[1691] | 1 | !> @file surface_layer_fluxes.f90 |
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| 2 | !--------------------------------------------------------------------------------! |
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| 3 | ! This file is part of PALM. |
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| 4 | ! |
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| 5 | ! PALM is free software: you can redistribute it and/or modify it under the terms |
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| 6 | ! of the GNU General Public License as published by the Free Software Foundation, |
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| 7 | ! either version 3 of the License, or (at your option) any later version. |
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| 8 | ! |
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| 9 | ! PALM is distributed in the hope that it will be useful, but WITHOUT ANY |
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| 10 | ! WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS FOR |
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| 11 | ! A PARTICULAR PURPOSE. See the GNU General Public License for more details. |
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| 12 | ! |
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| 13 | ! You should have received a copy of the GNU General Public License along with |
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| 14 | ! PALM. If not, see <http://www.gnu.org/licenses/>. |
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| 15 | ! |
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| 16 | ! Copyright 1997-2015 Leibniz Universitaet Hannover |
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| 17 | ! |
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| 18 | !--------------------------------------------------------------------------------! |
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| 19 | ! Current revisions: |
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[1747] | 20 | ! ------------------ |
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[1758] | 21 | ! |
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[1789] | 22 | ! |
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[1692] | 23 | ! Former revisions: |
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| 24 | ! ----------------- |
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| 25 | ! $Id: surface_layer_fluxes.f90 1789 2016-03-10 11:02:40Z maronga $ |
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| 26 | ! |
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[1789] | 27 | ! 1788 2016-03-10 11:01:04Z maronga |
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| 28 | ! Added parameter z0q which replaces z0h in the similarity functions for |
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| 29 | ! humidity. |
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| 30 | ! Syntax layout improved. |
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| 31 | ! |
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[1758] | 32 | ! 1757 2016-02-22 15:49:32Z maronga |
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| 33 | ! Minor fixes. |
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| 34 | ! |
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[1750] | 35 | ! 1749 2016-02-09 12:19:56Z raasch |
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| 36 | ! further OpenACC adjustments |
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| 37 | ! |
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[1748] | 38 | ! 1747 2016-02-08 12:25:53Z raasch |
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| 39 | ! adjustments for OpenACC usage |
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| 40 | ! |
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[1710] | 41 | ! 1709 2015-11-04 14:47:01Z maronga |
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| 42 | ! Bugfix: division by zero could occur when calculating rib at low wind speeds |
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| 43 | ! Bugfix: calculation of uv_total for neutral = .T., initial value for ol for |
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| 44 | ! neutral = .T. |
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| 45 | ! |
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[1706] | 46 | ! 1705 2015-11-02 14:28:56Z maronga |
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| 47 | ! Typo removed |
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| 48 | ! |
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[1698] | 49 | ! 1697 2015-10-28 17:14:10Z raasch |
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| 50 | ! FORTRAN and OpenMP errors removed |
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| 51 | ! |
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[1697] | 52 | ! 1696 2015-10-27 10:03:34Z maronga |
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[1691] | 53 | ! Modularized and completely re-written version of prandtl_fluxes.f90. In the |
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| 54 | ! course of the re-writing two additional methods have been implemented. See |
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| 55 | ! updated description. |
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| 56 | ! |
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| 57 | ! 1551 2015-03-03 14:18:16Z maronga |
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| 58 | ! Removed land surface model part. The surface fluxes are now always calculated |
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| 59 | ! within prandtl_fluxes, based on the given surface temperature/humidity (which |
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| 60 | ! is either provided by the land surface model, by large scale forcing data, or |
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| 61 | ! directly prescribed by the user. |
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| 62 | ! |
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| 63 | ! 1496 2014-12-02 17:25:50Z maronga |
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| 64 | ! Adapted for land surface model |
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| 65 | ! |
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| 66 | ! 1494 2014-11-21 17:14:03Z maronga |
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| 67 | ! Bugfixes: qs is now calculated before calculation of Rif. calculation of |
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| 68 | ! buoyancy flux in Rif corrected (added missing humidity term), allow use of |
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| 69 | ! topography for coupled runs (not tested) |
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| 70 | ! |
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| 71 | ! 1361 2014-04-16 15:17:48Z hoffmann |
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| 72 | ! Bugfix: calculation of turbulent fluxes of rain water content (qrsws) and rain |
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| 73 | ! drop concentration (nrsws) added |
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| 74 | ! |
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| 75 | ! 1340 2014-03-25 19:45:13Z kanani |
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| 76 | ! REAL constants defined as wp-kind |
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| 77 | ! |
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| 78 | ! 1320 2014-03-20 08:40:49Z raasch |
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| 79 | ! ONLY-attribute added to USE-statements, |
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| 80 | ! kind-parameters added to all INTEGER and REAL declaration statements, |
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| 81 | ! kinds are defined in new module kinds, |
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| 82 | ! old module precision_kind is removed, |
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| 83 | ! revision history before 2012 removed, |
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| 84 | ! comment fields (!:) to be used for variable explanations added to |
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| 85 | ! all variable declaration statements |
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| 86 | ! |
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| 87 | ! 1276 2014-01-15 13:40:41Z heinze |
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| 88 | ! Use LSF_DATA also in case of Dirichlet bottom boundary condition for scalars |
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| 89 | ! |
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| 90 | ! 1257 2013-11-08 15:18:40Z raasch |
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| 91 | ! openACC "kernels do" replaced by "kernels loop", "loop independent" added |
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| 92 | ! |
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| 93 | ! 1036 2012-10-22 13:43:42Z raasch |
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| 94 | ! code put under GPL (PALM 3.9) |
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| 95 | ! |
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| 96 | ! 1015 2012-09-27 09:23:24Z raasch |
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| 97 | ! OpenACC statements added |
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| 98 | ! |
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| 99 | ! 978 2012-08-09 08:28:32Z fricke |
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| 100 | ! roughness length for scalar quantities z0h added |
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| 101 | ! |
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| 102 | ! Revision 1.1 1998/01/23 10:06:06 raasch |
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| 103 | ! Initial revision |
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| 104 | ! |
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| 105 | ! |
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| 106 | ! Description: |
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| 107 | ! ------------ |
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| 108 | !> Diagnostic computation of vertical fluxes in the constant flux layer from the |
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| 109 | !> values of the variables at grid point k=1. Three different methods are |
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| 110 | !> available: |
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| 111 | !> 1) the "old" version (most_method = 'circular') which is fast, but inaccurate |
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| 112 | !> 2) a Newton iteration method (most_method = 'newton'), which is accurate, but |
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| 113 | !> slower |
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| 114 | !> 3) a method using a lookup table which is fast and accurate. Note, however, |
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| 115 | !> that this method cannot be used in case of roughness heterogeneity |
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| 116 | !> |
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| 117 | !> @todo (re)move large_scale_forcing actions |
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| 118 | !> @todo check/optimize OpenMP and OpenACC directives |
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| 119 | !------------------------------------------------------------------------------! |
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| 120 | MODULE surface_layer_fluxes_mod |
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| 121 | |
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| 122 | USE arrays_3d, & |
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| 123 | ONLY: e, kh, nr, nrs, nrsws, ol, pt, q, ql, qr, qrs, qrsws, qs, qsws, & |
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[1788] | 124 | shf, ts, u, us, usws, v, vpt, vsws, zu, zw, z0, z0h, z0q |
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[1691] | 125 | |
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| 126 | USE cloud_parameters, & |
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| 127 | ONLY: l_d_cp, pt_d_t |
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| 128 | |
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| 129 | USE constants, & |
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| 130 | ONLY: pi |
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| 131 | |
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| 132 | USE cpulog |
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| 133 | |
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| 134 | USE control_parameters, & |
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| 135 | ONLY: cloud_physics, constant_heatflux, constant_waterflux, & |
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| 136 | coupling_mode, g, humidity, ibc_e_b, ibc_pt_b, icloud_scheme, & |
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| 137 | initializing_actions, kappa, intermediate_timestep_count, & |
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| 138 | intermediate_timestep_count_max, large_scale_forcing, lsf_surf, & |
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| 139 | message_string, most_method, neutral, passive_scalar, & |
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| 140 | precipitation, pt_surface, q_surface, run_coupled, & |
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| 141 | surface_pressure, simulated_time, terminate_run, zeta_max, & |
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| 142 | zeta_min |
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| 143 | |
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| 144 | USE indices, & |
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| 145 | ONLY: nxl, nxlg, nxr, nxrg, nys, nysg, nyn, nyng, nzb_s_inner, & |
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| 146 | nzb_u_inner, nzb_v_inner |
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| 147 | |
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| 148 | USE kinds |
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| 149 | |
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| 150 | USE pegrid |
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| 151 | |
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| 152 | USE land_surface_model_mod, & |
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| 153 | ONLY: land_surface, skip_time_do_lsm |
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| 154 | |
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| 155 | IMPLICIT NONE |
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| 156 | |
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| 157 | INTEGER(iwp) :: i !< loop index x direction |
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| 158 | INTEGER(iwp) :: j !< loop index y direction |
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[1705] | 159 | INTEGER(iwp) :: k !< loop index z direction |
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[1691] | 160 | |
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| 161 | INTEGER(iwp), PARAMETER :: num_steps = 15000 !< number of steps in the lookup table |
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| 162 | |
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| 163 | LOGICAL :: coupled_run !< Flag for coupled atmosphere-ocean runs |
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| 164 | |
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| 165 | REAL(wp), DIMENSION(:,:), ALLOCATABLE :: pt1, & !< Potential temperature at first grid level (required for cloud_physics = .T.) |
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| 166 | qv1, & !< Specific humidity at first grid level (required for cloud_physics = .T.) |
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| 167 | uv_total !< Total velocity at first grid level |
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| 168 | |
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| 169 | REAL(wp), DIMENSION(0:num_steps-1) :: rib_tab, & !< Lookup table bulk Richardson number |
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| 170 | ol_tab !< Lookup table values of L |
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| 171 | |
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| 172 | REAL(wp) :: e_s, & !< Saturation water vapor pressure |
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| 173 | l_bnd = 7500, & !< Lookup table index of the last time step |
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| 174 | ol_max = 1.0E6_wp, & !< Maximum Obukhov length |
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| 175 | rib_max, & !< Maximum Richardson number in lookup table |
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| 176 | rib_min, & !< Minimum Richardson number in lookup table |
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| 177 | z_mo !< Height of the constant flux layer where MOST is assumed |
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| 178 | |
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| 179 | |
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| 180 | SAVE |
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| 181 | |
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| 182 | PRIVATE |
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| 183 | |
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[1747] | 184 | PUBLIC init_surface_layer_fluxes, pt1, qv1, surface_layer_fluxes, uv_total |
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[1691] | 185 | |
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| 186 | INTERFACE init_surface_layer_fluxes |
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| 187 | MODULE PROCEDURE init_surface_layer_fluxes |
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| 188 | END INTERFACE init_surface_layer_fluxes |
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| 189 | |
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| 190 | INTERFACE surface_layer_fluxes |
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| 191 | MODULE PROCEDURE surface_layer_fluxes |
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| 192 | END INTERFACE surface_layer_fluxes |
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| 193 | |
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| 194 | |
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| 195 | CONTAINS |
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| 196 | |
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| 197 | |
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| 198 | !------------------------------------------------------------------------------! |
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| 199 | ! Description: |
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| 200 | ! ------------ |
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| 201 | !> Main routine to compute the surface fluxes |
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| 202 | !------------------------------------------------------------------------------! |
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| 203 | SUBROUTINE surface_layer_fluxes |
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| 204 | |
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| 205 | IMPLICIT NONE |
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| 206 | |
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| 207 | ! |
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| 208 | !-- In case cloud physics is used, it is required to derive potential |
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| 209 | !-- temperature and specific humidity at first grid level from the fields pt |
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| 210 | !-- and q |
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| 211 | IF ( cloud_physics ) THEN |
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| 212 | CALL calc_pt_q |
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| 213 | ENDIF |
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| 214 | |
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| 215 | ! |
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| 216 | !-- First, calculate the new Obukhov length, then new friction velocity, |
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| 217 | !-- followed by the new scaling parameters (th*, q*, etc.), and the new |
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| 218 | !-- surface fluxes if required. The old routine ("circular") requires a |
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| 219 | !-- different order of calls as the scaling parameters from the previous time |
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| 220 | !-- steps are used to calculate the Obukhov length |
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| 221 | |
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| 222 | ! |
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| 223 | !-- Depending on setting of most_method use the "old" routine |
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| 224 | IF ( most_method == 'circular' ) THEN |
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| 225 | |
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| 226 | CALL calc_scaling_parameters |
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| 227 | |
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[1709] | 228 | CALL calc_uv_total |
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| 229 | |
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[1691] | 230 | IF ( .NOT. neutral ) THEN |
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| 231 | CALL calc_ol |
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| 232 | ENDIF |
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| 233 | |
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| 234 | CALL calc_us |
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| 235 | |
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| 236 | CALL calc_surface_fluxes |
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| 237 | |
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| 238 | ! |
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| 239 | !-- Use either Newton iteration or a lookup table for the bulk Richardson |
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| 240 | !-- number to calculate the Obukhov length |
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[1788] | 241 | ELSEIF ( most_method == 'newton' .OR. most_method == 'lookup' ) THEN |
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[1691] | 242 | |
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[1709] | 243 | CALL calc_uv_total |
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| 244 | |
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[1691] | 245 | IF ( .NOT. neutral ) THEN |
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| 246 | CALL calc_ol |
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| 247 | ENDIF |
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| 248 | |
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| 249 | CALL calc_us |
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| 250 | |
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| 251 | CALL calc_scaling_parameters |
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| 252 | |
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| 253 | CALL calc_surface_fluxes |
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| 254 | |
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| 255 | ENDIF |
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| 256 | |
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| 257 | END SUBROUTINE surface_layer_fluxes |
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| 258 | |
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| 259 | |
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| 260 | !------------------------------------------------------------------------------! |
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| 261 | ! Description: |
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| 262 | ! ------------ |
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| 263 | !> Initializing actions for the surface layer routine. Basically, this involves |
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| 264 | !> the preparation of a lookup table for the the bulk Richardson number vs |
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| 265 | !> Obukhov length L when using the lookup table method. |
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| 266 | !------------------------------------------------------------------------------! |
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| 267 | SUBROUTINE init_surface_layer_fluxes |
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| 268 | |
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| 269 | IMPLICIT NONE |
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| 270 | |
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| 271 | INTEGER(iwp) :: l, & !< Index for loop to create lookup table |
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| 272 | num_steps_n !< Number of non-stretched zeta steps |
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| 273 | |
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| 274 | LOGICAL :: terminate_run_l = .FALSE. !< Flag to terminate run (global) |
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| 275 | |
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| 276 | REAL(wp), PARAMETER :: zeta_stretch = -10.0_wp !< Start of stretching in the free convection limit |
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| 277 | |
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| 278 | REAL(wp), DIMENSION(:), ALLOCATABLE :: zeta_tmp |
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| 279 | |
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| 280 | |
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| 281 | REAL(wp) :: zeta_step, & !< Increment of zeta |
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| 282 | regr = 1.01_wp, & !< Stretching factor of zeta_step in the free convection limit |
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| 283 | regr_old = 1.0E9_wp, & !< Stretching factor of last iteration step |
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| 284 | z0h_min = 0.0_wp, & !< Minimum value of z0h to create table |
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| 285 | z0_min = 0.0_wp !< Minimum value of z0 to create table |
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| 286 | ! |
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| 287 | !-- When cloud physics is used, arrays for storing potential temperature and |
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| 288 | !-- specific humidity at first grid level are required |
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| 289 | IF ( cloud_physics ) THEN |
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| 290 | ALLOCATE ( pt1(nysg:nyng,nxlg:nxrg) ) |
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| 291 | ALLOCATE ( qv1(nysg:nyng,nxlg:nxrg) ) |
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| 292 | ENDIF |
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| 293 | |
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| 294 | ! |
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| 295 | !-- Allocate field for storing the horizontal velocity |
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| 296 | ALLOCATE ( uv_total(nysg:nyng,nxlg:nxrg) ) |
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| 297 | |
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[1709] | 298 | |
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| 299 | ! |
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| 300 | !-- In case of runs with neutral statification, set Obukhov length to a |
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| 301 | !-- large value |
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| 302 | IF ( neutral ) ol = 1.0E10_wp |
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| 303 | |
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[1691] | 304 | IF ( most_method == 'lookup' ) THEN |
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| 305 | |
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| 306 | ! |
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| 307 | !-- Check for roughness heterogeneity. In that case terminate run and |
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| 308 | !-- inform user |
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[1788] | 309 | IF ( MINVAL( z0h ) /= MAXVAL( z0h ) .OR. & |
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[1691] | 310 | MINVAL( z0 ) /= MAXVAL( z0 ) ) THEN |
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| 311 | terminate_run_l = .TRUE. |
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| 312 | ENDIF |
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| 313 | |
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| 314 | #if defined( __parallel ) |
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| 315 | ! |
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| 316 | !-- Make a logical OR for all processes. Force termiation of model if result |
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| 317 | !-- is TRUE |
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| 318 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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| 319 | CALL MPI_ALLREDUCE( terminate_run_l, terminate_run, 1, MPI_LOGICAL, & |
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| 320 | MPI_LOR, comm2d, ierr ) |
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| 321 | #else |
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| 322 | terminate_run = terminate_run_l |
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| 323 | #endif |
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| 324 | |
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| 325 | IF ( terminate_run ) THEN |
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| 326 | message_string = 'most_method = "lookup" cannot be used in ' // & |
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| 327 | 'combination with a prescribed roughness ' // & |
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| 328 | 'heterogeneity' |
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| 329 | CALL message( 'surface_layer_fluxes', 'PA0417', 1, 2, 0, 6, 0 ) |
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| 330 | ENDIF |
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| 331 | |
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| 332 | ALLOCATE( zeta_tmp(0:num_steps-1) ) |
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| 333 | |
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| 334 | ! |
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| 335 | !-- Use the lowest possible value for z_mo |
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| 336 | k = MINVAL(nzb_s_inner) |
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| 337 | z_mo = zu(k+1) - zw(k) |
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| 338 | |
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| 339 | ! |
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| 340 | !-- Calculate z/L range from zeta_stretch to zeta_max using 90% of the |
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| 341 | !-- available steps (num_steps). The calculation is done with negative |
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| 342 | !-- values of zeta in order to simplify the stretching in the free |
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| 343 | !-- convection limit for the remaining 10% of steps. |
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| 344 | zeta_tmp(0) = - zeta_max |
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| 345 | num_steps_n = ( num_steps * 9 / 10 ) - 1 |
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| 346 | zeta_step = (zeta_max - zeta_stretch) / REAL(num_steps_n) |
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| 347 | |
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| 348 | DO l = 1, num_steps_n |
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| 349 | zeta_tmp(l) = zeta_tmp(l-1) + zeta_step |
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| 350 | ENDDO |
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| 351 | |
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| 352 | ! |
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| 353 | !-- Calculate stretching factor for the free convection range |
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[1788] | 354 | DO WHILE ( ABS( (regr-regr_old) / regr_old ) > 1.0E-10_wp ) |
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[1691] | 355 | regr_old = regr |
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| 356 | regr = ( 1.0_wp - ( -zeta_min / zeta_step ) * ( 1.0_wp - regr ) & |
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| 357 | )**( 10.0_wp / REAL(num_steps) ) |
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| 358 | ENDDO |
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| 359 | |
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| 360 | ! |
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| 361 | !-- Calculate z/L range from zeta_min to zeta_stretch |
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| 362 | DO l = num_steps_n+1, num_steps-1 |
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| 363 | zeta_tmp(l) = zeta_tmp(l-1) + zeta_step |
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| 364 | zeta_step = zeta_step * regr |
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| 365 | ENDDO |
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| 366 | |
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| 367 | ! |
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[1757] | 368 | !-- Save roughness lengths to temporary variables |
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| 369 | z0h_min = z0h(nys,nxl) |
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| 370 | z0_min = z0(nys,nxl) |
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[1691] | 371 | |
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| 372 | ! |
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| 373 | !-- Calculate lookup table for the Richardson number versus Obukhov length |
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| 374 | !-- The Richardson number (rib) is defined depending on the choice of |
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| 375 | !-- boundary conditions for temperature |
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| 376 | IF ( ibc_pt_b == 1 ) THEN |
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| 377 | DO l = 0, num_steps-1 |
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| 378 | ol_tab(l) = - z_mo / zeta_tmp(num_steps-1-l) |
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| 379 | rib_tab(l) = z_mo / ol_tab(l) / ( LOG( z_mo / z0_min ) & |
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| 380 | - psi_m( z_mo / ol_tab(l) ) & |
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| 381 | + psi_m( z0_min / ol_tab(l) ) & |
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| 382 | )**3 |
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| 383 | ENDDO |
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| 384 | ELSE |
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| 385 | DO l = 0, num_steps-1 |
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| 386 | ol_tab(l) = - z_mo / zeta_tmp(num_steps-1-l) |
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| 387 | rib_tab(l) = z_mo / ol_tab(l) * ( LOG( z_mo / z0h_min ) & |
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| 388 | - psi_h( z_mo / ol_tab(l) ) & |
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| 389 | + psi_h( z0h_min / ol_tab(l) ) & |
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| 390 | ) & |
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| 391 | / ( LOG( z_mo / z0_min ) & |
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| 392 | - psi_m( z_mo / ol_tab(l) ) & |
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| 393 | + psi_m( z0_min / ol_tab(l) ) & |
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| 394 | )**2 |
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| 395 | ENDDO |
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| 396 | ENDIF |
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| 397 | |
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| 398 | ! |
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| 399 | !-- Determine minimum values of rib in the lookup table. Set upper limit |
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| 400 | !-- to critical Richardson number (0.25) |
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| 401 | rib_min = MINVAL(rib_tab) |
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| 402 | rib_max = 0.25 !MAXVAL(rib_tab) |
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| 403 | |
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| 404 | DEALLOCATE( zeta_tmp ) |
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| 405 | ENDIF |
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| 406 | |
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| 407 | END SUBROUTINE init_surface_layer_fluxes |
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| 408 | |
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| 409 | |
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| 410 | !------------------------------------------------------------------------------! |
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| 411 | ! Description: |
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| 412 | ! ------------ |
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[1709] | 413 | !> Compute the absolute value of the horizontal velocity (relative to the |
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| 414 | !> surface). This is required by all methods |
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[1691] | 415 | !------------------------------------------------------------------------------! |
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[1709] | 416 | SUBROUTINE calc_uv_total |
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[1691] | 417 | |
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| 418 | IMPLICIT NONE |
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| 419 | |
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| 420 | |
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[1747] | 421 | !$OMP PARALLEL DO PRIVATE( k ) |
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| 422 | !$acc kernels loop present( nzb_s_inner, u, uv_total, v ) private( j, k ) |
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[1691] | 423 | DO i = nxl, nxr |
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| 424 | DO j = nys, nyn |
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| 425 | |
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| 426 | k = nzb_s_inner(j,i) |
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| 427 | uv_total(j,i) = SQRT( ( 0.5_wp * ( u(k+1,j,i) + u(k+1,j,i+1) & |
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| 428 | - u(k,j,i) - u(k,j,i+1) ) )**2 + & |
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| 429 | ( 0.5_wp * ( v(k+1,j,i) + v(k+1,j+1,i) & |
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| 430 | - v(k,j,i) - v(k,j+1,i) ) )**2 ) |
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| 431 | |
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| 432 | ! |
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| 433 | !-- For too small values of the local wind, MOST does not work. A |
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| 434 | !-- threshold value is thus set if required |
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| 435 | ! uv_total(j,i) = MAX(0.01_wp,uv_total(j,i)) |
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| 436 | |
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| 437 | ENDDO |
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| 438 | ENDDO |
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| 439 | |
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| 440 | ! |
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| 441 | !-- Values of uv_total need to be exchanged at the ghost boundaries |
---|
| 442 | !$acc update host( uv_total ) |
---|
| 443 | CALL exchange_horiz_2d( uv_total ) |
---|
| 444 | !$acc update device( uv_total ) |
---|
| 445 | |
---|
[1709] | 446 | END SUBROUTINE calc_uv_total |
---|
| 447 | |
---|
| 448 | |
---|
| 449 | !------------------------------------------------------------------------------! |
---|
| 450 | ! Description: |
---|
| 451 | ! ------------ |
---|
| 452 | !> Calculate the Obukhov length (L) and Richardson flux number (z/L) |
---|
| 453 | !------------------------------------------------------------------------------! |
---|
| 454 | SUBROUTINE calc_ol |
---|
| 455 | |
---|
| 456 | IMPLICIT NONE |
---|
| 457 | |
---|
| 458 | INTEGER(iwp) :: iter, & !< Newton iteration step |
---|
| 459 | l !< look index |
---|
| 460 | |
---|
| 461 | REAL(wp), DIMENSION(nysg:nyng,nxlg:nxrg) :: rib !< Bulk Richardson number |
---|
| 462 | |
---|
| 463 | REAL(wp) :: f, & !< Function for Newton iteration: f = Ri - [...]/[...]^2 = 0 |
---|
| 464 | f_d_ol, & !< Derivative of f |
---|
| 465 | ol_l, & !< Lower bound of L for Newton iteration |
---|
| 466 | ol_m, & !< Previous value of L for Newton iteration |
---|
| 467 | ol_old, & !< Previous time step value of L |
---|
| 468 | ol_u !< Upper bound of L for Newton iteration |
---|
| 469 | |
---|
[1691] | 470 | IF ( TRIM( most_method ) /= 'circular' ) THEN |
---|
| 471 | |
---|
[1747] | 472 | !$acc data present( nzb_s_inner, pt, q, qsws, rib, shf, uv_total, vpt, zu, zw ) |
---|
| 473 | |
---|
[1691] | 474 | !$OMP PARALLEL DO PRIVATE( k, z_mo ) |
---|
[1747] | 475 | !$acc kernels loop private( j, k, z_mo ) |
---|
[1691] | 476 | DO i = nxl, nxr |
---|
| 477 | DO j = nys, nyn |
---|
| 478 | |
---|
| 479 | k = nzb_s_inner(j,i) |
---|
| 480 | z_mo = zu(k+1) - zw(k) |
---|
| 481 | |
---|
| 482 | ! |
---|
| 483 | !-- Evaluate bulk Richardson number (calculation depends on |
---|
| 484 | !-- definition based on setting of boundary conditions |
---|
| 485 | IF ( ibc_pt_b /= 1 ) THEN |
---|
| 486 | IF ( humidity ) THEN |
---|
| 487 | rib(j,i) = g * z_mo * ( vpt(k+1,j,i) - vpt(k,j,i) ) & |
---|
[1709] | 488 | / ( uv_total(j,i)**2 * vpt(k+1,j,i) + 1.0E-20_wp ) |
---|
[1691] | 489 | ELSE |
---|
| 490 | rib(j,i) = g * z_mo * ( pt(k+1,j,i) - pt(k,j,i) ) & |
---|
[1709] | 491 | / ( uv_total(j,i)**2 * pt(k+1,j,i) + 1.0E-20_wp ) |
---|
[1691] | 492 | ENDIF |
---|
| 493 | ELSE |
---|
| 494 | ! |
---|
| 495 | !-- When using Neumann boundary conditions, the buoyancy flux |
---|
| 496 | !-- is required but cannot be calculated at the surface, as pt |
---|
| 497 | !-- and q are not known at the surface. Hence the values at |
---|
| 498 | !-- first grid level are used to estimate the buoyancy flux |
---|
| 499 | IF ( humidity ) THEN |
---|
| 500 | rib(j,i) = - g * z_mo * ( ( 1.0_wp + 0.61_wp & |
---|
| 501 | * q(k+1,j,i) ) * shf(j,i) + 0.61_wp & |
---|
| 502 | * pt(k+1,j,i) * qsws(j,i) ) & |
---|
[1709] | 503 | / ( uv_total(j,i)**3 * vpt(k+1,j,i) * kappa**2& |
---|
| 504 | + 1.0E-20_wp) |
---|
[1691] | 505 | ELSE |
---|
| 506 | rib(j,i) = - g * z_mo * shf(j,i) & |
---|
[1709] | 507 | / ( uv_total(j,i)**3 * pt(k+1,j,i) * kappa**2 & |
---|
| 508 | + 1.0E-20_wp ) |
---|
[1691] | 509 | ENDIF |
---|
| 510 | ENDIF |
---|
| 511 | |
---|
| 512 | ENDDO |
---|
| 513 | ENDDO |
---|
[1747] | 514 | !$acc end data |
---|
[1691] | 515 | |
---|
| 516 | ENDIF |
---|
| 517 | |
---|
| 518 | ! |
---|
| 519 | !-- Calculate the Obukhov length either using a Newton iteration |
---|
| 520 | !-- method, via a lookup table, or using the old circular way |
---|
| 521 | IF ( TRIM( most_method ) == 'newton' ) THEN |
---|
| 522 | |
---|
| 523 | !$OMP PARALLEL DO PRIVATE( k, z_mo ) |
---|
[1749] | 524 | !# WARNING: does not work on GPU so far because of DO-loop with |
---|
| 525 | !# undetermined iterations |
---|
[1747] | 526 | !!!!!!$acc kernels loop |
---|
[1691] | 527 | DO i = nxl, nxr |
---|
| 528 | DO j = nys, nyn |
---|
| 529 | |
---|
| 530 | k = nzb_s_inner(j,i) |
---|
| 531 | z_mo = zu(k+1) - zw(k) |
---|
| 532 | |
---|
| 533 | ! |
---|
| 534 | !-- Store current value in case the Newton iteration fails |
---|
| 535 | ol_old = ol(j,i) |
---|
| 536 | |
---|
| 537 | ! |
---|
| 538 | !-- Ensure that the bulk Richardson number and the Obukhov |
---|
| 539 | !-- lengtH have the same sign |
---|
[1788] | 540 | IF ( rib(j,i) * ol(j,i) < 0.0_wp .OR. & |
---|
[1691] | 541 | ABS( ol(j,i) ) == ol_max ) THEN |
---|
| 542 | IF ( rib(j,i) > 0.0_wp ) ol(j,i) = 0.01_wp |
---|
| 543 | IF ( rib(j,i) < 0.0_wp ) ol(j,i) = -0.01_wp |
---|
| 544 | ENDIF |
---|
| 545 | ! |
---|
| 546 | !-- Iteration to find Obukhov length |
---|
| 547 | iter = 0 |
---|
| 548 | DO |
---|
| 549 | iter = iter + 1 |
---|
| 550 | ! |
---|
| 551 | !-- In case of divergence, use the value of the previous time step |
---|
| 552 | IF ( iter > 1000 ) THEN |
---|
| 553 | ol(j,i) = ol_old |
---|
| 554 | EXIT |
---|
| 555 | ENDIF |
---|
| 556 | |
---|
| 557 | ol_m = ol(j,i) |
---|
| 558 | ol_l = ol_m - 0.001_wp * ol_m |
---|
| 559 | ol_u = ol_m + 0.001_wp * ol_m |
---|
| 560 | |
---|
| 561 | |
---|
| 562 | IF ( ibc_pt_b /= 1 ) THEN |
---|
| 563 | ! |
---|
| 564 | !-- Calculate f = Ri - [...]/[...]^2 = 0 |
---|
| 565 | f = rib(j,i) - ( z_mo / ol_m ) * ( LOG( z_mo / z0h(j,i) )& |
---|
| 566 | - psi_h( z_mo / ol_m ) & |
---|
| 567 | + psi_h( z0h(j,i) / ol_m ) & |
---|
| 568 | ) & |
---|
| 569 | / ( LOG( z_mo / z0(j,i) ) & |
---|
| 570 | - psi_m( z_mo / ol_m ) & |
---|
| 571 | + psi_m( z0(j,i) / ol_m ) & |
---|
| 572 | )**2 |
---|
| 573 | |
---|
| 574 | ! |
---|
| 575 | !-- Calculate df/dL |
---|
| 576 | f_d_ol = ( - ( z_mo / ol_u ) * ( LOG( z_mo / z0h(j,i) ) & |
---|
| 577 | - psi_h( z_mo / ol_u ) & |
---|
| 578 | + psi_h( z0h(j,i) / ol_u ) & |
---|
| 579 | ) & |
---|
| 580 | / ( LOG( z_mo / z0(j,i) ) & |
---|
| 581 | - psi_m( z_mo / ol_u ) & |
---|
| 582 | + psi_m( z0(j,i) / ol_u ) & |
---|
| 583 | )**2 & |
---|
| 584 | + ( z_mo / ol_l ) * ( LOG( z_mo / z0h(j,i) ) & |
---|
| 585 | - psi_h( z_mo / ol_l ) & |
---|
| 586 | + psi_h( z0h(j,i) / ol_l ) & |
---|
| 587 | ) & |
---|
| 588 | / ( LOG( z_mo / z0(j,i) ) & |
---|
| 589 | - psi_m( z_mo / ol_l ) & |
---|
| 590 | + psi_m( z0(j,i) / ol_l ) & |
---|
| 591 | )**2 & |
---|
| 592 | ) / ( ol_u - ol_l ) |
---|
| 593 | ELSE |
---|
| 594 | ! |
---|
| 595 | !-- Calculate f = Ri - 1 /[...]^3 = 0 |
---|
| 596 | f = rib(j,i) - ( z_mo / ol_m ) / ( LOG( z_mo / z0(j,i) )& |
---|
| 597 | - psi_m( z_mo / ol_m ) & |
---|
| 598 | + psi_m( z0(j,i) / ol_m ) & |
---|
| 599 | )**3 |
---|
| 600 | |
---|
| 601 | ! |
---|
| 602 | !-- Calculate df/dL |
---|
| 603 | f_d_ol = ( - ( z_mo / ol_u ) / ( LOG( z_mo / z0(j,i) ) & |
---|
| 604 | - psi_m( z_mo / ol_u ) & |
---|
| 605 | + psi_m( z0(j,i) / ol_u ) & |
---|
| 606 | )**3 & |
---|
| 607 | + ( z_mo / ol_l ) / ( LOG( z_mo / z0(j,i) ) & |
---|
| 608 | - psi_m( z_mo / ol_l ) & |
---|
| 609 | + psi_m( z0(j,i) / ol_l ) & |
---|
| 610 | )**3 & |
---|
| 611 | ) / ( ol_u - ol_l ) |
---|
| 612 | ENDIF |
---|
| 613 | ! |
---|
| 614 | !-- Calculate new L |
---|
| 615 | ol(j,i) = ol_m - f / f_d_ol |
---|
| 616 | |
---|
| 617 | ! |
---|
| 618 | !-- Ensure that the bulk Richardson number and the Obukhov |
---|
| 619 | !-- length have the same sign and ensure convergence. |
---|
| 620 | IF ( ol(j,i) * ol_m < 0.0_wp ) ol(j,i) = ol_m * 0.5_wp |
---|
| 621 | |
---|
| 622 | ! |
---|
| 623 | !-- If unrealistic value occurs, set L to the maximum |
---|
| 624 | !-- value that is allowed |
---|
| 625 | IF ( ABS( ol(j,i) ) > ol_max ) THEN |
---|
| 626 | ol(j,i) = ol_max |
---|
| 627 | EXIT |
---|
| 628 | ENDIF |
---|
| 629 | ! |
---|
| 630 | !-- Check for convergence |
---|
| 631 | IF ( ABS( ( ol(j,i) - ol_m ) / ol(j,i) ) < 1.0E-4_wp ) THEN |
---|
| 632 | EXIT |
---|
| 633 | ELSE |
---|
| 634 | CYCLE |
---|
| 635 | ENDIF |
---|
| 636 | |
---|
| 637 | ENDDO |
---|
| 638 | |
---|
| 639 | ENDDO |
---|
| 640 | ENDDO |
---|
| 641 | |
---|
| 642 | ELSEIF ( TRIM( most_method ) == 'lookup' ) THEN |
---|
| 643 | |
---|
| 644 | !$OMP PARALLEL DO PRIVATE( k, z_mo ) |
---|
[1788] | 645 | !# WARNING: does not work on GPU so far because of DO WHILE construct |
---|
[1747] | 646 | !!!!!!$acc kernels loop |
---|
[1691] | 647 | DO i = nxl, nxr |
---|
| 648 | DO j = nys, nyn |
---|
| 649 | |
---|
| 650 | ! |
---|
| 651 | !-- If the bulk Richardson number is outside the range of the lookup |
---|
| 652 | !-- table, set it to the exceeding threshold value |
---|
| 653 | IF ( rib(j,i) < rib_min ) rib(j,i) = rib_min |
---|
| 654 | IF ( rib(j,i) > rib_max ) rib(j,i) = rib_max |
---|
| 655 | |
---|
| 656 | ! |
---|
| 657 | !-- Find the correct index bounds for linear interpolation. As the |
---|
| 658 | !-- Richardson number will not differ very much from time step to |
---|
| 659 | !-- time step , use the index from the last step and search in the |
---|
| 660 | !-- correct direction |
---|
| 661 | l = l_bnd |
---|
| 662 | IF ( rib_tab(l) - rib(j,i) > 0.0_wp ) THEN |
---|
[1788] | 663 | DO WHILE ( rib_tab(l-1) - rib(j,i) > 0.0_wp .AND. l > 0 ) |
---|
[1691] | 664 | l = l-1 |
---|
| 665 | ENDDO |
---|
| 666 | ELSE |
---|
[1788] | 667 | DO WHILE ( rib_tab(l) - rib(j,i) < 0.0_wp & |
---|
| 668 | .AND. l < num_steps-1 ) |
---|
[1691] | 669 | l = l+1 |
---|
| 670 | ENDDO |
---|
| 671 | ENDIF |
---|
| 672 | l_bnd = l |
---|
| 673 | |
---|
| 674 | ! |
---|
| 675 | !-- Linear interpolation to find the correct value of z/L |
---|
[1788] | 676 | ol(j,i) = ( ol_tab(l-1) + ( ol_tab(l) - ol_tab(l-1) ) & |
---|
| 677 | / ( rib_tab(l) - rib_tab(l-1) ) & |
---|
[1691] | 678 | * ( rib(j,i) - rib_tab(l-1) ) ) |
---|
| 679 | |
---|
| 680 | ENDDO |
---|
| 681 | ENDDO |
---|
| 682 | |
---|
| 683 | ELSEIF ( TRIM( most_method ) == 'circular' ) THEN |
---|
| 684 | |
---|
| 685 | !$OMP PARALLEL DO PRIVATE( k, z_mo ) |
---|
[1747] | 686 | !$acc kernels loop present( nzb_s_inner, ol, pt, pt1, q, ql, qs, qv1, ts, us, vpt, zu, zw ) private( j, k, z_mo ) |
---|
[1691] | 687 | DO i = nxl, nxr |
---|
| 688 | DO j = nys, nyn |
---|
| 689 | |
---|
| 690 | k = nzb_s_inner(j,i) |
---|
| 691 | z_mo = zu(k+1) - zw(k) |
---|
| 692 | |
---|
| 693 | IF ( .NOT. humidity ) THEN |
---|
| 694 | ol(j,i) = ( pt(k+1,j,i) * us(j,i)**2 ) / ( kappa * g & |
---|
| 695 | * ts(j,i) + 1E-30_wp ) |
---|
| 696 | ELSEIF ( cloud_physics ) THEN |
---|
| 697 | |
---|
| 698 | ol(j,i) = ( vpt(k+1,j,i) * us(j,i)**2 ) / ( kappa * g & |
---|
| 699 | * ( ts(j,i) + 0.61_wp * pt1(j,i) * qs(j,i) & |
---|
| 700 | + 0.61_wp * qv1(j,i) * ts(j,i) - ts(j,i) & |
---|
| 701 | * ql(k+1,j,i) ) + 1E-30_wp ) |
---|
| 702 | ELSE |
---|
| 703 | ol(j,i) = ( vpt(k+1,j,i) * us(j,i)**2 ) / ( kappa * g & |
---|
| 704 | * ( ts(j,i) + 0.61_wp * pt(k+1,j,i) * qs(j,i) & |
---|
| 705 | + 0.61_wp * q(k+1,j,i) * ts(j,i) ) + 1E-30_wp ) |
---|
| 706 | ENDIF |
---|
| 707 | ! |
---|
| 708 | !-- Limit the value range of the Obukhov length. |
---|
| 709 | !-- This is necessary for very small velocities (u,v --> 0), because |
---|
| 710 | !-- the absolute value of ol can then become very small, which in |
---|
| 711 | !-- consequence would result in very large shear stresses and very |
---|
| 712 | !-- small momentum fluxes (both are generally unrealistic). |
---|
| 713 | IF ( ( z_mo / ol(j,i) ) < zeta_min ) ol(j,i) = z_mo / zeta_min |
---|
| 714 | IF ( ( z_mo / ol(j,i) ) > zeta_max ) ol(j,i) = z_mo / zeta_max |
---|
| 715 | |
---|
| 716 | ENDDO |
---|
| 717 | ENDDO |
---|
| 718 | |
---|
| 719 | ENDIF |
---|
| 720 | |
---|
| 721 | ! |
---|
| 722 | !-- Values of ol at ghost point locations are needed for the evaluation |
---|
| 723 | !-- of usws and vsws. |
---|
| 724 | !$acc update host( ol ) |
---|
| 725 | CALL exchange_horiz_2d( ol ) |
---|
| 726 | !$acc update device( ol ) |
---|
| 727 | |
---|
| 728 | END SUBROUTINE calc_ol |
---|
| 729 | |
---|
| 730 | ! |
---|
| 731 | !-- Calculate friction velocity u* |
---|
| 732 | SUBROUTINE calc_us |
---|
| 733 | |
---|
| 734 | IMPLICIT NONE |
---|
| 735 | |
---|
[1697] | 736 | !$OMP PARALLEL DO PRIVATE( k, z_mo ) |
---|
[1749] | 737 | !$acc kernels loop present( nzb_s_inner, ol, us, uv_total, zu, zw, z0 ) private( j, k, z_mo ) |
---|
[1691] | 738 | DO i = nxlg, nxrg |
---|
| 739 | DO j = nysg, nyng |
---|
| 740 | |
---|
| 741 | k = nzb_s_inner(j,i)+1 |
---|
| 742 | z_mo = zu(k+1) - zw(k) |
---|
| 743 | |
---|
| 744 | ! |
---|
| 745 | !-- Compute u* at the scalars' grid points |
---|
| 746 | us(j,i) = kappa * uv_total(j,i) / ( LOG( z_mo / z0(j,i) ) & |
---|
| 747 | - psi_m( z_mo / ol(j,i) ) & |
---|
| 748 | + psi_m( z0(j,i) / ol(j,i) ) ) |
---|
| 749 | ENDDO |
---|
| 750 | ENDDO |
---|
| 751 | |
---|
| 752 | END SUBROUTINE calc_us |
---|
| 753 | |
---|
| 754 | ! |
---|
| 755 | !-- Calculate potential temperature and specific humidity at first grid level |
---|
| 756 | SUBROUTINE calc_pt_q |
---|
| 757 | |
---|
| 758 | IMPLICIT NONE |
---|
| 759 | |
---|
[1747] | 760 | !$acc kernels loop present( nzb_s_inner, pt, pt1, pt_d_t, q, ql, qv1 ) private( j, k ) |
---|
[1691] | 761 | DO i = nxlg, nxrg |
---|
| 762 | DO j = nysg, nyng |
---|
| 763 | k = nzb_s_inner(j,i)+1 |
---|
| 764 | pt1(j,i) = pt(k,j,i) + l_d_cp * pt_d_t(k) * ql(k,j,i) |
---|
| 765 | qv1(j,i) = q(k,j,i) - ql(k,j,i) |
---|
| 766 | ENDDO |
---|
| 767 | ENDDO |
---|
| 768 | |
---|
| 769 | END SUBROUTINE calc_pt_q |
---|
| 770 | |
---|
| 771 | ! |
---|
| 772 | !-- Calculate the other MOST scaling parameters theta*, q*, (qr*, nr*) |
---|
| 773 | SUBROUTINE calc_scaling_parameters |
---|
| 774 | |
---|
| 775 | IMPLICIT NONE |
---|
| 776 | |
---|
| 777 | ! |
---|
| 778 | !-- Data information for accelerators |
---|
| 779 | !$acc data present( e, nrsws, nzb_u_inner, nzb_v_inner, nzb_s_inner, pt ) & |
---|
| 780 | !$acc present( q, qs, qsws, qrsws, shf, ts, u, us, usws, v ) & |
---|
| 781 | !$acc present( vpt, vsws, zu, zw, z0, z0h ) |
---|
| 782 | ! |
---|
| 783 | !-- Compute theta* |
---|
| 784 | IF ( constant_heatflux ) THEN |
---|
| 785 | |
---|
| 786 | ! |
---|
| 787 | !-- For a given heat flux in the surface layer: |
---|
| 788 | !$OMP PARALLEL DO |
---|
[1747] | 789 | !$acc kernels loop private( j ) |
---|
[1691] | 790 | DO i = nxlg, nxrg |
---|
| 791 | DO j = nysg, nyng |
---|
| 792 | ts(j,i) = -shf(j,i) / ( us(j,i) + 1E-30_wp ) |
---|
| 793 | ! |
---|
| 794 | !-- ts must be limited, because otherwise overflow may occur in case |
---|
| 795 | !-- of us=0 when computing ol further below |
---|
| 796 | IF ( ts(j,i) < -1.05E5_wp ) ts(j,i) = -1.0E5_wp |
---|
| 797 | IF ( ts(j,i) > 1.0E5_wp ) ts(j,i) = 1.0E5_wp |
---|
| 798 | ENDDO |
---|
| 799 | ENDDO |
---|
| 800 | |
---|
| 801 | ELSE |
---|
| 802 | ! |
---|
| 803 | !-- For a given surface temperature: |
---|
[1788] | 804 | IF ( large_scale_forcing .AND. lsf_surf ) THEN |
---|
[1691] | 805 | !$OMP PARALLEL DO |
---|
[1747] | 806 | !$acc kernels loop private( j, k ) |
---|
[1691] | 807 | DO i = nxlg, nxrg |
---|
| 808 | DO j = nysg, nyng |
---|
| 809 | k = nzb_s_inner(j,i) |
---|
| 810 | pt(k,j,i) = pt_surface |
---|
| 811 | ENDDO |
---|
| 812 | ENDDO |
---|
| 813 | ENDIF |
---|
| 814 | |
---|
[1697] | 815 | !$OMP PARALLEL DO PRIVATE( k, z_mo ) |
---|
[1749] | 816 | !$acc kernels loop present( nzb_s_inner, ol, pt, pt1, ts, zu, zw, z0h ) private( j, k, z_mo ) |
---|
[1691] | 817 | DO i = nxlg, nxrg |
---|
| 818 | DO j = nysg, nyng |
---|
| 819 | |
---|
| 820 | k = nzb_s_inner(j,i) |
---|
| 821 | z_mo = zu(k+1) - zw(k) |
---|
| 822 | |
---|
| 823 | IF ( cloud_physics ) THEN |
---|
| 824 | ts(j,i) = kappa * ( pt1(j,i) - pt(k,j,i) ) & |
---|
| 825 | / ( LOG( z_mo / z0h(j,i) ) & |
---|
| 826 | - psi_h( z_mo / ol(j,i) ) & |
---|
| 827 | + psi_h( z0h(j,i) / ol(j,i) ) ) |
---|
| 828 | ELSE |
---|
| 829 | ts(j,i) = kappa * ( pt(k+1,j,i) - pt(k,j,i) ) & |
---|
| 830 | / ( LOG( z_mo / z0h(j,i) ) & |
---|
| 831 | - psi_h( z_mo / ol(j,i) ) & |
---|
| 832 | + psi_h( z0h(j,i) / ol(j,i) ) ) |
---|
| 833 | ENDIF |
---|
| 834 | |
---|
| 835 | ENDDO |
---|
| 836 | ENDDO |
---|
| 837 | ENDIF |
---|
| 838 | |
---|
| 839 | ! |
---|
| 840 | !-- If required compute q* |
---|
| 841 | IF ( humidity .OR. passive_scalar ) THEN |
---|
| 842 | IF ( constant_waterflux ) THEN |
---|
| 843 | ! |
---|
[1788] | 844 | !-- For a given water flux in the surface layer |
---|
[1691] | 845 | !$OMP PARALLEL DO |
---|
[1747] | 846 | !$acc kernels loop private( j ) |
---|
[1691] | 847 | DO i = nxlg, nxrg |
---|
| 848 | DO j = nysg, nyng |
---|
| 849 | qs(j,i) = -qsws(j,i) / ( us(j,i) + 1E-30_wp ) |
---|
| 850 | ENDDO |
---|
| 851 | ENDDO |
---|
| 852 | |
---|
| 853 | ELSE |
---|
[1788] | 854 | coupled_run = ( coupling_mode == 'atmosphere_to_ocean' .AND. & |
---|
[1691] | 855 | run_coupled ) |
---|
| 856 | |
---|
[1788] | 857 | IF ( large_scale_forcing .AND. lsf_surf ) THEN |
---|
[1691] | 858 | !$OMP PARALLEL DO |
---|
[1747] | 859 | !$acc kernels loop private( j, k ) |
---|
[1691] | 860 | DO i = nxlg, nxrg |
---|
| 861 | DO j = nysg, nyng |
---|
| 862 | k = nzb_s_inner(j,i) |
---|
| 863 | q(k,j,i) = q_surface |
---|
| 864 | ENDDO |
---|
| 865 | ENDDO |
---|
| 866 | ENDIF |
---|
| 867 | |
---|
[1697] | 868 | !$OMP PARALLEL DO PRIVATE( e_s, k, z_mo ) |
---|
[1788] | 869 | !$acc kernels loop independent present( nzb_s_inner, ol, pt, q, qs, qv1, zu, zw, z0q ) private( e_s, j, k, z_mo ) |
---|
[1691] | 870 | DO i = nxlg, nxrg |
---|
[1749] | 871 | !$acc loop independent |
---|
[1691] | 872 | DO j = nysg, nyng |
---|
| 873 | |
---|
| 874 | k = nzb_s_inner(j,i) |
---|
| 875 | z_mo = zu(k+1) - zw(k) |
---|
| 876 | |
---|
| 877 | ! |
---|
| 878 | !-- Assume saturation for atmosphere coupled to ocean (but not |
---|
| 879 | !-- in case of precursor runs) |
---|
| 880 | IF ( coupled_run ) THEN |
---|
| 881 | e_s = 6.1_wp * & |
---|
| 882 | EXP( 0.07_wp * ( MIN(pt(k,j,i),pt(k+1,j,i)) & |
---|
| 883 | - 273.15_wp ) ) |
---|
| 884 | q(k,j,i) = 0.622_wp * e_s / ( surface_pressure - e_s ) |
---|
| 885 | ENDIF |
---|
| 886 | |
---|
| 887 | IF ( cloud_physics ) THEN |
---|
| 888 | qs(j,i) = kappa * ( qv1(j,i) - q(k,j,i) ) & |
---|
[1788] | 889 | / ( LOG( z_mo / z0q(j,i) ) & |
---|
[1691] | 890 | - psi_h( z_mo / ol(j,i) ) & |
---|
[1788] | 891 | + psi_h( z0q(j,i) / ol(j,i) ) ) |
---|
[1691] | 892 | |
---|
| 893 | ELSE |
---|
| 894 | qs(j,i) = kappa * ( q(k+1,j,i) - q(k,j,i) ) & |
---|
[1788] | 895 | / ( LOG( z_mo / z0q(j,i) ) & |
---|
[1691] | 896 | - psi_h( z_mo / ol(j,i) ) & |
---|
[1788] | 897 | + psi_h( z0q(j,i) / ol(j,i) ) ) |
---|
[1691] | 898 | ENDIF |
---|
| 899 | |
---|
| 900 | ENDDO |
---|
| 901 | ENDDO |
---|
| 902 | ENDIF |
---|
| 903 | ENDIF |
---|
| 904 | |
---|
| 905 | |
---|
| 906 | ! |
---|
| 907 | !-- If required compute qr* and nr* |
---|
[1788] | 908 | IF ( cloud_physics .AND. icloud_scheme == 0 .AND. precipitation ) & |
---|
| 909 | THEN |
---|
[1691] | 910 | |
---|
[1697] | 911 | !$OMP PARALLEL DO PRIVATE( k, z_mo ) |
---|
[1788] | 912 | !$acc kernels loop independent present( nr, nrs, nzb_s_inner, ol, qr, qrs, zu, zw, z0q ) private( j, k, z_mo ) |
---|
[1691] | 913 | DO i = nxlg, nxrg |
---|
[1749] | 914 | !$acc loop independent |
---|
[1691] | 915 | DO j = nysg, nyng |
---|
| 916 | |
---|
| 917 | k = nzb_s_inner(j,i) |
---|
| 918 | z_mo = zu(k+1) - zw(k) |
---|
| 919 | |
---|
[1749] | 920 | qrs(j,i) = kappa * ( qr(k+1,j,i) - qr(k,j,i) ) & |
---|
[1788] | 921 | / ( LOG( z_mo / z0q(j,i) ) & |
---|
[1749] | 922 | - psi_h( z_mo / ol(j,i) ) & |
---|
[1788] | 923 | + psi_h( z0q(j,i) / ol(j,i) ) ) |
---|
[1691] | 924 | |
---|
[1749] | 925 | nrs(j,i) = kappa * ( nr(k+1,j,i) - nr(k,j,i) ) & |
---|
[1788] | 926 | / ( LOG( z_mo / z0q(j,i) ) & |
---|
[1749] | 927 | - psi_h( z_mo / ol(j,i) ) & |
---|
[1788] | 928 | + psi_h( z0q(j,i) / ol(j,i) ) ) |
---|
[1691] | 929 | ENDDO |
---|
| 930 | ENDDO |
---|
| 931 | |
---|
| 932 | ENDIF |
---|
[1747] | 933 | !$acc end data |
---|
[1691] | 934 | |
---|
| 935 | END SUBROUTINE calc_scaling_parameters |
---|
| 936 | |
---|
| 937 | |
---|
| 938 | |
---|
| 939 | ! |
---|
| 940 | !-- Calculate surface fluxes usws, vsws, shf, qsws, (qrsws, nrsws) |
---|
| 941 | SUBROUTINE calc_surface_fluxes |
---|
| 942 | |
---|
| 943 | IMPLICIT NONE |
---|
| 944 | |
---|
| 945 | REAL(wp) :: ol_mid !< Grid-interpolated L |
---|
| 946 | |
---|
| 947 | ! |
---|
| 948 | !-- Compute u'w' for the total model domain. |
---|
| 949 | !-- First compute the corresponding component of u* and square it. |
---|
| 950 | !$OMP PARALLEL DO PRIVATE( k, ol_mid, z_mo ) |
---|
[1749] | 951 | !$acc kernels loop present( nzb_u_inner, ol, u, us, usws, zu, zw, z0 ) private( j, k, z_mo ) |
---|
[1691] | 952 | DO i = nxl, nxr |
---|
| 953 | DO j = nys, nyn |
---|
| 954 | |
---|
| 955 | k = nzb_u_inner(j,i) |
---|
| 956 | z_mo = zu(k+1) - zw(k) |
---|
| 957 | ! |
---|
| 958 | !-- Compute bulk Obukhov length for this point |
---|
| 959 | ol_mid = 0.5_wp * ( ol(j,i-1) + ol(j,i) ) |
---|
| 960 | |
---|
| 961 | IF ( ol_mid == 0.0_wp ) THEN |
---|
| 962 | ol_mid = MIN(ol(j,i-1), ol(j,i)) |
---|
| 963 | ENDIF |
---|
| 964 | |
---|
| 965 | usws(j,i) = kappa * ( u(k+1,j,i) - u(k,j,i) ) & |
---|
| 966 | / ( LOG( z_mo / z0(j,i) ) & |
---|
| 967 | - psi_m( z_mo / ol_mid ) & |
---|
| 968 | + psi_m( z0(j,i) / ol_mid ) ) |
---|
| 969 | |
---|
| 970 | usws(j,i) = -usws(j,i) * 0.5_wp * ( us(j,i-1) + us(j,i) ) |
---|
| 971 | ENDDO |
---|
| 972 | ENDDO |
---|
| 973 | |
---|
| 974 | ! |
---|
| 975 | !-- Compute v'w' for the total model domain. |
---|
| 976 | !-- First compute the corresponding component of u* and square it. |
---|
| 977 | !$OMP PARALLEL DO PRIVATE( k, ol_mid, z_mo ) |
---|
[1749] | 978 | !$acc kernels loop present( nzb_v_inner, ol, v, us, vsws, zu, zw, z0 ) private( j, k, ol_mid, z_mo ) |
---|
[1691] | 979 | DO i = nxl, nxr |
---|
| 980 | DO j = nys, nyn |
---|
| 981 | |
---|
| 982 | k = nzb_v_inner(j,i) |
---|
| 983 | z_mo = zu(k+1) - zw(k) |
---|
| 984 | ! |
---|
| 985 | !-- Compute bulk Obukhov length for this point |
---|
| 986 | ol_mid = 0.5_wp * ( ol(j-1,i) + ol(j,i) ) |
---|
| 987 | |
---|
| 988 | IF ( ol_mid == 0.0_wp ) THEN |
---|
| 989 | ol_mid = MIN(ol(j-1,i), ol(j-1,i)) |
---|
| 990 | ENDIF |
---|
| 991 | |
---|
| 992 | vsws(j,i) = kappa * ( v(k+1,j,i) - v(k,j,i) ) & |
---|
| 993 | / ( LOG( z_mo / z0(j,i) ) & |
---|
| 994 | - psi_m( z_mo / ol_mid ) & |
---|
| 995 | + psi_m( z0(j,i) / ol_mid ) ) |
---|
| 996 | |
---|
| 997 | vsws(j,i) = -vsws(j,i) * 0.5_wp * ( us(j,i-1) + us(j,i) ) |
---|
| 998 | |
---|
| 999 | ENDDO |
---|
| 1000 | ENDDO |
---|
| 1001 | |
---|
| 1002 | ! |
---|
| 1003 | !-- Exchange the boundaries for the momentum fluxes (is this still required?) |
---|
[1749] | 1004 | !$acc update host( usws, vsws ) |
---|
[1691] | 1005 | CALL exchange_horiz_2d( usws ) |
---|
| 1006 | CALL exchange_horiz_2d( vsws ) |
---|
| 1007 | !$acc update device( usws, vsws ) |
---|
| 1008 | |
---|
| 1009 | ! |
---|
| 1010 | !-- Compute the vertical kinematic heat flux |
---|
[1788] | 1011 | IF ( .NOT. constant_heatflux .AND. ( simulated_time <= & |
---|
| 1012 | skip_time_do_lsm .OR. .NOT. land_surface ) ) THEN |
---|
[1691] | 1013 | !$OMP PARALLEL DO |
---|
[1747] | 1014 | !$acc kernels loop independent present( shf, ts, us ) |
---|
[1691] | 1015 | DO i = nxlg, nxrg |
---|
| 1016 | !$acc loop independent |
---|
| 1017 | DO j = nysg, nyng |
---|
| 1018 | shf(j,i) = -ts(j,i) * us(j,i) |
---|
| 1019 | ENDDO |
---|
| 1020 | ENDDO |
---|
| 1021 | |
---|
| 1022 | ENDIF |
---|
| 1023 | |
---|
| 1024 | ! |
---|
| 1025 | !-- Compute the vertical water/scalar flux |
---|
[1788] | 1026 | IF ( .NOT. constant_waterflux .AND. ( humidity .OR. & |
---|
| 1027 | passive_scalar ) .AND. ( simulated_time <= skip_time_do_lsm & |
---|
| 1028 | .OR. .NOT. land_surface ) ) THEN |
---|
[1691] | 1029 | !$OMP PARALLEL DO |
---|
[1747] | 1030 | !$acc kernels loop independent present( qs, qsws, us ) |
---|
[1691] | 1031 | DO i = nxlg, nxrg |
---|
| 1032 | !$acc loop independent |
---|
| 1033 | DO j = nysg, nyng |
---|
| 1034 | qsws(j,i) = -qs(j,i) * us(j,i) |
---|
| 1035 | ENDDO |
---|
| 1036 | ENDDO |
---|
| 1037 | |
---|
| 1038 | ENDIF |
---|
| 1039 | |
---|
| 1040 | ! |
---|
| 1041 | !-- Compute (turbulent) fluxes of rain water content and rain drop conc. |
---|
| 1042 | IF ( cloud_physics .AND. icloud_scheme == 0 .AND. & |
---|
| 1043 | precipitation ) THEN |
---|
| 1044 | !$OMP PARALLEL DO |
---|
[1747] | 1045 | !$acc kernels loop independent present( nrs, nrsws, qrs, qrsws, us ) |
---|
[1691] | 1046 | DO i = nxlg, nxrg |
---|
| 1047 | !$acc loop independent |
---|
| 1048 | DO j = nysg, nyng |
---|
| 1049 | qrsws(j,i) = -qrs(j,i) * us(j,i) |
---|
| 1050 | nrsws(j,i) = -nrs(j,i) * us(j,i) |
---|
| 1051 | ENDDO |
---|
| 1052 | ENDDO |
---|
| 1053 | ENDIF |
---|
| 1054 | |
---|
| 1055 | ! |
---|
| 1056 | !-- Bottom boundary condition for the TKE |
---|
| 1057 | IF ( ibc_e_b == 2 ) THEN |
---|
| 1058 | !$OMP PARALLEL DO |
---|
[1747] | 1059 | !$acc kernels loop independent present( e, nzb_s_inner, us ) |
---|
[1691] | 1060 | DO i = nxlg, nxrg |
---|
| 1061 | !$acc loop independent |
---|
| 1062 | DO j = nysg, nyng |
---|
[1757] | 1063 | k = nzb_s_inner(j,i) |
---|
| 1064 | e(k+1,j,i) = ( us(j,i) / 0.1_wp )**2 |
---|
[1691] | 1065 | ! |
---|
| 1066 | !-- As a test: cm = 0.4 |
---|
[1757] | 1067 | ! e(k+1,j,i) = ( us(j,i) / 0.4_wp )**2 |
---|
| 1068 | e(k,j,i) = e(k+1,j,i) |
---|
[1691] | 1069 | ENDDO |
---|
| 1070 | ENDDO |
---|
| 1071 | ENDIF |
---|
| 1072 | |
---|
| 1073 | END SUBROUTINE calc_surface_fluxes |
---|
| 1074 | |
---|
| 1075 | |
---|
| 1076 | ! |
---|
| 1077 | !-- Integrated stability function for momentum |
---|
| 1078 | FUNCTION psi_m( zeta ) |
---|
| 1079 | |
---|
| 1080 | USE kinds |
---|
| 1081 | |
---|
| 1082 | IMPLICIT NONE |
---|
| 1083 | |
---|
| 1084 | REAL(wp) :: psi_m !< Integrated similarity function result |
---|
| 1085 | REAL(wp) :: zeta !< Stability parameter z/L |
---|
| 1086 | REAL(wp) :: x !< dummy variable |
---|
| 1087 | |
---|
| 1088 | REAL(wp), PARAMETER :: a = 1.0_wp !< constant |
---|
| 1089 | REAL(wp), PARAMETER :: b = 0.66666666666_wp !< constant |
---|
| 1090 | REAL(wp), PARAMETER :: c = 5.0_wp !< constant |
---|
| 1091 | REAL(wp), PARAMETER :: d = 0.35_wp !< constant |
---|
| 1092 | REAL(wp), PARAMETER :: c_d_d = c / d !< constant |
---|
| 1093 | REAL(wp), PARAMETER :: bc_d_d = b * c / d !< constant |
---|
| 1094 | |
---|
| 1095 | |
---|
| 1096 | IF ( zeta < 0.0_wp ) THEN |
---|
[1788] | 1097 | x = SQRT( SQRT( 1.0_wp - 16.0_wp * zeta ) ) |
---|
[1691] | 1098 | psi_m = pi * 0.5_wp - 2.0_wp * ATAN( x ) + LOG( ( 1.0_wp + x )**2 & |
---|
| 1099 | * ( 1.0_wp + x**2 ) * 0.125_wp ) |
---|
| 1100 | ELSE |
---|
| 1101 | |
---|
| 1102 | psi_m = - b * ( zeta - c_d_d ) * EXP( -d * zeta ) - a * zeta & |
---|
| 1103 | - bc_d_d |
---|
| 1104 | ! |
---|
| 1105 | !-- Old version for stable conditions (only valid for z/L < 0.5) |
---|
| 1106 | !-- psi_m = - 5.0_wp * zeta |
---|
| 1107 | |
---|
| 1108 | ENDIF |
---|
| 1109 | |
---|
| 1110 | END FUNCTION psi_m |
---|
| 1111 | |
---|
| 1112 | |
---|
| 1113 | ! |
---|
| 1114 | !-- Integrated stability function for heat and moisture |
---|
| 1115 | FUNCTION psi_h( zeta ) |
---|
| 1116 | |
---|
| 1117 | USE kinds |
---|
| 1118 | |
---|
| 1119 | IMPLICIT NONE |
---|
| 1120 | |
---|
| 1121 | REAL(wp) :: psi_h !< Integrated similarity function result |
---|
| 1122 | REAL(wp) :: zeta !< Stability parameter z/L |
---|
| 1123 | REAL(wp) :: x !< dummy variable |
---|
| 1124 | |
---|
| 1125 | REAL(wp), PARAMETER :: a = 1.0_wp !< constant |
---|
| 1126 | REAL(wp), PARAMETER :: b = 0.66666666666_wp !< constant |
---|
| 1127 | REAL(wp), PARAMETER :: c = 5.0_wp !< constant |
---|
| 1128 | REAL(wp), PARAMETER :: d = 0.35_wp !< constant |
---|
| 1129 | REAL(wp), PARAMETER :: c_d_d = c / d !< constant |
---|
| 1130 | REAL(wp), PARAMETER :: bc_d_d = b * c / d !< constant |
---|
| 1131 | |
---|
| 1132 | |
---|
| 1133 | IF ( zeta < 0.0_wp ) THEN |
---|
[1788] | 1134 | x = SQRT( 1.0_wp - 16.0_wp * zeta ) |
---|
[1691] | 1135 | psi_h = 2.0_wp * LOG( (1.0_wp + x ) / 2.0_wp ) |
---|
| 1136 | ELSE |
---|
| 1137 | psi_h = - b * ( zeta - c_d_d ) * EXP( -d * zeta ) - (1.0_wp & |
---|
| 1138 | + 0.66666666666_wp * a * zeta )**1.5_wp - bc_d_d & |
---|
| 1139 | + 1.0_wp |
---|
| 1140 | ! |
---|
| 1141 | !-- Old version for stable conditions (only valid for z/L < 0.5) |
---|
| 1142 | !-- psi_h = - 5.0_wp * zeta |
---|
| 1143 | ENDIF |
---|
| 1144 | |
---|
| 1145 | END FUNCTION psi_h |
---|
| 1146 | |
---|
[1697] | 1147 | END MODULE surface_layer_fluxes_mod |
---|