[825] | 1 | MODULE limrhg |
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| 2 | !!====================================================================== |
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| 3 | !! *** MODULE limrhg *** |
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[834] | 4 | !! Ice rheology : sea ice rheology |
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[825] | 5 | !!====================================================================== |
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| 6 | #if defined key_lim3 |
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| 7 | !!---------------------------------------------------------------------- |
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[834] | 8 | !! 'key_lim3' LIM3 sea-ice model |
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[825] | 9 | !!---------------------------------------------------------------------- |
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| 10 | !! lim_rhg : computes ice velocities |
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| 11 | !!---------------------------------------------------------------------- |
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| 12 | !! * Modules used |
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| 13 | USE phycst |
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| 14 | USE par_oce |
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| 15 | USE ice_oce ! ice variables |
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| 16 | USE dom_oce |
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| 17 | USE dom_ice |
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| 18 | USE ice |
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| 19 | USE iceini |
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| 20 | USE lbclnk |
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| 21 | USE lib_mpp |
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| 22 | USE in_out_manager ! I/O manager |
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| 23 | USE limitd_me |
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| 24 | USE prtctl ! Print control |
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| 25 | |
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| 26 | |
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| 27 | IMPLICIT NONE |
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| 28 | PRIVATE |
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| 29 | |
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| 30 | !! * Routine accessibility |
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| 31 | PUBLIC lim_rhg ! routine called by lim_dyn |
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| 32 | |
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| 33 | !! * Module variables |
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| 34 | REAL(wp) :: & ! constant values |
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| 35 | rzero = 0.e0 , & |
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| 36 | rone = 1.e0 |
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| 37 | !!---------------------------------------------------------------------- |
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[834] | 38 | !! LIM 3.0, UCL-LOCEAN-IPSL (2008) |
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[825] | 39 | !! $Header: /home/opalod/NEMOCVSROOT/NEMO/LIM_SRC/limrhg.F90,v 1.5 2005/03/27 18:34:42 opalod Exp $ |
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| 40 | !! This software is governed by the CeCILL licence see modipsl/doc/NEMO_CeCILL.txt |
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| 41 | !!---------------------------------------------------------------------- |
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| 42 | |
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| 43 | CONTAINS |
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| 44 | |
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| 45 | SUBROUTINE lim_rhg( k_j1, k_jpj ) |
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[834] | 46 | |
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[825] | 47 | !!------------------------------------------------------------------- |
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[834] | 48 | !! *** SUBROUTINE lim_rhg *** |
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| 49 | !! EVP-C-grid |
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[825] | 50 | !! |
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[834] | 51 | !! ** purpose : determines sea ice drift from wind stress, ice-ocean |
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[825] | 52 | !! stress and sea-surface slope. Ice-ice interaction is described by |
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[834] | 53 | !! a non-linear elasto-viscous-plastic (EVP) law including shear |
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| 54 | !! strength and a bulk rheology (Hunke and Dukowicz, 2002). |
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[825] | 55 | !! |
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[834] | 56 | !! The points in the C-grid look like this, dear reader |
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[825] | 57 | !! |
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[834] | 58 | !! (ji,jj) |
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| 59 | !! | |
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| 60 | !! | |
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| 61 | !! (ji-1,jj) | (ji,jj) |
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| 62 | !! --------- |
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| 63 | !! | | |
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| 64 | !! | (ji,jj) |------(ji,jj) |
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| 65 | !! | | |
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| 66 | !! --------- |
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| 67 | !! (ji-1,jj-1) (ji,jj-1) |
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[825] | 68 | !! |
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[834] | 69 | !! ** Inputs : - wind forcing (stress), oceanic currents |
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| 70 | !! ice total volume (vt_i) per unit area |
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| 71 | !! snow total volume (vt_s) per unit area |
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[825] | 72 | !! |
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[834] | 73 | !! ** Action : - compute u_ice, v_ice : the components of the |
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| 74 | !! sea-ice velocity vector |
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| 75 | !! - compute delta_i, shear_i, divu_i, which are inputs |
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| 76 | !! of the ice thickness distribution |
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[825] | 77 | !! |
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[834] | 78 | !! ** Steps : 1) Compute ice snow mass, ice strength |
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| 79 | !! 2) Compute wind, oceanic stresses, mass terms and |
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| 80 | !! coriolis terms of the momentum equation |
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| 81 | !! 3) Solve the momentum equation (iterative procedure) |
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| 82 | !! 4) Prevent high velocities if the ice is thin |
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| 83 | !! 5) Recompute invariants of the strain rate tensor |
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| 84 | !! which are inputs of the ITD, store stress |
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| 85 | !! for the next time step |
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| 86 | !! 6) Control prints of residual (convergence) |
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| 87 | !! and charge ellipse. |
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| 88 | !! The user should make sure that the parameters |
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| 89 | !! nevp, telast and creepl maintain stress state |
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| 90 | !! on the charge ellipse for plastic flow |
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| 91 | !! e.g. in the Canadian Archipelago |
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| 92 | !! |
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| 93 | !! ** References : Hunke and Dukowicz, JPO97 |
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| 94 | !! Bouillon et al., 08, in prep (update this when |
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| 95 | !! published) |
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| 96 | !! Vancoppenolle et al., OM08 |
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| 97 | !! |
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[825] | 98 | !! History : |
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[834] | 99 | !! 1.0 ! 07-03 (M.A. Morales Maqueda, S. Bouillon) |
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| 100 | !! 2.0 ! 08-03 M. Vancoppenolle : LIM3 |
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[825] | 101 | !! |
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| 102 | !!------------------------------------------------------------------- |
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| 103 | ! * Arguments |
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| 104 | ! |
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| 105 | INTEGER, INTENT(in) :: & |
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[834] | 106 | k_j1 , & !: southern j-index for ice computation |
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| 107 | k_jpj !: northern j-index for ice computation |
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[825] | 108 | |
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| 109 | ! * Local variables |
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[834] | 110 | INTEGER :: ji, jj !: dummy loop indices |
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[825] | 111 | |
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| 112 | INTEGER :: & |
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[834] | 113 | iter, jter !: temporary integers |
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[825] | 114 | |
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| 115 | CHARACTER (len=50) :: charout |
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| 116 | |
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| 117 | REAL(wp) :: & |
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[834] | 118 | zt11, zt12, zt21, zt22, & !: temporary scalars |
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| 119 | ztagnx, ztagny, & !: wind stress on U/V points |
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| 120 | delta ! |
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[825] | 121 | |
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| 122 | REAL(wp) :: & |
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[834] | 123 | za, & !: |
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| 124 | zstms, & !: temporary scalar for ice strength |
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| 125 | zsang, & !: temporary scalar for coriolis term |
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| 126 | zmask !: mask for the computation of ice mass |
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[825] | 127 | |
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[834] | 128 | REAL(wp),DIMENSION(jpi,jpj) :: & |
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| 129 | zpresh , & !: temporary array for ice strength |
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| 130 | zpreshc , & !: Ice strength on grid cell corners (zpreshc) |
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| 131 | zfrld1, zfrld2, & !: lead fraction on U/V points |
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| 132 | zmass1, zmass2, & !: ice/snow mass on U/V points |
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| 133 | zcorl1, zcorl2, & !: coriolis parameter on U/V points |
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| 134 | za1ct, za2ct , & !: temporary arrays |
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| 135 | zc1 , & !: ice mass |
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| 136 | zusw , & !: temporary weight for the computation |
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| 137 | !: of ice strength |
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| 138 | u_oce1, v_oce1, & !: ocean u/v component on U points |
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| 139 | u_oce2, v_oce2, & !: ocean u/v component on V points |
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| 140 | u_ice2, & !: ice u component on V point |
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| 141 | v_ice1 !: ice v component on U point |
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[825] | 142 | |
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| 143 | REAL(wp) :: & |
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[834] | 144 | dtevp, & !: time step for subcycling |
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| 145 | dtotel, & !: |
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| 146 | ecc2, & !: square of yield ellipse eccenticity |
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| 147 | z0, & !: temporary scalar |
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| 148 | zr, & !: temporary scalar |
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| 149 | zcca, zccb, & !: temporary scalars |
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| 150 | zu_ice2, & !: |
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| 151 | zv_ice1, & !: |
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| 152 | zddc, zdtc, & !: temporary array for delta on corners |
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| 153 | zdst, & !: temporary array for delta on centre |
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| 154 | zdsshx, zdsshy, & !: term for the gradient of ocean surface |
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| 155 | sigma1, sigma2 !: internal ice stress |
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[825] | 156 | |
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[834] | 157 | REAL(wp),DIMENSION(jpi,jpj) :: & |
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| 158 | zf1, zf2 !: arrays for internal stresses |
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[825] | 159 | |
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[834] | 160 | REAL(wp),DIMENSION(jpi,jpj) :: & |
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| 161 | zdd, zdt, & !: Divergence and tension at centre of grid cells |
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| 162 | zds, & !: Shear on northeast corner of grid cells |
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| 163 | deltat, & !: Delta at centre of grid cells |
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| 164 | deltac, & !: Delta on corners |
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| 165 | zs1, zs2, & !: Diagonal stress tensor components zs1 and zs2 |
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| 166 | zs12 !: Non-diagonal stress tensor component zs12 |
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[825] | 167 | |
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[834] | 168 | REAL(wp) :: & |
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| 169 | zresm , & !: Maximal error on ice velocity |
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| 170 | zindb , & !: ice (1) or not (0) |
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| 171 | zdummy !: dummy argument |
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[825] | 172 | |
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[834] | 173 | REAL(wp),DIMENSION(jpi,jpj) :: & |
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| 174 | zu_ice , & !: Ice velocity on previous time step |
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| 175 | zv_ice , & |
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| 176 | zresr !: Local error on velocity |
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[825] | 177 | |
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| 178 | ! |
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| 179 | !------------------------------------------------------------------------------! |
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[834] | 180 | ! 1) Ice-Snow mass (zc1), ice strength (zpresh) ! |
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[825] | 181 | !------------------------------------------------------------------------------! |
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| 182 | ! |
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| 183 | ! Put every vector to 0 |
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| 184 | zpresh(:,:) = 0.0 ; zpreshc(:,:) = 0.0 ; zfrld1(:,:) = 0.0 |
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| 185 | zmass1(:,:) = 0.0 ; zcorl1(:,:) = 0.0 ; zcorl2(:,:) = 0.0 |
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| 186 | za1ct(:,:) = 0.0 ; za2ct(:,:) = 0.0 |
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| 187 | zc1(:,:) = 0.0 ; zusw(:,:) = 0.0 |
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| 188 | u_oce1(:,:) = 0.0 ; v_oce1(:,:) = 0.0 ; u_oce2(:,:) = 0.0 |
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| 189 | v_oce2(:,:) = 0.0 ; u_ice2(:,:) = 0.0 ; v_ice1(:,:) = 0.0 |
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[834] | 190 | zf1(:,:) = 0.0 ; zf2(:,:) = 0.0 |
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[825] | 191 | zdd(:,:) = 0.0 ; zdt(:,:) = 0.0 ; zds(:,:) = 0.0 |
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| 192 | deltat(:,:) = 0.0 ; deltac(:,:) = 0.0 |
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[834] | 193 | zpresh(:,:) = 0.0 |
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[825] | 194 | |
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[834] | 195 | ! Ice strength on T-points |
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[825] | 196 | CALL lim_itd_me_icestrength(ridge_scheme_swi) |
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| 197 | |
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[834] | 198 | ! Ice mass and temp variables |
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[825] | 199 | DO jj = k_j1 , k_jpj-1 |
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| 200 | DO ji = 1 , jpi |
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| 201 | zc1(ji,jj) = tms(ji,jj) * ( rhosn * vt_s(ji,jj) + rhoic * vt_i(ji,jj) ) |
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| 202 | zpresh(ji,jj) = tms(ji,jj) * strength(ji,jj) / 2. |
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[866] | 203 | ! tmi = 1 where there is ice or on land |
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| 204 | tmi(ji,jj) = 1.0 - ( 1.0 - MAX( 0.0 , SIGN ( 1.0 , vt_i(ji,jj) - & |
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[825] | 205 | epsd ) ) ) * tms(ji,jj) |
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| 206 | END DO |
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| 207 | END DO |
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| 208 | |
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| 209 | CALL lbc_lnk( zc1(:,:), 'T', 1. ) |
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| 210 | CALL lbc_lnk( zpresh(:,:), 'T', 1. ) |
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| 211 | |
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[866] | 212 | CALL lbc_lnk( tmi(:,:), 'T', 1. ) |
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[834] | 213 | |
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| 214 | ! Ice strength on grid cell corners (zpreshc) |
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| 215 | ! needed for calculation of shear stress |
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[825] | 216 | DO jj = k_j1+1, k_jpj-1 |
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| 217 | DO ji = 2, jpim1 |
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[834] | 218 | zstms = tms(ji+1,jj+1) * wght(ji+1,jj+1,2,2) + & |
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| 219 | & tms(ji,jj+1) * wght(ji+1,jj+1,1,2) + & |
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| 220 | & tms(ji+1,jj) * wght(ji+1,jj+1,2,1) + & |
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| 221 | & tms(ji,jj) * wght(ji+1,jj+1,1,1) |
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[825] | 222 | zusw(ji,jj) = 1.0 / MAX( zstms, epsd ) |
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[834] | 223 | zpreshc(ji,jj) = ( zpresh(ji+1,jj+1) * wght(ji+1,jj+1,2,2) + & |
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| 224 | & zpresh(ji,jj+1) * wght(ji+1,jj+1,1,2) + & |
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| 225 | & zpresh(ji+1,jj) * wght(ji+1,jj+1,2,1) + & |
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| 226 | & zpresh(ji,jj) * wght(ji+1,jj+1,1,1) & |
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| 227 | & ) * zusw(ji,jj) |
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[825] | 228 | END DO |
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| 229 | END DO |
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| 230 | |
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| 231 | CALL lbc_lnk( zpreshc(:,:), 'F', 1. ) |
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| 232 | ! |
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| 233 | !------------------------------------------------------------------------------! |
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| 234 | ! 2) Wind / ocean stress, mass terms, coriolis terms |
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| 235 | !------------------------------------------------------------------------------! |
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| 236 | ! |
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| 237 | ! Wind stress, coriolis and mass terms on the sides of the squares |
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| 238 | ! zfrld1: lead fraction on U-points |
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| 239 | ! zfrld2: lead fraction on V-points |
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| 240 | ! zmass1: ice/snow mass on U-points |
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| 241 | ! zmass2: ice/snow mass on V-points |
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| 242 | ! zcorl1: Coriolis parameter on U-points |
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| 243 | ! zcorl2: Coriolis parameter on V-points |
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| 244 | ! (ztagnx,ztagny): wind stress on U/V points |
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| 245 | ! u_oce1: ocean u component on u points |
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| 246 | ! v_oce1: ocean v component on u points |
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| 247 | ! u_oce2: ocean u component on v points |
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| 248 | ! v_oce2: ocean v component on v points |
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| 249 | |
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| 250 | DO jj = k_j1+1, k_jpj-1 |
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| 251 | DO ji = 2, jpim1 |
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| 252 | |
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| 253 | zt11 = tms(ji,jj)*e1t(ji,jj) |
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| 254 | zt12 = tms(ji+1,jj)*e1t(ji+1,jj) |
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| 255 | zt21 = tms(ji,jj)*e2t(ji,jj) |
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| 256 | zt22 = tms(ji,jj+1)*e2t(ji,jj+1) |
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| 257 | |
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| 258 | ! Leads area. |
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| 259 | zfrld1(ji,jj) = ( zt12 * ( 1.0 - at_i(ji,jj) ) + & |
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| 260 | & zt11 * ( 1.0 - at_i(ji+1,jj) ) ) / ( zt11 + zt12 + epsd ) |
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| 261 | zfrld2(ji,jj) = ( zt22 * ( 1.0 - at_i(ji,jj) ) + & |
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| 262 | & zt21 * ( 1.0 - at_i(ji,jj+1) ) ) / ( zt21 + zt22 + epsd ) |
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| 263 | |
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| 264 | ! Mass, coriolis coeff. and currents |
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[834] | 265 | zmass1(ji,jj) = ( zt12*zc1(ji,jj) + zt11*zc1(ji+1,jj) ) / (zt11+zt12+epsd) |
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| 266 | zmass2(ji,jj) = ( zt22*zc1(ji,jj) + zt21*zc1(ji,jj+1) ) / (zt21+zt22+epsd) |
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| 267 | zcorl1(ji,jj) = zmass1(ji,jj) * ( e1t(ji+1,jj)*fcor(ji,jj) + & |
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| 268 | e1t(ji,jj)*fcor(ji+1,jj) ) & |
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| 269 | / (e1t(ji,jj) + e1t(ji+1,jj) + epsd ) |
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| 270 | zcorl2(ji,jj) = zmass2(ji,jj) * ( e2t(ji,jj+1)*fcor(ji,jj) + & |
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| 271 | e2t(ji,jj)*fcor(ji,jj+1) ) & |
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| 272 | / ( e2t(ji,jj+1) + e2t(ji,jj) + epsd ) |
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[825] | 273 | ! |
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| 274 | u_oce1(ji,jj) = u_io(ji,jj) |
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[834] | 275 | v_oce2(ji,jj) = v_io(ji,jj) |
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[825] | 276 | |
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[834] | 277 | ! Ocean has no slip boundary condition |
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[866] | 278 | ! GG bug |
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| 279 | ! v_oce1(ji,jj) = 0.5*( (v_io(ji,jj)+v_io(ji,jj-1))*e1t(ji+1,jj) & |
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| 280 | ! & +(v_io(ji+1,jj)+v_io(ji+1,jj-1))*e1t(ji,jj)) & |
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| 281 | ! & /(e1t(ji+1,jj)+e1t(ji,jj)) * tmu(ji,jj) |
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| 282 | v_oce1(ji,jj) = 0.5*( (v_io(ji,jj)+v_io(ji,jj-1))*e1t(ji,jj) & |
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| 283 | & +(v_io(ji+1,jj)+v_io(ji+1,jj-1))*e1t(ji+1,jj)) & |
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[825] | 284 | & /(e1t(ji+1,jj)+e1t(ji,jj)) * tmu(ji,jj) |
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| 285 | |
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[866] | 286 | ! GG bug |
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| 287 | ! u_oce2(ji,jj) = 0.5*((u_io(ji,jj)+u_io(ji-1,jj))*e2t(ji,jj+1) & |
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| 288 | ! & +(u_io(ji,jj+1)+u_io(ji-1,jj+1))*e2t(ji,jj)) & |
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| 289 | ! & / (e2t(ji,jj+1)+e2t(ji,jj)) * tmv(ji,jj) |
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| 290 | u_oce2(ji,jj) = 0.5*((u_io(ji,jj)+u_io(ji-1,jj))*e2t(ji,jj) & |
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| 291 | & +(u_io(ji,jj+1)+u_io(ji-1,jj+1))*e2t(ji,jj+1)) & |
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[834] | 292 | & / (e2t(ji,jj+1)+e2t(ji,jj)) * tmv(ji,jj) |
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[825] | 293 | |
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| 294 | ! Wind stress. |
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| 295 | ztagnx = ( 1. - zfrld1(ji,jj) ) * gtaux(ji,jj) |
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| 296 | ztagny = ( 1. - zfrld2(ji,jj) ) * gtauy(ji,jj) |
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| 297 | |
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[834] | 298 | ! Computation of the velocity field taking into account the ice internal interaction. |
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[825] | 299 | ! Terms that are independent of the velocity field. |
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| 300 | |
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| 301 | ! SB On utilise maintenant le gradient de la pente de l'ocean |
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| 302 | ! include it later |
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| 303 | ! zdsshx = (ssh_io(ji+1,jj) - ssh_io(ji,jj))/e1u(ji,jj) |
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| 304 | ! zdsshy = (ssh_io(ji,jj+1) - ssh_io(ji,jj))/e2v(ji,jj) |
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[834] | 305 | |
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[825] | 306 | zdsshx = 0.0 |
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| 307 | zdsshy = 0.0 |
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| 308 | |
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| 309 | za1ct(ji,jj) = ztagnx - zmass1(ji,jj) * grav * zdsshx |
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| 310 | za2ct(ji,jj) = ztagny - zmass2(ji,jj) * grav * zdsshy |
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| 311 | |
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| 312 | END DO |
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| 313 | END DO |
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| 314 | |
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| 315 | ! |
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| 316 | !------------------------------------------------------------------------------! |
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[834] | 317 | ! 3) Solution of the momentum equation, iterative procedure |
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[825] | 318 | !------------------------------------------------------------------------------! |
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| 319 | ! |
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| 320 | ! Time step for subcycling |
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| 321 | dtevp = rdt_ice / nevp |
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| 322 | dtotel = dtevp / ( 2.0 * telast ) |
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| 323 | |
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| 324 | !-ecc2: square of yield ellipse eccenticrity (reminder: must become a namelist parameter) |
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| 325 | ecc2 = ecc*ecc |
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| 326 | |
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| 327 | !-Initialise stress tensor |
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[866] | 328 | zs1(:,:) = stress1_i(:,:) |
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| 329 | zs2(:,:) = stress2_i(:,:) |
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| 330 | zs12(:,:) = stress12_i(:,:) |
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[825] | 331 | |
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| 332 | v_ice1(:,:) = 0.0 |
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| 333 | u_ice2(:,:) = 0.0 |
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| 334 | |
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| 335 | zdd(:,:) = 0.0 |
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| 336 | zdt(:,:) = 0.0 |
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| 337 | zds(:,:) = 0.0 |
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| 338 | deltat(:,:) = 0.0 |
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| 339 | !----------------------! |
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| 340 | DO iter = 1 , nevp ! loop over iter ! |
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| 341 | !----------------------! |
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| 342 | DO jj = k_j1, k_jpj-1 |
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| 343 | zu_ice(:,jj) = u_ice(:,jj) ! velocity at previous time step |
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| 344 | zv_ice(:,jj) = v_ice(:,jj) |
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| 345 | END DO |
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| 346 | |
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[834] | 347 | DO jj = k_j1+1, k_jpj-1 |
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| 348 | DO ji = 2, jpim1 |
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[825] | 349 | |
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| 350 | ! |
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| 351 | !- Divergence, tension and shear (Section a. Appendix B of Hunke & Dukowicz, 2002) |
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| 352 | !- zdd(:,:), zdt(:,:): divergence and tension at centre of grid cells |
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| 353 | !- zds(:,:): shear on northeast corner of grid cells |
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| 354 | ! |
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[834] | 355 | !- IMPORTANT REMINDER: Dear Gurvan, note that, the way these terms are coded, |
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| 356 | ! there are many repeated calculations. |
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| 357 | ! Speed could be improved by regrouping terms. For |
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[825] | 358 | ! the moment, however, the stress is on clarity of coding to avoid |
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[834] | 359 | ! bugs (Martin, for Miguel). |
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| 360 | ! |
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| 361 | !- ALSO: arrays zdd, zdt, zds and delta could |
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| 362 | ! be removed in the future to minimise memory demand. |
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| 363 | ! |
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[825] | 364 | !- MORE NOTES: Note that we are calculating deformation rates and stresses on the corners of |
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| 365 | ! grid cells, exactly as in the B grid case. For simplicity, the indexation on |
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| 366 | ! the corners is the same as in the B grid. |
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| 367 | ! |
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| 368 | ! |
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| 369 | zdd(ji,jj) = ( e2u(ji,jj)*u_ice(ji,jj) & |
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| 370 | & -e2u(ji-1,jj)*u_ice(ji-1,jj) & |
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| 371 | & +e1v(ji,jj)*v_ice(ji,jj) & |
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| 372 | & -e1v(ji,jj-1)*v_ice(ji,jj-1) & |
---|
| 373 | & ) & |
---|
| 374 | & / area(ji,jj) |
---|
| 375 | |
---|
| 376 | zdt(ji,jj) = ( ( u_ice(ji,jj)/e2u(ji,jj) & |
---|
| 377 | & -u_ice(ji-1,jj)/e2u(ji-1,jj) & |
---|
| 378 | & )*e2t(ji,jj)*e2t(ji,jj) & |
---|
| 379 | & -( v_ice(ji,jj)/e1v(ji,jj) & |
---|
| 380 | & -v_ice(ji,jj-1)/e1v(ji,jj-1) & |
---|
| 381 | & )*e1t(ji,jj)*e1t(ji,jj) & |
---|
| 382 | & ) & |
---|
| 383 | & / area(ji,jj) |
---|
| 384 | |
---|
| 385 | ! |
---|
| 386 | zds(ji,jj) = ( ( u_ice(ji,jj+1)/e1u(ji,jj+1) & |
---|
| 387 | & -u_ice(ji,jj)/e1u(ji,jj) & |
---|
| 388 | & )*e1f(ji,jj)*e1f(ji,jj) & |
---|
| 389 | & +( v_ice(ji+1,jj)/e2v(ji+1,jj) & |
---|
| 390 | & -v_ice(ji,jj)/e2v(ji,jj) & |
---|
| 391 | & )*e2f(ji,jj)*e2f(ji,jj) & |
---|
| 392 | & ) & |
---|
| 393 | & / ( e1f(ji,jj) * e2f(ji,jj) ) * ( 2.0 - tmf(ji,jj) ) & |
---|
| 394 | & * tmi(ji,jj) * tmi(ji,jj+1) & |
---|
| 395 | & * tmi(ji+1,jj) * tmi(ji+1,jj+1) |
---|
| 396 | |
---|
| 397 | |
---|
| 398 | v_ice1(ji,jj) = 0.5*( (v_ice(ji,jj)+v_ice(ji,jj-1))*e1t(ji+1,jj) & |
---|
| 399 | & +(v_ice(ji+1,jj)+v_ice(ji+1,jj-1))*e1t(ji,jj)) & |
---|
| 400 | & /(e1t(ji+1,jj)+e1t(ji,jj)) * tmu(ji,jj) |
---|
| 401 | |
---|
| 402 | u_ice2(ji,jj) = 0.5*( (u_ice(ji,jj)+u_ice(ji-1,jj))*e2t(ji,jj+1) & |
---|
| 403 | & +(u_ice(ji,jj+1)+u_ice(ji-1,jj+1))*e2t(ji,jj)) & |
---|
| 404 | & /(e2t(ji,jj+1)+e2t(ji,jj)) * tmv(ji,jj) |
---|
| 405 | |
---|
| 406 | END DO |
---|
| 407 | END DO |
---|
| 408 | |
---|
| 409 | CALL lbc_lnk( zdd(:,:), 'T', 1. ) |
---|
| 410 | CALL lbc_lnk( zdt(:,:), 'T', 1. ) |
---|
| 411 | CALL lbc_lnk( zds(:,:), 'F', 1. ) |
---|
| 412 | |
---|
| 413 | DO jj = k_j1+1, k_jpj-1 |
---|
| 414 | DO ji = 2, jpim1 |
---|
| 415 | |
---|
| 416 | !- Calculate Delta at centre of grid cells |
---|
| 417 | zdst = ( e2u( ji , jj ) * v_ice1(ji,jj) & |
---|
| 418 | & - e2u( ji-1, jj ) * v_ice1(ji-1,jj) & |
---|
| 419 | & + e1v( ji , jj ) * u_ice2(ji,jj) & |
---|
| 420 | & - e1v( ji , jj-1 ) * u_ice2(ji,jj-1) & |
---|
| 421 | & ) & |
---|
| 422 | & / area(ji,jj) |
---|
| 423 | |
---|
| 424 | delta = SQRT( zdd(ji,jj)*zdd(ji,jj) + & |
---|
| 425 | & ( zdt(ji,jj)*zdt(ji,jj) + zdst*zdst ) * usecc2 ) |
---|
| 426 | deltat(ji,jj) = MAX( SQRT(zdd(ji,jj)**2 + & |
---|
| 427 | (zdt(ji,jj)**2 + zdst**2)*usecc2), creepl ) |
---|
| 428 | |
---|
| 429 | !-Calculate stress tensor components zs1 and zs2 |
---|
| 430 | !-at centre of grid cells (see section 3.5 of CICE user's guide). |
---|
| 431 | zs1(ji,jj) = ( zs1(ji,jj) & |
---|
| 432 | & - dtotel*( ( 1.0 - alphaevp) * zs1(ji,jj) + & |
---|
[834] | 433 | & ( delta / deltat(ji,jj) - zdd(ji,jj) / deltat(ji,jj) ) & |
---|
| 434 | * zpresh(ji,jj) ) ) & |
---|
[825] | 435 | & / ( 1.0 + alphaevp * dtotel ) |
---|
| 436 | |
---|
[834] | 437 | zs2(ji,jj) = ( zs2(ji,jj) & |
---|
| 438 | & - dtotel*((1.0-alphaevp)*ecc2*zs2(ji,jj) - & |
---|
| 439 | zdt(ji,jj)/deltat(ji,jj)*zpresh(ji,jj)) ) & |
---|
| 440 | & / ( 1.0 + alphaevp*ecc2*dtotel ) |
---|
[825] | 441 | |
---|
| 442 | END DO |
---|
| 443 | END DO |
---|
| 444 | |
---|
| 445 | CALL lbc_lnk( zs1(:,:), 'T', 1. ) |
---|
| 446 | CALL lbc_lnk( zs2(:,:), 'T', 1. ) |
---|
| 447 | |
---|
| 448 | DO jj = k_j1+1, k_jpj-1 |
---|
| 449 | DO ji = 2, jpim1 |
---|
| 450 | !- Calculate Delta on corners |
---|
| 451 | zddc = ( ( v_ice1(ji,jj+1)/e1u(ji,jj+1) & |
---|
| 452 | & -v_ice1(ji,jj)/e1u(ji,jj) & |
---|
| 453 | & )*e1f(ji,jj)*e1f(ji,jj) & |
---|
| 454 | & +( u_ice2(ji+1,jj)/e2v(ji+1,jj) & |
---|
| 455 | & -u_ice2(ji,jj)/e2v(ji,jj) & |
---|
| 456 | & )*e2f(ji,jj)*e2f(ji,jj) & |
---|
| 457 | & ) & |
---|
| 458 | & / ( e1f(ji,jj) * e2f(ji,jj) ) |
---|
| 459 | |
---|
| 460 | zdtc = (-( v_ice1(ji,jj+1)/e1u(ji,jj+1) & |
---|
| 461 | & -v_ice1(ji,jj)/e1u(ji,jj) & |
---|
| 462 | & )*e1f(ji,jj)*e1f(ji,jj) & |
---|
| 463 | & +( u_ice2(ji+1,jj)/e2v(ji+1,jj) & |
---|
| 464 | & -u_ice2(ji,jj)/e2v(ji,jj) & |
---|
| 465 | & )*e2f(ji,jj)*e2f(ji,jj) & |
---|
| 466 | & ) & |
---|
| 467 | & / ( e1f(ji,jj) * e2f(ji,jj) ) |
---|
| 468 | |
---|
[834] | 469 | deltac(ji,jj) = SQRT(zddc**2+(zdtc**2+zds(ji,jj)**2)*usecc2) + creepl |
---|
[825] | 470 | |
---|
| 471 | !-Calculate stress tensor component zs12 at corners (see section 3.5 of CICE user's guide). |
---|
[834] | 472 | zs12(ji,jj) = ( zs12(ji,jj) & |
---|
| 473 | & - dtotel*( (1.0-alphaevp)*ecc2*zs12(ji,jj) - zds(ji,jj) / & |
---|
| 474 | & ( 2.0*deltac(ji,jj) ) * zpreshc(ji,jj))) & |
---|
| 475 | & / ( 1.0 + alphaevp*ecc2*dtotel ) |
---|
[825] | 476 | |
---|
[834] | 477 | END DO ! ji |
---|
| 478 | END DO ! jj |
---|
[825] | 479 | |
---|
| 480 | CALL lbc_lnk( zs12(:,:), 'F', 1. ) |
---|
| 481 | |
---|
| 482 | ! Ice internal stresses (Appendix C of Hunke and Dukowicz, 2002) |
---|
| 483 | DO jj = k_j1+1, k_jpj-1 |
---|
| 484 | DO ji = 2, jpim1 |
---|
[834] | 485 | !- contribution of zs1, zs2 and zs12 to zf1 |
---|
| 486 | zf1(ji,jj) = 0.5*( (zs1(ji+1,jj)-zs1(ji,jj))*e2u(ji,jj) & |
---|
| 487 | & +(zs2(ji+1,jj)*e2t(ji+1,jj)**2-zs2(ji,jj)*e2t(ji,jj)**2)/e2u(ji,jj) & |
---|
| 488 | & +2.0*(zs12(ji,jj)*e1f(ji,jj)**2-zs12(ji,jj-1)*e1f(ji,jj-1)**2)/e1u(ji,jj) & |
---|
| 489 | & ) / ( e1u(ji,jj)*e2u(ji,jj) ) |
---|
| 490 | ! contribution of zs1, zs2 and zs12 to zf2 |
---|
| 491 | zf2(ji,jj) = 0.5*( (zs1(ji,jj+1)-zs1(ji,jj))*e1v(ji,jj) & |
---|
| 492 | & -(zs2(ji,jj+1)*e1t(ji,jj+1)**2 - zs2(ji,jj)*e1t(ji,jj)**2)/e1v(ji,jj) & |
---|
| 493 | & + 2.0*(zs12(ji,jj)*e2f(ji,jj)**2 - & |
---|
| 494 | zs12(ji-1,jj)*e2f(ji-1,jj)**2)/e2v(ji,jj) & |
---|
| 495 | & ) / ( e1v(ji,jj)*e2v(ji,jj) ) |
---|
[825] | 496 | END DO |
---|
| 497 | END DO |
---|
| 498 | ! |
---|
| 499 | ! Computation of ice velocity |
---|
| 500 | ! |
---|
| 501 | ! Both the Coriolis term and the ice-ocean drag are solved semi-implicitly. |
---|
| 502 | ! |
---|
[834] | 503 | IF (MOD(iter,2).eq.0) THEN |
---|
[825] | 504 | |
---|
| 505 | DO jj = k_j1+1, k_jpj-1 |
---|
| 506 | DO ji = 2, jpim1 |
---|
[834] | 507 | zmask = (1.0-MAX(rzero,SIGN(rone,-zmass1(ji,jj))))*tmu(ji,jj) |
---|
[825] | 508 | zsang = SIGN ( 1.0 , fcor(ji,jj) ) * sangvg |
---|
| 509 | z0 = zmass1(ji,jj)/dtevp |
---|
| 510 | |
---|
| 511 | ! SB modif because ocean has no slip boundary condition |
---|
[866] | 512 | ! GG bug |
---|
| 513 | ! zv_ice1 = 0.5*( (v_ice(ji,jj)+v_ice(ji,jj-1))*e1t(ji+1,jj) & |
---|
| 514 | ! & +(v_ice(ji+1,jj)+v_ice(ji+1,jj-1))*e1t(ji,jj)) & |
---|
| 515 | ! & /(e1t(ji+1,jj)+e1t(ji,jj)) * tmu(ji,jj) |
---|
| 516 | zv_ice1 = 0.5*( (v_ice(ji,jj)+v_ice(ji,jj-1))*e1t(ji,jj) & |
---|
| 517 | & +(v_ice(ji+1,jj)+v_ice(ji+1,jj-1))*e1t(ji+1,jj)) & |
---|
[825] | 518 | & /(e1t(ji+1,jj)+e1t(ji,jj)) * tmu(ji,jj) |
---|
[834] | 519 | za = rhoco*SQRT((u_ice(ji,jj)-u_oce1(ji,jj))**2 + & |
---|
| 520 | (zv_ice1-v_oce1(ji,jj))**2) * (1.0-zfrld1(ji,jj)) |
---|
| 521 | zr = z0*u_ice(ji,jj) + zf1(ji,jj) + za1ct(ji,jj) + & |
---|
| 522 | za*(cangvg*u_oce1(ji,jj)-zsang*v_oce1(ji,jj)) |
---|
[825] | 523 | zcca = z0+za*cangvg |
---|
| 524 | zccb = zcorl1(ji,jj)+za*zsang |
---|
| 525 | u_ice(ji,jj) = (zr+zccb*zv_ice1)/(zcca+epsd)*zmask |
---|
| 526 | |
---|
| 527 | END DO |
---|
| 528 | END DO |
---|
| 529 | |
---|
| 530 | CALL lbc_lnk( u_ice(:,:), 'U', -1. ) |
---|
| 531 | |
---|
| 532 | DO jj = k_j1+1, k_jpj-1 |
---|
| 533 | DO ji = 2, jpim1 |
---|
[834] | 534 | |
---|
[825] | 535 | zmask = (1.0-max(rzero,sign(rone,-zmass2(ji,jj))))*tmv(ji,jj) |
---|
| 536 | zsang = sign(1.0,fcor(ji,jj))*sangvg |
---|
| 537 | z0 = zmass2(ji,jj)/dtevp |
---|
| 538 | ! SB modif because ocean has no slip boundary condition |
---|
[866] | 539 | ! GG bug |
---|
| 540 | ! zu_ice2 = 0.5*( (u_ice(ji,jj)+u_ice(ji-1,jj))*e2t(ji,jj+1) & |
---|
| 541 | ! & + (u_ice(ji,jj+1)+u_ice(ji-1,jj+1))*e2t(ji,jj)) & |
---|
| 542 | ! & /(e2t(ji,jj+1)+e2t(ji,jj)) * tmv(ji,jj) |
---|
| 543 | zu_ice2 = 0.5*( (u_ice(ji,jj)+u_ice(ji-1,jj))*e2t(ji,jj) & |
---|
| 544 | & + (u_ice(ji,jj+1)+u_ice(ji-1,jj+1))*e2t(ji,jj+1)) & |
---|
[825] | 545 | & /(e2t(ji,jj+1)+e2t(ji,jj)) * tmv(ji,jj) |
---|
[834] | 546 | za = rhoco*SQRT((zu_ice2-u_oce2(ji,jj))**2 + & |
---|
| 547 | (v_ice(ji,jj)-v_oce2(ji,jj))**2)*(1.0-zfrld2(ji,jj)) |
---|
| 548 | zr = z0*v_ice(ji,jj) + zf2(ji,jj) + & |
---|
| 549 | za2ct(ji,jj) + za*(cangvg*v_oce2(ji,jj)+zsang*u_oce2(ji,jj)) |
---|
[825] | 550 | zcca = z0+za*cangvg |
---|
| 551 | zccb = zcorl2(ji,jj)+za*zsang |
---|
| 552 | v_ice(ji,jj) = (zr-zccb*zu_ice2)/(zcca+epsd)*zmask |
---|
| 553 | |
---|
| 554 | END DO |
---|
| 555 | END DO |
---|
| 556 | |
---|
| 557 | CALL lbc_lnk( v_ice(:,:), 'V', -1. ) |
---|
| 558 | |
---|
[834] | 559 | ELSE |
---|
[825] | 560 | DO jj = k_j1+1, k_jpj-1 |
---|
| 561 | DO ji = 2, jpim1 |
---|
| 562 | zmask = (1.0-max(rzero,sign(rone,-zmass2(ji,jj))))*tmv(ji,jj) |
---|
| 563 | zsang = sign(1.0,fcor(ji,jj))*sangvg |
---|
| 564 | z0 = zmass2(ji,jj)/dtevp |
---|
| 565 | ! SB modif because ocean has no slip boundary condition |
---|
[866] | 566 | ! GG Bug |
---|
| 567 | ! zu_ice2 = 0.5*( (u_ice(ji,jj)+u_ice(ji-1,jj))*e2t(ji,jj+1) & |
---|
| 568 | ! & +(u_ice(ji,jj+1)+u_ice(ji-1,jj+1))*e2t(ji,jj)) & |
---|
| 569 | ! & /(e2t(ji,jj+1)+e2t(ji,jj)) * tmv(ji,jj) |
---|
| 570 | zu_ice2 = 0.5*( (u_ice(ji,jj)+u_ice(ji-1,jj))*e2t(ji,jj) & |
---|
| 571 | & +(u_ice(ji,jj+1)+u_ice(ji-1,jj+1))*e2t(ji,jj+1)) & |
---|
[825] | 572 | & /(e2t(ji,jj+1)+e2t(ji,jj)) * tmv(ji,jj) |
---|
| 573 | |
---|
[834] | 574 | za = rhoco*SQRT((zu_ice2-u_oce2(ji,jj))**2 + & |
---|
| 575 | (v_ice(ji,jj)-v_oce2(ji,jj))**2)*(1.0-zfrld2(ji,jj)) |
---|
| 576 | zr = z0*v_ice(ji,jj) + zf2(ji,jj) + & |
---|
| 577 | za2ct(ji,jj) + za*(cangvg*v_oce2(ji,jj)+zsang*u_oce2(ji,jj)) |
---|
[825] | 578 | zcca = z0+za*cangvg |
---|
| 579 | zccb = zcorl2(ji,jj)+za*zsang |
---|
| 580 | v_ice(ji,jj) = (zr-zccb*zu_ice2)/(zcca+epsd)*zmask |
---|
| 581 | |
---|
| 582 | END DO |
---|
| 583 | END DO |
---|
| 584 | |
---|
| 585 | CALL lbc_lnk( v_ice(:,:), 'V', -1. ) |
---|
| 586 | |
---|
| 587 | DO jj = k_j1+1, k_jpj-1 |
---|
| 588 | DO ji = 2, jpim1 |
---|
[834] | 589 | zmask = (1.0-MAX(rzero,SIGN(rone,-zmass1(ji,jj))))*tmu(ji,jj) |
---|
| 590 | zsang = SIGN(1.0,fcor(ji,jj))*sangvg |
---|
[825] | 591 | z0 = zmass1(ji,jj)/dtevp |
---|
| 592 | ! SB modif because ocean has no slip boundary condition |
---|
[866] | 593 | ! GG Bug |
---|
| 594 | ! zv_ice1 = 0.5*( (v_ice(ji,jj)+v_ice(ji,jj-1))*e1t(ji+1,jj) & |
---|
| 595 | ! & +(v_ice(ji+1,jj)+v_ice(ji+1,jj-1))*e1t(ji,jj)) & |
---|
| 596 | ! & /(e1t(ji+1,jj)+e1t(ji,jj)) * tmu(ji,jj) |
---|
| 597 | zv_ice1 = 0.5*( (v_ice(ji,jj)+v_ice(ji,jj-1))*e1t(ji,jj) & |
---|
| 598 | & +(v_ice(ji+1,jj)+v_ice(ji+1,jj-1))*e1t(ji+1,jj)) & |
---|
[825] | 599 | & /(e1t(ji+1,jj)+e1t(ji,jj)) * tmu(ji,jj) |
---|
| 600 | |
---|
[834] | 601 | za = rhoco*SQRT((u_ice(ji,jj)-u_oce1(ji,jj))**2 + & |
---|
| 602 | (zv_ice1-v_oce1(ji,jj))**2)*(1.0-zfrld1(ji,jj)) |
---|
| 603 | zr = z0*u_ice(ji,jj) + zf1(ji,jj) + za1ct(ji,jj) + & |
---|
| 604 | za*(cangvg*u_oce1(ji,jj)-zsang*v_oce1(ji,jj)) |
---|
[825] | 605 | zcca = z0+za*cangvg |
---|
| 606 | zccb = zcorl1(ji,jj)+za*zsang |
---|
| 607 | u_ice(ji,jj) = (zr+zccb*zv_ice1)/(zcca+epsd)*zmask |
---|
[834] | 608 | END DO ! ji |
---|
| 609 | END DO ! jj |
---|
[825] | 610 | |
---|
| 611 | CALL lbc_lnk( u_ice(:,:), 'U', -1. ) |
---|
| 612 | |
---|
[834] | 613 | ENDIF |
---|
[825] | 614 | |
---|
[834] | 615 | !--- Convergence test. |
---|
| 616 | DO jj = k_j1+1 , k_jpj-1 |
---|
| 617 | zresr(:,jj) = MAX( ABS( u_ice(:,jj) - zu_ice(:,jj) ) , & |
---|
| 618 | ABS( v_ice(:,jj) - zv_ice(:,jj) ) ) |
---|
| 619 | END DO |
---|
| 620 | zresm = MAXVAL( zresr( 1:jpi , k_j1+1:k_jpj-1 ) ) |
---|
[825] | 621 | |
---|
| 622 | ! ! ==================== ! |
---|
| 623 | END DO ! end loop over iter ! |
---|
| 624 | ! ! ==================== ! |
---|
| 625 | |
---|
[834] | 626 | ! |
---|
| 627 | !------------------------------------------------------------------------------! |
---|
| 628 | ! 4) Prevent ice velocities when the ice is thin |
---|
| 629 | !------------------------------------------------------------------------------! |
---|
| 630 | ! |
---|
[825] | 631 | ! If the ice thickness is below 1cm then ice velocity should equal the |
---|
[834] | 632 | ! ocean velocity, |
---|
| 633 | ! This prevents high velocity when ice is thin |
---|
[825] | 634 | DO jj = k_j1+1, k_jpj-1 |
---|
| 635 | DO ji = 2, jpim1 |
---|
| 636 | zindb = MAX( 0.0, SIGN( 1.0, at_i(ji,jj) - 1.0e-6 ) ) |
---|
| 637 | zdummy = zindb * vt_i(ji,jj) / MAX(at_i(ji,jj) , 1.0e-06 ) |
---|
| 638 | IF ( zdummy .LE. 5.0e-2 ) THEN |
---|
| 639 | u_ice(ji,jj) = u_io(ji,jj) |
---|
| 640 | v_ice(ji,jj) = v_io(ji,jj) |
---|
| 641 | ENDIF ! zdummy |
---|
| 642 | END DO |
---|
| 643 | END DO |
---|
[866] | 644 | |
---|
| 645 | ! Recompute delta, shear and div, inputs for mechanical redistribution |
---|
[825] | 646 | DO jj = k_j1+1, k_jpj-1 |
---|
| 647 | DO ji = 2, jpim1 |
---|
| 648 | !- zdd(:,:), zdt(:,:): divergence and tension at centre |
---|
| 649 | !- zds(:,:): shear on northeast corner of grid cells |
---|
| 650 | zindb = MAX( 0.0, SIGN( 1.0, at_i(ji,jj) - 1.0e-6 ) ) |
---|
| 651 | zdummy = zindb * vt_i(ji,jj) / MAX(at_i(ji,jj) , 1.0e-06 ) |
---|
| 652 | |
---|
| 653 | IF ( zdummy .LE. 5.0e-2 ) THEN |
---|
| 654 | |
---|
| 655 | zdd(ji,jj) = ( e2u(ji,jj)*u_ice(ji,jj) & |
---|
| 656 | & -e2u(ji-1,jj)*u_ice(ji-1,jj) & |
---|
| 657 | & +e1v(ji,jj)*v_ice(ji,jj) & |
---|
| 658 | & -e1v(ji,jj-1)*v_ice(ji,jj-1) & |
---|
| 659 | & ) & |
---|
| 660 | & / area(ji,jj) |
---|
| 661 | |
---|
| 662 | zdt(ji,jj) = ( ( u_ice(ji,jj)/e2u(ji,jj) & |
---|
| 663 | & -u_ice(ji-1,jj)/e2u(ji-1,jj) & |
---|
| 664 | & )*e2t(ji,jj)*e2t(ji,jj) & |
---|
| 665 | & -( v_ice(ji,jj)/e1v(ji,jj) & |
---|
| 666 | & -v_ice(ji,jj-1)/e1v(ji,jj-1) & |
---|
| 667 | & )*e1t(ji,jj)*e1t(ji,jj) & |
---|
| 668 | & ) & |
---|
| 669 | & / area(ji,jj) |
---|
| 670 | ! |
---|
| 671 | ! SB modif because ocean has no slip boundary condition |
---|
| 672 | zds(ji,jj) = ( ( u_ice(ji,jj+1) / e1u(ji,jj+1) & |
---|
| 673 | & - u_ice(ji,jj) / e1u(ji,jj) ) & |
---|
| 674 | & * e1f(ji,jj) * e1f(ji,jj) & |
---|
| 675 | & + ( v_ice(ji+1,jj) / e2v(ji+1,jj) & |
---|
| 676 | & - v_ice(ji,jj) / e2v(ji,jj) ) & |
---|
| 677 | & * e2f(ji,jj) * e2f(ji,jj) ) & |
---|
| 678 | & / ( e1f(ji,jj) * e2f(ji,jj) ) * ( 2.0 - tmf(ji,jj) ) & |
---|
| 679 | & * tmi(ji,jj) * tmi(ji,jj+1) & |
---|
| 680 | & * tmi(ji+1,jj) * tmi(ji+1,jj+1) |
---|
| 681 | |
---|
| 682 | !- Calculate Delta at centre of grid cells |
---|
| 683 | v_ice1(ji,jj) = 0.5*( (v_ice(ji,jj)+v_ice(ji,jj-1))*e1t(ji+1,jj) & |
---|
| 684 | & +(v_ice(ji+1,jj)+v_ice(ji+1,jj-1))*e1t(ji,jj)) & |
---|
| 685 | & /(e1t(ji+1,jj)+e1t(ji,jj)) * tmu(ji,jj) |
---|
| 686 | |
---|
| 687 | u_ice2(ji,jj) = 0.5*( (u_ice(ji,jj)+u_ice(ji-1,jj))*e2t(ji,jj+1) & |
---|
| 688 | & +(u_ice(ji,jj+1)+u_ice(ji-1,jj+1))*e2t(ji,jj)) & |
---|
| 689 | & /(e2t(ji,jj+1)+e2t(ji,jj)) * tmv(ji,jj) |
---|
| 690 | |
---|
| 691 | zdst = ( e2u( ji , jj ) * v_ice1(ji,jj) & |
---|
| 692 | & - e2u( ji-1, jj ) * v_ice1(ji-1,jj) & |
---|
| 693 | & + e1v( ji , jj ) * u_ice2(ji,jj) & |
---|
| 694 | & - e1v( ji , jj-1 ) * u_ice2(ji,jj-1) & |
---|
| 695 | & ) & |
---|
| 696 | & / area(ji,jj) |
---|
| 697 | |
---|
| 698 | deltat(ji,jj) = SQRT( zdd(ji,jj)*zdd(ji,jj) + & |
---|
| 699 | & ( zdt(ji,jj)*zdt(ji,jj) + zdst*zdst ) * usecc2 & |
---|
| 700 | & ) + creepl |
---|
| 701 | |
---|
| 702 | ENDIF ! zdummy |
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| 703 | |
---|
| 704 | END DO !jj |
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| 705 | END DO !ji |
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[866] | 706 | ! |
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| 707 | !------------------------------------------------------------------------------! |
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| 708 | ! 5) Store stress tensor and its invariants |
---|
| 709 | !------------------------------------------------------------------------------! |
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| 710 | ! |
---|
| 711 | ! * Invariants of the stress tensor are required for limitd_me |
---|
| 712 | ! * Store the stress tensor for the next time step |
---|
| 713 | ! accelerates convergence and improves stability |
---|
| 714 | DO jj = k_j1+1, k_jpj-1 |
---|
| 715 | DO ji = 2, jpim1 |
---|
| 716 | divu_i(ji,jj) = zdd(ji,jj) |
---|
| 717 | delta_i(ji,jj) = deltat (ji,jj) |
---|
| 718 | shear_i(ji,jj) = zds (ji,jj) |
---|
| 719 | stress1_i(ji,jj) = zs1(ji,jj) |
---|
| 720 | stress2_i(ji,jj) = zs2(ji,jj) |
---|
| 721 | stress12_i(ji,jj) = zs12(ji,jj) |
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[825] | 722 | END DO |
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[866] | 723 | END DO |
---|
[825] | 724 | |
---|
[866] | 725 | ! Lateral boundary condition |
---|
[825] | 726 | CALL lbc_lnk( divu_i(:,:) , 'T', 1. ) |
---|
| 727 | CALL lbc_lnk( delta_i(:,:), 'T', 1. ) |
---|
| 728 | CALL lbc_lnk( shear_i(:,:), 'F', 1. ) |
---|
| 729 | CALL lbc_lnk( stress1_i(:,:), 'T', 1. ) |
---|
| 730 | CALL lbc_lnk( stress2_i(:,:), 'T', 1. ) |
---|
| 731 | CALL lbc_lnk( stress12_i(:,:), 'F', 1. ) |
---|
[866] | 732 | |
---|
[834] | 733 | ! |
---|
| 734 | !------------------------------------------------------------------------------! |
---|
| 735 | ! 6) Control prints of residual and charge ellipse |
---|
| 736 | !------------------------------------------------------------------------------! |
---|
| 737 | ! |
---|
| 738 | ! print the residual for convergence |
---|
| 739 | IF(ln_ctl) THEN |
---|
| 740 | WRITE(charout,FMT="('lim_rhg : res =',D23.16, ' iter =',I4)") zresm, iter |
---|
| 741 | CALL prt_ctl_info(charout) |
---|
| 742 | CALL prt_ctl(tab2d_1=u_ice, clinfo1=' lim_rhg : u_ice :', tab2d_2=v_ice, clinfo2=' v_ice :') |
---|
| 743 | ENDIF |
---|
[825] | 744 | |
---|
[834] | 745 | ! print charge ellipse |
---|
| 746 | ! This can be desactivated once the user is sure that the stress state |
---|
| 747 | ! lie on the charge ellipse. See Bouillon et al. 08 for more details |
---|
[825] | 748 | IF(ln_ctl) THEN |
---|
| 749 | CALL prt_ctl_info('lim_rhg : numit :',ivar1=numit) |
---|
| 750 | CALL prt_ctl_info('lim_rhg : nwrite :',ivar1=nwrite) |
---|
| 751 | CALL prt_ctl_info('lim_rhg : MOD :',ivar1=MOD(numit,nwrite)) |
---|
| 752 | IF( MOD(numit,nwrite) .EQ. 0 ) THEN |
---|
| 753 | WRITE(charout,FMT="('lim_rhg :', I4, I6, I1, I1, A10)") 1000, numit, 0, 0, ' ch. ell. ' |
---|
| 754 | CALL prt_ctl_info(charout) |
---|
| 755 | DO jj = k_j1+1, k_jpj-1 |
---|
| 756 | DO ji = 2, jpim1 |
---|
| 757 | IF (zpresh(ji,jj) .GT. 1.0) THEN |
---|
| 758 | sigma1 = ( zs1(ji,jj) + (zs2(ji,jj)**2 + 4*zs12(ji,jj)**2 )**0.5 ) / ( 2*zpresh(ji,jj) ) |
---|
| 759 | sigma2 = ( zs1(ji,jj) - (zs2(ji,jj)**2 + 4*zs12(ji,jj)**2 )**0.5 ) / ( 2*zpresh(ji,jj) ) |
---|
| 760 | WRITE(charout,FMT="('lim_rhg :', I4, I4, D23.16, D23.16, D23.16, D23.16, A10)") |
---|
| 761 | CALL prt_ctl_info(charout) |
---|
| 762 | ENDIF |
---|
| 763 | END DO |
---|
| 764 | END DO |
---|
| 765 | WRITE(charout,FMT="('lim_rhg :', I4, I6, I1, I1, A10)") 2000, numit, 0, 0, ' ch. ell. ' |
---|
| 766 | CALL prt_ctl_info(charout) |
---|
| 767 | ENDIF |
---|
| 768 | ENDIF |
---|
| 769 | |
---|
| 770 | END SUBROUTINE lim_rhg |
---|
| 771 | |
---|
| 772 | #else |
---|
| 773 | !!---------------------------------------------------------------------- |
---|
| 774 | !! Default option Dummy module NO LIM sea-ice model |
---|
| 775 | !!---------------------------------------------------------------------- |
---|
| 776 | CONTAINS |
---|
| 777 | SUBROUTINE lim_rhg( k1 , k2 ) ! Dummy routine |
---|
| 778 | WRITE(*,*) 'lim_rhg: You should not have seen this print! error?', k1, k2 |
---|
| 779 | END SUBROUTINE lim_rhg |
---|
| 780 | #endif |
---|
| 781 | |
---|
| 782 | !!============================================================================== |
---|
| 783 | END MODULE limrhg |
---|