 2d array va !----------------------------------------------------------------------- ! First recurrence : Dk = Dk - Lk * Uk-1 / Dk-1 (increasing k) DO jk = 2, jpkm1 DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. zwd(ji,jj,jk) = zwd(ji,jj,jk) - zwi(ji,jj,jk) * zws(ji,jj,jk-1) / zwd(ji,jj,jk-1) END DO END DO END DO ! second recurrence: SOLk = RHSk - Lk / Dk-1 Lk-1 DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. !!! change les resultats (derniers digit, pas significativement + rapide 1* de moins) !!! va(ji,jj,1) = vb(ji,jj,1) & !!! + z2dt * ( va(ji,jj,1) + tauy(ji,jj) / ( fse3v(ji,jj,1)*rau0 ) ) z2dtf = z2dt / ( fse3v(ji,jj,1)*rau0 ) va(ji,jj,1) = vb(ji,jj,1) & + z2dt * va(ji,jj,1) + z2dtf * tauy(ji,jj) END DO END DO DO jk = 2, jpkm1 DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. zrhs = vb(ji,jj,jk) + z2dt * va(ji,jj,jk) ! zrhs=right hand side va(ji,jj,jk) = zrhs - zwi(ji,jj,jk) / zwd(ji,jj,jk-1) * va(ji,jj,jk-1) END DO END DO END DO ! thrid recurrence : SOLk = ( Lk - Uk * SOLk+1 ) / Dk DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. va(ji,jj,jpkm1) = va(ji,jj,jpkm1) / zwd(ji,jj,jpkm1) END DO END DO DO jk = jpk-2, 1, -1 DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. va(ji,jj,jk) =( va(ji,jj,jk) - zws(ji,jj,jk) * va(ji,jj,jk+1) ) / zwd(ji,jj,jk) END DO END DO END DO #if defined key_trddyn || defined key_trd_vor ! diagnose surface and bottom momentum fluxes DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. ! save the surface forcing momentum fluxes tautrd(ji,jj,2) = tauy(ji,jj) / ( fse3v(ji,jj,1)*rau0 ) ! save bottom friction momentum fluxes ikbv = MIN( mbathy(ji,jj+1), mbathy(ji,jj) ) ikbvm1 = MAX( ikbv-1, 1 ) tautrd(ji,jj,4) = - avmv(ji,jj,ikbv) * va(ji,jj,ikbvm1) & / ( fse3v(ji,jj,ikbvm1)*fse3vw(ji,jj,ikbv) ) ! subtract surface forcing and bottom friction trend from vertical ! diffusive momentum trend vtrd(ji,jj,1 ,7) = vtrd(ji,jj,1 ,7) + tautrd(ji,jj,2) vtrd(ji,jj,ikbvm1,7) = vtrd(ji,jj,ikbvm1,7) + tautrd(ji,jj,4) END DO END DO #endif ! Normalization to obtain the general momentum trend va DO jk = 1, jpkm1 DO jj = 2, jpjm1 DO ji = fs_2, fs_jpim1 ! vector opt. zva = ( va(ji,jj,jk) - vb(ji,jj,jk) ) / z2dt #if defined key_trddyn || defined key_trd_vor ! save the vertical diffusive momentum fluxes vtrd(ji,jj,jk,7) = zva - vtrd(ji,jj,jk,7) #endif va(ji,jj,jk) = zva END DO END DO END DO IF(l_ctl) THEN ! print sum trends (used for debugging) zua = SUM( ua(2:nictl,2:njctl,1:jpkm1) * umask(2:nictl,2:njctl,1:jpkm1) ) zva = SUM( va(2:nictl,2:njctl,1:jpkm1) * vmask(2:nictl,2:njctl,1:jpkm1) ) WRITE(numout,*) ' zdf - Ua: ', zua-u_ctl, ' Va: ', zva-v_ctl u_ctl = zua ; v_ctl = zva ENDIF END SUBROUTINE dyn_zdf_imp !!============================================================================== END MODULE dynzdf_imp