1 | SUBROUTINE init_advec |
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2 | |
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3 | !------------------------------------------------------------------------------! |
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4 | ! Current revisions: |
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5 | ! ----------------- |
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6 | ! |
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7 | ! |
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8 | ! Former revisions: |
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9 | ! ----------------- |
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10 | ! $Id: init_advec.f90 484 2010-02-05 07:36:54Z weinreis $ |
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11 | ! RCS Log replace by Id keyword, revision history cleaned up |
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12 | ! |
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13 | ! Revision 1.6 2004/04/30 11:59:31 raasch |
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14 | ! impulse_advec renamed momentum_advec |
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15 | ! |
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16 | ! Revision 1.1 1999/02/05 09:07:38 raasch |
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17 | ! Initial revision |
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18 | ! |
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19 | ! |
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20 | ! Description: |
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21 | ! ------------ |
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22 | ! Initialize constant coefficients and parameters for certain advection schemes. |
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23 | !------------------------------------------------------------------------------! |
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24 | |
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25 | USE advection |
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26 | USE arrays_3d |
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27 | USE indices |
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28 | USE control_parameters |
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29 | |
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30 | IMPLICIT NONE |
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31 | |
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32 | INTEGER :: i, intervals, j, k |
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33 | REAL :: delt, dn, dnneu, ex1, ex2, ex3, ex4, ex5, ex6, spl_alpha, & |
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34 | spl_beta, sterm |
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35 | REAL, DIMENSION(:), ALLOCATABLE :: spl_u, temp |
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36 | |
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37 | |
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38 | IF ( scalar_advec == 'bc-scheme' ) THEN |
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39 | |
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40 | ! |
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41 | !-- Compute exponential coefficients for the Bott-Chlond scheme |
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42 | intervals = 1000 |
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43 | ALLOCATE( aex(intervals), bex(intervals), dex(intervals), eex(intervals) ) |
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44 | |
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45 | delt = 1.0 / REAL( intervals ) |
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46 | sterm = delt * 0.5 |
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47 | |
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48 | DO i = 1, intervals |
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49 | |
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50 | IF ( sterm > 0.5 ) THEN |
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51 | dn = -5.0 |
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52 | ELSE |
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53 | dn = 5.0 |
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54 | ENDIF |
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55 | |
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56 | DO j = 1, 15 |
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57 | ex1 = dn * EXP( -dn ) - EXP( 0.5 * dn ) + EXP( -0.5 * dn ) |
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58 | ex2 = EXP( dn ) - EXP( -dn ) |
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59 | ex3 = EXP( -dn ) * ( 1.0 - dn ) - 0.5 * EXP( 0.5 * dn ) & |
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60 | - 0.5 * EXP( -0.5 * dn ) |
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61 | ex4 = EXP( dn ) + EXP( -dn ) |
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62 | ex5 = dn * sterm + ex1 / ex2 |
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63 | ex6 = sterm + ( ex3 * ex2 - ex4 * ex1 ) / ( ex2 * ex2 ) |
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64 | dnneu = dn - ex5 / ex6 |
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65 | dn = dnneu |
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66 | ENDDO |
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67 | |
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68 | IF ( sterm < 0.5 ) dn = MAX( 2.95E-2, dn ) |
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69 | IF ( sterm > 0.5 ) dn = MIN( -2.95E-2, dn ) |
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70 | ex1 = EXP( -dn ) |
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71 | ex2 = EXP( dn ) - ex1 |
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72 | aex(i) = -ex1 / ex2 |
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73 | bex(i) = 1.0 / ex2 |
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74 | dex(i) = dn |
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75 | eex(i) = EXP( dex(i) * 0.5 ) |
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76 | sterm = sterm + delt |
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77 | |
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78 | ENDDO |
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79 | |
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80 | ENDIF |
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81 | |
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82 | IF ( momentum_advec == 'ups-scheme' .OR. scalar_advec == 'ups-scheme' ) & |
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83 | THEN |
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84 | |
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85 | ! |
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86 | !-- Provide the constant parameters for the Upstream-Spline advection scheme. |
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87 | !-- In x- und y-direction the Sherman-Morrison formula is applied |
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88 | !-- (cf. Press et al, 1986 (Numerical Recipes)). |
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89 | ! |
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90 | !-- Allocate nonlocal arrays |
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91 | ALLOCATE( spl_z_x(0:nx), spl_z_y(0:ny), spl_tri_x(5,0:nx), & |
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92 | spl_tri_y(5,0:ny), spl_tri_zu(5,nzb:nzt+1), & |
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93 | spl_tri_zw(5,nzb:nzt+1) ) |
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94 | |
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95 | ! |
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96 | !-- Provide diagonal elements of the tridiagonal matrices for all |
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97 | !-- directions |
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98 | spl_tri_x(1,:) = 2.0 |
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99 | spl_tri_y(1,:) = 2.0 |
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100 | spl_tri_zu(1,:) = 2.0 |
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101 | spl_tri_zw(1,:) = 2.0 |
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102 | |
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103 | ! |
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104 | !-- Elements of the cyclic tridiagonal matrix |
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105 | !-- (same for all horizontal directions) |
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106 | spl_alpha = 0.5 |
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107 | spl_beta = 0.5 |
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108 | |
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109 | ! |
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110 | !-- Sub- and superdiagonal elements, x-direction |
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111 | spl_tri_x(2,0:nx) = 0.5 |
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112 | spl_tri_x(3,0:nx) = 0.5 |
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113 | |
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114 | ! |
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115 | !-- mMdify the diagonal elements (Sherman-Morrison) |
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116 | spl_gamma_x = -spl_tri_x(1,0) |
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117 | spl_tri_x(1,0) = spl_tri_x(1,0) - spl_gamma_x |
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118 | spl_tri_x(1,nx) = spl_tri_x(1,nx) - spl_alpha * spl_beta / spl_gamma_x |
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119 | |
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120 | ! |
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121 | !-- Split the tridiagonal matrix for Thomas algorithm |
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122 | spl_tri_x(4,0) = spl_tri_x(1,0) |
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123 | DO i = 1, nx |
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124 | spl_tri_x(5,i) = spl_tri_x(2,i) / spl_tri_x(4,i-1) |
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125 | spl_tri_x(4,i) = spl_tri_x(1,i) - spl_tri_x(5,i) * spl_tri_x(3,i-1) |
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126 | ENDDO |
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127 | |
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128 | ! |
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129 | !-- Allocate arrays required locally |
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130 | ALLOCATE( temp(0:nx), spl_u(0:nx) ) |
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131 | |
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132 | ! |
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133 | !-- Provide "corrective vector", x-direction |
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134 | spl_u(0) = spl_gamma_x |
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135 | spl_u(1:nx-1) = 0.0 |
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136 | spl_u(nx) = spl_alpha |
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137 | |
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138 | ! |
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139 | !-- Solve the system of equations for the corrective vector |
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140 | !-- (Sherman-Morrison) |
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141 | temp(0) = spl_u(0) |
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142 | DO i = 1, nx |
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143 | temp(i) = spl_u(i) - spl_tri_x(5,i) * temp(i-1) |
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144 | ENDDO |
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145 | spl_z_x(nx) = temp(nx) / spl_tri_x(4,nx) |
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146 | DO i = nx-1, 0, -1 |
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147 | spl_z_x(i) = ( temp(i) - spl_tri_x(3,i) * spl_z_x(i+1) ) / & |
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148 | spl_tri_x(4,i) |
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149 | ENDDO |
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150 | |
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151 | ! |
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152 | !-- Deallocate local arrays, for they are allocated in a different way for |
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153 | !-- operations in y-direction |
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154 | DEALLOCATE( temp, spl_u ) |
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155 | |
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156 | ! |
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157 | !-- Provide sub- and superdiagonal elements, y-direction |
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158 | spl_tri_y(2,0:ny) = 0.5 |
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159 | spl_tri_y(3,0:ny) = 0.5 |
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160 | |
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161 | ! |
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162 | !-- Modify the diagonal elements (Sherman-Morrison) |
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163 | spl_gamma_y = -spl_tri_y(1,0) |
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164 | spl_tri_y(1,0) = spl_tri_y(1,0) - spl_gamma_y |
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165 | spl_tri_y(1,ny) = spl_tri_y(1,ny) - spl_alpha * spl_beta / spl_gamma_y |
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166 | |
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167 | ! |
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168 | !-- Split the tridiagonal matrix for Thomas algorithm |
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169 | spl_tri_y(4,0) = spl_tri_y(1,0) |
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170 | DO j = 1, ny |
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171 | spl_tri_y(5,j) = spl_tri_y(2,j) / spl_tri_y(4,j-1) |
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172 | spl_tri_y(4,j) = spl_tri_y(1,j) - spl_tri_y(5,j) * spl_tri_y(3,j-1) |
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173 | ENDDO |
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174 | |
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175 | ! |
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176 | !-- Allocate arrays required locally |
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177 | ALLOCATE( temp(0:ny), spl_u(0:ny) ) |
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178 | |
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179 | ! |
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180 | !-- Provide "corrective vector", y-direction |
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181 | spl_u(0) = spl_gamma_y |
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182 | spl_u(1:ny-1) = 0.0 |
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183 | spl_u(ny) = spl_alpha |
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184 | |
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185 | ! |
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186 | !-- Solve the system of equations for the corrective vector |
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187 | !-- (Sherman-Morrison) |
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188 | temp = 0.0 |
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189 | spl_z_y = 0.0 |
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190 | temp(0) = spl_u(0) |
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191 | DO j = 1, ny |
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192 | temp(j) = spl_u(j) - spl_tri_y(5,j) * temp(j-1) |
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193 | ENDDO |
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194 | spl_z_y(ny) = temp(ny) / spl_tri_y(4,ny) |
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195 | DO j = ny-1, 0, -1 |
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196 | spl_z_y(j) = ( temp(j) - spl_tri_y(3,j) * spl_z_y(j+1) ) / & |
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197 | spl_tri_y(4,j) |
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198 | ENDDO |
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199 | |
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200 | ! |
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201 | !-- deallocate local arrays, for they are no longer required |
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202 | DEALLOCATE( temp, spl_u ) |
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203 | |
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204 | ! |
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205 | !-- provide sub- and superdiagonal elements, z-direction |
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206 | spl_tri_zu(2,nzb) = 0.0 |
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207 | spl_tri_zu(2,nzt+1) = 1.0 |
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208 | spl_tri_zw(2,nzb) = 0.0 |
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209 | spl_tri_zw(2,nzt+1) = 1.0 |
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210 | |
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211 | spl_tri_zu(3,nzb) = 1.0 |
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212 | spl_tri_zu(3,nzt+1) = 0.0 |
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213 | spl_tri_zw(3,nzb) = 1.0 |
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214 | spl_tri_zw(3,nzt+1) = 0.0 |
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215 | |
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216 | DO k = nzb+1, nzt |
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217 | spl_tri_zu(2,k) = dzu(k) / ( dzu(k) + dzu(k+1) ) |
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218 | spl_tri_zw(2,k) = dzw(k) / ( dzw(k) + dzw(k+1) ) |
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219 | spl_tri_zu(3,k) = 1.0 - spl_tri_zu(2,k) |
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220 | spl_tri_zw(3,k) = 1.0 - spl_tri_zw(2,k) |
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221 | ENDDO |
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222 | |
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223 | spl_tri_zu(4,nzb) = spl_tri_zu(1,nzb) |
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224 | spl_tri_zw(4,nzb) = spl_tri_zw(1,nzb) |
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225 | DO k = nzb+1, nzt+1 |
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226 | spl_tri_zu(5,k) = spl_tri_zu(2,k) / spl_tri_zu(4,k-1) |
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227 | spl_tri_zw(5,k) = spl_tri_zw(2,k) / spl_tri_zw(4,k-1) |
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228 | spl_tri_zu(4,k) = spl_tri_zu(1,k) - spl_tri_zu(5,k) * & |
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229 | spl_tri_zu(3,k-1) |
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230 | spl_tri_zw(4,k) = spl_tri_zw(1,k) - spl_tri_zw(5,k) * & |
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231 | spl_tri_zw(3,k-1) |
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232 | ENDDO |
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233 | |
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234 | ENDIF |
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235 | |
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236 | END SUBROUTINE init_advec |
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