[1682] | 1 | !> @file boundary_conds.f90 |
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[2000] | 2 | !------------------------------------------------------------------------------! |
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[2696] | 3 | ! This file is part of the PALM model system. |
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[1036] | 4 | ! |
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[2000] | 5 | ! PALM is free software: you can redistribute it and/or modify it under the |
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| 6 | ! terms of the GNU General Public License as published by the Free Software |
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| 7 | ! Foundation, either version 3 of the License, or (at your option) any later |
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| 8 | ! version. |
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[1036] | 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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[2718] | 17 | ! Copyright 1997-2018 Leibniz Universitaet Hannover |
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[2000] | 18 | !------------------------------------------------------------------------------! |
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[1036] | 19 | ! |
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[484] | 20 | ! Current revisions: |
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[1] | 21 | ! ----------------- |
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[1933] | 22 | ! |
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[2233] | 23 | ! |
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[1321] | 24 | ! Former revisions: |
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| 25 | ! ----------------- |
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| 26 | ! $Id: boundary_conds.f90 2718 2018-01-02 08:49:38Z knoop $ |
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[2716] | 27 | ! Corrected "Former revisions" section |
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| 28 | ! |
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| 29 | ! 2696 2017-12-14 17:12:51Z kanani |
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| 30 | ! Change in file header (GPL part) |
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[2696] | 31 | ! Adjust boundary conditions for e and diss in case of TKE-e closure (TG) |
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| 32 | ! Implementation of chemistry module (FK) |
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| 33 | ! |
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| 34 | ! 2569 2017-10-20 11:54:42Z kanani |
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[2569] | 35 | ! Removed redundant code for ibc_s_b=1 and ibc_q_b=1 |
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| 36 | ! |
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| 37 | ! 2365 2017-08-21 14:59:59Z kanani |
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[2365] | 38 | ! Vertical grid nesting implemented: exclude setting vertical velocity to zero |
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| 39 | ! on fine grid (SadiqHuq) |
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| 40 | ! |
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| 41 | ! 2320 2017-07-21 12:47:43Z suehring |
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[2320] | 42 | ! Remove unused control parameter large_scale_forcing from only-list |
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| 43 | ! |
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| 44 | ! 2292 2017-06-20 09:51:42Z schwenkel |
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[2292] | 45 | ! Implementation of new microphysic scheme: cloud_scheme = 'morrison' |
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| 46 | ! includes two more prognostic equations for cloud drop concentration (nc) |
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| 47 | ! and cloud water content (qc). |
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| 48 | ! |
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| 49 | ! 2233 2017-05-30 18:08:54Z suehring |
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[1321] | 50 | ! |
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[2233] | 51 | ! 2232 2017-05-30 17:47:52Z suehring |
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| 52 | ! Set boundary conditions on topography top using flag method. |
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| 53 | ! |
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[2119] | 54 | ! 2118 2017-01-17 16:38:49Z raasch |
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| 55 | ! OpenACC directives removed |
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| 56 | ! |
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[2001] | 57 | ! 2000 2016-08-20 18:09:15Z knoop |
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| 58 | ! Forced header and separation lines into 80 columns |
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| 59 | ! |
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[1993] | 60 | ! 1992 2016-08-12 15:14:59Z suehring |
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| 61 | ! Adjustments for top boundary condition for passive scalar |
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| 62 | ! |
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[1961] | 63 | ! 1960 2016-07-12 16:34:24Z suehring |
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| 64 | ! Treat humidity and passive scalar separately |
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| 65 | ! |
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[1933] | 66 | ! 1823 2016-04-07 08:57:52Z hoffmann |
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| 67 | ! Initial version of purely vertical nesting introduced. |
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| 68 | ! |
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[1823] | 69 | ! 1822 2016-04-07 07:49:42Z hoffmann |
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| 70 | ! icloud_scheme removed. microphyisics_seifert added. |
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| 71 | ! |
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[1765] | 72 | ! 1764 2016-02-28 12:45:19Z raasch |
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| 73 | ! index bug for u_p at left outflow removed |
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| 74 | ! |
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[1763] | 75 | ! 1762 2016-02-25 12:31:13Z hellstea |
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| 76 | ! Introduction of nested domain feature |
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| 77 | ! |
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[1744] | 78 | ! 1742 2016-01-13 09:50:06Z raasch |
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| 79 | ! bugfix for outflow Neumann boundary conditions at bottom and top |
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| 80 | ! |
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[1718] | 81 | ! 1717 2015-11-11 15:09:47Z raasch |
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| 82 | ! Bugfix: index error in outflow conditions for left boundary |
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| 83 | ! |
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[1683] | 84 | ! 1682 2015-10-07 23:56:08Z knoop |
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| 85 | ! Code annotations made doxygen readable |
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| 86 | ! |
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[1717] | 87 | ! 1410 2014-05-23 12:16:18Z suehring |
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[1463] | 88 | ! Bugfix: set dirichlet boundary condition for passive_scalar at model domain |
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| 89 | ! top |
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| 90 | ! |
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[1410] | 91 | ! 1399 2014-05-07 11:16:25Z heinze |
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| 92 | ! Bugfix: set inflow boundary conditions also if no humidity or passive_scalar |
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| 93 | ! is used. |
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| 94 | ! |
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[1399] | 95 | ! 1398 2014-05-07 11:15:00Z heinze |
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| 96 | ! Dirichlet-condition at the top for u and v changed to u_init and v_init also |
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| 97 | ! for large_scale_forcing |
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| 98 | ! |
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[1381] | 99 | ! 1380 2014-04-28 12:40:45Z heinze |
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| 100 | ! Adjust Dirichlet-condition at the top for pt in case of nudging |
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| 101 | ! |
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[1362] | 102 | ! 1361 2014-04-16 15:17:48Z hoffmann |
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| 103 | ! Bottom and top boundary conditions of rain water content (qr) and |
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| 104 | ! rain drop concentration (nr) changed to Dirichlet |
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| 105 | ! |
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[1354] | 106 | ! 1353 2014-04-08 15:21:23Z heinze |
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| 107 | ! REAL constants provided with KIND-attribute |
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| 108 | ! |
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[1321] | 109 | ! 1320 2014-03-20 08:40:49Z raasch |
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[1320] | 110 | ! ONLY-attribute added to USE-statements, |
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| 111 | ! kind-parameters added to all INTEGER and REAL declaration statements, |
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| 112 | ! kinds are defined in new module kinds, |
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| 113 | ! revision history before 2012 removed, |
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| 114 | ! comment fields (!:) to be used for variable explanations added to |
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| 115 | ! all variable declaration statements |
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[1160] | 116 | ! |
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[1258] | 117 | ! 1257 2013-11-08 15:18:40Z raasch |
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| 118 | ! loop independent clauses added |
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| 119 | ! |
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[1242] | 120 | ! 1241 2013-10-30 11:36:58Z heinze |
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| 121 | ! Adjust ug and vg at each timestep in case of large_scale_forcing |
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| 122 | ! |
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[1160] | 123 | ! 1159 2013-05-21 11:58:22Z fricke |
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[1159] | 124 | ! Bugfix: Neumann boundary conditions for the velocity components at the |
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| 125 | ! outflow are in fact radiation boundary conditions using the maximum phase |
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| 126 | ! velocity that ensures numerical stability (CFL-condition). |
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| 127 | ! Hence, logical operator use_cmax is now used instead of bc_lr_dirneu/_neudir. |
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| 128 | ! Bugfix: In case of use_cmax at the outflow, u, v, w are replaced by |
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| 129 | ! u_p, v_p, w_p |
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[1116] | 130 | ! |
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| 131 | ! 1115 2013-03-26 18:16:16Z hoffmann |
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| 132 | ! boundary conditions of two-moment cloud scheme are restricted to Neumann- |
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| 133 | ! boundary-conditions |
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| 134 | ! |
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[1114] | 135 | ! 1113 2013-03-10 02:48:14Z raasch |
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| 136 | ! GPU-porting |
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| 137 | ! dummy argument "range" removed |
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| 138 | ! Bugfix: wrong index in loops of radiation boundary condition |
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[1113] | 139 | ! |
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[1054] | 140 | ! 1053 2012-11-13 17:11:03Z hoffmann |
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| 141 | ! boundary conditions for the two new prognostic equations (nr, qr) of the |
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| 142 | ! two-moment cloud scheme |
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| 143 | ! |
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[1037] | 144 | ! 1036 2012-10-22 13:43:42Z raasch |
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| 145 | ! code put under GPL (PALM 3.9) |
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| 146 | ! |
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[997] | 147 | ! 996 2012-09-07 10:41:47Z raasch |
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| 148 | ! little reformatting |
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| 149 | ! |
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[979] | 150 | ! 978 2012-08-09 08:28:32Z fricke |
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| 151 | ! Neumann boudnary conditions are added at the inflow boundary for the SGS-TKE. |
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| 152 | ! Outflow boundary conditions for the velocity components can be set to Neumann |
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| 153 | ! conditions or to radiation conditions with a horizontal averaged phase |
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| 154 | ! velocity. |
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| 155 | ! |
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[876] | 156 | ! 875 2012-04-02 15:35:15Z gryschka |
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| 157 | ! Bugfix in case of dirichlet inflow bc at the right or north boundary |
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| 158 | ! |
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[1] | 159 | ! Revision 1.1 1997/09/12 06:21:34 raasch |
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| 160 | ! Initial revision |
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| 161 | ! |
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| 162 | ! |
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| 163 | ! Description: |
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| 164 | ! ------------ |
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[1682] | 165 | !> Boundary conditions for the prognostic quantities. |
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| 166 | !> One additional bottom boundary condition is applied for the TKE (=(u*)**2) |
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| 167 | !> in prandtl_fluxes. The cyclic lateral boundary conditions are implicitly |
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| 168 | !> handled in routine exchange_horiz. Pressure boundary conditions are |
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| 169 | !> explicitly set in routines pres, poisfft, poismg and sor. |
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[1] | 170 | !------------------------------------------------------------------------------! |
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[1682] | 171 | SUBROUTINE boundary_conds |
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| 172 | |
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[1] | 173 | |
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[1320] | 174 | USE arrays_3d, & |
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| 175 | 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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[2696] | 176 | diss_p, dzu, e_p, nc_p, nr_p, pt, pt_p, q, q_p, qc_p, qr_p, s, & |
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| 177 | s_p, sa, sa_p, u, ug, u_init, u_m_l, u_m_n, u_m_r, u_m_s, u_p, & |
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[1320] | 178 | v, vg, v_init, v_m_l, v_m_n, v_m_r, v_m_s, v_p, & |
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[1960] | 179 | w, w_p, w_m_l, w_m_n, w_m_r, w_m_s, pt_init |
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[2696] | 180 | |
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| 181 | #if defined( __chem ) |
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| 182 | USE chemistry_model_mod, & |
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| 183 | ONLY: chem_boundary_conds |
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| 184 | #endif |
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| 185 | |
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[1320] | 186 | USE control_parameters, & |
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[2696] | 187 | ONLY: air_chemistry, bc_pt_t_val, bc_q_t_val, bc_s_t_val, & |
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| 188 | constant_diffusion, cloud_physics, coupling_mode, dt_3d, & |
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| 189 | force_bound_l, force_bound_s, forcing, humidity, & |
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[1960] | 190 | ibc_pt_b, ibc_pt_t, ibc_q_b, ibc_q_t, ibc_s_b, ibc_s_t, & |
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| 191 | ibc_sa_t, ibc_uv_b, ibc_uv_t, inflow_l, inflow_n, inflow_r, & |
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[2320] | 192 | inflow_s, intermediate_timestep_count, & |
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[2292] | 193 | microphysics_morrison, microphysics_seifert, nest_domain, & |
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| 194 | nest_bound_l, nest_bound_s, nudging, ocean, outflow_l, & |
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[2696] | 195 | outflow_n, outflow_r, outflow_s, passive_scalar, rans_tke_e, & |
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| 196 | tsc, use_cmax |
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[1320] | 197 | |
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| 198 | USE grid_variables, & |
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| 199 | ONLY: ddx, ddy, dx, dy |
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| 200 | |
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| 201 | USE indices, & |
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| 202 | ONLY: nx, nxl, nxlg, nxr, nxrg, ny, nyn, nyng, nys, nysg, & |
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[2232] | 203 | nzb, nzt, wall_flags_0 |
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[1320] | 204 | |
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| 205 | USE kinds |
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| 206 | |
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[1] | 207 | USE pegrid |
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| 208 | |
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[1933] | 209 | USE pmc_interface, & |
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| 210 | ONLY : nesting_mode |
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[1320] | 211 | |
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[2232] | 212 | USE surface_mod, & |
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| 213 | ONLY : bc_h |
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[1933] | 214 | |
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[1] | 215 | IMPLICIT NONE |
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| 216 | |
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[2232] | 217 | INTEGER(iwp) :: i !< grid index x direction |
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| 218 | INTEGER(iwp) :: j !< grid index y direction |
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| 219 | INTEGER(iwp) :: k !< grid index z direction |
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| 220 | INTEGER(iwp) :: kb !< variable to set respective boundary value, depends on facing. |
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| 221 | INTEGER(iwp) :: l !< running index boundary type, for up- and downward-facing walls |
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| 222 | INTEGER(iwp) :: m !< running index surface elements |
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[1] | 223 | |
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[1682] | 224 | REAL(wp) :: c_max !< |
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| 225 | REAL(wp) :: denom !< |
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[1] | 226 | |
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[73] | 227 | |
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[1] | 228 | ! |
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[1113] | 229 | !-- Bottom boundary |
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| 230 | IF ( ibc_uv_b == 1 ) THEN |
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| 231 | u_p(nzb,:,:) = u_p(nzb+1,:,:) |
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| 232 | v_p(nzb,:,:) = v_p(nzb+1,:,:) |
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| 233 | ENDIF |
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[2232] | 234 | ! |
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| 235 | !-- Set zero vertical velocity at topography top (l=0), or bottom (l=1) in case |
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| 236 | !-- of downward-facing surfaces. |
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| 237 | DO l = 0, 1 |
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| 238 | ! |
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| 239 | !-- Set kb, for upward-facing surfaces value at topography top (k-1) is set, |
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| 240 | !-- for downward-facing surfaces at topography bottom (k+1). |
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| 241 | kb = MERGE( -1, 1, l == 0 ) |
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| 242 | !$OMP PARALLEL DO PRIVATE( i, j, k ) |
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| 243 | DO m = 1, bc_h(l)%ns |
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| 244 | i = bc_h(l)%i(m) |
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| 245 | j = bc_h(l)%j(m) |
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| 246 | k = bc_h(l)%k(m) |
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| 247 | w_p(k+kb,j,i) = 0.0_wp |
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[1113] | 248 | ENDDO |
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| 249 | ENDDO |
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| 250 | |
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| 251 | ! |
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[1762] | 252 | !-- Top boundary. A nested domain ( ibc_uv_t = 3 ) does not require settings. |
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[1113] | 253 | IF ( ibc_uv_t == 0 ) THEN |
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| 254 | u_p(nzt+1,:,:) = u_init(nzt+1) |
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| 255 | v_p(nzt+1,:,:) = v_init(nzt+1) |
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[1762] | 256 | ELSEIF ( ibc_uv_t == 1 ) THEN |
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[1113] | 257 | u_p(nzt+1,:,:) = u_p(nzt,:,:) |
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| 258 | v_p(nzt+1,:,:) = v_p(nzt,:,:) |
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| 259 | ENDIF |
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| 260 | |
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[2365] | 261 | ! |
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| 262 | !-- Vertical nesting: Vertical velocity not zero at the top of the fine grid |
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| 263 | IF ( .NOT. nest_domain .AND. & |
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| 264 | TRIM(coupling_mode) /= 'vnested_fine' ) THEN |
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| 265 | w_p(nzt:nzt+1,:,:) = 0.0_wp !< nzt is not a prognostic level (but cf. pres) |
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[1762] | 266 | ENDIF |
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| 267 | |
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[1113] | 268 | ! |
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[2232] | 269 | !-- Temperature at bottom and top boundary. |
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[1113] | 270 | !-- In case of coupled runs (ibc_pt_b = 2) the temperature is given by |
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| 271 | !-- the sea surface temperature of the coupled ocean model. |
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[2232] | 272 | !-- Dirichlet |
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[1113] | 273 | IF ( ibc_pt_b == 0 ) THEN |
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[2232] | 274 | DO l = 0, 1 |
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| 275 | ! |
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| 276 | !-- Set kb, for upward-facing surfaces value at topography top (k-1) is set, |
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| 277 | !-- for downward-facing surfaces at topography bottom (k+1). |
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| 278 | kb = MERGE( -1, 1, l == 0 ) |
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| 279 | !$OMP PARALLEL DO PRIVATE( i, j, k ) |
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| 280 | DO m = 1, bc_h(l)%ns |
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| 281 | i = bc_h(l)%i(m) |
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| 282 | j = bc_h(l)%j(m) |
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| 283 | k = bc_h(l)%k(m) |
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| 284 | pt_p(k+kb,j,i) = pt(k+kb,j,i) |
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[1] | 285 | ENDDO |
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| 286 | ENDDO |
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[2232] | 287 | ! |
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| 288 | !-- Neumann, zero-gradient |
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[1113] | 289 | ELSEIF ( ibc_pt_b == 1 ) THEN |
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[2232] | 290 | DO l = 0, 1 |
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| 291 | ! |
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| 292 | !-- Set kb, for upward-facing surfaces value at topography top (k-1) is set, |
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| 293 | !-- for downward-facing surfaces at topography bottom (k+1). |
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| 294 | kb = MERGE( -1, 1, l == 0 ) |
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| 295 | !$OMP PARALLEL DO PRIVATE( i, j, k ) |
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| 296 | DO m = 1, bc_h(l)%ns |
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| 297 | i = bc_h(l)%i(m) |
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| 298 | j = bc_h(l)%j(m) |
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| 299 | k = bc_h(l)%k(m) |
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| 300 | pt_p(k+kb,j,i) = pt_p(k,j,i) |
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[1113] | 301 | ENDDO |
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| 302 | ENDDO |
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| 303 | ENDIF |
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[1] | 304 | |
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| 305 | ! |
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[1113] | 306 | !-- Temperature at top boundary |
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| 307 | IF ( ibc_pt_t == 0 ) THEN |
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| 308 | pt_p(nzt+1,:,:) = pt(nzt+1,:,:) |
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[1380] | 309 | ! |
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| 310 | !-- In case of nudging adjust top boundary to pt which is |
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| 311 | !-- read in from NUDGING-DATA |
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| 312 | IF ( nudging ) THEN |
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| 313 | pt_p(nzt+1,:,:) = pt_init(nzt+1) |
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| 314 | ENDIF |
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[1113] | 315 | ELSEIF ( ibc_pt_t == 1 ) THEN |
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| 316 | pt_p(nzt+1,:,:) = pt_p(nzt,:,:) |
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| 317 | ELSEIF ( ibc_pt_t == 2 ) THEN |
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[1992] | 318 | pt_p(nzt+1,:,:) = pt_p(nzt,:,:) + bc_pt_t_val * dzu(nzt+1) |
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[1113] | 319 | ENDIF |
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[1] | 320 | |
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| 321 | ! |
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[1113] | 322 | !-- Boundary conditions for TKE |
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| 323 | !-- Generally Neumann conditions with de/dz=0 are assumed |
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| 324 | IF ( .NOT. constant_diffusion ) THEN |
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[2232] | 325 | |
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[2696] | 326 | IF ( .NOT. rans_tke_e ) THEN |
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| 327 | DO l = 0, 1 |
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[2232] | 328 | ! |
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[2696] | 329 | !-- Set kb, for upward-facing surfaces value at topography top (k-1) is set, |
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| 330 | !-- for downward-facing surfaces at topography bottom (k+1). |
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| 331 | kb = MERGE( -1, 1, l == 0 ) |
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| 332 | !$OMP PARALLEL DO PRIVATE( i, j, k ) |
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| 333 | DO m = 1, bc_h(l)%ns |
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| 334 | i = bc_h(l)%i(m) |
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| 335 | j = bc_h(l)%j(m) |
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| 336 | k = bc_h(l)%k(m) |
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| 337 | e_p(k+kb,j,i) = e_p(k,j,i) |
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| 338 | ENDDO |
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[73] | 339 | ENDDO |
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[2696] | 340 | ENDIF |
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[2232] | 341 | |
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[1762] | 342 | IF ( .NOT. nest_domain ) THEN |
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| 343 | e_p(nzt+1,:,:) = e_p(nzt,:,:) |
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| 344 | ENDIF |
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[1113] | 345 | ENDIF |
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| 346 | |
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| 347 | ! |
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[2696] | 348 | !-- Boundary conditions for TKE dissipation rate |
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| 349 | IF ( rans_tke_e .AND. .NOT. nest_domain ) THEN |
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| 350 | diss_p(nzt+1,:,:) = diss_p(nzt,:,:) |
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| 351 | ENDIF |
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| 352 | |
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| 353 | ! |
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[1113] | 354 | !-- Boundary conditions for salinity |
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| 355 | IF ( ocean ) THEN |
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| 356 | ! |
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| 357 | !-- Bottom boundary: Neumann condition because salinity flux is always |
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[2232] | 358 | !-- given. |
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| 359 | DO l = 0, 1 |
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| 360 | ! |
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| 361 | !-- Set kb, for upward-facing surfaces value at topography top (k-1) is set, |
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| 362 | !-- for downward-facing surfaces at topography bottom (k+1). |
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| 363 | kb = MERGE( -1, 1, l == 0 ) |
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| 364 | !$OMP PARALLEL DO PRIVATE( i, j, k ) |
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| 365 | DO m = 1, bc_h(l)%ns |
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| 366 | i = bc_h(l)%i(m) |
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| 367 | j = bc_h(l)%j(m) |
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| 368 | k = bc_h(l)%k(m) |
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| 369 | sa_p(k+kb,j,i) = sa_p(k,j,i) |
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[1] | 370 | ENDDO |
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[1113] | 371 | ENDDO |
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[1] | 372 | ! |
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[1113] | 373 | !-- Top boundary: Dirichlet or Neumann |
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| 374 | IF ( ibc_sa_t == 0 ) THEN |
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| 375 | sa_p(nzt+1,:,:) = sa(nzt+1,:,:) |
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| 376 | ELSEIF ( ibc_sa_t == 1 ) THEN |
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| 377 | sa_p(nzt+1,:,:) = sa_p(nzt,:,:) |
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[1] | 378 | ENDIF |
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| 379 | |
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[1113] | 380 | ENDIF |
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| 381 | |
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[1] | 382 | ! |
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[1960] | 383 | !-- Boundary conditions for total water content, |
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[1113] | 384 | !-- bottom and top boundary (see also temperature) |
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[1960] | 385 | IF ( humidity ) THEN |
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[1113] | 386 | ! |
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| 387 | !-- Surface conditions for constant_humidity_flux |
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[2232] | 388 | !-- Run loop over all non-natural and natural walls. Note, in wall-datatype |
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| 389 | !-- the k coordinate belongs to the atmospheric grid point, therefore, set |
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| 390 | !-- q_p at k-1 |
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[1113] | 391 | IF ( ibc_q_b == 0 ) THEN |
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[2232] | 392 | |
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| 393 | DO l = 0, 1 |
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| 394 | ! |
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| 395 | !-- Set kb, for upward-facing surfaces value at topography top (k-1) is set, |
---|
| 396 | !-- for downward-facing surfaces at topography bottom (k+1). |
---|
| 397 | kb = MERGE( -1, 1, l == 0 ) |
---|
| 398 | !$OMP PARALLEL DO PRIVATE( i, j, k ) |
---|
| 399 | DO m = 1, bc_h(l)%ns |
---|
| 400 | i = bc_h(l)%i(m) |
---|
| 401 | j = bc_h(l)%j(m) |
---|
| 402 | k = bc_h(l)%k(m) |
---|
| 403 | q_p(k+kb,j,i) = q(k+kb,j,i) |
---|
[1] | 404 | ENDDO |
---|
| 405 | ENDDO |
---|
[2232] | 406 | |
---|
[1113] | 407 | ELSE |
---|
[2232] | 408 | |
---|
| 409 | DO l = 0, 1 |
---|
| 410 | ! |
---|
| 411 | !-- Set kb, for upward-facing surfaces value at topography top (k-1) is set, |
---|
| 412 | !-- for downward-facing surfaces at topography bottom (k+1). |
---|
| 413 | kb = MERGE( -1, 1, l == 0 ) |
---|
| 414 | !$OMP PARALLEL DO PRIVATE( i, j, k ) |
---|
| 415 | DO m = 1, bc_h(l)%ns |
---|
| 416 | i = bc_h(l)%i(m) |
---|
| 417 | j = bc_h(l)%j(m) |
---|
| 418 | k = bc_h(l)%k(m) |
---|
| 419 | q_p(k+kb,j,i) = q_p(k,j,i) |
---|
[95] | 420 | ENDDO |
---|
| 421 | ENDDO |
---|
[1113] | 422 | ENDIF |
---|
[95] | 423 | ! |
---|
[1113] | 424 | !-- Top boundary |
---|
[1462] | 425 | IF ( ibc_q_t == 0 ) THEN |
---|
| 426 | q_p(nzt+1,:,:) = q(nzt+1,:,:) |
---|
| 427 | ELSEIF ( ibc_q_t == 1 ) THEN |
---|
[1992] | 428 | q_p(nzt+1,:,:) = q_p(nzt,:,:) + bc_q_t_val * dzu(nzt+1) |
---|
[1462] | 429 | ENDIF |
---|
[95] | 430 | |
---|
[2292] | 431 | IF ( cloud_physics .AND. microphysics_morrison ) THEN |
---|
| 432 | ! |
---|
| 433 | !-- Surface conditions cloud water (Dirichlet) |
---|
| 434 | !-- Run loop over all non-natural and natural walls. Note, in wall-datatype |
---|
| 435 | !-- the k coordinate belongs to the atmospheric grid point, therefore, set |
---|
| 436 | !-- qr_p and nr_p at k-1 |
---|
| 437 | !$OMP PARALLEL DO PRIVATE( i, j, k ) |
---|
| 438 | DO m = 1, bc_h(0)%ns |
---|
| 439 | i = bc_h(0)%i(m) |
---|
| 440 | j = bc_h(0)%j(m) |
---|
| 441 | k = bc_h(0)%k(m) |
---|
| 442 | qc_p(k-1,j,i) = 0.0_wp |
---|
| 443 | nc_p(k-1,j,i) = 0.0_wp |
---|
| 444 | ENDDO |
---|
| 445 | ! |
---|
| 446 | !-- Top boundary condition for cloud water (Dirichlet) |
---|
| 447 | qc_p(nzt+1,:,:) = 0.0_wp |
---|
| 448 | nc_p(nzt+1,:,:) = 0.0_wp |
---|
| 449 | |
---|
| 450 | ENDIF |
---|
| 451 | |
---|
[1822] | 452 | IF ( cloud_physics .AND. microphysics_seifert ) THEN |
---|
[1113] | 453 | ! |
---|
[1361] | 454 | !-- Surface conditions rain water (Dirichlet) |
---|
[2232] | 455 | !-- Run loop over all non-natural and natural walls. Note, in wall-datatype |
---|
| 456 | !-- the k coordinate belongs to the atmospheric grid point, therefore, set |
---|
| 457 | !-- qr_p and nr_p at k-1 |
---|
| 458 | !$OMP PARALLEL DO PRIVATE( i, j, k ) |
---|
| 459 | DO m = 1, bc_h(0)%ns |
---|
| 460 | i = bc_h(0)%i(m) |
---|
| 461 | j = bc_h(0)%j(m) |
---|
| 462 | k = bc_h(0)%k(m) |
---|
| 463 | qr_p(k-1,j,i) = 0.0_wp |
---|
| 464 | nr_p(k-1,j,i) = 0.0_wp |
---|
[1115] | 465 | ENDDO |
---|
[1] | 466 | ! |
---|
[1361] | 467 | !-- Top boundary condition for rain water (Dirichlet) |
---|
| 468 | qr_p(nzt+1,:,:) = 0.0_wp |
---|
| 469 | nr_p(nzt+1,:,:) = 0.0_wp |
---|
[1115] | 470 | |
---|
[1] | 471 | ENDIF |
---|
[1409] | 472 | ENDIF |
---|
[1] | 473 | ! |
---|
[1960] | 474 | !-- Boundary conditions for scalar, |
---|
| 475 | !-- bottom and top boundary (see also temperature) |
---|
| 476 | IF ( passive_scalar ) THEN |
---|
| 477 | ! |
---|
| 478 | !-- Surface conditions for constant_humidity_flux |
---|
[2232] | 479 | !-- Run loop over all non-natural and natural walls. Note, in wall-datatype |
---|
| 480 | !-- the k coordinate belongs to the atmospheric grid point, therefore, set |
---|
| 481 | !-- s_p at k-1 |
---|
[1960] | 482 | IF ( ibc_s_b == 0 ) THEN |
---|
[2232] | 483 | |
---|
| 484 | DO l = 0, 1 |
---|
| 485 | ! |
---|
| 486 | !-- Set kb, for upward-facing surfaces value at topography top (k-1) is set, |
---|
| 487 | !-- for downward-facing surfaces at topography bottom (k+1). |
---|
| 488 | kb = MERGE( -1, 1, l == 0 ) |
---|
| 489 | !$OMP PARALLEL DO PRIVATE( i, j, k ) |
---|
| 490 | DO m = 1, bc_h(l)%ns |
---|
| 491 | i = bc_h(l)%i(m) |
---|
| 492 | j = bc_h(l)%j(m) |
---|
| 493 | k = bc_h(l)%k(m) |
---|
| 494 | s_p(k+kb,j,i) = s(k+kb,j,i) |
---|
[1960] | 495 | ENDDO |
---|
| 496 | ENDDO |
---|
[2232] | 497 | |
---|
[1960] | 498 | ELSE |
---|
[2232] | 499 | |
---|
| 500 | DO l = 0, 1 |
---|
| 501 | ! |
---|
| 502 | !-- Set kb, for upward-facing surfaces value at topography top (k-1) is set, |
---|
| 503 | !-- for downward-facing surfaces at topography bottom (k+1). |
---|
| 504 | kb = MERGE( -1, 1, l == 0 ) |
---|
| 505 | !$OMP PARALLEL DO PRIVATE( i, j, k ) |
---|
| 506 | DO m = 1, bc_h(l)%ns |
---|
| 507 | i = bc_h(l)%i(m) |
---|
| 508 | j = bc_h(l)%j(m) |
---|
| 509 | k = bc_h(l)%k(m) |
---|
| 510 | s_p(k+kb,j,i) = s_p(k,j,i) |
---|
[1960] | 511 | ENDDO |
---|
| 512 | ENDDO |
---|
| 513 | ENDIF |
---|
| 514 | ! |
---|
[1992] | 515 | !-- Top boundary condition |
---|
| 516 | IF ( ibc_s_t == 0 ) THEN |
---|
[1960] | 517 | s_p(nzt+1,:,:) = s(nzt+1,:,:) |
---|
[1992] | 518 | ELSEIF ( ibc_s_t == 1 ) THEN |
---|
| 519 | s_p(nzt+1,:,:) = s_p(nzt,:,:) |
---|
| 520 | ELSEIF ( ibc_s_t == 2 ) THEN |
---|
| 521 | s_p(nzt+1,:,:) = s_p(nzt,:,:) + bc_s_t_val * dzu(nzt+1) |
---|
[1960] | 522 | ENDIF |
---|
| 523 | |
---|
| 524 | ENDIF |
---|
| 525 | ! |
---|
[2696] | 526 | !-- Top/bottom boundary conditions for chemical species |
---|
| 527 | #if defined( __chem ) |
---|
| 528 | IF ( air_chemistry ) CALL chem_boundary_conds( 'set_bc_bottomtop' ) |
---|
| 529 | #endif |
---|
| 530 | ! |
---|
[1762] | 531 | !-- In case of inflow or nest boundary at the south boundary the boundary for v |
---|
| 532 | !-- is at nys and in case of inflow or nest boundary at the left boundary the |
---|
| 533 | !-- boundary for u is at nxl. Since in prognostic_equations (cache optimized |
---|
| 534 | !-- version) these levels are handled as a prognostic level, boundary values |
---|
| 535 | !-- have to be restored here. |
---|
[1409] | 536 | !-- For the SGS-TKE, Neumann boundary conditions are used at the inflow. |
---|
| 537 | IF ( inflow_s ) THEN |
---|
| 538 | v_p(:,nys,:) = v_p(:,nys-1,:) |
---|
| 539 | IF ( .NOT. constant_diffusion ) e_p(:,nys-1,:) = e_p(:,nys,:) |
---|
| 540 | ELSEIF ( inflow_n ) THEN |
---|
| 541 | IF ( .NOT. constant_diffusion ) e_p(:,nyn+1,:) = e_p(:,nyn,:) |
---|
| 542 | ELSEIF ( inflow_l ) THEN |
---|
| 543 | u_p(:,:,nxl) = u_p(:,:,nxl-1) |
---|
| 544 | IF ( .NOT. constant_diffusion ) e_p(:,:,nxl-1) = e_p(:,:,nxl) |
---|
| 545 | ELSEIF ( inflow_r ) THEN |
---|
| 546 | IF ( .NOT. constant_diffusion ) e_p(:,:,nxr+1) = e_p(:,:,nxr) |
---|
| 547 | ENDIF |
---|
[1] | 548 | |
---|
| 549 | ! |
---|
[1762] | 550 | !-- The same restoration for u at i=nxl and v at j=nys as above must be made |
---|
[1933] | 551 | !-- in case of nest boundaries. This must not be done in case of vertical nesting |
---|
| 552 | !-- mode as in that case the lateral boundaries are actually cyclic. |
---|
[2696] | 553 | IF ( nesting_mode /= 'vertical' .OR. forcing ) THEN |
---|
| 554 | IF ( nest_bound_s .OR. force_bound_s ) THEN |
---|
[1933] | 555 | v_p(:,nys,:) = v_p(:,nys-1,:) |
---|
| 556 | ENDIF |
---|
[2696] | 557 | IF ( nest_bound_l .OR. force_bound_l ) THEN |
---|
[1933] | 558 | u_p(:,:,nxl) = u_p(:,:,nxl-1) |
---|
| 559 | ENDIF |
---|
[1762] | 560 | ENDIF |
---|
| 561 | |
---|
| 562 | ! |
---|
[1409] | 563 | !-- Lateral boundary conditions for scalar quantities at the outflow |
---|
| 564 | IF ( outflow_s ) THEN |
---|
| 565 | pt_p(:,nys-1,:) = pt_p(:,nys,:) |
---|
[2232] | 566 | IF ( .NOT. constant_diffusion ) e_p(:,nys-1,:) = e_p(:,nys,:) |
---|
[2696] | 567 | IF ( rans_tke_e ) diss_p(:,nys-1,:) = diss_p(:,nys,:) |
---|
[1960] | 568 | IF ( humidity ) THEN |
---|
[1409] | 569 | q_p(:,nys-1,:) = q_p(:,nys,:) |
---|
[2292] | 570 | IF ( cloud_physics .AND. microphysics_morrison ) THEN |
---|
| 571 | qc_p(:,nys-1,:) = qc_p(:,nys,:) |
---|
| 572 | nc_p(:,nys-1,:) = nc_p(:,nys,:) |
---|
| 573 | ENDIF |
---|
[1822] | 574 | IF ( cloud_physics .AND. microphysics_seifert ) THEN |
---|
[1409] | 575 | qr_p(:,nys-1,:) = qr_p(:,nys,:) |
---|
| 576 | nr_p(:,nys-1,:) = nr_p(:,nys,:) |
---|
[1053] | 577 | ENDIF |
---|
[1409] | 578 | ENDIF |
---|
[1960] | 579 | IF ( passive_scalar ) s_p(:,nys-1,:) = s_p(:,nys,:) |
---|
[1409] | 580 | ELSEIF ( outflow_n ) THEN |
---|
| 581 | pt_p(:,nyn+1,:) = pt_p(:,nyn,:) |
---|
[2696] | 582 | IF ( .NOT. constant_diffusion ) e_p(:,nyn+1,:) = e_p(:,nyn,:) |
---|
| 583 | IF ( rans_tke_e ) diss_p(:,nyn+1,:) = diss_p(:,nyn,:) |
---|
[1960] | 584 | IF ( humidity ) THEN |
---|
[1409] | 585 | q_p(:,nyn+1,:) = q_p(:,nyn,:) |
---|
[2292] | 586 | IF ( cloud_physics .AND. microphysics_morrison ) THEN |
---|
| 587 | qc_p(:,nyn+1,:) = qc_p(:,nyn,:) |
---|
| 588 | nc_p(:,nyn+1,:) = nc_p(:,nyn,:) |
---|
| 589 | ENDIF |
---|
[1822] | 590 | IF ( cloud_physics .AND. microphysics_seifert ) THEN |
---|
[1409] | 591 | qr_p(:,nyn+1,:) = qr_p(:,nyn,:) |
---|
| 592 | nr_p(:,nyn+1,:) = nr_p(:,nyn,:) |
---|
[1053] | 593 | ENDIF |
---|
[1409] | 594 | ENDIF |
---|
[1960] | 595 | IF ( passive_scalar ) s_p(:,nyn+1,:) = s_p(:,nyn,:) |
---|
[1409] | 596 | ELSEIF ( outflow_l ) THEN |
---|
| 597 | pt_p(:,:,nxl-1) = pt_p(:,:,nxl) |
---|
[2696] | 598 | IF ( .NOT. constant_diffusion ) e_p(:,:,nxl-1) = e_p(:,:,nxl) |
---|
| 599 | IF ( rans_tke_e ) diss_p(:,:,nxl-1) = diss_p(:,:,nxl) |
---|
[1960] | 600 | IF ( humidity ) THEN |
---|
[1409] | 601 | q_p(:,:,nxl-1) = q_p(:,:,nxl) |
---|
[2292] | 602 | IF ( cloud_physics .AND. microphysics_morrison ) THEN |
---|
| 603 | qc_p(:,:,nxl-1) = qc_p(:,:,nxl) |
---|
| 604 | nc_p(:,:,nxl-1) = nc_p(:,:,nxl) |
---|
| 605 | ENDIF |
---|
[1822] | 606 | IF ( cloud_physics .AND. microphysics_seifert ) THEN |
---|
[1409] | 607 | qr_p(:,:,nxl-1) = qr_p(:,:,nxl) |
---|
| 608 | nr_p(:,:,nxl-1) = nr_p(:,:,nxl) |
---|
[1053] | 609 | ENDIF |
---|
[1409] | 610 | ENDIF |
---|
[1960] | 611 | IF ( passive_scalar ) s_p(:,:,nxl-1) = s_p(:,:,nxl) |
---|
[1409] | 612 | ELSEIF ( outflow_r ) THEN |
---|
| 613 | pt_p(:,:,nxr+1) = pt_p(:,:,nxr) |
---|
[2696] | 614 | IF ( .NOT. constant_diffusion ) e_p(:,:,nxr+1) = e_p(:,:,nxr) |
---|
| 615 | IF ( rans_tke_e ) diss_p(:,:,nxr+1) = diss_p(:,:,nxr) |
---|
[1960] | 616 | IF ( humidity ) THEN |
---|
[1409] | 617 | q_p(:,:,nxr+1) = q_p(:,:,nxr) |
---|
[2292] | 618 | IF ( cloud_physics .AND. microphysics_morrison ) THEN |
---|
| 619 | qc_p(:,:,nxr+1) = qc_p(:,:,nxr) |
---|
| 620 | nc_p(:,:,nxr+1) = nc_p(:,:,nxr) |
---|
| 621 | ENDIF |
---|
[1822] | 622 | IF ( cloud_physics .AND. microphysics_seifert ) THEN |
---|
[1409] | 623 | qr_p(:,:,nxr+1) = qr_p(:,:,nxr) |
---|
| 624 | nr_p(:,:,nxr+1) = nr_p(:,:,nxr) |
---|
[1053] | 625 | ENDIF |
---|
[1] | 626 | ENDIF |
---|
[1960] | 627 | IF ( passive_scalar ) s_p(:,:,nxr+1) = s_p(:,:,nxr) |
---|
[1] | 628 | ENDIF |
---|
| 629 | |
---|
| 630 | ! |
---|
[2696] | 631 | !-- Lateral boundary conditions for chemical species |
---|
| 632 | #if defined( __chem ) |
---|
| 633 | IF ( air_chemistry ) CALL chem_boundary_conds( 'set_bc_lateral' ) |
---|
| 634 | #endif |
---|
| 635 | |
---|
| 636 | |
---|
| 637 | ! |
---|
[1159] | 638 | !-- Radiation boundary conditions for the velocities at the respective outflow. |
---|
| 639 | !-- The phase velocity is either assumed to the maximum phase velocity that |
---|
| 640 | !-- ensures numerical stability (CFL-condition) or calculated after |
---|
| 641 | !-- Orlanski(1976) and averaged along the outflow boundary. |
---|
[106] | 642 | IF ( outflow_s ) THEN |
---|
[75] | 643 | |
---|
[1159] | 644 | IF ( use_cmax ) THEN |
---|
| 645 | u_p(:,-1,:) = u(:,0,:) |
---|
| 646 | v_p(:,0,:) = v(:,1,:) |
---|
| 647 | w_p(:,-1,:) = w(:,0,:) |
---|
| 648 | ELSEIF ( .NOT. use_cmax ) THEN |
---|
[75] | 649 | |
---|
[978] | 650 | c_max = dy / dt_3d |
---|
[75] | 651 | |
---|
[1353] | 652 | c_u_m_l = 0.0_wp |
---|
| 653 | c_v_m_l = 0.0_wp |
---|
| 654 | c_w_m_l = 0.0_wp |
---|
[978] | 655 | |
---|
[1353] | 656 | c_u_m = 0.0_wp |
---|
| 657 | c_v_m = 0.0_wp |
---|
| 658 | c_w_m = 0.0_wp |
---|
[978] | 659 | |
---|
[75] | 660 | ! |
---|
[996] | 661 | !-- Calculate the phase speeds for u, v, and w, first local and then |
---|
| 662 | !-- average along the outflow boundary. |
---|
| 663 | DO k = nzb+1, nzt+1 |
---|
| 664 | DO i = nxl, nxr |
---|
[75] | 665 | |
---|
[106] | 666 | denom = u_m_s(k,0,i) - u_m_s(k,1,i) |
---|
| 667 | |
---|
[1353] | 668 | IF ( denom /= 0.0_wp ) THEN |
---|
[996] | 669 | c_u(k,i) = -c_max * ( u(k,0,i) - u_m_s(k,0,i) ) / ( denom * tsc(2) ) |
---|
[1353] | 670 | IF ( c_u(k,i) < 0.0_wp ) THEN |
---|
| 671 | c_u(k,i) = 0.0_wp |
---|
[106] | 672 | ELSEIF ( c_u(k,i) > c_max ) THEN |
---|
| 673 | c_u(k,i) = c_max |
---|
| 674 | ENDIF |
---|
| 675 | ELSE |
---|
| 676 | c_u(k,i) = c_max |
---|
[75] | 677 | ENDIF |
---|
| 678 | |
---|
[106] | 679 | denom = v_m_s(k,1,i) - v_m_s(k,2,i) |
---|
| 680 | |
---|
[1353] | 681 | IF ( denom /= 0.0_wp ) THEN |
---|
[996] | 682 | c_v(k,i) = -c_max * ( v(k,1,i) - v_m_s(k,1,i) ) / ( denom * tsc(2) ) |
---|
[1353] | 683 | IF ( c_v(k,i) < 0.0_wp ) THEN |
---|
| 684 | c_v(k,i) = 0.0_wp |
---|
[106] | 685 | ELSEIF ( c_v(k,i) > c_max ) THEN |
---|
| 686 | c_v(k,i) = c_max |
---|
| 687 | ENDIF |
---|
| 688 | ELSE |
---|
| 689 | c_v(k,i) = c_max |
---|
[75] | 690 | ENDIF |
---|
| 691 | |
---|
[106] | 692 | denom = w_m_s(k,0,i) - w_m_s(k,1,i) |
---|
[75] | 693 | |
---|
[1353] | 694 | IF ( denom /= 0.0_wp ) THEN |
---|
[996] | 695 | c_w(k,i) = -c_max * ( w(k,0,i) - w_m_s(k,0,i) ) / ( denom * tsc(2) ) |
---|
[1353] | 696 | IF ( c_w(k,i) < 0.0_wp ) THEN |
---|
| 697 | c_w(k,i) = 0.0_wp |
---|
[106] | 698 | ELSEIF ( c_w(k,i) > c_max ) THEN |
---|
| 699 | c_w(k,i) = c_max |
---|
| 700 | ENDIF |
---|
| 701 | ELSE |
---|
| 702 | c_w(k,i) = c_max |
---|
[75] | 703 | ENDIF |
---|
[106] | 704 | |
---|
[978] | 705 | c_u_m_l(k) = c_u_m_l(k) + c_u(k,i) |
---|
| 706 | c_v_m_l(k) = c_v_m_l(k) + c_v(k,i) |
---|
| 707 | c_w_m_l(k) = c_w_m_l(k) + c_w(k,i) |
---|
[106] | 708 | |
---|
[978] | 709 | ENDDO |
---|
| 710 | ENDDO |
---|
[75] | 711 | |
---|
[978] | 712 | #if defined( __parallel ) |
---|
| 713 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dx, ierr ) |
---|
| 714 | CALL MPI_ALLREDUCE( c_u_m_l(nzb+1), c_u_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
| 715 | MPI_SUM, comm1dx, ierr ) |
---|
| 716 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dx, ierr ) |
---|
| 717 | CALL MPI_ALLREDUCE( c_v_m_l(nzb+1), c_v_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
| 718 | MPI_SUM, comm1dx, ierr ) |
---|
| 719 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dx, ierr ) |
---|
| 720 | CALL MPI_ALLREDUCE( c_w_m_l(nzb+1), c_w_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
| 721 | MPI_SUM, comm1dx, ierr ) |
---|
| 722 | #else |
---|
| 723 | c_u_m = c_u_m_l |
---|
| 724 | c_v_m = c_v_m_l |
---|
| 725 | c_w_m = c_w_m_l |
---|
| 726 | #endif |
---|
| 727 | |
---|
| 728 | c_u_m = c_u_m / (nx+1) |
---|
| 729 | c_v_m = c_v_m / (nx+1) |
---|
| 730 | c_w_m = c_w_m / (nx+1) |
---|
| 731 | |
---|
[75] | 732 | ! |
---|
[978] | 733 | !-- Save old timelevels for the next timestep |
---|
| 734 | IF ( intermediate_timestep_count == 1 ) THEN |
---|
| 735 | u_m_s(:,:,:) = u(:,0:1,:) |
---|
| 736 | v_m_s(:,:,:) = v(:,1:2,:) |
---|
| 737 | w_m_s(:,:,:) = w(:,0:1,:) |
---|
| 738 | ENDIF |
---|
| 739 | |
---|
| 740 | ! |
---|
| 741 | !-- Calculate the new velocities |
---|
[996] | 742 | DO k = nzb+1, nzt+1 |
---|
| 743 | DO i = nxlg, nxrg |
---|
[978] | 744 | u_p(k,-1,i) = u(k,-1,i) - dt_3d * tsc(2) * c_u_m(k) * & |
---|
[75] | 745 | ( u(k,-1,i) - u(k,0,i) ) * ddy |
---|
| 746 | |
---|
[978] | 747 | v_p(k,0,i) = v(k,0,i) - dt_3d * tsc(2) * c_v_m(k) * & |
---|
[106] | 748 | ( v(k,0,i) - v(k,1,i) ) * ddy |
---|
[75] | 749 | |
---|
[978] | 750 | w_p(k,-1,i) = w(k,-1,i) - dt_3d * tsc(2) * c_w_m(k) * & |
---|
[75] | 751 | ( w(k,-1,i) - w(k,0,i) ) * ddy |
---|
[978] | 752 | ENDDO |
---|
[75] | 753 | ENDDO |
---|
| 754 | |
---|
| 755 | ! |
---|
[978] | 756 | !-- Bottom boundary at the outflow |
---|
| 757 | IF ( ibc_uv_b == 0 ) THEN |
---|
[1353] | 758 | u_p(nzb,-1,:) = 0.0_wp |
---|
| 759 | v_p(nzb,0,:) = 0.0_wp |
---|
[978] | 760 | ELSE |
---|
| 761 | u_p(nzb,-1,:) = u_p(nzb+1,-1,:) |
---|
| 762 | v_p(nzb,0,:) = v_p(nzb+1,0,:) |
---|
| 763 | ENDIF |
---|
[1353] | 764 | w_p(nzb,-1,:) = 0.0_wp |
---|
[73] | 765 | |
---|
[75] | 766 | ! |
---|
[978] | 767 | !-- Top boundary at the outflow |
---|
| 768 | IF ( ibc_uv_t == 0 ) THEN |
---|
| 769 | u_p(nzt+1,-1,:) = u_init(nzt+1) |
---|
| 770 | v_p(nzt+1,0,:) = v_init(nzt+1) |
---|
| 771 | ELSE |
---|
[1742] | 772 | u_p(nzt+1,-1,:) = u_p(nzt,-1,:) |
---|
| 773 | v_p(nzt+1,0,:) = v_p(nzt,0,:) |
---|
[978] | 774 | ENDIF |
---|
[1353] | 775 | w_p(nzt:nzt+1,-1,:) = 0.0_wp |
---|
[978] | 776 | |
---|
[75] | 777 | ENDIF |
---|
[73] | 778 | |
---|
[75] | 779 | ENDIF |
---|
[73] | 780 | |
---|
[106] | 781 | IF ( outflow_n ) THEN |
---|
[73] | 782 | |
---|
[1159] | 783 | IF ( use_cmax ) THEN |
---|
| 784 | u_p(:,ny+1,:) = u(:,ny,:) |
---|
| 785 | v_p(:,ny+1,:) = v(:,ny,:) |
---|
| 786 | w_p(:,ny+1,:) = w(:,ny,:) |
---|
| 787 | ELSEIF ( .NOT. use_cmax ) THEN |
---|
[75] | 788 | |
---|
[978] | 789 | c_max = dy / dt_3d |
---|
[75] | 790 | |
---|
[1353] | 791 | c_u_m_l = 0.0_wp |
---|
| 792 | c_v_m_l = 0.0_wp |
---|
| 793 | c_w_m_l = 0.0_wp |
---|
[978] | 794 | |
---|
[1353] | 795 | c_u_m = 0.0_wp |
---|
| 796 | c_v_m = 0.0_wp |
---|
| 797 | c_w_m = 0.0_wp |
---|
[978] | 798 | |
---|
[1] | 799 | ! |
---|
[996] | 800 | !-- Calculate the phase speeds for u, v, and w, first local and then |
---|
| 801 | !-- average along the outflow boundary. |
---|
| 802 | DO k = nzb+1, nzt+1 |
---|
| 803 | DO i = nxl, nxr |
---|
[73] | 804 | |
---|
[106] | 805 | denom = u_m_n(k,ny,i) - u_m_n(k,ny-1,i) |
---|
| 806 | |
---|
[1353] | 807 | IF ( denom /= 0.0_wp ) THEN |
---|
[996] | 808 | c_u(k,i) = -c_max * ( u(k,ny,i) - u_m_n(k,ny,i) ) / ( denom * tsc(2) ) |
---|
[1353] | 809 | IF ( c_u(k,i) < 0.0_wp ) THEN |
---|
| 810 | c_u(k,i) = 0.0_wp |
---|
[106] | 811 | ELSEIF ( c_u(k,i) > c_max ) THEN |
---|
| 812 | c_u(k,i) = c_max |
---|
| 813 | ENDIF |
---|
| 814 | ELSE |
---|
| 815 | c_u(k,i) = c_max |
---|
[73] | 816 | ENDIF |
---|
| 817 | |
---|
[106] | 818 | denom = v_m_n(k,ny,i) - v_m_n(k,ny-1,i) |
---|
[73] | 819 | |
---|
[1353] | 820 | IF ( denom /= 0.0_wp ) THEN |
---|
[996] | 821 | c_v(k,i) = -c_max * ( v(k,ny,i) - v_m_n(k,ny,i) ) / ( denom * tsc(2) ) |
---|
[1353] | 822 | IF ( c_v(k,i) < 0.0_wp ) THEN |
---|
| 823 | c_v(k,i) = 0.0_wp |
---|
[106] | 824 | ELSEIF ( c_v(k,i) > c_max ) THEN |
---|
| 825 | c_v(k,i) = c_max |
---|
| 826 | ENDIF |
---|
| 827 | ELSE |
---|
| 828 | c_v(k,i) = c_max |
---|
[73] | 829 | ENDIF |
---|
| 830 | |
---|
[106] | 831 | denom = w_m_n(k,ny,i) - w_m_n(k,ny-1,i) |
---|
[73] | 832 | |
---|
[1353] | 833 | IF ( denom /= 0.0_wp ) THEN |
---|
[996] | 834 | c_w(k,i) = -c_max * ( w(k,ny,i) - w_m_n(k,ny,i) ) / ( denom * tsc(2) ) |
---|
[1353] | 835 | IF ( c_w(k,i) < 0.0_wp ) THEN |
---|
| 836 | c_w(k,i) = 0.0_wp |
---|
[106] | 837 | ELSEIF ( c_w(k,i) > c_max ) THEN |
---|
| 838 | c_w(k,i) = c_max |
---|
| 839 | ENDIF |
---|
| 840 | ELSE |
---|
| 841 | c_w(k,i) = c_max |
---|
[73] | 842 | ENDIF |
---|
[106] | 843 | |
---|
[978] | 844 | c_u_m_l(k) = c_u_m_l(k) + c_u(k,i) |
---|
| 845 | c_v_m_l(k) = c_v_m_l(k) + c_v(k,i) |
---|
| 846 | c_w_m_l(k) = c_w_m_l(k) + c_w(k,i) |
---|
[106] | 847 | |
---|
[978] | 848 | ENDDO |
---|
| 849 | ENDDO |
---|
[73] | 850 | |
---|
[978] | 851 | #if defined( __parallel ) |
---|
| 852 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dx, ierr ) |
---|
| 853 | CALL MPI_ALLREDUCE( c_u_m_l(nzb+1), c_u_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
| 854 | MPI_SUM, comm1dx, ierr ) |
---|
| 855 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dx, ierr ) |
---|
| 856 | CALL MPI_ALLREDUCE( c_v_m_l(nzb+1), c_v_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
| 857 | MPI_SUM, comm1dx, ierr ) |
---|
| 858 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dx, ierr ) |
---|
| 859 | CALL MPI_ALLREDUCE( c_w_m_l(nzb+1), c_w_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
| 860 | MPI_SUM, comm1dx, ierr ) |
---|
| 861 | #else |
---|
| 862 | c_u_m = c_u_m_l |
---|
| 863 | c_v_m = c_v_m_l |
---|
| 864 | c_w_m = c_w_m_l |
---|
| 865 | #endif |
---|
| 866 | |
---|
| 867 | c_u_m = c_u_m / (nx+1) |
---|
| 868 | c_v_m = c_v_m / (nx+1) |
---|
| 869 | c_w_m = c_w_m / (nx+1) |
---|
| 870 | |
---|
[73] | 871 | ! |
---|
[978] | 872 | !-- Save old timelevels for the next timestep |
---|
| 873 | IF ( intermediate_timestep_count == 1 ) THEN |
---|
| 874 | u_m_n(:,:,:) = u(:,ny-1:ny,:) |
---|
| 875 | v_m_n(:,:,:) = v(:,ny-1:ny,:) |
---|
| 876 | w_m_n(:,:,:) = w(:,ny-1:ny,:) |
---|
| 877 | ENDIF |
---|
[73] | 878 | |
---|
[978] | 879 | ! |
---|
| 880 | !-- Calculate the new velocities |
---|
[996] | 881 | DO k = nzb+1, nzt+1 |
---|
| 882 | DO i = nxlg, nxrg |
---|
[978] | 883 | u_p(k,ny+1,i) = u(k,ny+1,i) - dt_3d * tsc(2) * c_u_m(k) * & |
---|
| 884 | ( u(k,ny+1,i) - u(k,ny,i) ) * ddy |
---|
[73] | 885 | |
---|
[978] | 886 | v_p(k,ny+1,i) = v(k,ny+1,i) - dt_3d * tsc(2) * c_v_m(k) * & |
---|
| 887 | ( v(k,ny+1,i) - v(k,ny,i) ) * ddy |
---|
[73] | 888 | |
---|
[978] | 889 | w_p(k,ny+1,i) = w(k,ny+1,i) - dt_3d * tsc(2) * c_w_m(k) * & |
---|
| 890 | ( w(k,ny+1,i) - w(k,ny,i) ) * ddy |
---|
| 891 | ENDDO |
---|
[1] | 892 | ENDDO |
---|
| 893 | |
---|
| 894 | ! |
---|
[978] | 895 | !-- Bottom boundary at the outflow |
---|
| 896 | IF ( ibc_uv_b == 0 ) THEN |
---|
[1353] | 897 | u_p(nzb,ny+1,:) = 0.0_wp |
---|
| 898 | v_p(nzb,ny+1,:) = 0.0_wp |
---|
[978] | 899 | ELSE |
---|
| 900 | u_p(nzb,ny+1,:) = u_p(nzb+1,ny+1,:) |
---|
| 901 | v_p(nzb,ny+1,:) = v_p(nzb+1,ny+1,:) |
---|
| 902 | ENDIF |
---|
[1353] | 903 | w_p(nzb,ny+1,:) = 0.0_wp |
---|
[73] | 904 | |
---|
| 905 | ! |
---|
[978] | 906 | !-- Top boundary at the outflow |
---|
| 907 | IF ( ibc_uv_t == 0 ) THEN |
---|
| 908 | u_p(nzt+1,ny+1,:) = u_init(nzt+1) |
---|
| 909 | v_p(nzt+1,ny+1,:) = v_init(nzt+1) |
---|
| 910 | ELSE |
---|
| 911 | u_p(nzt+1,ny+1,:) = u_p(nzt,nyn+1,:) |
---|
| 912 | v_p(nzt+1,ny+1,:) = v_p(nzt,nyn+1,:) |
---|
| 913 | ENDIF |
---|
[1353] | 914 | w_p(nzt:nzt+1,ny+1,:) = 0.0_wp |
---|
[978] | 915 | |
---|
[1] | 916 | ENDIF |
---|
| 917 | |
---|
[75] | 918 | ENDIF |
---|
| 919 | |
---|
[106] | 920 | IF ( outflow_l ) THEN |
---|
[75] | 921 | |
---|
[1159] | 922 | IF ( use_cmax ) THEN |
---|
[1717] | 923 | u_p(:,:,0) = u(:,:,1) |
---|
| 924 | v_p(:,:,-1) = v(:,:,0) |
---|
[1159] | 925 | w_p(:,:,-1) = w(:,:,0) |
---|
| 926 | ELSEIF ( .NOT. use_cmax ) THEN |
---|
[75] | 927 | |
---|
[978] | 928 | c_max = dx / dt_3d |
---|
[75] | 929 | |
---|
[1353] | 930 | c_u_m_l = 0.0_wp |
---|
| 931 | c_v_m_l = 0.0_wp |
---|
| 932 | c_w_m_l = 0.0_wp |
---|
[978] | 933 | |
---|
[1353] | 934 | c_u_m = 0.0_wp |
---|
| 935 | c_v_m = 0.0_wp |
---|
| 936 | c_w_m = 0.0_wp |
---|
[978] | 937 | |
---|
[1] | 938 | ! |
---|
[996] | 939 | !-- Calculate the phase speeds for u, v, and w, first local and then |
---|
| 940 | !-- average along the outflow boundary. |
---|
| 941 | DO k = nzb+1, nzt+1 |
---|
| 942 | DO j = nys, nyn |
---|
[75] | 943 | |
---|
[106] | 944 | denom = u_m_l(k,j,1) - u_m_l(k,j,2) |
---|
| 945 | |
---|
[1353] | 946 | IF ( denom /= 0.0_wp ) THEN |
---|
[996] | 947 | c_u(k,j) = -c_max * ( u(k,j,1) - u_m_l(k,j,1) ) / ( denom * tsc(2) ) |
---|
[1353] | 948 | IF ( c_u(k,j) < 0.0_wp ) THEN |
---|
| 949 | c_u(k,j) = 0.0_wp |
---|
[107] | 950 | ELSEIF ( c_u(k,j) > c_max ) THEN |
---|
| 951 | c_u(k,j) = c_max |
---|
[106] | 952 | ENDIF |
---|
| 953 | ELSE |
---|
[107] | 954 | c_u(k,j) = c_max |
---|
[75] | 955 | ENDIF |
---|
| 956 | |
---|
[106] | 957 | denom = v_m_l(k,j,0) - v_m_l(k,j,1) |
---|
[75] | 958 | |
---|
[1353] | 959 | IF ( denom /= 0.0_wp ) THEN |
---|
[996] | 960 | c_v(k,j) = -c_max * ( v(k,j,0) - v_m_l(k,j,0) ) / ( denom * tsc(2) ) |
---|
[1353] | 961 | IF ( c_v(k,j) < 0.0_wp ) THEN |
---|
| 962 | c_v(k,j) = 0.0_wp |
---|
[106] | 963 | ELSEIF ( c_v(k,j) > c_max ) THEN |
---|
| 964 | c_v(k,j) = c_max |
---|
| 965 | ENDIF |
---|
| 966 | ELSE |
---|
| 967 | c_v(k,j) = c_max |
---|
[75] | 968 | ENDIF |
---|
| 969 | |
---|
[106] | 970 | denom = w_m_l(k,j,0) - w_m_l(k,j,1) |
---|
[75] | 971 | |
---|
[1353] | 972 | IF ( denom /= 0.0_wp ) THEN |
---|
[996] | 973 | c_w(k,j) = -c_max * ( w(k,j,0) - w_m_l(k,j,0) ) / ( denom * tsc(2) ) |
---|
[1353] | 974 | IF ( c_w(k,j) < 0.0_wp ) THEN |
---|
| 975 | c_w(k,j) = 0.0_wp |
---|
[106] | 976 | ELSEIF ( c_w(k,j) > c_max ) THEN |
---|
| 977 | c_w(k,j) = c_max |
---|
| 978 | ENDIF |
---|
| 979 | ELSE |
---|
| 980 | c_w(k,j) = c_max |
---|
[75] | 981 | ENDIF |
---|
[106] | 982 | |
---|
[978] | 983 | c_u_m_l(k) = c_u_m_l(k) + c_u(k,j) |
---|
| 984 | c_v_m_l(k) = c_v_m_l(k) + c_v(k,j) |
---|
| 985 | c_w_m_l(k) = c_w_m_l(k) + c_w(k,j) |
---|
[106] | 986 | |
---|
[978] | 987 | ENDDO |
---|
| 988 | ENDDO |
---|
[75] | 989 | |
---|
[978] | 990 | #if defined( __parallel ) |
---|
| 991 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dy, ierr ) |
---|
| 992 | CALL MPI_ALLREDUCE( c_u_m_l(nzb+1), c_u_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
| 993 | MPI_SUM, comm1dy, ierr ) |
---|
| 994 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dy, ierr ) |
---|
| 995 | CALL MPI_ALLREDUCE( c_v_m_l(nzb+1), c_v_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
| 996 | MPI_SUM, comm1dy, ierr ) |
---|
| 997 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dy, ierr ) |
---|
| 998 | CALL MPI_ALLREDUCE( c_w_m_l(nzb+1), c_w_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
| 999 | MPI_SUM, comm1dy, ierr ) |
---|
| 1000 | #else |
---|
| 1001 | c_u_m = c_u_m_l |
---|
| 1002 | c_v_m = c_v_m_l |
---|
| 1003 | c_w_m = c_w_m_l |
---|
| 1004 | #endif |
---|
| 1005 | |
---|
| 1006 | c_u_m = c_u_m / (ny+1) |
---|
| 1007 | c_v_m = c_v_m / (ny+1) |
---|
| 1008 | c_w_m = c_w_m / (ny+1) |
---|
| 1009 | |
---|
[73] | 1010 | ! |
---|
[978] | 1011 | !-- Save old timelevels for the next timestep |
---|
| 1012 | IF ( intermediate_timestep_count == 1 ) THEN |
---|
| 1013 | u_m_l(:,:,:) = u(:,:,1:2) |
---|
| 1014 | v_m_l(:,:,:) = v(:,:,0:1) |
---|
| 1015 | w_m_l(:,:,:) = w(:,:,0:1) |
---|
| 1016 | ENDIF |
---|
| 1017 | |
---|
| 1018 | ! |
---|
| 1019 | !-- Calculate the new velocities |
---|
[996] | 1020 | DO k = nzb+1, nzt+1 |
---|
[1113] | 1021 | DO j = nysg, nyng |
---|
[978] | 1022 | u_p(k,j,0) = u(k,j,0) - dt_3d * tsc(2) * c_u_m(k) * & |
---|
[106] | 1023 | ( u(k,j,0) - u(k,j,1) ) * ddx |
---|
[75] | 1024 | |
---|
[978] | 1025 | v_p(k,j,-1) = v(k,j,-1) - dt_3d * tsc(2) * c_v_m(k) * & |
---|
[75] | 1026 | ( v(k,j,-1) - v(k,j,0) ) * ddx |
---|
| 1027 | |
---|
[978] | 1028 | w_p(k,j,-1) = w(k,j,-1) - dt_3d * tsc(2) * c_w_m(k) * & |
---|
[75] | 1029 | ( w(k,j,-1) - w(k,j,0) ) * ddx |
---|
[978] | 1030 | ENDDO |
---|
[75] | 1031 | ENDDO |
---|
| 1032 | |
---|
| 1033 | ! |
---|
[978] | 1034 | !-- Bottom boundary at the outflow |
---|
| 1035 | IF ( ibc_uv_b == 0 ) THEN |
---|
[1353] | 1036 | u_p(nzb,:,0) = 0.0_wp |
---|
| 1037 | v_p(nzb,:,-1) = 0.0_wp |
---|
[978] | 1038 | ELSE |
---|
| 1039 | u_p(nzb,:,0) = u_p(nzb+1,:,0) |
---|
| 1040 | v_p(nzb,:,-1) = v_p(nzb+1,:,-1) |
---|
| 1041 | ENDIF |
---|
[1353] | 1042 | w_p(nzb,:,-1) = 0.0_wp |
---|
[1] | 1043 | |
---|
[75] | 1044 | ! |
---|
[978] | 1045 | !-- Top boundary at the outflow |
---|
| 1046 | IF ( ibc_uv_t == 0 ) THEN |
---|
[1764] | 1047 | u_p(nzt+1,:,0) = u_init(nzt+1) |
---|
[978] | 1048 | v_p(nzt+1,:,-1) = v_init(nzt+1) |
---|
| 1049 | ELSE |
---|
[1764] | 1050 | u_p(nzt+1,:,0) = u_p(nzt,:,0) |
---|
[978] | 1051 | v_p(nzt+1,:,-1) = v_p(nzt,:,-1) |
---|
| 1052 | ENDIF |
---|
[1353] | 1053 | w_p(nzt:nzt+1,:,-1) = 0.0_wp |
---|
[978] | 1054 | |
---|
[75] | 1055 | ENDIF |
---|
[73] | 1056 | |
---|
[75] | 1057 | ENDIF |
---|
[73] | 1058 | |
---|
[106] | 1059 | IF ( outflow_r ) THEN |
---|
[73] | 1060 | |
---|
[1159] | 1061 | IF ( use_cmax ) THEN |
---|
| 1062 | u_p(:,:,nx+1) = u(:,:,nx) |
---|
| 1063 | v_p(:,:,nx+1) = v(:,:,nx) |
---|
| 1064 | w_p(:,:,nx+1) = w(:,:,nx) |
---|
| 1065 | ELSEIF ( .NOT. use_cmax ) THEN |
---|
[75] | 1066 | |
---|
[978] | 1067 | c_max = dx / dt_3d |
---|
[75] | 1068 | |
---|
[1353] | 1069 | c_u_m_l = 0.0_wp |
---|
| 1070 | c_v_m_l = 0.0_wp |
---|
| 1071 | c_w_m_l = 0.0_wp |
---|
[978] | 1072 | |
---|
[1353] | 1073 | c_u_m = 0.0_wp |
---|
| 1074 | c_v_m = 0.0_wp |
---|
| 1075 | c_w_m = 0.0_wp |
---|
[978] | 1076 | |
---|
[1] | 1077 | ! |
---|
[996] | 1078 | !-- Calculate the phase speeds for u, v, and w, first local and then |
---|
| 1079 | !-- average along the outflow boundary. |
---|
| 1080 | DO k = nzb+1, nzt+1 |
---|
| 1081 | DO j = nys, nyn |
---|
[73] | 1082 | |
---|
[106] | 1083 | denom = u_m_r(k,j,nx) - u_m_r(k,j,nx-1) |
---|
| 1084 | |
---|
[1353] | 1085 | IF ( denom /= 0.0_wp ) THEN |
---|
[996] | 1086 | c_u(k,j) = -c_max * ( u(k,j,nx) - u_m_r(k,j,nx) ) / ( denom * tsc(2) ) |
---|
[1353] | 1087 | IF ( c_u(k,j) < 0.0_wp ) THEN |
---|
| 1088 | c_u(k,j) = 0.0_wp |
---|
[106] | 1089 | ELSEIF ( c_u(k,j) > c_max ) THEN |
---|
| 1090 | c_u(k,j) = c_max |
---|
| 1091 | ENDIF |
---|
| 1092 | ELSE |
---|
| 1093 | c_u(k,j) = c_max |
---|
[73] | 1094 | ENDIF |
---|
| 1095 | |
---|
[106] | 1096 | denom = v_m_r(k,j,nx) - v_m_r(k,j,nx-1) |
---|
[73] | 1097 | |
---|
[1353] | 1098 | IF ( denom /= 0.0_wp ) THEN |
---|
[996] | 1099 | c_v(k,j) = -c_max * ( v(k,j,nx) - v_m_r(k,j,nx) ) / ( denom * tsc(2) ) |
---|
[1353] | 1100 | IF ( c_v(k,j) < 0.0_wp ) THEN |
---|
| 1101 | c_v(k,j) = 0.0_wp |
---|
[106] | 1102 | ELSEIF ( c_v(k,j) > c_max ) THEN |
---|
| 1103 | c_v(k,j) = c_max |
---|
| 1104 | ENDIF |
---|
| 1105 | ELSE |
---|
| 1106 | c_v(k,j) = c_max |
---|
[73] | 1107 | ENDIF |
---|
| 1108 | |
---|
[106] | 1109 | denom = w_m_r(k,j,nx) - w_m_r(k,j,nx-1) |
---|
[73] | 1110 | |
---|
[1353] | 1111 | IF ( denom /= 0.0_wp ) THEN |
---|
[996] | 1112 | c_w(k,j) = -c_max * ( w(k,j,nx) - w_m_r(k,j,nx) ) / ( denom * tsc(2) ) |
---|
[1353] | 1113 | IF ( c_w(k,j) < 0.0_wp ) THEN |
---|
| 1114 | c_w(k,j) = 0.0_wp |
---|
[106] | 1115 | ELSEIF ( c_w(k,j) > c_max ) THEN |
---|
| 1116 | c_w(k,j) = c_max |
---|
| 1117 | ENDIF |
---|
| 1118 | ELSE |
---|
| 1119 | c_w(k,j) = c_max |
---|
[73] | 1120 | ENDIF |
---|
[106] | 1121 | |
---|
[978] | 1122 | c_u_m_l(k) = c_u_m_l(k) + c_u(k,j) |
---|
| 1123 | c_v_m_l(k) = c_v_m_l(k) + c_v(k,j) |
---|
| 1124 | c_w_m_l(k) = c_w_m_l(k) + c_w(k,j) |
---|
[106] | 1125 | |
---|
[978] | 1126 | ENDDO |
---|
| 1127 | ENDDO |
---|
[73] | 1128 | |
---|
[978] | 1129 | #if defined( __parallel ) |
---|
| 1130 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dy, ierr ) |
---|
| 1131 | CALL MPI_ALLREDUCE( c_u_m_l(nzb+1), c_u_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
| 1132 | MPI_SUM, comm1dy, ierr ) |
---|
| 1133 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dy, ierr ) |
---|
| 1134 | CALL MPI_ALLREDUCE( c_v_m_l(nzb+1), c_v_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
| 1135 | MPI_SUM, comm1dy, ierr ) |
---|
| 1136 | IF ( collective_wait ) CALL MPI_BARRIER( comm1dy, ierr ) |
---|
| 1137 | CALL MPI_ALLREDUCE( c_w_m_l(nzb+1), c_w_m(nzb+1), nzt-nzb, MPI_REAL, & |
---|
| 1138 | MPI_SUM, comm1dy, ierr ) |
---|
| 1139 | #else |
---|
| 1140 | c_u_m = c_u_m_l |
---|
| 1141 | c_v_m = c_v_m_l |
---|
| 1142 | c_w_m = c_w_m_l |
---|
| 1143 | #endif |
---|
| 1144 | |
---|
| 1145 | c_u_m = c_u_m / (ny+1) |
---|
| 1146 | c_v_m = c_v_m / (ny+1) |
---|
| 1147 | c_w_m = c_w_m / (ny+1) |
---|
| 1148 | |
---|
[73] | 1149 | ! |
---|
[978] | 1150 | !-- Save old timelevels for the next timestep |
---|
| 1151 | IF ( intermediate_timestep_count == 1 ) THEN |
---|
| 1152 | u_m_r(:,:,:) = u(:,:,nx-1:nx) |
---|
| 1153 | v_m_r(:,:,:) = v(:,:,nx-1:nx) |
---|
| 1154 | w_m_r(:,:,:) = w(:,:,nx-1:nx) |
---|
| 1155 | ENDIF |
---|
[73] | 1156 | |
---|
[978] | 1157 | ! |
---|
| 1158 | !-- Calculate the new velocities |
---|
[996] | 1159 | DO k = nzb+1, nzt+1 |
---|
[1113] | 1160 | DO j = nysg, nyng |
---|
[978] | 1161 | u_p(k,j,nx+1) = u(k,j,nx+1) - dt_3d * tsc(2) * c_u_m(k) * & |
---|
| 1162 | ( u(k,j,nx+1) - u(k,j,nx) ) * ddx |
---|
[73] | 1163 | |
---|
[978] | 1164 | v_p(k,j,nx+1) = v(k,j,nx+1) - dt_3d * tsc(2) * c_v_m(k) * & |
---|
| 1165 | ( v(k,j,nx+1) - v(k,j,nx) ) * ddx |
---|
[73] | 1166 | |
---|
[978] | 1167 | w_p(k,j,nx+1) = w(k,j,nx+1) - dt_3d * tsc(2) * c_w_m(k) * & |
---|
| 1168 | ( w(k,j,nx+1) - w(k,j,nx) ) * ddx |
---|
| 1169 | ENDDO |
---|
[73] | 1170 | ENDDO |
---|
| 1171 | |
---|
| 1172 | ! |
---|
[978] | 1173 | !-- Bottom boundary at the outflow |
---|
| 1174 | IF ( ibc_uv_b == 0 ) THEN |
---|
[1353] | 1175 | u_p(nzb,:,nx+1) = 0.0_wp |
---|
| 1176 | v_p(nzb,:,nx+1) = 0.0_wp |
---|
[978] | 1177 | ELSE |
---|
| 1178 | u_p(nzb,:,nx+1) = u_p(nzb+1,:,nx+1) |
---|
| 1179 | v_p(nzb,:,nx+1) = v_p(nzb+1,:,nx+1) |
---|
| 1180 | ENDIF |
---|
[1353] | 1181 | w_p(nzb,:,nx+1) = 0.0_wp |
---|
[73] | 1182 | |
---|
| 1183 | ! |
---|
[978] | 1184 | !-- Top boundary at the outflow |
---|
| 1185 | IF ( ibc_uv_t == 0 ) THEN |
---|
| 1186 | u_p(nzt+1,:,nx+1) = u_init(nzt+1) |
---|
| 1187 | v_p(nzt+1,:,nx+1) = v_init(nzt+1) |
---|
| 1188 | ELSE |
---|
| 1189 | u_p(nzt+1,:,nx+1) = u_p(nzt,:,nx+1) |
---|
| 1190 | v_p(nzt+1,:,nx+1) = v_p(nzt,:,nx+1) |
---|
| 1191 | ENDIF |
---|
[1742] | 1192 | w_p(nzt:nzt+1,:,nx+1) = 0.0_wp |
---|
[978] | 1193 | |
---|
[1] | 1194 | ENDIF |
---|
| 1195 | |
---|
| 1196 | ENDIF |
---|
| 1197 | |
---|
| 1198 | END SUBROUTINE boundary_conds |
---|