1 | MODULE dynzdf_imp_tam |
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2 | #ifdef key_tam |
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3 | !!============================================================================== |
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4 | !! *** MODULE dynzdf_imp_tam *** |
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5 | !! Ocean dynamics: vertical component(s) of the momentum mixing trend |
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6 | !! Tangent and Adjoint Module |
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7 | !!============================================================================== |
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8 | !! History of the direct module: |
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9 | !! ! 90-10 (B. Blanke) Original code |
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10 | !! ! 97-05 (G. Madec) vertical component of isopycnal |
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11 | !! 8.5 ! 02-08 (G. Madec) F90: Free form and module |
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12 | !! History of the TAM module: |
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13 | !! 9.0 ! 09-01 (A. Vidard) TAM of the 02-08 version |
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14 | !!---------------------------------------------------------------------- |
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15 | |
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16 | !!---------------------------------------------------------------------- |
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17 | !! dyn_zdf_imp : update the momentum trend with the vertical diffu- |
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18 | !! sion using an implicit time-stepping scheme. |
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19 | !!---------------------------------------------------------------------- |
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20 | !! * Modules used |
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21 | USE par_kind , ONLY: & ! Precision variables |
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22 | & wp |
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23 | USE par_oce , ONLY: & ! Ocean space and time domain variables |
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24 | & jpi, & |
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25 | & jpj, & |
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26 | & jpk, & |
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27 | & jpim1, & |
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28 | & jpjm1, & |
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29 | & jpkm1 |
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30 | USE oce_tam , ONLY: & ! ocean dynamics and tracers |
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31 | & ub_tl, & |
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32 | & ua_tl, & |
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33 | & vb_tl, & |
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34 | & va_tl, & |
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35 | & ub_ad, & |
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36 | & ua_ad, & |
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37 | & vb_ad, & |
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38 | & va_ad |
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39 | USE zdf_oce , ONLY: & ! ocean vertical physics |
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40 | & avmu, & |
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41 | & avmv |
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42 | USE dom_oce , ONLY: & ! ocean space and time domain |
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43 | #if defined key_zco |
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44 | & e3t_0, & |
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45 | & e3w_0, & |
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46 | #else |
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47 | & e3u, & |
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48 | & e3v, & |
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49 | & e3uw, & |
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50 | & e3vw, & |
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51 | #endif |
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52 | & umask, & |
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53 | & vmask |
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54 | USE phycst , ONLY: & ! physical constants |
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55 | & rau0 |
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56 | USE in_out_manager, ONLY: & ! I/O manager |
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57 | & nit000, & |
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58 | & nitend, & |
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59 | & numout, & |
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60 | & lwp |
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61 | |
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62 | |
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63 | IMPLICIT NONE |
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64 | PRIVATE |
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65 | |
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66 | !! * Routine accessibility |
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67 | PUBLIC dyn_zdf_imp_tan ! called by dynzdf_tam.F90 |
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68 | PUBLIC dyn_zdf_imp_adj ! called by dynzdf_tam.F90 |
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69 | |
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70 | !! * Substitutions |
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71 | # include "domzgr_substitute.h90" |
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72 | # include "vectopt_loop_substitute.h90" |
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73 | !!---------------------------------------------------------------------- |
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74 | |
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75 | CONTAINS |
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76 | |
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77 | SUBROUTINE dyn_zdf_imp_tan( kt, p2dt ) |
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78 | !!---------------------------------------------------------------------- |
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79 | !! *** ROUTINE dyn_zdf_imp_tan *** |
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80 | !! |
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81 | !! ** Purpose of the direct routine: |
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82 | !! Compute the trend due to the vert. momentum diffusion |
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83 | !! and the surface forcing, and add it to the general trend of |
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84 | !! the momentum equations. |
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85 | !! |
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86 | !! ** Method of the direct routine: |
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87 | !! The vertical momentum mixing trend is given by : |
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88 | !! dz( avmu dz(u) ) = 1/e3u dk+1( avmu/e3uw dk(ua) ) |
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89 | !! backward time stepping |
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90 | !! Surface boundary conditions: wind stress input |
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91 | !! Bottom boundary conditions : bottom stress (cf zdfbfr.F) |
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92 | !! Add this trend to the general trend ua : |
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93 | !! ua = ua + dz( avmu dz(u) )E |
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94 | !! |
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95 | !! ** Action : - Update (ua,va) arrays with the after vertical diffusive |
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96 | !! mixing trend. |
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97 | !!--------------------------------------------------------------------- |
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98 | !! * Modules used |
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99 | !! * Arguments |
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100 | INTEGER , INTENT( in ) :: kt ! ocean time-step index |
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101 | REAL(wp), INTENT( in ) :: p2dt ! time-step |
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102 | |
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103 | !! * Local declarations |
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104 | INTEGER :: ji, jj, jk ! dummy loop indices |
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105 | REAL(wp) :: zrau0r, z2dtf, zcoef, zzws, zrhstl ! temporary scalars |
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106 | REAL(wp), DIMENSION(jpi,jpj,jpk):: zwi, zws, zwd ! temporary workspace arrays |
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107 | !!---------------------------------------------------------------------- |
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108 | |
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109 | IF( kt == nit000 ) THEN |
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110 | IF(lwp) WRITE(numout,*) |
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111 | IF(lwp) WRITE(numout,*) 'dyn_zdf_imp_tan : vertical momentum diffusion explicit operator' |
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112 | IF(lwp) WRITE(numout,*) '~~~~~~~~~~~~~~~ ' |
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113 | ENDIF |
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114 | ! 0. Local constant initialization |
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115 | ! -------------------------------- |
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116 | zrau0r = 1. / rau0 ! inverse of the reference density |
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117 | |
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118 | ! 1. Vertical diffusion on u |
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119 | ! --------------------------- |
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120 | ! Matrix and second member construction |
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121 | ! bottom boundary condition: only zws must be masked as avmu can take |
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122 | ! non zero value at the ocean bottom depending on the bottom friction |
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123 | ! used (see zdfmix.F) |
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124 | DO jk = 1, jpkm1 |
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125 | DO jj = 2, jpjm1 |
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126 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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127 | zcoef = - p2dt / fse3u(ji,jj,jk) |
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128 | zwi(ji,jj,jk) = zcoef * avmu(ji,jj,jk ) / fse3uw(ji,jj,jk ) * umask(ji,jj,jk) |
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129 | zzws = zcoef * avmu(ji,jj,jk+1) / fse3uw(ji,jj,jk+1) |
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130 | zws(ji,jj,jk) = zzws * umask(ji,jj,jk+1) |
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131 | zwd(ji,jj,jk) = 1. - zwi(ji,jj,jk) - zzws |
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132 | END DO |
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133 | END DO |
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134 | END DO |
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135 | |
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136 | ! Surface boudary conditions |
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137 | DO jj = 2, jpjm1 |
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138 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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139 | zwi(ji,jj,1) = 0. |
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140 | zwd(ji,jj,1) = 1. - zws(ji,jj,1) |
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141 | END DO |
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142 | END DO |
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143 | |
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144 | ! Matrix inversion starting from the first level |
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145 | !----------------------------------------------------------------------- |
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146 | ! solve m.x = y where m is a tri diagonal matrix ( jpk*jpk ) |
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147 | ! |
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148 | ! ( zwd1 zws1 0 0 0 )( zwx1 ) ( zwy1 ) |
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149 | ! ( zwi2 zwd2 zws2 0 0 )( zwx2 ) ( zwy2 ) |
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150 | ! ( 0 zwi3 zwd3 zws3 0 )( zwx3 )=( zwy3 ) |
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151 | ! ( ... )( ... ) ( ... ) |
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152 | ! ( 0 0 0 zwik zwdk )( zwxk ) ( zwyk ) |
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153 | ! |
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154 | ! m is decomposed in the product of an upper and a lower triangular matrix |
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155 | ! The 3 diagonal terms are in 2d arrays: zwd, zws, zwi |
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156 | ! The solution (the after velocity) is in ua |
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157 | !----------------------------------------------------------------------- |
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158 | |
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159 | ! First recurrence : Dk = Dk - Lk * Uk-1 / Dk-1 (increasing k) |
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160 | DO jk = 2, jpkm1 |
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161 | DO jj = 2, jpjm1 |
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162 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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163 | zwd(ji,jj,jk) = zwd(ji,jj,jk) - zwi(ji,jj,jk) * zws(ji,jj,jk-1) / zwd(ji,jj,jk-1) |
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164 | END DO |
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165 | END DO |
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166 | END DO |
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167 | |
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168 | ! second recurrence: SOLk = RHSk - Lk / Dk-1 Lk-1 |
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169 | DO jj = 2, jpjm1 |
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170 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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171 | ua_tl(ji,jj,1) = ub_tl(ji,jj,1) & |
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172 | + p2dt * ua_tl(ji,jj,1) |
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173 | END DO |
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174 | END DO |
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175 | DO jk = 2, jpkm1 |
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176 | DO jj = 2, jpjm1 |
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177 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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178 | zrhstl = ub_tl(ji,jj,jk) + p2dt * ua_tl(ji,jj,jk) ! zrhs=right hand side |
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179 | ua_tl(ji,jj,jk) = zrhstl - zwi(ji,jj,jk) / zwd(ji,jj,jk-1) * ua_tl(ji,jj,jk-1) |
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180 | END DO |
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181 | END DO |
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182 | END DO |
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183 | |
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184 | ! thrid recurrence : SOLk = ( Lk - Uk * Ek+1 ) / Dk |
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185 | DO jj = 2, jpjm1 |
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186 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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187 | ua_tl(ji,jj,jpkm1) = ua_tl(ji,jj,jpkm1) / zwd(ji,jj,jpkm1) |
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188 | END DO |
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189 | END DO |
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190 | DO jk = jpk-2, 1, -1 |
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191 | DO jj = 2, jpjm1 |
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192 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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193 | ua_tl(ji,jj,jk) = ( ua_tl(ji,jj,jk) - zws(ji,jj,jk) * ua_tl(ji,jj,jk+1) ) / zwd(ji,jj,jk) |
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194 | END DO |
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195 | END DO |
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196 | END DO |
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197 | |
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198 | ! Normalization to obtain the general momentum trend ua |
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199 | DO jk = 1, jpkm1 |
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200 | DO jj = 2, jpjm1 |
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201 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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202 | ua_tl(ji,jj,jk) = ( ua_tl(ji,jj,jk) - ub_tl(ji,jj,jk) ) / p2dt |
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203 | END DO |
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204 | END DO |
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205 | END DO |
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206 | |
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207 | |
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208 | ! 2. Vertical diffusion on v |
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209 | ! --------------------------- |
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210 | ! Matrix and second member construction |
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211 | ! bottom boundary condition: only zws must be masked as avmv can take |
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212 | ! non zero value at the ocean bottom depending on the bottom friction |
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213 | ! used (see zdfmix.F) |
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214 | DO jk = 1, jpkm1 |
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215 | DO jj = 2, jpjm1 |
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216 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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217 | zcoef = -p2dt / fse3v(ji,jj,jk) |
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218 | zwi(ji,jj,jk) = zcoef * avmv(ji,jj,jk ) / fse3vw(ji,jj,jk ) |
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219 | zzws = zcoef * avmv(ji,jj,jk+1) / fse3vw(ji,jj,jk+1) |
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220 | zws(ji,jj,jk) = zzws * vmask(ji,jj,jk+1) |
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221 | zwd(ji,jj,jk) = 1. - zwi(ji,jj,jk) - zzws |
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222 | END DO |
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223 | END DO |
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224 | END DO |
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225 | |
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226 | ! Surface boudary conditions |
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227 | DO jj = 2, jpjm1 |
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228 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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229 | zwi(ji,jj,1) = 0._wp |
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230 | zwd(ji,jj,1) = 1. - zws(ji,jj,1) |
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231 | END DO |
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232 | END DO |
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233 | |
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234 | ! Matrix inversion |
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235 | !----------------------------------------------------------------------- |
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236 | ! solve m.x = y where m is a tri diagonal matrix ( jpk*jpk ) |
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237 | ! |
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238 | ! ( zwd1 zws1 0 0 0 )( zwx1 ) ( zwy1 ) |
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239 | ! ( zwi2 zwd2 zws2 0 0 )( zwx2 ) ( zwy2 ) |
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240 | ! ( 0 zwi3 zwd3 zws3 0 )( zwx3 )=( zwy3 ) |
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241 | ! ( ... )( ... ) ( ... ) |
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242 | ! ( 0 0 0 zwik zwdk )( zwxk ) ( zwyk ) |
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243 | ! |
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244 | ! m is decomposed in the product of an upper and lower triangular |
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245 | ! matrix |
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246 | ! The 3 diagonal terms are in 2d arrays: zwd, zws, zwi |
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247 | ! The solution (after velocity) is in 2d array va |
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248 | !----------------------------------------------------------------------- |
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249 | |
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250 | ! First recurrence : Dk = Dk - Lk * Uk-1 / Dk-1 (increasing k) |
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251 | DO jk = 2, jpkm1 |
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252 | DO jj = 2, jpjm1 |
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253 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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254 | zwd(ji,jj,jk) = zwd(ji,jj,jk) - zwi(ji,jj,jk) * zws(ji,jj,jk-1) / zwd(ji,jj,jk-1) |
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255 | END DO |
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256 | END DO |
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257 | END DO |
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258 | |
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259 | ! second recurrence: SOLk = RHSk - Lk / Dk-1 Lk-1 |
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260 | DO jj = 2, jpjm1 |
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261 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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262 | va_tl(ji,jj,1) = vb_tl(ji,jj,1) & |
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263 | + p2dt * va_tl(ji,jj,1) |
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264 | END DO |
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265 | END DO |
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266 | DO jk = 2, jpkm1 |
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267 | DO jj = 2, jpjm1 |
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268 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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269 | zrhstl = vb_tl(ji,jj,jk) + p2dt * va_tl(ji,jj,jk) ! zrhs=right hand side |
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270 | va_tl(ji,jj,jk) = zrhstl - zwi(ji,jj,jk) / zwd(ji,jj,jk-1) * va_tl(ji,jj,jk-1) |
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271 | END DO |
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272 | END DO |
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273 | END DO |
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274 | |
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275 | ! thrid recurrence : SOLk = ( Lk - Uk * SOLk+1 ) / Dk |
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276 | DO jj = 2, jpjm1 |
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277 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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278 | va_tl(ji,jj,jpkm1) = va_tl(ji,jj,jpkm1) / zwd(ji,jj,jpkm1) |
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279 | END DO |
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280 | END DO |
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281 | DO jk = jpk-2, 1, -1 |
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282 | DO jj = 2, jpjm1 |
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283 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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284 | va_tl(ji,jj,jk) = ( va_tl(ji,jj,jk) - zws(ji,jj,jk) * va_tl(ji,jj,jk+1) ) / zwd(ji,jj,jk) |
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285 | END DO |
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286 | END DO |
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287 | END DO |
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288 | |
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289 | ! Normalization to obtain the general momentum trend va |
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290 | DO jk = 1, jpkm1 |
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291 | DO jj = 2, jpjm1 |
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292 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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293 | va_tl(ji,jj,jk) = ( va_tl(ji,jj,jk) - vb_tl(ji,jj,jk) ) / p2dt |
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294 | END DO |
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295 | END DO |
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296 | END DO |
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297 | |
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298 | END SUBROUTINE dyn_zdf_imp_tan |
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299 | SUBROUTINE dyn_zdf_imp_adj( kt, p2dt ) |
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300 | !!---------------------------------------------------------------------- |
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301 | !! *** ROUTINE dyn_zdf_imp_adj *** |
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302 | !! |
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303 | !! ** Purpose of the direct routine: |
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304 | !! Compute the trend due to the vert. momentum diffusion |
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305 | !! and the surface forcing, and add it to the general trend of |
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306 | !! the momentum equations. |
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307 | !! |
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308 | !! ** Method of the direct routine: |
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309 | !! The vertical momentum mixing trend is given by : |
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310 | !! dz( avmu dz(u) ) = 1/e3u dk+1( avmu/e3uw dk(ua) ) |
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311 | !! backward time stepping |
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312 | !! Surface boundary conditions: wind stress input |
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313 | !! Bottom boundary conditions : bottom stress (cf zdfbfr.F) |
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314 | !! Add this trend to the general trend ua : |
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315 | !! ua = ua + dz( avmu dz(u) )E |
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316 | !! |
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317 | !! ** Action : - Update (ua,va) arrays with the after vertical diffusive |
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318 | !! mixing trend. |
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319 | !!--------------------------------------------------------------------- |
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320 | !! * Modules used |
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321 | !! * Arguments |
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322 | INTEGER , INTENT( in ) :: kt ! ocean time-step index |
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323 | REAL(wp), INTENT( in ) :: p2dt ! time-step |
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324 | |
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325 | !! * Local declarations |
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326 | !! * Local declarations |
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327 | INTEGER :: ji, jj, jk ! dummy loop indices |
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328 | REAL(wp) :: zrau0r, z2dtf, zcoef, zzws, zrhsad ! temporary scalars |
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329 | REAL(wp), DIMENSION(jpi,jpj,jpk) :: zwi, zws, zwd! temporary workspace arrays |
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330 | !!---------------------------------------------------------------------- |
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331 | |
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332 | IF( kt == nit000 ) THEN |
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333 | IF(lwp) WRITE(numout,*) |
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334 | IF(lwp) WRITE(numout,*) 'dyn_zdf_imp_adj : vertical momentum diffusion explicit operator' |
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335 | IF(lwp) WRITE(numout,*) '~~~~~~~~~~~~~~~ ' |
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336 | ENDIF |
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337 | ! 0. Local constant initialization |
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338 | ! -------------------------------- |
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339 | zrau0r = 1. / rau0 ! inverse of the reference density |
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340 | zrhsad = 0.0_wp |
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341 | |
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342 | |
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343 | |
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344 | |
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345 | ! 2. Vertical diffusion on v |
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346 | ! --------------------------- |
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347 | ! Matrix and second member construction |
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348 | ! bottom boundary condition: only zws must be masked as avmv can take |
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349 | ! non zero value at the ocean bottom depending on the bottom friction |
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350 | ! used (see zdfmix.F) |
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351 | DO jk = 1, jpkm1 |
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352 | DO jj = 2, jpjm1 |
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353 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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354 | zcoef = -p2dt / fse3v(ji,jj,jk) |
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355 | zwi(ji,jj,jk) = zcoef * avmv(ji,jj,jk ) / fse3vw(ji,jj,jk ) |
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356 | zzws = zcoef * avmv(ji,jj,jk+1) / fse3vw(ji,jj,jk+1) |
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357 | zws(ji,jj,jk) = zzws * vmask(ji,jj,jk+1) |
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358 | zwd(ji,jj,jk) = 1._wp - zwi(ji,jj,jk) - zzws |
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359 | END DO |
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360 | END DO |
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361 | END DO |
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362 | |
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363 | ! Surface boudary conditions |
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364 | DO jj = 2, jpjm1 |
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365 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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366 | zwi(ji,jj,1) = 0._wp |
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367 | zwd(ji,jj,1) = 1._wp - zws(ji,jj,1) |
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368 | END DO |
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369 | END DO |
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370 | |
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371 | ! Matrix inversion |
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372 | !----------------------------------------------------------------------- |
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373 | ! solve m.x = y where m is a tri diagonal matrix ( jpk*jpk ) |
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374 | ! |
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375 | ! ( zwd1 zws1 0 0 0 )( zwx1 ) ( zwy1 ) |
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376 | ! ( zwi2 zwd2 zws2 0 0 )( zwx2 ) ( zwy2 ) |
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377 | ! ( 0 zwi3 zwd3 zws3 0 )( zwx3 )=( zwy3 ) |
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378 | ! ( ... )( ... ) ( ... ) |
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379 | ! ( 0 0 0 zwik zwdk )( zwxk ) ( zwyk ) |
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380 | ! |
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381 | ! m is decomposed in the product of an upper and lower triangular |
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382 | ! matrix |
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383 | ! The 3 diagonal terms are in 2d arrays: zwd, zws, zwi |
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384 | ! The solution (after velocity) is in 2d array va |
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385 | !----------------------------------------------------------------------- |
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386 | |
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387 | ! First recurrence : Dk = Dk - Lk * Uk-1 / Dk-1 (increasing k) |
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388 | DO jk = 2, jpkm1 |
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389 | DO jj = 2, jpjm1 |
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390 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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391 | zwd(ji,jj,jk) = zwd(ji,jj,jk) - zwi(ji,jj,jk) * zws(ji,jj,jk-1) / zwd(ji,jj,jk-1) |
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392 | END DO |
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393 | END DO |
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394 | END DO |
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395 | |
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396 | ! Normalization to obtain the general momentum trend va |
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397 | DO jk = jpkm1, 1, -1 |
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398 | DO jj = jpjm1, 2, -1 |
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399 | DO ji = fs_jpim1, fs_2, -1 ! vector opt. |
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400 | vb_ad(ji,jj,jk) = vb_ad(ji,jj,jk) - va_ad(ji,jj,jk) / p2dt |
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401 | va_ad(ji,jj,jk) = va_ad(ji,jj,jk) / p2dt |
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402 | END DO |
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403 | END DO |
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404 | END DO |
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405 | ! thrid recurrence : SOLk = ( Lk - Uk * SOLk+1 ) / Dk |
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406 | DO jk = 1, jpk-2 |
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407 | DO jj = jpjm1, 2, -1 |
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408 | DO ji = fs_jpim1, fs_2, -1 ! vector opt. |
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409 | va_ad(ji,jj,jk+1) = va_ad(ji,jj,jk+1) - zws(ji,jj,jk) * va_ad(ji,jj,jk) / zwd(ji,jj,jk) |
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410 | va_ad(ji,jj,jk ) = va_ad(ji,jj,jk ) / zwd(ji,jj,jk) |
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411 | END DO |
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412 | END DO |
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413 | END DO |
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414 | DO jj = jpjm1, 2, -1 |
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415 | DO ji = fs_jpim1, fs_2, -1 ! vector opt. |
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416 | va_ad(ji,jj,jpkm1) = va_ad(ji,jj,jpkm1) / zwd(ji,jj,jpkm1) |
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417 | END DO |
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418 | END DO |
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419 | ! second recurrence: SOLk = RHSk - Lk / Dk-1 Lk-1 |
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420 | DO jk = jpkm1, 2, -1 |
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421 | DO jj = jpjm1, 2, -1 |
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422 | DO ji = fs_jpim1, fs_2, -1 ! vector opt. |
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423 | zrhsad = zrhsad + va_ad(ji,jj,jk) |
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424 | va_ad(ji,jj,jk-1) = va_ad(ji,jj,jk-1) - zwi(ji,jj,jk) / zwd(ji,jj,jk-1) * va_ad(ji,jj,jk) |
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425 | va_ad(ji,jj,jk ) = 0.0_wp |
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426 | vb_ad(ji,jj,jk) = vb_ad(ji,jj,jk) + zrhsad |
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427 | va_ad(ji,jj,jk) = va_ad(ji,jj,jk) + p2dt * zrhsad |
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428 | zrhsad = 0.0_wp |
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429 | END DO |
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430 | END DO |
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431 | END DO |
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432 | DO jj = jpjm1, 2, -1 |
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433 | DO ji = fs_jpim1, fs_2, -1 ! vector opt. |
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434 | vb_ad(ji,jj,1) = vb_ad(ji,jj,1) + va_ad(ji,jj,1) |
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435 | va_ad(ji,jj,1) = va_ad(ji,jj,1) * p2dt |
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436 | END DO |
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437 | END DO |
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438 | |
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439 | ! 1. Vertical diffusion on u |
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440 | ! --------------------------- |
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441 | ! Matrix and second member construction |
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442 | ! bottom boundary condition: only zws must be masked as avmu can take |
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443 | ! non zero value at the ocean bottom depending on the bottom friction |
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444 | ! used (see zdfmix.F) |
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445 | DO jk = 1, jpkm1 |
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446 | DO jj = 2, jpjm1 |
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447 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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448 | zcoef = - p2dt / fse3u(ji,jj,jk) |
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449 | zwi(ji,jj,jk) = zcoef * avmu(ji,jj,jk ) / fse3uw(ji,jj,jk ) |
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450 | zzws = zcoef * avmu(ji,jj,jk+1) / fse3uw(ji,jj,jk+1) |
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451 | zws(ji,jj,jk) = zzws * umask(ji,jj,jk+1) |
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452 | zwd(ji,jj,jk) = 1._wp - zwi(ji,jj,jk) - zzws |
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453 | END DO |
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454 | END DO |
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455 | END DO |
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456 | |
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457 | ! Surface boudary conditions |
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458 | DO jj = 2, jpjm1 |
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459 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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460 | zwi(ji,jj,1) = 0._wp |
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461 | zwd(ji,jj,1) = 1._wp - zws(ji,jj,1) |
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462 | END DO |
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463 | END DO |
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464 | |
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465 | ! Matrix inversion starting from the first level |
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466 | !----------------------------------------------------------------------- |
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467 | ! solve m.x = y where m is a tri diagonal matrix ( jpk*jpk ) |
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468 | ! |
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469 | ! ( zwd1 zws1 0 0 0 )( zwx1 ) ( zwy1 ) |
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470 | ! ( zwi2 zwd2 zws2 0 0 )( zwx2 ) ( zwy2 ) |
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471 | ! ( 0 zwi3 zwd3 zws3 0 )( zwx3 )=( zwy3 ) |
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472 | ! ( ... )( ... ) ( ... ) |
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473 | ! ( 0 0 0 zwik zwdk )( zwxk ) ( zwyk ) |
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474 | ! |
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475 | ! m is decomposed in the product of an upper and a lower triangular matrix |
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476 | ! The 3 diagonal terms are in 2d arrays: zwd, zws, zwi |
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477 | ! The solution (the after velocity) is in ua |
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478 | !----------------------------------------------------------------------- |
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479 | |
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480 | ! First recurrence : Dk = Dk - Lk * Uk-1 / Dk-1 (increasing k) |
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481 | DO jk = 2, jpkm1 |
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482 | DO jj = 2, jpjm1 |
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483 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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484 | zwd(ji,jj,jk) = zwd(ji,jj,jk) - zwi(ji,jj,jk) * zws(ji,jj,jk-1) / zwd(ji,jj,jk-1) |
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485 | END DO |
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486 | END DO |
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487 | END DO |
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488 | ! Normalization to obtain the general momentum trend ua |
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489 | DO jk = jpkm1, 1, -1 |
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490 | DO jj = jpjm1, 2, -1 |
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491 | DO ji = fs_jpim1, fs_2, -1 ! vector opt. |
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492 | ub_ad(ji,jj,jk) = ub_ad(ji,jj,jk) - ua_ad(ji,jj,jk) / p2dt |
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493 | ua_ad(ji,jj,jk) = ua_ad(ji,jj,jk) / p2dt |
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494 | END DO |
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495 | END DO |
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496 | END DO |
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497 | ! thrid recurrence : SOLk = ( Lk - Uk * Ek+1 ) / Dk |
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498 | DO jk = 1, jpk-2 |
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499 | DO jj = jpjm1, 2, -1 |
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500 | DO ji = fs_jpim1, fs_2, -1 ! vector opt. |
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501 | ua_ad(ji,jj,jk+1) = ua_ad(ji,jj,jk+1) - ua_ad(ji,jj,jk) * zws(ji,jj,jk) / zwd(ji,jj,jk) |
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502 | ua_ad(ji,jj,jk) = ua_ad(ji,jj,jk) / zwd(ji,jj,jk) |
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503 | END DO |
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504 | END DO |
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505 | END DO |
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506 | DO jj = jpjm1, 2, -1 |
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507 | DO ji = fs_jpim1, fs_2, -1 |
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508 | ua_ad(ji,jj,jpkm1) = ua_ad(ji,jj,jpkm1) / zwd(ji,jj,jpkm1) |
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509 | END DO |
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510 | END DO |
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511 | DO jk = jpkm1, 2, -1 |
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512 | DO jj = jpjm1, 2, -1 |
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513 | DO ji = fs_jpim1, fs_2, -1 ! vector opt. |
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514 | zrhsad = zrhsad + ua_ad(ji,jj,jk) |
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515 | ua_ad(ji,jj,jk-1) = ua_ad(ji,jj,jk-1) - zwi(ji,jj,jk) / zwd(ji,jj,jk-1) * ua_ad(ji,jj,jk) |
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516 | ua_ad(ji,jj,jk) = 0.0_wp |
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517 | ub_ad(ji,jj,jk) = ub_ad(ji,jj,jk) + zrhsad |
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518 | ua_ad(ji,jj,jk) = ua_ad(ji,jj,jk) + zrhsad * p2dt |
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519 | zrhsad = 0.0_wp |
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520 | END DO |
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521 | END DO |
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522 | END DO |
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523 | ! second recurrence: SOLk = RHSk - Lk / Dk-1 Lk-1 |
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524 | DO jj = 2, jpjm1 |
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525 | DO ji = fs_2, fs_jpim1 ! vector opt. |
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526 | ub_ad(ji,jj,1) = ub_ad(ji,jj,1) + ua_ad(ji,jj,1) |
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527 | ua_ad(ji,jj,1) = p2dt * ua_ad(ji,jj,1) |
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528 | END DO |
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529 | END DO |
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530 | |
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531 | |
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532 | |
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533 | END SUBROUTINE dyn_zdf_imp_adj |
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534 | #endif |
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535 | !!============================================================================== |
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536 | END MODULE dynzdf_imp_tam |
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