| 1 | MODULE icedyn_rhg_evp |
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| 2 | !!====================================================================== |
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| 3 | !! *** MODULE icedyn_rhg_evp *** |
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| 4 | !! Sea-Ice dynamics : rheology Elasto-Viscous-Plastic |
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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) adaptation to new model |
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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 case |
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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 + mEVP (Bouillon 2013) |
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| 13 | !! 3.7 ! 2017 (C. Rousset) add aEVP (Kimmritz 2016-2017) |
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| 14 | !! 4.0 ! 2018 (many people) SI3 [aka Sea Ice cube] |
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| 15 | !!---------------------------------------------------------------------- |
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| 16 | #if defined key_si3 |
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| 17 | !!---------------------------------------------------------------------- |
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| 18 | !! 'key_si3' SI3 sea-ice model |
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| 19 | !!---------------------------------------------------------------------- |
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| 20 | !! ice_dyn_rhg_evp : computes ice velocities from EVP rheology |
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| 21 | !! rhg_evp_rst : read/write EVP fields in ice restart |
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| 22 | !!---------------------------------------------------------------------- |
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| 23 | USE phycst ! Physical constant |
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| 24 | USE dom_oce ! Ocean domain |
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| 25 | USE sbc_oce , ONLY : ln_ice_embd, nn_fsbc, ssh_m |
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| 26 | USE sbc_ice , ONLY : utau_ice, vtau_ice, snwice_mass, snwice_mass_b |
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| 27 | USE ice ! sea-ice: ice variables |
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| 28 | USE icedyn_rdgrft ! sea-ice: ice strength |
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| 29 | USE bdy_oce , ONLY : ln_bdy |
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| 30 | USE bdyice |
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| 31 | #if defined key_agrif |
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| 32 | USE agrif_ice_interp |
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| 33 | #endif |
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| 34 | ! |
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| 35 | USE in_out_manager ! I/O manager |
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| 36 | USE iom ! I/O manager library |
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| 37 | USE lib_mpp ! MPP library |
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| 38 | USE lib_fortran ! fortran utilities (glob_sum + no signed zero) |
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| 39 | USE lbclnk ! lateral boundary conditions (or mpp links) |
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| 40 | USE prtctl ! Print control |
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| 41 | |
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| 42 | IMPLICIT NONE |
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| 43 | PRIVATE |
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| 44 | |
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| 45 | PUBLIC ice_dyn_rhg_evp ! called by icedyn_rhg.F90 |
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| 46 | PUBLIC rhg_evp_rst ! called by icedyn_rhg.F90 |
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| 47 | |
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| 48 | !! * Substitutions |
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| 49 | # include "vectopt_loop_substitute.h90" |
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| 50 | !!---------------------------------------------------------------------- |
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| 51 | !! NEMO/ICE 4.0 , NEMO Consortium (2018) |
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| 52 | !! $Id: icedyn_rhg_evp.F90 8378 2017-07-26 13:55:59Z clem $ |
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| 53 | !! Software governed by the CeCILL licence (./LICENSE) |
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| 54 | !!---------------------------------------------------------------------- |
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| 55 | CONTAINS |
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| 56 | |
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| 57 | SUBROUTINE ice_dyn_rhg_evp( kt, pstress1_i, pstress2_i, pstress12_i, pshear_i, pdivu_i, pdelta_i ) |
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| 58 | !!------------------------------------------------------------------- |
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| 59 | !! *** SUBROUTINE ice_dyn_rhg_evp *** |
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| 60 | !! EVP-C-grid |
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| 61 | !! |
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| 62 | !! ** purpose : determines sea ice drift from wind stress, ice-ocean |
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| 63 | !! stress and sea-surface slope. Ice-ice interaction is described by |
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| 64 | !! a non-linear elasto-viscous-plastic (EVP) law including shear |
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| 65 | !! strength and a bulk rheology (Hunke and Dukowicz, 2002). |
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| 66 | !! |
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| 67 | !! The points in the C-grid look like this, dear reader |
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| 68 | !! |
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| 69 | !! (ji,jj) |
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| 70 | !! | |
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| 71 | !! | |
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| 72 | !! (ji-1,jj) | (ji,jj) |
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| 73 | !! --------- |
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| 74 | !! | | |
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| 75 | !! | (ji,jj) |------(ji,jj) |
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| 76 | !! | | |
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| 77 | !! --------- |
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| 78 | !! (ji-1,jj-1) (ji,jj-1) |
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| 79 | !! |
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| 80 | !! ** Inputs : - wind forcing (stress), oceanic currents |
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| 81 | !! ice total volume (vt_i) per unit area |
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| 82 | !! snow total volume (vt_s) per unit area |
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| 83 | !! |
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| 84 | !! ** Action : - compute u_ice, v_ice : the components of the |
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| 85 | !! sea-ice velocity vector |
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| 86 | !! - compute delta_i, shear_i, divu_i, which are inputs |
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| 87 | !! of the ice thickness distribution |
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| 88 | !! |
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| 89 | !! ** Steps : 0) compute mask at F point |
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| 90 | !! 1) Compute ice snow mass, ice strength |
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| 91 | !! 2) Compute wind, oceanic stresses, mass terms and |
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| 92 | !! coriolis terms of the momentum equation |
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| 93 | !! 3) Solve the momentum equation (iterative procedure) |
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| 94 | !! 4) Recompute delta, shear and divergence |
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| 95 | !! (which are inputs of the ITD) & store stress |
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| 96 | !! for the next time step |
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| 97 | !! 5) Diagnostics including charge ellipse |
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| 98 | !! |
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| 99 | !! ** Notes : There is the possibility to use aEVP from the nice work of Kimmritz et al. (2016 & 2017) |
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| 100 | !! by setting up ln_aEVP=T (i.e. changing alpha and beta parameters). |
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| 101 | !! This is an upgraded version of mEVP from Bouillon et al. 2013 |
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| 102 | !! (i.e. more stable and better convergence) |
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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 | !! Kimmritz et al., Ocean Modelling 2016 & 2017 |
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| 108 | !!------------------------------------------------------------------- |
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| 109 | INTEGER , INTENT(in ) :: kt ! time step |
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| 110 | REAL(wp), DIMENSION(:,:), INTENT(inout) :: pstress1_i, pstress2_i, pstress12_i ! |
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| 111 | REAL(wp), DIMENSION(:,:), INTENT( out) :: pshear_i , pdivu_i , pdelta_i ! |
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| 112 | !! |
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| 113 | INTEGER :: ji, jj ! dummy loop indices |
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| 114 | INTEGER :: jter ! local integers |
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| 115 | ! |
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| 116 | REAL(wp) :: zrhoco ! rau0 * rn_cio |
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| 117 | REAL(wp) :: zdtevp, z1_dtevp ! time step for subcycling |
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| 118 | REAL(wp) :: ecc2, z1_ecc2 ! square of yield ellipse eccenticity |
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| 119 | REAL(wp) :: zalph1, z1_alph1, zalph2, z1_alph2 ! alpha coef from Bouillon 2009 or Kimmritz 2017 |
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| 120 | REAL(wp) :: zm1, zm2, zm3, zmassU, zmassV ! ice/snow mass |
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| 121 | REAL(wp) :: zdelta, zp_delf, zds2, zdt, zdt2, zdiv, zdiv2 ! temporary scalars |
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| 122 | REAL(wp) :: zTauO, zTauB, zTauE, zvel ! temporary scalars |
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| 123 | ! |
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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 | REAL(wp) :: zshear, zdum1, zdum2 |
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| 128 | ! |
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| 129 | REAL(wp), DIMENSION(jpi,jpj) :: z1_e1t0, z1_e2t0 ! scale factors |
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| 130 | REAL(wp), DIMENSION(jpi,jpj) :: zp_delt ! P/delta at T points |
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| 131 | REAL(wp), DIMENSION(jpi,jpj) :: zbeta ! beta coef from Kimmritz 2017 |
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| 132 | ! |
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| 133 | REAL(wp), DIMENSION(jpi,jpj) :: zdt_m ! (dt / ice-snow_mass) on T points |
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| 134 | REAL(wp), DIMENSION(jpi,jpj) :: zaU , zaV ! ice fraction on U/V points |
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| 135 | REAL(wp), DIMENSION(jpi,jpj) :: zmU_t, zmV_t ! (ice-snow_mass / dt) on U/V points |
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| 136 | REAL(wp), DIMENSION(jpi,jpj) :: zmf ! coriolis parameter at T points |
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| 137 | REAL(wp), DIMENSION(jpi,jpj) :: zTauU_ia , ztauV_ia ! ice-atm. stress at U-V points |
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| 138 | REAL(wp), DIMENSION(jpi,jpj) :: zspgU , zspgV ! surface pressure gradient at U/V points |
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| 139 | 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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| 140 | REAL(wp), DIMENSION(jpi,jpj) :: zfU , zfV ! internal stresses |
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| 141 | ! |
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| 142 | REAL(wp), DIMENSION(jpi,jpj) :: zds ! shear |
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| 143 | REAL(wp), DIMENSION(jpi,jpj) :: zs1, zs2, zs12 ! stress tensor components |
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| 144 | REAL(wp), DIMENSION(jpi,jpj) :: zu_ice, zv_ice, zresr ! check convergence |
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| 145 | REAL(wp), DIMENSION(jpi,jpj) :: zpice ! array used for the calculation of ice surface slope: |
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| 146 | ! ! ocean surface (ssh_m) if ice is not embedded |
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| 147 | ! ! ice top surface if ice is embedded |
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| 148 | REAL(wp), DIMENSION(jpi,jpj) :: zCorx, zCory ! Coriolis stress array |
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| 149 | REAL(wp), DIMENSION(jpi,jpj) :: ztaux_oi, ztauy_oi ! Ocean-to-ice stress array |
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| 150 | ! |
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| 151 | REAL(wp), DIMENSION(jpi,jpj) :: zswitchU, zswitchV ! dummy arrays |
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| 152 | REAL(wp), DIMENSION(jpi,jpj) :: zmaskU, zmaskV ! mask for ice presence |
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| 153 | REAL(wp), DIMENSION(jpi,jpj) :: zfmask, zwf ! mask at F points for the ice |
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| 154 | |
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| 155 | REAL(wp), PARAMETER :: zepsi = 1.0e-20_wp ! tolerance parameter |
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| 156 | REAL(wp), PARAMETER :: zmmin = 1._wp ! ice mass (kg/m2) below which ice velocity equals ocean velocity |
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| 157 | !! --- diags |
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| 158 | REAL(wp), DIMENSION(jpi,jpj) :: zswi |
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| 159 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: zsig1, zsig2, zsig3 |
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| 160 | !! --- SIMIP diags |
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| 161 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: zdiag_sig1 ! Average normal stress in sea ice |
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| 162 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: zdiag_sig2 ! Maximum shear stress in sea ice |
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| 163 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: zdiag_dssh_dx ! X-direction sea-surface tilt term (N/m2) |
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| 164 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: zdiag_dssh_dy ! X-direction sea-surface tilt term (N/m2) |
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| 165 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: zdiag_corstrx ! X-direction coriolis stress (N/m2) |
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| 166 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: zdiag_corstry ! Y-direction coriolis stress (N/m2) |
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| 167 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: zdiag_intstrx ! X-direction internal stress (N/m2) |
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| 168 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: zdiag_intstry ! Y-direction internal stress (N/m2) |
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| 169 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: zdiag_utau_oi ! X-direction ocean-ice stress |
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| 170 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: zdiag_vtau_oi ! Y-direction ocean-ice stress |
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| 171 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: zdiag_xmtrp_ice ! X-component of ice mass transport (kg/s) |
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| 172 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: zdiag_ymtrp_ice ! Y-component of ice mass transport (kg/s) |
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| 173 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: zdiag_xmtrp_snw ! X-component of snow mass transport (kg/s) |
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| 174 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: zdiag_ymtrp_snw ! Y-component of snow mass transport (kg/s) |
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| 175 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: zdiag_xatrp ! X-component of area transport (m2/s) |
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| 176 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: zdiag_yatrp ! Y-component of area transport (m2/s) |
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| 177 | !!------------------------------------------------------------------- |
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| 178 | |
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| 179 | IF( kt == nit000 .AND. lwp ) WRITE(numout,*) '-- ice_dyn_rhg_evp: EVP sea-ice rheology' |
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| 180 | ! |
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| 181 | !!gm for Clem: OPTIMIZATION: I think zfmask can be computed one for all at the initialization.... |
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| 182 | !------------------------------------------------------------------------------! |
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| 183 | ! 0) mask at F points for the ice |
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| 184 | !------------------------------------------------------------------------------! |
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| 185 | ! ocean/land mask |
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| 186 | DO jj = 1, jpjm1 |
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| 187 | DO ji = 1, jpim1 ! NO vector opt. |
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| 188 | 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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| 189 | END DO |
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| 190 | END DO |
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| 191 | CALL lbc_lnk( zfmask, 'F', 1._wp ) |
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| 192 | |
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| 193 | ! Lateral boundary conditions on velocity (modify zfmask) |
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| 194 | zwf(:,:) = zfmask(:,:) |
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| 195 | DO jj = 2, jpjm1 |
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| 196 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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| 197 | IF( zfmask(ji,jj) == 0._wp ) THEN |
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| 198 | 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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| 199 | ENDIF |
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| 200 | END DO |
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| 201 | END DO |
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| 202 | DO jj = 2, jpjm1 |
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| 203 | IF( zfmask(1,jj) == 0._wp ) THEN |
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| 204 | zfmask(1 ,jj) = rn_ishlat * MIN( 1._wp , MAX( zwf(2,jj), zwf(1,jj+1), zwf(1,jj-1) ) ) |
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| 205 | ENDIF |
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| 206 | IF( zfmask(jpi,jj) == 0._wp ) THEN |
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| 207 | zfmask(jpi,jj) = rn_ishlat * MIN( 1._wp , MAX( zwf(jpi,jj+1), zwf(jpim1,jj), zwf(jpi,jj-1) ) ) |
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| 208 | ENDIF |
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| 209 | END DO |
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| 210 | DO ji = 2, jpim1 |
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| 211 | IF( zfmask(ji,1) == 0._wp ) THEN |
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| 212 | zfmask(ji,1 ) = rn_ishlat * MIN( 1._wp , MAX( zwf(ji+1,1), zwf(ji,2), zwf(ji-1,1) ) ) |
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| 213 | ENDIF |
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| 214 | IF( zfmask(ji,jpj) == 0._wp ) THEN |
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| 215 | zfmask(ji,jpj) = rn_ishlat * MIN( 1._wp , MAX( zwf(ji+1,jpj), zwf(ji-1,jpj), zwf(ji,jpjm1) ) ) |
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| 216 | ENDIF |
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| 217 | END DO |
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| 218 | CALL lbc_lnk( zfmask, 'F', 1._wp ) |
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| 219 | |
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| 220 | !------------------------------------------------------------------------------! |
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| 221 | ! 1) define some variables and initialize arrays |
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| 222 | !------------------------------------------------------------------------------! |
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| 223 | zrhoco = rau0 * rn_cio |
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| 224 | |
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| 225 | ! ecc2: square of yield ellipse eccenticrity |
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| 226 | ecc2 = rn_ecc * rn_ecc |
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| 227 | z1_ecc2 = 1._wp / ecc2 |
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| 228 | |
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| 229 | ! Time step for subcycling |
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| 230 | zdtevp = rdt_ice / REAL( nn_nevp ) |
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| 231 | z1_dtevp = 1._wp / zdtevp |
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| 232 | |
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| 233 | ! alpha parameters (Bouillon 2009) |
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| 234 | IF( .NOT. ln_aEVP ) THEN |
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| 235 | zalph1 = ( 2._wp * rn_relast * rdt_ice ) * z1_dtevp |
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| 236 | zalph2 = zalph1 * z1_ecc2 |
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| 237 | |
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| 238 | z1_alph1 = 1._wp / ( zalph1 + 1._wp ) |
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| 239 | z1_alph2 = 1._wp / ( zalph2 + 1._wp ) |
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| 240 | ENDIF |
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| 241 | |
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| 242 | ! Initialise stress tensor |
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| 243 | zs1 (:,:) = pstress1_i (:,:) |
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| 244 | zs2 (:,:) = pstress2_i (:,:) |
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| 245 | zs12(:,:) = pstress12_i(:,:) |
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| 246 | |
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| 247 | ! Ice strength |
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| 248 | CALL ice_strength |
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| 249 | |
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| 250 | ! scale factors |
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| 251 | DO jj = 2, jpjm1 |
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| 252 | DO ji = fs_2, fs_jpim1 |
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| 253 | z1_e1t0(ji,jj) = 1._wp / ( e1t(ji+1,jj ) + e1t(ji,jj ) ) |
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| 254 | z1_e2t0(ji,jj) = 1._wp / ( e2t(ji ,jj+1) + e2t(ji,jj ) ) |
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| 255 | END DO |
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| 256 | END DO |
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| 257 | |
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| 258 | ! |
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| 259 | !------------------------------------------------------------------------------! |
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| 260 | ! 2) Wind / ocean stress, mass terms, coriolis terms |
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| 261 | !------------------------------------------------------------------------------! |
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| 262 | |
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| 263 | IF( ln_ice_embd ) THEN !== embedded sea ice: compute representative ice top surface ==! |
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| 264 | ! |
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| 265 | ! average interpolation coeff as used in dynspg = (1/nn_fsbc) * {SUM[n/nn_fsbc], n=0,nn_fsbc-1} |
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| 266 | ! = (1/nn_fsbc)^2 * {SUM[n] , n=0,nn_fsbc-1} |
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| 267 | zintn = REAL( nn_fsbc - 1 ) / REAL( nn_fsbc ) * 0.5_wp |
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| 268 | ! |
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| 269 | ! average interpolation coeff as used in dynspg = (1/nn_fsbc) * {SUM[1-n/nn_fsbc], n=0,nn_fsbc-1} |
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| 270 | ! = (1/nn_fsbc)^2 * (nn_fsbc^2 - {SUM[n], n=0,nn_fsbc-1}) |
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| 271 | zintb = REAL( nn_fsbc + 1 ) / REAL( nn_fsbc ) * 0.5_wp |
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| 272 | ! |
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| 273 | zpice(:,:) = ssh_m(:,:) + ( zintn * snwice_mass(:,:) + zintb * snwice_mass_b(:,:) ) * r1_rau0 |
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| 274 | ! |
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| 275 | ELSE !== non-embedded sea ice: use ocean surface for slope calculation ==! |
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| 276 | zpice(:,:) = ssh_m(:,:) |
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| 277 | ENDIF |
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| 278 | |
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| 279 | DO jj = 2, jpjm1 |
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| 280 | DO ji = fs_2, fs_jpim1 |
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| 281 | |
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| 282 | ! ice fraction at U-V points |
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| 283 | 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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| 284 | 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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| 285 | |
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| 286 | ! Ice/snow mass at U-V points |
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| 287 | zm1 = ( rhosn * vt_s(ji ,jj ) + rhoic * vt_i(ji ,jj ) ) |
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| 288 | zm2 = ( rhosn * vt_s(ji+1,jj ) + rhoic * vt_i(ji+1,jj ) ) |
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| 289 | zm3 = ( rhosn * vt_s(ji ,jj+1) + rhoic * vt_i(ji ,jj+1) ) |
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| 290 | 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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| 291 | 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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| 292 | |
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| 293 | ! Ocean currents at U-V points |
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| 294 | v_oceU(ji,jj) = 0.5_wp * ( ( v_oce(ji ,jj) + v_oce(ji ,jj-1) ) * e1t(ji+1,jj) & |
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| 295 | & + ( 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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| 296 | |
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| 297 | u_oceV(ji,jj) = 0.5_wp * ( ( u_oce(ji,jj ) + u_oce(ji-1,jj ) ) * e2t(ji,jj+1) & |
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| 298 | & + ( 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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| 299 | |
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| 300 | ! Coriolis at T points (m*f) |
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| 301 | zmf(ji,jj) = zm1 * ff_t(ji,jj) |
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| 302 | |
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| 303 | ! dt/m at T points (for alpha and beta coefficients) |
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| 304 | zdt_m(ji,jj) = zdtevp / MAX( zm1, zmmin ) |
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| 305 | |
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| 306 | ! m/dt |
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| 307 | zmU_t(ji,jj) = zmassU * z1_dtevp |
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| 308 | zmV_t(ji,jj) = zmassV * z1_dtevp |
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| 309 | |
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| 310 | ! Drag ice-atm. |
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| 311 | zTauU_ia(ji,jj) = zaU(ji,jj) * utau_ice(ji,jj) |
|---|
| 312 | zTauV_ia(ji,jj) = zaV(ji,jj) * vtau_ice(ji,jj) |
|---|
| 313 | |
|---|
| 314 | ! Surface pressure gradient (- m*g*GRAD(ssh)) at U-V points |
|---|
| 315 | zspgU(ji,jj) = - zmassU * grav * ( zpice(ji+1,jj) - zpice(ji,jj) ) * r1_e1u(ji,jj) |
|---|
| 316 | zspgV(ji,jj) = - zmassV * grav * ( zpice(ji,jj+1) - zpice(ji,jj) ) * r1_e2v(ji,jj) |
|---|
| 317 | |
|---|
| 318 | ! masks |
|---|
| 319 | zmaskU(ji,jj) = 1._wp - MAX( 0._wp, SIGN( 1._wp, -zmassU ) ) ! 0 if no ice |
|---|
| 320 | zmaskV(ji,jj) = 1._wp - MAX( 0._wp, SIGN( 1._wp, -zmassV ) ) ! 0 if no ice |
|---|
| 321 | |
|---|
| 322 | ! switches |
|---|
| 323 | zswitchU(ji,jj) = MAX( 0._wp, SIGN( 1._wp, zmassU - zmmin ) ) ! 0 if ice mass < zmmin |
|---|
| 324 | zswitchV(ji,jj) = MAX( 0._wp, SIGN( 1._wp, zmassV - zmmin ) ) ! 0 if ice mass < zmmin |
|---|
| 325 | |
|---|
| 326 | END DO |
|---|
| 327 | END DO |
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| 328 | CALL lbc_lnk_multi( zmf, 'T', 1., zdt_m, 'T', 1. ) |
|---|
| 329 | ! |
|---|
| 330 | !------------------------------------------------------------------------------! |
|---|
| 331 | ! 3) Solution of the momentum equation, iterative procedure |
|---|
| 332 | !------------------------------------------------------------------------------! |
|---|
| 333 | ! |
|---|
| 334 | ! !----------------------! |
|---|
| 335 | DO jter = 1 , nn_nevp ! loop over jter ! |
|---|
| 336 | ! !----------------------! |
|---|
| 337 | IF(ln_ctl) THEN ! Convergence test |
|---|
| 338 | DO jj = 1, jpjm1 |
|---|
| 339 | zu_ice(:,jj) = u_ice(:,jj) ! velocity at previous time step |
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| 340 | zv_ice(:,jj) = v_ice(:,jj) |
|---|
| 341 | END DO |
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| 342 | ENDIF |
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| 343 | |
|---|
| 344 | ! --- divergence, tension & shear (Appendix B of Hunke & Dukowicz, 2002) --- ! |
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| 345 | 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 |
|---|
| 346 | DO ji = 1, jpim1 |
|---|
| 347 | |
|---|
| 348 | ! shear at F points |
|---|
| 349 | 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) & |
|---|
| 350 | & + ( v_ice(ji+1,jj) * r1_e2v(ji+1,jj) - v_ice(ji,jj) * r1_e2v(ji,jj) ) * e2f(ji,jj) * e2f(ji,jj) & |
|---|
| 351 | & ) * r1_e1e2f(ji,jj) * zfmask(ji,jj) |
|---|
| 352 | |
|---|
| 353 | END DO |
|---|
| 354 | END DO |
|---|
| 355 | CALL lbc_lnk( zds, 'F', 1. ) |
|---|
| 356 | |
|---|
| 357 | DO jj = 2, jpj ! loop to jpi,jpj to avoid making a communication for zs1,zs2,zs12 |
|---|
| 358 | DO ji = 2, jpi ! no vector loop |
|---|
| 359 | |
|---|
| 360 | ! shear**2 at T points (doc eq. A16) |
|---|
| 361 | zds2 = ( zds(ji,jj ) * zds(ji,jj ) * e1e2f(ji,jj ) + zds(ji-1,jj ) * zds(ji-1,jj ) * e1e2f(ji-1,jj ) & |
|---|
| 362 | & + 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) & |
|---|
| 363 | & ) * 0.25_wp * r1_e1e2t(ji,jj) |
|---|
| 364 | |
|---|
| 365 | ! divergence at T points |
|---|
| 366 | zdiv = ( e2u(ji,jj) * u_ice(ji,jj) - e2u(ji-1,jj) * u_ice(ji-1,jj) & |
|---|
| 367 | & + e1v(ji,jj) * v_ice(ji,jj) - e1v(ji,jj-1) * v_ice(ji,jj-1) & |
|---|
| 368 | & ) * r1_e1e2t(ji,jj) |
|---|
| 369 | zdiv2 = zdiv * zdiv |
|---|
| 370 | |
|---|
| 371 | ! tension at T points |
|---|
| 372 | 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) & |
|---|
| 373 | & - ( v_ice(ji,jj) * r1_e1v(ji,jj) - v_ice(ji,jj-1) * r1_e1v(ji,jj-1) ) * e1t(ji,jj) * e1t(ji,jj) & |
|---|
| 374 | & ) * r1_e1e2t(ji,jj) |
|---|
| 375 | zdt2 = zdt * zdt |
|---|
| 376 | |
|---|
| 377 | ! delta at T points |
|---|
| 378 | zdelta = SQRT( zdiv2 + ( zdt2 + zds2 ) * z1_ecc2 ) |
|---|
| 379 | |
|---|
| 380 | ! P/delta at T points |
|---|
| 381 | zp_delt(ji,jj) = strength(ji,jj) / ( zdelta + rn_creepl ) |
|---|
| 382 | |
|---|
| 383 | ! alpha & beta for aEVP |
|---|
| 384 | ! gamma = 0.5*P/(delta+creepl) * (c*pi)**2/Area * dt/m |
|---|
| 385 | ! alpha = beta = sqrt(4*gamma) |
|---|
| 386 | IF( ln_aEVP ) THEN |
|---|
| 387 | zalph1 = MAX( 50._wp, rpi * SQRT( 0.5_wp * zp_delt(ji,jj) * r1_e1e2t(ji,jj) * zdt_m(ji,jj) ) ) |
|---|
| 388 | z1_alph1 = 1._wp / ( zalph1 + 1._wp ) |
|---|
| 389 | zalph2 = zalph1 |
|---|
| 390 | z1_alph2 = z1_alph1 |
|---|
| 391 | ENDIF |
|---|
| 392 | |
|---|
| 393 | ! stress at T points |
|---|
| 394 | zs1(ji,jj) = ( zs1(ji,jj) * zalph1 + zp_delt(ji,jj) * ( zdiv - zdelta ) ) * z1_alph1 |
|---|
| 395 | zs2(ji,jj) = ( zs2(ji,jj) * zalph2 + zp_delt(ji,jj) * ( zdt * z1_ecc2 ) ) * z1_alph2 |
|---|
| 396 | |
|---|
| 397 | END DO |
|---|
| 398 | END DO |
|---|
| 399 | CALL lbc_lnk( zp_delt, 'T', 1. ) |
|---|
| 400 | |
|---|
| 401 | DO jj = 1, jpjm1 |
|---|
| 402 | DO ji = 1, jpim1 |
|---|
| 403 | |
|---|
| 404 | ! alpha & beta for aEVP |
|---|
| 405 | IF( ln_aEVP ) THEN |
|---|
| 406 | zalph2 = MAX( 50._wp, rpi * SQRT( 0.5_wp * zp_delt(ji,jj) * r1_e1e2t(ji,jj) * zdt_m(ji,jj) ) ) |
|---|
| 407 | z1_alph2 = 1._wp / ( zalph2 + 1._wp ) |
|---|
| 408 | zbeta(ji,jj) = zalph2 |
|---|
| 409 | ENDIF |
|---|
| 410 | |
|---|
| 411 | ! P/delta at F points |
|---|
| 412 | 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) ) |
|---|
| 413 | |
|---|
| 414 | ! stress at F points |
|---|
| 415 | zs12(ji,jj)= ( zs12(ji,jj) * zalph2 + zp_delf * ( zds(ji,jj) * z1_ecc2 ) * 0.5_wp ) * z1_alph2 |
|---|
| 416 | |
|---|
| 417 | END DO |
|---|
| 418 | END DO |
|---|
| 419 | |
|---|
| 420 | ! --- Ice internal stresses (Appendix C of Hunke and Dukowicz, 2002) --- ! |
|---|
| 421 | DO jj = 2, jpjm1 |
|---|
| 422 | DO ji = fs_2, fs_jpim1 |
|---|
| 423 | ! !--- U points |
|---|
| 424 | zfU(ji,jj) = 0.5_wp * ( ( zs1(ji+1,jj) - zs1(ji,jj) ) * e2u(ji,jj) & |
|---|
| 425 | & + ( zs2(ji+1,jj) * e2t(ji+1,jj) * e2t(ji+1,jj) - zs2(ji,jj) * e2t(ji,jj) * e2t(ji,jj) & |
|---|
| 426 | & ) * r1_e2u(ji,jj) & |
|---|
| 427 | & + ( zs12(ji,jj) * e1f(ji,jj) * e1f(ji,jj) - zs12(ji,jj-1) * e1f(ji,jj-1) * e1f(ji,jj-1) & |
|---|
| 428 | & ) * 2._wp * r1_e1u(ji,jj) & |
|---|
| 429 | & ) * r1_e1e2u(ji,jj) |
|---|
| 430 | ! |
|---|
| 431 | ! !--- V points |
|---|
| 432 | zfV(ji,jj) = 0.5_wp * ( ( zs1(ji,jj+1) - zs1(ji,jj) ) * e1v(ji,jj) & |
|---|
| 433 | & - ( zs2(ji,jj+1) * e1t(ji,jj+1) * e1t(ji,jj+1) - zs2(ji,jj) * e1t(ji,jj) * e1t(ji,jj) & |
|---|
| 434 | & ) * r1_e1v(ji,jj) & |
|---|
| 435 | & + ( zs12(ji,jj) * e2f(ji,jj) * e2f(ji,jj) - zs12(ji-1,jj) * e2f(ji-1,jj) * e2f(ji-1,jj) & |
|---|
| 436 | & ) * 2._wp * r1_e2v(ji,jj) & |
|---|
| 437 | & ) * r1_e1e2v(ji,jj) |
|---|
| 438 | ! |
|---|
| 439 | ! !--- u_ice at V point |
|---|
| 440 | u_iceV(ji,jj) = 0.5_wp * ( ( u_ice(ji,jj ) + u_ice(ji-1,jj ) ) * e2t(ji,jj+1) & |
|---|
| 441 | & + ( u_ice(ji,jj+1) + u_ice(ji-1,jj+1) ) * e2t(ji,jj ) ) * z1_e2t0(ji,jj) * vmask(ji,jj,1) |
|---|
| 442 | ! |
|---|
| 443 | ! !--- v_ice at U point |
|---|
| 444 | v_iceU(ji,jj) = 0.5_wp * ( ( v_ice(ji ,jj) + v_ice(ji ,jj-1) ) * e1t(ji+1,jj) & |
|---|
| 445 | & + ( v_ice(ji+1,jj) + v_ice(ji+1,jj-1) ) * e1t(ji ,jj) ) * z1_e1t0(ji,jj) * umask(ji,jj,1) |
|---|
| 446 | END DO |
|---|
| 447 | END DO |
|---|
| 448 | ! |
|---|
| 449 | ! --- Computation of ice velocity --- ! |
|---|
| 450 | ! Bouillon et al. 2013 (eq 47-48) => unstable unless alpha, beta vary as in Kimmritz 2016 & 2017 |
|---|
| 451 | ! Bouillon et al. 2009 (eq 34-35) => stable |
|---|
| 452 | IF( MOD(jter,2) == 0 ) THEN ! even iterations |
|---|
| 453 | ! |
|---|
| 454 | DO jj = 2, jpjm1 |
|---|
| 455 | DO ji = fs_2, fs_jpim1 |
|---|
| 456 | ! !--- tau_io/(v_oce - v_ice) |
|---|
| 457 | zTauO = zaV(ji,jj) * zrhoco * SQRT( ( v_ice (ji,jj) - v_oce (ji,jj) ) * ( v_ice (ji,jj) - v_oce (ji,jj) ) & |
|---|
| 458 | & + ( u_iceV(ji,jj) - u_oceV(ji,jj) ) * ( u_iceV(ji,jj) - u_oceV(ji,jj) ) ) |
|---|
| 459 | ! !--- Ocean-to-Ice stress |
|---|
| 460 | ztauy_oi(ji,jj) = zTauO * ( v_oce(ji,jj) - v_ice(ji,jj) ) |
|---|
| 461 | ! |
|---|
| 462 | ! !--- tau_bottom/v_ice |
|---|
| 463 | zvel = MAX( zepsi, SQRT( v_ice(ji,jj) * v_ice(ji,jj) + u_iceV(ji,jj) * u_iceV(ji,jj) ) ) |
|---|
| 464 | zTauB = - tau_icebfr(ji,jj) / zvel |
|---|
| 465 | ! |
|---|
| 466 | ! !--- Coriolis at V-points (energy conserving formulation) |
|---|
| 467 | zCory(ji,jj) = - 0.25_wp * r1_e2v(ji,jj) * & |
|---|
| 468 | & ( zmf(ji,jj ) * ( e2u(ji,jj ) * u_ice(ji,jj ) + e2u(ji-1,jj ) * u_ice(ji-1,jj ) ) & |
|---|
| 469 | & + zmf(ji,jj+1) * ( e2u(ji,jj+1) * u_ice(ji,jj+1) + e2u(ji-1,jj+1) * u_ice(ji-1,jj+1) ) ) |
|---|
| 470 | ! |
|---|
| 471 | ! !--- Sum of external forces (explicit solution) = F + tau_ia + Coriolis + spg + tau_io |
|---|
| 472 | zTauE = zfV(ji,jj) + zTauV_ia(ji,jj) + zCory(ji,jj) + zspgV(ji,jj) + ztauy_oi(ji,jj) |
|---|
| 473 | ! |
|---|
| 474 | ! !--- landfast switch => 0 = static friction ; 1 = sliding friction |
|---|
| 475 | rswitch = 1._wp - MIN( 1._wp, ABS( SIGN( 1._wp, ztauE - tau_icebfr(ji,jj) ) - SIGN( 1._wp, zTauE ) ) ) |
|---|
| 476 | ! |
|---|
| 477 | IF( ln_aEVP ) THEN !--- ice velocity using aEVP (Kimmritz et al 2016 & 2017) |
|---|
| 478 | v_ice(ji,jj) = ( ( rswitch * ( zmV_t(ji,jj) * ( zbeta(ji,jj) * v_ice(ji,jj) + v_ice_b(ji,jj) ) & ! previous velocity |
|---|
| 479 | & + zTauE + zTauO * v_ice(ji,jj) & ! F + tau_ia + Coriolis + spg + tau_io(only ocean part) |
|---|
| 480 | & ) / MAX( zepsi, zmV_t(ji,jj) * ( zbeta(ji,jj) + 1._wp ) + zTauO - zTauB ) & ! m/dt + tau_io(only ice part) + landfast |
|---|
| 481 | & + ( 1._wp - rswitch ) * v_ice(ji,jj) * MAX( 0._wp, 1._wp - zdtevp * rn_lfrelax ) & ! static friction => slow decrease to v=0 |
|---|
| 482 | & ) * zswitchV(ji,jj) + v_oce(ji,jj) * ( 1._wp - zswitchV(ji,jj) ) & ! v_ice = v_oce if mass < zmmin |
|---|
| 483 | & ) * zmaskV(ji,jj) |
|---|
| 484 | ELSE !--- ice velocity using EVP implicit formulation (cf Madec doc & Bouillon 2009) |
|---|
| 485 | v_ice(ji,jj) = ( ( rswitch * ( zmV_t(ji,jj) * v_ice(ji,jj) & ! previous velocity |
|---|
| 486 | & + zTauE + zTauO * v_ice(ji,jj) & ! F + tau_ia + Coriolis + spg + tau_io(only ocean part) |
|---|
| 487 | & ) / MAX( zepsi, zmV_t(ji,jj) + zTauO - zTauB ) & ! m/dt + tau_io(only ice part) + landfast |
|---|
| 488 | & + ( 1._wp - rswitch ) * v_ice(ji,jj) * MAX( 0._wp, 1._wp - zdtevp * rn_lfrelax ) & ! static friction => slow decrease to v=0 |
|---|
| 489 | & ) * zswitchV(ji,jj) + v_oce(ji,jj) * ( 1._wp - zswitchV(ji,jj) ) & ! v_ice = v_oce if mass < zmmin |
|---|
| 490 | & ) * zmaskV(ji,jj) |
|---|
| 491 | ENDIF |
|---|
| 492 | END DO |
|---|
| 493 | END DO |
|---|
| 494 | CALL lbc_lnk( v_ice, 'V', -1. ) |
|---|
| 495 | ! |
|---|
| 496 | #if defined key_agrif |
|---|
| 497 | !! CALL agrif_interp_ice( 'V', jter, nn_nevp ) |
|---|
| 498 | CALL agrif_interp_ice( 'V' ) |
|---|
| 499 | #endif |
|---|
| 500 | !clem: this call makes rheology numerically unstable, thus I removed it but one has to check the effect on the boundaries |
|---|
| 501 | ! IF( ln_bdy ) CALL bdy_ice_dyn( 'V' ) |
|---|
| 502 | ! |
|---|
| 503 | DO jj = 2, jpjm1 |
|---|
| 504 | DO ji = fs_2, fs_jpim1 |
|---|
| 505 | ! !--- tau_io/(u_oce - u_ice) |
|---|
| 506 | zTauO = zaU(ji,jj) * zrhoco * SQRT( ( u_ice (ji,jj) - u_oce (ji,jj) ) * ( u_ice (ji,jj) - u_oce (ji,jj) ) & |
|---|
| 507 | & + ( v_iceU(ji,jj) - v_oceU(ji,jj) ) * ( v_iceU(ji,jj) - v_oceU(ji,jj) ) ) |
|---|
| 508 | ! !--- Ocean-to-Ice stress |
|---|
| 509 | ztaux_oi(ji,jj) = zTauO * ( u_oce(ji,jj) - u_ice(ji,jj) ) |
|---|
| 510 | ! |
|---|
| 511 | ! !--- tau_bottom/u_ice |
|---|
| 512 | zvel = MAX( zepsi, SQRT( v_iceU(ji,jj) * v_iceU(ji,jj) + u_ice(ji,jj) * u_ice(ji,jj) ) ) |
|---|
| 513 | zTauB = - tau_icebfr(ji,jj) / zvel |
|---|
| 514 | ! |
|---|
| 515 | ! !--- Coriolis at U-points (energy conserving formulation) |
|---|
| 516 | zCorx(ji,jj) = 0.25_wp * r1_e1u(ji,jj) * & |
|---|
| 517 | & ( zmf(ji ,jj) * ( e1v(ji ,jj) * v_ice(ji ,jj) + e1v(ji ,jj-1) * v_ice(ji ,jj-1) ) & |
|---|
| 518 | & + zmf(ji+1,jj) * ( e1v(ji+1,jj) * v_ice(ji+1,jj) + e1v(ji+1,jj-1) * v_ice(ji+1,jj-1) ) ) |
|---|
| 519 | ! |
|---|
| 520 | ! !--- Sum of external forces (explicit solution) = F + tau_ia + Coriolis + spg + tau_io |
|---|
| 521 | zTauE = zfU(ji,jj) + zTauU_ia(ji,jj) + zCorx(ji,jj) + zspgU(ji,jj) + ztaux_oi(ji,jj) |
|---|
| 522 | ! |
|---|
| 523 | ! !--- landfast switch => 0 = static friction ; 1 = sliding friction |
|---|
| 524 | rswitch = 1._wp - MIN( 1._wp, ABS( SIGN( 1._wp, ztauE - tau_icebfr(ji,jj) ) - SIGN( 1._wp, zTauE ) ) ) |
|---|
| 525 | ! |
|---|
| 526 | IF( ln_aEVP ) THEN !--- ice velocity using aEVP (Kimmritz et al 2016 & 2017) |
|---|
| 527 | u_ice(ji,jj) = ( ( rswitch * ( zmU_t(ji,jj) * ( zbeta(ji,jj) * u_ice(ji,jj) + u_ice_b(ji,jj) ) & ! previous velocity |
|---|
| 528 | & + zTauE + zTauO * u_ice(ji,jj) & ! F + tau_ia + Coriolis + spg + tau_io(only ocean part) |
|---|
| 529 | & ) / MAX( zepsi, zmU_t(ji,jj) * ( zbeta(ji,jj) + 1._wp ) + zTauO - zTauB ) & ! m/dt + tau_io(only ice part) + landfast |
|---|
| 530 | & + ( 1._wp - rswitch ) * u_ice(ji,jj) * MAX( 0._wp, 1._wp - zdtevp * rn_lfrelax ) & ! static friction => slow decrease to v=0 |
|---|
| 531 | & ) * zswitchU(ji,jj) + u_oce(ji,jj) * ( 1._wp - zswitchU(ji,jj) ) & ! v_ice = v_oce if mass < zmmin |
|---|
| 532 | & ) * zmaskU(ji,jj) |
|---|
| 533 | ELSE !--- ice velocity using EVP implicit formulation (cf Madec doc & Bouillon 2009) |
|---|
| 534 | u_ice(ji,jj) = ( ( rswitch * ( zmU_t(ji,jj) * u_ice(ji,jj) & ! previous velocity |
|---|
| 535 | & + zTauE + zTauO * u_ice(ji,jj) & ! F + tau_ia + Coriolis + spg + tau_io(only ocean part) |
|---|
| 536 | & ) / MAX( zepsi, zmU_t(ji,jj) + zTauO - zTauB ) & ! m/dt + tau_io(only ice part) + landfast |
|---|
| 537 | & + ( 1._wp - rswitch ) * u_ice(ji,jj) * MAX( 0._wp, 1._wp - zdtevp * rn_lfrelax ) & ! static friction => slow decrease to v=0 |
|---|
| 538 | & ) * zswitchU(ji,jj) + u_oce(ji,jj) * ( 1._wp - zswitchU(ji,jj) ) & ! v_ice = v_oce if mass < zmmin |
|---|
| 539 | & ) * zmaskU(ji,jj) |
|---|
| 540 | ENDIF |
|---|
| 541 | END DO |
|---|
| 542 | END DO |
|---|
| 543 | CALL lbc_lnk( u_ice, 'U', -1. ) |
|---|
| 544 | ! |
|---|
| 545 | #if defined key_agrif |
|---|
| 546 | !! CALL agrif_interp_ice( 'U', jter, nn_nevp ) |
|---|
| 547 | CALL agrif_interp_ice( 'U' ) |
|---|
| 548 | #endif |
|---|
| 549 | !clem: this call makes rheology numerically unstable, thus I removed it but one has to check the effect on the boundaries |
|---|
| 550 | ! IF( ln_bdy ) CALL bdy_ice_dyn( 'U' ) |
|---|
| 551 | ! |
|---|
| 552 | ELSE ! odd iterations |
|---|
| 553 | ! |
|---|
| 554 | DO jj = 2, jpjm1 |
|---|
| 555 | DO ji = fs_2, fs_jpim1 |
|---|
| 556 | ! !--- tau_io/(u_oce - u_ice) |
|---|
| 557 | zTauO = zaU(ji,jj) * zrhoco * SQRT( ( u_ice (ji,jj) - u_oce (ji,jj) ) * ( u_ice (ji,jj) - u_oce (ji,jj) ) & |
|---|
| 558 | & + ( v_iceU(ji,jj) - v_oceU(ji,jj) ) * ( v_iceU(ji,jj) - v_oceU(ji,jj) ) ) |
|---|
| 559 | ! !--- Ocean-to-Ice stress |
|---|
| 560 | ztaux_oi(ji,jj) = zTauO * ( u_oce(ji,jj) - u_ice(ji,jj) ) |
|---|
| 561 | ! |
|---|
| 562 | ! !--- tau_bottom/u_ice |
|---|
| 563 | zvel = MAX( zepsi, SQRT( v_iceU(ji,jj) * v_iceU(ji,jj) + u_ice(ji,jj) * u_ice(ji,jj) ) ) |
|---|
| 564 | zTauB = - tau_icebfr(ji,jj) / zvel |
|---|
| 565 | ! |
|---|
| 566 | ! !--- Coriolis at U-points (energy conserving formulation) |
|---|
| 567 | zCorx(ji,jj) = 0.25_wp * r1_e1u(ji,jj) * & |
|---|
| 568 | & ( zmf(ji ,jj) * ( e1v(ji ,jj) * v_ice(ji ,jj) + e1v(ji ,jj-1) * v_ice(ji ,jj-1) ) & |
|---|
| 569 | & + zmf(ji+1,jj) * ( e1v(ji+1,jj) * v_ice(ji+1,jj) + e1v(ji+1,jj-1) * v_ice(ji+1,jj-1) ) ) |
|---|
| 570 | ! |
|---|
| 571 | ! !--- Sum of external forces (explicit solution) = F + tau_ia + Coriolis + spg + tau_io |
|---|
| 572 | zTauE = zfU(ji,jj) + zTauU_ia(ji,jj) + zCorx(ji,jj) + zspgU(ji,jj) + ztaux_oi(ji,jj) |
|---|
| 573 | ! |
|---|
| 574 | ! !--- landfast switch => 0 = static friction ; 1 = sliding friction |
|---|
| 575 | rswitch = 1._wp - MIN( 1._wp, ABS( SIGN( 1._wp, ztauE - tau_icebfr(ji,jj) ) - SIGN( 1._wp, zTauE ) ) ) |
|---|
| 576 | ! |
|---|
| 577 | IF( ln_aEVP ) THEN !--- ice velocity using aEVP (Kimmritz et al 2016 & 2017) |
|---|
| 578 | u_ice(ji,jj) = ( ( rswitch * ( zmU_t(ji,jj) * ( zbeta(ji,jj) * u_ice(ji,jj) + u_ice_b(ji,jj) ) & ! previous velocity |
|---|
| 579 | & + zTauE + zTauO * u_ice(ji,jj) & ! F + tau_ia + Coriolis + spg + tau_io(only ocean part) |
|---|
| 580 | & ) / MAX( zepsi, zmU_t(ji,jj) * ( zbeta(ji,jj) + 1._wp ) + zTauO - zTauB ) & ! m/dt + tau_io(only ice part) + landfast |
|---|
| 581 | & + ( 1._wp - rswitch ) * u_ice(ji,jj) * MAX( 0._wp, 1._wp - zdtevp * rn_lfrelax ) & ! static friction => slow decrease to v=0 |
|---|
| 582 | & ) * zswitchU(ji,jj) + u_oce(ji,jj) * ( 1._wp - zswitchU(ji,jj) ) & ! v_ice = v_oce if mass < zmmin |
|---|
| 583 | & ) * zmaskU(ji,jj) |
|---|
| 584 | ELSE !--- ice velocity using EVP implicit formulation (cf Madec doc & Bouillon 2009) |
|---|
| 585 | u_ice(ji,jj) = ( ( rswitch * ( zmU_t(ji,jj) * u_ice(ji,jj) & ! previous velocity |
|---|
| 586 | & + zTauE + zTauO * u_ice(ji,jj) & ! F + tau_ia + Coriolis + spg + tau_io(only ocean part) |
|---|
| 587 | & ) / MAX( zepsi, zmU_t(ji,jj) + zTauO - zTauB ) & ! m/dt + tau_io(only ice part) + landfast |
|---|
| 588 | & + ( 1._wp - rswitch ) * u_ice(ji,jj) * MAX( 0._wp, 1._wp - zdtevp * rn_lfrelax ) & ! static friction => slow decrease to v=0 |
|---|
| 589 | & ) * zswitchU(ji,jj) + u_oce(ji,jj) * ( 1._wp - zswitchU(ji,jj) ) & ! v_ice = v_oce if mass < zmmin |
|---|
| 590 | & ) * zmaskU(ji,jj) |
|---|
| 591 | ENDIF |
|---|
| 592 | END DO |
|---|
| 593 | END DO |
|---|
| 594 | CALL lbc_lnk( u_ice, 'U', -1. ) |
|---|
| 595 | ! |
|---|
| 596 | #if defined key_agrif |
|---|
| 597 | !! CALL agrif_interp_ice( 'U', jter, nn_nevp ) |
|---|
| 598 | CALL agrif_interp_ice( 'U' ) |
|---|
| 599 | #endif |
|---|
| 600 | !clem: this call makes rheology numerically unstable, thus I removed it but one has to check the effect on the boundaries |
|---|
| 601 | ! IF( ln_bdy ) CALL bdy_ice_dyn( 'U' ) |
|---|
| 602 | ! |
|---|
| 603 | DO jj = 2, jpjm1 |
|---|
| 604 | DO ji = fs_2, fs_jpim1 |
|---|
| 605 | ! !--- tau_io/(v_oce - v_ice) |
|---|
| 606 | zTauO = zaV(ji,jj) * zrhoco * SQRT( ( v_ice (ji,jj) - v_oce (ji,jj) ) * ( v_ice (ji,jj) - v_oce (ji,jj) ) & |
|---|
| 607 | & + ( u_iceV(ji,jj) - u_oceV(ji,jj) ) * ( u_iceV(ji,jj) - u_oceV(ji,jj) ) ) |
|---|
| 608 | ! !--- Ocean-to-Ice stress |
|---|
| 609 | ztauy_oi(ji,jj) = zTauO * ( v_oce(ji,jj) - v_ice(ji,jj) ) |
|---|
| 610 | ! |
|---|
| 611 | ! !--- tau_bottom/v_ice |
|---|
| 612 | zvel = MAX( zepsi, SQRT( v_ice(ji,jj) * v_ice(ji,jj) + u_iceV(ji,jj) * u_iceV(ji,jj) ) ) |
|---|
| 613 | ztauB = - tau_icebfr(ji,jj) / zvel |
|---|
| 614 | ! |
|---|
| 615 | ! !--- Coriolis at v-points (energy conserving formulation) |
|---|
| 616 | zCory(ji,jj) = - 0.25_wp * r1_e2v(ji,jj) * & |
|---|
| 617 | & ( zmf(ji,jj ) * ( e2u(ji,jj ) * u_ice(ji,jj ) + e2u(ji-1,jj ) * u_ice(ji-1,jj ) ) & |
|---|
| 618 | & + zmf(ji,jj+1) * ( e2u(ji,jj+1) * u_ice(ji,jj+1) + e2u(ji-1,jj+1) * u_ice(ji-1,jj+1) ) ) |
|---|
| 619 | ! |
|---|
| 620 | ! !--- Sum of external forces (explicit solution) = F + tau_ia + Coriolis + spg + tau_io |
|---|
| 621 | zTauE = zfV(ji,jj) + zTauV_ia(ji,jj) + zCory(ji,jj) + zspgV(ji,jj) + ztauy_oi(ji,jj) |
|---|
| 622 | ! |
|---|
| 623 | ! !--- landfast switch => 0 = static friction ; 1 = sliding friction |
|---|
| 624 | rswitch = 1._wp - MIN( 1._wp, ABS( SIGN( 1._wp, zTauE - tau_icebfr(ji,jj) ) - SIGN( 1._wp, zTauE ) ) ) |
|---|
| 625 | ! |
|---|
| 626 | IF( ln_aEVP ) THEN !--- ice velocity using aEVP (Kimmritz et al 2016 & 2017) |
|---|
| 627 | v_ice(ji,jj) = ( ( rswitch * ( zmV_t(ji,jj) * ( zbeta(ji,jj) * v_ice(ji,jj) + v_ice_b(ji,jj) ) & ! previous velocity |
|---|
| 628 | & + zTauE + zTauO * v_ice(ji,jj) & ! F + tau_ia + Coriolis + spg + tau_io(only ocean part) |
|---|
| 629 | & ) / MAX( zepsi, zmV_t(ji,jj) * ( zbeta(ji,jj) + 1._wp ) + zTauO - zTauB ) & ! m/dt + tau_io(only ice part) + landfast |
|---|
| 630 | & + ( 1._wp - rswitch ) * v_ice(ji,jj) * MAX( 0._wp, 1._wp - zdtevp * rn_lfrelax ) & ! static friction => slow decrease to v=0 |
|---|
| 631 | & ) * zswitchV(ji,jj) + v_oce(ji,jj) * ( 1._wp - zswitchV(ji,jj) ) & ! v_ice = v_oce if mass < zmmin |
|---|
| 632 | & ) * zmaskV(ji,jj) |
|---|
| 633 | ELSE !--- ice velocity using EVP implicit formulation (cf Madec doc & Bouillon 2009) |
|---|
| 634 | v_ice(ji,jj) = ( ( rswitch * ( zmV_t(ji,jj) * v_ice(ji,jj) & ! previous velocity |
|---|
| 635 | & + zTauE + zTauO * v_ice(ji,jj) & ! F + tau_ia + Coriolis + spg + tau_io(only ocean part) |
|---|
| 636 | & ) / MAX( zepsi, zmV_t(ji,jj) + zTauO - zTauB ) & ! m/dt + tau_io(only ice part) + landfast |
|---|
| 637 | & + ( 1._wp - rswitch ) * v_ice(ji,jj) * MAX( 0._wp, 1._wp - zdtevp * rn_lfrelax ) & ! static friction => slow decrease to v=0 |
|---|
| 638 | & ) * zswitchV(ji,jj) + v_oce(ji,jj) * ( 1._wp - zswitchV(ji,jj) ) & ! v_ice = v_oce if mass < zmmin |
|---|
| 639 | & ) * zmaskV(ji,jj) |
|---|
| 640 | ENDIF |
|---|
| 641 | END DO |
|---|
| 642 | END DO |
|---|
| 643 | CALL lbc_lnk( v_ice, 'V', -1. ) |
|---|
| 644 | ! |
|---|
| 645 | #if defined key_agrif |
|---|
| 646 | !! CALL agrif_interp_ice( 'V', jter, nn_nevp ) |
|---|
| 647 | CALL agrif_interp_ice( 'V' ) |
|---|
| 648 | #endif |
|---|
| 649 | !clem: this call makes rheology numerically unstable, thus I removed it but one has to check the effect on the boundaries |
|---|
| 650 | ! IF( ln_bdy ) CALL bdy_ice_dyn( 'V' ) |
|---|
| 651 | ! |
|---|
| 652 | ENDIF |
|---|
| 653 | |
|---|
| 654 | IF(ln_ctl) THEN ! Convergence test |
|---|
| 655 | DO jj = 2 , jpjm1 |
|---|
| 656 | zresr(:,jj) = MAX( ABS( u_ice(:,jj) - zu_ice(:,jj) ), ABS( v_ice(:,jj) - zv_ice(:,jj) ) ) |
|---|
| 657 | END DO |
|---|
| 658 | zresm = MAXVAL( zresr( 1:jpi, 2:jpjm1 ) ) |
|---|
| 659 | IF( lk_mpp ) CALL mpp_max( zresm ) ! max over the global domain |
|---|
| 660 | ENDIF |
|---|
| 661 | ! |
|---|
| 662 | ! ! ==================== ! |
|---|
| 663 | END DO ! end loop over jter ! |
|---|
| 664 | ! ! ==================== ! |
|---|
| 665 | ! |
|---|
| 666 | !------------------------------------------------------------------------------! |
|---|
| 667 | ! 4) Recompute delta, shear and div (inputs for mechanical redistribution) |
|---|
| 668 | !------------------------------------------------------------------------------! |
|---|
| 669 | DO jj = 1, jpjm1 |
|---|
| 670 | DO ji = 1, jpim1 |
|---|
| 671 | |
|---|
| 672 | ! shear at F points |
|---|
| 673 | 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) & |
|---|
| 674 | & + ( v_ice(ji+1,jj) * r1_e2v(ji+1,jj) - v_ice(ji,jj) * r1_e2v(ji,jj) ) * e2f(ji,jj) * e2f(ji,jj) & |
|---|
| 675 | & ) * r1_e1e2f(ji,jj) * zfmask(ji,jj) |
|---|
| 676 | |
|---|
| 677 | END DO |
|---|
| 678 | END DO |
|---|
| 679 | |
|---|
| 680 | DO jj = 2, jpjm1 |
|---|
| 681 | DO ji = 2, jpim1 ! no vector loop |
|---|
| 682 | |
|---|
| 683 | ! tension**2 at T points |
|---|
| 684 | 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) & |
|---|
| 685 | & - ( v_ice(ji,jj) * r1_e1v(ji,jj) - v_ice(ji,jj-1) * r1_e1v(ji,jj-1) ) * e1t(ji,jj) * e1t(ji,jj) & |
|---|
| 686 | & ) * r1_e1e2t(ji,jj) |
|---|
| 687 | zdt2 = zdt * zdt |
|---|
| 688 | |
|---|
| 689 | ! shear**2 at T points (doc eq. A16) |
|---|
| 690 | zds2 = ( zds(ji,jj ) * zds(ji,jj ) * e1e2f(ji,jj ) + zds(ji-1,jj ) * zds(ji-1,jj ) * e1e2f(ji-1,jj ) & |
|---|
| 691 | & + 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) & |
|---|
| 692 | & ) * 0.25_wp * r1_e1e2t(ji,jj) |
|---|
| 693 | |
|---|
| 694 | ! shear at T points |
|---|
| 695 | pshear_i(ji,jj) = SQRT( zdt2 + zds2 ) |
|---|
| 696 | |
|---|
| 697 | ! divergence at T points |
|---|
| 698 | pdivu_i(ji,jj) = ( e2u(ji,jj) * u_ice(ji,jj) - e2u(ji-1,jj) * u_ice(ji-1,jj) & |
|---|
| 699 | & + e1v(ji,jj) * v_ice(ji,jj) - e1v(ji,jj-1) * v_ice(ji,jj-1) & |
|---|
| 700 | & ) * r1_e1e2t(ji,jj) |
|---|
| 701 | |
|---|
| 702 | ! delta at T points |
|---|
| 703 | zdelta = SQRT( pdivu_i(ji,jj) * pdivu_i(ji,jj) + ( zdt2 + zds2 ) * z1_ecc2 ) |
|---|
| 704 | rswitch = 1._wp - MAX( 0._wp, SIGN( 1._wp, -zdelta ) ) ! 0 if delta=0 |
|---|
| 705 | pdelta_i(ji,jj) = zdelta + rn_creepl * rswitch |
|---|
| 706 | |
|---|
| 707 | END DO |
|---|
| 708 | END DO |
|---|
| 709 | CALL lbc_lnk_multi( pshear_i, 'T', 1., pdivu_i, 'T', 1., pdelta_i, 'T', 1. ) |
|---|
| 710 | |
|---|
| 711 | ! --- Store the stress tensor for the next time step --- ! |
|---|
| 712 | CALL lbc_lnk_multi( zs1, 'T', 1., zs2, 'T', 1., zs12, 'F', 1. ) |
|---|
| 713 | pstress1_i (:,:) = zs1 (:,:) |
|---|
| 714 | pstress2_i (:,:) = zs2 (:,:) |
|---|
| 715 | pstress12_i(:,:) = zs12(:,:) |
|---|
| 716 | ! |
|---|
| 717 | |
|---|
| 718 | !------------------------------------------------------------------------------! |
|---|
| 719 | ! 5) diagnostics |
|---|
| 720 | !------------------------------------------------------------------------------! |
|---|
| 721 | DO jj = 1, jpj |
|---|
| 722 | DO ji = 1, jpi |
|---|
| 723 | zswi(ji,jj) = MAX( 0._wp , SIGN( 1._wp , at_i(ji,jj) - epsi06 ) ) ! 1 if ice, 0 if no ice |
|---|
| 724 | END DO |
|---|
| 725 | END DO |
|---|
| 726 | |
|---|
| 727 | ! --- divergence, shear and strength --- ! |
|---|
| 728 | IF( iom_use('icediv') ) CALL iom_put( "icediv" , pdivu_i (:,:) * zswi(:,:) ) ! divergence |
|---|
| 729 | IF( iom_use('iceshe') ) CALL iom_put( "iceshe" , pshear_i(:,:) * zswi(:,:) ) ! shear |
|---|
| 730 | IF( iom_use('icestr') ) CALL iom_put( "icestr" , strength(:,:) * zswi(:,:) ) ! Ice strength |
|---|
| 731 | |
|---|
| 732 | ! --- charge ellipse --- ! |
|---|
| 733 | IF( iom_use('isig1') .OR. iom_use('isig2') .OR. iom_use('isig3') ) THEN |
|---|
| 734 | ! |
|---|
| 735 | ALLOCATE( zsig1(jpi,jpj) , zsig2(jpi,jpj) , zsig3(jpi,jpj) ) |
|---|
| 736 | ! |
|---|
| 737 | DO jj = 2, jpjm1 |
|---|
| 738 | DO ji = 2, jpim1 |
|---|
| 739 | zdum1 = ( zswi(ji-1,jj) * pstress12_i(ji-1,jj) + zswi(ji ,jj-1) * pstress12_i(ji ,jj-1) + & ! stress12_i at T-point |
|---|
| 740 | & zswi(ji ,jj) * pstress12_i(ji ,jj) + zswi(ji-1,jj-1) * pstress12_i(ji-1,jj-1) ) & |
|---|
| 741 | & / MAX( 1._wp, zswi(ji-1,jj) + zswi(ji,jj-1) + zswi(ji,jj) + zswi(ji-1,jj-1) ) |
|---|
| 742 | |
|---|
| 743 | zshear = SQRT( pstress2_i(ji,jj) * pstress2_i(ji,jj) + 4._wp * zdum1 * zdum1 ) ! shear stress |
|---|
| 744 | |
|---|
| 745 | zdum2 = zswi(ji,jj) / MAX( 1._wp, strength(ji,jj) ) |
|---|
| 746 | |
|---|
| 747 | !! zsig1(ji,jj) = 0.5_wp * zdum2 * ( pstress1_i(ji,jj) + zshear ) ! principal stress (y-direction, see Hunke & Dukowicz 2002) |
|---|
| 748 | !! zsig2(ji,jj) = 0.5_wp * zdum2 * ( pstress1_i(ji,jj) - zshear ) ! principal stress (x-direction, see Hunke & Dukowicz 2002) |
|---|
| 749 | !! zsig3(ji,jj) = zdum2**2 * ( ( pstress1_i(ji,jj) + strength(ji,jj) )**2 + ( rn_ecc * zshear )**2 ) ! quadratic relation linking compressive stress to shear stress |
|---|
| 750 | !! ! (scheme converges if this value is ~1, see Bouillon et al 2009 (eq. 11)) |
|---|
| 751 | zsig1(ji,jj) = 0.5_wp * zdum2 * ( pstress1_i(ji,jj) ) ! compressive stress, see Bouillon et al. 2015 |
|---|
| 752 | zsig2(ji,jj) = 0.5_wp * zdum2 * ( zshear ) ! shear stress |
|---|
| 753 | zsig3(ji,jj) = zdum2**2 * ( ( pstress1_i(ji,jj) + strength(ji,jj) )**2 + ( rn_ecc * zshear )**2 ) |
|---|
| 754 | END DO |
|---|
| 755 | END DO |
|---|
| 756 | CALL lbc_lnk_multi( zsig1, 'T', 1., zsig2, 'T', 1., zsig3, 'T', 1. ) |
|---|
| 757 | ! |
|---|
| 758 | IF( iom_use('isig1') ) CALL iom_put( "isig1" , zsig1 ) |
|---|
| 759 | IF( iom_use('isig2') ) CALL iom_put( "isig2" , zsig2 ) |
|---|
| 760 | IF( iom_use('isig3') ) CALL iom_put( "isig3" , zsig3 ) |
|---|
| 761 | ! |
|---|
| 762 | DEALLOCATE( zsig1 , zsig2 , zsig3 ) |
|---|
| 763 | ENDIF |
|---|
| 764 | |
|---|
| 765 | ! --- SIMIP --- ! |
|---|
| 766 | IF ( iom_use( 'normstr' ) .OR. iom_use( 'sheastr' ) .OR. iom_use( 'dssh_dx' ) .OR. iom_use( 'dssh_dy' ) .OR. & |
|---|
| 767 | & iom_use( 'corstrx' ) .OR. iom_use( 'corstry' ) .OR. iom_use( 'intstrx' ) .OR. iom_use( 'intstry' ) .OR. & |
|---|
| 768 | & iom_use( 'utau_oi' ) .OR. iom_use( 'vtau_oi' ) .OR. iom_use( 'xmtrpice' ) .OR. iom_use( 'ymtrpice' ) .OR. & |
|---|
| 769 | & iom_use( 'xmtrpsnw' ) .OR. iom_use( 'ymtrpsnw' ) .OR. iom_use( 'xatrp' ) .OR. iom_use( 'yatrp' ) ) THEN |
|---|
| 770 | |
|---|
| 771 | ALLOCATE( zdiag_sig1 (jpi,jpj) , zdiag_sig2 (jpi,jpj) , zdiag_dssh_dx (jpi,jpj) , zdiag_dssh_dy (jpi,jpj) , & |
|---|
| 772 | & zdiag_corstrx (jpi,jpj) , zdiag_corstry (jpi,jpj) , zdiag_intstrx (jpi,jpj) , zdiag_intstry (jpi,jpj) , & |
|---|
| 773 | & zdiag_utau_oi (jpi,jpj) , zdiag_vtau_oi (jpi,jpj) , zdiag_xmtrp_ice(jpi,jpj) , zdiag_ymtrp_ice(jpi,jpj) , & |
|---|
| 774 | & zdiag_xmtrp_snw(jpi,jpj) , zdiag_ymtrp_snw(jpi,jpj) , zdiag_xatrp (jpi,jpj) , zdiag_yatrp (jpi,jpj) ) |
|---|
| 775 | |
|---|
| 776 | DO jj = 2, jpjm1 |
|---|
| 777 | DO ji = 2, jpim1 |
|---|
| 778 | rswitch = MAX( 0._wp , SIGN( 1._wp , at_i(ji,jj) - epsi06 ) ) ! 1 if ice, 0 if no ice |
|---|
| 779 | |
|---|
| 780 | ! Stress tensor invariants (normal and shear stress N/m) |
|---|
| 781 | zdiag_sig1(ji,jj) = ( zs1(ji,jj) + zs2(ji,jj) ) * rswitch ! normal stress |
|---|
| 782 | zdiag_sig2(ji,jj) = SQRT( ( zs1(ji,jj) - zs2(ji,jj) )**2 + 4*zs12(ji,jj)**2 ) * rswitch ! shear stress |
|---|
| 783 | |
|---|
| 784 | ! Stress terms of the momentum equation (N/m2) |
|---|
| 785 | zdiag_dssh_dx(ji,jj) = zspgU(ji,jj) * rswitch ! sea surface slope stress term |
|---|
| 786 | zdiag_dssh_dy(ji,jj) = zspgV(ji,jj) * rswitch |
|---|
| 787 | |
|---|
| 788 | zdiag_corstrx(ji,jj) = zCorx(ji,jj) * rswitch ! Coriolis stress term |
|---|
| 789 | zdiag_corstry(ji,jj) = zCory(ji,jj) * rswitch |
|---|
| 790 | |
|---|
| 791 | zdiag_intstrx(ji,jj) = zfU(ji,jj) * rswitch ! internal stress term |
|---|
| 792 | zdiag_intstry(ji,jj) = zfV(ji,jj) * rswitch |
|---|
| 793 | |
|---|
| 794 | zdiag_utau_oi(ji,jj) = ztaux_oi(ji,jj) * rswitch ! oceanic stress |
|---|
| 795 | zdiag_vtau_oi(ji,jj) = ztauy_oi(ji,jj) * rswitch |
|---|
| 796 | |
|---|
| 797 | ! 2D ice mass, snow mass, area transport arrays (X, Y) |
|---|
| 798 | zfac_x = 0.5 * u_ice(ji,jj) * e2u(ji,jj) * rswitch |
|---|
| 799 | zfac_y = 0.5 * v_ice(ji,jj) * e1v(ji,jj) * rswitch |
|---|
| 800 | |
|---|
| 801 | zdiag_xmtrp_ice(ji,jj) = rhoic * zfac_x * ( vt_i(ji+1,jj) + vt_i(ji,jj) ) ! ice mass transport, X-component |
|---|
| 802 | zdiag_ymtrp_ice(ji,jj) = rhoic * zfac_y * ( vt_i(ji,jj+1) + vt_i(ji,jj) ) ! '' Y- '' |
|---|
| 803 | |
|---|
| 804 | zdiag_xmtrp_snw(ji,jj) = rhosn * zfac_x * ( vt_s(ji+1,jj) + vt_s(ji,jj) ) ! snow mass transport, X-component |
|---|
| 805 | zdiag_ymtrp_snw(ji,jj) = rhosn * zfac_y * ( vt_s(ji,jj+1) + vt_s(ji,jj) ) ! '' Y- '' |
|---|
| 806 | |
|---|
| 807 | zdiag_xatrp(ji,jj) = zfac_x * ( at_i(ji+1,jj) + at_i(ji,jj) ) ! area transport, X-component |
|---|
| 808 | zdiag_yatrp(ji,jj) = zfac_y * ( at_i(ji,jj+1) + at_i(ji,jj) ) ! '' Y- '' |
|---|
| 809 | |
|---|
| 810 | END DO |
|---|
| 811 | END DO |
|---|
| 812 | |
|---|
| 813 | CALL lbc_lnk_multi( zdiag_sig1 , 'T', 1., zdiag_sig2 , 'T', 1., & |
|---|
| 814 | & zdiag_dssh_dx, 'U', -1., zdiag_dssh_dy, 'V', -1., & |
|---|
| 815 | & zdiag_corstrx, 'U', -1., zdiag_corstry, 'V', -1., & |
|---|
| 816 | & zdiag_intstrx, 'U', -1., zdiag_intstry, 'V', -1. ) |
|---|
| 817 | |
|---|
| 818 | CALL lbc_lnk_multi( zdiag_utau_oi , 'U', -1., zdiag_vtau_oi , 'V', -1., & |
|---|
| 819 | & zdiag_xmtrp_ice, 'U', -1., zdiag_xmtrp_snw, 'U', -1., & |
|---|
| 820 | & zdiag_xatrp , 'U', -1., zdiag_ymtrp_ice, 'V', -1., & |
|---|
| 821 | & zdiag_ymtrp_snw, 'V', -1., zdiag_yatrp , 'V', -1. ) |
|---|
| 822 | |
|---|
| 823 | IF( iom_use('normstr' ) ) CALL iom_put( 'normstr' , zdiag_sig1(:,:) ) ! Normal stress |
|---|
| 824 | IF( iom_use('sheastr' ) ) CALL iom_put( 'sheastr' , zdiag_sig2(:,:) ) ! Shear stress |
|---|
| 825 | IF( iom_use('dssh_dx' ) ) CALL iom_put( 'dssh_dx' , zdiag_dssh_dx(:,:) ) ! Sea-surface tilt term in force balance (x) |
|---|
| 826 | IF( iom_use('dssh_dy' ) ) CALL iom_put( 'dssh_dy' , zdiag_dssh_dy(:,:) ) ! Sea-surface tilt term in force balance (y) |
|---|
| 827 | IF( iom_use('corstrx' ) ) CALL iom_put( 'corstrx' , zdiag_corstrx(:,:) ) ! Coriolis force term in force balance (x) |
|---|
| 828 | IF( iom_use('corstry' ) ) CALL iom_put( 'corstry' , zdiag_corstry(:,:) ) ! Coriolis force term in force balance (y) |
|---|
| 829 | IF( iom_use('intstrx' ) ) CALL iom_put( 'intstrx' , zdiag_intstrx(:,:) ) ! Internal force term in force balance (x) |
|---|
| 830 | IF( iom_use('intstry' ) ) CALL iom_put( 'intstry' , zdiag_intstry(:,:) ) ! Internal force term in force balance (y) |
|---|
| 831 | IF( iom_use('utau_oi' ) ) CALL iom_put( 'utau_oi' , zdiag_utau_oi(:,:) ) ! Ocean stress term in force balance (x) |
|---|
| 832 | IF( iom_use('vtau_oi' ) ) CALL iom_put( 'vtau_oi' , zdiag_vtau_oi(:,:) ) ! Ocean stress term in force balance (y) |
|---|
| 833 | IF( iom_use('xmtrpice') ) CALL iom_put( 'xmtrpice' , zdiag_xmtrp_ice(:,:) ) ! X-component of sea-ice mass transport (kg/s) |
|---|
| 834 | IF( iom_use('ymtrpice') ) CALL iom_put( 'ymtrpice' , zdiag_ymtrp_ice(:,:) ) ! Y-component of sea-ice mass transport |
|---|
| 835 | IF( iom_use('xmtrpsnw') ) CALL iom_put( 'xmtrpsnw' , zdiag_xmtrp_snw(:,:) ) ! X-component of snow mass transport (kg/s) |
|---|
| 836 | IF( iom_use('ymtrpsnw') ) CALL iom_put( 'ymtrpsnw' , zdiag_ymtrp_snw(:,:) ) ! Y-component of snow mass transport |
|---|
| 837 | IF( iom_use('xatrp' ) ) CALL iom_put( 'xatrp' , zdiag_xatrp(:,:) ) ! X-component of ice area transport |
|---|
| 838 | IF( iom_use('yatrp' ) ) CALL iom_put( 'yatrp' , zdiag_yatrp(:,:) ) ! Y-component of ice area transport |
|---|
| 839 | |
|---|
| 840 | DEALLOCATE( zdiag_sig1 , zdiag_sig2 , zdiag_dssh_dx , zdiag_dssh_dy , & |
|---|
| 841 | & zdiag_corstrx , zdiag_corstry , zdiag_intstrx , zdiag_intstry , & |
|---|
| 842 | & zdiag_utau_oi , zdiag_vtau_oi , zdiag_xmtrp_ice , zdiag_ymtrp_ice , & |
|---|
| 843 | & zdiag_xmtrp_snw , zdiag_ymtrp_snw , zdiag_xatrp , zdiag_yatrp ) |
|---|
| 844 | |
|---|
| 845 | ENDIF |
|---|
| 846 | ! |
|---|
| 847 | END SUBROUTINE ice_dyn_rhg_evp |
|---|
| 848 | |
|---|
| 849 | |
|---|
| 850 | SUBROUTINE rhg_evp_rst( cdrw, kt ) |
|---|
| 851 | !!--------------------------------------------------------------------- |
|---|
| 852 | !! *** ROUTINE rhg_evp_rst *** |
|---|
| 853 | !! |
|---|
| 854 | !! ** Purpose : Read or write RHG file in restart file |
|---|
| 855 | !! |
|---|
| 856 | !! ** Method : use of IOM library |
|---|
| 857 | !!---------------------------------------------------------------------- |
|---|
| 858 | CHARACTER(len=*) , INTENT(in) :: cdrw ! "READ"/"WRITE" flag |
|---|
| 859 | INTEGER, OPTIONAL, INTENT(in) :: kt ! ice time-step |
|---|
| 860 | ! |
|---|
| 861 | INTEGER :: iter ! local integer |
|---|
| 862 | INTEGER :: id1, id2, id3 ! local integers |
|---|
| 863 | !!---------------------------------------------------------------------- |
|---|
| 864 | ! |
|---|
| 865 | IF( TRIM(cdrw) == 'READ' ) THEN ! Read/initialize |
|---|
| 866 | ! ! --------------- |
|---|
| 867 | IF( ln_rstart ) THEN !* Read the restart file |
|---|
| 868 | ! |
|---|
| 869 | id1 = iom_varid( numrir, 'stress1_i' , ldstop = .FALSE. ) |
|---|
| 870 | id2 = iom_varid( numrir, 'stress2_i' , ldstop = .FALSE. ) |
|---|
| 871 | id3 = iom_varid( numrir, 'stress12_i', ldstop = .FALSE. ) |
|---|
| 872 | ! |
|---|
| 873 | IF( MIN( id1, id2, id3 ) > 0 ) THEN ! fields exist |
|---|
| 874 | CALL iom_get( numrir, jpdom_autoglo, 'stress1_i' , stress1_i ) |
|---|
| 875 | CALL iom_get( numrir, jpdom_autoglo, 'stress2_i' , stress2_i ) |
|---|
| 876 | CALL iom_get( numrir, jpdom_autoglo, 'stress12_i', stress12_i ) |
|---|
| 877 | ELSE ! start rheology from rest |
|---|
| 878 | IF(lwp) WRITE(numout,*) |
|---|
| 879 | IF(lwp) WRITE(numout,*) ' ==>>> previous run without rheology, set stresses to 0' |
|---|
| 880 | stress1_i (:,:) = 0._wp |
|---|
| 881 | stress2_i (:,:) = 0._wp |
|---|
| 882 | stress12_i(:,:) = 0._wp |
|---|
| 883 | ENDIF |
|---|
| 884 | ELSE !* Start from rest |
|---|
| 885 | IF(lwp) WRITE(numout,*) |
|---|
| 886 | IF(lwp) WRITE(numout,*) ' ==>>> start from rest: set stresses to 0' |
|---|
| 887 | stress1_i (:,:) = 0._wp |
|---|
| 888 | stress2_i (:,:) = 0._wp |
|---|
| 889 | stress12_i(:,:) = 0._wp |
|---|
| 890 | ENDIF |
|---|
| 891 | ! |
|---|
| 892 | ELSEIF( TRIM(cdrw) == 'WRITE' ) THEN ! Create restart file |
|---|
| 893 | ! ! ------------------- |
|---|
| 894 | IF(lwp) WRITE(numout,*) '---- rhg-rst ----' |
|---|
| 895 | iter = kt + nn_fsbc - 1 ! ice restarts are written at kt == nitrst - nn_fsbc + 1 |
|---|
| 896 | ! |
|---|
| 897 | CALL iom_rstput( iter, nitrst, numriw, 'stress1_i' , stress1_i ) |
|---|
| 898 | CALL iom_rstput( iter, nitrst, numriw, 'stress2_i' , stress2_i ) |
|---|
| 899 | CALL iom_rstput( iter, nitrst, numriw, 'stress12_i', stress12_i ) |
|---|
| 900 | ! |
|---|
| 901 | ENDIF |
|---|
| 902 | ! |
|---|
| 903 | END SUBROUTINE rhg_evp_rst |
|---|
| 904 | |
|---|
| 905 | #else |
|---|
| 906 | !!---------------------------------------------------------------------- |
|---|
| 907 | !! Default option Empty module NO SI3 sea-ice model |
|---|
| 908 | !!---------------------------------------------------------------------- |
|---|
| 909 | #endif |
|---|
| 910 | |
|---|
| 911 | !!============================================================================== |
|---|
| 912 | END MODULE icedyn_rhg_evp |
|---|
