[2338] | 1 | !> @file model_1d_mod.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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[254] | 20 | ! Current revisions: |
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[1] | 21 | ! ----------------- |
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[1961] | 22 | ! |
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[3049] | 23 | ! |
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[1961] | 24 | ! Former revisions: |
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| 25 | ! ----------------- |
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| 26 | ! $Id: model_1d_mod.f90 3135 2018-07-16 14:43:04Z raasch $ |
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[3135] | 27 | ! Bugfix: add +1 to c_3 according to Sogachev et al. (2012) |
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| 28 | ! |
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| 29 | ! 3126 2018-07-13 15:13:54Z gronemeier |
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[3126] | 30 | ! Bugfix: define c_0 = 0.03^0.25 = 0.416179145 |
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| 31 | ! |
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| 32 | ! 3083 2018-06-19 14:03:12Z gronemeier |
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[3083] | 33 | ! Bugfixes: |
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| 34 | ! - preset te_diss and te_e to avoid runtime errors |
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| 35 | ! - implementation of buoyancy term to dissipation |
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| 36 | ! according to Sogachev et al. (2012) |
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| 37 | ! - where diss_p < 0 set diss_p = 0.1 diss |
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| 38 | ! - calculate progn eq(diss) starting from nzb+1 |
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| 39 | ! Changes: |
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| 40 | ! - add sig_e to TKE equation |
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| 41 | ! - adjust prognostic equation of diss |
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| 42 | ! - set model constants according to Koblitz (2013) |
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| 43 | ! - renamed c_m to c_0 |
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| 44 | ! - rename l_black into l1d_init |
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| 45 | ! - calculate l_grid within init_1d_model and save it as l1d_init |
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| 46 | ! - calculate l1d according to DE85 if dissipation is a prognostic value |
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| 47 | ! - made annotations doxygen-readable |
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| 48 | ! |
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| 49 | ! 3049 2018-05-29 13:52:36Z Giersch |
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[3049] | 50 | ! Error messages revised |
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| 51 | ! |
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| 52 | ! 3045 2018-05-28 07:55:41Z Giersch |
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[3045] | 53 | ! Error message revised |
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| 54 | ! |
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| 55 | ! 2965 2018-04-13 07:37:25Z scharf |
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[2965] | 56 | ! adjusted format string for 1D run control output |
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| 57 | ! |
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| 58 | ! 2918 2018-03-21 15:52:14Z gronemeier |
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[2918] | 59 | ! - rename l_black into l1d_init |
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| 60 | ! - calculate l_grid within init_1d_model and save it as l1d_init |
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| 61 | ! |
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| 62 | ! 2718 2018-01-02 08:49:38Z maronga |
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[2716] | 63 | ! Corrected "Former revisions" section |
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| 64 | ! |
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| 65 | ! 2696 2017-12-14 17:12:51Z kanani |
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| 66 | ! Change in file header (GPL part) |
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[2696] | 67 | ! implement TKE-e closure |
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| 68 | ! modification of dissipation production according to Detering and Etling |
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| 69 | ! reduced factor for timestep criterion to 0.125 and first dt to 1s (TG) |
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| 70 | ! |
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| 71 | ! 2339 2017-08-07 13:55:26Z gronemeier |
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[2339] | 72 | ! corrected timestamp in header |
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| 73 | ! |
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| 74 | ! 2338 2017-08-07 12:15:38Z gronemeier |
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[2338] | 75 | ! renamed init_1d_model to model_1d_mod and and formatted it as a module; |
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| 76 | ! reformatted output of profiles |
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| 77 | ! |
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[2339] | 78 | ! 2337 2017-08-07 08:59:53Z gronemeier |
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[2337] | 79 | ! revised calculation of mixing length |
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| 80 | ! removed rounding of time step |
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| 81 | ! corrected calculation of virtual potential temperature |
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| 82 | ! |
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| 83 | ! 2334 2017-08-04 11:57:04Z gronemeier |
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[2334] | 84 | ! set c_m = 0.4 according to Detering and Etling (1985) |
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| 85 | ! |
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| 86 | ! 2299 2017-06-29 10:14:38Z maronga |
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[2299] | 87 | ! Removed german text |
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[1961] | 88 | ! |
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[2299] | 89 | ! 2101 2017-01-05 16:42:31Z suehring |
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| 90 | ! |
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[2060] | 91 | ! 2059 2016-11-10 14:20:40Z maronga |
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| 92 | ! Corrected min/max values of Rif. |
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| 93 | ! |
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[2001] | 94 | ! 2000 2016-08-20 18:09:15Z knoop |
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| 95 | ! Forced header and separation lines into 80 columns |
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| 96 | ! |
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[1961] | 97 | ! 1960 2016-07-12 16:34:24Z suehring |
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[1960] | 98 | ! Remove passive_scalar from IF-statements, as 1D-scalar profile is effectively |
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| 99 | ! not used. |
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| 100 | ! Formatting adjustment |
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[1809] | 101 | ! |
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| 102 | ! 1808 2016-04-05 19:44:00Z raasch |
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| 103 | ! routine local_flush replaced by FORTRAN statement |
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| 104 | ! |
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[1710] | 105 | ! 1709 2015-11-04 14:47:01Z maronga |
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| 106 | ! Set initial time step to 10 s to avoid instability of the 1d model for small |
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| 107 | ! grid spacings |
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| 108 | ! |
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[1698] | 109 | ! 1697 2015-10-28 17:14:10Z raasch |
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| 110 | ! small E- and F-FORMAT changes to avoid informative compiler messages about |
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| 111 | ! insufficient field width |
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| 112 | ! |
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[1692] | 113 | ! 1691 2015-10-26 16:17:44Z maronga |
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| 114 | ! Renamed prandtl_layer to constant_flux_layer. rif is replaced by ol and zeta. |
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| 115 | ! |
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[1683] | 116 | ! 1682 2015-10-07 23:56:08Z knoop |
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| 117 | ! Code annotations made doxygen readable |
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| 118 | ! |
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[1354] | 119 | ! 1353 2014-04-08 15:21:23Z heinze |
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| 120 | ! REAL constants provided with KIND-attribute |
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| 121 | ! |
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[1347] | 122 | ! 1346 2014-03-27 13:18:20Z heinze |
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| 123 | ! Bugfix: REAL constants provided with KIND-attribute especially in call of |
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| 124 | ! intrinsic function like MAX, MIN, SIGN |
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| 125 | ! |
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[1323] | 126 | ! 1322 2014-03-20 16:38:49Z raasch |
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| 127 | ! REAL functions provided with KIND-attribute |
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| 128 | ! |
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[1321] | 129 | ! 1320 2014-03-20 08:40:49Z raasch |
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[1320] | 130 | ! ONLY-attribute added to USE-statements, |
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| 131 | ! kind-parameters added to all INTEGER and REAL declaration statements, |
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| 132 | ! kinds are defined in new module kinds, |
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| 133 | ! revision history before 2012 removed, |
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| 134 | ! comment fields (!:) to be used for variable explanations added to |
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| 135 | ! all variable declaration statements |
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[1321] | 136 | ! |
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[1037] | 137 | ! 1036 2012-10-22 13:43:42Z raasch |
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| 138 | ! code put under GPL (PALM 3.9) |
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| 139 | ! |
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[1017] | 140 | ! 1015 2012-09-27 09:23:24Z raasch |
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| 141 | ! adjustment of mixing length to the Prandtl mixing length at first grid point |
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| 142 | ! above ground removed |
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| 143 | ! |
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[1002] | 144 | ! 1001 2012-09-13 14:08:46Z raasch |
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| 145 | ! all actions concerning leapfrog scheme removed |
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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 | ! roughness length for scalar quantities z0h1d added |
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| 152 | ! |
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[1] | 153 | ! Revision 1.1 1998/03/09 16:22:10 raasch |
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| 154 | ! Initial revision |
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| 155 | ! |
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| 156 | ! |
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| 157 | ! Description: |
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| 158 | ! ------------ |
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[1682] | 159 | !> 1D-model to initialize the 3D-arrays. |
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| 160 | !> The temperature profile is set as steady and a corresponding steady solution |
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| 161 | !> of the wind profile is being computed. |
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| 162 | !> All subroutines required can be found within this file. |
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[1691] | 163 | !> |
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| 164 | !> @todo harmonize code with new surface_layer_fluxes module |
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[1709] | 165 | !> @bug 1D model crashes when using small grid spacings in the order of 1 m |
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[2965] | 166 | !> @fixme option "as_in_3d_model" seems to be an inappropriate option because |
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[2918] | 167 | !> the 1D model uses different turbulence closure approaches at least if |
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| 168 | !> the 3D model is set to LES-mode. |
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[1] | 169 | !------------------------------------------------------------------------------! |
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[2338] | 170 | MODULE model_1d_mod |
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[1] | 171 | |
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[1320] | 172 | USE arrays_3d, & |
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[2918] | 173 | ONLY: dd2zu, ddzu, ddzw, dzu, dzw, pt_init, q_init, ug, u_init, & |
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[2338] | 174 | vg, v_init, zu |
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[1320] | 175 | |
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[2338] | 176 | USE control_parameters, & |
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| 177 | ONLY: constant_diffusion, constant_flux_layer, dissipation_1d, f, g, & |
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| 178 | humidity, ibc_e_b, intermediate_timestep_count, & |
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| 179 | intermediate_timestep_count_max, kappa, km_constant, & |
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| 180 | message_string, mixing_length_1d, prandtl_number, & |
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[2696] | 181 | roughness_length, run_description_header, simulated_time_chr, & |
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| 182 | timestep_scheme, tsc, z0h_factor |
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[2338] | 183 | |
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[1320] | 184 | USE indices, & |
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[2338] | 185 | ONLY: nzb, nzb_diff, nzt |
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[1320] | 186 | |
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| 187 | USE kinds |
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[1] | 188 | |
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[3083] | 189 | USE pegrid, & |
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| 190 | ONLY: myid |
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[2338] | 191 | |
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| 192 | |
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[1] | 193 | IMPLICIT NONE |
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| 194 | |
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[2338] | 195 | INTEGER(iwp) :: current_timestep_number_1d = 0 !< current timestep number (1d-model) |
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[2696] | 196 | INTEGER(iwp) :: damp_level_ind_1d !< lower grid index of damping layer (1d-model) |
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[2338] | 197 | |
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| 198 | LOGICAL :: run_control_header_1d = .FALSE. !< flag for output of run control header (1d-model) |
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| 199 | LOGICAL :: stop_dt_1d = .FALSE. !< termination flag, used in case of too small timestep (1d-model) |
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| 200 | |
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[3083] | 201 | REAL(wp) :: alpha_buoyancy !< model constant according to Koblitz (2013) |
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[3126] | 202 | REAL(wp) :: c_0 = 0.416179145_wp !< = 0.03^0.25; model constant according to Koblitz (2013) |
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[3083] | 203 | REAL(wp) :: c_1 = 1.52_wp !< model constant according to Koblitz (2013) |
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| 204 | REAL(wp) :: c_2 = 1.83_wp !< model constant according to Koblitz (2013) |
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| 205 | REAL(wp) :: c_3 !< model constant |
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| 206 | REAL(wp) :: c_mu !< model constant |
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[2696] | 207 | REAL(wp) :: damp_level_1d = -1.0_wp !< namelist parameter |
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[2338] | 208 | REAL(wp) :: dt_1d = 60.0_wp !< dynamic timestep (1d-model) |
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| 209 | REAL(wp) :: dt_max_1d = 300.0_wp !< timestep limit (1d-model) |
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[2696] | 210 | REAL(wp) :: dt_pr_1d = 9999999.9_wp !< namelist parameter |
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| 211 | REAL(wp) :: dt_run_control_1d = 60.0_wp !< namelist parameter |
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| 212 | REAL(wp) :: end_time_1d = 864000.0_wp !< namelist parameter |
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[3083] | 213 | REAL(wp) :: lambda !< maximum mixing length |
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[2338] | 214 | REAL(wp) :: qs1d !< characteristic humidity scale (1d-model) |
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| 215 | REAL(wp) :: simulated_time_1d = 0.0_wp !< updated simulated time (1d-model) |
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[3083] | 216 | REAL(wp) :: sig_diss = 2.95_wp !< model constant according to Koblitz (2013) |
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| 217 | REAL(wp) :: sig_e = 2.95_wp !< model constant according to Koblitz (2013) |
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[2338] | 218 | REAL(wp) :: time_pr_1d = 0.0_wp !< updated simulated time for profile output (1d-model) |
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| 219 | REAL(wp) :: time_run_control_1d = 0.0_wp !< updated simulated time for run-control output (1d-model) |
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| 220 | REAL(wp) :: ts1d !< characteristic temperature scale (1d-model) |
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[2696] | 221 | REAL(wp) :: us1d !< friction velocity (1d-model) |
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| 222 | REAL(wp) :: usws1d !< u-component of the momentum flux (1d-model) |
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| 223 | REAL(wp) :: vsws1d !< v-component of the momentum flux (1d-model) |
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[2338] | 224 | REAL(wp) :: z01d !< roughness length for momentum (1d-model) |
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| 225 | REAL(wp) :: z0h1d !< roughness length for scalars (1d-model) |
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| 226 | |
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[2696] | 227 | REAL(wp), DIMENSION(:), ALLOCATABLE :: diss1d !< tke dissipation rate (1d-model) |
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| 228 | REAL(wp), DIMENSION(:), ALLOCATABLE :: diss1d_p !< prognostic value of tke dissipation rate (1d-model) |
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| 229 | REAL(wp), DIMENSION(:), ALLOCATABLE :: e1d !< tke (1d-model) |
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[2338] | 230 | REAL(wp), DIMENSION(:), ALLOCATABLE :: e1d_p !< prognostic value of tke (1d-model) |
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[2696] | 231 | REAL(wp), DIMENSION(:), ALLOCATABLE :: kh1d !< turbulent diffusion coefficient for heat (1d-model) |
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| 232 | REAL(wp), DIMENSION(:), ALLOCATABLE :: km1d !< turbulent diffusion coefficient for momentum (1d-model) |
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| 233 | REAL(wp), DIMENSION(:), ALLOCATABLE :: l1d !< mixing length for turbulent diffusion coefficients (1d-model) |
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[2918] | 234 | REAL(wp), DIMENSION(:), ALLOCATABLE :: l1d_init !< initial mixing length (1d-model) |
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[2338] | 235 | REAL(wp), DIMENSION(:), ALLOCATABLE :: l1d_diss !< mixing length for dissipation (1d-model) |
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[2696] | 236 | REAL(wp), DIMENSION(:), ALLOCATABLE :: rif1d !< Richardson flux number (1d-model) |
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| 237 | REAL(wp), DIMENSION(:), ALLOCATABLE :: te_diss !< tendency of diss (1d-model) |
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| 238 | REAL(wp), DIMENSION(:), ALLOCATABLE :: te_dissm !< weighted tendency of diss for previous sub-timestep (1d-model) |
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[2338] | 239 | REAL(wp), DIMENSION(:), ALLOCATABLE :: te_e !< tendency of e (1d-model) |
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| 240 | REAL(wp), DIMENSION(:), ALLOCATABLE :: te_em !< weighted tendency of e for previous sub-timestep (1d-model) |
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| 241 | REAL(wp), DIMENSION(:), ALLOCATABLE :: te_u !< tendency of u (1d-model) |
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| 242 | REAL(wp), DIMENSION(:), ALLOCATABLE :: te_um !< weighted tendency of u for previous sub-timestep (1d-model) |
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| 243 | REAL(wp), DIMENSION(:), ALLOCATABLE :: te_v !< tendency of v (1d-model) |
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| 244 | REAL(wp), DIMENSION(:), ALLOCATABLE :: te_vm !< weighted tendency of v for previous sub-timestep (1d-model) |
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[2696] | 245 | REAL(wp), DIMENSION(:), ALLOCATABLE :: u1d !< u-velocity component (1d-model) |
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[2338] | 246 | REAL(wp), DIMENSION(:), ALLOCATABLE :: u1d_p !< prognostic value of u-velocity component (1d-model) |
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[2696] | 247 | REAL(wp), DIMENSION(:), ALLOCATABLE :: v1d !< v-velocity component (1d-model) |
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[2338] | 248 | REAL(wp), DIMENSION(:), ALLOCATABLE :: v1d_p !< prognostic value of v-velocity component (1d-model) |
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| 249 | |
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| 250 | ! |
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| 251 | !-- Initialize 1D model |
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| 252 | INTERFACE init_1d_model |
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| 253 | MODULE PROCEDURE init_1d_model |
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| 254 | END INTERFACE init_1d_model |
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| 255 | |
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| 256 | ! |
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| 257 | !-- Print profiles |
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| 258 | INTERFACE print_1d_model |
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| 259 | MODULE PROCEDURE print_1d_model |
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| 260 | END INTERFACE print_1d_model |
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| 261 | |
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| 262 | ! |
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| 263 | !-- Print run control information |
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| 264 | INTERFACE run_control_1d |
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| 265 | MODULE PROCEDURE run_control_1d |
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| 266 | END INTERFACE run_control_1d |
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| 267 | |
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| 268 | ! |
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| 269 | !-- Main procedure |
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| 270 | INTERFACE time_integration_1d |
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| 271 | MODULE PROCEDURE time_integration_1d |
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| 272 | END INTERFACE time_integration_1d |
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| 273 | |
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| 274 | ! |
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| 275 | !-- Calculate time step |
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| 276 | INTERFACE timestep_1d |
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| 277 | MODULE PROCEDURE timestep_1d |
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| 278 | END INTERFACE timestep_1d |
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| 279 | |
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| 280 | SAVE |
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| 281 | |
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| 282 | PRIVATE |
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| 283 | ! |
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| 284 | !-- Public interfaces |
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| 285 | PUBLIC init_1d_model |
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| 286 | |
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| 287 | ! |
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| 288 | !-- Public variables |
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[2696] | 289 | PUBLIC damp_level_1d, damp_level_ind_1d, diss1d, dt_pr_1d, & |
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| 290 | dt_run_control_1d, e1d, end_time_1d, kh1d, km1d, l1d, rif1d, u1d, & |
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| 291 | us1d, usws1d, v1d, vsws1d |
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[2338] | 292 | |
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| 293 | |
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| 294 | CONTAINS |
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| 295 | |
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| 296 | SUBROUTINE init_1d_model |
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| 297 | |
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[2918] | 298 | USE grid_variables, & |
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| 299 | ONLY: dx, dy |
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| 300 | |
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[2338] | 301 | IMPLICIT NONE |
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| 302 | |
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[2696] | 303 | CHARACTER (LEN=9) :: time_to_string !< function to transform time from real to character string |
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| 304 | |
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| 305 | INTEGER(iwp) :: k !< loop index |
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[1] | 306 | |
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| 307 | ! |
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| 308 | !-- Allocate required 1D-arrays |
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[2696] | 309 | ALLOCATE( diss1d(nzb:nzt+1), diss1d_p(nzb:nzt+1), & |
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| 310 | e1d(nzb:nzt+1), e1d_p(nzb:nzt+1), kh1d(nzb:nzt+1), & |
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[2918] | 311 | km1d(nzb:nzt+1), l1d(nzb:nzt+1), l1d_init(nzb:nzt+1), & |
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[2696] | 312 | l1d_diss(nzb:nzt+1), rif1d(nzb:nzt+1), te_diss(nzb:nzt+1), & |
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| 313 | te_dissm(nzb:nzt+1), te_e(nzb:nzt+1), & |
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[2338] | 314 | te_em(nzb:nzt+1), te_u(nzb:nzt+1), te_um(nzb:nzt+1), & |
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| 315 | te_v(nzb:nzt+1), te_vm(nzb:nzt+1), u1d(nzb:nzt+1), & |
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| 316 | u1d_p(nzb:nzt+1), v1d(nzb:nzt+1), v1d_p(nzb:nzt+1) ) |
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[1] | 317 | |
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| 318 | ! |
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| 319 | !-- Initialize arrays |
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| 320 | IF ( constant_diffusion ) THEN |
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[1001] | 321 | km1d = km_constant |
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| 322 | kh1d = km_constant / prandtl_number |
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[1] | 323 | ELSE |
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[2696] | 324 | diss1d = 0.0_wp; diss1d_p = 0.0_wp |
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[1353] | 325 | e1d = 0.0_wp; e1d_p = 0.0_wp |
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| 326 | kh1d = 0.0_wp; km1d = 0.0_wp |
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| 327 | rif1d = 0.0_wp |
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[1] | 328 | ! |
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| 329 | !-- Compute the mixing length |
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[2918] | 330 | l1d_init(nzb) = 0.0_wp |
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[1] | 331 | |
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| 332 | IF ( TRIM( mixing_length_1d ) == 'blackadar' ) THEN |
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| 333 | ! |
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| 334 | !-- Blackadar mixing length |
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[1353] | 335 | IF ( f /= 0.0_wp ) THEN |
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| 336 | lambda = 2.7E-4_wp * SQRT( ug(nzt+1)**2 + vg(nzt+1)**2 ) / & |
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| 337 | ABS( f ) + 1E-10_wp |
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[1] | 338 | ELSE |
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[1353] | 339 | lambda = 30.0_wp |
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[1] | 340 | ENDIF |
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| 341 | |
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| 342 | DO k = nzb+1, nzt+1 |
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[2918] | 343 | l1d_init(k) = kappa * zu(k) / ( 1.0_wp + kappa * zu(k) / lambda ) |
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[1] | 344 | ENDDO |
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| 345 | |
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| 346 | ELSEIF ( TRIM( mixing_length_1d ) == 'as_in_3d_model' ) THEN |
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| 347 | ! |
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[2918] | 348 | !-- Use the same mixing length as in 3D model (LES-mode) |
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[3083] | 349 | !> @todo rename (delete?) this option |
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| 350 | !> As the mixing length is different between RANS and LES mode, it |
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| 351 | !> must be distinguished here between these modes. For RANS mode, |
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| 352 | !> the mixing length is calculated accoding to Blackadar, which is |
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| 353 | !> the other option at this point. |
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| 354 | !> Maybe delete this option entirely (not appropriate in LES case) |
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| 355 | !> 2018-03-20, gronemeier |
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[2918] | 356 | DO k = nzb+1, nzt |
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| 357 | l1d_init(k) = ( dx * dy * dzw(k) )**0.33333333333333_wp |
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| 358 | ENDDO |
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| 359 | l1d_init(nzt+1) = l1d_init(nzt) |
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[1] | 360 | |
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| 361 | ENDIF |
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| 362 | ENDIF |
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[2918] | 363 | l1d = l1d_init |
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| 364 | l1d_diss = l1d_init |
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[2337] | 365 | u1d = u_init |
---|
| 366 | u1d_p = u_init |
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| 367 | v1d = v_init |
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| 368 | v1d_p = v_init |
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[1] | 369 | |
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| 370 | ! |
---|
| 371 | !-- Set initial horizontal velocities at the lowest grid levels to a very small |
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| 372 | !-- value in order to avoid too small time steps caused by the diffusion limit |
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| 373 | !-- in the initial phase of a run (at k=1, dz/2 occurs in the limiting formula!) |
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[1353] | 374 | u1d(0:1) = 0.1_wp |
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| 375 | u1d_p(0:1) = 0.1_wp |
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| 376 | v1d(0:1) = 0.1_wp |
---|
| 377 | v1d_p(0:1) = 0.1_wp |
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[1] | 378 | |
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| 379 | ! |
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| 380 | !-- For u*, theta* and the momentum fluxes plausible values are set |
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[1691] | 381 | IF ( constant_flux_layer ) THEN |
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[1353] | 382 | us1d = 0.1_wp ! without initial friction the flow would not change |
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[1] | 383 | ELSE |
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[3083] | 384 | diss1d(nzb+1) = 0.001_wp |
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[1353] | 385 | e1d(nzb+1) = 1.0_wp |
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| 386 | km1d(nzb+1) = 1.0_wp |
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| 387 | us1d = 0.0_wp |
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[1] | 388 | ENDIF |
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[1353] | 389 | ts1d = 0.0_wp |
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| 390 | usws1d = 0.0_wp |
---|
| 391 | vsws1d = 0.0_wp |
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[996] | 392 | z01d = roughness_length |
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[978] | 393 | z0h1d = z0h_factor * z01d |
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[1960] | 394 | IF ( humidity ) qs1d = 0.0_wp |
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[1] | 395 | |
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| 396 | ! |
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[3083] | 397 | !-- Tendencies must be preset in order to avoid runtime errors |
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| 398 | te_diss = 0.0_wp |
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[2696] | 399 | te_dissm = 0.0_wp |
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[3083] | 400 | te_e = 0.0_wp |
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[1353] | 401 | te_em = 0.0_wp |
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| 402 | te_um = 0.0_wp |
---|
| 403 | te_vm = 0.0_wp |
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[46] | 404 | |
---|
| 405 | ! |
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[2338] | 406 | !-- Set model constant |
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[3083] | 407 | IF ( dissipation_1d == 'as_in_3d_model' ) c_0 = 0.1_wp |
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| 408 | c_mu = c_0**4 |
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[2338] | 409 | |
---|
| 410 | ! |
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[1] | 411 | !-- Set start time in hh:mm:ss - format |
---|
| 412 | simulated_time_chr = time_to_string( simulated_time_1d ) |
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| 413 | |
---|
| 414 | ! |
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[2337] | 415 | !-- Integrate the 1D-model equations using the Runge-Kutta scheme |
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[1] | 416 | CALL time_integration_1d |
---|
| 417 | |
---|
| 418 | |
---|
| 419 | END SUBROUTINE init_1d_model |
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| 420 | |
---|
| 421 | |
---|
| 422 | |
---|
| 423 | !------------------------------------------------------------------------------! |
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| 424 | ! Description: |
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| 425 | ! ------------ |
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[2338] | 426 | !> Runge-Kutta time differencing scheme for the 1D-model. |
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[1] | 427 | !------------------------------------------------------------------------------! |
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[1682] | 428 | |
---|
| 429 | SUBROUTINE time_integration_1d |
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[1] | 430 | |
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| 431 | IMPLICIT NONE |
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| 432 | |
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[2696] | 433 | CHARACTER (LEN=9) :: time_to_string !< function to transform time from real to character string |
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| 434 | |
---|
[2338] | 435 | INTEGER(iwp) :: k !< loop index |
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[2696] | 436 | |
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[2338] | 437 | REAL(wp) :: a !< auxiliary variable |
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| 438 | REAL(wp) :: b !< auxiliary variable |
---|
| 439 | REAL(wp) :: dpt_dz !< vertical temperature gradient |
---|
| 440 | REAL(wp) :: flux !< vertical temperature gradient |
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| 441 | REAL(wp) :: kmzm !< Km(z-dz/2) |
---|
| 442 | REAL(wp) :: kmzp !< Km(z+dz/2) |
---|
| 443 | REAL(wp) :: l_stable !< mixing length for stable case |
---|
| 444 | REAL(wp) :: pt_0 !< reference temperature |
---|
| 445 | REAL(wp) :: uv_total !< horizontal wind speed |
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[1] | 446 | |
---|
| 447 | ! |
---|
| 448 | !-- Determine the time step at the start of a 1D-simulation and |
---|
| 449 | !-- determine and printout quantities used for run control |
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[3083] | 450 | dt_1d = 0.01_wp |
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[1] | 451 | CALL run_control_1d |
---|
| 452 | |
---|
| 453 | ! |
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| 454 | !-- Start of time loop |
---|
| 455 | DO WHILE ( simulated_time_1d < end_time_1d .AND. .NOT. stop_dt_1d ) |
---|
| 456 | |
---|
| 457 | ! |
---|
| 458 | !-- Depending on the timestep scheme, carry out one or more intermediate |
---|
| 459 | !-- timesteps |
---|
| 460 | |
---|
| 461 | intermediate_timestep_count = 0 |
---|
| 462 | DO WHILE ( intermediate_timestep_count < & |
---|
| 463 | intermediate_timestep_count_max ) |
---|
| 464 | |
---|
| 465 | intermediate_timestep_count = intermediate_timestep_count + 1 |
---|
| 466 | |
---|
| 467 | CALL timestep_scheme_steering |
---|
| 468 | |
---|
| 469 | ! |
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[2696] | 470 | !-- Compute all tendency terms. If a constant-flux layer is simulated, |
---|
| 471 | !-- k starts at nzb+2. |
---|
[1] | 472 | DO k = nzb_diff, nzt |
---|
| 473 | |
---|
[1353] | 474 | kmzm = 0.5_wp * ( km1d(k-1) + km1d(k) ) |
---|
| 475 | kmzp = 0.5_wp * ( km1d(k) + km1d(k+1) ) |
---|
[1] | 476 | ! |
---|
| 477 | !-- u-component |
---|
| 478 | te_u(k) = f * ( v1d(k) - vg(k) ) + ( & |
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[1001] | 479 | kmzp * ( u1d(k+1) - u1d(k) ) * ddzu(k+1) & |
---|
| 480 | - kmzm * ( u1d(k) - u1d(k-1) ) * ddzu(k) & |
---|
| 481 | ) * ddzw(k) |
---|
[1] | 482 | ! |
---|
| 483 | !-- v-component |
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[1001] | 484 | te_v(k) = -f * ( u1d(k) - ug(k) ) + ( & |
---|
| 485 | kmzp * ( v1d(k+1) - v1d(k) ) * ddzu(k+1) & |
---|
| 486 | - kmzm * ( v1d(k) - v1d(k-1) ) * ddzu(k) & |
---|
| 487 | ) * ddzw(k) |
---|
[1] | 488 | ENDDO |
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| 489 | IF ( .NOT. constant_diffusion ) THEN |
---|
| 490 | DO k = nzb_diff, nzt |
---|
| 491 | ! |
---|
[2696] | 492 | !-- TKE and dissipation rate |
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[1353] | 493 | kmzm = 0.5_wp * ( km1d(k-1) + km1d(k) ) |
---|
| 494 | kmzp = 0.5_wp * ( km1d(k) + km1d(k+1) ) |
---|
[75] | 495 | IF ( .NOT. humidity ) THEN |
---|
[1] | 496 | pt_0 = pt_init(k) |
---|
| 497 | flux = ( pt_init(k+1)-pt_init(k-1) ) * dd2zu(k) |
---|
| 498 | ELSE |
---|
[1353] | 499 | pt_0 = pt_init(k) * ( 1.0_wp + 0.61_wp * q_init(k) ) |
---|
| 500 | flux = ( ( pt_init(k+1) - pt_init(k-1) ) + & |
---|
[2337] | 501 | 0.61_wp * ( pt_init(k+1) * q_init(k+1) - & |
---|
| 502 | pt_init(k-1) * q_init(k-1) ) & |
---|
| 503 | ) * dd2zu(k) |
---|
[1] | 504 | ENDIF |
---|
| 505 | |
---|
[2696] | 506 | ! |
---|
| 507 | !-- Calculate dissipation rate if no prognostic equation is used for |
---|
| 508 | !-- dissipation rate |
---|
[1] | 509 | IF ( dissipation_1d == 'detering' ) THEN |
---|
[3083] | 510 | diss1d(k) = c_0**3 * e1d(k) * SQRT( e1d(k) ) / l1d_diss(k) |
---|
[1] | 511 | ELSEIF ( dissipation_1d == 'as_in_3d_model' ) THEN |
---|
[2918] | 512 | diss1d(k) = ( 0.19_wp + 0.74_wp * l1d_diss(k) / l1d_init(k) & |
---|
[2696] | 513 | ) * e1d(k) * SQRT( e1d(k) ) / l1d_diss(k) |
---|
[1] | 514 | ENDIF |
---|
[2696] | 515 | ! |
---|
| 516 | !-- TKE |
---|
[1] | 517 | te_e(k) = km1d(k) * ( ( ( u1d(k+1) - u1d(k-1) ) * dd2zu(k) )**2& |
---|
| 518 | + ( ( v1d(k+1) - v1d(k-1) ) * dd2zu(k) )**2& |
---|
| 519 | ) & |
---|
| 520 | - g / pt_0 * kh1d(k) * flux & |
---|
| 521 | + ( & |
---|
[1001] | 522 | kmzp * ( e1d(k+1) - e1d(k) ) * ddzu(k+1) & |
---|
| 523 | - kmzm * ( e1d(k) - e1d(k-1) ) * ddzu(k) & |
---|
[3083] | 524 | ) * ddzw(k) / sig_e & |
---|
[2696] | 525 | - diss1d(k) |
---|
| 526 | |
---|
| 527 | IF ( dissipation_1d == 'prognostic' ) THEN |
---|
| 528 | ! |
---|
| 529 | !-- dissipation rate |
---|
[3083] | 530 | IF ( rif1d(k) >= 0.0_wp ) THEN |
---|
| 531 | alpha_buoyancy = 1.0_wp - l1d(k) / lambda |
---|
| 532 | ELSE |
---|
| 533 | alpha_buoyancy = 1.0_wp - ( 1.0_wp + ( c_2 - 1.0_wp ) & |
---|
| 534 | / ( c_2 - c_1 ) ) & |
---|
| 535 | * l1d(k) / lambda |
---|
| 536 | ENDIF |
---|
[3135] | 537 | c_3 = ( c_1 - c_2 ) * alpha_buoyancy + 1.0_wp |
---|
[3083] | 538 | te_diss(k) = ( km1d(k) * & |
---|
[2696] | 539 | ( ( ( u1d(k+1) - u1d(k-1) ) * dd2zu(k) )**2 & |
---|
| 540 | + ( ( v1d(k+1) - v1d(k-1) ) * dd2zu(k) )**2 & |
---|
[3083] | 541 | ) * ( c_1 + (c_2 - c_1) * l1d(k) / lambda ) & |
---|
[2696] | 542 | - g / pt_0 * kh1d(k) * flux * c_3 & |
---|
[3083] | 543 | - c_2 * diss1d(k) & |
---|
| 544 | ) * diss1d(k) / ( e1d(k) + 1.0E-20_wp ) & |
---|
| 545 | + ( kmzp * ( diss1d(k+1) - diss1d(k) ) & |
---|
[2696] | 546 | * ddzu(k+1) & |
---|
| 547 | - kmzm * ( diss1d(k) - diss1d(k-1) ) & |
---|
| 548 | * ddzu(k) & |
---|
[3083] | 549 | ) * ddzw(k) / sig_diss |
---|
[2696] | 550 | |
---|
| 551 | ENDIF |
---|
| 552 | |
---|
[1] | 553 | ENDDO |
---|
| 554 | ENDIF |
---|
| 555 | |
---|
| 556 | ! |
---|
[2696] | 557 | !-- Tendency terms at the top of the constant-flux layer. |
---|
[1] | 558 | !-- Finite differences of the momentum fluxes are computed using half the |
---|
| 559 | !-- normal grid length (2.0*ddzw(k)) for the sake of enhanced accuracy |
---|
[1691] | 560 | IF ( constant_flux_layer ) THEN |
---|
[1] | 561 | |
---|
| 562 | k = nzb+1 |
---|
[1353] | 563 | kmzm = 0.5_wp * ( km1d(k-1) + km1d(k) ) |
---|
| 564 | kmzp = 0.5_wp * ( km1d(k) + km1d(k+1) ) |
---|
[75] | 565 | IF ( .NOT. humidity ) THEN |
---|
[1] | 566 | pt_0 = pt_init(k) |
---|
| 567 | flux = ( pt_init(k+1)-pt_init(k-1) ) * dd2zu(k) |
---|
| 568 | ELSE |
---|
[1353] | 569 | pt_0 = pt_init(k) * ( 1.0_wp + 0.61_wp * q_init(k) ) |
---|
| 570 | flux = ( ( pt_init(k+1) - pt_init(k-1) ) + & |
---|
[2337] | 571 | 0.61_wp * ( pt_init(k+1) * q_init(k+1) - & |
---|
| 572 | pt_init(k-1) * q_init(k-1) ) & |
---|
[1] | 573 | ) * dd2zu(k) |
---|
| 574 | ENDIF |
---|
| 575 | |
---|
[2696] | 576 | ! |
---|
| 577 | !-- Calculate dissipation rate if no prognostic equation is used for |
---|
| 578 | !-- dissipation rate |
---|
[1] | 579 | IF ( dissipation_1d == 'detering' ) THEN |
---|
[3083] | 580 | diss1d(k) = c_0**3 * e1d(k) * SQRT( e1d(k) ) / l1d_diss(k) |
---|
[1] | 581 | ELSEIF ( dissipation_1d == 'as_in_3d_model' ) THEN |
---|
[2918] | 582 | diss1d(k) = ( 0.19_wp + 0.74_wp * l1d_diss(k) / l1d_init(k) ) & |
---|
[2696] | 583 | * e1d(k) * SQRT( e1d(k) ) / l1d_diss(k) |
---|
[1] | 584 | ENDIF |
---|
| 585 | |
---|
| 586 | ! |
---|
| 587 | !-- u-component |
---|
[1001] | 588 | te_u(k) = f * ( v1d(k) - vg(k) ) + ( & |
---|
| 589 | kmzp * ( u1d(k+1) - u1d(k) ) * ddzu(k+1) + usws1d & |
---|
[1353] | 590 | ) * 2.0_wp * ddzw(k) |
---|
[1] | 591 | ! |
---|
| 592 | !-- v-component |
---|
[1001] | 593 | te_v(k) = -f * ( u1d(k) - ug(k) ) + ( & |
---|
| 594 | kmzp * ( v1d(k+1) - v1d(k) ) * ddzu(k+1) + vsws1d & |
---|
[1353] | 595 | ) * 2.0_wp * ddzw(k) |
---|
[1] | 596 | ! |
---|
| 597 | !-- TKE |
---|
[2696] | 598 | IF ( .NOT. dissipation_1d == 'prognostic' ) THEN |
---|
[3083] | 599 | !> @query why integrate over 2dz |
---|
| 600 | !> Why is it allowed to integrate over two delta-z for e |
---|
| 601 | !> while for u and v it is not? |
---|
| 602 | !> 2018-04-23, gronemeier |
---|
[2696] | 603 | te_e(k) = km1d(k) * ( ( ( u1d(k+1) - u1d(k-1) ) * dd2zu(k) )**2& |
---|
| 604 | + ( ( v1d(k+1) - v1d(k-1) ) * dd2zu(k) )**2& |
---|
| 605 | ) & |
---|
| 606 | - g / pt_0 * kh1d(k) * flux & |
---|
| 607 | + ( & |
---|
| 608 | kmzp * ( e1d(k+1) - e1d(k) ) * ddzu(k+1) & |
---|
| 609 | - kmzm * ( e1d(k) - e1d(k-1) ) * ddzu(k) & |
---|
[3083] | 610 | ) * ddzw(k) / sig_e & |
---|
[2696] | 611 | - diss1d(k) |
---|
| 612 | ENDIF |
---|
| 613 | |
---|
[1] | 614 | ENDIF |
---|
| 615 | |
---|
| 616 | ! |
---|
| 617 | !-- Prognostic equations for all 1D variables |
---|
| 618 | DO k = nzb+1, nzt |
---|
| 619 | |
---|
[1001] | 620 | u1d_p(k) = u1d(k) + dt_1d * ( tsc(2) * te_u(k) + & |
---|
| 621 | tsc(3) * te_um(k) ) |
---|
| 622 | v1d_p(k) = v1d(k) + dt_1d * ( tsc(2) * te_v(k) + & |
---|
| 623 | tsc(3) * te_vm(k) ) |
---|
[1] | 624 | |
---|
| 625 | ENDDO |
---|
| 626 | IF ( .NOT. constant_diffusion ) THEN |
---|
[2696] | 627 | |
---|
[1] | 628 | DO k = nzb+1, nzt |
---|
[1001] | 629 | e1d_p(k) = e1d(k) + dt_1d * ( tsc(2) * te_e(k) + & |
---|
| 630 | tsc(3) * te_em(k) ) |
---|
[2696] | 631 | ENDDO |
---|
[1] | 632 | |
---|
| 633 | ! |
---|
| 634 | !-- Eliminate negative TKE values, which can result from the |
---|
| 635 | !-- integration due to numerical inaccuracies. In such cases the TKE |
---|
| 636 | !-- value is reduced to 10 percent of its old value. |
---|
[1353] | 637 | WHERE ( e1d_p < 0.0_wp ) e1d_p = 0.1_wp * e1d |
---|
[3083] | 638 | |
---|
| 639 | IF ( dissipation_1d == 'prognostic' ) THEN |
---|
| 640 | DO k = nzb+1, nzt |
---|
| 641 | diss1d_p(k) = diss1d(k) + dt_1d * ( tsc(2) * te_diss(k) + & |
---|
| 642 | tsc(3) * te_dissm(k) ) |
---|
| 643 | ENDDO |
---|
| 644 | WHERE ( diss1d_p < 0.0_wp ) diss1d_p = 0.1_wp * diss1d |
---|
| 645 | ENDIF |
---|
[1] | 646 | ENDIF |
---|
| 647 | |
---|
| 648 | ! |
---|
| 649 | !-- Calculate tendencies for the next Runge-Kutta step |
---|
| 650 | IF ( timestep_scheme(1:5) == 'runge' ) THEN |
---|
| 651 | IF ( intermediate_timestep_count == 1 ) THEN |
---|
| 652 | |
---|
| 653 | DO k = nzb+1, nzt |
---|
| 654 | te_um(k) = te_u(k) |
---|
| 655 | te_vm(k) = te_v(k) |
---|
| 656 | ENDDO |
---|
| 657 | |
---|
| 658 | IF ( .NOT. constant_diffusion ) THEN |
---|
| 659 | DO k = nzb+1, nzt |
---|
| 660 | te_em(k) = te_e(k) |
---|
| 661 | ENDDO |
---|
[2696] | 662 | IF ( dissipation_1d == 'prognostic' ) THEN |
---|
| 663 | DO k = nzb+1, nzt |
---|
| 664 | te_dissm(k) = te_diss(k) |
---|
| 665 | ENDDO |
---|
| 666 | ENDIF |
---|
[1] | 667 | ENDIF |
---|
| 668 | |
---|
| 669 | ELSEIF ( intermediate_timestep_count < & |
---|
| 670 | intermediate_timestep_count_max ) THEN |
---|
| 671 | |
---|
| 672 | DO k = nzb+1, nzt |
---|
[1353] | 673 | te_um(k) = -9.5625_wp * te_u(k) + 5.3125_wp * te_um(k) |
---|
| 674 | te_vm(k) = -9.5625_wp * te_v(k) + 5.3125_wp * te_vm(k) |
---|
[1] | 675 | ENDDO |
---|
| 676 | |
---|
| 677 | IF ( .NOT. constant_diffusion ) THEN |
---|
| 678 | DO k = nzb+1, nzt |
---|
[1353] | 679 | te_em(k) = -9.5625_wp * te_e(k) + 5.3125_wp * te_em(k) |
---|
[1] | 680 | ENDDO |
---|
[2696] | 681 | IF ( dissipation_1d == 'prognostic' ) THEN |
---|
| 682 | DO k = nzb+1, nzt |
---|
[3083] | 683 | te_dissm(k) = -9.5625_wp * te_diss(k) & |
---|
| 684 | + 5.3125_wp * te_dissm(k) |
---|
[2696] | 685 | ENDDO |
---|
| 686 | ENDIF |
---|
[1] | 687 | ENDIF |
---|
| 688 | |
---|
| 689 | ENDIF |
---|
| 690 | ENDIF |
---|
| 691 | |
---|
| 692 | ! |
---|
| 693 | !-- Boundary conditions for the prognostic variables. |
---|
[2696] | 694 | !-- At the top boundary (nzt+1) u, v, e, and diss keep their initial |
---|
| 695 | !-- values (ug(nzt+1), vg(nzt+1), 0, 0). |
---|
[2334] | 696 | !-- At the bottom boundary, Dirichlet condition is used for u and v (0) |
---|
[2696] | 697 | !-- and Neumann condition for e and diss (e(nzb)=e(nzb+1)). |
---|
[1353] | 698 | u1d_p(nzb) = 0.0_wp |
---|
| 699 | v1d_p(nzb) = 0.0_wp |
---|
[667] | 700 | |
---|
[1] | 701 | ! |
---|
| 702 | !-- Swap the time levels in preparation for the next time step. |
---|
| 703 | u1d = u1d_p |
---|
| 704 | v1d = v1d_p |
---|
| 705 | IF ( .NOT. constant_diffusion ) THEN |
---|
| 706 | e1d = e1d_p |
---|
[2696] | 707 | IF ( dissipation_1d == 'prognostic' ) THEN |
---|
| 708 | diss1d = diss1d_p |
---|
| 709 | ENDIF |
---|
[1] | 710 | ENDIF |
---|
| 711 | |
---|
| 712 | ! |
---|
| 713 | !-- Compute diffusion quantities |
---|
| 714 | IF ( .NOT. constant_diffusion ) THEN |
---|
| 715 | |
---|
| 716 | ! |
---|
[2696] | 717 | !-- First compute the vertical fluxes in the constant-flux layer |
---|
[1691] | 718 | IF ( constant_flux_layer ) THEN |
---|
[1] | 719 | ! |
---|
| 720 | !-- Compute theta* using Rif numbers of the previous time step |
---|
[2334] | 721 | IF ( rif1d(nzb+1) >= 0.0_wp ) THEN |
---|
[1] | 722 | ! |
---|
| 723 | !-- Stable stratification |
---|
[1353] | 724 | ts1d = kappa * ( pt_init(nzb+1) - pt_init(nzb) ) / & |
---|
| 725 | ( LOG( zu(nzb+1) / z0h1d ) + 5.0_wp * rif1d(nzb+1) * & |
---|
| 726 | ( zu(nzb+1) - z0h1d ) / zu(nzb+1) & |
---|
[1] | 727 | ) |
---|
| 728 | ELSE |
---|
| 729 | ! |
---|
| 730 | !-- Unstable stratification |
---|
[1353] | 731 | a = SQRT( 1.0_wp - 16.0_wp * rif1d(nzb+1) ) |
---|
| 732 | b = SQRT( 1.0_wp - 16.0_wp * rif1d(nzb+1) / & |
---|
| 733 | zu(nzb+1) * z0h1d ) |
---|
[2337] | 734 | |
---|
| 735 | ts1d = kappa * ( pt_init(nzb+1) - pt_init(nzb) ) / & |
---|
| 736 | LOG( (a-1.0_wp) / (a+1.0_wp) * & |
---|
| 737 | (b+1.0_wp) / (b-1.0_wp) ) |
---|
[1] | 738 | ENDIF |
---|
| 739 | |
---|
[1691] | 740 | ENDIF ! constant_flux_layer |
---|
[3083] | 741 | !> @todo combine if clauses |
---|
| 742 | !> The previous and following if clauses can be combined into a |
---|
| 743 | !> single clause |
---|
| 744 | !> 2018-04-23, gronemeier |
---|
[1] | 745 | ! |
---|
| 746 | !-- Compute the Richardson-flux numbers, |
---|
[2696] | 747 | !-- first at the top of the constant-flux layer using u* of the |
---|
| 748 | !-- previous time step (+1E-30, if u* = 0), then in the remaining area. |
---|
| 749 | !-- There the rif-numbers of the previous time step are used. |
---|
[1] | 750 | |
---|
[1691] | 751 | IF ( constant_flux_layer ) THEN |
---|
[75] | 752 | IF ( .NOT. humidity ) THEN |
---|
[1] | 753 | pt_0 = pt_init(nzb+1) |
---|
| 754 | flux = ts1d |
---|
| 755 | ELSE |
---|
[1353] | 756 | pt_0 = pt_init(nzb+1) * ( 1.0_wp + 0.61_wp * q_init(nzb+1) ) |
---|
| 757 | flux = ts1d + 0.61_wp * pt_init(k) * qs1d |
---|
[1] | 758 | ENDIF |
---|
| 759 | rif1d(nzb+1) = zu(nzb+1) * kappa * g * flux / & |
---|
[1353] | 760 | ( pt_0 * ( us1d**2 + 1E-30_wp ) ) |
---|
[1] | 761 | ENDIF |
---|
| 762 | |
---|
| 763 | DO k = nzb_diff, nzt |
---|
[75] | 764 | IF ( .NOT. humidity ) THEN |
---|
[1] | 765 | pt_0 = pt_init(k) |
---|
| 766 | flux = ( pt_init(k+1) - pt_init(k-1) ) * dd2zu(k) |
---|
| 767 | ELSE |
---|
[1353] | 768 | pt_0 = pt_init(k) * ( 1.0_wp + 0.61_wp * q_init(k) ) |
---|
[1] | 769 | flux = ( ( pt_init(k+1) - pt_init(k-1) ) & |
---|
[2337] | 770 | + 0.61_wp & |
---|
| 771 | * ( pt_init(k+1) * q_init(k+1) & |
---|
| 772 | - pt_init(k-1) * q_init(k-1) ) & |
---|
[1] | 773 | ) * dd2zu(k) |
---|
| 774 | ENDIF |
---|
[1353] | 775 | IF ( rif1d(k) >= 0.0_wp ) THEN |
---|
| 776 | rif1d(k) = g / pt_0 * flux / & |
---|
| 777 | ( ( ( u1d(k+1) - u1d(k-1) ) * dd2zu(k) )**2 & |
---|
| 778 | + ( ( v1d(k+1) - v1d(k-1) ) * dd2zu(k) )**2 & |
---|
| 779 | + 1E-30_wp & |
---|
[1] | 780 | ) |
---|
| 781 | ELSE |
---|
[1353] | 782 | rif1d(k) = g / pt_0 * flux / & |
---|
| 783 | ( ( ( u1d(k+1) - u1d(k-1) ) * dd2zu(k) )**2 & |
---|
| 784 | + ( ( v1d(k+1) - v1d(k-1) ) * dd2zu(k) )**2 & |
---|
| 785 | + 1E-30_wp & |
---|
| 786 | ) * ( 1.0_wp - 16.0_wp * rif1d(k) )**0.25_wp |
---|
[1] | 787 | ENDIF |
---|
| 788 | ENDDO |
---|
| 789 | ! |
---|
| 790 | !-- Richardson-numbers must remain restricted to a realistic value |
---|
| 791 | !-- range. It is exceeded excessively for very small velocities |
---|
| 792 | !-- (u,v --> 0). |
---|
[2059] | 793 | WHERE ( rif1d < -5.0_wp ) rif1d = -5.0_wp |
---|
| 794 | WHERE ( rif1d > 1.0_wp ) rif1d = 1.0_wp |
---|
[1] | 795 | |
---|
| 796 | ! |
---|
| 797 | !-- Compute u* from the absolute velocity value |
---|
[1691] | 798 | IF ( constant_flux_layer ) THEN |
---|
[1] | 799 | uv_total = SQRT( u1d(nzb+1)**2 + v1d(nzb+1)**2 ) |
---|
| 800 | |
---|
[1353] | 801 | IF ( rif1d(nzb+1) >= 0.0_wp ) THEN |
---|
[1] | 802 | ! |
---|
| 803 | !-- Stable stratification |
---|
| 804 | us1d = kappa * uv_total / ( & |
---|
[1353] | 805 | LOG( zu(nzb+1) / z01d ) + 5.0_wp * rif1d(nzb+1) * & |
---|
[1] | 806 | ( zu(nzb+1) - z01d ) / zu(nzb+1) & |
---|
| 807 | ) |
---|
| 808 | ELSE |
---|
| 809 | ! |
---|
| 810 | !-- Unstable stratification |
---|
[1353] | 811 | a = 1.0_wp / SQRT( SQRT( 1.0_wp - 16.0_wp * rif1d(nzb+1) ) ) |
---|
| 812 | b = 1.0_wp / SQRT( SQRT( 1.0_wp - 16.0_wp * rif1d(nzb+1) / & |
---|
| 813 | zu(nzb+1) * z01d ) ) |
---|
[2337] | 814 | us1d = kappa * uv_total / ( & |
---|
| 815 | LOG( (1.0_wp+b) / (1.0_wp-b) * (1.0_wp-a) / & |
---|
| 816 | (1.0_wp+a) ) + & |
---|
| 817 | 2.0_wp * ( ATAN( b ) - ATAN( a ) ) & |
---|
| 818 | ) |
---|
[1] | 819 | ENDIF |
---|
| 820 | |
---|
| 821 | ! |
---|
| 822 | !-- Compute the momentum fluxes for the diffusion terms |
---|
| 823 | usws1d = - u1d(nzb+1) / uv_total * us1d**2 |
---|
| 824 | vsws1d = - v1d(nzb+1) / uv_total * us1d**2 |
---|
| 825 | |
---|
| 826 | ! |
---|
[2696] | 827 | !-- Boundary condition for the turbulent kinetic energy and |
---|
| 828 | !-- dissipation rate at the top of the constant-flux layer. |
---|
[1] | 829 | !-- Additional Neumann condition de/dz = 0 at nzb is set to ensure |
---|
| 830 | !-- compatibility with the 3D model. |
---|
| 831 | IF ( ibc_e_b == 2 ) THEN |
---|
[3083] | 832 | e1d(nzb+1) = ( us1d / c_0 )**2 |
---|
[1] | 833 | ENDIF |
---|
[2696] | 834 | IF ( dissipation_1d == 'prognostic' ) THEN |
---|
[3083] | 835 | e1d(nzb+1) = ( us1d / c_0 )**2 |
---|
[2696] | 836 | diss1d(nzb+1) = us1d**3 / ( kappa * zu(nzb+1) ) |
---|
| 837 | diss1d(nzb) = diss1d(nzb+1) |
---|
| 838 | ENDIF |
---|
[1] | 839 | e1d(nzb) = e1d(nzb+1) |
---|
| 840 | |
---|
[1960] | 841 | IF ( humidity ) THEN |
---|
[1] | 842 | ! |
---|
| 843 | !-- Compute q* |
---|
[2334] | 844 | IF ( rif1d(nzb+1) >= 0.0_wp ) THEN |
---|
[1] | 845 | ! |
---|
[1960] | 846 | !-- Stable stratification |
---|
| 847 | qs1d = kappa * ( q_init(nzb+1) - q_init(nzb) ) / & |
---|
[1353] | 848 | ( LOG( zu(nzb+1) / z0h1d ) + 5.0_wp * rif1d(nzb+1) * & |
---|
| 849 | ( zu(nzb+1) - z0h1d ) / zu(nzb+1) & |
---|
[1] | 850 | ) |
---|
[1960] | 851 | ELSE |
---|
[1] | 852 | ! |
---|
[1960] | 853 | !-- Unstable stratification |
---|
| 854 | a = SQRT( 1.0_wp - 16.0_wp * rif1d(nzb+1) ) |
---|
| 855 | b = SQRT( 1.0_wp - 16.0_wp * rif1d(nzb+1) / & |
---|
| 856 | zu(nzb+1) * z0h1d ) |
---|
[2337] | 857 | qs1d = kappa * ( q_init(nzb+1) - q_init(nzb) ) / & |
---|
| 858 | LOG( (a-1.0_wp) / (a+1.0_wp) * & |
---|
| 859 | (b+1.0_wp) / (b-1.0_wp) ) |
---|
| 860 | ENDIF |
---|
[1] | 861 | ELSE |
---|
[1353] | 862 | qs1d = 0.0_wp |
---|
[2337] | 863 | ENDIF |
---|
[1] | 864 | |
---|
[1691] | 865 | ENDIF ! constant_flux_layer |
---|
[1] | 866 | |
---|
| 867 | ! |
---|
[2337] | 868 | !-- Compute the diabatic mixing length. The unstable stratification |
---|
| 869 | !-- must not be considered for l1d (km1d) as it is already considered |
---|
| 870 | !-- in the dissipation of TKE via l1d_diss. Otherwise, km1d would be |
---|
| 871 | !-- too large. |
---|
[3083] | 872 | IF ( dissipation_1d /= 'prognostic' ) THEN |
---|
| 873 | IF ( mixing_length_1d == 'blackadar' ) THEN |
---|
| 874 | DO k = nzb+1, nzt |
---|
| 875 | IF ( rif1d(k) >= 0.0_wp ) THEN |
---|
| 876 | l1d(k) = l1d_init(k) / ( 1.0_wp + 5.0_wp * rif1d(k) ) |
---|
| 877 | l1d_diss(k) = l1d(k) |
---|
| 878 | ELSE |
---|
| 879 | l1d(k) = l1d_init(k) |
---|
| 880 | l1d_diss(k) = l1d_init(k) * & |
---|
| 881 | SQRT( 1.0_wp - 16.0_wp * rif1d(k) ) |
---|
| 882 | ENDIF |
---|
| 883 | ENDDO |
---|
| 884 | ELSEIF ( mixing_length_1d == 'as_in_3d_model' ) THEN |
---|
| 885 | DO k = nzb+1, nzt |
---|
| 886 | dpt_dz = ( pt_init(k+1) - pt_init(k-1) ) * dd2zu(k) |
---|
| 887 | IF ( dpt_dz > 0.0_wp ) THEN |
---|
| 888 | l_stable = 0.76_wp * SQRT( e1d(k) ) & |
---|
| 889 | / SQRT( g / pt_init(k) * dpt_dz ) + 1E-5_wp |
---|
| 890 | ELSE |
---|
| 891 | l_stable = l1d_init(k) |
---|
| 892 | ENDIF |
---|
| 893 | l1d(k) = MIN( l1d_init(k), l_stable ) |
---|
[2337] | 894 | l1d_diss(k) = l1d(k) |
---|
[3083] | 895 | ENDDO |
---|
| 896 | ENDIF |
---|
| 897 | ELSE |
---|
[1] | 898 | DO k = nzb+1, nzt |
---|
[3083] | 899 | l1d(k) = c_0**3 * e1d(k) * SQRT( e1d(k) ) & |
---|
| 900 | / ( diss1d(k) + 1.0E-30_wp ) |
---|
[1] | 901 | ENDDO |
---|
| 902 | ENDIF |
---|
| 903 | |
---|
| 904 | ! |
---|
| 905 | !-- Compute the diffusion coefficients for momentum via the |
---|
| 906 | !-- corresponding Prandtl-layer relationship and according to |
---|
[2337] | 907 | !-- Prandtl-Kolmogorov, respectively |
---|
[1691] | 908 | IF ( constant_flux_layer ) THEN |
---|
[1353] | 909 | IF ( rif1d(nzb+1) >= 0.0_wp ) THEN |
---|
| 910 | km1d(nzb+1) = us1d * kappa * zu(nzb+1) / & |
---|
| 911 | ( 1.0_wp + 5.0_wp * rif1d(nzb+1) ) |
---|
[1] | 912 | ELSE |
---|
[1353] | 913 | km1d(nzb+1) = us1d * kappa * zu(nzb+1) * & |
---|
| 914 | ( 1.0_wp - 16.0_wp * rif1d(nzb+1) )**0.25_wp |
---|
[1] | 915 | ENDIF |
---|
| 916 | ENDIF |
---|
[3083] | 917 | |
---|
[2696] | 918 | IF ( dissipation_1d == 'prognostic' ) THEN |
---|
| 919 | DO k = nzb_diff, nzt |
---|
| 920 | km1d(k) = c_mu * e1d(k)**2 / ( diss1d(k) + 1.0E-30_wp ) |
---|
| 921 | ENDDO |
---|
| 922 | ELSE |
---|
| 923 | DO k = nzb_diff, nzt |
---|
[3083] | 924 | km1d(k) = c_0 * SQRT( e1d(k) ) * l1d(k) |
---|
[2696] | 925 | ENDDO |
---|
| 926 | ENDIF |
---|
[1] | 927 | |
---|
| 928 | ! |
---|
| 929 | !-- Add damping layer |
---|
| 930 | DO k = damp_level_ind_1d+1, nzt+1 |
---|
[1353] | 931 | km1d(k) = 1.1_wp * km1d(k-1) |
---|
[1346] | 932 | km1d(k) = MIN( km1d(k), 10.0_wp ) |
---|
[1] | 933 | ENDDO |
---|
| 934 | |
---|
| 935 | ! |
---|
| 936 | !-- Compute the diffusion coefficient for heat via the relationship |
---|
| 937 | !-- kh = phim / phih * km |
---|
| 938 | DO k = nzb+1, nzt |
---|
[1353] | 939 | IF ( rif1d(k) >= 0.0_wp ) THEN |
---|
[1] | 940 | kh1d(k) = km1d(k) |
---|
| 941 | ELSE |
---|
[1353] | 942 | kh1d(k) = km1d(k) * ( 1.0_wp - 16.0_wp * rif1d(k) )**0.25_wp |
---|
[1] | 943 | ENDIF |
---|
| 944 | ENDDO |
---|
| 945 | |
---|
| 946 | ENDIF ! .NOT. constant_diffusion |
---|
| 947 | |
---|
| 948 | ENDDO ! intermediate step loop |
---|
| 949 | |
---|
| 950 | ! |
---|
| 951 | !-- Increment simulated time and output times |
---|
| 952 | current_timestep_number_1d = current_timestep_number_1d + 1 |
---|
| 953 | simulated_time_1d = simulated_time_1d + dt_1d |
---|
| 954 | simulated_time_chr = time_to_string( simulated_time_1d ) |
---|
| 955 | time_pr_1d = time_pr_1d + dt_1d |
---|
| 956 | time_run_control_1d = time_run_control_1d + dt_1d |
---|
| 957 | |
---|
| 958 | ! |
---|
| 959 | !-- Determine and print out quantities for run control |
---|
| 960 | IF ( time_run_control_1d >= dt_run_control_1d ) THEN |
---|
| 961 | CALL run_control_1d |
---|
| 962 | time_run_control_1d = time_run_control_1d - dt_run_control_1d |
---|
| 963 | ENDIF |
---|
| 964 | |
---|
| 965 | ! |
---|
| 966 | !-- Profile output on file |
---|
| 967 | IF ( time_pr_1d >= dt_pr_1d ) THEN |
---|
| 968 | CALL print_1d_model |
---|
| 969 | time_pr_1d = time_pr_1d - dt_pr_1d |
---|
| 970 | ENDIF |
---|
| 971 | |
---|
| 972 | ! |
---|
| 973 | !-- Determine size of next time step |
---|
| 974 | CALL timestep_1d |
---|
| 975 | |
---|
| 976 | ENDDO ! time loop |
---|
| 977 | |
---|
| 978 | |
---|
| 979 | END SUBROUTINE time_integration_1d |
---|
| 980 | |
---|
| 981 | |
---|
| 982 | !------------------------------------------------------------------------------! |
---|
| 983 | ! Description: |
---|
| 984 | ! ------------ |
---|
[1682] | 985 | !> Compute and print out quantities for run control of the 1D model. |
---|
[1] | 986 | !------------------------------------------------------------------------------! |
---|
[1682] | 987 | |
---|
| 988 | SUBROUTINE run_control_1d |
---|
[1] | 989 | |
---|
[1682] | 990 | |
---|
[1320] | 991 | USE constants, & |
---|
| 992 | ONLY: pi |
---|
[1] | 993 | |
---|
| 994 | IMPLICIT NONE |
---|
| 995 | |
---|
[2338] | 996 | INTEGER(iwp) :: k !< loop index |
---|
[1320] | 997 | |
---|
[2338] | 998 | REAL(wp) :: alpha !< angle of wind vector at top of constant-flux layer |
---|
| 999 | REAL(wp) :: energy !< kinetic energy |
---|
| 1000 | REAL(wp) :: umax !< maximum of u |
---|
| 1001 | REAL(wp) :: uv_total !< horizontal wind speed |
---|
| 1002 | REAL(wp) :: vmax !< maximum of v |
---|
[1] | 1003 | |
---|
| 1004 | ! |
---|
| 1005 | !-- Output |
---|
| 1006 | IF ( myid == 0 ) THEN |
---|
| 1007 | ! |
---|
| 1008 | !-- If necessary, write header |
---|
| 1009 | IF ( .NOT. run_control_header_1d ) THEN |
---|
[184] | 1010 | CALL check_open( 15 ) |
---|
[1] | 1011 | WRITE ( 15, 100 ) |
---|
| 1012 | run_control_header_1d = .TRUE. |
---|
| 1013 | ENDIF |
---|
| 1014 | |
---|
| 1015 | ! |
---|
| 1016 | !-- Compute control quantities |
---|
| 1017 | !-- grid level nzp is excluded due to mirror boundary condition |
---|
[1353] | 1018 | umax = 0.0_wp; vmax = 0.0_wp; energy = 0.0_wp |
---|
[1] | 1019 | DO k = nzb+1, nzt+1 |
---|
| 1020 | umax = MAX( ABS( umax ), ABS( u1d(k) ) ) |
---|
| 1021 | vmax = MAX( ABS( vmax ), ABS( v1d(k) ) ) |
---|
[1353] | 1022 | energy = energy + 0.5_wp * ( u1d(k)**2 + v1d(k)**2 ) |
---|
[1] | 1023 | ENDDO |
---|
[1322] | 1024 | energy = energy / REAL( nzt - nzb + 1, KIND=wp ) |
---|
[1] | 1025 | |
---|
| 1026 | uv_total = SQRT( u1d(nzb+1)**2 + v1d(nzb+1)**2 ) |
---|
[1691] | 1027 | IF ( ABS( v1d(nzb+1) ) < 1.0E-5_wp ) THEN |
---|
[1346] | 1028 | alpha = ACOS( SIGN( 1.0_wp , u1d(nzb+1) ) ) |
---|
[1] | 1029 | ELSE |
---|
| 1030 | alpha = ACOS( u1d(nzb+1) / uv_total ) |
---|
[1353] | 1031 | IF ( v1d(nzb+1) <= 0.0_wp ) alpha = 2.0_wp * pi - alpha |
---|
[1] | 1032 | ENDIF |
---|
[1353] | 1033 | alpha = alpha / ( 2.0_wp * pi ) * 360.0_wp |
---|
[1] | 1034 | |
---|
| 1035 | WRITE ( 15, 101 ) current_timestep_number_1d, simulated_time_chr, & |
---|
| 1036 | dt_1d, umax, vmax, us1d, alpha, energy |
---|
| 1037 | ! |
---|
| 1038 | !-- Write buffer contents to disc immediately |
---|
[1808] | 1039 | FLUSH( 15 ) |
---|
[1] | 1040 | |
---|
| 1041 | ENDIF |
---|
| 1042 | |
---|
| 1043 | ! |
---|
| 1044 | !-- formats |
---|
[2299] | 1045 | 100 FORMAT (///'1D run control output:'/ & |
---|
[1] | 1046 | &'------------------------------'// & |
---|
[2965] | 1047 | &'ITER. HH:MM:SS DT UMAX VMAX U* ALPHA ENERG.'/ & |
---|
[1] | 1048 | &'-------------------------------------------------------------') |
---|
[2965] | 1049 | 101 FORMAT (I7,1X,A9,1X,F6.2,2X,F6.2,1X,F6.2,1X,F6.3,2X,F5.1,2X,F7.2) |
---|
[1] | 1050 | |
---|
| 1051 | |
---|
| 1052 | END SUBROUTINE run_control_1d |
---|
| 1053 | |
---|
| 1054 | |
---|
| 1055 | |
---|
| 1056 | !------------------------------------------------------------------------------! |
---|
| 1057 | ! Description: |
---|
| 1058 | ! ------------ |
---|
[1682] | 1059 | !> Compute the time step w.r.t. the diffusion criterion |
---|
[1] | 1060 | !------------------------------------------------------------------------------! |
---|
[1682] | 1061 | |
---|
| 1062 | SUBROUTINE timestep_1d |
---|
[1] | 1063 | |
---|
| 1064 | IMPLICIT NONE |
---|
| 1065 | |
---|
[2338] | 1066 | INTEGER(iwp) :: k !< loop index |
---|
[1] | 1067 | |
---|
[2338] | 1068 | REAL(wp) :: dt_diff !< time step accorind to diffusion criterion |
---|
[3083] | 1069 | REAL(wp) :: dt_old !< previous time step |
---|
[2338] | 1070 | REAL(wp) :: fac !< factor of criterion |
---|
| 1071 | REAL(wp) :: value !< auxiliary variable |
---|
[1] | 1072 | |
---|
| 1073 | ! |
---|
[3083] | 1074 | !-- Save previous time step |
---|
| 1075 | dt_old = dt_1d |
---|
| 1076 | |
---|
| 1077 | ! |
---|
[1] | 1078 | !-- Compute the currently feasible time step according to the diffusion |
---|
| 1079 | !-- criterion. At nzb+1 the half grid length is used. |
---|
[3083] | 1080 | fac = 0.125 |
---|
[1] | 1081 | dt_diff = dt_max_1d |
---|
| 1082 | DO k = nzb+2, nzt |
---|
[1353] | 1083 | value = fac * dzu(k) * dzu(k) / ( km1d(k) + 1E-20_wp ) |
---|
[1] | 1084 | dt_diff = MIN( value, dt_diff ) |
---|
| 1085 | ENDDO |
---|
[1353] | 1086 | value = fac * zu(nzb+1) * zu(nzb+1) / ( km1d(nzb+1) + 1E-20_wp ) |
---|
[1] | 1087 | dt_1d = MIN( value, dt_diff ) |
---|
| 1088 | |
---|
| 1089 | ! |
---|
[3083] | 1090 | !-- Limit the new time step to a maximum of 10 times the previous time step |
---|
| 1091 | dt_1d = MIN( dt_old * 10.0_wp, dt_1d ) |
---|
| 1092 | |
---|
| 1093 | ! |
---|
[1] | 1094 | !-- Set flag when the time step becomes too small |
---|
[3083] | 1095 | IF ( dt_1d < ( 1.0E-15_wp * dt_max_1d ) ) THEN |
---|
[1] | 1096 | stop_dt_1d = .TRUE. |
---|
[254] | 1097 | |
---|
[3046] | 1098 | WRITE( message_string, * ) 'timestep has exceeded the lower limit&', & |
---|
[254] | 1099 | 'dt_1d = ',dt_1d,' s simulation stopped!' |
---|
| 1100 | CALL message( 'timestep_1d', 'PA0192', 1, 2, 0, 6, 0 ) |
---|
| 1101 | |
---|
[1] | 1102 | ENDIF |
---|
| 1103 | |
---|
| 1104 | END SUBROUTINE timestep_1d |
---|
| 1105 | |
---|
| 1106 | |
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| 1107 | |
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| 1108 | !------------------------------------------------------------------------------! |
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| 1109 | ! Description: |
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| 1110 | ! ------------ |
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[1682] | 1111 | !> List output of profiles from the 1D-model |
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[1] | 1112 | !------------------------------------------------------------------------------! |
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[1682] | 1113 | |
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| 1114 | SUBROUTINE print_1d_model |
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[1] | 1115 | |
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| 1116 | IMPLICIT NONE |
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| 1117 | |
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[2338] | 1118 | INTEGER(iwp) :: k !< loop parameter |
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[1] | 1119 | |
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[2338] | 1120 | LOGICAL, SAVE :: write_first = .TRUE. !< flag for writing header |
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[1] | 1121 | |
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| 1122 | |
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| 1123 | IF ( myid == 0 ) THEN |
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| 1124 | ! |
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| 1125 | !-- Open list output file for profiles from the 1D-model |
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| 1126 | CALL check_open( 17 ) |
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| 1127 | |
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| 1128 | ! |
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| 1129 | !-- Write Header |
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[2338] | 1130 | IF ( write_first ) THEN |
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| 1131 | WRITE ( 17, 100 ) TRIM( run_description_header ) |
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| 1132 | write_first = .FALSE. |
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| 1133 | ENDIF |
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[1] | 1134 | |
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| 1135 | ! |
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| 1136 | !-- Write the values |
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[2338] | 1137 | WRITE ( 17, 104 ) TRIM( simulated_time_chr ) |
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| 1138 | WRITE ( 17, 101 ) |
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[1] | 1139 | WRITE ( 17, 102 ) |
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| 1140 | WRITE ( 17, 101 ) |
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| 1141 | DO k = nzt+1, nzb, -1 |
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| 1142 | WRITE ( 17, 103) k, zu(k), u1d(k), v1d(k), pt_init(k), e1d(k), & |
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[2696] | 1143 | rif1d(k), km1d(k), kh1d(k), l1d(k), diss1d(k) |
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[1] | 1144 | ENDDO |
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| 1145 | WRITE ( 17, 101 ) |
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| 1146 | WRITE ( 17, 102 ) |
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| 1147 | WRITE ( 17, 101 ) |
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| 1148 | |
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| 1149 | ! |
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| 1150 | !-- Write buffer contents to disc immediately |
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[1808] | 1151 | FLUSH( 17 ) |
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[1] | 1152 | |
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| 1153 | ENDIF |
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| 1154 | |
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| 1155 | ! |
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| 1156 | !-- Formats |
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[2338] | 1157 | 100 FORMAT ('# ',A/'#',10('-')/'# 1d-model profiles') |
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| 1158 | 104 FORMAT (//'# Time: ',A) |
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[2696] | 1159 | 101 FORMAT ('#',111('-')) |
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| 1160 | 102 FORMAT ('# k zu u v pt e ', & |
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| 1161 | 'rif Km Kh l diss ') |
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| 1162 | 103 FORMAT (1X,I4,1X,F7.1,9(1X,E10.3)) |
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[1] | 1163 | |
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| 1164 | |
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| 1165 | END SUBROUTINE print_1d_model |
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[2338] | 1166 | |
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| 1167 | |
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[3045] | 1168 | END MODULE |
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