1 | MODULE limthd_dif |
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2 | !!====================================================================== |
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3 | !! *** MODULE limthd_dif *** |
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4 | !! heat diffusion in sea ice |
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5 | !! computation of surface and inner T |
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6 | !!====================================================================== |
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7 | !! History : LIM ! 02-2003 (M. Vancoppenolle) original 1D code |
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8 | !! ! 06-2005 (M. Vancoppenolle) 3d version |
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9 | !! ! 11-2006 (X Fettweis) Vectorization by Xavier |
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10 | !! ! 04-2007 (M. Vancoppenolle) Energy conservation |
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11 | !! 4.0 ! 2011-02 (G. Madec) dynamical allocation |
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12 | !! - ! 2012-05 (C. Rousset) add penetration solar flux |
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13 | !!---------------------------------------------------------------------- |
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14 | #if defined key_lim3 |
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15 | !!---------------------------------------------------------------------- |
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16 | !! 'key_lim3' LIM3 sea-ice model |
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17 | !!---------------------------------------------------------------------- |
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18 | USE par_oce ! ocean parameters |
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19 | USE phycst ! physical constants (ocean directory) |
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20 | USE ice ! LIM-3 variables |
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21 | USE par_ice ! LIM-3 parameters |
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22 | USE thd_ice ! LIM-3: thermodynamics |
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23 | USE in_out_manager ! I/O manager |
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24 | USE lib_mpp ! MPP library |
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25 | USE wrk_nemo ! work arrays |
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26 | USE lib_fortran ! Fortran utilities (allows no signed zero when 'key_nosignedzero' defined) |
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27 | USE cpl_oasis3, ONLY : lk_cpl |
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28 | |
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29 | IMPLICIT NONE |
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30 | PRIVATE |
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31 | |
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32 | PUBLIC lim_thd_dif ! called by lim_thd |
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33 | |
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34 | REAL(wp) :: epsi10 = 1.e-10_wp ! |
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35 | !!---------------------------------------------------------------------- |
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36 | !! NEMO/LIM3 4.0 , UCL - NEMO Consortium (2011) |
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37 | !! $Id$ |
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38 | !! Software governed by the CeCILL licence (NEMOGCM/NEMO_CeCILL.txt) |
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39 | !!---------------------------------------------------------------------- |
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40 | CONTAINS |
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41 | |
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42 | SUBROUTINE lim_thd_dif( kideb , kiut ) |
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43 | !!------------------------------------------------------------------ |
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44 | !! *** ROUTINE lim_thd_dif *** |
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45 | !! ** Purpose : |
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46 | !! This routine determines the time evolution of snow and sea-ice |
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47 | !! temperature profiles. |
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48 | !! ** Method : |
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49 | !! This is done by solving the heat equation diffusion with |
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50 | !! a Neumann boundary condition at the surface and a Dirichlet one |
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51 | !! at the bottom. Solar radiation is partially absorbed into the ice. |
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52 | !! The specific heat and thermal conductivities depend on ice salinity |
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53 | !! and temperature to take into account brine pocket melting. The |
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54 | !! numerical |
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55 | !! scheme is an iterative Crank-Nicolson on a non-uniform multilayer grid |
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56 | !! in the ice and snow system. |
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57 | !! |
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58 | !! The successive steps of this routine are |
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59 | !! 1. Thermal conductivity at the interfaces of the ice layers |
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60 | !! 2. Internal absorbed radiation |
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61 | !! 3. Scale factors due to non-uniform grid |
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62 | !! 4. Kappa factors |
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63 | !! Then iterative procedure begins |
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64 | !! 5. specific heat in the ice |
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65 | !! 6. eta factors |
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66 | !! 7. surface flux computation |
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67 | !! 8. tridiagonal system terms |
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68 | !! 9. solving the tridiagonal system with Gauss elimination |
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69 | !! Iterative procedure ends according to a criterion on evolution |
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70 | !! of temperature |
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71 | !! |
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72 | !! ** Arguments : |
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73 | !! kideb , kiut : Starting and ending points on which the |
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74 | !! the computation is applied |
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75 | !! |
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76 | !! ** Inputs / Ouputs : (global commons) |
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77 | !! surface temperature : t_su_b |
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78 | !! ice/snow temperatures : t_i_b, t_s_b |
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79 | !! ice salinities : s_i_b |
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80 | !! number of layers in the ice/snow: nlay_i, nlay_s |
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81 | !! profile of the ice/snow layers : z_i, z_s |
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82 | !! total ice/snow thickness : ht_i_b, ht_s_b |
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83 | !! |
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84 | !! ** External : |
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85 | !! |
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86 | !! ** References : |
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87 | !! |
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88 | !! ** History : |
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89 | !! (02-2003) Martin Vancoppenolle, Louvain-la-Neuve, Belgium |
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90 | !! (06-2005) Martin Vancoppenolle, 3d version |
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91 | !! (11-2006) Vectorized by Xavier Fettweis (UCL-ASTR) |
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92 | !! (04-2007) Energy conservation tested by M. Vancoppenolle |
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93 | !!------------------------------------------------------------------ |
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94 | INTEGER , INTENT(in) :: kideb, kiut ! Start/End point on which the the computation is applied |
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95 | |
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96 | !! * Local variables |
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97 | INTEGER :: ji ! spatial loop index |
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98 | INTEGER :: ii, ij ! temporary dummy loop index |
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99 | INTEGER :: numeq ! current reference number of equation |
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100 | INTEGER :: layer ! vertical dummy loop index |
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101 | INTEGER :: nconv ! number of iterations in iterative procedure |
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102 | INTEGER :: minnumeqmin, maxnumeqmax |
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103 | INTEGER, POINTER, DIMENSION(:) :: numeqmin ! reference number of top equation |
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104 | INTEGER, POINTER, DIMENSION(:) :: numeqmax ! reference number of bottom equation |
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105 | INTEGER, POINTER, DIMENSION(:) :: isnow ! switch for presence (1) or absence (0) of snow |
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106 | REAL(wp) :: zg1s = 2._wp ! for the tridiagonal system |
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107 | REAL(wp) :: zg1 = 2._wp ! |
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108 | REAL(wp) :: zgamma = 18009._wp ! for specific heat |
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109 | REAL(wp) :: zbeta = 0.117_wp ! for thermal conductivity (could be 0.13) |
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110 | REAL(wp) :: zraext_s = 1.e+8_wp ! extinction coefficient of radiation in the snow |
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111 | REAL(wp) :: zkimin = 0.10_wp ! minimum ice thermal conductivity |
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112 | REAL(wp) :: ztsu_err = 1.e-5_wp ! range around which t_su is considered as 0°C |
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113 | REAL(wp) :: ztmelt_i ! ice melting temperature |
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114 | REAL(wp) :: zerritmax ! current maximal error on temperature |
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115 | REAL(wp), POINTER, DIMENSION(:) :: ztfs ! ice melting point |
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116 | REAL(wp), POINTER, DIMENSION(:) :: ztsuold ! old surface temperature (before the iterative procedure ) |
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117 | REAL(wp), POINTER, DIMENSION(:) :: ztsuoldit ! surface temperature at previous iteration |
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118 | REAL(wp), POINTER, DIMENSION(:) :: zh_i ! ice layer thickness |
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119 | REAL(wp), POINTER, DIMENSION(:) :: zh_s ! snow layer thickness |
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120 | REAL(wp), POINTER, DIMENSION(:) :: zfsw ! solar radiation absorbed at the surface |
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121 | REAL(wp), POINTER, DIMENSION(:) :: zf ! surface flux function |
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122 | REAL(wp), POINTER, DIMENSION(:) :: dzf ! derivative of the surface flux function |
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123 | REAL(wp), POINTER, DIMENSION(:) :: zerrit ! current error on temperature |
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124 | REAL(wp), POINTER, DIMENSION(:) :: zdifcase ! case of the equation resolution (1->4) |
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125 | REAL(wp), POINTER, DIMENSION(:) :: zftrice ! solar radiation transmitted through the ice |
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126 | REAL(wp), POINTER, DIMENSION(:) :: zihic, zhsu |
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127 | REAL(wp), POINTER, DIMENSION(:,:) :: ztcond_i ! Ice thermal conductivity |
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128 | REAL(wp), POINTER, DIMENSION(:,:) :: zradtr_i ! Radiation transmitted through the ice |
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129 | REAL(wp), POINTER, DIMENSION(:,:) :: zradab_i ! Radiation absorbed in the ice |
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130 | REAL(wp), POINTER, DIMENSION(:,:) :: zkappa_i ! Kappa factor in the ice |
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131 | REAL(wp), POINTER, DIMENSION(:,:) :: ztiold ! Old temperature in the ice |
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132 | REAL(wp), POINTER, DIMENSION(:,:) :: zeta_i ! Eta factor in the ice |
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133 | REAL(wp), POINTER, DIMENSION(:,:) :: ztitemp ! Temporary temperature in the ice to check the convergence |
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134 | REAL(wp), POINTER, DIMENSION(:,:) :: zspeche_i ! Ice specific heat |
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135 | REAL(wp), POINTER, DIMENSION(:,:) :: z_i ! Vertical cotes of the layers in the ice |
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136 | REAL(wp), POINTER, DIMENSION(:,:) :: zradtr_s ! Radiation transmited through the snow |
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137 | REAL(wp), POINTER, DIMENSION(:,:) :: zradab_s ! Radiation absorbed in the snow |
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138 | REAL(wp), POINTER, DIMENSION(:,:) :: zkappa_s ! Kappa factor in the snow |
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139 | REAL(wp), POINTER, DIMENSION(:,:) :: zeta_s ! Eta factor in the snow |
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140 | REAL(wp), POINTER, DIMENSION(:,:) :: ztstemp ! Temporary temperature in the snow to check the convergence |
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141 | REAL(wp), POINTER, DIMENSION(:,:) :: ztsold ! Temporary temperature in the snow |
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142 | REAL(wp), POINTER, DIMENSION(:,:) :: z_s ! Vertical cotes of the layers in the snow |
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143 | REAL(wp), POINTER, DIMENSION(:,:) :: zindterm ! Independent term |
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144 | REAL(wp), POINTER, DIMENSION(:,:) :: zindtbis ! temporary independent term |
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145 | REAL(wp), POINTER, DIMENSION(:,:) :: zdiagbis |
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146 | REAL(wp), POINTER, DIMENSION(:,:,:) :: ztrid ! tridiagonal system terms |
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147 | ! diag errors on heat |
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148 | REAL(wp), POINTER, DIMENSION(:) :: zdq, zq_ini |
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149 | REAL(wp) :: zhfx_err |
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150 | !!------------------------------------------------------------------ |
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151 | ! |
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152 | CALL wrk_alloc( jpij, numeqmin, numeqmax, isnow ) |
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153 | CALL wrk_alloc( jpij, ztfs, ztsuold, ztsuoldit, zh_i, zh_s, zfsw ) |
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154 | CALL wrk_alloc( jpij, zf, dzf, zerrit, zdifcase, zftrice, zihic, zhsu ) |
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155 | CALL wrk_alloc( jpij, nlay_i+1, ztcond_i, zradtr_i, zradab_i, zkappa_i, ztiold, zeta_i, ztitemp, z_i, zspeche_i, kjstart=0) |
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156 | CALL wrk_alloc( jpij, nlay_s+1, zradtr_s, zradab_s, zkappa_s, ztsold, zeta_s, ztstemp, z_s, kjstart=0) |
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157 | CALL wrk_alloc( jpij, jkmax+2, zindterm, zindtbis, zdiagbis ) |
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158 | CALL wrk_alloc( jpij, jkmax+2, 3, ztrid ) |
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159 | |
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160 | CALL wrk_alloc( jpij, zdq, zq_ini ) |
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161 | |
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162 | ! --- diag error on heat diffusion - PART 1 --- ! |
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163 | zdq(:) = 0._wp ; zq_ini(:) = 0._wp |
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164 | DO ji = kideb, kiut |
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165 | zq_ini(ji) = ( SUM( q_i_b(ji,1:nlay_i) ) * ht_i_b(ji) / REAL( nlay_i ) + & |
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166 | & SUM( q_s_b(ji,1:nlay_s) ) * ht_s_b(ji) / REAL( nlay_s ) ) |
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167 | END DO |
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168 | |
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169 | !------------------------------------------------------------------------------! |
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170 | ! 1) Initialization ! |
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171 | !------------------------------------------------------------------------------! |
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172 | ! clem clean: replace just ztfs by rtt |
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173 | DO ji = kideb , kiut |
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174 | ! is there snow or not |
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175 | isnow(ji)= NINT( 1._wp - MAX( 0._wp , SIGN(1._wp, - ht_s_b(ji) ) ) ) |
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176 | ! surface temperature of fusion |
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177 | ztfs(ji) = REAL( isnow(ji) ) * rtt + REAL( 1 - isnow(ji) ) * rtt |
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178 | ! layer thickness |
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179 | zh_i(ji) = ht_i_b(ji) / REAL( nlay_i ) |
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180 | zh_s(ji) = ht_s_b(ji) / REAL( nlay_s ) |
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181 | END DO |
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182 | |
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183 | !-------------------- |
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184 | ! Ice / snow layers |
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185 | !-------------------- |
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186 | |
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187 | z_s(:,0) = 0._wp ! vert. coord. of the up. lim. of the 1st snow layer |
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188 | z_i(:,0) = 0._wp ! vert. coord. of the up. lim. of the 1st ice layer |
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189 | |
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190 | DO layer = 1, nlay_s ! vert. coord of the up. lim. of the layer-th snow layer |
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191 | DO ji = kideb , kiut |
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192 | z_s(ji,layer) = z_s(ji,layer-1) + ht_s_b(ji) / REAL( nlay_s ) |
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193 | END DO |
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194 | END DO |
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195 | |
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196 | DO layer = 1, nlay_i ! vert. coord of the up. lim. of the layer-th ice layer |
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197 | DO ji = kideb , kiut |
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198 | z_i(ji,layer) = z_i(ji,layer-1) + ht_i_b(ji) / REAL( nlay_i ) |
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199 | END DO |
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200 | END DO |
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201 | ! |
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202 | !------------------------------------------------------------------------------| |
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203 | ! 2) Radiations | |
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204 | !------------------------------------------------------------------------------| |
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205 | ! |
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206 | !------------------- |
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207 | ! Computation of i0 |
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208 | !------------------- |
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209 | ! i0 describes the fraction of solar radiation which does not contribute |
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210 | ! to the surface energy budget but rather penetrates inside the ice. |
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211 | ! We assume that no radiation is transmitted through the snow |
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212 | ! If there is no no snow |
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213 | ! zfsw = (1-i0).qsr_ice is absorbed at the surface |
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214 | ! zftrice = io.qsr_ice is below the surface |
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215 | ! ftr_ice = io.qsr_ice.exp(-k(h_i)) transmitted below the ice |
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216 | |
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217 | DO ji = kideb , kiut |
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218 | ! switches |
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219 | isnow(ji) = NINT( 1._wp - MAX( 0._wp , SIGN( 1._wp , - ht_s_b(ji) ) ) ) |
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220 | ! hs > 0, isnow = 1 |
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221 | zhsu (ji) = hnzst ! threshold for the computation of i0 |
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222 | zihic(ji) = MAX( 0._wp , 1._wp - ( ht_i_b(ji) / zhsu(ji) ) ) |
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223 | |
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224 | i0(ji) = REAL( 1 - isnow(ji) ) * ( fr1_i0_1d(ji) + zihic(ji) * fr2_i0_1d(ji) ) |
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225 | !fr1_i0_1d = i0 for a thin ice surface |
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226 | !fr1_i0_2d = i0 for a thick ice surface |
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227 | ! a function of the cloud cover |
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228 | ! |
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229 | !i0(ji) = (1.0-FLOAT(isnow(ji)))*3.0/(100*ht_s_b(ji)+10.0) |
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230 | !formula used in Cice |
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231 | END DO |
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232 | |
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233 | !------------------------------------------------------- |
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234 | ! Solar radiation absorbed / transmitted at the surface |
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235 | ! Derivative of the non solar flux |
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236 | !------------------------------------------------------- |
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237 | DO ji = kideb , kiut |
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238 | zfsw (ji) = qsr_ice_1d(ji) * ( 1 - i0(ji) ) ! Shortwave radiation absorbed at surface |
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239 | zftrice(ji) = qsr_ice_1d(ji) * i0(ji) ! Solar radiation transmitted below the surface layer |
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240 | dzf (ji) = dqns_ice_1d(ji) ! derivative of incoming nonsolar flux |
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241 | END DO |
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242 | |
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243 | !--------------------------------------------------------- |
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244 | ! Transmission - absorption of solar radiation in the ice |
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245 | !--------------------------------------------------------- |
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246 | |
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247 | DO ji = kideb, kiut ! snow initialization |
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248 | zradtr_s(ji,0) = zftrice(ji) ! radiation penetrating through snow |
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249 | END DO |
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250 | |
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251 | DO layer = 1, nlay_s ! Radiation through snow |
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252 | DO ji = kideb, kiut |
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253 | ! ! radiation transmitted below the layer-th snow layer |
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254 | zradtr_s(ji,layer) = zradtr_s(ji,0) * EXP( - zraext_s * ( MAX ( 0._wp , z_s(ji,layer) ) ) ) |
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255 | ! ! radiation absorbed by the layer-th snow layer |
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256 | zradab_s(ji,layer) = zradtr_s(ji,layer-1) - zradtr_s(ji,layer) |
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257 | END DO |
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258 | END DO |
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259 | |
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260 | DO ji = kideb, kiut ! ice initialization |
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261 | zradtr_i(ji,0) = zradtr_s(ji,nlay_s) * REAL( isnow(ji) ) + zftrice(ji) * REAL( 1 - isnow(ji) ) |
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262 | END DO |
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263 | |
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264 | DO layer = 1, nlay_i ! Radiation through ice |
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265 | DO ji = kideb, kiut |
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266 | ! ! radiation transmitted below the layer-th ice layer |
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267 | zradtr_i(ji,layer) = zradtr_i(ji,0) * EXP( - kappa_i * ( MAX ( 0._wp , z_i(ji,layer) ) ) ) |
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268 | ! ! radiation absorbed by the layer-th ice layer |
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269 | zradab_i(ji,layer) = zradtr_i(ji,layer-1) - zradtr_i(ji,layer) |
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270 | END DO |
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271 | END DO |
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272 | |
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273 | DO ji = kideb, kiut ! Radiation transmitted below the ice |
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274 | !!!ftr_ice_1d(ji) = ftr_ice_1d(ji) + iatte_1d(ji) * zradtr_i(ji,nlay_i) * a_i_b(ji) / at_i_b(ji) ! clem modif |
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275 | ftr_ice_1d(ji) = zradtr_i(ji,nlay_i) |
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276 | END DO |
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277 | |
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278 | ! |
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279 | !------------------------------------------------------------------------------| |
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280 | ! 3) Iterative procedure begins | |
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281 | !------------------------------------------------------------------------------| |
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282 | ! |
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283 | DO ji = kideb, kiut ! Old surface temperature |
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284 | ztsuold (ji) = t_su_b(ji) ! temperature at the beg of iter pr. |
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285 | ztsuoldit(ji) = t_su_b(ji) ! temperature at the previous iter |
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286 | t_su_b (ji) = MIN( t_su_b(ji), ztfs(ji) - ztsu_err ) ! necessary |
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287 | zerrit (ji) = 1000._wp ! initial value of error |
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288 | END DO |
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289 | |
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290 | DO layer = 1, nlay_s ! Old snow temperature |
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291 | DO ji = kideb , kiut |
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292 | ztsold(ji,layer) = t_s_b(ji,layer) |
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293 | END DO |
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294 | END DO |
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295 | |
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296 | DO layer = 1, nlay_i ! Old ice temperature |
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297 | DO ji = kideb , kiut |
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298 | ztiold(ji,layer) = t_i_b(ji,layer) |
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299 | END DO |
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300 | END DO |
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301 | |
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302 | nconv = 0 ! number of iterations |
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303 | zerritmax = 1000._wp ! maximal value of error on all points |
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304 | |
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305 | DO WHILE ( zerritmax > maxer_i_thd .AND. nconv < nconv_i_thd ) |
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306 | ! |
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307 | nconv = nconv + 1 |
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308 | ! |
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309 | !------------------------------------------------------------------------------| |
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310 | ! 4) Sea ice thermal conductivity | |
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311 | !------------------------------------------------------------------------------| |
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312 | ! |
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313 | IF( thcon_i_swi == 0 ) THEN ! Untersteiner (1964) formula |
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314 | DO ji = kideb , kiut |
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315 | ztcond_i(ji,0) = rcdic + zbeta*s_i_b(ji,1) / MIN(-epsi10,t_i_b(ji,1)-rtt) |
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316 | ztcond_i(ji,0) = MAX(ztcond_i(ji,0),zkimin) |
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317 | END DO |
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318 | DO layer = 1, nlay_i-1 |
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319 | DO ji = kideb , kiut |
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320 | ztcond_i(ji,layer) = rcdic + zbeta*( s_i_b(ji,layer) + s_i_b(ji,layer+1) ) / & |
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321 | MIN(-2.0_wp * epsi10, t_i_b(ji,layer)+t_i_b(ji,layer+1) - 2.0_wp * rtt) |
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322 | ztcond_i(ji,layer) = MAX(ztcond_i(ji,layer),zkimin) |
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323 | END DO |
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324 | END DO |
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325 | ENDIF |
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326 | |
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327 | IF( thcon_i_swi == 1 ) THEN ! Pringle et al formula included: 2.11 + 0.09 S/T - 0.011.T |
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328 | DO ji = kideb , kiut |
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329 | ztcond_i(ji,0) = rcdic + 0.090_wp * s_i_b(ji,1) / MIN( -epsi10, t_i_b(ji,1)-rtt ) & |
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330 | & - 0.011_wp * ( t_i_b(ji,1) - rtt ) |
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331 | ztcond_i(ji,0) = MAX( ztcond_i(ji,0), zkimin ) |
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332 | END DO |
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333 | DO layer = 1, nlay_i-1 |
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334 | DO ji = kideb , kiut |
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335 | ztcond_i(ji,layer) = rcdic + 0.090_wp * ( s_i_b(ji,layer) + s_i_b(ji,layer+1) ) & |
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336 | & / MIN(-2.0_wp * epsi10, t_i_b(ji,layer)+t_i_b(ji,layer+1) - 2.0_wp * rtt) & |
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337 | & - 0.0055_wp* ( t_i_b(ji,layer) + t_i_b(ji,layer+1) - 2.0*rtt ) |
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338 | ztcond_i(ji,layer) = MAX( ztcond_i(ji,layer), zkimin ) |
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339 | END DO |
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340 | END DO |
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341 | DO ji = kideb , kiut |
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342 | ztcond_i(ji,nlay_i) = rcdic + 0.090_wp * s_i_b(ji,nlay_i) / MIN(-epsi10,t_bo_b(ji)-rtt) & |
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343 | & - 0.011_wp * ( t_bo_b(ji) - rtt ) |
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344 | ztcond_i(ji,nlay_i) = MAX( ztcond_i(ji,nlay_i), zkimin ) |
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345 | END DO |
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346 | ENDIF |
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347 | ! |
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348 | !------------------------------------------------------------------------------| |
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349 | ! 5) kappa factors | |
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350 | !------------------------------------------------------------------------------| |
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351 | ! |
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352 | DO ji = kideb, kiut |
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353 | |
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354 | !-- Snow kappa factors |
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355 | zkappa_s(ji,0) = rcdsn / MAX(epsi10,zh_s(ji)) |
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356 | zkappa_s(ji,nlay_s) = rcdsn / MAX(epsi10,zh_s(ji)) |
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357 | END DO |
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358 | |
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359 | DO layer = 1, nlay_s-1 |
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360 | DO ji = kideb , kiut |
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361 | zkappa_s(ji,layer) = 2.0 * rcdsn / & |
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362 | MAX(epsi10,2.0*zh_s(ji)) |
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363 | END DO |
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364 | END DO |
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365 | |
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366 | DO layer = 1, nlay_i-1 |
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367 | DO ji = kideb , kiut |
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368 | !-- Ice kappa factors |
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369 | zkappa_i(ji,layer) = 2.0*ztcond_i(ji,layer)/ & |
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370 | MAX(epsi10,2.0*zh_i(ji)) |
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371 | END DO |
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372 | END DO |
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373 | |
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374 | DO ji = kideb , kiut |
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375 | zkappa_i(ji,0) = ztcond_i(ji,0)/MAX(epsi10,zh_i(ji)) |
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376 | zkappa_i(ji,nlay_i) = ztcond_i(ji,nlay_i) / MAX(epsi10,zh_i(ji)) |
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377 | !-- Interface |
---|
378 | zkappa_s(ji,nlay_s) = 2.0*rcdsn*ztcond_i(ji,0)/MAX(epsi10, & |
---|
379 | (ztcond_i(ji,0)*zh_s(ji) + rcdsn*zh_i(ji))) |
---|
380 | zkappa_i(ji,0) = zkappa_s(ji,nlay_s)*REAL( isnow(ji) ) & |
---|
381 | + zkappa_i(ji,0)*REAL( 1 - isnow(ji) ) |
---|
382 | END DO |
---|
383 | ! |
---|
384 | !------------------------------------------------------------------------------| |
---|
385 | ! 6) Sea ice specific heat, eta factors | |
---|
386 | !------------------------------------------------------------------------------| |
---|
387 | ! |
---|
388 | DO layer = 1, nlay_i |
---|
389 | DO ji = kideb , kiut |
---|
390 | ztitemp(ji,layer) = t_i_b(ji,layer) |
---|
391 | zspeche_i(ji,layer) = cpic + zgamma*s_i_b(ji,layer)/ & |
---|
392 | MAX((t_i_b(ji,layer)-rtt)*(ztiold(ji,layer)-rtt),epsi10) |
---|
393 | zeta_i(ji,layer) = rdt_ice / MAX(rhoic*zspeche_i(ji,layer)*zh_i(ji), & |
---|
394 | epsi10) |
---|
395 | END DO |
---|
396 | END DO |
---|
397 | |
---|
398 | DO layer = 1, nlay_s |
---|
399 | DO ji = kideb , kiut |
---|
400 | ztstemp(ji,layer) = t_s_b(ji,layer) |
---|
401 | zeta_s(ji,layer) = rdt_ice / MAX(rhosn*cpic*zh_s(ji),epsi10) |
---|
402 | END DO |
---|
403 | END DO |
---|
404 | ! |
---|
405 | !------------------------------------------------------------------------------| |
---|
406 | ! 7) surface flux computation | |
---|
407 | !------------------------------------------------------------------------------| |
---|
408 | ! |
---|
409 | DO ji = kideb , kiut |
---|
410 | ! update of the non solar flux according to the update in T_su |
---|
411 | qns_ice_1d(ji) = qns_ice_1d(ji) + dqns_ice_1d(ji) * ( t_su_b(ji) - ztsuoldit(ji) ) |
---|
412 | |
---|
413 | ! update incoming flux |
---|
414 | zf(ji) = zfsw(ji) & ! net absorbed solar radiation |
---|
415 | + qns_ice_1d(ji) ! non solar total flux |
---|
416 | ! (LWup, LWdw, SH, LH) |
---|
417 | END DO |
---|
418 | |
---|
419 | ! |
---|
420 | !------------------------------------------------------------------------------| |
---|
421 | ! 8) tridiagonal system terms | |
---|
422 | !------------------------------------------------------------------------------| |
---|
423 | ! |
---|
424 | !!layer denotes the number of the layer in the snow or in the ice |
---|
425 | !!numeq denotes the reference number of the equation in the tridiagonal |
---|
426 | !!system, terms of tridiagonal system are indexed as following : |
---|
427 | !!1 is subdiagonal term, 2 is diagonal and 3 is superdiagonal one |
---|
428 | |
---|
429 | !!ice interior terms (top equation has the same form as the others) |
---|
430 | |
---|
431 | DO numeq=1,jkmax+2 |
---|
432 | DO ji = kideb , kiut |
---|
433 | ztrid(ji,numeq,1) = 0. |
---|
434 | ztrid(ji,numeq,2) = 0. |
---|
435 | ztrid(ji,numeq,3) = 0. |
---|
436 | zindterm(ji,numeq)= 0. |
---|
437 | zindtbis(ji,numeq)= 0. |
---|
438 | zdiagbis(ji,numeq)= 0. |
---|
439 | ENDDO |
---|
440 | ENDDO |
---|
441 | |
---|
442 | DO numeq = nlay_s + 2, nlay_s + nlay_i |
---|
443 | DO ji = kideb , kiut |
---|
444 | layer = numeq - nlay_s - 1 |
---|
445 | ztrid(ji,numeq,1) = - zeta_i(ji,layer)*zkappa_i(ji,layer-1) |
---|
446 | ztrid(ji,numeq,2) = 1.0 + zeta_i(ji,layer)*(zkappa_i(ji,layer-1) + & |
---|
447 | zkappa_i(ji,layer)) |
---|
448 | ztrid(ji,numeq,3) = - zeta_i(ji,layer)*zkappa_i(ji,layer) |
---|
449 | zindterm(ji,numeq) = ztiold(ji,layer) + zeta_i(ji,layer)* & |
---|
450 | zradab_i(ji,layer) |
---|
451 | END DO |
---|
452 | ENDDO |
---|
453 | |
---|
454 | numeq = nlay_s + nlay_i + 1 |
---|
455 | DO ji = kideb , kiut |
---|
456 | !!ice bottom term |
---|
457 | ztrid(ji,numeq,1) = - zeta_i(ji,nlay_i)*zkappa_i(ji,nlay_i-1) |
---|
458 | ztrid(ji,numeq,2) = 1.0 + zeta_i(ji,nlay_i)*( zkappa_i(ji,nlay_i)*zg1 & |
---|
459 | + zkappa_i(ji,nlay_i-1) ) |
---|
460 | ztrid(ji,numeq,3) = 0.0 |
---|
461 | zindterm(ji,numeq) = ztiold(ji,nlay_i) + zeta_i(ji,nlay_i)* & |
---|
462 | ( zradab_i(ji,nlay_i) + zkappa_i(ji,nlay_i)*zg1 & |
---|
463 | * t_bo_b(ji) ) |
---|
464 | ENDDO |
---|
465 | |
---|
466 | |
---|
467 | DO ji = kideb , kiut |
---|
468 | IF ( ht_s_b(ji).gt.0.0 ) THEN |
---|
469 | ! |
---|
470 | !------------------------------------------------------------------------------| |
---|
471 | ! snow-covered cells | |
---|
472 | !------------------------------------------------------------------------------| |
---|
473 | ! |
---|
474 | !!snow interior terms (bottom equation has the same form as the others) |
---|
475 | DO numeq = 3, nlay_s + 1 |
---|
476 | layer = numeq - 1 |
---|
477 | ztrid(ji,numeq,1) = - zeta_s(ji,layer)*zkappa_s(ji,layer-1) |
---|
478 | ztrid(ji,numeq,2) = 1.0 + zeta_s(ji,layer)*( zkappa_s(ji,layer-1) + & |
---|
479 | zkappa_s(ji,layer) ) |
---|
480 | ztrid(ji,numeq,3) = - zeta_s(ji,layer)*zkappa_s(ji,layer) |
---|
481 | zindterm(ji,numeq) = ztsold(ji,layer) + zeta_s(ji,layer)* & |
---|
482 | zradab_s(ji,layer) |
---|
483 | END DO |
---|
484 | |
---|
485 | !!case of only one layer in the ice (ice equation is altered) |
---|
486 | IF ( nlay_i.eq.1 ) THEN |
---|
487 | ztrid(ji,nlay_s+2,3) = 0.0 |
---|
488 | zindterm(ji,nlay_s+2) = zindterm(ji,nlay_s+2) + zkappa_i(ji,1)* & |
---|
489 | t_bo_b(ji) |
---|
490 | ENDIF |
---|
491 | |
---|
492 | IF ( t_su_b(ji) .LT. rtt ) THEN |
---|
493 | |
---|
494 | !------------------------------------------------------------------------------| |
---|
495 | ! case 1 : no surface melting - snow present | |
---|
496 | !------------------------------------------------------------------------------| |
---|
497 | zdifcase(ji) = 1.0 |
---|
498 | numeqmin(ji) = 1 |
---|
499 | numeqmax(ji) = nlay_i + nlay_s + 1 |
---|
500 | |
---|
501 | !!surface equation |
---|
502 | ztrid(ji,1,1) = 0.0 |
---|
503 | ztrid(ji,1,2) = dzf(ji) - zg1s*zkappa_s(ji,0) |
---|
504 | ztrid(ji,1,3) = zg1s*zkappa_s(ji,0) |
---|
505 | zindterm(ji,1) = dzf(ji)*t_su_b(ji) - zf(ji) |
---|
506 | |
---|
507 | !!first layer of snow equation |
---|
508 | ztrid(ji,2,1) = - zkappa_s(ji,0)*zg1s*zeta_s(ji,1) |
---|
509 | ztrid(ji,2,2) = 1.0 + zeta_s(ji,1)*(zkappa_s(ji,1) + zkappa_s(ji,0)*zg1s) |
---|
510 | ztrid(ji,2,3) = - zeta_s(ji,1)* zkappa_s(ji,1) |
---|
511 | zindterm(ji,2) = ztsold(ji,1) + zeta_s(ji,1)*zradab_s(ji,1) |
---|
512 | |
---|
513 | ELSE |
---|
514 | ! |
---|
515 | !------------------------------------------------------------------------------| |
---|
516 | ! case 2 : surface is melting - snow present | |
---|
517 | !------------------------------------------------------------------------------| |
---|
518 | ! |
---|
519 | zdifcase(ji) = 2.0 |
---|
520 | numeqmin(ji) = 2 |
---|
521 | numeqmax(ji) = nlay_i + nlay_s + 1 |
---|
522 | |
---|
523 | !!first layer of snow equation |
---|
524 | ztrid(ji,2,1) = 0.0 |
---|
525 | ztrid(ji,2,2) = 1.0 + zeta_s(ji,1) * ( zkappa_s(ji,1) + & |
---|
526 | zkappa_s(ji,0) * zg1s ) |
---|
527 | ztrid(ji,2,3) = - zeta_s(ji,1)*zkappa_s(ji,1) |
---|
528 | zindterm(ji,2) = ztsold(ji,1) + zeta_s(ji,1) * & |
---|
529 | ( zradab_s(ji,1) + & |
---|
530 | zkappa_s(ji,0) * zg1s * t_su_b(ji) ) |
---|
531 | ENDIF |
---|
532 | ELSE |
---|
533 | ! |
---|
534 | !------------------------------------------------------------------------------| |
---|
535 | ! cells without snow | |
---|
536 | !------------------------------------------------------------------------------| |
---|
537 | ! |
---|
538 | IF (t_su_b(ji) .LT. rtt) THEN |
---|
539 | ! |
---|
540 | !------------------------------------------------------------------------------| |
---|
541 | ! case 3 : no surface melting - no snow | |
---|
542 | !------------------------------------------------------------------------------| |
---|
543 | ! |
---|
544 | zdifcase(ji) = 3.0 |
---|
545 | numeqmin(ji) = nlay_s + 1 |
---|
546 | numeqmax(ji) = nlay_i + nlay_s + 1 |
---|
547 | |
---|
548 | !!surface equation |
---|
549 | ztrid(ji,numeqmin(ji),1) = 0.0 |
---|
550 | ztrid(ji,numeqmin(ji),2) = dzf(ji) - zkappa_i(ji,0)*zg1 |
---|
551 | ztrid(ji,numeqmin(ji),3) = zkappa_i(ji,0)*zg1 |
---|
552 | zindterm(ji,numeqmin(ji)) = dzf(ji)*t_su_b(ji) - zf(ji) |
---|
553 | |
---|
554 | !!first layer of ice equation |
---|
555 | ztrid(ji,numeqmin(ji)+1,1) = - zkappa_i(ji,0) * zg1 * zeta_i(ji,1) |
---|
556 | ztrid(ji,numeqmin(ji)+1,2) = 1.0 + zeta_i(ji,1) * ( zkappa_i(ji,1) & |
---|
557 | + zkappa_i(ji,0) * zg1 ) |
---|
558 | ztrid(ji,numeqmin(ji)+1,3) = - zeta_i(ji,1)*zkappa_i(ji,1) |
---|
559 | zindterm(ji,numeqmin(ji)+1)= ztiold(ji,1) + zeta_i(ji,1)*zradab_i(ji,1) |
---|
560 | |
---|
561 | !!case of only one layer in the ice (surface & ice equations are altered) |
---|
562 | |
---|
563 | IF (nlay_i.eq.1) THEN |
---|
564 | ztrid(ji,numeqmin(ji),1) = 0.0 |
---|
565 | ztrid(ji,numeqmin(ji),2) = dzf(ji) - zkappa_i(ji,0)*2.0 |
---|
566 | ztrid(ji,numeqmin(ji),3) = zkappa_i(ji,0)*2.0 |
---|
567 | ztrid(ji,numeqmin(ji)+1,1) = -zkappa_i(ji,0)*2.0*zeta_i(ji,1) |
---|
568 | ztrid(ji,numeqmin(ji)+1,2) = 1.0 + zeta_i(ji,1)*(zkappa_i(ji,0)*2.0 + & |
---|
569 | zkappa_i(ji,1)) |
---|
570 | ztrid(ji,numeqmin(ji)+1,3) = 0.0 |
---|
571 | |
---|
572 | zindterm(ji,numeqmin(ji)+1) = ztiold(ji,1) + zeta_i(ji,1)* & |
---|
573 | ( zradab_i(ji,1) + zkappa_i(ji,1)*t_bo_b(ji) ) |
---|
574 | ENDIF |
---|
575 | |
---|
576 | ELSE |
---|
577 | |
---|
578 | ! |
---|
579 | !------------------------------------------------------------------------------| |
---|
580 | ! case 4 : surface is melting - no snow | |
---|
581 | !------------------------------------------------------------------------------| |
---|
582 | ! |
---|
583 | zdifcase(ji) = 4.0 |
---|
584 | numeqmin(ji) = nlay_s + 2 |
---|
585 | numeqmax(ji) = nlay_i + nlay_s + 1 |
---|
586 | |
---|
587 | !!first layer of ice equation |
---|
588 | ztrid(ji,numeqmin(ji),1) = 0.0 |
---|
589 | ztrid(ji,numeqmin(ji),2) = 1.0 + zeta_i(ji,1)*(zkappa_i(ji,1) + zkappa_i(ji,0)* & |
---|
590 | zg1) |
---|
591 | ztrid(ji,numeqmin(ji),3) = - zeta_i(ji,1) * zkappa_i(ji,1) |
---|
592 | zindterm(ji,numeqmin(ji)) = ztiold(ji,1) + zeta_i(ji,1)*( zradab_i(ji,1) + & |
---|
593 | zkappa_i(ji,0) * zg1 * t_su_b(ji) ) |
---|
594 | |
---|
595 | !!case of only one layer in the ice (surface & ice equations are altered) |
---|
596 | IF (nlay_i.eq.1) THEN |
---|
597 | ztrid(ji,numeqmin(ji),1) = 0.0 |
---|
598 | ztrid(ji,numeqmin(ji),2) = 1.0 + zeta_i(ji,1)*(zkappa_i(ji,0)*2.0 + & |
---|
599 | zkappa_i(ji,1)) |
---|
600 | ztrid(ji,numeqmin(ji),3) = 0.0 |
---|
601 | zindterm(ji,numeqmin(ji)) = ztiold(ji,1) + zeta_i(ji,1)* & |
---|
602 | (zradab_i(ji,1) + zkappa_i(ji,1)*t_bo_b(ji)) & |
---|
603 | + t_su_b(ji)*zeta_i(ji,1)*zkappa_i(ji,0)*2.0 |
---|
604 | ENDIF |
---|
605 | |
---|
606 | ENDIF |
---|
607 | ENDIF |
---|
608 | |
---|
609 | END DO |
---|
610 | |
---|
611 | ! |
---|
612 | !------------------------------------------------------------------------------| |
---|
613 | ! 9) tridiagonal system solving | |
---|
614 | !------------------------------------------------------------------------------| |
---|
615 | ! |
---|
616 | |
---|
617 | ! Solve the tridiagonal system with Gauss elimination method. |
---|
618 | ! Thomas algorithm, from Computational fluid Dynamics, J.D. ANDERSON, |
---|
619 | ! McGraw-Hill 1984. |
---|
620 | |
---|
621 | maxnumeqmax = 0 |
---|
622 | minnumeqmin = jkmax+4 |
---|
623 | |
---|
624 | DO ji = kideb , kiut |
---|
625 | zindtbis(ji,numeqmin(ji)) = zindterm(ji,numeqmin(ji)) |
---|
626 | zdiagbis(ji,numeqmin(ji)) = ztrid(ji,numeqmin(ji),2) |
---|
627 | minnumeqmin = MIN(numeqmin(ji),minnumeqmin) |
---|
628 | maxnumeqmax = MAX(numeqmax(ji),maxnumeqmax) |
---|
629 | END DO |
---|
630 | |
---|
631 | DO layer = minnumeqmin+1, maxnumeqmax |
---|
632 | DO ji = kideb , kiut |
---|
633 | numeq = min(max(numeqmin(ji)+1,layer),numeqmax(ji)) |
---|
634 | zdiagbis(ji,numeq) = ztrid(ji,numeq,2) - ztrid(ji,numeq,1)* & |
---|
635 | ztrid(ji,numeq-1,3)/zdiagbis(ji,numeq-1) |
---|
636 | zindtbis(ji,numeq) = zindterm(ji,numeq) - ztrid(ji,numeq,1)* & |
---|
637 | zindtbis(ji,numeq-1)/zdiagbis(ji,numeq-1) |
---|
638 | END DO |
---|
639 | END DO |
---|
640 | |
---|
641 | DO ji = kideb , kiut |
---|
642 | ! ice temperatures |
---|
643 | t_i_b(ji,nlay_i) = zindtbis(ji,numeqmax(ji))/zdiagbis(ji,numeqmax(ji)) |
---|
644 | END DO |
---|
645 | |
---|
646 | DO numeq = nlay_i + nlay_s + 1, nlay_s + 2, -1 |
---|
647 | DO ji = kideb , kiut |
---|
648 | layer = numeq - nlay_s - 1 |
---|
649 | t_i_b(ji,layer) = (zindtbis(ji,numeq) - ztrid(ji,numeq,3)* & |
---|
650 | t_i_b(ji,layer+1))/zdiagbis(ji,numeq) |
---|
651 | END DO |
---|
652 | END DO |
---|
653 | |
---|
654 | DO ji = kideb , kiut |
---|
655 | ! snow temperatures |
---|
656 | IF (ht_s_b(ji).GT.0._wp) & |
---|
657 | t_s_b(ji,nlay_s) = (zindtbis(ji,nlay_s+1) - ztrid(ji,nlay_s+1,3) & |
---|
658 | * t_i_b(ji,1))/zdiagbis(ji,nlay_s+1) & |
---|
659 | * MAX(0.0,SIGN(1.0,ht_s_b(ji))) |
---|
660 | |
---|
661 | ! surface temperature |
---|
662 | isnow(ji) = NINT( 1.0 - MAX( 0.0 , SIGN( 1.0 , -ht_s_b(ji) ) ) ) |
---|
663 | ztsuoldit(ji) = t_su_b(ji) |
---|
664 | IF( t_su_b(ji) < ztfs(ji) ) & |
---|
665 | t_su_b(ji) = ( zindtbis(ji,numeqmin(ji)) - ztrid(ji,numeqmin(ji),3)* ( REAL( isnow(ji) )*t_s_b(ji,1) & |
---|
666 | & + REAL( 1 - isnow(ji) )*t_i_b(ji,1) ) ) / zdiagbis(ji,numeqmin(ji)) |
---|
667 | END DO |
---|
668 | ! |
---|
669 | !-------------------------------------------------------------------------- |
---|
670 | ! 10) Has the scheme converged ?, end of the iterative procedure | |
---|
671 | !-------------------------------------------------------------------------- |
---|
672 | ! |
---|
673 | ! check that nowhere it has started to melt |
---|
674 | ! zerrit(ji) is a measure of error, it has to be under maxer_i_thd |
---|
675 | DO ji = kideb , kiut |
---|
676 | t_su_b(ji) = MAX( MIN( t_su_b(ji) , ztfs(ji) ) , 190._wp ) |
---|
677 | zerrit(ji) = ABS( t_su_b(ji) - ztsuoldit(ji) ) |
---|
678 | END DO |
---|
679 | |
---|
680 | DO layer = 1, nlay_s |
---|
681 | DO ji = kideb , kiut |
---|
682 | t_s_b(ji,layer) = MAX( MIN( t_s_b(ji,layer), rtt ), 190._wp ) |
---|
683 | zerrit(ji) = MAX(zerrit(ji),ABS(t_s_b(ji,layer) - ztstemp(ji,layer))) |
---|
684 | END DO |
---|
685 | END DO |
---|
686 | |
---|
687 | DO layer = 1, nlay_i |
---|
688 | DO ji = kideb , kiut |
---|
689 | ztmelt_i = -tmut * s_i_b(ji,layer) + rtt |
---|
690 | t_i_b(ji,layer) = MAX(MIN(t_i_b(ji,layer),ztmelt_i), 190._wp) |
---|
691 | zerrit(ji) = MAX(zerrit(ji),ABS(t_i_b(ji,layer) - ztitemp(ji,layer))) |
---|
692 | END DO |
---|
693 | END DO |
---|
694 | |
---|
695 | ! Compute spatial maximum over all errors |
---|
696 | ! note that this could be optimized substantially by iterating only the non-converging points |
---|
697 | zerritmax = 0._wp |
---|
698 | DO ji = kideb, kiut |
---|
699 | zerritmax = MAX( zerritmax, zerrit(ji) ) |
---|
700 | END DO |
---|
701 | IF( lk_mpp ) CALL mpp_max( zerritmax, kcom=ncomm_ice ) |
---|
702 | |
---|
703 | END DO ! End of the do while iterative procedure |
---|
704 | |
---|
705 | IF( ln_nicep .AND. lwp ) THEN |
---|
706 | WRITE(numout,*) ' zerritmax : ', zerritmax |
---|
707 | WRITE(numout,*) ' nconv : ', nconv |
---|
708 | ENDIF |
---|
709 | |
---|
710 | ! |
---|
711 | !-------------------------------------------------------------------------! |
---|
712 | ! 11) Fluxes at the interfaces ! |
---|
713 | !-------------------------------------------------------------------------! |
---|
714 | DO ji = kideb, kiut |
---|
715 | ! forced mode only : update of latent heat fluxes (sublimation) (always >=0, upward flux) |
---|
716 | IF( .NOT. lk_cpl) qla_ice_1d (ji) = MAX( 0._wp, qla_ice_1d (ji) + dqla_ice_1d(ji) * ( t_su_b(ji) - ztsuold(ji) ) ) |
---|
717 | ! ! surface ice conduction flux |
---|
718 | isnow(ji) = NINT( 1._wp - MAX( 0._wp, SIGN( 1._wp, -ht_s_b(ji) ) ) ) |
---|
719 | fc_su(ji) = - REAL( isnow(ji) ) * zkappa_s(ji,0) * zg1s * (t_s_b(ji,1) - t_su_b(ji)) & |
---|
720 | & - REAL( 1 - isnow(ji) ) * zkappa_i(ji,0) * zg1 * (t_i_b(ji,1) - t_su_b(ji)) |
---|
721 | ! ! bottom ice conduction flux |
---|
722 | fc_bo_i(ji) = - zkappa_i(ji,nlay_i) * ( zg1*(t_bo_b(ji) - t_i_b(ji,nlay_i)) ) |
---|
723 | END DO |
---|
724 | |
---|
725 | !----------------------------------------- |
---|
726 | ! Heat flux used to warm/cool ice in W.m-2 |
---|
727 | !----------------------------------------- |
---|
728 | DO ji = kideb, kiut |
---|
729 | IF( t_su_b(ji) < rtt ) THEN ! case T_su < 0degC |
---|
730 | hfx_dif_1d(ji) = hfx_dif_1d(ji) + ( qns_ice_1d(ji) + qsr_ice_1d(ji) - zradtr_i(ji,nlay_i) - fc_bo_i(ji) ) * a_i_b(ji) |
---|
731 | ELSE ! case T_su = 0degC |
---|
732 | hfx_dif_1d(ji) = hfx_dif_1d(ji) + ( fc_su(ji) + i0(ji) * qsr_ice_1d(ji) - zradtr_i(ji,nlay_i) - fc_bo_i(ji) ) * a_i_b(ji) |
---|
733 | ENDIF |
---|
734 | END DO |
---|
735 | |
---|
736 | ! --- computes sea ice energy of melting compulsory for limthd_dh --- ! |
---|
737 | CALL lim_thd_enmelt( kideb, kiut ) |
---|
738 | |
---|
739 | ! --- diag error on heat diffusion - PART 2 --- ! |
---|
740 | DO ji = kideb, kiut |
---|
741 | zdq(ji) = - zq_ini(ji) + ( SUM( q_i_b(ji,1:nlay_i) ) * ht_i_b(ji) / REAL( nlay_i ) + & |
---|
742 | & SUM( q_s_b(ji,1:nlay_s) ) * ht_s_b(ji) / REAL( nlay_s ) ) |
---|
743 | zhfx_err = ( fc_su(ji) + i0(ji) * qsr_ice_1d(ji) - zradtr_i(ji,nlay_i) - fc_bo_i(ji) + zdq(ji) * r1_rdtice ) |
---|
744 | hfx_err_1d(ji) = hfx_err_1d(ji) + zhfx_err * a_i_b(ji) |
---|
745 | ! --- correction of qns_ice and surface conduction flux --- ! |
---|
746 | qns_ice_1d(ji) = qns_ice_1d(ji) - zhfx_err |
---|
747 | fc_su (ji) = fc_su (ji) - zhfx_err |
---|
748 | ! --- Heat flux at the ice surface in W.m-2 --- ! |
---|
749 | ii = MOD( npb(ji) - 1, jpi ) + 1 ; ij = ( npb(ji) - 1 ) / jpi + 1 |
---|
750 | hfx_in (ii,ij) = hfx_in (ii,ij) + a_i_b(ji) * ( qsr_ice_1d(ji) + qns_ice_1d(ji) ) |
---|
751 | END DO |
---|
752 | |
---|
753 | ! |
---|
754 | CALL wrk_dealloc( jpij, numeqmin, numeqmax, isnow ) |
---|
755 | CALL wrk_dealloc( jpij, ztfs, ztsuold, ztsuoldit, zh_i, zh_s, zfsw ) |
---|
756 | CALL wrk_dealloc( jpij, zf, dzf, zerrit, zdifcase, zftrice, zihic, zhsu ) |
---|
757 | CALL wrk_dealloc( jpij, nlay_i+1, ztcond_i, zradtr_i, zradab_i, zkappa_i, ztiold, zeta_i, ztitemp, z_i, zspeche_i, kjstart = 0 ) |
---|
758 | CALL wrk_dealloc( jpij, nlay_s+1, zradtr_s, zradab_s, zkappa_s, ztsold, zeta_s, ztstemp, z_s, kjstart = 0 ) |
---|
759 | CALL wrk_dealloc( jpij, jkmax+2, zindterm, zindtbis, zdiagbis ) |
---|
760 | CALL wrk_dealloc( jpij, jkmax+2, 3, ztrid ) |
---|
761 | CALL wrk_dealloc( jpij, zdq, zq_ini ) |
---|
762 | |
---|
763 | END SUBROUTINE lim_thd_dif |
---|
764 | |
---|
765 | SUBROUTINE lim_thd_enmelt( kideb, kiut ) |
---|
766 | !!----------------------------------------------------------------------- |
---|
767 | !! *** ROUTINE lim_thd_enmelt *** |
---|
768 | !! |
---|
769 | !! ** Purpose : Computes sea ice energy of melting q_i (J.m-3) from temperature |
---|
770 | !! |
---|
771 | !! ** Method : Formula (Bitz and Lipscomb, 1999) |
---|
772 | !!------------------------------------------------------------------- |
---|
773 | INTEGER, INTENT(in) :: kideb, kiut ! bounds for the spatial loop |
---|
774 | ! |
---|
775 | INTEGER :: ji, jk ! dummy loop indices |
---|
776 | REAL(wp) :: ztmelts, zindb ! local scalar |
---|
777 | !!------------------------------------------------------------------- |
---|
778 | ! |
---|
779 | DO jk = 1, nlay_i ! Sea ice energy of melting |
---|
780 | DO ji = kideb, kiut |
---|
781 | ztmelts = - tmut * s_i_b(ji,jk) + rtt |
---|
782 | zindb = MAX( 0._wp , SIGN( 1._wp , -(t_i_b(ji,jk) - rtt) - epsi10 ) ) |
---|
783 | q_i_b(ji,jk) = rhoic * ( cpic * ( ztmelts - t_i_b(ji,jk) ) & |
---|
784 | & + lfus * ( 1.0 - zindb * ( ztmelts-rtt ) / MIN( t_i_b(ji,jk)-rtt, -epsi10 ) ) & |
---|
785 | & - rcp * ( ztmelts-rtt ) ) |
---|
786 | END DO |
---|
787 | END DO |
---|
788 | DO jk = 1, nlay_s ! Snow energy of melting |
---|
789 | DO ji = kideb, kiut |
---|
790 | q_s_b(ji,jk) = rhosn * ( cpic * ( rtt - t_s_b(ji,jk) ) + lfus ) |
---|
791 | END DO |
---|
792 | END DO |
---|
793 | ! |
---|
794 | END SUBROUTINE lim_thd_enmelt |
---|
795 | |
---|
796 | #else |
---|
797 | !!---------------------------------------------------------------------- |
---|
798 | !! Dummy Module No LIM-3 sea-ice model |
---|
799 | !!---------------------------------------------------------------------- |
---|
800 | CONTAINS |
---|
801 | SUBROUTINE lim_thd_dif ! Empty routine |
---|
802 | END SUBROUTINE lim_thd_dif |
---|
803 | #endif |
---|
804 | !!====================================================================== |
---|
805 | END MODULE limthd_dif |
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