[3] | 1 | MODULE dynvor |
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| 2 | !!====================================================================== |
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| 3 | !! *** MODULE dynvor *** |
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| 4 | !! Ocean dynamics: Update the momentum trend with the relative and |
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| 5 | !! planetary vorticity trends |
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| 6 | !!====================================================================== |
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[2715] | 7 | !! History : OPA ! 1989-12 (P. Andrich) vor_ens: Original code |
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[9528] | 8 | !! 5.0 ! 1991-11 (G. Madec) vor_ene, vor_mix: Original code |
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[2715] | 9 | !! 6.0 ! 1996-01 (G. Madec) s-coord, suppress work arrays |
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| 10 | !! NEMO 0.5 ! 2002-08 (G. Madec) F90: Free form and module |
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| 11 | !! 1.0 ! 2004-02 (G. Madec) vor_een: Original code |
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| 12 | !! - ! 2003-08 (G. Madec) add vor_ctl |
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| 13 | !! - ! 2005-11 (G. Madec) add dyn_vor (new step architecture) |
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| 14 | !! 2.0 ! 2006-11 (G. Madec) flux form advection: add metric term |
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| 15 | !! 3.2 ! 2009-04 (R. Benshila) vvl: correction of een scheme |
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[9019] | 16 | !! 3.3 ! 2010-10 (C. Ethe, G. Madec) reorganisation of initialisation phase |
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| 17 | !! 3.7 ! 2014-04 (G. Madec) trend simplification: suppress jpdyn_trd_dat vorticity |
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| 18 | !! - ! 2014-06 (G. Madec) suppression of velocity curl from in-core memory |
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[7646] | 19 | !! - ! 2016-12 (G. Madec, E. Clementi) add Stokes-Coriolis trends (ln_stcor=T) |
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[9019] | 20 | !! 4.0 ! 2017-07 (G. Madec) linear dynamics + trends diag. with Stokes-Coriolis |
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[9528] | 21 | !! - ! 2018-03 (G. Madec) add two new schemes (ln_dynvor_enT and ln_dynvor_eet) |
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| 22 | !! - ! 2018-04 (G. Madec) add pre-computed gradient for metric term calculation |
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[503] | 23 | !!---------------------------------------------------------------------- |
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[3] | 24 | |
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| 25 | !!---------------------------------------------------------------------- |
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[9019] | 26 | !! dyn_vor : Update the momentum trend with the vorticity trend |
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| 27 | !! vor_ens : enstrophy conserving scheme (ln_dynvor_ens=T) |
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| 28 | !! vor_ene : energy conserving scheme (ln_dynvor_ene=T) |
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| 29 | !! vor_een : energy and enstrophy conserving (ln_dynvor_een=T) |
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| 30 | !! dyn_vor_init : set and control of the different vorticity option |
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[3] | 31 | !!---------------------------------------------------------------------- |
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[503] | 32 | USE oce ! ocean dynamics and tracers |
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| 33 | USE dom_oce ! ocean space and time domain |
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[3294] | 34 | USE dommsk ! ocean mask |
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[9019] | 35 | USE dynadv ! momentum advection |
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[4990] | 36 | USE trd_oce ! trends: ocean variables |
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| 37 | USE trddyn ! trend manager: dynamics |
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[7646] | 38 | USE sbcwave ! Surface Waves (add Stokes-Coriolis force) |
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| 39 | USE sbc_oce , ONLY : ln_stcor ! use Stoke-Coriolis force |
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[5836] | 40 | ! |
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[503] | 41 | USE lbclnk ! ocean lateral boundary conditions (or mpp link) |
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| 42 | USE prtctl ! Print control |
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| 43 | USE in_out_manager ! I/O manager |
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[3294] | 44 | USE lib_mpp ! MPP library |
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| 45 | USE timing ! Timing |
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[3] | 46 | |
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| 47 | IMPLICIT NONE |
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| 48 | PRIVATE |
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| 49 | |
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[2528] | 50 | PUBLIC dyn_vor ! routine called by step.F90 |
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[5836] | 51 | PUBLIC dyn_vor_init ! routine called by nemogcm.F90 |
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[3] | 52 | |
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[4147] | 53 | ! !!* Namelist namdyn_vor: vorticity term |
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[9528] | 54 | LOGICAL, PUBLIC :: ln_dynvor_ens !: enstrophy conserving scheme (ENS) |
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| 55 | LOGICAL, PUBLIC :: ln_dynvor_ene !: f-point energy conserving scheme (ENE) |
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| 56 | LOGICAL, PUBLIC :: ln_dynvor_enT !: t-point energy conserving scheme (ENT) |
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| 57 | LOGICAL, PUBLIC :: ln_dynvor_eeT !: t-point energy conserving scheme (EET) |
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| 58 | LOGICAL, PUBLIC :: ln_dynvor_een !: energy & enstrophy conserving scheme (EEN) |
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[5836] | 59 | INTEGER, PUBLIC :: nn_een_e3f !: e3f=masked averaging of e3t divided by 4 (=0) or by the sum of mask (=1) |
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[9528] | 60 | LOGICAL, PUBLIC :: ln_dynvor_mix !: mixed scheme (MIX) |
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[5836] | 61 | LOGICAL, PUBLIC :: ln_dynvor_msk !: vorticity multiplied by fmask (=T) or not (=F) (all vorticity schemes) |
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[3] | 62 | |
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[9528] | 63 | INTEGER, PUBLIC :: nvor_scheme !: choice of the type of advection scheme |
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| 64 | ! ! associated indices: |
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| 65 | INTEGER, PUBLIC, PARAMETER :: np_ENS = 0 ! ENS scheme |
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[5836] | 66 | INTEGER, PUBLIC, PARAMETER :: np_ENE = 1 ! ENE scheme |
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[9528] | 67 | INTEGER, PUBLIC, PARAMETER :: np_ENT = 2 ! ENT scheme (t-point vorticity) |
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| 68 | INTEGER, PUBLIC, PARAMETER :: np_EET = 3 ! EET scheme (EEN using e3t) |
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[5836] | 69 | INTEGER, PUBLIC, PARAMETER :: np_EEN = 4 ! EEN scheme |
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[9528] | 70 | INTEGER, PUBLIC, PARAMETER :: np_MIX = 5 ! MIX scheme |
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[455] | 71 | |
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[5836] | 72 | INTEGER :: ncor, nrvm, ntot ! choice of calculated vorticity |
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| 73 | ! ! associated indices: |
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[9528] | 74 | INTEGER, PUBLIC, PARAMETER :: np_COR = 1 ! Coriolis (planetary) |
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| 75 | INTEGER, PUBLIC, PARAMETER :: np_RVO = 2 ! relative vorticity |
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| 76 | INTEGER, PUBLIC, PARAMETER :: np_MET = 3 ! metric term |
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| 77 | INTEGER, PUBLIC, PARAMETER :: np_CRV = 4 ! relative + planetary (total vorticity) |
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| 78 | INTEGER, PUBLIC, PARAMETER :: np_CME = 5 ! Coriolis + metric term |
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| 79 | |
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| 80 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: di_e2u_2 ! = di(e2u)/2 used in T-point metric term calculation |
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| 81 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: dj_e1v_2 ! = dj(e1v)/2 - - - - |
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| 82 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: di_e2v_2e1e2f ! = di(e2u)/(2*e1e2f) used in F-point metric term calculation |
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| 83 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: dj_e1u_2e1e2f ! = dj(e1v)/(2*e1e2f) - - - - |
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[5836] | 84 | |
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| 85 | REAL(wp) :: r1_4 = 0.250_wp ! =1/4 |
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| 86 | REAL(wp) :: r1_8 = 0.125_wp ! =1/8 |
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| 87 | REAL(wp) :: r1_12 = 1._wp / 12._wp ! 1/12 |
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| 88 | |
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[3] | 89 | !! * Substitutions |
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[12377] | 90 | # include "do_loop_substitute.h90" |
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[3] | 91 | !!---------------------------------------------------------------------- |
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[9598] | 92 | !! NEMO/OCE 4.0 , NEMO Consortium (2018) |
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[1152] | 93 | !! $Id$ |
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[10068] | 94 | !! Software governed by the CeCILL license (see ./LICENSE) |
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[3] | 95 | !!---------------------------------------------------------------------- |
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| 96 | CONTAINS |
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| 97 | |
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[12377] | 98 | SUBROUTINE dyn_vor( kt, Kmm, puu, pvv, Krhs ) |
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[3] | 99 | !!---------------------------------------------------------------------- |
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| 100 | !! |
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[455] | 101 | !! ** Purpose : compute the lateral ocean tracer physics. |
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| 102 | !! |
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[12377] | 103 | !! ** Action : - Update (puu(:,:,:,Krhs),pvv(:,:,:,Krhs)) with the now vorticity term trend |
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[503] | 104 | !! - save the trends in (ztrdu,ztrdv) in 2 parts (relative |
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[4990] | 105 | !! and planetary vorticity trends) and send them to trd_dyn |
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| 106 | !! for futher diagnostics (l_trddyn=T) |
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[503] | 107 | !!---------------------------------------------------------------------- |
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[12377] | 108 | INTEGER , INTENT( in ) :: kt ! ocean time-step index |
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| 109 | INTEGER , INTENT( in ) :: Kmm, Krhs ! ocean time level indices |
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| 110 | REAL(wp), DIMENSION(jpi,jpj,jpk,jpt), INTENT(inout) :: puu, pvv ! ocean velocity field and RHS of momentum equation |
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[2715] | 111 | ! |
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[9019] | 112 | REAL(wp), ALLOCATABLE, DIMENSION(:,:,:) :: ztrdu, ztrdv |
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[455] | 113 | !!---------------------------------------------------------------------- |
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[2715] | 114 | ! |
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[9019] | 115 | IF( ln_timing ) CALL timing_start('dyn_vor') |
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[3294] | 116 | ! |
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[9019] | 117 | IF( l_trddyn ) THEN !== trend diagnostics case : split the added trend in two parts ==! |
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| 118 | ! |
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| 119 | ALLOCATE( ztrdu(jpi,jpj,jpk), ztrdv(jpi,jpj,jpk) ) |
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| 120 | ! |
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[12377] | 121 | ztrdu(:,:,:) = puu(:,:,:,Krhs) !* planetary vorticity trend (including Stokes-Coriolis force) |
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| 122 | ztrdv(:,:,:) = pvv(:,:,:,Krhs) |
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[9019] | 123 | SELECT CASE( nvor_scheme ) |
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[12377] | 124 | CASE( np_ENS ) ; CALL vor_ens( kt, Kmm, ncor, puu(:,:,:,Kmm) , pvv(:,:,:,Kmm) , puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! enstrophy conserving scheme |
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| 125 | IF( ln_stcor ) CALL vor_ens( kt, Kmm, ncor, usd, vsd, puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! add the Stokes-Coriolis trend |
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| 126 | CASE( np_ENE, np_MIX ) ; CALL vor_ene( kt, Kmm, ncor, puu(:,:,:,Kmm) , pvv(:,:,:,Kmm) , puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! energy conserving scheme |
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| 127 | IF( ln_stcor ) CALL vor_ene( kt, Kmm, ncor, usd, vsd, puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! add the Stokes-Coriolis trend |
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| 128 | CASE( np_ENT ) ; CALL vor_enT( kt, Kmm, ncor, puu(:,:,:,Kmm) , pvv(:,:,:,Kmm) , puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! energy conserving scheme (T-pts) |
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| 129 | IF( ln_stcor ) CALL vor_enT( kt, Kmm, ncor, usd, vsd, puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! add the Stokes-Coriolis trend |
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| 130 | CASE( np_EET ) ; CALL vor_eeT( kt, Kmm, ncor, puu(:,:,:,Kmm) , pvv(:,:,:,Kmm) , puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! energy conserving scheme (een with e3t) |
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| 131 | IF( ln_stcor ) CALL vor_eeT( kt, Kmm, ncor, usd, vsd, puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! add the Stokes-Coriolis trend |
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| 132 | CASE( np_EEN ) ; CALL vor_een( kt, Kmm, ncor, puu(:,:,:,Kmm) , pvv(:,:,:,Kmm) , puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! energy & enstrophy scheme |
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| 133 | IF( ln_stcor ) CALL vor_een( kt, Kmm, ncor, usd, vsd, puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! add the Stokes-Coriolis trend |
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[9019] | 134 | END SELECT |
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[12377] | 135 | ztrdu(:,:,:) = puu(:,:,:,Krhs) - ztrdu(:,:,:) |
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| 136 | ztrdv(:,:,:) = pvv(:,:,:,Krhs) - ztrdv(:,:,:) |
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| 137 | CALL trd_dyn( ztrdu, ztrdv, jpdyn_pvo, kt, Kmm ) |
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[9019] | 138 | ! |
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| 139 | IF( n_dynadv /= np_LIN_dyn ) THEN !* relative vorticity or metric trend (only in non-linear case) |
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[12377] | 140 | ztrdu(:,:,:) = puu(:,:,:,Krhs) |
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| 141 | ztrdv(:,:,:) = pvv(:,:,:,Krhs) |
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[9019] | 142 | SELECT CASE( nvor_scheme ) |
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[12377] | 143 | CASE( np_ENT ) ; CALL vor_enT( kt, Kmm, nrvm, puu(:,:,:,Kmm) , pvv(:,:,:,Kmm) , puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! energy conserving scheme (T-pts) |
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| 144 | CASE( np_EET ) ; CALL vor_eeT( kt, Kmm, nrvm, puu(:,:,:,Kmm) , pvv(:,:,:,Kmm) , puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! energy conserving scheme (een with e3t) |
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| 145 | CASE( np_ENE ) ; CALL vor_ene( kt, Kmm, nrvm, puu(:,:,:,Kmm) , pvv(:,:,:,Kmm) , puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! energy conserving scheme |
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| 146 | CASE( np_ENS, np_MIX ) ; CALL vor_ens( kt, Kmm, nrvm, puu(:,:,:,Kmm) , pvv(:,:,:,Kmm) , puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! enstrophy conserving scheme |
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| 147 | CASE( np_EEN ) ; CALL vor_een( kt, Kmm, nrvm, puu(:,:,:,Kmm) , pvv(:,:,:,Kmm) , puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! energy & enstrophy scheme |
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[9019] | 148 | END SELECT |
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[12377] | 149 | ztrdu(:,:,:) = puu(:,:,:,Krhs) - ztrdu(:,:,:) |
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| 150 | ztrdv(:,:,:) = pvv(:,:,:,Krhs) - ztrdv(:,:,:) |
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| 151 | CALL trd_dyn( ztrdu, ztrdv, jpdyn_rvo, kt, Kmm ) |
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[9019] | 152 | ENDIF |
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| 153 | ! |
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| 154 | DEALLOCATE( ztrdu, ztrdv ) |
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| 155 | ! |
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| 156 | ELSE !== total vorticity trend added to the general trend ==! |
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| 157 | ! |
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| 158 | SELECT CASE ( nvor_scheme ) !== vorticity trend added to the general trend ==! |
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[9528] | 159 | CASE( np_ENT ) !* energy conserving scheme (T-pts) |
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[12377] | 160 | CALL vor_enT( kt, Kmm, ntot, puu(:,:,:,Kmm) , pvv(:,:,:,Kmm) , puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! total vorticity trend |
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| 161 | IF( ln_stcor ) CALL vor_enT( kt, Kmm, ncor, usd, vsd, puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! add the Stokes-Coriolis trend |
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[9528] | 162 | CASE( np_EET ) !* energy conserving scheme (een scheme using e3t) |
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[12377] | 163 | CALL vor_eeT( kt, Kmm, ntot, puu(:,:,:,Kmm) , pvv(:,:,:,Kmm) , puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! total vorticity trend |
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| 164 | IF( ln_stcor ) CALL vor_eeT( kt, Kmm, ncor, usd, vsd, puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! add the Stokes-Coriolis trend |
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[9019] | 165 | CASE( np_ENE ) !* energy conserving scheme |
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[12377] | 166 | CALL vor_ene( kt, Kmm, ntot, puu(:,:,:,Kmm) , pvv(:,:,:,Kmm) , puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! total vorticity trend |
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| 167 | IF( ln_stcor ) CALL vor_ene( kt, Kmm, ncor, usd, vsd, puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! add the Stokes-Coriolis trend |
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[9019] | 168 | CASE( np_ENS ) !* enstrophy conserving scheme |
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[12377] | 169 | CALL vor_ens( kt, Kmm, ntot, puu(:,:,:,Kmm) , pvv(:,:,:,Kmm) , puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! total vorticity trend |
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| 170 | IF( ln_stcor ) CALL vor_ens( kt, Kmm, ncor, usd, vsd, puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! add the Stokes-Coriolis trend |
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[9019] | 171 | CASE( np_MIX ) !* mixed ene-ens scheme |
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[12377] | 172 | CALL vor_ens( kt, Kmm, nrvm, puu(:,:,:,Kmm) , pvv(:,:,:,Kmm) , puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! relative vorticity or metric trend (ens) |
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| 173 | CALL vor_ene( kt, Kmm, ncor, puu(:,:,:,Kmm) , pvv(:,:,:,Kmm) , puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! planetary vorticity trend (ene) |
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| 174 | IF( ln_stcor ) CALL vor_ene( kt, Kmm, ncor, usd, vsd, puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! add the Stokes-Coriolis trend |
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[9019] | 175 | CASE( np_EEN ) !* energy and enstrophy conserving scheme |
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[12377] | 176 | CALL vor_een( kt, Kmm, ntot, puu(:,:,:,Kmm) , pvv(:,:,:,Kmm) , puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! total vorticity trend |
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| 177 | IF( ln_stcor ) CALL vor_een( kt, Kmm, ncor, usd, vsd, puu(:,:,:,Krhs), pvv(:,:,:,Krhs) ) ! add the Stokes-Coriolis trend |
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[9019] | 178 | END SELECT |
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[643] | 179 | ! |
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[9019] | 180 | ENDIF |
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[2715] | 181 | ! |
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[455] | 182 | ! ! print sum trends (used for debugging) |
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[12377] | 183 | IF(sn_cfctl%l_prtctl) CALL prt_ctl( tab3d_1=puu(:,:,:,Krhs), clinfo1=' vor - Ua: ', mask1=umask, & |
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| 184 | & tab3d_2=pvv(:,:,:,Krhs), clinfo2= ' Va: ', mask2=vmask, clinfo3='dyn' ) |
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[1438] | 185 | ! |
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[9019] | 186 | IF( ln_timing ) CALL timing_stop('dyn_vor') |
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[3294] | 187 | ! |
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[455] | 188 | END SUBROUTINE dyn_vor |
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| 189 | |
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| 190 | |
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[12377] | 191 | SUBROUTINE vor_enT( kt, Kmm, kvor, pu, pv, pu_rhs, pv_rhs ) |
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[9528] | 192 | !!---------------------------------------------------------------------- |
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| 193 | !! *** ROUTINE vor_enT *** |
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| 194 | !! |
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| 195 | !! ** Purpose : Compute the now total vorticity trend and add it to |
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| 196 | !! the general trend of the momentum equation. |
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| 197 | !! |
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| 198 | !! ** Method : Trend evaluated using now fields (centered in time) |
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| 199 | !! and t-point evaluation of vorticity (planetary and relative). |
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| 200 | !! conserves the horizontal kinetic energy. |
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| 201 | !! The general trend of momentum is increased due to the vorticity |
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| 202 | !! term which is given by: |
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| 203 | !! voru = 1/bu mj[ ( mi(mj(bf*rvor))+bt*f_t)/e3t mj[vn] ] |
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| 204 | !! vorv = 1/bv mi[ ( mi(mj(bf*rvor))+bt*f_t)/e3f mj[un] ] |
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| 205 | !! where rvor is the relative vorticity at f-point |
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| 206 | !! |
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[12377] | 207 | !! ** Action : - Update (pu_rhs,pv_rhs) with the now vorticity term trend |
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[9528] | 208 | !!---------------------------------------------------------------------- |
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| 209 | INTEGER , INTENT(in ) :: kt ! ocean time-step index |
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[12377] | 210 | INTEGER , INTENT(in ) :: Kmm ! ocean time level index |
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[9528] | 211 | INTEGER , INTENT(in ) :: kvor ! total, planetary, relative, or metric |
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| 212 | REAL(wp), DIMENSION(jpi,jpj,jpk), INTENT(inout) :: pu, pv ! now velocities |
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| 213 | REAL(wp), DIMENSION(jpi,jpj,jpk), INTENT(inout) :: pu_rhs, pv_rhs ! total v-trend |
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| 214 | ! |
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| 215 | INTEGER :: ji, jj, jk ! dummy loop indices |
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| 216 | REAL(wp) :: zx1, zy1, zx2, zy2 ! local scalars |
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[10425] | 217 | REAL(wp), DIMENSION(jpi,jpj) :: zwx, zwy, zwt ! 2D workspace |
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| 218 | REAL(wp), DIMENSION(jpi,jpj,jpk) :: zwz ! 3D workspace |
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[9528] | 219 | !!---------------------------------------------------------------------- |
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| 220 | ! |
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| 221 | IF( kt == nit000 ) THEN |
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| 222 | IF(lwp) WRITE(numout,*) |
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| 223 | IF(lwp) WRITE(numout,*) 'dyn:vor_enT : vorticity term: t-point energy conserving scheme' |
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| 224 | IF(lwp) WRITE(numout,*) '~~~~~~~~~~~' |
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| 225 | ENDIF |
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| 226 | ! |
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[10425] | 227 | ! |
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| 228 | SELECT CASE( kvor ) !== volume weighted vorticity considered ==! |
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| 229 | CASE ( np_RVO ) !* relative vorticity |
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| 230 | DO jk = 1, jpkm1 ! Horizontal slab |
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[12377] | 231 | DO_2D_10_10 |
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| 232 | zwz(ji,jj,jk) = ( e2v(ji+1,jj) * pv(ji+1,jj,jk) - e2v(ji,jj) * pv(ji,jj,jk) & |
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| 233 | & - e1u(ji,jj+1) * pu(ji,jj+1,jk) + e1u(ji,jj) * pu(ji,jj,jk) ) * r1_e1e2f(ji,jj) |
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| 234 | END_2D |
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[9528] | 235 | IF( ln_dynvor_msk ) THEN ! mask/unmask relative vorticity |
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[12377] | 236 | DO_2D_10_10 |
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| 237 | zwz(ji,jj,jk) = zwz(ji,jj,jk) * fmask(ji,jj,jk) |
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| 238 | END_2D |
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[9528] | 239 | ENDIF |
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[10425] | 240 | END DO |
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| 241 | |
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| 242 | CALL lbc_lnk( 'dynvor', zwz, 'F', 1. ) |
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| 243 | |
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| 244 | CASE ( np_CRV ) !* Coriolis + relative vorticity |
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| 245 | DO jk = 1, jpkm1 ! Horizontal slab |
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[12377] | 246 | DO_2D_10_10 |
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| 247 | zwz(ji,jj,jk) = ( e2v(ji+1,jj) * pv(ji+1,jj,jk) - e2v(ji,jj) * pv(ji,jj,jk) & |
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| 248 | & - e1u(ji,jj+1) * pu(ji,jj+1,jk) + e1u(ji,jj) * pu(ji,jj,jk) ) * r1_e1e2f(ji,jj) |
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| 249 | END_2D |
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[10425] | 250 | IF( ln_dynvor_msk ) THEN ! mask/unmask relative vorticity |
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[12377] | 251 | DO_2D_10_10 |
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| 252 | zwz(ji,jj,jk) = zwz(ji,jj,jk) * fmask(ji,jj,jk) |
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| 253 | END_2D |
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[10425] | 254 | ENDIF |
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| 255 | END DO |
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| 256 | |
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| 257 | CALL lbc_lnk( 'dynvor', zwz, 'F', 1. ) |
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| 258 | |
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| 259 | END SELECT |
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| 260 | |
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| 261 | ! ! =============== |
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| 262 | DO jk = 1, jpkm1 ! Horizontal slab |
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| 263 | ! ! =============== |
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| 264 | |
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| 265 | SELECT CASE( kvor ) !== volume weighted vorticity considered ==! |
---|
| 266 | CASE ( np_COR ) !* Coriolis (planetary vorticity) |
---|
[12377] | 267 | zwt(:,:) = ff_t(:,:) * e1e2t(:,:)*e3t(:,:,jk,Kmm) |
---|
[10425] | 268 | CASE ( np_RVO ) !* relative vorticity |
---|
[12377] | 269 | DO_2D_01_01 |
---|
| 270 | zwt(ji,jj) = r1_4 * ( zwz(ji-1,jj ,jk) + zwz(ji,jj ,jk) & |
---|
| 271 | & + zwz(ji-1,jj-1,jk) + zwz(ji,jj-1,jk) ) * e1e2t(ji,jj)*e3t(ji,jj,jk,Kmm) |
---|
| 272 | END_2D |
---|
[9528] | 273 | CASE ( np_MET ) !* metric term |
---|
[12377] | 274 | DO_2D_01_01 |
---|
| 275 | zwt(ji,jj) = ( ( pv(ji,jj,jk) + pv(ji,jj-1,jk) ) * di_e2u_2(ji,jj) & |
---|
| 276 | & - ( pu(ji,jj,jk) + pu(ji-1,jj,jk) ) * dj_e1v_2(ji,jj) ) * e3t(ji,jj,jk,Kmm) |
---|
| 277 | END_2D |
---|
[9528] | 278 | CASE ( np_CRV ) !* Coriolis + relative vorticity |
---|
[12377] | 279 | DO_2D_01_01 |
---|
| 280 | zwt(ji,jj) = ( ff_t(ji,jj) + r1_4 * ( zwz(ji-1,jj ,jk) + zwz(ji,jj ,jk) & |
---|
| 281 | & + zwz(ji-1,jj-1,jk) + zwz(ji,jj-1,jk) ) ) * e1e2t(ji,jj)*e3t(ji,jj,jk,Kmm) |
---|
| 282 | END_2D |
---|
[9528] | 283 | CASE ( np_CME ) !* Coriolis + metric |
---|
[12377] | 284 | DO_2D_01_01 |
---|
| 285 | zwt(ji,jj) = ( ff_t(ji,jj) * e1e2t(ji,jj) & |
---|
| 286 | & + ( pv(ji,jj,jk) + pv(ji,jj-1,jk) ) * di_e2u_2(ji,jj) & |
---|
| 287 | & - ( pu(ji,jj,jk) + pu(ji-1,jj,jk) ) * dj_e1v_2(ji,jj) ) * e3t(ji,jj,jk,Kmm) |
---|
| 288 | END_2D |
---|
[9528] | 289 | CASE DEFAULT ! error |
---|
| 290 | CALL ctl_stop('STOP','dyn_vor: wrong value for kvor' ) |
---|
| 291 | END SELECT |
---|
| 292 | ! |
---|
| 293 | ! !== compute and add the vorticity term trend =! |
---|
[12377] | 294 | DO_2D_00_00 |
---|
| 295 | pu_rhs(ji,jj,jk) = pu_rhs(ji,jj,jk) + r1_4 * r1_e1e2u(ji,jj) / e3u(ji,jj,jk,Kmm) & |
---|
| 296 | & * ( zwt(ji+1,jj) * ( pv(ji+1,jj,jk) + pv(ji+1,jj-1,jk) ) & |
---|
| 297 | & + zwt(ji ,jj) * ( pv(ji ,jj,jk) + pv(ji ,jj-1,jk) ) ) |
---|
| 298 | ! |
---|
| 299 | pv_rhs(ji,jj,jk) = pv_rhs(ji,jj,jk) - r1_4 * r1_e1e2v(ji,jj) / e3v(ji,jj,jk,Kmm) & |
---|
| 300 | & * ( zwt(ji,jj+1) * ( pu(ji,jj+1,jk) + pu(ji-1,jj+1,jk) ) & |
---|
| 301 | & + zwt(ji,jj ) * ( pu(ji,jj ,jk) + pu(ji-1,jj ,jk) ) ) |
---|
| 302 | END_2D |
---|
[9528] | 303 | ! ! =============== |
---|
| 304 | END DO ! End of slab |
---|
| 305 | ! ! =============== |
---|
| 306 | END SUBROUTINE vor_enT |
---|
| 307 | |
---|
| 308 | |
---|
[12377] | 309 | SUBROUTINE vor_ene( kt, Kmm, kvor, pu, pv, pu_rhs, pv_rhs ) |
---|
[455] | 310 | !!---------------------------------------------------------------------- |
---|
| 311 | !! *** ROUTINE vor_ene *** |
---|
| 312 | !! |
---|
[3] | 313 | !! ** Purpose : Compute the now total vorticity trend and add it to |
---|
| 314 | !! the general trend of the momentum equation. |
---|
| 315 | !! |
---|
| 316 | !! ** Method : Trend evaluated using now fields (centered in time) |
---|
[5836] | 317 | !! and the Sadourny (1975) flux form formulation : conserves the |
---|
| 318 | !! horizontal kinetic energy. |
---|
| 319 | !! The general trend of momentum is increased due to the vorticity |
---|
| 320 | !! term which is given by: |
---|
[12377] | 321 | !! voru = 1/e1u mj-1[ (rvor+f)/e3f mi(e1v*e3v pvv(:,:,:,Kmm)) ] |
---|
| 322 | !! vorv = 1/e2v mi-1[ (rvor+f)/e3f mj(e2u*e3u puu(:,:,:,Kmm)) ] |
---|
[5836] | 323 | !! where rvor is the relative vorticity |
---|
[3] | 324 | !! |
---|
[12377] | 325 | !! ** Action : - Update (pu_rhs,pv_rhs) with the now vorticity term trend |
---|
[3] | 326 | !! |
---|
[503] | 327 | !! References : Sadourny, r., 1975, j. atmos. sciences, 32, 680-689. |
---|
[3] | 328 | !!---------------------------------------------------------------------- |
---|
[9019] | 329 | INTEGER , INTENT(in ) :: kt ! ocean time-step index |
---|
[12377] | 330 | INTEGER , INTENT(in ) :: Kmm ! ocean time level index |
---|
[9019] | 331 | INTEGER , INTENT(in ) :: kvor ! total, planetary, relative, or metric |
---|
[12377] | 332 | REAL(wp), DIMENSION(jpi,jpj,jpk), INTENT(inout) :: pu, pv ! now velocities |
---|
| 333 | REAL(wp), DIMENSION(jpi,jpj,jpk), INTENT(inout) :: pu_rhs, pv_rhs ! total v-trend |
---|
[2715] | 334 | ! |
---|
[5836] | 335 | INTEGER :: ji, jj, jk ! dummy loop indices |
---|
| 336 | REAL(wp) :: zx1, zy1, zx2, zy2 ! local scalars |
---|
[9019] | 337 | REAL(wp), DIMENSION(jpi,jpj) :: zwx, zwy, zwz ! 2D workspace |
---|
[3] | 338 | !!---------------------------------------------------------------------- |
---|
[3294] | 339 | ! |
---|
[52] | 340 | IF( kt == nit000 ) THEN |
---|
| 341 | IF(lwp) WRITE(numout,*) |
---|
[455] | 342 | IF(lwp) WRITE(numout,*) 'dyn:vor_ene : vorticity term: energy conserving scheme' |
---|
| 343 | IF(lwp) WRITE(numout,*) '~~~~~~~~~~~' |
---|
[52] | 344 | ENDIF |
---|
[5836] | 345 | ! |
---|
[3] | 346 | ! ! =============== |
---|
| 347 | DO jk = 1, jpkm1 ! Horizontal slab |
---|
| 348 | ! ! =============== |
---|
[1438] | 349 | ! |
---|
[5836] | 350 | SELECT CASE( kvor ) !== vorticity considered ==! |
---|
| 351 | CASE ( np_COR ) !* Coriolis (planetary vorticity) |
---|
[7753] | 352 | zwz(:,:) = ff_f(:,:) |
---|
[5836] | 353 | CASE ( np_RVO ) !* relative vorticity |
---|
[12377] | 354 | DO_2D_10_10 |
---|
| 355 | zwz(ji,jj) = ( e2v(ji+1,jj ) * pv(ji+1,jj ,jk) - e2v(ji,jj) * pv(ji,jj,jk) & |
---|
| 356 | & - e1u(ji ,jj+1) * pu(ji ,jj+1,jk) + e1u(ji,jj) * pu(ji,jj,jk) ) * r1_e1e2f(ji,jj) |
---|
| 357 | END_2D |
---|
[5836] | 358 | CASE ( np_MET ) !* metric term |
---|
[12377] | 359 | DO_2D_10_10 |
---|
| 360 | zwz(ji,jj) = ( pv(ji+1,jj ,jk) + pv(ji,jj,jk) ) * di_e2v_2e1e2f(ji,jj) & |
---|
| 361 | & - ( pu(ji ,jj+1,jk) + pu(ji,jj,jk) ) * dj_e1u_2e1e2f(ji,jj) |
---|
| 362 | END_2D |
---|
[5836] | 363 | CASE ( np_CRV ) !* Coriolis + relative vorticity |
---|
[12377] | 364 | DO_2D_10_10 |
---|
| 365 | zwz(ji,jj) = ff_f(ji,jj) + ( e2v(ji+1,jj) * pv(ji+1,jj,jk) - e2v(ji,jj) * pv(ji,jj,jk) & |
---|
| 366 | & - e1u(ji,jj+1) * pu(ji,jj+1,jk) + e1u(ji,jj) * pu(ji,jj,jk) ) * r1_e1e2f(ji,jj) |
---|
| 367 | END_2D |
---|
[5836] | 368 | CASE ( np_CME ) !* Coriolis + metric |
---|
[12377] | 369 | DO_2D_10_10 |
---|
| 370 | zwz(ji,jj) = ff_f(ji,jj) + ( pv(ji+1,jj ,jk) + pv(ji,jj,jk) ) * di_e2v_2e1e2f(ji,jj) & |
---|
| 371 | & - ( pu(ji ,jj+1,jk) + pu(ji,jj,jk) ) * dj_e1u_2e1e2f(ji,jj) |
---|
| 372 | END_2D |
---|
[5836] | 373 | CASE DEFAULT ! error |
---|
| 374 | CALL ctl_stop('STOP','dyn_vor: wrong value for kvor' ) |
---|
[455] | 375 | END SELECT |
---|
[5836] | 376 | ! |
---|
| 377 | IF( ln_dynvor_msk ) THEN !== mask/unmask vorticity ==! |
---|
[12377] | 378 | DO_2D_10_10 |
---|
| 379 | zwz(ji,jj) = zwz(ji,jj) * fmask(ji,jj,jk) |
---|
| 380 | END_2D |
---|
[5836] | 381 | ENDIF |
---|
[455] | 382 | |
---|
| 383 | IF( ln_sco ) THEN |
---|
[12377] | 384 | zwz(:,:) = zwz(:,:) / e3f(:,:,jk) |
---|
| 385 | zwx(:,:) = e2u(:,:) * e3u(:,:,jk,Kmm) * pu(:,:,jk) |
---|
| 386 | zwy(:,:) = e1v(:,:) * e3v(:,:,jk,Kmm) * pv(:,:,jk) |
---|
[3] | 387 | ELSE |
---|
[12377] | 388 | zwx(:,:) = e2u(:,:) * pu(:,:,jk) |
---|
| 389 | zwy(:,:) = e1v(:,:) * pv(:,:,jk) |
---|
[3] | 390 | ENDIF |
---|
[5836] | 391 | ! !== compute and add the vorticity term trend =! |
---|
[12377] | 392 | DO_2D_00_00 |
---|
| 393 | zy1 = zwy(ji,jj-1) + zwy(ji+1,jj-1) |
---|
| 394 | zy2 = zwy(ji,jj ) + zwy(ji+1,jj ) |
---|
| 395 | zx1 = zwx(ji-1,jj) + zwx(ji-1,jj+1) |
---|
| 396 | zx2 = zwx(ji ,jj) + zwx(ji ,jj+1) |
---|
| 397 | pu_rhs(ji,jj,jk) = pu_rhs(ji,jj,jk) + r1_4 * r1_e1u(ji,jj) * ( zwz(ji ,jj-1) * zy1 + zwz(ji,jj) * zy2 ) |
---|
| 398 | pv_rhs(ji,jj,jk) = pv_rhs(ji,jj,jk) - r1_4 * r1_e2v(ji,jj) * ( zwz(ji-1,jj ) * zx1 + zwz(ji,jj) * zx2 ) |
---|
| 399 | END_2D |
---|
[3] | 400 | ! ! =============== |
---|
| 401 | END DO ! End of slab |
---|
| 402 | ! ! =============== |
---|
[455] | 403 | END SUBROUTINE vor_ene |
---|
[216] | 404 | |
---|
| 405 | |
---|
[12377] | 406 | SUBROUTINE vor_ens( kt, Kmm, kvor, pu, pv, pu_rhs, pv_rhs ) |
---|
[3] | 407 | !!---------------------------------------------------------------------- |
---|
[455] | 408 | !! *** ROUTINE vor_ens *** |
---|
[3] | 409 | !! |
---|
| 410 | !! ** Purpose : Compute the now total vorticity trend and add it to |
---|
| 411 | !! the general trend of the momentum equation. |
---|
| 412 | !! |
---|
| 413 | !! ** Method : Trend evaluated using now fields (centered in time) |
---|
| 414 | !! and the Sadourny (1975) flux FORM formulation : conserves the |
---|
| 415 | !! potential enstrophy of a horizontally non-divergent flow. the |
---|
| 416 | !! trend of the vorticity term is given by: |
---|
[12377] | 417 | !! voru = 1/e1u mj-1[ (rvor+f)/e3f ] mj-1[ mi(e1v*e3v pvv(:,:,:,Kmm)) ] |
---|
| 418 | !! vorv = 1/e2v mi-1[ (rvor+f)/e3f ] mi-1[ mj(e2u*e3u puu(:,:,:,Kmm)) ] |
---|
| 419 | !! Add this trend to the general momentum trend: |
---|
| 420 | !! (u(rhs),v(Krhs)) = (u(rhs),v(Krhs)) + ( voru , vorv ) |
---|
[3] | 421 | !! |
---|
[12377] | 422 | !! ** Action : - Update (pu_rhs,pv_rhs)) arrays with the now vorticity term trend |
---|
[3] | 423 | !! |
---|
[503] | 424 | !! References : Sadourny, r., 1975, j. atmos. sciences, 32, 680-689. |
---|
[3] | 425 | !!---------------------------------------------------------------------- |
---|
[9019] | 426 | INTEGER , INTENT(in ) :: kt ! ocean time-step index |
---|
[12377] | 427 | INTEGER , INTENT(in ) :: Kmm ! ocean time level index |
---|
[9019] | 428 | INTEGER , INTENT(in ) :: kvor ! total, planetary, relative, or metric |
---|
[12377] | 429 | REAL(wp), DIMENSION(jpi,jpj,jpk), INTENT(inout) :: pu, pv ! now velocities |
---|
| 430 | REAL(wp), DIMENSION(jpi,jpj,jpk), INTENT(inout) :: pu_rhs, pv_rhs ! total v-trend |
---|
[2715] | 431 | ! |
---|
[5836] | 432 | INTEGER :: ji, jj, jk ! dummy loop indices |
---|
| 433 | REAL(wp) :: zuav, zvau ! local scalars |
---|
[9019] | 434 | REAL(wp), DIMENSION(jpi,jpj) :: zwx, zwy, zwz, zww ! 2D workspace |
---|
[3] | 435 | !!---------------------------------------------------------------------- |
---|
[3294] | 436 | ! |
---|
[52] | 437 | IF( kt == nit000 ) THEN |
---|
| 438 | IF(lwp) WRITE(numout,*) |
---|
[455] | 439 | IF(lwp) WRITE(numout,*) 'dyn:vor_ens : vorticity term: enstrophy conserving scheme' |
---|
| 440 | IF(lwp) WRITE(numout,*) '~~~~~~~~~~~' |
---|
[52] | 441 | ENDIF |
---|
[3] | 442 | ! ! =============== |
---|
| 443 | DO jk = 1, jpkm1 ! Horizontal slab |
---|
| 444 | ! ! =============== |
---|
[1438] | 445 | ! |
---|
[5836] | 446 | SELECT CASE( kvor ) !== vorticity considered ==! |
---|
| 447 | CASE ( np_COR ) !* Coriolis (planetary vorticity) |
---|
[7646] | 448 | zwz(:,:) = ff_f(:,:) |
---|
[5836] | 449 | CASE ( np_RVO ) !* relative vorticity |
---|
[12377] | 450 | DO_2D_10_10 |
---|
| 451 | zwz(ji,jj) = ( e2v(ji+1,jj ) * pv(ji+1,jj ,jk) - e2v(ji,jj) * pv(ji,jj,jk) & |
---|
| 452 | & - e1u(ji ,jj+1) * pu(ji ,jj+1,jk) + e1u(ji,jj) * pu(ji,jj,jk) ) * r1_e1e2f(ji,jj) |
---|
| 453 | END_2D |
---|
[5836] | 454 | CASE ( np_MET ) !* metric term |
---|
[12377] | 455 | DO_2D_10_10 |
---|
| 456 | zwz(ji,jj) = ( pv(ji+1,jj ,jk) + pv(ji,jj,jk) ) * di_e2v_2e1e2f(ji,jj) & |
---|
| 457 | & - ( pu(ji ,jj+1,jk) + pu(ji,jj,jk) ) * dj_e1u_2e1e2f(ji,jj) |
---|
| 458 | END_2D |
---|
[5836] | 459 | CASE ( np_CRV ) !* Coriolis + relative vorticity |
---|
[12377] | 460 | DO_2D_10_10 |
---|
| 461 | zwz(ji,jj) = ff_f(ji,jj) + ( e2v(ji+1,jj ) * pv(ji+1,jj ,jk) - e2v(ji,jj) * pv(ji,jj,jk) & |
---|
| 462 | & - e1u(ji ,jj+1) * pu(ji ,jj+1,jk) + e1u(ji,jj) * pu(ji,jj,jk) ) * r1_e1e2f(ji,jj) |
---|
| 463 | END_2D |
---|
[5836] | 464 | CASE ( np_CME ) !* Coriolis + metric |
---|
[12377] | 465 | DO_2D_10_10 |
---|
| 466 | zwz(ji,jj) = ff_f(ji,jj) + ( pv(ji+1,jj ,jk) + pv(ji,jj,jk) ) * di_e2v_2e1e2f(ji,jj) & |
---|
| 467 | & - ( pu(ji ,jj+1,jk) + pu(ji,jj,jk) ) * dj_e1u_2e1e2f(ji,jj) |
---|
| 468 | END_2D |
---|
[5836] | 469 | CASE DEFAULT ! error |
---|
| 470 | CALL ctl_stop('STOP','dyn_vor: wrong value for kvor' ) |
---|
[455] | 471 | END SELECT |
---|
[1438] | 472 | ! |
---|
[5836] | 473 | IF( ln_dynvor_msk ) THEN !== mask/unmask vorticity ==! |
---|
[12377] | 474 | DO_2D_10_10 |
---|
| 475 | zwz(ji,jj) = zwz(ji,jj) * fmask(ji,jj,jk) |
---|
| 476 | END_2D |
---|
[5836] | 477 | ENDIF |
---|
| 478 | ! |
---|
| 479 | IF( ln_sco ) THEN !== horizontal fluxes ==! |
---|
[12377] | 480 | zwz(:,:) = zwz(:,:) / e3f(:,:,jk) |
---|
| 481 | zwx(:,:) = e2u(:,:) * e3u(:,:,jk,Kmm) * pu(:,:,jk) |
---|
| 482 | zwy(:,:) = e1v(:,:) * e3v(:,:,jk,Kmm) * pv(:,:,jk) |
---|
[3] | 483 | ELSE |
---|
[12377] | 484 | zwx(:,:) = e2u(:,:) * pu(:,:,jk) |
---|
| 485 | zwy(:,:) = e1v(:,:) * pv(:,:,jk) |
---|
[3] | 486 | ENDIF |
---|
[5836] | 487 | ! !== compute and add the vorticity term trend =! |
---|
[12377] | 488 | DO_2D_00_00 |
---|
| 489 | zuav = r1_8 * r1_e1u(ji,jj) * ( zwy(ji ,jj-1) + zwy(ji+1,jj-1) & |
---|
| 490 | & + zwy(ji ,jj ) + zwy(ji+1,jj ) ) |
---|
| 491 | zvau =-r1_8 * r1_e2v(ji,jj) * ( zwx(ji-1,jj ) + zwx(ji-1,jj+1) & |
---|
| 492 | & + zwx(ji ,jj ) + zwx(ji ,jj+1) ) |
---|
| 493 | pu_rhs(ji,jj,jk) = pu_rhs(ji,jj,jk) + zuav * ( zwz(ji ,jj-1) + zwz(ji,jj) ) |
---|
| 494 | pv_rhs(ji,jj,jk) = pv_rhs(ji,jj,jk) + zvau * ( zwz(ji-1,jj ) + zwz(ji,jj) ) |
---|
| 495 | END_2D |
---|
[3] | 496 | ! ! =============== |
---|
| 497 | END DO ! End of slab |
---|
| 498 | ! ! =============== |
---|
[455] | 499 | END SUBROUTINE vor_ens |
---|
[216] | 500 | |
---|
| 501 | |
---|
[12377] | 502 | SUBROUTINE vor_een( kt, Kmm, kvor, pu, pv, pu_rhs, pv_rhs ) |
---|
[108] | 503 | !!---------------------------------------------------------------------- |
---|
[455] | 504 | !! *** ROUTINE vor_een *** |
---|
[108] | 505 | !! |
---|
| 506 | !! ** Purpose : Compute the now total vorticity trend and add it to |
---|
| 507 | !! the general trend of the momentum equation. |
---|
| 508 | !! |
---|
| 509 | !! ** Method : Trend evaluated using now fields (centered in time) |
---|
[1438] | 510 | !! and the Arakawa and Lamb (1980) flux form formulation : conserves |
---|
[108] | 511 | !! both the horizontal kinetic energy and the potential enstrophy |
---|
[1438] | 512 | !! when horizontal divergence is zero (see the NEMO documentation) |
---|
[12377] | 513 | !! Add this trend to the general momentum trend (pu_rhs,pv_rhs). |
---|
[108] | 514 | !! |
---|
[12377] | 515 | !! ** Action : - Update (pu_rhs,pv_rhs) with the now vorticity term trend |
---|
[108] | 516 | !! |
---|
[503] | 517 | !! References : Arakawa and Lamb 1980, Mon. Wea. Rev., 109, 18-36 |
---|
| 518 | !!---------------------------------------------------------------------- |
---|
[9019] | 519 | INTEGER , INTENT(in ) :: kt ! ocean time-step index |
---|
[12377] | 520 | INTEGER , INTENT(in ) :: Kmm ! ocean time level index |
---|
[9019] | 521 | INTEGER , INTENT(in ) :: kvor ! total, planetary, relative, or metric |
---|
[12377] | 522 | REAL(wp), DIMENSION(jpi,jpj,jpk), INTENT(inout) :: pu, pv ! now velocities |
---|
| 523 | REAL(wp), DIMENSION(jpi,jpj,jpk), INTENT(inout) :: pu_rhs, pv_rhs ! total v-trend |
---|
[5836] | 524 | ! |
---|
| 525 | INTEGER :: ji, jj, jk ! dummy loop indices |
---|
| 526 | INTEGER :: ierr ! local integer |
---|
| 527 | REAL(wp) :: zua, zva ! local scalars |
---|
[9528] | 528 | REAL(wp) :: zmsk, ze3f ! local scalars |
---|
[10425] | 529 | REAL(wp), DIMENSION(jpi,jpj) :: zwx , zwy , z1_e3f |
---|
| 530 | REAL(wp), DIMENSION(jpi,jpj) :: ztnw, ztne, ztsw, ztse |
---|
| 531 | REAL(wp), DIMENSION(jpi,jpj,jpk) :: zwz |
---|
[108] | 532 | !!---------------------------------------------------------------------- |
---|
[3294] | 533 | ! |
---|
[108] | 534 | IF( kt == nit000 ) THEN |
---|
| 535 | IF(lwp) WRITE(numout,*) |
---|
[455] | 536 | IF(lwp) WRITE(numout,*) 'dyn:vor_een : vorticity term: energy and enstrophy conserving scheme' |
---|
| 537 | IF(lwp) WRITE(numout,*) '~~~~~~~~~~~' |
---|
[1438] | 538 | ENDIF |
---|
[5836] | 539 | ! |
---|
| 540 | ! ! =============== |
---|
| 541 | DO jk = 1, jpkm1 ! Horizontal slab |
---|
| 542 | ! ! =============== |
---|
| 543 | ! |
---|
| 544 | SELECT CASE( nn_een_e3f ) ! == reciprocal of e3 at F-point |
---|
| 545 | CASE ( 0 ) ! original formulation (masked averaging of e3t divided by 4) |
---|
[12377] | 546 | DO_2D_10_10 |
---|
| 547 | ze3f = ( e3t(ji,jj+1,jk,Kmm)*tmask(ji,jj+1,jk) + e3t(ji+1,jj+1,jk,Kmm)*tmask(ji+1,jj+1,jk) & |
---|
| 548 | & + e3t(ji,jj ,jk,Kmm)*tmask(ji,jj ,jk) + e3t(ji+1,jj ,jk,Kmm)*tmask(ji+1,jj ,jk) ) |
---|
| 549 | IF( ze3f /= 0._wp ) THEN ; z1_e3f(ji,jj) = 4._wp / ze3f |
---|
| 550 | ELSE ; z1_e3f(ji,jj) = 0._wp |
---|
| 551 | ENDIF |
---|
| 552 | END_2D |
---|
[5836] | 553 | CASE ( 1 ) ! new formulation (masked averaging of e3t divided by the sum of mask) |
---|
[12377] | 554 | DO_2D_10_10 |
---|
| 555 | ze3f = ( e3t(ji,jj+1,jk,Kmm)*tmask(ji,jj+1,jk) + e3t(ji+1,jj+1,jk,Kmm)*tmask(ji+1,jj+1,jk) & |
---|
| 556 | & + e3t(ji,jj ,jk,Kmm)*tmask(ji,jj ,jk) + e3t(ji+1,jj ,jk,Kmm)*tmask(ji+1,jj ,jk) ) |
---|
| 557 | zmsk = ( tmask(ji,jj+1,jk) + tmask(ji+1,jj+1,jk) & |
---|
| 558 | & + tmask(ji,jj ,jk) + tmask(ji+1,jj ,jk) ) |
---|
| 559 | IF( ze3f /= 0._wp ) THEN ; z1_e3f(ji,jj) = zmsk / ze3f |
---|
| 560 | ELSE ; z1_e3f(ji,jj) = 0._wp |
---|
| 561 | ENDIF |
---|
| 562 | END_2D |
---|
[5836] | 563 | END SELECT |
---|
| 564 | ! |
---|
| 565 | SELECT CASE( kvor ) !== vorticity considered ==! |
---|
| 566 | CASE ( np_COR ) !* Coriolis (planetary vorticity) |
---|
[12377] | 567 | DO_2D_10_10 |
---|
| 568 | zwz(ji,jj,jk) = ff_f(ji,jj) * z1_e3f(ji,jj) |
---|
| 569 | END_2D |
---|
[5836] | 570 | CASE ( np_RVO ) !* relative vorticity |
---|
[12377] | 571 | DO_2D_10_10 |
---|
| 572 | zwz(ji,jj,jk) = ( e2v(ji+1,jj ) * pv(ji+1,jj,jk) - e2v(ji,jj) * pv(ji,jj,jk) & |
---|
| 573 | & - e1u(ji ,jj+1) * pu(ji,jj+1,jk) + e1u(ji,jj) * pu(ji,jj,jk) ) * r1_e1e2f(ji,jj)*z1_e3f(ji,jj) |
---|
| 574 | END_2D |
---|
[5836] | 575 | CASE ( np_MET ) !* metric term |
---|
[12377] | 576 | DO_2D_10_10 |
---|
| 577 | zwz(ji,jj,jk) = ( ( pv(ji+1,jj,jk) + pv(ji,jj,jk) ) * di_e2v_2e1e2f(ji,jj) & |
---|
| 578 | & - ( pu(ji,jj+1,jk) + pu(ji,jj,jk) ) * dj_e1u_2e1e2f(ji,jj) ) * z1_e3f(ji,jj) |
---|
| 579 | END_2D |
---|
[5836] | 580 | CASE ( np_CRV ) !* Coriolis + relative vorticity |
---|
[12377] | 581 | DO_2D_10_10 |
---|
| 582 | zwz(ji,jj,jk) = ( ff_f(ji,jj) + ( e2v(ji+1,jj ) * pv(ji+1,jj,jk) - e2v(ji,jj) * pv(ji,jj,jk) & |
---|
| 583 | & - e1u(ji ,jj+1) * pu(ji,jj+1,jk) + e1u(ji,jj) * pu(ji,jj,jk) ) & |
---|
| 584 | & * r1_e1e2f(ji,jj) ) * z1_e3f(ji,jj) |
---|
| 585 | END_2D |
---|
[5836] | 586 | CASE ( np_CME ) !* Coriolis + metric |
---|
[12377] | 587 | DO_2D_10_10 |
---|
| 588 | zwz(ji,jj,jk) = ( ff_f(ji,jj) + ( pv(ji+1,jj ,jk) + pv(ji,jj,jk) ) * di_e2v_2e1e2f(ji,jj) & |
---|
| 589 | & - ( pu(ji ,jj+1,jk) + pu(ji,jj,jk) ) * dj_e1u_2e1e2f(ji,jj) ) * z1_e3f(ji,jj) |
---|
| 590 | END_2D |
---|
[5836] | 591 | CASE DEFAULT ! error |
---|
| 592 | CALL ctl_stop('STOP','dyn_vor: wrong value for kvor' ) |
---|
[455] | 593 | END SELECT |
---|
[5836] | 594 | ! |
---|
| 595 | IF( ln_dynvor_msk ) THEN !== mask/unmask vorticity ==! |
---|
[12377] | 596 | DO_2D_10_10 |
---|
| 597 | zwz(ji,jj,jk) = zwz(ji,jj,jk) * fmask(ji,jj,jk) |
---|
| 598 | END_2D |
---|
[5836] | 599 | ENDIF |
---|
[10425] | 600 | END DO ! End of slab |
---|
[5836] | 601 | ! |
---|
[10425] | 602 | CALL lbc_lnk( 'dynvor', zwz, 'F', 1. ) |
---|
| 603 | |
---|
| 604 | DO jk = 1, jpkm1 ! Horizontal slab |
---|
[5907] | 605 | ! |
---|
[5836] | 606 | ! !== horizontal fluxes ==! |
---|
[12377] | 607 | zwx(:,:) = e2u(:,:) * e3u(:,:,jk,Kmm) * pu(:,:,jk) |
---|
| 608 | zwy(:,:) = e1v(:,:) * e3v(:,:,jk,Kmm) * pv(:,:,jk) |
---|
[108] | 609 | |
---|
[5836] | 610 | ! !== compute and add the vorticity term trend =! |
---|
[1438] | 611 | jj = 2 |
---|
| 612 | ztne(1,:) = 0 ; ztnw(1,:) = 0 ; ztse(1,:) = 0 ; ztsw(1,:) = 0 |
---|
[5836] | 613 | DO ji = 2, jpi ! split in 2 parts due to vector opt. |
---|
[10425] | 614 | ztne(ji,jj) = zwz(ji-1,jj ,jk) + zwz(ji ,jj ,jk) + zwz(ji ,jj-1,jk) |
---|
| 615 | ztnw(ji,jj) = zwz(ji-1,jj-1,jk) + zwz(ji-1,jj ,jk) + zwz(ji ,jj ,jk) |
---|
| 616 | ztse(ji,jj) = zwz(ji ,jj ,jk) + zwz(ji ,jj-1,jk) + zwz(ji-1,jj-1,jk) |
---|
| 617 | ztsw(ji,jj) = zwz(ji ,jj-1,jk) + zwz(ji-1,jj-1,jk) + zwz(ji-1,jj ,jk) |
---|
[108] | 618 | END DO |
---|
| 619 | DO jj = 3, jpj |
---|
[12377] | 620 | DO ji = 2, jpi ! vector opt. ok because we start at jj = 3 |
---|
[10425] | 621 | ztne(ji,jj) = zwz(ji-1,jj ,jk) + zwz(ji ,jj ,jk) + zwz(ji ,jj-1,jk) |
---|
| 622 | ztnw(ji,jj) = zwz(ji-1,jj-1,jk) + zwz(ji-1,jj ,jk) + zwz(ji ,jj ,jk) |
---|
| 623 | ztse(ji,jj) = zwz(ji ,jj ,jk) + zwz(ji ,jj-1,jk) + zwz(ji-1,jj-1,jk) |
---|
| 624 | ztsw(ji,jj) = zwz(ji ,jj-1,jk) + zwz(ji-1,jj-1,jk) + zwz(ji-1,jj ,jk) |
---|
[108] | 625 | END DO |
---|
| 626 | END DO |
---|
[12377] | 627 | DO_2D_00_00 |
---|
| 628 | zua = + r1_12 * r1_e1u(ji,jj) * ( ztne(ji,jj ) * zwy(ji ,jj ) + ztnw(ji+1,jj) * zwy(ji+1,jj ) & |
---|
| 629 | & + ztse(ji,jj ) * zwy(ji ,jj-1) + ztsw(ji+1,jj) * zwy(ji+1,jj-1) ) |
---|
| 630 | zva = - r1_12 * r1_e2v(ji,jj) * ( ztsw(ji,jj+1) * zwx(ji-1,jj+1) + ztse(ji,jj+1) * zwx(ji ,jj+1) & |
---|
| 631 | & + ztnw(ji,jj ) * zwx(ji-1,jj ) + ztne(ji,jj ) * zwx(ji ,jj ) ) |
---|
| 632 | pu_rhs(ji,jj,jk) = pu_rhs(ji,jj,jk) + zua |
---|
| 633 | pv_rhs(ji,jj,jk) = pv_rhs(ji,jj,jk) + zva |
---|
| 634 | END_2D |
---|
[108] | 635 | ! ! =============== |
---|
| 636 | END DO ! End of slab |
---|
| 637 | ! ! =============== |
---|
[455] | 638 | END SUBROUTINE vor_een |
---|
[216] | 639 | |
---|
| 640 | |
---|
[9528] | 641 | |
---|
[12377] | 642 | SUBROUTINE vor_eeT( kt, Kmm, kvor, pu, pv, pu_rhs, pv_rhs ) |
---|
[9528] | 643 | !!---------------------------------------------------------------------- |
---|
| 644 | !! *** ROUTINE vor_eeT *** |
---|
| 645 | !! |
---|
| 646 | !! ** Purpose : Compute the now total vorticity trend and add it to |
---|
| 647 | !! the general trend of the momentum equation. |
---|
| 648 | !! |
---|
| 649 | !! ** Method : Trend evaluated using now fields (centered in time) |
---|
| 650 | !! and the Arakawa and Lamb (1980) vector form formulation using |
---|
| 651 | !! a modified version of Arakawa and Lamb (1980) scheme (see vor_een). |
---|
| 652 | !! The change consists in |
---|
[12377] | 653 | !! Add this trend to the general momentum trend (pu_rhs,pv_rhs). |
---|
[9528] | 654 | !! |
---|
[12377] | 655 | !! ** Action : - Update (pu_rhs,pv_rhs) with the now vorticity term trend |
---|
[9528] | 656 | !! |
---|
| 657 | !! References : Arakawa and Lamb 1980, Mon. Wea. Rev., 109, 18-36 |
---|
| 658 | !!---------------------------------------------------------------------- |
---|
| 659 | INTEGER , INTENT(in ) :: kt ! ocean time-step index |
---|
[12377] | 660 | INTEGER , INTENT(in ) :: Kmm ! ocean time level index |
---|
[9528] | 661 | INTEGER , INTENT(in ) :: kvor ! total, planetary, relative, or metric |
---|
[12377] | 662 | REAL(wp), DIMENSION(jpi,jpj,jpk), INTENT(inout) :: pu, pv ! now velocities |
---|
| 663 | REAL(wp), DIMENSION(jpi,jpj,jpk), INTENT(inout) :: pu_rhs, pv_rhs ! total v-trend |
---|
[9528] | 664 | ! |
---|
| 665 | INTEGER :: ji, jj, jk ! dummy loop indices |
---|
| 666 | INTEGER :: ierr ! local integer |
---|
| 667 | REAL(wp) :: zua, zva ! local scalars |
---|
| 668 | REAL(wp) :: zmsk, z1_e3t ! local scalars |
---|
[10425] | 669 | REAL(wp), DIMENSION(jpi,jpj) :: zwx , zwy |
---|
| 670 | REAL(wp), DIMENSION(jpi,jpj) :: ztnw, ztne, ztsw, ztse |
---|
| 671 | REAL(wp), DIMENSION(jpi,jpj,jpk) :: zwz |
---|
[9528] | 672 | !!---------------------------------------------------------------------- |
---|
| 673 | ! |
---|
| 674 | IF( kt == nit000 ) THEN |
---|
| 675 | IF(lwp) WRITE(numout,*) |
---|
| 676 | IF(lwp) WRITE(numout,*) 'dyn:vor_een : vorticity term: energy and enstrophy conserving scheme' |
---|
| 677 | IF(lwp) WRITE(numout,*) '~~~~~~~~~~~' |
---|
| 678 | ENDIF |
---|
| 679 | ! |
---|
| 680 | ! ! =============== |
---|
| 681 | DO jk = 1, jpkm1 ! Horizontal slab |
---|
| 682 | ! ! =============== |
---|
| 683 | ! |
---|
| 684 | ! |
---|
| 685 | SELECT CASE( kvor ) !== vorticity considered ==! |
---|
| 686 | CASE ( np_COR ) !* Coriolis (planetary vorticity) |
---|
[12377] | 687 | DO_2D_10_10 |
---|
| 688 | zwz(ji,jj,jk) = ff_f(ji,jj) |
---|
| 689 | END_2D |
---|
[9528] | 690 | CASE ( np_RVO ) !* relative vorticity |
---|
[12377] | 691 | DO_2D_10_10 |
---|
| 692 | zwz(ji,jj,jk) = ( e2v(ji+1,jj ) * pv(ji+1,jj ,jk) - e2v(ji,jj) * pv(ji,jj,jk) & |
---|
| 693 | & - e1u(ji ,jj+1) * pu(ji ,jj+1,jk) + e1u(ji,jj) * pu(ji,jj,jk) ) & |
---|
| 694 | & * r1_e1e2f(ji,jj) |
---|
| 695 | END_2D |
---|
[9528] | 696 | CASE ( np_MET ) !* metric term |
---|
[12377] | 697 | DO_2D_10_10 |
---|
| 698 | zwz(ji,jj,jk) = ( pv(ji+1,jj ,jk) + pv(ji,jj,jk) ) * di_e2v_2e1e2f(ji,jj) & |
---|
| 699 | & - ( pu(ji ,jj+1,jk) + pu(ji,jj,jk) ) * dj_e1u_2e1e2f(ji,jj) |
---|
| 700 | END_2D |
---|
[9528] | 701 | CASE ( np_CRV ) !* Coriolis + relative vorticity |
---|
[12377] | 702 | DO_2D_10_10 |
---|
| 703 | zwz(ji,jj,jk) = ( ff_f(ji,jj) + ( e2v(ji+1,jj ) * pv(ji+1,jj ,jk) - e2v(ji,jj) * pv(ji,jj,jk) & |
---|
| 704 | & - e1u(ji ,jj+1) * pu(ji ,jj+1,jk) + e1u(ji,jj) * pu(ji,jj,jk) ) & |
---|
| 705 | & * r1_e1e2f(ji,jj) ) |
---|
| 706 | END_2D |
---|
[9528] | 707 | CASE ( np_CME ) !* Coriolis + metric |
---|
[12377] | 708 | DO_2D_10_10 |
---|
| 709 | zwz(ji,jj,jk) = ff_f(ji,jj) + ( pv(ji+1,jj ,jk) + pv(ji,jj,jk) ) * di_e2v_2e1e2f(ji,jj) & |
---|
| 710 | & - ( pu(ji ,jj+1,jk) + pu(ji,jj,jk) ) * dj_e1u_2e1e2f(ji,jj) |
---|
| 711 | END_2D |
---|
[9528] | 712 | CASE DEFAULT ! error |
---|
| 713 | CALL ctl_stop('STOP','dyn_vor: wrong value for kvor' ) |
---|
| 714 | END SELECT |
---|
| 715 | ! |
---|
| 716 | IF( ln_dynvor_msk ) THEN !== mask/unmask vorticity ==! |
---|
[12377] | 717 | DO_2D_10_10 |
---|
| 718 | zwz(ji,jj,jk) = zwz(ji,jj,jk) * fmask(ji,jj,jk) |
---|
| 719 | END_2D |
---|
[9528] | 720 | ENDIF |
---|
[10425] | 721 | END DO |
---|
| 722 | ! |
---|
| 723 | CALL lbc_lnk( 'dynvor', zwz, 'F', 1. ) |
---|
| 724 | ! |
---|
| 725 | DO jk = 1, jpkm1 ! Horizontal slab |
---|
| 726 | |
---|
| 727 | ! !== horizontal fluxes ==! |
---|
[12377] | 728 | zwx(:,:) = e2u(:,:) * e3u(:,:,jk,Kmm) * pu(:,:,jk) |
---|
| 729 | zwy(:,:) = e1v(:,:) * e3v(:,:,jk,Kmm) * pv(:,:,jk) |
---|
[9528] | 730 | |
---|
| 731 | ! !== compute and add the vorticity term trend =! |
---|
| 732 | jj = 2 |
---|
| 733 | ztne(1,:) = 0 ; ztnw(1,:) = 0 ; ztse(1,:) = 0 ; ztsw(1,:) = 0 |
---|
| 734 | DO ji = 2, jpi ! split in 2 parts due to vector opt. |
---|
[12377] | 735 | z1_e3t = 1._wp / e3t(ji,jj,jk,Kmm) |
---|
[10425] | 736 | ztne(ji,jj) = ( zwz(ji-1,jj ,jk) + zwz(ji ,jj ,jk) + zwz(ji ,jj-1,jk) ) * z1_e3t |
---|
| 737 | ztnw(ji,jj) = ( zwz(ji-1,jj-1,jk) + zwz(ji-1,jj ,jk) + zwz(ji ,jj ,jk) ) * z1_e3t |
---|
| 738 | ztse(ji,jj) = ( zwz(ji ,jj ,jk) + zwz(ji ,jj-1,jk) + zwz(ji-1,jj-1,jk) ) * z1_e3t |
---|
| 739 | ztsw(ji,jj) = ( zwz(ji ,jj-1,jk) + zwz(ji-1,jj-1,jk) + zwz(ji-1,jj ,jk) ) * z1_e3t |
---|
[9528] | 740 | END DO |
---|
| 741 | DO jj = 3, jpj |
---|
[12377] | 742 | DO ji = 2, jpi ! vector opt. ok because we start at jj = 3 |
---|
| 743 | z1_e3t = 1._wp / e3t(ji,jj,jk,Kmm) |
---|
[10425] | 744 | ztne(ji,jj) = ( zwz(ji-1,jj ,jk) + zwz(ji ,jj ,jk) + zwz(ji ,jj-1,jk) ) * z1_e3t |
---|
| 745 | ztnw(ji,jj) = ( zwz(ji-1,jj-1,jk) + zwz(ji-1,jj ,jk) + zwz(ji ,jj ,jk) ) * z1_e3t |
---|
| 746 | ztse(ji,jj) = ( zwz(ji ,jj ,jk) + zwz(ji ,jj-1,jk) + zwz(ji-1,jj-1,jk) ) * z1_e3t |
---|
| 747 | ztsw(ji,jj) = ( zwz(ji ,jj-1,jk) + zwz(ji-1,jj-1,jk) + zwz(ji-1,jj ,jk) ) * z1_e3t |
---|
[9528] | 748 | END DO |
---|
| 749 | END DO |
---|
[12377] | 750 | DO_2D_00_00 |
---|
| 751 | zua = + r1_12 * r1_e1u(ji,jj) * ( ztne(ji,jj ) * zwy(ji ,jj ) + ztnw(ji+1,jj) * zwy(ji+1,jj ) & |
---|
| 752 | & + ztse(ji,jj ) * zwy(ji ,jj-1) + ztsw(ji+1,jj) * zwy(ji+1,jj-1) ) |
---|
| 753 | zva = - r1_12 * r1_e2v(ji,jj) * ( ztsw(ji,jj+1) * zwx(ji-1,jj+1) + ztse(ji,jj+1) * zwx(ji ,jj+1) & |
---|
| 754 | & + ztnw(ji,jj ) * zwx(ji-1,jj ) + ztne(ji,jj ) * zwx(ji ,jj ) ) |
---|
| 755 | pu_rhs(ji,jj,jk) = pu_rhs(ji,jj,jk) + zua |
---|
| 756 | pv_rhs(ji,jj,jk) = pv_rhs(ji,jj,jk) + zva |
---|
| 757 | END_2D |
---|
[9528] | 758 | ! ! =============== |
---|
| 759 | END DO ! End of slab |
---|
| 760 | ! ! =============== |
---|
| 761 | END SUBROUTINE vor_eeT |
---|
| 762 | |
---|
| 763 | |
---|
[2528] | 764 | SUBROUTINE dyn_vor_init |
---|
[3] | 765 | !!--------------------------------------------------------------------- |
---|
[2528] | 766 | !! *** ROUTINE dyn_vor_init *** |
---|
[3] | 767 | !! |
---|
| 768 | !! ** Purpose : Control the consistency between cpp options for |
---|
[1438] | 769 | !! tracer advection schemes |
---|
[3] | 770 | !!---------------------------------------------------------------------- |
---|
[9528] | 771 | INTEGER :: ji, jj, jk ! dummy loop indices |
---|
| 772 | INTEGER :: ioptio, ios ! local integer |
---|
[2715] | 773 | !! |
---|
[9528] | 774 | NAMELIST/namdyn_vor/ ln_dynvor_ens, ln_dynvor_ene, ln_dynvor_enT, ln_dynvor_eeT, & |
---|
| 775 | & ln_dynvor_een, nn_een_e3f , ln_dynvor_mix, ln_dynvor_msk |
---|
[3] | 776 | !!---------------------------------------------------------------------- |
---|
[9528] | 777 | ! |
---|
| 778 | IF(lwp) THEN |
---|
| 779 | WRITE(numout,*) |
---|
| 780 | WRITE(numout,*) 'dyn_vor_init : vorticity term : read namelist and control the consistency' |
---|
| 781 | WRITE(numout,*) '~~~~~~~~~~~~' |
---|
| 782 | ENDIF |
---|
| 783 | ! |
---|
[4147] | 784 | READ ( numnam_ref, namdyn_vor, IOSTAT = ios, ERR = 901) |
---|
[11536] | 785 | 901 IF( ios /= 0 ) CALL ctl_nam ( ios , 'namdyn_vor in reference namelist' ) |
---|
[4147] | 786 | READ ( numnam_cfg, namdyn_vor, IOSTAT = ios, ERR = 902 ) |
---|
[11536] | 787 | 902 IF( ios > 0 ) CALL ctl_nam ( ios , 'namdyn_vor in configuration namelist' ) |
---|
[4624] | 788 | IF(lwm) WRITE ( numond, namdyn_vor ) |
---|
[9528] | 789 | ! |
---|
[503] | 790 | IF(lwp) THEN ! Namelist print |
---|
[7646] | 791 | WRITE(numout,*) ' Namelist namdyn_vor : choice of the vorticity term scheme' |
---|
| 792 | WRITE(numout,*) ' enstrophy conserving scheme ln_dynvor_ens = ', ln_dynvor_ens |
---|
[9528] | 793 | WRITE(numout,*) ' f-point energy conserving scheme ln_dynvor_ene = ', ln_dynvor_ene |
---|
| 794 | WRITE(numout,*) ' t-point energy conserving scheme ln_dynvor_enT = ', ln_dynvor_enT |
---|
| 795 | WRITE(numout,*) ' energy conserving scheme (een using e3t) ln_dynvor_eeT = ', ln_dynvor_eeT |
---|
[7646] | 796 | WRITE(numout,*) ' enstrophy and energy conserving scheme ln_dynvor_een = ', ln_dynvor_een |
---|
| 797 | WRITE(numout,*) ' e3f = averaging /4 (=0) or /sum(tmask) (=1) nn_een_e3f = ', nn_een_e3f |
---|
[9528] | 798 | WRITE(numout,*) ' mixed enstrophy/energy conserving scheme ln_dynvor_mix = ', ln_dynvor_mix |
---|
[7646] | 799 | WRITE(numout,*) ' masked (=T) or unmasked(=F) vorticity ln_dynvor_msk = ', ln_dynvor_msk |
---|
[52] | 800 | ENDIF |
---|
| 801 | |
---|
[9528] | 802 | IF( ln_dynvor_msk ) CALL ctl_stop( 'dyn_vor_init: masked vorticity is not currently not available') |
---|
| 803 | |
---|
[5836] | 804 | !!gm this should be removed when choosing a unique strategy for fmask at the coast |
---|
[3294] | 805 | ! If energy, enstrophy or mixed advection of momentum in vector form change the value for masks |
---|
| 806 | ! at angles with three ocean points and one land point |
---|
[5836] | 807 | IF(lwp) WRITE(numout,*) |
---|
[7646] | 808 | IF(lwp) WRITE(numout,*) ' change fmask value in the angles (T) ln_vorlat = ', ln_vorlat |
---|
[3294] | 809 | IF( ln_vorlat .AND. ( ln_dynvor_ene .OR. ln_dynvor_ens .OR. ln_dynvor_mix ) ) THEN |
---|
[12377] | 810 | DO_3D_10_10( 1, jpk ) |
---|
| 811 | IF( tmask(ji,jj+1,jk) + tmask(ji+1,jj+1,jk) & |
---|
[13159] | 812 | & + tmask(ji,jj ,jk) + tmask(ji+1,jj ,jk) == 3._wp ) fmask(ji,jj,jk) = 1._wp |
---|
[12377] | 813 | END_3D |
---|
[9528] | 814 | ! |
---|
[10425] | 815 | CALL lbc_lnk( 'dynvor', fmask, 'F', 1._wp ) ! Lateral boundary conditions on fmask |
---|
[9528] | 816 | ! |
---|
[3294] | 817 | ENDIF |
---|
[5836] | 818 | !!gm end |
---|
[3294] | 819 | |
---|
[5836] | 820 | ioptio = 0 ! type of scheme for vorticity (set nvor_scheme) |
---|
[9528] | 821 | IF( ln_dynvor_ens ) THEN ; ioptio = ioptio + 1 ; nvor_scheme = np_ENS ; ENDIF |
---|
| 822 | IF( ln_dynvor_ene ) THEN ; ioptio = ioptio + 1 ; nvor_scheme = np_ENE ; ENDIF |
---|
| 823 | IF( ln_dynvor_enT ) THEN ; ioptio = ioptio + 1 ; nvor_scheme = np_ENT ; ENDIF |
---|
| 824 | IF( ln_dynvor_eeT ) THEN ; ioptio = ioptio + 1 ; nvor_scheme = np_EET ; ENDIF |
---|
| 825 | IF( ln_dynvor_een ) THEN ; ioptio = ioptio + 1 ; nvor_scheme = np_EEN ; ENDIF |
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| 826 | IF( ln_dynvor_mix ) THEN ; ioptio = ioptio + 1 ; nvor_scheme = np_MIX ; ENDIF |
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[5836] | 827 | ! |
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[6140] | 828 | IF( ioptio /= 1 ) CALL ctl_stop( ' use ONE and ONLY one vorticity scheme' ) |
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[5836] | 829 | ! |
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| 830 | IF(lwp) WRITE(numout,*) ! type of calculated vorticity (set ncor, nrvm, ntot) |
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[9019] | 831 | ncor = np_COR ! planetary vorticity |
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| 832 | SELECT CASE( n_dynadv ) |
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| 833 | CASE( np_LIN_dyn ) |
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[9190] | 834 | IF(lwp) WRITE(numout,*) ' ==>>> linear dynamics : total vorticity = Coriolis' |
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[9019] | 835 | nrvm = np_COR ! planetary vorticity |
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| 836 | ntot = np_COR ! - - |
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| 837 | CASE( np_VEC_c2 ) |
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[9190] | 838 | IF(lwp) WRITE(numout,*) ' ==>>> vector form dynamics : total vorticity = Coriolis + relative vorticity' |
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[5836] | 839 | nrvm = np_RVO ! relative vorticity |
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[9019] | 840 | ntot = np_CRV ! relative + planetary vorticity |
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| 841 | CASE( np_FLX_c2 , np_FLX_ubs ) |
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[9190] | 842 | IF(lwp) WRITE(numout,*) ' ==>>> flux form dynamics : total vorticity = Coriolis + metric term' |
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[5836] | 843 | nrvm = np_MET ! metric term |
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| 844 | ntot = np_CME ! Coriolis + metric term |
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[9528] | 845 | ! |
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| 846 | SELECT CASE( nvor_scheme ) ! pre-computed gradients for the metric term: |
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| 847 | CASE( np_ENT ) !* T-point metric term : pre-compute di(e2u)/2 and dj(e1v)/2 |
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| 848 | ALLOCATE( di_e2u_2(jpi,jpj), dj_e1v_2(jpi,jpj) ) |
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[12377] | 849 | DO_2D_00_00 |
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| 850 | di_e2u_2(ji,jj) = ( e2u(ji,jj) - e2u(ji-1,jj ) ) * 0.5_wp |
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| 851 | dj_e1v_2(ji,jj) = ( e1v(ji,jj) - e1v(ji ,jj-1) ) * 0.5_wp |
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| 852 | END_2D |
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[10425] | 853 | CALL lbc_lnk_multi( 'dynvor', di_e2u_2, 'T', -1. , dj_e1v_2, 'T', -1. ) ! Lateral boundary conditions |
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[9528] | 854 | ! |
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| 855 | CASE DEFAULT !* F-point metric term : pre-compute di(e2u)/(2*e1e2f) and dj(e1v)/(2*e1e2f) |
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| 856 | ALLOCATE( di_e2v_2e1e2f(jpi,jpj), dj_e1u_2e1e2f(jpi,jpj) ) |
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[12377] | 857 | DO_2D_10_10 |
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| 858 | di_e2v_2e1e2f(ji,jj) = ( e2v(ji+1,jj ) - e2v(ji,jj) ) * 0.5 * r1_e1e2f(ji,jj) |
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| 859 | dj_e1u_2e1e2f(ji,jj) = ( e1u(ji ,jj+1) - e1u(ji,jj) ) * 0.5 * r1_e1e2f(ji,jj) |
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| 860 | END_2D |
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[10425] | 861 | CALL lbc_lnk_multi( 'dynvor', di_e2v_2e1e2f, 'F', -1. , dj_e1u_2e1e2f, 'F', -1. ) ! Lateral boundary conditions |
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[9528] | 862 | END SELECT |
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| 863 | ! |
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[9019] | 864 | END SELECT |
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[643] | 865 | |
---|
[503] | 866 | IF(lwp) THEN ! Print the choice |
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| 867 | WRITE(numout,*) |
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[9019] | 868 | SELECT CASE( nvor_scheme ) |
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[9528] | 869 | CASE( np_ENS ) ; WRITE(numout,*) ' ==>>> enstrophy conserving scheme (ENS)' |
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| 870 | CASE( np_ENE ) ; WRITE(numout,*) ' ==>>> energy conserving scheme (Coriolis at F-points) (ENE)' |
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| 871 | CASE( np_ENT ) ; WRITE(numout,*) ' ==>>> energy conserving scheme (Coriolis at T-points) (ENT)' |
---|
| 872 | CASE( np_EET ) ; WRITE(numout,*) ' ==>>> energy conserving scheme (EEN scheme using e3t) (EET)' |
---|
| 873 | CASE( np_EEN ) ; WRITE(numout,*) ' ==>>> energy and enstrophy conserving scheme (EEN)' |
---|
| 874 | CASE( np_MIX ) ; WRITE(numout,*) ' ==>>> mixed enstrophy/energy conserving scheme (MIX)' |
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[9019] | 875 | END SELECT |
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[3] | 876 | ENDIF |
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[503] | 877 | ! |
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[2528] | 878 | END SUBROUTINE dyn_vor_init |
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[3] | 879 | |
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[503] | 880 | !!============================================================================== |
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[3] | 881 | END MODULE dynvor |
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