[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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[1244] | 6 | !! History : - ! 2007-03 (M.A. Morales Maqueda, S. Bouillon) Original code |
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| 7 | !! 3.0 ! 2008-03 (M. Vancoppenolle) LIM3 |
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| 8 | !! - ! 2008-11 (M. Vancoppenolle, S. Bouillon, Y. Aksenov) add surface tilt in ice rheolohy |
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| 9 | !!---------------------------------------------------------------------- |
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[825] | 10 | #if defined key_lim3 |
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| 11 | !!---------------------------------------------------------------------- |
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[834] | 12 | !! 'key_lim3' LIM3 sea-ice model |
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[825] | 13 | !!---------------------------------------------------------------------- |
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| 14 | !! lim_rhg : computes ice velocities |
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| 15 | !!---------------------------------------------------------------------- |
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| 16 | !! * Modules used |
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| 17 | USE phycst |
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| 18 | USE par_oce |
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| 19 | USE dom_oce |
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| 20 | USE dom_ice |
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[1244] | 21 | USE sbc_oce ! Surface boundary condition: ocean fields |
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[888] | 22 | USE sbc_ice ! Surface boundary condition: ice fields |
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[825] | 23 | USE ice |
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| 24 | USE iceini |
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| 25 | USE lbclnk |
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| 26 | USE lib_mpp |
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| 27 | USE in_out_manager ! I/O manager |
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| 28 | USE limitd_me |
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| 29 | USE prtctl ! Print control |
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| 30 | |
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| 31 | |
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| 32 | IMPLICIT NONE |
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| 33 | PRIVATE |
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| 34 | |
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| 35 | !! * Routine accessibility |
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| 36 | PUBLIC lim_rhg ! routine called by lim_dyn |
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| 37 | |
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[868] | 38 | !! * Substitutions |
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| 39 | # include "vectopt_loop_substitute.h90" |
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| 40 | |
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[825] | 41 | !! * Module variables |
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| 42 | REAL(wp) :: & ! constant values |
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| 43 | rzero = 0.e0 , & |
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| 44 | rone = 1.e0 |
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| 45 | !!---------------------------------------------------------------------- |
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[834] | 46 | !! LIM 3.0, UCL-LOCEAN-IPSL (2008) |
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[1156] | 47 | !! $Id$ |
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[888] | 48 | !! Software governed by the CeCILL licence (modipsl/doc/NEMO_CeCILL.txt) |
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[825] | 49 | !!---------------------------------------------------------------------- |
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| 50 | |
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| 51 | CONTAINS |
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| 52 | |
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| 53 | SUBROUTINE lim_rhg( k_j1, k_jpj ) |
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[834] | 54 | |
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[825] | 55 | !!------------------------------------------------------------------- |
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[834] | 56 | !! *** SUBROUTINE lim_rhg *** |
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| 57 | !! EVP-C-grid |
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[825] | 58 | !! |
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[834] | 59 | !! ** purpose : determines sea ice drift from wind stress, ice-ocean |
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[825] | 60 | !! stress and sea-surface slope. Ice-ice interaction is described by |
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[834] | 61 | !! a non-linear elasto-viscous-plastic (EVP) law including shear |
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| 62 | !! strength and a bulk rheology (Hunke and Dukowicz, 2002). |
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[825] | 63 | !! |
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[834] | 64 | !! The points in the C-grid look like this, dear reader |
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[825] | 65 | !! |
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[834] | 66 | !! (ji,jj) |
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| 67 | !! | |
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| 68 | !! | |
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| 69 | !! (ji-1,jj) | (ji,jj) |
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| 70 | !! --------- |
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| 71 | !! | | |
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| 72 | !! | (ji,jj) |------(ji,jj) |
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| 73 | !! | | |
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| 74 | !! --------- |
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| 75 | !! (ji-1,jj-1) (ji,jj-1) |
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[825] | 76 | !! |
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[834] | 77 | !! ** Inputs : - wind forcing (stress), oceanic currents |
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| 78 | !! ice total volume (vt_i) per unit area |
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| 79 | !! snow total volume (vt_s) per unit area |
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[825] | 80 | !! |
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[834] | 81 | !! ** Action : - compute u_ice, v_ice : the components of the |
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| 82 | !! sea-ice velocity vector |
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| 83 | !! - compute delta_i, shear_i, divu_i, which are inputs |
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| 84 | !! of the ice thickness distribution |
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[825] | 85 | !! |
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[834] | 86 | !! ** Steps : 1) Compute ice snow mass, ice strength |
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| 87 | !! 2) Compute wind, oceanic stresses, mass terms and |
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| 88 | !! coriolis terms of the momentum equation |
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| 89 | !! 3) Solve the momentum equation (iterative procedure) |
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| 90 | !! 4) Prevent high velocities if the ice is thin |
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| 91 | !! 5) Recompute invariants of the strain rate tensor |
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| 92 | !! which are inputs of the ITD, store stress |
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| 93 | !! for the next time step |
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| 94 | !! 6) Control prints of residual (convergence) |
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| 95 | !! and charge ellipse. |
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| 96 | !! The user should make sure that the parameters |
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| 97 | !! nevp, telast and creepl maintain stress state |
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| 98 | !! on the charge ellipse for plastic flow |
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| 99 | !! e.g. in the Canadian Archipelago |
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| 100 | !! |
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| 101 | !! ** References : Hunke and Dukowicz, JPO97 |
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| 102 | !! Bouillon et al., 08, in prep (update this when |
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| 103 | !! published) |
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| 104 | !! Vancoppenolle et al., OM08 |
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| 105 | !! |
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[825] | 106 | !!------------------------------------------------------------------- |
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| 107 | ! * Arguments |
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| 108 | ! |
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| 109 | INTEGER, INTENT(in) :: & |
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[834] | 110 | k_j1 , & !: southern j-index for ice computation |
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| 111 | k_jpj !: northern j-index for ice computation |
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[825] | 112 | |
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| 113 | ! * Local variables |
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[834] | 114 | INTEGER :: ji, jj !: dummy loop indices |
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[825] | 115 | |
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| 116 | INTEGER :: & |
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[868] | 117 | jter !: temporary integers |
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[825] | 118 | |
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| 119 | CHARACTER (len=50) :: charout |
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| 120 | |
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| 121 | REAL(wp) :: & |
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[834] | 122 | zt11, zt12, zt21, zt22, & !: temporary scalars |
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| 123 | ztagnx, ztagny, & !: wind stress on U/V points |
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| 124 | delta ! |
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[825] | 125 | |
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| 126 | REAL(wp) :: & |
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[834] | 127 | za, & !: |
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| 128 | zstms, & !: temporary scalar for ice strength |
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| 129 | zsang, & !: temporary scalar for coriolis term |
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| 130 | zmask !: mask for the computation of ice mass |
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[825] | 131 | |
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[834] | 132 | REAL(wp),DIMENSION(jpi,jpj) :: & |
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| 133 | zpresh , & !: temporary array for ice strength |
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| 134 | zpreshc , & !: Ice strength on grid cell corners (zpreshc) |
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| 135 | zfrld1, zfrld2, & !: lead fraction on U/V points |
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| 136 | zmass1, zmass2, & !: ice/snow mass on U/V points |
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| 137 | zcorl1, zcorl2, & !: coriolis parameter on U/V points |
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| 138 | za1ct, za2ct , & !: temporary arrays |
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| 139 | zc1 , & !: ice mass |
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| 140 | zusw , & !: temporary weight for the computation |
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[921] | 141 | !: of ice strength |
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[834] | 142 | u_oce1, v_oce1, & !: ocean u/v component on U points |
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| 143 | u_oce2, v_oce2, & !: ocean u/v component on V points |
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| 144 | u_ice2, & !: ice u component on V point |
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| 145 | v_ice1 !: ice v component on U point |
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[825] | 146 | |
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| 147 | REAL(wp) :: & |
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[834] | 148 | dtevp, & !: time step for subcycling |
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| 149 | dtotel, & !: |
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| 150 | ecc2, & !: square of yield ellipse eccenticity |
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| 151 | z0, & !: temporary scalar |
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| 152 | zr, & !: temporary scalar |
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| 153 | zcca, zccb, & !: temporary scalars |
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| 154 | zu_ice2, & !: |
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| 155 | zv_ice1, & !: |
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| 156 | zddc, zdtc, & !: temporary array for delta on corners |
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| 157 | zdst, & !: temporary array for delta on centre |
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| 158 | zdsshx, zdsshy, & !: term for the gradient of ocean surface |
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| 159 | sigma1, sigma2 !: internal ice stress |
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[825] | 160 | |
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[834] | 161 | REAL(wp),DIMENSION(jpi,jpj) :: & |
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| 162 | zf1, zf2 !: arrays for internal stresses |
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[825] | 163 | |
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[834] | 164 | REAL(wp),DIMENSION(jpi,jpj) :: & |
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| 165 | zdd, zdt, & !: Divergence and tension at centre of grid cells |
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| 166 | zds, & !: Shear on northeast corner of grid cells |
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| 167 | deltat, & !: Delta at centre of grid cells |
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| 168 | deltac, & !: Delta on corners |
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| 169 | zs1, zs2, & !: Diagonal stress tensor components zs1 and zs2 |
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| 170 | zs12 !: Non-diagonal stress tensor component zs12 |
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[825] | 171 | |
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[834] | 172 | REAL(wp) :: & |
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| 173 | zresm , & !: Maximal error on ice velocity |
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| 174 | zindb , & !: ice (1) or not (0) |
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| 175 | zdummy !: dummy argument |
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[825] | 176 | |
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[834] | 177 | REAL(wp),DIMENSION(jpi,jpj) :: & |
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| 178 | zu_ice , & !: Ice velocity on previous time step |
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| 179 | zv_ice , & |
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| 180 | zresr !: Local error on velocity |
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[825] | 181 | |
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[921] | 182 | ! |
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| 183 | !------------------------------------------------------------------------------! |
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| 184 | ! 1) Ice-Snow mass (zc1), ice strength (zpresh) ! |
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| 185 | !------------------------------------------------------------------------------! |
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| 186 | ! |
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[825] | 187 | ! Put every vector to 0 |
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[868] | 188 | zpresh(:,:) = 0.0 ; zc1(:,:) = 0.0 |
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| 189 | zpreshc(:,:) = 0.0 |
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| 190 | u_ice2(:,:) = 0.0 ; v_ice1(:,:) = 0.0 |
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[825] | 191 | zdd(:,:) = 0.0 ; zdt(:,:) = 0.0 ; zds(:,:) = 0.0 |
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| 192 | |
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[834] | 193 | ! Ice strength on T-points |
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[825] | 194 | CALL lim_itd_me_icestrength(ridge_scheme_swi) |
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| 195 | |
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[834] | 196 | ! Ice mass and temp variables |
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[868] | 197 | !CDIR NOVERRCHK |
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| 198 | DO jj = k_j1 , k_jpj |
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| 199 | !CDIR NOVERRCHK |
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[825] | 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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[921] | 205 | epsd ) ) ) * tms(ji,jj) |
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[825] | 206 | END DO |
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| 207 | END DO |
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| 208 | |
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[834] | 209 | ! Ice strength on grid cell corners (zpreshc) |
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| 210 | ! needed for calculation of shear stress |
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[868] | 211 | !CDIR NOVERRCHK |
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[825] | 212 | DO jj = k_j1+1, k_jpj-1 |
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[868] | 213 | !CDIR NOVERRCHK |
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| 214 | DO ji = 2, jpim1 !RB caution no fs_ (ji+1,jj+1) |
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[921] | 215 | zstms = tms(ji+1,jj+1) * wght(ji+1,jj+1,2,2) + & |
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| 216 | & tms(ji,jj+1) * wght(ji+1,jj+1,1,2) + & |
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| 217 | & tms(ji+1,jj) * wght(ji+1,jj+1,2,1) + & |
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| 218 | & tms(ji,jj) * wght(ji+1,jj+1,1,1) |
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| 219 | zusw(ji,jj) = 1.0 / MAX( zstms, epsd ) |
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| 220 | zpreshc(ji,jj) = ( zpresh(ji+1,jj+1) * wght(ji+1,jj+1,2,2) + & |
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| 221 | & zpresh(ji,jj+1) * wght(ji+1,jj+1,1,2) + & |
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| 222 | & zpresh(ji+1,jj) * wght(ji+1,jj+1,2,1) + & |
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| 223 | & zpresh(ji,jj) * wght(ji+1,jj+1,1,1) & |
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| 224 | & ) * zusw(ji,jj) |
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[825] | 225 | END DO |
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| 226 | END DO |
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| 227 | |
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| 228 | CALL lbc_lnk( zpreshc(:,:), 'F', 1. ) |
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[921] | 229 | ! |
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| 230 | !------------------------------------------------------------------------------! |
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| 231 | ! 2) Wind / ocean stress, mass terms, coriolis terms |
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| 232 | !------------------------------------------------------------------------------! |
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| 233 | ! |
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[825] | 234 | ! Wind stress, coriolis and mass terms on the sides of the squares |
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| 235 | ! zfrld1: lead fraction on U-points |
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| 236 | ! zfrld2: lead fraction on V-points |
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| 237 | ! zmass1: ice/snow mass on U-points |
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| 238 | ! zmass2: ice/snow mass on V-points |
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| 239 | ! zcorl1: Coriolis parameter on U-points |
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| 240 | ! zcorl2: Coriolis parameter on V-points |
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| 241 | ! (ztagnx,ztagny): wind stress on U/V points |
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| 242 | ! u_oce1: ocean u component on u points |
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| 243 | ! v_oce1: ocean v component on u points |
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| 244 | ! u_oce2: ocean u component on v points |
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| 245 | ! v_oce2: ocean v component on v points |
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[921] | 246 | |
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[825] | 247 | DO jj = k_j1+1, k_jpj-1 |
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[868] | 248 | DO ji = fs_2, fs_jpim1 |
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[825] | 249 | |
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| 250 | zt11 = tms(ji,jj)*e1t(ji,jj) |
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| 251 | zt12 = tms(ji+1,jj)*e1t(ji+1,jj) |
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| 252 | zt21 = tms(ji,jj)*e2t(ji,jj) |
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| 253 | zt22 = tms(ji,jj+1)*e2t(ji,jj+1) |
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| 254 | |
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| 255 | ! Leads area. |
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| 256 | zfrld1(ji,jj) = ( zt12 * ( 1.0 - at_i(ji,jj) ) + & |
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[921] | 257 | & zt11 * ( 1.0 - at_i(ji+1,jj) ) ) / ( zt11 + zt12 + epsd ) |
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[825] | 258 | zfrld2(ji,jj) = ( zt22 * ( 1.0 - at_i(ji,jj) ) + & |
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[921] | 259 | & zt21 * ( 1.0 - at_i(ji,jj+1) ) ) / ( zt21 + zt22 + epsd ) |
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[825] | 260 | |
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| 261 | ! Mass, coriolis coeff. and currents |
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[834] | 262 | zmass1(ji,jj) = ( zt12*zc1(ji,jj) + zt11*zc1(ji+1,jj) ) / (zt11+zt12+epsd) |
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| 263 | zmass2(ji,jj) = ( zt22*zc1(ji,jj) + zt21*zc1(ji,jj+1) ) / (zt21+zt22+epsd) |
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| 264 | zcorl1(ji,jj) = zmass1(ji,jj) * ( e1t(ji+1,jj)*fcor(ji,jj) + & |
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[921] | 265 | e1t(ji,jj)*fcor(ji+1,jj) ) & |
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| 266 | / (e1t(ji,jj) + e1t(ji+1,jj) + epsd ) |
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[834] | 267 | zcorl2(ji,jj) = zmass2(ji,jj) * ( e2t(ji,jj+1)*fcor(ji,jj) + & |
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[921] | 268 | e2t(ji,jj)*fcor(ji,jj+1) ) & |
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| 269 | / ( e2t(ji,jj+1) + e2t(ji,jj) + epsd ) |
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[825] | 270 | ! |
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[888] | 271 | u_oce1(ji,jj) = u_oce(ji,jj) |
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| 272 | v_oce2(ji,jj) = v_oce(ji,jj) |
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[825] | 273 | |
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[834] | 274 | ! Ocean has no slip boundary condition |
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[888] | 275 | v_oce1(ji,jj) = 0.5*( (v_oce(ji,jj)+v_oce(ji,jj-1))*e1t(ji,jj) & |
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[921] | 276 | & +(v_oce(ji+1,jj)+v_oce(ji+1,jj-1))*e1t(ji+1,jj)) & |
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| 277 | & /(e1t(ji+1,jj)+e1t(ji,jj)) * tmu(ji,jj) |
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[825] | 278 | |
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[888] | 279 | u_oce2(ji,jj) = 0.5*((u_oce(ji,jj)+u_oce(ji-1,jj))*e2t(ji,jj) & |
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[921] | 280 | & +(u_oce(ji,jj+1)+u_oce(ji-1,jj+1))*e2t(ji,jj+1)) & |
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| 281 | & / (e2t(ji,jj+1)+e2t(ji,jj)) * tmv(ji,jj) |
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[825] | 282 | |
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[1469] | 283 | ! Wind stress at U,V-point |
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| 284 | ztagnx = ( 1. - zfrld1(ji,jj) ) * utau_ice(ji,jj) |
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| 285 | ztagny = ( 1. - zfrld2(ji,jj) ) * vtau_ice(ji,jj) |
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[825] | 286 | |
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[834] | 287 | ! Computation of the velocity field taking into account the ice internal interaction. |
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[825] | 288 | ! Terms that are independent of the velocity field. |
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| 289 | |
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| 290 | ! SB On utilise maintenant le gradient de la pente de l'ocean |
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| 291 | ! include it later |
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[834] | 292 | |
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[1244] | 293 | zdsshx = (ssh_m(ji+1,jj) - ssh_m(ji,jj))/e1u(ji,jj) |
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| 294 | zdsshy = (ssh_m(ji,jj+1) - ssh_m(ji,jj))/e2v(ji,jj) |
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[825] | 295 | |
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| 296 | za1ct(ji,jj) = ztagnx - zmass1(ji,jj) * grav * zdsshx |
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| 297 | za2ct(ji,jj) = ztagny - zmass2(ji,jj) * grav * zdsshy |
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| 298 | |
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| 299 | END DO |
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| 300 | END DO |
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| 301 | |
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[921] | 302 | ! |
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| 303 | !------------------------------------------------------------------------------! |
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| 304 | ! 3) Solution of the momentum equation, iterative procedure |
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| 305 | !------------------------------------------------------------------------------! |
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| 306 | ! |
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[825] | 307 | ! Time step for subcycling |
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| 308 | dtevp = rdt_ice / nevp |
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| 309 | dtotel = dtevp / ( 2.0 * telast ) |
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| 310 | |
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| 311 | !-ecc2: square of yield ellipse eccenticrity (reminder: must become a namelist parameter) |
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| 312 | ecc2 = ecc*ecc |
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| 313 | |
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| 314 | !-Initialise stress tensor |
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[869] | 315 | zs1(:,:) = stress1_i(:,:) |
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[866] | 316 | zs2(:,:) = stress2_i(:,:) |
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| 317 | zs12(:,:) = stress12_i(:,:) |
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[825] | 318 | |
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[921] | 319 | !----------------------! |
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[868] | 320 | DO jter = 1 , nevp ! loop over jter ! |
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[921] | 321 | !----------------------! |
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[825] | 322 | DO jj = k_j1, k_jpj-1 |
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| 323 | zu_ice(:,jj) = u_ice(:,jj) ! velocity at previous time step |
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| 324 | zv_ice(:,jj) = v_ice(:,jj) |
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[921] | 325 | END DO |
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[825] | 326 | |
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[834] | 327 | DO jj = k_j1+1, k_jpj-1 |
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[988] | 328 | DO ji = fs_2, jpim1 !RB bug no vect opt due to tmi |
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[825] | 329 | |
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[921] | 330 | ! |
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| 331 | !- Divergence, tension and shear (Section a. Appendix B of Hunke & Dukowicz, 2002) |
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| 332 | !- zdd(:,:), zdt(:,:): divergence and tension at centre of grid cells |
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| 333 | !- zds(:,:): shear on northeast corner of grid cells |
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| 334 | ! |
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| 335 | !- IMPORTANT REMINDER: Dear Gurvan, note that, the way these terms are coded, |
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| 336 | ! there are many repeated calculations. |
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| 337 | ! Speed could be improved by regrouping terms. For |
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| 338 | ! the moment, however, the stress is on clarity of coding to avoid |
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| 339 | ! bugs (Martin, for Miguel). |
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| 340 | ! |
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| 341 | !- ALSO: arrays zdd, zdt, zds and delta could |
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| 342 | ! be removed in the future to minimise memory demand. |
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| 343 | ! |
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| 344 | !- MORE NOTES: Note that we are calculating deformation rates and stresses on the corners of |
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| 345 | ! grid cells, exactly as in the B grid case. For simplicity, the indexation on |
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| 346 | ! the corners is the same as in the B grid. |
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| 347 | ! |
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| 348 | ! |
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| 349 | zdd(ji,jj) = ( e2u(ji,jj)*u_ice(ji,jj) & |
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| 350 | & -e2u(ji-1,jj)*u_ice(ji-1,jj) & |
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| 351 | & +e1v(ji,jj)*v_ice(ji,jj) & |
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| 352 | & -e1v(ji,jj-1)*v_ice(ji,jj-1) & |
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| 353 | & ) & |
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| 354 | & / area(ji,jj) |
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[825] | 355 | |
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[921] | 356 | zdt(ji,jj) = ( ( u_ice(ji,jj)/e2u(ji,jj) & |
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| 357 | & -u_ice(ji-1,jj)/e2u(ji-1,jj) & |
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| 358 | & )*e2t(ji,jj)*e2t(ji,jj) & |
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| 359 | & -( v_ice(ji,jj)/e1v(ji,jj) & |
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| 360 | & -v_ice(ji,jj-1)/e1v(ji,jj-1) & |
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| 361 | & )*e1t(ji,jj)*e1t(ji,jj) & |
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| 362 | & ) & |
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| 363 | & / area(ji,jj) |
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[825] | 364 | |
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[921] | 365 | ! |
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| 366 | zds(ji,jj) = ( ( u_ice(ji,jj+1)/e1u(ji,jj+1) & |
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| 367 | & -u_ice(ji,jj)/e1u(ji,jj) & |
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| 368 | & )*e1f(ji,jj)*e1f(ji,jj) & |
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| 369 | & +( v_ice(ji+1,jj)/e2v(ji+1,jj) & |
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| 370 | & -v_ice(ji,jj)/e2v(ji,jj) & |
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| 371 | & )*e2f(ji,jj)*e2f(ji,jj) & |
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| 372 | & ) & |
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| 373 | & / ( e1f(ji,jj) * e2f(ji,jj) ) * ( 2.0 - tmf(ji,jj) ) & |
---|
| 374 | & * tmi(ji,jj) * tmi(ji,jj+1) & |
---|
| 375 | & * tmi(ji+1,jj) * tmi(ji+1,jj+1) |
---|
[825] | 376 | |
---|
| 377 | |
---|
[921] | 378 | v_ice1(ji,jj) = 0.5*( (v_ice(ji,jj)+v_ice(ji,jj-1))*e1t(ji+1,jj) & |
---|
| 379 | & +(v_ice(ji+1,jj)+v_ice(ji+1,jj-1))*e1t(ji,jj)) & |
---|
| 380 | & /(e1t(ji+1,jj)+e1t(ji,jj)) * tmu(ji,jj) |
---|
[825] | 381 | |
---|
[921] | 382 | u_ice2(ji,jj) = 0.5*( (u_ice(ji,jj)+u_ice(ji-1,jj))*e2t(ji,jj+1) & |
---|
| 383 | & +(u_ice(ji,jj+1)+u_ice(ji-1,jj+1))*e2t(ji,jj)) & |
---|
| 384 | & /(e2t(ji,jj+1)+e2t(ji,jj)) * tmv(ji,jj) |
---|
[825] | 385 | |
---|
[921] | 386 | END DO |
---|
| 387 | END DO |
---|
| 388 | CALL lbc_lnk( v_ice1(:,:), 'U', -1. ) |
---|
| 389 | CALL lbc_lnk( u_ice2(:,:), 'V', -1. ) |
---|
| 390 | |
---|
[868] | 391 | !CDIR NOVERRCHK |
---|
[921] | 392 | DO jj = k_j1+1, k_jpj-1 |
---|
[868] | 393 | !CDIR NOVERRCHK |
---|
[921] | 394 | DO ji = fs_2, fs_jpim1 |
---|
[825] | 395 | |
---|
[921] | 396 | !- Calculate Delta at centre of grid cells |
---|
| 397 | zdst = ( e2u( ji , jj ) * v_ice1(ji,jj) & |
---|
| 398 | & - e2u( ji-1, jj ) * v_ice1(ji-1,jj) & |
---|
| 399 | & + e1v( ji , jj ) * u_ice2(ji,jj) & |
---|
| 400 | & - e1v( ji , jj-1 ) * u_ice2(ji,jj-1) & |
---|
| 401 | & ) & |
---|
| 402 | & / area(ji,jj) |
---|
[825] | 403 | |
---|
[921] | 404 | delta = SQRT( zdd(ji,jj)*zdd(ji,jj) + & |
---|
| 405 | & ( zdt(ji,jj)*zdt(ji,jj) + zdst*zdst ) * usecc2 ) |
---|
| 406 | deltat(ji,jj) = MAX( SQRT(zdd(ji,jj)**2 + & |
---|
| 407 | (zdt(ji,jj)**2 + zdst**2)*usecc2), creepl ) |
---|
[825] | 408 | |
---|
[921] | 409 | !-Calculate stress tensor components zs1 and zs2 |
---|
| 410 | !-at centre of grid cells (see section 3.5 of CICE user's guide). |
---|
| 411 | zs1(ji,jj) = ( zs1(ji,jj) & |
---|
| 412 | & - dtotel*( ( 1.0 - alphaevp) * zs1(ji,jj) + & |
---|
| 413 | & ( delta / deltat(ji,jj) - zdd(ji,jj) / deltat(ji,jj) ) & |
---|
| 414 | * zpresh(ji,jj) ) ) & |
---|
| 415 | & / ( 1.0 + alphaevp * dtotel ) |
---|
[825] | 416 | |
---|
[921] | 417 | zs2(ji,jj) = ( zs2(ji,jj) & |
---|
| 418 | & - dtotel*((1.0-alphaevp)*ecc2*zs2(ji,jj) - & |
---|
| 419 | zdt(ji,jj)/deltat(ji,jj)*zpresh(ji,jj)) ) & |
---|
| 420 | & / ( 1.0 + alphaevp*ecc2*dtotel ) |
---|
[825] | 421 | |
---|
[921] | 422 | END DO |
---|
| 423 | END DO |
---|
[825] | 424 | |
---|
[921] | 425 | CALL lbc_lnk( zs1(:,:), 'T', 1. ) |
---|
| 426 | CALL lbc_lnk( zs2(:,:), 'T', 1. ) |
---|
[825] | 427 | |
---|
[868] | 428 | !CDIR NOVERRCHK |
---|
[921] | 429 | DO jj = k_j1+1, k_jpj-1 |
---|
[868] | 430 | !CDIR NOVERRCHK |
---|
[921] | 431 | DO ji = fs_2, fs_jpim1 |
---|
| 432 | !- Calculate Delta on corners |
---|
| 433 | zddc = ( ( v_ice1(ji,jj+1)/e1u(ji,jj+1) & |
---|
| 434 | & -v_ice1(ji,jj)/e1u(ji,jj) & |
---|
| 435 | & )*e1f(ji,jj)*e1f(ji,jj) & |
---|
| 436 | & +( u_ice2(ji+1,jj)/e2v(ji+1,jj) & |
---|
| 437 | & -u_ice2(ji,jj)/e2v(ji,jj) & |
---|
| 438 | & )*e2f(ji,jj)*e2f(ji,jj) & |
---|
| 439 | & ) & |
---|
| 440 | & / ( e1f(ji,jj) * e2f(ji,jj) ) |
---|
[825] | 441 | |
---|
[921] | 442 | zdtc = (-( v_ice1(ji,jj+1)/e1u(ji,jj+1) & |
---|
| 443 | & -v_ice1(ji,jj)/e1u(ji,jj) & |
---|
| 444 | & )*e1f(ji,jj)*e1f(ji,jj) & |
---|
| 445 | & +( u_ice2(ji+1,jj)/e2v(ji+1,jj) & |
---|
| 446 | & -u_ice2(ji,jj)/e2v(ji,jj) & |
---|
| 447 | & )*e2f(ji,jj)*e2f(ji,jj) & |
---|
| 448 | & ) & |
---|
| 449 | & / ( e1f(ji,jj) * e2f(ji,jj) ) |
---|
[825] | 450 | |
---|
[921] | 451 | deltac(ji,jj) = SQRT(zddc**2+(zdtc**2+zds(ji,jj)**2)*usecc2) + creepl |
---|
[825] | 452 | |
---|
[921] | 453 | !-Calculate stress tensor component zs12 at corners (see section 3.5 of CICE user's guide). |
---|
| 454 | zs12(ji,jj) = ( zs12(ji,jj) & |
---|
| 455 | & - dtotel*( (1.0-alphaevp)*ecc2*zs12(ji,jj) - zds(ji,jj) / & |
---|
| 456 | & ( 2.0*deltac(ji,jj) ) * zpreshc(ji,jj))) & |
---|
| 457 | & / ( 1.0 + alphaevp*ecc2*dtotel ) |
---|
[825] | 458 | |
---|
[921] | 459 | END DO ! ji |
---|
| 460 | END DO ! jj |
---|
[825] | 461 | |
---|
[921] | 462 | CALL lbc_lnk( zs12(:,:), 'F', 1. ) |
---|
[825] | 463 | |
---|
[921] | 464 | ! Ice internal stresses (Appendix C of Hunke and Dukowicz, 2002) |
---|
| 465 | DO jj = k_j1+1, k_jpj-1 |
---|
| 466 | DO ji = fs_2, fs_jpim1 |
---|
| 467 | !- contribution of zs1, zs2 and zs12 to zf1 |
---|
| 468 | zf1(ji,jj) = 0.5*( (zs1(ji+1,jj)-zs1(ji,jj))*e2u(ji,jj) & |
---|
| 469 | & +(zs2(ji+1,jj)*e2t(ji+1,jj)**2-zs2(ji,jj)*e2t(ji,jj)**2)/e2u(ji,jj) & |
---|
| 470 | & +2.0*(zs12(ji,jj)*e1f(ji,jj)**2-zs12(ji,jj-1)*e1f(ji,jj-1)**2)/e1u(ji,jj) & |
---|
| 471 | & ) / ( e1u(ji,jj)*e2u(ji,jj) ) |
---|
| 472 | ! contribution of zs1, zs2 and zs12 to zf2 |
---|
| 473 | zf2(ji,jj) = 0.5*( (zs1(ji,jj+1)-zs1(ji,jj))*e1v(ji,jj) & |
---|
| 474 | & -(zs2(ji,jj+1)*e1t(ji,jj+1)**2 - zs2(ji,jj)*e1t(ji,jj)**2)/e1v(ji,jj) & |
---|
| 475 | & + 2.0*(zs12(ji,jj)*e2f(ji,jj)**2 - & |
---|
| 476 | zs12(ji-1,jj)*e2f(ji-1,jj)**2)/e2v(ji,jj) & |
---|
| 477 | & ) / ( e1v(ji,jj)*e2v(ji,jj) ) |
---|
| 478 | END DO |
---|
| 479 | END DO |
---|
[825] | 480 | ! |
---|
| 481 | ! Computation of ice velocity |
---|
| 482 | ! |
---|
| 483 | ! Both the Coriolis term and the ice-ocean drag are solved semi-implicitly. |
---|
| 484 | ! |
---|
[921] | 485 | IF (MOD(jter,2).eq.0) THEN |
---|
[825] | 486 | |
---|
[868] | 487 | !CDIR NOVERRCHK |
---|
[921] | 488 | DO jj = k_j1+1, k_jpj-1 |
---|
[868] | 489 | !CDIR NOVERRCHK |
---|
[921] | 490 | DO ji = fs_2, fs_jpim1 |
---|
| 491 | zmask = (1.0-MAX(rzero,SIGN(rone,-zmass1(ji,jj))))*tmu(ji,jj) |
---|
| 492 | zsang = SIGN ( 1.0 , fcor(ji,jj) ) * sangvg |
---|
| 493 | z0 = zmass1(ji,jj)/dtevp |
---|
[825] | 494 | |
---|
[921] | 495 | ! SB modif because ocean has no slip boundary condition |
---|
| 496 | zv_ice1 = 0.5*( (v_ice(ji,jj)+v_ice(ji,jj-1))*e1t(ji,jj) & |
---|
| 497 | & +(v_ice(ji+1,jj)+v_ice(ji+1,jj-1))*e1t(ji+1,jj)) & |
---|
| 498 | & /(e1t(ji+1,jj)+e1t(ji,jj)) * tmu(ji,jj) |
---|
| 499 | za = rhoco*SQRT((u_ice(ji,jj)-u_oce1(ji,jj))**2 + & |
---|
| 500 | (zv_ice1-v_oce1(ji,jj))**2) * (1.0-zfrld1(ji,jj)) |
---|
| 501 | zr = z0*u_ice(ji,jj) + zf1(ji,jj) + za1ct(ji,jj) + & |
---|
| 502 | za*(cangvg*u_oce1(ji,jj)-zsang*v_oce1(ji,jj)) |
---|
| 503 | zcca = z0+za*cangvg |
---|
| 504 | zccb = zcorl1(ji,jj)+za*zsang |
---|
| 505 | u_ice(ji,jj) = (zr+zccb*zv_ice1)/(zcca+epsd)*zmask |
---|
[825] | 506 | |
---|
[921] | 507 | END DO |
---|
| 508 | END DO |
---|
[825] | 509 | |
---|
[921] | 510 | CALL lbc_lnk( u_ice(:,:), 'U', -1. ) |
---|
[825] | 511 | |
---|
[868] | 512 | !CDIR NOVERRCHK |
---|
[921] | 513 | DO jj = k_j1+1, k_jpj-1 |
---|
[868] | 514 | !CDIR NOVERRCHK |
---|
[921] | 515 | DO ji = fs_2, fs_jpim1 |
---|
[834] | 516 | |
---|
[921] | 517 | zmask = (1.0-MAX(rzero,SIGN(rone,-zmass2(ji,jj))))*tmv(ji,jj) |
---|
| 518 | zsang = SIGN(1.0,fcor(ji,jj))*sangvg |
---|
| 519 | z0 = zmass2(ji,jj)/dtevp |
---|
| 520 | ! SB modif because ocean has no slip boundary condition |
---|
| 521 | zu_ice2 = 0.5*( (u_ice(ji,jj)+u_ice(ji-1,jj))*e2t(ji,jj) & |
---|
| 522 | & + (u_ice(ji,jj+1)+u_ice(ji-1,jj+1))*e2t(ji,jj+1)) & |
---|
| 523 | & /(e2t(ji,jj+1)+e2t(ji,jj)) * tmv(ji,jj) |
---|
| 524 | za = rhoco*SQRT((zu_ice2-u_oce2(ji,jj))**2 + & |
---|
| 525 | (v_ice(ji,jj)-v_oce2(ji,jj))**2)*(1.0-zfrld2(ji,jj)) |
---|
| 526 | zr = z0*v_ice(ji,jj) + zf2(ji,jj) + & |
---|
| 527 | za2ct(ji,jj) + za*(cangvg*v_oce2(ji,jj)+zsang*u_oce2(ji,jj)) |
---|
| 528 | zcca = z0+za*cangvg |
---|
| 529 | zccb = zcorl2(ji,jj)+za*zsang |
---|
| 530 | v_ice(ji,jj) = (zr-zccb*zu_ice2)/(zcca+epsd)*zmask |
---|
[825] | 531 | |
---|
[921] | 532 | END DO |
---|
| 533 | END DO |
---|
[825] | 534 | |
---|
[921] | 535 | CALL lbc_lnk( v_ice(:,:), 'V', -1. ) |
---|
[825] | 536 | |
---|
[834] | 537 | ELSE |
---|
[868] | 538 | !CDIR NOVERRCHK |
---|
[921] | 539 | DO jj = k_j1+1, k_jpj-1 |
---|
[868] | 540 | !CDIR NOVERRCHK |
---|
[921] | 541 | DO ji = fs_2, fs_jpim1 |
---|
| 542 | zmask = (1.0-MAX(rzero,SIGN(rone,-zmass2(ji,jj))))*tmv(ji,jj) |
---|
| 543 | zsang = SIGN(1.0,fcor(ji,jj))*sangvg |
---|
| 544 | z0 = zmass2(ji,jj)/dtevp |
---|
| 545 | ! SB modif because ocean has no slip boundary condition |
---|
| 546 | zu_ice2 = 0.5*( (u_ice(ji,jj)+u_ice(ji-1,jj))*e2t(ji,jj) & |
---|
| 547 | & +(u_ice(ji,jj+1)+u_ice(ji-1,jj+1))*e2t(ji,jj+1)) & |
---|
| 548 | & /(e2t(ji,jj+1)+e2t(ji,jj)) * tmv(ji,jj) |
---|
[825] | 549 | |
---|
[921] | 550 | za = rhoco*SQRT((zu_ice2-u_oce2(ji,jj))**2 + & |
---|
| 551 | (v_ice(ji,jj)-v_oce2(ji,jj))**2)*(1.0-zfrld2(ji,jj)) |
---|
| 552 | zr = z0*v_ice(ji,jj) + zf2(ji,jj) + & |
---|
| 553 | za2ct(ji,jj) + za*(cangvg*v_oce2(ji,jj)+zsang*u_oce2(ji,jj)) |
---|
| 554 | zcca = z0+za*cangvg |
---|
| 555 | zccb = zcorl2(ji,jj)+za*zsang |
---|
| 556 | v_ice(ji,jj) = (zr-zccb*zu_ice2)/(zcca+epsd)*zmask |
---|
[825] | 557 | |
---|
[921] | 558 | END DO |
---|
| 559 | END DO |
---|
[825] | 560 | |
---|
[921] | 561 | CALL lbc_lnk( v_ice(:,:), 'V', -1. ) |
---|
[825] | 562 | |
---|
[868] | 563 | !CDIR NOVERRCHK |
---|
[921] | 564 | DO jj = k_j1+1, k_jpj-1 |
---|
[868] | 565 | !CDIR NOVERRCHK |
---|
[921] | 566 | DO ji = fs_2, fs_jpim1 |
---|
| 567 | zmask = (1.0-MAX(rzero,SIGN(rone,-zmass1(ji,jj))))*tmu(ji,jj) |
---|
| 568 | zsang = SIGN(1.0,fcor(ji,jj))*sangvg |
---|
| 569 | z0 = zmass1(ji,jj)/dtevp |
---|
| 570 | ! SB modif because ocean has no slip boundary condition |
---|
| 571 | ! GG Bug |
---|
| 572 | ! zv_ice1 = 0.5*( (v_ice(ji,jj)+v_ice(ji,jj-1))*e1t(ji+1,jj) & |
---|
| 573 | ! & +(v_ice(ji+1,jj)+v_ice(ji+1,jj-1))*e1t(ji,jj)) & |
---|
| 574 | ! & /(e1t(ji+1,jj)+e1t(ji,jj)) * tmu(ji,jj) |
---|
| 575 | zv_ice1 = 0.5*( (v_ice(ji,jj)+v_ice(ji,jj-1))*e1t(ji,jj) & |
---|
| 576 | & +(v_ice(ji+1,jj)+v_ice(ji+1,jj-1))*e1t(ji+1,jj)) & |
---|
| 577 | & /(e1t(ji+1,jj)+e1t(ji,jj)) * tmu(ji,jj) |
---|
[825] | 578 | |
---|
[921] | 579 | za = rhoco*SQRT((u_ice(ji,jj)-u_oce1(ji,jj))**2 + & |
---|
| 580 | (zv_ice1-v_oce1(ji,jj))**2)*(1.0-zfrld1(ji,jj)) |
---|
| 581 | zr = z0*u_ice(ji,jj) + zf1(ji,jj) + za1ct(ji,jj) + & |
---|
| 582 | za*(cangvg*u_oce1(ji,jj)-zsang*v_oce1(ji,jj)) |
---|
| 583 | zcca = z0+za*cangvg |
---|
| 584 | zccb = zcorl1(ji,jj)+za*zsang |
---|
| 585 | u_ice(ji,jj) = (zr+zccb*zv_ice1)/(zcca+epsd)*zmask |
---|
| 586 | END DO ! ji |
---|
| 587 | END DO ! jj |
---|
[825] | 588 | |
---|
[921] | 589 | CALL lbc_lnk( u_ice(:,:), 'U', -1. ) |
---|
[825] | 590 | |
---|
[921] | 591 | ENDIF |
---|
[825] | 592 | |
---|
[921] | 593 | IF(ln_ctl) THEN |
---|
| 594 | !--- Convergence test. |
---|
| 595 | DO jj = k_j1+1 , k_jpj-1 |
---|
| 596 | zresr(:,jj) = MAX( ABS( u_ice(:,jj) - zu_ice(:,jj) ) , & |
---|
| 597 | ABS( v_ice(:,jj) - zv_ice(:,jj) ) ) |
---|
| 598 | END DO |
---|
| 599 | zresm = MAXVAL( zresr( 1:jpi , k_j1+1:k_jpj-1 ) ) |
---|
| 600 | IF( lk_mpp ) CALL mpp_max( zresm ) ! max over the global domain |
---|
| 601 | ENDIF |
---|
| 602 | |
---|
| 603 | ! ! ==================== ! |
---|
[868] | 604 | END DO ! end loop over jter ! |
---|
[825] | 605 | ! ! ==================== ! |
---|
| 606 | |
---|
[921] | 607 | ! |
---|
| 608 | !------------------------------------------------------------------------------! |
---|
| 609 | ! 4) Prevent ice velocities when the ice is thin |
---|
| 610 | !------------------------------------------------------------------------------! |
---|
| 611 | ! |
---|
[825] | 612 | ! If the ice thickness is below 1cm then ice velocity should equal the |
---|
[834] | 613 | ! ocean velocity, |
---|
| 614 | ! This prevents high velocity when ice is thin |
---|
[868] | 615 | !CDIR NOVERRCHK |
---|
[825] | 616 | DO jj = k_j1+1, k_jpj-1 |
---|
[868] | 617 | !CDIR NOVERRCHK |
---|
| 618 | DO ji = fs_2, fs_jpim1 |
---|
[825] | 619 | zindb = MAX( 0.0, SIGN( 1.0, at_i(ji,jj) - 1.0e-6 ) ) |
---|
| 620 | zdummy = zindb * vt_i(ji,jj) / MAX(at_i(ji,jj) , 1.0e-06 ) |
---|
| 621 | IF ( zdummy .LE. 5.0e-2 ) THEN |
---|
[888] | 622 | u_ice(ji,jj) = u_oce(ji,jj) |
---|
| 623 | v_ice(ji,jj) = v_oce(ji,jj) |
---|
[825] | 624 | ENDIF ! zdummy |
---|
| 625 | END DO |
---|
| 626 | END DO |
---|
[866] | 627 | |
---|
[869] | 628 | CALL lbc_lnk( u_ice(:,:), 'U', -1. ) |
---|
| 629 | CALL lbc_lnk( v_ice(:,:), 'V', -1. ) |
---|
| 630 | |
---|
[868] | 631 | DO jj = k_j1+1, k_jpj-1 |
---|
| 632 | DO ji = fs_2, fs_jpim1 |
---|
| 633 | zindb = MAX( 0.0, SIGN( 1.0, at_i(ji,jj) - 1.0e-6 ) ) |
---|
| 634 | zdummy = zindb * vt_i(ji,jj) / MAX(at_i(ji,jj) , 1.0e-06 ) |
---|
| 635 | IF ( zdummy .LE. 5.0e-2 ) THEN |
---|
[921] | 636 | v_ice1(ji,jj) = 0.5*( (v_ice(ji,jj)+v_ice(ji,jj-1))*e1t(ji+1,jj) & |
---|
| 637 | & +(v_ice(ji+1,jj)+v_ice(ji+1,jj-1))*e1t(ji,jj)) & |
---|
| 638 | & /(e1t(ji+1,jj)+e1t(ji,jj)) * tmu(ji,jj) |
---|
[868] | 639 | |
---|
[921] | 640 | u_ice2(ji,jj) = 0.5*( (u_ice(ji,jj)+u_ice(ji-1,jj))*e2t(ji,jj+1) & |
---|
| 641 | & +(u_ice(ji,jj+1)+u_ice(ji-1,jj+1))*e2t(ji,jj)) & |
---|
| 642 | & /(e2t(ji,jj+1)+e2t(ji,jj)) * tmv(ji,jj) |
---|
| 643 | ENDIF ! zdummy |
---|
[868] | 644 | END DO |
---|
| 645 | END DO |
---|
| 646 | |
---|
[869] | 647 | CALL lbc_lnk( u_ice2(:,:), 'V', -1. ) |
---|
| 648 | CALL lbc_lnk( v_ice1(:,:), 'U', -1. ) |
---|
[868] | 649 | |
---|
[866] | 650 | ! Recompute delta, shear and div, inputs for mechanical redistribution |
---|
[868] | 651 | !CDIR NOVERRCHK |
---|
[825] | 652 | DO jj = k_j1+1, k_jpj-1 |
---|
[868] | 653 | !CDIR NOVERRCHK |
---|
[988] | 654 | DO ji = fs_2, jpim1 !RB bug no vect opt due to tmi |
---|
[825] | 655 | !- zdd(:,:), zdt(:,:): divergence and tension at centre |
---|
| 656 | !- zds(:,:): shear on northeast corner of grid cells |
---|
| 657 | zindb = MAX( 0.0, SIGN( 1.0, at_i(ji,jj) - 1.0e-6 ) ) |
---|
| 658 | zdummy = zindb * vt_i(ji,jj) / MAX(at_i(ji,jj) , 1.0e-06 ) |
---|
| 659 | |
---|
| 660 | IF ( zdummy .LE. 5.0e-2 ) THEN |
---|
| 661 | |
---|
[921] | 662 | zdd(ji,jj) = ( e2u(ji,jj)*u_ice(ji,jj) & |
---|
| 663 | & -e2u(ji-1,jj)*u_ice(ji-1,jj) & |
---|
| 664 | & +e1v(ji,jj)*v_ice(ji,jj) & |
---|
| 665 | & -e1v(ji,jj-1)*v_ice(ji,jj-1) & |
---|
| 666 | & ) & |
---|
| 667 | & / area(ji,jj) |
---|
[825] | 668 | |
---|
[921] | 669 | zdt(ji,jj) = ( ( u_ice(ji,jj)/e2u(ji,jj) & |
---|
| 670 | & -u_ice(ji-1,jj)/e2u(ji-1,jj) & |
---|
| 671 | & )*e2t(ji,jj)*e2t(ji,jj) & |
---|
| 672 | & -( v_ice(ji,jj)/e1v(ji,jj) & |
---|
| 673 | & -v_ice(ji,jj-1)/e1v(ji,jj-1) & |
---|
| 674 | & )*e1t(ji,jj)*e1t(ji,jj) & |
---|
| 675 | & ) & |
---|
| 676 | & / area(ji,jj) |
---|
| 677 | ! |
---|
| 678 | ! SB modif because ocean has no slip boundary condition |
---|
| 679 | zds(ji,jj) = ( ( u_ice(ji,jj+1) / e1u(ji,jj+1) & |
---|
| 680 | & - u_ice(ji,jj) / e1u(ji,jj) ) & |
---|
| 681 | & * e1f(ji,jj) * e1f(ji,jj) & |
---|
| 682 | & + ( v_ice(ji+1,jj) / e2v(ji+1,jj) & |
---|
| 683 | & - v_ice(ji,jj) / e2v(ji,jj) ) & |
---|
| 684 | & * e2f(ji,jj) * e2f(ji,jj) ) & |
---|
| 685 | & / ( e1f(ji,jj) * e2f(ji,jj) ) * ( 2.0 - tmf(ji,jj) ) & |
---|
| 686 | & * tmi(ji,jj) * tmi(ji,jj+1) & |
---|
| 687 | & * tmi(ji+1,jj) * tmi(ji+1,jj+1) |
---|
[825] | 688 | |
---|
[921] | 689 | zdst = ( e2u( ji , jj ) * v_ice1(ji,jj) & |
---|
| 690 | & - e2u( ji-1, jj ) * v_ice1(ji-1,jj) & |
---|
| 691 | & + e1v( ji , jj ) * u_ice2(ji,jj) & |
---|
| 692 | & - e1v( ji , jj-1 ) * u_ice2(ji,jj-1) & |
---|
| 693 | & ) & |
---|
| 694 | & / area(ji,jj) |
---|
[825] | 695 | |
---|
[921] | 696 | deltat(ji,jj) = SQRT( zdd(ji,jj)*zdd(ji,jj) + & |
---|
| 697 | & ( zdt(ji,jj)*zdt(ji,jj) + zdst*zdst ) * usecc2 & |
---|
| 698 | & ) + creepl |
---|
[825] | 699 | |
---|
[921] | 700 | ENDIF ! zdummy |
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[825] | 701 | |
---|
| 702 | END DO !jj |
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| 703 | END DO !ji |
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[921] | 704 | ! |
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| 705 | !------------------------------------------------------------------------------! |
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| 706 | ! 5) Store stress tensor and its invariants |
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| 707 | !------------------------------------------------------------------------------! |
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| 708 | ! |
---|
[866] | 709 | ! * Invariants of the stress tensor are required for limitd_me |
---|
| 710 | ! accelerates convergence and improves stability |
---|
| 711 | DO jj = k_j1+1, k_jpj-1 |
---|
[868] | 712 | DO ji = fs_2, fs_jpim1 |
---|
| 713 | divu_i (ji,jj) = zdd (ji,jj) |
---|
| 714 | delta_i(ji,jj) = deltat(ji,jj) |
---|
| 715 | shear_i(ji,jj) = zds (ji,jj) |
---|
[825] | 716 | END DO |
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[866] | 717 | END DO |
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[825] | 718 | |
---|
[866] | 719 | ! Lateral boundary condition |
---|
[868] | 720 | CALL lbc_lnk( divu_i (:,:), 'T', 1. ) |
---|
[825] | 721 | CALL lbc_lnk( delta_i(:,:), 'T', 1. ) |
---|
| 722 | CALL lbc_lnk( shear_i(:,:), 'F', 1. ) |
---|
[866] | 723 | |
---|
[868] | 724 | ! * Store the stress tensor for the next time step |
---|
| 725 | stress1_i (:,:) = zs1 (:,:) |
---|
| 726 | stress2_i (:,:) = zs2 (:,:) |
---|
| 727 | stress12_i(:,:) = zs12(:,:) |
---|
| 728 | |
---|
[921] | 729 | ! |
---|
| 730 | !------------------------------------------------------------------------------! |
---|
| 731 | ! 6) Control prints of residual and charge ellipse |
---|
| 732 | !------------------------------------------------------------------------------! |
---|
| 733 | ! |
---|
[834] | 734 | ! print the residual for convergence |
---|
| 735 | IF(ln_ctl) THEN |
---|
[868] | 736 | WRITE(charout,FMT="('lim_rhg : res =',D23.16, ' iter =',I4)") zresm, jter |
---|
[834] | 737 | CALL prt_ctl_info(charout) |
---|
| 738 | CALL prt_ctl(tab2d_1=u_ice, clinfo1=' lim_rhg : u_ice :', tab2d_2=v_ice, clinfo2=' v_ice :') |
---|
| 739 | ENDIF |
---|
[825] | 740 | |
---|
[834] | 741 | ! print charge ellipse |
---|
| 742 | ! This can be desactivated once the user is sure that the stress state |
---|
| 743 | ! lie on the charge ellipse. See Bouillon et al. 08 for more details |
---|
[825] | 744 | IF(ln_ctl) THEN |
---|
| 745 | CALL prt_ctl_info('lim_rhg : numit :',ivar1=numit) |
---|
| 746 | CALL prt_ctl_info('lim_rhg : nwrite :',ivar1=nwrite) |
---|
| 747 | CALL prt_ctl_info('lim_rhg : MOD :',ivar1=MOD(numit,nwrite)) |
---|
| 748 | IF( MOD(numit,nwrite) .EQ. 0 ) THEN |
---|
| 749 | WRITE(charout,FMT="('lim_rhg :', I4, I6, I1, I1, A10)") 1000, numit, 0, 0, ' ch. ell. ' |
---|
| 750 | CALL prt_ctl_info(charout) |
---|
| 751 | DO jj = k_j1+1, k_jpj-1 |
---|
| 752 | DO ji = 2, jpim1 |
---|
| 753 | IF (zpresh(ji,jj) .GT. 1.0) THEN |
---|
| 754 | sigma1 = ( zs1(ji,jj) + (zs2(ji,jj)**2 + 4*zs12(ji,jj)**2 )**0.5 ) / ( 2*zpresh(ji,jj) ) |
---|
| 755 | sigma2 = ( zs1(ji,jj) - (zs2(ji,jj)**2 + 4*zs12(ji,jj)**2 )**0.5 ) / ( 2*zpresh(ji,jj) ) |
---|
| 756 | WRITE(charout,FMT="('lim_rhg :', I4, I4, D23.16, D23.16, D23.16, D23.16, A10)") |
---|
| 757 | CALL prt_ctl_info(charout) |
---|
| 758 | ENDIF |
---|
| 759 | END DO |
---|
| 760 | END DO |
---|
| 761 | WRITE(charout,FMT="('lim_rhg :', I4, I6, I1, I1, A10)") 2000, numit, 0, 0, ' ch. ell. ' |
---|
| 762 | CALL prt_ctl_info(charout) |
---|
| 763 | ENDIF |
---|
| 764 | ENDIF |
---|
| 765 | |
---|
| 766 | END SUBROUTINE lim_rhg |
---|
| 767 | |
---|
| 768 | #else |
---|
| 769 | !!---------------------------------------------------------------------- |
---|
| 770 | !! Default option Dummy module NO LIM sea-ice model |
---|
| 771 | !!---------------------------------------------------------------------- |
---|
| 772 | CONTAINS |
---|
| 773 | SUBROUTINE lim_rhg( k1 , k2 ) ! Dummy routine |
---|
| 774 | WRITE(*,*) 'lim_rhg: You should not have seen this print! error?', k1, k2 |
---|
| 775 | END SUBROUTINE lim_rhg |
---|
| 776 | #endif |
---|
| 777 | |
---|
| 778 | !!============================================================================== |
---|
| 779 | END MODULE limrhg |
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