| 1 | MODULE icerhg_evp |
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| 2 | !!====================================================================== |
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| 3 | !! *** MODULE icerhg_evp *** |
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| 4 | !! Ice rheology : sea ice rheology |
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| 5 | !!====================================================================== |
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| 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 | !! 3.3 ! 2009-05 (G.Garric) addition of the evp cas |
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| 10 | !! 3.4 ! 2011-01 (A. Porter) dynamical allocation |
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| 11 | !! 3.5 ! 2012-08 (R. Benshila) AGRIF |
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| 12 | !! 3.6 ! 2016-06 (C. Rousset) Rewriting + landfast ice + possibility to use mEVP (Bouillon 2013) |
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| 13 | !!---------------------------------------------------------------------- |
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| 14 | #if defined key_lim3 |
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| 15 | !!---------------------------------------------------------------------- |
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| 16 | !! 'key_lim3' LIM-3 sea-ice model |
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| 17 | !!---------------------------------------------------------------------- |
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| 18 | !! ice_rhg_evp : computes ice velocities |
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| 19 | !!---------------------------------------------------------------------- |
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| 20 | USE phycst ! Physical constant |
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| 21 | USE par_oce ! Ocean parameters |
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| 22 | USE dom_oce ! Ocean domain |
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| 23 | USE sbc_oce , ONLY : ln_ice_embd, nn_fsbc, ssh_m |
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| 24 | USE sbc_ice , ONLY : utau_ice, vtau_ice, snwice_mass, snwice_mass_b |
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| 25 | USE ice ! ice variables |
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| 26 | USE limitd_me ! ice strength |
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| 27 | ! |
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| 28 | USE lbclnk ! Lateral Boundary Condition / MPP link |
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| 29 | USE lib_mpp ! MPP library |
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| 30 | USE in_out_manager ! I/O manager |
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| 31 | USE prtctl ! Print control |
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| 32 | USE lib_fortran ! Fortran utilities (allows no signed zero when 'key_nosignedzero' defined) |
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| 33 | #if defined key_agrif |
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| 34 | USE agrif_lim3_interp |
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| 35 | #endif |
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| 36 | USE bdy_oce , ONLY: ln_bdy |
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| 37 | USE bdyice |
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| 38 | |
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| 39 | IMPLICIT NONE |
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| 40 | PRIVATE |
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| 41 | |
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| 42 | PUBLIC ice_rhg_evp ! routine called by icerhg.F90 |
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| 43 | |
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| 44 | !! * Substitutions |
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| 45 | # include "vectopt_loop_substitute.h90" |
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| 46 | !!---------------------------------------------------------------------- |
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| 47 | !! NEMO/LIM3 4.0 , UCL - NEMO Consortium (2011) |
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| 48 | !! $Id: icerhg_evp.F90 8378 2017-07-26 13:55:59Z clem $ |
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| 49 | !! Software governed by the CeCILL licence (NEMOGCM/NEMO_CeCILL.txt) |
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| 50 | !!---------------------------------------------------------------------- |
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| 51 | CONTAINS |
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| 52 | |
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| 53 | SUBROUTINE ice_rhg_evp( stress1_i, stress2_i, stress12_i, u_ice, v_ice, shear_i, divu_i, delta_i ) |
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| 54 | !!------------------------------------------------------------------- |
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| 55 | !! *** SUBROUTINE ice_rhg_evp *** |
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| 56 | !! EVP-C-grid |
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| 57 | !! |
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| 58 | !! ** purpose : determines sea ice drift from wind stress, ice-ocean |
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| 59 | !! stress and sea-surface slope. Ice-ice interaction is described by |
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| 60 | !! a non-linear elasto-viscous-plastic (EVP) law including shear |
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| 61 | !! strength and a bulk rheology (Hunke and Dukowicz, 2002). |
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| 62 | !! |
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| 63 | !! The points in the C-grid look like this, dear reader |
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| 64 | !! |
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| 65 | !! (ji,jj) |
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| 66 | !! | |
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| 67 | !! | |
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| 68 | !! (ji-1,jj) | (ji,jj) |
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| 69 | !! --------- |
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| 70 | !! | | |
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| 71 | !! | (ji,jj) |------(ji,jj) |
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| 72 | !! | | |
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| 73 | !! --------- |
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| 74 | !! (ji-1,jj-1) (ji,jj-1) |
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| 75 | !! |
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| 76 | !! ** Inputs : - wind forcing (stress), oceanic currents |
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| 77 | !! ice total volume (vt_i) per unit area |
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| 78 | !! snow total volume (vt_s) per unit area |
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| 79 | !! |
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| 80 | !! ** Action : - compute u_ice, v_ice : the components of the |
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| 81 | !! sea-ice velocity vector |
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| 82 | !! - compute delta_i, shear_i, divu_i, which are inputs |
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| 83 | !! of the ice thickness distribution |
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| 84 | !! |
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| 85 | !! ** Steps : 1) Compute ice snow mass, ice strength |
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| 86 | !! 2) Compute wind, oceanic stresses, mass terms and |
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| 87 | !! coriolis terms of the momentum equation |
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| 88 | !! 3) Solve the momentum equation (iterative procedure) |
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| 89 | !! 4) Prevent high velocities if the ice is thin |
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| 90 | !! 5) Recompute invariants of the strain rate tensor |
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| 91 | !! which are inputs of the ITD, store stress |
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| 92 | !! for the next time step |
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| 93 | !! 6) Control prints of residual (convergence) |
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| 94 | !! and charge ellipse. |
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| 95 | !! The user should make sure that the parameters |
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| 96 | !! nn_nevp, elastic time scale and rn_creepl maintain stress state |
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| 97 | !! on the charge ellipse for plastic flow |
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| 98 | !! e.g. in the Canadian Archipelago |
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| 99 | !! |
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| 100 | !! ** Notes : There is the possibility to use mEVP from Bouillon 2013 |
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| 101 | !! (by uncommenting some lines in part 3 and changing alpha and beta parameters) |
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| 102 | !! but this solution appears very unstable (see Kimmritz et al 2016) |
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| 103 | !! |
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| 104 | !! References : Hunke and Dukowicz, JPO97 |
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| 105 | !! Bouillon et al., Ocean Modelling 2009 |
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| 106 | !! Bouillon et al., Ocean Modelling 2013 |
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| 107 | !!------------------------------------------------------------------- |
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| 108 | REAL(wp), DIMENSION(jpi,jpj), INTENT(inout) :: stress1_i, stress2_i, stress12_i |
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| 109 | REAL(wp), DIMENSION(jpi,jpj), INTENT( out) :: u_ice, v_ice, shear_i, divu_i, delta_i |
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| 110 | !! |
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| 111 | INTEGER :: ji, jj ! dummy loop indices |
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| 112 | INTEGER :: jter ! local integers |
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| 113 | CHARACTER (len=50) :: charout |
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| 114 | |
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| 115 | REAL(wp) :: zrhoco ! rau0 * rn_cio |
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| 116 | REAL(wp) :: zdtevp, z1_dtevp ! time step for subcycling |
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| 117 | REAL(wp) :: ecc2, z1_ecc2 ! square of yield ellipse eccenticity |
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| 118 | REAL(wp) :: zbeta, zalph1, z1_alph1, zalph2, z1_alph2 ! alpha and beta from Bouillon 2009 and 2013 |
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| 119 | REAL(wp) :: zm1, zm2, zm3, zmassU, zmassV ! ice/snow mass |
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| 120 | REAL(wp) :: zdelta, zp_delf, zds2, zdt, zdt2, zdiv, zdiv2 ! temporary scalars |
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| 121 | REAL(wp) :: zTauO, zTauB, zTauE, zvel ! temporary scalars |
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| 122 | |
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| 123 | REAL(wp) :: zsig1, zsig2 ! internal ice stress |
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| 124 | REAL(wp) :: zresm ! Maximal error on ice velocity |
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| 125 | REAL(wp) :: zintb, zintn ! dummy argument |
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| 126 | REAL(wp) :: zfac_x, zfac_y |
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| 127 | |
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| 128 | REAL(wp), DIMENSION(jpi,jpj) :: z1_e1t0, z1_e2t0 ! scale factors |
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| 129 | REAL(wp), DIMENSION(jpi,jpj) :: zp_delt ! P/delta at T points |
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| 130 | ! |
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| 131 | REAL(wp), DIMENSION(jpi,jpj) :: zaU , zaV ! ice fraction on U/V points |
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| 132 | REAL(wp), DIMENSION(jpi,jpj) :: zmU_t, zmV_t ! ice/snow mass/dt on U/V points |
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| 133 | REAL(wp), DIMENSION(jpi,jpj) :: zmf ! coriolis parameter at T points |
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| 134 | REAL(wp), DIMENSION(jpi,jpj) :: zTauU_ia , ztauV_ia ! ice-atm. stress at U-V points |
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| 135 | REAL(wp), DIMENSION(jpi,jpj) :: zspgU , zspgV ! surface pressure gradient at U/V points |
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| 136 | REAL(wp), DIMENSION(jpi,jpj) :: v_oceU, u_oceV, v_iceU, u_iceV ! ocean/ice u/v component on V/U points |
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| 137 | REAL(wp), DIMENSION(jpi,jpj) :: zfU , zfV ! internal stresses |
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| 138 | |
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| 139 | REAL(wp), DIMENSION(jpi,jpj) :: zds ! shear |
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| 140 | REAL(wp), DIMENSION(jpi,jpj) :: zs1, zs2, zs12 ! stress tensor components |
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| 141 | REAL(wp), DIMENSION(jpi,jpj) :: zu_ice, zv_ice, zresr ! check convergence |
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| 142 | REAL(wp), DIMENSION(jpi,jpj) :: zpice ! array used for the calculation of ice surface slope: |
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| 143 | ! ocean surface (ssh_m) if ice is not embedded |
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| 144 | ! ice top surface if ice is embedded |
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| 145 | REAL(wp), DIMENSION(jpi,jpj) :: zCorx, zCory ! Coriolis stress array |
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| 146 | REAL(wp), DIMENSION(jpi,jpj) :: ztaux_oi, ztauy_oi ! Ocean-to-ice stress array |
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| 147 | |
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| 148 | REAL(wp), DIMENSION(jpi,jpj) :: zswitchU, zswitchV ! dummy arrays |
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| 149 | REAL(wp), DIMENSION(jpi,jpj) :: zmaskU, zmaskV ! mask for ice presence |
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| 150 | REAL(wp), DIMENSION(jpi,jpj) :: zfmask, zwf ! mask at F points for the ice |
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| 151 | |
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| 152 | REAL(wp), PARAMETER :: zepsi = 1.0e-20_wp ! tolerance parameter |
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| 153 | REAL(wp), PARAMETER :: zmmin = 1._wp ! ice mass (kg/m2) below which ice velocity equals ocean velocity |
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| 154 | !!------------------------------------------------------------------- |
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| 155 | |
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| 156 | #if defined key_agrif |
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| 157 | CALL agrif_interp_lim3( 'U', 0, nn_nevp ) ! First interpolation of coarse values |
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| 158 | CALL agrif_interp_lim3( 'V', 0, nn_nevp ) |
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| 159 | #endif |
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| 160 | ! |
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| 161 | !------------------------------------------------------------------------------! |
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| 162 | ! 0) mask at F points for the ice |
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| 163 | !------------------------------------------------------------------------------! |
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| 164 | ! ocean/land mask |
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| 165 | DO jj = 1, jpjm1 |
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| 166 | DO ji = 1, jpim1 ! NO vector opt. |
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| 167 | zfmask(ji,jj) = tmask(ji,jj,1) * tmask(ji+1,jj,1) * tmask(ji,jj+1,1) * tmask(ji+1,jj+1,1) |
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| 168 | END DO |
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| 169 | END DO |
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| 170 | CALL lbc_lnk( zfmask, 'F', 1._wp ) |
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| 171 | |
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| 172 | ! Lateral boundary conditions on velocity (modify zfmask) |
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| 173 | zwf(:,:) = zfmask(:,:) |
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| 174 | DO jj = 2, jpjm1 |
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| 175 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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| 176 | IF( zfmask(ji,jj) == 0._wp ) THEN |
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| 177 | zfmask(ji,jj) = rn_ishlat * MIN( 1._wp , MAX( zwf(ji+1,jj), zwf(ji,jj+1), zwf(ji-1,jj), zwf(ji,jj-1) ) ) |
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| 178 | ENDIF |
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| 179 | END DO |
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| 180 | END DO |
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| 181 | DO jj = 2, jpjm1 |
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| 182 | IF( zfmask(1,jj) == 0._wp ) THEN |
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| 183 | zfmask(1 ,jj) = rn_ishlat * MIN( 1._wp , MAX( zwf(2,jj), zwf(1,jj+1), zwf(1,jj-1) ) ) |
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| 184 | ENDIF |
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| 185 | IF( zfmask(jpi,jj) == 0._wp ) THEN |
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| 186 | zfmask(jpi,jj) = rn_ishlat * MIN( 1._wp , MAX( zwf(jpi,jj+1), zwf(jpim1,jj), zwf(jpi,jj-1) ) ) |
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| 187 | ENDIF |
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| 188 | END DO |
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| 189 | DO ji = 2, jpim1 |
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| 190 | IF( zfmask(ji,1) == 0._wp ) THEN |
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| 191 | zfmask(ji,1 ) = rn_ishlat * MIN( 1._wp , MAX( zwf(ji+1,1), zwf(ji,2), zwf(ji-1,1) ) ) |
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| 192 | ENDIF |
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| 193 | IF( zfmask(ji,jpj) == 0._wp ) THEN |
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| 194 | zfmask(ji,jpj) = rn_ishlat * MIN( 1._wp , MAX( zwf(ji+1,jpj), zwf(ji-1,jpj), zwf(ji,jpjm1) ) ) |
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| 195 | ENDIF |
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| 196 | END DO |
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| 197 | CALL lbc_lnk( zfmask, 'F', 1._wp ) |
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| 198 | |
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| 199 | !------------------------------------------------------------------------------! |
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| 200 | ! 1) define some variables and initialize arrays |
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| 201 | !------------------------------------------------------------------------------! |
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| 202 | zrhoco = rau0 * rn_cio |
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| 203 | |
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| 204 | ! ecc2: square of yield ellipse eccenticrity |
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| 205 | ecc2 = rn_ecc * rn_ecc |
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| 206 | z1_ecc2 = 1._wp / ecc2 |
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| 207 | |
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| 208 | ! Time step for subcycling |
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| 209 | zdtevp = rdt_ice / REAL( nn_nevp ) |
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| 210 | z1_dtevp = 1._wp / zdtevp |
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| 211 | |
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| 212 | ! alpha parameters (Bouillon 2009) |
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| 213 | zalph1 = ( 2._wp * rn_relast * rdt_ice ) * z1_dtevp |
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| 214 | zalph2 = zalph1 * z1_ecc2 |
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| 215 | |
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| 216 | ! alpha and beta parameters (Bouillon 2013) |
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| 217 | !!zalph1 = 40. |
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| 218 | !!zalph2 = 40. |
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| 219 | !!zbeta = 3000. |
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| 220 | !!zbeta = REAL( nn_nevp ) ! close to classical EVP of Hunke (2001) |
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| 221 | |
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| 222 | z1_alph1 = 1._wp / ( zalph1 + 1._wp ) |
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| 223 | z1_alph2 = 1._wp / ( zalph2 + 1._wp ) |
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| 224 | |
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| 225 | ! Initialise stress tensor |
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| 226 | zs1 (:,:) = stress1_i (:,:) |
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| 227 | zs2 (:,:) = stress2_i (:,:) |
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| 228 | zs12(:,:) = stress12_i(:,:) |
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| 229 | |
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| 230 | ! Ice strength |
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| 231 | CALL lim_itd_me_icestrength( nn_icestr ) |
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| 232 | |
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| 233 | ! scale factors |
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| 234 | DO jj = 2, jpjm1 |
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| 235 | DO ji = fs_2, fs_jpim1 |
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| 236 | z1_e1t0(ji,jj) = 1._wp / ( e1t(ji+1,jj ) + e1t(ji,jj ) ) |
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| 237 | z1_e2t0(ji,jj) = 1._wp / ( e2t(ji ,jj+1) + e2t(ji,jj ) ) |
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| 238 | END DO |
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| 239 | END DO |
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| 240 | |
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| 241 | ! |
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| 242 | !------------------------------------------------------------------------------! |
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| 243 | ! 2) Wind / ocean stress, mass terms, coriolis terms |
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| 244 | !------------------------------------------------------------------------------! |
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| 245 | |
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| 246 | IF( ln_ice_embd ) THEN !== embedded sea ice: compute representative ice top surface ==! |
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| 247 | ! |
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| 248 | ! average interpolation coeff as used in dynspg = (1/nn_fsbc) * {SUM[n/nn_fsbc], n=0,nn_fsbc-1} |
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| 249 | ! = (1/nn_fsbc)^2 * {SUM[n], n=0,nn_fsbc-1} |
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| 250 | zintn = REAL( nn_fsbc - 1 ) / REAL( nn_fsbc ) * 0.5_wp |
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| 251 | ! |
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| 252 | ! average interpolation coeff as used in dynspg = (1/nn_fsbc) * {SUM[1-n/nn_fsbc], n=0,nn_fsbc-1} |
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| 253 | ! = (1/nn_fsbc)^2 * (nn_fsbc^2 - {SUM[n], n=0,nn_fsbc-1}) |
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| 254 | zintb = REAL( nn_fsbc + 1 ) / REAL( nn_fsbc ) * 0.5_wp |
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| 255 | ! |
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| 256 | zpice(:,:) = ssh_m(:,:) + ( zintn * snwice_mass(:,:) + zintb * snwice_mass_b(:,:) ) * r1_rau0 |
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| 257 | ! |
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| 258 | ELSE !== non-embedded sea ice: use ocean surface for slope calculation ==! |
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| 259 | zpice(:,:) = ssh_m(:,:) |
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| 260 | ENDIF |
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| 261 | |
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| 262 | DO jj = 2, jpjm1 |
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| 263 | DO ji = fs_2, fs_jpim1 |
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| 264 | |
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| 265 | ! ice fraction at U-V points |
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| 266 | zaU(ji,jj) = 0.5_wp * ( at_i(ji,jj) * e1e2t(ji,jj) + at_i(ji+1,jj) * e1e2t(ji+1,jj) ) * r1_e1e2u(ji,jj) * umask(ji,jj,1) |
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| 267 | zaV(ji,jj) = 0.5_wp * ( at_i(ji,jj) * e1e2t(ji,jj) + at_i(ji,jj+1) * e1e2t(ji,jj+1) ) * r1_e1e2v(ji,jj) * vmask(ji,jj,1) |
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| 268 | |
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| 269 | ! Ice/snow mass at U-V points |
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| 270 | zm1 = ( rhosn * vt_s(ji ,jj ) + rhoic * vt_i(ji ,jj ) ) |
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| 271 | zm2 = ( rhosn * vt_s(ji+1,jj ) + rhoic * vt_i(ji+1,jj ) ) |
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| 272 | zm3 = ( rhosn * vt_s(ji ,jj+1) + rhoic * vt_i(ji ,jj+1) ) |
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| 273 | zmassU = 0.5_wp * ( zm1 * e1e2t(ji,jj) + zm2 * e1e2t(ji+1,jj) ) * r1_e1e2u(ji,jj) * umask(ji,jj,1) |
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| 274 | zmassV = 0.5_wp * ( zm1 * e1e2t(ji,jj) + zm3 * e1e2t(ji,jj+1) ) * r1_e1e2v(ji,jj) * vmask(ji,jj,1) |
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| 275 | |
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| 276 | ! Ocean currents at U-V points |
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| 277 | v_oceU(ji,jj) = 0.5_wp * ( ( v_oce(ji ,jj) + v_oce(ji ,jj-1) ) * e1t(ji+1,jj) & |
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| 278 | & + ( v_oce(ji+1,jj) + v_oce(ji+1,jj-1) ) * e1t(ji ,jj) ) * z1_e1t0(ji,jj) * umask(ji,jj,1) |
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| 279 | |
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| 280 | u_oceV(ji,jj) = 0.5_wp * ( ( u_oce(ji,jj ) + u_oce(ji-1,jj ) ) * e2t(ji,jj+1) & |
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| 281 | & + ( u_oce(ji,jj+1) + u_oce(ji-1,jj+1) ) * e2t(ji,jj ) ) * z1_e2t0(ji,jj) * vmask(ji,jj,1) |
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| 282 | |
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| 283 | ! Coriolis at T points (m*f) |
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| 284 | zmf(ji,jj) = zm1 * ff_t(ji,jj) |
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| 285 | |
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| 286 | ! m/dt |
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| 287 | zmU_t(ji,jj) = zmassU * z1_dtevp |
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| 288 | zmV_t(ji,jj) = zmassV * z1_dtevp |
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| 289 | |
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| 290 | ! Drag ice-atm. |
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| 291 | zTauU_ia(ji,jj) = zaU(ji,jj) * utau_ice(ji,jj) |
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| 292 | zTauV_ia(ji,jj) = zaV(ji,jj) * vtau_ice(ji,jj) |
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| 293 | |
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| 294 | ! Surface pressure gradient (- m*g*GRAD(ssh)) at U-V points |
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| 295 | zspgU(ji,jj) = - zmassU * grav * ( zpice(ji+1,jj) - zpice(ji,jj) ) * r1_e1u(ji,jj) |
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| 296 | zspgV(ji,jj) = - zmassV * grav * ( zpice(ji,jj+1) - zpice(ji,jj) ) * r1_e2v(ji,jj) |
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| 297 | |
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| 298 | ! masks |
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| 299 | zmaskU(ji,jj) = 1._wp - MAX( 0._wp, SIGN( 1._wp, -zmassU ) ) ! 0 if no ice |
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| 300 | zmaskV(ji,jj) = 1._wp - MAX( 0._wp, SIGN( 1._wp, -zmassV ) ) ! 0 if no ice |
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| 301 | |
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| 302 | ! switches |
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| 303 | zswitchU(ji,jj) = MAX( 0._wp, SIGN( 1._wp, zmassU - zmmin ) ) ! 0 if ice mass < zmmin |
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| 304 | zswitchV(ji,jj) = MAX( 0._wp, SIGN( 1._wp, zmassV - zmmin ) ) ! 0 if ice mass < zmmin |
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| 305 | |
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| 306 | END DO |
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| 307 | END DO |
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| 308 | CALL lbc_lnk( zmf, 'T', 1. ) |
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| 309 | ! |
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| 310 | !------------------------------------------------------------------------------! |
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| 311 | ! 3) Solution of the momentum equation, iterative procedure |
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| 312 | !------------------------------------------------------------------------------! |
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| 313 | ! |
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| 314 | ! !----------------------! |
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| 315 | DO jter = 1 , nn_nevp ! loop over jter ! |
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| 316 | ! !----------------------! |
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| 317 | IF(ln_ctl) THEN ! Convergence test |
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| 318 | DO jj = 1, jpjm1 |
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| 319 | zu_ice(:,jj) = u_ice(:,jj) ! velocity at previous time step |
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| 320 | zv_ice(:,jj) = v_ice(:,jj) |
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| 321 | END DO |
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| 322 | ENDIF |
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| 323 | |
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| 324 | ! --- divergence, tension & shear (Appendix B of Hunke & Dukowicz, 2002) --- ! |
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| 325 | DO jj = 1, jpjm1 ! loops start at 1 since there is no boundary condition (lbc_lnk) at i=1 and j=1 for F points |
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| 326 | DO ji = 1, jpim1 |
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| 327 | |
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| 328 | ! shear at F points |
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| 329 | zds(ji,jj) = ( ( u_ice(ji,jj+1) * r1_e1u(ji,jj+1) - u_ice(ji,jj) * r1_e1u(ji,jj) ) * e1f(ji,jj) * e1f(ji,jj) & |
|---|
| 330 | & + ( v_ice(ji+1,jj) * r1_e2v(ji+1,jj) - v_ice(ji,jj) * r1_e2v(ji,jj) ) * e2f(ji,jj) * e2f(ji,jj) & |
|---|
| 331 | & ) * r1_e1e2f(ji,jj) * zfmask(ji,jj) |
|---|
| 332 | |
|---|
| 333 | END DO |
|---|
| 334 | END DO |
|---|
| 335 | CALL lbc_lnk( zds, 'F', 1. ) |
|---|
| 336 | |
|---|
| 337 | DO jj = 2, jpjm1 |
|---|
| 338 | DO ji = 2, jpim1 ! no vector loop |
|---|
| 339 | |
|---|
| 340 | ! shear**2 at T points (doc eq. A16) |
|---|
| 341 | zds2 = ( zds(ji,jj ) * zds(ji,jj ) * e1e2f(ji,jj ) + zds(ji-1,jj ) * zds(ji-1,jj ) * e1e2f(ji-1,jj ) & |
|---|
| 342 | & + zds(ji,jj-1) * zds(ji,jj-1) * e1e2f(ji,jj-1) + zds(ji-1,jj-1) * zds(ji-1,jj-1) * e1e2f(ji-1,jj-1) & |
|---|
| 343 | & ) * 0.25_wp * r1_e1e2t(ji,jj) |
|---|
| 344 | |
|---|
| 345 | ! divergence at T points |
|---|
| 346 | zdiv = ( e2u(ji,jj) * u_ice(ji,jj) - e2u(ji-1,jj) * u_ice(ji-1,jj) & |
|---|
| 347 | & + e1v(ji,jj) * v_ice(ji,jj) - e1v(ji,jj-1) * v_ice(ji,jj-1) & |
|---|
| 348 | & ) * r1_e1e2t(ji,jj) |
|---|
| 349 | zdiv2 = zdiv * zdiv |
|---|
| 350 | |
|---|
| 351 | ! tension at T points |
|---|
| 352 | zdt = ( ( u_ice(ji,jj) * r1_e2u(ji,jj) - u_ice(ji-1,jj) * r1_e2u(ji-1,jj) ) * e2t(ji,jj) * e2t(ji,jj) & |
|---|
| 353 | & - ( v_ice(ji,jj) * r1_e1v(ji,jj) - v_ice(ji,jj-1) * r1_e1v(ji,jj-1) ) * e1t(ji,jj) * e1t(ji,jj) & |
|---|
| 354 | & ) * r1_e1e2t(ji,jj) |
|---|
| 355 | zdt2 = zdt * zdt |
|---|
| 356 | |
|---|
| 357 | ! delta at T points |
|---|
| 358 | zdelta = SQRT( zdiv2 + ( zdt2 + zds2 ) * z1_ecc2 ) |
|---|
| 359 | |
|---|
| 360 | ! P/delta at T points |
|---|
| 361 | zp_delt(ji,jj) = strength(ji,jj) / ( zdelta + rn_creepl ) |
|---|
| 362 | |
|---|
| 363 | ! stress at T points |
|---|
| 364 | zs1(ji,jj) = ( zs1(ji,jj) * zalph1 + zp_delt(ji,jj) * ( zdiv - zdelta ) ) * z1_alph1 |
|---|
| 365 | zs2(ji,jj) = ( zs2(ji,jj) * zalph2 + zp_delt(ji,jj) * ( zdt * z1_ecc2 ) ) * z1_alph2 |
|---|
| 366 | |
|---|
| 367 | END DO |
|---|
| 368 | END DO |
|---|
| 369 | CALL lbc_lnk( zp_delt, 'T', 1. ) |
|---|
| 370 | |
|---|
| 371 | DO jj = 1, jpjm1 |
|---|
| 372 | DO ji = 1, jpim1 |
|---|
| 373 | |
|---|
| 374 | ! P/delta at F points |
|---|
| 375 | zp_delf = 0.25_wp * ( zp_delt(ji,jj) + zp_delt(ji+1,jj) + zp_delt(ji,jj+1) + zp_delt(ji+1,jj+1) ) |
|---|
| 376 | |
|---|
| 377 | ! stress at F points |
|---|
| 378 | zs12(ji,jj)= ( zs12(ji,jj) * zalph2 + zp_delf * ( zds(ji,jj) * z1_ecc2 ) * 0.5_wp ) * z1_alph2 |
|---|
| 379 | |
|---|
| 380 | END DO |
|---|
| 381 | END DO |
|---|
| 382 | CALL lbc_lnk_multi( zs1, 'T', 1., zs2, 'T', 1., zs12, 'F', 1. ) |
|---|
| 383 | |
|---|
| 384 | |
|---|
| 385 | ! --- Ice internal stresses (Appendix C of Hunke and Dukowicz, 2002) --- ! |
|---|
| 386 | DO jj = 2, jpjm1 |
|---|
| 387 | DO ji = fs_2, fs_jpim1 |
|---|
| 388 | |
|---|
| 389 | ! U points |
|---|
| 390 | zfU(ji,jj) = 0.5_wp * ( ( zs1(ji+1,jj) - zs1(ji,jj) ) * e2u(ji,jj) & |
|---|
| 391 | & + ( zs2(ji+1,jj) * e2t(ji+1,jj) * e2t(ji+1,jj) - zs2(ji,jj) * e2t(ji,jj) * e2t(ji,jj) & |
|---|
| 392 | & ) * r1_e2u(ji,jj) & |
|---|
| 393 | & + ( zs12(ji,jj) * e1f(ji,jj) * e1f(ji,jj) - zs12(ji,jj-1) * e1f(ji,jj-1) * e1f(ji,jj-1) & |
|---|
| 394 | & ) * 2._wp * r1_e1u(ji,jj) & |
|---|
| 395 | & ) * r1_e1e2u(ji,jj) |
|---|
| 396 | |
|---|
| 397 | ! V points |
|---|
| 398 | zfV(ji,jj) = 0.5_wp * ( ( zs1(ji,jj+1) - zs1(ji,jj) ) * e1v(ji,jj) & |
|---|
| 399 | & - ( zs2(ji,jj+1) * e1t(ji,jj+1) * e1t(ji,jj+1) - zs2(ji,jj) * e1t(ji,jj) * e1t(ji,jj) & |
|---|
| 400 | & ) * r1_e1v(ji,jj) & |
|---|
| 401 | & + ( zs12(ji,jj) * e2f(ji,jj) * e2f(ji,jj) - zs12(ji-1,jj) * e2f(ji-1,jj) * e2f(ji-1,jj) & |
|---|
| 402 | & ) * 2._wp * r1_e2v(ji,jj) & |
|---|
| 403 | & ) * r1_e1e2v(ji,jj) |
|---|
| 404 | |
|---|
| 405 | ! u_ice at V point |
|---|
| 406 | u_iceV(ji,jj) = 0.5_wp * ( ( u_ice(ji,jj ) + u_ice(ji-1,jj ) ) * e2t(ji,jj+1) & |
|---|
| 407 | & + ( u_ice(ji,jj+1) + u_ice(ji-1,jj+1) ) * e2t(ji,jj ) ) * z1_e2t0(ji,jj) * vmask(ji,jj,1) |
|---|
| 408 | |
|---|
| 409 | ! v_ice at U point |
|---|
| 410 | v_iceU(ji,jj) = 0.5_wp * ( ( v_ice(ji ,jj) + v_ice(ji ,jj-1) ) * e1t(ji+1,jj) & |
|---|
| 411 | & + ( v_ice(ji+1,jj) + v_ice(ji+1,jj-1) ) * e1t(ji ,jj) ) * z1_e1t0(ji,jj) * umask(ji,jj,1) |
|---|
| 412 | |
|---|
| 413 | END DO |
|---|
| 414 | END DO |
|---|
| 415 | ! |
|---|
| 416 | ! --- Computation of ice velocity --- ! |
|---|
| 417 | ! Bouillon et al. 2013 (eq 47-48) => unstable unless alpha, beta are chosen wisely and large nn_nevp |
|---|
| 418 | ! Bouillon et al. 2009 (eq 34-35) => stable |
|---|
| 419 | IF( MOD(jter,2) .EQ. 0 ) THEN ! even iterations |
|---|
| 420 | |
|---|
| 421 | DO jj = 2, jpjm1 |
|---|
| 422 | DO ji = fs_2, fs_jpim1 |
|---|
| 423 | |
|---|
| 424 | ! tau_io/(v_oce - v_ice) |
|---|
| 425 | zTauO = zaV(ji,jj) * zrhoco * SQRT( ( v_ice (ji,jj) - v_oce (ji,jj) ) * ( v_ice (ji,jj) - v_oce (ji,jj) ) & |
|---|
| 426 | & + ( u_iceV(ji,jj) - u_oceV(ji,jj) ) * ( u_iceV(ji,jj) - u_oceV(ji,jj) ) ) |
|---|
| 427 | |
|---|
| 428 | ! Ocean-to-Ice stress |
|---|
| 429 | ztauy_oi(ji,jj) = zTauO * ( v_oce(ji,jj) - v_ice(ji,jj) ) |
|---|
| 430 | |
|---|
| 431 | ! tau_bottom/v_ice |
|---|
| 432 | zvel = MAX( zepsi, SQRT( v_ice(ji,jj) * v_ice(ji,jj) + u_iceV(ji,jj) * u_iceV(ji,jj) ) ) |
|---|
| 433 | zTauB = - tau_icebfr(ji,jj) / zvel |
|---|
| 434 | |
|---|
| 435 | ! Coriolis at V-points (energy conserving formulation) |
|---|
| 436 | zCory(ji,jj) = - 0.25_wp * r1_e2v(ji,jj) * & |
|---|
| 437 | & ( zmf(ji,jj ) * ( e2u(ji,jj ) * u_ice(ji,jj ) + e2u(ji-1,jj ) * u_ice(ji-1,jj ) ) & |
|---|
| 438 | & + zmf(ji,jj+1) * ( e2u(ji,jj+1) * u_ice(ji,jj+1) + e2u(ji-1,jj+1) * u_ice(ji-1,jj+1) ) ) |
|---|
| 439 | |
|---|
| 440 | ! Sum of external forces (explicit solution) = F + tau_ia + Coriolis + spg + tau_io |
|---|
| 441 | zTauE = zfV(ji,jj) + zTauV_ia(ji,jj) + zCory(ji,jj) + zspgV(ji,jj) + ztauy_oi(ji,jj) |
|---|
| 442 | |
|---|
| 443 | ! landfast switch => 0 = static friction ; 1 = sliding friction |
|---|
| 444 | rswitch = 1._wp - MIN( 1._wp, ABS( SIGN( 1._wp, ztauE - tau_icebfr(ji,jj) ) - SIGN( 1._wp, zTauE ) ) ) |
|---|
| 445 | |
|---|
| 446 | ! ice velocity using implicit formulation (cf Madec doc & Bouillon 2009) |
|---|
| 447 | v_ice(ji,jj) = ( ( rswitch * ( zmV_t(ji,jj) * v_ice(ji,jj) & ! previous velocity |
|---|
| 448 | & + zTauE + zTauO * v_ice(ji,jj) & ! F + tau_ia + Coriolis + spg + tau_io(only ocean part) |
|---|
| 449 | & ) / MAX( zepsi, zmV_t(ji,jj) + zTauO - zTauB ) & ! m/dt + tau_io(only ice part) + landfast |
|---|
| 450 | & + ( 1._wp - rswitch ) * v_ice(ji,jj) * MAX( 0._wp, 1._wp - zdtevp * rn_lfrelax ) & ! static friction => slow decrease to v=0 |
|---|
| 451 | & ) * zswitchV(ji,jj) + v_oce(ji,jj) * ( 1._wp - zswitchV(ji,jj) ) & ! v_ice = v_oce if mass < zmmin |
|---|
| 452 | & ) * zmaskV(ji,jj) |
|---|
| 453 | ! Bouillon 2013 |
|---|
| 454 | !!v_ice(ji,jj) = ( zmV_t(ji,jj) * ( zbeta * v_ice(ji,jj) + v_ice_b(ji,jj) ) & |
|---|
| 455 | !! & + zfV(ji,jj) + zCory(ji,jj) + zTauV_ia(ji,jj) + zTauO * v_oce(ji,jj) + zspgV(ji,jj) & |
|---|
| 456 | !! & ) / MAX( zmV_t(ji,jj) * ( zbeta + 1._wp ) + zTauO - zTauB, zepsi ) * zswitchV(ji,jj) |
|---|
| 457 | |
|---|
| 458 | END DO |
|---|
| 459 | END DO |
|---|
| 460 | CALL lbc_lnk( v_ice, 'V', -1. ) |
|---|
| 461 | |
|---|
| 462 | #if defined key_agrif |
|---|
| 463 | !! CALL agrif_interp_lim3( 'V', jter, nn_nevp ) |
|---|
| 464 | CALL agrif_interp_lim3( 'V' ) |
|---|
| 465 | #endif |
|---|
| 466 | IF( ln_bdy ) CALL bdy_ice_dyn( 'V' ) |
|---|
| 467 | |
|---|
| 468 | DO jj = 2, jpjm1 |
|---|
| 469 | DO ji = fs_2, fs_jpim1 |
|---|
| 470 | |
|---|
| 471 | ! tau_io/(u_oce - u_ice) |
|---|
| 472 | zTauO = zaU(ji,jj) * zrhoco * SQRT( ( u_ice (ji,jj) - u_oce (ji,jj) ) * ( u_ice (ji,jj) - u_oce (ji,jj) ) & |
|---|
| 473 | & + ( v_iceU(ji,jj) - v_oceU(ji,jj) ) * ( v_iceU(ji,jj) - v_oceU(ji,jj) ) ) |
|---|
| 474 | |
|---|
| 475 | ! Ocean-to-Ice stress |
|---|
| 476 | ztaux_oi(ji,jj) = zTauO * ( u_oce(ji,jj) - u_ice(ji,jj) ) |
|---|
| 477 | |
|---|
| 478 | ! tau_bottom/u_ice |
|---|
| 479 | zvel = MAX( zepsi, SQRT( v_iceU(ji,jj) * v_iceU(ji,jj) + u_ice(ji,jj) * u_ice(ji,jj) ) ) |
|---|
| 480 | zTauB = - tau_icebfr(ji,jj) / zvel |
|---|
| 481 | |
|---|
| 482 | ! Coriolis at U-points (energy conserving formulation) |
|---|
| 483 | zCorx(ji,jj) = 0.25_wp * r1_e1u(ji,jj) * & |
|---|
| 484 | & ( zmf(ji ,jj) * ( e1v(ji ,jj) * v_ice(ji ,jj) + e1v(ji ,jj-1) * v_ice(ji ,jj-1) ) & |
|---|
| 485 | & + zmf(ji+1,jj) * ( e1v(ji+1,jj) * v_ice(ji+1,jj) + e1v(ji+1,jj-1) * v_ice(ji+1,jj-1) ) ) |
|---|
| 486 | |
|---|
| 487 | ! Sum of external forces (explicit solution) = F + tau_ia + Coriolis + spg + tau_io |
|---|
| 488 | zTauE = zfU(ji,jj) + zTauU_ia(ji,jj) + zCorx(ji,jj) + zspgU(ji,jj) + ztaux_oi(ji,jj) |
|---|
| 489 | |
|---|
| 490 | ! landfast switch => 0 = static friction ; 1 = sliding friction |
|---|
| 491 | rswitch = 1._wp - MIN( 1._wp, ABS( SIGN( 1._wp, ztauE - tau_icebfr(ji,jj) ) - SIGN( 1._wp, zTauE ) ) ) |
|---|
| 492 | |
|---|
| 493 | ! ice velocity using implicit formulation (cf Madec doc & Bouillon 2009) |
|---|
| 494 | u_ice(ji,jj) = ( ( rswitch * ( zmU_t(ji,jj) * u_ice(ji,jj) & ! previous velocity |
|---|
| 495 | & + zTauE + zTauO * u_ice(ji,jj) & ! F + tau_ia + Coriolis + spg + tau_io(only ocean part) |
|---|
| 496 | & ) / MAX( zepsi, zmU_t(ji,jj) + zTauO - zTauB ) & ! m/dt + tau_io(only ice part) + landfast |
|---|
| 497 | & + ( 1._wp - rswitch ) * u_ice(ji,jj) * MAX( 0._wp, 1._wp - zdtevp * rn_lfrelax ) & ! static friction => slow decrease to v=0 |
|---|
| 498 | & ) * zswitchU(ji,jj) + u_oce(ji,jj) * ( 1._wp - zswitchU(ji,jj) ) & ! v_ice = v_oce if mass < zmmin |
|---|
| 499 | & ) * zmaskU(ji,jj) |
|---|
| 500 | ! Bouillon 2013 |
|---|
| 501 | !!u_ice(ji,jj) = ( zmU_t(ji,jj) * ( zbeta * u_ice(ji,jj) + u_ice_b(ji,jj) ) & |
|---|
| 502 | !! & + zfU(ji,jj) + zCorx(ji,jj) + zTauU_ia(ji,jj) + zTauO * u_oce(ji,jj) + zspgU(ji,jj) & |
|---|
| 503 | !! & ) / MAX( zmU_t(ji,jj) * ( zbeta + 1._wp ) + zTauO - zTauB, zepsi ) * zswitchU(ji,jj) |
|---|
| 504 | END DO |
|---|
| 505 | END DO |
|---|
| 506 | CALL lbc_lnk( u_ice, 'U', -1. ) |
|---|
| 507 | |
|---|
| 508 | #if defined key_agrif |
|---|
| 509 | !! CALL agrif_interp_lim3( 'U', jter, nn_nevp ) |
|---|
| 510 | CALL agrif_interp_lim3( 'U' ) |
|---|
| 511 | #endif |
|---|
| 512 | IF( ln_bdy ) CALL bdy_ice_dyn( 'U' ) |
|---|
| 513 | |
|---|
| 514 | ELSE ! odd iterations |
|---|
| 515 | |
|---|
| 516 | DO jj = 2, jpjm1 |
|---|
| 517 | DO ji = fs_2, fs_jpim1 |
|---|
| 518 | |
|---|
| 519 | ! tau_io/(u_oce - u_ice) |
|---|
| 520 | zTauO = zaU(ji,jj) * zrhoco * SQRT( ( u_ice (ji,jj) - u_oce (ji,jj) ) * ( u_ice (ji,jj) - u_oce (ji,jj) ) & |
|---|
| 521 | & + ( v_iceU(ji,jj) - v_oceU(ji,jj) ) * ( v_iceU(ji,jj) - v_oceU(ji,jj) ) ) |
|---|
| 522 | |
|---|
| 523 | ! Ocean-to-Ice stress |
|---|
| 524 | ztaux_oi(ji,jj) = zTauO * ( u_oce(ji,jj) - u_ice(ji,jj) ) |
|---|
| 525 | |
|---|
| 526 | ! tau_bottom/u_ice |
|---|
| 527 | zvel = MAX( zepsi, SQRT( v_iceU(ji,jj) * v_iceU(ji,jj) + u_ice(ji,jj) * u_ice(ji,jj) ) ) |
|---|
| 528 | zTauB = - tau_icebfr(ji,jj) / zvel |
|---|
| 529 | |
|---|
| 530 | ! Coriolis at U-points (energy conserving formulation) |
|---|
| 531 | zCorx(ji,jj) = 0.25_wp * r1_e1u(ji,jj) * & |
|---|
| 532 | & ( zmf(ji ,jj) * ( e1v(ji ,jj) * v_ice(ji ,jj) + e1v(ji ,jj-1) * v_ice(ji ,jj-1) ) & |
|---|
| 533 | & + zmf(ji+1,jj) * ( e1v(ji+1,jj) * v_ice(ji+1,jj) + e1v(ji+1,jj-1) * v_ice(ji+1,jj-1) ) ) |
|---|
| 534 | |
|---|
| 535 | ! Sum of external forces (explicit solution) = F + tau_ia + Coriolis + spg + tau_io |
|---|
| 536 | zTauE = zfU(ji,jj) + zTauU_ia(ji,jj) + zCorx(ji,jj) + zspgU(ji,jj) + ztaux_oi(ji,jj) |
|---|
| 537 | |
|---|
| 538 | ! landfast switch => 0 = static friction ; 1 = sliding friction |
|---|
| 539 | rswitch = 1._wp - MIN( 1._wp, ABS( SIGN( 1._wp, ztauE - tau_icebfr(ji,jj) ) - SIGN( 1._wp, zTauE ) ) ) |
|---|
| 540 | |
|---|
| 541 | ! ice velocity using implicit formulation (cf Madec doc & Bouillon 2009) |
|---|
| 542 | u_ice(ji,jj) = ( ( rswitch * ( zmU_t(ji,jj) * u_ice(ji,jj) & ! previous velocity |
|---|
| 543 | & + zTauE + zTauO * u_ice(ji,jj) & ! F + tau_ia + Coriolis + spg + tau_io(only ocean part) |
|---|
| 544 | & ) / MAX( zepsi, zmU_t(ji,jj) + zTauO - zTauB ) & ! m/dt + tau_io(only ice part) + landfast |
|---|
| 545 | & + ( 1._wp - rswitch ) * u_ice(ji,jj) * MAX( 0._wp, 1._wp - zdtevp * rn_lfrelax ) & ! static friction => slow decrease to v=0 |
|---|
| 546 | & ) * zswitchU(ji,jj) + u_oce(ji,jj) * ( 1._wp - zswitchU(ji,jj) ) & ! v_ice = v_oce if mass < zmmin |
|---|
| 547 | & ) * zmaskU(ji,jj) |
|---|
| 548 | ! Bouillon 2013 |
|---|
| 549 | !!u_ice(ji,jj) = ( zmU_t(ji,jj) * ( zbeta * u_ice(ji,jj) + u_ice_b(ji,jj) ) & |
|---|
| 550 | !! & + zfU(ji,jj) + zCorx(ji,jj) + zTauU_ia(ji,jj) + zTauO * u_oce(ji,jj) + zspgU(ji,jj) & |
|---|
| 551 | !! & ) / MAX( zmU_t(ji,jj) * ( zbeta + 1._wp ) + zTauO - zTauB, zepsi ) * zswitchU(ji,jj) |
|---|
| 552 | END DO |
|---|
| 553 | END DO |
|---|
| 554 | CALL lbc_lnk( u_ice, 'U', -1. ) |
|---|
| 555 | |
|---|
| 556 | #if defined key_agrif |
|---|
| 557 | !! CALL agrif_interp_lim3( 'U', jter, nn_nevp ) |
|---|
| 558 | CALL agrif_interp_lim3( 'U' ) |
|---|
| 559 | #endif |
|---|
| 560 | IF( ln_bdy ) CALL bdy_ice_dyn( 'U' ) |
|---|
| 561 | |
|---|
| 562 | DO jj = 2, jpjm1 |
|---|
| 563 | DO ji = fs_2, fs_jpim1 |
|---|
| 564 | |
|---|
| 565 | ! tau_io/(v_oce - v_ice) |
|---|
| 566 | zTauO = zaV(ji,jj) * zrhoco * SQRT( ( v_ice (ji,jj) - v_oce (ji,jj) ) * ( v_ice (ji,jj) - v_oce (ji,jj) ) & |
|---|
| 567 | & + ( u_iceV(ji,jj) - u_oceV(ji,jj) ) * ( u_iceV(ji,jj) - u_oceV(ji,jj) ) ) |
|---|
| 568 | |
|---|
| 569 | ! Ocean-to-Ice stress |
|---|
| 570 | ztauy_oi(ji,jj) = zTauO * ( v_oce(ji,jj) - v_ice(ji,jj) ) |
|---|
| 571 | |
|---|
| 572 | ! tau_bottom/v_ice |
|---|
| 573 | zvel = MAX( zepsi, SQRT( v_ice(ji,jj) * v_ice(ji,jj) + u_iceV(ji,jj) * u_iceV(ji,jj) ) ) |
|---|
| 574 | ztauB = - tau_icebfr(ji,jj) / zvel |
|---|
| 575 | |
|---|
| 576 | ! Coriolis at V-points (energy conserving formulation) |
|---|
| 577 | zCory(ji,jj) = - 0.25_wp * r1_e2v(ji,jj) * & |
|---|
| 578 | & ( zmf(ji,jj ) * ( e2u(ji,jj ) * u_ice(ji,jj ) + e2u(ji-1,jj ) * u_ice(ji-1,jj ) ) & |
|---|
| 579 | & + zmf(ji,jj+1) * ( e2u(ji,jj+1) * u_ice(ji,jj+1) + e2u(ji-1,jj+1) * u_ice(ji-1,jj+1) ) ) |
|---|
| 580 | |
|---|
| 581 | ! Sum of external forces (explicit solution) = F + tau_ia + Coriolis + spg + tau_io |
|---|
| 582 | zTauE = zfV(ji,jj) + zTauV_ia(ji,jj) + zCory(ji,jj) + zspgV(ji,jj) + ztauy_oi(ji,jj) |
|---|
| 583 | |
|---|
| 584 | ! landfast switch => 0 = static friction (tau_icebfr > zTauE); 1 = sliding friction |
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| 585 | rswitch = 1._wp - MIN( 1._wp, ABS( SIGN( 1._wp, zTauE - tau_icebfr(ji,jj) ) - SIGN( 1._wp, zTauE ) ) ) |
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| 586 | |
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| 587 | ! ice velocity using implicit formulation (cf Madec doc & Bouillon 2009) |
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| 588 | v_ice(ji,jj) = ( ( rswitch * ( zmV_t(ji,jj) * v_ice(ji,jj) & ! previous velocity |
|---|
| 589 | & + zTauE + zTauO * v_ice(ji,jj) & ! F + tau_ia + Coriolis + spg + tau_io(only ocean part) |
|---|
| 590 | & ) / MAX( zepsi, zmV_t(ji,jj) + zTauO - zTauB ) & ! m/dt + tau_io(only ice part) + landfast |
|---|
| 591 | & + ( 1._wp - rswitch ) * v_ice(ji,jj) * MAX( 0._wp, 1._wp - zdtevp * rn_lfrelax ) & ! static friction => slow decrease to v=0 |
|---|
| 592 | & ) * zswitchV(ji,jj) + v_oce(ji,jj) * ( 1._wp - zswitchV(ji,jj) ) & ! v_ice = v_oce if mass < zmmin |
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| 593 | & ) * zmaskV(ji,jj) |
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| 594 | ! Bouillon 2013 |
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| 595 | !!v_ice(ji,jj) = ( zmV_t(ji,jj) * ( zbeta * v_ice(ji,jj) + v_ice_b(ji,jj) ) & |
|---|
| 596 | !! & + zfV(ji,jj) + zCory(ji,jj) + zTauV_ia(ji,jj) + zTauO * v_oce(ji,jj) + zspgV(ji,jj) & |
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| 597 | !! & ) / MAX( zmV_t(ji,jj) * ( zbeta + 1._wp ) + zTauO - zTauB, zepsi ) * zswitchV(ji,jj) |
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| 598 | END DO |
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| 599 | END DO |
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| 600 | CALL lbc_lnk( v_ice, 'V', -1. ) |
|---|
| 601 | |
|---|
| 602 | #if defined key_agrif |
|---|
| 603 | !! CALL agrif_interp_lim3( 'V', jter, nn_nevp ) |
|---|
| 604 | CALL agrif_interp_lim3( 'V' ) |
|---|
| 605 | #endif |
|---|
| 606 | IF( ln_bdy ) CALL bdy_ice_dyn( 'V' ) |
|---|
| 607 | |
|---|
| 608 | ENDIF |
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| 609 | |
|---|
| 610 | IF(ln_ctl) THEN ! Convergence test |
|---|
| 611 | DO jj = 2 , jpjm1 |
|---|
| 612 | zresr(:,jj) = MAX( ABS( u_ice(:,jj) - zu_ice(:,jj) ), ABS( v_ice(:,jj) - zv_ice(:,jj) ) ) |
|---|
| 613 | END DO |
|---|
| 614 | zresm = MAXVAL( zresr( 1:jpi, 2:jpjm1 ) ) |
|---|
| 615 | IF( lk_mpp ) CALL mpp_max( zresm ) ! max over the global domain |
|---|
| 616 | ENDIF |
|---|
| 617 | ! |
|---|
| 618 | ! ! ==================== ! |
|---|
| 619 | END DO ! end loop over jter ! |
|---|
| 620 | ! ! ==================== ! |
|---|
| 621 | ! |
|---|
| 622 | !------------------------------------------------------------------------------! |
|---|
| 623 | ! 4) Recompute delta, shear and div (inputs for mechanical redistribution) |
|---|
| 624 | !------------------------------------------------------------------------------! |
|---|
| 625 | DO jj = 1, jpjm1 |
|---|
| 626 | DO ji = 1, jpim1 |
|---|
| 627 | |
|---|
| 628 | ! shear at F points |
|---|
| 629 | zds(ji,jj) = ( ( u_ice(ji,jj+1) * r1_e1u(ji,jj+1) - u_ice(ji,jj) * r1_e1u(ji,jj) ) * e1f(ji,jj) * e1f(ji,jj) & |
|---|
| 630 | & + ( v_ice(ji+1,jj) * r1_e2v(ji+1,jj) - v_ice(ji,jj) * r1_e2v(ji,jj) ) * e2f(ji,jj) * e2f(ji,jj) & |
|---|
| 631 | & ) * r1_e1e2f(ji,jj) * zfmask(ji,jj) |
|---|
| 632 | |
|---|
| 633 | END DO |
|---|
| 634 | END DO |
|---|
| 635 | CALL lbc_lnk( zds, 'F', 1. ) |
|---|
| 636 | |
|---|
| 637 | DO jj = 2, jpjm1 |
|---|
| 638 | DO ji = 2, jpim1 ! no vector loop |
|---|
| 639 | |
|---|
| 640 | ! tension**2 at T points |
|---|
| 641 | zdt = ( ( u_ice(ji,jj) * r1_e2u(ji,jj) - u_ice(ji-1,jj) * r1_e2u(ji-1,jj) ) * e2t(ji,jj) * e2t(ji,jj) & |
|---|
| 642 | & - ( v_ice(ji,jj) * r1_e1v(ji,jj) - v_ice(ji,jj-1) * r1_e1v(ji,jj-1) ) * e1t(ji,jj) * e1t(ji,jj) & |
|---|
| 643 | & ) * r1_e1e2t(ji,jj) |
|---|
| 644 | zdt2 = zdt * zdt |
|---|
| 645 | |
|---|
| 646 | ! shear**2 at T points (doc eq. A16) |
|---|
| 647 | zds2 = ( zds(ji,jj ) * zds(ji,jj ) * e1e2f(ji,jj ) + zds(ji-1,jj ) * zds(ji-1,jj ) * e1e2f(ji-1,jj ) & |
|---|
| 648 | & + zds(ji,jj-1) * zds(ji,jj-1) * e1e2f(ji,jj-1) + zds(ji-1,jj-1) * zds(ji-1,jj-1) * e1e2f(ji-1,jj-1) & |
|---|
| 649 | & ) * 0.25_wp * r1_e1e2t(ji,jj) |
|---|
| 650 | |
|---|
| 651 | ! shear at T points |
|---|
| 652 | shear_i(ji,jj) = SQRT( zdt2 + zds2 ) |
|---|
| 653 | |
|---|
| 654 | ! divergence at T points |
|---|
| 655 | divu_i(ji,jj) = ( e2u(ji,jj) * u_ice(ji,jj) - e2u(ji-1,jj) * u_ice(ji-1,jj) & |
|---|
| 656 | & + e1v(ji,jj) * v_ice(ji,jj) - e1v(ji,jj-1) * v_ice(ji,jj-1) & |
|---|
| 657 | & ) * r1_e1e2t(ji,jj) |
|---|
| 658 | |
|---|
| 659 | ! delta at T points |
|---|
| 660 | zdelta = SQRT( divu_i(ji,jj) * divu_i(ji,jj) + ( zdt2 + zds2 ) * z1_ecc2 ) |
|---|
| 661 | rswitch = 1._wp - MAX( 0._wp, SIGN( 1._wp, -zdelta ) ) ! 0 if delta=0 |
|---|
| 662 | delta_i(ji,jj) = zdelta + rn_creepl * rswitch |
|---|
| 663 | |
|---|
| 664 | END DO |
|---|
| 665 | END DO |
|---|
| 666 | CALL lbc_lnk_multi( shear_i, 'T', 1., divu_i, 'T', 1., delta_i, 'T', 1. ) |
|---|
| 667 | |
|---|
| 668 | ! --- Store the stress tensor for the next time step --- ! |
|---|
| 669 | stress1_i (:,:) = zs1 (:,:) |
|---|
| 670 | stress2_i (:,:) = zs2 (:,:) |
|---|
| 671 | stress12_i(:,:) = zs12(:,:) |
|---|
| 672 | ! |
|---|
| 673 | |
|---|
| 674 | !------------------------------------------------------------------------------! |
|---|
| 675 | ! 5) SIMIP diagnostics |
|---|
| 676 | !------------------------------------------------------------------------------! |
|---|
| 677 | |
|---|
| 678 | DO jj = 2, jpjm1 |
|---|
| 679 | DO ji = 2, jpim1 |
|---|
| 680 | rswitch = MAX( 0._wp , SIGN( 1._wp , at_i(ji,jj) - epsi06 ) ) ! 1 if ice, 0 if no ice |
|---|
| 681 | |
|---|
| 682 | ! Stress tensor invariants (normal and shear stress N/m) |
|---|
| 683 | diag_sig1(ji,jj) = ( zs1(ji,jj) + zs2(ji,jj) ) * rswitch ! normal stress |
|---|
| 684 | diag_sig2(ji,jj) = SQRT( ( zs1(ji,jj) - zs2(ji,jj) )**2 + 4*zs12(ji,jj)**2 ) * rswitch ! shear stress |
|---|
| 685 | |
|---|
| 686 | ! Stress terms of the momentum equation (N/m2) |
|---|
| 687 | diag_dssh_dx(ji,jj) = zspgU(ji,jj) * rswitch ! sea surface slope stress term |
|---|
| 688 | diag_dssh_dy(ji,jj) = zspgV(ji,jj) * rswitch |
|---|
| 689 | |
|---|
| 690 | diag_corstrx(ji,jj) = zCorx(ji,jj) * rswitch ! Coriolis stress term |
|---|
| 691 | diag_corstry(ji,jj) = zCory(ji,jj) * rswitch |
|---|
| 692 | |
|---|
| 693 | diag_intstrx(ji,jj) = zfU(ji,jj) * rswitch ! internal stress term |
|---|
| 694 | diag_intstry(ji,jj) = zfV(ji,jj) * rswitch |
|---|
| 695 | |
|---|
| 696 | diag_utau_oi(ji,jj) = ztaux_oi(ji,jj) * rswitch ! oceanic stress |
|---|
| 697 | diag_vtau_oi(ji,jj) = ztauy_oi(ji,jj) * rswitch |
|---|
| 698 | |
|---|
| 699 | ! 2D ice mass, snow mass, area transport arrays (X, Y) |
|---|
| 700 | zfac_x = 0.5 * u_ice(ji,jj) * e2u(ji,jj) * rswitch |
|---|
| 701 | zfac_y = 0.5 * v_ice(ji,jj) * e1v(ji,jj) * rswitch |
|---|
| 702 | |
|---|
| 703 | diag_xmtrp_ice(ji,jj) = rhoic * zfac_x * ( vt_i(ji+1,jj) + vt_i(ji,jj) ) ! ice mass transport, X-component |
|---|
| 704 | diag_ymtrp_ice(ji,jj) = rhoic * zfac_y * ( vt_i(ji,jj+1) + vt_i(ji,jj) ) ! '' Y- '' |
|---|
| 705 | |
|---|
| 706 | diag_xmtrp_snw(ji,jj) = rhosn * zfac_x * ( vt_s(ji+1,jj) + vt_s(ji,jj) ) ! snow mass transport, X-component |
|---|
| 707 | diag_ymtrp_snw(ji,jj) = rhosn * zfac_y * ( vt_s(ji,jj+1) + vt_s(ji,jj) ) ! '' Y- '' |
|---|
| 708 | |
|---|
| 709 | diag_xatrp(ji,jj) = zfac_x * ( at_i(ji+1,jj) + at_i(ji,jj) ) ! area transport, X-component |
|---|
| 710 | diag_yatrp(ji,jj) = zfac_y * ( at_i(ji,jj+1) + at_i(ji,jj) ) ! '' Y- '' |
|---|
| 711 | |
|---|
| 712 | END DO |
|---|
| 713 | END DO |
|---|
| 714 | |
|---|
| 715 | CALL lbc_lnk_multi( diag_sig1 , 'T', 1., diag_sig2 , 'T', 1., & |
|---|
| 716 | & diag_dssh_dx, 'U', -1., diag_dssh_dy, 'V', -1., & |
|---|
| 717 | & diag_corstrx, 'U', -1., diag_corstry, 'V', -1., & |
|---|
| 718 | & diag_intstrx, 'U', -1., diag_intstry, 'V', -1. ) |
|---|
| 719 | |
|---|
| 720 | CALL lbc_lnk_multi( diag_utau_oi, 'U', -1., diag_vtau_oi, 'V', -1. ) |
|---|
| 721 | |
|---|
| 722 | CALL lbc_lnk_multi( diag_xmtrp_ice, 'U', -1., diag_xmtrp_snw, 'U', -1., & |
|---|
| 723 | & diag_xatrp , 'U', -1., diag_ymtrp_ice, 'V', -1., & |
|---|
| 724 | & diag_ymtrp_snw, 'V', -1., diag_yatrp , 'V', -1. ) |
|---|
| 725 | |
|---|
| 726 | ! |
|---|
| 727 | !------------------------------------------------------------------------------! |
|---|
| 728 | ! 6) Control prints of residual and charge ellipse |
|---|
| 729 | !------------------------------------------------------------------------------! |
|---|
| 730 | ! |
|---|
| 731 | ! print the residual for convergence |
|---|
| 732 | IF(ln_ctl) THEN |
|---|
| 733 | WRITE(charout,FMT="('ice_rhg_evp : res =',D23.16, ' iter =',I4)") zresm, jter |
|---|
| 734 | CALL prt_ctl_info(charout) |
|---|
| 735 | CALL prt_ctl(tab2d_1=u_ice, clinfo1=' ice_rhg_evp : u_ice :', tab2d_2=v_ice, clinfo2=' v_ice :') |
|---|
| 736 | ENDIF |
|---|
| 737 | |
|---|
| 738 | ! print charge ellipse |
|---|
| 739 | ! This can be desactivated once the user is sure that the stress state |
|---|
| 740 | ! lie on the charge ellipse. See Bouillon et al. 08 for more details |
|---|
| 741 | IF(ln_ctl) THEN |
|---|
| 742 | IF( MOD(kt_ice+nn_fsbc-1,nwrite) == 0 ) THEN |
|---|
| 743 | WRITE(charout,FMT="('ice_rhg_evp :', I4, I6, I1, I1, A10)") 1000, kt_ice, 0, 0, ' ch. ell. ' |
|---|
| 744 | CALL prt_ctl_info(charout) |
|---|
| 745 | DO jj = 2, jpjm1 |
|---|
| 746 | DO ji = 2, jpim1 |
|---|
| 747 | IF (strength(ji,jj) > 1.0) THEN |
|---|
| 748 | zsig1 = ( zs1(ji,jj) + SQRT(zs2(ji,jj)**2 + 4*zs12(ji,jj)**2 ) ) / ( 2*strength(ji,jj) ) |
|---|
| 749 | zsig2 = ( zs1(ji,jj) - SQRT(zs2(ji,jj)**2 + 4*zs12(ji,jj)**2 ) ) / ( 2*strength(ji,jj) ) |
|---|
| 750 | WRITE(charout,FMT="('ice_rhg_evp :', I4, I4, D23.16, D23.16, D23.16, D23.16, A10)") |
|---|
| 751 | CALL prt_ctl_info(charout) |
|---|
| 752 | ENDIF |
|---|
| 753 | END DO |
|---|
| 754 | END DO |
|---|
| 755 | WRITE(charout,FMT="('ice_rhg_evp :', I4, I6, I1, I1, A10)") 2000, kt_ice, 0, 0, ' ch. ell. ' |
|---|
| 756 | CALL prt_ctl_info(charout) |
|---|
| 757 | ENDIF |
|---|
| 758 | ENDIF |
|---|
| 759 | ! |
|---|
| 760 | END SUBROUTINE ice_rhg_evp |
|---|
| 761 | |
|---|
| 762 | #endif |
|---|
| 763 | |
|---|
| 764 | !!============================================================================== |
|---|
| 765 | END MODULE icerhg_evp |
|---|
