1 | !> @file init_rankine.f90 |
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2 | !--------------------------------------------------------------------------------------------------! |
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3 | ! This file is part of the PALM model system. |
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4 | ! |
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5 | ! PALM is free software: you can redistribute it and/or modify it under the terms of the GNU General |
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6 | ! Public License as published by the Free Software Foundation, either version 3 of the License, or |
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7 | ! (at your option) any later version. |
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8 | ! |
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9 | ! PALM is distributed in the hope that it will be useful, but WITHOUT ANY WARRANTY; without even the |
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10 | ! implied warranty of MERCHANTABILITY or FITNESS FOR A PARTICULAR PURPOSE. See the GNU General |
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11 | ! Public License for more details. |
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12 | ! |
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13 | ! You should have received a copy of the GNU General Public License along with PALM. If not, see |
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14 | ! <http://www.gnu.org/licenses/>. |
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15 | ! |
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16 | ! Copyright 1997-2020 Leibniz Universitaet Hannover |
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17 | !--------------------------------------------------------------------------------------------------! |
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18 | ! |
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19 | ! Current revisions: |
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20 | ! ----------------- |
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21 | ! |
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22 | ! |
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23 | ! Former revisions: |
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24 | ! ----------------- |
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25 | ! $Id: init_rankine.f90 4648 2020-08-25 07:52:08Z raasch $ |
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26 | ! file re-formatted to follow the PALM coding standard |
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27 | ! |
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28 | ! 4457 2020-03-11 14:20:43Z raasch |
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29 | ! use statement for exchange horiz added |
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30 | ! |
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31 | ! 4360 2020-01-07 11:25:50Z suehring |
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32 | ! Corrected "Former revisions" section |
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33 | ! |
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34 | ! 3655 2019-01-07 16:51:22Z knoop |
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35 | ! Modularization of all bulk cloud physics code components |
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36 | ! |
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37 | ! Revision 1.1 1997/08/11 06:18:43 raasch |
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38 | ! Initial revision |
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39 | ! |
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40 | ! |
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41 | ! Description: |
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42 | ! ------------ |
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43 | !> Initialize a (nondivergent) Rankine eddy with a vertical axis in order to test the advection |
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44 | !> terms and the pressure solver. |
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45 | !--------------------------------------------------------------------------------------------------! |
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46 | SUBROUTINE init_rankine |
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47 | |
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48 | |
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49 | USE arrays_3d, & |
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50 | ONLY: pt, pt_init, u, u_init, v, v_init |
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51 | |
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52 | USE control_parameters, & |
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53 | ONLY: initializing_actions, n_sor, nsor, nsor_ini |
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54 | |
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55 | USE basic_constants_and_equations_mod, & |
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56 | ONLY: pi |
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57 | |
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58 | USE exchange_horiz_mod, & |
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59 | ONLY: exchange_horiz |
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60 | |
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61 | USE grid_variables, & |
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62 | ONLY: dx, dy |
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63 | |
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64 | USE indices, & |
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65 | ONLY: nbgp, nx, nxl, nxlg, nxr, nxrg, nyn, nyng, nys, nysg, nzb, nzt |
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66 | |
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67 | USE kinds |
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68 | |
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69 | IMPLICIT NONE |
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70 | |
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71 | INTEGER(iwp) :: i !< |
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72 | INTEGER(iwp) :: ic !< |
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73 | INTEGER(iwp) :: j !< |
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74 | INTEGER(iwp) :: jc !< |
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75 | INTEGER(iwp) :: k !< |
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76 | INTEGER(iwp) :: kc1 !< |
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77 | INTEGER(iwp) :: kc2 !< |
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78 | |
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79 | REAL(wp) :: alpha !< |
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80 | REAL(wp) :: betrag !< |
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81 | REAL(wp) :: radius !< |
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82 | REAL(wp) :: rc !< |
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83 | REAL(wp) :: uw !< |
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84 | REAL(wp) :: vw !< |
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85 | REAL(wp) :: x !< |
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86 | REAL(wp) :: y !< |
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87 | |
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88 | ! |
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89 | !-- Default: eddy radius rc, eddy strength z, |
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90 | !-- position of eddy centre: ic, jc, kc1, kc2 |
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91 | rc = 4.0_wp * dx |
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92 | ic = ( nx+1 ) / 2 |
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93 | jc = ic |
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94 | kc1 = nzb |
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95 | kc2 = nzt+1 |
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96 | |
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97 | ! |
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98 | !-- Reset initial profiles to constant profiles |
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99 | IF ( INDEX(initializing_actions, 'set_constant_profiles') /= 0 ) THEN |
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100 | DO i = nxlg, nxrg |
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101 | DO j = nysg, nyng |
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102 | pt(:,j,i) = pt_init |
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103 | u(:,j,i) = u_init |
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104 | v(:,j,i) = v_init |
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105 | ENDDO |
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106 | ENDDO |
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107 | ENDIF |
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108 | |
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109 | ! |
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110 | !-- Compute the u-component. |
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111 | DO i = nxl, nxr |
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112 | DO j = nys, nyn |
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113 | x = ( i - ic - 0.5_wp ) * dx |
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114 | y = ( j - jc ) * dy |
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115 | radius = SQRT( x**2 + y**2 ) |
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116 | IF ( radius <= 2.0_wp * rc ) THEN |
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117 | betrag = radius / ( 2.0_wp * rc ) * 0.08_wp |
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118 | ELSEIF ( radius > 2.0_wp * rc .AND. radius < 8.0_wp * rc ) THEN |
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119 | betrag = 0.08_wp * EXP( -( radius - 2.0_wp * rc ) / 2.0_wp ) |
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120 | ELSE |
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121 | betrag = 0.0_wp |
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122 | ENDIF |
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123 | |
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124 | IF ( x == 0.0_wp ) THEN |
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125 | IF ( y > 0.0_wp ) THEN |
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126 | alpha = pi / 2.0_wp |
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127 | ELSEIF ( y < 0.0_wp ) THEN |
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128 | alpha = 3.0_wp * pi / 2.0_wp |
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129 | ENDIF |
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130 | ELSE |
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131 | IF ( x < 0.0_wp ) THEN |
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132 | alpha = ATAN( y / x ) + pi |
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133 | ELSE |
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134 | IF ( y < 0.0_wp ) THEN |
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135 | alpha = ATAN( y / x ) + 2.0_wp * pi |
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136 | ELSE |
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137 | alpha = ATAN( y / x ) |
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138 | ENDIF |
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139 | ENDIF |
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140 | ENDIF |
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141 | |
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142 | uw = -SIN( alpha ) * betrag |
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143 | |
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144 | DO k = kc1, kc2 |
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145 | u(k,j,i) = u(k,j,i) + uw |
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146 | ENDDO |
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147 | ENDDO |
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148 | ENDDO |
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149 | |
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150 | ! |
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151 | !-- Compute the v-component. |
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152 | DO i = nxl, nxr |
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153 | DO j = nys, nyn |
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154 | x = ( i - ic ) * dx |
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155 | y = ( j - jc - 0.5_wp ) * dy |
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156 | radius = SQRT( x**2 + y**2 ) |
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157 | IF ( radius <= 2.0_wp * rc ) THEN |
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158 | betrag = radius / ( 2.0_wp * rc ) * 0.08_wp |
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159 | ELSEIF ( radius > 2.0_wp * rc .AND. radius < 8.0_wp * rc ) THEN |
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160 | betrag = 0.08_wp * EXP( -( radius - 2.0_wp * rc ) / 2.0_wp ) |
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161 | ELSE |
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162 | betrag = 0.0_wp |
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163 | ENDIF |
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164 | |
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165 | IF ( x == 0.0_wp ) THEN |
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166 | IF ( y > 0.0_wp ) THEN |
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167 | alpha = pi / 2.0_wp |
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168 | ELSEIF ( y < 0.0_wp ) THEN |
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169 | alpha = 3.0_wp * pi / 2.0_wp |
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170 | ENDIF |
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171 | ELSE |
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172 | IF ( x < 0.0_wp ) THEN |
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173 | alpha = ATAN( y / x ) + pi |
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174 | ELSE |
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175 | IF ( y < 0.0_wp ) THEN |
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176 | alpha = ATAN( y / x ) + 2.0_wp * pi |
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177 | ELSE |
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178 | alpha = ATAN( y / x ) |
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179 | ENDIF |
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180 | ENDIF |
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181 | ENDIF |
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182 | |
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183 | vw = COS( alpha ) * betrag |
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184 | |
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185 | DO k = kc1, kc2 |
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186 | v(k,j,i) = v(k,j,i) + vw |
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187 | ENDDO |
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188 | ENDDO |
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189 | ENDDO |
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190 | |
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191 | ! |
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192 | !-- Exchange of boundary values for the velocities. |
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193 | CALL exchange_horiz( u, nbgp) |
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194 | CALL exchange_horiz( v, nbgp ) |
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195 | ! |
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196 | !-- Make velocity field nondivergent. |
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197 | n_sor = nsor_ini |
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198 | CALL pres |
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199 | n_sor = nsor |
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200 | |
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201 | END SUBROUTINE init_rankine |
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