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, split-explicit scheme |
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5 | !!====================================================================== |
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6 | !! History : 1.0 ! 2004-12 (L. Bessieres, G. Madec) Original code |
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7 | !! - ! 2005-11 (V. Garnier, G. Madec) optimization |
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8 | !! - ! 2006-08 (S. Masson) distributed restart using iom |
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9 | !! 2.0 ! 2007-07 (D. Storkey) calls to BDY routines |
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10 | !! - ! 2008-01 (R. Benshila) change averaging method |
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11 | !! 3.2 ! 2009-07 (R. Benshila, G. Madec) Complete revisit associated to vvl reactivation |
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12 | !! 3.3 ! 2010-09 (D. Storkey, E. O'Dea) update for BDY for Shelf configurations |
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13 | !! 3.3 ! 2011-03 (R. Benshila, R. Hordoir, P. Oddo) update calculation of ub_b |
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14 | !! 3.5 ! 2013-07 (J. Chanut) Switch to Forward-backward time stepping |
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15 | !! 3.6 ! 2013-11 (A. Coward) Update for z-tilde compatibility |
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16 | !! 3.7 ! 2015-11 (J. Chanut) free surface simplification |
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17 | !! - ! 2016-12 (G. Madec, E. Clementi) update for Stoke-Drift divergence |
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18 | !! 4.0 ! 2017-05 (G. Madec) drag coef. defined at t-point (zdfdrg.F90) |
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19 | !!--------------------------------------------------------------------- |
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20 | |
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21 | !!---------------------------------------------------------------------- |
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22 | !! dyn_spg_ts : compute surface pressure gradient trend using a time-splitting scheme |
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23 | !! dyn_spg_ts_init: initialisation of the time-splitting scheme |
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24 | !! ts_wgt : set time-splitting weights for temporal averaging (or not) |
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25 | !! ts_rst : read/write time-splitting fields in restart file |
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26 | !!---------------------------------------------------------------------- |
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27 | USE oce ! ocean dynamics and tracers |
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28 | USE dom_oce ! ocean space and time domain |
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29 | USE sbc_oce ! surface boundary condition: ocean |
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30 | USE zdf_oce ! vertical physics: variables |
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31 | USE zdfdrg ! vertical physics: top/bottom drag coef. |
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32 | USE sbcisf ! ice shelf variable (fwfisf) |
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33 | USE sbcapr ! surface boundary condition: atmospheric pressure |
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34 | USE dynadv , ONLY: ln_dynadv_vec |
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35 | USE phycst ! physical constants |
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36 | USE dynvor ! vorticity term |
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37 | USE wet_dry ! wetting/drying flux limter |
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38 | USE bdy_oce ! open boundary |
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39 | USE bdytides ! open boundary condition data |
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40 | USE bdydyn2d ! open boundary conditions on barotropic variables |
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41 | USE sbctide ! tides |
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42 | USE updtide ! tide potential |
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43 | USE sbcwave ! surface wave |
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44 | USE diatmb ! Top,middle,bottom output |
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45 | #if defined key_agrif |
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46 | USE agrif_opa_interp ! agrif |
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47 | #endif |
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48 | #if defined key_asminc |
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49 | USE asminc ! Assimilation increment |
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50 | #endif |
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51 | ! |
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52 | USE in_out_manager ! I/O manager |
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53 | USE lib_mpp ! distributed memory computing library |
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54 | USE lbclnk ! ocean lateral boundary conditions (or mpp link) |
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55 | USE prtctl ! Print control |
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56 | USE iom ! IOM library |
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57 | USE restart ! only for lrst_oce |
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58 | USE timing ! Timing |
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59 | |
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60 | IMPLICIT NONE |
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61 | PRIVATE |
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62 | |
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63 | PUBLIC dyn_spg_ts ! routine called in dynspg.F90 |
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64 | PUBLIC dyn_spg_ts_alloc ! " " " " |
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65 | PUBLIC dyn_spg_ts_init ! " " " " |
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66 | PUBLIC ts_rst ! " " " " |
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67 | |
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68 | !! Time filtered arrays at baroclinic time step: |
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69 | REAL(wp), PUBLIC, ALLOCATABLE, SAVE, DIMENSION(:,:) :: un_adv , vn_adv !: Advection vel. at "now" barocl. step |
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70 | |
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71 | INTEGER , SAVE :: icycle ! Number of barotropic sub-steps for each internal step nn_baro <= 2.5 nn_baro |
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72 | REAL(wp), SAVE :: rdtbt ! Barotropic time step |
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73 | ! |
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74 | REAL(wp), ALLOCATABLE, SAVE, DIMENSION(:) :: wgtbtp1, wgtbtp2 ! 1st & 2nd weights used in time filtering of barotropic fields |
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75 | REAL(wp), ALLOCATABLE, SAVE, DIMENSION(:,:) :: zwz ! ff_f/h at F points |
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76 | REAL(wp), ALLOCATABLE, SAVE, DIMENSION(:,:) :: ftnw, ftne ! triad of coriolis parameter |
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77 | REAL(wp), ALLOCATABLE, SAVE, DIMENSION(:,:) :: ftsw, ftse ! (only used with een vorticity scheme) |
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78 | |
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79 | REAL(wp) :: r1_12 = 1._wp / 12._wp ! local ratios |
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80 | REAL(wp) :: r1_8 = 0.125_wp ! |
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81 | REAL(wp) :: r1_4 = 0.25_wp ! |
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82 | REAL(wp) :: r1_2 = 0.5_wp ! |
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83 | |
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84 | !! * Substitutions |
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85 | # include "vectopt_loop_substitute.h90" |
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86 | !!---------------------------------------------------------------------- |
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87 | !! NEMO/OPA 4.0 , NEMO Consortium (2017) |
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88 | !! $Id$ |
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89 | !! Software governed by the CeCILL licence (NEMOGCM/NEMO_CeCILL.txt) |
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90 | !!---------------------------------------------------------------------- |
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91 | CONTAINS |
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92 | |
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93 | INTEGER FUNCTION dyn_spg_ts_alloc() |
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94 | !!---------------------------------------------------------------------- |
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95 | !! *** routine dyn_spg_ts_alloc *** |
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96 | !!---------------------------------------------------------------------- |
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97 | INTEGER :: ierr(3) |
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98 | !!---------------------------------------------------------------------- |
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99 | ierr(:) = 0 |
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100 | ! |
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101 | ALLOCATE( wgtbtp1(3*nn_baro), wgtbtp2(3*nn_baro), zwz(jpi,jpj), STAT=ierr(1) ) |
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102 | ! |
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103 | IF( ln_dynvor_een ) ALLOCATE( ftnw(jpi,jpj) , ftne(jpi,jpj) , & |
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104 | & ftsw(jpi,jpj) , ftse(jpi,jpj) , STAT=ierr(2) ) |
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105 | ! |
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106 | ALLOCATE( un_adv(jpi,jpj), vn_adv(jpi,jpj) , STAT=ierr(3) ) |
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107 | ! |
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108 | dyn_spg_ts_alloc = MAXVAL( ierr(:) ) |
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109 | ! |
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110 | IF( lk_mpp ) CALL mpp_sum( dyn_spg_ts_alloc ) |
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111 | IF( dyn_spg_ts_alloc /= 0 ) CALL ctl_warn('dyn_spg_ts_alloc: failed to allocate arrays') |
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112 | ! |
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113 | END FUNCTION dyn_spg_ts_alloc |
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114 | |
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115 | |
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116 | SUBROUTINE dyn_spg_ts( kt ) |
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117 | !!---------------------------------------------------------------------- |
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118 | !! |
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119 | !! ** Purpose : - Compute the now trend due to the explicit time stepping |
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120 | !! of the quasi-linear barotropic system, and add it to the |
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121 | !! general momentum trend. |
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122 | !! |
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123 | !! ** Method : - split-explicit schem (time splitting) : |
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124 | !! Barotropic variables are advanced from internal time steps |
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125 | !! "n" to "n+1" if ln_bt_fw=T |
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126 | !! or from |
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127 | !! "n-1" to "n+1" if ln_bt_fw=F |
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128 | !! thanks to a generalized forward-backward time stepping (see ref. below). |
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129 | !! |
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130 | !! ** Action : |
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131 | !! -Update the filtered free surface at step "n+1" : ssha |
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132 | !! -Update filtered barotropic velocities at step "n+1" : ua_b, va_b |
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133 | !! -Compute barotropic advective velocities at step "n" : un_adv, vn_adv |
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134 | !! These are used to advect tracers and are compliant with discrete |
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135 | !! continuity equation taken at the baroclinic time steps. This |
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136 | !! ensures tracers conservation. |
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137 | !! - (ua, va) momentum trend updated with barotropic component. |
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138 | !! |
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139 | !! References : Shchepetkin and McWilliams, Ocean Modelling, 2005. |
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140 | !!--------------------------------------------------------------------- |
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141 | INTEGER, INTENT(in) :: kt ! ocean time-step index |
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142 | ! |
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143 | INTEGER :: ji, jj, jk, jn ! dummy loop indices |
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144 | LOGICAL :: ll_fw_start ! =T : forward integration |
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145 | LOGICAL :: ll_init ! =T : special startup of 2d equations |
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146 | LOGICAL :: ll_tmp1, ll_tmp2 ! local logical variables used in W/D |
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147 | INTEGER :: ikbu, iktu, noffset ! local integers |
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148 | INTEGER :: ikbv, iktv ! - - |
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149 | REAL(wp) :: z1_2dt_b, z2dt_bf ! local scalars |
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150 | REAL(wp) :: zx1, zx2, zu_spg, zhura ! - - |
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151 | REAL(wp) :: zy1, zy2, zv_spg, zhvra ! - - |
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152 | REAL(wp) :: za0, za1, za2, za3 ! - - |
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153 | REAL(wp) :: zmdi, zztmp ! - - |
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154 | REAL(wp), DIMENSION(jpi,jpj) :: zsshp2_e, zhf |
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155 | REAL(wp), DIMENSION(jpi,jpj) :: zwx, zu_trd, zu_frc, zssh_frc |
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156 | REAL(wp), DIMENSION(jpi,jpj) :: zwy, zv_trd, zv_frc, zhdiv |
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157 | REAL(wp), DIMENSION(jpi,jpj) :: zsshu_a, zhup2_e, zhust_e |
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158 | REAL(wp), DIMENSION(jpi,jpj) :: zsshv_a, zhvp2_e, zhvst_e |
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159 | REAL(wp), DIMENSION(jpi,jpj) :: zCdU_u, zCdU_v ! top/bottom stress at u- & v-points |
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160 | ! |
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161 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: zcpx, zcpy ! Wetting/Dying gravity filter coef. |
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162 | !!---------------------------------------------------------------------- |
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163 | ! |
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164 | IF( nn_timing == 1 ) CALL timing_start('dyn_spg_ts') |
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165 | ! |
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166 | IF( ln_wd ) ALLOCATE( zcpx(jpi,jpj), zcpy(jpi,jpj) ) |
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167 | ! |
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168 | zmdi=1.e+20 ! missing data indicator for masking |
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169 | ! |
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170 | ! ! reciprocal of baroclinic time step |
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171 | IF( kt == nit000 .AND. neuler == 0 ) THEN ; z2dt_bf = rdt |
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172 | ELSE ; z2dt_bf = 2.0_wp * rdt |
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173 | ENDIF |
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174 | z1_2dt_b = 1.0_wp / z2dt_bf |
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175 | ! |
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176 | ll_init = ln_bt_av ! if no time averaging, then no specific restart |
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177 | ll_fw_start = .FALSE. |
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178 | ! ! time offset in steps for bdy data update |
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179 | IF( .NOT.ln_bt_fw ) THEN ; noffset = - nn_baro |
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180 | ELSE ; noffset = 0 |
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181 | ENDIF |
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182 | ! |
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183 | IF( kt == nit000 ) THEN !* initialisation |
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184 | ! |
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185 | IF(lwp) WRITE(numout,*) |
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186 | IF(lwp) WRITE(numout,*) 'dyn_spg_ts : surface pressure gradient trend' |
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187 | IF(lwp) WRITE(numout,*) '~~~~~~~~~~ free surface with time splitting' |
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188 | IF(lwp) WRITE(numout,*) |
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189 | ! |
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190 | IF( neuler == 0 ) ll_init=.TRUE. |
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191 | ! |
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192 | IF( ln_bt_fw .OR. neuler == 0 ) THEN |
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193 | ll_fw_start =.TRUE. |
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194 | noffset = 0 |
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195 | ELSE |
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196 | ll_fw_start =.FALSE. |
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197 | ENDIF |
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198 | ! |
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199 | ! Set averaging weights and cycle length: |
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200 | CALL ts_wgt( ln_bt_av, ll_fw_start, icycle, wgtbtp1, wgtbtp2 ) |
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201 | ! |
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202 | ENDIF |
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203 | ! |
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204 | IF( ln_isfcav ) THEN ! top+bottom friction (ocean cavities) |
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205 | DO jj = 2, jpjm1 |
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206 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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207 | zCdU_u(ji,jj) = 0.5*( rCdU_bot(ji+1,jj)+rCdU_bot(ji,jj) + rCdU_top(ji+1,jj)+rCdU_top(ji,jj) ) |
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208 | zCdU_v(ji,jj) = 0.5*( rCdU_bot(ji,jj+1)+rCdU_bot(ji,jj) + rCdU_top(ji+1,jj)+rCdU_top(ji,jj) ) |
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209 | END DO |
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210 | END DO |
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211 | ELSE ! bottom friction only |
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212 | DO jj = 2, jpjm1 |
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213 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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214 | zCdU_u(ji,jj) = 0.5*( rCdU_bot(ji+1,jj)+rCdU_bot(ji,jj) ) |
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215 | zCdU_v(ji,jj) = 0.5*( rCdU_bot(ji,jj+1)+rCdU_bot(ji,jj) ) |
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216 | END DO |
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217 | END DO |
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218 | ENDIF |
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219 | ! |
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220 | ! Set arrays to remove/compute coriolis trend. |
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221 | ! Do it once at kt=nit000 if volume is fixed, else at each long time step. |
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222 | ! Note that these arrays are also used during barotropic loop. These are however frozen |
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223 | ! although they should be updated in the variable volume case. Not a big approximation. |
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224 | ! To remove this approximation, copy lines below inside barotropic loop |
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225 | ! and update depths at T-F points (ht and zhf resp.) at each barotropic time step |
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226 | ! |
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227 | IF( kt == nit000 .OR. .NOT.ln_linssh ) THEN |
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228 | IF( ln_dynvor_een ) THEN !== EEN scheme ==! |
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229 | SELECT CASE( nn_een_e3f ) !* ff_f/e3 at F-point |
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230 | CASE ( 0 ) ! original formulation (masked averaging of e3t divided by 4) |
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231 | DO jj = 1, jpjm1 |
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232 | DO ji = 1, jpim1 |
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233 | zwz(ji,jj) = ( ht_n(ji ,jj+1) + ht_n(ji+1,jj+1) + & |
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234 | & ht_n(ji ,jj ) + ht_n(ji+1,jj ) ) * 0.25_wp |
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235 | IF( zwz(ji,jj) /= 0._wp ) zwz(ji,jj) = ff_f(ji,jj) / zwz(ji,jj) |
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236 | END DO |
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237 | END DO |
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238 | CASE ( 1 ) ! new formulation (masked averaging of e3t divided by the sum of mask) |
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239 | DO jj = 1, jpjm1 |
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240 | DO ji = 1, jpim1 |
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241 | zwz(ji,jj) = ( ht_n(ji ,jj+1) + ht_n(ji+1,jj+1) + & |
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242 | & ht_n(ji ,jj ) + ht_n(ji+1,jj ) ) & |
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243 | & / ( MAX( 1._wp, tmask(ji ,jj+1, 1) + tmask(ji+1,jj+1, 1) + & |
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244 | & tmask(ji ,jj , 1) + tmask(ji+1,jj , 1) ) ) |
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245 | IF( zwz(ji,jj) /= 0._wp ) zwz(ji,jj) = ff_f(ji,jj) / zwz(ji,jj) |
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246 | END DO |
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247 | END DO |
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248 | END SELECT |
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249 | CALL lbc_lnk( zwz, 'F', 1._wp ) |
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250 | ! |
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251 | ftne(1,:) = 0._wp ; ftnw(1,:) = 0._wp ; ftse(1,:) = 0._wp ; ftsw(1,:) = 0._wp |
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252 | DO jj = 2, jpj |
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253 | DO ji = 2, jpi |
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254 | ftne(ji,jj) = zwz(ji-1,jj ) + zwz(ji ,jj ) + zwz(ji ,jj-1) |
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255 | ftnw(ji,jj) = zwz(ji-1,jj-1) + zwz(ji-1,jj ) + zwz(ji ,jj ) |
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256 | ftse(ji,jj) = zwz(ji ,jj ) + zwz(ji ,jj-1) + zwz(ji-1,jj-1) |
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257 | ftsw(ji,jj) = zwz(ji ,jj-1) + zwz(ji-1,jj-1) + zwz(ji-1,jj ) |
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258 | END DO |
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259 | END DO |
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260 | ! |
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261 | ELSE !== all other schemes (ENE, ENS, MIX) |
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262 | zwz(:,:) = 0._wp |
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263 | zhf(:,:) = 0._wp |
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264 | |
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265 | !!gm assume 0 in both cases (xhich is almost surely WRONG ! ) as hvatf has been removed |
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266 | !!gm A priori a better value should be something like : |
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267 | !!gm zhf(i,j) = masked sum of ht(i,j) , ht(i+1,j) , ht(i,j+1) , (i+1,j+1) |
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268 | !!gm divided by the sum of the corresponding mask |
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269 | !!gm |
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270 | !! |
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271 | IF( .NOT.ln_sco ) THEN |
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272 | |
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273 | !!gm agree the JC comment : this should be done in a much clear way |
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274 | |
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275 | ! JC: It not clear yet what should be the depth at f-points over land in z-coordinate case |
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276 | ! Set it to zero for the time being |
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277 | ! IF( rn_hmin < 0._wp ) THEN ; jk = - INT( rn_hmin ) ! from a nb of level |
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278 | ! ELSE ; jk = MINLOC( gdepw_0, mask = gdepw_0 > rn_hmin, dim = 1 ) ! from a depth |
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279 | ! ENDIF |
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280 | ! zhf(:,:) = gdepw_0(:,:,jk+1) |
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281 | ELSE |
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282 | !zhf(:,:) = hbatf(:,:) |
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283 | DO jj = 1, jpjm1 |
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284 | DO ji = 1, jpim1 |
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285 | zhf(ji,jj) = MAX( 0._wp, & |
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286 | & ( ht_0(ji ,jj )*tmask(ji ,jj ,1) + & |
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287 | & ht_0(ji+1,jj )*tmask(ji+1,jj ,1) + & |
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288 | & ht_0(ji ,jj+1)*tmask(ji ,jj+1,1) + & |
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289 | & ht_0(ji+1,jj+1)*tmask(ji+1,jj+1,1) ) / & |
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290 | & ( tmask(ji ,jj ,1) + tmask(ji+1,jj ,1) +& |
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291 | & tmask(ji ,jj+1,1) + tmask(ji+1,jj+1,1) +& |
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292 | & rsmall ) ) |
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293 | END DO |
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294 | END DO |
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295 | END IF |
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296 | |
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297 | DO jj = 1, jpjm1 |
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298 | zhf(:,jj) = zhf(:,jj) * (1._wp- umask(:,jj,1) * umask(:,jj+1,1)) |
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299 | END DO |
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300 | !!gm end |
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301 | |
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302 | DO jk = 1, jpkm1 |
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303 | DO jj = 1, jpjm1 |
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304 | zhf(:,jj) = zhf(:,jj) + e3f_n(:,jj,jk) * umask(:,jj,jk) * umask(:,jj+1,jk) |
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305 | END DO |
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306 | END DO |
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307 | CALL lbc_lnk( zhf, 'F', 1._wp ) |
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308 | ! JC: TBC. hf should be greater than 0 |
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309 | DO jj = 1, jpj |
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310 | DO ji = 1, jpi |
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311 | IF( zhf(ji,jj) /= 0._wp ) zwz(ji,jj) = 1._wp / zhf(ji,jj) ! zhf is actually hf here but it saves an array |
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312 | END DO |
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313 | END DO |
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314 | zwz(:,:) = ff_f(:,:) * zwz(:,:) |
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315 | ENDIF |
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316 | ENDIF |
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317 | ! |
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318 | ! If forward start at previous time step, and centered integration, |
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319 | ! then update averaging weights: |
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320 | IF (.NOT.ln_bt_fw .AND.( neuler==0 .AND. kt==nit000+1 ) ) THEN |
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321 | ll_fw_start=.FALSE. |
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322 | CALL ts_wgt( ln_bt_av, ll_fw_start, icycle, wgtbtp1, wgtbtp2 ) |
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323 | ENDIF |
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324 | |
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325 | ! ----------------------------------------------------------------------------- |
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326 | ! Phase 1 : Coupling between general trend and barotropic estimates (1st step) |
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327 | ! ----------------------------------------------------------------------------- |
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328 | ! |
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329 | ! |
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330 | ! !* e3*d/dt(Ua) (Vertically integrated) |
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331 | ! ! -------------------------------------------------- |
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332 | zu_frc(:,:) = 0._wp |
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333 | zv_frc(:,:) = 0._wp |
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334 | ! |
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335 | DO jk = 1, jpkm1 |
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336 | zu_frc(:,:) = zu_frc(:,:) + e3u_n(:,:,jk) * ua(:,:,jk) * umask(:,:,jk) |
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337 | zv_frc(:,:) = zv_frc(:,:) + e3v_n(:,:,jk) * va(:,:,jk) * vmask(:,:,jk) |
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338 | END DO |
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339 | ! |
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340 | zu_frc(:,:) = zu_frc(:,:) * r1_hu_n(:,:) |
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341 | zv_frc(:,:) = zv_frc(:,:) * r1_hv_n(:,:) |
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342 | ! |
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343 | ! |
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344 | ! !* baroclinic momentum trend (remove the vertical mean trend) |
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345 | DO jk = 1, jpkm1 ! ----------------------------------------------------------- |
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346 | DO jj = 2, jpjm1 |
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347 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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348 | ua(ji,jj,jk) = ua(ji,jj,jk) - zu_frc(ji,jj) * umask(ji,jj,jk) |
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349 | va(ji,jj,jk) = va(ji,jj,jk) - zv_frc(ji,jj) * vmask(ji,jj,jk) |
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350 | END DO |
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351 | END DO |
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352 | END DO |
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353 | |
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354 | !!gm Question here when removing the Vertically integrated trends, we remove the vertically integrated NL trends on momentum.... |
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355 | !!gm Is it correct to do so ? I think so... |
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356 | |
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357 | |
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358 | ! !* barotropic Coriolis trends (vorticity scheme dependent) |
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359 | ! ! -------------------------------------------------------- |
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360 | zwx(:,:) = un_b(:,:) * hu_n(:,:) * e2u(:,:) ! now fluxes |
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361 | zwy(:,:) = vn_b(:,:) * hv_n(:,:) * e1v(:,:) |
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362 | ! |
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363 | IF( ln_dynvor_ene .OR. ln_dynvor_mix ) THEN ! energy conserving or mixed scheme |
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364 | DO jj = 2, jpjm1 |
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365 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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366 | zy1 = ( zwy(ji,jj-1) + zwy(ji+1,jj-1) ) * r1_e1u(ji,jj) |
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367 | zy2 = ( zwy(ji,jj ) + zwy(ji+1,jj ) ) * r1_e1u(ji,jj) |
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368 | zx1 = ( zwx(ji-1,jj) + zwx(ji-1,jj+1) ) * r1_e2v(ji,jj) |
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369 | zx2 = ( zwx(ji ,jj) + zwx(ji ,jj+1) ) * r1_e2v(ji,jj) |
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370 | ! energy conserving formulation for planetary vorticity term |
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371 | zu_trd(ji,jj) = r1_4 * ( zwz(ji ,jj-1) * zy1 + zwz(ji,jj) * zy2 ) |
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372 | zv_trd(ji,jj) = - r1_4 * ( zwz(ji-1,jj ) * zx1 + zwz(ji,jj) * zx2 ) |
---|
373 | END DO |
---|
374 | END DO |
---|
375 | ! |
---|
376 | ELSEIF ( ln_dynvor_ens ) THEN ! enstrophy conserving scheme |
---|
377 | DO jj = 2, jpjm1 |
---|
378 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
379 | zy1 = r1_8 * ( zwy(ji ,jj-1) + zwy(ji+1,jj-1) & |
---|
380 | & + zwy(ji ,jj ) + zwy(ji+1,jj ) ) * r1_e1u(ji,jj) |
---|
381 | zx1 = - r1_8 * ( zwx(ji-1,jj ) + zwx(ji-1,jj+1) & |
---|
382 | & + zwx(ji ,jj ) + zwx(ji ,jj+1) ) * r1_e2v(ji,jj) |
---|
383 | zu_trd(ji,jj) = zy1 * ( zwz(ji ,jj-1) + zwz(ji,jj) ) |
---|
384 | zv_trd(ji,jj) = zx1 * ( zwz(ji-1,jj ) + zwz(ji,jj) ) |
---|
385 | END DO |
---|
386 | END DO |
---|
387 | ! |
---|
388 | ELSEIF ( ln_dynvor_een ) THEN ! enstrophy and energy conserving scheme |
---|
389 | DO jj = 2, jpjm1 |
---|
390 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
391 | zu_trd(ji,jj) = + r1_12 * r1_e1u(ji,jj) * ( ftne(ji,jj ) * zwy(ji ,jj ) & |
---|
392 | & + ftnw(ji+1,jj) * zwy(ji+1,jj ) & |
---|
393 | & + ftse(ji,jj ) * zwy(ji ,jj-1) & |
---|
394 | & + ftsw(ji+1,jj) * zwy(ji+1,jj-1) ) |
---|
395 | zv_trd(ji,jj) = - r1_12 * r1_e2v(ji,jj) * ( ftsw(ji,jj+1) * zwx(ji-1,jj+1) & |
---|
396 | & + ftse(ji,jj+1) * zwx(ji ,jj+1) & |
---|
397 | & + ftnw(ji,jj ) * zwx(ji-1,jj ) & |
---|
398 | & + ftne(ji,jj ) * zwx(ji ,jj ) ) |
---|
399 | END DO |
---|
400 | END DO |
---|
401 | ! |
---|
402 | ENDIF |
---|
403 | ! |
---|
404 | ! !* Right-Hand-Side of the barotropic momentum equation |
---|
405 | ! ! ---------------------------------------------------- |
---|
406 | IF( .NOT.ln_linssh ) THEN ! Variable volume : remove surface pressure gradient |
---|
407 | IF( ln_wd ) THEN ! Calculating and applying W/D gravity filters |
---|
408 | DO jj = 2, jpjm1 |
---|
409 | DO ji = 2, jpim1 |
---|
410 | ll_tmp1 = MIN( sshn(ji,jj) , sshn(ji+1,jj) ) > & |
---|
411 | & MAX( -ht_wd(ji,jj) , -ht_wd(ji+1,jj) ) .AND. & |
---|
412 | & MAX( sshn(ji,jj) + ht_wd(ji,jj), sshn(ji+1,jj) + ht_wd(ji+1,jj) ) & |
---|
413 | & > rn_wdmin1 + rn_wdmin2 |
---|
414 | ll_tmp2 = ( ABS( sshn(ji+1,jj) - sshn(ji ,jj)) > 1.E-12 ).AND.( & |
---|
415 | & MAX( sshn(ji,jj) , sshn(ji+1,jj) ) > & |
---|
416 | & MAX( -ht_wd(ji,jj) , -ht_wd(ji+1,jj) ) + rn_wdmin1 + rn_wdmin2 ) |
---|
417 | ! |
---|
418 | IF(ll_tmp1) THEN |
---|
419 | zcpx(ji,jj) = 1.0_wp |
---|
420 | ELSE IF(ll_tmp2) THEN ! no worries about sshn(ji+1,jj) - sshn(ji ,jj) = 0, it won't happen ! here |
---|
421 | zcpx(ji,jj) = ABS( (sshn(ji+1,jj) + ht_wd(ji+1,jj) - sshn(ji,jj) - ht_wd(ji,jj)) & |
---|
422 | & / (sshn(ji+1,jj) - sshn(ji ,jj)) ) |
---|
423 | ELSE |
---|
424 | zcpx(ji,jj) = 0._wp |
---|
425 | ENDIF |
---|
426 | ! |
---|
427 | ll_tmp1 = MIN( sshn(ji,jj) , sshn(ji,jj+1) ) > & |
---|
428 | & MAX( -ht_wd(ji,jj) , -ht_wd(ji,jj+1) ) .AND. & |
---|
429 | & MAX( sshn(ji,jj) + ht_wd(ji,jj), sshn(ji,jj+1) + ht_wd(ji,jj+1) ) & |
---|
430 | & > rn_wdmin1 + rn_wdmin2 |
---|
431 | ll_tmp2 = ( ABS( sshn(ji,jj) - sshn(ji,jj+1)) > 1.E-12 ).AND.( & |
---|
432 | & MAX( sshn(ji,jj) , sshn(ji,jj+1) ) > & |
---|
433 | & MAX( -ht_wd(ji,jj) , -ht_wd(ji,jj+1) ) + rn_wdmin1 + rn_wdmin2 ) |
---|
434 | ! |
---|
435 | IF(ll_tmp1) THEN |
---|
436 | zcpy(ji,jj) = 1.0_wp |
---|
437 | ELSE IF(ll_tmp2) THEN |
---|
438 | ! no worries about sshn(ji,jj+1) - sshn(ji,jj ) = 0, it won't happen ! here |
---|
439 | zcpy(ji,jj) = ABS( (sshn(ji,jj+1) + ht_wd(ji,jj+1) - sshn(ji,jj) - ht_wd(ji,jj)) & |
---|
440 | & / (sshn(ji,jj+1) - sshn(ji,jj )) ) |
---|
441 | ELSE |
---|
442 | zcpy(ji,jj) = 0._wp |
---|
443 | ENDIF |
---|
444 | END DO |
---|
445 | END DO |
---|
446 | ! |
---|
447 | DO jj = 2, jpjm1 |
---|
448 | DO ji = 2, jpim1 |
---|
449 | zu_trd(ji,jj) = zu_trd(ji,jj) - grav * ( sshn(ji+1,jj ) - sshn(ji ,jj ) ) & |
---|
450 | & * r1_e1u(ji,jj) * zcpx(ji,jj) |
---|
451 | zv_trd(ji,jj) = zv_trd(ji,jj) - grav * ( sshn(ji ,jj+1) - sshn(ji ,jj ) ) & |
---|
452 | & * r1_e2v(ji,jj) * zcpy(ji,jj) |
---|
453 | END DO |
---|
454 | END DO |
---|
455 | ! |
---|
456 | ELSE |
---|
457 | ! |
---|
458 | DO jj = 2, jpjm1 |
---|
459 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
460 | zu_trd(ji,jj) = zu_trd(ji,jj) - grav * ( sshn(ji+1,jj ) - sshn(ji ,jj ) ) * r1_e1u(ji,jj) |
---|
461 | zv_trd(ji,jj) = zv_trd(ji,jj) - grav * ( sshn(ji ,jj+1) - sshn(ji ,jj ) ) * r1_e2v(ji,jj) |
---|
462 | END DO |
---|
463 | END DO |
---|
464 | ENDIF |
---|
465 | ! |
---|
466 | ENDIF |
---|
467 | ! |
---|
468 | DO jj = 2, jpjm1 ! Remove coriolis term (and possibly spg) from barotropic trend |
---|
469 | DO ji = fs_2, fs_jpim1 |
---|
470 | zu_frc(ji,jj) = zu_frc(ji,jj) - zu_trd(ji,jj) * ssumask(ji,jj) |
---|
471 | zv_frc(ji,jj) = zv_frc(ji,jj) - zv_trd(ji,jj) * ssvmask(ji,jj) |
---|
472 | END DO |
---|
473 | END DO |
---|
474 | ! |
---|
475 | ! ! Add BOTTOM stress contribution from baroclinic velocities: |
---|
476 | IF( ln_bt_fw ) THEN |
---|
477 | DO jj = 2, jpjm1 |
---|
478 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
479 | ikbu = mbku(ji,jj) |
---|
480 | ikbv = mbkv(ji,jj) |
---|
481 | zwx(ji,jj) = un(ji,jj,ikbu) - un_b(ji,jj) ! NOW bottom baroclinic velocities |
---|
482 | zwy(ji,jj) = vn(ji,jj,ikbv) - vn_b(ji,jj) |
---|
483 | END DO |
---|
484 | END DO |
---|
485 | ELSE |
---|
486 | DO jj = 2, jpjm1 |
---|
487 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
488 | ikbu = mbku(ji,jj) |
---|
489 | ikbv = mbkv(ji,jj) |
---|
490 | zwx(ji,jj) = ub(ji,jj,ikbu) - ub_b(ji,jj) ! BEFORE bottom baroclinic velocities |
---|
491 | zwy(ji,jj) = vb(ji,jj,ikbv) - vb_b(ji,jj) |
---|
492 | END DO |
---|
493 | END DO |
---|
494 | ENDIF |
---|
495 | ! |
---|
496 | ! Note that the "unclipped" bottom friction parameter is used even with explicit drag |
---|
497 | IF( ln_wd ) THEN |
---|
498 | zztmp = - 1._wp / rdtbt |
---|
499 | DO jj = 2, jpjm1 |
---|
500 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
501 | zu_frc(ji,jj) = zu_frc(ji,jj) + MAX( r1_hu_n(ji,jj) * 0.5*( rCdU_bot(ji+1,jj)+rCdU_bot(ji,jj) ) , zztmp ) * zwx(ji,jj) |
---|
502 | zv_frc(ji,jj) = zv_frc(ji,jj) + MAX( r1_hv_n(ji,jj) * 0.5*( rCdU_bot(ji,jj+1)+rCdU_bot(ji,jj) ) , zztmp ) * zwy(ji,jj) |
---|
503 | END DO |
---|
504 | END DO |
---|
505 | ELSE |
---|
506 | DO jj = 2, jpjm1 |
---|
507 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
508 | zu_frc(ji,jj) = zu_frc(ji,jj) + r1_hu_n(ji,jj) * 0.5*( rCdU_bot(ji+1,jj)+rCdU_bot(ji,jj) ) * zwx(ji,jj) |
---|
509 | zv_frc(ji,jj) = zv_frc(ji,jj) + r1_hv_n(ji,jj) * 0.5*( rCdU_bot(ji,jj+1)+rCdU_bot(ji,jj) ) * zwy(ji,jj) |
---|
510 | END DO |
---|
511 | END DO |
---|
512 | END IF |
---|
513 | ! |
---|
514 | IF( ln_isfcav ) THEN ! Add TOP stress contribution from baroclinic velocities: |
---|
515 | IF( ln_bt_fw ) THEN |
---|
516 | DO jj = 2, jpjm1 |
---|
517 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
518 | iktu = miku(ji,jj) |
---|
519 | iktv = mikv(ji,jj) |
---|
520 | zwx(ji,jj) = un(ji,jj,iktu) - un_b(ji,jj) ! NOW top baroclinic velocities |
---|
521 | zwy(ji,jj) = vn(ji,jj,iktv) - vn_b(ji,jj) |
---|
522 | END DO |
---|
523 | END DO |
---|
524 | ELSE |
---|
525 | DO jj = 2, jpjm1 |
---|
526 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
527 | iktu = miku(ji,jj) |
---|
528 | iktv = mikv(ji,jj) |
---|
529 | zwx(ji,jj) = ub(ji,jj,iktu) - ub_b(ji,jj) ! BEFORE top baroclinic velocities |
---|
530 | zwy(ji,jj) = vb(ji,jj,iktv) - vb_b(ji,jj) |
---|
531 | END DO |
---|
532 | END DO |
---|
533 | ENDIF |
---|
534 | ! |
---|
535 | ! Note that the "unclipped" top friction parameter is used even with explicit drag |
---|
536 | DO jj = 2, jpjm1 |
---|
537 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
538 | zu_frc(ji,jj) = zu_frc(ji,jj) + r1_hu_n(ji,jj) * 0.5*( rCdU_top(ji+1,jj)+rCdU_top(ji,jj) ) * zwx(ji,jj) |
---|
539 | zv_frc(ji,jj) = zv_frc(ji,jj) + r1_hv_n(ji,jj) * 0.5*( rCdU_top(ji,jj+1)+rCdU_top(ji,jj) ) * zwy(ji,jj) |
---|
540 | END DO |
---|
541 | END DO |
---|
542 | ENDIF |
---|
543 | ! |
---|
544 | IF( ln_bt_fw ) THEN ! Add wind forcing |
---|
545 | DO jj = 2, jpjm1 |
---|
546 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
547 | zu_frc(ji,jj) = zu_frc(ji,jj) + r1_rau0 * utau(ji,jj) * r1_hu_n(ji,jj) |
---|
548 | zv_frc(ji,jj) = zv_frc(ji,jj) + r1_rau0 * vtau(ji,jj) * r1_hv_n(ji,jj) |
---|
549 | END DO |
---|
550 | END DO |
---|
551 | ELSE |
---|
552 | zztmp = r1_rau0 * r1_2 |
---|
553 | DO jj = 2, jpjm1 |
---|
554 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
555 | zu_frc(ji,jj) = zu_frc(ji,jj) + zztmp * ( utau_b(ji,jj) + utau(ji,jj) ) * r1_hu_n(ji,jj) |
---|
556 | zv_frc(ji,jj) = zv_frc(ji,jj) + zztmp * ( vtau_b(ji,jj) + vtau(ji,jj) ) * r1_hv_n(ji,jj) |
---|
557 | END DO |
---|
558 | END DO |
---|
559 | ENDIF |
---|
560 | ! |
---|
561 | IF( ln_apr_dyn ) THEN ! Add atm pressure forcing |
---|
562 | IF( ln_bt_fw ) THEN |
---|
563 | DO jj = 2, jpjm1 |
---|
564 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
565 | zu_spg = grav * ( ssh_ib (ji+1,jj ) - ssh_ib (ji,jj) ) * r1_e1u(ji,jj) |
---|
566 | zv_spg = grav * ( ssh_ib (ji ,jj+1) - ssh_ib (ji,jj) ) * r1_e2v(ji,jj) |
---|
567 | zu_frc(ji,jj) = zu_frc(ji,jj) + zu_spg |
---|
568 | zv_frc(ji,jj) = zv_frc(ji,jj) + zv_spg |
---|
569 | END DO |
---|
570 | END DO |
---|
571 | ELSE |
---|
572 | zztmp = grav * r1_2 |
---|
573 | DO jj = 2, jpjm1 |
---|
574 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
575 | zu_spg = zztmp * ( ssh_ib (ji+1,jj ) - ssh_ib (ji,jj) & |
---|
576 | & + ssh_ibb(ji+1,jj ) - ssh_ibb(ji,jj) ) * r1_e1u(ji,jj) |
---|
577 | zv_spg = zztmp * ( ssh_ib (ji ,jj+1) - ssh_ib (ji,jj) & |
---|
578 | & + ssh_ibb(ji ,jj+1) - ssh_ibb(ji,jj) ) * r1_e2v(ji,jj) |
---|
579 | zu_frc(ji,jj) = zu_frc(ji,jj) + zu_spg |
---|
580 | zv_frc(ji,jj) = zv_frc(ji,jj) + zv_spg |
---|
581 | END DO |
---|
582 | END DO |
---|
583 | ENDIF |
---|
584 | ENDIF |
---|
585 | ! !* Right-Hand-Side of the barotropic ssh equation |
---|
586 | ! ! ----------------------------------------------- |
---|
587 | ! ! Surface net water flux and rivers |
---|
588 | IF (ln_bt_fw) THEN |
---|
589 | zssh_frc(:,:) = r1_rau0 * ( emp(:,:) - rnf(:,:) + fwfisf(:,:) ) |
---|
590 | ELSE |
---|
591 | zztmp = r1_rau0 * r1_2 |
---|
592 | zssh_frc(:,:) = zztmp * ( emp(:,:) + emp_b(:,:) - rnf(:,:) - rnf_b(:,:) & |
---|
593 | & + fwfisf(:,:) + fwfisf_b(:,:) ) |
---|
594 | ENDIF |
---|
595 | ! |
---|
596 | IF( ln_sdw ) THEN ! Stokes drift divergence added if necessary |
---|
597 | zssh_frc(:,:) = zssh_frc(:,:) + div_sd(:,:) |
---|
598 | ENDIF |
---|
599 | ! |
---|
600 | #if defined key_asminc |
---|
601 | ! ! Include the IAU weighted SSH increment |
---|
602 | IF( lk_asminc .AND. ln_sshinc .AND. ln_asmiau ) THEN |
---|
603 | zssh_frc(:,:) = zssh_frc(:,:) - ssh_iau(:,:) |
---|
604 | ENDIF |
---|
605 | #endif |
---|
606 | ! !* Fill boundary data arrays for AGRIF |
---|
607 | ! ! ------------------------------------ |
---|
608 | #if defined key_agrif |
---|
609 | IF( .NOT.Agrif_Root() ) CALL agrif_dta_ts( kt ) |
---|
610 | #endif |
---|
611 | ! |
---|
612 | ! ----------------------------------------------------------------------- |
---|
613 | ! Phase 2 : Integration of the barotropic equations |
---|
614 | ! ----------------------------------------------------------------------- |
---|
615 | ! |
---|
616 | ! ! ==================== ! |
---|
617 | ! ! Initialisations ! |
---|
618 | ! ! ==================== ! |
---|
619 | ! Initialize barotropic variables: |
---|
620 | IF( ll_init )THEN |
---|
621 | sshbb_e(:,:) = 0._wp |
---|
622 | ubb_e (:,:) = 0._wp |
---|
623 | vbb_e (:,:) = 0._wp |
---|
624 | sshb_e (:,:) = 0._wp |
---|
625 | ub_e (:,:) = 0._wp |
---|
626 | vb_e (:,:) = 0._wp |
---|
627 | ENDIF |
---|
628 | |
---|
629 | ! |
---|
630 | IF (ln_bt_fw) THEN ! FORWARD integration: start from NOW fields |
---|
631 | sshn_e(:,:) = sshn(:,:) |
---|
632 | un_e (:,:) = un_b(:,:) |
---|
633 | vn_e (:,:) = vn_b(:,:) |
---|
634 | ! |
---|
635 | hu_e (:,:) = hu_n(:,:) |
---|
636 | hv_e (:,:) = hv_n(:,:) |
---|
637 | hur_e (:,:) = r1_hu_n(:,:) |
---|
638 | hvr_e (:,:) = r1_hv_n(:,:) |
---|
639 | ELSE ! CENTRED integration: start from BEFORE fields |
---|
640 | sshn_e(:,:) = sshb(:,:) |
---|
641 | un_e (:,:) = ub_b(:,:) |
---|
642 | vn_e (:,:) = vb_b(:,:) |
---|
643 | ! |
---|
644 | hu_e (:,:) = hu_b(:,:) |
---|
645 | hv_e (:,:) = hv_b(:,:) |
---|
646 | hur_e (:,:) = r1_hu_b(:,:) |
---|
647 | hvr_e (:,:) = r1_hv_b(:,:) |
---|
648 | ENDIF |
---|
649 | ! |
---|
650 | ! |
---|
651 | ! |
---|
652 | ! Initialize sums: |
---|
653 | ua_b (:,:) = 0._wp ! After barotropic velocities (or transport if flux form) |
---|
654 | va_b (:,:) = 0._wp |
---|
655 | ssha (:,:) = 0._wp ! Sum for after averaged sea level |
---|
656 | un_adv(:,:) = 0._wp ! Sum for now transport issued from ts loop |
---|
657 | vn_adv(:,:) = 0._wp |
---|
658 | ! ! ==================== ! |
---|
659 | DO jn = 1, icycle ! sub-time-step loop ! |
---|
660 | ! ! ==================== ! |
---|
661 | ! !* Update the forcing (BDY and tides) |
---|
662 | ! ! ------------------ |
---|
663 | ! Update only tidal forcing at open boundaries |
---|
664 | IF( ln_bdy .AND. ln_tide ) CALL bdy_dta_tides( kt, kit=jn, time_offset= noffset+1 ) |
---|
665 | IF( ln_tide_pot .AND. ln_tide ) CALL upd_tide ( kt, kit=jn, time_offset= noffset ) |
---|
666 | ! |
---|
667 | ! Set extrapolation coefficients for predictor step: |
---|
668 | IF ((jn<3).AND.ll_init) THEN ! Forward |
---|
669 | za1 = 1._wp |
---|
670 | za2 = 0._wp |
---|
671 | za3 = 0._wp |
---|
672 | ELSE ! AB3-AM4 Coefficients: bet=0.281105 |
---|
673 | za1 = 1.781105_wp ! za1 = 3/2 + bet |
---|
674 | za2 = -1.06221_wp ! za2 = -(1/2 + 2*bet) |
---|
675 | za3 = 0.281105_wp ! za3 = bet |
---|
676 | ENDIF |
---|
677 | |
---|
678 | ! Extrapolate barotropic velocities at step jit+0.5: |
---|
679 | ua_e(:,:) = za1 * un_e(:,:) + za2 * ub_e(:,:) + za3 * ubb_e(:,:) |
---|
680 | va_e(:,:) = za1 * vn_e(:,:) + za2 * vb_e(:,:) + za3 * vbb_e(:,:) |
---|
681 | |
---|
682 | IF( .NOT.ln_linssh ) THEN !* Update ocean depth (variable volume case only) |
---|
683 | ! ! ------------------ |
---|
684 | ! Extrapolate Sea Level at step jit+0.5: |
---|
685 | zsshp2_e(:,:) = za1 * sshn_e(:,:) + za2 * sshb_e(:,:) + za3 * sshbb_e(:,:) |
---|
686 | ! |
---|
687 | DO jj = 2, jpjm1 ! Sea Surface Height at u- & v-points |
---|
688 | DO ji = 2, fs_jpim1 ! Vector opt. |
---|
689 | zwx(ji,jj) = r1_2 * ssumask(ji,jj) * r1_e1e2u(ji,jj) & |
---|
690 | & * ( e1e2t(ji ,jj) * zsshp2_e(ji ,jj) & |
---|
691 | & + e1e2t(ji+1,jj) * zsshp2_e(ji+1,jj) ) |
---|
692 | zwy(ji,jj) = r1_2 * ssvmask(ji,jj) * r1_e1e2v(ji,jj) & |
---|
693 | & * ( e1e2t(ji,jj ) * zsshp2_e(ji,jj ) & |
---|
694 | & + e1e2t(ji,jj+1) * zsshp2_e(ji,jj+1) ) |
---|
695 | END DO |
---|
696 | END DO |
---|
697 | CALL lbc_lnk_multi( zwx, 'U', 1._wp, zwy, 'V', 1._wp ) |
---|
698 | ! |
---|
699 | zhup2_e (:,:) = hu_0(:,:) + zwx(:,:) ! Ocean depth at U- and V-points |
---|
700 | zhvp2_e (:,:) = hv_0(:,:) + zwy(:,:) |
---|
701 | ELSE |
---|
702 | zhup2_e (:,:) = hu_n(:,:) |
---|
703 | zhvp2_e (:,:) = hv_n(:,:) |
---|
704 | ENDIF |
---|
705 | ! !* after ssh |
---|
706 | ! ! ----------- |
---|
707 | ! One should enforce volume conservation at open boundaries here |
---|
708 | ! considering fluxes below: |
---|
709 | ! |
---|
710 | zwx(:,:) = e2u(:,:) * ua_e(:,:) * zhup2_e(:,:) ! fluxes at jn+0.5 |
---|
711 | zwy(:,:) = e1v(:,:) * va_e(:,:) * zhvp2_e(:,:) |
---|
712 | ! |
---|
713 | #if defined key_agrif |
---|
714 | ! Set fluxes during predictor step to ensure volume conservation |
---|
715 | IF( .NOT.Agrif_Root() .AND. ln_bt_fw ) THEN |
---|
716 | IF((nbondi == -1).OR.(nbondi == 2)) THEN |
---|
717 | DO jj=1,jpj |
---|
718 | zwx(2,jj) = ubdy_w(jj) * e2u(2,jj) |
---|
719 | END DO |
---|
720 | ENDIF |
---|
721 | IF((nbondi == 1).OR.(nbondi == 2)) THEN |
---|
722 | DO jj=1,jpj |
---|
723 | zwx(nlci-2,jj) = ubdy_e(jj) * e2u(nlci-2,jj) |
---|
724 | END DO |
---|
725 | ENDIF |
---|
726 | IF((nbondj == -1).OR.(nbondj == 2)) THEN |
---|
727 | DO ji=1,jpi |
---|
728 | zwy(ji,2) = vbdy_s(ji) * e1v(ji,2) |
---|
729 | END DO |
---|
730 | ENDIF |
---|
731 | IF((nbondj == 1).OR.(nbondj == 2)) THEN |
---|
732 | DO ji=1,jpi |
---|
733 | zwy(ji,nlcj-2) = vbdy_n(ji) * e1v(ji,nlcj-2) |
---|
734 | END DO |
---|
735 | ENDIF |
---|
736 | ENDIF |
---|
737 | #endif |
---|
738 | IF( ln_wd ) CALL wad_lmt_bt(zwx, zwy, sshn_e, zssh_frc, rdtbt) |
---|
739 | ! |
---|
740 | ! Sum over sub-time-steps to compute advective velocities |
---|
741 | za2 = wgtbtp2(jn) |
---|
742 | un_adv(:,:) = un_adv(:,:) + za2 * zwx(:,:) * r1_e2u(:,:) |
---|
743 | vn_adv(:,:) = vn_adv(:,:) + za2 * zwy(:,:) * r1_e1v(:,:) |
---|
744 | ! |
---|
745 | ! Set next sea level: |
---|
746 | DO jj = 2, jpjm1 |
---|
747 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
748 | zhdiv(ji,jj) = ( zwx(ji,jj) - zwx(ji-1,jj) & |
---|
749 | & + zwy(ji,jj) - zwy(ji,jj-1) ) * r1_e1e2t(ji,jj) |
---|
750 | END DO |
---|
751 | END DO |
---|
752 | ssha_e(:,:) = ( sshn_e(:,:) - rdtbt * ( zssh_frc(:,:) + zhdiv(:,:) ) ) * ssmask(:,:) |
---|
753 | |
---|
754 | CALL lbc_lnk( ssha_e, 'T', 1._wp ) |
---|
755 | |
---|
756 | ! Duplicate sea level across open boundaries (this is only cosmetic if linssh=T) |
---|
757 | IF( ln_bdy ) CALL bdy_ssh( ssha_e ) |
---|
758 | #if defined key_agrif |
---|
759 | IF( .NOT.Agrif_Root() ) CALL agrif_ssh_ts( jn ) |
---|
760 | #endif |
---|
761 | ! |
---|
762 | ! Sea Surface Height at u-,v-points (vvl case only) |
---|
763 | IF( .NOT.ln_linssh ) THEN |
---|
764 | DO jj = 2, jpjm1 |
---|
765 | DO ji = 2, jpim1 ! NO Vector Opt. |
---|
766 | zsshu_a(ji,jj) = r1_2 * ssumask(ji,jj) * r1_e1e2u(ji,jj) & |
---|
767 | & * ( e1e2t(ji ,jj ) * ssha_e(ji ,jj ) & |
---|
768 | & + e1e2t(ji+1,jj ) * ssha_e(ji+1,jj ) ) |
---|
769 | zsshv_a(ji,jj) = r1_2 * ssvmask(ji,jj) * r1_e1e2v(ji,jj) & |
---|
770 | & * ( e1e2t(ji ,jj ) * ssha_e(ji ,jj ) & |
---|
771 | & + e1e2t(ji ,jj+1) * ssha_e(ji ,jj+1) ) |
---|
772 | END DO |
---|
773 | END DO |
---|
774 | CALL lbc_lnk_multi( zsshu_a, 'U', 1._wp, zsshv_a, 'V', 1._wp ) |
---|
775 | ENDIF |
---|
776 | ! |
---|
777 | ! Half-step back interpolation of SSH for surface pressure computation: |
---|
778 | !---------------------------------------------------------------------- |
---|
779 | IF ((jn==1).AND.ll_init) THEN |
---|
780 | za0=1._wp ! Forward-backward |
---|
781 | za1=0._wp |
---|
782 | za2=0._wp |
---|
783 | za3=0._wp |
---|
784 | ELSEIF ((jn==2).AND.ll_init) THEN ! AB2-AM3 Coefficients; bet=0 ; gam=-1/6 ; eps=1/12 |
---|
785 | za0= 1.0833333333333_wp ! za0 = 1-gam-eps |
---|
786 | za1=-0.1666666666666_wp ! za1 = gam |
---|
787 | za2= 0.0833333333333_wp ! za2 = eps |
---|
788 | za3= 0._wp |
---|
789 | ELSE ! AB3-AM4 Coefficients; bet=0.281105 ; eps=0.013 ; gam=0.0880 |
---|
790 | za0=0.614_wp ! za0 = 1/2 + gam + 2*eps |
---|
791 | za1=0.285_wp ! za1 = 1/2 - 2*gam - 3*eps |
---|
792 | za2=0.088_wp ! za2 = gam |
---|
793 | za3=0.013_wp ! za3 = eps |
---|
794 | ENDIF |
---|
795 | ! |
---|
796 | zsshp2_e(:,:) = za0 * ssha_e(:,:) + za1 * sshn_e (:,:) & |
---|
797 | & + za2 * sshb_e(:,:) + za3 * sshbb_e(:,:) |
---|
798 | IF( ln_wd ) THEN ! Calculating and applying W/D gravity filters |
---|
799 | DO jj = 2, jpjm1 |
---|
800 | DO ji = 2, jpim1 |
---|
801 | ll_tmp1 = MIN( zsshp2_e(ji,jj) , zsshp2_e(ji+1,jj) ) > & |
---|
802 | & MAX( -ht_wd(ji,jj) , -ht_wd(ji+1,jj) ) .AND. & |
---|
803 | & MAX( zsshp2_e(ji,jj) + ht_wd(ji,jj), zsshp2_e(ji+1,jj) + ht_wd(ji+1,jj) ) & |
---|
804 | & > rn_wdmin1 + rn_wdmin2 |
---|
805 | ll_tmp2 = (ABS(zsshp2_e(ji,jj) - zsshp2_e(ji+1,jj)) > 1.E-12 ).AND.( & |
---|
806 | & MAX( zsshp2_e(ji,jj) , zsshp2_e(ji+1,jj) ) > & |
---|
807 | & MAX( -ht_wd(ji,jj) , -ht_wd(ji+1,jj) ) + rn_wdmin1 + rn_wdmin2 ) |
---|
808 | |
---|
809 | IF(ll_tmp1) THEN |
---|
810 | zcpx(ji,jj) = 1.0_wp |
---|
811 | ELSE IF(ll_tmp2) THEN |
---|
812 | ! no worries about zsshp2_e(ji+1,jj) - zsshp2_e(ji ,jj) = 0, it won't happen ! here |
---|
813 | zcpx(ji,jj) = ABS( (zsshp2_e(ji+1,jj) + ht_wd(ji+1,jj) - zsshp2_e(ji,jj) - ht_wd(ji,jj)) & |
---|
814 | & / (zsshp2_e(ji+1,jj) - zsshp2_e(ji ,jj)) ) |
---|
815 | ELSE |
---|
816 | zcpx(ji,jj) = 0._wp |
---|
817 | END IF |
---|
818 | |
---|
819 | ll_tmp1 = MIN( zsshp2_e(ji,jj) , zsshp2_e(ji,jj+1) ) > & |
---|
820 | & MAX( -ht_wd(ji,jj) , -ht_wd(ji,jj+1) ) .AND. & |
---|
821 | & MAX( zsshp2_e(ji,jj) + ht_wd(ji,jj), zsshp2_e(ji,jj+1) + ht_wd(ji,jj+1) ) & |
---|
822 | & > rn_wdmin1 + rn_wdmin2 |
---|
823 | ll_tmp2 = (ABS(zsshp2_e(ji,jj) - zsshp2_e(ji,jj+1)) > 1.E-12 ).AND.( & |
---|
824 | & MAX( zsshp2_e(ji,jj) , zsshp2_e(ji,jj+1) ) > & |
---|
825 | & MAX( -ht_wd(ji,jj) , -ht_wd(ji,jj+1) ) + rn_wdmin1 + rn_wdmin2 ) |
---|
826 | |
---|
827 | IF(ll_tmp1) THEN |
---|
828 | zcpy(ji,jj) = 1.0_wp |
---|
829 | ELSE IF(ll_tmp2) THEN |
---|
830 | ! no worries about zsshp2_e(ji,jj+1) - zsshp2_e(ji,jj ) = 0, it won't happen ! here |
---|
831 | zcpy(ji,jj) = ABS( (zsshp2_e(ji,jj+1) + ht_wd(ji,jj+1) - zsshp2_e(ji,jj) - ht_wd(ji,jj)) & |
---|
832 | & / (zsshp2_e(ji,jj+1) - zsshp2_e(ji,jj )) ) |
---|
833 | ELSE |
---|
834 | zcpy(ji,jj) = 0._wp |
---|
835 | END IF |
---|
836 | END DO |
---|
837 | END DO |
---|
838 | END IF |
---|
839 | ! |
---|
840 | ! Compute associated depths at U and V points: |
---|
841 | IF( .NOT.ln_linssh .AND. .NOT.ln_dynadv_vec ) THEN !* Vector form |
---|
842 | ! |
---|
843 | DO jj = 2, jpjm1 |
---|
844 | DO ji = 2, jpim1 |
---|
845 | zx1 = r1_2 * ssumask(ji ,jj) * r1_e1e2u(ji ,jj) & |
---|
846 | & * ( e1e2t(ji ,jj ) * zsshp2_e(ji ,jj) & |
---|
847 | & + e1e2t(ji+1,jj ) * zsshp2_e(ji+1,jj ) ) |
---|
848 | zy1 = r1_2 * ssvmask(ji ,jj) * r1_e1e2v(ji ,jj ) & |
---|
849 | & * ( e1e2t(ji ,jj ) * zsshp2_e(ji ,jj ) & |
---|
850 | & + e1e2t(ji ,jj+1) * zsshp2_e(ji ,jj+1) ) |
---|
851 | zhust_e(ji,jj) = hu_0(ji,jj) + zx1 |
---|
852 | zhvst_e(ji,jj) = hv_0(ji,jj) + zy1 |
---|
853 | END DO |
---|
854 | END DO |
---|
855 | |
---|
856 | ENDIF |
---|
857 | ! |
---|
858 | ! Add Coriolis trend: |
---|
859 | ! zwz array below or triads normally depend on sea level with ln_linssh=F and should be updated |
---|
860 | ! at each time step. We however keep them constant here for optimization. |
---|
861 | ! Recall that zwx and zwy arrays hold fluxes at this stage: |
---|
862 | ! zwx(:,:) = e2u(:,:) * ua_e(:,:) * zhup2_e(:,:) ! fluxes at jn+0.5 |
---|
863 | ! zwy(:,:) = e1v(:,:) * va_e(:,:) * zhvp2_e(:,:) |
---|
864 | ! |
---|
865 | IF( ln_dynvor_ene .OR. ln_dynvor_mix ) THEN !== energy conserving or mixed scheme ==! |
---|
866 | DO jj = 2, jpjm1 |
---|
867 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
868 | zy1 = ( zwy(ji ,jj-1) + zwy(ji+1,jj-1) ) * r1_e1u(ji,jj) |
---|
869 | zy2 = ( zwy(ji ,jj ) + zwy(ji+1,jj ) ) * r1_e1u(ji,jj) |
---|
870 | zx1 = ( zwx(ji-1,jj ) + zwx(ji-1,jj+1) ) * r1_e2v(ji,jj) |
---|
871 | zx2 = ( zwx(ji ,jj ) + zwx(ji ,jj+1) ) * r1_e2v(ji,jj) |
---|
872 | zu_trd(ji,jj) = r1_4 * ( zwz(ji ,jj-1) * zy1 + zwz(ji,jj) * zy2 ) |
---|
873 | zv_trd(ji,jj) =-r1_4 * ( zwz(ji-1,jj ) * zx1 + zwz(ji,jj) * zx2 ) |
---|
874 | END DO |
---|
875 | END DO |
---|
876 | ! |
---|
877 | ELSEIF ( ln_dynvor_ens ) THEN !== enstrophy conserving scheme ==! |
---|
878 | DO jj = 2, jpjm1 |
---|
879 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
880 | zy1 = r1_8 * ( zwy(ji ,jj-1) + zwy(ji+1,jj-1) & |
---|
881 | & + zwy(ji ,jj ) + zwy(ji+1,jj ) ) * r1_e1u(ji,jj) |
---|
882 | zx1 = - r1_8 * ( zwx(ji-1,jj ) + zwx(ji-1,jj+1) & |
---|
883 | & + zwx(ji ,jj ) + zwx(ji ,jj+1) ) * r1_e2v(ji,jj) |
---|
884 | zu_trd(ji,jj) = zy1 * ( zwz(ji ,jj-1) + zwz(ji,jj) ) |
---|
885 | zv_trd(ji,jj) = zx1 * ( zwz(ji-1,jj ) + zwz(ji,jj) ) |
---|
886 | END DO |
---|
887 | END DO |
---|
888 | ! |
---|
889 | ELSEIF ( ln_dynvor_een ) THEN !== energy and enstrophy conserving scheme ==! |
---|
890 | DO jj = 2, jpjm1 |
---|
891 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
892 | zu_trd(ji,jj) = + r1_12 * r1_e1u(ji,jj) * ( ftne(ji,jj ) * zwy(ji ,jj ) & |
---|
893 | & + ftnw(ji+1,jj) * zwy(ji+1,jj ) & |
---|
894 | & + ftse(ji,jj ) * zwy(ji ,jj-1) & |
---|
895 | & + ftsw(ji+1,jj) * zwy(ji+1,jj-1) ) |
---|
896 | zv_trd(ji,jj) = - r1_12 * r1_e2v(ji,jj) * ( ftsw(ji,jj+1) * zwx(ji-1,jj+1) & |
---|
897 | & + ftse(ji,jj+1) * zwx(ji ,jj+1) & |
---|
898 | & + ftnw(ji,jj ) * zwx(ji-1,jj ) & |
---|
899 | & + ftne(ji,jj ) * zwx(ji ,jj ) ) |
---|
900 | END DO |
---|
901 | END DO |
---|
902 | ! |
---|
903 | ENDIF |
---|
904 | ! |
---|
905 | ! Add tidal astronomical forcing if defined |
---|
906 | IF ( ln_tide .AND. ln_tide_pot ) THEN |
---|
907 | DO jj = 2, jpjm1 |
---|
908 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
909 | zu_spg = grav * ( pot_astro(ji+1,jj) - pot_astro(ji,jj) ) * r1_e1u(ji,jj) |
---|
910 | zv_spg = grav * ( pot_astro(ji,jj+1) - pot_astro(ji,jj) ) * r1_e2v(ji,jj) |
---|
911 | zu_trd(ji,jj) = zu_trd(ji,jj) + zu_spg |
---|
912 | zv_trd(ji,jj) = zv_trd(ji,jj) + zv_spg |
---|
913 | END DO |
---|
914 | END DO |
---|
915 | ENDIF |
---|
916 | ! |
---|
917 | DO jj = 2, jpjm1 |
---|
918 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
919 | ! Add top/bottom stresses: |
---|
920 | !!gm old/new |
---|
921 | zu_trd(ji,jj) = zu_trd(ji,jj) + zCdU_u(ji,jj) * un_e(ji,jj) * hur_e(ji,jj) |
---|
922 | zv_trd(ji,jj) = zv_trd(ji,jj) + zCdU_v(ji,jj) * vn_e(ji,jj) * hvr_e(ji,jj) |
---|
923 | !!gm |
---|
924 | END DO |
---|
925 | END DO |
---|
926 | ! |
---|
927 | ! Surface pressure trend: |
---|
928 | |
---|
929 | IF( ln_wd ) THEN |
---|
930 | DO jj = 2, jpjm1 |
---|
931 | DO ji = 2, jpim1 |
---|
932 | ! Add surface pressure gradient |
---|
933 | zu_spg = - grav * ( zsshp2_e(ji+1,jj) - zsshp2_e(ji,jj) ) * r1_e1u(ji,jj) |
---|
934 | zv_spg = - grav * ( zsshp2_e(ji,jj+1) - zsshp2_e(ji,jj) ) * r1_e2v(ji,jj) |
---|
935 | zwx(ji,jj) = zu_spg * zcpx(ji,jj) |
---|
936 | zwy(ji,jj) = zv_spg * zcpy(ji,jj) |
---|
937 | END DO |
---|
938 | END DO |
---|
939 | ELSE |
---|
940 | DO jj = 2, jpjm1 |
---|
941 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
942 | ! Add surface pressure gradient |
---|
943 | zu_spg = - grav * ( zsshp2_e(ji+1,jj) - zsshp2_e(ji,jj) ) * r1_e1u(ji,jj) |
---|
944 | zv_spg = - grav * ( zsshp2_e(ji,jj+1) - zsshp2_e(ji,jj) ) * r1_e2v(ji,jj) |
---|
945 | zwx(ji,jj) = zu_spg |
---|
946 | zwy(ji,jj) = zv_spg |
---|
947 | END DO |
---|
948 | END DO |
---|
949 | END IF |
---|
950 | |
---|
951 | ! |
---|
952 | ! Set next velocities: |
---|
953 | IF( ln_dynadv_vec .OR. ln_linssh ) THEN !* Vector form |
---|
954 | DO jj = 2, jpjm1 |
---|
955 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
956 | ua_e(ji,jj) = ( un_e(ji,jj) & |
---|
957 | & + rdtbt * ( zwx(ji,jj) & |
---|
958 | & + zu_trd(ji,jj) & |
---|
959 | & + zu_frc(ji,jj) ) & |
---|
960 | & ) * ssumask(ji,jj) |
---|
961 | |
---|
962 | va_e(ji,jj) = ( vn_e(ji,jj) & |
---|
963 | & + rdtbt * ( zwy(ji,jj) & |
---|
964 | & + zv_trd(ji,jj) & |
---|
965 | & + zv_frc(ji,jj) ) & |
---|
966 | & ) * ssvmask(ji,jj) |
---|
967 | END DO |
---|
968 | END DO |
---|
969 | ! |
---|
970 | ELSE !* Flux form |
---|
971 | DO jj = 2, jpjm1 |
---|
972 | DO ji = fs_2, fs_jpim1 ! vector opt. |
---|
973 | |
---|
974 | IF( ln_wd ) THEN |
---|
975 | zhura = MAX(hu_0(ji,jj) + zsshu_a(ji,jj), rn_wdmin1) |
---|
976 | zhvra = MAX(hv_0(ji,jj) + zsshv_a(ji,jj), rn_wdmin1) |
---|
977 | ELSE |
---|
978 | zhura = hu_0(ji,jj) + zsshu_a(ji,jj) |
---|
979 | zhvra = hv_0(ji,jj) + zsshv_a(ji,jj) |
---|
980 | END IF |
---|
981 | zhura = ssumask(ji,jj)/(zhura + 1._wp - ssumask(ji,jj)) |
---|
982 | zhvra = ssvmask(ji,jj)/(zhvra + 1._wp - ssvmask(ji,jj)) |
---|
983 | |
---|
984 | ua_e(ji,jj) = ( hu_e(ji,jj) * un_e(ji,jj) & |
---|
985 | & + rdtbt * ( zhust_e(ji,jj) * zwx(ji,jj) & |
---|
986 | & + zhup2_e(ji,jj) * zu_trd(ji,jj) & |
---|
987 | & + hu_n(ji,jj) * zu_frc(ji,jj) ) & |
---|
988 | & ) * zhura |
---|
989 | |
---|
990 | va_e(ji,jj) = ( hv_e(ji,jj) * vn_e(ji,jj) & |
---|
991 | & + rdtbt * ( zhvst_e(ji,jj) * zwy(ji,jj) & |
---|
992 | & + zhvp2_e(ji,jj) * zv_trd(ji,jj) & |
---|
993 | & + hv_n(ji,jj) * zv_frc(ji,jj) ) & |
---|
994 | & ) * zhvra |
---|
995 | END DO |
---|
996 | END DO |
---|
997 | ENDIF |
---|
998 | ! |
---|
999 | IF( .NOT.ln_linssh ) THEN !* Update ocean depth (variable volume case only) |
---|
1000 | IF( ln_wd ) THEN |
---|
1001 | hu_e (:,:) = MAX(hu_0(:,:) + zsshu_a(:,:), rn_wdmin1) |
---|
1002 | hv_e (:,:) = MAX(hv_0(:,:) + zsshv_a(:,:), rn_wdmin1) |
---|
1003 | ELSE |
---|
1004 | hu_e (:,:) = hu_0(:,:) + zsshu_a(:,:) |
---|
1005 | hv_e (:,:) = hv_0(:,:) + zsshv_a(:,:) |
---|
1006 | END IF |
---|
1007 | hur_e(:,:) = ssumask(:,:) / ( hu_e(:,:) + 1._wp - ssumask(:,:) ) |
---|
1008 | hvr_e(:,:) = ssvmask(:,:) / ( hv_e(:,:) + 1._wp - ssvmask(:,:) ) |
---|
1009 | ! |
---|
1010 | ENDIF |
---|
1011 | ! !* domain lateral boundary |
---|
1012 | CALL lbc_lnk_multi( ua_e, 'U', -1._wp, va_e , 'V', -1._wp ) |
---|
1013 | ! |
---|
1014 | ! ! open boundaries |
---|
1015 | IF( ln_bdy ) CALL bdy_dyn2d( jn, ua_e, va_e, un_e, vn_e, hur_e, hvr_e, ssha_e ) |
---|
1016 | #if defined key_agrif |
---|
1017 | IF( .NOT.Agrif_Root() ) CALL agrif_dyn_ts( jn ) ! Agrif |
---|
1018 | #endif |
---|
1019 | ! !* Swap |
---|
1020 | ! ! ---- |
---|
1021 | ubb_e (:,:) = ub_e (:,:) |
---|
1022 | ub_e (:,:) = un_e (:,:) |
---|
1023 | un_e (:,:) = ua_e (:,:) |
---|
1024 | ! |
---|
1025 | vbb_e (:,:) = vb_e (:,:) |
---|
1026 | vb_e (:,:) = vn_e (:,:) |
---|
1027 | vn_e (:,:) = va_e (:,:) |
---|
1028 | ! |
---|
1029 | sshbb_e(:,:) = sshb_e(:,:) |
---|
1030 | sshb_e (:,:) = sshn_e(:,:) |
---|
1031 | sshn_e (:,:) = ssha_e(:,:) |
---|
1032 | |
---|
1033 | ! !* Sum over whole bt loop |
---|
1034 | ! ! ---------------------- |
---|
1035 | za1 = wgtbtp1(jn) |
---|
1036 | IF( ln_dynadv_vec .OR. ln_linssh ) THEN ! Sum velocities |
---|
1037 | ua_b (:,:) = ua_b (:,:) + za1 * ua_e (:,:) |
---|
1038 | va_b (:,:) = va_b (:,:) + za1 * va_e (:,:) |
---|
1039 | ELSE ! Sum transports |
---|
1040 | ua_b (:,:) = ua_b (:,:) + za1 * ua_e (:,:) * hu_e (:,:) |
---|
1041 | va_b (:,:) = va_b (:,:) + za1 * va_e (:,:) * hv_e (:,:) |
---|
1042 | ENDIF |
---|
1043 | ! ! Sum sea level |
---|
1044 | ssha(:,:) = ssha(:,:) + za1 * ssha_e(:,:) |
---|
1045 | ! ! ==================== ! |
---|
1046 | END DO ! end loop ! |
---|
1047 | ! ! ==================== ! |
---|
1048 | ! ----------------------------------------------------------------------------- |
---|
1049 | ! Phase 3. update the general trend with the barotropic trend |
---|
1050 | ! ----------------------------------------------------------------------------- |
---|
1051 | ! |
---|
1052 | ! Set advection velocity correction: |
---|
1053 | zwx(:,:) = un_adv(:,:) |
---|
1054 | zwy(:,:) = vn_adv(:,:) |
---|
1055 | IF( ( kt == nit000 .AND. neuler==0 ) .OR. .NOT.ln_bt_fw ) THEN |
---|
1056 | un_adv(:,:) = zwx(:,:) * r1_hu_n(:,:) |
---|
1057 | vn_adv(:,:) = zwy(:,:) * r1_hv_n(:,:) |
---|
1058 | ELSE |
---|
1059 | un_adv(:,:) = r1_2 * ( ub2_b(:,:) + zwx(:,:) ) * r1_hu_n(:,:) |
---|
1060 | vn_adv(:,:) = r1_2 * ( vb2_b(:,:) + zwy(:,:) ) * r1_hv_n(:,:) |
---|
1061 | END IF |
---|
1062 | |
---|
1063 | IF( ln_bt_fw ) THEN ! Save integrated transport for next computation |
---|
1064 | ub2_b(:,:) = zwx(:,:) |
---|
1065 | vb2_b(:,:) = zwy(:,:) |
---|
1066 | ENDIF |
---|
1067 | ! |
---|
1068 | ! Update barotropic trend: |
---|
1069 | IF( ln_dynadv_vec .OR. ln_linssh ) THEN |
---|
1070 | DO jk=1,jpkm1 |
---|
1071 | ua(:,:,jk) = ua(:,:,jk) + ( ua_b(:,:) - ub_b(:,:) ) * z1_2dt_b |
---|
1072 | va(:,:,jk) = va(:,:,jk) + ( va_b(:,:) - vb_b(:,:) ) * z1_2dt_b |
---|
1073 | END DO |
---|
1074 | ELSE |
---|
1075 | ! At this stage, ssha has been corrected: compute new depths at velocity points |
---|
1076 | DO jj = 1, jpjm1 |
---|
1077 | DO ji = 1, jpim1 ! NO Vector Opt. |
---|
1078 | zsshu_a(ji,jj) = r1_2 * umask(ji,jj,1) * r1_e1e2u(ji,jj) & |
---|
1079 | & * ( e1e2t(ji ,jj) * ssha(ji ,jj) & |
---|
1080 | & + e1e2t(ji+1,jj) * ssha(ji+1,jj) ) |
---|
1081 | zsshv_a(ji,jj) = r1_2 * vmask(ji,jj,1) * r1_e1e2v(ji,jj) & |
---|
1082 | & * ( e1e2t(ji,jj ) * ssha(ji,jj ) & |
---|
1083 | & + e1e2t(ji,jj+1) * ssha(ji,jj+1) ) |
---|
1084 | END DO |
---|
1085 | END DO |
---|
1086 | CALL lbc_lnk_multi( zsshu_a, 'U', 1._wp, zsshv_a, 'V', 1._wp ) ! Boundary conditions |
---|
1087 | ! |
---|
1088 | DO jk=1,jpkm1 |
---|
1089 | ua(:,:,jk) = ua(:,:,jk) + r1_hu_n(:,:) * ( ua_b(:,:) - ub_b(:,:) * hu_b(:,:) ) * z1_2dt_b |
---|
1090 | va(:,:,jk) = va(:,:,jk) + r1_hv_n(:,:) * ( va_b(:,:) - vb_b(:,:) * hv_b(:,:) ) * z1_2dt_b |
---|
1091 | END DO |
---|
1092 | ! Save barotropic velocities not transport: |
---|
1093 | ua_b(:,:) = ua_b(:,:) / ( hu_0(:,:) + zsshu_a(:,:) + 1._wp - ssumask(:,:) ) |
---|
1094 | va_b(:,:) = va_b(:,:) / ( hv_0(:,:) + zsshv_a(:,:) + 1._wp - ssvmask(:,:) ) |
---|
1095 | ENDIF |
---|
1096 | ! |
---|
1097 | DO jk = 1, jpkm1 |
---|
1098 | ! Correct velocities: |
---|
1099 | un(:,:,jk) = ( un(:,:,jk) + un_adv(:,:) - un_b(:,:) ) * umask(:,:,jk) |
---|
1100 | vn(:,:,jk) = ( vn(:,:,jk) + vn_adv(:,:) - vn_b(:,:) ) * vmask(:,:,jk) |
---|
1101 | ! |
---|
1102 | END DO |
---|
1103 | ! |
---|
1104 | CALL iom_put( "ubar", un_adv(:,:) ) ! barotropic i-current |
---|
1105 | CALL iom_put( "vbar", vn_adv(:,:) ) ! barotropic i-current |
---|
1106 | ! |
---|
1107 | #if defined key_agrif |
---|
1108 | ! Save time integrated fluxes during child grid integration |
---|
1109 | ! (used to update coarse grid transports at next time step) |
---|
1110 | ! |
---|
1111 | IF( .NOT.Agrif_Root() .AND. ln_bt_fw ) THEN |
---|
1112 | IF( Agrif_NbStepint() == 0 ) THEN |
---|
1113 | ub2_i_b(:,:) = 0._wp |
---|
1114 | vb2_i_b(:,:) = 0._wp |
---|
1115 | END IF |
---|
1116 | ! |
---|
1117 | za1 = 1._wp / REAL(Agrif_rhot(), wp) |
---|
1118 | ub2_i_b(:,:) = ub2_i_b(:,:) + za1 * ub2_b(:,:) |
---|
1119 | vb2_i_b(:,:) = vb2_i_b(:,:) + za1 * vb2_b(:,:) |
---|
1120 | ENDIF |
---|
1121 | #endif |
---|
1122 | ! !* write time-spliting arrays in the restart |
---|
1123 | IF( lrst_oce .AND.ln_bt_fw ) CALL ts_rst( kt, 'WRITE' ) |
---|
1124 | ! |
---|
1125 | IF( ln_wd ) DEALLOCATE( zcpx, zcpy ) |
---|
1126 | ! |
---|
1127 | IF ( ln_diatmb ) THEN |
---|
1128 | CALL iom_put( "baro_u" , un_b*umask(:,:,1)+zmdi*(1-umask(:,:,1 ) ) ) ! Barotropic U Velocity |
---|
1129 | CALL iom_put( "baro_v" , vn_b*vmask(:,:,1)+zmdi*(1-vmask(:,:,1 ) ) ) ! Barotropic V Velocity |
---|
1130 | ENDIF |
---|
1131 | IF( nn_timing == 1 ) CALL timing_stop('dyn_spg_ts') |
---|
1132 | ! |
---|
1133 | END SUBROUTINE dyn_spg_ts |
---|
1134 | |
---|
1135 | |
---|
1136 | SUBROUTINE ts_wgt( ll_av, ll_fw, jpit, zwgt1, zwgt2) |
---|
1137 | !!--------------------------------------------------------------------- |
---|
1138 | !! *** ROUTINE ts_wgt *** |
---|
1139 | !! |
---|
1140 | !! ** Purpose : Set time-splitting weights for temporal averaging (or not) |
---|
1141 | !!---------------------------------------------------------------------- |
---|
1142 | LOGICAL, INTENT(in) :: ll_av ! temporal averaging=.true. |
---|
1143 | LOGICAL, INTENT(in) :: ll_fw ! forward time splitting =.true. |
---|
1144 | INTEGER, INTENT(inout) :: jpit ! cycle length |
---|
1145 | REAL(wp), DIMENSION(3*nn_baro), INTENT(inout) :: zwgt1, & ! Primary weights |
---|
1146 | zwgt2 ! Secondary weights |
---|
1147 | |
---|
1148 | INTEGER :: jic, jn, ji ! temporary integers |
---|
1149 | REAL(wp) :: za1, za2 |
---|
1150 | !!---------------------------------------------------------------------- |
---|
1151 | |
---|
1152 | zwgt1(:) = 0._wp |
---|
1153 | zwgt2(:) = 0._wp |
---|
1154 | |
---|
1155 | ! Set time index when averaged value is requested |
---|
1156 | IF (ll_fw) THEN |
---|
1157 | jic = nn_baro |
---|
1158 | ELSE |
---|
1159 | jic = 2 * nn_baro |
---|
1160 | ENDIF |
---|
1161 | |
---|
1162 | ! Set primary weights: |
---|
1163 | IF (ll_av) THEN |
---|
1164 | ! Define simple boxcar window for primary weights |
---|
1165 | ! (width = nn_baro, centered around jic) |
---|
1166 | SELECT CASE ( nn_bt_flt ) |
---|
1167 | CASE( 0 ) ! No averaging |
---|
1168 | zwgt1(jic) = 1._wp |
---|
1169 | jpit = jic |
---|
1170 | |
---|
1171 | CASE( 1 ) ! Boxcar, width = nn_baro |
---|
1172 | DO jn = 1, 3*nn_baro |
---|
1173 | za1 = ABS(float(jn-jic))/float(nn_baro) |
---|
1174 | IF (za1 < 0.5_wp) THEN |
---|
1175 | zwgt1(jn) = 1._wp |
---|
1176 | jpit = jn |
---|
1177 | ENDIF |
---|
1178 | ENDDO |
---|
1179 | |
---|
1180 | CASE( 2 ) ! Boxcar, width = 2 * nn_baro |
---|
1181 | DO jn = 1, 3*nn_baro |
---|
1182 | za1 = ABS(float(jn-jic))/float(nn_baro) |
---|
1183 | IF (za1 < 1._wp) THEN |
---|
1184 | zwgt1(jn) = 1._wp |
---|
1185 | jpit = jn |
---|
1186 | ENDIF |
---|
1187 | ENDDO |
---|
1188 | CASE DEFAULT ; CALL ctl_stop( 'unrecognised value for nn_bt_flt' ) |
---|
1189 | END SELECT |
---|
1190 | |
---|
1191 | ELSE ! No time averaging |
---|
1192 | zwgt1(jic) = 1._wp |
---|
1193 | jpit = jic |
---|
1194 | ENDIF |
---|
1195 | |
---|
1196 | ! Set secondary weights |
---|
1197 | DO jn = 1, jpit |
---|
1198 | DO ji = jn, jpit |
---|
1199 | zwgt2(jn) = zwgt2(jn) + zwgt1(ji) |
---|
1200 | END DO |
---|
1201 | END DO |
---|
1202 | |
---|
1203 | ! Normalize weigths: |
---|
1204 | za1 = 1._wp / SUM(zwgt1(1:jpit)) |
---|
1205 | za2 = 1._wp / SUM(zwgt2(1:jpit)) |
---|
1206 | DO jn = 1, jpit |
---|
1207 | zwgt1(jn) = zwgt1(jn) * za1 |
---|
1208 | zwgt2(jn) = zwgt2(jn) * za2 |
---|
1209 | END DO |
---|
1210 | ! |
---|
1211 | END SUBROUTINE ts_wgt |
---|
1212 | |
---|
1213 | |
---|
1214 | SUBROUTINE ts_rst( kt, cdrw ) |
---|
1215 | !!--------------------------------------------------------------------- |
---|
1216 | !! *** ROUTINE ts_rst *** |
---|
1217 | !! |
---|
1218 | !! ** Purpose : Read or write time-splitting arrays in restart file |
---|
1219 | !!---------------------------------------------------------------------- |
---|
1220 | INTEGER , INTENT(in) :: kt ! ocean time-step |
---|
1221 | CHARACTER(len=*), INTENT(in) :: cdrw ! "READ"/"WRITE" flag |
---|
1222 | ! |
---|
1223 | !!---------------------------------------------------------------------- |
---|
1224 | ! |
---|
1225 | IF( TRIM(cdrw) == 'READ' ) THEN |
---|
1226 | CALL iom_get( numror, jpdom_autoglo, 'ub2_b' , ub2_b (:,:) ) |
---|
1227 | CALL iom_get( numror, jpdom_autoglo, 'vb2_b' , vb2_b (:,:) ) |
---|
1228 | IF( .NOT.ln_bt_av ) THEN |
---|
1229 | CALL iom_get( numror, jpdom_autoglo, 'sshbb_e' , sshbb_e(:,:) ) |
---|
1230 | CALL iom_get( numror, jpdom_autoglo, 'ubb_e' , ubb_e(:,:) ) |
---|
1231 | CALL iom_get( numror, jpdom_autoglo, 'vbb_e' , vbb_e(:,:) ) |
---|
1232 | CALL iom_get( numror, jpdom_autoglo, 'sshb_e' , sshb_e(:,:) ) |
---|
1233 | CALL iom_get( numror, jpdom_autoglo, 'ub_e' , ub_e(:,:) ) |
---|
1234 | CALL iom_get( numror, jpdom_autoglo, 'vb_e' , vb_e(:,:) ) |
---|
1235 | ENDIF |
---|
1236 | #if defined key_agrif |
---|
1237 | ! Read time integrated fluxes |
---|
1238 | IF ( .NOT.Agrif_Root() ) THEN |
---|
1239 | CALL iom_get( numror, jpdom_autoglo, 'ub2_i_b' , ub2_i_b(:,:) ) |
---|
1240 | CALL iom_get( numror, jpdom_autoglo, 'vb2_i_b' , vb2_i_b(:,:) ) |
---|
1241 | ENDIF |
---|
1242 | #endif |
---|
1243 | ! |
---|
1244 | ELSEIF( TRIM(cdrw) == 'WRITE' ) THEN |
---|
1245 | CALL iom_rstput( kt, nitrst, numrow, 'ub2_b' , ub2_b (:,:) ) |
---|
1246 | CALL iom_rstput( kt, nitrst, numrow, 'vb2_b' , vb2_b (:,:) ) |
---|
1247 | ! |
---|
1248 | IF (.NOT.ln_bt_av) THEN |
---|
1249 | CALL iom_rstput( kt, nitrst, numrow, 'sshbb_e' , sshbb_e(:,:) ) |
---|
1250 | CALL iom_rstput( kt, nitrst, numrow, 'ubb_e' , ubb_e(:,:) ) |
---|
1251 | CALL iom_rstput( kt, nitrst, numrow, 'vbb_e' , vbb_e(:,:) ) |
---|
1252 | CALL iom_rstput( kt, nitrst, numrow, 'sshb_e' , sshb_e(:,:) ) |
---|
1253 | CALL iom_rstput( kt, nitrst, numrow, 'ub_e' , ub_e(:,:) ) |
---|
1254 | CALL iom_rstput( kt, nitrst, numrow, 'vb_e' , vb_e(:,:) ) |
---|
1255 | ENDIF |
---|
1256 | #if defined key_agrif |
---|
1257 | ! Save time integrated fluxes |
---|
1258 | IF ( .NOT.Agrif_Root() ) THEN |
---|
1259 | CALL iom_rstput( kt, nitrst, numrow, 'ub2_i_b' , ub2_i_b(:,:) ) |
---|
1260 | CALL iom_rstput( kt, nitrst, numrow, 'vb2_i_b' , vb2_i_b(:,:) ) |
---|
1261 | ENDIF |
---|
1262 | #endif |
---|
1263 | ENDIF |
---|
1264 | ! |
---|
1265 | END SUBROUTINE ts_rst |
---|
1266 | |
---|
1267 | |
---|
1268 | SUBROUTINE dyn_spg_ts_init |
---|
1269 | !!--------------------------------------------------------------------- |
---|
1270 | !! *** ROUTINE dyn_spg_ts_init *** |
---|
1271 | !! |
---|
1272 | !! ** Purpose : Set time splitting options |
---|
1273 | !!---------------------------------------------------------------------- |
---|
1274 | INTEGER :: ji ,jj ! dummy loop indices |
---|
1275 | REAL(wp) :: zxr2, zyr2, zcmax ! local scalar |
---|
1276 | REAL(wp), DIMENSION(jpi,jpj) :: zcu |
---|
1277 | !!---------------------------------------------------------------------- |
---|
1278 | ! |
---|
1279 | ! Max courant number for ext. grav. waves |
---|
1280 | ! |
---|
1281 | DO jj = 1, jpj |
---|
1282 | DO ji =1, jpi |
---|
1283 | zxr2 = r1_e1t(ji,jj) * r1_e1t(ji,jj) |
---|
1284 | zyr2 = r1_e2t(ji,jj) * r1_e2t(ji,jj) |
---|
1285 | zcu(ji,jj) = SQRT( grav * MAX(ht_0(ji,jj),0._wp) * (zxr2 + zyr2) ) |
---|
1286 | END DO |
---|
1287 | END DO |
---|
1288 | ! |
---|
1289 | zcmax = MAXVAL( zcu(:,:) ) |
---|
1290 | IF( lk_mpp ) CALL mpp_max( zcmax ) |
---|
1291 | |
---|
1292 | ! Estimate number of iterations to satisfy a max courant number= rn_bt_cmax |
---|
1293 | IF( ln_bt_auto ) nn_baro = CEILING( rdt / rn_bt_cmax * zcmax) |
---|
1294 | |
---|
1295 | rdtbt = rdt / REAL( nn_baro , wp ) |
---|
1296 | zcmax = zcmax * rdtbt |
---|
1297 | ! Print results |
---|
1298 | IF(lwp) WRITE(numout,*) |
---|
1299 | IF(lwp) WRITE(numout,*) 'dyn_spg_ts : split-explicit free surface' |
---|
1300 | IF(lwp) WRITE(numout,*) '~~~~~~~~~~' |
---|
1301 | IF( ln_bt_auto ) THEN |
---|
1302 | IF(lwp) WRITE(numout,*) ' ln_ts_auto=.true. Automatically set nn_baro ' |
---|
1303 | IF(lwp) WRITE(numout,*) ' Max. courant number allowed: ', rn_bt_cmax |
---|
1304 | ELSE |
---|
1305 | IF(lwp) WRITE(numout,*) ' ln_ts_auto=.false.: Use nn_baro in namelist ' |
---|
1306 | ENDIF |
---|
1307 | |
---|
1308 | IF(ln_bt_av) THEN |
---|
1309 | IF(lwp) WRITE(numout,*) ' ln_bt_av=.true. => Time averaging over nn_baro time steps is on ' |
---|
1310 | ELSE |
---|
1311 | IF(lwp) WRITE(numout,*) ' ln_bt_av=.false. => No time averaging of barotropic variables ' |
---|
1312 | ENDIF |
---|
1313 | ! |
---|
1314 | ! |
---|
1315 | IF(ln_bt_fw) THEN |
---|
1316 | IF(lwp) WRITE(numout,*) ' ln_bt_fw=.true. => Forward integration of barotropic variables ' |
---|
1317 | ELSE |
---|
1318 | IF(lwp) WRITE(numout,*) ' ln_bt_fw =.false.=> Centred integration of barotropic variables ' |
---|
1319 | ENDIF |
---|
1320 | ! |
---|
1321 | #if defined key_agrif |
---|
1322 | ! Restrict the use of Agrif to the forward case only |
---|
1323 | IF( .NOT.ln_bt_fw .AND. .NOT.Agrif_Root() ) CALL ctl_stop( 'AGRIF not implemented if ln_bt_fw=.FALSE.' ) |
---|
1324 | #endif |
---|
1325 | ! |
---|
1326 | IF(lwp) WRITE(numout,*) ' Time filter choice, nn_bt_flt: ', nn_bt_flt |
---|
1327 | SELECT CASE ( nn_bt_flt ) |
---|
1328 | CASE( 0 ) ; IF(lwp) WRITE(numout,*) ' Dirac' |
---|
1329 | CASE( 1 ) ; IF(lwp) WRITE(numout,*) ' Boxcar: width = nn_baro' |
---|
1330 | CASE( 2 ) ; IF(lwp) WRITE(numout,*) ' Boxcar: width = 2*nn_baro' |
---|
1331 | CASE DEFAULT ; CALL ctl_stop( 'unrecognised value for nn_bt_flt: should 0,1,2' ) |
---|
1332 | END SELECT |
---|
1333 | ! |
---|
1334 | IF(lwp) WRITE(numout,*) ' ' |
---|
1335 | IF(lwp) WRITE(numout,*) ' nn_baro = ', nn_baro |
---|
1336 | IF(lwp) WRITE(numout,*) ' Barotropic time step [s] is :', rdtbt |
---|
1337 | IF(lwp) WRITE(numout,*) ' Maximum Courant number is :', zcmax |
---|
1338 | ! |
---|
1339 | IF( .NOT.ln_bt_av .AND. .NOT.ln_bt_fw ) THEN |
---|
1340 | CALL ctl_stop( 'dynspg_ts ERROR: No time averaging => only forward integration is possible' ) |
---|
1341 | ENDIF |
---|
1342 | IF( zcmax>0.9_wp ) THEN |
---|
1343 | CALL ctl_stop( 'dynspg_ts ERROR: Maximum Courant number is greater than 0.9: Inc. nn_baro !' ) |
---|
1344 | ENDIF |
---|
1345 | ! |
---|
1346 | END SUBROUTINE dyn_spg_ts_init |
---|
1347 | |
---|
1348 | !!====================================================================== |
---|
1349 | END MODULE dynspg_ts |
---|