1 | MODULE diffusion_v_mod |
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2 | |
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3 | !--------------------------------------------------------------------------------! |
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4 | ! This file is part of PALM. |
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5 | ! |
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6 | ! PALM is free software: you can redistribute it and/or modify it under the terms |
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7 | ! of the GNU General Public License as published by the Free Software Foundation, |
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8 | ! either version 3 of the License, or (at your option) any later version. |
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9 | ! |
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10 | ! PALM is distributed in the hope that it will be useful, but WITHOUT ANY |
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11 | ! WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS FOR |
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12 | ! A PARTICULAR PURPOSE. See the GNU General Public License for more details. |
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13 | ! |
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14 | ! You should have received a copy of the GNU General Public License along with |
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15 | ! PALM. If not, see <http://www.gnu.org/licenses/>. |
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16 | ! |
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17 | ! Copyright 1997-2014 Leibniz Universitaet Hannover |
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18 | !--------------------------------------------------------------------------------! |
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19 | ! |
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20 | ! Current revisions: |
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21 | ! ----------------- |
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22 | ! |
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23 | ! |
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24 | ! Former revisions: |
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25 | ! ----------------- |
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26 | ! $Id: diffusion_v.f90 1321 2014-03-20 09:40:40Z suehring $ |
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27 | ! |
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28 | ! 1320 2014-03-20 08:40:49Z raasch |
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29 | ! ONLY-attribute added to USE-statements, |
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30 | ! kind-parameters added to all INTEGER and REAL declaration statements, |
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31 | ! kinds are defined in new module kinds, |
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32 | ! revision history before 2012 removed, |
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33 | ! comment fields (!:) to be used for variable explanations added to |
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34 | ! all variable declaration statements |
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35 | ! |
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36 | ! 1257 2013-11-08 15:18:40Z raasch |
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37 | ! openacc loop and loop vector clauses removed, declare create moved after |
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38 | ! the FORTRAN declaration statement |
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39 | ! |
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40 | ! 1128 2013-04-12 06:19:32Z raasch |
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41 | ! loop index bounds in accelerator version replaced by i_left, i_right, j_south, |
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42 | ! j_north |
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43 | ! |
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44 | ! 1036 2012-10-22 13:43:42Z raasch |
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45 | ! code put under GPL (PALM 3.9) |
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46 | ! |
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47 | ! 1015 2012-09-27 09:23:24Z raasch |
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48 | ! accelerator version (*_acc) added |
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49 | ! |
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50 | ! 1001 2012-09-13 14:08:46Z raasch |
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51 | ! arrays comunicated by module instead of parameter list |
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52 | ! |
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53 | ! 978 2012-08-09 08:28:32Z fricke |
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54 | ! outflow damping layer removed |
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55 | ! kmxm_x/_y and kmxp_x/_y change to kmxm and kmxp |
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56 | ! |
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57 | ! Revision 1.1 1997/09/12 06:24:01 raasch |
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58 | ! Initial revision |
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59 | ! |
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60 | ! |
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61 | ! Description: |
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62 | ! ------------ |
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63 | ! Diffusion term of the v-component |
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64 | !------------------------------------------------------------------------------! |
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65 | |
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66 | USE wall_fluxes_mod |
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67 | |
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68 | PRIVATE |
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69 | PUBLIC diffusion_v, diffusion_v_acc |
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70 | |
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71 | INTERFACE diffusion_v |
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72 | MODULE PROCEDURE diffusion_v |
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73 | MODULE PROCEDURE diffusion_v_ij |
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74 | END INTERFACE diffusion_v |
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75 | |
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76 | INTERFACE diffusion_v_acc |
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77 | MODULE PROCEDURE diffusion_v_acc |
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78 | END INTERFACE diffusion_v_acc |
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79 | |
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80 | CONTAINS |
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81 | |
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82 | |
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83 | !------------------------------------------------------------------------------! |
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84 | ! Call for all grid points |
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85 | !------------------------------------------------------------------------------! |
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86 | SUBROUTINE diffusion_v |
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87 | |
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88 | USE arrays_3d, & |
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89 | ONLY: ddzu, ddzw, km, tend, u, v, vsws, vswst, w |
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90 | |
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91 | USE control_parameters, & |
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92 | ONLY: constant_top_momentumflux, topography, use_surface_fluxes, & |
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93 | use_top_fluxes |
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94 | |
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95 | USE grid_variables, & |
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96 | ONLY: ddx, ddy, ddy2, fxm, fxp, wall_v |
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97 | |
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98 | USE indices, & |
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99 | ONLY: nxl, nxr, nyn, nys, nysv, nzb, nzb_diff_v, nzb_v_inner, & |
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100 | nzb_v_outer, nzt, nzt_diff |
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101 | |
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102 | USE kinds |
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103 | |
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104 | IMPLICIT NONE |
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105 | |
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106 | INTEGER(iwp) :: i !: |
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107 | INTEGER(iwp) :: j !: |
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108 | INTEGER(iwp) :: k !: |
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109 | REAL(wp) :: kmxm !: |
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110 | REAL(wp) :: kmxp !: |
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111 | REAL(wp) :: kmzm !: |
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112 | REAL(wp) :: kmzp !: |
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113 | |
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114 | REAL(wp), DIMENSION(nzb:nzt+1,nys:nyn,nxl:nxr) :: vsus !: |
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115 | |
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116 | ! |
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117 | !-- First calculate horizontal momentum flux v'u' at vertical walls, |
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118 | !-- if neccessary |
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119 | IF ( topography /= 'flat' ) THEN |
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120 | CALL wall_fluxes( vsus, 0.0_wp, 1.0_wp, 0.0_wp, 0.0_wp, nzb_v_inner, & |
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121 | nzb_v_outer, wall_v ) |
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122 | ENDIF |
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123 | |
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124 | DO i = nxl, nxr |
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125 | DO j = nysv, nyn |
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126 | ! |
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127 | !-- Compute horizontal diffusion |
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128 | DO k = nzb_v_outer(j,i)+1, nzt |
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129 | ! |
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130 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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131 | kmxp = 0.25 * & |
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132 | ( km(k,j,i)+km(k,j,i+1)+km(k,j-1,i)+km(k,j-1,i+1) ) |
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133 | kmxm = 0.25 * & |
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134 | ( km(k,j,i)+km(k,j,i-1)+km(k,j-1,i)+km(k,j-1,i-1) ) |
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135 | |
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136 | tend(k,j,i) = tend(k,j,i) & |
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137 | & + ( kmxp * ( v(k,j,i+1) - v(k,j,i) ) * ddx & |
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138 | & + kmxp * ( u(k,j,i+1) - u(k,j-1,i+1) ) * ddy & |
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139 | & - kmxm * ( v(k,j,i) - v(k,j,i-1) ) * ddx & |
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140 | & - kmxm * ( u(k,j,i) - u(k,j-1,i) ) * ddy & |
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141 | & ) * ddx & |
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142 | & + 2.0 * ( & |
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143 | & km(k,j,i) * ( v(k,j+1,i) - v(k,j,i) ) & |
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144 | & - km(k,j-1,i) * ( v(k,j,i) - v(k,j-1,i) ) & |
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145 | & ) * ddy2 |
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146 | ENDDO |
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147 | |
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148 | ! |
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149 | !-- Wall functions at the left and right walls, respectively |
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150 | IF ( wall_v(j,i) /= 0.0 ) THEN |
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151 | |
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152 | DO k = nzb_v_inner(j,i)+1, nzb_v_outer(j,i) |
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153 | kmxp = 0.25 * & |
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154 | ( km(k,j,i)+km(k,j,i+1)+km(k,j-1,i)+km(k,j-1,i+1) ) |
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155 | kmxm = 0.25 * & |
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156 | ( km(k,j,i)+km(k,j,i-1)+km(k,j-1,i)+km(k,j-1,i-1) ) |
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157 | |
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158 | tend(k,j,i) = tend(k,j,i) & |
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159 | + 2.0 * ( & |
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160 | km(k,j,i) * ( v(k,j+1,i) - v(k,j,i) ) & |
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161 | - km(k,j-1,i) * ( v(k,j,i) - v(k,j-1,i) ) & |
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162 | ) * ddy2 & |
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163 | + ( fxp(j,i) * ( & |
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164 | kmxp * ( v(k,j,i+1) - v(k,j,i) ) * ddx & |
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165 | + kmxp * ( u(k,j,i+1) - u(k,j-1,i+1) ) * ddy & |
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166 | ) & |
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167 | - fxm(j,i) * ( & |
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168 | kmxm * ( v(k,j,i) - v(k,j,i-1) ) * ddx & |
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169 | + kmxm * ( u(k,j,i) - u(k,j-1,i) ) * ddy & |
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170 | ) & |
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171 | + wall_v(j,i) * vsus(k,j,i) & |
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172 | ) * ddx |
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173 | ENDDO |
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174 | ENDIF |
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175 | |
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176 | ! |
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177 | !-- Compute vertical diffusion. In case of simulating a Prandtl |
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178 | !-- layer, index k starts at nzb_v_inner+2. |
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179 | DO k = nzb_diff_v(j,i), nzt_diff |
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180 | ! |
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181 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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182 | kmzp = 0.25 * & |
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183 | ( km(k,j,i)+km(k+1,j,i)+km(k,j-1,i)+km(k+1,j-1,i) ) |
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184 | kmzm = 0.25 * & |
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185 | ( km(k,j,i)+km(k-1,j,i)+km(k,j-1,i)+km(k-1,j-1,i) ) |
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186 | |
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187 | tend(k,j,i) = tend(k,j,i) & |
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188 | & + ( kmzp * ( ( v(k+1,j,i) - v(k,j,i) ) * ddzu(k+1) & |
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189 | & + ( w(k,j,i) - w(k,j-1,i) ) * ddy & |
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190 | & ) & |
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191 | & - kmzm * ( ( v(k,j,i) - v(k-1,j,i) ) * ddzu(k) & |
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192 | & + ( w(k-1,j,i) - w(k-1,j-1,i) ) * ddy & |
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193 | & ) & |
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194 | & ) * ddzw(k) |
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195 | ENDDO |
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196 | |
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197 | ! |
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198 | !-- Vertical diffusion at the first grid point above the surface, |
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199 | !-- if the momentum flux at the bottom is given by the Prandtl law |
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200 | !-- or if it is prescribed by the user. |
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201 | !-- Difference quotient of the momentum flux is not formed over |
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202 | !-- half of the grid spacing (2.0*ddzw(k)) any more, since the |
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203 | !-- comparison with other (LES) models showed that the values of |
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204 | !-- the momentum flux becomes too large in this case. |
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205 | !-- The term containing w(k-1,..) (see above equation) is removed here |
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206 | !-- because the vertical velocity is assumed to be zero at the surface. |
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207 | IF ( use_surface_fluxes ) THEN |
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208 | k = nzb_v_inner(j,i)+1 |
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209 | ! |
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210 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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211 | kmzp = 0.25 * & |
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212 | ( km(k,j,i)+km(k+1,j,i)+km(k,j-1,i)+km(k+1,j-1,i) ) |
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213 | kmzm = 0.25 * & |
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214 | ( km(k,j,i)+km(k-1,j,i)+km(k,j-1,i)+km(k-1,j-1,i) ) |
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215 | |
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216 | tend(k,j,i) = tend(k,j,i) & |
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217 | & + ( kmzp * ( w(k,j,i) - w(k,j-1,i) ) * ddy & |
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218 | & ) * ddzw(k) & |
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219 | & + ( kmzp * ( v(k+1,j,i) - v(k,j,i) ) * ddzu(k+1) & |
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220 | & + vsws(j,i) & |
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221 | & ) * ddzw(k) |
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222 | ENDIF |
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223 | |
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224 | ! |
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225 | !-- Vertical diffusion at the first gridpoint below the top boundary, |
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226 | !-- if the momentum flux at the top is prescribed by the user |
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227 | IF ( use_top_fluxes .AND. constant_top_momentumflux ) THEN |
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228 | k = nzt |
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229 | ! |
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230 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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231 | kmzp = 0.25 * & |
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232 | ( km(k,j,i)+km(k+1,j,i)+km(k,j-1,i)+km(k+1,j-1,i) ) |
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233 | kmzm = 0.25 * & |
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234 | ( km(k,j,i)+km(k-1,j,i)+km(k,j-1,i)+km(k-1,j-1,i) ) |
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235 | |
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236 | tend(k,j,i) = tend(k,j,i) & |
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237 | & - ( kmzm * ( w(k-1,j,i) - w(k-1,j-1,i) ) * ddy & |
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238 | & ) * ddzw(k) & |
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239 | & + ( -vswst(j,i) & |
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240 | & - kmzm * ( v(k,j,i) - v(k-1,j,i) ) * ddzu(k) & |
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241 | & ) * ddzw(k) |
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242 | ENDIF |
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243 | |
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244 | ENDDO |
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245 | ENDDO |
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246 | |
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247 | END SUBROUTINE diffusion_v |
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248 | |
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249 | |
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250 | !------------------------------------------------------------------------------! |
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251 | ! Call for all grid points - accelerator version |
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252 | !------------------------------------------------------------------------------! |
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253 | SUBROUTINE diffusion_v_acc |
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254 | |
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255 | USE arrays_3d, & |
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256 | ONLY: ddzu, ddzw, km, tend, u, v, vsws, vswst, w |
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257 | |
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258 | USE control_parameters, & |
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259 | ONLY: constant_top_momentumflux, topography, use_surface_fluxes, & |
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260 | use_top_fluxes |
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261 | |
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262 | USE grid_variables, & |
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263 | ONLY: ddx, ddy, ddy2, fxm, fxp, wall_v |
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264 | |
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265 | USE indices, & |
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266 | ONLY: i_left, i_right, j_north, j_south, nxl, nxr, nyn, nys, nzb, & |
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267 | nzb_diff_v, nzb_v_inner, nzb_v_outer, nzt, nzt_diff |
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268 | |
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269 | USE kinds |
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270 | |
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271 | IMPLICIT NONE |
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272 | |
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273 | INTEGER(iwp) :: i !: |
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274 | INTEGER(iwp) :: j !: |
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275 | INTEGER(iwp) :: k !: |
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276 | REAL(wp) :: kmxm !: |
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277 | REAL(wp) :: kmxp !: |
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278 | REAL(wp) :: kmzm !: |
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279 | REAL(wp) :: kmzp !: |
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280 | |
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281 | REAL(wp), DIMENSION(nzb:nzt+1,nys:nyn,nxl:nxr) :: vsus !: |
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282 | !$acc declare create ( vsus ) |
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283 | |
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284 | ! |
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285 | !-- First calculate horizontal momentum flux v'u' at vertical walls, |
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286 | !-- if neccessary |
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287 | IF ( topography /= 'flat' ) THEN |
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288 | CALL wall_fluxes_acc( vsus, 0.0_wp, 1.0_wp, 0.0_wp, 0.0_wp, & |
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289 | nzb_v_inner, nzb_v_outer, wall_v ) |
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290 | ENDIF |
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291 | |
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292 | !$acc kernels present ( u, v, w, km, tend, vsws, vswst ) & |
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293 | !$acc present ( ddzu, ddzw, fxm, fxp, wall_v ) & |
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294 | !$acc present ( nzb_v_inner, nzb_v_outer, nzb_diff_v ) |
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295 | DO i = i_left, i_right |
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296 | DO j = j_south, j_north |
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297 | ! |
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298 | !-- Compute horizontal diffusion |
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299 | DO k = 1, nzt |
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300 | IF ( k > nzb_v_outer(j,i) ) THEN |
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301 | ! |
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302 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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303 | kmxp = 0.25 * & |
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304 | ( km(k,j,i)+km(k,j,i+1)+km(k,j-1,i)+km(k,j-1,i+1) ) |
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305 | kmxm = 0.25 * & |
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306 | ( km(k,j,i)+km(k,j,i-1)+km(k,j-1,i)+km(k,j-1,i-1) ) |
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307 | |
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308 | tend(k,j,i) = tend(k,j,i) & |
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309 | & + ( kmxp * ( v(k,j,i+1) - v(k,j,i) ) * ddx & |
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310 | & + kmxp * ( u(k,j,i+1) - u(k,j-1,i+1) ) * ddy & |
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311 | & - kmxm * ( v(k,j,i) - v(k,j,i-1) ) * ddx & |
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312 | & - kmxm * ( u(k,j,i) - u(k,j-1,i) ) * ddy & |
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313 | & ) * ddx & |
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314 | & + 2.0 * ( & |
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315 | & km(k,j,i) * ( v(k,j+1,i) - v(k,j,i) ) & |
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316 | & - km(k,j-1,i) * ( v(k,j,i) - v(k,j-1,i) ) & |
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317 | & ) * ddy2 |
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318 | ENDIF |
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319 | ENDDO |
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320 | |
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321 | ! |
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322 | !-- Wall functions at the left and right walls, respectively |
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323 | DO k = 1, nzt |
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324 | IF( k > nzb_v_inner(j,i) .AND. k <= nzb_v_outer(j,i) .AND. & |
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325 | wall_v(j,i) /= 0.0 ) THEN |
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326 | |
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327 | kmxp = 0.25 * & |
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328 | ( km(k,j,i)+km(k,j,i+1)+km(k,j-1,i)+km(k,j-1,i+1) ) |
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329 | kmxm = 0.25 * & |
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330 | ( km(k,j,i)+km(k,j,i-1)+km(k,j-1,i)+km(k,j-1,i-1) ) |
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331 | |
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332 | tend(k,j,i) = tend(k,j,i) & |
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333 | + 2.0 * ( & |
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334 | km(k,j,i) * ( v(k,j+1,i) - v(k,j,i) ) & |
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335 | - km(k,j-1,i) * ( v(k,j,i) - v(k,j-1,i) ) & |
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336 | ) * ddy2 & |
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337 | + ( fxp(j,i) * ( & |
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338 | kmxp * ( v(k,j,i+1) - v(k,j,i) ) * ddx & |
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339 | + kmxp * ( u(k,j,i+1) - u(k,j-1,i+1) ) * ddy & |
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340 | ) & |
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341 | - fxm(j,i) * ( & |
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342 | kmxm * ( v(k,j,i) - v(k,j,i-1) ) * ddx & |
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343 | + kmxm * ( u(k,j,i) - u(k,j-1,i) ) * ddy & |
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344 | ) & |
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345 | + wall_v(j,i) * vsus(k,j,i) & |
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346 | ) * ddx |
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347 | ENDIF |
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348 | ENDDO |
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349 | |
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350 | ! |
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351 | !-- Compute vertical diffusion. In case of simulating a Prandtl |
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352 | !-- layer, index k starts at nzb_v_inner+2. |
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353 | DO k = 1, nzt_diff |
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354 | IF ( k >= nzb_diff_v(j,i) ) THEN |
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355 | ! |
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356 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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357 | kmzp = 0.25 * & |
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358 | ( km(k,j,i)+km(k+1,j,i)+km(k,j-1,i)+km(k+1,j-1,i) ) |
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359 | kmzm = 0.25 * & |
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360 | ( km(k,j,i)+km(k-1,j,i)+km(k,j-1,i)+km(k-1,j-1,i) ) |
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361 | |
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362 | tend(k,j,i) = tend(k,j,i) & |
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363 | & + ( kmzp * ( ( v(k+1,j,i) - v(k,j,i) ) * ddzu(k+1)& |
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364 | & + ( w(k,j,i) - w(k,j-1,i) ) * ddy & |
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365 | & ) & |
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366 | & - kmzm * ( ( v(k,j,i) - v(k-1,j,i) ) * ddzu(k)& |
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367 | & + ( w(k-1,j,i) - w(k-1,j-1,i) ) * ddy & |
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368 | & ) & |
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369 | & ) * ddzw(k) |
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370 | ENDIF |
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371 | ENDDO |
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372 | |
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373 | ENDDO |
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374 | ENDDO |
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375 | |
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376 | ! |
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377 | !-- Vertical diffusion at the first grid point above the surface, |
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378 | !-- if the momentum flux at the bottom is given by the Prandtl law |
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379 | !-- or if it is prescribed by the user. |
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380 | !-- Difference quotient of the momentum flux is not formed over |
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381 | !-- half of the grid spacing (2.0*ddzw(k)) any more, since the |
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382 | !-- comparison with other (LES) models showed that the values of |
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383 | !-- the momentum flux becomes too large in this case. |
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384 | !-- The term containing w(k-1,..) (see above equation) is removed here |
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385 | !-- because the vertical velocity is assumed to be zero at the surface. |
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386 | IF ( use_surface_fluxes ) THEN |
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387 | |
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388 | DO i = i_left, i_right |
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389 | DO j = j_south, j_north |
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390 | |
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391 | k = nzb_v_inner(j,i)+1 |
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392 | ! |
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393 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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394 | kmzp = 0.25 * & |
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395 | ( km(k,j,i)+km(k+1,j,i)+km(k,j-1,i)+km(k+1,j-1,i) ) |
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396 | kmzm = 0.25 * & |
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397 | ( km(k,j,i)+km(k-1,j,i)+km(k,j-1,i)+km(k-1,j-1,i) ) |
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398 | |
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399 | tend(k,j,i) = tend(k,j,i) & |
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400 | & + ( kmzp * ( w(k,j,i) - w(k,j-1,i) ) * ddy & |
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401 | & ) * ddzw(k) & |
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402 | & + ( kmzp * ( v(k+1,j,i) - v(k,j,i) ) * ddzu(k+1) & |
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403 | & + vsws(j,i) & |
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404 | & ) * ddzw(k) |
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405 | ENDDO |
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406 | ENDDO |
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407 | |
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408 | ENDIF |
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409 | |
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410 | ! |
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411 | !-- Vertical diffusion at the first gridpoint below the top boundary, |
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412 | !-- if the momentum flux at the top is prescribed by the user |
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413 | IF ( use_top_fluxes .AND. constant_top_momentumflux ) THEN |
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414 | |
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415 | k = nzt |
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416 | |
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417 | DO i = i_left, i_right |
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418 | DO j = j_south, j_north |
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419 | |
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420 | ! |
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421 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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422 | kmzp = 0.25 * & |
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423 | ( km(k,j,i)+km(k+1,j,i)+km(k,j-1,i)+km(k+1,j-1,i) ) |
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424 | kmzm = 0.25 * & |
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425 | ( km(k,j,i)+km(k-1,j,i)+km(k,j-1,i)+km(k-1,j-1,i) ) |
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426 | |
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427 | tend(k,j,i) = tend(k,j,i) & |
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428 | & - ( kmzm * ( w(k-1,j,i) - w(k-1,j-1,i) ) * ddy & |
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429 | & ) * ddzw(k) & |
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430 | & + ( -vswst(j,i) & |
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431 | & - kmzm * ( v(k,j,i) - v(k-1,j,i) ) * ddzu(k) & |
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432 | & ) * ddzw(k) |
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433 | ENDDO |
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434 | ENDDO |
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435 | |
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436 | ENDIF |
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437 | !$acc end kernels |
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438 | |
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439 | END SUBROUTINE diffusion_v_acc |
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440 | |
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441 | |
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442 | !------------------------------------------------------------------------------! |
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443 | ! Call for grid point i,j |
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444 | !------------------------------------------------------------------------------! |
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445 | SUBROUTINE diffusion_v_ij( i, j ) |
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446 | |
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447 | USE arrays_3d, & |
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448 | ONLY: ddzu, ddzw, km, tend, u, v, vsws, vswst, w |
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449 | |
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450 | USE control_parameters, & |
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451 | ONLY: constant_top_momentumflux, use_surface_fluxes, use_top_fluxes |
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452 | |
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453 | USE grid_variables, & |
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454 | ONLY: ddx, ddy, ddy2, fxm, fxp, wall_v |
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455 | |
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456 | USE indices, & |
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457 | ONLY: nzb, nzb_diff_v, nzb_v_inner, nzb_v_outer, nzt, nzt_diff |
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458 | |
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459 | USE kinds |
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460 | |
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461 | IMPLICIT NONE |
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462 | |
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463 | INTEGER(iwp) :: i !: |
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464 | INTEGER(iwp) :: j !: |
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465 | INTEGER(iwp) :: k !: |
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466 | REAL(wp) :: kmxm !: |
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467 | REAL(wp) :: kmxp !: |
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468 | REAL(wp) :: kmzm !: |
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469 | REAL(wp) :: kmzp !: |
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470 | |
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471 | REAL(wp), DIMENSION(nzb:nzt+1) :: vsus !: |
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472 | |
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473 | ! |
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474 | !-- Compute horizontal diffusion |
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475 | DO k = nzb_v_outer(j,i)+1, nzt |
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476 | ! |
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477 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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478 | kmxp = 0.25 * ( km(k,j,i)+km(k,j,i+1)+km(k,j-1,i)+km(k,j-1,i+1) ) |
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479 | kmxm = 0.25 * ( km(k,j,i)+km(k,j,i-1)+km(k,j-1,i)+km(k,j-1,i-1) ) |
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480 | |
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481 | tend(k,j,i) = tend(k,j,i) & |
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482 | & + ( kmxp * ( v(k,j,i+1) - v(k,j,i) ) * ddx & |
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483 | & + kmxp * ( u(k,j,i+1) - u(k,j-1,i+1) ) * ddy & |
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484 | & - kmxm * ( v(k,j,i) - v(k,j,i-1) ) * ddx & |
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485 | & - kmxm * ( u(k,j,i) - u(k,j-1,i) ) * ddy & |
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486 | & ) * ddx & |
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487 | & + 2.0 * ( & |
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488 | & km(k,j,i) * ( v(k,j+1,i) - v(k,j,i) ) & |
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489 | & - km(k,j-1,i) * ( v(k,j,i) - v(k,j-1,i) ) & |
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490 | & ) * ddy2 |
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491 | ENDDO |
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492 | |
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493 | ! |
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494 | !-- Wall functions at the left and right walls, respectively |
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495 | IF ( wall_v(j,i) /= 0.0 ) THEN |
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496 | |
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497 | ! |
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498 | !-- Calculate the horizontal momentum flux v'u' |
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499 | CALL wall_fluxes( i, j, nzb_v_inner(j,i)+1, nzb_v_outer(j,i), & |
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500 | vsus, 0.0_wp, 1.0_wp, 0.0_wp, 0.0_wp ) |
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501 | |
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502 | DO k = nzb_v_inner(j,i)+1, nzb_v_outer(j,i) |
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503 | kmxp = 0.25 * & |
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504 | ( km(k,j,i)+km(k,j,i+1)+km(k,j-1,i)+km(k,j-1,i+1) ) |
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505 | kmxm = 0.25 * & |
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506 | ( km(k,j,i)+km(k,j,i-1)+km(k,j-1,i)+km(k,j-1,i-1) ) |
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507 | |
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508 | tend(k,j,i) = tend(k,j,i) & |
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509 | + 2.0 * ( & |
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510 | km(k,j,i) * ( v(k,j+1,i) - v(k,j,i) ) & |
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511 | - km(k,j-1,i) * ( v(k,j,i) - v(k,j-1,i) ) & |
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512 | ) * ddy2 & |
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513 | + ( fxp(j,i) * ( & |
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514 | kmxp * ( v(k,j,i+1) - v(k,j,i) ) * ddx & |
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515 | + kmxp * ( u(k,j,i+1) - u(k,j-1,i+1) ) * ddy & |
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516 | ) & |
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517 | - fxm(j,i) * ( & |
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518 | kmxm * ( v(k,j,i) - v(k,j,i-1) ) * ddx & |
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519 | + kmxm * ( u(k,j,i) - u(k,j-1,i) ) * ddy & |
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520 | ) & |
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521 | + wall_v(j,i) * vsus(k) & |
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522 | ) * ddx |
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523 | ENDDO |
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524 | ENDIF |
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525 | |
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526 | ! |
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527 | !-- Compute vertical diffusion. In case of simulating a Prandtl layer, |
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528 | !-- index k starts at nzb_v_inner+2. |
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529 | DO k = nzb_diff_v(j,i), nzt_diff |
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530 | ! |
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531 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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532 | kmzp = 0.25 * ( km(k,j,i)+km(k+1,j,i)+km(k,j-1,i)+km(k+1,j-1,i) ) |
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533 | kmzm = 0.25 * ( km(k,j,i)+km(k-1,j,i)+km(k,j-1,i)+km(k-1,j-1,i) ) |
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534 | |
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535 | tend(k,j,i) = tend(k,j,i) & |
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536 | & + ( kmzp * ( ( v(k+1,j,i) - v(k,j,i) ) * ddzu(k+1) & |
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537 | & + ( w(k,j,i) - w(k,j-1,i) ) * ddy & |
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538 | & ) & |
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539 | & - kmzm * ( ( v(k,j,i) - v(k-1,j,i) ) * ddzu(k) & |
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540 | & + ( w(k-1,j,i) - w(k-1,j-1,i) ) * ddy & |
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541 | & ) & |
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542 | & ) * ddzw(k) |
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543 | ENDDO |
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544 | |
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545 | ! |
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546 | !-- Vertical diffusion at the first grid point above the surface, if the |
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547 | !-- momentum flux at the bottom is given by the Prandtl law or if it is |
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548 | !-- prescribed by the user. |
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549 | !-- Difference quotient of the momentum flux is not formed over half of |
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550 | !-- the grid spacing (2.0*ddzw(k)) any more, since the comparison with |
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551 | !-- other (LES) models showed that the values of the momentum flux becomes |
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552 | !-- too large in this case. |
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553 | !-- The term containing w(k-1,..) (see above equation) is removed here |
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554 | !-- because the vertical velocity is assumed to be zero at the surface. |
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555 | IF ( use_surface_fluxes ) THEN |
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556 | k = nzb_v_inner(j,i)+1 |
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557 | ! |
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558 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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559 | kmzp = 0.25 * ( km(k,j,i)+km(k+1,j,i)+km(k,j-1,i)+km(k+1,j-1,i) ) |
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560 | kmzm = 0.25 * ( km(k,j,i)+km(k-1,j,i)+km(k,j-1,i)+km(k-1,j-1,i) ) |
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561 | |
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562 | tend(k,j,i) = tend(k,j,i) & |
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563 | & + ( kmzp * ( w(k,j,i) - w(k,j-1,i) ) * ddy & |
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564 | & ) * ddzw(k) & |
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565 | & + ( kmzp * ( v(k+1,j,i) - v(k,j,i) ) * ddzu(k+1) & |
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566 | & + vsws(j,i) & |
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567 | & ) * ddzw(k) |
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568 | ENDIF |
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569 | |
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570 | ! |
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571 | !-- Vertical diffusion at the first gridpoint below the top boundary, |
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572 | !-- if the momentum flux at the top is prescribed by the user |
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573 | IF ( use_top_fluxes .AND. constant_top_momentumflux ) THEN |
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574 | k = nzt |
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575 | ! |
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576 | !-- Interpolate eddy diffusivities on staggered gridpoints |
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577 | kmzp = 0.25 * & |
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578 | ( km(k,j,i)+km(k+1,j,i)+km(k,j-1,i)+km(k+1,j-1,i) ) |
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579 | kmzm = 0.25 * & |
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580 | ( km(k,j,i)+km(k-1,j,i)+km(k,j-1,i)+km(k-1,j-1,i) ) |
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581 | |
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582 | tend(k,j,i) = tend(k,j,i) & |
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583 | & - ( kmzm * ( w(k-1,j,i) - w(k-1,j-1,i) ) * ddy & |
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584 | & ) * ddzw(k) & |
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585 | & + ( -vswst(j,i) & |
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586 | & - kmzm * ( v(k,j,i) - v(k-1,j,i) ) * ddzu(k) & |
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587 | & ) * ddzw(k) |
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588 | ENDIF |
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589 | |
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590 | END SUBROUTINE diffusion_v_ij |
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591 | |
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592 | END MODULE diffusion_v_mod |
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