[358] | 1 | MODULE dynspg_ts |
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| 2 | !!====================================================================== |
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[1502] | 3 | !! History : 1.0 ! 2004-12 (L. Bessieres, G. Madec) Original code |
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| 4 | !! - ! 2005-11 (V. Garnier, G. Madec) optimization |
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| 5 | !! - ! 2006-08 (S. Masson) distributed restart using iom |
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| 6 | !! 2.0 ! 2007-07 (D. Storkey) calls to BDY routines |
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| 7 | !! - ! 2008-01 (R. Benshila) change averaging method |
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| 8 | !! 3.2 ! 2009-07 (R. Benshila, G. Madec) Complete revisit associated to vvl reactivation |
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[1438] | 9 | !!--------------------------------------------------------------------- |
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[575] | 10 | #if defined key_dynspg_ts || defined key_esopa |
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[358] | 11 | !!---------------------------------------------------------------------- |
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[455] | 12 | !! 'key_dynspg_ts' free surface cst volume with time splitting |
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[358] | 13 | !!---------------------------------------------------------------------- |
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| 14 | !! dyn_spg_ts : compute surface pressure gradient trend using a time- |
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| 15 | !! splitting scheme and add to the general trend |
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[508] | 16 | !! ts_rst : read/write the time-splitting restart fields in the ocean restart file |
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[358] | 17 | !!---------------------------------------------------------------------- |
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| 18 | USE oce ! ocean dynamics and tracers |
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| 19 | USE dom_oce ! ocean space and time domain |
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[888] | 20 | USE sbc_oce ! surface boundary condition: ocean |
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| 21 | USE dynspg_oce ! surface pressure gradient variables |
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[358] | 22 | USE phycst ! physical constants |
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[888] | 23 | USE domvvl ! variable volume |
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[1662] | 24 | USE zdfbfr ! bottom friction |
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[367] | 25 | USE obcdta ! open boundary condition data |
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| 26 | USE obcfla ! Flather open boundary condition |
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[358] | 27 | USE dynvor ! vorticity term |
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| 28 | USE obc_oce ! Lateral open boundary condition |
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[371] | 29 | USE obc_par ! open boundary condition parameters |
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[911] | 30 | USE bdy_oce ! unstructured open boundaries |
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| 31 | USE bdy_par ! unstructured open boundaries |
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| 32 | USE bdydta ! unstructured open boundaries |
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| 33 | USE bdydyn ! unstructured open boundaries |
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| 34 | USE bdytides ! tidal forcing at unstructured open boundaries. |
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[358] | 35 | USE lib_mpp ! distributed memory computing library |
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| 36 | USE lbclnk ! ocean lateral boundary conditions (or mpp link) |
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| 37 | USE prtctl ! Print control |
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| 38 | USE in_out_manager ! I/O manager |
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[508] | 39 | USE iom |
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| 40 | USE restart ! only for lrst_oce |
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[358] | 41 | |
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| 42 | IMPLICIT NONE |
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| 43 | PRIVATE |
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| 44 | |
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| 45 | PUBLIC dyn_spg_ts ! routine called by step.F90 |
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[800] | 46 | PUBLIC ts_rst ! routine called by istate.F90 |
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[358] | 47 | |
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[1502] | 48 | |
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[1438] | 49 | REAL(wp), DIMENSION(jpi,jpj) :: ftnw, ftne ! triad of coriolis parameter |
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| 50 | REAL(wp), DIMENSION(jpi,jpj) :: ftsw, ftse ! (only used with een vorticity scheme) |
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[508] | 51 | |
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[1502] | 52 | REAL(wp), PUBLIC, DIMENSION(jpi,jpj) :: un_b, vn_b ! averaged velocity |
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| 53 | |
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[358] | 54 | !! * Substitutions |
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| 55 | # include "domzgr_substitute.h90" |
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| 56 | # include "vectopt_loop_substitute.h90" |
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[1438] | 57 | !!------------------------------------------------------------------------- |
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| 58 | !! NEMO/OPA 3.2 , LOCEAN-IPSL (2009) |
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[888] | 59 | !! $Id$ |
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[1438] | 60 | !! Software is governed by the CeCILL licence (modipsl/doc/NEMO_CeCILL.txt) |
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| 61 | !!------------------------------------------------------------------------- |
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[358] | 62 | |
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| 63 | CONTAINS |
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| 64 | |
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| 65 | SUBROUTINE dyn_spg_ts( kt ) |
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| 66 | !!---------------------------------------------------------------------- |
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| 67 | !! *** routine dyn_spg_ts *** |
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| 68 | !! |
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| 69 | !! ** Purpose : Compute the now trend due to the surface pressure |
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| 70 | !! gradient in case of free surface formulation with time-splitting. |
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| 71 | !! Add it to the general trend of momentum equation. |
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| 72 | !! |
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| 73 | !! ** Method : Free surface formulation with time-splitting |
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| 74 | !! -1- Save the vertically integrated trend. This general trend is |
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| 75 | !! held constant over the barotropic integration. |
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| 76 | !! The Coriolis force is removed from the general trend as the |
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| 77 | !! surface gradient and the Coriolis force are updated within |
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| 78 | !! the barotropic integration. |
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[367] | 79 | !! -2- Barotropic loop : updates of sea surface height (ssha_e) and |
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[1502] | 80 | !! barotropic velocity (ua_e and va_e) through barotropic |
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[358] | 81 | !! momentum and continuity integration. Barotropic former |
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| 82 | !! variables are time averaging over the full barotropic cycle |
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[1502] | 83 | !! (= 2 * baroclinic time step) and saved in zuX_b |
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[358] | 84 | !! and zvX_b (X specifying after, now or before). |
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[1438] | 85 | !! -3- The new general trend becomes : |
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[1502] | 86 | !! ua = ua - sum_k(ua)/H + ( ua_e - sum_k(ub) ) |
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[358] | 87 | !! |
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| 88 | !! ** Action : - Update (ua,va) with the surf. pressure gradient trend |
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| 89 | !! |
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[508] | 90 | !! References : Griffies et al., (2003): A technical guide to MOM4. NOAA/GFDL |
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[358] | 91 | !!--------------------------------------------------------------------- |
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[1502] | 92 | INTEGER, INTENT(in) :: kt ! ocean time-step index |
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[1438] | 93 | !! |
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[1662] | 94 | INTEGER :: ji, jj, jk, jn ! dummy loop indices |
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| 95 | INTEGER :: icycle ! temporary scalar |
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[1708] | 96 | INTEGER :: ikbu, ikbv ! temporary scalar |
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[1662] | 97 | |
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| 98 | REAL(wp) :: zraur, zcoef, z2dt_e, z2dt_b ! temporary scalars |
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| 99 | REAL(wp) :: z1_8, zx1, zy1 ! - - |
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| 100 | REAL(wp) :: z1_4, zx2, zy2 ! - - |
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| 101 | REAL(wp) :: zu_spg, zu_cor, zu_sld, zu_asp ! - - |
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| 102 | REAL(wp) :: zv_spg, zv_cor, zv_sld, zv_asp ! - - |
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| 103 | !! |
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[1502] | 104 | REAL(wp), DIMENSION(jpi,jpj) :: zhdiv, zsshb_e |
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[1662] | 105 | !! |
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[1708] | 106 | REAL(wp), DIMENSION(jpi,jpj) :: zbfru , zbfrv ! 2D workspace |
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| 107 | !! |
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[1502] | 108 | REAL(wp), DIMENSION(jpi,jpj) :: zsshun_e, zsshvn_e ! 2D workspace |
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| 109 | !! |
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| 110 | REAL(wp), DIMENSION(jpi,jpj) :: zcu, zwx, zua, zun, zub ! 2D workspace |
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| 111 | REAL(wp), DIMENSION(jpi,jpj) :: zcv, zwy, zva, zvn, zvb ! - - |
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| 112 | REAL(wp), DIMENSION(jpi,jpj) :: zun_e, zub_e, zu_sum ! 2D workspace |
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| 113 | REAL(wp), DIMENSION(jpi,jpj) :: zvn_e, zvb_e, zv_sum ! - - |
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| 114 | REAL(wp), DIMENSION(jpi,jpj) :: zssh_sum ! - - |
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[358] | 115 | !!---------------------------------------------------------------------- |
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| 116 | |
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[1502] | 117 | IF( kt == nit000 ) THEN !* initialisation |
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[508] | 118 | ! |
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[358] | 119 | IF(lwp) WRITE(numout,*) |
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| 120 | IF(lwp) WRITE(numout,*) 'dyn_spg_ts : surface pressure gradient trend' |
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| 121 | IF(lwp) WRITE(numout,*) '~~~~~~~~~~ free surface with time splitting' |
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[1241] | 122 | IF(lwp) WRITE(numout,*) ' Number of sub cycle in 1 time-step (2 rdt) : icycle = ', 2*nn_baro |
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[1502] | 123 | ! |
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[1708] | 124 | CALL ts_rst( nit000, 'READ' ) ! read or initialize the following fields: un_b, vn_b |
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[1502] | 125 | ! |
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| 126 | ua_e (:,:) = un_b (:,:) |
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| 127 | va_e (:,:) = vn_b (:,:) |
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| 128 | hu_e (:,:) = hu (:,:) |
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| 129 | hv_e (:,:) = hv (:,:) |
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| 130 | hur_e (:,:) = hur (:,:) |
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| 131 | hvr_e (:,:) = hvr (:,:) |
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[358] | 132 | IF( ln_dynvor_een ) THEN |
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[508] | 133 | ftne(1,:) = 0.e0 ; ftnw(1,:) = 0.e0 ; ftse(1,:) = 0.e0 ; ftsw(1,:) = 0.e0 |
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[358] | 134 | DO jj = 2, jpj |
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[1708] | 135 | DO ji = fs_2, jpi ! vector opt. |
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[508] | 136 | ftne(ji,jj) = ( ff(ji-1,jj ) + ff(ji ,jj ) + ff(ji ,jj-1) ) / 3. |
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| 137 | ftnw(ji,jj) = ( ff(ji-1,jj-1) + ff(ji-1,jj ) + ff(ji ,jj ) ) / 3. |
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| 138 | ftse(ji,jj) = ( ff(ji ,jj ) + ff(ji ,jj-1) + ff(ji-1,jj-1) ) / 3. |
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| 139 | ftsw(ji,jj) = ( ff(ji ,jj-1) + ff(ji-1,jj-1) + ff(ji-1,jj ) ) / 3. |
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[358] | 140 | END DO |
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| 141 | END DO |
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| 142 | ENDIF |
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[508] | 143 | ! |
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| 144 | ENDIF |
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[358] | 145 | |
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[1502] | 146 | ! !* Local constant initialization |
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[358] | 147 | z2dt_b = 2.0 * rdt ! baroclinic time step |
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[1502] | 148 | z1_8 = 0.5 * 0.25 ! coefficient for vorticity estimates |
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| 149 | z1_4 = 0.5 * 0.5 |
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[1739] | 150 | zraur = 1. / rau0 ! 1 / volumic mass |
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[1502] | 151 | ! |
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| 152 | zhdiv(:,:) = 0.e0 ! barotropic divergence |
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[1662] | 153 | zu_sld = 0.e0 ; zu_asp = 0.e0 ! tides trends (lk_tide=F) |
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| 154 | zv_sld = 0.e0 ; zv_asp = 0.e0 |
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[1438] | 155 | |
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[358] | 156 | ! ----------------------------------------------------------------------------- |
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| 157 | ! Phase 1 : Coupling between general trend and barotropic estimates (1st step) |
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| 158 | ! ----------------------------------------------------------------------------- |
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[1502] | 159 | ! |
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| 160 | ! !* e3*d/dt(Ua), e3*Ub, e3*Vn (Vertically integrated) |
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| 161 | ! ! -------------------------- |
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| 162 | zua(:,:) = 0.e0 ; zun(:,:) = 0.e0 ; zub(:,:) = 0.e0 |
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| 163 | zva(:,:) = 0.e0 ; zvn(:,:) = 0.e0 ; zvb(:,:) = 0.e0 |
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| 164 | ! |
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| 165 | DO jk = 1, jpkm1 |
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| 166 | #if defined key_vectopt_loop |
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| 167 | DO jj = 1, 1 !Vector opt. => forced unrolling |
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[358] | 168 | DO ji = 1, jpij |
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[1502] | 169 | #else |
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| 170 | DO jj = 1, jpj |
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| 171 | DO ji = 1, jpi |
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| 172 | #endif |
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| 173 | ! ! now trend |
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| 174 | zua(ji,jj) = zua(ji,jj) + fse3u (ji,jj,jk) * ua(ji,jj,jk) * umask(ji,jj,jk) |
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| 175 | zva(ji,jj) = zva(ji,jj) + fse3v (ji,jj,jk) * va(ji,jj,jk) * vmask(ji,jj,jk) |
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| 176 | ! ! now velocity |
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| 177 | zun(ji,jj) = zun(ji,jj) + fse3u (ji,jj,jk) * un(ji,jj,jk) |
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| 178 | zvn(ji,jj) = zvn(ji,jj) + fse3v (ji,jj,jk) * vn(ji,jj,jk) |
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| 179 | ! ! before velocity |
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| 180 | zub(ji,jj) = zub(ji,jj) + fse3u_b(ji,jj,jk) * ub(ji,jj,jk) |
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| 181 | zvb(ji,jj) = zvb(ji,jj) + fse3v_b(ji,jj,jk) * vb(ji,jj,jk) |
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[358] | 182 | END DO |
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| 183 | END DO |
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[1502] | 184 | END DO |
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| 185 | |
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| 186 | ! !* baroclinic momentum trend (remove the vertical mean trend) |
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| 187 | DO jk = 1, jpkm1 ! -------------------------- |
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| 188 | DO jj = 2, jpjm1 |
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| 189 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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| 190 | ua(ji,jj,jk) = ua(ji,jj,jk) - zua(ji,jj) * hur(ji,jj) |
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| 191 | va(ji,jj,jk) = va(ji,jj,jk) - zva(ji,jj) * hvr(ji,jj) |
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| 192 | END DO |
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[358] | 193 | END DO |
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[1502] | 194 | END DO |
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[358] | 195 | |
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[1502] | 196 | ! !* barotropic Coriolis trends * H (vorticity scheme dependent) |
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| 197 | ! ! ---------------------------==== |
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| 198 | zwx(:,:) = zun(:,:) * e2u(:,:) ! now transport |
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| 199 | zwy(:,:) = zvn(:,:) * e1v(:,:) |
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| 200 | ! |
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[358] | 201 | IF( ln_dynvor_ene .OR. ln_dynvor_mix ) THEN ! energy conserving or mixed scheme |
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| 202 | DO jj = 2, jpjm1 |
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| 203 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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| 204 | zy1 = ( zwy(ji,jj-1) + zwy(ji+1,jj-1) ) / e1u(ji,jj) |
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| 205 | zy2 = ( zwy(ji,jj ) + zwy(ji+1,jj ) ) / e1u(ji,jj) |
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| 206 | zx1 = ( zwx(ji-1,jj) + zwx(ji-1,jj+1) ) / e2v(ji,jj) |
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| 207 | zx2 = ( zwx(ji ,jj) + zwx(ji ,jj+1) ) / e2v(ji,jj) |
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| 208 | ! energy conserving formulation for planetary vorticity term |
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[1502] | 209 | zcu(ji,jj) = z1_4 * ( ff(ji ,jj-1) * zy1 + ff(ji,jj) * zy2 ) |
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| 210 | zcv(ji,jj) =-z1_4 * ( ff(ji-1,jj ) * zx1 + ff(ji,jj) * zx2 ) |
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[358] | 211 | END DO |
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| 212 | END DO |
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[508] | 213 | ! |
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[358] | 214 | ELSEIF ( ln_dynvor_ens ) THEN ! enstrophy conserving scheme |
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| 215 | DO jj = 2, jpjm1 |
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| 216 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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[1502] | 217 | zy1 = z1_8 * ( zwy(ji ,jj-1) + zwy(ji+1,jj-1) + zwy(ji,jj) + zwy(ji+1,jj ) ) / e1u(ji,jj) |
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| 218 | zx1 = - z1_8 * ( zwx(ji-1,jj ) + zwx(ji-1,jj+1) + zwx(ji,jj) + zwx(ji ,jj+1) ) / e2v(ji,jj) |
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[358] | 219 | zcu(ji,jj) = zy1 * ( ff(ji ,jj-1) + ff(ji,jj) ) |
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| 220 | zcv(ji,jj) = zx1 * ( ff(ji-1,jj ) + ff(ji,jj) ) |
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| 221 | END DO |
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| 222 | END DO |
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[508] | 223 | ! |
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[358] | 224 | ELSEIF ( ln_dynvor_een ) THEN ! enstrophy and energy conserving scheme |
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| 225 | DO jj = 2, jpjm1 |
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| 226 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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[1502] | 227 | zcu(ji,jj) = + z1_4 / e1u(ji,jj) * ( ftne(ji,jj ) * zwy(ji ,jj ) + ftnw(ji+1,jj) * zwy(ji+1,jj ) & |
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| 228 | & + ftse(ji,jj ) * zwy(ji ,jj-1) + ftsw(ji+1,jj) * zwy(ji+1,jj-1) ) |
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| 229 | zcv(ji,jj) = - z1_4 / e2v(ji,jj) * ( ftsw(ji,jj+1) * zwx(ji-1,jj+1) + ftse(ji,jj+1) * zwx(ji ,jj+1) & |
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| 230 | & + ftnw(ji,jj ) * zwx(ji-1,jj ) + ftne(ji,jj ) * zwx(ji ,jj ) ) |
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[358] | 231 | END DO |
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| 232 | END DO |
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[508] | 233 | ! |
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[358] | 234 | ENDIF |
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| 235 | |
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[1502] | 236 | ! !* Right-Hand-Side of the barotropic momentum equation |
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| 237 | ! ! ---------------------------------------------------- |
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| 238 | IF( lk_vvl ) THEN ! Variable volume : remove both Coriolis and Surface pressure gradient |
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| 239 | DO jj = 2, jpjm1 |
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[358] | 240 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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[1502] | 241 | zcu(ji,jj) = zcu(ji,jj) - grav * ( ( rhd(ji+1,jj ,1) + 1 ) * sshn(ji+1,jj ) & |
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| 242 | & - ( rhd(ji ,jj ,1) + 1 ) * sshn(ji ,jj ) ) * hu(ji,jj) / e1u(ji,jj) |
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| 243 | zcv(ji,jj) = zcv(ji,jj) - grav * ( ( rhd(ji ,jj+1,1) + 1 ) * sshn(ji ,jj+1) & |
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| 244 | & - ( rhd(ji ,jj ,1) + 1 ) * sshn(ji ,jj ) ) * hv(ji,jj) / e2v(ji,jj) |
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[358] | 245 | END DO |
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| 246 | END DO |
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[1502] | 247 | ENDIF |
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[358] | 248 | |
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[1502] | 249 | DO jj = 2, jpjm1 ! Remove coriolis term (and possibly spg) from barotropic trend |
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[358] | 250 | DO ji = fs_2, fs_jpim1 |
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| 251 | zua(ji,jj) = zua(ji,jj) - zcu(ji,jj) |
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| 252 | zva(ji,jj) = zva(ji,jj) - zcv(ji,jj) |
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| 253 | END DO |
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| 254 | END DO |
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| 255 | |
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[1708] | 256 | |
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| 257 | ! ! Remove barotropic contribution of bottom friction |
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| 258 | ! ! from the barotropic transport trend |
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| 259 | zcoef = -1. / z2dt_b |
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| 260 | # if defined key_vectopt_loop |
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| 261 | DO jj = 1, 1 |
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[1779] | 262 | DO ji = 1, jpij-jpi ! vector opt. (forced unrolling) |
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[1708] | 263 | # else |
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| 264 | DO jj = 2, jpjm1 |
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| 265 | DO ji = 2, jpim1 |
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| 266 | # endif |
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| 267 | ikbu = MIN( mbathy(ji+1,jj), mbathy(ji,jj) ) |
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| 268 | ikbv = MIN( mbathy(ji,jj+1), mbathy(ji,jj) ) |
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| 269 | ! |
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| 270 | ! Apply stability criteria for bottom friction |
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| 271 | !RBbug for vvl and external mode we may need to |
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| 272 | ! use varying fse3 |
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| 273 | zbfru (ji,jj) = MAX( bfrua(ji,jj), fse3u(ji,jj,ikbu)*zcoef ) |
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| 274 | zbfrv (ji,jj) = MAX( bfrva(ji,jj), fse3v(ji,jj,ikbv)*zcoef ) |
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| 275 | END DO |
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| 276 | END DO |
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| 277 | |
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[1662] | 278 | IF( lk_vvl ) THEN |
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[1708] | 279 | DO jj = 2, jpjm1 |
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| 280 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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| 281 | zua(ji,jj) = zua(ji,jj) - zbfru(ji,jj) * zub(ji,jj) & |
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| 282 | & / ( hu_0(ji,jj) + sshu_b(ji,jj) + 1.e0 - umask(ji,jj,1) ) |
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| 283 | zva(ji,jj) = zva(ji,jj) - zbfrv(ji,jj) * zvb(ji,jj) & |
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| 284 | & / ( hv_0(ji,jj) + sshv_b(ji,jj) + 1.e0 - vmask(ji,jj,1) ) |
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| 285 | END DO |
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| 286 | END DO |
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[1662] | 287 | ELSE |
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[1708] | 288 | DO jj = 2, jpjm1 |
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| 289 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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| 290 | zua(ji,jj) = zua(ji,jj) - zbfru(ji,jj) * zub(ji,jj) * hur(ji,jj) |
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| 291 | zva(ji,jj) = zva(ji,jj) - zbfrv(ji,jj) * zvb(ji,jj) * hvr(ji,jj) |
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| 292 | END DO |
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| 293 | END DO |
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[1662] | 294 | ENDIF |
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| 295 | |
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[1502] | 296 | ! !* d/dt(Ua), Ub, Vn (Vertical mean velocity) |
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| 297 | ! ! -------------------------- |
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| 298 | zua(:,:) = zua(:,:) * hur(:,:) |
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| 299 | zva(:,:) = zva(:,:) * hvr(:,:) |
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| 300 | ! |
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| 301 | IF( lk_vvl ) THEN |
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| 302 | zub(:,:) = zub(:,:) * umask(:,:,1) / ( hu_0(:,:) + sshu_b(:,:) + 1.e0 - umask(:,:,1) ) |
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| 303 | zvb(:,:) = zvb(:,:) * vmask(:,:,1) / ( hv_0(:,:) + sshv_b(:,:) + 1.e0 - vmask(:,:,1) ) |
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| 304 | ELSE |
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| 305 | zub(:,:) = zub(:,:) * hur(:,:) |
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| 306 | zvb(:,:) = zvb(:,:) * hvr(:,:) |
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| 307 | ENDIF |
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| 308 | |
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[358] | 309 | ! ----------------------------------------------------------------------- |
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| 310 | ! Phase 2 : Integration of the barotropic equations with time splitting |
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| 311 | ! ----------------------------------------------------------------------- |
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[1502] | 312 | ! |
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| 313 | ! ! ==================== ! |
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| 314 | ! ! Initialisations ! |
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| 315 | ! ! ==================== ! |
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| 316 | icycle = 2 * nn_baro ! Number of barotropic sub time-step |
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| 317 | |
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| 318 | ! ! Start from NOW field |
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| 319 | hu_e (:,:) = hu (:,:) ! ocean depth at u- and v-points |
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| 320 | hv_e (:,:) = hv (:,:) |
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| 321 | hur_e (:,:) = hur (:,:) ! ocean depth inverted at u- and v-points |
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| 322 | hvr_e (:,:) = hvr (:,:) |
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[1662] | 323 | !RBbug zsshb_e(:,:) = sshn (:,:) |
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| 324 | zsshb_e(:,:) = sshn_b(:,:) ! sea surface height (before and now) |
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[1502] | 325 | sshn_e (:,:) = sshn (:,:) |
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| 326 | |
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| 327 | zun_e (:,:) = un_b (:,:) ! barotropic velocity (external) |
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| 328 | zvn_e (:,:) = vn_b (:,:) |
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| 329 | zub_e (:,:) = un_b (:,:) |
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| 330 | zvb_e (:,:) = vn_b (:,:) |
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[358] | 331 | |
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[1502] | 332 | zu_sum (:,:) = un_b (:,:) ! summation |
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| 333 | zv_sum (:,:) = vn_b (:,:) |
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| 334 | zssh_sum(:,:) = sshn (:,:) |
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[358] | 335 | |
---|
[1502] | 336 | #if defined key_obc |
---|
[367] | 337 | ! set ssh corrections to 0 |
---|
| 338 | ! ssh corrections are applied to normal velocities (Flather's algorithm) and averaged over the barotropic loop |
---|
| 339 | IF( lp_obc_east ) sshfoe_b(:,:) = 0.e0 |
---|
| 340 | IF( lp_obc_west ) sshfow_b(:,:) = 0.e0 |
---|
| 341 | IF( lp_obc_south ) sshfos_b(:,:) = 0.e0 |
---|
| 342 | IF( lp_obc_north ) sshfon_b(:,:) = 0.e0 |
---|
| 343 | #endif |
---|
| 344 | |
---|
[1502] | 345 | ! ! ==================== ! |
---|
| 346 | DO jn = 1, icycle ! sub-time-step loop ! (from NOW to AFTER+1) |
---|
| 347 | ! ! ==================== ! |
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[1241] | 348 | z2dt_e = 2. * ( rdt / nn_baro ) |
---|
[1502] | 349 | IF( jn == 1 ) z2dt_e = rdt / nn_baro |
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[358] | 350 | |
---|
[1502] | 351 | ! !* Update the forcing (OBC, BDY and tides) |
---|
| 352 | ! ! ------------------ |
---|
| 353 | IF( lk_obc ) CALL obc_dta_bt( kt, jn ) |
---|
| 354 | IF( lk_bdy .OR. ln_bdy_tides ) CALL bdy_dta_bt( kt, jn+1 ) |
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[367] | 355 | |
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[1502] | 356 | ! !* after ssh_e |
---|
| 357 | ! ! ----------- |
---|
| 358 | DO jj = 2, jpjm1 ! Horizontal divergence of barotropic transports |
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[358] | 359 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
[1502] | 360 | zhdiv(ji,jj) = ( e2u(ji ,jj) * zun_e(ji ,jj) * hu_e(ji ,jj) & |
---|
| 361 | & - e2u(ji-1,jj) * zun_e(ji-1,jj) * hu_e(ji-1,jj) & |
---|
| 362 | & + e1v(ji,jj ) * zvn_e(ji,jj ) * hv_e(ji,jj ) & |
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| 363 | & - e1v(ji,jj-1) * zvn_e(ji,jj-1) * hv_e(ji,jj-1) ) / ( e1t(ji,jj) * e2t(ji,jj) ) |
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[358] | 364 | END DO |
---|
| 365 | END DO |
---|
[1502] | 366 | ! |
---|
[358] | 367 | #if defined key_obc |
---|
[1502] | 368 | ! ! OBC : zhdiv must be zero behind the open boundary |
---|
| 369 | !! mpp remark: The zeroing of hdiv can probably be extended to 1->jpi/jpj for the correct row/column |
---|
| 370 | IF( lp_obc_east ) zhdiv(nie0p1:nie1p1,nje0 :nje1 ) = 0.e0 ! east |
---|
| 371 | IF( lp_obc_west ) zhdiv(niw0 :niw1 ,njw0 :njw1 ) = 0.e0 ! west |
---|
[367] | 372 | IF( lp_obc_north ) zhdiv(nin0 :nin1 ,njn0p1:njn1p1) = 0.e0 ! north |
---|
[1502] | 373 | IF( lp_obc_south ) zhdiv(nis0 :nis1 ,njs0 :njs1 ) = 0.e0 ! south |
---|
[358] | 374 | #endif |
---|
[1170] | 375 | #if defined key_bdy |
---|
[1502] | 376 | zhdiv(:,:) = zhdiv(:,:) * bdytmask(:,:) ! BDY mask |
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[1170] | 377 | #endif |
---|
[1502] | 378 | ! |
---|
| 379 | DO jj = 2, jpjm1 ! leap-frog on ssh_e |
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[358] | 380 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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[1502] | 381 | ssha_e(ji,jj) = ( zsshb_e(ji,jj) - z2dt_e * ( zraur * emp(ji,jj) + zhdiv(ji,jj) ) ) * tmask(ji,jj,1) |
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[358] | 382 | END DO |
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| 383 | END DO |
---|
| 384 | |
---|
[1502] | 385 | ! !* after barotropic velocities (vorticity scheme dependent) |
---|
| 386 | ! ! --------------------------- |
---|
| 387 | zwx(:,:) = e2u(:,:) * zun_e(:,:) * hu_e(:,:) ! now_e transport |
---|
| 388 | zwy(:,:) = e1v(:,:) * zvn_e(:,:) * hv_e(:,:) |
---|
| 389 | ! |
---|
| 390 | IF( ln_dynvor_ene .OR. ln_dynvor_mix ) THEN !== energy conserving or mixed scheme ==! |
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[358] | 391 | DO jj = 2, jpjm1 |
---|
| 392 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
| 393 | ! surface pressure gradient |
---|
[592] | 394 | IF( lk_vvl) THEN |
---|
[1662] | 395 | zu_spg = -grav * ( ( rhd(ji+1,jj ,1) + 1 ) * sshn_e(ji+1,jj ) & |
---|
| 396 | & - ( rhd(ji ,jj ,1) + 1 ) * sshn_e(ji ,jj ) ) / e1u(ji,jj) |
---|
| 397 | zv_spg = -grav * ( ( rhd(ji ,jj+1,1) + 1 ) * sshn_e(ji ,jj+1) & |
---|
| 398 | & - ( rhd(ji ,jj ,1) + 1 ) * sshn_e(ji ,jj ) ) / e2v(ji,jj) |
---|
[592] | 399 | ELSE |
---|
[1662] | 400 | zu_spg = -grav * ( sshn_e(ji+1,jj) - sshn_e(ji,jj) ) / e1u(ji,jj) |
---|
| 401 | zv_spg = -grav * ( sshn_e(ji,jj+1) - sshn_e(ji,jj) ) / e2v(ji,jj) |
---|
[592] | 402 | ENDIF |
---|
[358] | 403 | ! energy conserving formulation for planetary vorticity term |
---|
| 404 | zy1 = ( zwy(ji ,jj-1) + zwy(ji+1,jj-1) ) / e1u(ji,jj) |
---|
| 405 | zy2 = ( zwy(ji ,jj ) + zwy(ji+1,jj ) ) / e1u(ji,jj) |
---|
| 406 | zx1 = ( zwx(ji-1,jj ) + zwx(ji-1,jj+1) ) / e2v(ji,jj) |
---|
| 407 | zx2 = ( zwx(ji ,jj ) + zwx(ji ,jj+1) ) / e2v(ji,jj) |
---|
[1662] | 408 | zu_cor = z1_4 * ( ff(ji ,jj-1) * zy1 + ff(ji,jj) * zy2 ) * hur_e(ji,jj) |
---|
| 409 | zv_cor =-z1_4 * ( ff(ji-1,jj ) * zx1 + ff(ji,jj) * zx2 ) * hvr_e(ji,jj) |
---|
| 410 | ! after velocities with implicit bottom friction |
---|
| 411 | ua_e(ji,jj) = ( zub_e(ji,jj) + z2dt_e * ( zu_cor + zu_spg + zu_sld + zu_asp + zua(ji,jj) ) ) * umask(ji,jj,1) & |
---|
| 412 | & / ( 1.e0 - z2dt_e * bfrua(ji,jj) * hur_e(ji,jj) ) |
---|
| 413 | va_e(ji,jj) = ( zvb_e(ji,jj) + z2dt_e * ( zv_cor + zv_spg + zv_sld + zv_asp + zva(ji,jj) ) ) * vmask(ji,jj,1) & |
---|
| 414 | & / ( 1.e0 - z2dt_e * bfrva(ji,jj) * hvr_e(ji,jj) ) |
---|
[358] | 415 | END DO |
---|
| 416 | END DO |
---|
[508] | 417 | ! |
---|
[1502] | 418 | ELSEIF ( ln_dynvor_ens ) THEN !== enstrophy conserving scheme ==! |
---|
[358] | 419 | DO jj = 2, jpjm1 |
---|
| 420 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
[1502] | 421 | ! surface pressure gradient |
---|
[592] | 422 | IF( lk_vvl) THEN |
---|
[1662] | 423 | zu_spg = -grav * ( ( rhd(ji+1,jj ,1) + 1 ) * sshn_e(ji+1,jj ) & |
---|
| 424 | & - ( rhd(ji ,jj ,1) + 1 ) * sshn_e(ji ,jj ) ) / e1u(ji,jj) |
---|
| 425 | zv_spg = -grav * ( ( rhd(ji ,jj+1,1) + 1 ) * sshn_e(ji ,jj+1) & |
---|
| 426 | & - ( rhd(ji ,jj ,1) + 1 ) * sshn_e(ji ,jj ) ) / e2v(ji,jj) |
---|
[592] | 427 | ELSE |
---|
[1662] | 428 | zu_spg = -grav * ( sshn_e(ji+1,jj) - sshn_e(ji,jj) ) / e1u(ji,jj) |
---|
| 429 | zv_spg = -grav * ( sshn_e(ji,jj+1) - sshn_e(ji,jj) ) / e2v(ji,jj) |
---|
[592] | 430 | ENDIF |
---|
[358] | 431 | ! enstrophy conserving formulation for planetary vorticity term |
---|
[1502] | 432 | zy1 = z1_8 * ( zwy(ji ,jj-1) + zwy(ji+1,jj-1) + zwy(ji,jj) + zwy(ji+1,jj ) ) / e1u(ji,jj) |
---|
| 433 | zx1 = - z1_8 * ( zwx(ji-1,jj ) + zwx(ji-1,jj+1) + zwx(ji,jj) + zwx(ji ,jj+1) ) / e2v(ji,jj) |
---|
[1662] | 434 | zu_cor = zy1 * ( ff(ji ,jj-1) + ff(ji,jj) ) * hur_e(ji,jj) |
---|
| 435 | zv_cor = zx1 * ( ff(ji-1,jj ) + ff(ji,jj) ) * hvr_e(ji,jj) |
---|
| 436 | ! after velocities with implicit bottom friction |
---|
| 437 | ua_e(ji,jj) = ( zub_e(ji,jj) + z2dt_e * ( zu_cor + zu_spg + zu_sld + zu_asp + zua(ji,jj) ) ) * umask(ji,jj,1) & |
---|
| 438 | & / ( 1.e0 - z2dt_e * bfrua(ji,jj) * hur_e(ji,jj) ) |
---|
| 439 | va_e(ji,jj) = ( zvb_e(ji,jj) + z2dt_e * ( zv_cor + zv_spg + zv_sld + zv_asp + zva(ji,jj) ) ) * vmask(ji,jj,1) & |
---|
| 440 | & / ( 1.e0 - z2dt_e * bfrva(ji,jj) * hvr_e(ji,jj) ) |
---|
[358] | 441 | END DO |
---|
| 442 | END DO |
---|
[508] | 443 | ! |
---|
[1502] | 444 | ELSEIF ( ln_dynvor_een ) THEN !== energy and enstrophy conserving scheme ==! |
---|
[358] | 445 | DO jj = 2, jpjm1 |
---|
| 446 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
| 447 | ! surface pressure gradient |
---|
[592] | 448 | IF( lk_vvl) THEN |
---|
[1662] | 449 | zu_spg = -grav * ( ( rhd(ji+1,jj ,1) + 1 ) * sshn_e(ji+1,jj ) & |
---|
| 450 | & - ( rhd(ji ,jj ,1) + 1 ) * sshn_e(ji ,jj ) ) / e1u(ji,jj) |
---|
| 451 | zv_spg = -grav * ( ( rhd(ji ,jj+1,1) + 1 ) * sshn_e(ji ,jj+1) & |
---|
| 452 | & - ( rhd(ji ,jj ,1) + 1 ) * sshn_e(ji ,jj ) ) / e2v(ji,jj) |
---|
[592] | 453 | ELSE |
---|
[1662] | 454 | zu_spg = -grav * ( sshn_e(ji+1,jj) - sshn_e(ji,jj) ) / e1u(ji,jj) |
---|
| 455 | zv_spg = -grav * ( sshn_e(ji,jj+1) - sshn_e(ji,jj) ) / e2v(ji,jj) |
---|
[592] | 456 | ENDIF |
---|
[358] | 457 | ! energy/enstrophy conserving formulation for planetary vorticity term |
---|
[1662] | 458 | zu_cor = + z1_4 / e1u(ji,jj) * ( ftne(ji,jj ) * zwy(ji ,jj ) + ftnw(ji+1,jj) * zwy(ji+1,jj ) & |
---|
[1502] | 459 | & + ftse(ji,jj ) * zwy(ji ,jj-1) + ftsw(ji+1,jj) * zwy(ji+1,jj-1) ) * hur_e(ji,jj) |
---|
[1662] | 460 | zv_cor = - z1_4 / e2v(ji,jj) * ( ftsw(ji,jj+1) * zwx(ji-1,jj+1) + ftse(ji,jj+1) * zwx(ji ,jj+1) & |
---|
[1502] | 461 | & + ftnw(ji,jj ) * zwx(ji-1,jj ) + ftne(ji,jj ) * zwx(ji ,jj ) ) * hvr_e(ji,jj) |
---|
[1662] | 462 | ! after velocities with implicit bottom friction |
---|
| 463 | ua_e(ji,jj) = ( zub_e(ji,jj) + z2dt_e * ( zu_cor + zu_spg + zu_sld + zu_asp + zua(ji,jj) ) ) * umask(ji,jj,1) & |
---|
| 464 | & / ( 1.e0 - z2dt_e * bfrua(ji,jj) * hur_e(ji,jj) ) |
---|
| 465 | va_e(ji,jj) = ( zvb_e(ji,jj) + z2dt_e * ( zv_cor + zv_spg + zv_sld + zv_asp + zva(ji,jj) ) ) * vmask(ji,jj,1) & |
---|
| 466 | & / ( 1.e0 - z2dt_e * bfrva(ji,jj) * hvr_e(ji,jj) ) |
---|
[358] | 467 | END DO |
---|
| 468 | END DO |
---|
[508] | 469 | ! |
---|
[358] | 470 | ENDIF |
---|
[1502] | 471 | ! !* domain lateral boundary |
---|
| 472 | ! ! ----------------------- |
---|
| 473 | ! ! Flather's boundary condition for the barotropic loop : |
---|
| 474 | ! ! - Update sea surface height on each open boundary |
---|
| 475 | ! ! - Correct the velocity |
---|
[358] | 476 | |
---|
[1502] | 477 | IF( lk_obc ) CALL obc_fla_ts |
---|
| 478 | IF( lk_bdy .OR. ln_bdy_tides ) CALL bdy_dyn_fla( sshn_e ) |
---|
| 479 | ! |
---|
| 480 | CALL lbc_lnk( ua_e , 'U', -1. ) ! local domain boundaries |
---|
| 481 | CALL lbc_lnk( va_e , 'V', -1. ) |
---|
| 482 | CALL lbc_lnk( ssha_e, 'T', 1. ) |
---|
[358] | 483 | |
---|
[1502] | 484 | zu_sum (:,:) = zu_sum (:,:) + ua_e (:,:) ! Sum over sub-time-steps |
---|
| 485 | zv_sum (:,:) = zv_sum (:,:) + va_e (:,:) |
---|
| 486 | zssh_sum(:,:) = zssh_sum(:,:) + ssha_e(:,:) |
---|
[367] | 487 | |
---|
[1502] | 488 | ! !* Time filter and swap |
---|
| 489 | ! ! -------------------- |
---|
| 490 | IF( jn == 1 ) THEN ! Swap only (1st Euler time step) |
---|
| 491 | zsshb_e(:,:) = sshn_e(:,:) |
---|
| 492 | zub_e (:,:) = zun_e (:,:) |
---|
| 493 | zvb_e (:,:) = zvn_e (:,:) |
---|
| 494 | sshn_e (:,:) = ssha_e(:,:) |
---|
| 495 | zun_e (:,:) = ua_e (:,:) |
---|
| 496 | zvn_e (:,:) = va_e (:,:) |
---|
| 497 | ELSE ! Swap + Filter |
---|
| 498 | zsshb_e(:,:) = atfp * ( zsshb_e(:,:) + ssha_e(:,:) ) + atfp1 * sshn_e(:,:) |
---|
| 499 | zub_e (:,:) = atfp * ( zub_e (:,:) + ua_e (:,:) ) + atfp1 * zun_e (:,:) |
---|
| 500 | zvb_e (:,:) = atfp * ( zvb_e (:,:) + va_e (:,:) ) + atfp1 * zvn_e (:,:) |
---|
| 501 | sshn_e (:,:) = ssha_e(:,:) |
---|
| 502 | zun_e (:,:) = ua_e (:,:) |
---|
| 503 | zvn_e (:,:) = va_e (:,:) |
---|
[358] | 504 | ENDIF |
---|
| 505 | |
---|
[1502] | 506 | IF( lk_vvl ) THEN !* Update ocean depth (variable volume case only) |
---|
| 507 | ! ! ------------------ |
---|
| 508 | DO jj = 1, jpjm1 ! Sea Surface Height at u- & v-points |
---|
| 509 | DO ji = 1, fs_jpim1 ! Vector opt. |
---|
| 510 | zsshun_e(ji,jj) = 0.5 * umask(ji,jj,1) / ( e1u(ji,jj) * e2u(ji,jj) ) & |
---|
| 511 | & * ( e1t(ji ,jj) * e2t(ji ,jj) * sshn_e(ji ,jj) & |
---|
| 512 | & + e1t(ji+1,jj) * e2t(ji+1,jj) * sshn_e(ji+1,jj) ) |
---|
| 513 | zsshvn_e(ji,jj) = 0.5 * vmask(ji,jj,1) / ( e1v(ji,jj) * e2v(ji,jj) ) & |
---|
| 514 | & * ( e1t(ji,jj ) * e2t(ji,jj ) * sshn_e(ji,jj ) & |
---|
| 515 | & + e1t(ji,jj+1) * e2t(ji,jj+1) * sshn_e(ji,jj+1) ) |
---|
[592] | 516 | END DO |
---|
| 517 | END DO |
---|
[1502] | 518 | CALL lbc_lnk( zsshun_e, 'U', 1. ) ! lateral boundaries conditions |
---|
| 519 | CALL lbc_lnk( zsshvn_e, 'V', 1. ) |
---|
[1438] | 520 | ! |
---|
[1502] | 521 | hu_e (:,:) = hu_0(:,:) + zsshun_e(:,:) ! Ocean depth at U- and V-points |
---|
| 522 | hv_e (:,:) = hv_0(:,:) + zsshvn_e(:,:) |
---|
| 523 | hur_e(:,:) = umask(:,:,1) / ( hu_e(:,:) + 1.e0 - umask(:,:,1) ) |
---|
| 524 | hvr_e(:,:) = vmask(:,:,1) / ( hv_e(:,:) + 1.e0 - vmask(:,:,1) ) |
---|
| 525 | ! |
---|
[1438] | 526 | ENDIF |
---|
[358] | 527 | ! ! ==================== ! |
---|
| 528 | END DO ! end loop ! |
---|
| 529 | ! ! ==================== ! |
---|
| 530 | |
---|
[367] | 531 | #if defined key_obc |
---|
[1502] | 532 | IF( lp_obc_east ) sshfoe_b(:,:) = zcoef * sshfoe_b(:,:) !!gm totally useless ????? |
---|
[1241] | 533 | IF( lp_obc_west ) sshfow_b(:,:) = zcoef * sshfow_b(:,:) |
---|
| 534 | IF( lp_obc_north ) sshfon_b(:,:) = zcoef * sshfon_b(:,:) |
---|
| 535 | IF( lp_obc_south ) sshfos_b(:,:) = zcoef * sshfos_b(:,:) |
---|
[367] | 536 | #endif |
---|
[358] | 537 | |
---|
[1438] | 538 | ! ----------------------------------------------------------------------------- |
---|
[1502] | 539 | ! Phase 3. update the general trend with the barotropic trend |
---|
[1438] | 540 | ! ----------------------------------------------------------------------------- |
---|
[1502] | 541 | ! |
---|
| 542 | ! !* Time average ==> after barotropic u, v, ssh |
---|
| 543 | zcoef = 1.e0 / ( 2 * nn_baro + 1 ) |
---|
| 544 | un_b (:,:) = zcoef * zu_sum (:,:) |
---|
| 545 | vn_b (:,:) = zcoef * zv_sum (:,:) |
---|
| 546 | sshn_b(:,:) = zcoef * zssh_sum(:,:) |
---|
| 547 | ! |
---|
| 548 | ! !* update the general momentum trend |
---|
[358] | 549 | DO jk=1,jpkm1 |
---|
[1502] | 550 | ua(:,:,jk) = ua(:,:,jk) + ( un_b(:,:) - zub(:,:) ) / z2dt_b |
---|
| 551 | va(:,:,jk) = va(:,:,jk) + ( vn_b(:,:) - zvb(:,:) ) / z2dt_b |
---|
[358] | 552 | END DO |
---|
[1502] | 553 | ! |
---|
| 554 | ! !* write time-spliting arrays in the restart |
---|
[508] | 555 | IF( lrst_oce ) CALL ts_rst( kt, 'WRITE' ) |
---|
| 556 | ! |
---|
[1662] | 557 | ! |
---|
[508] | 558 | END SUBROUTINE dyn_spg_ts |
---|
| 559 | |
---|
| 560 | |
---|
| 561 | SUBROUTINE ts_rst( kt, cdrw ) |
---|
| 562 | !!--------------------------------------------------------------------- |
---|
| 563 | !! *** ROUTINE ts_rst *** |
---|
| 564 | !! |
---|
| 565 | !! ** Purpose : Read or write time-splitting arrays in restart file |
---|
| 566 | !!---------------------------------------------------------------------- |
---|
| 567 | INTEGER , INTENT(in) :: kt ! ocean time-step |
---|
| 568 | CHARACTER(len=*), INTENT(in) :: cdrw ! "READ"/"WRITE" flag |
---|
| 569 | ! |
---|
| 570 | INTEGER :: ji, jk ! dummy loop indices |
---|
| 571 | !!---------------------------------------------------------------------- |
---|
| 572 | ! |
---|
| 573 | IF( TRIM(cdrw) == 'READ' ) THEN |
---|
[1502] | 574 | IF( iom_varid( numror, 'un_b', ldstop = .FALSE. ) > 0 ) THEN |
---|
| 575 | CALL iom_get( numror, jpdom_autoglo, 'un_b' , un_b (:,:) ) ! external velocity issued |
---|
| 576 | CALL iom_get( numror, jpdom_autoglo, 'vn_b' , vn_b (:,:) ) ! from barotropic loop |
---|
[508] | 577 | ELSE |
---|
[1502] | 578 | un_b (:,:) = 0.e0 |
---|
| 579 | vn_b (:,:) = 0.e0 |
---|
[508] | 580 | ! vertical sum |
---|
| 581 | IF( lk_vopt_loop ) THEN ! vector opt., forced unroll |
---|
| 582 | DO jk = 1, jpkm1 |
---|
| 583 | DO ji = 1, jpij |
---|
[1502] | 584 | un_b(ji,1) = un_b(ji,1) + fse3u(ji,1,jk) * un(ji,1,jk) |
---|
| 585 | vn_b(ji,1) = vn_b(ji,1) + fse3v(ji,1,jk) * vn(ji,1,jk) |
---|
[508] | 586 | END DO |
---|
| 587 | END DO |
---|
| 588 | ELSE ! No vector opt. |
---|
| 589 | DO jk = 1, jpkm1 |
---|
[1502] | 590 | un_b(:,:) = un_b(:,:) + fse3u(:,:,jk) * un(:,:,jk) |
---|
| 591 | vn_b(:,:) = vn_b(:,:) + fse3v(:,:,jk) * vn(:,:,jk) |
---|
[508] | 592 | END DO |
---|
| 593 | ENDIF |
---|
[1502] | 594 | un_b (:,:) = un_b(:,:) * hur(:,:) |
---|
| 595 | vn_b (:,:) = vn_b(:,:) * hvr(:,:) |
---|
[508] | 596 | ENDIF |
---|
| 597 | ELSEIF( TRIM(cdrw) == 'WRITE' ) THEN |
---|
[1502] | 598 | CALL iom_rstput( kt, nitrst, numrow, 'un_b' , un_b (:,:) ) ! external velocity issued |
---|
| 599 | CALL iom_rstput( kt, nitrst, numrow, 'vn_b' , vn_b (:,:) ) ! from barotropic loop |
---|
[358] | 600 | ENDIF |
---|
[508] | 601 | ! |
---|
| 602 | END SUBROUTINE ts_rst |
---|
| 603 | |
---|
[358] | 604 | #else |
---|
| 605 | !!---------------------------------------------------------------------- |
---|
| 606 | !! Default case : Empty module No standart free surface cst volume |
---|
| 607 | !!---------------------------------------------------------------------- |
---|
| 608 | CONTAINS |
---|
| 609 | SUBROUTINE dyn_spg_ts( kt ) ! Empty routine |
---|
| 610 | WRITE(*,*) 'dyn_spg_ts: You should not have seen this print! error?', kt |
---|
| 611 | END SUBROUTINE dyn_spg_ts |
---|
[657] | 612 | SUBROUTINE ts_rst( kt, cdrw ) ! Empty routine |
---|
| 613 | INTEGER , INTENT(in) :: kt ! ocean time-step |
---|
| 614 | CHARACTER(len=*), INTENT(in) :: cdrw ! "READ"/"WRITE" flag |
---|
| 615 | WRITE(*,*) 'ts_rst : You should not have seen this print! error?', kt, cdrw |
---|
| 616 | END SUBROUTINE ts_rst |
---|
[358] | 617 | #endif |
---|
| 618 | |
---|
| 619 | !!====================================================================== |
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| 620 | END MODULE dynspg_ts |
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