[1682] | 1 | !> @file boundary_conds.f90 |
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[1036] | 2 | !--------------------------------------------------------------------------------! |
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| 3 | ! This file is part of PALM. |
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| 4 | ! |
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| 5 | ! PALM is free software: you can redistribute it and/or modify it under the terms |
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| 6 | ! of the GNU General Public License as published by the Free Software Foundation, |
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| 7 | ! either version 3 of the License, or (at your option) any later version. |
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| 8 | ! |
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| 9 | ! PALM is distributed in the hope that it will be useful, but WITHOUT ANY |
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| 10 | ! WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS FOR |
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| 11 | ! A PARTICULAR PURPOSE. See the GNU General Public License for more details. |
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| 12 | ! |
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| 13 | ! You should have received a copy of the GNU General Public License along with |
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| 14 | ! PALM. If not, see <http://www.gnu.org/licenses/>. |
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| 15 | ! |
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[1310] | 16 | ! Copyright 1997-2014 Leibniz Universitaet Hannover |
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[1036] | 17 | !--------------------------------------------------------------------------------! |
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| 18 | ! |
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[484] | 19 | ! Current revisions: |
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[1] | 20 | ! ----------------- |
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[1354] | 21 | ! |
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[1683] | 22 | ! |
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[1321] | 23 | ! Former revisions: |
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| 24 | ! ----------------- |
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| 25 | ! $Id: boundary_conds.f90 1683 2015-10-07 23:57:51Z raasch $ |
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| 26 | ! |
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[1683] | 27 | ! 1682 2015-10-07 23:56:08Z knoop |
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| 28 | ! Code annotations made doxygen readable |
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| 29 | ! |
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[1463] | 30 | !1410 2014-05-23 12:16:18Z suehring |
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| 31 | ! Bugfix: set dirichlet boundary condition for passive_scalar at model domain |
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| 32 | ! top |
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| 33 | ! |
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[1410] | 34 | ! 1399 2014-05-07 11:16:25Z heinze |
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| 35 | ! Bugfix: set inflow boundary conditions also if no humidity or passive_scalar |
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| 36 | ! is used. |
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| 37 | ! |
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[1399] | 38 | ! 1398 2014-05-07 11:15:00Z heinze |
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| 39 | ! Dirichlet-condition at the top for u and v changed to u_init and v_init also |
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| 40 | ! for large_scale_forcing |
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| 41 | ! |
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[1381] | 42 | ! 1380 2014-04-28 12:40:45Z heinze |
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| 43 | ! Adjust Dirichlet-condition at the top for pt in case of nudging |
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| 44 | ! |
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[1362] | 45 | ! 1361 2014-04-16 15:17:48Z hoffmann |
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| 46 | ! Bottom and top boundary conditions of rain water content (qr) and |
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| 47 | ! rain drop concentration (nr) changed to Dirichlet |
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| 48 | ! |
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[1354] | 49 | ! 1353 2014-04-08 15:21:23Z heinze |
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| 50 | ! REAL constants provided with KIND-attribute |
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| 51 | ! |
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[1321] | 52 | ! 1320 2014-03-20 08:40:49Z raasch |
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[1320] | 53 | ! ONLY-attribute added to USE-statements, |
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| 54 | ! kind-parameters added to all INTEGER and REAL declaration statements, |
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| 55 | ! kinds are defined in new module kinds, |
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| 56 | ! revision history before 2012 removed, |
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| 57 | ! comment fields (!:) to be used for variable explanations added to |
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| 58 | ! all variable declaration statements |
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[1160] | 59 | ! |
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[1258] | 60 | ! 1257 2013-11-08 15:18:40Z raasch |
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| 61 | ! loop independent clauses added |
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| 62 | ! |
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[1242] | 63 | ! 1241 2013-10-30 11:36:58Z heinze |
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| 64 | ! Adjust ug and vg at each timestep in case of large_scale_forcing |
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| 65 | ! |
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[1160] | 66 | ! 1159 2013-05-21 11:58:22Z fricke |
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[1159] | 67 | ! Bugfix: Neumann boundary conditions for the velocity components at the |
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| 68 | ! outflow are in fact radiation boundary conditions using the maximum phase |
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| 69 | ! velocity that ensures numerical stability (CFL-condition). |
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| 70 | ! Hence, logical operator use_cmax is now used instead of bc_lr_dirneu/_neudir. |
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| 71 | ! Bugfix: In case of use_cmax at the outflow, u, v, w are replaced by |
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| 72 | ! u_p, v_p, w_p |
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[1116] | 73 | ! |
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| 74 | ! 1115 2013-03-26 18:16:16Z hoffmann |
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| 75 | ! boundary conditions of two-moment cloud scheme are restricted to Neumann- |
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| 76 | ! boundary-conditions |
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| 77 | ! |
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[1114] | 78 | ! 1113 2013-03-10 02:48:14Z raasch |
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| 79 | ! GPU-porting |
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| 80 | ! dummy argument "range" removed |
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| 81 | ! Bugfix: wrong index in loops of radiation boundary condition |
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[1113] | 82 | ! |
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[1054] | 83 | ! 1053 2012-11-13 17:11:03Z hoffmann |
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| 84 | ! boundary conditions for the two new prognostic equations (nr, qr) of the |
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| 85 | ! two-moment cloud scheme |
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| 86 | ! |
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[1037] | 87 | ! 1036 2012-10-22 13:43:42Z raasch |
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| 88 | ! code put under GPL (PALM 3.9) |
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| 89 | ! |
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[997] | 90 | ! 996 2012-09-07 10:41:47Z raasch |
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| 91 | ! little reformatting |
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| 92 | ! |
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[979] | 93 | ! 978 2012-08-09 08:28:32Z fricke |
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| 94 | ! Neumann boudnary conditions are added at the inflow boundary for the SGS-TKE. |
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| 95 | ! Outflow boundary conditions for the velocity components can be set to Neumann |
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| 96 | ! conditions or to radiation conditions with a horizontal averaged phase |
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| 97 | ! velocity. |
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| 98 | ! |
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[876] | 99 | ! 875 2012-04-02 15:35:15Z gryschka |
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| 100 | ! Bugfix in case of dirichlet inflow bc at the right or north boundary |
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| 101 | ! |
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[1] | 102 | ! Revision 1.1 1997/09/12 06:21:34 raasch |
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| 103 | ! Initial revision |
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| 104 | ! |
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| 105 | ! |
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| 106 | ! Description: |
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| 107 | ! ------------ |
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[1682] | 108 | !> Boundary conditions for the prognostic quantities. |
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| 109 | !> One additional bottom boundary condition is applied for the TKE (=(u*)**2) |
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| 110 | !> in prandtl_fluxes. The cyclic lateral boundary conditions are implicitly |
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| 111 | !> handled in routine exchange_horiz. Pressure boundary conditions are |
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| 112 | !> explicitly set in routines pres, poisfft, poismg and sor. |
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[1] | 113 | !------------------------------------------------------------------------------! |
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[1682] | 114 | SUBROUTINE boundary_conds |
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| 115 | |
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[1] | 116 | |
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[1320] | 117 | USE arrays_3d, & |
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| 118 | 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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| 119 | dzu, e_p, nr_p, pt, pt_p, q, q_p, qr_p, sa, sa_p, & |
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| 120 | u, ug, u_init, u_m_l, u_m_n, u_m_r, u_m_s, u_p, & |
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| 121 | v, vg, v_init, v_m_l, v_m_n, v_m_r, v_m_s, v_p, & |
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[1380] | 122 | w, w_p, w_m_l, w_m_n, w_m_r, w_m_s,& |
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| 123 | pt_init |
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[1320] | 124 | |
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| 125 | USE control_parameters, & |
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| 126 | ONLY: bc_pt_t_val, bc_q_t_val, constant_diffusion, & |
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| 127 | cloud_physics, dt_3d, humidity, & |
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[1462] | 128 | ibc_pt_b, ibc_pt_t, ibc_q_b, ibc_q_t, ibc_sa_t, ibc_uv_b, & |
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| 129 | ibc_uv_t, icloud_scheme, inflow_l, inflow_n, inflow_r, inflow_s,& |
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[1320] | 130 | intermediate_timestep_count, large_scale_forcing, ocean, & |
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| 131 | outflow_l, outflow_n, outflow_r, outflow_s, passive_scalar, & |
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[1380] | 132 | precipitation, tsc, use_cmax, & |
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| 133 | nudging |
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[1320] | 134 | |
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| 135 | USE grid_variables, & |
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| 136 | ONLY: ddx, ddy, dx, dy |
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| 137 | |
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| 138 | USE indices, & |
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| 139 | ONLY: nx, nxl, nxlg, nxr, nxrg, ny, nyn, nyng, nys, nysg, & |
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| 140 | nzb, nzb_s_inner, nzb_w_inner, nzt |
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| 141 | |
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| 142 | USE kinds |
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| 143 | |
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[1] | 144 | USE pegrid |
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| 145 | |
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[1320] | 146 | |
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[1] | 147 | IMPLICIT NONE |
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| 148 | |
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[1682] | 149 | INTEGER(iwp) :: i !< |
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| 150 | INTEGER(iwp) :: j !< |
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| 151 | INTEGER(iwp) :: k !< |
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[1] | 152 | |
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[1682] | 153 | REAL(wp) :: c_max !< |
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| 154 | REAL(wp) :: denom !< |
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[1] | 155 | |
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[73] | 156 | |
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[1] | 157 | ! |
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[1113] | 158 | !-- Bottom boundary |
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| 159 | IF ( ibc_uv_b == 1 ) THEN |
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| 160 | !$acc kernels present( u_p, v_p ) |
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| 161 | u_p(nzb,:,:) = u_p(nzb+1,:,:) |
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| 162 | v_p(nzb,:,:) = v_p(nzb+1,:,:) |
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| 163 | !$acc end kernels |
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| 164 | ENDIF |
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| 165 | |
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| 166 | !$acc kernels present( nzb_w_inner, w_p ) |
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| 167 | DO i = nxlg, nxrg |
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| 168 | DO j = nysg, nyng |
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[1353] | 169 | w_p(nzb_w_inner(j,i),j,i) = 0.0_wp |
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[1113] | 170 | ENDDO |
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| 171 | ENDDO |
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| 172 | !$acc end kernels |
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| 173 | |
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| 174 | ! |
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| 175 | !-- Top boundary |
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| 176 | IF ( ibc_uv_t == 0 ) THEN |
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| 177 | !$acc kernels present( u_init, u_p, v_init, v_p ) |
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| 178 | u_p(nzt+1,:,:) = u_init(nzt+1) |
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| 179 | v_p(nzt+1,:,:) = v_init(nzt+1) |
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| 180 | !$acc end kernels |
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| 181 | ELSE |
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| 182 | !$acc kernels present( u_p, v_p ) |
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| 183 | u_p(nzt+1,:,:) = u_p(nzt,:,:) |
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| 184 | v_p(nzt+1,:,:) = v_p(nzt,:,:) |
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| 185 | !$acc end kernels |
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| 186 | ENDIF |
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| 187 | !$acc kernels present( w_p ) |
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[1353] | 188 | w_p(nzt:nzt+1,:,:) = 0.0_wp ! nzt is not a prognostic level (but cf. pres) |
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[1113] | 189 | !$acc end kernels |
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| 190 | |
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| 191 | ! |
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| 192 | !-- Temperature at bottom boundary. |
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| 193 | !-- In case of coupled runs (ibc_pt_b = 2) the temperature is given by |
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| 194 | !-- the sea surface temperature of the coupled ocean model. |
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| 195 | IF ( ibc_pt_b == 0 ) THEN |
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| 196 | !$acc kernels present( nzb_s_inner, pt, pt_p ) |
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[1257] | 197 | !$acc loop independent |
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[667] | 198 | DO i = nxlg, nxrg |
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[1257] | 199 | !$acc loop independent |
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[667] | 200 | DO j = nysg, nyng |
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[1113] | 201 | pt_p(nzb_s_inner(j,i),j,i) = pt(nzb_s_inner(j,i),j,i) |
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[1] | 202 | ENDDO |
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| 203 | ENDDO |
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[1113] | 204 | !$acc end kernels |
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| 205 | ELSEIF ( ibc_pt_b == 1 ) THEN |
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| 206 | !$acc kernels present( nzb_s_inner, pt_p ) |
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[1257] | 207 | !$acc loop independent |
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[1113] | 208 | DO i = nxlg, nxrg |
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[1257] | 209 | !$acc loop independent |
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[1113] | 210 | DO j = nysg, nyng |
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| 211 | pt_p(nzb_s_inner(j,i),j,i) = pt_p(nzb_s_inner(j,i)+1,j,i) |
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| 212 | ENDDO |
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| 213 | ENDDO |
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| 214 | !$acc end kernels |
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| 215 | ENDIF |
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[1] | 216 | |
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| 217 | ! |
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[1113] | 218 | !-- Temperature at top boundary |
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| 219 | IF ( ibc_pt_t == 0 ) THEN |
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| 220 | !$acc kernels present( pt, pt_p ) |
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| 221 | pt_p(nzt+1,:,:) = pt(nzt+1,:,:) |
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[1380] | 222 | ! |
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| 223 | !-- In case of nudging adjust top boundary to pt which is |
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| 224 | !-- read in from NUDGING-DATA |
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| 225 | IF ( nudging ) THEN |
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| 226 | pt_p(nzt+1,:,:) = pt_init(nzt+1) |
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| 227 | ENDIF |
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[1113] | 228 | !$acc end kernels |
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| 229 | ELSEIF ( ibc_pt_t == 1 ) THEN |
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| 230 | !$acc kernels present( pt_p ) |
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| 231 | pt_p(nzt+1,:,:) = pt_p(nzt,:,:) |
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| 232 | !$acc end kernels |
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| 233 | ELSEIF ( ibc_pt_t == 2 ) THEN |
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| 234 | !$acc kernels present( dzu, pt_p ) |
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| 235 | pt_p(nzt+1,:,:) = pt_p(nzt,:,:) + bc_pt_t_val * dzu(nzt+1) |
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| 236 | !$acc end kernels |
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| 237 | ENDIF |
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[1] | 238 | |
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| 239 | ! |
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[1113] | 240 | !-- Boundary conditions for TKE |
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| 241 | !-- Generally Neumann conditions with de/dz=0 are assumed |
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| 242 | IF ( .NOT. constant_diffusion ) THEN |
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| 243 | !$acc kernels present( e_p, nzb_s_inner ) |
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[1257] | 244 | !$acc loop independent |
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[1113] | 245 | DO i = nxlg, nxrg |
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[1257] | 246 | !$acc loop independent |
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[1113] | 247 | DO j = nysg, nyng |
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| 248 | e_p(nzb_s_inner(j,i),j,i) = e_p(nzb_s_inner(j,i)+1,j,i) |
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[73] | 249 | ENDDO |
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[1113] | 250 | ENDDO |
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| 251 | e_p(nzt+1,:,:) = e_p(nzt,:,:) |
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| 252 | !$acc end kernels |
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| 253 | ENDIF |
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| 254 | |
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| 255 | ! |
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| 256 | !-- Boundary conditions for salinity |
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| 257 | IF ( ocean ) THEN |
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| 258 | ! |
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| 259 | !-- Bottom boundary: Neumann condition because salinity flux is always |
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| 260 | !-- given |
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| 261 | DO i = nxlg, nxrg |
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| 262 | DO j = nysg, nyng |
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| 263 | sa_p(nzb_s_inner(j,i),j,i) = sa_p(nzb_s_inner(j,i)+1,j,i) |
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[1] | 264 | ENDDO |
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[1113] | 265 | ENDDO |
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[1] | 266 | |
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| 267 | ! |
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[1113] | 268 | !-- Top boundary: Dirichlet or Neumann |
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| 269 | IF ( ibc_sa_t == 0 ) THEN |
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| 270 | sa_p(nzt+1,:,:) = sa(nzt+1,:,:) |
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| 271 | ELSEIF ( ibc_sa_t == 1 ) THEN |
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| 272 | sa_p(nzt+1,:,:) = sa_p(nzt,:,:) |
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[1] | 273 | ENDIF |
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| 274 | |
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[1113] | 275 | ENDIF |
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| 276 | |
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[1] | 277 | ! |
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[1113] | 278 | !-- Boundary conditions for total water content or scalar, |
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| 279 | !-- bottom and top boundary (see also temperature) |
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| 280 | IF ( humidity .OR. passive_scalar ) THEN |
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| 281 | ! |
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| 282 | !-- Surface conditions for constant_humidity_flux |
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| 283 | IF ( ibc_q_b == 0 ) THEN |
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[667] | 284 | DO i = nxlg, nxrg |
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| 285 | DO j = nysg, nyng |
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[1113] | 286 | q_p(nzb_s_inner(j,i),j,i) = q(nzb_s_inner(j,i),j,i) |
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[1] | 287 | ENDDO |
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| 288 | ENDDO |
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[1113] | 289 | ELSE |
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[667] | 290 | DO i = nxlg, nxrg |
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| 291 | DO j = nysg, nyng |
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[1113] | 292 | q_p(nzb_s_inner(j,i),j,i) = q_p(nzb_s_inner(j,i)+1,j,i) |
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[95] | 293 | ENDDO |
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| 294 | ENDDO |
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[1113] | 295 | ENDIF |
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[95] | 296 | ! |
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[1113] | 297 | !-- Top boundary |
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[1462] | 298 | IF ( ibc_q_t == 0 ) THEN |
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| 299 | q_p(nzt+1,:,:) = q(nzt+1,:,:) |
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| 300 | ELSEIF ( ibc_q_t == 1 ) THEN |
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| 301 | q_p(nzt+1,:,:) = q_p(nzt,:,:) + bc_q_t_val * dzu(nzt+1) |
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| 302 | ENDIF |
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[95] | 303 | |
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[1361] | 304 | IF ( cloud_physics .AND. icloud_scheme == 0 .AND. precipitation ) THEN |
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[1113] | 305 | ! |
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[1361] | 306 | !-- Surface conditions rain water (Dirichlet) |
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[1115] | 307 | DO i = nxlg, nxrg |
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| 308 | DO j = nysg, nyng |
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[1361] | 309 | qr_p(nzb_s_inner(j,i),j,i) = 0.0_wp |
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| 310 | nr_p(nzb_s_inner(j,i),j,i) = 0.0_wp |
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[73] | 311 | ENDDO |
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[1115] | 312 | ENDDO |
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[1] | 313 | ! |
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[1361] | 314 | !-- Top boundary condition for rain water (Dirichlet) |
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| 315 | qr_p(nzt+1,:,:) = 0.0_wp |
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| 316 | nr_p(nzt+1,:,:) = 0.0_wp |
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[1115] | 317 | |
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[1] | 318 | ENDIF |
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[1409] | 319 | ENDIF |
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[1] | 320 | ! |
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[1409] | 321 | !-- In case of inflow at the south boundary the boundary for v is at nys |
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| 322 | !-- and in case of inflow at the left boundary the boundary for u is at nxl. |
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| 323 | !-- Since in prognostic_equations (cache optimized version) these levels are |
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| 324 | !-- handled as a prognostic level, boundary values have to be restored here. |
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| 325 | !-- For the SGS-TKE, Neumann boundary conditions are used at the inflow. |
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| 326 | IF ( inflow_s ) THEN |
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| 327 | v_p(:,nys,:) = v_p(:,nys-1,:) |
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| 328 | IF ( .NOT. constant_diffusion ) e_p(:,nys-1,:) = e_p(:,nys,:) |
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| 329 | ELSEIF ( inflow_n ) THEN |
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| 330 | IF ( .NOT. constant_diffusion ) e_p(:,nyn+1,:) = e_p(:,nyn,:) |
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| 331 | ELSEIF ( inflow_l ) THEN |
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| 332 | u_p(:,:,nxl) = u_p(:,:,nxl-1) |
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| 333 | IF ( .NOT. constant_diffusion ) e_p(:,:,nxl-1) = e_p(:,:,nxl) |
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| 334 | ELSEIF ( inflow_r ) THEN |
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| 335 | IF ( .NOT. constant_diffusion ) e_p(:,:,nxr+1) = e_p(:,:,nxr) |
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| 336 | ENDIF |
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[1] | 337 | |
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| 338 | ! |
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[1409] | 339 | !-- Lateral boundary conditions for scalar quantities at the outflow |
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| 340 | IF ( outflow_s ) THEN |
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| 341 | pt_p(:,nys-1,:) = pt_p(:,nys,:) |
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| 342 | IF ( .NOT. constant_diffusion ) e_p(:,nys-1,:) = e_p(:,nys,:) |
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| 343 | IF ( humidity .OR. passive_scalar ) THEN |
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| 344 | q_p(:,nys-1,:) = q_p(:,nys,:) |
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| 345 | IF ( cloud_physics .AND. icloud_scheme == 0 .AND. & |
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| 346 | precipitation) THEN |
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| 347 | qr_p(:,nys-1,:) = qr_p(:,nys,:) |
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| 348 | nr_p(:,nys-1,:) = nr_p(:,nys,:) |
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[1053] | 349 | ENDIF |
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[1409] | 350 | ENDIF |
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| 351 | ELSEIF ( outflow_n ) THEN |
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| 352 | pt_p(:,nyn+1,:) = pt_p(:,nyn,:) |
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| 353 | IF ( .NOT. constant_diffusion ) e_p(:,nyn+1,:) = e_p(:,nyn,:) |
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| 354 | IF ( humidity .OR. passive_scalar ) THEN |
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| 355 | q_p(:,nyn+1,:) = q_p(:,nyn,:) |
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| 356 | IF ( cloud_physics .AND. icloud_scheme == 0 .AND. & |
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| 357 | precipitation ) THEN |
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| 358 | qr_p(:,nyn+1,:) = qr_p(:,nyn,:) |
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| 359 | nr_p(:,nyn+1,:) = nr_p(:,nyn,:) |
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[1053] | 360 | ENDIF |
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[1409] | 361 | ENDIF |
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| 362 | ELSEIF ( outflow_l ) THEN |
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| 363 | pt_p(:,:,nxl-1) = pt_p(:,:,nxl) |
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| 364 | IF ( .NOT. constant_diffusion ) e_p(:,:,nxl-1) = e_p(:,:,nxl) |
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| 365 | IF ( humidity .OR. passive_scalar ) THEN |
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| 366 | q_p(:,:,nxl-1) = q_p(:,:,nxl) |
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| 367 | IF ( cloud_physics .AND. icloud_scheme == 0 .AND. & |
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| 368 | precipitation ) THEN |
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| 369 | qr_p(:,:,nxl-1) = qr_p(:,:,nxl) |
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| 370 | nr_p(:,:,nxl-1) = nr_p(:,:,nxl) |
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[1053] | 371 | ENDIF |
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[1409] | 372 | ENDIF |
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| 373 | ELSEIF ( outflow_r ) THEN |
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| 374 | pt_p(:,:,nxr+1) = pt_p(:,:,nxr) |
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| 375 | IF ( .NOT. constant_diffusion ) e_p(:,:,nxr+1) = e_p(:,:,nxr) |
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| 376 | IF ( humidity .OR. passive_scalar ) THEN |
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| 377 | q_p(:,:,nxr+1) = q_p(:,:,nxr) |
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| 378 | IF ( cloud_physics .AND. icloud_scheme == 0 .AND. precipitation ) THEN |
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| 379 | qr_p(:,:,nxr+1) = qr_p(:,:,nxr) |
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| 380 | nr_p(:,:,nxr+1) = nr_p(:,:,nxr) |
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[1053] | 381 | ENDIF |
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[1] | 382 | ENDIF |
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| 383 | ENDIF |
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| 384 | |
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| 385 | ! |
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[1159] | 386 | !-- Radiation boundary conditions for the velocities at the respective outflow. |
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| 387 | !-- The phase velocity is either assumed to the maximum phase velocity that |
---|
| 388 | !-- ensures numerical stability (CFL-condition) or calculated after |
---|
| 389 | !-- Orlanski(1976) and averaged along the outflow boundary. |
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[106] | 390 | IF ( outflow_s ) THEN |
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[75] | 391 | |
---|
[1159] | 392 | IF ( use_cmax ) THEN |
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| 393 | u_p(:,-1,:) = u(:,0,:) |
---|
| 394 | v_p(:,0,:) = v(:,1,:) |
---|
| 395 | w_p(:,-1,:) = w(:,0,:) |
---|
| 396 | ELSEIF ( .NOT. use_cmax ) THEN |
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[75] | 397 | |
---|
[978] | 398 | c_max = dy / dt_3d |
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[75] | 399 | |
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[1353] | 400 | c_u_m_l = 0.0_wp |
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| 401 | c_v_m_l = 0.0_wp |
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| 402 | c_w_m_l = 0.0_wp |
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[978] | 403 | |
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[1353] | 404 | c_u_m = 0.0_wp |
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| 405 | c_v_m = 0.0_wp |
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| 406 | c_w_m = 0.0_wp |
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[978] | 407 | |
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[75] | 408 | ! |
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[996] | 409 | !-- Calculate the phase speeds for u, v, and w, first local and then |
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| 410 | !-- average along the outflow boundary. |
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| 411 | DO k = nzb+1, nzt+1 |
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| 412 | DO i = nxl, nxr |
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[75] | 413 | |
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[106] | 414 | denom = u_m_s(k,0,i) - u_m_s(k,1,i) |
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| 415 | |
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[1353] | 416 | IF ( denom /= 0.0_wp ) THEN |
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[996] | 417 | c_u(k,i) = -c_max * ( u(k,0,i) - u_m_s(k,0,i) ) / ( denom * tsc(2) ) |
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[1353] | 418 | IF ( c_u(k,i) < 0.0_wp ) THEN |
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| 419 | c_u(k,i) = 0.0_wp |
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[106] | 420 | ELSEIF ( c_u(k,i) > c_max ) THEN |
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| 421 | c_u(k,i) = c_max |
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| 422 | ENDIF |
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| 423 | ELSE |
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| 424 | c_u(k,i) = c_max |
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[75] | 425 | ENDIF |
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| 426 | |
---|
[106] | 427 | denom = v_m_s(k,1,i) - v_m_s(k,2,i) |
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| 428 | |
---|
[1353] | 429 | IF ( denom /= 0.0_wp ) THEN |
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[996] | 430 | c_v(k,i) = -c_max * ( v(k,1,i) - v_m_s(k,1,i) ) / ( denom * tsc(2) ) |
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[1353] | 431 | IF ( c_v(k,i) < 0.0_wp ) THEN |
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| 432 | c_v(k,i) = 0.0_wp |
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[106] | 433 | ELSEIF ( c_v(k,i) > c_max ) THEN |
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| 434 | c_v(k,i) = c_max |
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| 435 | ENDIF |
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| 436 | ELSE |
---|
| 437 | c_v(k,i) = c_max |
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[75] | 438 | ENDIF |
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| 439 | |
---|
[106] | 440 | denom = w_m_s(k,0,i) - w_m_s(k,1,i) |
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[75] | 441 | |
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[1353] | 442 | IF ( denom /= 0.0_wp ) THEN |
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[996] | 443 | c_w(k,i) = -c_max * ( w(k,0,i) - w_m_s(k,0,i) ) / ( denom * tsc(2) ) |
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[1353] | 444 | IF ( c_w(k,i) < 0.0_wp ) THEN |
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| 445 | c_w(k,i) = 0.0_wp |
---|
[106] | 446 | ELSEIF ( c_w(k,i) > c_max ) THEN |
---|
| 447 | c_w(k,i) = c_max |
---|
| 448 | ENDIF |
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| 449 | ELSE |
---|
| 450 | c_w(k,i) = c_max |
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[75] | 451 | ENDIF |
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[106] | 452 | |
---|
[978] | 453 | c_u_m_l(k) = c_u_m_l(k) + c_u(k,i) |
---|
| 454 | c_v_m_l(k) = c_v_m_l(k) + c_v(k,i) |
---|
| 455 | c_w_m_l(k) = c_w_m_l(k) + c_w(k,i) |
---|
[106] | 456 | |
---|
[978] | 457 | ENDDO |
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| 458 | ENDDO |
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[75] | 459 | |
---|
[978] | 460 | #if defined( __parallel ) |
---|
| 461 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dx, ierr ) |
---|
| 462 | CALL MPI_ALLREDUCE( c_u_m_l(nzb+1), c_u_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
| 463 | MPI_SUM, comm1dx, ierr ) |
---|
| 464 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dx, ierr ) |
---|
| 465 | CALL MPI_ALLREDUCE( c_v_m_l(nzb+1), c_v_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
| 466 | MPI_SUM, comm1dx, ierr ) |
---|
| 467 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dx, ierr ) |
---|
| 468 | CALL MPI_ALLREDUCE( c_w_m_l(nzb+1), c_w_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
| 469 | MPI_SUM, comm1dx, ierr ) |
---|
| 470 | #else |
---|
| 471 | c_u_m = c_u_m_l |
---|
| 472 | c_v_m = c_v_m_l |
---|
| 473 | c_w_m = c_w_m_l |
---|
| 474 | #endif |
---|
| 475 | |
---|
| 476 | c_u_m = c_u_m / (nx+1) |
---|
| 477 | c_v_m = c_v_m / (nx+1) |
---|
| 478 | c_w_m = c_w_m / (nx+1) |
---|
| 479 | |
---|
[75] | 480 | ! |
---|
[978] | 481 | !-- Save old timelevels for the next timestep |
---|
| 482 | IF ( intermediate_timestep_count == 1 ) THEN |
---|
| 483 | u_m_s(:,:,:) = u(:,0:1,:) |
---|
| 484 | v_m_s(:,:,:) = v(:,1:2,:) |
---|
| 485 | w_m_s(:,:,:) = w(:,0:1,:) |
---|
| 486 | ENDIF |
---|
| 487 | |
---|
| 488 | ! |
---|
| 489 | !-- Calculate the new velocities |
---|
[996] | 490 | DO k = nzb+1, nzt+1 |
---|
| 491 | DO i = nxlg, nxrg |
---|
[978] | 492 | u_p(k,-1,i) = u(k,-1,i) - dt_3d * tsc(2) * c_u_m(k) * & |
---|
[75] | 493 | ( u(k,-1,i) - u(k,0,i) ) * ddy |
---|
| 494 | |
---|
[978] | 495 | v_p(k,0,i) = v(k,0,i) - dt_3d * tsc(2) * c_v_m(k) * & |
---|
[106] | 496 | ( v(k,0,i) - v(k,1,i) ) * ddy |
---|
[75] | 497 | |
---|
[978] | 498 | w_p(k,-1,i) = w(k,-1,i) - dt_3d * tsc(2) * c_w_m(k) * & |
---|
[75] | 499 | ( w(k,-1,i) - w(k,0,i) ) * ddy |
---|
[978] | 500 | ENDDO |
---|
[75] | 501 | ENDDO |
---|
| 502 | |
---|
| 503 | ! |
---|
[978] | 504 | !-- Bottom boundary at the outflow |
---|
| 505 | IF ( ibc_uv_b == 0 ) THEN |
---|
[1353] | 506 | u_p(nzb,-1,:) = 0.0_wp |
---|
| 507 | v_p(nzb,0,:) = 0.0_wp |
---|
[978] | 508 | ELSE |
---|
| 509 | u_p(nzb,-1,:) = u_p(nzb+1,-1,:) |
---|
| 510 | v_p(nzb,0,:) = v_p(nzb+1,0,:) |
---|
| 511 | ENDIF |
---|
[1353] | 512 | w_p(nzb,-1,:) = 0.0_wp |
---|
[73] | 513 | |
---|
[75] | 514 | ! |
---|
[978] | 515 | !-- Top boundary at the outflow |
---|
| 516 | IF ( ibc_uv_t == 0 ) THEN |
---|
| 517 | u_p(nzt+1,-1,:) = u_init(nzt+1) |
---|
| 518 | v_p(nzt+1,0,:) = v_init(nzt+1) |
---|
| 519 | ELSE |
---|
| 520 | u_p(nzt+1,-1,:) = u(nzt,-1,:) |
---|
| 521 | v_p(nzt+1,0,:) = v(nzt,0,:) |
---|
| 522 | ENDIF |
---|
[1353] | 523 | w_p(nzt:nzt+1,-1,:) = 0.0_wp |
---|
[978] | 524 | |
---|
[75] | 525 | ENDIF |
---|
[73] | 526 | |
---|
[75] | 527 | ENDIF |
---|
[73] | 528 | |
---|
[106] | 529 | IF ( outflow_n ) THEN |
---|
[73] | 530 | |
---|
[1159] | 531 | IF ( use_cmax ) THEN |
---|
| 532 | u_p(:,ny+1,:) = u(:,ny,:) |
---|
| 533 | v_p(:,ny+1,:) = v(:,ny,:) |
---|
| 534 | w_p(:,ny+1,:) = w(:,ny,:) |
---|
| 535 | ELSEIF ( .NOT. use_cmax ) THEN |
---|
[75] | 536 | |
---|
[978] | 537 | c_max = dy / dt_3d |
---|
[75] | 538 | |
---|
[1353] | 539 | c_u_m_l = 0.0_wp |
---|
| 540 | c_v_m_l = 0.0_wp |
---|
| 541 | c_w_m_l = 0.0_wp |
---|
[978] | 542 | |
---|
[1353] | 543 | c_u_m = 0.0_wp |
---|
| 544 | c_v_m = 0.0_wp |
---|
| 545 | c_w_m = 0.0_wp |
---|
[978] | 546 | |
---|
[1] | 547 | ! |
---|
[996] | 548 | !-- Calculate the phase speeds for u, v, and w, first local and then |
---|
| 549 | !-- average along the outflow boundary. |
---|
| 550 | DO k = nzb+1, nzt+1 |
---|
| 551 | DO i = nxl, nxr |
---|
[73] | 552 | |
---|
[106] | 553 | denom = u_m_n(k,ny,i) - u_m_n(k,ny-1,i) |
---|
| 554 | |
---|
[1353] | 555 | IF ( denom /= 0.0_wp ) THEN |
---|
[996] | 556 | c_u(k,i) = -c_max * ( u(k,ny,i) - u_m_n(k,ny,i) ) / ( denom * tsc(2) ) |
---|
[1353] | 557 | IF ( c_u(k,i) < 0.0_wp ) THEN |
---|
| 558 | c_u(k,i) = 0.0_wp |
---|
[106] | 559 | ELSEIF ( c_u(k,i) > c_max ) THEN |
---|
| 560 | c_u(k,i) = c_max |
---|
| 561 | ENDIF |
---|
| 562 | ELSE |
---|
| 563 | c_u(k,i) = c_max |
---|
[73] | 564 | ENDIF |
---|
| 565 | |
---|
[106] | 566 | denom = v_m_n(k,ny,i) - v_m_n(k,ny-1,i) |
---|
[73] | 567 | |
---|
[1353] | 568 | IF ( denom /= 0.0_wp ) THEN |
---|
[996] | 569 | c_v(k,i) = -c_max * ( v(k,ny,i) - v_m_n(k,ny,i) ) / ( denom * tsc(2) ) |
---|
[1353] | 570 | IF ( c_v(k,i) < 0.0_wp ) THEN |
---|
| 571 | c_v(k,i) = 0.0_wp |
---|
[106] | 572 | ELSEIF ( c_v(k,i) > c_max ) THEN |
---|
| 573 | c_v(k,i) = c_max |
---|
| 574 | ENDIF |
---|
| 575 | ELSE |
---|
| 576 | c_v(k,i) = c_max |
---|
[73] | 577 | ENDIF |
---|
| 578 | |
---|
[106] | 579 | denom = w_m_n(k,ny,i) - w_m_n(k,ny-1,i) |
---|
[73] | 580 | |
---|
[1353] | 581 | IF ( denom /= 0.0_wp ) THEN |
---|
[996] | 582 | c_w(k,i) = -c_max * ( w(k,ny,i) - w_m_n(k,ny,i) ) / ( denom * tsc(2) ) |
---|
[1353] | 583 | IF ( c_w(k,i) < 0.0_wp ) THEN |
---|
| 584 | c_w(k,i) = 0.0_wp |
---|
[106] | 585 | ELSEIF ( c_w(k,i) > c_max ) THEN |
---|
| 586 | c_w(k,i) = c_max |
---|
| 587 | ENDIF |
---|
| 588 | ELSE |
---|
| 589 | c_w(k,i) = c_max |
---|
[73] | 590 | ENDIF |
---|
[106] | 591 | |
---|
[978] | 592 | c_u_m_l(k) = c_u_m_l(k) + c_u(k,i) |
---|
| 593 | c_v_m_l(k) = c_v_m_l(k) + c_v(k,i) |
---|
| 594 | c_w_m_l(k) = c_w_m_l(k) + c_w(k,i) |
---|
[106] | 595 | |
---|
[978] | 596 | ENDDO |
---|
| 597 | ENDDO |
---|
[73] | 598 | |
---|
[978] | 599 | #if defined( __parallel ) |
---|
| 600 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dx, ierr ) |
---|
| 601 | CALL MPI_ALLREDUCE( c_u_m_l(nzb+1), c_u_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
| 602 | MPI_SUM, comm1dx, ierr ) |
---|
| 603 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dx, ierr ) |
---|
| 604 | CALL MPI_ALLREDUCE( c_v_m_l(nzb+1), c_v_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
| 605 | MPI_SUM, comm1dx, ierr ) |
---|
| 606 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dx, ierr ) |
---|
| 607 | CALL MPI_ALLREDUCE( c_w_m_l(nzb+1), c_w_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
| 608 | MPI_SUM, comm1dx, ierr ) |
---|
| 609 | #else |
---|
| 610 | c_u_m = c_u_m_l |
---|
| 611 | c_v_m = c_v_m_l |
---|
| 612 | c_w_m = c_w_m_l |
---|
| 613 | #endif |
---|
| 614 | |
---|
| 615 | c_u_m = c_u_m / (nx+1) |
---|
| 616 | c_v_m = c_v_m / (nx+1) |
---|
| 617 | c_w_m = c_w_m / (nx+1) |
---|
| 618 | |
---|
[73] | 619 | ! |
---|
[978] | 620 | !-- Save old timelevels for the next timestep |
---|
| 621 | IF ( intermediate_timestep_count == 1 ) THEN |
---|
| 622 | u_m_n(:,:,:) = u(:,ny-1:ny,:) |
---|
| 623 | v_m_n(:,:,:) = v(:,ny-1:ny,:) |
---|
| 624 | w_m_n(:,:,:) = w(:,ny-1:ny,:) |
---|
| 625 | ENDIF |
---|
[73] | 626 | |
---|
[978] | 627 | ! |
---|
| 628 | !-- Calculate the new velocities |
---|
[996] | 629 | DO k = nzb+1, nzt+1 |
---|
| 630 | DO i = nxlg, nxrg |
---|
[978] | 631 | u_p(k,ny+1,i) = u(k,ny+1,i) - dt_3d * tsc(2) * c_u_m(k) * & |
---|
| 632 | ( u(k,ny+1,i) - u(k,ny,i) ) * ddy |
---|
[73] | 633 | |
---|
[978] | 634 | v_p(k,ny+1,i) = v(k,ny+1,i) - dt_3d * tsc(2) * c_v_m(k) * & |
---|
| 635 | ( v(k,ny+1,i) - v(k,ny,i) ) * ddy |
---|
[73] | 636 | |
---|
[978] | 637 | w_p(k,ny+1,i) = w(k,ny+1,i) - dt_3d * tsc(2) * c_w_m(k) * & |
---|
| 638 | ( w(k,ny+1,i) - w(k,ny,i) ) * ddy |
---|
| 639 | ENDDO |
---|
[1] | 640 | ENDDO |
---|
| 641 | |
---|
| 642 | ! |
---|
[978] | 643 | !-- Bottom boundary at the outflow |
---|
| 644 | IF ( ibc_uv_b == 0 ) THEN |
---|
[1353] | 645 | u_p(nzb,ny+1,:) = 0.0_wp |
---|
| 646 | v_p(nzb,ny+1,:) = 0.0_wp |
---|
[978] | 647 | ELSE |
---|
| 648 | u_p(nzb,ny+1,:) = u_p(nzb+1,ny+1,:) |
---|
| 649 | v_p(nzb,ny+1,:) = v_p(nzb+1,ny+1,:) |
---|
| 650 | ENDIF |
---|
[1353] | 651 | w_p(nzb,ny+1,:) = 0.0_wp |
---|
[73] | 652 | |
---|
| 653 | ! |
---|
[978] | 654 | !-- Top boundary at the outflow |
---|
| 655 | IF ( ibc_uv_t == 0 ) THEN |
---|
| 656 | u_p(nzt+1,ny+1,:) = u_init(nzt+1) |
---|
| 657 | v_p(nzt+1,ny+1,:) = v_init(nzt+1) |
---|
| 658 | ELSE |
---|
| 659 | u_p(nzt+1,ny+1,:) = u_p(nzt,nyn+1,:) |
---|
| 660 | v_p(nzt+1,ny+1,:) = v_p(nzt,nyn+1,:) |
---|
| 661 | ENDIF |
---|
[1353] | 662 | w_p(nzt:nzt+1,ny+1,:) = 0.0_wp |
---|
[978] | 663 | |
---|
[1] | 664 | ENDIF |
---|
| 665 | |
---|
[75] | 666 | ENDIF |
---|
| 667 | |
---|
[106] | 668 | IF ( outflow_l ) THEN |
---|
[75] | 669 | |
---|
[1159] | 670 | IF ( use_cmax ) THEN |
---|
| 671 | u_p(:,:,-1) = u(:,:,0) |
---|
| 672 | v_p(:,:,0) = v(:,:,1) |
---|
| 673 | w_p(:,:,-1) = w(:,:,0) |
---|
| 674 | ELSEIF ( .NOT. use_cmax ) THEN |
---|
[75] | 675 | |
---|
[978] | 676 | c_max = dx / dt_3d |
---|
[75] | 677 | |
---|
[1353] | 678 | c_u_m_l = 0.0_wp |
---|
| 679 | c_v_m_l = 0.0_wp |
---|
| 680 | c_w_m_l = 0.0_wp |
---|
[978] | 681 | |
---|
[1353] | 682 | c_u_m = 0.0_wp |
---|
| 683 | c_v_m = 0.0_wp |
---|
| 684 | c_w_m = 0.0_wp |
---|
[978] | 685 | |
---|
[1] | 686 | ! |
---|
[996] | 687 | !-- Calculate the phase speeds for u, v, and w, first local and then |
---|
| 688 | !-- average along the outflow boundary. |
---|
| 689 | DO k = nzb+1, nzt+1 |
---|
| 690 | DO j = nys, nyn |
---|
[75] | 691 | |
---|
[106] | 692 | denom = u_m_l(k,j,1) - u_m_l(k,j,2) |
---|
| 693 | |
---|
[1353] | 694 | IF ( denom /= 0.0_wp ) THEN |
---|
[996] | 695 | c_u(k,j) = -c_max * ( u(k,j,1) - u_m_l(k,j,1) ) / ( denom * tsc(2) ) |
---|
[1353] | 696 | IF ( c_u(k,j) < 0.0_wp ) THEN |
---|
| 697 | c_u(k,j) = 0.0_wp |
---|
[107] | 698 | ELSEIF ( c_u(k,j) > c_max ) THEN |
---|
| 699 | c_u(k,j) = c_max |
---|
[106] | 700 | ENDIF |
---|
| 701 | ELSE |
---|
[107] | 702 | c_u(k,j) = c_max |
---|
[75] | 703 | ENDIF |
---|
| 704 | |
---|
[106] | 705 | denom = v_m_l(k,j,0) - v_m_l(k,j,1) |
---|
[75] | 706 | |
---|
[1353] | 707 | IF ( denom /= 0.0_wp ) THEN |
---|
[996] | 708 | c_v(k,j) = -c_max * ( v(k,j,0) - v_m_l(k,j,0) ) / ( denom * tsc(2) ) |
---|
[1353] | 709 | IF ( c_v(k,j) < 0.0_wp ) THEN |
---|
| 710 | c_v(k,j) = 0.0_wp |
---|
[106] | 711 | ELSEIF ( c_v(k,j) > c_max ) THEN |
---|
| 712 | c_v(k,j) = c_max |
---|
| 713 | ENDIF |
---|
| 714 | ELSE |
---|
| 715 | c_v(k,j) = c_max |
---|
[75] | 716 | ENDIF |
---|
| 717 | |
---|
[106] | 718 | denom = w_m_l(k,j,0) - w_m_l(k,j,1) |
---|
[75] | 719 | |
---|
[1353] | 720 | IF ( denom /= 0.0_wp ) THEN |
---|
[996] | 721 | c_w(k,j) = -c_max * ( w(k,j,0) - w_m_l(k,j,0) ) / ( denom * tsc(2) ) |
---|
[1353] | 722 | IF ( c_w(k,j) < 0.0_wp ) THEN |
---|
| 723 | c_w(k,j) = 0.0_wp |
---|
[106] | 724 | ELSEIF ( c_w(k,j) > c_max ) THEN |
---|
| 725 | c_w(k,j) = c_max |
---|
| 726 | ENDIF |
---|
| 727 | ELSE |
---|
| 728 | c_w(k,j) = c_max |
---|
[75] | 729 | ENDIF |
---|
[106] | 730 | |
---|
[978] | 731 | c_u_m_l(k) = c_u_m_l(k) + c_u(k,j) |
---|
| 732 | c_v_m_l(k) = c_v_m_l(k) + c_v(k,j) |
---|
| 733 | c_w_m_l(k) = c_w_m_l(k) + c_w(k,j) |
---|
[106] | 734 | |
---|
[978] | 735 | ENDDO |
---|
| 736 | ENDDO |
---|
[75] | 737 | |
---|
[978] | 738 | #if defined( __parallel ) |
---|
| 739 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dy, ierr ) |
---|
| 740 | CALL MPI_ALLREDUCE( c_u_m_l(nzb+1), c_u_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
| 741 | MPI_SUM, comm1dy, ierr ) |
---|
| 742 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dy, ierr ) |
---|
| 743 | CALL MPI_ALLREDUCE( c_v_m_l(nzb+1), c_v_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
| 744 | MPI_SUM, comm1dy, ierr ) |
---|
| 745 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dy, ierr ) |
---|
| 746 | CALL MPI_ALLREDUCE( c_w_m_l(nzb+1), c_w_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
| 747 | MPI_SUM, comm1dy, ierr ) |
---|
| 748 | #else |
---|
| 749 | c_u_m = c_u_m_l |
---|
| 750 | c_v_m = c_v_m_l |
---|
| 751 | c_w_m = c_w_m_l |
---|
| 752 | #endif |
---|
| 753 | |
---|
| 754 | c_u_m = c_u_m / (ny+1) |
---|
| 755 | c_v_m = c_v_m / (ny+1) |
---|
| 756 | c_w_m = c_w_m / (ny+1) |
---|
| 757 | |
---|
[73] | 758 | ! |
---|
[978] | 759 | !-- Save old timelevels for the next timestep |
---|
| 760 | IF ( intermediate_timestep_count == 1 ) THEN |
---|
| 761 | u_m_l(:,:,:) = u(:,:,1:2) |
---|
| 762 | v_m_l(:,:,:) = v(:,:,0:1) |
---|
| 763 | w_m_l(:,:,:) = w(:,:,0:1) |
---|
| 764 | ENDIF |
---|
| 765 | |
---|
| 766 | ! |
---|
| 767 | !-- Calculate the new velocities |
---|
[996] | 768 | DO k = nzb+1, nzt+1 |
---|
[1113] | 769 | DO j = nysg, nyng |
---|
[978] | 770 | u_p(k,j,0) = u(k,j,0) - dt_3d * tsc(2) * c_u_m(k) * & |
---|
[106] | 771 | ( u(k,j,0) - u(k,j,1) ) * ddx |
---|
[75] | 772 | |
---|
[978] | 773 | v_p(k,j,-1) = v(k,j,-1) - dt_3d * tsc(2) * c_v_m(k) * & |
---|
[75] | 774 | ( v(k,j,-1) - v(k,j,0) ) * ddx |
---|
| 775 | |
---|
[978] | 776 | w_p(k,j,-1) = w(k,j,-1) - dt_3d * tsc(2) * c_w_m(k) * & |
---|
[75] | 777 | ( w(k,j,-1) - w(k,j,0) ) * ddx |
---|
[978] | 778 | ENDDO |
---|
[75] | 779 | ENDDO |
---|
| 780 | |
---|
| 781 | ! |
---|
[978] | 782 | !-- Bottom boundary at the outflow |
---|
| 783 | IF ( ibc_uv_b == 0 ) THEN |
---|
[1353] | 784 | u_p(nzb,:,0) = 0.0_wp |
---|
| 785 | v_p(nzb,:,-1) = 0.0_wp |
---|
[978] | 786 | ELSE |
---|
| 787 | u_p(nzb,:,0) = u_p(nzb+1,:,0) |
---|
| 788 | v_p(nzb,:,-1) = v_p(nzb+1,:,-1) |
---|
| 789 | ENDIF |
---|
[1353] | 790 | w_p(nzb,:,-1) = 0.0_wp |
---|
[1] | 791 | |
---|
[75] | 792 | ! |
---|
[978] | 793 | !-- Top boundary at the outflow |
---|
| 794 | IF ( ibc_uv_t == 0 ) THEN |
---|
| 795 | u_p(nzt+1,:,-1) = u_init(nzt+1) |
---|
| 796 | v_p(nzt+1,:,-1) = v_init(nzt+1) |
---|
| 797 | ELSE |
---|
| 798 | u_p(nzt+1,:,-1) = u_p(nzt,:,-1) |
---|
| 799 | v_p(nzt+1,:,-1) = v_p(nzt,:,-1) |
---|
| 800 | ENDIF |
---|
[1353] | 801 | w_p(nzt:nzt+1,:,-1) = 0.0_wp |
---|
[978] | 802 | |
---|
[75] | 803 | ENDIF |
---|
[73] | 804 | |
---|
[75] | 805 | ENDIF |
---|
[73] | 806 | |
---|
[106] | 807 | IF ( outflow_r ) THEN |
---|
[73] | 808 | |
---|
[1159] | 809 | IF ( use_cmax ) THEN |
---|
| 810 | u_p(:,:,nx+1) = u(:,:,nx) |
---|
| 811 | v_p(:,:,nx+1) = v(:,:,nx) |
---|
| 812 | w_p(:,:,nx+1) = w(:,:,nx) |
---|
| 813 | ELSEIF ( .NOT. use_cmax ) THEN |
---|
[75] | 814 | |
---|
[978] | 815 | c_max = dx / dt_3d |
---|
[75] | 816 | |
---|
[1353] | 817 | c_u_m_l = 0.0_wp |
---|
| 818 | c_v_m_l = 0.0_wp |
---|
| 819 | c_w_m_l = 0.0_wp |
---|
[978] | 820 | |
---|
[1353] | 821 | c_u_m = 0.0_wp |
---|
| 822 | c_v_m = 0.0_wp |
---|
| 823 | c_w_m = 0.0_wp |
---|
[978] | 824 | |
---|
[1] | 825 | ! |
---|
[996] | 826 | !-- Calculate the phase speeds for u, v, and w, first local and then |
---|
| 827 | !-- average along the outflow boundary. |
---|
| 828 | DO k = nzb+1, nzt+1 |
---|
| 829 | DO j = nys, nyn |
---|
[73] | 830 | |
---|
[106] | 831 | denom = u_m_r(k,j,nx) - u_m_r(k,j,nx-1) |
---|
| 832 | |
---|
[1353] | 833 | IF ( denom /= 0.0_wp ) THEN |
---|
[996] | 834 | c_u(k,j) = -c_max * ( u(k,j,nx) - u_m_r(k,j,nx) ) / ( denom * tsc(2) ) |
---|
[1353] | 835 | IF ( c_u(k,j) < 0.0_wp ) THEN |
---|
| 836 | c_u(k,j) = 0.0_wp |
---|
[106] | 837 | ELSEIF ( c_u(k,j) > c_max ) THEN |
---|
| 838 | c_u(k,j) = c_max |
---|
| 839 | ENDIF |
---|
| 840 | ELSE |
---|
| 841 | c_u(k,j) = c_max |
---|
[73] | 842 | ENDIF |
---|
| 843 | |
---|
[106] | 844 | denom = v_m_r(k,j,nx) - v_m_r(k,j,nx-1) |
---|
[73] | 845 | |
---|
[1353] | 846 | IF ( denom /= 0.0_wp ) THEN |
---|
[996] | 847 | c_v(k,j) = -c_max * ( v(k,j,nx) - v_m_r(k,j,nx) ) / ( denom * tsc(2) ) |
---|
[1353] | 848 | IF ( c_v(k,j) < 0.0_wp ) THEN |
---|
| 849 | c_v(k,j) = 0.0_wp |
---|
[106] | 850 | ELSEIF ( c_v(k,j) > c_max ) THEN |
---|
| 851 | c_v(k,j) = c_max |
---|
| 852 | ENDIF |
---|
| 853 | ELSE |
---|
| 854 | c_v(k,j) = c_max |
---|
[73] | 855 | ENDIF |
---|
| 856 | |
---|
[106] | 857 | denom = w_m_r(k,j,nx) - w_m_r(k,j,nx-1) |
---|
[73] | 858 | |
---|
[1353] | 859 | IF ( denom /= 0.0_wp ) THEN |
---|
[996] | 860 | c_w(k,j) = -c_max * ( w(k,j,nx) - w_m_r(k,j,nx) ) / ( denom * tsc(2) ) |
---|
[1353] | 861 | IF ( c_w(k,j) < 0.0_wp ) THEN |
---|
| 862 | c_w(k,j) = 0.0_wp |
---|
[106] | 863 | ELSEIF ( c_w(k,j) > c_max ) THEN |
---|
| 864 | c_w(k,j) = c_max |
---|
| 865 | ENDIF |
---|
| 866 | ELSE |
---|
| 867 | c_w(k,j) = c_max |
---|
[73] | 868 | ENDIF |
---|
[106] | 869 | |
---|
[978] | 870 | c_u_m_l(k) = c_u_m_l(k) + c_u(k,j) |
---|
| 871 | c_v_m_l(k) = c_v_m_l(k) + c_v(k,j) |
---|
| 872 | c_w_m_l(k) = c_w_m_l(k) + c_w(k,j) |
---|
[106] | 873 | |
---|
[978] | 874 | ENDDO |
---|
| 875 | ENDDO |
---|
[73] | 876 | |
---|
[978] | 877 | #if defined( __parallel ) |
---|
| 878 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dy, ierr ) |
---|
| 879 | CALL MPI_ALLREDUCE( c_u_m_l(nzb+1), c_u_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
| 880 | MPI_SUM, comm1dy, ierr ) |
---|
| 881 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dy, ierr ) |
---|
| 882 | CALL MPI_ALLREDUCE( c_v_m_l(nzb+1), c_v_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
| 883 | MPI_SUM, comm1dy, ierr ) |
---|
| 884 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dy, ierr ) |
---|
| 885 | CALL MPI_ALLREDUCE( c_w_m_l(nzb+1), c_w_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
| 886 | MPI_SUM, comm1dy, ierr ) |
---|
| 887 | #else |
---|
| 888 | c_u_m = c_u_m_l |
---|
| 889 | c_v_m = c_v_m_l |
---|
| 890 | c_w_m = c_w_m_l |
---|
| 891 | #endif |
---|
| 892 | |
---|
| 893 | c_u_m = c_u_m / (ny+1) |
---|
| 894 | c_v_m = c_v_m / (ny+1) |
---|
| 895 | c_w_m = c_w_m / (ny+1) |
---|
| 896 | |
---|
[73] | 897 | ! |
---|
[978] | 898 | !-- Save old timelevels for the next timestep |
---|
| 899 | IF ( intermediate_timestep_count == 1 ) THEN |
---|
| 900 | u_m_r(:,:,:) = u(:,:,nx-1:nx) |
---|
| 901 | v_m_r(:,:,:) = v(:,:,nx-1:nx) |
---|
| 902 | w_m_r(:,:,:) = w(:,:,nx-1:nx) |
---|
| 903 | ENDIF |
---|
[73] | 904 | |
---|
[978] | 905 | ! |
---|
| 906 | !-- Calculate the new velocities |
---|
[996] | 907 | DO k = nzb+1, nzt+1 |
---|
[1113] | 908 | DO j = nysg, nyng |
---|
[978] | 909 | u_p(k,j,nx+1) = u(k,j,nx+1) - dt_3d * tsc(2) * c_u_m(k) * & |
---|
| 910 | ( u(k,j,nx+1) - u(k,j,nx) ) * ddx |
---|
[73] | 911 | |
---|
[978] | 912 | v_p(k,j,nx+1) = v(k,j,nx+1) - dt_3d * tsc(2) * c_v_m(k) * & |
---|
| 913 | ( v(k,j,nx+1) - v(k,j,nx) ) * ddx |
---|
[73] | 914 | |
---|
[978] | 915 | w_p(k,j,nx+1) = w(k,j,nx+1) - dt_3d * tsc(2) * c_w_m(k) * & |
---|
| 916 | ( w(k,j,nx+1) - w(k,j,nx) ) * ddx |
---|
| 917 | ENDDO |
---|
[73] | 918 | ENDDO |
---|
| 919 | |
---|
| 920 | ! |
---|
[978] | 921 | !-- Bottom boundary at the outflow |
---|
| 922 | IF ( ibc_uv_b == 0 ) THEN |
---|
[1353] | 923 | u_p(nzb,:,nx+1) = 0.0_wp |
---|
| 924 | v_p(nzb,:,nx+1) = 0.0_wp |
---|
[978] | 925 | ELSE |
---|
| 926 | u_p(nzb,:,nx+1) = u_p(nzb+1,:,nx+1) |
---|
| 927 | v_p(nzb,:,nx+1) = v_p(nzb+1,:,nx+1) |
---|
| 928 | ENDIF |
---|
[1353] | 929 | w_p(nzb,:,nx+1) = 0.0_wp |
---|
[73] | 930 | |
---|
| 931 | ! |
---|
[978] | 932 | !-- Top boundary at the outflow |
---|
| 933 | IF ( ibc_uv_t == 0 ) THEN |
---|
| 934 | u_p(nzt+1,:,nx+1) = u_init(nzt+1) |
---|
| 935 | v_p(nzt+1,:,nx+1) = v_init(nzt+1) |
---|
| 936 | ELSE |
---|
| 937 | u_p(nzt+1,:,nx+1) = u_p(nzt,:,nx+1) |
---|
| 938 | v_p(nzt+1,:,nx+1) = v_p(nzt,:,nx+1) |
---|
| 939 | ENDIF |
---|
[1353] | 940 | w(nzt:nzt+1,:,nx+1) = 0.0_wp |
---|
[978] | 941 | |
---|
[1] | 942 | ENDIF |
---|
| 943 | |
---|
| 944 | ENDIF |
---|
| 945 | |
---|
| 946 | END SUBROUTINE boundary_conds |
---|