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 | ! Bottom and top boundary conditions of rain water content (qr) and |
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23 | ! rain drop concentration (nr) changed to Dirichlet |
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24 | ! |
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25 | ! Former revisions: |
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26 | ! ----------------- |
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27 | ! $Id: boundary_conds.f90 1361 2014-04-16 15:17:48Z hoffmann $ |
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28 | ! |
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29 | ! 1353 2014-04-08 15:21:23Z heinze |
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30 | ! REAL constants provided with KIND-attribute |
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31 | ! |
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32 | ! 1320 2014-03-20 08:40:49Z raasch |
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33 | ! ONLY-attribute added to USE-statements, |
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34 | ! kind-parameters added to all INTEGER and REAL declaration statements, |
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35 | ! kinds are defined in new module kinds, |
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36 | ! revision history before 2012 removed, |
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37 | ! comment fields (!:) to be used for variable explanations added to |
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38 | ! all variable declaration statements |
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39 | ! |
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40 | ! 1257 2013-11-08 15:18:40Z raasch |
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41 | ! loop independent clauses added |
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42 | ! |
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43 | ! 1241 2013-10-30 11:36:58Z heinze |
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44 | ! Adjust ug and vg at each timestep in case of large_scale_forcing |
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45 | ! |
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46 | ! 1159 2013-05-21 11:58:22Z fricke |
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47 | ! Bugfix: Neumann boundary conditions for the velocity components at the |
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48 | ! outflow are in fact radiation boundary conditions using the maximum phase |
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49 | ! velocity that ensures numerical stability (CFL-condition). |
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50 | ! Hence, logical operator use_cmax is now used instead of bc_lr_dirneu/_neudir. |
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51 | ! Bugfix: In case of use_cmax at the outflow, u, v, w are replaced by |
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52 | ! u_p, v_p, w_p |
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53 | ! |
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54 | ! 1115 2013-03-26 18:16:16Z hoffmann |
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55 | ! boundary conditions of two-moment cloud scheme are restricted to Neumann- |
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56 | ! boundary-conditions |
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57 | ! |
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58 | ! 1113 2013-03-10 02:48:14Z raasch |
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59 | ! GPU-porting |
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60 | ! dummy argument "range" removed |
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61 | ! Bugfix: wrong index in loops of radiation boundary condition |
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62 | ! |
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63 | ! 1053 2012-11-13 17:11:03Z hoffmann |
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64 | ! boundary conditions for the two new prognostic equations (nr, qr) of the |
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65 | ! two-moment cloud scheme |
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66 | ! |
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67 | ! 1036 2012-10-22 13:43:42Z raasch |
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68 | ! code put under GPL (PALM 3.9) |
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69 | ! |
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70 | ! 996 2012-09-07 10:41:47Z raasch |
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71 | ! little reformatting |
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72 | ! |
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73 | ! 978 2012-08-09 08:28:32Z fricke |
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74 | ! Neumann boudnary conditions are added at the inflow boundary for the SGS-TKE. |
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75 | ! Outflow boundary conditions for the velocity components can be set to Neumann |
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76 | ! conditions or to radiation conditions with a horizontal averaged phase |
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77 | ! velocity. |
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78 | ! |
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79 | ! 875 2012-04-02 15:35:15Z gryschka |
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80 | ! Bugfix in case of dirichlet inflow bc at the right or north boundary |
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81 | ! |
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82 | ! Revision 1.1 1997/09/12 06:21:34 raasch |
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83 | ! Initial revision |
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84 | ! |
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85 | ! |
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86 | ! Description: |
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87 | ! ------------ |
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88 | ! Boundary conditions for the prognostic quantities. |
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89 | ! One additional bottom boundary condition is applied for the TKE (=(u*)**2) |
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90 | ! in prandtl_fluxes. The cyclic lateral boundary conditions are implicitly |
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91 | ! handled in routine exchange_horiz. Pressure boundary conditions are |
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92 | ! explicitly set in routines pres, poisfft, poismg and sor. |
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93 | !------------------------------------------------------------------------------! |
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94 | |
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95 | USE arrays_3d, & |
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96 | 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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97 | dzu, e_p, nr_p, pt, pt_p, q, q_p, qr_p, sa, sa_p, & |
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98 | u, ug, u_init, u_m_l, u_m_n, u_m_r, u_m_s, u_p, & |
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99 | v, vg, v_init, v_m_l, v_m_n, v_m_r, v_m_s, v_p, & |
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100 | w, w_p, w_m_l, w_m_n, w_m_r, w_m_s |
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101 | |
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102 | USE control_parameters, & |
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103 | ONLY: bc_pt_t_val, bc_q_t_val, constant_diffusion, & |
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104 | cloud_physics, dt_3d, humidity, & |
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105 | ibc_pt_b, ibc_pt_t, ibc_q_b, ibc_sa_t, ibc_uv_b, ibc_uv_t, & |
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106 | icloud_scheme, inflow_l, inflow_n, inflow_r, inflow_s, & |
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107 | intermediate_timestep_count, large_scale_forcing, ocean, & |
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108 | outflow_l, outflow_n, outflow_r, outflow_s, passive_scalar, & |
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109 | precipitation, tsc, use_cmax |
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110 | |
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111 | USE grid_variables, & |
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112 | ONLY: ddx, ddy, dx, dy |
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113 | |
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114 | USE indices, & |
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115 | ONLY: nx, nxl, nxlg, nxr, nxrg, ny, nyn, nyng, nys, nysg, & |
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116 | nzb, nzb_s_inner, nzb_w_inner, nzt |
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117 | |
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118 | USE kinds |
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119 | |
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120 | USE pegrid |
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121 | |
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122 | |
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123 | IMPLICIT NONE |
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124 | |
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125 | INTEGER(iwp) :: i !: |
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126 | INTEGER(iwp) :: j !: |
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127 | INTEGER(iwp) :: k !: |
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128 | |
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129 | REAL(wp) :: c_max !: |
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130 | REAL(wp) :: denom !: |
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131 | |
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132 | |
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133 | ! |
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134 | !-- Bottom boundary |
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135 | IF ( ibc_uv_b == 1 ) THEN |
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136 | !$acc kernels present( u_p, v_p ) |
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137 | u_p(nzb,:,:) = u_p(nzb+1,:,:) |
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138 | v_p(nzb,:,:) = v_p(nzb+1,:,:) |
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139 | !$acc end kernels |
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140 | ENDIF |
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141 | |
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142 | !$acc kernels present( nzb_w_inner, w_p ) |
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143 | DO i = nxlg, nxrg |
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144 | DO j = nysg, nyng |
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145 | w_p(nzb_w_inner(j,i),j,i) = 0.0_wp |
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146 | ENDDO |
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147 | ENDDO |
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148 | !$acc end kernels |
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149 | |
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150 | ! |
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151 | !-- Top boundary |
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152 | IF ( ibc_uv_t == 0 ) THEN |
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153 | !$acc kernels present( u_init, u_p, v_init, v_p ) |
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154 | u_p(nzt+1,:,:) = u_init(nzt+1) |
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155 | v_p(nzt+1,:,:) = v_init(nzt+1) |
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156 | IF ( large_scale_forcing) THEN |
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157 | u_p(nzt+1,:,:) = ug(nzt+1) |
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158 | v_p(nzt+1,:,:) = vg(nzt+1) |
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159 | END IF |
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160 | !$acc end kernels |
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161 | ELSE |
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162 | !$acc kernels present( u_p, v_p ) |
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163 | u_p(nzt+1,:,:) = u_p(nzt,:,:) |
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164 | v_p(nzt+1,:,:) = v_p(nzt,:,:) |
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165 | !$acc end kernels |
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166 | ENDIF |
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167 | !$acc kernels present( w_p ) |
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168 | w_p(nzt:nzt+1,:,:) = 0.0_wp ! nzt is not a prognostic level (but cf. pres) |
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169 | !$acc end kernels |
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170 | |
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171 | ! |
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172 | !-- Temperature at bottom boundary. |
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173 | !-- In case of coupled runs (ibc_pt_b = 2) the temperature is given by |
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174 | !-- the sea surface temperature of the coupled ocean model. |
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175 | IF ( ibc_pt_b == 0 ) THEN |
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176 | !$acc kernels present( nzb_s_inner, pt, pt_p ) |
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177 | !$acc loop independent |
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178 | DO i = nxlg, nxrg |
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179 | !$acc loop independent |
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180 | DO j = nysg, nyng |
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181 | pt_p(nzb_s_inner(j,i),j,i) = pt(nzb_s_inner(j,i),j,i) |
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182 | ENDDO |
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183 | ENDDO |
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184 | !$acc end kernels |
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185 | ELSEIF ( ibc_pt_b == 1 ) THEN |
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186 | !$acc kernels present( nzb_s_inner, pt_p ) |
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187 | !$acc loop independent |
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188 | DO i = nxlg, nxrg |
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189 | !$acc loop independent |
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190 | DO j = nysg, nyng |
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191 | pt_p(nzb_s_inner(j,i),j,i) = pt_p(nzb_s_inner(j,i)+1,j,i) |
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192 | ENDDO |
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193 | ENDDO |
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194 | !$acc end kernels |
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195 | ENDIF |
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196 | |
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197 | ! |
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198 | !-- Temperature at top boundary |
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199 | IF ( ibc_pt_t == 0 ) THEN |
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200 | !$acc kernels present( pt, pt_p ) |
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201 | pt_p(nzt+1,:,:) = pt(nzt+1,:,:) |
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202 | !$acc end kernels |
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203 | ELSEIF ( ibc_pt_t == 1 ) THEN |
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204 | !$acc kernels present( pt_p ) |
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205 | pt_p(nzt+1,:,:) = pt_p(nzt,:,:) |
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206 | !$acc end kernels |
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207 | ELSEIF ( ibc_pt_t == 2 ) THEN |
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208 | !$acc kernels present( dzu, pt_p ) |
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209 | pt_p(nzt+1,:,:) = pt_p(nzt,:,:) + bc_pt_t_val * dzu(nzt+1) |
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210 | !$acc end kernels |
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211 | ENDIF |
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212 | |
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213 | ! |
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214 | !-- Boundary conditions for TKE |
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215 | !-- Generally Neumann conditions with de/dz=0 are assumed |
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216 | IF ( .NOT. constant_diffusion ) THEN |
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217 | !$acc kernels present( e_p, nzb_s_inner ) |
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218 | !$acc loop independent |
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219 | DO i = nxlg, nxrg |
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220 | !$acc loop independent |
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221 | DO j = nysg, nyng |
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222 | e_p(nzb_s_inner(j,i),j,i) = e_p(nzb_s_inner(j,i)+1,j,i) |
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223 | ENDDO |
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224 | ENDDO |
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225 | e_p(nzt+1,:,:) = e_p(nzt,:,:) |
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226 | !$acc end kernels |
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227 | ENDIF |
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228 | |
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229 | ! |
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230 | !-- Boundary conditions for salinity |
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231 | IF ( ocean ) THEN |
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232 | ! |
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233 | !-- Bottom boundary: Neumann condition because salinity flux is always |
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234 | !-- given |
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235 | DO i = nxlg, nxrg |
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236 | DO j = nysg, nyng |
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237 | sa_p(nzb_s_inner(j,i),j,i) = sa_p(nzb_s_inner(j,i)+1,j,i) |
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238 | ENDDO |
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239 | ENDDO |
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240 | |
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241 | ! |
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242 | !-- Top boundary: Dirichlet or Neumann |
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243 | IF ( ibc_sa_t == 0 ) THEN |
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244 | sa_p(nzt+1,:,:) = sa(nzt+1,:,:) |
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245 | ELSEIF ( ibc_sa_t == 1 ) THEN |
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246 | sa_p(nzt+1,:,:) = sa_p(nzt,:,:) |
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247 | ENDIF |
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248 | |
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249 | ENDIF |
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250 | |
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251 | ! |
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252 | !-- Boundary conditions for total water content or scalar, |
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253 | !-- bottom and top boundary (see also temperature) |
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254 | IF ( humidity .OR. passive_scalar ) THEN |
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255 | ! |
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256 | !-- Surface conditions for constant_humidity_flux |
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257 | IF ( ibc_q_b == 0 ) THEN |
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258 | DO i = nxlg, nxrg |
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259 | DO j = nysg, nyng |
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260 | q_p(nzb_s_inner(j,i),j,i) = q(nzb_s_inner(j,i),j,i) |
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261 | ENDDO |
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262 | ENDDO |
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263 | ELSE |
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264 | DO i = nxlg, nxrg |
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265 | DO j = nysg, nyng |
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266 | q_p(nzb_s_inner(j,i),j,i) = q_p(nzb_s_inner(j,i)+1,j,i) |
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267 | ENDDO |
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268 | ENDDO |
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269 | ENDIF |
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270 | ! |
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271 | !-- Top boundary |
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272 | q_p(nzt+1,:,:) = q_p(nzt,:,:) + bc_q_t_val * dzu(nzt+1) |
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273 | |
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274 | IF ( cloud_physics .AND. icloud_scheme == 0 .AND. precipitation ) THEN |
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275 | ! |
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276 | !-- Surface conditions rain water (Dirichlet) |
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277 | DO i = nxlg, nxrg |
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278 | DO j = nysg, nyng |
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279 | qr_p(nzb_s_inner(j,i),j,i) = 0.0_wp |
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280 | nr_p(nzb_s_inner(j,i),j,i) = 0.0_wp |
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281 | ENDDO |
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282 | ENDDO |
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283 | ! |
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284 | !-- Top boundary condition for rain water (Dirichlet) |
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285 | qr_p(nzt+1,:,:) = 0.0_wp |
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286 | nr_p(nzt+1,:,:) = 0.0_wp |
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287 | |
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288 | ENDIF |
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289 | ! |
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290 | !-- In case of inflow at the south boundary the boundary for v is at nys |
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291 | !-- and in case of inflow at the left boundary the boundary for u is at nxl. |
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292 | !-- Since in prognostic_equations (cache optimized version) these levels are |
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293 | !-- handled as a prognostic level, boundary values have to be restored here. |
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294 | !-- For the SGS-TKE, Neumann boundary conditions are used at the inflow. |
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295 | IF ( inflow_s ) THEN |
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296 | v_p(:,nys,:) = v_p(:,nys-1,:) |
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297 | IF ( .NOT. constant_diffusion ) e_p(:,nys-1,:) = e_p(:,nys,:) |
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298 | ELSEIF ( inflow_n ) THEN |
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299 | IF ( .NOT. constant_diffusion ) e_p(:,nyn+1,:) = e_p(:,nyn,:) |
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300 | ELSEIF ( inflow_l ) THEN |
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301 | u_p(:,:,nxl) = u_p(:,:,nxl-1) |
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302 | IF ( .NOT. constant_diffusion ) e_p(:,:,nxl-1) = e_p(:,:,nxl) |
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303 | ELSEIF ( inflow_r ) THEN |
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304 | IF ( .NOT. constant_diffusion ) e_p(:,:,nxr+1) = e_p(:,:,nxr) |
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305 | ENDIF |
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306 | |
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307 | ! |
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308 | !-- Lateral boundary conditions for scalar quantities at the outflow |
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309 | IF ( outflow_s ) THEN |
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310 | pt_p(:,nys-1,:) = pt_p(:,nys,:) |
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311 | IF ( .NOT. constant_diffusion ) e_p(:,nys-1,:) = e_p(:,nys,:) |
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312 | IF ( humidity .OR. passive_scalar ) THEN |
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313 | q_p(:,nys-1,:) = q_p(:,nys,:) |
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314 | IF ( cloud_physics .AND. icloud_scheme == 0 .AND. & |
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315 | precipitation) THEN |
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316 | qr_p(:,nys-1,:) = qr_p(:,nys,:) |
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317 | nr_p(:,nys-1,:) = nr_p(:,nys,:) |
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318 | ENDIF |
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319 | ENDIF |
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320 | ELSEIF ( outflow_n ) THEN |
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321 | pt_p(:,nyn+1,:) = pt_p(:,nyn,:) |
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322 | IF ( .NOT. constant_diffusion ) e_p(:,nyn+1,:) = e_p(:,nyn,:) |
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323 | IF ( humidity .OR. passive_scalar ) THEN |
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324 | q_p(:,nyn+1,:) = q_p(:,nyn,:) |
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325 | IF ( cloud_physics .AND. icloud_scheme == 0 .AND. & |
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326 | precipitation ) THEN |
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327 | qr_p(:,nyn+1,:) = qr_p(:,nyn,:) |
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328 | nr_p(:,nyn+1,:) = nr_p(:,nyn,:) |
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329 | ENDIF |
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330 | ENDIF |
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331 | ELSEIF ( outflow_l ) THEN |
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332 | pt_p(:,:,nxl-1) = pt_p(:,:,nxl) |
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333 | IF ( .NOT. constant_diffusion ) e_p(:,:,nxl-1) = e_p(:,:,nxl) |
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334 | IF ( humidity .OR. passive_scalar ) THEN |
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335 | q_p(:,:,nxl-1) = q_p(:,:,nxl) |
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336 | IF ( cloud_physics .AND. icloud_scheme == 0 .AND. & |
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337 | precipitation ) THEN |
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338 | qr_p(:,:,nxl-1) = qr_p(:,:,nxl) |
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339 | nr_p(:,:,nxl-1) = nr_p(:,:,nxl) |
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340 | ENDIF |
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341 | ENDIF |
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342 | ELSEIF ( outflow_r ) THEN |
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343 | pt_p(:,:,nxr+1) = pt_p(:,:,nxr) |
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344 | IF ( .NOT. constant_diffusion ) e_p(:,:,nxr+1) = e_p(:,:,nxr) |
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345 | IF ( humidity .OR. passive_scalar ) THEN |
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346 | q_p(:,:,nxr+1) = q_p(:,:,nxr) |
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347 | IF ( cloud_physics .AND. icloud_scheme == 0 .AND. precipitation ) THEN |
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348 | qr_p(:,:,nxr+1) = qr_p(:,:,nxr) |
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349 | nr_p(:,:,nxr+1) = nr_p(:,:,nxr) |
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350 | ENDIF |
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351 | ENDIF |
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352 | ENDIF |
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353 | |
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354 | ENDIF |
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355 | |
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356 | ! |
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357 | !-- Radiation boundary conditions for the velocities at the respective outflow. |
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358 | !-- The phase velocity is either assumed to the maximum phase velocity that |
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359 | !-- ensures numerical stability (CFL-condition) or calculated after |
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360 | !-- Orlanski(1976) and averaged along the outflow boundary. |
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361 | IF ( outflow_s ) THEN |
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362 | |
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363 | IF ( use_cmax ) THEN |
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364 | u_p(:,-1,:) = u(:,0,:) |
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365 | v_p(:,0,:) = v(:,1,:) |
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366 | w_p(:,-1,:) = w(:,0,:) |
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367 | ELSEIF ( .NOT. use_cmax ) THEN |
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368 | |
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369 | c_max = dy / dt_3d |
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370 | |
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371 | c_u_m_l = 0.0_wp |
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372 | c_v_m_l = 0.0_wp |
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373 | c_w_m_l = 0.0_wp |
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374 | |
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375 | c_u_m = 0.0_wp |
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376 | c_v_m = 0.0_wp |
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377 | c_w_m = 0.0_wp |
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378 | |
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379 | ! |
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380 | !-- Calculate the phase speeds for u, v, and w, first local and then |
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381 | !-- average along the outflow boundary. |
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382 | DO k = nzb+1, nzt+1 |
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383 | DO i = nxl, nxr |
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384 | |
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385 | denom = u_m_s(k,0,i) - u_m_s(k,1,i) |
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386 | |
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387 | IF ( denom /= 0.0_wp ) THEN |
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388 | c_u(k,i) = -c_max * ( u(k,0,i) - u_m_s(k,0,i) ) / ( denom * tsc(2) ) |
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389 | IF ( c_u(k,i) < 0.0_wp ) THEN |
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390 | c_u(k,i) = 0.0_wp |
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391 | ELSEIF ( c_u(k,i) > c_max ) THEN |
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392 | c_u(k,i) = c_max |
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393 | ENDIF |
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394 | ELSE |
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395 | c_u(k,i) = c_max |
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396 | ENDIF |
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397 | |
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398 | denom = v_m_s(k,1,i) - v_m_s(k,2,i) |
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399 | |
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400 | IF ( denom /= 0.0_wp ) THEN |
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401 | c_v(k,i) = -c_max * ( v(k,1,i) - v_m_s(k,1,i) ) / ( denom * tsc(2) ) |
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402 | IF ( c_v(k,i) < 0.0_wp ) THEN |
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403 | c_v(k,i) = 0.0_wp |
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404 | ELSEIF ( c_v(k,i) > c_max ) THEN |
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405 | c_v(k,i) = c_max |
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406 | ENDIF |
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407 | ELSE |
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408 | c_v(k,i) = c_max |
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409 | ENDIF |
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410 | |
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411 | denom = w_m_s(k,0,i) - w_m_s(k,1,i) |
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412 | |
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413 | IF ( denom /= 0.0_wp ) THEN |
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414 | c_w(k,i) = -c_max * ( w(k,0,i) - w_m_s(k,0,i) ) / ( denom * tsc(2) ) |
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415 | IF ( c_w(k,i) < 0.0_wp ) THEN |
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416 | c_w(k,i) = 0.0_wp |
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417 | ELSEIF ( c_w(k,i) > c_max ) THEN |
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418 | c_w(k,i) = c_max |
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419 | ENDIF |
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420 | ELSE |
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421 | c_w(k,i) = c_max |
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422 | ENDIF |
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423 | |
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424 | c_u_m_l(k) = c_u_m_l(k) + c_u(k,i) |
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425 | c_v_m_l(k) = c_v_m_l(k) + c_v(k,i) |
---|
426 | c_w_m_l(k) = c_w_m_l(k) + c_w(k,i) |
---|
427 | |
---|
428 | ENDDO |
---|
429 | ENDDO |
---|
430 | |
---|
431 | #if defined( __parallel ) |
---|
432 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dx, ierr ) |
---|
433 | CALL MPI_ALLREDUCE( c_u_m_l(nzb+1), c_u_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
434 | MPI_SUM, comm1dx, ierr ) |
---|
435 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dx, ierr ) |
---|
436 | CALL MPI_ALLREDUCE( c_v_m_l(nzb+1), c_v_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_w_m_l(nzb+1), c_w_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
440 | MPI_SUM, comm1dx, ierr ) |
---|
441 | #else |
---|
442 | c_u_m = c_u_m_l |
---|
443 | c_v_m = c_v_m_l |
---|
444 | c_w_m = c_w_m_l |
---|
445 | #endif |
---|
446 | |
---|
447 | c_u_m = c_u_m / (nx+1) |
---|
448 | c_v_m = c_v_m / (nx+1) |
---|
449 | c_w_m = c_w_m / (nx+1) |
---|
450 | |
---|
451 | ! |
---|
452 | !-- Save old timelevels for the next timestep |
---|
453 | IF ( intermediate_timestep_count == 1 ) THEN |
---|
454 | u_m_s(:,:,:) = u(:,0:1,:) |
---|
455 | v_m_s(:,:,:) = v(:,1:2,:) |
---|
456 | w_m_s(:,:,:) = w(:,0:1,:) |
---|
457 | ENDIF |
---|
458 | |
---|
459 | ! |
---|
460 | !-- Calculate the new velocities |
---|
461 | DO k = nzb+1, nzt+1 |
---|
462 | DO i = nxlg, nxrg |
---|
463 | u_p(k,-1,i) = u(k,-1,i) - dt_3d * tsc(2) * c_u_m(k) * & |
---|
464 | ( u(k,-1,i) - u(k,0,i) ) * ddy |
---|
465 | |
---|
466 | v_p(k,0,i) = v(k,0,i) - dt_3d * tsc(2) * c_v_m(k) * & |
---|
467 | ( v(k,0,i) - v(k,1,i) ) * ddy |
---|
468 | |
---|
469 | w_p(k,-1,i) = w(k,-1,i) - dt_3d * tsc(2) * c_w_m(k) * & |
---|
470 | ( w(k,-1,i) - w(k,0,i) ) * ddy |
---|
471 | ENDDO |
---|
472 | ENDDO |
---|
473 | |
---|
474 | ! |
---|
475 | !-- Bottom boundary at the outflow |
---|
476 | IF ( ibc_uv_b == 0 ) THEN |
---|
477 | u_p(nzb,-1,:) = 0.0_wp |
---|
478 | v_p(nzb,0,:) = 0.0_wp |
---|
479 | ELSE |
---|
480 | u_p(nzb,-1,:) = u_p(nzb+1,-1,:) |
---|
481 | v_p(nzb,0,:) = v_p(nzb+1,0,:) |
---|
482 | ENDIF |
---|
483 | w_p(nzb,-1,:) = 0.0_wp |
---|
484 | |
---|
485 | ! |
---|
486 | !-- Top boundary at the outflow |
---|
487 | IF ( ibc_uv_t == 0 ) THEN |
---|
488 | u_p(nzt+1,-1,:) = u_init(nzt+1) |
---|
489 | v_p(nzt+1,0,:) = v_init(nzt+1) |
---|
490 | ELSE |
---|
491 | u_p(nzt+1,-1,:) = u(nzt,-1,:) |
---|
492 | v_p(nzt+1,0,:) = v(nzt,0,:) |
---|
493 | ENDIF |
---|
494 | w_p(nzt:nzt+1,-1,:) = 0.0_wp |
---|
495 | |
---|
496 | ENDIF |
---|
497 | |
---|
498 | ENDIF |
---|
499 | |
---|
500 | IF ( outflow_n ) THEN |
---|
501 | |
---|
502 | IF ( use_cmax ) THEN |
---|
503 | u_p(:,ny+1,:) = u(:,ny,:) |
---|
504 | v_p(:,ny+1,:) = v(:,ny,:) |
---|
505 | w_p(:,ny+1,:) = w(:,ny,:) |
---|
506 | ELSEIF ( .NOT. use_cmax ) THEN |
---|
507 | |
---|
508 | c_max = dy / dt_3d |
---|
509 | |
---|
510 | c_u_m_l = 0.0_wp |
---|
511 | c_v_m_l = 0.0_wp |
---|
512 | c_w_m_l = 0.0_wp |
---|
513 | |
---|
514 | c_u_m = 0.0_wp |
---|
515 | c_v_m = 0.0_wp |
---|
516 | c_w_m = 0.0_wp |
---|
517 | |
---|
518 | ! |
---|
519 | !-- Calculate the phase speeds for u, v, and w, first local and then |
---|
520 | !-- average along the outflow boundary. |
---|
521 | DO k = nzb+1, nzt+1 |
---|
522 | DO i = nxl, nxr |
---|
523 | |
---|
524 | denom = u_m_n(k,ny,i) - u_m_n(k,ny-1,i) |
---|
525 | |
---|
526 | IF ( denom /= 0.0_wp ) THEN |
---|
527 | c_u(k,i) = -c_max * ( u(k,ny,i) - u_m_n(k,ny,i) ) / ( denom * tsc(2) ) |
---|
528 | IF ( c_u(k,i) < 0.0_wp ) THEN |
---|
529 | c_u(k,i) = 0.0_wp |
---|
530 | ELSEIF ( c_u(k,i) > c_max ) THEN |
---|
531 | c_u(k,i) = c_max |
---|
532 | ENDIF |
---|
533 | ELSE |
---|
534 | c_u(k,i) = c_max |
---|
535 | ENDIF |
---|
536 | |
---|
537 | denom = v_m_n(k,ny,i) - v_m_n(k,ny-1,i) |
---|
538 | |
---|
539 | IF ( denom /= 0.0_wp ) THEN |
---|
540 | c_v(k,i) = -c_max * ( v(k,ny,i) - v_m_n(k,ny,i) ) / ( denom * tsc(2) ) |
---|
541 | IF ( c_v(k,i) < 0.0_wp ) THEN |
---|
542 | c_v(k,i) = 0.0_wp |
---|
543 | ELSEIF ( c_v(k,i) > c_max ) THEN |
---|
544 | c_v(k,i) = c_max |
---|
545 | ENDIF |
---|
546 | ELSE |
---|
547 | c_v(k,i) = c_max |
---|
548 | ENDIF |
---|
549 | |
---|
550 | denom = w_m_n(k,ny,i) - w_m_n(k,ny-1,i) |
---|
551 | |
---|
552 | IF ( denom /= 0.0_wp ) THEN |
---|
553 | c_w(k,i) = -c_max * ( w(k,ny,i) - w_m_n(k,ny,i) ) / ( denom * tsc(2) ) |
---|
554 | IF ( c_w(k,i) < 0.0_wp ) THEN |
---|
555 | c_w(k,i) = 0.0_wp |
---|
556 | ELSEIF ( c_w(k,i) > c_max ) THEN |
---|
557 | c_w(k,i) = c_max |
---|
558 | ENDIF |
---|
559 | ELSE |
---|
560 | c_w(k,i) = c_max |
---|
561 | ENDIF |
---|
562 | |
---|
563 | c_u_m_l(k) = c_u_m_l(k) + c_u(k,i) |
---|
564 | c_v_m_l(k) = c_v_m_l(k) + c_v(k,i) |
---|
565 | c_w_m_l(k) = c_w_m_l(k) + c_w(k,i) |
---|
566 | |
---|
567 | ENDDO |
---|
568 | ENDDO |
---|
569 | |
---|
570 | #if defined( __parallel ) |
---|
571 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dx, ierr ) |
---|
572 | CALL MPI_ALLREDUCE( c_u_m_l(nzb+1), c_u_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
573 | MPI_SUM, comm1dx, ierr ) |
---|
574 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dx, ierr ) |
---|
575 | CALL MPI_ALLREDUCE( c_v_m_l(nzb+1), c_v_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_w_m_l(nzb+1), c_w_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
579 | MPI_SUM, comm1dx, ierr ) |
---|
580 | #else |
---|
581 | c_u_m = c_u_m_l |
---|
582 | c_v_m = c_v_m_l |
---|
583 | c_w_m = c_w_m_l |
---|
584 | #endif |
---|
585 | |
---|
586 | c_u_m = c_u_m / (nx+1) |
---|
587 | c_v_m = c_v_m / (nx+1) |
---|
588 | c_w_m = c_w_m / (nx+1) |
---|
589 | |
---|
590 | ! |
---|
591 | !-- Save old timelevels for the next timestep |
---|
592 | IF ( intermediate_timestep_count == 1 ) THEN |
---|
593 | u_m_n(:,:,:) = u(:,ny-1:ny,:) |
---|
594 | v_m_n(:,:,:) = v(:,ny-1:ny,:) |
---|
595 | w_m_n(:,:,:) = w(:,ny-1:ny,:) |
---|
596 | ENDIF |
---|
597 | |
---|
598 | ! |
---|
599 | !-- Calculate the new velocities |
---|
600 | DO k = nzb+1, nzt+1 |
---|
601 | DO i = nxlg, nxrg |
---|
602 | u_p(k,ny+1,i) = u(k,ny+1,i) - dt_3d * tsc(2) * c_u_m(k) * & |
---|
603 | ( u(k,ny+1,i) - u(k,ny,i) ) * ddy |
---|
604 | |
---|
605 | v_p(k,ny+1,i) = v(k,ny+1,i) - dt_3d * tsc(2) * c_v_m(k) * & |
---|
606 | ( v(k,ny+1,i) - v(k,ny,i) ) * ddy |
---|
607 | |
---|
608 | w_p(k,ny+1,i) = w(k,ny+1,i) - dt_3d * tsc(2) * c_w_m(k) * & |
---|
609 | ( w(k,ny+1,i) - w(k,ny,i) ) * ddy |
---|
610 | ENDDO |
---|
611 | ENDDO |
---|
612 | |
---|
613 | ! |
---|
614 | !-- Bottom boundary at the outflow |
---|
615 | IF ( ibc_uv_b == 0 ) THEN |
---|
616 | u_p(nzb,ny+1,:) = 0.0_wp |
---|
617 | v_p(nzb,ny+1,:) = 0.0_wp |
---|
618 | ELSE |
---|
619 | u_p(nzb,ny+1,:) = u_p(nzb+1,ny+1,:) |
---|
620 | v_p(nzb,ny+1,:) = v_p(nzb+1,ny+1,:) |
---|
621 | ENDIF |
---|
622 | w_p(nzb,ny+1,:) = 0.0_wp |
---|
623 | |
---|
624 | ! |
---|
625 | !-- Top boundary at the outflow |
---|
626 | IF ( ibc_uv_t == 0 ) THEN |
---|
627 | u_p(nzt+1,ny+1,:) = u_init(nzt+1) |
---|
628 | v_p(nzt+1,ny+1,:) = v_init(nzt+1) |
---|
629 | ELSE |
---|
630 | u_p(nzt+1,ny+1,:) = u_p(nzt,nyn+1,:) |
---|
631 | v_p(nzt+1,ny+1,:) = v_p(nzt,nyn+1,:) |
---|
632 | ENDIF |
---|
633 | w_p(nzt:nzt+1,ny+1,:) = 0.0_wp |
---|
634 | |
---|
635 | ENDIF |
---|
636 | |
---|
637 | ENDIF |
---|
638 | |
---|
639 | IF ( outflow_l ) THEN |
---|
640 | |
---|
641 | IF ( use_cmax ) THEN |
---|
642 | u_p(:,:,-1) = u(:,:,0) |
---|
643 | v_p(:,:,0) = v(:,:,1) |
---|
644 | w_p(:,:,-1) = w(:,:,0) |
---|
645 | ELSEIF ( .NOT. use_cmax ) THEN |
---|
646 | |
---|
647 | c_max = dx / dt_3d |
---|
648 | |
---|
649 | c_u_m_l = 0.0_wp |
---|
650 | c_v_m_l = 0.0_wp |
---|
651 | c_w_m_l = 0.0_wp |
---|
652 | |
---|
653 | c_u_m = 0.0_wp |
---|
654 | c_v_m = 0.0_wp |
---|
655 | c_w_m = 0.0_wp |
---|
656 | |
---|
657 | ! |
---|
658 | !-- Calculate the phase speeds for u, v, and w, first local and then |
---|
659 | !-- average along the outflow boundary. |
---|
660 | DO k = nzb+1, nzt+1 |
---|
661 | DO j = nys, nyn |
---|
662 | |
---|
663 | denom = u_m_l(k,j,1) - u_m_l(k,j,2) |
---|
664 | |
---|
665 | IF ( denom /= 0.0_wp ) THEN |
---|
666 | c_u(k,j) = -c_max * ( u(k,j,1) - u_m_l(k,j,1) ) / ( denom * tsc(2) ) |
---|
667 | IF ( c_u(k,j) < 0.0_wp ) THEN |
---|
668 | c_u(k,j) = 0.0_wp |
---|
669 | ELSEIF ( c_u(k,j) > c_max ) THEN |
---|
670 | c_u(k,j) = c_max |
---|
671 | ENDIF |
---|
672 | ELSE |
---|
673 | c_u(k,j) = c_max |
---|
674 | ENDIF |
---|
675 | |
---|
676 | denom = v_m_l(k,j,0) - v_m_l(k,j,1) |
---|
677 | |
---|
678 | IF ( denom /= 0.0_wp ) THEN |
---|
679 | c_v(k,j) = -c_max * ( v(k,j,0) - v_m_l(k,j,0) ) / ( denom * tsc(2) ) |
---|
680 | IF ( c_v(k,j) < 0.0_wp ) THEN |
---|
681 | c_v(k,j) = 0.0_wp |
---|
682 | ELSEIF ( c_v(k,j) > c_max ) THEN |
---|
683 | c_v(k,j) = c_max |
---|
684 | ENDIF |
---|
685 | ELSE |
---|
686 | c_v(k,j) = c_max |
---|
687 | ENDIF |
---|
688 | |
---|
689 | denom = w_m_l(k,j,0) - w_m_l(k,j,1) |
---|
690 | |
---|
691 | IF ( denom /= 0.0_wp ) THEN |
---|
692 | c_w(k,j) = -c_max * ( w(k,j,0) - w_m_l(k,j,0) ) / ( denom * tsc(2) ) |
---|
693 | IF ( c_w(k,j) < 0.0_wp ) THEN |
---|
694 | c_w(k,j) = 0.0_wp |
---|
695 | ELSEIF ( c_w(k,j) > c_max ) THEN |
---|
696 | c_w(k,j) = c_max |
---|
697 | ENDIF |
---|
698 | ELSE |
---|
699 | c_w(k,j) = c_max |
---|
700 | ENDIF |
---|
701 | |
---|
702 | c_u_m_l(k) = c_u_m_l(k) + c_u(k,j) |
---|
703 | c_v_m_l(k) = c_v_m_l(k) + c_v(k,j) |
---|
704 | c_w_m_l(k) = c_w_m_l(k) + c_w(k,j) |
---|
705 | |
---|
706 | ENDDO |
---|
707 | ENDDO |
---|
708 | |
---|
709 | #if defined( __parallel ) |
---|
710 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dy, ierr ) |
---|
711 | CALL MPI_ALLREDUCE( c_u_m_l(nzb+1), c_u_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
712 | MPI_SUM, comm1dy, ierr ) |
---|
713 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dy, ierr ) |
---|
714 | CALL MPI_ALLREDUCE( c_v_m_l(nzb+1), c_v_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_w_m_l(nzb+1), c_w_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
718 | MPI_SUM, comm1dy, ierr ) |
---|
719 | #else |
---|
720 | c_u_m = c_u_m_l |
---|
721 | c_v_m = c_v_m_l |
---|
722 | c_w_m = c_w_m_l |
---|
723 | #endif |
---|
724 | |
---|
725 | c_u_m = c_u_m / (ny+1) |
---|
726 | c_v_m = c_v_m / (ny+1) |
---|
727 | c_w_m = c_w_m / (ny+1) |
---|
728 | |
---|
729 | ! |
---|
730 | !-- Save old timelevels for the next timestep |
---|
731 | IF ( intermediate_timestep_count == 1 ) THEN |
---|
732 | u_m_l(:,:,:) = u(:,:,1:2) |
---|
733 | v_m_l(:,:,:) = v(:,:,0:1) |
---|
734 | w_m_l(:,:,:) = w(:,:,0:1) |
---|
735 | ENDIF |
---|
736 | |
---|
737 | ! |
---|
738 | !-- Calculate the new velocities |
---|
739 | DO k = nzb+1, nzt+1 |
---|
740 | DO j = nysg, nyng |
---|
741 | u_p(k,j,0) = u(k,j,0) - dt_3d * tsc(2) * c_u_m(k) * & |
---|
742 | ( u(k,j,0) - u(k,j,1) ) * ddx |
---|
743 | |
---|
744 | v_p(k,j,-1) = v(k,j,-1) - dt_3d * tsc(2) * c_v_m(k) * & |
---|
745 | ( v(k,j,-1) - v(k,j,0) ) * ddx |
---|
746 | |
---|
747 | w_p(k,j,-1) = w(k,j,-1) - dt_3d * tsc(2) * c_w_m(k) * & |
---|
748 | ( w(k,j,-1) - w(k,j,0) ) * ddx |
---|
749 | ENDDO |
---|
750 | ENDDO |
---|
751 | |
---|
752 | ! |
---|
753 | !-- Bottom boundary at the outflow |
---|
754 | IF ( ibc_uv_b == 0 ) THEN |
---|
755 | u_p(nzb,:,0) = 0.0_wp |
---|
756 | v_p(nzb,:,-1) = 0.0_wp |
---|
757 | ELSE |
---|
758 | u_p(nzb,:,0) = u_p(nzb+1,:,0) |
---|
759 | v_p(nzb,:,-1) = v_p(nzb+1,:,-1) |
---|
760 | ENDIF |
---|
761 | w_p(nzb,:,-1) = 0.0_wp |
---|
762 | |
---|
763 | ! |
---|
764 | !-- Top boundary at the outflow |
---|
765 | IF ( ibc_uv_t == 0 ) THEN |
---|
766 | u_p(nzt+1,:,-1) = u_init(nzt+1) |
---|
767 | v_p(nzt+1,:,-1) = v_init(nzt+1) |
---|
768 | ELSE |
---|
769 | u_p(nzt+1,:,-1) = u_p(nzt,:,-1) |
---|
770 | v_p(nzt+1,:,-1) = v_p(nzt,:,-1) |
---|
771 | ENDIF |
---|
772 | w_p(nzt:nzt+1,:,-1) = 0.0_wp |
---|
773 | |
---|
774 | ENDIF |
---|
775 | |
---|
776 | ENDIF |
---|
777 | |
---|
778 | IF ( outflow_r ) THEN |
---|
779 | |
---|
780 | IF ( use_cmax ) THEN |
---|
781 | u_p(:,:,nx+1) = u(:,:,nx) |
---|
782 | v_p(:,:,nx+1) = v(:,:,nx) |
---|
783 | w_p(:,:,nx+1) = w(:,:,nx) |
---|
784 | ELSEIF ( .NOT. use_cmax ) THEN |
---|
785 | |
---|
786 | c_max = dx / dt_3d |
---|
787 | |
---|
788 | c_u_m_l = 0.0_wp |
---|
789 | c_v_m_l = 0.0_wp |
---|
790 | c_w_m_l = 0.0_wp |
---|
791 | |
---|
792 | c_u_m = 0.0_wp |
---|
793 | c_v_m = 0.0_wp |
---|
794 | c_w_m = 0.0_wp |
---|
795 | |
---|
796 | ! |
---|
797 | !-- Calculate the phase speeds for u, v, and w, first local and then |
---|
798 | !-- average along the outflow boundary. |
---|
799 | DO k = nzb+1, nzt+1 |
---|
800 | DO j = nys, nyn |
---|
801 | |
---|
802 | denom = u_m_r(k,j,nx) - u_m_r(k,j,nx-1) |
---|
803 | |
---|
804 | IF ( denom /= 0.0_wp ) THEN |
---|
805 | c_u(k,j) = -c_max * ( u(k,j,nx) - u_m_r(k,j,nx) ) / ( denom * tsc(2) ) |
---|
806 | IF ( c_u(k,j) < 0.0_wp ) THEN |
---|
807 | c_u(k,j) = 0.0_wp |
---|
808 | ELSEIF ( c_u(k,j) > c_max ) THEN |
---|
809 | c_u(k,j) = c_max |
---|
810 | ENDIF |
---|
811 | ELSE |
---|
812 | c_u(k,j) = c_max |
---|
813 | ENDIF |
---|
814 | |
---|
815 | denom = v_m_r(k,j,nx) - v_m_r(k,j,nx-1) |
---|
816 | |
---|
817 | IF ( denom /= 0.0_wp ) THEN |
---|
818 | c_v(k,j) = -c_max * ( v(k,j,nx) - v_m_r(k,j,nx) ) / ( denom * tsc(2) ) |
---|
819 | IF ( c_v(k,j) < 0.0_wp ) THEN |
---|
820 | c_v(k,j) = 0.0_wp |
---|
821 | ELSEIF ( c_v(k,j) > c_max ) THEN |
---|
822 | c_v(k,j) = c_max |
---|
823 | ENDIF |
---|
824 | ELSE |
---|
825 | c_v(k,j) = c_max |
---|
826 | ENDIF |
---|
827 | |
---|
828 | denom = w_m_r(k,j,nx) - w_m_r(k,j,nx-1) |
---|
829 | |
---|
830 | IF ( denom /= 0.0_wp ) THEN |
---|
831 | c_w(k,j) = -c_max * ( w(k,j,nx) - w_m_r(k,j,nx) ) / ( denom * tsc(2) ) |
---|
832 | IF ( c_w(k,j) < 0.0_wp ) THEN |
---|
833 | c_w(k,j) = 0.0_wp |
---|
834 | ELSEIF ( c_w(k,j) > c_max ) THEN |
---|
835 | c_w(k,j) = c_max |
---|
836 | ENDIF |
---|
837 | ELSE |
---|
838 | c_w(k,j) = c_max |
---|
839 | ENDIF |
---|
840 | |
---|
841 | c_u_m_l(k) = c_u_m_l(k) + c_u(k,j) |
---|
842 | c_v_m_l(k) = c_v_m_l(k) + c_v(k,j) |
---|
843 | c_w_m_l(k) = c_w_m_l(k) + c_w(k,j) |
---|
844 | |
---|
845 | ENDDO |
---|
846 | ENDDO |
---|
847 | |
---|
848 | #if defined( __parallel ) |
---|
849 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dy, ierr ) |
---|
850 | CALL MPI_ALLREDUCE( c_u_m_l(nzb+1), c_u_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
851 | MPI_SUM, comm1dy, ierr ) |
---|
852 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dy, ierr ) |
---|
853 | CALL MPI_ALLREDUCE( c_v_m_l(nzb+1), c_v_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_w_m_l(nzb+1), c_w_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
857 | MPI_SUM, comm1dy, ierr ) |
---|
858 | #else |
---|
859 | c_u_m = c_u_m_l |
---|
860 | c_v_m = c_v_m_l |
---|
861 | c_w_m = c_w_m_l |
---|
862 | #endif |
---|
863 | |
---|
864 | c_u_m = c_u_m / (ny+1) |
---|
865 | c_v_m = c_v_m / (ny+1) |
---|
866 | c_w_m = c_w_m / (ny+1) |
---|
867 | |
---|
868 | ! |
---|
869 | !-- Save old timelevels for the next timestep |
---|
870 | IF ( intermediate_timestep_count == 1 ) THEN |
---|
871 | u_m_r(:,:,:) = u(:,:,nx-1:nx) |
---|
872 | v_m_r(:,:,:) = v(:,:,nx-1:nx) |
---|
873 | w_m_r(:,:,:) = w(:,:,nx-1:nx) |
---|
874 | ENDIF |
---|
875 | |
---|
876 | ! |
---|
877 | !-- Calculate the new velocities |
---|
878 | DO k = nzb+1, nzt+1 |
---|
879 | DO j = nysg, nyng |
---|
880 | u_p(k,j,nx+1) = u(k,j,nx+1) - dt_3d * tsc(2) * c_u_m(k) * & |
---|
881 | ( u(k,j,nx+1) - u(k,j,nx) ) * ddx |
---|
882 | |
---|
883 | v_p(k,j,nx+1) = v(k,j,nx+1) - dt_3d * tsc(2) * c_v_m(k) * & |
---|
884 | ( v(k,j,nx+1) - v(k,j,nx) ) * ddx |
---|
885 | |
---|
886 | w_p(k,j,nx+1) = w(k,j,nx+1) - dt_3d * tsc(2) * c_w_m(k) * & |
---|
887 | ( w(k,j,nx+1) - w(k,j,nx) ) * ddx |
---|
888 | ENDDO |
---|
889 | ENDDO |
---|
890 | |
---|
891 | ! |
---|
892 | !-- Bottom boundary at the outflow |
---|
893 | IF ( ibc_uv_b == 0 ) THEN |
---|
894 | u_p(nzb,:,nx+1) = 0.0_wp |
---|
895 | v_p(nzb,:,nx+1) = 0.0_wp |
---|
896 | ELSE |
---|
897 | u_p(nzb,:,nx+1) = u_p(nzb+1,:,nx+1) |
---|
898 | v_p(nzb,:,nx+1) = v_p(nzb+1,:,nx+1) |
---|
899 | ENDIF |
---|
900 | w_p(nzb,:,nx+1) = 0.0_wp |
---|
901 | |
---|
902 | ! |
---|
903 | !-- Top boundary at the outflow |
---|
904 | IF ( ibc_uv_t == 0 ) THEN |
---|
905 | u_p(nzt+1,:,nx+1) = u_init(nzt+1) |
---|
906 | v_p(nzt+1,:,nx+1) = v_init(nzt+1) |
---|
907 | ELSE |
---|
908 | u_p(nzt+1,:,nx+1) = u_p(nzt,:,nx+1) |
---|
909 | v_p(nzt+1,:,nx+1) = v_p(nzt,:,nx+1) |
---|
910 | ENDIF |
---|
911 | w(nzt:nzt+1,:,nx+1) = 0.0_wp |
---|
912 | |
---|
913 | ENDIF |
---|
914 | |
---|
915 | ENDIF |
---|
916 | |
---|
917 | END SUBROUTINE boundary_conds |
---|