1 | SUBROUTINE boundary_conds |
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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: boundary_conds.f90 1362 2014-04-16 15:19:12Z hoffmann $ |
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27 | ! |
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28 | ! 1361 2014-04-16 15:17:48Z hoffmann |
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29 | ! Bottom and top boundary conditions of rain water content (qr) and |
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30 | ! rain drop concentration (nr) changed to Dirichlet |
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31 | ! |
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32 | ! 1353 2014-04-08 15:21:23Z heinze |
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33 | ! REAL constants provided with KIND-attribute |
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34 | ! |
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35 | ! 1320 2014-03-20 08:40:49Z raasch |
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36 | ! ONLY-attribute added to USE-statements, |
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37 | ! kind-parameters added to all INTEGER and REAL declaration statements, |
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38 | ! kinds are defined in new module kinds, |
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39 | ! revision history before 2012 removed, |
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40 | ! comment fields (!:) to be used for variable explanations added to |
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41 | ! all variable declaration statements |
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42 | ! |
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43 | ! 1257 2013-11-08 15:18:40Z raasch |
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44 | ! loop independent clauses added |
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45 | ! |
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46 | ! 1241 2013-10-30 11:36:58Z heinze |
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47 | ! Adjust ug and vg at each timestep in case of large_scale_forcing |
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48 | ! |
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49 | ! 1159 2013-05-21 11:58:22Z fricke |
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50 | ! Bugfix: Neumann boundary conditions for the velocity components at the |
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51 | ! outflow are in fact radiation boundary conditions using the maximum phase |
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52 | ! velocity that ensures numerical stability (CFL-condition). |
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53 | ! Hence, logical operator use_cmax is now used instead of bc_lr_dirneu/_neudir. |
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54 | ! Bugfix: In case of use_cmax at the outflow, u, v, w are replaced by |
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55 | ! u_p, v_p, w_p |
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56 | ! |
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57 | ! 1115 2013-03-26 18:16:16Z hoffmann |
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58 | ! boundary conditions of two-moment cloud scheme are restricted to Neumann- |
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59 | ! boundary-conditions |
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60 | ! |
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61 | ! 1113 2013-03-10 02:48:14Z raasch |
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62 | ! GPU-porting |
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63 | ! dummy argument "range" removed |
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64 | ! Bugfix: wrong index in loops of radiation boundary condition |
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65 | ! |
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66 | ! 1053 2012-11-13 17:11:03Z hoffmann |
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67 | ! boundary conditions for the two new prognostic equations (nr, qr) of the |
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68 | ! two-moment cloud scheme |
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69 | ! |
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70 | ! 1036 2012-10-22 13:43:42Z raasch |
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71 | ! code put under GPL (PALM 3.9) |
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72 | ! |
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73 | ! 996 2012-09-07 10:41:47Z raasch |
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74 | ! little reformatting |
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75 | ! |
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76 | ! 978 2012-08-09 08:28:32Z fricke |
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77 | ! Neumann boudnary conditions are added at the inflow boundary for the SGS-TKE. |
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78 | ! Outflow boundary conditions for the velocity components can be set to Neumann |
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79 | ! conditions or to radiation conditions with a horizontal averaged phase |
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80 | ! velocity. |
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81 | ! |
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82 | ! 875 2012-04-02 15:35:15Z gryschka |
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83 | ! Bugfix in case of dirichlet inflow bc at the right or north boundary |
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84 | ! |
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85 | ! Revision 1.1 1997/09/12 06:21:34 raasch |
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86 | ! Initial revision |
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87 | ! |
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88 | ! |
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89 | ! Description: |
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90 | ! ------------ |
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91 | ! Boundary conditions for the prognostic quantities. |
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92 | ! One additional bottom boundary condition is applied for the TKE (=(u*)**2) |
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93 | ! in prandtl_fluxes. The cyclic lateral boundary conditions are implicitly |
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94 | ! handled in routine exchange_horiz. Pressure boundary conditions are |
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95 | ! explicitly set in routines pres, poisfft, poismg and sor. |
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96 | !------------------------------------------------------------------------------! |
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97 | |
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98 | USE arrays_3d, & |
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99 | ONLY: c_u, c_u_m, c_u_m_l, c_v, c_v_m, c_v_m_l, c_w, c_w_m, c_w_m_l, & |
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100 | dzu, e_p, nr_p, pt, pt_p, q, q_p, qr_p, sa, sa_p, & |
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101 | u, ug, u_init, u_m_l, u_m_n, u_m_r, u_m_s, u_p, & |
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102 | v, vg, v_init, v_m_l, v_m_n, v_m_r, v_m_s, v_p, & |
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103 | w, w_p, w_m_l, w_m_n, w_m_r, w_m_s |
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104 | |
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105 | USE control_parameters, & |
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106 | ONLY: bc_pt_t_val, bc_q_t_val, constant_diffusion, & |
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107 | cloud_physics, dt_3d, humidity, & |
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108 | ibc_pt_b, ibc_pt_t, ibc_q_b, ibc_sa_t, ibc_uv_b, ibc_uv_t, & |
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109 | icloud_scheme, inflow_l, inflow_n, inflow_r, inflow_s, & |
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110 | intermediate_timestep_count, large_scale_forcing, ocean, & |
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111 | outflow_l, outflow_n, outflow_r, outflow_s, passive_scalar, & |
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112 | precipitation, tsc, use_cmax |
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113 | |
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114 | USE grid_variables, & |
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115 | ONLY: ddx, ddy, dx, dy |
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116 | |
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117 | USE indices, & |
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118 | ONLY: nx, nxl, nxlg, nxr, nxrg, ny, nyn, nyng, nys, nysg, & |
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119 | nzb, nzb_s_inner, nzb_w_inner, nzt |
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120 | |
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121 | USE kinds |
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122 | |
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123 | USE pegrid |
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124 | |
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125 | |
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126 | IMPLICIT NONE |
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127 | |
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128 | INTEGER(iwp) :: i !: |
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129 | INTEGER(iwp) :: j !: |
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130 | INTEGER(iwp) :: k !: |
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131 | |
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132 | REAL(wp) :: c_max !: |
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133 | REAL(wp) :: denom !: |
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134 | |
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135 | |
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136 | ! |
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137 | !-- Bottom boundary |
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138 | IF ( ibc_uv_b == 1 ) THEN |
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139 | !$acc kernels present( u_p, v_p ) |
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140 | u_p(nzb,:,:) = u_p(nzb+1,:,:) |
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141 | v_p(nzb,:,:) = v_p(nzb+1,:,:) |
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142 | !$acc end kernels |
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143 | ENDIF |
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144 | |
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145 | !$acc kernels present( nzb_w_inner, w_p ) |
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146 | DO i = nxlg, nxrg |
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147 | DO j = nysg, nyng |
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148 | w_p(nzb_w_inner(j,i),j,i) = 0.0_wp |
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149 | ENDDO |
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150 | ENDDO |
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151 | !$acc end kernels |
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152 | |
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153 | ! |
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154 | !-- Top boundary |
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155 | IF ( ibc_uv_t == 0 ) THEN |
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156 | !$acc kernels present( u_init, u_p, v_init, v_p ) |
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157 | u_p(nzt+1,:,:) = u_init(nzt+1) |
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158 | v_p(nzt+1,:,:) = v_init(nzt+1) |
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159 | IF ( large_scale_forcing) THEN |
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160 | u_p(nzt+1,:,:) = ug(nzt+1) |
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161 | v_p(nzt+1,:,:) = vg(nzt+1) |
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162 | END IF |
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163 | !$acc end kernels |
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164 | ELSE |
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165 | !$acc kernels present( u_p, v_p ) |
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166 | u_p(nzt+1,:,:) = u_p(nzt,:,:) |
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167 | v_p(nzt+1,:,:) = v_p(nzt,:,:) |
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168 | !$acc end kernels |
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169 | ENDIF |
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170 | !$acc kernels present( w_p ) |
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171 | w_p(nzt:nzt+1,:,:) = 0.0_wp ! nzt is not a prognostic level (but cf. pres) |
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172 | !$acc end kernels |
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173 | |
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174 | ! |
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175 | !-- Temperature at bottom boundary. |
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176 | !-- In case of coupled runs (ibc_pt_b = 2) the temperature is given by |
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177 | !-- the sea surface temperature of the coupled ocean model. |
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178 | IF ( ibc_pt_b == 0 ) THEN |
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179 | !$acc kernels present( nzb_s_inner, pt, pt_p ) |
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180 | !$acc loop independent |
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181 | DO i = nxlg, nxrg |
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182 | !$acc loop independent |
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183 | DO j = nysg, nyng |
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184 | pt_p(nzb_s_inner(j,i),j,i) = pt(nzb_s_inner(j,i),j,i) |
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185 | ENDDO |
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186 | ENDDO |
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187 | !$acc end kernels |
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188 | ELSEIF ( ibc_pt_b == 1 ) THEN |
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189 | !$acc kernels present( nzb_s_inner, pt_p ) |
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190 | !$acc loop independent |
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191 | DO i = nxlg, nxrg |
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192 | !$acc loop independent |
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193 | DO j = nysg, nyng |
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194 | pt_p(nzb_s_inner(j,i),j,i) = pt_p(nzb_s_inner(j,i)+1,j,i) |
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195 | ENDDO |
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196 | ENDDO |
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197 | !$acc end kernels |
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198 | ENDIF |
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199 | |
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200 | ! |
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201 | !-- Temperature at top boundary |
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202 | IF ( ibc_pt_t == 0 ) THEN |
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203 | !$acc kernels present( pt, pt_p ) |
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204 | pt_p(nzt+1,:,:) = pt(nzt+1,:,:) |
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205 | !$acc end kernels |
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206 | ELSEIF ( ibc_pt_t == 1 ) THEN |
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207 | !$acc kernels present( pt_p ) |
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208 | pt_p(nzt+1,:,:) = pt_p(nzt,:,:) |
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209 | !$acc end kernels |
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210 | ELSEIF ( ibc_pt_t == 2 ) THEN |
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211 | !$acc kernels present( dzu, pt_p ) |
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212 | pt_p(nzt+1,:,:) = pt_p(nzt,:,:) + bc_pt_t_val * dzu(nzt+1) |
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213 | !$acc end kernels |
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214 | ENDIF |
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215 | |
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216 | ! |
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217 | !-- Boundary conditions for TKE |
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218 | !-- Generally Neumann conditions with de/dz=0 are assumed |
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219 | IF ( .NOT. constant_diffusion ) THEN |
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220 | !$acc kernels present( e_p, nzb_s_inner ) |
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221 | !$acc loop independent |
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222 | DO i = nxlg, nxrg |
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223 | !$acc loop independent |
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224 | DO j = nysg, nyng |
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225 | e_p(nzb_s_inner(j,i),j,i) = e_p(nzb_s_inner(j,i)+1,j,i) |
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226 | ENDDO |
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227 | ENDDO |
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228 | e_p(nzt+1,:,:) = e_p(nzt,:,:) |
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229 | !$acc end kernels |
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230 | ENDIF |
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231 | |
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232 | ! |
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233 | !-- Boundary conditions for salinity |
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234 | IF ( ocean ) THEN |
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235 | ! |
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236 | !-- Bottom boundary: Neumann condition because salinity flux is always |
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237 | !-- given |
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238 | DO i = nxlg, nxrg |
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239 | DO j = nysg, nyng |
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240 | sa_p(nzb_s_inner(j,i),j,i) = sa_p(nzb_s_inner(j,i)+1,j,i) |
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241 | ENDDO |
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242 | ENDDO |
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243 | |
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244 | ! |
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245 | !-- Top boundary: Dirichlet or Neumann |
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246 | IF ( ibc_sa_t == 0 ) THEN |
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247 | sa_p(nzt+1,:,:) = sa(nzt+1,:,:) |
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248 | ELSEIF ( ibc_sa_t == 1 ) THEN |
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249 | sa_p(nzt+1,:,:) = sa_p(nzt,:,:) |
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250 | ENDIF |
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251 | |
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252 | ENDIF |
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253 | |
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254 | ! |
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255 | !-- Boundary conditions for total water content or scalar, |
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256 | !-- bottom and top boundary (see also temperature) |
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257 | IF ( humidity .OR. passive_scalar ) THEN |
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258 | ! |
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259 | !-- Surface conditions for constant_humidity_flux |
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260 | IF ( ibc_q_b == 0 ) THEN |
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261 | DO i = nxlg, nxrg |
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262 | DO j = nysg, nyng |
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263 | q_p(nzb_s_inner(j,i),j,i) = q(nzb_s_inner(j,i),j,i) |
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264 | ENDDO |
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265 | ENDDO |
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266 | ELSE |
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267 | DO i = nxlg, nxrg |
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268 | DO j = nysg, nyng |
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269 | q_p(nzb_s_inner(j,i),j,i) = q_p(nzb_s_inner(j,i)+1,j,i) |
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270 | ENDDO |
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271 | ENDDO |
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272 | ENDIF |
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273 | ! |
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274 | !-- Top boundary |
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275 | q_p(nzt+1,:,:) = q_p(nzt,:,:) + bc_q_t_val * dzu(nzt+1) |
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276 | |
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277 | IF ( cloud_physics .AND. icloud_scheme == 0 .AND. precipitation ) THEN |
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278 | ! |
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279 | !-- Surface conditions rain water (Dirichlet) |
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280 | DO i = nxlg, nxrg |
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281 | DO j = nysg, nyng |
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282 | qr_p(nzb_s_inner(j,i),j,i) = 0.0_wp |
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283 | nr_p(nzb_s_inner(j,i),j,i) = 0.0_wp |
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284 | ENDDO |
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285 | ENDDO |
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286 | ! |
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287 | !-- Top boundary condition for rain water (Dirichlet) |
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288 | qr_p(nzt+1,:,:) = 0.0_wp |
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289 | nr_p(nzt+1,:,:) = 0.0_wp |
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290 | |
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291 | ENDIF |
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292 | ! |
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293 | !-- In case of inflow at the south boundary the boundary for v is at nys |
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294 | !-- and in case of inflow at the left boundary the boundary for u is at nxl. |
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295 | !-- Since in prognostic_equations (cache optimized version) these levels are |
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296 | !-- handled as a prognostic level, boundary values have to be restored here. |
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297 | !-- For the SGS-TKE, Neumann boundary conditions are used at the inflow. |
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298 | IF ( inflow_s ) THEN |
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299 | v_p(:,nys,:) = v_p(:,nys-1,:) |
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300 | IF ( .NOT. constant_diffusion ) e_p(:,nys-1,:) = e_p(:,nys,:) |
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301 | ELSEIF ( inflow_n ) THEN |
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302 | IF ( .NOT. constant_diffusion ) e_p(:,nyn+1,:) = e_p(:,nyn,:) |
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303 | ELSEIF ( inflow_l ) THEN |
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304 | u_p(:,:,nxl) = u_p(:,:,nxl-1) |
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305 | IF ( .NOT. constant_diffusion ) e_p(:,:,nxl-1) = e_p(:,:,nxl) |
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306 | ELSEIF ( inflow_r ) THEN |
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307 | IF ( .NOT. constant_diffusion ) e_p(:,:,nxr+1) = e_p(:,:,nxr) |
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308 | ENDIF |
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309 | |
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310 | ! |
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311 | !-- Lateral boundary conditions for scalar quantities at the outflow |
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312 | IF ( outflow_s ) THEN |
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313 | pt_p(:,nys-1,:) = pt_p(:,nys,:) |
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314 | IF ( .NOT. constant_diffusion ) e_p(:,nys-1,:) = e_p(:,nys,:) |
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315 | IF ( humidity .OR. passive_scalar ) THEN |
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316 | q_p(:,nys-1,:) = q_p(:,nys,:) |
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317 | IF ( cloud_physics .AND. icloud_scheme == 0 .AND. & |
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318 | precipitation) THEN |
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319 | qr_p(:,nys-1,:) = qr_p(:,nys,:) |
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320 | nr_p(:,nys-1,:) = nr_p(:,nys,:) |
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321 | ENDIF |
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322 | ENDIF |
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323 | ELSEIF ( outflow_n ) THEN |
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324 | pt_p(:,nyn+1,:) = pt_p(:,nyn,:) |
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325 | IF ( .NOT. constant_diffusion ) e_p(:,nyn+1,:) = e_p(:,nyn,:) |
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326 | IF ( humidity .OR. passive_scalar ) THEN |
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327 | q_p(:,nyn+1,:) = q_p(:,nyn,:) |
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328 | IF ( cloud_physics .AND. icloud_scheme == 0 .AND. & |
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329 | precipitation ) THEN |
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330 | qr_p(:,nyn+1,:) = qr_p(:,nyn,:) |
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331 | nr_p(:,nyn+1,:) = nr_p(:,nyn,:) |
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332 | ENDIF |
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333 | ENDIF |
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334 | ELSEIF ( outflow_l ) THEN |
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335 | pt_p(:,:,nxl-1) = pt_p(:,:,nxl) |
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336 | IF ( .NOT. constant_diffusion ) e_p(:,:,nxl-1) = e_p(:,:,nxl) |
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337 | IF ( humidity .OR. passive_scalar ) THEN |
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338 | q_p(:,:,nxl-1) = q_p(:,:,nxl) |
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339 | IF ( cloud_physics .AND. icloud_scheme == 0 .AND. & |
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340 | precipitation ) THEN |
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341 | qr_p(:,:,nxl-1) = qr_p(:,:,nxl) |
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342 | nr_p(:,:,nxl-1) = nr_p(:,:,nxl) |
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343 | ENDIF |
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344 | ENDIF |
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345 | ELSEIF ( outflow_r ) THEN |
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346 | pt_p(:,:,nxr+1) = pt_p(:,:,nxr) |
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347 | IF ( .NOT. constant_diffusion ) e_p(:,:,nxr+1) = e_p(:,:,nxr) |
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348 | IF ( humidity .OR. passive_scalar ) THEN |
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349 | q_p(:,:,nxr+1) = q_p(:,:,nxr) |
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350 | IF ( cloud_physics .AND. icloud_scheme == 0 .AND. precipitation ) THEN |
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351 | qr_p(:,:,nxr+1) = qr_p(:,:,nxr) |
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352 | nr_p(:,:,nxr+1) = nr_p(:,:,nxr) |
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353 | ENDIF |
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354 | ENDIF |
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355 | ENDIF |
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356 | |
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357 | ENDIF |
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358 | |
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359 | ! |
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360 | !-- Radiation boundary conditions for the velocities at the respective outflow. |
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361 | !-- The phase velocity is either assumed to the maximum phase velocity that |
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362 | !-- ensures numerical stability (CFL-condition) or calculated after |
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363 | !-- Orlanski(1976) and averaged along the outflow boundary. |
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364 | IF ( outflow_s ) THEN |
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365 | |
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366 | IF ( use_cmax ) THEN |
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367 | u_p(:,-1,:) = u(:,0,:) |
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368 | v_p(:,0,:) = v(:,1,:) |
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369 | w_p(:,-1,:) = w(:,0,:) |
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370 | ELSEIF ( .NOT. use_cmax ) THEN |
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371 | |
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372 | c_max = dy / dt_3d |
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373 | |
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374 | c_u_m_l = 0.0_wp |
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375 | c_v_m_l = 0.0_wp |
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376 | c_w_m_l = 0.0_wp |
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377 | |
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378 | c_u_m = 0.0_wp |
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379 | c_v_m = 0.0_wp |
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380 | c_w_m = 0.0_wp |
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381 | |
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382 | ! |
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383 | !-- Calculate the phase speeds for u, v, and w, first local and then |
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384 | !-- average along the outflow boundary. |
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385 | DO k = nzb+1, nzt+1 |
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386 | DO i = nxl, nxr |
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387 | |
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388 | denom = u_m_s(k,0,i) - u_m_s(k,1,i) |
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389 | |
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390 | IF ( denom /= 0.0_wp ) THEN |
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391 | c_u(k,i) = -c_max * ( u(k,0,i) - u_m_s(k,0,i) ) / ( denom * tsc(2) ) |
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392 | IF ( c_u(k,i) < 0.0_wp ) THEN |
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393 | c_u(k,i) = 0.0_wp |
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394 | ELSEIF ( c_u(k,i) > c_max ) THEN |
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395 | c_u(k,i) = c_max |
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396 | ENDIF |
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397 | ELSE |
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398 | c_u(k,i) = c_max |
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399 | ENDIF |
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400 | |
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401 | denom = v_m_s(k,1,i) - v_m_s(k,2,i) |
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402 | |
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403 | IF ( denom /= 0.0_wp ) THEN |
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404 | c_v(k,i) = -c_max * ( v(k,1,i) - v_m_s(k,1,i) ) / ( denom * tsc(2) ) |
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405 | IF ( c_v(k,i) < 0.0_wp ) THEN |
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406 | c_v(k,i) = 0.0_wp |
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407 | ELSEIF ( c_v(k,i) > c_max ) THEN |
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408 | c_v(k,i) = c_max |
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409 | ENDIF |
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410 | ELSE |
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411 | c_v(k,i) = c_max |
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412 | ENDIF |
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413 | |
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414 | denom = w_m_s(k,0,i) - w_m_s(k,1,i) |
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415 | |
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416 | IF ( denom /= 0.0_wp ) THEN |
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417 | c_w(k,i) = -c_max * ( w(k,0,i) - w_m_s(k,0,i) ) / ( denom * tsc(2) ) |
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418 | IF ( c_w(k,i) < 0.0_wp ) THEN |
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419 | c_w(k,i) = 0.0_wp |
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420 | ELSEIF ( c_w(k,i) > c_max ) THEN |
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421 | c_w(k,i) = c_max |
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422 | ENDIF |
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423 | ELSE |
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424 | c_w(k,i) = c_max |
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425 | ENDIF |
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426 | |
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427 | c_u_m_l(k) = c_u_m_l(k) + c_u(k,i) |
---|
428 | c_v_m_l(k) = c_v_m_l(k) + c_v(k,i) |
---|
429 | c_w_m_l(k) = c_w_m_l(k) + c_w(k,i) |
---|
430 | |
---|
431 | ENDDO |
---|
432 | ENDDO |
---|
433 | |
---|
434 | #if defined( __parallel ) |
---|
435 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dx, ierr ) |
---|
436 | CALL MPI_ALLREDUCE( c_u_m_l(nzb+1), c_u_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
437 | MPI_SUM, comm1dx, ierr ) |
---|
438 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dx, ierr ) |
---|
439 | CALL MPI_ALLREDUCE( c_v_m_l(nzb+1), c_v_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
440 | MPI_SUM, comm1dx, ierr ) |
---|
441 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dx, ierr ) |
---|
442 | CALL MPI_ALLREDUCE( c_w_m_l(nzb+1), c_w_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
443 | MPI_SUM, comm1dx, ierr ) |
---|
444 | #else |
---|
445 | c_u_m = c_u_m_l |
---|
446 | c_v_m = c_v_m_l |
---|
447 | c_w_m = c_w_m_l |
---|
448 | #endif |
---|
449 | |
---|
450 | c_u_m = c_u_m / (nx+1) |
---|
451 | c_v_m = c_v_m / (nx+1) |
---|
452 | c_w_m = c_w_m / (nx+1) |
---|
453 | |
---|
454 | ! |
---|
455 | !-- Save old timelevels for the next timestep |
---|
456 | IF ( intermediate_timestep_count == 1 ) THEN |
---|
457 | u_m_s(:,:,:) = u(:,0:1,:) |
---|
458 | v_m_s(:,:,:) = v(:,1:2,:) |
---|
459 | w_m_s(:,:,:) = w(:,0:1,:) |
---|
460 | ENDIF |
---|
461 | |
---|
462 | ! |
---|
463 | !-- Calculate the new velocities |
---|
464 | DO k = nzb+1, nzt+1 |
---|
465 | DO i = nxlg, nxrg |
---|
466 | u_p(k,-1,i) = u(k,-1,i) - dt_3d * tsc(2) * c_u_m(k) * & |
---|
467 | ( u(k,-1,i) - u(k,0,i) ) * ddy |
---|
468 | |
---|
469 | v_p(k,0,i) = v(k,0,i) - dt_3d * tsc(2) * c_v_m(k) * & |
---|
470 | ( v(k,0,i) - v(k,1,i) ) * ddy |
---|
471 | |
---|
472 | w_p(k,-1,i) = w(k,-1,i) - dt_3d * tsc(2) * c_w_m(k) * & |
---|
473 | ( w(k,-1,i) - w(k,0,i) ) * ddy |
---|
474 | ENDDO |
---|
475 | ENDDO |
---|
476 | |
---|
477 | ! |
---|
478 | !-- Bottom boundary at the outflow |
---|
479 | IF ( ibc_uv_b == 0 ) THEN |
---|
480 | u_p(nzb,-1,:) = 0.0_wp |
---|
481 | v_p(nzb,0,:) = 0.0_wp |
---|
482 | ELSE |
---|
483 | u_p(nzb,-1,:) = u_p(nzb+1,-1,:) |
---|
484 | v_p(nzb,0,:) = v_p(nzb+1,0,:) |
---|
485 | ENDIF |
---|
486 | w_p(nzb,-1,:) = 0.0_wp |
---|
487 | |
---|
488 | ! |
---|
489 | !-- Top boundary at the outflow |
---|
490 | IF ( ibc_uv_t == 0 ) THEN |
---|
491 | u_p(nzt+1,-1,:) = u_init(nzt+1) |
---|
492 | v_p(nzt+1,0,:) = v_init(nzt+1) |
---|
493 | ELSE |
---|
494 | u_p(nzt+1,-1,:) = u(nzt,-1,:) |
---|
495 | v_p(nzt+1,0,:) = v(nzt,0,:) |
---|
496 | ENDIF |
---|
497 | w_p(nzt:nzt+1,-1,:) = 0.0_wp |
---|
498 | |
---|
499 | ENDIF |
---|
500 | |
---|
501 | ENDIF |
---|
502 | |
---|
503 | IF ( outflow_n ) THEN |
---|
504 | |
---|
505 | IF ( use_cmax ) THEN |
---|
506 | u_p(:,ny+1,:) = u(:,ny,:) |
---|
507 | v_p(:,ny+1,:) = v(:,ny,:) |
---|
508 | w_p(:,ny+1,:) = w(:,ny,:) |
---|
509 | ELSEIF ( .NOT. use_cmax ) THEN |
---|
510 | |
---|
511 | c_max = dy / dt_3d |
---|
512 | |
---|
513 | c_u_m_l = 0.0_wp |
---|
514 | c_v_m_l = 0.0_wp |
---|
515 | c_w_m_l = 0.0_wp |
---|
516 | |
---|
517 | c_u_m = 0.0_wp |
---|
518 | c_v_m = 0.0_wp |
---|
519 | c_w_m = 0.0_wp |
---|
520 | |
---|
521 | ! |
---|
522 | !-- Calculate the phase speeds for u, v, and w, first local and then |
---|
523 | !-- average along the outflow boundary. |
---|
524 | DO k = nzb+1, nzt+1 |
---|
525 | DO i = nxl, nxr |
---|
526 | |
---|
527 | denom = u_m_n(k,ny,i) - u_m_n(k,ny-1,i) |
---|
528 | |
---|
529 | IF ( denom /= 0.0_wp ) THEN |
---|
530 | c_u(k,i) = -c_max * ( u(k,ny,i) - u_m_n(k,ny,i) ) / ( denom * tsc(2) ) |
---|
531 | IF ( c_u(k,i) < 0.0_wp ) THEN |
---|
532 | c_u(k,i) = 0.0_wp |
---|
533 | ELSEIF ( c_u(k,i) > c_max ) THEN |
---|
534 | c_u(k,i) = c_max |
---|
535 | ENDIF |
---|
536 | ELSE |
---|
537 | c_u(k,i) = c_max |
---|
538 | ENDIF |
---|
539 | |
---|
540 | denom = v_m_n(k,ny,i) - v_m_n(k,ny-1,i) |
---|
541 | |
---|
542 | IF ( denom /= 0.0_wp ) THEN |
---|
543 | c_v(k,i) = -c_max * ( v(k,ny,i) - v_m_n(k,ny,i) ) / ( denom * tsc(2) ) |
---|
544 | IF ( c_v(k,i) < 0.0_wp ) THEN |
---|
545 | c_v(k,i) = 0.0_wp |
---|
546 | ELSEIF ( c_v(k,i) > c_max ) THEN |
---|
547 | c_v(k,i) = c_max |
---|
548 | ENDIF |
---|
549 | ELSE |
---|
550 | c_v(k,i) = c_max |
---|
551 | ENDIF |
---|
552 | |
---|
553 | denom = w_m_n(k,ny,i) - w_m_n(k,ny-1,i) |
---|
554 | |
---|
555 | IF ( denom /= 0.0_wp ) THEN |
---|
556 | c_w(k,i) = -c_max * ( w(k,ny,i) - w_m_n(k,ny,i) ) / ( denom * tsc(2) ) |
---|
557 | IF ( c_w(k,i) < 0.0_wp ) THEN |
---|
558 | c_w(k,i) = 0.0_wp |
---|
559 | ELSEIF ( c_w(k,i) > c_max ) THEN |
---|
560 | c_w(k,i) = c_max |
---|
561 | ENDIF |
---|
562 | ELSE |
---|
563 | c_w(k,i) = c_max |
---|
564 | ENDIF |
---|
565 | |
---|
566 | c_u_m_l(k) = c_u_m_l(k) + c_u(k,i) |
---|
567 | c_v_m_l(k) = c_v_m_l(k) + c_v(k,i) |
---|
568 | c_w_m_l(k) = c_w_m_l(k) + c_w(k,i) |
---|
569 | |
---|
570 | ENDDO |
---|
571 | ENDDO |
---|
572 | |
---|
573 | #if defined( __parallel ) |
---|
574 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dx, ierr ) |
---|
575 | CALL MPI_ALLREDUCE( c_u_m_l(nzb+1), c_u_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
576 | MPI_SUM, comm1dx, ierr ) |
---|
577 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dx, ierr ) |
---|
578 | CALL MPI_ALLREDUCE( c_v_m_l(nzb+1), c_v_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
579 | MPI_SUM, comm1dx, ierr ) |
---|
580 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dx, ierr ) |
---|
581 | CALL MPI_ALLREDUCE( c_w_m_l(nzb+1), c_w_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
582 | MPI_SUM, comm1dx, ierr ) |
---|
583 | #else |
---|
584 | c_u_m = c_u_m_l |
---|
585 | c_v_m = c_v_m_l |
---|
586 | c_w_m = c_w_m_l |
---|
587 | #endif |
---|
588 | |
---|
589 | c_u_m = c_u_m / (nx+1) |
---|
590 | c_v_m = c_v_m / (nx+1) |
---|
591 | c_w_m = c_w_m / (nx+1) |
---|
592 | |
---|
593 | ! |
---|
594 | !-- Save old timelevels for the next timestep |
---|
595 | IF ( intermediate_timestep_count == 1 ) THEN |
---|
596 | u_m_n(:,:,:) = u(:,ny-1:ny,:) |
---|
597 | v_m_n(:,:,:) = v(:,ny-1:ny,:) |
---|
598 | w_m_n(:,:,:) = w(:,ny-1:ny,:) |
---|
599 | ENDIF |
---|
600 | |
---|
601 | ! |
---|
602 | !-- Calculate the new velocities |
---|
603 | DO k = nzb+1, nzt+1 |
---|
604 | DO i = nxlg, nxrg |
---|
605 | u_p(k,ny+1,i) = u(k,ny+1,i) - dt_3d * tsc(2) * c_u_m(k) * & |
---|
606 | ( u(k,ny+1,i) - u(k,ny,i) ) * ddy |
---|
607 | |
---|
608 | v_p(k,ny+1,i) = v(k,ny+1,i) - dt_3d * tsc(2) * c_v_m(k) * & |
---|
609 | ( v(k,ny+1,i) - v(k,ny,i) ) * ddy |
---|
610 | |
---|
611 | w_p(k,ny+1,i) = w(k,ny+1,i) - dt_3d * tsc(2) * c_w_m(k) * & |
---|
612 | ( w(k,ny+1,i) - w(k,ny,i) ) * ddy |
---|
613 | ENDDO |
---|
614 | ENDDO |
---|
615 | |
---|
616 | ! |
---|
617 | !-- Bottom boundary at the outflow |
---|
618 | IF ( ibc_uv_b == 0 ) THEN |
---|
619 | u_p(nzb,ny+1,:) = 0.0_wp |
---|
620 | v_p(nzb,ny+1,:) = 0.0_wp |
---|
621 | ELSE |
---|
622 | u_p(nzb,ny+1,:) = u_p(nzb+1,ny+1,:) |
---|
623 | v_p(nzb,ny+1,:) = v_p(nzb+1,ny+1,:) |
---|
624 | ENDIF |
---|
625 | w_p(nzb,ny+1,:) = 0.0_wp |
---|
626 | |
---|
627 | ! |
---|
628 | !-- Top boundary at the outflow |
---|
629 | IF ( ibc_uv_t == 0 ) THEN |
---|
630 | u_p(nzt+1,ny+1,:) = u_init(nzt+1) |
---|
631 | v_p(nzt+1,ny+1,:) = v_init(nzt+1) |
---|
632 | ELSE |
---|
633 | u_p(nzt+1,ny+1,:) = u_p(nzt,nyn+1,:) |
---|
634 | v_p(nzt+1,ny+1,:) = v_p(nzt,nyn+1,:) |
---|
635 | ENDIF |
---|
636 | w_p(nzt:nzt+1,ny+1,:) = 0.0_wp |
---|
637 | |
---|
638 | ENDIF |
---|
639 | |
---|
640 | ENDIF |
---|
641 | |
---|
642 | IF ( outflow_l ) THEN |
---|
643 | |
---|
644 | IF ( use_cmax ) THEN |
---|
645 | u_p(:,:,-1) = u(:,:,0) |
---|
646 | v_p(:,:,0) = v(:,:,1) |
---|
647 | w_p(:,:,-1) = w(:,:,0) |
---|
648 | ELSEIF ( .NOT. use_cmax ) THEN |
---|
649 | |
---|
650 | c_max = dx / dt_3d |
---|
651 | |
---|
652 | c_u_m_l = 0.0_wp |
---|
653 | c_v_m_l = 0.0_wp |
---|
654 | c_w_m_l = 0.0_wp |
---|
655 | |
---|
656 | c_u_m = 0.0_wp |
---|
657 | c_v_m = 0.0_wp |
---|
658 | c_w_m = 0.0_wp |
---|
659 | |
---|
660 | ! |
---|
661 | !-- Calculate the phase speeds for u, v, and w, first local and then |
---|
662 | !-- average along the outflow boundary. |
---|
663 | DO k = nzb+1, nzt+1 |
---|
664 | DO j = nys, nyn |
---|
665 | |
---|
666 | denom = u_m_l(k,j,1) - u_m_l(k,j,2) |
---|
667 | |
---|
668 | IF ( denom /= 0.0_wp ) THEN |
---|
669 | c_u(k,j) = -c_max * ( u(k,j,1) - u_m_l(k,j,1) ) / ( denom * tsc(2) ) |
---|
670 | IF ( c_u(k,j) < 0.0_wp ) THEN |
---|
671 | c_u(k,j) = 0.0_wp |
---|
672 | ELSEIF ( c_u(k,j) > c_max ) THEN |
---|
673 | c_u(k,j) = c_max |
---|
674 | ENDIF |
---|
675 | ELSE |
---|
676 | c_u(k,j) = c_max |
---|
677 | ENDIF |
---|
678 | |
---|
679 | denom = v_m_l(k,j,0) - v_m_l(k,j,1) |
---|
680 | |
---|
681 | IF ( denom /= 0.0_wp ) THEN |
---|
682 | c_v(k,j) = -c_max * ( v(k,j,0) - v_m_l(k,j,0) ) / ( denom * tsc(2) ) |
---|
683 | IF ( c_v(k,j) < 0.0_wp ) THEN |
---|
684 | c_v(k,j) = 0.0_wp |
---|
685 | ELSEIF ( c_v(k,j) > c_max ) THEN |
---|
686 | c_v(k,j) = c_max |
---|
687 | ENDIF |
---|
688 | ELSE |
---|
689 | c_v(k,j) = c_max |
---|
690 | ENDIF |
---|
691 | |
---|
692 | denom = w_m_l(k,j,0) - w_m_l(k,j,1) |
---|
693 | |
---|
694 | IF ( denom /= 0.0_wp ) THEN |
---|
695 | c_w(k,j) = -c_max * ( w(k,j,0) - w_m_l(k,j,0) ) / ( denom * tsc(2) ) |
---|
696 | IF ( c_w(k,j) < 0.0_wp ) THEN |
---|
697 | c_w(k,j) = 0.0_wp |
---|
698 | ELSEIF ( c_w(k,j) > c_max ) THEN |
---|
699 | c_w(k,j) = c_max |
---|
700 | ENDIF |
---|
701 | ELSE |
---|
702 | c_w(k,j) = c_max |
---|
703 | ENDIF |
---|
704 | |
---|
705 | c_u_m_l(k) = c_u_m_l(k) + c_u(k,j) |
---|
706 | c_v_m_l(k) = c_v_m_l(k) + c_v(k,j) |
---|
707 | c_w_m_l(k) = c_w_m_l(k) + c_w(k,j) |
---|
708 | |
---|
709 | ENDDO |
---|
710 | ENDDO |
---|
711 | |
---|
712 | #if defined( __parallel ) |
---|
713 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dy, ierr ) |
---|
714 | CALL MPI_ALLREDUCE( c_u_m_l(nzb+1), c_u_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
715 | MPI_SUM, comm1dy, ierr ) |
---|
716 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dy, ierr ) |
---|
717 | CALL MPI_ALLREDUCE( c_v_m_l(nzb+1), c_v_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
718 | MPI_SUM, comm1dy, ierr ) |
---|
719 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dy, ierr ) |
---|
720 | CALL MPI_ALLREDUCE( c_w_m_l(nzb+1), c_w_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
721 | MPI_SUM, comm1dy, ierr ) |
---|
722 | #else |
---|
723 | c_u_m = c_u_m_l |
---|
724 | c_v_m = c_v_m_l |
---|
725 | c_w_m = c_w_m_l |
---|
726 | #endif |
---|
727 | |
---|
728 | c_u_m = c_u_m / (ny+1) |
---|
729 | c_v_m = c_v_m / (ny+1) |
---|
730 | c_w_m = c_w_m / (ny+1) |
---|
731 | |
---|
732 | ! |
---|
733 | !-- Save old timelevels for the next timestep |
---|
734 | IF ( intermediate_timestep_count == 1 ) THEN |
---|
735 | u_m_l(:,:,:) = u(:,:,1:2) |
---|
736 | v_m_l(:,:,:) = v(:,:,0:1) |
---|
737 | w_m_l(:,:,:) = w(:,:,0:1) |
---|
738 | ENDIF |
---|
739 | |
---|
740 | ! |
---|
741 | !-- Calculate the new velocities |
---|
742 | DO k = nzb+1, nzt+1 |
---|
743 | DO j = nysg, nyng |
---|
744 | u_p(k,j,0) = u(k,j,0) - dt_3d * tsc(2) * c_u_m(k) * & |
---|
745 | ( u(k,j,0) - u(k,j,1) ) * ddx |
---|
746 | |
---|
747 | v_p(k,j,-1) = v(k,j,-1) - dt_3d * tsc(2) * c_v_m(k) * & |
---|
748 | ( v(k,j,-1) - v(k,j,0) ) * ddx |
---|
749 | |
---|
750 | w_p(k,j,-1) = w(k,j,-1) - dt_3d * tsc(2) * c_w_m(k) * & |
---|
751 | ( w(k,j,-1) - w(k,j,0) ) * ddx |
---|
752 | ENDDO |
---|
753 | ENDDO |
---|
754 | |
---|
755 | ! |
---|
756 | !-- Bottom boundary at the outflow |
---|
757 | IF ( ibc_uv_b == 0 ) THEN |
---|
758 | u_p(nzb,:,0) = 0.0_wp |
---|
759 | v_p(nzb,:,-1) = 0.0_wp |
---|
760 | ELSE |
---|
761 | u_p(nzb,:,0) = u_p(nzb+1,:,0) |
---|
762 | v_p(nzb,:,-1) = v_p(nzb+1,:,-1) |
---|
763 | ENDIF |
---|
764 | w_p(nzb,:,-1) = 0.0_wp |
---|
765 | |
---|
766 | ! |
---|
767 | !-- Top boundary at the outflow |
---|
768 | IF ( ibc_uv_t == 0 ) THEN |
---|
769 | u_p(nzt+1,:,-1) = u_init(nzt+1) |
---|
770 | v_p(nzt+1,:,-1) = v_init(nzt+1) |
---|
771 | ELSE |
---|
772 | u_p(nzt+1,:,-1) = u_p(nzt,:,-1) |
---|
773 | v_p(nzt+1,:,-1) = v_p(nzt,:,-1) |
---|
774 | ENDIF |
---|
775 | w_p(nzt:nzt+1,:,-1) = 0.0_wp |
---|
776 | |
---|
777 | ENDIF |
---|
778 | |
---|
779 | ENDIF |
---|
780 | |
---|
781 | IF ( outflow_r ) THEN |
---|
782 | |
---|
783 | IF ( use_cmax ) THEN |
---|
784 | u_p(:,:,nx+1) = u(:,:,nx) |
---|
785 | v_p(:,:,nx+1) = v(:,:,nx) |
---|
786 | w_p(:,:,nx+1) = w(:,:,nx) |
---|
787 | ELSEIF ( .NOT. use_cmax ) THEN |
---|
788 | |
---|
789 | c_max = dx / dt_3d |
---|
790 | |
---|
791 | c_u_m_l = 0.0_wp |
---|
792 | c_v_m_l = 0.0_wp |
---|
793 | c_w_m_l = 0.0_wp |
---|
794 | |
---|
795 | c_u_m = 0.0_wp |
---|
796 | c_v_m = 0.0_wp |
---|
797 | c_w_m = 0.0_wp |
---|
798 | |
---|
799 | ! |
---|
800 | !-- Calculate the phase speeds for u, v, and w, first local and then |
---|
801 | !-- average along the outflow boundary. |
---|
802 | DO k = nzb+1, nzt+1 |
---|
803 | DO j = nys, nyn |
---|
804 | |
---|
805 | denom = u_m_r(k,j,nx) - u_m_r(k,j,nx-1) |
---|
806 | |
---|
807 | IF ( denom /= 0.0_wp ) THEN |
---|
808 | c_u(k,j) = -c_max * ( u(k,j,nx) - u_m_r(k,j,nx) ) / ( denom * tsc(2) ) |
---|
809 | IF ( c_u(k,j) < 0.0_wp ) THEN |
---|
810 | c_u(k,j) = 0.0_wp |
---|
811 | ELSEIF ( c_u(k,j) > c_max ) THEN |
---|
812 | c_u(k,j) = c_max |
---|
813 | ENDIF |
---|
814 | ELSE |
---|
815 | c_u(k,j) = c_max |
---|
816 | ENDIF |
---|
817 | |
---|
818 | denom = v_m_r(k,j,nx) - v_m_r(k,j,nx-1) |
---|
819 | |
---|
820 | IF ( denom /= 0.0_wp ) THEN |
---|
821 | c_v(k,j) = -c_max * ( v(k,j,nx) - v_m_r(k,j,nx) ) / ( denom * tsc(2) ) |
---|
822 | IF ( c_v(k,j) < 0.0_wp ) THEN |
---|
823 | c_v(k,j) = 0.0_wp |
---|
824 | ELSEIF ( c_v(k,j) > c_max ) THEN |
---|
825 | c_v(k,j) = c_max |
---|
826 | ENDIF |
---|
827 | ELSE |
---|
828 | c_v(k,j) = c_max |
---|
829 | ENDIF |
---|
830 | |
---|
831 | denom = w_m_r(k,j,nx) - w_m_r(k,j,nx-1) |
---|
832 | |
---|
833 | IF ( denom /= 0.0_wp ) THEN |
---|
834 | c_w(k,j) = -c_max * ( w(k,j,nx) - w_m_r(k,j,nx) ) / ( denom * tsc(2) ) |
---|
835 | IF ( c_w(k,j) < 0.0_wp ) THEN |
---|
836 | c_w(k,j) = 0.0_wp |
---|
837 | ELSEIF ( c_w(k,j) > c_max ) THEN |
---|
838 | c_w(k,j) = c_max |
---|
839 | ENDIF |
---|
840 | ELSE |
---|
841 | c_w(k,j) = c_max |
---|
842 | ENDIF |
---|
843 | |
---|
844 | c_u_m_l(k) = c_u_m_l(k) + c_u(k,j) |
---|
845 | c_v_m_l(k) = c_v_m_l(k) + c_v(k,j) |
---|
846 | c_w_m_l(k) = c_w_m_l(k) + c_w(k,j) |
---|
847 | |
---|
848 | ENDDO |
---|
849 | ENDDO |
---|
850 | |
---|
851 | #if defined( __parallel ) |
---|
852 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dy, ierr ) |
---|
853 | CALL MPI_ALLREDUCE( c_u_m_l(nzb+1), c_u_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
854 | MPI_SUM, comm1dy, ierr ) |
---|
855 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dy, ierr ) |
---|
856 | CALL MPI_ALLREDUCE( c_v_m_l(nzb+1), c_v_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
857 | MPI_SUM, comm1dy, ierr ) |
---|
858 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dy, ierr ) |
---|
859 | CALL MPI_ALLREDUCE( c_w_m_l(nzb+1), c_w_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
860 | MPI_SUM, comm1dy, ierr ) |
---|
861 | #else |
---|
862 | c_u_m = c_u_m_l |
---|
863 | c_v_m = c_v_m_l |
---|
864 | c_w_m = c_w_m_l |
---|
865 | #endif |
---|
866 | |
---|
867 | c_u_m = c_u_m / (ny+1) |
---|
868 | c_v_m = c_v_m / (ny+1) |
---|
869 | c_w_m = c_w_m / (ny+1) |
---|
870 | |
---|
871 | ! |
---|
872 | !-- Save old timelevels for the next timestep |
---|
873 | IF ( intermediate_timestep_count == 1 ) THEN |
---|
874 | u_m_r(:,:,:) = u(:,:,nx-1:nx) |
---|
875 | v_m_r(:,:,:) = v(:,:,nx-1:nx) |
---|
876 | w_m_r(:,:,:) = w(:,:,nx-1:nx) |
---|
877 | ENDIF |
---|
878 | |
---|
879 | ! |
---|
880 | !-- Calculate the new velocities |
---|
881 | DO k = nzb+1, nzt+1 |
---|
882 | DO j = nysg, nyng |
---|
883 | u_p(k,j,nx+1) = u(k,j,nx+1) - dt_3d * tsc(2) * c_u_m(k) * & |
---|
884 | ( u(k,j,nx+1) - u(k,j,nx) ) * ddx |
---|
885 | |
---|
886 | v_p(k,j,nx+1) = v(k,j,nx+1) - dt_3d * tsc(2) * c_v_m(k) * & |
---|
887 | ( v(k,j,nx+1) - v(k,j,nx) ) * ddx |
---|
888 | |
---|
889 | w_p(k,j,nx+1) = w(k,j,nx+1) - dt_3d * tsc(2) * c_w_m(k) * & |
---|
890 | ( w(k,j,nx+1) - w(k,j,nx) ) * ddx |
---|
891 | ENDDO |
---|
892 | ENDDO |
---|
893 | |
---|
894 | ! |
---|
895 | !-- Bottom boundary at the outflow |
---|
896 | IF ( ibc_uv_b == 0 ) THEN |
---|
897 | u_p(nzb,:,nx+1) = 0.0_wp |
---|
898 | v_p(nzb,:,nx+1) = 0.0_wp |
---|
899 | ELSE |
---|
900 | u_p(nzb,:,nx+1) = u_p(nzb+1,:,nx+1) |
---|
901 | v_p(nzb,:,nx+1) = v_p(nzb+1,:,nx+1) |
---|
902 | ENDIF |
---|
903 | w_p(nzb,:,nx+1) = 0.0_wp |
---|
904 | |
---|
905 | ! |
---|
906 | !-- Top boundary at the outflow |
---|
907 | IF ( ibc_uv_t == 0 ) THEN |
---|
908 | u_p(nzt+1,:,nx+1) = u_init(nzt+1) |
---|
909 | v_p(nzt+1,:,nx+1) = v_init(nzt+1) |
---|
910 | ELSE |
---|
911 | u_p(nzt+1,:,nx+1) = u_p(nzt,:,nx+1) |
---|
912 | v_p(nzt+1,:,nx+1) = v_p(nzt,:,nx+1) |
---|
913 | ENDIF |
---|
914 | w(nzt:nzt+1,:,nx+1) = 0.0_wp |
---|
915 | |
---|
916 | ENDIF |
---|
917 | |
---|
918 | ENDIF |
---|
919 | |
---|
920 | END SUBROUTINE boundary_conds |
---|