1 | MODULE icedyn_rhg_vp |
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2 | !!====================================================================== |
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3 | !! *** MODULE icedyn_rhg_vp *** |
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4 | !! Sea-Ice dynamics : Viscous-plastic rheology with LSR technique |
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5 | !!====================================================================== |
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6 | !! |
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7 | !! History : - ! 1997-20 (J. Zhang, M. Losch) Original code, implementation into mitGCM |
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8 | !! 4.0 ! 2020-09 (M. Vancoppenolle) Adaptation to SI3 |
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9 | !! |
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10 | !!---------------------------------------------------------------------- |
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11 | #if defined key_si3 |
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12 | !!---------------------------------------------------------------------- |
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13 | !! 'key_si3' SI3 sea-ice model |
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14 | !!---------------------------------------------------------------------- |
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15 | !! ice_dyn_rhg_vp : computes ice velocities from VP rheolog with LSR solvery |
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16 | !!---------------------------------------------------------------------- |
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17 | USE phycst ! Physical constants |
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18 | USE dom_oce ! Ocean domain |
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19 | USE sbc_oce , ONLY : ln_ice_embd, nn_fsbc, ssh_m |
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20 | USE sbc_ice , ONLY : utau_ice, vtau_ice, snwice_mass, snwice_mass_b |
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21 | USE ice ! sea-ice: ice variables |
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22 | USE icevar ! ice_var_sshdyn |
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23 | USE icedyn_rdgrft ! sea-ice: ice strength |
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24 | USE bdy_oce , ONLY : ln_bdy |
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25 | USE bdyice |
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26 | #if defined key_agrif |
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27 | USE agrif_ice_interp |
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28 | #endif |
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29 | ! |
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30 | USE in_out_manager ! I/O manager |
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31 | USE iom ! I/O manager library |
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32 | USE lib_mpp ! MPP library |
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33 | USE lib_fortran ! fortran utilities (glob_sum + no signed zero) |
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34 | USE lbclnk ! lateral boundary conditions (or mpp links) |
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35 | USE prtctl ! Print control |
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36 | |
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37 | USE netcdf ! NetCDF library for convergence test |
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38 | IMPLICIT NONE |
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39 | PRIVATE |
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40 | |
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41 | PUBLIC ice_dyn_rhg_vp ! called by icedyn_rhg.F90 |
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42 | |
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43 | |
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44 | LOGICAL :: lp_zebra_vp =.TRUE. ! activate zebra (solve the linear system problem every odd j-band, then one every even one) |
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45 | REAL(wp) :: zrelaxu_vp=0.95 ! U-relaxation factor (MV: can probably be merged with V-factor once ok) |
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46 | REAL(wp) :: zrelaxv_vp=0.95 ! V-relaxation factor |
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47 | REAL(wp) :: zuerr_max_vp=0.80 ! maximum velocity error, above which a forcing error is considered and solver is stopped |
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48 | REAL(wp) :: zuerr_min_vp=1.e-04 ! minimum velocity error, beyond which convergence is assumed |
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49 | |
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50 | !! for convergence tests |
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51 | INTEGER :: ncvgid ! netcdf file id |
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52 | INTEGER :: nvarid_ures |
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53 | INTEGER :: nvarid_vres |
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54 | INTEGER :: nvarid_velres |
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55 | INTEGER :: nvarid_udif |
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56 | INTEGER :: nvarid_vdif |
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57 | INTEGER :: nvarid_veldif |
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58 | INTEGER :: nvarid_mke |
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59 | INTEGER :: nvarid_ures_xy, nvarid_vres_xy |
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60 | |
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61 | REAL(wp), DIMENSION(:,:), ALLOCATABLE :: fimask ! mask at F points for the ice |
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62 | |
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63 | !! * Substitutions |
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64 | # include "do_loop_substitute.h90" |
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65 | !!---------------------------------------------------------------------- |
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66 | !! NEMO/ICE 4.0 , NEMO Consortium (2018) |
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67 | !! $Id: icedyn_rhg_vp.F90 13279 2020-07-09 10:39:43Z clem $ |
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68 | !! Software governed by the CeCILL license (see ./LICENSE) |
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69 | !!---------------------------------------------------------------------- |
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70 | |
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71 | CONTAINS |
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72 | |
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73 | SUBROUTINE ice_dyn_rhg_vp( kt, pshear_i, pdivu_i, pdelta_i ) |
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74 | !!------------------------------------------------------------------- |
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75 | !! |
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76 | !! *** SUBROUTINE ice_dyn_rhg_vp *** |
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77 | !! VP-LSR-C-grid |
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78 | !! |
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79 | !! ** Purpose : determines sea ice drift from wind stress, ice-ocean |
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80 | !! stress and sea-surface slope. Internal forces assume viscous-plastic rheology (Hibler, 1979) |
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81 | !! |
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82 | !! ** Method |
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83 | !! |
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84 | !! The resolution algorithm follows from Zhang and Hibler (1997) and Losch (2010) |
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85 | !! with elements from Lemieux and Tremblay (2008) and Lemieux and Tremblay (2009) |
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86 | !! |
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87 | !! The components of the momentum equations are arranged following the ideas of Zhang and Hibler (1997) |
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88 | !! |
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89 | !! f1(u) = g1(v) |
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90 | !! f2(v) = g2(v) |
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91 | !! |
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92 | !! The right-hand side (RHS) is explicit |
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93 | !! The left-hand side (LHS) is implicit |
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94 | !! Coriolis is part of explicit terms, whereas ice-ocean drag is implicit |
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95 | !! |
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96 | !! Two iteration levels (outer and inner loops) are used to solve the equations |
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97 | !! |
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98 | !! The outer loop (OL, typically 10 iterations) is there to deal with the (strong) non-linearities in the equation |
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99 | !! |
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100 | !! The inner loop (IL, typically 1500 iterations) is there to solve the linear problem with a line-successive-relaxation algorithm |
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101 | !! |
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102 | !! The velocity used in the non-linear terms uses a "modified euler time step" (not sure its the correct term), |
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103 | !!! with uk = ( uk-1 + uk-2 ) / 2. |
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104 | !! |
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105 | !! * Spatial discretization |
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106 | !! |
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107 | !! Assumes a C-grid |
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108 | !! |
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109 | !! The points in the C-grid look like this, my darling |
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110 | !! |
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111 | !! (ji,jj) |
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112 | !! | |
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113 | !! | |
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114 | !! (ji-1,jj) | (ji,jj) |
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115 | !! --------- |
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116 | !! | | |
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117 | !! | (ji,jj) |------(ji,jj) |
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118 | !! | | |
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119 | !! --------- |
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120 | !! (ji-1,jj-1) (ji,jj-1) |
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121 | !! |
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122 | !! ** Inputs : - wind forcing (stress), oceanic currents |
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123 | !! ice total volume (vt_i) per unit area |
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124 | !! snow total volume (vt_s) per unit area |
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125 | !! |
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126 | !! ** Action : |
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127 | !! |
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128 | !! ** Steps : |
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129 | !! |
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130 | !! ** Notes : |
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131 | !! |
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132 | !! References : Zhang and Hibler, JGR 1997; Losch et al., OM 2010., Lemieux et al., 2008, 2009, ... |
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133 | !! |
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134 | !! |
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135 | !!------------------------------------------------------------------- |
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136 | !! |
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137 | INTEGER , INTENT(in ) :: kt ! time step |
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138 | REAL(wp), DIMENSION(:,:), INTENT( out) :: pshear_i , pdivu_i , pdelta_i ! |
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139 | !! |
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140 | LOGICAL :: ll_u_iterate, ll_v_iterate ! continue iteration or not |
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141 | ! |
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142 | INTEGER :: ji, ji2, jj, jj2, jn ! dummy loop indices |
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143 | INTEGER :: jter, i_out, i_inn ! |
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144 | INTEGER :: ji_min, jj_min ! |
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145 | INTEGER :: nn_zebra_vp ! number of zebra steps |
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146 | |
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147 | INTEGER :: nn_nvp ! total number of VP iterations (n_out_vp*n_inn_vp) |
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148 | ! |
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149 | REAL(wp) :: zrhoco ! rho0 * rn_cio |
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150 | REAL(wp) :: ecc2, z1_ecc2 ! square of yield ellipse eccenticity |
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151 | REAL(wp) :: zglob_area ! global ice area for diagnostics |
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152 | REAL(wp) :: zkt ! isotropic tensile strength for landfast ice |
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153 | REAL(wp) :: zm1, zm2, zm3, zmassU, zmassV ! ice/snow mass and volume |
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154 | REAL(wp) :: zdeltat, zds2, zdt, zdt2, zdiv, zdiv2 ! temporary scalars |
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155 | REAL(wp) :: zp_deltastar_f ! |
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156 | REAL(wp) :: zu_cV, zv_cU ! |
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157 | REAL(wp) :: zfac, zfac1, zfac2, zfac3 |
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158 | REAL(wp) :: zt12U, zt11U, zt22U, zt21U, zt122U, zt121U |
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159 | REAL(wp) :: zt12V, zt11V, zt22V, zt21V, zt122V, zt121V |
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160 | REAL(wp) :: zAA3, zw, ztau, zuerr_max, zverr_max |
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161 | ! |
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162 | REAL(wp), DIMENSION(jpi,jpj) :: za_iU , za_iV ! ice fraction on U/V points |
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163 | REAL(wp), DIMENSION(jpi,jpj) :: zmU_t, zmV_t ! Acceleration term contribution to RHS |
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164 | REAL(wp), DIMENSION(jpi,jpj) :: zmassU_t, zmassV_t ! Mass per unit area divided by time step |
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165 | ! |
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166 | REAL(wp), DIMENSION(jpi,jpj) :: zdeltastar_t ! Delta* at T-points |
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167 | REAL(wp), DIMENSION(jpi,jpj) :: zten_i ! Tension |
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168 | REAL(wp), DIMENSION(jpi,jpj) :: zp_deltastar_t ! P/delta* at T points |
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169 | REAL(wp), DIMENSION(jpi,jpj) :: zzt, zet ! Viscosity pre-factors at T points |
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170 | REAL(wp), DIMENSION(jpi,jpj) :: zef ! Viscosity pre-factor at F point |
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171 | ! |
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172 | REAL(wp), DIMENSION(jpi,jpj) :: zmt ! Mass per unit area at t-point |
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173 | REAL(wp), DIMENSION(jpi,jpj) :: zmf ! Coriolis factor (m*f) at t-point |
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174 | 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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175 | REAL(wp), DIMENSION(jpi,jpj) :: zu_c, zv_c ! "current" ice velocity (m/s), average of previous two OL iterates |
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176 | REAL(wp), DIMENSION(jpi,jpj) :: zu_b, zv_b ! velocity at previous sub-iterate |
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177 | REAL(wp), DIMENSION(jpi,jpj) :: zuerr, zverr ! absolute U/Vvelocity difference between current and previous sub-iterates |
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178 | ! |
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179 | REAL(wp), DIMENSION(jpi,jpj) :: zds ! shear |
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180 | REAL(wp), DIMENSION(jpi,jpj) :: zsshdyn ! array used for the calculation of ice surface slope: |
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181 | ! ! ocean surface (ssh_m) if ice is not embedded |
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182 | ! ! ice bottom surface if ice is embedded |
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183 | REAL(wp), DIMENSION(jpi,jpj) :: zCwU, zCwV ! ice-ocean drag pre-factor (rho*c*module(u)) |
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184 | REAL(wp), DIMENSION(jpi,jpj) :: zspgU, zspgV ! surface pressure gradient at U/V points |
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185 | REAL(wp), DIMENSION(jpi,jpj) :: zCorU, zCorV ! Coriolis stress array |
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186 | REAL(wp), DIMENSION(jpi,jpj) :: ztaux_ai, ztauy_ai ! ice-atm. stress at U-V points |
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187 | REAL(wp), DIMENSION(jpi,jpj) :: ztaux_oi_rhsu, ztauy_oi_rhsv ! ice-ocean stress RHS contribution at U-V points |
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188 | REAL(wp), DIMENSION(jpi,jpj) :: zs1_rhsu, zs2_rhsu, zs12_rhsu ! internal stress contributions to RHSU |
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189 | REAL(wp), DIMENSION(jpi,jpj) :: zs1_rhsv, zs2_rhsv, zs12_rhsv ! internal stress contributions to RHSV |
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190 | REAL(wp), DIMENSION(jpi,jpj) :: zf_rhsu, zf_rhsv ! U- and V- components of internal force RHS contributions |
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191 | REAL(wp), DIMENSION(jpi,jpj) :: zrhsu, zrhsv ! U and V RHS |
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192 | REAL(wp), DIMENSION(jpi,jpj) :: zAU, zBU, zCU, zDU, zEU ! Linear system coefficients, U equation |
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193 | REAL(wp), DIMENSION(jpi,jpj) :: zAV, zBV, zCV, zDV, zEV ! Linear system coefficients, V equation |
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194 | REAL(wp), DIMENSION(jpi,jpj) :: zFU, zFU_prime, zBU_prime ! Rearranged linear system coefficients, U equation |
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195 | REAL(wp), DIMENSION(jpi,jpj) :: zFV, zFV_prime, zBV_prime ! Rearranged linear system coefficients, V equation |
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196 | REAL(wp), DIMENSION(jpi,jpj) :: zCU_prime, zCV_prime ! Rearranged linear system coefficients, V equation |
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197 | !!! REAL(wp), DIMENSION(jpi,jpj) :: ztaux_bi, ztauy_bi ! ice-OceanBottom stress at U-V points (landfast) |
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198 | !!! REAL(wp), DIMENSION(jpi,jpj) :: ztaux_base, ztauy_base ! ice-bottom stress at U-V points (landfast) |
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199 | ! |
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200 | REAL(wp), DIMENSION(jpi,jpj) :: zmsk00, zmsk15 |
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201 | REAL(wp), DIMENSION(jpi,jpj) :: zmsk01x, zmsk01y ! mask for lots of ice (1), little ice (0) |
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202 | REAL(wp), DIMENSION(jpi,jpj) :: zmsk00x, zmsk00y ! mask for ice presence (1), no ice (0) |
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203 | ! |
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204 | REAL(wp), PARAMETER :: zepsi = 1.0e-20_wp ! tolerance parameter |
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205 | REAL(wp), PARAMETER :: zmmin = 1._wp ! ice mass (kg/m2) below which ice velocity becomes very small |
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206 | REAL(wp), PARAMETER :: zamin = 0.001_wp ! ice concentration below which ice velocity becomes very small |
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207 | !! --- diags |
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208 | REAL(wp) :: zsig1, zsig2, zsig12, zdelta, z1_strength, zfac_x, zfac_y |
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209 | REAL(wp), DIMENSION(jpi,jpj) :: zs1, zs2, zs12, zs12f ! stress tensor components |
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210 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: zsig_I, zsig_II, zsig1_p, zsig2_p |
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211 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: ztaux_oi, ztauy_oi |
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212 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: zdiag_xmtrp_ice, zdiag_ymtrp_ice ! X/Y-component of ice mass transport (kg/s, SIMIP) |
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213 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: zdiag_xmtrp_snw, zdiag_ymtrp_snw ! X/Y-component of snow mass transport (kg/s, SIMIP) |
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214 | REAL(wp), ALLOCATABLE, DIMENSION(:,:) :: zdiag_xatrp, zdiag_yatrp ! X/Y-component of area transport (m2/s, SIMIP) |
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215 | |
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216 | |
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217 | CALL ctl_stop( 'STOP', 'icedyn_rhg_vp: stop because vp rheology is an ongoing work and should not be used' ) |
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218 | |
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219 | !!---------------------------------------------------------------------------------------------------------------------- |
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220 | !!$ ! DEBUG put all forcing terms to zero |
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221 | !!$ ! air-ice drag |
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222 | !!$ utau_ice(:,:) = 0._wp |
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223 | !!$ vtau_ice(:,:) = 0._wp |
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224 | !!$ ! coriolis |
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225 | !!$ ff_t(:,:) = 0._wp |
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226 | !!$ ! ice-ocean drag |
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227 | !!$ rn_cio = 0._wp |
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228 | !!$ ! ssh |
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229 | !!$ ! done line 330 !!! dont forget to act there |
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230 | !!$ ! END DEBUG |
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231 | |
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232 | IF( kt == nit000 .AND. lwp ) WRITE(numout,*) '-- ice_dyn_rhg_vp: VP sea-ice rheology (LSR solver)' |
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233 | IF( lwp ) WRITE(numout,*) '-- ice_dyn_rhg_vp: VP sea-ice rheology (LSR solver)' |
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234 | |
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235 | !------------------------------------------------------------------------------! |
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236 | ! |
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237 | ! --- Initialization |
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238 | ! |
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239 | !------------------------------------------------------------------------------! |
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240 | |
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241 | ! for diagnostics and convergence tests |
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242 | DO_2D( nn_hls, nn_hls, nn_hls, nn_hls ) |
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243 | zmsk00(ji,jj) = MAX( 0._wp , SIGN( 1._wp , at_i(ji,jj) - epsi06 ) ) ! 1 if ice , 0 if no ice |
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244 | END_2D |
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245 | IF( nn_rhg_chkcvg > 0 ) THEN |
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246 | DO_2D( nn_hls, nn_hls, nn_hls, nn_hls ) |
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247 | zmsk15(ji,jj) = MAX( 0._wp , SIGN( 1._wp , at_i(ji,jj) - 0.15_wp ) ) ! 1 if 15% ice, 0 if less |
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248 | END_2D |
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249 | ENDIF |
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250 | |
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251 | IF ( lp_zebra_vp ) THEN; nn_zebra_vp = 2 |
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252 | ELSE; nn_zebra_vp = 1; ENDIF |
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253 | |
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254 | nn_nvp = nn_vp_nout * nn_vp_ninn ! maximum number of iterations |
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255 | |
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256 | IF( lwp ) WRITE(numout,*) ' lp_zebra_vp : ', lp_zebra_vp |
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257 | IF( lwp ) WRITE(numout,*) ' nn_zebra_vp : ', nn_zebra_vp |
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258 | IF( lwp ) WRITE(numout,*) ' nn_nvp : ', nn_nvp |
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259 | |
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260 | zrhoco = rho0 * rn_cio |
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261 | |
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262 | ! ecc2: square of yield ellipse eccentricity |
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263 | ecc2 = rn_ecc * rn_ecc |
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264 | z1_ecc2 = 1._wp / ecc2 |
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265 | |
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266 | ! Initialise convergence checks |
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267 | IF( nn_rhg_chkcvg /= 0 ) THEN |
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268 | |
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269 | ! ice area for global mean kinetic energy |
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270 | zglob_area = glob_sum( 'ice_rhg_vp', at_i(:,:) * e1e2t(:,:) ) ! global ice area (km2) |
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271 | |
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272 | ENDIF |
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273 | |
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274 | ! Landfast param from Lemieux(2016): add isotropic tensile strength (following Konig Beatty and Holland, 2010) |
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275 | ! MV: Not working yet... |
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276 | IF( ln_landfast_L16 ) THEN ; zkt = rn_lf_tensile |
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277 | ELSE ; zkt = 0._wp |
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278 | ENDIF |
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279 | |
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280 | zs1_rhsu(:,:) = 0._wp; zs2_rhsu(:,:) = 0._wp; zs1_rhsv(:,:) = 0._wp; zs2_rhsv(:,:) = 0._wp |
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281 | zAU(:,:) = 0._wp; zBU(:,:) = 0._wp; zCU(:,:) = 0._wp; zDU(:,:) = 0._wp; zEU(:,:) = 0._wp; |
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282 | zAV(:,:) = 0._wp; zBV(:,:) = 0._wp; zCV(:,:) = 0._wp; zDV(:,:) = 0._wp; zEV(:,:) = 0._wp; |
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283 | zrhsu(:,:) = 0._wp; zrhsv(:,:) = 0._wp |
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284 | zf_rhsu(:,:) = 0._wp; zf_rhsv(:,:) = 0._wp |
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285 | |
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286 | !------------------------------------------------------------------------------! |
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287 | ! |
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288 | ! --- Time-independent quantities |
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289 | ! |
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290 | !------------------------------------------------------------------------------! |
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291 | |
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292 | CALL ice_strength ! strength at T points |
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293 | |
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294 | !------------------------------ |
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295 | ! -- F-mask (code from EVP) |
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296 | !------------------------------ |
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297 | IF( kt == nit000 ) THEN |
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298 | ! MartinV: |
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299 | ! In EVP routine, fimask is applied on shear at F-points, in order to enforce the lateral boundary condition (no-slip, ..., free-slip) |
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300 | ! I am not sure the same recipe applies here |
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301 | |
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302 | ! - ocean/land mask |
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303 | ALLOCATE( fimask(jpi,jpj) ) |
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304 | IF( rn_ishlat == 0._wp ) THEN |
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305 | DO_2D( 0, 0, 0, 0 ) |
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306 | fimask(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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307 | END_2D |
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308 | ELSE |
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309 | DO_2D( 0, 0, 0, 0 ) |
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310 | fimask(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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311 | ! Lateral boundary conditions on velocity (modify fimask) |
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312 | IF( fimask(ji,jj) == 0._wp ) THEN |
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313 | fimask(ji,jj) = rn_ishlat * MIN( 1._wp , MAX( umask(ji,jj,1), umask(ji,jj+1,1), & |
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314 | & vmask(ji,jj,1), vmask(ji+1,jj,1) ) ) |
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315 | ENDIF |
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316 | END_2D |
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317 | ENDIF |
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318 | |
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319 | CALL lbc_lnk( 'icedyn_rhg_vp', fimask, 'F', 1._wp ) |
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320 | ENDIF |
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321 | |
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322 | !---------------------------------------------------------------------------------------------------------- |
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323 | ! -- Time-independent pre-factors for acceleration, ocean drag, coriolis, atmospheric drag, surface tilt |
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324 | !---------------------------------------------------------------------------------------------------------- |
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325 | ! Compute all terms & factors independent of velocities, or only depending on velocities at previous time step |
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326 | |
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327 | ! sea surface height |
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328 | ! embedded sea ice: compute representative ice top surface |
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329 | ! non-embedded sea ice: use ocean surface for slope calculation |
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330 | zsshdyn(:,:) = ice_var_sshdyn( ssh_m, snwice_mass, snwice_mass_b) |
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331 | !!$ zsshdyn(:,:) = 0._wp ! DEBUG CAREFUL !!! |
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332 | |
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333 | DO_2D( nn_hls, nn_hls, nn_hls, nn_hls ) |
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334 | zm1 = ( rhos * vt_s(ji,jj) + rhoi * vt_i(ji,jj) ) ! Ice/snow mass at U-V points |
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335 | zmf (ji,jj) = zm1 * ff_t(ji,jj) ! Coriolis at T points (m*f) |
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336 | END_2D |
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337 | |
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338 | DO_2D( nn_hls-1, nn_hls-1, nn_hls-1, nn_hls-1 ) |
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339 | |
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340 | ! Ice fraction at U-V points |
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341 | za_iU(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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342 | za_iV(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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343 | |
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344 | ! Ice/snow mass at U-V points |
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345 | zm1 = ( rhos * vt_s(ji ,jj ) + rhoi * vt_i(ji ,jj ) ) |
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346 | zm2 = ( rhos * vt_s(ji+1,jj ) + rhoi * vt_i(ji+1,jj ) ) |
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347 | zm3 = ( rhos * vt_s(ji ,jj+1) + rhoi * vt_i(ji ,jj+1) ) |
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348 | 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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349 | 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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350 | |
---|
351 | ! Mass per unit area divided by time step |
---|
352 | zmassU_t(ji,jj) = zmassU * r1_Dt_ice |
---|
353 | zmassV_t(ji,jj) = zmassV * r1_Dt_ice |
---|
354 | |
---|
355 | ! Acceleration term contribution to RHS (depends on velocity at previous time step) |
---|
356 | zmU_t(ji,jj) = zmassU_t(ji,jj) * u_ice(ji,jj) |
---|
357 | zmV_t(ji,jj) = zmassV_t(ji,jj) * v_ice(ji,jj) |
---|
358 | |
---|
359 | ! Ocean currents at U-V points |
---|
360 | v_oceU(ji,jj) = 0.25_wp * ( v_oce(ji,jj) + v_oce(ji,jj-1) + v_oce(ji+1,jj) + v_oce(ji+1,jj-1) ) * umask(ji,jj,1) |
---|
361 | u_oceV(ji,jj) = 0.25_wp * ( u_oce(ji,jj) + u_oce(ji-1,jj) + u_oce(ji,jj+1) + u_oce(ji-1,jj+1) ) * vmask(ji,jj,1) |
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362 | |
---|
363 | ! Wind stress |
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364 | ztaux_ai(ji,jj) = za_iU(ji,jj) * utau_ice(ji,jj) |
---|
365 | ztauy_ai(ji,jj) = za_iV(ji,jj) * vtau_ice(ji,jj) |
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366 | |
---|
367 | ! Force due to sea surface tilt(- m*g*GRAD(ssh)) |
---|
368 | zspgU(ji,jj) = - zmassU * grav * ( zsshdyn(ji+1,jj) - zsshdyn(ji,jj) ) * r1_e1u(ji,jj) |
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369 | zspgV(ji,jj) = - zmassV * grav * ( zsshdyn(ji,jj+1) - zsshdyn(ji,jj) ) * r1_e2v(ji,jj) |
---|
370 | |
---|
371 | ! Mask for ice presence (1) or absence (0) |
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372 | zmsk00x(ji,jj) = 1._wp - MAX( 0._wp, SIGN( 1._wp, -zmassU ) ) ! 0 if no ice |
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373 | zmsk00y(ji,jj) = 1._wp - MAX( 0._wp, SIGN( 1._wp, -zmassV ) ) ! 0 if no ice |
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374 | |
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375 | ! Mask for lots of ice (1) or little ice (0) |
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376 | IF ( zmassU <= zmmin .AND. za_iU(ji,jj) <= zamin ) THEN ; zmsk01x(ji,jj) = 0._wp |
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377 | ELSE ; zmsk01x(ji,jj) = 1._wp ; ENDIF |
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378 | IF ( zmassV <= zmmin .AND. za_iV(ji,jj) <= zamin ) THEN ; zmsk01y(ji,jj) = 0._wp |
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379 | ELSE ; zmsk01y(ji,jj) = 1._wp ; ENDIF |
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380 | |
---|
381 | ! MV TEST DEBUG |
---|
382 | !!$ IF ( ( zmt(ji,jj) <= zmmin .OR. zmt(ji+1,jj) <= zmmin ) .AND. & |
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383 | !!$ & ( at_i(ji,jj) <= zamin .OR. at_i(ji+1,jj) <= zamin ) ) THEN ; zmsk01x(ji,jj) = 0._wp |
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384 | !!$ ELSE ; zmsk01x(ji,jj) = 1._wp ; ENDIF |
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385 | !!$ |
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386 | !!$ IF ( ( zmt(ji,jj) <= zmmin .OR. zmt(ji,jj+1) <= zmmin ) .AND. & |
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387 | !!$ & ( at_i(ji,jj) <= zamin .OR. at_i(ji,jj+1) <= zamin ) ) THEN ; zmsk01y(ji,jj) = 0._wp |
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388 | !!$ ELSE ; zmsk01y(ji,jj) = 1._wp ; ENDIF |
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389 | ! END MV TEST DEBUG |
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390 | |
---|
391 | END_2D |
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392 | |
---|
393 | !!$ CALL iom_put( 'zmsk00x' , zmsk00x ) ! MV DEBUG |
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394 | !!$ CALL iom_put( 'zmsk00y' , zmsk00y ) ! MV DEBUG |
---|
395 | !!$ CALL iom_put( 'zmsk01x' , zmsk01x ) ! MV DEBUG |
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396 | !!$ CALL iom_put( 'zmsk01y' , zmsk01y ) ! MV DEBUG |
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397 | !!$ CALL iom_put( 'ztaux_ai' , ztaux_ai ) ! MV DEBUG |
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398 | !!$ CALL iom_put( 'ztauy_ai' , ztauy_ai ) ! MV DEBUG |
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399 | !!$ CALL iom_put( 'zspgU' , zspgU ) ! MV DEBUG |
---|
400 | !!$ CALL iom_put( 'zspgV' , zspgV ) ! MV DEBUG |
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401 | !!$ |
---|
402 | !------------------------------------------------------------------------------! |
---|
403 | ! |
---|
404 | ! --- Start outer loop |
---|
405 | ! |
---|
406 | !------------------------------------------------------------------------------! |
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407 | |
---|
408 | zu_c(:,:) = u_ice(:,:) |
---|
409 | zv_c(:,:) = v_ice(:,:) |
---|
410 | |
---|
411 | jter = 0 |
---|
412 | |
---|
413 | DO i_out = 1, nn_vp_nout |
---|
414 | |
---|
415 | IF( lwp ) WRITE(numout,*) ' outer loop i_out : ', i_out |
---|
416 | |
---|
417 | ! Velocities used in the non linear terms are the average of the past two iterates |
---|
418 | ! u_it = 0.5 * ( u_{it-1} + u_{it-2}) |
---|
419 | ! Also used in Hibler and Ackley (1983); Zhang and Hibler (1997); Lemieux and Tremblay (2009) |
---|
420 | zu_c(:,:) = 0.5_wp * ( u_ice(:,:) + zu_c(:,:) ) |
---|
421 | zv_c(:,:) = 0.5_wp * ( v_ice(:,:) + zv_c(:,:) ) |
---|
422 | |
---|
423 | !------------------------------------------------------------------------------! |
---|
424 | ! |
---|
425 | ! --- Right-hand side (RHS) of the linear problem |
---|
426 | ! |
---|
427 | !------------------------------------------------------------------------------! |
---|
428 | ! In the outer loop, one needs to update all RHS terms |
---|
429 | ! with explicit velocity dependencies (viscosities, coriolis, ocean stress) |
---|
430 | ! as a function of uc |
---|
431 | ! |
---|
432 | |
---|
433 | !------------------------------------------ |
---|
434 | ! -- Strain rates, viscosities and P/Delta |
---|
435 | !------------------------------------------ |
---|
436 | |
---|
437 | ! --- divergence, tension & shear (Appendix B of Hunke & Dukowicz, 2002) --- ! |
---|
438 | DO_2D( nn_hls, nn_hls-1, nn_hls, nn_hls-1 ) |
---|
439 | |
---|
440 | ! shear at F points |
---|
441 | zds(ji,jj) = ( ( zu_c(ji,jj+1) * r1_e1u(ji,jj+1) - zu_c(ji,jj) * r1_e1u(ji,jj) ) * e1f(ji,jj) * e1f(ji,jj) & |
---|
442 | & + ( zv_c(ji+1,jj) * r1_e2v(ji+1,jj) - zv_c(ji,jj) * r1_e2v(ji,jj) ) * e2f(ji,jj) * e2f(ji,jj) & |
---|
443 | & ) * r1_e1e2f(ji,jj) * fimask(ji,jj) |
---|
444 | |
---|
445 | END_2D |
---|
446 | |
---|
447 | CALL lbc_lnk( 'icedyn_rhg_vp', zds, 'F', 1. ) ! MV TEST could be un-necessary according to Gurvan |
---|
448 | !!$ CALL iom_put( 'zds' , zds ) ! MV DEBUG |
---|
449 | |
---|
450 | IF( lwp ) WRITE(numout,*) ' outer loop 1a i_out : ', i_out |
---|
451 | |
---|
452 | !DO jj = 2, jpj - 1 ! loop to jpi,jpj to avoid making a communication for zs1,zs2,zs12 |
---|
453 | ! DO ji = 2, jpi - 1 ! |
---|
454 | |
---|
455 | ! MV DEBUG |
---|
456 | DO jj = 2, jpj ! loop to jpi,jpj to avoid making a communication for zs1,zs2,zs12 |
---|
457 | DO ji = 2, jpi ! |
---|
458 | ! END MV DEBUG |
---|
459 | |
---|
460 | ! shear**2 at T points (doc eq. A16) |
---|
461 | zds2 = ( zds(ji,jj ) * zds(ji,jj ) * e1e2f(ji,jj ) + zds(ji-1,jj ) * zds(ji-1,jj ) * e1e2f(ji-1,jj ) & |
---|
462 | & + 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) & |
---|
463 | & ) * 0.25_wp * r1_e1e2t(ji,jj) |
---|
464 | |
---|
465 | ! divergence at T points |
---|
466 | zdiv = ( e2u(ji,jj) * zu_c(ji,jj) - e2u(ji-1,jj) * zu_c(ji-1,jj) & |
---|
467 | & + e1v(ji,jj) * zv_c(ji,jj) - e1v(ji,jj-1) * zv_c(ji,jj-1) & |
---|
468 | & ) * r1_e1e2t(ji,jj) |
---|
469 | zdiv2 = zdiv * zdiv |
---|
470 | |
---|
471 | ! tension at T points |
---|
472 | zdt = ( ( zu_c(ji,jj) * r1_e2u(ji,jj) - zu_c(ji-1,jj) * r1_e2u(ji-1,jj) ) * e2t(ji,jj) * e2t(ji,jj) & |
---|
473 | & - ( zv_c(ji,jj) * r1_e1v(ji,jj) - zv_c(ji,jj-1) * r1_e1v(ji,jj-1) ) * e1t(ji,jj) * e1t(ji,jj) & |
---|
474 | & ) * r1_e1e2t(ji,jj) |
---|
475 | zdt2 = zdt * zdt |
---|
476 | |
---|
477 | ! delta at T points |
---|
478 | zdeltat = SQRT( zdiv2 + ( zdt2 + zds2 ) * z1_ecc2 ) |
---|
479 | |
---|
480 | ! delta* at T points (following Lemieux and Dupont, GMD 2020) |
---|
481 | zdeltastar_t(ji,jj) = zdeltat + rn_creepl |
---|
482 | |
---|
483 | ! P/delta at T-points |
---|
484 | zp_deltastar_t(ji,jj) = strength(ji,jj) / zdeltastar_t(ji,jj) |
---|
485 | |
---|
486 | ! Temporary zzt and zet factors at T-points |
---|
487 | zzt(ji,jj) = zp_deltastar_t(ji,jj) * r1_e1e2t(ji,jj) |
---|
488 | zet(ji,jj) = zzt(ji,jj) * z1_ecc2 |
---|
489 | |
---|
490 | END DO |
---|
491 | END DO |
---|
492 | |
---|
493 | CALL lbc_lnk( 'icedyn_rhg_vp', zp_deltastar_t , 'T', 1. , zzt , 'T', 1., zet, 'T', 1. ) |
---|
494 | |
---|
495 | !!$ CALL iom_put( 'zzt' , zzt ) ! MV DEBUG |
---|
496 | !!$ CALL iom_put( 'zet' , zet ) ! MV DEBUG |
---|
497 | !!$ CALL iom_put( 'zp_deltastar_t', zp_deltastar_t ) ! MV DEBUG |
---|
498 | |
---|
499 | IF( lwp ) WRITE(numout,*) ' outer loop 1b i_out : ', i_out |
---|
500 | |
---|
501 | DO jj = 1, jpj - 1 |
---|
502 | DO ji = 1, jpi - 1 |
---|
503 | |
---|
504 | ! P/delta* at F points |
---|
505 | zp_deltastar_f = 0.25_wp * ( zp_deltastar_t(ji,jj) + zp_deltastar_t(ji+1,jj) + zp_deltastar_t(ji,jj+1) + zp_deltastar_t(ji+1,jj+1) ) |
---|
506 | |
---|
507 | ! Temporary zef factor at F-point |
---|
508 | zef(ji,jj) = zp_deltastar_f * r1_e1e2f(ji,jj) * z1_ecc2 * fimask(ji,jj) |
---|
509 | |
---|
510 | END DO |
---|
511 | END DO |
---|
512 | |
---|
513 | CALL lbc_lnk( 'icedyn_rhg_vp', zef, 'F', 1. ) |
---|
514 | !!$ CALL iom_put( 'zef' , zef ) ! MV DEBUG |
---|
515 | IF( lwp ) WRITE(numout,*) ' outer loop 1c i_out : ', i_out |
---|
516 | |
---|
517 | !--------------------------------------------------- |
---|
518 | ! -- Ocean-ice drag and Coriolis RHS contributions |
---|
519 | !--------------------------------------------------- |
---|
520 | |
---|
521 | DO jj = 2, jpj - 1 |
---|
522 | DO ji = 2, jpi - 1 |
---|
523 | |
---|
524 | !--- ice u-velocity @V points, v-velocity @U points (for non-linear drag computation) |
---|
525 | zu_cV = 0.25_wp * ( zu_c(ji,jj) + zu_c(ji-1,jj) + zu_c(ji,jj+1) + zu_c(ji-1,jj+1) ) * vmask(ji,jj,1) |
---|
526 | zv_cU = 0.25_wp * ( zv_c(ji,jj) + zv_c(ji,jj-1) + zv_c(ji+1,jj) + zv_c(ji+1,jj-1) ) * umask(ji,jj,1) |
---|
527 | |
---|
528 | !--- non-linear drag coefficients (need to be updated at each outer loop, see Lemieux and Tremblay JGR09, p.3, beginning of Section 3) |
---|
529 | zCwU(ji,jj) = za_iU(ji,jj) * zrhoco * SQRT( ( zu_c (ji,jj) - u_oce (ji,jj) ) * ( zu_c (ji,jj) - u_oce (ji,jj) ) & |
---|
530 | & + ( zv_cU - v_oceU(ji,jj) ) * ( zv_cU - v_oceU(ji,jj) ) ) |
---|
531 | zCwV(ji,jj) = za_iV(ji,jj) * zrhoco * SQRT( ( zv_c (ji,jj) - v_oce (ji,jj) ) * ( zv_c (ji,jj) - v_oce (ji,jj) ) & |
---|
532 | & + ( zu_cV - u_oceV(ji,jj) ) * ( zu_cV - u_oceV(ji,jj) ) ) |
---|
533 | |
---|
534 | !--- Ocean-ice drag contributions to RHS |
---|
535 | ztaux_oi_rhsu(ji,jj) = zCwU(ji,jj) * u_oce(ji,jj) |
---|
536 | ztauy_oi_rhsv(ji,jj) = zCwV(ji,jj) * v_oce(ji,jj) |
---|
537 | |
---|
538 | ! --- U-component of Coriolis Force (energy conserving formulation) |
---|
539 | ! Note Lemieux et al 2008 recommend to do that implicitly, but I don't really see how this could be done |
---|
540 | zCorU(ji,jj) = 0.25_wp * r1_e1u(ji,jj) * & |
---|
541 | & ( zmf(ji ,jj) * ( e1v(ji ,jj) * zv_c(ji ,jj) + e1v(ji ,jj-1) * zv_c(ji ,jj-1) ) & |
---|
542 | & + zmf(ji+1,jj) * ( e1v(ji+1,jj) * zv_c(ji+1,jj) + e1v(ji+1,jj-1) * zv_c(ji+1,jj-1) ) ) |
---|
543 | |
---|
544 | ! --- V-component of Coriolis Force (energy conserving formulation) |
---|
545 | zCorV(ji,jj) = - 0.25_wp * r1_e2v(ji,jj) * & |
---|
546 | & ( zmf(ji,jj ) * ( e2u(ji,jj ) * zu_c(ji,jj ) + e2u(ji-1,jj ) * zu_c(ji-1,jj ) ) & |
---|
547 | & + zmf(ji,jj+1) * ( e2u(ji,jj+1) * zu_c(ji,jj+1) + e2u(ji-1,jj+1) * zu_c(ji-1,jj+1) ) ) |
---|
548 | |
---|
549 | END DO |
---|
550 | END DO |
---|
551 | |
---|
552 | IF( lwp ) WRITE(numout,*) ' outer loop 1d i_out : ', i_out |
---|
553 | |
---|
554 | CALL lbc_lnk( 'icedyn_rhg_vp', zCwU , 'U', -1., zCwV, 'V', -1. ) |
---|
555 | CALL lbc_lnk( 'icedyn_rhg_vp', zCorU, 'U', -1., zCorV, 'V', -1. ) |
---|
556 | |
---|
557 | !!$ CALL iom_put( 'zCwU' , zCwU ) ! MV DEBUG |
---|
558 | !!$ CALL iom_put( 'zCwV' , zCwV ) ! MV DEBUG |
---|
559 | !!$ CALL iom_put( 'zCorU' , zCorU ) ! MV DEBUG |
---|
560 | !!$ CALL iom_put( 'zCorV' , zCorV ) ! MV DEBUG |
---|
561 | |
---|
562 | IF( lwp ) WRITE(numout,*) ' outer loop 1f i_out : ', i_out |
---|
563 | |
---|
564 | ! a priori, Coriolis and drag terms only affect diagonal or independent term of the linear system, |
---|
565 | ! so there is no need for lbclnk on drag and coriolis |
---|
566 | |
---|
567 | !------------------------------------- |
---|
568 | ! -- Internal stress RHS contribution |
---|
569 | !------------------------------------- |
---|
570 | |
---|
571 | ! --- Stress contributions at T-points |
---|
572 | DO jj = 2, jpj ! loop to jpi,jpj to avoid making a communication for zs1,zs2,zs12 |
---|
573 | DO ji = 2, jpi ! |
---|
574 | |
---|
575 | ! sig1 contribution to RHS of U-equation at T-points |
---|
576 | zs1_rhsu(ji,jj) = zzt(ji,jj) * ( e1v(ji,jj) * zv_c(ji,jj) - e1v(ji,jj-1) * zv_c(ji,jj-1) - 1.0_wp ) |
---|
577 | |
---|
578 | ! sig2 contribution to RHS of U-equation at T-points |
---|
579 | zs2_rhsu(ji,jj) = - zet(ji,jj) * ( r1_e1v(ji,jj) * zv_c(ji,jj) - r1_e1v(ji,jj-1) * zv_c(ji,jj-1) ) * e1t(ji,jj) * e1t(ji,jj) |
---|
580 | |
---|
581 | ! sig1 contribution to RHS of V-equation at T-points |
---|
582 | zs1_rhsv(ji,jj) = zzt(ji,jj) * ( e2u(ji,jj) * zu_c(ji,jj) - e2u(ji-1,jj) * zu_c(ji-1,jj) - 1.0_wp ) |
---|
583 | |
---|
584 | ! sig2 contribution to RHS of V-equation at T-points |
---|
585 | zs2_rhsv(ji,jj) = zet(ji,jj) * ( r1_e2u(ji,jj) * zu_c(ji,jj) - r1_e2u(ji-1,jj) * zu_c(ji-1,jj) ) * e2t(ji,jj) * e2t(ji,jj) |
---|
586 | |
---|
587 | END DO |
---|
588 | END DO |
---|
589 | |
---|
590 | !!$ CALL iom_put( 'zs1_rhsu' , zs1_rhsu ) ! MV DEBUG |
---|
591 | !!$ CALL iom_put( 'zs2_rhsu' , zs2_rhsu ) ! MV DEBUG |
---|
592 | !!$ CALL iom_put( 'zs1_rhsv' , zs1_rhsv ) ! MV DEBUG |
---|
593 | !!$ CALL iom_put( 'zs2_rhsv' , zs2_rhsv ) ! MV DEBUG |
---|
594 | |
---|
595 | ! a priori, no lbclnk, because rhsu is only used in the inner domain |
---|
596 | |
---|
597 | ! --- Stress contributions at f-points |
---|
598 | ! MV NOTE: I applied fimask on zds, by mimetism on EVP, but without deep understanding of what I was doing |
---|
599 | ! My guess is that this is the way to enforce boundary conditions on strain rate tensor |
---|
600 | |
---|
601 | IF( lwp ) WRITE(numout,*) ' outer loop 2 i_out : ', i_out |
---|
602 | |
---|
603 | DO jj = 1, jpj - 1 |
---|
604 | DO ji = 1, jpi - 1 |
---|
605 | |
---|
606 | ! sig12 contribution to RHS of U equation at F-points |
---|
607 | zs12_rhsu(ji,jj) = - zef(ji,jj) * ( r1_e2v(ji+1,jj) * zv_c(ji+1,jj) - r1_e2v(ji,jj) * zv_c(ji,jj) ) * e2f(ji,jj) * e2f(ji,jj) * fimask(ji,jj) |
---|
608 | |
---|
609 | ! sig12 contribution to RHS of V equation at F-points |
---|
610 | zs12_rhsv(ji,jj) = zef(ji,jj) * ( r1_e1u(ji,jj+1) * zu_c(ji,jj+1) - r1_e1u(ji,jj) * zu_c(ji,jj) ) * e1f(ji,jj) * e1f(ji,jj) * fimask(ji,jj) |
---|
611 | |
---|
612 | END DO |
---|
613 | END DO |
---|
614 | |
---|
615 | CALL lbc_lnk( 'icedyn_rhg_vp', zs12_rhsu, 'F', 1. ) |
---|
616 | CALL lbc_lnk( 'icedyn_rhg_vp', zs12_rhsv, 'F', 1. ) |
---|
617 | |
---|
618 | !!$ CALL iom_put( 'zs12_rhsu' , zs12_rhsu ) ! MV DEBUG |
---|
619 | !!$ CALL iom_put( 'zs12_rhsv' , zs12_rhsv ) ! MV DEBUG |
---|
620 | |
---|
621 | ! a priori, no lbclnk, because rhsu are only used in the inner domain |
---|
622 | |
---|
623 | ! --- Internal force contributions to RHS, taken as divergence of stresses (Appendix C of Hunke and Dukowicz, 2002) |
---|
624 | ! OPT: merge with next loop and use intermediate scalars for zf_rhsu |
---|
625 | |
---|
626 | DO jj = 2, jpj - 1 |
---|
627 | DO ji = 2, jpi - 1 |
---|
628 | ! --- U component of internal force contribution to RHS at U points |
---|
629 | zf_rhsu(ji,jj) = 0.5_wp * r1_e1e2u(ji,jj) * & |
---|
630 | ( e2u(ji,jj) * ( zs1_rhsu(ji+1,jj) - zs1_rhsu(ji,jj) ) & |
---|
631 | & + r1_e2u(ji,jj) * ( e2t(ji+1,jj) * e2t(ji+1,jj) * zs2_rhsu(ji+1,jj) - e2t(ji,jj) * e2t(ji,jj) * zs2_rhsu(ji,jj) ) & |
---|
632 | & + 2._wp * r1_e1u(ji,jj) * ( e1f(ji,jj) * e1f(ji,jj) * zs12_rhsu(ji,jj) - e1f(ji,jj-1) * e1f(ji,jj-1) * zs12_rhsu(ji,jj-1) ) ) |
---|
633 | |
---|
634 | ! --- V component of internal force contribution to RHS at V points |
---|
635 | zf_rhsv(ji,jj) = 0.5_wp * r1_e1e2v(ji,jj) * & |
---|
636 | & ( e1v(ji,jj) * ( zs1_rhsv(ji,jj+1) - zs1_rhsv(ji,jj) ) & |
---|
637 | & + r1_e1v(ji,jj) * ( e1t(ji,jj+1) * e1t(ji,jj+1) * zs2_rhsv(ji,jj+1) - e1t(ji,jj) * e1t(ji,jj) * zs2_rhsv(ji,jj) ) & |
---|
638 | & + 2._wp * r1_e2v(ji,jj) * ( e2f(ji,jj) * e2f(ji,jj) * zs12_rhsv(ji,jj) - e2f(ji-1,jj) * e2f(ji-1,jj) * zs12_rhsv(ji-1,jj) ) ) |
---|
639 | |
---|
640 | END DO |
---|
641 | END DO |
---|
642 | |
---|
643 | !!$ CALL iom_put( 'zf_rhsu' , zf_rhsu ) ! MV DEBUG |
---|
644 | !!$ CALL iom_put( 'zf_rhsv' , zf_rhsv ) ! MV DEBUG |
---|
645 | |
---|
646 | !--------------------------- |
---|
647 | ! -- Sum RHS contributions |
---|
648 | !--------------------------- |
---|
649 | ! |
---|
650 | ! OPT: could use intermediate scalars to reduce memory access |
---|
651 | DO jj = 2, jpj - 1 |
---|
652 | DO ji = 2, jpi - 1 |
---|
653 | |
---|
654 | ! still miss ice ocean stress and acceleration contribution |
---|
655 | zrhsu(ji,jj) = zmU_t(ji,jj) + ztaux_ai(ji,jj) + ztaux_oi_rhsu(ji,jj) + zspgU(ji,jj) + zCorU(ji,jj) + zf_rhsu(ji,jj) |
---|
656 | zrhsv(ji,jj) = zmV_t(ji,jj) + ztauy_ai(ji,jj) + ztauy_oi_rhsv(ji,jj) + zspgV(ji,jj) + zCorV(ji,jj) + zf_rhsu(ji,jj) |
---|
657 | |
---|
658 | END DO |
---|
659 | END DO |
---|
660 | |
---|
661 | CALL lbc_lnk( 'icedyn_rhg_vp', zrhsu, 'U', -1., zrhsv, 'V', -1.) |
---|
662 | CALL lbc_lnk( 'icedyn_rhg_vp', zmU_t, 'U', -1., zmV_t, 'V', -1.) |
---|
663 | CALL lbc_lnk( 'icedyn_rhg_vp', ztaux_oi_rhsu, 'U', -1., ztauy_oi_rhsv, 'V', -1.) |
---|
664 | |
---|
665 | !!$ CALL iom_put( 'zmU_t' , zmU_t ) ! MV DEBUG |
---|
666 | !!$ CALL iom_put( 'zmV_t' , zmV_t ) ! MV DEBUG |
---|
667 | !!$ CALL iom_put( 'ztaux_oi_rhsu' , ztaux_oi_rhsu ) ! MV DEBUG |
---|
668 | !!$ CALL iom_put( 'ztauy_oi_rhsv' , ztauy_oi_rhsv ) ! MV DEBUG |
---|
669 | !!$ CALL iom_put( 'zrhsu' , zrhsu ) ! MV DEBUG |
---|
670 | !!$ CALL iom_put( 'zrhsv' , zrhsv ) ! MV DEBUG |
---|
671 | !!$ |
---|
672 | ! inner domain calculations -> no lbclnk |
---|
673 | |
---|
674 | IF( lwp ) WRITE(numout,*) ' outer loop 4 i_out : ', i_out |
---|
675 | |
---|
676 | !---------------------------------------------------------------------------------------! |
---|
677 | ! |
---|
678 | ! --- Linear system matrix |
---|
679 | ! |
---|
680 | !---------------------------------------------------------------------------------------! |
---|
681 | |
---|
682 | ! Linear system matrix contains all implicit contributions |
---|
683 | ! 1) internal forces, 2) acceleration, 3) ice-ocean drag |
---|
684 | |
---|
685 | ! The linear system equation is written as follows |
---|
686 | ! AU * u_{i-1,j} + BU * u_{i,j} + CU * u_{i+1,j} |
---|
687 | ! = DU * u_{i,j-1} + EU * u_{i,j+1} + RHS (! my convention, not the same as ZH97 ) |
---|
688 | |
---|
689 | ! MV Note 1: martin losch applies boundary condition to BU in mitGCM - check whether it is necessary here ? |
---|
690 | ! MV Note 2: "T" factor calculations can be optimized by putting things out of the loop |
---|
691 | ! only zzt and zet are iteration-dependent, other only depend on scale factors |
---|
692 | |
---|
693 | DO ji = 2, jpi - 1 ! internal domain do loop |
---|
694 | DO jj = 2, jpj - 1 |
---|
695 | |
---|
696 | !------------------------------------- |
---|
697 | ! -- Internal forces LHS contribution |
---|
698 | !------------------------------------- |
---|
699 | ! |
---|
700 | ! --- U-component |
---|
701 | ! |
---|
702 | ! "T" factors (intermediate results) |
---|
703 | ! |
---|
704 | zfac = 0.5_wp * r1_e1e2u(ji,jj) |
---|
705 | zfac1 = zfac * e2u(ji,jj) |
---|
706 | zfac2 = zfac * r1_e2u(ji,jj) |
---|
707 | zfac3 = 2._wp * zfac * r1_e1u(ji,jj) |
---|
708 | |
---|
709 | zt12U = - zfac1 * zzt(ji+1,jj) |
---|
710 | zt11U = zfac1 * zzt(ji,jj) |
---|
711 | |
---|
712 | zt22U = - zfac2 * zet(ji+1,jj) * e2t(ji+1,jj) * e2t(ji+1,jj) * e2t(ji+1,jj) * e2t(ji+1,jj) |
---|
713 | zt21U = zfac2 * zet(ji,jj) * e2t(ji,jj) * e2t(ji,jj) * e2t(ji,jj) * e2t(ji,jj) |
---|
714 | |
---|
715 | zt122U = - zfac3 * zef(ji,jj) * e1f(ji,jj) * e1f(ji,jj) * e1f(ji,jj) * e1f(ji,jj) |
---|
716 | zt121U = zfac3 * zef(ji,jj-1) * e1f(ji,jj-1) * e1f(ji,jj-1) * e1f(ji,jj-1) * e1f(ji,jj-1) |
---|
717 | |
---|
718 | ! |
---|
719 | ! Linear system coefficients |
---|
720 | ! |
---|
721 | zAU(ji,jj) = - zt11U * e2u(ji-1,jj) - zt21U * r1_e2u(ji-1,jj) |
---|
722 | zBU(ji,jj) = ( zt12U + zt11U ) * e2u(ji,jj) + ( zt22U + zt21U ) * r1_e2u(ji,jj) + ( zt122U + zt121U ) * r1_e1u(ji,jj) |
---|
723 | zCU(ji,jj) = - zt12U * e2u(ji+1,jj) - zt22U * r1_e2u(ji+1,jj) |
---|
724 | |
---|
725 | zDU(ji,jj) = zt121U * r1_e1u(ji,jj-1) |
---|
726 | zEU(ji,jj) = zt122U * r1_e1u(ji,jj+1) |
---|
727 | |
---|
728 | ! |
---|
729 | ! --- V-component |
---|
730 | ! |
---|
731 | ! "T" factors (intermediate results) |
---|
732 | ! |
---|
733 | zfac = 0.5_wp * r1_e1e2v(ji,jj) |
---|
734 | zfac1 = zfac * e2v(ji,jj) |
---|
735 | zfac2 = zfac * r1_e1v(ji,jj) |
---|
736 | zfac3 = 2._wp * zfac * r1_e2v(ji,jj) |
---|
737 | |
---|
738 | zt12V = - zfac1 * zzt(ji,jj+1) |
---|
739 | zt11V = zfac1 * zzt(ji,jj) |
---|
740 | |
---|
741 | zt22V = zfac2 * zet(ji,jj+1) * e1t(ji,jj+1) * e1t(ji,jj+1) * e1t(ji,jj+1) * e1t(ji,jj+1) |
---|
742 | zt21V = - zfac2 * zet(ji,jj) * e1t(ji,jj) * e1t(ji,jj) * e1t(ji,jj) * e1t(ji,jj) |
---|
743 | |
---|
744 | zt122V = zfac3 * zef(ji,jj) * e2f(ji,jj) * e2f(ji,jj) * e2f(ji,jj) * e2f(ji,jj) |
---|
745 | zt121V = - zfac3 * zef(ji-1,jj) * e2f(ji-1,jj) * e2f(ji-1,jj) * e2f(ji-1,jj) * e2f(ji-1,jj) |
---|
746 | |
---|
747 | ! |
---|
748 | ! Linear system coefficients |
---|
749 | ! |
---|
750 | zAV(ji,jj) = - zt11V * e1v(ji,jj-1) + zt21V * r1_e1v(ji,jj-1) |
---|
751 | zBV(ji,jj) = ( zt12V + zt11V ) * e1v(ji,jj) - ( zt22V + zt21V ) * r1_e1v(ji,jj) - ( zt122V + zt121V ) * r1_e2v(ji,jj) |
---|
752 | zCV(ji,jj) = - zt12V * e1v(ji,jj+1) + zt22V * r1_e1v(ji,jj+1) |
---|
753 | |
---|
754 | zDV(ji,jj) = - zt121V * r1_e2v(ji-1,jj) ! mistake is in the pdf notes not here |
---|
755 | zEV(ji,jj) = - zt122V * r1_e2v(ji+1,jj) |
---|
756 | |
---|
757 | !----------------------------------------------------- |
---|
758 | ! -- Ocean-ice drag and acceleration LHS contribution |
---|
759 | !----------------------------------------------------- |
---|
760 | zBU(ji,jj) = zBU(ji,jj) + zCwU(ji,jj) + zmassU_t(ji,jj) |
---|
761 | zBV(ji,jj) = ZBV(ji,jj) + zCwV(ji,jj) + zmassV_t(ji,jj) |
---|
762 | |
---|
763 | END DO |
---|
764 | END DO |
---|
765 | |
---|
766 | CALL lbc_lnk( 'icedyn_rhg_vp', zAU , 'U', 1., zAV , 'V', 1. ) |
---|
767 | CALL lbc_lnk( 'icedyn_rhg_vp', zBU , 'U', 1., zBV , 'V', 1. ) |
---|
768 | CALL lbc_lnk( 'icedyn_rhg_vp', zCU , 'U', 1., zCV , 'V', 1. ) |
---|
769 | CALL lbc_lnk( 'icedyn_rhg_vp', zDU , 'U', 1., zDV , 'V', 1. ) |
---|
770 | CALL lbc_lnk( 'icedyn_rhg_vp', zEU , 'U', 1., zEV , 'V', 1. ) |
---|
771 | |
---|
772 | !!$ CALL iom_put( 'zAU' , zAU ) ! MV DEBUG |
---|
773 | !!$ CALL iom_put( 'zBU' , zBU ) ! MV DEBUG |
---|
774 | !!$ CALL iom_put( 'zCU' , zCU ) ! MV DEBUG |
---|
775 | !!$ CALL iom_put( 'zDU' , zDU ) ! MV DEBUG |
---|
776 | !!$ CALL iom_put( 'zEU' , zEU ) ! MV DEBUG |
---|
777 | !!$ CALL iom_put( 'zAV' , zAV ) ! MV DEBUG |
---|
778 | !!$ CALL iom_put( 'zBV' , zBV ) ! MV DEBUG |
---|
779 | !!$ CALL iom_put( 'zCV' , zCV ) ! MV DEBUG |
---|
780 | !!$ CALL iom_put( 'zDV' , zDV ) ! MV DEBUG |
---|
781 | !!$ CALL iom_put( 'zEV' , zEV ) ! MV DEBUG |
---|
782 | |
---|
783 | !------------------------------------------------------------------------------! |
---|
784 | ! |
---|
785 | ! --- Inner loop: solve linear system, check convergence |
---|
786 | ! |
---|
787 | !------------------------------------------------------------------------------! |
---|
788 | |
---|
789 | ! Inner loop solves the linear problem .. requires 1500 iterations |
---|
790 | ll_u_iterate = .TRUE. |
---|
791 | ll_v_iterate = .TRUE. |
---|
792 | |
---|
793 | DO i_inn = 1, nn_vp_ninn ! inner loop iterations |
---|
794 | |
---|
795 | IF( lwp ) WRITE(numout,*) ' inner loop 1 i_inn : ', i_inn |
---|
796 | |
---|
797 | !--- mitgcm computes initial value of residual here... |
---|
798 | |
---|
799 | jter = jter + 1 |
---|
800 | ! l_full_nf_update = jter == nn_nvp ! false: disable full North fold update (performances) for iter = 1 to nn_nevp-1 |
---|
801 | |
---|
802 | zu_b(:,:) = u_ice(:,:) ! velocity at previous sub-iterate |
---|
803 | zv_b(:,:) = v_ice(:,:) |
---|
804 | |
---|
805 | ! zAU(:,:) = 0._wp; zBU(:,:) = 0._wp; zCU(:,:) = 0._wp; zDU(:,:) = 0._wp; zEU(:,:) = 0._wp |
---|
806 | ! zAV(:,:) = 0._wp; zBV(:,:) = 0._wp; zCV(:,:) = 0._wp; zDV(:,:) = 0._wp; zEV(:,:) = 0._wp |
---|
807 | |
---|
808 | IF ( ll_u_iterate .OR. ll_v_iterate ) THEN |
---|
809 | |
---|
810 | ! ---------------------------- ! |
---|
811 | IF ( ll_u_iterate ) THEN ! --- Solve for u-velocity --- ! |
---|
812 | ! ---------------------------- ! |
---|
813 | |
---|
814 | ! What follows could be subroutinized... |
---|
815 | |
---|
816 | ! Thomas Algorithm for tridiagonal solver |
---|
817 | ! A*u(i-1,j)+B*u(i,j)+C*u(i+1,j) = F |
---|
818 | |
---|
819 | zFU(:,:) = 0._wp ; zFU_prime(:,:) = 0._wp ; zBU_prime(:,:) = 0._wp; zCU_prime(:,:) = 0._wp |
---|
820 | |
---|
821 | DO jn = 1, nn_zebra_vp ! "zebra" loop (! red-black-sor!!! ) |
---|
822 | |
---|
823 | ! OPT: could be even better optimized with a true red-black SOR |
---|
824 | |
---|
825 | IF ( jn == 1 ) THEN ; jj_min = 2 |
---|
826 | ELSE ; jj_min = 3 |
---|
827 | ENDIF |
---|
828 | |
---|
829 | IF ( lwp ) WRITE(numout,*) ' Into the U-zebra loop at step jn = ', jn, ', with jj_min = ', jj_min |
---|
830 | |
---|
831 | DO jj = jj_min, jpj - 1, nn_zebra_vp |
---|
832 | |
---|
833 | !------------------------ |
---|
834 | ! Independent term (zFU) |
---|
835 | !------------------------ |
---|
836 | DO ji = 2, jpi - 1 |
---|
837 | |
---|
838 | ! boundary condition substitution |
---|
839 | ! see Zhang and Hibler, 1997, Appendix B |
---|
840 | zAA3 = 0._wp |
---|
841 | IF ( ji == 2 ) zAA3 = zAA3 - zAU(ji,jj) * u_ice(ji-1,jj) |
---|
842 | IF ( ji == jpi - 1 ) zAA3 = zAA3 - zCU(ji,jj) * u_ice(ji+1,jj) |
---|
843 | |
---|
844 | ! right hand side |
---|
845 | zFU(ji,jj) = ( zrhsu(ji,jj) & ! right-hand side terms |
---|
846 | & + zAA3 & ! boundary condition translation |
---|
847 | & + zDU(ji,jj) * u_ice(ji,jj-1) & ! internal force, j-1 |
---|
848 | & + zEU(ji,jj) * u_ice(ji,jj+1) ) * umask(ji,jj,1) ! internal force, j+1 |
---|
849 | |
---|
850 | END DO |
---|
851 | |
---|
852 | END DO |
---|
853 | |
---|
854 | CALL lbc_lnk( 'icedyn_rhg_vp', zFU, 'U', 1. ) |
---|
855 | |
---|
856 | !--------------- |
---|
857 | ! Forward sweep |
---|
858 | !--------------- |
---|
859 | DO jj = jj_min, jpj - 1, nn_zebra_vp |
---|
860 | |
---|
861 | DO ji = 3, jpi - 1 |
---|
862 | |
---|
863 | zfac = SIGN( 1._wp , zBU(ji-1,jj) ) * MAX( 0._wp , SIGN( 1._wp , ABS( zBU(ji-1,jj) ) - epsi20 ) ) |
---|
864 | zw = zfac * zAU(ji,jj) / MAX ( ABS( zBU(ji-1,jj) ) , epsi20 ) |
---|
865 | zBU_prime(ji,jj) = zBU(ji,jj) - zw * zCU(ji-1,jj) |
---|
866 | zFU_prime(ji,jj) = zFU(ji,jj) - zw * zFU(ji-1,jj) |
---|
867 | |
---|
868 | END DO |
---|
869 | |
---|
870 | END DO |
---|
871 | |
---|
872 | CALL lbc_lnk( 'icedyn_rhg_vp', zFU_prime, 'U', 1., zBU_prime, 'U', 1. ) |
---|
873 | |
---|
874 | !----------------------------- |
---|
875 | ! Backward sweep & relaxation |
---|
876 | !----------------------------- |
---|
877 | |
---|
878 | DO jj = jj_min, jpj - 1, nn_zebra_vp |
---|
879 | |
---|
880 | ! --- Backward sweep |
---|
881 | ! last row |
---|
882 | zfac = SIGN( 1._wp , zBU_prime(jpi-1,jj) ) * MAX( 0._wp , SIGN( 1._wp , ABS( zBU_prime(jpi-1,jj) ) - epsi20 ) ) |
---|
883 | u_ice(jpi-1,jj) = zfac * zFU_prime(jpi-1,jj) / MAX( ABS ( zBU_prime(jpi-1,jj) ) , epsi20 ) & |
---|
884 | & * umask(jpi-1,jj,1) |
---|
885 | DO ji = jpi-2 , 2, -1 ! all other rows ! ---> original backward loop |
---|
886 | zfac = SIGN( 1._wp , zBU_prime(ji,jj) ) * MAX( 0._wp , SIGN( 1._wp , ABS( zBU_prime(ji,jj) ) - epsi20 ) ) |
---|
887 | u_ice(ji,jj) = zfac * ( zFU_prime(ji,jj) - zCU(ji,jj) * u_ice(ji+1,jj) ) * umask(ji,jj,1) & |
---|
888 | & / MAX ( ABS ( zBU_prime(ji,jj) ) , epsi20 ) |
---|
889 | END DO |
---|
890 | |
---|
891 | !--- Relaxation |
---|
892 | ! and velocity masking for little-ice and no-ice cases |
---|
893 | DO ji = 2, jpi - 1 |
---|
894 | |
---|
895 | u_ice(ji,jj) = zu_b(ji,jj) + zrelaxu_vp * ( u_ice(ji,jj) - zu_b(ji,jj) ) ! relaxation |
---|
896 | |
---|
897 | u_ice(ji,jj) = zmsk00x(ji,jj) & ! masking |
---|
898 | & * ( zmsk01x(ji,jj) * u_ice(ji,jj) & |
---|
899 | & + ( 1._wp - zmsk01x(ji,jj) ) * u_oce(ji,jj) * 0.01_wp ) * umask(ji,jj,1) |
---|
900 | |
---|
901 | END DO |
---|
902 | |
---|
903 | END DO ! jj |
---|
904 | |
---|
905 | END DO ! zebra loop |
---|
906 | |
---|
907 | ENDIF ! ll_u_iterate |
---|
908 | |
---|
909 | ! ! ---------------------------- ! |
---|
910 | IF ( ll_v_iterate ) THEN ! --- Solve for V-velocity --- ! |
---|
911 | ! ! ---------------------------- ! |
---|
912 | |
---|
913 | ! MV OPT: what follows could be subroutinized... |
---|
914 | ! Thomas Algorithm for tridiagonal solver |
---|
915 | ! A*v(i,j-1)+B*v(i,j)+C*v(i,j+1) = F |
---|
916 | ! It is intentional to have a ji then jj loop for V-velocity |
---|
917 | !!! ZH97 explain it is critical for convergence speed |
---|
918 | |
---|
919 | zFV(:,:) = 0._wp ; zFV_prime(:,:) = 0._wp ; zBV_prime(:,:) = 0._wp; zCV_prime(:,:) = 0._wp |
---|
920 | |
---|
921 | DO jn = 1, nn_zebra_vp ! "zebra" loop |
---|
922 | |
---|
923 | IF ( jn == 1 ) THEN ; ji_min = 2 |
---|
924 | ELSE ; ji_min = 3 |
---|
925 | ENDIF |
---|
926 | |
---|
927 | IF ( lwp ) WRITE(numout,*) ' Into the V-zebra loop at step jn = ', jn, ', with ji_min = ', ji_min |
---|
928 | |
---|
929 | DO ji = ji_min, jpi - 1, nn_zebra_vp |
---|
930 | |
---|
931 | !------------------------ |
---|
932 | ! Independent term (zFV) |
---|
933 | !------------------------ |
---|
934 | DO jj = 2, jpj - 1 |
---|
935 | |
---|
936 | ! boundary condition substitution (check it is correctly applied !!!) |
---|
937 | ! see Zhang and Hibler, 1997, Appendix B |
---|
938 | zAA3 = 0._wp |
---|
939 | IF ( jj == 2 ) zAA3 = zAA3 - zAV(ji,jj) * v_ice(ji,jj-1) |
---|
940 | IF ( jj == jpj - 1 ) zAA3 = zAA3 - zCV(ji,jj) * v_ice(ji,jj+1) |
---|
941 | |
---|
942 | ! right hand side |
---|
943 | zFV(ji,jj) = ( zrhsv(ji,jj) & ! right-hand side terms |
---|
944 | & + zAA3 & ! boundary condition translation |
---|
945 | & + zDV(ji,jj) * v_ice(ji-1,jj) & ! internal force, j-1 |
---|
946 | & + zEV(ji,jj) * v_ice(ji+1,jj) ) * vmask(ji,jj,1) ! internal force, j+1 |
---|
947 | |
---|
948 | END DO |
---|
949 | |
---|
950 | END DO |
---|
951 | |
---|
952 | CALL lbc_lnk( 'icedyn_rhg_vp', zFV, 'V', 1.) |
---|
953 | |
---|
954 | !--------------- |
---|
955 | ! Forward sweep |
---|
956 | !--------------- |
---|
957 | DO ji = ji_min, jpi - 1, nn_zebra_vp |
---|
958 | |
---|
959 | DO jj = 3, jpj - 1 |
---|
960 | |
---|
961 | zfac = SIGN( 1._wp , zBV(ji,jj-1) ) * MAX( 0._wp , SIGN( 1._wp , ABS( zBV(ji,jj-1) ) - epsi20 ) ) |
---|
962 | zw = zfac * zAV(ji,jj) / MAX ( ABS( zBV(ji,jj-1) ) , epsi20 ) |
---|
963 | zBV_prime(ji,jj) = zBV(ji,jj) - zw * zCV(ji,jj-1) |
---|
964 | zFV_prime(ji,jj) = zFV(ji,jj) - zw * zFV(ji,jj-1) |
---|
965 | |
---|
966 | END DO |
---|
967 | |
---|
968 | END DO |
---|
969 | |
---|
970 | CALL lbc_lnk( 'icedyn_rhg_vp', zFV_prime, 'V', 1., zBV_prime, 'V', 1. ) |
---|
971 | |
---|
972 | !----------------------------- |
---|
973 | ! Backward sweep & relaxation |
---|
974 | !----------------------------- |
---|
975 | DO ji = ji_min, jpi - 1, nn_zebra_vp |
---|
976 | |
---|
977 | ! --- Backward sweep |
---|
978 | ! last row |
---|
979 | zfac = SIGN( 1._wp , zBV_prime(ji,jpj-1) ) * MAX( 0._wp , SIGN( 1._wp , ABS( zBV_prime(ji,jpj-1) ) - epsi20 ) ) |
---|
980 | v_ice(ji,jpj-1) = zfac * zFV_prime(ji,jpj-1) / MAX ( ABS(zBV_prime(ji,jpj-1) ) , epsi20 ) & |
---|
981 | & * vmask(ji,jpj-1,1) ! last row |
---|
982 | |
---|
983 | ! other rows |
---|
984 | DO jj = jpj-2, 2, -1 ! original back loop |
---|
985 | zfac = SIGN( 1._wp , zBV_prime(ji,jj) ) * MAX( 0._wp , SIGN( 1._wp , ABS( zBV_prime(ji,jj) ) - epsi20 ) ) |
---|
986 | v_ice(ji,jj) = zfac * ( zFV_prime(ji,jj) - zCV(ji,jj) * v_ice(ji,jj+1) ) * vmask(ji,jj,1) & |
---|
987 | & / MAX ( ABS( zBV_prime(ji,jj) ) , epsi20 ) |
---|
988 | END DO |
---|
989 | |
---|
990 | ! --- Relaxation & masking (should it be now or later) |
---|
991 | DO jj = 2, jpj - 1 |
---|
992 | |
---|
993 | v_ice(ji,jj) = zv_b(ji,jj) + zrelaxv_vp * ( v_ice(ji,jj) - zv_b(ji,jj) ) ! relaxation |
---|
994 | |
---|
995 | v_ice(ji,jj) = zmsk00y(ji,jj) & ! masking |
---|
996 | & * ( zmsk01y(ji,jj) * v_ice(ji,jj) & |
---|
997 | & + ( 1._wp - zmsk01y(ji,jj) ) * v_oce(ji,jj) * 0.01_wp ) * vmask(ji,jj,1) |
---|
998 | |
---|
999 | END DO ! jj |
---|
1000 | |
---|
1001 | END DO ! ji |
---|
1002 | |
---|
1003 | END DO ! zebra loop |
---|
1004 | |
---|
1005 | ENDIF ! ll_v_iterate |
---|
1006 | |
---|
1007 | CALL lbc_lnk( 'icedyn_rhg_vp', u_ice, 'U', -1., v_ice, 'V', -1. ) |
---|
1008 | |
---|
1009 | !-------------------------------------------------------------------------------------- |
---|
1010 | ! -- Check convergence based on maximum velocity difference, continue or stop the loop |
---|
1011 | !-------------------------------------------------------------------------------------- |
---|
1012 | |
---|
1013 | !------ |
---|
1014 | ! on U |
---|
1015 | !------ |
---|
1016 | ! MV OPT: if the number of iterations to convergence is really variable, and keep the convergence check |
---|
1017 | ! then we must optimize the use of the mpp_max, which is prohibitive |
---|
1018 | zuerr_max = 0._wp |
---|
1019 | |
---|
1020 | IF ( ll_u_iterate .AND. MOD ( i_inn, nn_vp_chkcvg ) == 0 ) THEN |
---|
1021 | |
---|
1022 | ! - Maximum U-velocity difference |
---|
1023 | zuerr(:,:) = 0._wp |
---|
1024 | DO jj = 2, jpj - 1 |
---|
1025 | DO ji = 2, jpi - 1 |
---|
1026 | zuerr(ji,jj) = ABS ( ( u_ice(ji,jj) - zu_b(ji,jj) ) ) * umask(ji,jj,1) |
---|
1027 | END DO |
---|
1028 | END DO |
---|
1029 | zuerr_max = MAXVAL( zuerr ) |
---|
1030 | CALL mpp_max( 'icedyn_rhg_evp', zuerr_max ) ! max over the global domain - damned! |
---|
1031 | |
---|
1032 | ! - Stop if error is too large ("safeguard against bad forcing" of original Zhang routine) |
---|
1033 | IF ( i_inn > 1 .AND. zuerr_max > zuerr_max_vp ) THEN |
---|
1034 | IF ( lwp ) WRITE(numout,*) " VP rheology error was too large : ", zuerr_max, " in outer U-iteration ", i_out, " after ", i_inn, " iterations, we stopped " |
---|
1035 | ll_u_iterate = .FALSE. |
---|
1036 | ENDIF |
---|
1037 | |
---|
1038 | ! - Stop if error small enough |
---|
1039 | IF ( zuerr_max < zuerr_min_vp ) THEN |
---|
1040 | IF ( lwp ) WRITE(numout,*) " VP rheology nicely done in outer U-iteration ", i_out, " after ", i_inn, " iterations, finished! " |
---|
1041 | ll_u_iterate = .FALSE. |
---|
1042 | ENDIF |
---|
1043 | |
---|
1044 | ENDIF ! ll_u_iterate |
---|
1045 | |
---|
1046 | !------ |
---|
1047 | ! on V |
---|
1048 | !------ |
---|
1049 | zverr_max = 0._wp |
---|
1050 | |
---|
1051 | IF ( ll_v_iterate .AND. MOD ( i_inn, nn_vp_chkcvg ) == 0 ) THEN |
---|
1052 | |
---|
1053 | ! - Maximum V-velocity difference |
---|
1054 | zverr(:,:) = 0._wp |
---|
1055 | DO jj = 2, jpj - 1 |
---|
1056 | DO ji = 2, jpi - 1 |
---|
1057 | zverr(ji,jj) = ABS ( ( v_ice(ji,jj) - zv_b(ji,jj) ) ) * vmask(ji,jj,1) |
---|
1058 | END DO |
---|
1059 | END DO |
---|
1060 | |
---|
1061 | zverr_max = MAXVAL( zverr ) |
---|
1062 | CALL mpp_max( 'icedyn_rhg_evp', zverr_max ) ! max over the global domain - damned! |
---|
1063 | |
---|
1064 | ! - Stop if error is too large ("safeguard against bad forcing" of original Zhang routine) |
---|
1065 | IF ( i_inn > 1 .AND. zverr_max > zuerr_max_vp ) THEN |
---|
1066 | IF ( lwp ) WRITE(numout,*) " VP rheology error was too large : ", zverr_max, " in outer V-iteration ", i_out, " after ", i_inn, " iterations, we stopped " |
---|
1067 | ll_v_iterate = .FALSE. |
---|
1068 | ENDIF |
---|
1069 | |
---|
1070 | ! - Stop if error small enough |
---|
1071 | IF ( zverr_max < zuerr_min_vp ) THEN |
---|
1072 | IF ( lwp ) WRITE(numout,*) " VP rheology nicely done in outer V-iteration ", i_out, " after ", i_inn, " iterations, finished! " |
---|
1073 | ll_v_iterate = .FALSE. |
---|
1074 | ENDIF |
---|
1075 | |
---|
1076 | ENDIF ! ll_v_iterate |
---|
1077 | |
---|
1078 | ENDIF ! --- end ll_u_iterate or ll_v_iterate |
---|
1079 | |
---|
1080 | !--------------------------------------------------------------------------------------- |
---|
1081 | ! |
---|
1082 | ! --- Calculate extra convergence diagnostics and save them |
---|
1083 | ! |
---|
1084 | !--------------------------------------------------------------------------------------- |
---|
1085 | |
---|
1086 | IF( nn_rhg_chkcvg/=0 .AND. MOD ( i_inn - 1, nn_vp_chkcvg ) == 0 ) CALL rhg_cvg_vp( kt, jter, nn_nvp, u_ice, v_ice, zmt, zuerr_max, zverr_max, zglob_area, & |
---|
1087 | & zrhsu, zAU, zBU, zCU, zDU, zEU, zrhsv, zAV, zBV, zCV, zDV, zEV ) |
---|
1088 | |
---|
1089 | IF ( lwp ) WRITE(numout,*) ' Done convergence tests ' |
---|
1090 | |
---|
1091 | END DO ! i_inn, end of inner loop |
---|
1092 | |
---|
1093 | END DO ! End of outer loop (i_out) ============================================================================================= |
---|
1094 | |
---|
1095 | IF ( lwp ) WRITE(numout,*) ' We are out of outer loop ' |
---|
1096 | |
---|
1097 | CALL lbc_lnk( 'icedyn_rhg_vp', zFU , 'U', 1., zFV , 'V', 1. ) |
---|
1098 | CALL lbc_lnk( 'icedyn_rhg_vp', zBU_prime , 'U', 1., zBV_prime , 'V', 1. ) |
---|
1099 | CALL lbc_lnk( 'icedyn_rhg_vp', zFU_prime , 'U', 1., zFV_prime , 'V', 1. ) |
---|
1100 | CALL lbc_lnk( 'icedyn_rhg_vp', zCU_prime , 'U', 1., zCV_prime , 'V', 1. ) |
---|
1101 | |
---|
1102 | !!$ CALL iom_put( 'zFU' , zFU ) ! MV DEBUG |
---|
1103 | !!$ CALL iom_put( 'zBU_prime' , zBU_prime ) ! MV DEBUG |
---|
1104 | !!$ CALL iom_put( 'zCU_prime' , zCU_prime ) ! MV DEBUG |
---|
1105 | !!$ CALL iom_put( 'zFU_prime' , zFU_prime ) ! MV DEBUG |
---|
1106 | !!$ |
---|
1107 | !!$ CALL iom_put( 'zFV' , zFV ) ! MV DEBUG |
---|
1108 | !!$ CALL iom_put( 'zBV_prime' , zBV_prime ) ! MV DEBUG |
---|
1109 | !!$ CALL iom_put( 'zCV_prime' , zCV_prime ) ! MV DEBUG |
---|
1110 | !!$ CALL iom_put( 'zFV_prime' , zFV_prime ) ! MV DEBUG |
---|
1111 | |
---|
1112 | CALL lbc_lnk( 'icedyn_rhg_vp', u_ice, 'U', -1., v_ice, 'V', -1. ) |
---|
1113 | |
---|
1114 | !!$ IF ( lwp ) WRITE(numout,*) ' We are about to output uice_dbg ' |
---|
1115 | !!$ IF( iom_use('uice_dbg' ) ) CALL iom_put( 'uice_dbg' , u_ice ) ! ice velocity u after solver |
---|
1116 | !!$ IF( iom_use('vice_dbg' ) ) CALL iom_put( 'vice_dbg' , v_ice ) ! ice velocity v after solver |
---|
1117 | |
---|
1118 | !------------------------------------------------------------------------------! |
---|
1119 | ! |
---|
1120 | ! --- Convergence diagnostics |
---|
1121 | ! |
---|
1122 | !------------------------------------------------------------------------------! |
---|
1123 | |
---|
1124 | IF( nn_rhg_chkcvg /= 0 ) THEN |
---|
1125 | |
---|
1126 | IF( iom_use('uice_cvg') ) THEN |
---|
1127 | CALL iom_put( 'uice_cvg', MAX( ABS( u_ice(:,:) - zu_b(:,:) ) * umask(:,:,1) , & ! ice velocity difference at last iteration |
---|
1128 | & ABS( v_ice(:,:) - zv_b(:,:) ) * vmask(:,:,1) ) * zmsk15(:,:) ) |
---|
1129 | ENDIF |
---|
1130 | |
---|
1131 | ENDIF |
---|
1132 | |
---|
1133 | !!$ ! MV DEBUG test - replace ice velocity by ocean current to give the model the means to go ahead |
---|
1134 | !!$ DO jj = 2, jpj - 1 |
---|
1135 | !!$ DO ji = 2, jpi - 1 |
---|
1136 | !!$ |
---|
1137 | !!$ u_ice(ji,jj) = zmsk00x(ji,jj) & |
---|
1138 | !!$ & * ( zmsk01x(ji,jj) * u_oce(ji,jj) * 0.01_wp & |
---|
1139 | !!$ + ( 1._wp - zmsk01x(ji,jj) ) * u_oce(ji,jj) * 0.01_wp ) |
---|
1140 | !!$ |
---|
1141 | !!$ v_ice(ji,jj) = zmsk00y(ji,jj) & |
---|
1142 | !!$ & * ( zmsk01y(ji,jj) * v_oce(ji,jj) * 0.01_wp & |
---|
1143 | !!$ + ( 1._wp - zmsk01y(ji,jj) ) * v_oce(ji,jj) * 0.01_wp ) |
---|
1144 | !!$ |
---|
1145 | !!$ END DO |
---|
1146 | !!$ END DO |
---|
1147 | !!$ |
---|
1148 | !!$ CALL lbc_lnk( 'icedyn_rhg_vp', u_ice, 'U', -1., v_ice, 'V', -1. ) |
---|
1149 | !!$ |
---|
1150 | !!$ IF ( lwp ) WRITE(numout,*) ' Velocity replaced ' |
---|
1151 | |
---|
1152 | ! END DEBUG |
---|
1153 | |
---|
1154 | !------------------------------------------------------------------------------! |
---|
1155 | ! |
---|
1156 | ! --- Recompute delta, shear and div (inputs for mechanical redistribution) |
---|
1157 | ! |
---|
1158 | !------------------------------------------------------------------------------! |
---|
1159 | ! |
---|
1160 | ! MV OPT: subroutinize ? |
---|
1161 | |
---|
1162 | DO jj = 1, jpj - 1 |
---|
1163 | DO ji = 1, jpi - 1 |
---|
1164 | |
---|
1165 | ! shear at F points |
---|
1166 | 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) & |
---|
1167 | & + ( v_ice(ji+1,jj) * r1_e2v(ji+1,jj) - v_ice(ji,jj) * r1_e2v(ji,jj) ) * e2f(ji,jj) * e2f(ji,jj) & |
---|
1168 | & ) * r1_e1e2f(ji,jj) * fimask(ji,jj) |
---|
1169 | |
---|
1170 | END DO |
---|
1171 | END DO |
---|
1172 | |
---|
1173 | DO jj = 2, jpj - 1 |
---|
1174 | DO ji = 2, jpi - 1 ! |
---|
1175 | |
---|
1176 | ! tension**2 at T points |
---|
1177 | 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) & |
---|
1178 | & - ( v_ice(ji,jj) * r1_e1v(ji,jj) - v_ice(ji,jj-1) * r1_e1v(ji,jj-1) ) * e1t(ji,jj) * e1t(ji,jj) & |
---|
1179 | & ) * r1_e1e2t(ji,jj) |
---|
1180 | zdt2 = zdt * zdt |
---|
1181 | |
---|
1182 | zten_i(ji,jj) = zdt |
---|
1183 | |
---|
1184 | ! shear**2 at T points (doc eq. A16) |
---|
1185 | zds2 = ( zds(ji,jj ) * zds(ji,jj ) * e1e2f(ji,jj ) + zds(ji-1,jj ) * zds(ji-1,jj ) * e1e2f(ji-1,jj ) & |
---|
1186 | & + 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) & |
---|
1187 | & ) * 0.25_wp * r1_e1e2t(ji,jj) |
---|
1188 | |
---|
1189 | ! shear at T points |
---|
1190 | pshear_i(ji,jj) = SQRT( zdt2 + zds2 ) |
---|
1191 | |
---|
1192 | ! divergence at T points |
---|
1193 | pdivu_i(ji,jj) = ( e2u(ji,jj) * u_ice(ji,jj) - e2u(ji-1,jj) * u_ice(ji-1,jj) & |
---|
1194 | & + e1v(ji,jj) * v_ice(ji,jj) - e1v(ji,jj-1) * v_ice(ji,jj-1) & |
---|
1195 | & ) * r1_e1e2t(ji,jj) |
---|
1196 | |
---|
1197 | ! delta at T points |
---|
1198 | zdelta = SQRT( pdivu_i(ji,jj) * pdivu_i(ji,jj) + ( zdt2 + zds2 ) * z1_ecc2 ) |
---|
1199 | rswitch = 1._wp - MAX( 0._wp, SIGN( 1._wp, -zdelta ) ) ! 0 if delta=0 |
---|
1200 | |
---|
1201 | !pdelta_i(ji,jj) = zdelta + rn_creepl * rswitch |
---|
1202 | pdelta_i(ji,jj) = zdelta + rn_creepl |
---|
1203 | |
---|
1204 | END DO |
---|
1205 | END DO |
---|
1206 | |
---|
1207 | IF ( lwp ) WRITE(numout,*) ' Deformation recalculated ' |
---|
1208 | |
---|
1209 | CALL lbc_lnk( 'icedyn_rhg_vp', pshear_i, 'T', 1., pdivu_i, 'T', 1., pdelta_i, 'T', 1. ) |
---|
1210 | |
---|
1211 | !------------------------------------------------------------------------------! |
---|
1212 | ! |
---|
1213 | ! --- Diagnostics |
---|
1214 | ! |
---|
1215 | !------------------------------------------------------------------------------! |
---|
1216 | ! |
---|
1217 | ! MV OPT: subroutinize ? |
---|
1218 | ! |
---|
1219 | !---------------------------------- |
---|
1220 | ! --- Recompute stresses if needed |
---|
1221 | !---------------------------------- |
---|
1222 | ! |
---|
1223 | ! ---- Sea ice stresses at T-points |
---|
1224 | IF ( iom_use('normstr') .OR. iom_use('sheastr') .OR. iom_use('intstrx') .OR. iom_use('intstry') ) THEN |
---|
1225 | |
---|
1226 | DO jj = 2, jpj - 1 |
---|
1227 | DO ji = 2, jpi - 1 |
---|
1228 | zp_deltastar_t(ji,jj) = strength(ji,jj) / pdelta_i(ji,jj) |
---|
1229 | zfac = zp_deltastar_t(ji,jj) |
---|
1230 | zs1(ji,jj) = zfac * ( pdivu_i(ji,jj) - pdelta_i(ji,jj) ) |
---|
1231 | zs2(ji,jj) = zfac * z1_ecc2 * zten_i(ji,jj) |
---|
1232 | zs12(ji,jj) = zfac * z1_ecc2 * pshear_i(ji,jj) |
---|
1233 | END DO |
---|
1234 | END DO |
---|
1235 | |
---|
1236 | CALL lbc_lnk( 'icedyn_rhg_vp', zs1, 'T', 1., zs2, 'T', 1., zs12, 'T', 1. ) |
---|
1237 | |
---|
1238 | ENDIF |
---|
1239 | |
---|
1240 | ! ---- s12 at F-points |
---|
1241 | IF ( iom_use('intstrx') .OR. iom_use('intstry') ) THEN |
---|
1242 | |
---|
1243 | DO jj = 1, jpj - 1 |
---|
1244 | DO ji = 1, jpi - 1 |
---|
1245 | |
---|
1246 | ! P/delta* at F points |
---|
1247 | zp_deltastar_f = 0.25_wp * ( zp_deltastar_t(ji,jj) + zp_deltastar_t(ji+1,jj) + zp_deltastar_t(ji,jj+1) + zp_deltastar_t(ji+1,jj+1) ) |
---|
1248 | |
---|
1249 | ! s12 at F-points |
---|
1250 | zs12f(ji,jj) = zp_deltastar_f * z1_ecc2 * zds(ji,jj) |
---|
1251 | |
---|
1252 | END DO |
---|
1253 | END DO |
---|
1254 | |
---|
1255 | CALL lbc_lnk( 'icedyn_rhg_vp', zs12f, 'F', 1. ) |
---|
1256 | |
---|
1257 | ENDIF |
---|
1258 | |
---|
1259 | IF ( lwp ) WRITE(numout,*) ' zs12f recalculated ' |
---|
1260 | |
---|
1261 | ! |
---|
1262 | !----------------------- |
---|
1263 | ! --- Store diagnostics |
---|
1264 | !----------------------- |
---|
1265 | ! |
---|
1266 | ! --- Ice-ocean, ice-atm. & ice-ocean bottom (landfast) stresses --- ! |
---|
1267 | IF( iom_use('utau_oi') .OR. iom_use('vtau_oi') .OR. iom_use('utau_ai') .OR. iom_use('vtau_ai') .OR. & |
---|
1268 | & iom_use('utau_bi') .OR. iom_use('vtau_bi') ) THEN |
---|
1269 | |
---|
1270 | ALLOCATE( ztaux_oi(jpi,jpj) , ztauy_oi(jpi,jpj) ) |
---|
1271 | |
---|
1272 | !--- Recalculate oceanic stress at last inner iteration |
---|
1273 | DO jj = 2, jpj - 1 |
---|
1274 | DO ji = 2, jpi - 1 |
---|
1275 | |
---|
1276 | !--- ice u-velocity @V points, v-velocity @U points (for non-linear drag computation) |
---|
1277 | zu_cV = 0.25_wp * ( u_ice(ji,jj) + u_ice(ji-1,jj) + u_ice(ji,jj+1) + u_ice(ji-1,jj+1) ) * vmask(ji,jj,1) |
---|
1278 | zv_cU = 0.25_wp * ( v_ice(ji,jj) + v_ice(ji,jj-1) + v_ice(ji+1,jj) + v_ice(ji+1,jj-1) ) * umask(ji,jj,1) |
---|
1279 | |
---|
1280 | !--- non-linear drag coefficients (need to be updated at each outer loop, see Lemieux and Tremblay JGR09, p.3, beginning of Section 3) |
---|
1281 | zCwU(ji,jj) = za_iU(ji,jj) * zrhoco * SQRT( ( u_ice(ji,jj) - u_oce (ji,jj) ) * ( u_ice(ji,jj) - u_oce (ji,jj) ) & |
---|
1282 | & + ( zv_cU - v_oceU(ji,jj) ) * ( zv_cU - v_oceU(ji,jj) ) ) |
---|
1283 | zCwV(ji,jj) = za_iV(ji,jj) * zrhoco * SQRT( ( v_ice(ji,jj) - v_oce (ji,jj) ) * ( v_ice(ji,jj) - v_oce (ji,jj) ) & |
---|
1284 | & + ( zu_cV - u_oceV(ji,jj) ) * ( zu_cV - u_oceV(ji,jj) ) ) |
---|
1285 | |
---|
1286 | !--- Ocean-ice stress |
---|
1287 | ztaux_oi(ji,jj) = zCwU(ji,jj) * ( u_oce(ji,jj) - u_ice(ji,jj) ) |
---|
1288 | ztauy_oi(ji,jj) = zCwV(ji,jj) * ( v_oce(ji,jj) - v_ice(ji,jj) ) |
---|
1289 | |
---|
1290 | END DO |
---|
1291 | END DO |
---|
1292 | |
---|
1293 | ! |
---|
1294 | CALL lbc_lnk( 'icedyn_rhg_vp', ztaux_oi, 'U', -1., ztauy_oi, 'V', -1., ztaux_ai, 'U', -1., ztauy_ai, 'V', -1. ) !, & |
---|
1295 | ! & ztaux_bi, 'U', -1., ztauy_bi, 'V', -1. ) |
---|
1296 | ! |
---|
1297 | CALL iom_put( 'utau_oi' , ztaux_oi * zmsk00 ) |
---|
1298 | CALL iom_put( 'vtau_oi' , ztauy_oi * zmsk00 ) |
---|
1299 | CALL iom_put( 'utau_ai' , ztaux_ai * zmsk00 ) |
---|
1300 | CALL iom_put( 'vtau_ai' , ztauy_ai * zmsk00 ) |
---|
1301 | ! CALL iom_put( 'utau_bi' , ztaux_bi * zmsk00 ) |
---|
1302 | ! CALL iom_put( 'vtau_bi' , ztauy_bi * zmsk00 ) |
---|
1303 | |
---|
1304 | DEALLOCATE( ztaux_oi , ztauy_oi ) |
---|
1305 | |
---|
1306 | ENDIF |
---|
1307 | |
---|
1308 | ! --- Divergence, shear and strength --- ! |
---|
1309 | IF( iom_use('icediv') ) CALL iom_put( 'icediv' , pdivu_i * zmsk00 ) ! divergence |
---|
1310 | IF( iom_use('iceshe') ) CALL iom_put( 'iceshe' , pshear_i * zmsk00 ) ! shear |
---|
1311 | IF( iom_use('icedlt') ) CALL iom_put( 'icedlt' , pdelta_i * zmsk00 ) ! delta |
---|
1312 | IF( iom_use('icestr') ) CALL iom_put( 'icestr' , strength * zmsk00 ) ! strength |
---|
1313 | |
---|
1314 | IF ( lwp ) WRITE(numout,*) 'Some terms recalculated ' |
---|
1315 | |
---|
1316 | ! --- Stress tensor invariants (SIMIP diags) --- ! |
---|
1317 | IF( iom_use('normstr') .OR. iom_use('sheastr') ) THEN |
---|
1318 | ! |
---|
1319 | ! Stress tensor invariants (normal and shear stress N/m) - SIMIP diags. |
---|
1320 | ! Definitions following Coon (1974) and Feltham (2008) |
---|
1321 | ! |
---|
1322 | ! sigma1, sigma2, sigma12 are useful (Hunke and Dukowicz MWR 2002, Bouillon et al., OM2013) |
---|
1323 | ! however these are NOT stress tensor components, neither stress invariants, nor stress principal components |
---|
1324 | ! |
---|
1325 | ALLOCATE( zsig_I(jpi,jpj) , zsig_II(jpi,jpj) ) |
---|
1326 | ! |
---|
1327 | DO jj = 2, jpj - 1 |
---|
1328 | DO ji = 2, jpi - 1 |
---|
1329 | ! Stress invariants |
---|
1330 | zsig_I(ji,jj) = zs1(ji,jj) * 0.5_wp ! 1st invariant, aka average normal stress aka negative pressure |
---|
1331 | zsig_II(ji,jj) = SQRT ( zs2(ji,jj) * zs2(ji,jj) * 0.25_wp + zs12(ji,jj) ) ! 2nd invariant, aka maximum shear stress |
---|
1332 | END DO |
---|
1333 | END DO |
---|
1334 | |
---|
1335 | CALL lbc_lnk( 'icedyn_rhg_vp', zsig_I, 'T', 1., zsig_II, 'T', 1.) |
---|
1336 | |
---|
1337 | IF( iom_use('normstr') ) CALL iom_put( 'normstr' , zsig_I(:,:) * zmsk00(:,:) ) ! Normal stress |
---|
1338 | IF( iom_use('sheastr') ) CALL iom_put( 'sheastr' , zsig_II(:,:) * zmsk00(:,:) ) ! Maximum shear stress |
---|
1339 | |
---|
1340 | DEALLOCATE ( zsig_I, zsig_II ) |
---|
1341 | |
---|
1342 | ENDIF |
---|
1343 | |
---|
1344 | IF ( lwp ) WRITE(numout,*) 'SIMIP work done' |
---|
1345 | |
---|
1346 | ! --- Normalized stress tensor principal components --- ! |
---|
1347 | ! These are used to plot the normalized yield curve (Lemieux & Dupont, GMD 2020) |
---|
1348 | ! To plot the yield curve and evaluate physical convergence, they have two recommendations |
---|
1349 | ! Recommendation 1 : Use ice strength, not replacement pressure |
---|
1350 | ! Recommendation 2 : Need to use deformations at PREVIOUS iterate for viscosities (see p. 1765) |
---|
1351 | ! R2 means we need to recompute stresses |
---|
1352 | |
---|
1353 | IF( iom_use('sig1_pnorm') .OR. iom_use('sig2_pnorm') ) THEN |
---|
1354 | ! |
---|
1355 | ALLOCATE( zsig1_p(jpi,jpj) , zsig2_p(jpi,jpj) , zsig_I(jpi,jpj) , zsig_II(jpi,jpj) ) |
---|
1356 | ! |
---|
1357 | DO jj = 2, jpj - 1 |
---|
1358 | DO ji = 2, jpi - 1 |
---|
1359 | ! Ice stresses computed with **viscosities** (delta, p/delta) at **previous** iterates |
---|
1360 | ! and **deformations** at current iterates |
---|
1361 | ! following Lemieux & Dupont (2020) |
---|
1362 | zfac = zp_deltastar_t(ji,jj) |
---|
1363 | zsig1 = zfac * ( pdivu_i(ji,jj) - zdeltastar_t(ji,jj) ) |
---|
1364 | !!$ zsig1 = 0._wp !!! FUCKING DEBUG TEST !!! |
---|
1365 | zsig2 = zfac * z1_ecc2 * zten_i(ji,jj) |
---|
1366 | zsig12 = zfac * z1_ecc2 * pshear_i(ji,jj) |
---|
1367 | |
---|
1368 | ! Stress invariants (sigma_I, sigma_II, Coon 1974, Feltham 2008), T-point |
---|
1369 | zsig_I(ji,jj) = zsig1 * 0.5_wp ! 1st invariant |
---|
1370 | zsig_II(ji,jj) = SQRT ( zsig2 * zsig2 * 0.25_wp + zsig12 ) ! 2nd invariant |
---|
1371 | |
---|
1372 | ! Normalized principal stresses (used to display the ellipse) |
---|
1373 | z1_strength = 1._wp / MAX ( 1._wp , strength(ji,jj) ) |
---|
1374 | zsig1_p(ji,jj) = ( zsig_I(ji,jj) + zsig_II(ji,jj) ) * z1_strength |
---|
1375 | zsig2_p(ji,jj) = ( zsig_I(ji,jj) - zsig_II(ji,jj) ) * z1_strength |
---|
1376 | END DO |
---|
1377 | END DO |
---|
1378 | IF ( lwp ) WRITE(numout,*) 'Some shitty stress work done' |
---|
1379 | ! |
---|
1380 | CALL lbc_lnk( 'icedyn_rhg_vp', zsig1_p, 'T', 1., zsig2_p, 'T', 1.) |
---|
1381 | ! |
---|
1382 | IF ( lwp ) WRITE(numout,*) ' Beauaaaarflblbllll ' |
---|
1383 | ! |
---|
1384 | CALL iom_put( 'sig1_pnorm' , zsig1_p ) |
---|
1385 | CALL iom_put( 'sig2_pnorm' , zsig2_p ) |
---|
1386 | |
---|
1387 | DEALLOCATE( zsig1_p , zsig2_p , zsig_I , zsig_II ) |
---|
1388 | |
---|
1389 | IF ( lwp ) WRITE(numout,*) ' So what ??? ' |
---|
1390 | |
---|
1391 | ENDIF |
---|
1392 | |
---|
1393 | ! --- SIMIP, terms of tendency for momentum equation --- ! |
---|
1394 | IF( iom_use('dssh_dx') .OR. iom_use('dssh_dy') .OR. & |
---|
1395 | & iom_use('corstrx') .OR. iom_use('corstry') ) THEN |
---|
1396 | |
---|
1397 | ! --- Recalculate Coriolis stress at last inner iteration |
---|
1398 | DO jj = 2, jpj - 1 |
---|
1399 | DO ji = 2, jpi - 1 |
---|
1400 | ! --- U-component |
---|
1401 | zCorU(ji,jj) = 0.25_wp * r1_e1u(ji,jj) * & |
---|
1402 | & ( zmf(ji ,jj) * ( e1v(ji ,jj) * v_ice(ji ,jj) + e1v(ji ,jj-1) * v_ice(ji ,jj-1) ) & |
---|
1403 | & + zmf(ji+1,jj) * ( e1v(ji+1,jj) * v_ice(ji+1,jj) + e1v(ji+1,jj-1) * v_ice(ji+1,jj-1) ) ) |
---|
1404 | zCorV(ji,jj) = - 0.25_wp * r1_e2v(ji,jj) * & |
---|
1405 | & ( zmf(ji,jj ) * ( e2u(ji,jj ) * u_ice(ji,jj ) + e2u(ji-1,jj ) * u_ice(ji-1,jj ) ) & |
---|
1406 | & + zmf(ji,jj+1) * ( e2u(ji,jj+1) * u_ice(ji,jj+1) + e2u(ji-1,jj+1) * u_ice(ji-1,jj+1) ) ) |
---|
1407 | END DO |
---|
1408 | END DO |
---|
1409 | ! |
---|
1410 | CALL lbc_lnk( 'icedyn_rhg_vp', zspgU, 'U', -1., zspgV, 'V', -1., & |
---|
1411 | & zCorU, 'U', -1., zCorV, 'V', -1. ) |
---|
1412 | ! |
---|
1413 | CALL iom_put( 'dssh_dx' , zspgU * zmsk00 ) ! Sea-surface tilt term in force balance (x) |
---|
1414 | CALL iom_put( 'dssh_dy' , zspgV * zmsk00 ) ! Sea-surface tilt term in force balance (y) |
---|
1415 | CALL iom_put( 'corstrx' , zCorU * zmsk00 ) ! Coriolis force term in force balance (x) |
---|
1416 | CALL iom_put( 'corstry' , zCorV * zmsk00 ) ! Coriolis force term in force balance (y) |
---|
1417 | |
---|
1418 | ENDIF |
---|
1419 | |
---|
1420 | IF ( iom_use('intstrx') .OR. iom_use('intstry') ) THEN |
---|
1421 | |
---|
1422 | ! Recalculate internal forces (divergence of stress tensor) at last inner iteration |
---|
1423 | DO jj = 2, jpj - 1 |
---|
1424 | DO ji = 2, jpi - 1 |
---|
1425 | zfU(ji,jj) = 0.5_wp * ( ( zs1(ji+1,jj) - zs1(ji,jj) ) * e2u(ji,jj) & |
---|
1426 | & + ( zs2(ji+1,jj) * e2t(ji+1,jj) * e2t(ji+1,jj) - zs2(ji,jj) * e2t(ji,jj) * e2t(ji,jj) & |
---|
1427 | & ) * r1_e2u(ji,jj) & |
---|
1428 | & + ( zs12f(ji,jj) * e1f(ji,jj) * e1f(ji,jj) - zs12f(ji,jj-1) * e1f(ji,jj-1) * e1f(ji,jj-1) & |
---|
1429 | & ) * 2._wp * r1_e1u(ji,jj) & |
---|
1430 | & ) * r1_e1e2u(ji,jj) |
---|
1431 | zfV(ji,jj) = 0.5_wp * ( ( zs1(ji,jj+1) - zs1(ji,jj) ) * e1v(ji,jj) & |
---|
1432 | & - ( zs2(ji,jj+1) * e1t(ji,jj+1) * e1t(ji,jj+1) - zs2(ji,jj) * e1t(ji,jj) * e1t(ji,jj) & |
---|
1433 | & ) * r1_e1v(ji,jj) & |
---|
1434 | & + ( zs12f(ji,jj) * e2f(ji,jj) * e2f(ji,jj) - zs12f(ji-1,jj) * e2f(ji-1,jj) * e2f(ji-1,jj) & |
---|
1435 | & ) * 2._wp * r1_e2v(ji,jj) & |
---|
1436 | & ) * r1_e1e2v(ji,jj) |
---|
1437 | END DO |
---|
1438 | END DO |
---|
1439 | |
---|
1440 | CALL lbc_lnk( 'icedyn_rhg_vp', zfU, 'U', -1., zfV, 'V', -1. ) |
---|
1441 | |
---|
1442 | CALL iom_put( 'intstrx' , zfU * zmsk00 ) ! Internal force term in force balance (x) |
---|
1443 | CALL iom_put( 'intstry' , zfV * zmsk00 ) ! Internal force term in force balance (y) |
---|
1444 | |
---|
1445 | ENDIF |
---|
1446 | |
---|
1447 | ! --- Ice & snow mass and ice area transports |
---|
1448 | IF( iom_use('xmtrpice') .OR. iom_use('ymtrpice') .OR. & |
---|
1449 | & iom_use('xmtrpsnw') .OR. iom_use('ymtrpsnw') .OR. iom_use('xatrp') .OR. iom_use('yatrp') ) THEN |
---|
1450 | ! |
---|
1451 | ALLOCATE( zdiag_xmtrp_ice(jpi,jpj) , zdiag_ymtrp_ice(jpi,jpj) , & |
---|
1452 | & zdiag_xmtrp_snw(jpi,jpj) , zdiag_ymtrp_snw(jpi,jpj) , zdiag_xatrp(jpi,jpj) , zdiag_yatrp(jpi,jpj) ) |
---|
1453 | ! |
---|
1454 | DO jj = 2, jpj - 1 |
---|
1455 | DO ji = 2, jpi - 1 |
---|
1456 | ! 2D ice mass, snow mass, area transport arrays (X, Y) |
---|
1457 | zfac_x = 0.5 * u_ice(ji,jj) * e2u(ji,jj) * zmsk00(ji,jj) |
---|
1458 | zfac_y = 0.5 * v_ice(ji,jj) * e1v(ji,jj) * zmsk00(ji,jj) |
---|
1459 | |
---|
1460 | zdiag_xmtrp_ice(ji,jj) = rhoi * zfac_x * ( vt_i(ji+1,jj) + vt_i(ji,jj) ) ! ice mass transport, X-component |
---|
1461 | zdiag_ymtrp_ice(ji,jj) = rhoi * zfac_y * ( vt_i(ji,jj+1) + vt_i(ji,jj) ) ! '' Y- '' |
---|
1462 | |
---|
1463 | zdiag_xmtrp_snw(ji,jj) = rhos * zfac_x * ( vt_s(ji+1,jj) + vt_s(ji,jj) ) ! snow mass transport, X-component |
---|
1464 | zdiag_ymtrp_snw(ji,jj) = rhos * zfac_y * ( vt_s(ji,jj+1) + vt_s(ji,jj) ) ! '' Y- '' |
---|
1465 | |
---|
1466 | zdiag_xatrp(ji,jj) = zfac_x * ( at_i(ji+1,jj) + at_i(ji,jj) ) ! area transport, X-component |
---|
1467 | zdiag_yatrp(ji,jj) = zfac_y * ( at_i(ji,jj+1) + at_i(ji,jj) ) ! '' Y- '' |
---|
1468 | |
---|
1469 | END DO |
---|
1470 | END DO |
---|
1471 | |
---|
1472 | CALL lbc_lnk( 'icedyn_rhg_vp', zdiag_xmtrp_ice, 'U', -1., zdiag_ymtrp_ice, 'V', -1., & |
---|
1473 | & zdiag_xmtrp_snw, 'U', -1., zdiag_ymtrp_snw, 'V', -1., & |
---|
1474 | & zdiag_xatrp , 'U', -1., zdiag_yatrp , 'V', -1. ) |
---|
1475 | |
---|
1476 | CALL iom_put( 'xmtrpice' , zdiag_xmtrp_ice ) ! X-component of sea-ice mass transport (kg/s) |
---|
1477 | CALL iom_put( 'ymtrpice' , zdiag_ymtrp_ice ) ! Y-component of sea-ice mass transport |
---|
1478 | CALL iom_put( 'xmtrpsnw' , zdiag_xmtrp_snw ) ! X-component of snow mass transport (kg/s) |
---|
1479 | CALL iom_put( 'ymtrpsnw' , zdiag_ymtrp_snw ) ! Y-component of snow mass transport |
---|
1480 | CALL iom_put( 'xatrp' , zdiag_xatrp ) ! X-component of ice area transport |
---|
1481 | CALL iom_put( 'yatrp' , zdiag_yatrp ) ! Y-component of ice area transport |
---|
1482 | |
---|
1483 | DEALLOCATE( zdiag_xmtrp_ice , zdiag_ymtrp_ice , & |
---|
1484 | & zdiag_xmtrp_snw , zdiag_ymtrp_snw , zdiag_xatrp , zdiag_yatrp ) |
---|
1485 | |
---|
1486 | ENDIF |
---|
1487 | |
---|
1488 | END SUBROUTINE ice_dyn_rhg_vp |
---|
1489 | |
---|
1490 | |
---|
1491 | |
---|
1492 | SUBROUTINE rhg_cvg_vp( kt, kiter, kitermax, pu, pv, pmt, puerr_max, pverr_max, pglob_area, & |
---|
1493 | & prhsu, pAU, pBU, pCU, pDU, pEU, prhsv, pAV, pBV, pCV, pDV, pEV ) |
---|
1494 | |
---|
1495 | !!---------------------------------------------------------------------- |
---|
1496 | !! *** ROUTINE rhg_cvg_vp *** |
---|
1497 | !! |
---|
1498 | !! ** Purpose : check convergence of VP ice rheology |
---|
1499 | !! |
---|
1500 | !! ** Method : create a file ice_cvg.nc containing a few convergence diagnostics |
---|
1501 | !! This routine is called every sub-iteration, so it is cpu expensive |
---|
1502 | !! |
---|
1503 | !! Calculates / stores |
---|
1504 | !! - maximum absolute U-V difference (uice_cvg, u_dif, v_dif, m/s) |
---|
1505 | !! - residuals in U, V and UV-mean taken as square-root of area-weighted mean square residual (u_res, v_res, vel_res, N/m2) |
---|
1506 | !! - mean kinetic energy (mke_ice, J/m2) |
---|
1507 | !! |
---|
1508 | !! ** Note : for the first sub-iteration, uice_cvg is set to 0 (too large otherwise) |
---|
1509 | !!---------------------------------------------------------------------- |
---|
1510 | INTEGER , INTENT(in) :: kt, kiter, kitermax ! ocean time-step index |
---|
1511 | REAL(wp), DIMENSION(:,:), INTENT(in) :: pu, pv, pmt ! now velocity and mass per unit area |
---|
1512 | REAL(wp), INTENT(in) :: puerr_max, pverr_max ! absolute mean velocity difference |
---|
1513 | REAL(wp), INTENT(in) :: pglob_area ! global ice area |
---|
1514 | REAL(wp), DIMENSION(:,:), INTENT(in) :: prhsu, pAU, pBU, pCU, pDU, pEU ! linear system coefficients |
---|
1515 | REAL(wp), DIMENSION(:,:), INTENT(in) :: prhsv, pAV, pBV, pCV, pDV, pEV |
---|
1516 | !! |
---|
1517 | INTEGER :: it, idtime, istatus, ix_dim, iy_dim |
---|
1518 | INTEGER :: ji, jj ! dummy loop indices |
---|
1519 | REAL(wp) :: zveldif, zu_res_mean, zv_res_mean, zvelres, zmke, zu, zv ! local scalars |
---|
1520 | REAL(wp) :: z1_pglob_area |
---|
1521 | REAL(wp), DIMENSION(jpi,jpj) :: zu_res, zv_res, zvel2 ! local arrays |
---|
1522 | |
---|
1523 | CHARACTER(len=20) :: clname |
---|
1524 | !!---------------------------------------------------------------------- |
---|
1525 | |
---|
1526 | IF( lwp ) THEN |
---|
1527 | WRITE(numout,*) |
---|
1528 | WRITE(numout,*) 'rhg_cvg_vp : ice rheology convergence control' |
---|
1529 | WRITE(numout,*) '~~~~~~~~~~~' |
---|
1530 | WRITE(numout,*) ' kiter = : ', kiter |
---|
1531 | WRITE(numout,*) ' kitermax = : ', kitermax |
---|
1532 | ENDIF |
---|
1533 | |
---|
1534 | ! create file |
---|
1535 | IF( kt == nit000 .AND. kiter == 1 ) THEN |
---|
1536 | ! |
---|
1537 | IF( lwm ) THEN |
---|
1538 | |
---|
1539 | clname = 'ice_cvg.nc' |
---|
1540 | IF( .NOT. Agrif_Root() ) clname = TRIM(Agrif_CFixed())//"_"//TRIM(clname) |
---|
1541 | istatus = NF90_CREATE( TRIM(clname), NF90_CLOBBER, ncvgid ) |
---|
1542 | |
---|
1543 | istatus = NF90_DEF_DIM( ncvgid, 'time' , NF90_UNLIMITED, idtime ) |
---|
1544 | istatus = NF90_DEF_DIM( ncvgid, 'x' , jpi, ix_dim ) |
---|
1545 | istatus = NF90_DEF_DIM( ncvgid, 'y' , jpj, iy_dim ) |
---|
1546 | |
---|
1547 | ! i suggest vel_dif instead |
---|
1548 | istatus = NF90_DEF_VAR( ncvgid, 'u_res' , NF90_DOUBLE , (/ idtime /), nvarid_ures ) |
---|
1549 | istatus = NF90_DEF_VAR( ncvgid, 'v_res' , NF90_DOUBLE , (/ idtime /), nvarid_vres ) |
---|
1550 | istatus = NF90_DEF_VAR( ncvgid, 'vel_res', NF90_DOUBLE , (/ idtime /), nvarid_velres ) |
---|
1551 | istatus = NF90_DEF_VAR( ncvgid, 'u_dif' , NF90_DOUBLE , (/ idtime /), nvarid_udif ) |
---|
1552 | istatus = NF90_DEF_VAR( ncvgid, 'v_dif' , NF90_DOUBLE , (/ idtime /), nvarid_vdif ) |
---|
1553 | istatus = NF90_DEF_VAR( ncvgid, 'vel_dif', NF90_DOUBLE , (/ idtime /), nvarid_veldif ) |
---|
1554 | istatus = NF90_DEF_VAR( ncvgid, 'mke_ice', NF90_DOUBLE , (/ idtime /), nvarid_mke ) |
---|
1555 | |
---|
1556 | istatus = NF90_DEF_VAR( ncvgid, 'u_res_xy', NF90_DOUBLE, (/ ix_dim, iy_dim /), nvarid_ures_xy) |
---|
1557 | istatus = NF90_DEF_VAR( ncvgid, 'v_res_xy', NF90_DOUBLE, (/ ix_dim, iy_dim /), nvarid_vres_xy) |
---|
1558 | |
---|
1559 | istatus = NF90_ENDDEF(ncvgid) |
---|
1560 | |
---|
1561 | ENDIF |
---|
1562 | ! |
---|
1563 | ENDIF |
---|
1564 | |
---|
1565 | IF ( lwp ) WRITE(numout,*) ' File created ' |
---|
1566 | |
---|
1567 | ! --- Max absolute velocity difference with previous iterate (zveldif) |
---|
1568 | zveldif = MAX( puerr_max, pverr_max ) ! velocity difference with previous iterate, should nearly be equivalent to evp code |
---|
1569 | ! if puerrmask and pverrmax are masked at 15% (TEST) |
---|
1570 | |
---|
1571 | ! --- Mean residual and kinetic energy |
---|
1572 | IF ( kiter == 1 ) THEN |
---|
1573 | |
---|
1574 | zu_res_mean = 0._wp |
---|
1575 | zv_res_mean = 0._wp |
---|
1576 | zvelres = 0._wp |
---|
1577 | zmke = 0._wp |
---|
1578 | |
---|
1579 | ELSE |
---|
1580 | |
---|
1581 | ! -- Mean residual (N/m^2), zu_res_mean |
---|
1582 | ! Here we take the residual of the linear system (N/m^2), |
---|
1583 | ! We define it as in mitgcm: square-root of area-weighted mean square residual |
---|
1584 | ! Local residual r = Ax - B expresses to which extent the momentum balance is verified |
---|
1585 | ! i.e., how close we are to a solution |
---|
1586 | |
---|
1587 | IF ( lwp ) WRITE(numout,*) ' TEST 1 ' |
---|
1588 | |
---|
1589 | z1_pglob_area = 1._wp / pglob_area |
---|
1590 | |
---|
1591 | zu_res(:,:) = 0._wp; zv_res(:,:) = 0._wp |
---|
1592 | |
---|
1593 | DO jj = 2, jpj - 1 |
---|
1594 | DO ji = 2, jpi - 1 |
---|
1595 | zu_res(ji,jj) = ( prhsu(ji,jj) + pDU(ji,jj) * pu(ji,jj-1) + pEU(ji,jj) * pu(ji,jj+1) & |
---|
1596 | & - pAU(ji,jj) * pu(ji-1,jj) - pBU(ji,jj) * pu(ji,jj) - pCU(ji,jj) * pu(ji+1,jj) ) |
---|
1597 | |
---|
1598 | zv_res(ji,jj) = ( prhsv(ji,jj) + pDV(ji,jj) * pv(ji-1,jj) + pEV(ji,jj) * pv(ji+1,jj) & |
---|
1599 | & - pAV(ji,jj) * pv(ji,jj-1) - pBV(ji,jj) * pv(ji,jj) - pCV(ji,jj) * pv(ji,jj+1) ) |
---|
1600 | |
---|
1601 | zu_res(ji,jj) = SQRT( zu_res(ji,jj) * zu_res(ji,jj) ) * umask(ji,jj,1) * e1e2u(ji,jj) * z1_pglob_area |
---|
1602 | zv_res(ji,jj) = SQRT( zv_res(ji,jj) * zv_res(ji,jj) ) * vmask(ji,jj,1) * e1e2v(ji,jj) * z1_pglob_area |
---|
1603 | |
---|
1604 | END DO |
---|
1605 | END DO |
---|
1606 | |
---|
1607 | IF ( lwp ) WRITE(numout,*) ' TEST 2 ' |
---|
1608 | zu_res_mean = glob_sum( 'ice_rhg_vp', zu_res(:,:) ) |
---|
1609 | zv_res_mean = glob_sum( 'ice_rhg_vp', zv_res(:,:) ) |
---|
1610 | IF ( lwp ) WRITE(numout,*) ' TEST 3 ' |
---|
1611 | zvelres = 0.5_wp * ( zu_res_mean + zv_res_mean ) |
---|
1612 | |
---|
1613 | IF ( lwp ) WRITE(numout,*) ' TEST 4 ' |
---|
1614 | |
---|
1615 | ! -- Global mean kinetic energy per unit area (J/m2) |
---|
1616 | zvel2(:,:) = 0._wp |
---|
1617 | DO jj = 2, jpj - 1 |
---|
1618 | DO ji = 2, jpi - 1 |
---|
1619 | zu = 0.5_wp * ( pu(ji-1,jj) + pu(ji,jj) ) ! u-vel at T-point |
---|
1620 | zv = 0.5_wp * ( pv(ji,jj-1) + pv(ji,jj) ) |
---|
1621 | zvel2(ji,jj) = zu*zu + zv*zv ! square of ice velocity at T-point |
---|
1622 | END DO |
---|
1623 | END DO |
---|
1624 | |
---|
1625 | IF ( lwp ) WRITE(numout,*) ' TEST 5 ' |
---|
1626 | |
---|
1627 | zmke = 0.5_wp * glob_sum( 'ice_rhg_vp', pmt(:,:) * e1e2t(:,:) * zvel2(:,:) ) / pglob_area |
---|
1628 | |
---|
1629 | IF ( lwp ) WRITE(numout,*) ' TEST 6 ' |
---|
1630 | |
---|
1631 | ENDIF ! kiter |
---|
1632 | |
---|
1633 | ! ! ==================== ! |
---|
1634 | |
---|
1635 | ! time |
---|
1636 | it = ( kt - 1 ) * kitermax + kiter |
---|
1637 | |
---|
1638 | |
---|
1639 | IF( lwm ) THEN |
---|
1640 | ! write variables |
---|
1641 | istatus = NF90_PUT_VAR( ncvgid, nvarid_ures, (/zu_res_mean/), (/it/), (/1/) ) ! U-residual of the linear system |
---|
1642 | istatus = NF90_PUT_VAR( ncvgid, nvarid_vres, (/zv_res_mean/), (/it/), (/1/) ) ! V-residual of the linear system |
---|
1643 | istatus = NF90_PUT_VAR( ncvgid, nvarid_velres, (/zvelres/), (/it/), (/1/) ) ! average of u- and v- residuals |
---|
1644 | istatus = NF90_PUT_VAR( ncvgid, nvarid_udif, (/puerr_max/), (/it/), (/1/) ) ! max U velocity difference, inner iterations |
---|
1645 | istatus = NF90_PUT_VAR( ncvgid, nvarid_vdif, (/pverr_max/), (/it/), (/1/) ) ! max V velocity difference, inner iterations |
---|
1646 | istatus = NF90_PUT_VAR( ncvgid, nvarid_veldif, (/zveldif/), (/it/), (/1/) ) ! max U or V velocity diff between subiterations |
---|
1647 | istatus = NF90_PUT_VAR( ncvgid, nvarid_mke, (/zmke/), (/it/), (/1/) ) ! mean kinetic energy |
---|
1648 | |
---|
1649 | ! |
---|
1650 | IF ( kiter == kitermax ) THEN |
---|
1651 | WRITE(numout,*) ' Should plot the spatially dependent residual ' |
---|
1652 | istatus = NF90_PUT_VAR( ncvgid, nvarid_ures_xy, (/zu_res/) ) ! U-residual, spatially dependent |
---|
1653 | istatus = NF90_PUT_VAR( ncvgid, nvarid_vres_xy, (/zv_res/) ) ! V-residual, spatially dependent |
---|
1654 | ENDIF |
---|
1655 | |
---|
1656 | ! close file |
---|
1657 | IF( kt == nitend ) istatus = NF90_CLOSE( ncvgid ) |
---|
1658 | ENDIF |
---|
1659 | |
---|
1660 | END SUBROUTINE rhg_cvg_vp |
---|
1661 | |
---|
1662 | |
---|
1663 | |
---|
1664 | #else |
---|
1665 | !!---------------------------------------------------------------------- |
---|
1666 | !! Default option Empty module NO SI3 sea-ice model |
---|
1667 | !!---------------------------------------------------------------------- |
---|
1668 | #endif |
---|
1669 | |
---|
1670 | !!============================================================================== |
---|
1671 | END MODULE icedyn_rhg_vp |
---|
1672 | |
---|