[1850] | 1 | !> @file surface_layer_fluxes_mod.f90 |
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[2000] | 2 | !------------------------------------------------------------------------------! |
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[1691] | 3 | ! This file is part of PALM. |
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| 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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[1691] | 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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[2101] | 17 | ! Copyright 1997-2017 Leibniz Universitaet Hannover |
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[1691] | 18 | ! |
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[2000] | 19 | !------------------------------------------------------------------------------! |
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[1691] | 20 | ! Current revisions: |
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[1747] | 21 | ! ------------------ |
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[1758] | 22 | ! |
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[2233] | 23 | ! |
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[1692] | 24 | ! Former revisions: |
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| 25 | ! ----------------- |
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| 26 | ! $Id: surface_layer_fluxes_mod.f90 2321 2017-07-24 15:57:07Z Giersch $ |
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[2321] | 27 | ! Bugfix: Correct index in lookup table for Obukhov length |
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| 28 | ! |
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| 29 | ! 2299 2017-06-29 10:14:38Z suehring |
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[2299] | 30 | ! Adjusted for allow separate spinups of LSM and atmosphere code |
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| 31 | ! |
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| 32 | ! 2292 2017-06-20 09:51:42Z schwenkel |
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[2292] | 33 | ! Implementation of new microphysic scheme: cloud_scheme = 'morrison' |
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| 34 | ! includes two more prognostic equations for cloud drop concentration (nc) |
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| 35 | ! and cloud water content (qc). |
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| 36 | ! |
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| 37 | ! 2281 2017-06-13 11:34:50Z suehring |
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[2281] | 38 | ! Clean-up unnecessary index access to surface type |
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| 39 | ! |
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| 40 | ! 2233 2017-05-30 18:08:54Z suehring |
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[1692] | 41 | ! |
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[2233] | 42 | ! 2232 2017-05-30 17:47:52Z suehring |
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| 43 | ! Adjustments to new surface concept |
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| 44 | ! OpenMP bugfix |
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| 45 | ! |
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[2119] | 46 | ! 2118 2017-01-17 16:38:49Z raasch |
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| 47 | ! OpenACC directives and related code removed |
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| 48 | ! |
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[2092] | 49 | ! 2091 2016-12-21 16:38:18Z suehring |
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| 50 | ! Bugfix in calculation of vsws ( incorrect linear interpolation of us ) |
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| 51 | ! |
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[2077] | 52 | ! 2076 2016-12-02 13:54:20Z raasch |
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| 53 | ! further openmp bugfix for lookup method |
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| 54 | ! |
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[2074] | 55 | ! 2073 2016-11-30 14:34:05Z raasch |
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| 56 | ! openmp bugfix for lookup method |
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| 57 | ! |
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[2038] | 58 | ! 2037 2016-10-26 11:15:40Z knoop |
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| 59 | ! Anelastic approximation implemented |
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| 60 | ! |
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[2012] | 61 | ! 2011 2016-09-19 17:29:57Z kanani |
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| 62 | ! Flag urban_surface is now defined in module control_parameters. |
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| 63 | ! |
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[2008] | 64 | ! 2007 2016-08-24 15:47:17Z kanani |
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| 65 | ! Account for urban surface model in computation of vertical kinematic heatflux |
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| 66 | ! |
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[2001] | 67 | ! 2000 2016-08-20 18:09:15Z knoop |
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| 68 | ! Forced header and separation lines into 80 columns |
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| 69 | ! |
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[1993] | 70 | ! 1992 2016-08-12 15:14:59Z suehring |
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| 71 | ! Minor bug, declaration of look-up index as INTEGER |
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| 72 | ! |
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[1961] | 73 | ! 1960 2016-07-12 16:34:24Z suehring |
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| 74 | ! Treat humidity and passive scalar separately |
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| 75 | ! |
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[1930] | 76 | ! 1929 2016-06-09 16:25:25Z suehring |
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| 77 | ! Bugfix: avoid segmentation fault in case one grid point is horizontally |
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| 78 | ! completely surrounded by topography |
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| 79 | ! |
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[1921] | 80 | ! 1920 2016-05-30 10:50:15Z suehring |
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| 81 | ! Avoid segmentation fault (see change in 1915) by different initialization of |
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| 82 | ! us instead of adding a very small number in the denominator |
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| 83 | ! |
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[1916] | 84 | ! 1915 2016-05-27 11:05:02Z suehring |
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| 85 | ! Bugfix: avoid segmentation fault in case of most_method = 'circular' at first |
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| 86 | ! timestep |
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| 87 | ! |
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[1851] | 88 | ! 1850 2016-04-08 13:29:27Z maronga |
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| 89 | ! Module renamed |
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| 90 | ! |
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| 91 | ! |
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[1823] | 92 | ! 1822 2016-04-07 07:49:42Z hoffmann |
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| 93 | ! icloud_scheme replaced by microphysics_* |
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| 94 | ! |
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[1789] | 95 | ! 1788 2016-03-10 11:01:04Z maronga |
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| 96 | ! Added parameter z0q which replaces z0h in the similarity functions for |
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| 97 | ! humidity. |
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| 98 | ! Syntax layout improved. |
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| 99 | ! |
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[1758] | 100 | ! 1757 2016-02-22 15:49:32Z maronga |
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| 101 | ! Minor fixes. |
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| 102 | ! |
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[1750] | 103 | ! 1749 2016-02-09 12:19:56Z raasch |
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| 104 | ! further OpenACC adjustments |
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| 105 | ! |
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[1748] | 106 | ! 1747 2016-02-08 12:25:53Z raasch |
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| 107 | ! adjustments for OpenACC usage |
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| 108 | ! |
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[1710] | 109 | ! 1709 2015-11-04 14:47:01Z maronga |
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| 110 | ! Bugfix: division by zero could occur when calculating rib at low wind speeds |
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| 111 | ! Bugfix: calculation of uv_total for neutral = .T., initial value for ol for |
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| 112 | ! neutral = .T. |
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| 113 | ! |
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[1706] | 114 | ! 1705 2015-11-02 14:28:56Z maronga |
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| 115 | ! Typo removed |
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| 116 | ! |
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[1698] | 117 | ! 1697 2015-10-28 17:14:10Z raasch |
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| 118 | ! FORTRAN and OpenMP errors removed |
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| 119 | ! |
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[1697] | 120 | ! 1696 2015-10-27 10:03:34Z maronga |
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[1691] | 121 | ! Modularized and completely re-written version of prandtl_fluxes.f90. In the |
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| 122 | ! course of the re-writing two additional methods have been implemented. See |
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| 123 | ! updated description. |
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| 124 | ! |
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| 125 | ! 1551 2015-03-03 14:18:16Z maronga |
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| 126 | ! Removed land surface model part. The surface fluxes are now always calculated |
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| 127 | ! within prandtl_fluxes, based on the given surface temperature/humidity (which |
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| 128 | ! is either provided by the land surface model, by large scale forcing data, or |
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| 129 | ! directly prescribed by the user. |
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| 130 | ! |
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| 131 | ! 1496 2014-12-02 17:25:50Z maronga |
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| 132 | ! Adapted for land surface model |
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| 133 | ! |
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| 134 | ! 1494 2014-11-21 17:14:03Z maronga |
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| 135 | ! Bugfixes: qs is now calculated before calculation of Rif. calculation of |
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| 136 | ! buoyancy flux in Rif corrected (added missing humidity term), allow use of |
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| 137 | ! topography for coupled runs (not tested) |
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| 138 | ! |
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| 139 | ! 1361 2014-04-16 15:17:48Z hoffmann |
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| 140 | ! Bugfix: calculation of turbulent fluxes of rain water content (qrsws) and rain |
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| 141 | ! drop concentration (nrsws) added |
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| 142 | ! |
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| 143 | ! 1340 2014-03-25 19:45:13Z kanani |
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| 144 | ! REAL constants defined as wp-kind |
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| 145 | ! |
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| 146 | ! 1320 2014-03-20 08:40:49Z raasch |
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| 147 | ! ONLY-attribute added to USE-statements, |
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| 148 | ! kind-parameters added to all INTEGER and REAL declaration statements, |
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| 149 | ! kinds are defined in new module kinds, |
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| 150 | ! old module precision_kind is removed, |
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| 151 | ! revision history before 2012 removed, |
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| 152 | ! comment fields (!:) to be used for variable explanations added to |
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| 153 | ! all variable declaration statements |
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| 154 | ! |
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| 155 | ! 1276 2014-01-15 13:40:41Z heinze |
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| 156 | ! Use LSF_DATA also in case of Dirichlet bottom boundary condition for scalars |
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| 157 | ! |
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| 158 | ! 1257 2013-11-08 15:18:40Z raasch |
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| 159 | ! openACC "kernels do" replaced by "kernels loop", "loop independent" added |
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| 160 | ! |
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| 161 | ! 1036 2012-10-22 13:43:42Z raasch |
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| 162 | ! code put under GPL (PALM 3.9) |
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| 163 | ! |
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| 164 | ! 1015 2012-09-27 09:23:24Z raasch |
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| 165 | ! OpenACC statements added |
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| 166 | ! |
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| 167 | ! 978 2012-08-09 08:28:32Z fricke |
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| 168 | ! roughness length for scalar quantities z0h added |
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| 169 | ! |
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| 170 | ! Revision 1.1 1998/01/23 10:06:06 raasch |
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| 171 | ! Initial revision |
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| 172 | ! |
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| 173 | ! |
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| 174 | ! Description: |
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| 175 | ! ------------ |
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| 176 | !> Diagnostic computation of vertical fluxes in the constant flux layer from the |
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| 177 | !> values of the variables at grid point k=1. Three different methods are |
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| 178 | !> available: |
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| 179 | !> 1) the "old" version (most_method = 'circular') which is fast, but inaccurate |
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| 180 | !> 2) a Newton iteration method (most_method = 'newton'), which is accurate, but |
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| 181 | !> slower |
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| 182 | !> 3) a method using a lookup table which is fast and accurate. Note, however, |
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| 183 | !> that this method cannot be used in case of roughness heterogeneity |
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| 184 | !> |
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| 185 | !> @todo (re)move large_scale_forcing actions |
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[2118] | 186 | !> @todo check/optimize OpenMP directives |
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[1691] | 187 | !------------------------------------------------------------------------------! |
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| 188 | MODULE surface_layer_fluxes_mod |
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| 189 | |
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| 190 | USE arrays_3d, & |
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[2292] | 191 | ONLY: e, kh, nc, nr, pt, q, ql, qc, qr, s, u, v, vpt, w, zu, zw, & |
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| 192 | drho_air_zw, rho_air_zw |
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[1691] | 193 | |
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| 194 | USE cloud_parameters, & |
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| 195 | ONLY: l_d_cp, pt_d_t |
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| 196 | |
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| 197 | USE constants, & |
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| 198 | ONLY: pi |
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| 199 | |
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| 200 | USE cpulog |
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| 201 | |
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| 202 | USE control_parameters, & |
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[1960] | 203 | ONLY: cloud_physics, constant_heatflux, constant_scalarflux, & |
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| 204 | constant_waterflux, coupling_mode, g, humidity, ibc_e_b, & |
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| 205 | ibc_pt_b, initializing_actions, kappa, & |
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[2232] | 206 | intermediate_timestep_count, intermediate_timestep_count_max, & |
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| 207 | land_surface, large_scale_forcing, lsf_surf, & |
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[2292] | 208 | message_string, microphysics_morrison, microphysics_seifert, & |
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| 209 | most_method, neutral, passive_scalar, pt_surface, q_surface, & |
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| 210 | run_coupled, surface_pressure, simulated_time, terminate_run, & |
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[2299] | 211 | time_since_reference_point, urban_surface, zeta_max, zeta_min |
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[1691] | 212 | |
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[2232] | 213 | USE grid_variables, & |
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| 214 | ONLY: dx, dy |
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| 215 | |
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[1691] | 216 | USE indices, & |
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[2232] | 217 | ONLY: nxl, nxr, nys, nyn, nzb |
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[1691] | 218 | |
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| 219 | USE kinds |
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| 220 | |
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| 221 | USE pegrid |
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| 222 | |
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| 223 | USE land_surface_model_mod, & |
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[2232] | 224 | ONLY: aero_resist_kray, skip_time_do_lsm |
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[2011] | 225 | |
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[2232] | 226 | USE surface_mod, & |
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| 227 | ONLY : surf_def_h, surf_def_v, surf_lsm_h, surf_lsm_v, surf_type, & |
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| 228 | surf_usm_h, surf_usm_v |
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[2007] | 229 | |
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[1691] | 230 | |
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| 231 | IMPLICIT NONE |
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| 232 | |
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[1992] | 233 | INTEGER(iwp) :: i !< loop index x direction |
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| 234 | INTEGER(iwp) :: j !< loop index y direction |
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| 235 | INTEGER(iwp) :: k !< loop index z direction |
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[2232] | 236 | INTEGER(iwp) :: l !< loop index for surf type |
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| 237 | INTEGER(iwp) :: li_bnd = 7500 !< Lookup table index of the last time step |
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[1691] | 238 | |
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[2232] | 239 | INTEGER(iwp), PARAMETER :: num_steps = 15000 !< number of steps in the lookup table |
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[1691] | 240 | |
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[2232] | 241 | LOGICAL :: coupled_run !< Flag for coupled atmosphere-ocean runs |
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| 242 | LOGICAL :: downward = .FALSE.!< Flag indicating downward-facing horizontal surface |
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| 243 | LOGICAL :: mom_uv = .FALSE. !< Flag indicating calculation of usvs and vsus at vertical surfaces |
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| 244 | LOGICAL :: mom_w = .FALSE. !< Flag indicating calculation of wsus and wsvs at vertical surfaces |
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| 245 | LOGICAL :: mom_tke = .FALSE. !< Flag indicating calculation of momentum fluxes at vertical surfaces used for TKE production |
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| 246 | LOGICAL :: surf_vertical !< Flag indicating vertical surfaces |
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[1691] | 247 | |
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| 248 | REAL(wp), DIMENSION(0:num_steps-1) :: rib_tab, & !< Lookup table bulk Richardson number |
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| 249 | ol_tab !< Lookup table values of L |
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| 250 | |
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| 251 | REAL(wp) :: e_s, & !< Saturation water vapor pressure |
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| 252 | ol_max = 1.0E6_wp, & !< Maximum Obukhov length |
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| 253 | rib_max, & !< Maximum Richardson number in lookup table |
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| 254 | rib_min, & !< Minimum Richardson number in lookup table |
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| 255 | z_mo !< Height of the constant flux layer where MOST is assumed |
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| 256 | |
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[2232] | 257 | TYPE(surf_type), POINTER :: surf !< surf-type array, used to generalize subroutines |
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[1691] | 258 | |
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[2232] | 259 | |
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[1691] | 260 | SAVE |
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| 261 | |
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| 262 | PRIVATE |
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| 263 | |
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[2232] | 264 | PUBLIC init_surface_layer_fluxes, surface_layer_fluxes |
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[1691] | 265 | |
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| 266 | INTERFACE init_surface_layer_fluxes |
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| 267 | MODULE PROCEDURE init_surface_layer_fluxes |
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| 268 | END INTERFACE init_surface_layer_fluxes |
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| 269 | |
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| 270 | INTERFACE surface_layer_fluxes |
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| 271 | MODULE PROCEDURE surface_layer_fluxes |
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| 272 | END INTERFACE surface_layer_fluxes |
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| 273 | |
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| 274 | |
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| 275 | CONTAINS |
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| 276 | |
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| 277 | |
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| 278 | !------------------------------------------------------------------------------! |
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| 279 | ! Description: |
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| 280 | ! ------------ |
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| 281 | !> Main routine to compute the surface fluxes |
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| 282 | !------------------------------------------------------------------------------! |
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| 283 | SUBROUTINE surface_layer_fluxes |
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| 284 | |
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| 285 | IMPLICIT NONE |
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| 286 | |
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[2232] | 287 | surf_vertical = .FALSE. |
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| 288 | downward = .FALSE. |
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[1691] | 289 | ! |
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| 290 | !-- In case cloud physics is used, it is required to derive potential |
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| 291 | !-- temperature and specific humidity at first grid level from the fields pt |
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| 292 | !-- and q |
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| 293 | IF ( cloud_physics ) THEN |
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[2232] | 294 | ! |
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| 295 | !-- First call for horizontal default-type surfaces (l=0 - upward facing, |
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| 296 | !-- l=1 - downward facing) |
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| 297 | DO l = 0, 1 |
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| 298 | IF ( surf_def_h(l)%ns >= 1 ) THEN |
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| 299 | surf => surf_def_h(l) |
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| 300 | CALL calc_pt_q |
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| 301 | ENDIF |
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| 302 | ENDDO |
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| 303 | ! |
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| 304 | !-- Call for natural-type surfaces |
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| 305 | IF ( surf_lsm_h%ns >= 1 ) THEN |
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| 306 | surf => surf_lsm_h |
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| 307 | CALL calc_pt_q |
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| 308 | ENDIF |
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| 309 | ! |
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| 310 | !-- Call for urban-type surfaces |
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| 311 | IF ( surf_usm_h%ns >= 1 ) THEN |
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| 312 | surf => surf_usm_h |
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| 313 | CALL calc_pt_q |
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| 314 | ENDIF |
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[1691] | 315 | ENDIF |
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| 316 | |
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| 317 | ! |
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| 318 | !-- First, calculate the new Obukhov length, then new friction velocity, |
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| 319 | !-- followed by the new scaling parameters (th*, q*, etc.), and the new |
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| 320 | !-- surface fluxes if required. The old routine ("circular") requires a |
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| 321 | !-- different order of calls as the scaling parameters from the previous time |
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| 322 | !-- steps are used to calculate the Obukhov length |
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| 323 | |
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| 324 | ! |
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| 325 | !-- Depending on setting of most_method use the "old" routine |
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[2232] | 326 | !-- Note, each routine is called for different surface types. |
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| 327 | !-- First call for default-type horizontal surfaces, for natural- and |
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| 328 | !-- urban-type surfaces. Note, at this place only upward-facing horizontal |
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| 329 | !-- surfaces are treted. |
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[1691] | 330 | IF ( most_method == 'circular' ) THEN |
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[2232] | 331 | ! |
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| 332 | !-- Default-type upward-facing horizontal surfaces |
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| 333 | IF ( surf_def_h(0)%ns >= 1 ) THEN |
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| 334 | surf => surf_def_h(0) |
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| 335 | CALL calc_scaling_parameters |
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| 336 | CALL calc_uvw_abs |
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| 337 | IF ( .NOT. neutral ) CALL calc_ol |
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| 338 | CALL calc_us |
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| 339 | CALL calc_surface_fluxes |
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[1691] | 340 | ENDIF |
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| 341 | ! |
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[2232] | 342 | !-- Natural-type horizontal surfaces |
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| 343 | IF ( surf_lsm_h%ns >= 1 ) THEN |
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| 344 | surf => surf_lsm_h |
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| 345 | CALL calc_scaling_parameters |
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| 346 | CALL calc_uvw_abs |
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| 347 | IF ( .NOT. neutral ) CALL calc_ol |
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| 348 | CALL calc_us |
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| 349 | CALL calc_surface_fluxes |
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| 350 | ENDIF |
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| 351 | ! |
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| 352 | !-- Urban-type horizontal surfaces |
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| 353 | IF ( surf_usm_h%ns >= 1 ) THEN |
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| 354 | surf => surf_usm_h |
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| 355 | CALL calc_scaling_parameters |
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| 356 | CALL calc_uvw_abs |
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| 357 | IF ( .NOT. neutral ) CALL calc_ol |
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| 358 | CALL calc_us |
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| 359 | CALL calc_surface_fluxes |
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| 360 | ENDIF |
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| 361 | ! |
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[1691] | 362 | !-- Use either Newton iteration or a lookup table for the bulk Richardson |
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| 363 | !-- number to calculate the Obukhov length |
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[1788] | 364 | ELSEIF ( most_method == 'newton' .OR. most_method == 'lookup' ) THEN |
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[2232] | 365 | ! |
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| 366 | !-- Default-type upward-facing horizontal surfaces |
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| 367 | IF ( surf_def_h(0)%ns >= 1 ) THEN |
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| 368 | surf => surf_def_h(0) |
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| 369 | CALL calc_uvw_abs |
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| 370 | IF ( .NOT. neutral ) CALL calc_ol |
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| 371 | CALL calc_us |
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| 372 | CALL calc_scaling_parameters |
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| 373 | CALL calc_surface_fluxes |
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[1691] | 374 | ENDIF |
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[2232] | 375 | ! |
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| 376 | !-- Natural-type horizontal surfaces |
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| 377 | IF ( surf_lsm_h%ns >= 1 ) THEN |
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| 378 | surf => surf_lsm_h |
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| 379 | CALL calc_uvw_abs |
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| 380 | IF ( .NOT. neutral ) CALL calc_ol |
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| 381 | CALL calc_us |
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| 382 | CALL calc_scaling_parameters |
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| 383 | CALL calc_surface_fluxes |
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| 384 | ENDIF |
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| 385 | ! |
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| 386 | !-- Urban-type horizontal surfaces |
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| 387 | IF ( surf_usm_h%ns >= 1 ) THEN |
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| 388 | surf => surf_usm_h |
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| 389 | CALL calc_uvw_abs |
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| 390 | IF ( .NOT. neutral ) CALL calc_ol |
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| 391 | CALL calc_us |
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| 392 | CALL calc_scaling_parameters |
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| 393 | CALL calc_surface_fluxes |
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| 394 | ENDIF |
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[1691] | 395 | |
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[2232] | 396 | ENDIF |
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| 397 | ! |
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| 398 | !-- Treat downward-facing horizontal surfaces. Note, so far, these are |
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| 399 | !-- always default type. Stratification is not considered |
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| 400 | !-- in this case, hence, no further distinction between different |
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| 401 | !-- most_method is required. |
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| 402 | IF ( surf_def_h(1)%ns >= 1 ) THEN |
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| 403 | downward = .TRUE. |
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| 404 | surf => surf_def_h(1) |
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| 405 | CALL calc_uvw_abs |
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[1691] | 406 | CALL calc_us |
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| 407 | CALL calc_surface_fluxes |
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[2232] | 408 | downward = .FALSE. |
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[1691] | 409 | ENDIF |
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[2232] | 410 | ! |
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| 411 | !-- Calculate surfaces fluxes at vertical surfaces for momentum |
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| 412 | !-- and subgrid-scale TKE. |
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| 413 | !-- No stability is considered. Therefore, scaling parameters and Obukhov- |
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| 414 | !-- length do not need to be calculated and no distinction in 'circular', |
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| 415 | !-- 'Newton' or 'lookup' is necessary so far. |
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| 416 | !-- Note, this will change if stability is once considered. |
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| 417 | surf_vertical = .TRUE. |
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| 418 | ! |
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| 419 | !-- Calculate horizontal momentum fluxes at north- and south-facing |
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| 420 | !-- surfaces(usvs). |
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| 421 | !-- For default-type surfaces |
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| 422 | mom_uv = .TRUE. |
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| 423 | DO l = 0, 1 |
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| 424 | IF ( surf_def_v(l)%ns >= 1 ) THEN |
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| 425 | surf => surf_def_v(l) |
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| 426 | ! |
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| 427 | !-- Compute surface-parallel velocity |
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| 428 | CALL calc_uvw_abs_v_ugrid |
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| 429 | ! |
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| 430 | !-- Compute respective friction velocity on staggered grid |
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| 431 | CALL calc_us |
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| 432 | ! |
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| 433 | !-- Compute respective surface fluxes for momentum and TKE |
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| 434 | CALL calc_surface_fluxes |
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| 435 | ENDIF |
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| 436 | ENDDO |
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| 437 | ! |
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| 438 | !-- For natural-type surfaces. Please note, even though stability is not |
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| 439 | !-- considered for the calculation of momentum fluxes at vertical surfaces, |
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| 440 | !-- scaling parameters and Obukov length are calculated nevertheless in this |
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| 441 | !-- case. This is due to the requirement of ts in parameterization of heat |
---|
| 442 | !-- flux in land-surface model in case of aero_resist_kray is not true. |
---|
| 443 | IF ( .NOT. aero_resist_kray ) THEN |
---|
| 444 | IF ( most_method == 'circular' ) THEN |
---|
| 445 | DO l = 0, 1 |
---|
| 446 | IF ( surf_lsm_v(l)%ns >= 1 ) THEN |
---|
| 447 | surf => surf_lsm_v(l) |
---|
| 448 | ! |
---|
| 449 | !-- Compute scaling parameters |
---|
| 450 | CALL calc_scaling_parameters |
---|
| 451 | ! |
---|
| 452 | !-- Compute surface-parallel velocity |
---|
| 453 | CALL calc_uvw_abs_v_ugrid |
---|
| 454 | ! |
---|
| 455 | !-- Compute Obukhov length |
---|
| 456 | IF ( .NOT. neutral ) CALL calc_ol |
---|
| 457 | ! |
---|
| 458 | !-- Compute respective friction velocity on staggered grid |
---|
| 459 | CALL calc_us |
---|
| 460 | ! |
---|
| 461 | !-- Compute respective surface fluxes for momentum and TKE |
---|
| 462 | CALL calc_surface_fluxes |
---|
| 463 | ENDIF |
---|
| 464 | ENDDO |
---|
| 465 | ELSE |
---|
| 466 | DO l = 0, 1 |
---|
| 467 | IF ( surf_lsm_v(l)%ns >= 1 ) THEN |
---|
| 468 | surf => surf_lsm_v(l) |
---|
| 469 | ! |
---|
| 470 | !-- Compute surface-parallel velocity |
---|
| 471 | CALL calc_uvw_abs_v_ugrid |
---|
| 472 | ! |
---|
| 473 | !-- Compute Obukhov length |
---|
| 474 | IF ( .NOT. neutral ) CALL calc_ol |
---|
| 475 | ! |
---|
| 476 | !-- Compute respective friction velocity on staggered grid |
---|
| 477 | CALL calc_us |
---|
| 478 | ! |
---|
| 479 | !-- Compute scaling parameters |
---|
| 480 | CALL calc_scaling_parameters |
---|
| 481 | ! |
---|
| 482 | !-- Compute respective surface fluxes for momentum and TKE |
---|
| 483 | CALL calc_surface_fluxes |
---|
| 484 | ENDIF |
---|
| 485 | ENDDO |
---|
| 486 | ENDIF |
---|
| 487 | ! |
---|
| 488 | !-- No ts is required, so scaling parameters and Obukhov length do not need |
---|
| 489 | !-- to be computed. |
---|
| 490 | ELSE |
---|
| 491 | DO l = 0, 1 |
---|
| 492 | IF ( surf_lsm_v(l)%ns >= 1 ) THEN |
---|
| 493 | surf => surf_lsm_v(l) |
---|
| 494 | ! |
---|
| 495 | !-- Compute surface-parallel velocity |
---|
| 496 | CALL calc_uvw_abs_v_ugrid |
---|
| 497 | ! |
---|
| 498 | !-- Compute respective friction velocity on staggered grid |
---|
| 499 | CALL calc_us |
---|
| 500 | ! |
---|
| 501 | !-- Compute respective surface fluxes for momentum and TKE |
---|
| 502 | CALL calc_surface_fluxes |
---|
| 503 | ENDIF |
---|
| 504 | ENDDO |
---|
| 505 | ENDIF |
---|
| 506 | ! |
---|
| 507 | !-- For urban-type surfaces |
---|
| 508 | DO l = 0, 1 |
---|
| 509 | IF ( surf_usm_v(l)%ns >= 1 ) THEN |
---|
| 510 | surf => surf_usm_v(l) |
---|
| 511 | ! |
---|
| 512 | !-- Compute surface-parallel velocity |
---|
| 513 | CALL calc_uvw_abs_v_ugrid |
---|
| 514 | ! |
---|
| 515 | !-- Compute respective friction velocity on staggered grid |
---|
| 516 | CALL calc_us |
---|
| 517 | ! |
---|
| 518 | !-- Compute respective surface fluxes for momentum and TKE |
---|
| 519 | CALL calc_surface_fluxes |
---|
| 520 | ENDIF |
---|
| 521 | ENDDO |
---|
| 522 | ! |
---|
| 523 | !-- Calculate horizontal momentum fluxes at east- and west-facing |
---|
| 524 | !-- surfaces (vsus). |
---|
| 525 | !-- For default-type surfaces |
---|
| 526 | DO l = 2, 3 |
---|
| 527 | IF ( surf_def_v(l)%ns >= 1 ) THEN |
---|
| 528 | surf => surf_def_v(l) |
---|
| 529 | ! |
---|
| 530 | !-- Compute surface-parallel velocity |
---|
| 531 | CALL calc_uvw_abs_v_vgrid |
---|
| 532 | ! |
---|
| 533 | !-- Compute respective friction velocity on staggered grid |
---|
| 534 | CALL calc_us |
---|
| 535 | ! |
---|
| 536 | !-- Compute respective surface fluxes for momentum and TKE |
---|
| 537 | CALL calc_surface_fluxes |
---|
| 538 | ENDIF |
---|
| 539 | ENDDO |
---|
| 540 | ! |
---|
| 541 | !-- For natural-type surfaces. Please note, even though stability is not |
---|
| 542 | !-- considered for the calculation of momentum fluxes at vertical surfaces, |
---|
| 543 | !-- scaling parameters and Obukov length are calculated nevertheless in this |
---|
| 544 | !-- case. This is due to the requirement of ts in parameterization of heat |
---|
| 545 | !-- flux in land-surface model in case of aero_resist_kray is not true. |
---|
| 546 | IF ( .NOT. aero_resist_kray ) THEN |
---|
| 547 | IF ( most_method == 'circular' ) THEN |
---|
| 548 | DO l = 2, 3 |
---|
| 549 | IF ( surf_lsm_v(l)%ns >= 1 ) THEN |
---|
| 550 | surf => surf_lsm_v(l) |
---|
| 551 | ! |
---|
| 552 | !-- Compute scaling parameters |
---|
| 553 | CALL calc_scaling_parameters |
---|
| 554 | ! |
---|
| 555 | !-- Compute surface-parallel velocity |
---|
| 556 | CALL calc_uvw_abs_v_vgrid |
---|
| 557 | ! |
---|
| 558 | !-- Compute Obukhov length |
---|
| 559 | IF ( .NOT. neutral ) CALL calc_ol |
---|
| 560 | ! |
---|
| 561 | !-- Compute respective friction velocity on staggered grid |
---|
| 562 | CALL calc_us |
---|
| 563 | ! |
---|
| 564 | !-- Compute respective surface fluxes for momentum and TKE |
---|
| 565 | CALL calc_surface_fluxes |
---|
| 566 | ENDIF |
---|
| 567 | ENDDO |
---|
| 568 | ELSE |
---|
| 569 | DO l = 2, 3 |
---|
| 570 | IF ( surf_lsm_v(l)%ns >= 1 ) THEN |
---|
| 571 | surf => surf_lsm_v(l) |
---|
| 572 | ! |
---|
| 573 | !-- Compute surface-parallel velocity |
---|
| 574 | CALL calc_uvw_abs_v_vgrid |
---|
| 575 | ! |
---|
| 576 | !-- Compute Obukhov length |
---|
| 577 | IF ( .NOT. neutral ) CALL calc_ol |
---|
| 578 | ! |
---|
| 579 | !-- Compute respective friction velocity on staggered grid |
---|
| 580 | CALL calc_us |
---|
| 581 | ! |
---|
| 582 | !-- Compute scaling parameters |
---|
| 583 | CALL calc_scaling_parameters |
---|
| 584 | ! |
---|
| 585 | !-- Compute respective surface fluxes for momentum and TKE |
---|
| 586 | CALL calc_surface_fluxes |
---|
| 587 | ENDIF |
---|
| 588 | ENDDO |
---|
| 589 | ENDIF |
---|
| 590 | ELSE |
---|
| 591 | DO l = 2, 3 |
---|
| 592 | IF ( surf_lsm_v(l)%ns >= 1 ) THEN |
---|
| 593 | surf => surf_lsm_v(l) |
---|
| 594 | ! |
---|
| 595 | !-- Compute surface-parallel velocity |
---|
| 596 | CALL calc_uvw_abs_v_vgrid |
---|
| 597 | ! |
---|
| 598 | !-- Compute respective friction velocity on staggered grid |
---|
| 599 | CALL calc_us |
---|
| 600 | ! |
---|
| 601 | !-- Compute respective surface fluxes for momentum and TKE |
---|
| 602 | CALL calc_surface_fluxes |
---|
| 603 | ENDIF |
---|
| 604 | ENDDO |
---|
| 605 | ENDIF |
---|
| 606 | ! |
---|
| 607 | !-- For urban-type surfaces |
---|
| 608 | DO l = 2, 3 |
---|
| 609 | IF ( surf_usm_v(l)%ns >= 1 ) THEN |
---|
| 610 | surf => surf_usm_v(l) |
---|
| 611 | ! |
---|
| 612 | !-- Compute surface-parallel velocity |
---|
| 613 | CALL calc_uvw_abs_v_vgrid |
---|
| 614 | ! |
---|
| 615 | !-- Compute respective friction velocity on staggered grid |
---|
| 616 | CALL calc_us |
---|
| 617 | ! |
---|
| 618 | !-- Compute respective surface fluxes for momentum and TKE |
---|
| 619 | CALL calc_surface_fluxes |
---|
| 620 | ENDIF |
---|
| 621 | ENDDO |
---|
| 622 | mom_uv = .FALSE. |
---|
| 623 | ! |
---|
| 624 | !-- Calculate horizontal momentum fluxes of w (wsus and wsvs) at vertial |
---|
| 625 | !-- surfaces. |
---|
| 626 | mom_w = .TRUE. |
---|
| 627 | ! |
---|
| 628 | !-- Default-type surfaces |
---|
| 629 | DO l = 0, 3 |
---|
| 630 | IF ( surf_def_v(l)%ns >= 1 ) THEN |
---|
| 631 | surf => surf_def_v(l) |
---|
| 632 | CALL calc_uvw_abs_v_wgrid |
---|
| 633 | CALL calc_us |
---|
| 634 | CALL calc_surface_fluxes |
---|
| 635 | ENDIF |
---|
| 636 | ENDDO |
---|
| 637 | ! |
---|
| 638 | !-- Natural-type surfaces |
---|
| 639 | DO l = 0, 3 |
---|
| 640 | IF ( surf_lsm_v(l)%ns >= 1 ) THEN |
---|
| 641 | surf => surf_lsm_v(l) |
---|
| 642 | CALL calc_uvw_abs_v_wgrid |
---|
| 643 | CALL calc_us |
---|
| 644 | CALL calc_surface_fluxes |
---|
| 645 | ENDIF |
---|
| 646 | ENDDO |
---|
| 647 | ! |
---|
| 648 | !-- Urban-type surfaces |
---|
| 649 | DO l = 0, 3 |
---|
| 650 | IF ( surf_usm_v(l)%ns >= 1 ) THEN |
---|
| 651 | surf => surf_usm_v(l) |
---|
| 652 | CALL calc_uvw_abs_v_wgrid |
---|
| 653 | CALL calc_us |
---|
| 654 | CALL calc_surface_fluxes |
---|
| 655 | ENDIF |
---|
| 656 | ENDDO |
---|
| 657 | mom_w = .FALSE. |
---|
| 658 | ! |
---|
| 659 | !-- Calculate momentum fluxes usvs, vsus, wsus and wsvs at vertical |
---|
| 660 | !-- surfaces for TKE production. Note, here, momentum fluxes are defined |
---|
| 661 | !-- at grid center and are not staggered as before. |
---|
| 662 | mom_tke = .TRUE. |
---|
| 663 | ! |
---|
| 664 | !-- Default-type surfaces |
---|
| 665 | DO l = 0, 3 |
---|
| 666 | IF ( surf_def_v(l)%ns >= 1 ) THEN |
---|
| 667 | surf => surf_def_v(l) |
---|
| 668 | CALL calc_uvw_abs_v_sgrid |
---|
| 669 | CALL calc_us |
---|
| 670 | CALL calc_surface_fluxes |
---|
| 671 | ENDIF |
---|
| 672 | ENDDO |
---|
| 673 | ! |
---|
| 674 | !-- Natural-type surfaces |
---|
| 675 | DO l = 0, 3 |
---|
| 676 | IF ( surf_lsm_v(l)%ns >= 1 ) THEN |
---|
| 677 | surf => surf_lsm_v(l) |
---|
| 678 | CALL calc_uvw_abs_v_sgrid |
---|
| 679 | CALL calc_us |
---|
| 680 | CALL calc_surface_fluxes |
---|
| 681 | ENDIF |
---|
| 682 | ENDDO |
---|
| 683 | ! |
---|
| 684 | !-- Urban-type surfaces |
---|
| 685 | DO l = 0, 3 |
---|
| 686 | IF ( surf_usm_v(l)%ns >= 1 ) THEN |
---|
| 687 | surf => surf_usm_v(l) |
---|
| 688 | CALL calc_uvw_abs_v_sgrid |
---|
| 689 | CALL calc_us |
---|
| 690 | CALL calc_surface_fluxes |
---|
| 691 | ENDIF |
---|
| 692 | ENDDO |
---|
| 693 | mom_tke = .FALSE. |
---|
| 694 | |
---|
[1691] | 695 | |
---|
| 696 | END SUBROUTINE surface_layer_fluxes |
---|
| 697 | |
---|
| 698 | |
---|
| 699 | !------------------------------------------------------------------------------! |
---|
| 700 | ! Description: |
---|
| 701 | ! ------------ |
---|
| 702 | !> Initializing actions for the surface layer routine. Basically, this involves |
---|
| 703 | !> the preparation of a lookup table for the the bulk Richardson number vs |
---|
| 704 | !> Obukhov length L when using the lookup table method. |
---|
| 705 | !------------------------------------------------------------------------------! |
---|
| 706 | SUBROUTINE init_surface_layer_fluxes |
---|
| 707 | |
---|
| 708 | IMPLICIT NONE |
---|
| 709 | |
---|
[2232] | 710 | INTEGER(iwp) :: li, & !< Index for loop to create lookup table |
---|
[1691] | 711 | num_steps_n !< Number of non-stretched zeta steps |
---|
| 712 | |
---|
| 713 | LOGICAL :: terminate_run_l = .FALSE. !< Flag to terminate run (global) |
---|
| 714 | |
---|
| 715 | REAL(wp), PARAMETER :: zeta_stretch = -10.0_wp !< Start of stretching in the free convection limit |
---|
| 716 | |
---|
| 717 | REAL(wp), DIMENSION(:), ALLOCATABLE :: zeta_tmp |
---|
| 718 | |
---|
| 719 | |
---|
| 720 | REAL(wp) :: zeta_step, & !< Increment of zeta |
---|
| 721 | regr = 1.01_wp, & !< Stretching factor of zeta_step in the free convection limit |
---|
| 722 | regr_old = 1.0E9_wp, & !< Stretching factor of last iteration step |
---|
| 723 | z0h_min = 0.0_wp, & !< Minimum value of z0h to create table |
---|
| 724 | z0_min = 0.0_wp !< Minimum value of z0 to create table |
---|
| 725 | |
---|
| 726 | |
---|
[1709] | 727 | |
---|
[2232] | 728 | |
---|
[1709] | 729 | ! |
---|
| 730 | !-- In case of runs with neutral statification, set Obukhov length to a |
---|
| 731 | !-- large value |
---|
[2232] | 732 | IF ( neutral ) THEN |
---|
| 733 | IF ( surf_def_h(0)%ns >= 1 ) surf_def_h(0)%ol = 1.0E10_wp |
---|
| 734 | IF ( surf_lsm_h%ns >= 1 ) surf_lsm_h%ol = 1.0E10_wp |
---|
| 735 | IF ( surf_usm_h%ns >= 1 ) surf_usm_h%ol = 1.0E10_wp |
---|
| 736 | ENDIF |
---|
[1709] | 737 | |
---|
[1691] | 738 | IF ( most_method == 'lookup' ) THEN |
---|
| 739 | |
---|
| 740 | ! |
---|
| 741 | !-- Check for roughness heterogeneity. In that case terminate run and |
---|
[2232] | 742 | !-- inform user. Check for both, natural and non-natural walls. |
---|
| 743 | IF ( surf_def_h(0)%ns >= 1 ) THEN |
---|
| 744 | IF ( MINVAL( surf_def_h(0)%z0h ) /= MAXVAL( surf_def_h(0)%z0h ) .OR. & |
---|
| 745 | MINVAL( surf_def_h(0)%z0 ) /= MAXVAL( surf_def_h(0)%z0 ) ) THEN |
---|
| 746 | terminate_run_l = .TRUE. |
---|
| 747 | ENDIF |
---|
[1691] | 748 | ENDIF |
---|
[2232] | 749 | IF ( surf_lsm_h%ns >= 1 ) THEN |
---|
| 750 | IF ( MINVAL( surf_lsm_h%z0h ) /= MAXVAL( surf_lsm_h%z0h ) .OR. & |
---|
| 751 | MINVAL( surf_lsm_h%z0 ) /= MAXVAL( surf_lsm_h%z0 ) ) THEN |
---|
| 752 | terminate_run_l = .TRUE. |
---|
| 753 | ENDIF |
---|
| 754 | ENDIF |
---|
| 755 | IF ( surf_usm_h%ns >= 1 ) THEN |
---|
| 756 | IF ( MINVAL( surf_usm_h%z0h ) /= MAXVAL( surf_usm_h%z0h ) .OR. & |
---|
| 757 | MINVAL( surf_usm_h%z0 ) /= MAXVAL( surf_usm_h%z0 ) ) THEN |
---|
| 758 | terminate_run_l = .TRUE. |
---|
| 759 | ENDIF |
---|
| 760 | ENDIF |
---|
| 761 | ! |
---|
| 762 | !-- Check roughness homogeneity between differt surface types. |
---|
| 763 | IF ( surf_lsm_h%ns >= 1 .AND. surf_def_h(0)%ns >= 1 ) THEN |
---|
| 764 | IF ( MINVAL( surf_lsm_h%z0h ) /= MAXVAL( surf_def_h(0)%z0h ) .OR. & |
---|
| 765 | MINVAL( surf_lsm_h%z0 ) /= MAXVAL( surf_def_h(0)%z0 ) ) THEN |
---|
| 766 | terminate_run_l = .TRUE. |
---|
| 767 | ENDIF |
---|
| 768 | ENDIF |
---|
| 769 | IF ( surf_usm_h%ns >= 1 .AND. surf_def_h(0)%ns >= 1 ) THEN |
---|
| 770 | IF ( MINVAL( surf_usm_h%z0h ) /= MAXVAL( surf_def_h(0)%z0h ) .OR. & |
---|
| 771 | MINVAL( surf_usm_h%z0 ) /= MAXVAL( surf_def_h(0)%z0 ) ) THEN |
---|
| 772 | terminate_run_l = .TRUE. |
---|
| 773 | ENDIF |
---|
| 774 | ENDIF |
---|
| 775 | IF ( surf_usm_h%ns >= 1 .AND. surf_lsm_h%ns >= 1 ) THEN |
---|
| 776 | IF ( MINVAL( surf_usm_h%z0h ) /= MAXVAL( surf_lsm_h%z0h ) .OR. & |
---|
| 777 | MINVAL( surf_usm_h%z0 ) /= MAXVAL( surf_lsm_h%z0 ) ) THEN |
---|
| 778 | terminate_run_l = .TRUE. |
---|
| 779 | ENDIF |
---|
| 780 | ENDIF |
---|
[1691] | 781 | |
---|
[2232] | 782 | |
---|
[1691] | 783 | #if defined( __parallel ) |
---|
| 784 | ! |
---|
| 785 | !-- Make a logical OR for all processes. Force termiation of model if result |
---|
| 786 | !-- is TRUE |
---|
| 787 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
---|
| 788 | CALL MPI_ALLREDUCE( terminate_run_l, terminate_run, 1, MPI_LOGICAL, & |
---|
| 789 | MPI_LOR, comm2d, ierr ) |
---|
| 790 | #else |
---|
| 791 | terminate_run = terminate_run_l |
---|
| 792 | #endif |
---|
| 793 | |
---|
| 794 | IF ( terminate_run ) THEN |
---|
| 795 | message_string = 'most_method = "lookup" cannot be used in ' // & |
---|
| 796 | 'combination with a prescribed roughness ' // & |
---|
| 797 | 'heterogeneity' |
---|
| 798 | CALL message( 'surface_layer_fluxes', 'PA0417', 1, 2, 0, 6, 0 ) |
---|
| 799 | ENDIF |
---|
| 800 | |
---|
| 801 | ALLOCATE( zeta_tmp(0:num_steps-1) ) |
---|
| 802 | |
---|
| 803 | ! |
---|
| 804 | !-- Use the lowest possible value for z_mo |
---|
[2232] | 805 | k = nzb |
---|
[1691] | 806 | z_mo = zu(k+1) - zw(k) |
---|
| 807 | |
---|
| 808 | ! |
---|
| 809 | !-- Calculate z/L range from zeta_stretch to zeta_max using 90% of the |
---|
| 810 | !-- available steps (num_steps). The calculation is done with negative |
---|
| 811 | !-- values of zeta in order to simplify the stretching in the free |
---|
| 812 | !-- convection limit for the remaining 10% of steps. |
---|
| 813 | zeta_tmp(0) = - zeta_max |
---|
| 814 | num_steps_n = ( num_steps * 9 / 10 ) - 1 |
---|
| 815 | zeta_step = (zeta_max - zeta_stretch) / REAL(num_steps_n) |
---|
| 816 | |
---|
[2232] | 817 | DO li = 1, num_steps_n |
---|
| 818 | zeta_tmp(li) = zeta_tmp(li-1) + zeta_step |
---|
[1691] | 819 | ENDDO |
---|
| 820 | |
---|
| 821 | ! |
---|
| 822 | !-- Calculate stretching factor for the free convection range |
---|
[1788] | 823 | DO WHILE ( ABS( (regr-regr_old) / regr_old ) > 1.0E-10_wp ) |
---|
[1691] | 824 | regr_old = regr |
---|
| 825 | regr = ( 1.0_wp - ( -zeta_min / zeta_step ) * ( 1.0_wp - regr ) & |
---|
| 826 | )**( 10.0_wp / REAL(num_steps) ) |
---|
| 827 | ENDDO |
---|
| 828 | |
---|
| 829 | ! |
---|
| 830 | !-- Calculate z/L range from zeta_min to zeta_stretch |
---|
[2232] | 831 | DO li = num_steps_n+1, num_steps-1 |
---|
| 832 | zeta_tmp(li) = zeta_tmp(li-1) + zeta_step |
---|
[1691] | 833 | zeta_step = zeta_step * regr |
---|
| 834 | ENDDO |
---|
| 835 | |
---|
| 836 | ! |
---|
[1757] | 837 | !-- Save roughness lengths to temporary variables |
---|
[2232] | 838 | IF ( surf_def_h(0)%ns >= 1 ) THEN |
---|
| 839 | z0h_min = surf_def_h(0)%z0h(1) |
---|
| 840 | z0_min = surf_def_h(0)%z0(1) |
---|
| 841 | ELSEIF ( surf_lsm_h%ns >= 1 ) THEN |
---|
| 842 | z0h_min = surf_lsm_h%z0h(1) |
---|
| 843 | z0_min = surf_lsm_h%z0(1) |
---|
| 844 | ELSEIF ( surf_usm_h%ns >= 1 ) THEN |
---|
| 845 | z0h_min = surf_usm_h%z0h(1) |
---|
| 846 | z0_min = surf_usm_h%z0(1) |
---|
| 847 | ENDIF |
---|
[1691] | 848 | ! |
---|
| 849 | !-- Calculate lookup table for the Richardson number versus Obukhov length |
---|
| 850 | !-- The Richardson number (rib) is defined depending on the choice of |
---|
| 851 | !-- boundary conditions for temperature |
---|
| 852 | IF ( ibc_pt_b == 1 ) THEN |
---|
[2232] | 853 | DO li = 0, num_steps-1 |
---|
| 854 | ol_tab(li) = - z_mo / zeta_tmp(num_steps-1-li) |
---|
| 855 | rib_tab(li) = z_mo / ol_tab(li) / ( LOG( z_mo / z0_min ) & |
---|
| 856 | - psi_m( z_mo / ol_tab(li) ) & |
---|
| 857 | + psi_m( z0_min / ol_tab(li) ) & |
---|
[1691] | 858 | )**3 |
---|
| 859 | ENDDO |
---|
| 860 | ELSE |
---|
[2232] | 861 | DO li = 0, num_steps-1 |
---|
| 862 | ol_tab(li) = - z_mo / zeta_tmp(num_steps-1-li) |
---|
| 863 | rib_tab(li) = z_mo / ol_tab(li) * ( LOG( z_mo / z0h_min ) & |
---|
| 864 | - psi_h( z_mo / ol_tab(li) ) & |
---|
| 865 | + psi_h( z0h_min / ol_tab(li) ) & |
---|
[1691] | 866 | ) & |
---|
| 867 | / ( LOG( z_mo / z0_min ) & |
---|
[2232] | 868 | - psi_m( z_mo / ol_tab(li) ) & |
---|
| 869 | + psi_m( z0_min / ol_tab(li) ) & |
---|
[1691] | 870 | )**2 |
---|
| 871 | ENDDO |
---|
| 872 | ENDIF |
---|
| 873 | |
---|
| 874 | ! |
---|
| 875 | !-- Determine minimum values of rib in the lookup table. Set upper limit |
---|
| 876 | !-- to critical Richardson number (0.25) |
---|
| 877 | rib_min = MINVAL(rib_tab) |
---|
| 878 | rib_max = 0.25 !MAXVAL(rib_tab) |
---|
| 879 | |
---|
| 880 | DEALLOCATE( zeta_tmp ) |
---|
| 881 | ENDIF |
---|
| 882 | |
---|
| 883 | END SUBROUTINE init_surface_layer_fluxes |
---|
| 884 | |
---|
| 885 | |
---|
| 886 | !------------------------------------------------------------------------------! |
---|
| 887 | ! Description: |
---|
| 888 | ! ------------ |
---|
[1709] | 889 | !> Compute the absolute value of the horizontal velocity (relative to the |
---|
[2232] | 890 | !> surface) for horizontal surface elements. This is required by all methods. |
---|
[1691] | 891 | !------------------------------------------------------------------------------! |
---|
[2232] | 892 | SUBROUTINE calc_uvw_abs |
---|
[1691] | 893 | |
---|
| 894 | IMPLICIT NONE |
---|
| 895 | |
---|
[2232] | 896 | INTEGER(iwp) :: i !< running index x direction |
---|
| 897 | INTEGER(iwp) :: ibit !< flag to mask computation of relative velocity in case of downward-facing surfaces |
---|
| 898 | INTEGER(iwp) :: j !< running index y direction |
---|
| 899 | INTEGER(iwp) :: k !< running index z direction |
---|
| 900 | INTEGER(iwp) :: m !< running index surface elements |
---|
[1691] | 901 | |
---|
[2232] | 902 | ! |
---|
| 903 | !-- ibit is 1 for upward-facing surfaces, zero for downward-facing surfaces. |
---|
| 904 | ibit = MERGE( 1, 0, .NOT. downward ) |
---|
[1691] | 905 | |
---|
[2232] | 906 | DO m = 1, surf%ns |
---|
[1691] | 907 | |
---|
[2232] | 908 | i = surf%i(m) |
---|
| 909 | j = surf%j(m) |
---|
| 910 | k = surf%k(m) |
---|
[1691] | 911 | ! |
---|
[2232] | 912 | !-- Compute the absolute value of the horizontal velocity. |
---|
| 913 | !-- (relative to the surface in case the lower surface is the ocean). |
---|
| 914 | !-- Please note, in new surface modelling concept the index values changed, |
---|
| 915 | !-- i.e. the reference grid point is not the surface-grid point itself but |
---|
| 916 | !-- the first grid point outside of the topography. |
---|
| 917 | !-- Note, in case of coupled ocean-atmosphere simulations relative velocity |
---|
| 918 | !-- with respect to the ocean surface is used, hence, (k-1,j,i) values |
---|
| 919 | !-- are used to calculate the absolute velocity. |
---|
| 920 | !-- However, this do not apply for downward-facing walls. To mask this, |
---|
| 921 | !-- use ibit, which checks for upward/downward-facing surfaces. |
---|
[1691] | 922 | |
---|
[2232] | 923 | surf%uvw_abs(m) = SQRT( & |
---|
| 924 | ( 0.5_wp * ( u(k,j,i) + u(k,j,i+1) & |
---|
| 925 | - ( u(k-1,j,i) + u(k-1,j,i+1) & |
---|
| 926 | ) * ibit & |
---|
| 927 | ) & |
---|
| 928 | )**2 + & |
---|
| 929 | ( 0.5_wp * ( v(k,j,i) + v(k,j+1,i) & |
---|
| 930 | - ( v(k-1,j,i) + v(k-1,j+1,i) & |
---|
| 931 | ) * ibit & |
---|
| 932 | ) & |
---|
| 933 | )**2 & |
---|
| 934 | ) |
---|
| 935 | |
---|
[1691] | 936 | ENDDO |
---|
| 937 | |
---|
[2232] | 938 | END SUBROUTINE calc_uvw_abs |
---|
| 939 | |
---|
| 940 | |
---|
| 941 | !------------------------------------------------------------------------------! |
---|
| 942 | ! Description: |
---|
| 943 | ! ------------ |
---|
| 944 | !> Compute the absolute value of the horizontal velocity (relative to the |
---|
| 945 | !> surface) for horizontal surface elements. This is required by all methods. |
---|
| 946 | !------------------------------------------------------------------------------! |
---|
| 947 | SUBROUTINE calc_uvw_abs_v_ugrid |
---|
| 948 | |
---|
| 949 | IMPLICIT NONE |
---|
| 950 | |
---|
| 951 | INTEGER(iwp) :: i !< running index x direction |
---|
| 952 | INTEGER(iwp) :: j !< running index y direction |
---|
| 953 | INTEGER(iwp) :: k !< running index z direction |
---|
| 954 | INTEGER(iwp) :: m !< running index surface elements |
---|
| 955 | |
---|
| 956 | REAL(wp) :: u_i |
---|
| 957 | REAL(wp) :: w_i |
---|
| 958 | |
---|
| 959 | |
---|
| 960 | DO m = 1, surf%ns |
---|
| 961 | i = surf%i(m) |
---|
| 962 | j = surf%j(m) |
---|
| 963 | k = surf%k(m) |
---|
[1691] | 964 | ! |
---|
[2232] | 965 | !-- Compute the absolute value of the surface parallel velocity on u-grid. |
---|
| 966 | u_i = u(k,j,i) |
---|
| 967 | w_i = 0.25_wp * ( w(k-1,j,i-1) + w(k-1,j,i) + & |
---|
| 968 | w(k,j,i-1) + w(k,j,i) ) |
---|
[1691] | 969 | |
---|
[2232] | 970 | surf%uvw_abs(m) = SQRT( u_i**2 + w_i**2 ) |
---|
[1709] | 971 | |
---|
[2232] | 972 | ENDDO |
---|
[1709] | 973 | |
---|
[2232] | 974 | END SUBROUTINE calc_uvw_abs_v_ugrid |
---|
| 975 | |
---|
[1709] | 976 | !------------------------------------------------------------------------------! |
---|
| 977 | ! Description: |
---|
| 978 | ! ------------ |
---|
[2232] | 979 | !> Compute the absolute value of the horizontal velocity (relative to the |
---|
| 980 | !> surface) for horizontal surface elements. This is required by all methods. |
---|
| 981 | !------------------------------------------------------------------------------! |
---|
| 982 | SUBROUTINE calc_uvw_abs_v_vgrid |
---|
| 983 | |
---|
| 984 | IMPLICIT NONE |
---|
| 985 | |
---|
| 986 | INTEGER(iwp) :: i !< running index x direction |
---|
| 987 | INTEGER(iwp) :: j !< running index y direction |
---|
| 988 | INTEGER(iwp) :: k !< running index z direction |
---|
| 989 | INTEGER(iwp) :: m !< running index surface elements |
---|
| 990 | |
---|
| 991 | REAL(wp) :: v_i |
---|
| 992 | REAL(wp) :: w_i |
---|
| 993 | |
---|
| 994 | |
---|
| 995 | DO m = 1, surf%ns |
---|
| 996 | i = surf%i(m) |
---|
| 997 | j = surf%j(m) |
---|
| 998 | k = surf%k(m) |
---|
| 999 | |
---|
| 1000 | v_i = u(k,j,i) |
---|
| 1001 | w_i = 0.25_wp * ( w(k-1,j-1,i) + w(k-1,j,i) + & |
---|
| 1002 | w(k,j-1,i) + w(k,j,i) ) |
---|
| 1003 | |
---|
| 1004 | surf%uvw_abs(m) = SQRT( v_i**2 + w_i**2 ) |
---|
| 1005 | |
---|
| 1006 | ENDDO |
---|
| 1007 | |
---|
| 1008 | END SUBROUTINE calc_uvw_abs_v_vgrid |
---|
| 1009 | |
---|
| 1010 | !------------------------------------------------------------------------------! |
---|
| 1011 | ! Description: |
---|
| 1012 | ! ------------ |
---|
| 1013 | !> Compute the absolute value of the horizontal velocity (relative to the |
---|
| 1014 | !> surface) for horizontal surface elements. This is required by all methods. |
---|
| 1015 | !------------------------------------------------------------------------------! |
---|
| 1016 | SUBROUTINE calc_uvw_abs_v_wgrid |
---|
| 1017 | |
---|
| 1018 | IMPLICIT NONE |
---|
| 1019 | |
---|
| 1020 | INTEGER(iwp) :: i !< running index x direction |
---|
| 1021 | INTEGER(iwp) :: j !< running index y direction |
---|
| 1022 | INTEGER(iwp) :: k !< running index z direction |
---|
| 1023 | INTEGER(iwp) :: m !< running index surface elements |
---|
| 1024 | |
---|
| 1025 | REAL(wp) :: u_i |
---|
| 1026 | REAL(wp) :: v_i |
---|
| 1027 | REAL(wp) :: w_i |
---|
| 1028 | ! |
---|
| 1029 | !-- North- (l=0) and south-facing (l=1) surfaces |
---|
| 1030 | IF ( l == 0 .OR. l == 1 ) THEN |
---|
| 1031 | DO m = 1, surf%ns |
---|
| 1032 | i = surf%i(m) |
---|
| 1033 | j = surf%j(m) |
---|
| 1034 | k = surf%k(m) |
---|
| 1035 | |
---|
| 1036 | u_i = 0.25_wp * ( u(k+1,j,i+1) + u(k+1,j,i) + & |
---|
| 1037 | u(k,j,i+1) + u(k,j,i) ) |
---|
| 1038 | v_i = 0.0_wp |
---|
| 1039 | w_i = w(k,j,i) |
---|
| 1040 | |
---|
| 1041 | surf%uvw_abs(m) = SQRT( u_i**2 + v_i**2 + w_i**2 ) |
---|
| 1042 | ENDDO |
---|
| 1043 | ! |
---|
| 1044 | !-- East- (l=2) and west-facing (l=3) surfaces |
---|
| 1045 | ELSE |
---|
| 1046 | DO m = 1, surf%ns |
---|
| 1047 | i = surf%i(m) |
---|
| 1048 | j = surf%j(m) |
---|
| 1049 | k = surf%k(m) |
---|
| 1050 | |
---|
| 1051 | u_i = 0.0_wp |
---|
| 1052 | v_i = 0.25_wp * ( v(k+1,j+1,i) + v(k+1,j,i) + & |
---|
| 1053 | v(k,j+1,i) + v(k,j,i) ) |
---|
| 1054 | w_i = w(k,j,i) |
---|
| 1055 | |
---|
| 1056 | surf%uvw_abs(m) = SQRT( u_i**2 + v_i**2 + w_i**2 ) |
---|
| 1057 | ENDDO |
---|
| 1058 | ENDIF |
---|
| 1059 | |
---|
| 1060 | END SUBROUTINE calc_uvw_abs_v_wgrid |
---|
| 1061 | |
---|
| 1062 | !------------------------------------------------------------------------------! |
---|
| 1063 | ! Description: |
---|
| 1064 | ! ------------ |
---|
| 1065 | !> Compute the absolute value of the horizontal velocity (relative to the |
---|
| 1066 | !> surface) for horizontal surface elements. This is required by all methods. |
---|
| 1067 | !------------------------------------------------------------------------------! |
---|
| 1068 | SUBROUTINE calc_uvw_abs_v_sgrid |
---|
| 1069 | |
---|
| 1070 | IMPLICIT NONE |
---|
| 1071 | |
---|
| 1072 | INTEGER(iwp) :: i !< running index x direction |
---|
| 1073 | INTEGER(iwp) :: j !< running index y direction |
---|
| 1074 | INTEGER(iwp) :: k !< running index z direction |
---|
| 1075 | INTEGER(iwp) :: m !< running index surface elements |
---|
| 1076 | |
---|
| 1077 | REAL(wp) :: u_i |
---|
| 1078 | REAL(wp) :: v_i |
---|
| 1079 | REAL(wp) :: w_i |
---|
| 1080 | |
---|
| 1081 | ! |
---|
| 1082 | !-- North- (l=0) and south-facing (l=1) walls |
---|
| 1083 | IF ( l == 0 .OR. l == 1 ) THEN |
---|
| 1084 | DO m = 1, surf%ns |
---|
| 1085 | i = surf%i(m) |
---|
| 1086 | j = surf%j(m) |
---|
| 1087 | k = surf%k(m) |
---|
| 1088 | |
---|
| 1089 | u_i = 0.5_wp * ( u(k,j,i) + u(k,j,i+1) ) |
---|
| 1090 | v_i = 0.0_wp |
---|
| 1091 | w_i = 0.5_wp * ( w(k,j,i) + w(k-1,j,i) ) |
---|
| 1092 | |
---|
| 1093 | surf%uvw_abs(m) = SQRT( u_i**2 + v_i**2 + w_i**2 ) |
---|
| 1094 | ENDDO |
---|
| 1095 | ! |
---|
| 1096 | !-- East- (l=2) and west-facing (l=3) walls |
---|
| 1097 | ELSE |
---|
| 1098 | DO m = 1, surf%ns |
---|
| 1099 | i = surf%i(m) |
---|
| 1100 | j = surf%j(m) |
---|
| 1101 | k = surf%k(m) |
---|
| 1102 | |
---|
| 1103 | u_i = 0.0_wp |
---|
| 1104 | v_i = 0.5_wp * ( v(k,j,i) + v(k,j+1,i) ) |
---|
| 1105 | w_i = 0.5_wp * ( w(k,j,i) + w(k-1,j,i) ) |
---|
| 1106 | |
---|
| 1107 | surf%uvw_abs(m) = SQRT( u_i**2 + v_i**2 + w_i**2 ) |
---|
| 1108 | ENDDO |
---|
| 1109 | ENDIF |
---|
| 1110 | |
---|
| 1111 | END SUBROUTINE calc_uvw_abs_v_sgrid |
---|
| 1112 | |
---|
| 1113 | |
---|
| 1114 | !------------------------------------------------------------------------------! |
---|
| 1115 | ! Description: |
---|
| 1116 | ! ------------ |
---|
[1709] | 1117 | !> Calculate the Obukhov length (L) and Richardson flux number (z/L) |
---|
| 1118 | !------------------------------------------------------------------------------! |
---|
| 1119 | SUBROUTINE calc_ol |
---|
| 1120 | |
---|
| 1121 | IMPLICIT NONE |
---|
| 1122 | |
---|
[2232] | 1123 | INTEGER(iwp) :: iter !< Newton iteration step |
---|
| 1124 | INTEGER(iwp) :: li !< look index |
---|
| 1125 | INTEGER(iwp) :: m !< loop variable over all horizontal wall elements |
---|
[1709] | 1126 | |
---|
| 1127 | REAL(wp) :: f, & !< Function for Newton iteration: f = Ri - [...]/[...]^2 = 0 |
---|
| 1128 | f_d_ol, & !< Derivative of f |
---|
| 1129 | ol_l, & !< Lower bound of L for Newton iteration |
---|
| 1130 | ol_m, & !< Previous value of L for Newton iteration |
---|
| 1131 | ol_old, & !< Previous time step value of L |
---|
| 1132 | ol_u !< Upper bound of L for Newton iteration |
---|
| 1133 | |
---|
[1691] | 1134 | IF ( TRIM( most_method ) /= 'circular' ) THEN |
---|
[2232] | 1135 | ! |
---|
| 1136 | !-- Evaluate bulk Richardson number (calculation depends on |
---|
| 1137 | !-- definition based on setting of boundary conditions |
---|
| 1138 | IF ( ibc_pt_b /= 1 ) THEN |
---|
| 1139 | IF ( humidity ) THEN |
---|
| 1140 | !$OMP PARALLEL DO PRIVATE( i, j, k, z_mo ) |
---|
| 1141 | DO m = 1, surf%ns |
---|
[1691] | 1142 | |
---|
[2232] | 1143 | i = surf%i(m) |
---|
| 1144 | j = surf%j(m) |
---|
| 1145 | k = surf%k(m) |
---|
[1691] | 1146 | |
---|
[2232] | 1147 | z_mo = surf%z_mo(m) |
---|
| 1148 | |
---|
| 1149 | surf%rib(m) = g * z_mo * & |
---|
| 1150 | ( vpt(k,j,i) - vpt(k-1,j,i) ) / & |
---|
| 1151 | ( surf%uvw_abs(m)**2 * vpt(k,j,i) + 1.0E-20_wp ) |
---|
| 1152 | ENDDO |
---|
| 1153 | ELSE |
---|
| 1154 | !$OMP PARALLEL DO PRIVATE( i, j, k, z_mo ) |
---|
| 1155 | DO m = 1, surf%ns |
---|
| 1156 | |
---|
| 1157 | i = surf%i(m) |
---|
| 1158 | j = surf%j(m) |
---|
| 1159 | k = surf%k(m) |
---|
| 1160 | |
---|
| 1161 | z_mo = surf%z_mo(m) |
---|
| 1162 | |
---|
| 1163 | surf%rib(m) = g * z_mo * & |
---|
| 1164 | ( pt(k,j,i) - pt(k-1,j,i) ) / & |
---|
| 1165 | ( surf%uvw_abs(m)**2 * pt(k,j,i) + 1.0E-20_wp ) |
---|
| 1166 | ENDDO |
---|
| 1167 | ENDIF |
---|
| 1168 | ELSE |
---|
| 1169 | IF ( humidity ) THEN |
---|
| 1170 | !$OMP PARALLEL DO PRIVATE( i, j, k, z_mo ) |
---|
| 1171 | DO m = 1, surf%ns |
---|
| 1172 | |
---|
| 1173 | i = surf%i(m) |
---|
| 1174 | j = surf%j(m) |
---|
| 1175 | k = surf%k(m) |
---|
| 1176 | |
---|
| 1177 | z_mo = surf%z_mo(m) |
---|
| 1178 | |
---|
| 1179 | surf%rib(m) = - g * z_mo * ( ( 1.0_wp + 0.61_wp & |
---|
| 1180 | * q(k,j,i) ) * surf%shf(m) + 0.61_wp & |
---|
| 1181 | * pt(k,j,i) * surf%qsws(m) ) * & |
---|
| 1182 | drho_air_zw(k-1) / & |
---|
| 1183 | ( surf%uvw_abs(m)**3 * vpt(k,j,i) * kappa**2 & |
---|
[1709] | 1184 | + 1.0E-20_wp ) |
---|
[2232] | 1185 | ENDDO |
---|
| 1186 | ELSE |
---|
| 1187 | !$OMP PARALLEL DO PRIVATE( i, j, k, z_mo ) |
---|
| 1188 | DO m = 1, surf%ns |
---|
[1691] | 1189 | |
---|
[2232] | 1190 | i = surf%i(m) |
---|
| 1191 | j = surf%j(m) |
---|
| 1192 | k = surf%k(m) |
---|
| 1193 | |
---|
| 1194 | z_mo = surf%z_mo(m) |
---|
| 1195 | |
---|
| 1196 | surf%rib(m) = - g * z_mo * surf%shf(m) * & |
---|
| 1197 | drho_air_zw(k-1) / & |
---|
| 1198 | ( surf%uvw_abs(m)**3 * pt(k,j,i) * kappa**2 & |
---|
| 1199 | + 1.0E-20_wp ) |
---|
| 1200 | ENDDO |
---|
| 1201 | ENDIF |
---|
| 1202 | ENDIF |
---|
| 1203 | |
---|
[1691] | 1204 | ENDIF |
---|
| 1205 | |
---|
[2232] | 1206 | |
---|
[1691] | 1207 | ! |
---|
| 1208 | !-- Calculate the Obukhov length either using a Newton iteration |
---|
| 1209 | !-- method, via a lookup table, or using the old circular way |
---|
| 1210 | IF ( TRIM( most_method ) == 'newton' ) THEN |
---|
| 1211 | |
---|
[2232] | 1212 | DO m = 1, surf%ns |
---|
[1691] | 1213 | |
---|
[2232] | 1214 | i = surf%i(m) |
---|
| 1215 | j = surf%j(m) |
---|
[1691] | 1216 | |
---|
[2232] | 1217 | z_mo = surf%z_mo(m) |
---|
| 1218 | |
---|
[1691] | 1219 | ! |
---|
[2232] | 1220 | !-- Store current value in case the Newton iteration fails |
---|
| 1221 | ol_old = surf%ol(m) |
---|
[1691] | 1222 | |
---|
| 1223 | ! |
---|
[2232] | 1224 | !-- Ensure that the bulk Richardson number and the Obukhov |
---|
| 1225 | !-- length have the same sign |
---|
| 1226 | IF ( surf%rib(m) * surf%ol(m) < 0.0_wp .OR. & |
---|
| 1227 | ABS( surf%ol(m) ) == ol_max ) THEN |
---|
| 1228 | IF ( surf%rib(m) > 1.0_wp ) surf%ol(m) = 0.01_wp |
---|
| 1229 | IF ( surf%rib(m) < 0.0_wp ) surf%ol(m) = -0.01_wp |
---|
| 1230 | ENDIF |
---|
[1691] | 1231 | ! |
---|
[2232] | 1232 | !-- Iteration to find Obukhov length |
---|
| 1233 | iter = 0 |
---|
| 1234 | DO |
---|
| 1235 | iter = iter + 1 |
---|
[1691] | 1236 | ! |
---|
[2232] | 1237 | !-- In case of divergence, use the value of the previous time step |
---|
| 1238 | IF ( iter > 1000 ) THEN |
---|
| 1239 | surf%ol(m) = ol_old |
---|
| 1240 | EXIT |
---|
| 1241 | ENDIF |
---|
[1691] | 1242 | |
---|
[2232] | 1243 | ol_m = surf%ol(m) |
---|
| 1244 | ol_l = ol_m - 0.001_wp * ol_m |
---|
| 1245 | ol_u = ol_m + 0.001_wp * ol_m |
---|
[1691] | 1246 | |
---|
| 1247 | |
---|
[2232] | 1248 | IF ( ibc_pt_b /= 1 ) THEN |
---|
[1691] | 1249 | ! |
---|
[2232] | 1250 | !-- Calculate f = Ri - [...]/[...]^2 = 0 |
---|
| 1251 | f = surf%rib(m) - ( z_mo / ol_m ) * ( & |
---|
| 1252 | LOG( z_mo / surf%z0h(m) ) & |
---|
| 1253 | - psi_h( z_mo / ol_m ) & |
---|
| 1254 | + psi_h( surf%z0h(m) / & |
---|
| 1255 | ol_m ) & |
---|
| 1256 | ) & |
---|
| 1257 | / ( LOG( z_mo / surf%z0(m) ) & |
---|
| 1258 | - psi_m( z_mo / ol_m ) & |
---|
| 1259 | + psi_m( surf%z0(m) / & |
---|
| 1260 | ol_m ) & |
---|
| 1261 | )**2 |
---|
[1691] | 1262 | |
---|
| 1263 | ! |
---|
[2232] | 1264 | !-- Calculate df/dL |
---|
| 1265 | f_d_ol = ( - ( z_mo / ol_u ) * ( LOG( z_mo / & |
---|
| 1266 | surf%z0h(m) ) & |
---|
| 1267 | - psi_h( z_mo / ol_u ) & |
---|
| 1268 | + psi_h( surf%z0h(m) / ol_u ) & |
---|
| 1269 | ) & |
---|
| 1270 | / ( LOG( z_mo / surf%z0(m) ) & |
---|
| 1271 | - psi_m( z_mo / ol_u ) & |
---|
| 1272 | + psi_m( surf%z0(m) / ol_u ) & |
---|
| 1273 | )**2 & |
---|
| 1274 | + ( z_mo / ol_l ) * ( LOG( z_mo / surf%z0h(m) ) & |
---|
| 1275 | - psi_h( z_mo / ol_l ) & |
---|
| 1276 | + psi_h( surf%z0h(m) / ol_l ) & |
---|
| 1277 | ) & |
---|
| 1278 | / ( LOG( z_mo / surf%z0(m) ) & |
---|
| 1279 | - psi_m( z_mo / ol_l ) & |
---|
| 1280 | + psi_m( surf%z0(m) / ol_l ) & |
---|
| 1281 | )**2 & |
---|
| 1282 | ) / ( ol_u - ol_l ) |
---|
| 1283 | ELSE |
---|
[1691] | 1284 | ! |
---|
[2232] | 1285 | !-- Calculate f = Ri - 1 /[...]^3 = 0 |
---|
| 1286 | f = surf%rib(m) - ( z_mo / ol_m ) / & |
---|
| 1287 | ( LOG( z_mo / surf%z0(m) ) & |
---|
| 1288 | - psi_m( z_mo / ol_m ) & |
---|
| 1289 | + psi_m( surf%z0(m) / ol_m ) & |
---|
| 1290 | )**3 |
---|
[1691] | 1291 | |
---|
| 1292 | ! |
---|
[2232] | 1293 | !-- Calculate df/dL |
---|
| 1294 | f_d_ol = ( - ( z_mo / ol_u ) / ( LOG( z_mo / & |
---|
| 1295 | surf%z0(m) ) & |
---|
| 1296 | - psi_m( z_mo / ol_u ) & |
---|
| 1297 | + psi_m( surf%z0(m) / ol_u ) & |
---|
| 1298 | )**3 & |
---|
| 1299 | + ( z_mo / ol_l ) / ( LOG( z_mo / surf%z0(m) ) & |
---|
| 1300 | - psi_m( z_mo / ol_l ) & |
---|
| 1301 | + psi_m( surf%z0(m) / ol_l ) & |
---|
| 1302 | )**3 & |
---|
| 1303 | ) / ( ol_u - ol_l ) |
---|
| 1304 | ENDIF |
---|
[1691] | 1305 | ! |
---|
[2232] | 1306 | !-- Calculate new L |
---|
| 1307 | surf%ol(m) = ol_m - f / f_d_ol |
---|
[1691] | 1308 | |
---|
| 1309 | ! |
---|
[2232] | 1310 | !-- Ensure that the bulk Richardson number and the Obukhov |
---|
| 1311 | !-- length have the same sign and ensure convergence. |
---|
| 1312 | IF ( surf%ol(m) * ol_m < 0.0_wp ) surf%ol(m) = ol_m * 0.5_wp |
---|
[1691] | 1313 | ! |
---|
[2232] | 1314 | !-- If unrealistic value occurs, set L to the maximum |
---|
| 1315 | !-- value that is allowed |
---|
| 1316 | IF ( ABS( surf%ol(m) ) > ol_max ) THEN |
---|
| 1317 | surf%ol(m) = ol_max |
---|
| 1318 | EXIT |
---|
| 1319 | ENDIF |
---|
[1691] | 1320 | ! |
---|
[2232] | 1321 | !-- Check for convergence |
---|
| 1322 | IF ( ABS( ( surf%ol(m) - ol_m ) / & |
---|
| 1323 | surf%ol(m) ) < 1.0E-4_wp ) THEN |
---|
| 1324 | EXIT |
---|
| 1325 | ELSE |
---|
| 1326 | CYCLE |
---|
| 1327 | ENDIF |
---|
[1691] | 1328 | |
---|
| 1329 | ENDDO |
---|
| 1330 | ENDDO |
---|
| 1331 | |
---|
| 1332 | ELSEIF ( TRIM( most_method ) == 'lookup' ) THEN |
---|
| 1333 | |
---|
[2281] | 1334 | !$OMP PARALLEL DO PRIVATE( i, j, z_mo, li ) FIRSTPRIVATE( li_bnd ) LASTPRIVATE( li_bnd ) |
---|
[2232] | 1335 | DO m = 1, surf%ns |
---|
[1691] | 1336 | |
---|
[2232] | 1337 | i = surf%i(m) |
---|
| 1338 | j = surf%j(m) |
---|
[1691] | 1339 | ! |
---|
[2232] | 1340 | !-- If the bulk Richardson number is outside the range of the lookup |
---|
| 1341 | !-- table, set it to the exceeding threshold value |
---|
| 1342 | IF ( surf%rib(m) < rib_min ) surf%rib(m) = rib_min |
---|
| 1343 | IF ( surf%rib(m) > rib_max ) surf%rib(m) = rib_max |
---|
[1691] | 1344 | |
---|
| 1345 | ! |
---|
[2232] | 1346 | !-- Find the correct index bounds for linear interpolation. As the |
---|
| 1347 | !-- Richardson number will not differ very much from time step to |
---|
| 1348 | !-- time step , use the index from the last step and search in the |
---|
| 1349 | !-- correct direction |
---|
| 1350 | li = li_bnd |
---|
[2321] | 1351 | IF ( rib_tab(li) - surf%rib(m) > 0.0_wp ) THEN |
---|
| 1352 | DO WHILE ( rib_tab(li-1) - surf%rib(m) > 0.0_wp .AND. li > 0 ) |
---|
[2232] | 1353 | li = li-1 |
---|
| 1354 | ENDDO |
---|
| 1355 | ELSE |
---|
| 1356 | DO WHILE ( rib_tab(li) - surf%rib(m) < 0.0_wp & |
---|
| 1357 | .AND. li < num_steps-1 ) |
---|
| 1358 | li = li+1 |
---|
| 1359 | ENDDO |
---|
| 1360 | ENDIF |
---|
| 1361 | li_bnd = li |
---|
[1691] | 1362 | |
---|
| 1363 | ! |
---|
[2232] | 1364 | !-- Linear interpolation to find the correct value of z/L |
---|
| 1365 | surf%ol(m) = ( ol_tab(li-1) + ( ol_tab(li) - ol_tab(li-1) ) & |
---|
| 1366 | / ( rib_tab(li) - rib_tab(li-1) ) & |
---|
| 1367 | * ( surf%rib(m) - rib_tab(li-1) ) ) |
---|
[1691] | 1368 | |
---|
| 1369 | ENDDO |
---|
| 1370 | |
---|
| 1371 | ELSEIF ( TRIM( most_method ) == 'circular' ) THEN |
---|
| 1372 | |
---|
[2232] | 1373 | IF ( .NOT. humidity ) THEN |
---|
| 1374 | !$OMP PARALLEL DO PRIVATE( i, j, k, z_mo ) |
---|
| 1375 | DO m = 1, surf%ns |
---|
[1691] | 1376 | |
---|
[2232] | 1377 | i = surf%i(m) |
---|
| 1378 | j = surf%j(m) |
---|
| 1379 | k = surf%k(m) |
---|
[1691] | 1380 | |
---|
[2232] | 1381 | z_mo = surf%z_mo(m) |
---|
[1691] | 1382 | |
---|
[2232] | 1383 | surf%ol(m) = ( pt(k,j,i) * surf%us(m)**2 ) / & |
---|
| 1384 | ( kappa * g * & |
---|
| 1385 | surf%ts(m) + 1E-30_wp ) |
---|
[1691] | 1386 | ! |
---|
| 1387 | !-- Limit the value range of the Obukhov length. |
---|
[2232] | 1388 | !-- This is necessary for very small velocities (u,v --> 1), because |
---|
[1691] | 1389 | !-- the absolute value of ol can then become very small, which in |
---|
| 1390 | !-- consequence would result in very large shear stresses and very |
---|
| 1391 | !-- small momentum fluxes (both are generally unrealistic). |
---|
[2232] | 1392 | IF ( ( z_mo / ( surf%ol(m) + 1E-30_wp ) ) < zeta_min ) & |
---|
| 1393 | surf%ol(m) = z_mo / zeta_min |
---|
| 1394 | IF ( ( z_mo / ( surf%ol(m) + 1E-30_wp ) ) > zeta_max ) & |
---|
| 1395 | surf%ol(m) = z_mo / zeta_max |
---|
| 1396 | |
---|
[1691] | 1397 | ENDDO |
---|
[2232] | 1398 | ELSEIF ( cloud_physics ) THEN |
---|
| 1399 | !$OMP PARALLEL DO PRIVATE( i, j, k, z_mo ) |
---|
| 1400 | DO m = 1, surf%ns |
---|
[1691] | 1401 | |
---|
[2232] | 1402 | i = surf%i(m) |
---|
| 1403 | j = surf%j(m) |
---|
| 1404 | k = surf%k(m) |
---|
[1691] | 1405 | |
---|
[2232] | 1406 | z_mo = surf%z_mo(m) |
---|
| 1407 | |
---|
| 1408 | |
---|
| 1409 | surf%ol(m) = ( vpt(k,j,i) * surf%us(m)**2 ) / & |
---|
| 1410 | ( kappa * g * ( surf%ts(m) + & |
---|
| 1411 | 0.61_wp * surf%pt1(m) * surf%us(m) & |
---|
| 1412 | + 0.61_wp * surf%qv1(m) * surf%ts(m) - & |
---|
| 1413 | surf%ts(m) * ql(k,j,i) ) + 1E-30_wp ) |
---|
[1691] | 1414 | ! |
---|
[2232] | 1415 | !-- Limit the value range of the Obukhov length. |
---|
| 1416 | !-- This is necessary for very small velocities (u,v --> 1), because |
---|
| 1417 | !-- the absolute value of ol can then become very small, which in |
---|
| 1418 | !-- consequence would result in very large shear stresses and very |
---|
| 1419 | !-- small momentum fluxes (both are generally unrealistic). |
---|
| 1420 | IF ( ( z_mo / ( surf%ol(m) + 1E-30_wp ) ) < zeta_min ) & |
---|
| 1421 | surf%ol(m) = z_mo / zeta_min |
---|
| 1422 | IF ( ( z_mo / ( surf%ol(m) + 1E-30_wp ) ) > zeta_max ) & |
---|
| 1423 | surf%ol(m) = z_mo / zeta_max |
---|
[1691] | 1424 | |
---|
[2232] | 1425 | ENDDO |
---|
| 1426 | ELSE |
---|
| 1427 | |
---|
| 1428 | !$OMP PARALLEL DO PRIVATE( i, j, k, z_mo ) |
---|
| 1429 | DO m = 1, surf%ns |
---|
| 1430 | |
---|
| 1431 | i = surf%i(m) |
---|
| 1432 | j = surf%j(m) |
---|
| 1433 | k = surf%k(m) |
---|
| 1434 | |
---|
| 1435 | z_mo = surf%z_mo(m) |
---|
| 1436 | |
---|
| 1437 | surf%ol(m) = ( vpt(k,j,i) * surf%us(m)**2 ) / & |
---|
| 1438 | ( kappa * g * ( surf%ts(m) + 0.61_wp * pt(k,j,i) * & |
---|
| 1439 | surf%qs(m) + 0.61_wp * q(k,j,i) * & |
---|
| 1440 | surf%ts(m) ) + 1E-30_wp ) |
---|
| 1441 | |
---|
| 1442 | ! |
---|
| 1443 | !-- Limit the value range of the Obukhov length. |
---|
| 1444 | !-- This is necessary for very small velocities (u,v --> 1), because |
---|
| 1445 | !-- the absolute value of ol can then become very small, which in |
---|
| 1446 | !-- consequence would result in very large shear stresses and very |
---|
| 1447 | !-- small momentum fluxes (both are generally unrealistic). |
---|
| 1448 | IF ( ( z_mo / ( surf%ol(m) + 1E-30_wp ) ) < zeta_min ) & |
---|
| 1449 | surf%ol(m) = z_mo / zeta_min |
---|
| 1450 | IF ( ( z_mo / ( surf%ol(m) + 1E-30_wp ) ) > zeta_max ) & |
---|
| 1451 | surf%ol(m) = z_mo / zeta_max |
---|
| 1452 | |
---|
| 1453 | ENDDO |
---|
| 1454 | |
---|
| 1455 | ENDIF |
---|
| 1456 | |
---|
| 1457 | ENDIF |
---|
| 1458 | |
---|
[1691] | 1459 | END SUBROUTINE calc_ol |
---|
| 1460 | |
---|
| 1461 | ! |
---|
| 1462 | !-- Calculate friction velocity u* |
---|
| 1463 | SUBROUTINE calc_us |
---|
| 1464 | |
---|
| 1465 | IMPLICIT NONE |
---|
| 1466 | |
---|
[2232] | 1467 | INTEGER(iwp) :: m !< loop variable over all horizontal surf elements |
---|
[1691] | 1468 | |
---|
[2232] | 1469 | ! |
---|
| 1470 | !-- Compute u* at horizontal surfaces at the scalars' grid points |
---|
| 1471 | IF ( .NOT. surf_vertical ) THEN |
---|
| 1472 | ! |
---|
| 1473 | !-- Compute u* at upward-facing surfaces |
---|
| 1474 | IF ( .NOT. downward ) THEN |
---|
[2281] | 1475 | !$OMP PARALLEL DO PRIVATE( z_mo ) |
---|
[2232] | 1476 | DO m = 1, surf%ns |
---|
[1691] | 1477 | |
---|
[2232] | 1478 | z_mo = surf%z_mo(m) |
---|
[1691] | 1479 | ! |
---|
[2232] | 1480 | !-- Compute u* at the scalars' grid points |
---|
| 1481 | surf%us(m) = kappa * surf%uvw_abs(m) / & |
---|
| 1482 | ( LOG( z_mo / surf%z0(m) ) & |
---|
| 1483 | - psi_m( z_mo / surf%ol(m) ) & |
---|
| 1484 | + psi_m( surf%z0(m) / surf%ol(m) ) ) |
---|
| 1485 | |
---|
| 1486 | ENDDO |
---|
| 1487 | ! |
---|
| 1488 | !-- Compute u* at downward-facing surfaces. This case, do not consider |
---|
| 1489 | !-- any stability. |
---|
| 1490 | ELSE |
---|
[2281] | 1491 | !$OMP PARALLEL DO PRIVATE( z_mo ) |
---|
[2232] | 1492 | DO m = 1, surf%ns |
---|
| 1493 | |
---|
| 1494 | z_mo = surf%z_mo(m) |
---|
| 1495 | ! |
---|
| 1496 | !-- Compute u* at the scalars' grid points |
---|
| 1497 | surf%us(m) = kappa * surf%uvw_abs(m) / LOG( z_mo / surf%z0(m) ) |
---|
| 1498 | |
---|
| 1499 | ENDDO |
---|
| 1500 | ENDIF |
---|
| 1501 | ! |
---|
| 1502 | !-- Compute u* at vertical surfaces at the u/v/v grid, respectively. |
---|
| 1503 | !-- No stability is considered in this case. |
---|
| 1504 | ELSE |
---|
| 1505 | !$OMP PARALLEL DO PRIVATE( z_mo ) |
---|
| 1506 | DO m = 1, surf%ns |
---|
| 1507 | z_mo = surf%z_mo(m) |
---|
| 1508 | |
---|
| 1509 | surf%us(m) = kappa * surf%uvw_abs(m) / LOG( z_mo / surf%z0(m) ) |
---|
[1691] | 1510 | ENDDO |
---|
[2232] | 1511 | ENDIF |
---|
[1691] | 1512 | |
---|
| 1513 | END SUBROUTINE calc_us |
---|
| 1514 | |
---|
| 1515 | ! |
---|
| 1516 | !-- Calculate potential temperature and specific humidity at first grid level |
---|
[2232] | 1517 | !-- ( only for upward-facing surfs ) |
---|
[1691] | 1518 | SUBROUTINE calc_pt_q |
---|
| 1519 | |
---|
| 1520 | IMPLICIT NONE |
---|
| 1521 | |
---|
[2232] | 1522 | INTEGER(iwp) :: m !< loop variable over all horizontal surf elements |
---|
| 1523 | |
---|
| 1524 | !$OMP PARALLEL DO PRIVATE( i, j, k ) |
---|
| 1525 | DO m = 1, surf%ns |
---|
| 1526 | |
---|
| 1527 | i = surf%i(m) |
---|
| 1528 | j = surf%j(m) |
---|
| 1529 | k = surf%k(m) |
---|
| 1530 | |
---|
| 1531 | surf%pt1(m) = pt(k,j,i) + l_d_cp * pt_d_t(k) * ql(k,j,i) |
---|
| 1532 | surf%qv1(m) = q(k,j,i) - ql(k,j,i) |
---|
| 1533 | |
---|
[1691] | 1534 | ENDDO |
---|
| 1535 | |
---|
| 1536 | END SUBROUTINE calc_pt_q |
---|
| 1537 | |
---|
| 1538 | ! |
---|
[2292] | 1539 | !-- Calculate the other MOST scaling parameters theta*, q*, (qc*, qr*, nc*, nr*) |
---|
[1691] | 1540 | SUBROUTINE calc_scaling_parameters |
---|
| 1541 | |
---|
| 1542 | IMPLICIT NONE |
---|
| 1543 | |
---|
[2232] | 1544 | |
---|
| 1545 | INTEGER(iwp) :: m !< loop variable over all horizontal surf elements |
---|
| 1546 | |
---|
[1691] | 1547 | ! |
---|
[2232] | 1548 | !-- Compute theta* at horizontal surfaces |
---|
| 1549 | IF ( constant_heatflux .AND. .NOT. surf_vertical ) THEN |
---|
[1691] | 1550 | ! |
---|
| 1551 | !-- For a given heat flux in the surface layer: |
---|
[2232] | 1552 | |
---|
| 1553 | !$OMP PARALLEL DO PRIVATE( i, j, k ) |
---|
| 1554 | DO m = 1, surf%ns |
---|
| 1555 | |
---|
| 1556 | i = surf%i(m) |
---|
| 1557 | j = surf%j(m) |
---|
| 1558 | k = surf%k(m) |
---|
| 1559 | |
---|
| 1560 | surf%ts(m) = -surf%shf(m) * drho_air_zw(k-1) / & |
---|
| 1561 | ( surf%us(m) + 1E-30_wp ) |
---|
| 1562 | |
---|
[1691] | 1563 | ! |
---|
[2232] | 1564 | !-- ts must be limited, because otherwise overflow may occur in case |
---|
| 1565 | !-- of us=0 when computing ol further below |
---|
| 1566 | IF ( surf%ts(m) < -1.05E5_wp ) surf%ts(m) = -1.0E5_wp |
---|
| 1567 | IF ( surf%ts(m) > 1.0E5_wp ) surf%ts(m) = 1.0E5_wp |
---|
| 1568 | |
---|
[1691] | 1569 | ENDDO |
---|
| 1570 | |
---|
[2232] | 1571 | ELSEIF ( .NOT. surf_vertical ) THEN |
---|
[1691] | 1572 | ! |
---|
| 1573 | !-- For a given surface temperature: |
---|
[1788] | 1574 | IF ( large_scale_forcing .AND. lsf_surf ) THEN |
---|
[2232] | 1575 | |
---|
| 1576 | !$OMP PARALLEL DO PRIVATE( i, j, k ) |
---|
| 1577 | DO m = 1, surf%ns |
---|
| 1578 | i = surf%i(m) |
---|
| 1579 | j = surf%j(m) |
---|
| 1580 | k = surf%k(m) |
---|
| 1581 | |
---|
| 1582 | pt(k-1,j,i) = pt_surface |
---|
[1691] | 1583 | ENDDO |
---|
| 1584 | ENDIF |
---|
| 1585 | |
---|
[2232] | 1586 | IF ( cloud_physics ) THEN |
---|
| 1587 | !$OMP PARALLEL DO PRIVATE( i, j, k, z_mo ) |
---|
| 1588 | DO m = 1, surf%ns |
---|
[1691] | 1589 | |
---|
[2232] | 1590 | i = surf%i(m) |
---|
| 1591 | j = surf%j(m) |
---|
| 1592 | k = surf%k(m) |
---|
[1691] | 1593 | |
---|
[2232] | 1594 | z_mo = surf%z_mo(m) |
---|
[1691] | 1595 | |
---|
[2232] | 1596 | surf%ts(m) = kappa * ( surf%pt1(m) - pt(k-1,j,i) ) & |
---|
| 1597 | / ( LOG( z_mo / surf%z0h(m) ) & |
---|
| 1598 | - psi_h( z_mo / surf%ol(m) ) & |
---|
| 1599 | + psi_h( surf%z0h(m) / surf%ol(m) ) ) |
---|
| 1600 | |
---|
[1691] | 1601 | ENDDO |
---|
[2232] | 1602 | ELSE |
---|
| 1603 | !$OMP PARALLEL DO PRIVATE( i, j, k, z_mo ) |
---|
| 1604 | DO m = 1, surf%ns |
---|
| 1605 | |
---|
| 1606 | i = surf%i(m) |
---|
| 1607 | j = surf%j(m) |
---|
| 1608 | k = surf%k(m) |
---|
| 1609 | |
---|
| 1610 | z_mo = surf%z_mo(m) |
---|
| 1611 | |
---|
| 1612 | surf%ts(m) = kappa * ( pt(k,j,i) - pt(k-1,j,i) ) & |
---|
| 1613 | / ( LOG( z_mo / surf%z0h(m) ) & |
---|
| 1614 | - psi_h( z_mo / surf%ol(m) ) & |
---|
| 1615 | + psi_h( surf%z0h(m) / surf%ol(m) ) ) |
---|
| 1616 | ENDDO |
---|
| 1617 | ENDIF |
---|
| 1618 | ENDIF |
---|
| 1619 | ! |
---|
| 1620 | !-- Compute theta* at vertical surfaces. This is only required in case of |
---|
| 1621 | !-- land-surface model, in order to compute aerodynamical resistance. |
---|
| 1622 | IF ( surf_vertical ) THEN |
---|
[2281] | 1623 | !$OMP PARALLEL DO PRIVATE( i, j ) |
---|
[2232] | 1624 | DO m = 1, surf%ns |
---|
| 1625 | |
---|
| 1626 | i = surf%i(m) |
---|
| 1627 | j = surf%j(m) |
---|
| 1628 | surf%ts(m) = -surf%shf(m) / ( surf%us(m) + 1E-30_wp ) |
---|
| 1629 | ! |
---|
| 1630 | !-- ts must be limited, because otherwise overflow may occur in case |
---|
| 1631 | !-- of us=0 when computing ol further below |
---|
| 1632 | IF ( surf%ts(m) < -1.05E5_wp ) surf%ts(m) = -1.0E5_wp |
---|
| 1633 | IF ( surf%ts(m) > 1.0E5_wp ) surf%ts(m) = 1.0E5_wp |
---|
| 1634 | |
---|
[1691] | 1635 | ENDDO |
---|
| 1636 | ENDIF |
---|
| 1637 | |
---|
| 1638 | ! |
---|
[2232] | 1639 | !-- If required compute q* at horizontal surfaces |
---|
[1960] | 1640 | IF ( humidity ) THEN |
---|
[2232] | 1641 | IF ( constant_waterflux .AND. .NOT. surf_vertical ) THEN |
---|
[1691] | 1642 | ! |
---|
[1788] | 1643 | !-- For a given water flux in the surface layer |
---|
[2232] | 1644 | !$OMP PARALLEL DO PRIVATE( i, j, k ) |
---|
| 1645 | DO m = 1, surf%ns |
---|
| 1646 | |
---|
| 1647 | i = surf%i(m) |
---|
| 1648 | j = surf%j(m) |
---|
| 1649 | k = surf%k(m) |
---|
| 1650 | surf%qs(m) = -surf%qsws(m) * drho_air_zw(k-1) / & |
---|
| 1651 | ( surf%us(m) + 1E-30_wp ) |
---|
| 1652 | |
---|
[1691] | 1653 | ENDDO |
---|
| 1654 | |
---|
[2232] | 1655 | ELSEIF ( .NOT. surf_vertical ) THEN |
---|
[1788] | 1656 | coupled_run = ( coupling_mode == 'atmosphere_to_ocean' .AND. & |
---|
[1691] | 1657 | run_coupled ) |
---|
| 1658 | |
---|
[1788] | 1659 | IF ( large_scale_forcing .AND. lsf_surf ) THEN |
---|
[2232] | 1660 | !$OMP PARALLEL DO PRIVATE( i, j, k ) |
---|
| 1661 | DO m = 1, surf%ns |
---|
| 1662 | |
---|
| 1663 | i = surf%i(m) |
---|
| 1664 | j = surf%j(m) |
---|
| 1665 | k = surf%k(m) |
---|
| 1666 | q(k-1,j,i) = q_surface |
---|
| 1667 | |
---|
[1691] | 1668 | ENDDO |
---|
| 1669 | ENDIF |
---|
| 1670 | |
---|
| 1671 | ! |
---|
[2232] | 1672 | !-- Assume saturation for atmosphere coupled to ocean (but not |
---|
| 1673 | !-- in case of precursor runs) |
---|
| 1674 | IF ( coupled_run ) THEN |
---|
| 1675 | !$OMP PARALLEL DO PRIVATE( i, j, k, e_s ) |
---|
| 1676 | DO m = 1, surf%ns |
---|
| 1677 | i = surf%i(m) |
---|
| 1678 | j = surf%j(m) |
---|
| 1679 | k = surf%k(m) |
---|
| 1680 | e_s = 6.1_wp * & |
---|
| 1681 | EXP( 0.07_wp * ( MIN(pt(k-1,j,i),pt(k,j,i)) & |
---|
[1691] | 1682 | - 273.15_wp ) ) |
---|
[2232] | 1683 | q(k-1,j,i) = 0.622_wp * e_s / ( surface_pressure - e_s ) |
---|
| 1684 | ENDDO |
---|
| 1685 | ENDIF |
---|
[1691] | 1686 | |
---|
[2232] | 1687 | IF ( cloud_physics ) THEN |
---|
| 1688 | !$OMP PARALLEL DO PRIVATE( i, j, k, z_mo ) |
---|
| 1689 | DO m = 1, surf%ns |
---|
[1691] | 1690 | |
---|
[2232] | 1691 | i = surf%i(m) |
---|
| 1692 | j = surf%j(m) |
---|
| 1693 | k = surf%k(m) |
---|
| 1694 | |
---|
| 1695 | z_mo = surf%z_mo(m) |
---|
[1691] | 1696 | |
---|
[2232] | 1697 | surf%qs(m) = kappa * ( surf%qv1(m) - q(k-1,j,i) ) & |
---|
| 1698 | / ( LOG( z_mo / surf%z0q(m) ) & |
---|
| 1699 | - psi_h( z_mo / surf%ol(m) ) & |
---|
| 1700 | + psi_h( surf%z0q(m) / & |
---|
| 1701 | surf%ol(m) ) ) |
---|
[1691] | 1702 | ENDDO |
---|
[2232] | 1703 | ELSE |
---|
| 1704 | !$OMP PARALLEL DO PRIVATE( i, j, k, z_mo ) |
---|
| 1705 | DO m = 1, surf%ns |
---|
| 1706 | |
---|
| 1707 | i = surf%i(m) |
---|
| 1708 | j = surf%j(m) |
---|
| 1709 | k = surf%k(m) |
---|
| 1710 | |
---|
| 1711 | z_mo = surf%z_mo(m) |
---|
| 1712 | |
---|
| 1713 | surf%qs(m) = kappa * ( q(k,j,i) - q(k-1,j,i) ) & |
---|
| 1714 | / ( LOG( z_mo / surf%z0q(m) ) & |
---|
| 1715 | - psi_h( z_mo / surf%ol(m) ) & |
---|
| 1716 | + psi_h( surf%z0q(m) / & |
---|
| 1717 | surf%ol(m) ) ) |
---|
| 1718 | ENDDO |
---|
| 1719 | ENDIF |
---|
| 1720 | ENDIF |
---|
| 1721 | ! |
---|
| 1722 | !-- Compute q* at vertical surfaces |
---|
| 1723 | IF ( surf_vertical ) THEN |
---|
[2281] | 1724 | !$OMP PARALLEL DO PRIVATE( i, j ) |
---|
[2232] | 1725 | DO m = 1, surf%ns |
---|
| 1726 | |
---|
| 1727 | i = surf%i(m) |
---|
| 1728 | j = surf%j(m) |
---|
| 1729 | surf%qs(m) = -surf%qsws(m) / ( surf%us(m) + 1E-30_wp ) |
---|
| 1730 | |
---|
[1691] | 1731 | ENDDO |
---|
| 1732 | ENDIF |
---|
| 1733 | ENDIF |
---|
[1960] | 1734 | |
---|
| 1735 | ! |
---|
| 1736 | !-- If required compute s* |
---|
| 1737 | IF ( passive_scalar ) THEN |
---|
| 1738 | ! |
---|
[2232] | 1739 | !-- At horizontal surfaces |
---|
| 1740 | IF ( constant_scalarflux .AND. .NOT. surf_vertical ) THEN |
---|
| 1741 | ! |
---|
| 1742 | !-- For a given scalar flux in the surface layer |
---|
[2281] | 1743 | !$OMP PARALLEL DO PRIVATE( i, j ) |
---|
[2232] | 1744 | DO m = 1, surf%ns |
---|
| 1745 | i = surf%i(m) |
---|
| 1746 | j = surf%j(m) |
---|
| 1747 | surf%ss(m) = -surf%ssws(m) / ( surf%us(m) + 1E-30_wp ) |
---|
[1960] | 1748 | ENDDO |
---|
| 1749 | ENDIF |
---|
[2232] | 1750 | ! |
---|
| 1751 | !-- At vertical surfaces |
---|
| 1752 | IF ( surf_vertical ) THEN |
---|
[2281] | 1753 | !$OMP PARALLEL DO PRIVATE( i, j ) |
---|
[2232] | 1754 | DO m = 1, surf%ns |
---|
| 1755 | i = surf%i(m) |
---|
| 1756 | j = surf%j(m) |
---|
| 1757 | surf%ss(m) = -surf%ssws(m) / ( surf%us(m) + 1E-30_wp ) |
---|
| 1758 | ENDDO |
---|
| 1759 | ENDIF |
---|
[1960] | 1760 | ENDIF |
---|
[1691] | 1761 | |
---|
[2292] | 1762 | ! |
---|
| 1763 | !-- If required compute qc* and nc* |
---|
| 1764 | IF ( cloud_physics .AND. microphysics_morrison .AND. & |
---|
| 1765 | .NOT. surf_vertical ) THEN |
---|
| 1766 | !$OMP PARALLEL DO PRIVATE( i, j, k, z_mo ) |
---|
| 1767 | DO m = 1, surf%ns |
---|
[1691] | 1768 | |
---|
[2292] | 1769 | i = surf%i(m) |
---|
| 1770 | j = surf%j(m) |
---|
| 1771 | k = surf%k(m) |
---|
| 1772 | |
---|
| 1773 | z_mo = surf%z_mo(m) |
---|
| 1774 | |
---|
| 1775 | surf%qcs(m) = kappa * ( qc(k,j,i) - qc(k-1,j,i) ) & |
---|
| 1776 | / ( LOG( z_mo / surf%z0q(m) ) & |
---|
| 1777 | - psi_h( z_mo / surf%ol(m) ) & |
---|
| 1778 | + psi_h( surf%z0q(m) / surf%ol(m) ) ) |
---|
| 1779 | |
---|
| 1780 | surf%ncs(m) = kappa * ( nc(k,j,i) - nc(k-1,j,i) ) & |
---|
| 1781 | / ( LOG( z_mo / surf%z0q(m) ) & |
---|
| 1782 | - psi_h( z_mo / surf%ol(m) ) & |
---|
| 1783 | + psi_h( surf%z0q(m) / surf%ol(m) ) ) |
---|
| 1784 | ENDDO |
---|
| 1785 | |
---|
| 1786 | ENDIF |
---|
| 1787 | |
---|
[1691] | 1788 | ! |
---|
| 1789 | !-- If required compute qr* and nr* |
---|
[2232] | 1790 | IF ( cloud_physics .AND. microphysics_seifert .AND. & |
---|
| 1791 | .NOT. surf_vertical ) THEN |
---|
| 1792 | !$OMP PARALLEL DO PRIVATE( i, j, k, z_mo ) |
---|
| 1793 | DO m = 1, surf%ns |
---|
[1691] | 1794 | |
---|
[2232] | 1795 | i = surf%i(m) |
---|
| 1796 | j = surf%j(m) |
---|
| 1797 | k = surf%k(m) |
---|
[1691] | 1798 | |
---|
[2232] | 1799 | z_mo = surf%z_mo(m) |
---|
[1691] | 1800 | |
---|
[2232] | 1801 | surf%qrs(m) = kappa * ( qr(k,j,i) - qr(k-1,j,i) ) & |
---|
| 1802 | / ( LOG( z_mo / surf%z0q(m) ) & |
---|
| 1803 | - psi_h( z_mo / surf%ol(m) ) & |
---|
| 1804 | + psi_h( surf%z0q(m) / surf%ol(m) ) ) |
---|
[1691] | 1805 | |
---|
[2232] | 1806 | surf%nrs(m) = kappa * ( nr(k,j,i) - nr(k-1,j,i) ) & |
---|
| 1807 | / ( LOG( z_mo / surf%z0q(m) ) & |
---|
| 1808 | - psi_h( z_mo / surf%ol(m) ) & |
---|
| 1809 | + psi_h( surf%z0q(m) / surf%ol(m) ) ) |
---|
[1691] | 1810 | ENDDO |
---|
| 1811 | |
---|
| 1812 | ENDIF |
---|
| 1813 | |
---|
| 1814 | END SUBROUTINE calc_scaling_parameters |
---|
| 1815 | |
---|
| 1816 | |
---|
| 1817 | |
---|
| 1818 | ! |
---|
[2292] | 1819 | !-- Calculate surface fluxes usws, vsws, shf, qsws, (qcsws, qrsws, ncsws, nrsws) |
---|
[1691] | 1820 | SUBROUTINE calc_surface_fluxes |
---|
| 1821 | |
---|
| 1822 | IMPLICIT NONE |
---|
| 1823 | |
---|
[2232] | 1824 | INTEGER(iwp) :: m !< loop variable over all horizontal surf elements |
---|
[1691] | 1825 | |
---|
[2232] | 1826 | REAL(wp) :: dum !< dummy to precalculate logarithm |
---|
| 1827 | REAL(wp) :: flag_u !< flag indicating u-grid, used for calculation of horizontal momentum fluxes at vertical surfaces |
---|
| 1828 | REAL(wp) :: flag_v !< flag indicating v-grid, used for calculation of horizontal momentum fluxes at vertical surfaces |
---|
| 1829 | REAL(wp), DIMENSION(:), ALLOCATABLE :: u_i !< u-component interpolated onto scalar grid point, required for momentum fluxes at vertical surfaces |
---|
| 1830 | REAL(wp), DIMENSION(:), ALLOCATABLE :: v_i !< v-component interpolated onto scalar grid point, required for momentum fluxes at vertical surfaces |
---|
| 1831 | REAL(wp), DIMENSION(:), ALLOCATABLE :: w_i !< w-component interpolated onto scalar grid point, required for momentum fluxes at vertical surfaces |
---|
[1691] | 1832 | |
---|
| 1833 | ! |
---|
[2232] | 1834 | !-- Calcuate surface fluxes at horizontal walls |
---|
| 1835 | IF ( .NOT. surf_vertical ) THEN |
---|
| 1836 | ! |
---|
| 1837 | !-- Compute u'w' for the total model domain at upward-facing surfaces. |
---|
| 1838 | !-- First compute the corresponding component of u* and square it. |
---|
| 1839 | IF ( .NOT. downward ) THEN |
---|
| 1840 | !$OMP PARALLEL DO PRIVATE( i, j, k, z_mo ) |
---|
| 1841 | DO m = 1, surf%ns |
---|
| 1842 | |
---|
| 1843 | i = surf%i(m) |
---|
| 1844 | j = surf%j(m) |
---|
| 1845 | k = surf%k(m) |
---|
[1691] | 1846 | |
---|
[2232] | 1847 | z_mo = surf%z_mo(m) |
---|
[1691] | 1848 | |
---|
[2232] | 1849 | surf%usws(m) = kappa * ( u(k,j,i) - u(k-1,j,i) ) & |
---|
| 1850 | / ( LOG( z_mo / surf%z0(m) ) & |
---|
| 1851 | - psi_m( z_mo / surf%ol(m) ) & |
---|
| 1852 | + psi_m( surf%z0(m) / surf%ol(m) ) ) |
---|
| 1853 | ! |
---|
| 1854 | !-- Please note, the computation of usws is not fully accurate. Actually |
---|
| 1855 | !-- a further interpolation of us onto the u-grid, where usws is defined, |
---|
| 1856 | !-- is required. However, this is not done as this would require several |
---|
| 1857 | !-- data transfers between 2D-grid and the surf-type. |
---|
| 1858 | !-- The impact of the missing interpolation is negligible as several |
---|
| 1859 | !-- tests had shown. |
---|
| 1860 | !-- Same also for ol. |
---|
| 1861 | surf%usws(m) = -surf%usws(m) * surf%us(m) * rho_air_zw(k-1) |
---|
[1691] | 1862 | |
---|
[2232] | 1863 | ENDDO |
---|
[1691] | 1864 | ! |
---|
[2232] | 1865 | !-- At downward-facing surfaces |
---|
| 1866 | ELSE |
---|
| 1867 | !$OMP PARALLEL DO PRIVATE( i, j, k, z_mo ) |
---|
| 1868 | DO m = 1, surf%ns |
---|
| 1869 | |
---|
| 1870 | i = surf%i(m) |
---|
| 1871 | j = surf%j(m) |
---|
| 1872 | k = surf%k(m) |
---|
[1691] | 1873 | |
---|
[2232] | 1874 | z_mo = surf%z_mo(m) |
---|
| 1875 | |
---|
| 1876 | surf%usws(m) = kappa * u(k,j,i) / LOG( z_mo / surf%z0(m) ) |
---|
[1691] | 1877 | ! |
---|
[2232] | 1878 | !-- To Do: Is the sign correct??? |
---|
| 1879 | surf%usws(m) = surf%usws(m) * surf%us(m) * rho_air_zw(k) |
---|
[1691] | 1880 | |
---|
[2232] | 1881 | ENDDO |
---|
| 1882 | ENDIF |
---|
[1691] | 1883 | |
---|
[2232] | 1884 | ! |
---|
| 1885 | !-- Compute v'w' for the total model domain. |
---|
| 1886 | !-- First compute the corresponding component of u* and square it. |
---|
| 1887 | !-- Upward-facing surfaces |
---|
| 1888 | IF ( .NOT. downward ) THEN |
---|
| 1889 | !$OMP PARALLEL DO PRIVATE( i, j, k, z_mo ) |
---|
| 1890 | DO m = 1, surf%ns |
---|
| 1891 | i = surf%i(m) |
---|
| 1892 | j = surf%j(m) |
---|
| 1893 | k = surf%k(m) |
---|
[1691] | 1894 | |
---|
[2232] | 1895 | z_mo = surf%z_mo(m) |
---|
[1691] | 1896 | |
---|
[2232] | 1897 | surf%vsws(m) = kappa * ( v(k,j,i) - v(k-1,j,i) ) & |
---|
| 1898 | / ( LOG( z_mo / surf%z0(m) ) & |
---|
| 1899 | - psi_m( z_mo / surf%ol(m) ) & |
---|
| 1900 | + psi_m( surf%z0(m) / surf%ol(m) ) ) |
---|
[1691] | 1901 | ! |
---|
[2232] | 1902 | !-- Please note, the computation of vsws is not fully accurate. Actually |
---|
| 1903 | !-- a further interpolation of us onto the v-grid, where vsws is defined, |
---|
| 1904 | !-- is required. However, this is not done as this would require several |
---|
| 1905 | !-- data transfers between 2D-grid and the surf-type. |
---|
| 1906 | !-- The impact of the missing interpolation is negligible as several |
---|
| 1907 | !-- tests had shown. |
---|
| 1908 | !-- Same also for ol. |
---|
| 1909 | surf%vsws(m) = -surf%vsws(m) * surf%us(m) * rho_air_zw(k-1) |
---|
| 1910 | ENDDO |
---|
| 1911 | ! |
---|
| 1912 | !-- Downward-facing surfaces |
---|
| 1913 | ELSE |
---|
| 1914 | !$OMP PARALLEL DO PRIVATE( i, j, k, z_mo ) |
---|
| 1915 | DO m = 1, surf%ns |
---|
| 1916 | i = surf%i(m) |
---|
| 1917 | j = surf%j(m) |
---|
| 1918 | k = surf%k(m) |
---|
[1691] | 1919 | |
---|
[2232] | 1920 | z_mo = surf%z_mo(m) |
---|
| 1921 | |
---|
| 1922 | surf%vsws(m) = kappa * v(k,j,i) / LOG( z_mo / surf%z0(m) ) |
---|
| 1923 | |
---|
| 1924 | surf%vsws(m) = surf%vsws(m) * surf%us(m) * rho_air_zw(k) |
---|
| 1925 | ENDDO |
---|
| 1926 | ENDIF |
---|
[1691] | 1927 | ! |
---|
[2232] | 1928 | !-- Compute the vertical kinematic heat flux |
---|
[2299] | 1929 | IF ( .NOT. constant_heatflux .AND. ( ( time_since_reference_point& |
---|
| 1930 | <= skip_time_do_lsm .AND. simulated_time > 0.0_wp ) .OR. & |
---|
| 1931 | .NOT. land_surface ) .AND. .NOT. urban_surface .AND. & |
---|
| 1932 | .NOT. downward ) THEN |
---|
[2232] | 1933 | !$OMP PARALLEL DO PRIVATE( i, j, k ) |
---|
| 1934 | DO m = 1, surf%ns |
---|
| 1935 | i = surf%i(m) |
---|
| 1936 | j = surf%j(m) |
---|
| 1937 | k = surf%k(m) |
---|
| 1938 | surf%shf(m) = -surf%ts(m) * surf%us(m) * rho_air_zw(k-1) |
---|
[1691] | 1939 | ENDDO |
---|
[2232] | 1940 | ENDIF |
---|
| 1941 | ! |
---|
| 1942 | !-- Compute the vertical water flux |
---|
| 1943 | IF ( .NOT. constant_waterflux .AND. humidity .AND. & |
---|
[2299] | 1944 | ( ( time_since_reference_point <= skip_time_do_lsm .AND. & |
---|
| 1945 | simulated_time > 0.0_wp ) .OR. .NOT. land_surface ) .AND. & |
---|
| 1946 | .NOT. downward ) THEN |
---|
[2232] | 1947 | !$OMP PARALLEL DO PRIVATE( i, j, k ) |
---|
| 1948 | DO m = 1, surf%ns |
---|
| 1949 | i = surf%i(m) |
---|
| 1950 | j = surf%j(m) |
---|
| 1951 | k = surf%k(m) |
---|
| 1952 | surf%qsws(m) = -surf%qs(m) * surf%us(m) * rho_air_zw(k-1) |
---|
| 1953 | ENDDO |
---|
| 1954 | ENDIF |
---|
| 1955 | ! |
---|
| 1956 | !-- Compute the vertical scalar flux |
---|
| 1957 | IF ( .NOT. constant_scalarflux .AND. passive_scalar .AND. & |
---|
| 1958 | .NOT. downward ) THEN |
---|
[2281] | 1959 | !$OMP PARALLEL DO PRIVATE( i, j ) |
---|
[2232] | 1960 | DO m = 1, surf%ns |
---|
[1691] | 1961 | |
---|
[2232] | 1962 | i = surf%i(m) |
---|
| 1963 | j = surf%j(m) |
---|
| 1964 | surf%ssws(m) = -surf%ss(m) * surf%us(m) |
---|
[1691] | 1965 | |
---|
[2232] | 1966 | ENDDO |
---|
[2292] | 1967 | ENDIF |
---|
[1691] | 1968 | ! |
---|
[2292] | 1969 | !-- Compute (turbulent) fluxes of cloud water content and cloud drop conc. |
---|
| 1970 | IF ( cloud_physics .AND. microphysics_morrison .AND. & |
---|
| 1971 | .NOT. downward) THEN |
---|
| 1972 | !$OMP PARALLEL DO PRIVATE( i, j ) |
---|
| 1973 | DO m = 1, surf%ns |
---|
| 1974 | |
---|
| 1975 | i = surf%i(m) |
---|
| 1976 | j = surf%j(m) |
---|
| 1977 | |
---|
| 1978 | surf%qcsws(m) = -surf%qcs(m) * surf%us(m) |
---|
| 1979 | surf%ncsws(m) = -surf%ncs(m) * surf%us(m) |
---|
| 1980 | ENDDO |
---|
| 1981 | ENDIF |
---|
| 1982 | ! |
---|
[2232] | 1983 | !-- Compute (turbulent) fluxes of rain water content and rain drop conc. |
---|
[2292] | 1984 | IF ( cloud_physics .AND. microphysics_seifert .AND. & |
---|
[2232] | 1985 | .NOT. downward) THEN |
---|
[2281] | 1986 | !$OMP PARALLEL DO PRIVATE( i, j ) |
---|
[2232] | 1987 | DO m = 1, surf%ns |
---|
| 1988 | |
---|
| 1989 | i = surf%i(m) |
---|
| 1990 | j = surf%j(m) |
---|
| 1991 | |
---|
| 1992 | surf%qrsws(m) = -surf%qrs(m) * surf%us(m) |
---|
| 1993 | surf%nrsws(m) = -surf%nrs(m) * surf%us(m) |
---|
[1691] | 1994 | ENDDO |
---|
[2232] | 1995 | ENDIF |
---|
[1691] | 1996 | |
---|
[1960] | 1997 | ! |
---|
[2232] | 1998 | !-- Bottom boundary condition for the TKE. |
---|
| 1999 | IF ( ibc_e_b == 2 ) THEN |
---|
| 2000 | !$OMP PARALLEL DO PRIVATE( i, j, k ) |
---|
| 2001 | DO m = 1, surf%ns |
---|
| 2002 | |
---|
| 2003 | i = surf%i(m) |
---|
| 2004 | j = surf%j(m) |
---|
| 2005 | k = surf%k(m) |
---|
| 2006 | |
---|
| 2007 | e(k,j,i) = ( surf%us(m) / 0.1_wp )**2 |
---|
| 2008 | ! |
---|
| 2009 | !-- As a test: cm = 0.4 |
---|
| 2010 | ! e(k,j,i) = ( us(j,i) / 0.4_wp )**2 |
---|
| 2011 | e(k-1,j,i) = e(k,j,i) |
---|
| 2012 | |
---|
[1960] | 2013 | ENDDO |
---|
[2232] | 2014 | ENDIF |
---|
| 2015 | ! |
---|
| 2016 | !-- Calcuate surface fluxes at vertical surfaces. No stability is considered. |
---|
| 2017 | ELSE |
---|
| 2018 | ! |
---|
| 2019 | !-- Compute usvs l={0,1} and vsus l={2,3} |
---|
| 2020 | IF ( mom_uv ) THEN |
---|
| 2021 | ! |
---|
| 2022 | !-- Generalize computation by introducing flags. At north- and south- |
---|
| 2023 | !-- facing surfaces u-component is used, at east- and west-facing |
---|
| 2024 | !-- surfaces v-component is used. |
---|
| 2025 | flag_u = MERGE( 1.0_wp, 0.0_wp, l == 0 .OR. l == 1 ) |
---|
| 2026 | flag_v = MERGE( 1.0_wp, 0.0_wp, l == 2 .OR. l == 3 ) |
---|
| 2027 | !$OMP PARALLEL DO PRIVATE( i, j, k, z_mo ) |
---|
| 2028 | DO m = 1, surf%ns |
---|
| 2029 | i = surf%i(m) |
---|
| 2030 | j = surf%j(m) |
---|
| 2031 | k = surf%k(m) |
---|
[1691] | 2032 | |
---|
[2232] | 2033 | z_mo = surf%z_mo(m) |
---|
[1960] | 2034 | |
---|
[2232] | 2035 | surf%mom_flux_uv(m) = kappa * & |
---|
| 2036 | ( flag_u * u(k,j,i) + flag_v * v(k,j,i) ) / & |
---|
| 2037 | LOG( z_mo / surf%z0(m) ) |
---|
| 2038 | |
---|
| 2039 | surf%mom_flux_uv(m) = & |
---|
| 2040 | - surf%mom_flux_uv(m) * surf%us(m) |
---|
| 2041 | ENDDO |
---|
| 2042 | ENDIF |
---|
[1691] | 2043 | ! |
---|
[2232] | 2044 | !-- Compute wsus l={0,1} and wsvs l={2,3} |
---|
| 2045 | IF ( mom_w ) THEN |
---|
| 2046 | !$OMP PARALLEL DO PRIVATE( i, j, k, z_mo ) |
---|
| 2047 | DO m = 1, surf%ns |
---|
| 2048 | i = surf%i(m) |
---|
| 2049 | j = surf%j(m) |
---|
| 2050 | k = surf%k(m) |
---|
| 2051 | |
---|
| 2052 | z_mo = surf%z_mo(m) |
---|
| 2053 | |
---|
| 2054 | surf%mom_flux_w(m) = kappa * w(k,j,i) / LOG( z_mo / surf%z0(m) ) |
---|
| 2055 | |
---|
| 2056 | surf%mom_flux_w(m) = & |
---|
| 2057 | - surf%mom_flux_w(m) * surf%us(m) |
---|
[1691] | 2058 | ENDDO |
---|
[2232] | 2059 | ENDIF |
---|
| 2060 | ! |
---|
| 2061 | !-- Compute momentum fluxes used for subgrid-scale TKE production at |
---|
| 2062 | !-- vertical surfaces. In constrast to the calculated momentum fluxes at |
---|
| 2063 | !-- vertical surfaces before, which are defined on the u/v/w-grid, |
---|
| 2064 | !-- respectively), the TKE fluxes are defined at the scalar grid. |
---|
| 2065 | !-- |
---|
| 2066 | IF ( mom_tke ) THEN |
---|
| 2067 | ! |
---|
| 2068 | !-- Precalculate velocity components at scalar grid point. |
---|
| 2069 | ALLOCATE( u_i(1:surf%ns) ) |
---|
| 2070 | ALLOCATE( v_i(1:surf%ns) ) |
---|
| 2071 | ALLOCATE( w_i(1:surf%ns) ) |
---|
[1691] | 2072 | |
---|
[2232] | 2073 | IF ( l == 0 .OR. l == 1 ) THEN |
---|
| 2074 | !$OMP PARALLEL DO PRIVATE( i, j, k ) |
---|
| 2075 | DO m = 1, surf%ns |
---|
| 2076 | i = surf%i(m) |
---|
| 2077 | j = surf%j(m) |
---|
| 2078 | k = surf%k(m) |
---|
| 2079 | |
---|
| 2080 | u_i(m) = 0.5_wp * ( u(k,j,i) + u(k,j,i+1) ) |
---|
| 2081 | v_i(m) = 0.0_wp |
---|
| 2082 | w_i(m) = 0.5_wp * ( w(k,j,i) + w(k-1,j,i) ) |
---|
| 2083 | ENDDO |
---|
| 2084 | ELSE |
---|
| 2085 | !$OMP PARALLEL DO PRIVATE( i, j, k ) |
---|
| 2086 | DO m = 1, surf%ns |
---|
| 2087 | i = surf%i(m) |
---|
| 2088 | j = surf%j(m) |
---|
| 2089 | k = surf%k(m) |
---|
| 2090 | |
---|
| 2091 | u_i(m) = 0.0_wp |
---|
| 2092 | v_i(m) = 0.5_wp * ( v(k,j,i) + v(k,j+1,i) ) |
---|
| 2093 | w_i(m) = 0.5_wp * ( w(k,j,i) + w(k-1,j,i) ) |
---|
| 2094 | ENDDO |
---|
| 2095 | ENDIF |
---|
| 2096 | |
---|
[2281] | 2097 | !$OMP PARALLEL DO PRIVATE( i, j, dum, z_mo ) |
---|
[2232] | 2098 | DO m = 1, surf%ns |
---|
| 2099 | i = surf%i(m) |
---|
| 2100 | j = surf%j(m) |
---|
| 2101 | |
---|
| 2102 | z_mo = surf%z_mo(m) |
---|
| 2103 | |
---|
| 2104 | dum = kappa / LOG( z_mo / surf%z0(m) ) |
---|
[1691] | 2105 | ! |
---|
[2232] | 2106 | !-- usvs (l=0,1) and vsus (l=2,3) |
---|
| 2107 | surf%mom_flux_tke(0,m) = dum * ( u_i(m) + v_i(m) ) |
---|
[1691] | 2108 | ! |
---|
[2232] | 2109 | !-- wsvs (l=0,1) and wsus (l=2,3) |
---|
| 2110 | surf%mom_flux_tke(1,m) = dum * w_i(m) |
---|
| 2111 | |
---|
| 2112 | surf%mom_flux_tke(0:1,m) = & |
---|
| 2113 | - surf%mom_flux_tke(0:1,m) * surf%us(m) |
---|
[1691] | 2114 | ENDDO |
---|
[2232] | 2115 | ! |
---|
| 2116 | !-- Deallocate temporary arrays |
---|
| 2117 | DEALLOCATE( u_i ) |
---|
| 2118 | DEALLOCATE( v_i ) |
---|
| 2119 | DEALLOCATE( w_i ) |
---|
| 2120 | ENDIF |
---|
[1691] | 2121 | ENDIF |
---|
| 2122 | |
---|
| 2123 | END SUBROUTINE calc_surface_fluxes |
---|
| 2124 | |
---|
| 2125 | |
---|
| 2126 | ! |
---|
| 2127 | !-- Integrated stability function for momentum |
---|
| 2128 | FUNCTION psi_m( zeta ) |
---|
| 2129 | |
---|
| 2130 | USE kinds |
---|
| 2131 | |
---|
| 2132 | IMPLICIT NONE |
---|
| 2133 | |
---|
| 2134 | REAL(wp) :: psi_m !< Integrated similarity function result |
---|
| 2135 | REAL(wp) :: zeta !< Stability parameter z/L |
---|
| 2136 | REAL(wp) :: x !< dummy variable |
---|
| 2137 | |
---|
| 2138 | REAL(wp), PARAMETER :: a = 1.0_wp !< constant |
---|
| 2139 | REAL(wp), PARAMETER :: b = 0.66666666666_wp !< constant |
---|
| 2140 | REAL(wp), PARAMETER :: c = 5.0_wp !< constant |
---|
| 2141 | REAL(wp), PARAMETER :: d = 0.35_wp !< constant |
---|
| 2142 | REAL(wp), PARAMETER :: c_d_d = c / d !< constant |
---|
| 2143 | REAL(wp), PARAMETER :: bc_d_d = b * c / d !< constant |
---|
| 2144 | |
---|
| 2145 | |
---|
| 2146 | IF ( zeta < 0.0_wp ) THEN |
---|
[1788] | 2147 | x = SQRT( SQRT( 1.0_wp - 16.0_wp * zeta ) ) |
---|
[1691] | 2148 | psi_m = pi * 0.5_wp - 2.0_wp * ATAN( x ) + LOG( ( 1.0_wp + x )**2 & |
---|
| 2149 | * ( 1.0_wp + x**2 ) * 0.125_wp ) |
---|
| 2150 | ELSE |
---|
| 2151 | |
---|
| 2152 | psi_m = - b * ( zeta - c_d_d ) * EXP( -d * zeta ) - a * zeta & |
---|
| 2153 | - bc_d_d |
---|
| 2154 | ! |
---|
| 2155 | !-- Old version for stable conditions (only valid for z/L < 0.5) |
---|
| 2156 | !-- psi_m = - 5.0_wp * zeta |
---|
| 2157 | |
---|
| 2158 | ENDIF |
---|
| 2159 | |
---|
| 2160 | END FUNCTION psi_m |
---|
| 2161 | |
---|
| 2162 | |
---|
| 2163 | ! |
---|
| 2164 | !-- Integrated stability function for heat and moisture |
---|
| 2165 | FUNCTION psi_h( zeta ) |
---|
| 2166 | |
---|
| 2167 | USE kinds |
---|
| 2168 | |
---|
| 2169 | IMPLICIT NONE |
---|
| 2170 | |
---|
| 2171 | REAL(wp) :: psi_h !< Integrated similarity function result |
---|
| 2172 | REAL(wp) :: zeta !< Stability parameter z/L |
---|
| 2173 | REAL(wp) :: x !< dummy variable |
---|
| 2174 | |
---|
| 2175 | REAL(wp), PARAMETER :: a = 1.0_wp !< constant |
---|
| 2176 | REAL(wp), PARAMETER :: b = 0.66666666666_wp !< constant |
---|
| 2177 | REAL(wp), PARAMETER :: c = 5.0_wp !< constant |
---|
| 2178 | REAL(wp), PARAMETER :: d = 0.35_wp !< constant |
---|
| 2179 | REAL(wp), PARAMETER :: c_d_d = c / d !< constant |
---|
| 2180 | REAL(wp), PARAMETER :: bc_d_d = b * c / d !< constant |
---|
| 2181 | |
---|
| 2182 | |
---|
| 2183 | IF ( zeta < 0.0_wp ) THEN |
---|
[1788] | 2184 | x = SQRT( 1.0_wp - 16.0_wp * zeta ) |
---|
[1691] | 2185 | psi_h = 2.0_wp * LOG( (1.0_wp + x ) / 2.0_wp ) |
---|
| 2186 | ELSE |
---|
| 2187 | psi_h = - b * ( zeta - c_d_d ) * EXP( -d * zeta ) - (1.0_wp & |
---|
| 2188 | + 0.66666666666_wp * a * zeta )**1.5_wp - bc_d_d & |
---|
| 2189 | + 1.0_wp |
---|
| 2190 | ! |
---|
| 2191 | !-- Old version for stable conditions (only valid for z/L < 0.5) |
---|
| 2192 | !-- psi_h = - 5.0_wp * zeta |
---|
| 2193 | ENDIF |
---|
| 2194 | |
---|
| 2195 | END FUNCTION psi_h |
---|
| 2196 | |
---|
[1697] | 2197 | END MODULE surface_layer_fluxes_mod |
---|