[3] | 1 | MODULE dynnxt |
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[1502] | 2 | !!========================================================================= |
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[3] | 3 | !! *** MODULE dynnxt *** |
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| 4 | !! Ocean dynamics: time stepping |
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[1502] | 5 | !!========================================================================= |
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[1438] | 6 | !! History : OPA ! 1987-02 (P. Andrich, D. L Hostis) Original code |
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| 7 | !! ! 1990-10 (C. Levy, G. Madec) |
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| 8 | !! 7.0 ! 1993-03 (M. Guyon) symetrical conditions |
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| 9 | !! 8.0 ! 1997-02 (G. Madec & M. Imbard) opa, release 8.0 |
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| 10 | !! 8.2 ! 1997-04 (A. Weaver) Euler forward step |
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| 11 | !! - ! 1997-06 (G. Madec) lateral boudary cond., lbc routine |
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| 12 | !! NEMO 1.0 ! 2002-08 (G. Madec) F90: Free form and module |
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| 13 | !! - ! 2002-10 (C. Talandier, A-M. Treguier) Open boundary cond. |
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| 14 | !! 2.0 ! 2005-11 (V. Garnier) Surface pressure gradient organization |
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| 15 | !! 2.3 ! 2007-07 (D. Storkey) Calls to BDY routines. |
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[1502] | 16 | !! 3.2 ! 2009-06 (G. Madec, R.Benshila) re-introduce the vvl option |
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[2528] | 17 | !! 3.3 ! 2010-09 (D. Storkey, E.O'Dea) Bug fix for BDY module |
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[2723] | 18 | !! 3.3 ! 2011-03 (P. Oddo) Bug fix for time-splitting+(BDY-OBC) and not VVL |
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[4292] | 19 | !! 3.5 ! 2013-07 (J. Chanut) Compliant with time splitting changes |
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[4990] | 20 | !! 3.7 ! 2014-04 (G. Madec) add the diagnostic of the time filter trends |
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[1502] | 21 | !!------------------------------------------------------------------------- |
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[1438] | 22 | |
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[1502] | 23 | !!------------------------------------------------------------------------- |
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| 24 | !! dyn_nxt : obtain the next (after) horizontal velocity |
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| 25 | !!------------------------------------------------------------------------- |
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[3] | 26 | USE oce ! ocean dynamics and tracers |
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| 27 | USE dom_oce ! ocean space and time domain |
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[2528] | 28 | USE sbc_oce ! Surface boundary condition: ocean fields |
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| 29 | USE phycst ! physical constants |
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[1502] | 30 | USE dynspg_oce ! type of surface pressure gradient |
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| 31 | USE dynadv ! dynamics: vector invariant versus flux form |
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| 32 | USE domvvl ! variable volume |
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[3294] | 33 | USE bdy_oce ! ocean open boundary conditions |
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| 34 | USE bdydta ! ocean open boundary conditions |
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| 35 | USE bdydyn ! ocean open boundary conditions |
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| 36 | USE bdyvol ! ocean open boundary condition (bdy_vol routines) |
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[4990] | 37 | USE trd_oce ! trends: ocean variables |
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| 38 | USE trddyn ! trend manager: dynamics |
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| 39 | USE trdken ! trend manager: kinetic energy |
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| 40 | ! |
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[1502] | 41 | USE in_out_manager ! I/O manager |
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[4990] | 42 | USE iom ! I/O manager library |
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[3] | 43 | USE lbclnk ! lateral boundary condition (or mpp link) |
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[2715] | 44 | USE lib_mpp ! MPP library |
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[3294] | 45 | USE wrk_nemo ! Memory Allocation |
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[258] | 46 | USE prtctl ! Print control |
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[4990] | 47 | USE timing ! Timing |
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[2528] | 48 | #if defined key_agrif |
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| 49 | USE agrif_opa_interp |
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| 50 | #endif |
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[3] | 51 | |
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| 52 | IMPLICIT NONE |
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| 53 | PRIVATE |
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| 54 | |
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[1438] | 55 | PUBLIC dyn_nxt ! routine called by step.F90 |
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| 56 | |
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[592] | 57 | !! * Substitutions |
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| 58 | # include "domzgr_substitute.h90" |
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[2715] | 59 | !!---------------------------------------------------------------------- |
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[2528] | 60 | !! NEMO/OPA 3.3 , NEMO Consortium (2010) |
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[1438] | 61 | !! $Id$ |
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[2715] | 62 | !! Software governed by the CeCILL licence (NEMOGCM/NEMO_CeCILL.txt) |
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| 63 | !!---------------------------------------------------------------------- |
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[3] | 64 | CONTAINS |
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| 65 | |
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| 66 | SUBROUTINE dyn_nxt ( kt ) |
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| 67 | !!---------------------------------------------------------------------- |
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| 68 | !! *** ROUTINE dyn_nxt *** |
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| 69 | !! |
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[1502] | 70 | !! ** Purpose : Compute the after horizontal velocity. Apply the boundary |
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| 71 | !! condition on the after velocity, achieved the time stepping |
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| 72 | !! by applying the Asselin filter on now fields and swapping |
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| 73 | !! the fields. |
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[3] | 74 | !! |
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[1502] | 75 | !! ** Method : * After velocity is compute using a leap-frog scheme: |
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| 76 | !! (ua,va) = (ub,vb) + 2 rdt (ua,va) |
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| 77 | !! Note that with flux form advection and variable volume layer |
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| 78 | !! (lk_vvl=T), the leap-frog is applied on thickness weighted |
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| 79 | !! velocity. |
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| 80 | !! Note also that in filtered free surface (lk_dynspg_flt=T), |
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| 81 | !! the time stepping has already been done in dynspg module |
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[3] | 82 | !! |
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[1502] | 83 | !! * Apply lateral boundary conditions on after velocity |
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| 84 | !! at the local domain boundaries through lbc_lnk call, |
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[4328] | 85 | !! at the one-way open boundaries (lk_bdy=T), |
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[4990] | 86 | !! at the AGRIF zoom boundaries (lk_agrif=T) |
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[3] | 87 | !! |
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[1502] | 88 | !! * Apply the time filter applied and swap of the dynamics |
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| 89 | !! arrays to start the next time step: |
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| 90 | !! (ub,vb) = (un,vn) + atfp [ (ub,vb) + (ua,va) - 2 (un,vn) ] |
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| 91 | !! (un,vn) = (ua,va). |
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| 92 | !! Note that with flux form advection and variable volume layer |
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| 93 | !! (lk_vvl=T), the time filter is applied on thickness weighted |
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| 94 | !! velocity. |
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| 95 | !! |
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| 96 | !! ** Action : ub,vb filtered before horizontal velocity of next time-step |
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| 97 | !! un,vn now horizontal velocity of next time-step |
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[3] | 98 | !!---------------------------------------------------------------------- |
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| 99 | INTEGER, INTENT( in ) :: kt ! ocean time-step index |
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[2715] | 100 | ! |
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[3] | 101 | INTEGER :: ji, jj, jk ! dummy loop indices |
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[3294] | 102 | INTEGER :: iku, ikv ! local integers |
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[1566] | 103 | #if ! defined key_dynspg_flt |
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[3] | 104 | REAL(wp) :: z2dt ! temporary scalar |
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[1566] | 105 | #endif |
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[4990] | 106 | REAL(wp) :: zue3a, zue3n, zue3b, zuf, zec ! local scalars |
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| 107 | REAL(wp) :: zve3a, zve3n, zve3b, zvf, z1_2dt ! - - |
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| 108 | REAL(wp), POINTER, DIMENSION(:,:) :: zue, zve |
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| 109 | REAL(wp), POINTER, DIMENSION(:,:,:) :: ze3u_f, ze3v_f, zua, zva |
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[1502] | 110 | !!---------------------------------------------------------------------- |
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[3294] | 111 | ! |
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[4990] | 112 | IF( nn_timing == 1 ) CALL timing_start('dyn_nxt') |
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[3294] | 113 | ! |
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[4990] | 114 | CALL wrk_alloc( jpi,jpj,jpk, ze3u_f, ze3v_f, zua, zva ) |
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| 115 | IF( lk_dynspg_ts ) CALL wrk_alloc( jpi,jpj, zue, zve ) |
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[3294] | 116 | ! |
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[3] | 117 | IF( kt == nit000 ) THEN |
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| 118 | IF(lwp) WRITE(numout,*) |
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| 119 | IF(lwp) WRITE(numout,*) 'dyn_nxt : time stepping' |
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| 120 | IF(lwp) WRITE(numout,*) '~~~~~~~' |
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| 121 | ENDIF |
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| 122 | |
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[1502] | 123 | #if defined key_dynspg_flt |
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| 124 | ! |
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| 125 | ! Next velocity : Leap-frog time stepping already done in dynspg_flt.F routine |
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| 126 | ! ------------- |
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[3] | 127 | |
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[1502] | 128 | ! Update after velocity on domain lateral boundaries (only local domain required) |
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| 129 | ! -------------------------------------------------- |
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| 130 | CALL lbc_lnk( ua, 'U', -1. ) ! local domain boundaries |
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| 131 | CALL lbc_lnk( va, 'V', -1. ) |
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| 132 | ! |
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| 133 | #else |
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[4292] | 134 | |
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| 135 | # if defined key_dynspg_exp |
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[1502] | 136 | ! Next velocity : Leap-frog time stepping |
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[1438] | 137 | ! ------------- |
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[1502] | 138 | z2dt = 2. * rdt ! Euler or leap-frog time step |
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| 139 | IF( neuler == 0 .AND. kt == nit000 ) z2dt = rdt |
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| 140 | ! |
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| 141 | IF( ln_dynadv_vec .OR. .NOT. lk_vvl ) THEN ! applied on velocity |
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[1438] | 142 | DO jk = 1, jpkm1 |
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[1502] | 143 | ua(:,:,jk) = ( ub(:,:,jk) + z2dt * ua(:,:,jk) ) * umask(:,:,jk) |
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| 144 | va(:,:,jk) = ( vb(:,:,jk) + z2dt * va(:,:,jk) ) * vmask(:,:,jk) |
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| 145 | END DO |
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| 146 | ELSE ! applied on thickness weighted velocity |
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| 147 | DO jk = 1, jpkm1 |
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| 148 | ua(:,:,jk) = ( ub(:,:,jk) * fse3u_b(:,:,jk) & |
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| 149 | & + z2dt * ua(:,:,jk) * fse3u_n(:,:,jk) ) & |
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[1438] | 150 | & / fse3u_a(:,:,jk) * umask(:,:,jk) |
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[1502] | 151 | va(:,:,jk) = ( vb(:,:,jk) * fse3v_b(:,:,jk) & |
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| 152 | & + z2dt * va(:,:,jk) * fse3v_n(:,:,jk) ) & |
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[1438] | 153 | & / fse3v_a(:,:,jk) * vmask(:,:,jk) |
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[592] | 154 | END DO |
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| 155 | ENDIF |
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[4292] | 156 | # endif |
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[592] | 157 | |
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[4292] | 158 | # if defined key_dynspg_ts |
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[4990] | 159 | !!gm IF ( lk_dynspg_ts ) THEN .... |
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[4292] | 160 | ! Ensure below that barotropic velocities match time splitting estimate |
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| 161 | ! Compute actual transport and replace it with ts estimate at "after" time step |
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[4990] | 162 | zue(:,:) = fse3u_a(:,:,1) * ua(:,:,1) * umask(:,:,1) |
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| 163 | zve(:,:) = fse3v_a(:,:,1) * va(:,:,1) * vmask(:,:,1) |
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| 164 | DO jk = 2, jpkm1 |
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| 165 | zue(:,:) = zue(:,:) + fse3u_a(:,:,jk) * ua(:,:,jk) * umask(:,:,jk) |
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| 166 | zve(:,:) = zve(:,:) + fse3v_a(:,:,jk) * va(:,:,jk) * vmask(:,:,jk) |
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[4370] | 167 | END DO |
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| 168 | DO jk = 1, jpkm1 |
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[4990] | 169 | ua(:,:,jk) = ( ua(:,:,jk) - zue(:,:) * hur_a(:,:) + ua_b(:,:) ) * umask(:,:,jk) |
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| 170 | va(:,:,jk) = ( va(:,:,jk) - zve(:,:) * hvr_a(:,:) + va_b(:,:) ) * vmask(:,:,jk) |
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[4370] | 171 | END DO |
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[1502] | 172 | |
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[4292] | 173 | IF (lk_dynspg_ts.AND.(.NOT.ln_bt_fw)) THEN |
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| 174 | ! Remove advective velocity from "now velocities" |
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| 175 | ! prior to asselin filtering |
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[4312] | 176 | ! In the forward case, this is done below after asselin filtering |
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| 177 | ! so that asselin contribution is removed at the same time |
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[4292] | 178 | DO jk = 1, jpkm1 |
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| 179 | un(:,:,jk) = ( un(:,:,jk) - un_adv(:,:) + un_b(:,:) )*umask(:,:,jk) |
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| 180 | vn(:,:,jk) = ( vn(:,:,jk) - vn_adv(:,:) + vn_b(:,:) )*vmask(:,:,jk) |
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| 181 | END DO |
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| 182 | ENDIF |
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[4990] | 183 | !!gm ENDIF |
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[4292] | 184 | # endif |
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| 185 | |
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[1502] | 186 | ! Update after velocity on domain lateral boundaries |
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| 187 | ! -------------------------------------------------- |
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| 188 | CALL lbc_lnk( ua, 'U', -1. ) !* local domain boundaries |
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| 189 | CALL lbc_lnk( va, 'V', -1. ) |
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| 190 | ! |
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[4328] | 191 | # if defined key_bdy |
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[1502] | 192 | ! !* BDY open boundaries |
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[3764] | 193 | IF( lk_bdy .AND. lk_dynspg_exp ) CALL bdy_dyn( kt ) |
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| 194 | IF( lk_bdy .AND. lk_dynspg_ts ) CALL bdy_dyn( kt, dyn3d_only=.true. ) |
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[3294] | 195 | |
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| 196 | !!$ Do we need a call to bdy_vol here?? |
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| 197 | ! |
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[1438] | 198 | # endif |
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[1502] | 199 | ! |
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[392] | 200 | # if defined key_agrif |
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[1502] | 201 | CALL Agrif_dyn( kt ) !* AGRIF zoom boundaries |
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[389] | 202 | # endif |
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[3] | 203 | #endif |
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[592] | 204 | |
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[4990] | 205 | IF( l_trddyn ) THEN ! prepare the atf trend computation + some diagnostics |
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| 206 | z1_2dt = 1._wp / (2. * rdt) ! Euler or leap-frog time step |
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| 207 | IF( neuler == 0 .AND. kt == nit000 ) z1_2dt = 1._wp / rdt |
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| 208 | ! |
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| 209 | ! ! Kinetic energy and Conversion |
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| 210 | IF( ln_KE_trd ) CALL trd_dyn( ua, va, jpdyn_ken, kt ) |
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| 211 | ! |
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| 212 | IF( ln_dyn_trd ) THEN ! 3D output: total momentum trends |
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| 213 | zua(:,:,:) = ( ua(:,:,:) - ub(:,:,:) ) * z1_2dt |
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| 214 | zva(:,:,:) = ( va(:,:,:) - vb(:,:,:) ) * z1_2dt |
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| 215 | CALL iom_put( "utrd_tot", zua ) ! total momentum trends, except the asselin time filter |
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| 216 | CALL iom_put( "vtrd_tot", zva ) |
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| 217 | ENDIF |
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| 218 | ! |
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| 219 | zua(:,:,:) = un(:,:,:) ! save the now velocity before the asselin filter |
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| 220 | zva(:,:,:) = vn(:,:,:) ! (caution: there will be a shift by 1 timestep in the |
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| 221 | ! ! computation of the asselin filter trends) |
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| 222 | ENDIF |
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| 223 | |
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[1438] | 224 | ! Time filter and swap of dynamics arrays |
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| 225 | ! ------------------------------------------ |
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[1502] | 226 | IF( neuler == 0 .AND. kt == nit000 ) THEN !* Euler at first time-step: only swap |
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| 227 | DO jk = 1, jpkm1 |
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| 228 | un(:,:,jk) = ua(:,:,jk) ! un <-- ua |
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[1438] | 229 | vn(:,:,jk) = va(:,:,jk) |
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| 230 | END DO |
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[4292] | 231 | IF (lk_vvl) THEN |
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| 232 | DO jk = 1, jpkm1 |
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| 233 | fse3t_b(:,:,jk) = fse3t_n(:,:,jk) |
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| 234 | fse3u_b(:,:,jk) = fse3u_n(:,:,jk) |
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| 235 | fse3v_b(:,:,jk) = fse3v_n(:,:,jk) |
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| 236 | ENDDO |
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| 237 | ENDIF |
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[1502] | 238 | ELSE !* Leap-Frog : Asselin filter and swap |
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[2528] | 239 | ! ! =============! |
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| 240 | IF( .NOT. lk_vvl ) THEN ! Fixed volume ! |
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| 241 | ! ! =============! |
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[1502] | 242 | DO jk = 1, jpkm1 |
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[592] | 243 | DO jj = 1, jpj |
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[1502] | 244 | DO ji = 1, jpi |
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[4990] | 245 | zuf = un(ji,jj,jk) + atfp * ( ub(ji,jj,jk) - 2._wp * un(ji,jj,jk) + ua(ji,jj,jk) ) |
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| 246 | zvf = vn(ji,jj,jk) + atfp * ( vb(ji,jj,jk) - 2._wp * vn(ji,jj,jk) + va(ji,jj,jk) ) |
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[1502] | 247 | ! |
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| 248 | ub(ji,jj,jk) = zuf ! ub <-- filtered velocity |
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| 249 | vb(ji,jj,jk) = zvf |
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| 250 | un(ji,jj,jk) = ua(ji,jj,jk) ! un <-- ua |
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| 251 | vn(ji,jj,jk) = va(ji,jj,jk) |
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| 252 | END DO |
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| 253 | END DO |
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| 254 | END DO |
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[2528] | 255 | ! ! ================! |
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| 256 | ELSE ! Variable volume ! |
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| 257 | ! ! ================! |
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[4292] | 258 | ! Before scale factor at t-points |
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| 259 | ! (used as a now filtered scale factor until the swap) |
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| 260 | ! ---------------------------------------------------- |
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| 261 | IF (lk_dynspg_ts.AND.ln_bt_fw) THEN |
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[4338] | 262 | ! No asselin filtering on thicknesses if forward time splitting |
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[4292] | 263 | fse3t_b(:,:,:) = fse3t_n(:,:,:) |
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| 264 | ELSE |
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| 265 | fse3t_b(:,:,:) = fse3t_n(:,:,:) + atfp * ( fse3t_b(:,:,:) - 2._wp * fse3t_n(:,:,:) + fse3t_a(:,:,:) ) |
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| 266 | ! Add volume filter correction: compatibility with tracer advection scheme |
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| 267 | ! => time filter + conservation correction (only at the first level) |
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[5628] | 268 | IF ( nn_isf == 0) THEN ! if no ice shelf melting |
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| 269 | fse3t_b(:,:,1) = fse3t_b(:,:,1) - atfp * rdt * r1_rau0 * ( emp_b(:,:) - emp(:,:) & |
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| 270 | & -rnf_b(:,:) + rnf(:,:) ) * tmask(:,:,1) |
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| 271 | ELSE ! if ice shelf melting |
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| 272 | DO jj = 1,jpj |
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| 273 | DO ji = 1,jpi |
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| 274 | jk = mikt(ji,jj) |
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| 275 | fse3t_b(ji,jj,jk) = fse3t_b(ji,jj,jk) - atfp * rdt * r1_rau0 & |
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| 276 | & * ( (emp_b(ji,jj) - emp(ji,jj) ) & |
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| 277 | & - (rnf_b(ji,jj) - rnf(ji,jj) ) & |
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| 278 | & + (fwfisf_b(ji,jj) - fwfisf(ji,jj)) ) * tmask(ji,jj,jk) |
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| 279 | END DO |
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| 280 | END DO |
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| 281 | END IF |
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[4292] | 282 | ENDIF |
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[2528] | 283 | ! |
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[4292] | 284 | IF( ln_dynadv_vec ) THEN |
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| 285 | ! Before scale factor at (u/v)-points |
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| 286 | ! ----------------------------------- |
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| 287 | CALL dom_vvl_interpol( fse3t_b(:,:,:), fse3u_b(:,:,:), 'U' ) |
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| 288 | CALL dom_vvl_interpol( fse3t_b(:,:,:), fse3v_b(:,:,:), 'V' ) |
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| 289 | ! Leap-Frog - Asselin filter and swap: applied on velocity |
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| 290 | ! ----------------------------------- |
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| 291 | DO jk = 1, jpkm1 |
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| 292 | DO jj = 1, jpj |
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[2528] | 293 | DO ji = 1, jpi |
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[4292] | 294 | zuf = un(ji,jj,jk) + atfp * ( ub(ji,jj,jk) - 2._wp * un(ji,jj,jk) + ua(ji,jj,jk) ) |
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| 295 | zvf = vn(ji,jj,jk) + atfp * ( vb(ji,jj,jk) - 2._wp * vn(ji,jj,jk) + va(ji,jj,jk) ) |
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[2528] | 296 | ! |
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| 297 | ub(ji,jj,jk) = zuf ! ub <-- filtered velocity |
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| 298 | vb(ji,jj,jk) = zvf |
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| 299 | un(ji,jj,jk) = ua(ji,jj,jk) ! un <-- ua |
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| 300 | vn(ji,jj,jk) = va(ji,jj,jk) |
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| 301 | END DO |
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| 302 | END DO |
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| 303 | END DO |
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| 304 | ! |
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[4292] | 305 | ELSE |
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| 306 | ! Temporary filtered scale factor at (u/v)-points (will become before scale factor) |
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| 307 | !------------------------------------------------ |
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| 308 | CALL dom_vvl_interpol( fse3t_b(:,:,:), ze3u_f, 'U' ) |
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| 309 | CALL dom_vvl_interpol( fse3t_b(:,:,:), ze3v_f, 'V' ) |
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| 310 | ! Leap-Frog - Asselin filter and swap: applied on thickness weighted velocity |
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| 311 | ! ----------------------------------- =========================== |
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| 312 | DO jk = 1, jpkm1 |
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| 313 | DO jj = 1, jpj |
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[4312] | 314 | DO ji = 1, jpi |
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[2528] | 315 | zue3a = ua(ji,jj,jk) * fse3u_a(ji,jj,jk) |
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| 316 | zve3a = va(ji,jj,jk) * fse3v_a(ji,jj,jk) |
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| 317 | zue3n = un(ji,jj,jk) * fse3u_n(ji,jj,jk) |
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| 318 | zve3n = vn(ji,jj,jk) * fse3v_n(ji,jj,jk) |
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| 319 | zue3b = ub(ji,jj,jk) * fse3u_b(ji,jj,jk) |
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| 320 | zve3b = vb(ji,jj,jk) * fse3v_b(ji,jj,jk) |
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| 321 | ! |
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[3294] | 322 | zuf = ( zue3n + atfp * ( zue3b - 2._wp * zue3n + zue3a ) ) / ze3u_f(ji,jj,jk) |
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| 323 | zvf = ( zve3n + atfp * ( zve3b - 2._wp * zve3n + zve3a ) ) / ze3v_f(ji,jj,jk) |
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[2528] | 324 | ! |
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[3294] | 325 | ub(ji,jj,jk) = zuf ! ub <-- filtered velocity |
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[2528] | 326 | vb(ji,jj,jk) = zvf |
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[3294] | 327 | un(ji,jj,jk) = ua(ji,jj,jk) ! un <-- ua |
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[2528] | 328 | vn(ji,jj,jk) = va(ji,jj,jk) |
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| 329 | END DO |
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| 330 | END DO |
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| 331 | END DO |
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[3294] | 332 | fse3u_b(:,:,1:jpkm1) = ze3u_f(:,:,1:jpkm1) ! e3u_b <-- filtered scale factor |
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| 333 | fse3v_b(:,:,1:jpkm1) = ze3v_f(:,:,1:jpkm1) |
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[2528] | 334 | ENDIF |
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| 335 | ! |
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[3] | 336 | ENDIF |
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[2528] | 337 | ! |
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[4292] | 338 | IF (lk_dynspg_ts.AND.ln_bt_fw) THEN |
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[4312] | 339 | ! Revert "before" velocities to time split estimate |
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| 340 | ! Doing it here also means that asselin filter contribution is removed |
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[4990] | 341 | zue(:,:) = fse3u_b(:,:,1) * ub(:,:,1) * umask(:,:,1) |
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| 342 | zve(:,:) = fse3v_b(:,:,1) * vb(:,:,1) * vmask(:,:,1) |
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| 343 | DO jk = 2, jpkm1 |
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| 344 | zue(:,:) = zue(:,:) + fse3u_b(:,:,jk) * ub(:,:,jk) * umask(:,:,jk) |
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| 345 | zve(:,:) = zve(:,:) + fse3v_b(:,:,jk) * vb(:,:,jk) * vmask(:,:,jk) |
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[4370] | 346 | END DO |
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| 347 | DO jk = 1, jpkm1 |
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[4990] | 348 | ub(:,:,jk) = ub(:,:,jk) - (zue(:,:) * hur(:,:) - un_b(:,:)) * umask(:,:,jk) |
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| 349 | vb(:,:,jk) = vb(:,:,jk) - (zve(:,:) * hvr(:,:) - vn_b(:,:)) * vmask(:,:,jk) |
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[4292] | 350 | END DO |
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| 351 | ENDIF |
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| 352 | ! |
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| 353 | ENDIF ! neuler =/0 |
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[4354] | 354 | ! |
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| 355 | ! Set "now" and "before" barotropic velocities for next time step: |
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| 356 | ! JC: Would be more clever to swap variables than to make a full vertical |
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| 357 | ! integration |
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| 358 | ! |
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[4370] | 359 | ! |
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| 360 | IF (lk_vvl) THEN |
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| 361 | hu_b(:,:) = 0. |
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| 362 | hv_b(:,:) = 0. |
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| 363 | DO jk = 1, jpkm1 |
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| 364 | hu_b(:,:) = hu_b(:,:) + fse3u_b(:,:,jk) * umask(:,:,jk) |
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| 365 | hv_b(:,:) = hv_b(:,:) + fse3v_b(:,:,jk) * vmask(:,:,jk) |
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[4354] | 366 | END DO |
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[4990] | 367 | hur_b(:,:) = umask_i(:,:) / ( hu_b(:,:) + 1._wp - umask_i(:,:) ) |
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| 368 | hvr_b(:,:) = vmask_i(:,:) / ( hv_b(:,:) + 1._wp - vmask_i(:,:) ) |
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[4354] | 369 | ENDIF |
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| 370 | ! |
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| 371 | un_b(:,:) = 0._wp ; vn_b(:,:) = 0._wp |
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| 372 | ub_b(:,:) = 0._wp ; vb_b(:,:) = 0._wp |
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| 373 | ! |
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| 374 | DO jk = 1, jpkm1 |
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| 375 | DO jj = 1, jpj |
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| 376 | DO ji = 1, jpi |
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[4370] | 377 | un_b(ji,jj) = un_b(ji,jj) + fse3u_a(ji,jj,jk) * un(ji,jj,jk) * umask(ji,jj,jk) |
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| 378 | vn_b(ji,jj) = vn_b(ji,jj) + fse3v_a(ji,jj,jk) * vn(ji,jj,jk) * vmask(ji,jj,jk) |
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[4354] | 379 | ! |
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[4370] | 380 | ub_b(ji,jj) = ub_b(ji,jj) + fse3u_b(ji,jj,jk) * ub(ji,jj,jk) * umask(ji,jj,jk) |
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| 381 | vb_b(ji,jj) = vb_b(ji,jj) + fse3v_b(ji,jj,jk) * vb(ji,jj,jk) * vmask(ji,jj,jk) |
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[4354] | 382 | END DO |
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| 383 | END DO |
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| 384 | END DO |
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| 385 | ! |
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| 386 | ! |
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[4370] | 387 | un_b(:,:) = un_b(:,:) * hur_a(:,:) |
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| 388 | vn_b(:,:) = vn_b(:,:) * hvr_a(:,:) |
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| 389 | ub_b(:,:) = ub_b(:,:) * hur_b(:,:) |
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| 390 | vb_b(:,:) = vb_b(:,:) * hvr_b(:,:) |
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[4354] | 391 | ! |
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| 392 | ! |
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[4990] | 393 | |
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| 394 | IF( l_trddyn ) THEN ! 3D output: asselin filter trends on momentum |
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| 395 | zua(:,:,:) = ( ub(:,:,:) - zua(:,:,:) ) * z1_2dt |
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| 396 | zva(:,:,:) = ( vb(:,:,:) - zva(:,:,:) ) * z1_2dt |
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| 397 | CALL trd_dyn( zua, zva, jpdyn_atf, kt ) |
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| 398 | ENDIF |
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| 399 | ! |
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[1438] | 400 | IF(ln_ctl) CALL prt_ctl( tab3d_1=un, clinfo1=' nxt - Un: ', mask1=umask, & |
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| 401 | & tab3d_2=vn, clinfo2=' Vn: ' , mask2=vmask ) |
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| 402 | ! |
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[4990] | 403 | CALL wrk_dealloc( jpi,jpj,jpk, ze3u_f, ze3v_f, zua, zva ) |
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| 404 | IF( lk_dynspg_ts ) CALL wrk_dealloc( jpi,jpj, zue, zve ) |
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[2715] | 405 | ! |
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[3294] | 406 | IF( nn_timing == 1 ) CALL timing_stop('dyn_nxt') |
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| 407 | ! |
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[3] | 408 | END SUBROUTINE dyn_nxt |
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| 409 | |
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[1502] | 410 | !!========================================================================= |
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[3] | 411 | END MODULE dynnxt |
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