1 | MODULE limthd |
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2 | !!====================================================================== |
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3 | !! *** MODULE limthd *** |
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4 | !! LIM-3 : ice thermodynamic |
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5 | !!====================================================================== |
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6 | !! History : LIM ! 2000-01 (M.A. Morales Maqueda, H. Goosse, T. Fichefet) LIM-1 |
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7 | !! 2.0 ! 2002-07 (C. Ethe, G. Madec) LIM-2 (F90 rewriting) |
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8 | !! 3.0 ! 2005-11 (M. Vancoppenolle) LIM-3 : Multi-layer thermodynamics + salinity variations |
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9 | !! - ! 2007-04 (M. Vancoppenolle) add lim_thd_glohec, lim_thd_con_dh and lim_thd_con_dif |
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10 | !! 3.2 ! 2009-07 (M. Vancoppenolle, Y. Aksenov, G. Madec) bug correction in wfx_snw |
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11 | !! 3.3 ! 2010-11 (G. Madec) corrected snow melting heat (due to factor betas) |
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12 | !! 4.0 ! 2011-02 (G. Madec) dynamical allocation |
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13 | !! - ! 2012-05 (C. Rousset) add penetration solar flux |
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14 | !!---------------------------------------------------------------------- |
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15 | #if defined key_lim3 |
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16 | !!---------------------------------------------------------------------- |
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17 | !! 'key_lim3' LIM3 sea-ice model |
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18 | !!---------------------------------------------------------------------- |
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19 | !! lim_thd : thermodynamic of sea ice |
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20 | !! lim_thd_init : initialisation of sea-ice thermodynamic |
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21 | !!---------------------------------------------------------------------- |
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22 | USE phycst ! physical constants |
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23 | USE dom_oce ! ocean space and time domain variables |
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24 | USE oce , ONLY : iatte, oatte |
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25 | USE ice ! LIM: sea-ice variables |
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26 | USE par_ice ! LIM: sea-ice parameters |
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27 | USE sbc_oce ! Surface boundary condition: ocean fields |
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28 | USE sbc_ice ! Surface boundary condition: ice fields |
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29 | USE thd_ice ! LIM thermodynamic sea-ice variables |
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30 | USE dom_ice ! LIM sea-ice domain |
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31 | USE domvvl ! domain: variable volume level |
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32 | USE limthd_dif ! LIM: thermodynamics, vertical diffusion |
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33 | USE limthd_dh ! LIM: thermodynamics, ice and snow thickness variation |
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34 | USE limthd_sal ! LIM: thermodynamics, ice salinity |
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35 | USE limthd_ent ! LIM: thermodynamics, ice enthalpy redistribution |
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36 | USE limtab ! LIM: 1D <==> 2D transformation |
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37 | USE limvar ! LIM: sea-ice variables |
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38 | USE lbclnk ! lateral boundary condition - MPP links |
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39 | USE lib_mpp ! MPP library |
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40 | USE wrk_nemo ! work arrays |
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41 | USE in_out_manager ! I/O manager |
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42 | USE prtctl ! Print control |
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43 | USE lib_fortran ! Fortran utilities (allows no signed zero when 'key_nosignedzero' defined) |
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44 | USE timing ! Timing |
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45 | USE cpl_oasis3, ONLY : lk_cpl |
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46 | |
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47 | IMPLICIT NONE |
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48 | PRIVATE |
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49 | |
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50 | PUBLIC lim_thd ! called by limstp module |
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51 | PUBLIC lim_thd_init ! called by iceini module |
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52 | |
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53 | REAL(wp) :: epsi10 = 1.e-10_wp ! |
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54 | |
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55 | !! * Substitutions |
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56 | # include "domzgr_substitute.h90" |
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57 | # include "vectopt_loop_substitute.h90" |
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58 | !!---------------------------------------------------------------------- |
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59 | !! NEMO/LIM3 3.3 , UCL - NEMO Consortium (2010) |
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60 | !! $Id$ |
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61 | !! Software governed by the CeCILL licence (NEMOGCM/NEMO_CeCILL.txt) |
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62 | !!---------------------------------------------------------------------- |
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63 | CONTAINS |
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64 | |
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65 | SUBROUTINE lim_thd( kt ) |
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66 | !!------------------------------------------------------------------- |
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67 | !! *** ROUTINE lim_thd *** |
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68 | !! |
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69 | !! ** Purpose : This routine manages the ice thermodynamic. |
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70 | !! |
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71 | !! ** Action : - Initialisation of some variables |
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72 | !! - Some preliminary computation (oceanic heat flux |
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73 | !! at the ice base, snow acc.,heat budget of the leads) |
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74 | !! - selection of the icy points and put them in an array |
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75 | !! - call lim_vert_ther for vert ice thermodynamic |
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76 | !! - back to the geographic grid |
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77 | !! - selection of points for lateral accretion |
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78 | !! - call lim_lat_acc for the ice accretion |
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79 | !! - back to the geographic grid |
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80 | !! |
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81 | !! ** References : H. Goosse et al. 1996, Bul. Soc. Roy. Sc. Liege, 65, 87-90 |
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82 | !!--------------------------------------------------------------------- |
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83 | INTEGER, INTENT(in) :: kt ! number of iteration |
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84 | !! |
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85 | INTEGER :: ji, jj, jk, jl ! dummy loop indices |
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86 | INTEGER :: nbpb ! nb of icy pts for thermo. cal. |
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87 | INTEGER :: ii, ij ! temporary dummy loop index |
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88 | REAL(wp) :: zfric_umin = 5e-03_wp ! lower bound for the friction velocity |
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89 | REAL(wp) :: zfric_umax = 2e-02_wp ! upper bound for the friction velocity |
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90 | REAL(wp) :: zinda, zindb, zfric_u ! local scalar |
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91 | REAL(wp) :: zareamin ! - - |
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92 | REAL(wp) :: zchk_v_i, zchk_smv, zchk_e_i, zchk_fs, zchk_fw, zchk_ft, zchk_v_i_b, zchk_smv_b, zchk_e_i_b, zchk_fs_b, zchk_fw_b, zchk_ft_b |
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93 | REAL(wp) :: zchk_vmin, zchk_amin, zchk_amax ! Check errors (C Rousset) |
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94 | REAL(wp) :: zqld, zqfr |
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95 | REAL(wp), POINTER, DIMENSION(:) :: zdq, zq_ini, zhfx, zqfx |
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96 | REAL(wp) :: zhfx_err, ztest |
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97 | !!------------------------------------------------------------------- |
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98 | IF( nn_timing == 1 ) CALL timing_start('limthd') |
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99 | |
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100 | CALL wrk_alloc( jpij, zdq, zq_ini, zhfx, zqfx ) |
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101 | |
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102 | ! init debug |
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103 | zdq(:) = 0._wp ; zq_ini(:) = 0._wp ; zhfx(:) = 0._wp ; zqfx(:) = 0._wp |
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104 | |
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105 | ! ------------------------------- |
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106 | !- check conservation (C Rousset) |
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107 | IF (ln_limdiahsb) THEN |
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108 | zchk_v_i_b = glob_sum( SUM( v_i(:,:,:)*rhoic + v_s(:,:,:)*rhosn, dim=3 ) * area(:,:) * tms(:,:) ) |
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109 | zchk_smv_b = glob_sum( SUM( smv_i(:,:,:), dim=3 ) * area(:,:) * tms(:,:) ) |
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110 | zchk_e_i_b = glob_sum( SUM( e_i(:,:,1:nlay_i,:), dim=3 ) + SUM( e_s(:,:,1:nlay_s,:), dim=3 ) ) |
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111 | zchk_fw_b = glob_sum( ( wfx_bog(:,:) + wfx_bom(:,:) + wfx_sum(:,:) + wfx_sni(:,:) + wfx_opw(:,:) + wfx_res(:,:) + wfx_dyn(:,:) + wfx_snw(:,:) ) * area(:,:) * tms(:,:) ) |
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112 | zchk_fs_b = glob_sum( ( sfx_bri(:,:) + sfx_bog(:,:) + sfx_bom(:,:) + sfx_sum(:,:) + sfx_sni(:,:) + sfx_opw(:,:) + sfx_res(:,:) + sfx_dyn(:,:) ) * area(:,:) * tms(:,:) ) |
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113 | zchk_ft_b = glob_sum( ( hfx_tot(:,:) - hfx_thd(:,:) - hfx_dyn(:,:) - hfx_res(:,:) ) * area(:,:) / unit_fac * tms(:,:) ) |
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114 | ENDIF |
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115 | !- check conservation (C Rousset) |
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116 | ! ------------------------------- |
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117 | |
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118 | !------------------------------------------------------------------------------! |
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119 | ! 1) Initialization of diagnostic variables ! |
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120 | !------------------------------------------------------------------------------! |
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121 | |
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122 | !-------------------- |
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123 | ! 1.2) Heat content |
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124 | !-------------------- |
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125 | ! Change the units of heat content; from global units to J.m3 |
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126 | DO jl = 1, jpl |
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127 | DO jk = 1, nlay_i |
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128 | DO jj = 1, jpj |
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129 | DO ji = 1, jpi |
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130 | !0 if no ice and 1 if yes |
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131 | zindb = 1.0 - MAX( 0.0 , SIGN( 1.0 , - v_i(ji,jj,jl) + epsi10 ) ) |
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132 | !Energy of melting q(S,T) [J.m-3] |
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133 | e_i(ji,jj,jk,jl) = zindb * e_i(ji,jj,jk,jl) / ( area(ji,jj) * MAX( v_i(ji,jj,jl) , epsi10 ) ) * REAL( nlay_i ) |
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134 | !convert units ! very important that this line is here |
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135 | e_i(ji,jj,jk,jl) = e_i(ji,jj,jk,jl) * unit_fac |
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136 | END DO |
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137 | END DO |
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138 | END DO |
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139 | DO jk = 1, nlay_s |
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140 | DO jj = 1, jpj |
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141 | DO ji = 1, jpi |
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142 | !0 if no ice and 1 if yes |
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143 | zindb = 1.0 - MAX( 0.0 , SIGN( 1.0 , - v_s(ji,jj,jl) + epsi10 ) ) |
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144 | !Energy of melting q(S,T) [J.m-3] |
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145 | e_s(ji,jj,jk,jl) = zindb * e_s(ji,jj,jk,jl) / ( area(ji,jj) * MAX( v_s(ji,jj,jl) , epsi10 ) ) * REAL( nlay_s ) |
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146 | !convert units ! very important that this line is here |
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147 | e_s(ji,jj,jk,jl) = e_s(ji,jj,jk,jl) * unit_fac |
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148 | END DO |
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149 | END DO |
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150 | END DO |
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151 | END DO |
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152 | |
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153 | ! 2) Partial computation of forcing for the thermodynamic sea ice model. ! |
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154 | !-----------------------------------------------------------------------------! |
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155 | |
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156 | !CDIR NOVERRCHK |
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157 | DO jj = 1, jpj |
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158 | !CDIR NOVERRCHK |
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159 | DO ji = 1, jpi |
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160 | zinda = tms(ji,jj) * ( 1.0 - MAX( 0._wp , SIGN( 1._wp , - at_i(ji,jj) + epsi10 ) ) ) ! 0 if no ice |
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161 | ! |
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162 | ! ! solar irradiance transmission at the mixed layer bottom and used in the lead heat budget |
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163 | ! ! practically no "direct lateral ablation" |
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164 | ! |
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165 | ! ! net downward heat flux from the ice to the ocean, expressed as a function of ocean |
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166 | ! ! temperature and turbulent mixing (McPhee, 1992) |
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167 | |
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168 | ! friction velocity |
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169 | zfric_u = MAX ( MIN( SQRT( ust2s(ji,jj) ) , zfric_umax ) , zfric_umin ) |
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170 | |
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171 | !-- Energy from the turbulent oceanic heat flux. here the drag will depend on ice thickness and type (0.006) |
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172 | fhtur(ji,jj) = zinda * rau0 * rcp * 0.006 * zfric_u * ( ( sst_m(ji,jj) + rt0 ) - t_bo(ji,jj) ) ! W.m-2 |
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173 | ! clem: why not the following? |
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174 | !fhtur(ji,jj) = zinda * rau0 * rcp * 0.006 * SQRT( ust2s(ji,jj) ) * ( ( sst_m(ji,jj) + rt0 ) - t_bo(ji,jj) ) |
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175 | |
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176 | !-- Energy received in the lead, zqld is defined everywhere (J.m-2) |
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177 | ! It includes turbulent ocean heat flux (only in the leads, the rest is used for bottom melting) |
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178 | zqld = tms(ji,jj) * rdt_ice * & |
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179 | & ( pfrld(ji,jj) * ( qsr(ji,jj) * oatte(ji,jj) & ! solar heat + clem modif |
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180 | & + qns(ji,jj) & ! non solar heat |
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181 | & + fhtur(ji,jj) ) & ! turbulent ice-ocean heat (0 if no ice) |
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182 | ! latent heat of precip (note that precip is included in qns but not in qns_ice) |
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183 | & + ( pfrld(ji,jj)**betas - pfrld(ji,jj) ) * sprecip(ji,jj) * ( cpic * ( MIN( tatm_ice(ji,jj), rt0_snow ) - rtt ) - lfus ) & |
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184 | & + ( 1._wp - pfrld(ji,jj) ) * ( tprecip(ji,jj) - sprecip(ji,jj) ) * rcp * ( tatm_ice(ji,jj) - rtt ) ) |
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185 | |
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186 | !-- Energy needed to bring ocean surface layer until its freezing (<0, J.m-2) |
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187 | zqfr = tms(ji,jj) * rau0 * rcp * fse3t_m(ji,jj,1) * ( t_bo(ji,jj) - ( sst_m(ji,jj) + rt0 ) ) |
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188 | |
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189 | !-- Energy Budget of the leads (J.m-2). Must be < 0 to form ice |
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190 | qlead(ji,jj) = MIN( 0._wp , zqld - zqfr ) |
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191 | |
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192 | ! If there is ice and leads are warming, then transfer energy from the lead budget and use it for bottom melting |
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193 | IF( at_i(ji,jj) > epsi10 .AND. zqld > 0._wp ) THEN |
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194 | fhld (ji,jj) = zqld * r1_rdtice / at_i(ji,jj) ! divided by a_i since this is (re)multiplied by a_i in limthd_dh.F90 |
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195 | qlead(ji,jj) = 0._wp |
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196 | ENDIF |
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197 | ! |
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198 | IF( qlead(ji,jj) == 0._wp ) zqld = 0._wp ; zqfr = 0._wp |
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199 | ! |
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200 | ! ----------------------------------------- |
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201 | ! Net heat flux on top of ice-ocean [W.m-2] |
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202 | ! ----------------------------------------- |
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203 | ! First step here : heat flux at the ocean surface + precip |
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204 | ! Second step below : heat flux at the ice surface (after limthd_dif) |
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205 | hfx_in(ji,jj) = hfx_in(ji,jj) & |
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206 | ! heat flux above the ocean |
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207 | & + pfrld(ji,jj) * ( qns(ji,jj) + qsr(ji,jj) ) & |
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208 | ! latent heat of precip (note that precip is included in qns but not in qns_ice) |
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209 | & + ( 1._wp - pfrld(ji,jj) ) * sprecip(ji,jj) * ( cpic * ( MIN( tatm_ice(ji,jj), rt0_snow ) - rtt ) - lfus ) & |
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210 | & + ( 1._wp - pfrld(ji,jj) ) * ( tprecip(ji,jj) - sprecip(ji,jj) ) * rcp * ( tatm_ice(ji,jj) - rtt ) |
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211 | |
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212 | ! ----------------------------------------------------------------------------- |
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213 | ! Net heat flux that is retroceded to the ocean or taken from the ocean [W.m-2] |
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214 | ! ----------------------------------------------------------------------------- |
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215 | ! First step here : non solar + precip - qlead - qturb |
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216 | ! Second step in limthd_dh : heat remaining if total melt (zq_rema) |
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217 | ! Third step in limsbc : heat from ice-ocean mass exchange (zf_mass) + solar |
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218 | hfx_out(ji,jj) = hfx_out(ji,jj) & |
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219 | ! Non solar heat flux received by the ocean |
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220 | & + pfrld(ji,jj) * qns(ji,jj) & |
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221 | ! latent heat of precip (note that precip is included in qns but not in qns_ice) |
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222 | & + ( pfrld(ji,jj)**betas - pfrld(ji,jj) ) * sprecip(ji,jj) * ( cpic * ( MIN( tatm_ice(ji,jj), rt0_snow ) - rtt ) - lfus ) & |
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223 | & + ( 1._wp - pfrld(ji,jj) ) * ( tprecip(ji,jj) - sprecip(ji,jj) ) * rcp * ( tatm_ice(ji,jj) - rtt ) & |
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224 | ! heat flux taken from the ocean where there is open water ice formation |
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225 | & - qlead(ji,jj) * r1_rdtice & |
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226 | ! heat flux taken from the ocean during bottom growth/melt (fhld should be 0 while bott growth) |
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227 | & - at_i(ji,jj) * fhtur(ji,jj) & |
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228 | & - at_i(ji,jj) * fhld(ji,jj) |
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229 | |
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230 | END DO |
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231 | END DO |
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232 | |
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233 | !------------------------------------------------------------------------------! |
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234 | ! 3) Select icy points and fulfill arrays for the vectorial grid. |
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235 | !------------------------------------------------------------------------------! |
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236 | |
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237 | DO jl = 1, jpl !loop over ice categories |
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238 | |
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239 | IF( kt == nit000 .AND. lwp ) THEN |
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240 | WRITE(numout,*) ' lim_thd : transfer to 1D vectors. Category no : ', jl |
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241 | WRITE(numout,*) ' ~~~~~~~~' |
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242 | ENDIF |
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243 | |
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244 | zareamin = epsi10 |
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245 | nbpb = 0 |
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246 | DO jj = 1, jpj |
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247 | DO ji = 1, jpi |
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248 | IF ( a_i(ji,jj,jl) .gt. zareamin ) THEN |
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249 | nbpb = nbpb + 1 |
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250 | npb(nbpb) = (jj - 1) * jpi + ji |
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251 | ENDIF |
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252 | END DO |
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253 | END DO |
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254 | |
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255 | ! debug point to follow |
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256 | jiindex_1d = 0 |
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257 | IF( ln_nicep ) THEN |
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258 | DO ji = mi0(jiindx), mi1(jiindx) |
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259 | DO jj = mj0(jjindx), mj1(jjindx) |
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260 | jiindex_1d = (jj - 1) * jpi + ji |
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261 | WRITE(numout,*) ' lim_thd : Category no : ', jl |
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262 | END DO |
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263 | END DO |
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264 | ENDIF |
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265 | |
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266 | !------------------------------------------------------------------------------! |
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267 | ! 4) Thermodynamic computation |
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268 | !------------------------------------------------------------------------------! |
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269 | |
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270 | IF( lk_mpp ) CALL mpp_ini_ice( nbpb , numout ) |
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271 | |
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272 | IF( nbpb > 0 ) THEN ! If there is no ice, do nothing. |
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273 | |
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274 | !------------------------- |
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275 | ! 4.1 Move to 1D arrays |
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276 | !------------------------- |
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277 | |
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278 | CALL tab_2d_1d( nbpb, at_i_b (1:nbpb), at_i , jpi, jpj, npb(1:nbpb) ) |
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279 | CALL tab_2d_1d( nbpb, a_i_b (1:nbpb), a_i(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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280 | CALL tab_2d_1d( nbpb, ht_i_b (1:nbpb), ht_i(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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281 | CALL tab_2d_1d( nbpb, ht_s_b (1:nbpb), ht_s(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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282 | |
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283 | CALL tab_2d_1d( nbpb, t_su_b (1:nbpb), t_su(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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284 | CALL tab_2d_1d( nbpb, sm_i_b (1:nbpb), sm_i(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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285 | DO jk = 1, nlay_s |
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286 | CALL tab_2d_1d( nbpb, t_s_b(1:nbpb,jk), t_s(:,:,jk,jl) , jpi, jpj, npb(1:nbpb) ) |
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287 | CALL tab_2d_1d( nbpb, q_s_b(1:nbpb,jk), e_s(:,:,jk,jl) , jpi, jpj, npb(1:nbpb) ) |
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288 | END DO |
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289 | DO jk = 1, nlay_i |
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290 | CALL tab_2d_1d( nbpb, t_i_b(1:nbpb,jk), t_i(:,:,jk,jl) , jpi, jpj, npb(1:nbpb) ) |
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291 | CALL tab_2d_1d( nbpb, q_i_b(1:nbpb,jk), e_i(:,:,jk,jl) , jpi, jpj, npb(1:nbpb) ) |
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292 | CALL tab_2d_1d( nbpb, s_i_b(1:nbpb,jk), s_i(:,:,jk,jl) , jpi, jpj, npb(1:nbpb) ) |
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293 | END DO |
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294 | |
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295 | CALL tab_2d_1d( nbpb, tatm_ice_1d(1:nbpb), tatm_ice(:,:) , jpi, jpj, npb(1:nbpb) ) |
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296 | CALL tab_2d_1d( nbpb, qsr_ice_1d (1:nbpb), qsr_ice(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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297 | CALL tab_2d_1d( nbpb, fr1_i0_1d (1:nbpb), fr1_i0 , jpi, jpj, npb(1:nbpb) ) |
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298 | CALL tab_2d_1d( nbpb, fr2_i0_1d (1:nbpb), fr2_i0 , jpi, jpj, npb(1:nbpb) ) |
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299 | CALL tab_2d_1d( nbpb, qns_ice_1d (1:nbpb), qns_ice(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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300 | CALL tab_2d_1d( nbpb, ftr_ice_1d (1:nbpb), ftr_ice(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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301 | IF( .NOT. lk_cpl ) THEN |
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302 | CALL tab_2d_1d( nbpb, qla_ice_1d (1:nbpb), qla_ice(:,:,jl) , jpi, jpj, npb(1:nbpb) ) |
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303 | CALL tab_2d_1d( nbpb, dqla_ice_1d(1:nbpb), dqla_ice(:,:,jl), jpi, jpj, npb(1:nbpb) ) |
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304 | ENDIF |
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305 | CALL tab_2d_1d( nbpb, dqns_ice_1d(1:nbpb), dqns_ice(:,:,jl), jpi, jpj, npb(1:nbpb) ) |
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306 | CALL tab_2d_1d( nbpb, t_bo_b (1:nbpb), t_bo , jpi, jpj, npb(1:nbpb) ) |
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307 | CALL tab_2d_1d( nbpb, sprecip_1d (1:nbpb), sprecip , jpi, jpj, npb(1:nbpb) ) |
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308 | CALL tab_2d_1d( nbpb, fhtur_1d (1:nbpb), fhtur , jpi, jpj, npb(1:nbpb) ) |
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309 | CALL tab_2d_1d( nbpb, qlead_1d (1:nbpb), qlead , jpi, jpj, npb(1:nbpb) ) |
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310 | CALL tab_2d_1d( nbpb, fhld_1d (1:nbpb), fhld , jpi, jpj, npb(1:nbpb) ) |
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311 | |
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312 | CALL tab_2d_1d( nbpb, wfx_snw_1d (1:nbpb), wfx_snw , jpi, jpj, npb(1:nbpb) ) |
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313 | CALL tab_2d_1d( nbpb, wfx_sub_1d (1:nbpb), wfx_sub , jpi, jpj, npb(1:nbpb) ) |
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314 | |
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315 | CALL tab_2d_1d( nbpb, wfx_bog_1d (1:nbpb), wfx_bog , jpi, jpj, npb(1:nbpb) ) |
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316 | CALL tab_2d_1d( nbpb, wfx_bom_1d (1:nbpb), wfx_bom , jpi, jpj, npb(1:nbpb) ) |
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317 | CALL tab_2d_1d( nbpb, wfx_sum_1d (1:nbpb), wfx_sum , jpi, jpj, npb(1:nbpb) ) |
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318 | CALL tab_2d_1d( nbpb, wfx_sni_1d (1:nbpb), wfx_sni , jpi, jpj, npb(1:nbpb) ) |
---|
319 | |
---|
320 | CALL tab_2d_1d( nbpb, sfx_bog_1d (1:nbpb), sfx_bog , jpi, jpj, npb(1:nbpb) ) |
---|
321 | CALL tab_2d_1d( nbpb, sfx_bom_1d (1:nbpb), sfx_bom , jpi, jpj, npb(1:nbpb) ) |
---|
322 | CALL tab_2d_1d( nbpb, sfx_sum_1d (1:nbpb), sfx_sum , jpi, jpj, npb(1:nbpb) ) |
---|
323 | CALL tab_2d_1d( nbpb, sfx_sni_1d (1:nbpb), sfx_sni , jpi, jpj, npb(1:nbpb) ) |
---|
324 | CALL tab_2d_1d( nbpb, sfx_bri_1d (1:nbpb), sfx_bri , jpi, jpj, npb(1:nbpb) ) |
---|
325 | |
---|
326 | CALL tab_2d_1d( nbpb, iatte_1d (1:nbpb), iatte , jpi, jpj, npb(1:nbpb) ) |
---|
327 | CALL tab_2d_1d( nbpb, oatte_1d (1:nbpb), oatte , jpi, jpj, npb(1:nbpb) ) |
---|
328 | |
---|
329 | CALL tab_2d_1d( nbpb, hfx_thd_1d (1:nbpb), hfx_thd , jpi, jpj, npb(1:nbpb) ) |
---|
330 | CALL tab_2d_1d( nbpb, hfx_spr_1d (1:nbpb), hfx_spr , jpi, jpj, npb(1:nbpb) ) |
---|
331 | CALL tab_2d_1d( nbpb, hfx_tot_1d (1:nbpb), hfx_tot , jpi, jpj, npb(1:nbpb) ) |
---|
332 | CALL tab_2d_1d( nbpb, hfx_snw_1d (1:nbpb), hfx_snw , jpi, jpj, npb(1:nbpb) ) |
---|
333 | CALL tab_2d_1d( nbpb, hfx_sub_1d (1:nbpb), hfx_sub , jpi, jpj, npb(1:nbpb) ) |
---|
334 | CALL tab_2d_1d( nbpb, hfx_err_1d (1:nbpb), hfx_err , jpi, jpj, npb(1:nbpb) ) |
---|
335 | CALL tab_2d_1d( nbpb, hfx_res_1d (1:nbpb), hfx_res , jpi, jpj, npb(1:nbpb) ) |
---|
336 | CALL tab_2d_1d( nbpb, hfx_err_rem_1d (1:nbpb), hfx_err_rem , jpi, jpj, npb(1:nbpb) ) |
---|
337 | |
---|
338 | !-------------------------------- |
---|
339 | ! 4.3) Thermodynamic processes |
---|
340 | !-------------------------------- |
---|
341 | ! --- diag error on heat diffusion - PART 1 --- ! |
---|
342 | DO ji = 1, nbpb |
---|
343 | zq_ini(ji) = ( SUM( q_i_b(ji,1:nlay_i) ) * ht_i_b(ji) / REAL( nlay_i ) + & |
---|
344 | & SUM( q_s_b(ji,1:nlay_s) ) * ht_s_b(ji) / REAL( nlay_s ) ) |
---|
345 | END DO |
---|
346 | |
---|
347 | !---------------------------------! |
---|
348 | ! Ice/Snow Temperature profile ! |
---|
349 | !---------------------------------! |
---|
350 | CALL lim_thd_dif( 1, nbpb, jl ) |
---|
351 | |
---|
352 | ! --- computes sea ice energy of melting compulsory for limthd_dh --- ! |
---|
353 | CALL lim_thd_enmelt( 1, nbpb ) |
---|
354 | |
---|
355 | DO ji = 1, nbpb |
---|
356 | ! --- diag error on heat diffusion - PART 2 --- ! |
---|
357 | zdq(ji) = - zq_ini(ji) + ( SUM( q_i_b(ji,1:nlay_i) ) * ht_i_b(ji) / REAL( nlay_i ) + & |
---|
358 | & SUM( q_s_b(ji,1:nlay_s) ) * ht_s_b(ji) / REAL( nlay_s ) ) |
---|
359 | zhfx_err = ( fc_su(ji) + i0(ji) * qsr_ice_1d(ji) - ftr_ice_1d(ji) - fc_bo_i(ji) + zdq(ji) * r1_rdtice ) |
---|
360 | hfx_err_1d(ji) = hfx_err_1d(ji) + zhfx_err * a_i_b(ji) |
---|
361 | ! --- correction of qns_ice and surface conduction flux --- ! |
---|
362 | qns_ice_1d(ji) = qns_ice_1d(ji) - zhfx_err |
---|
363 | fc_su (ji) = fc_su (ji) - zhfx_err |
---|
364 | ! --- Heat flux at the ice surface in W.m-2 --- ! |
---|
365 | ii = MOD( npb(ji) - 1, jpi ) + 1 ; ij = ( npb(ji) - 1 ) / jpi + 1 |
---|
366 | hfx_in (ii,ij) = hfx_in (ii,ij) + a_i_b(ji) * ( qsr_ice_1d(ji) + qns_ice_1d(ji) ) |
---|
367 | |
---|
368 | END DO |
---|
369 | |
---|
370 | !---------------------------------! |
---|
371 | ! Ice/Snow thicnkess ! |
---|
372 | !---------------------------------! |
---|
373 | ! --- diag error on heat remapping - PART 1 --- ! |
---|
374 | DO ji = 1, nbpb |
---|
375 | zq_ini(ji) = ( SUM( q_i_b(ji,1:nlay_i) ) * ht_i_b(ji) / REAL( nlay_i ) + & |
---|
376 | & SUM( q_s_b(ji,1:nlay_s) ) * ht_s_b(ji) / REAL( nlay_s ) ) |
---|
377 | END DO |
---|
378 | |
---|
379 | CALL lim_thd_dh( 1, nbpb, jl ) |
---|
380 | |
---|
381 | ! --- Ice/Snow enthalpy remapping --- ! |
---|
382 | CALL lim_thd_ent( 1, nbpb, jl ) |
---|
383 | ! |
---|
384 | ! --- diag error on heat remapping - PART 2 --- ! |
---|
385 | DO ji = 1, nbpb |
---|
386 | zdq(ji) = - ( zq_ini(ji) + dq_i(ji) + dq_s(ji) ) & |
---|
387 | & + ( SUM( q_i_b(ji,1:nlay_i) ) * ht_i_b(ji) / REAL( nlay_i ) + & |
---|
388 | & SUM( q_s_b(ji,1:nlay_s) ) * ht_s_b(ji) / REAL( nlay_s ) ) |
---|
389 | hfx_err_rem_1d(ji) = hfx_err_rem_1d(ji) + zdq(ji) * a_i_b(ji) * r1_rdtice |
---|
390 | END DO |
---|
391 | |
---|
392 | !---------------------------------! |
---|
393 | ! Ice salinity ! |
---|
394 | !---------------------------------! |
---|
395 | CALL lim_thd_sal( 1, nbpb ) |
---|
396 | |
---|
397 | ! CALL lim_thd_enmelt(1,nbpb) ! computes sea ice energy of melting |
---|
398 | !-------------------------------- |
---|
399 | ! 4.4) Move 1D to 2D vectors |
---|
400 | !-------------------------------- |
---|
401 | |
---|
402 | CALL tab_1d_2d( nbpb, at_i , npb, at_i_b (1:nbpb) , jpi, jpj ) |
---|
403 | CALL tab_1d_2d( nbpb, ht_i(:,:,jl) , npb, ht_i_b (1:nbpb) , jpi, jpj ) |
---|
404 | CALL tab_1d_2d( nbpb, ht_s(:,:,jl) , npb, ht_s_b (1:nbpb) , jpi, jpj ) |
---|
405 | CALL tab_1d_2d( nbpb, a_i (:,:,jl) , npb, a_i_b (1:nbpb) , jpi, jpj ) |
---|
406 | CALL tab_1d_2d( nbpb, t_su(:,:,jl) , npb, t_su_b (1:nbpb) , jpi, jpj ) |
---|
407 | CALL tab_1d_2d( nbpb, sm_i(:,:,jl) , npb, sm_i_b (1:nbpb) , jpi, jpj ) |
---|
408 | DO jk = 1, nlay_s |
---|
409 | CALL tab_1d_2d( nbpb, t_s(:,:,jk,jl), npb, t_s_b (1:nbpb,jk), jpi, jpj) |
---|
410 | CALL tab_1d_2d( nbpb, e_s(:,:,jk,jl), npb, q_s_b (1:nbpb,jk), jpi, jpj) |
---|
411 | END DO |
---|
412 | DO jk = 1, nlay_i |
---|
413 | CALL tab_1d_2d( nbpb, t_i(:,:,jk,jl), npb, t_i_b (1:nbpb,jk), jpi, jpj) |
---|
414 | CALL tab_1d_2d( nbpb, e_i(:,:,jk,jl), npb, q_i_b (1:nbpb,jk), jpi, jpj) |
---|
415 | CALL tab_1d_2d( nbpb, s_i(:,:,jk,jl), npb, s_i_b (1:nbpb,jk), jpi, jpj) |
---|
416 | END DO |
---|
417 | CALL tab_1d_2d( nbpb, qlead , npb, qlead_1d (1:nbpb) , jpi, jpj ) |
---|
418 | |
---|
419 | CALL tab_1d_2d( nbpb, wfx_snw , npb, wfx_snw_1d(1:nbpb) , jpi, jpj ) |
---|
420 | CALL tab_1d_2d( nbpb, wfx_sub , npb, wfx_sub_1d(1:nbpb) , jpi, jpj ) |
---|
421 | |
---|
422 | CALL tab_1d_2d( nbpb, wfx_bog , npb, wfx_bog_1d(1:nbpb) , jpi, jpj ) |
---|
423 | CALL tab_1d_2d( nbpb, wfx_bom , npb, wfx_bom_1d(1:nbpb) , jpi, jpj ) |
---|
424 | CALL tab_1d_2d( nbpb, wfx_sum , npb, wfx_sum_1d(1:nbpb) , jpi, jpj ) |
---|
425 | CALL tab_1d_2d( nbpb, wfx_sni , npb, wfx_sni_1d(1:nbpb) , jpi, jpj ) |
---|
426 | |
---|
427 | CALL tab_1d_2d( nbpb, sfx_bog , npb, sfx_bog_1d(1:nbpb) , jpi, jpj ) |
---|
428 | CALL tab_1d_2d( nbpb, sfx_bom , npb, sfx_bom_1d(1:nbpb) , jpi, jpj ) |
---|
429 | CALL tab_1d_2d( nbpb, sfx_sum , npb, sfx_sum_1d(1:nbpb) , jpi, jpj ) |
---|
430 | CALL tab_1d_2d( nbpb, sfx_sni , npb, sfx_sni_1d(1:nbpb) , jpi, jpj ) |
---|
431 | ! |
---|
432 | IF( num_sal == 2 ) THEN |
---|
433 | CALL tab_1d_2d( nbpb, sfx_bri , npb, sfx_bri_1d(1:nbpb) , jpi, jpj ) |
---|
434 | ENDIF |
---|
435 | |
---|
436 | CALL tab_1d_2d( nbpb, hfx_thd , npb, hfx_thd_1d(1:nbpb) , jpi, jpj ) |
---|
437 | CALL tab_1d_2d( nbpb, hfx_spr , npb, hfx_spr_1d(1:nbpb) , jpi, jpj ) |
---|
438 | CALL tab_1d_2d( nbpb, hfx_tot , npb, hfx_tot_1d(1:nbpb) , jpi, jpj ) |
---|
439 | CALL tab_1d_2d( nbpb, hfx_snw , npb, hfx_snw_1d(1:nbpb) , jpi, jpj ) |
---|
440 | CALL tab_1d_2d( nbpb, hfx_sub , npb, hfx_sub_1d(1:nbpb) , jpi, jpj ) |
---|
441 | CALL tab_1d_2d( nbpb, hfx_err , npb, hfx_err_1d(1:nbpb) , jpi, jpj ) |
---|
442 | CALL tab_1d_2d( nbpb, hfx_res , npb, hfx_res_1d(1:nbpb) , jpi, jpj ) |
---|
443 | CALL tab_1d_2d( nbpb, hfx_err_rem , npb, hfx_err_rem_1d(1:nbpb) , jpi, jpj ) |
---|
444 | ! |
---|
445 | !+++++ temporary stuff for a dummy version |
---|
446 | CALL tab_1d_2d( nbpb, dh_i_surf2D, npb, dh_i_surf(1:nbpb) , jpi, jpj ) |
---|
447 | CALL tab_1d_2d( nbpb, dh_i_bott2D, npb, dh_i_bott(1:nbpb) , jpi, jpj ) |
---|
448 | CALL tab_1d_2d( nbpb, s_i_newice , npb, s_i_new (1:nbpb) , jpi, jpj ) |
---|
449 | CALL tab_1d_2d( nbpb, izero(:,:,jl) , npb, i0 (1:nbpb) , jpi, jpj ) |
---|
450 | !+++++ |
---|
451 | CALL tab_1d_2d( nbpb, qns_ice(:,:,jl), npb, qns_ice_1d(1:nbpb) , jpi, jpj) |
---|
452 | CALL tab_1d_2d( nbpb, ftr_ice(:,:,jl), npb, ftr_ice_1d(1:nbpb) , jpi, jpj ) |
---|
453 | ! |
---|
454 | IF( lk_mpp ) CALL mpp_comm_free( ncomm_ice ) !RB necessary ?? |
---|
455 | ENDIF |
---|
456 | ! |
---|
457 | END DO |
---|
458 | |
---|
459 | !------------------------------------------------------------------------------! |
---|
460 | ! 5) Global variables, diagnostics |
---|
461 | !------------------------------------------------------------------------------! |
---|
462 | |
---|
463 | !------------------------ |
---|
464 | ! 5.1) Ice heat content |
---|
465 | !------------------------ |
---|
466 | ! Enthalpies are global variables we have to readjust the units (heat content in Joules) |
---|
467 | DO jl = 1, jpl |
---|
468 | DO jk = 1, nlay_i |
---|
469 | e_i(:,:,jk,jl) = e_i(:,:,jk,jl) * area(:,:) * a_i(:,:,jl) * ht_i(:,:,jl) / ( unit_fac * REAL( nlay_i ) ) |
---|
470 | END DO |
---|
471 | END DO |
---|
472 | |
---|
473 | !------------------------ |
---|
474 | ! 5.2) Snow heat content |
---|
475 | !------------------------ |
---|
476 | ! Enthalpies are global variables we have to readjust the units (heat content in Joules) |
---|
477 | DO jl = 1, jpl |
---|
478 | DO jk = 1, nlay_s |
---|
479 | e_s(:,:,jk,jl) = e_s(:,:,jk,jl) * area(:,:) * a_i(:,:,jl) * ht_s(:,:,jl) / ( unit_fac * REAL( nlay_s ) ) |
---|
480 | END DO |
---|
481 | END DO |
---|
482 | |
---|
483 | !---------------------------------- |
---|
484 | ! 5.3) Change thickness to volume |
---|
485 | !---------------------------------- |
---|
486 | CALL lim_var_eqv2glo |
---|
487 | |
---|
488 | !-------------------------------------------- |
---|
489 | ! 5.4) Diagnostic thermodynamic growth rates |
---|
490 | !-------------------------------------------- |
---|
491 | IF(ln_ctl) THEN ! Control print |
---|
492 | CALL prt_ctl_info(' ') |
---|
493 | CALL prt_ctl_info(' - Cell values : ') |
---|
494 | CALL prt_ctl_info(' ~~~~~~~~~~~~~ ') |
---|
495 | CALL prt_ctl(tab2d_1=area , clinfo1=' lim_thd : cell area :') |
---|
496 | CALL prt_ctl(tab2d_1=at_i , clinfo1=' lim_thd : at_i :') |
---|
497 | CALL prt_ctl(tab2d_1=vt_i , clinfo1=' lim_thd : vt_i :') |
---|
498 | CALL prt_ctl(tab2d_1=vt_s , clinfo1=' lim_thd : vt_s :') |
---|
499 | DO jl = 1, jpl |
---|
500 | CALL prt_ctl_info(' ') |
---|
501 | CALL prt_ctl_info(' - Category : ', ivar1=jl) |
---|
502 | CALL prt_ctl_info(' ~~~~~~~~~~') |
---|
503 | CALL prt_ctl(tab2d_1=a_i (:,:,jl) , clinfo1= ' lim_thd : a_i : ') |
---|
504 | CALL prt_ctl(tab2d_1=ht_i (:,:,jl) , clinfo1= ' lim_thd : ht_i : ') |
---|
505 | CALL prt_ctl(tab2d_1=ht_s (:,:,jl) , clinfo1= ' lim_thd : ht_s : ') |
---|
506 | CALL prt_ctl(tab2d_1=v_i (:,:,jl) , clinfo1= ' lim_thd : v_i : ') |
---|
507 | CALL prt_ctl(tab2d_1=v_s (:,:,jl) , clinfo1= ' lim_thd : v_s : ') |
---|
508 | CALL prt_ctl(tab2d_1=e_s (:,:,1,jl) , clinfo1= ' lim_thd : e_s : ') |
---|
509 | CALL prt_ctl(tab2d_1=t_su (:,:,jl) , clinfo1= ' lim_thd : t_su : ') |
---|
510 | CALL prt_ctl(tab2d_1=t_s (:,:,1,jl) , clinfo1= ' lim_thd : t_snow : ') |
---|
511 | CALL prt_ctl(tab2d_1=sm_i (:,:,jl) , clinfo1= ' lim_thd : sm_i : ') |
---|
512 | CALL prt_ctl(tab2d_1=smv_i (:,:,jl) , clinfo1= ' lim_thd : smv_i : ') |
---|
513 | DO jk = 1, nlay_i |
---|
514 | CALL prt_ctl_info(' ') |
---|
515 | CALL prt_ctl_info(' - Layer : ', ivar1=jk) |
---|
516 | CALL prt_ctl_info(' ~~~~~~~') |
---|
517 | CALL prt_ctl(tab2d_1=t_i(:,:,jk,jl) , clinfo1= ' lim_thd : t_i : ') |
---|
518 | CALL prt_ctl(tab2d_1=e_i(:,:,jk,jl) , clinfo1= ' lim_thd : e_i : ') |
---|
519 | END DO |
---|
520 | END DO |
---|
521 | ENDIF |
---|
522 | ! |
---|
523 | ! ------------------------------- |
---|
524 | !- check conservation (C Rousset) |
---|
525 | IF (ln_limdiahsb) THEN |
---|
526 | zchk_fs = glob_sum( ( sfx_bri(:,:) + sfx_bog(:,:) + sfx_bom(:,:) + sfx_sum(:,:) + sfx_sni(:,:) + sfx_opw(:,:) + sfx_res(:,:) + sfx_dyn(:,:) ) * area(:,:) * tms(:,:) ) - zchk_fs_b |
---|
527 | zchk_fw = glob_sum( ( wfx_bog(:,:) + wfx_bom(:,:) + wfx_sum(:,:) + wfx_sni(:,:) + wfx_opw(:,:) + wfx_res(:,:) + wfx_dyn(:,:) + wfx_snw(:,:) ) * area(:,:) * tms(:,:) ) - zchk_fw_b |
---|
528 | zchk_ft = glob_sum( ( hfx_tot(:,:) - hfx_thd(:,:) - hfx_dyn(:,:) - hfx_res(:,:) ) * area(:,:) / unit_fac * tms(:,:) ) - zchk_ft_b |
---|
529 | |
---|
530 | zchk_v_i = ( glob_sum( SUM( v_i(:,:,:)*rhoic + v_s(:,:,:)*rhosn, dim=3 ) * area(:,:) * tms(:,:) ) - zchk_v_i_b ) * r1_rdtice - zchk_fw |
---|
531 | zchk_smv = ( glob_sum( SUM( smv_i(:,:,:), dim=3 ) * area(:,:) * tms(:,:) ) - zchk_smv_b ) * r1_rdtice + ( zchk_fs / rhoic ) |
---|
532 | zchk_e_i = glob_sum( SUM( e_i(:,:,1:nlay_i,:), dim=3 ) + SUM( e_s(:,:,1:nlay_s,:), dim=3 ) ) * r1_rdtice - zchk_e_i_b * r1_rdtice + zchk_ft |
---|
533 | |
---|
534 | zchk_vmin = glob_min(v_i) |
---|
535 | zchk_amax = glob_max(SUM(a_i,dim=3)) |
---|
536 | zchk_amin = glob_min(a_i) |
---|
537 | |
---|
538 | IF(lwp) THEN |
---|
539 | IF ( ABS( zchk_v_i ) > 1.e-4 ) WRITE(numout,*) 'violation volume [kg/day] (limthd) = ',(zchk_v_i * rday) |
---|
540 | IF ( ABS( zchk_smv ) > 1.e-4 ) WRITE(numout,*) 'violation saline [psu*m3/day] (limthd) = ',(zchk_smv * rday) |
---|
541 | IF ( ABS( zchk_e_i ) > 1.e-2 ) WRITE(numout,*) 'violation enthalpy [1e9 J] (limthd) = ',(zchk_e_i) |
---|
542 | IF ( zchk_vmin < 0. ) WRITE(numout,*) 'violation v_i<0 [mm] (limthd) = ',(zchk_vmin * 1.e-3) |
---|
543 | IF ( zchk_amax > amax+epsi10 ) WRITE(numout,*) 'violation a_i>amax (limthd) = ',zchk_amax |
---|
544 | IF ( zchk_amin < 0. ) WRITE(numout,*) 'violation a_i<0 (limthd) = ',zchk_amin |
---|
545 | ENDIF |
---|
546 | ENDIF |
---|
547 | !- check conservation (C Rousset) |
---|
548 | ! ------------------------------- |
---|
549 | ! |
---|
550 | CALL wrk_dealloc( jpij, zdq, zq_ini, zhfx, zqfx ) |
---|
551 | |
---|
552 | IF( nn_timing == 1 ) CALL timing_stop('limthd') |
---|
553 | END SUBROUTINE lim_thd |
---|
554 | |
---|
555 | |
---|
556 | SUBROUTINE lim_thd_enmelt( kideb, kiut ) |
---|
557 | !!----------------------------------------------------------------------- |
---|
558 | !! *** ROUTINE lim_thd_enmelt *** |
---|
559 | !! |
---|
560 | !! ** Purpose : Computes sea ice energy of melting q_i (J.m-3) |
---|
561 | !! |
---|
562 | !! ** Method : Formula (Bitz and Lipscomb, 1999) |
---|
563 | !!------------------------------------------------------------------- |
---|
564 | INTEGER, INTENT(in) :: kideb, kiut ! bounds for the spatial loop |
---|
565 | !! |
---|
566 | INTEGER :: ji, jk ! dummy loop indices |
---|
567 | REAL(wp) :: ztmelts ! local scalar |
---|
568 | !!------------------------------------------------------------------- |
---|
569 | ! |
---|
570 | DO jk = 1, nlay_i ! Sea ice energy of melting |
---|
571 | DO ji = kideb, kiut |
---|
572 | ztmelts = - tmut * s_i_b(ji,jk) + rtt |
---|
573 | q_i_b(ji,jk) = rhoic * ( cpic * ( ztmelts - t_i_b(ji,jk) ) & |
---|
574 | & + lfus * ( 1.0 - (ztmelts-rtt) / MIN( t_i_b(ji,jk)-rtt, -epsi10 ) ) & |
---|
575 | & - rcp * ( ztmelts-rtt ) ) |
---|
576 | END DO |
---|
577 | END DO |
---|
578 | DO jk = 1, nlay_s ! Snow energy of melting |
---|
579 | DO ji = kideb, kiut |
---|
580 | q_s_b(ji,jk) = rhosn * ( cpic * ( rtt - t_s_b(ji,jk) ) + lfus ) |
---|
581 | END DO |
---|
582 | END DO |
---|
583 | ! |
---|
584 | END SUBROUTINE lim_thd_enmelt |
---|
585 | |
---|
586 | |
---|
587 | SUBROUTINE lim_thd_init |
---|
588 | !!----------------------------------------------------------------------- |
---|
589 | !! *** ROUTINE lim_thd_init *** |
---|
590 | !! |
---|
591 | !! ** Purpose : Physical constants and parameters linked to the ice |
---|
592 | !! thermodynamics |
---|
593 | !! |
---|
594 | !! ** Method : Read the namicethd namelist and check the ice-thermo |
---|
595 | !! parameter values called at the first timestep (nit000) |
---|
596 | !! |
---|
597 | !! ** input : Namelist namicether |
---|
598 | !!------------------------------------------------------------------- |
---|
599 | NAMELIST/namicethd/ hmelt , hiccrit, fraz_swi, maxfrazb, vfrazb, Cfrazb, & |
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600 | & hicmin, hiclim, & |
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601 | & sbeta , parlat, hakspl, hibspl, exld, & |
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602 | & hakdif, hnzst , thth , parsub, alphs, betas, & |
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603 | & kappa_i, nconv_i_thd, maxer_i_thd, thcon_i_swi |
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604 | !!------------------------------------------------------------------- |
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605 | ! |
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606 | IF(lwp) THEN |
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607 | WRITE(numout,*) |
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608 | WRITE(numout,*) 'lim_thd : Ice Thermodynamics' |
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609 | WRITE(numout,*) '~~~~~~~' |
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610 | ENDIF |
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611 | ! |
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612 | REWIND( numnam_ice ) ! read Namelist numnam_ice |
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613 | READ ( numnam_ice , namicethd ) |
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614 | ! |
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615 | IF(lwp) THEN ! control print |
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616 | WRITE(numout,*) |
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617 | WRITE(numout,*)' Namelist of ice parameters for ice thermodynamic computation ' |
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618 | WRITE(numout,*)' maximum melting at the bottom hmelt = ', hmelt |
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619 | WRITE(numout,*)' ice thick. for lateral accretion in NH (SH) hiccrit(1/2) = ', hiccrit |
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620 | WRITE(numout,*)' Frazil ice thickness as a function of wind or not fraz_swi = ', fraz_swi |
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621 | WRITE(numout,*)' Maximum proportion of frazil ice collecting at bottom maxfrazb = ', maxfrazb |
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622 | WRITE(numout,*)' Thresold relative drift speed for collection of frazil vfrazb = ', vfrazb |
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623 | WRITE(numout,*)' Squeezing coefficient for collection of frazil Cfrazb = ', Cfrazb |
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624 | WRITE(numout,*)' ice thick. corr. to max. energy stored in brine pocket hicmin = ', hicmin |
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625 | WRITE(numout,*)' minimum ice thickness hiclim = ', hiclim |
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626 | WRITE(numout,*)' numerical carac. of the scheme for diffusion in ice ' |
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627 | WRITE(numout,*)' Cranck-Nicholson (=0.5), implicit (=1), explicit (=0) sbeta = ', sbeta |
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628 | WRITE(numout,*)' percentage of energy used for lateral ablation parlat = ', parlat |
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629 | WRITE(numout,*)' slope of distr. for Hakkinen-Mellor lateral melting hakspl = ', hakspl |
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630 | WRITE(numout,*)' slope of distribution for Hibler lateral melting hibspl = ', hibspl |
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631 | WRITE(numout,*)' exponent for leads-closure rate exld = ', exld |
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632 | WRITE(numout,*)' coefficient for diffusions of ice and snow hakdif = ', hakdif |
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633 | WRITE(numout,*)' threshold thick. for comp. of eq. thermal conductivity zhth = ', thth |
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634 | WRITE(numout,*)' thickness of the surf. layer in temp. computation hnzst = ', hnzst |
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635 | WRITE(numout,*)' switch for snow sublimation (=1) or not (=0) parsub = ', parsub |
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636 | WRITE(numout,*)' coefficient for snow density when snow ice formation alphs = ', alphs |
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637 | WRITE(numout,*)' coefficient for ice-lead partition of snowfall betas = ', betas |
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638 | WRITE(numout,*)' extinction radiation parameter in sea ice (1.0) kappa_i = ', kappa_i |
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639 | WRITE(numout,*)' maximal n. of iter. for heat diffusion computation nconv_i_thd = ', nconv_i_thd |
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640 | WRITE(numout,*)' maximal err. on T for heat diffusion computation maxer_i_thd = ', maxer_i_thd |
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641 | WRITE(numout,*)' switch for comp. of thermal conductivity in the ice thcon_i_swi = ', thcon_i_swi |
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642 | WRITE(numout,*)' check heat conservation in the ice/snow con_i = ', con_i |
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643 | ENDIF |
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644 | ! |
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645 | rcdsn = hakdif * rcdsn |
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646 | rcdic = hakdif * rcdic |
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647 | ! |
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648 | END SUBROUTINE lim_thd_init |
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649 | |
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650 | #else |
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651 | !!---------------------------------------------------------------------- |
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652 | !! Default option Dummy module NO LIM3 sea-ice model |
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653 | !!---------------------------------------------------------------------- |
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654 | #endif |
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655 | |
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656 | !!====================================================================== |
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657 | END MODULE limthd |
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