[358] | 1 | MODULE dynspg_ts |
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| 2 | !!====================================================================== |
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| 3 | !! *** MODULE dynspg_ts *** |
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| 4 | !! Ocean dynamics: surface pressure gradient trend |
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| 5 | !!====================================================================== |
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[508] | 6 | !! History : 9.0 ! 04-12 (L. Bessieres, G. Madec) Original code |
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| 7 | !! " " ! 05-11 (V. Garnier, G. Madec) optimization |
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| 8 | !! 9.0 ! 06-08 (S. Masson) distributed restart using iom |
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| 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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[508] | 14 | !!---------------------------------------------------------------------- |
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[358] | 15 | !! dyn_spg_ts : compute surface pressure gradient trend using a time- |
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| 16 | !! splitting scheme and add to the general trend |
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[508] | 17 | !! ts_rst : read/write the time-splitting restart fields in the ocean restart file |
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[358] | 18 | !!---------------------------------------------------------------------- |
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| 19 | !! * Modules used |
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| 20 | USE oce ! ocean dynamics and tracers |
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| 21 | USE dom_oce ! ocean space and time domain |
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| 22 | USE phycst ! physical constants |
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[719] | 23 | USE ocesbc ! ocean surface boundary condition |
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[367] | 24 | USE obcdta ! open boundary condition data |
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| 25 | USE obcfla ! Flather open boundary condition |
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[358] | 26 | USE dynvor ! vorticity term |
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| 27 | USE obc_oce ! Lateral open boundary condition |
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[371] | 28 | USE obc_par ! open boundary condition parameters |
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[358] | 29 | USE lib_mpp ! distributed memory computing library |
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| 30 | USE lbclnk ! ocean lateral boundary conditions (or mpp link) |
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| 31 | USE prtctl ! Print control |
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[719] | 32 | USE dynspg_oce ! surface pressure gradient variables |
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[358] | 33 | USE in_out_manager ! I/O manager |
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[508] | 34 | USE iom |
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| 35 | USE restart ! only for lrst_oce |
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[719] | 36 | USE domvvl ! variable volume |
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[358] | 37 | |
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| 38 | IMPLICIT NONE |
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| 39 | PRIVATE |
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| 40 | |
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| 41 | PUBLIC dyn_spg_ts ! routine called by step.F90 |
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[575] | 42 | PUBLIC ts_rst ! routine called by j-k-i subroutine |
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[358] | 43 | |
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[508] | 44 | REAL(wp), DIMENSION(jpi,jpj) :: ftnw, ftne, & ! triad of coriolis parameter |
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| 45 | & ftsw, ftse ! (only used with een vorticity scheme) |
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| 46 | |
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| 47 | |
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[358] | 48 | !! * Substitutions |
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| 49 | # include "domzgr_substitute.h90" |
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| 50 | # include "vectopt_loop_substitute.h90" |
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| 51 | !!---------------------------------------------------------------------- |
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[359] | 52 | !! OPA 9.0 , LOCEAN-IPSL (2005) |
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[719] | 53 | !! $Header: /home/opalod/NEMOCVSROOT/NEMO/OPA_SRC/DYN/dynspg_ts.F90,v 1.16 2007/06/05 10:38:27 opalod Exp $ |
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[359] | 54 | !! This software is governed by the CeCILL licence see modipsl/doc/NEMO_CeCILL.txt |
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[358] | 55 | !!---------------------------------------------------------------------- |
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| 56 | |
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| 57 | CONTAINS |
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| 58 | |
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| 59 | SUBROUTINE dyn_spg_ts( kt ) |
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| 60 | !!---------------------------------------------------------------------- |
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| 61 | !! *** routine dyn_spg_ts *** |
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| 62 | !! |
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| 63 | !! ** Purpose : Compute the now trend due to the surface pressure |
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| 64 | !! gradient in case of free surface formulation with time-splitting. |
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| 65 | !! Add it to the general trend of momentum equation. |
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| 66 | !! Compute the free surface. |
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| 67 | !! |
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| 68 | !! ** Method : Free surface formulation with time-splitting |
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| 69 | !! -1- Save the vertically integrated trend. This general trend is |
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| 70 | !! held constant over the barotropic integration. |
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| 71 | !! The Coriolis force is removed from the general trend as the |
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| 72 | !! surface gradient and the Coriolis force are updated within |
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| 73 | !! the barotropic integration. |
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[367] | 74 | !! -2- Barotropic loop : updates of sea surface height (ssha_e) and |
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| 75 | !! barotropic transports (ua_e and va_e) through barotropic |
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[358] | 76 | !! momentum and continuity integration. Barotropic former |
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| 77 | !! variables are time averaging over the full barotropic cycle |
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| 78 | !! (= 2 * baroclinic time step) and saved in zsshX_b, zuX_b |
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| 79 | !! and zvX_b (X specifying after, now or before). |
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| 80 | !! -3- Update of sea surface height from time averaged barotropic |
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| 81 | !! variables. |
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| 82 | !! - apply lateral boundary conditions on sshn. |
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| 83 | !! -4- The new general trend becomes : |
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| 84 | !! ua = ua - sum_k(ua)/H + ( zua_b - sum_k(ub) )/H |
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| 85 | !! |
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| 86 | !! ** Action : - Update (ua,va) with the surf. pressure gradient trend |
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| 87 | !! |
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[508] | 88 | !! References : Griffies et al., (2003): A technical guide to MOM4. NOAA/GFDL |
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[358] | 89 | !!--------------------------------------------------------------------- |
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| 90 | INTEGER, INTENT( in ) :: kt ! ocean time-step index |
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| 91 | |
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| 92 | !! * Local declarations |
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| 93 | INTEGER :: ji, jj, jk, jit ! dummy loop indices |
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| 94 | INTEGER :: icycle ! temporary scalar |
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| 95 | REAL(wp) :: & |
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| 96 | zraur, zcoef, z2dt_e, z2dt_b, zfac25, & ! temporary scalars |
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| 97 | zfact1, zspgu, zcubt, zx1, zy1, & ! " " |
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| 98 | zfact2, zspgv, zcvbt, zx2, zy2 ! " " |
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| 99 | REAL(wp), DIMENSION(jpi,jpj) :: & |
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| 100 | zcu, zcv, zwx, zwy, zhdiv, & ! temporary arrays |
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| 101 | zua, zva, zub, zvb, & ! " " |
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| 102 | zssha_b, zua_b, zva_b, & ! " " |
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| 103 | zsshb_e, zub_e, zvb_e, & ! " " |
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[367] | 104 | zun_e, zvn_e ! " " |
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[592] | 105 | !! Variable volume |
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| 106 | REAL(wp), DIMENSION(jpi,jpj) :: & |
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| 107 | zspgu_1, zspgv_1, zsshun_e, zsshvn_e, hu_e, hv_e ! 2D workspace |
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| 108 | REAL(wp), DIMENSION(jpi,jpj,jpk) :: zfse3un_e, zfse3vn_e ! 3D workspace |
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[358] | 109 | !!---------------------------------------------------------------------- |
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| 110 | |
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| 111 | ! Arrays initialization |
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| 112 | ! --------------------- |
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[367] | 113 | zua_b(:,:) = 0.e0 ; zub_e(:,:) = 0.e0 ; zun_e(:,:) = 0.e0 |
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| 114 | zva_b(:,:) = 0.e0 ; zvb_e(:,:) = 0.e0 ; zvn_e(:,:) = 0.e0 |
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[363] | 115 | zhdiv(:,:) = 0.e0 |
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[358] | 116 | |
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| 117 | |
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| 118 | IF( kt == nit000 ) THEN |
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[508] | 119 | ! |
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[358] | 120 | IF(lwp) WRITE(numout,*) |
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| 121 | IF(lwp) WRITE(numout,*) 'dyn_spg_ts : surface pressure gradient trend' |
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| 122 | IF(lwp) WRITE(numout,*) '~~~~~~~~~~ free surface with time splitting' |
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| 123 | IF(lwp) WRITE(numout,*) ' Number of sub cycle in 1 time-step (2 rdt) : icycle = ', FLOOR( 2*rdt/rdtbt ) |
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| 124 | |
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[508] | 125 | CALL ts_rst( nit000, 'READ' ) ! read or initialize the following fields: |
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| 126 | ! ! sshb, sshn, sshb_b, sshn_b, un_b, vn_b |
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| 127 | |
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[367] | 128 | ssha_e(:,:) = sshn(:,:) |
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| 129 | ua_e(:,:) = un_b(:,:) |
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| 130 | va_e(:,:) = vn_b(:,:) |
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[358] | 131 | |
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| 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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| 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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[592] | 146 | ! Substract the surface pressure gradient from the momentum |
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| 147 | ! --------------------------------------------------------- |
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| 148 | IF( lk_vvl ) THEN ! Variable volume |
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| 149 | |
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| 150 | ! 0. Local initialization |
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| 151 | ! ----------------------- |
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| 152 | zspgu_1(:,:) = 0.e0 |
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| 153 | zspgv_1(:,:) = 0.e0 |
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| 154 | |
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| 155 | ! 1. Surface pressure gradient (now) |
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| 156 | ! ---------------------------- |
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| 157 | DO jj = 2, jpjm1 |
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| 158 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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| 159 | zspgu_1(ji,jj) = -grav * ( ( rhd(ji+1,jj ,1) + 1 ) * sshn(ji+1,jj ) & |
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| 160 | & - ( rhd(ji ,jj ,1) + 1 ) * sshn(ji ,jj ) ) / e1u(ji,jj) |
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| 161 | zspgv_1(ji,jj) = -grav * ( ( rhd(ji ,jj+1,1) + 1 ) * sshn(ji ,jj+1) & |
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| 162 | & - ( rhd(ji ,jj ,1) + 1 ) * sshn(ji ,jj ) ) / e2v(ji,jj) |
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| 163 | END DO |
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| 164 | END DO |
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| 165 | |
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| 166 | ! 2. Substract the surface pressure trend from the general trend |
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| 167 | ! ------------------------------------------------------ |
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| 168 | DO jk = 1, jpkm1 |
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| 169 | DO jj = 2, jpjm1 |
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| 170 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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| 171 | ua(ji,jj,jk) = ua(ji,jj,jk) - zspgu_1(ji,jj) |
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| 172 | va(ji,jj,jk) = va(ji,jj,jk) - zspgv_1(ji,jj) |
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| 173 | END DO |
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| 174 | END DO |
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| 175 | END DO |
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| 176 | |
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| 177 | ENDIF |
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| 178 | |
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[358] | 179 | ! Local constant initialization |
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| 180 | ! -------------------------------- |
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| 181 | z2dt_b = 2.0 * rdt ! baroclinic time step |
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| 182 | IF ( neuler == 0 .AND. kt == nit000 ) z2dt_b = rdt |
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[374] | 183 | zfact1 = 0.5 * 0.25 ! coefficient for vorticity estimates |
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[358] | 184 | zfact2 = 0.5 * 0.5 |
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[374] | 185 | zraur = 1. / rauw ! 1 / volumic mass of pure water |
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[358] | 186 | |
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| 187 | ! ----------------------------------------------------------------------------- |
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| 188 | ! Phase 1 : Coupling between general trend and barotropic estimates (1st step) |
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| 189 | ! ----------------------------------------------------------------------------- |
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| 190 | |
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| 191 | ! Vertically integrated quantities |
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| 192 | ! -------------------------------- |
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| 193 | zua(:,:) = 0.e0 |
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| 194 | zva(:,:) = 0.e0 |
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| 195 | zub(:,:) = 0.e0 |
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| 196 | zvb(:,:) = 0.e0 |
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| 197 | zwx(:,:) = 0.e0 |
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| 198 | zwy(:,:) = 0.e0 |
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| 199 | |
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| 200 | ! vertical sum |
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| 201 | IF( lk_vopt_loop ) THEN ! vector opt., forced unroll |
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| 202 | DO jk = 1, jpkm1 |
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| 203 | DO ji = 1, jpij |
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| 204 | ! ! Vertically integrated momentum trends |
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| 205 | zua(ji,1) = zua(ji,1) + fse3u(ji,1,jk) * umask(ji,1,jk) * ua(ji,1,jk) |
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| 206 | zva(ji,1) = zva(ji,1) + fse3v(ji,1,jk) * vmask(ji,1,jk) * va(ji,1,jk) |
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| 207 | ! ! Vertically integrated transports (before) |
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| 208 | zub(ji,1) = zub(ji,1) + fse3u(ji,1,jk) * ub(ji,1,jk) |
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| 209 | zvb(ji,1) = zvb(ji,1) + fse3v(ji,1,jk) * vb(ji,1,jk) |
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| 210 | ! ! Planetary vorticity transport fluxes (now) |
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| 211 | zwx(ji,1) = zwx(ji,1) + e2u(ji,1) * fse3u(ji,1,jk) * un(ji,1,jk) |
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| 212 | zwy(ji,1) = zwy(ji,1) + e1v(ji,1) * fse3v(ji,1,jk) * vn(ji,1,jk) |
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| 213 | END DO |
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| 214 | END DO |
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| 215 | ELSE ! No vector opt. |
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| 216 | DO jk = 1, jpkm1 |
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| 217 | ! ! Vertically integrated momentum trends |
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| 218 | zua(:,:) = zua(:,:) + fse3u(:,:,jk) * umask(:,:,jk) * ua(:,:,jk) |
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| 219 | zva(:,:) = zva(:,:) + fse3v(:,:,jk) * vmask(:,:,jk) * va(:,:,jk) |
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| 220 | ! ! Vertically integrated transports (before) |
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| 221 | zub(:,:) = zub(:,:) + fse3u(:,:,jk) * ub(:,:,jk) |
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| 222 | zvb(:,:) = zvb(:,:) + fse3v(:,:,jk) * vb(:,:,jk) |
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| 223 | ! ! Planetary vorticity (now) |
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| 224 | zwx(:,:) = zwx(:,:) + e2u(:,:) * fse3u(:,:,jk) * un(:,:,jk) |
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| 225 | zwy(:,:) = zwy(:,:) + e1v(:,:) * fse3v(:,:,jk) * vn(:,:,jk) |
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| 226 | END DO |
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| 227 | ENDIF |
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| 228 | |
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| 229 | IF( ln_dynvor_ene .OR. ln_dynvor_mix ) THEN ! energy conserving or mixed scheme |
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| 230 | DO jj = 2, jpjm1 |
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| 231 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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| 232 | zy1 = ( zwy(ji,jj-1) + zwy(ji+1,jj-1) ) / e1u(ji,jj) |
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| 233 | zy2 = ( zwy(ji,jj ) + zwy(ji+1,jj ) ) / e1u(ji,jj) |
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| 234 | zx1 = ( zwx(ji-1,jj) + zwx(ji-1,jj+1) ) / e2v(ji,jj) |
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| 235 | zx2 = ( zwx(ji ,jj) + zwx(ji ,jj+1) ) / e2v(ji,jj) |
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| 236 | ! energy conserving formulation for planetary vorticity term |
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| 237 | zcu(ji,jj) = zfact2 * ( ff(ji ,jj-1) * zy1 + ff(ji,jj) * zy2 ) |
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| 238 | zcv(ji,jj) =-zfact2 * ( ff(ji-1,jj ) * zx1 + ff(ji,jj) * zx2 ) |
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| 239 | END DO |
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| 240 | END DO |
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[508] | 241 | ! |
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[358] | 242 | ELSEIF ( ln_dynvor_ens ) THEN ! enstrophy conserving scheme |
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| 243 | DO jj = 2, jpjm1 |
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| 244 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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| 245 | zy1 = zfact1 * ( zwy(ji ,jj-1) + zwy(ji+1,jj-1) & |
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| 246 | + zwy(ji ,jj ) + zwy(ji+1,jj ) ) / e1u(ji,jj) |
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| 247 | zx1 =-zfact1 * ( zwx(ji-1,jj ) + zwx(ji-1,jj+1) & |
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| 248 | + zwx(ji ,jj ) + zwx(ji ,jj+1) ) / e2v(ji,jj) |
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| 249 | zcu(ji,jj) = zy1 * ( ff(ji ,jj-1) + ff(ji,jj) ) |
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| 250 | zcv(ji,jj) = zx1 * ( ff(ji-1,jj ) + ff(ji,jj) ) |
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| 251 | END DO |
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| 252 | END DO |
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[508] | 253 | ! |
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[358] | 254 | ELSEIF ( ln_dynvor_een ) THEN ! enstrophy and energy conserving scheme |
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| 255 | zfac25 = 0.25 |
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| 256 | DO jj = 2, jpjm1 |
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| 257 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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| 258 | zcu(ji,jj) = + zfac25 / e1u(ji,jj) & |
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[553] | 259 | & * ( ftne(ji,jj ) * zwy(ji ,jj ) + ftnw(ji+1,jj) * zwy(ji+1,jj ) & |
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| 260 | & + ftse(ji,jj ) * zwy(ji ,jj-1) + ftsw(ji+1,jj) * zwy(ji+1,jj-1) ) |
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[358] | 261 | zcv(ji,jj) = - zfac25 / e2v(ji,jj) & |
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[553] | 262 | & * ( ftsw(ji,jj+1) * zwx(ji-1,jj+1) + ftse(ji,jj+1) * zwx(ji ,jj+1) & |
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| 263 | & + ftnw(ji,jj ) * zwx(ji-1,jj ) + ftne(ji,jj ) * zwx(ji ,jj ) ) |
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[358] | 264 | END DO |
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| 265 | END DO |
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[508] | 266 | ! |
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[358] | 267 | ENDIF |
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| 268 | |
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| 269 | |
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| 270 | ! Remove barotropic trend from general momentum trend |
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| 271 | ! --------------------------------------------------- |
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| 272 | DO jk = 1 , jpkm1 |
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| 273 | DO jj = 2, jpjm1 |
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| 274 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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| 275 | ua(ji,jj,jk) = ua(ji,jj,jk) - zua(ji,jj) * hur(ji,jj) |
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| 276 | va(ji,jj,jk) = va(ji,jj,jk) - zva(ji,jj) * hvr(ji,jj) |
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| 277 | END DO |
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| 278 | END DO |
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| 279 | END DO |
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| 280 | |
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| 281 | ! Remove coriolis term from barotropic trend |
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| 282 | ! ------------------------------------------ |
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| 283 | DO jj = 2, jpjm1 |
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| 284 | DO ji = fs_2, fs_jpim1 |
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| 285 | zua(ji,jj) = zua(ji,jj) - zcu(ji,jj) |
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| 286 | zva(ji,jj) = zva(ji,jj) - zcv(ji,jj) |
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| 287 | END DO |
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| 288 | END DO |
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| 289 | |
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| 290 | ! ----------------------------------------------------------------------- |
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| 291 | ! Phase 2 : Integration of the barotropic equations with time splitting |
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| 292 | ! ----------------------------------------------------------------------- |
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| 293 | |
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| 294 | ! Initialisations |
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| 295 | !---------------- |
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| 296 | ! Number of iteration of the barotropic loop |
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| 297 | icycle = FLOOR( z2dt_b / rdtbt ) |
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| 298 | |
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| 299 | ! variables for the barotropic equations |
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| 300 | zsshb_e(:,:) = sshn_b(:,:) ! (barotropic) sea surface height (before and now) |
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[367] | 301 | sshn_e (:,:) = sshn_b(:,:) |
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| 302 | zub_e (:,:) = un_b (:,:) ! barotropic transports issued from the barotropic equations (before and now) |
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| 303 | zvb_e (:,:) = vn_b (:,:) |
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| 304 | zun_e (:,:) = un_b (:,:) |
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| 305 | zvn_e (:,:) = vn_b (:,:) |
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| 306 | zssha_b(:,:) = sshn (:,:) ! time averaged variables over all sub-timesteps |
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| 307 | zua_b (:,:) = un_b (:,:) |
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| 308 | zva_b (:,:) = vn_b (:,:) |
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[592] | 309 | IF( lk_vvl ) THEN |
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| 310 | zsshun_e(:,:) = sshu (:,:) ! (barotropic) sea surface height (now) at u-point |
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| 311 | zsshvn_e(:,:) = sshv (:,:) ! (barotropic) sea surface height (now) at v-point |
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| 312 | hu_e(:,:) = hu (:,:) ! (barotropic) ocean depth at u-point |
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| 313 | hv_e(:,:) = hv (:,:) ! (barotropic) ocean depth at v-point |
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| 314 | zfse3un_e(:,:,:) = fse3u(:,:,:) ! (barotropic) scale factors at u-point |
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| 315 | zfse3un_e(:,:,:) = fse3v(:,:,:) ! (barotropic) scale factors at v-point |
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| 316 | ENDIF |
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[358] | 317 | |
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[367] | 318 | ! set ssh corrections to 0 |
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| 319 | ! ssh corrections are applied to normal velocities (Flather's algorithm) and averaged over the barotropic loop |
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| 320 | #if defined key_obc |
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| 321 | IF( lp_obc_east ) sshfoe_b(:,:) = 0.e0 |
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| 322 | IF( lp_obc_west ) sshfow_b(:,:) = 0.e0 |
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| 323 | IF( lp_obc_south ) sshfos_b(:,:) = 0.e0 |
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| 324 | IF( lp_obc_north ) sshfon_b(:,:) = 0.e0 |
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| 325 | #endif |
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| 326 | |
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[358] | 327 | ! Barotropic integration over 2 baroclinic time steps |
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| 328 | ! --------------------------------------------------- |
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| 329 | |
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| 330 | ! ! ==================== ! |
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| 331 | DO jit = 1, icycle ! sub-time-step loop ! |
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| 332 | ! ! ==================== ! |
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| 333 | z2dt_e = 2. * rdtbt |
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| 334 | IF ( jit == 1 ) z2dt_e = rdtbt |
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| 335 | |
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[367] | 336 | ! Time interpolation of open boundary condition data |
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| 337 | IF( lk_obc ) CALL obc_dta_bt( kt, jit ) |
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| 338 | |
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[358] | 339 | ! Horizontal divergence of barotropic transports |
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| 340 | !-------------------------------------------------- |
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| 341 | DO jj = 2, jpjm1 |
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| 342 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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| 343 | zhdiv(ji,jj) = ( e2u(ji ,jj ) * zun_e(ji ,jj) & |
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| 344 | & -e2u(ji-1,jj ) * zun_e(ji-1,jj) & |
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| 345 | & +e1v(ji ,jj ) * zvn_e(ji ,jj) & |
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| 346 | & -e1v(ji ,jj-1) * zvn_e(ji ,jj-1) ) & |
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| 347 | & / (e1t(ji,jj)*e2t(ji,jj)) |
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| 348 | END DO |
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| 349 | END DO |
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| 350 | |
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| 351 | #if defined key_obc |
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| 352 | ! open boundaries (div must be zero behind the open boundary) |
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| 353 | ! mpp remark: The zeroing of hdiv can probably be extended to 1->jpi/jpj for the correct row/column |
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[367] | 354 | IF( lp_obc_east ) zhdiv(nie0p1:nie1p1,nje0 :nje1) = 0.e0 ! east |
---|
| 355 | IF( lp_obc_west ) zhdiv(niw0 :niw1 ,njw0 :njw1) = 0.e0 ! west |
---|
| 356 | IF( lp_obc_north ) zhdiv(nin0 :nin1 ,njn0p1:njn1p1) = 0.e0 ! north |
---|
| 357 | IF( lp_obc_south ) zhdiv(nis0 :nis1 ,njs0 :njs1) = 0.e0 ! south |
---|
[358] | 358 | #endif |
---|
| 359 | |
---|
| 360 | ! Sea surface height from the barotropic system |
---|
| 361 | !---------------------------------------------- |
---|
| 362 | DO jj = 2, jpjm1 |
---|
| 363 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
[367] | 364 | ssha_e(ji,jj) = ( zsshb_e(ji,jj) - z2dt_e * ( zraur * emp(ji,jj) & |
---|
[358] | 365 | & + zhdiv(ji,jj) ) ) * tmask(ji,jj,1) |
---|
| 366 | END DO |
---|
| 367 | END DO |
---|
| 368 | |
---|
| 369 | ! evolution of the barotropic transport ( following the vorticity scheme used) |
---|
| 370 | ! ---------------------------------------------------------------------------- |
---|
| 371 | zwx(:,:) = e2u(:,:) * zun_e(:,:) |
---|
| 372 | zwy(:,:) = e1v(:,:) * zvn_e(:,:) |
---|
| 373 | |
---|
| 374 | IF( ln_dynvor_ene .OR. ln_dynvor_mix ) THEN ! energy conserving or mixed scheme |
---|
| 375 | DO jj = 2, jpjm1 |
---|
| 376 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
| 377 | ! surface pressure gradient |
---|
[592] | 378 | IF( lk_vvl) THEN |
---|
| 379 | zspgu = -grav * ( ( rhd(ji+1,jj,1) + 1 ) * sshn_e(ji+1,jj) & |
---|
| 380 | & - ( rhd(ji,jj,1) + 1 ) * sshn_e(ji,jj) ) * hu_e(ji,jj) / e1u(ji,jj) |
---|
| 381 | zspgv = -grav * ( ( rhd(ji,jj+1,1) + 1 ) * sshn_e(ji,jj+1) & |
---|
| 382 | & - ( rhd(ji,jj,1) + 1 ) * sshn_e(ji,jj) ) * hv_e(ji,jj) / e2v(ji,jj) |
---|
| 383 | ELSE |
---|
| 384 | zspgu = -grav * ( sshn_e(ji+1,jj) - sshn_e(ji,jj) ) * hu(ji,jj) / e1u(ji,jj) |
---|
| 385 | zspgv = -grav * ( sshn_e(ji,jj+1) - sshn_e(ji,jj) ) * hv(ji,jj) / e2v(ji,jj) |
---|
| 386 | ENDIF |
---|
[358] | 387 | ! energy conserving formulation for planetary vorticity term |
---|
| 388 | zy1 = ( zwy(ji ,jj-1) + zwy(ji+1,jj-1) ) / e1u(ji,jj) |
---|
| 389 | zy2 = ( zwy(ji ,jj ) + zwy(ji+1,jj ) ) / e1u(ji,jj) |
---|
| 390 | zx1 = ( zwx(ji-1,jj ) + zwx(ji-1,jj+1) ) / e2v(ji,jj) |
---|
| 391 | zx2 = ( zwx(ji ,jj ) + zwx(ji ,jj+1) ) / e2v(ji,jj) |
---|
| 392 | zcubt = zfact2 * ( ff(ji ,jj-1) * zy1 + ff(ji,jj) * zy2 ) |
---|
| 393 | zcvbt =-zfact2 * ( ff(ji-1,jj ) * zx1 + ff(ji,jj) * zx2 ) |
---|
| 394 | ! after transports |
---|
[367] | 395 | ua_e(ji,jj) = ( zub_e(ji,jj) + z2dt_e * ( zcubt + zspgu + zua(ji,jj) ) ) * umask(ji,jj,1) |
---|
| 396 | va_e(ji,jj) = ( zvb_e(ji,jj) + z2dt_e * ( zcvbt + zspgv + zva(ji,jj) ) ) * vmask(ji,jj,1) |
---|
[358] | 397 | END DO |
---|
| 398 | END DO |
---|
[508] | 399 | ! |
---|
[358] | 400 | ELSEIF ( ln_dynvor_ens ) THEN ! enstrophy conserving scheme |
---|
| 401 | DO jj = 2, jpjm1 |
---|
| 402 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
| 403 | ! surface pressure gradient |
---|
[592] | 404 | IF( lk_vvl) THEN |
---|
| 405 | zspgu = -grav * ( ( rhd(ji+1,jj,1) + 1 ) * sshn_e(ji+1,jj) & |
---|
| 406 | & - ( rhd(ji,jj,1) + 1 ) * sshn_e(ji,jj) ) * hu_e(ji,jj) / e1u(ji,jj) |
---|
| 407 | zspgv = -grav * ( ( rhd(ji,jj+1,1) + 1 ) * sshn_e(ji,jj+1) & |
---|
| 408 | & - ( rhd(ji,jj,1) + 1 ) * sshn_e(ji,jj) ) * hv_e(ji,jj) / e2v(ji,jj) |
---|
| 409 | ELSE |
---|
| 410 | zspgu = -grav * ( sshn_e(ji+1,jj) - sshn_e(ji,jj) ) * hu(ji,jj) / e1u(ji,jj) |
---|
| 411 | zspgv = -grav * ( sshn_e(ji,jj+1) - sshn_e(ji,jj) ) * hv(ji,jj) / e2v(ji,jj) |
---|
| 412 | ENDIF |
---|
[358] | 413 | ! enstrophy conserving formulation for planetary vorticity term |
---|
| 414 | zy1 = zfact1 * ( zwy(ji ,jj-1) + zwy(ji+1,jj-1) & |
---|
| 415 | + zwy(ji ,jj ) + zwy(ji+1,jj ) ) / e1u(ji,jj) |
---|
| 416 | zx1 =-zfact1 * ( zwx(ji-1,jj ) + zwx(ji-1,jj+1) & |
---|
| 417 | + zwx(ji ,jj ) + zwx(ji ,jj+1) ) / e2v(ji,jj) |
---|
| 418 | zcubt = zy1 * ( ff(ji ,jj-1) + ff(ji,jj) ) |
---|
| 419 | zcvbt = zx1 * ( ff(ji-1,jj ) + ff(ji,jj) ) |
---|
| 420 | ! after transports |
---|
[367] | 421 | ua_e(ji,jj) = ( zub_e(ji,jj) + z2dt_e * ( zcubt + zspgu + zua(ji,jj) ) ) * umask(ji,jj,1) |
---|
| 422 | va_e(ji,jj) = ( zvb_e(ji,jj) + z2dt_e * ( zcvbt + zspgv + zva(ji,jj) ) ) * vmask(ji,jj,1) |
---|
[358] | 423 | END DO |
---|
| 424 | END DO |
---|
[508] | 425 | ! |
---|
[358] | 426 | ELSEIF ( ln_dynvor_een ) THEN ! energy and enstrophy conserving scheme |
---|
| 427 | zfac25 = 0.25 |
---|
| 428 | DO jj = 2, jpjm1 |
---|
| 429 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
| 430 | ! surface pressure gradient |
---|
[592] | 431 | IF( lk_vvl) THEN |
---|
| 432 | zspgu = -grav * ( ( rhd(ji+1,jj,1) + 1 ) * sshn_e(ji+1,jj) & |
---|
| 433 | & - ( rhd(ji,jj,1) + 1 ) * sshn_e(ji,jj) ) * hu_e(ji,jj) / e1u(ji,jj) |
---|
| 434 | zspgv = -grav * ( ( rhd(ji,jj+1,1) + 1 ) * sshn_e(ji,jj+1) & |
---|
| 435 | & - ( rhd(ji,jj,1) + 1 ) * sshn_e(ji,jj) ) * hv_e(ji,jj) / e2v(ji,jj) |
---|
| 436 | ELSE |
---|
| 437 | zspgu = -grav * ( sshn_e(ji+1,jj) - sshn_e(ji,jj) ) * hu(ji,jj) / e1u(ji,jj) |
---|
| 438 | zspgv = -grav * ( sshn_e(ji,jj+1) - sshn_e(ji,jj) ) * hv(ji,jj) / e2v(ji,jj) |
---|
| 439 | ENDIF |
---|
[358] | 440 | ! energy/enstrophy conserving formulation for planetary vorticity term |
---|
[553] | 441 | zcubt = + zfac25 / e1u(ji,jj) * ( ftne(ji,jj ) * zwy(ji ,jj ) + ftnw(ji+1,jj) * zwy(ji+1,jj ) & |
---|
| 442 | & + ftse(ji,jj ) * zwy(ji ,jj-1) + ftsw(ji+1,jj) * zwy(ji+1,jj-1) ) |
---|
| 443 | zcvbt = - zfac25 / e2v(ji,jj) * ( ftsw(ji,jj+1) * zwx(ji-1,jj+1) + ftse(ji,jj+1) * zwx(ji ,jj+1) & |
---|
| 444 | & + ftnw(ji,jj ) * zwx(ji-1,jj ) + ftne(ji,jj ) * zwx(ji ,jj ) ) |
---|
[358] | 445 | ! after transports |
---|
[367] | 446 | ua_e(ji,jj) = ( zub_e(ji,jj) + z2dt_e * ( zcubt + zspgu + zua(ji,jj) ) ) * umask(ji,jj,1) |
---|
| 447 | va_e(ji,jj) = ( zvb_e(ji,jj) + z2dt_e * ( zcvbt + zspgv + zva(ji,jj) ) ) * vmask(ji,jj,1) |
---|
[358] | 448 | END DO |
---|
| 449 | END DO |
---|
[508] | 450 | ! |
---|
[358] | 451 | ENDIF |
---|
| 452 | |
---|
[367] | 453 | ! Flather's boundary condition for the barotropic loop : |
---|
| 454 | ! - Update sea surface height on each open boundary |
---|
| 455 | ! - Correct the barotropic transports |
---|
[371] | 456 | IF( lk_obc ) CALL obc_fla_ts |
---|
[358] | 457 | |
---|
[367] | 458 | |
---|
| 459 | ! ... Boundary conditions on ua_e, va_e, ssha_e |
---|
| 460 | CALL lbc_lnk( ua_e , 'U', -1. ) |
---|
| 461 | CALL lbc_lnk( va_e , 'V', -1. ) |
---|
| 462 | CALL lbc_lnk( ssha_e, 'T', 1. ) |
---|
| 463 | |
---|
[358] | 464 | ! temporal sum |
---|
| 465 | !------------- |
---|
[367] | 466 | zssha_b(:,:) = zssha_b(:,:) + ssha_e(:,:) |
---|
| 467 | zua_b (:,:) = zua_b (:,:) + ua_e (:,:) |
---|
| 468 | zva_b (:,:) = zva_b (:,:) + va_e (:,:) |
---|
[358] | 469 | |
---|
| 470 | ! Time filter and swap of dynamics arrays |
---|
| 471 | ! --------------------------------------- |
---|
[592] | 472 | IF( neuler == 0 .AND. jit == 1 ) THEN ! Euler (forward) time stepping |
---|
[367] | 473 | zsshb_e(:,:) = sshn_e(:,:) |
---|
| 474 | zub_e (:,:) = zun_e (:,:) |
---|
| 475 | zvb_e (:,:) = zvn_e (:,:) |
---|
| 476 | sshn_e (:,:) = ssha_e(:,:) |
---|
| 477 | zun_e (:,:) = ua_e (:,:) |
---|
| 478 | zvn_e (:,:) = va_e (:,:) |
---|
[358] | 479 | ELSE ! Asselin filtering |
---|
[367] | 480 | zsshb_e(:,:) = atfp * ( zsshb_e(:,:) + ssha_e(:,:) ) + atfp1 * sshn_e(:,:) |
---|
| 481 | zub_e (:,:) = atfp * ( zub_e (:,:) + ua_e (:,:) ) + atfp1 * zun_e (:,:) |
---|
| 482 | zvb_e (:,:) = atfp * ( zvb_e (:,:) + va_e (:,:) ) + atfp1 * zvn_e (:,:) |
---|
| 483 | sshn_e (:,:) = ssha_e(:,:) |
---|
| 484 | zun_e (:,:) = ua_e (:,:) |
---|
| 485 | zvn_e (:,:) = va_e (:,:) |
---|
[358] | 486 | ENDIF |
---|
| 487 | |
---|
[592] | 488 | IF( lk_vvl ) THEN ! Variable volume |
---|
| 489 | |
---|
| 490 | ! Sea surface elevation |
---|
| 491 | ! --------------------- |
---|
| 492 | DO jj = 1, jpjm1 |
---|
| 493 | DO ji = 1,jpim1 |
---|
| 494 | |
---|
| 495 | ! Sea Surface Height at u-point before |
---|
| 496 | zsshun_e(ji,jj) = 0.5 * umask(ji,jj,1) / ( e1u(ji,jj) * e2u(ji,jj) ) & |
---|
| 497 | & * ( e1t(ji ,jj) * e2t(ji ,jj) * sshn_e(ji ,jj) & |
---|
| 498 | & + e1t(ji+1,jj) * e2t(ji+1,jj) * sshn_e(ji+1,jj) ) |
---|
| 499 | |
---|
| 500 | ! Sea Surface Height at v-point before |
---|
| 501 | zsshvn_e(ji,jj) = 0.5 * vmask(ji,jj,1) / ( e1v(ji,jj) * e2v(ji,jj) ) & |
---|
| 502 | & * ( e1t(ji,jj ) * e2t(ji,jj ) * sshn_e(ji,jj ) & |
---|
| 503 | & + e1t(ji,jj+1) * e2t(ji,jj+1) * sshn_e(ji,jj+1) ) |
---|
| 504 | |
---|
| 505 | END DO |
---|
| 506 | END DO |
---|
| 507 | |
---|
| 508 | ! Boundaries conditions |
---|
| 509 | CALL lbc_lnk( zsshun_e, 'U', 1. ) ; CALL lbc_lnk( zsshvn_e, 'V', 1. ) |
---|
| 510 | |
---|
| 511 | ! Scale factors at before and after time step |
---|
| 512 | ! ------------------------------------------- |
---|
[661] | 513 | CALL dom_vvl_sf( zsshun_e, 'U', zfse3un_e ) ; CALL dom_vvl_sf( zsshvn_e, 'V', zfse3vn_e ) |
---|
[592] | 514 | |
---|
| 515 | ! Ocean depth at U- and V-points |
---|
| 516 | hu_e(:,:) = 0.e0 |
---|
| 517 | hv_e(:,:) = 0.e0 |
---|
| 518 | |
---|
| 519 | DO jk = 1, jpk |
---|
| 520 | hu_e(:,:) = hu_e(:,:) + zfse3un_e(:,:,jk) * umask(:,:,jk) |
---|
| 521 | hv_e(:,:) = hv_e(:,:) + zfse3vn_e(:,:,jk) * vmask(:,:,jk) |
---|
| 522 | END DO |
---|
| 523 | |
---|
| 524 | ENDIF ! End variable volume case |
---|
| 525 | |
---|
[358] | 526 | ! ! ==================== ! |
---|
| 527 | END DO ! end loop ! |
---|
| 528 | ! ! ==================== ! |
---|
| 529 | |
---|
| 530 | |
---|
| 531 | ! Time average of after barotropic variables |
---|
| 532 | zcoef = 1.e0 / ( FLOAT( icycle +1 ) ) |
---|
| 533 | zssha_b(:,:) = zcoef * zssha_b(:,:) |
---|
[367] | 534 | zua_b (:,:) = zcoef * zua_b (:,:) |
---|
| 535 | zva_b (:,:) = zcoef * zva_b (:,:) |
---|
| 536 | #if defined key_obc |
---|
| 537 | IF( lp_obc_east ) sshfoe_b(:,:) = zcoef * sshfoe_b(:,:) |
---|
| 538 | IF( lp_obc_west ) sshfow_b(:,:) = zcoef * sshfow_b(:,:) |
---|
| 539 | IF( lp_obc_north ) sshfon_b(:,:) = zcoef * sshfon_b(:,:) |
---|
| 540 | IF( lp_obc_south ) sshfos_b(:,:) = zcoef * sshfos_b(:,:) |
---|
| 541 | #endif |
---|
[358] | 542 | |
---|
| 543 | |
---|
| 544 | ! --------------------------------------------------------------------------- |
---|
| 545 | ! Phase 3 : Update sea surface height from time averaged barotropic variables |
---|
| 546 | ! --------------------------------------------------------------------------- |
---|
| 547 | |
---|
| 548 | |
---|
| 549 | ! Horizontal divergence of time averaged barotropic transports |
---|
| 550 | !------------------------------------------------------------- |
---|
[592] | 551 | IF( .NOT. lk_vvl ) THEN |
---|
| 552 | DO jj = 2, jpjm1 |
---|
| 553 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
| 554 | zhdiv(ji,jj) = ( e2u(ji,jj) * un_b(ji,jj) - e2u(ji-1,jj ) * un_b(ji-1,jj ) & |
---|
| 555 | & +e1v(ji,jj) * vn_b(ji,jj) - e1v(ji ,jj-1) * vn_b(ji ,jj-1) ) & |
---|
| 556 | & / ( e1t(ji,jj) * e2t(ji,jj) ) |
---|
| 557 | END DO |
---|
[358] | 558 | END DO |
---|
[592] | 559 | ENDIF |
---|
[358] | 560 | |
---|
[592] | 561 | #if defined key_obc && ! defined key_vvl |
---|
[358] | 562 | ! open boundaries (div must be zero behind the open boundary) |
---|
| 563 | ! mpp remark: The zeroing of hdiv can probably be extended to 1->jpi/jpj for the correct row/column |
---|
[367] | 564 | IF( lp_obc_east ) zhdiv(nie0p1:nie1p1,nje0 :nje1) = 0.e0 ! east |
---|
| 565 | IF( lp_obc_west ) zhdiv(niw0 :niw1 ,njw0 :njw1) = 0.e0 ! west |
---|
[358] | 566 | IF( lp_obc_north ) zhdiv(nin0 :nin1 ,njn0p1:njn1p1) = 0.e0 ! north |
---|
[367] | 567 | IF( lp_obc_south ) zhdiv(nis0 :nis1 ,njs0 :njs1) = 0.e0 ! south |
---|
[358] | 568 | #endif |
---|
| 569 | |
---|
| 570 | ! sea surface height |
---|
| 571 | !------------------- |
---|
[592] | 572 | IF( lk_vvl ) THEN |
---|
| 573 | sshbb(:,:) = sshb(:,:) |
---|
| 574 | sshb (:,:) = sshn(:,:) |
---|
| 575 | sshn (:,:) = ssha(:,:) |
---|
| 576 | ELSE |
---|
| 577 | sshb (:,:) = sshn(:,:) |
---|
| 578 | sshn(:,:) = ( sshb_b(:,:) - z2dt_b * ( zraur * emp(:,:) + zhdiv(:,:) ) ) * tmask(:,:,1) |
---|
| 579 | ENDIF |
---|
[358] | 580 | |
---|
| 581 | ! ... Boundary conditions on sshn |
---|
[367] | 582 | IF( .NOT. lk_obc ) CALL lbc_lnk( sshn, 'T', 1. ) |
---|
[358] | 583 | |
---|
| 584 | |
---|
| 585 | ! ----------------------------------------------------------------------------- |
---|
| 586 | ! Phase 4. Coupling between general trend and barotropic estimates - (2nd step) |
---|
| 587 | ! ----------------------------------------------------------------------------- |
---|
| 588 | |
---|
| 589 | ! Swap on time averaged barotropic variables |
---|
| 590 | ! ------------------------------------------ |
---|
| 591 | sshb_b(:,:) = sshn_b (:,:) |
---|
[592] | 592 | IF ( kt == nit000 ) zssha_b(:,:) = sshn(:,:) |
---|
[358] | 593 | sshn_b(:,:) = zssha_b(:,:) |
---|
| 594 | un_b (:,:) = zua_b (:,:) |
---|
| 595 | vn_b (:,:) = zva_b (:,:) |
---|
| 596 | |
---|
| 597 | ! add time averaged barotropic coriolis and surface pressure gradient |
---|
| 598 | ! terms to the general momentum trend |
---|
| 599 | ! -------------------------------------------------------------------- |
---|
| 600 | DO jk=1,jpkm1 |
---|
| 601 | ua(:,:,jk) = ua(:,:,jk) + hur(:,:) * ( zua_b(:,:) - zub(:,:) ) / z2dt_b |
---|
| 602 | va(:,:,jk) = va(:,:,jk) + hvr(:,:) * ( zva_b(:,:) - zvb(:,:) ) / z2dt_b |
---|
| 603 | END DO |
---|
| 604 | |
---|
[508] | 605 | ! write filtered free surface arrays in restart file |
---|
| 606 | ! -------------------------------------------------- |
---|
| 607 | IF( lrst_oce ) CALL ts_rst( kt, 'WRITE' ) |
---|
| 608 | |
---|
| 609 | ! print sum trends (used for debugging) |
---|
| 610 | IF( ln_ctl ) CALL prt_ctl( tab2d_1=sshn, clinfo1=' ssh : ', mask1=tmask ) |
---|
| 611 | ! |
---|
| 612 | END SUBROUTINE dyn_spg_ts |
---|
| 613 | |
---|
| 614 | |
---|
| 615 | SUBROUTINE ts_rst( kt, cdrw ) |
---|
| 616 | !!--------------------------------------------------------------------- |
---|
| 617 | !! *** ROUTINE ts_rst *** |
---|
| 618 | !! |
---|
| 619 | !! ** Purpose : Read or write time-splitting arrays in restart file |
---|
| 620 | !!---------------------------------------------------------------------- |
---|
| 621 | INTEGER , INTENT(in) :: kt ! ocean time-step |
---|
| 622 | CHARACTER(len=*), INTENT(in) :: cdrw ! "READ"/"WRITE" flag |
---|
| 623 | ! |
---|
| 624 | INTEGER :: ji, jk ! dummy loop indices |
---|
| 625 | !!---------------------------------------------------------------------- |
---|
| 626 | ! |
---|
| 627 | IF( TRIM(cdrw) == 'READ' ) THEN |
---|
[746] | 628 | IF( iom_varid( numror, 'sshn', ldstop = .FALSE. ) > 0 ) THEN |
---|
[683] | 629 | CALL iom_get( numror, jpdom_autoglo, 'sshb' , sshb(:,:) ) |
---|
| 630 | CALL iom_get( numror, jpdom_autoglo, 'sshn' , sshn(:,:) ) |
---|
[508] | 631 | IF( neuler == 0 ) sshb(:,:) = sshn(:,:) |
---|
| 632 | ELSE |
---|
[558] | 633 | IF( nn_rstssh == 1 ) THEN |
---|
| 634 | sshb(:,:) = 0.e0 |
---|
| 635 | sshn(:,:) = 0.e0 |
---|
| 636 | ENDIF |
---|
[508] | 637 | ENDIF |
---|
[746] | 638 | IF( iom_varid( numror, 'sshn_b', ldstop = .FALSE. ) > 0 ) THEN |
---|
[683] | 639 | CALL iom_get( numror, jpdom_autoglo, 'sshb_b', sshb_b(:,:) ) ! free surface issued |
---|
| 640 | CALL iom_get( numror, jpdom_autoglo, 'sshn_b', sshn_b(:,:) ) ! from time-splitting loop |
---|
| 641 | CALL iom_get( numror, jpdom_autoglo, 'un_b' , un_b (:,:) ) ! horizontal transports issued |
---|
| 642 | CALL iom_get( numror, jpdom_autoglo, 'vn_b' , vn_b (:,:) ) ! from barotropic loop |
---|
[508] | 643 | IF( neuler == 0 ) sshb_b(:,:) = sshn_b(:,:) |
---|
| 644 | ELSE |
---|
| 645 | sshb_b(:,:) = sshb(:,:) |
---|
| 646 | sshn_b(:,:) = sshn(:,:) |
---|
| 647 | un_b (:,:) = 0.e0 |
---|
| 648 | vn_b (:,:) = 0.e0 |
---|
| 649 | ! vertical sum |
---|
| 650 | IF( lk_vopt_loop ) THEN ! vector opt., forced unroll |
---|
| 651 | DO jk = 1, jpkm1 |
---|
| 652 | DO ji = 1, jpij |
---|
| 653 | un_b(ji,1) = un_b(ji,1) + fse3u(ji,1,jk) * un(ji,1,jk) |
---|
| 654 | vn_b(ji,1) = vn_b(ji,1) + fse3v(ji,1,jk) * vn(ji,1,jk) |
---|
| 655 | END DO |
---|
| 656 | END DO |
---|
| 657 | ELSE ! No vector opt. |
---|
| 658 | DO jk = 1, jpkm1 |
---|
| 659 | un_b(:,:) = un_b(:,:) + fse3u(:,:,jk) * un(:,:,jk) |
---|
| 660 | vn_b(:,:) = vn_b(:,:) + fse3v(:,:,jk) * vn(:,:,jk) |
---|
| 661 | END DO |
---|
| 662 | ENDIF |
---|
| 663 | ENDIF |
---|
| 664 | ELSEIF( TRIM(cdrw) == 'WRITE' ) THEN |
---|
| 665 | CALL iom_rstput( kt, nitrst, numrow, 'sshb' , sshb (:,:) ) |
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| 666 | CALL iom_rstput( kt, nitrst, numrow, 'sshn' , sshn (:,:) ) |
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| 667 | CALL iom_rstput( kt, nitrst, numrow, 'sshb_b', sshb_b(:,:) ) ! free surface issued |
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| 668 | CALL iom_rstput( kt, nitrst, numrow, 'sshn_b', sshn_b(:,:) ) ! from barotropic loop |
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| 669 | CALL iom_rstput( kt, nitrst, numrow, 'un_b' , un_b (:,:) ) ! horizontal transports issued |
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| 670 | CALL iom_rstput( kt, nitrst, numrow, 'vn_b' , vn_b (:,:) ) ! from barotropic loop |
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[358] | 671 | ENDIF |
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[508] | 672 | ! |
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| 673 | END SUBROUTINE ts_rst |
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| 674 | |
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[358] | 675 | #else |
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| 676 | !!---------------------------------------------------------------------- |
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| 677 | !! Default case : Empty module No standart free surface cst volume |
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| 678 | !!---------------------------------------------------------------------- |
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| 679 | CONTAINS |
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| 680 | SUBROUTINE dyn_spg_ts( kt ) ! Empty routine |
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| 681 | WRITE(*,*) 'dyn_spg_ts: You should not have seen this print! error?', kt |
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| 682 | END SUBROUTINE dyn_spg_ts |
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[657] | 683 | SUBROUTINE ts_rst( kt, cdrw ) ! Empty routine |
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| 684 | INTEGER , INTENT(in) :: kt ! ocean time-step |
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| 685 | CHARACTER(len=*), INTENT(in) :: cdrw ! "READ"/"WRITE" flag |
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| 686 | WRITE(*,*) 'ts_rst : You should not have seen this print! error?', kt, cdrw |
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| 687 | END SUBROUTINE ts_rst |
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[358] | 688 | #endif |
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| 689 | |
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| 690 | !!====================================================================== |
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| 691 | END MODULE dynspg_ts |
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