| 1 | !> @file lpm_advec.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 1997-2016 Leibniz Universitaet Hannover |
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| 17 | !--------------------------------------------------------------------------------! |
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| 18 | ! |
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| 19 | ! Current revisions: |
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| 20 | ! ------------------ |
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| 21 | ! |
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| 22 | ! |
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| 23 | ! Former revisions: |
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| 24 | ! ----------------- |
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| 25 | ! $Id: lpm_advec.f90 1930 2016-06-09 16:32:12Z suehring $ |
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| 26 | ! |
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| 27 | ! 1929 2016-06-09 16:25:25Z suehring |
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| 28 | ! Put stochastic equation in an extra subroutine. |
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| 29 | ! Set flag for stochastic equation to communicate whether a particle is near |
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| 30 | ! topography. This case, memory and drift term are disabled in the Weil equation. |
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| 31 | ! |
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| 32 | ! Enable vertical logarithmic interpolation also above topography. This case, |
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| 33 | ! set a lower limit for the friction velocity, as it can become very small |
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| 34 | ! in narrow street canyons, leading to too large particle speeds. |
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| 35 | ! |
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| 36 | ! 1888 2016-04-21 12:20:49Z suehring |
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| 37 | ! Bugfix concerning logarithmic interpolation of particle speed |
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| 38 | ! |
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| 39 | ! 1822 2016-04-07 07:49:42Z hoffmann |
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| 40 | ! Random velocity fluctuations for particles added. Terminal fall velocity |
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| 41 | ! for droplets is calculated from a parameterization (which is better than |
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| 42 | ! the previous, physically correct calculation, which demands a very short |
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| 43 | ! time step that is not used in the model). |
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| 44 | ! |
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| 45 | ! Unused variables deleted. |
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| 46 | ! |
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| 47 | ! 1691 2015-10-26 16:17:44Z maronga |
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| 48 | ! Renamed prandtl_layer to constant_flux_layer. |
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| 49 | ! |
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| 50 | ! 1685 2015-10-08 07:32:13Z raasch |
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| 51 | ! TKE check for negative values (so far, only zero value was checked) |
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| 52 | ! offset_ocean_nzt_m1 removed |
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| 53 | ! |
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| 54 | ! 1682 2015-10-07 23:56:08Z knoop |
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| 55 | ! Code annotations made doxygen readable |
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| 56 | ! |
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| 57 | ! 1583 2015-04-15 12:16:27Z suehring |
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| 58 | ! Bugfix: particle advection within Prandtl-layer in case of Galilei |
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| 59 | ! transformation. |
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| 60 | ! |
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| 61 | ! 1369 2014-04-24 05:57:38Z raasch |
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| 62 | ! usage of module interfaces removed |
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| 63 | ! |
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| 64 | ! 1359 2014-04-11 17:15:14Z hoffmann |
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| 65 | ! New particle structure integrated. |
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| 66 | ! Kind definition added to all floating point numbers. |
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| 67 | ! |
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| 68 | ! 1322 2014-03-20 16:38:49Z raasch |
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| 69 | ! REAL constants defined as wp_kind |
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| 70 | ! |
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| 71 | ! 1320 2014-03-20 08:40:49Z raasch |
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| 72 | ! ONLY-attribute added to USE-statements, |
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| 73 | ! kind-parameters added to all INTEGER and REAL declaration statements, |
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| 74 | ! kinds are defined in new module kinds, |
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| 75 | ! revision history before 2012 removed, |
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| 76 | ! comment fields (!:) to be used for variable explanations added to |
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| 77 | ! all variable declaration statements |
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| 78 | ! |
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| 79 | ! 1314 2014-03-14 18:25:17Z suehring |
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| 80 | ! Vertical logarithmic interpolation of horizontal particle speed for particles |
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| 81 | ! between roughness height and first vertical grid level. |
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| 82 | ! |
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| 83 | ! 1036 2012-10-22 13:43:42Z raasch |
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| 84 | ! code put under GPL (PALM 3.9) |
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| 85 | ! |
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| 86 | ! 849 2012-03-15 10:35:09Z raasch |
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| 87 | ! initial revision (former part of advec_particles) |
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| 88 | ! |
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| 89 | ! |
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| 90 | ! Description: |
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| 91 | ! ------------ |
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| 92 | !> Calculation of new particle positions due to advection using a simple Euler |
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| 93 | !> scheme. Particles may feel inertia effects. SGS transport can be included |
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| 94 | !> using the stochastic model of Weil et al. (2004, JAS, 61, 2877-2887). |
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| 95 | !------------------------------------------------------------------------------! |
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| 96 | SUBROUTINE lpm_advec (ip,jp,kp) |
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| 97 | |
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| 98 | |
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| 99 | USE arrays_3d, & |
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| 100 | ONLY: de_dx, de_dy, de_dz, diss, e, km, u, us, usws, v, vsws, w, zu, zw |
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| 101 | |
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| 102 | USE cpulog |
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| 103 | |
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| 104 | USE pegrid |
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| 105 | |
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| 106 | USE control_parameters, & |
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| 107 | ONLY: atmos_ocean_sign, cloud_droplets, constant_flux_layer, dt_3d, & |
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| 108 | dt_3d_reached_l, dz, g, kappa, topography, u_gtrans, v_gtrans |
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| 109 | |
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| 110 | USE grid_variables, & |
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| 111 | ONLY: ddx, dx, ddy, dy |
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| 112 | |
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| 113 | USE indices, & |
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| 114 | ONLY: nzb, nzb_s_inner, nzt |
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| 115 | |
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| 116 | USE kinds |
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| 117 | |
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| 118 | USE particle_attributes, & |
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| 119 | ONLY: block_offset, c_0, dt_min_part, grid_particles, & |
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| 120 | iran_part, log_z_z0, number_of_particles, number_of_sublayers, & |
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| 121 | particles, particle_groups, offset_ocean_nzt, sgs_wf_part, & |
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| 122 | use_sgs_for_particles, vertical_particle_advection, z0_av_global |
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| 123 | |
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| 124 | USE statistics, & |
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| 125 | ONLY: hom |
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| 126 | |
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| 127 | IMPLICIT NONE |
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| 128 | |
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| 129 | INTEGER(iwp) :: agp !< loop variable |
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| 130 | INTEGER(iwp) :: gp_outside_of_building(1:8) !< number of grid points used for particle interpolation in case of topography |
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| 131 | INTEGER(iwp) :: i !< index variable along x |
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| 132 | INTEGER(iwp) :: ip !< index variable along x |
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| 133 | INTEGER(iwp) :: ilog !< index variable along x |
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| 134 | INTEGER(iwp) :: j !< index variable along y |
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| 135 | INTEGER(iwp) :: jp !< index variable along y |
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| 136 | INTEGER(iwp) :: jlog !< index variable along y |
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| 137 | INTEGER(iwp) :: k !< index variable along z |
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| 138 | INTEGER(iwp) :: kp !< index variable along z |
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| 139 | INTEGER(iwp) :: kw !< index variable along z |
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| 140 | INTEGER(iwp) :: n !< loop variable over all particles in a grid box |
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| 141 | INTEGER(iwp) :: nb !< block number particles are sorted in |
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| 142 | INTEGER(iwp) :: num_gp !< number of adjacent grid points inside topography |
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| 143 | |
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| 144 | INTEGER(iwp), DIMENSION(0:7) :: start_index !< start particle index for current block |
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| 145 | INTEGER(iwp), DIMENSION(0:7) :: end_index !< start particle index for current block |
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| 146 | |
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| 147 | REAL(wp) :: aa !< dummy argument for horizontal particle interpolation |
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| 148 | REAL(wp) :: bb !< dummy argument for horizontal particle interpolation |
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| 149 | REAL(wp) :: cc !< dummy argument for horizontal particle interpolation |
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| 150 | REAL(wp) :: d_sum !< dummy argument for horizontal particle interpolation in case of topography |
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| 151 | REAL(wp) :: d_z_p_z0 !< inverse of interpolation length for logarithmic interpolation |
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| 152 | REAL(wp) :: dd !< dummy argument for horizontal particle interpolation |
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| 153 | REAL(wp) :: de_dx_int_l !< x/y-interpolated TKE gradient (x) at particle position at lower vertical level |
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| 154 | REAL(wp) :: de_dx_int_u !< x/y-interpolated TKE gradient (x) at particle position at upper vertical level |
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| 155 | REAL(wp) :: de_dy_int_l !< x/y-interpolated TKE gradient (y) at particle position at lower vertical level |
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| 156 | REAL(wp) :: de_dy_int_u !< x/y-interpolated TKE gradient (y) at particle position at upper vertical level |
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| 157 | REAL(wp) :: de_dt !< temporal derivative of TKE experienced by the particle |
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| 158 | REAL(wp) :: de_dt_min !< lower level for temporal TKE derivative |
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| 159 | REAL(wp) :: de_dz_int_l !< x/y-interpolated TKE gradient (z) at particle position at lower vertical level |
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| 160 | REAL(wp) :: de_dz_int_u !< x/y-interpolated TKE gradient (z) at particle position at upper vertical level |
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| 161 | REAL(wp) :: diameter !< diamter of droplet |
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| 162 | REAL(wp) :: diss_int_l !< x/y-interpolated dissipation at particle position at lower vertical level |
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| 163 | REAL(wp) :: diss_int_u !< x/y-interpolated dissipation at particle position at upper vertical level |
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| 164 | REAL(wp) :: dt_gap !< remaining time until particle time integration reaches LES time |
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| 165 | REAL(wp) :: dt_particle_m !< previous particle time step |
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| 166 | REAL(wp) :: e_int_l !< x/y-interpolated TKE at particle position at lower vertical level |
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| 167 | REAL(wp) :: e_int_u !< x/y-interpolated TKE at particle position at upper vertical level |
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| 168 | REAL(wp) :: e_mean_int !< horizontal mean TKE at particle height |
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| 169 | REAL(wp) :: exp_arg !< |
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| 170 | REAL(wp) :: exp_term !< |
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| 171 | REAL(wp) :: gg !< dummy argument for horizontal particle interpolation |
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| 172 | REAL(wp) :: height_p !< dummy argument for logarithmic interpolation |
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| 173 | REAL(wp) :: lagr_timescale !< Lagrangian timescale |
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| 174 | REAL(wp) :: location(1:30,1:3) !< wall locations |
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| 175 | REAL(wp) :: log_z_z0_int !< logarithmus used for surface_layer interpolation |
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| 176 | REAL(wp) :: random_gauss !< |
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| 177 | REAL(wp) :: RL !< Lagrangian autocorrelation coefficient |
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| 178 | REAL(wp) :: rg1 !< Gaussian distributed random number |
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| 179 | REAL(wp) :: rg2 !< Gaussian distributed random number |
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| 180 | REAL(wp) :: rg3 !< Gaussian distributed random number |
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| 181 | REAL(wp) :: sigma !< velocity standard deviation |
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| 182 | REAL(wp) :: u_int_l !< x/y-interpolated u-component at particle position at lower vertical level |
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| 183 | REAL(wp) :: u_int_u !< x/y-interpolated u-component at particle position at upper vertical level |
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| 184 | REAL(wp) :: us_int !< friction velocity at particle grid box |
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| 185 | REAL(wp) :: v_int_l !< x/y-interpolated v-component at particle position at lower vertical level |
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| 186 | REAL(wp) :: v_int_u !< x/y-interpolated v-component at particle position at upper vertical level |
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| 187 | REAL(wp) :: vv_int !< |
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| 188 | REAL(wp) :: w_int_l !< x/y-interpolated w-component at particle position at lower vertical level |
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| 189 | REAL(wp) :: w_int_u !< x/y-interpolated w-component at particle position at upper vertical level |
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| 190 | REAL(wp) :: w_s !< terminal velocity of droplets |
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| 191 | REAL(wp) :: x !< dummy argument for horizontal particle interpolation |
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| 192 | REAL(wp) :: y !< dummy argument for horizontal particle interpolation |
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| 193 | REAL(wp) :: z_p !< surface layer height (0.5 dz) |
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| 194 | |
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| 195 | REAL(wp), PARAMETER :: a_rog = 9.65_wp !< parameter for fall velocity |
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| 196 | REAL(wp), PARAMETER :: b_rog = 10.43_wp !< parameter for fall velocity |
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| 197 | REAL(wp), PARAMETER :: c_rog = 0.6_wp !< parameter for fall velocity |
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| 198 | REAL(wp), PARAMETER :: k_cap_rog = 4.0_wp !< parameter for fall velocity |
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| 199 | REAL(wp), PARAMETER :: k_low_rog = 12.0_wp !< parameter for fall velocity |
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| 200 | REAL(wp), PARAMETER :: d0_rog = 0.745_wp !< separation diameter |
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| 201 | |
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| 202 | REAL(wp), DIMENSION(1:30) :: d_gp_pl !< dummy argument for particle interpolation scheme in case of topography |
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| 203 | REAL(wp), DIMENSION(1:30) :: de_dxi !< horizontal TKE gradient along x at adjacent wall |
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| 204 | REAL(wp), DIMENSION(1:30) :: de_dyi !< horizontal TKE gradient along y at adjacent wall |
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| 205 | REAL(wp), DIMENSION(1:30) :: de_dzi !< horizontal TKE gradient along z at adjacent wall |
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| 206 | REAL(wp), DIMENSION(1:30) :: dissi !< dissipation at adjacent wall |
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| 207 | REAL(wp), DIMENSION(1:30) :: ei !< TKE at adjacent wall |
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| 208 | |
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| 209 | REAL(wp), DIMENSION(number_of_particles) :: term_1_2 !< flag to communicate whether a particle is near topography or not |
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| 210 | REAL(wp), DIMENSION(number_of_particles) :: dens_ratio !< |
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| 211 | REAL(wp), DIMENSION(number_of_particles) :: de_dx_int !< horizontal TKE gradient along x at particle position |
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| 212 | REAL(wp), DIMENSION(number_of_particles) :: de_dy_int !< horizontal TKE gradient along y at particle position |
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| 213 | REAL(wp), DIMENSION(number_of_particles) :: de_dz_int !< horizontal TKE gradient along z at particle position |
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| 214 | REAL(wp), DIMENSION(number_of_particles) :: diss_int !< dissipation at particle position |
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| 215 | REAL(wp), DIMENSION(number_of_particles) :: dt_particle !< particle time step |
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| 216 | REAL(wp), DIMENSION(number_of_particles) :: e_int !< TKE at particle position |
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| 217 | REAL(wp), DIMENSION(number_of_particles) :: fs_int !< weighting factor for subgrid-scale particle speed |
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| 218 | REAL(wp), DIMENSION(number_of_particles) :: u_int !< u-component of particle speed |
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| 219 | REAL(wp), DIMENSION(number_of_particles) :: v_int !< v-component of particle speed |
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| 220 | REAL(wp), DIMENSION(number_of_particles) :: w_int !< w-component of particle speed |
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| 221 | REAL(wp), DIMENSION(number_of_particles) :: xv !< x-position |
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| 222 | REAL(wp), DIMENSION(number_of_particles) :: yv !< y-position |
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| 223 | REAL(wp), DIMENSION(number_of_particles) :: zv !< z-position |
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| 224 | |
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| 225 | REAL(wp), DIMENSION(number_of_particles, 3) :: rg !< vector of Gaussian distributed random numbers |
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| 226 | |
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| 227 | CALL cpu_log( log_point_s(44), 'lpm_advec', 'continue' ) |
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| 228 | |
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| 229 | ! |
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| 230 | !-- Determine height of Prandtl layer and distance between Prandtl-layer |
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| 231 | !-- height and horizontal mean roughness height, which are required for |
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| 232 | !-- vertical logarithmic interpolation of horizontal particle speeds |
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| 233 | !-- (for particles below first vertical grid level). |
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| 234 | z_p = zu(nzb+1) - zw(nzb) |
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| 235 | d_z_p_z0 = 1.0_wp / ( z_p - z0_av_global ) |
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| 236 | |
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| 237 | start_index = grid_particles(kp,jp,ip)%start_index |
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| 238 | end_index = grid_particles(kp,jp,ip)%end_index |
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| 239 | |
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| 240 | xv = particles(1:number_of_particles)%x |
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| 241 | yv = particles(1:number_of_particles)%y |
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| 242 | zv = particles(1:number_of_particles)%z |
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| 243 | |
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| 244 | DO nb = 0, 7 |
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| 245 | |
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| 246 | i = ip |
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| 247 | j = jp + block_offset(nb)%j_off |
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| 248 | k = kp + block_offset(nb)%k_off |
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| 249 | |
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| 250 | |
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| 251 | ! |
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| 252 | !-- Interpolate u velocity-component |
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| 253 | DO n = start_index(nb), end_index(nb) |
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| 254 | ! |
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| 255 | !-- Interpolation of the u velocity component onto particle position. |
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| 256 | !-- Particles are interpolation bi-linearly in the horizontal and a |
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| 257 | !-- linearly in the vertical. An exception is made for particles below |
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| 258 | !-- the first vertical grid level in case of a prandtl layer. In this |
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| 259 | !-- case the horizontal particle velocity components are determined using |
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| 260 | !-- Monin-Obukhov relations (if branch). |
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| 261 | !-- First, check if particle is located below first vertical grid level |
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| 262 | !-- (Prandtl-layer height) |
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| 263 | ilog = ( particles(n)%x + 0.5_wp * dx ) * ddx |
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| 264 | jlog = ( particles(n)%y + 0.5_wp * dy ) * ddy |
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| 265 | |
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| 266 | IF ( constant_flux_layer .AND. zv(n) - zw(nzb_s_inner(jlog,ilog)) < z_p ) THEN |
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| 267 | ! |
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| 268 | !-- Resolved-scale horizontal particle velocity is zero below z0. |
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| 269 | IF ( zv(n) - zw(nzb_s_inner(jlog,ilog)) < z0_av_global ) THEN |
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| 270 | u_int(n) = 0.0_wp |
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| 271 | ELSE |
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| 272 | ! |
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| 273 | !-- Determine the sublayer. Further used as index. |
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| 274 | height_p = ( zv(n) - zw(nzb_s_inner(jlog,ilog)) - z0_av_global ) & |
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| 275 | * REAL( number_of_sublayers, KIND=wp ) & |
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| 276 | * d_z_p_z0 |
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| 277 | ! |
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| 278 | !-- Calculate LOG(z/z0) for exact particle height. Therefore, |
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| 279 | !-- interpolate linearly between precalculated logarithm. |
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| 280 | log_z_z0_int = log_z_z0(INT(height_p)) & |
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| 281 | + ( height_p - INT(height_p) ) & |
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| 282 | * ( log_z_z0(INT(height_p)+1) & |
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| 283 | - log_z_z0(INT(height_p)) & |
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| 284 | ) |
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| 285 | ! |
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| 286 | !-- Limit friction velocity. In narrow canyons or holes the |
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| 287 | !-- friction velocity can become very small, resulting in a too |
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| 288 | !-- large particle speed. |
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| 289 | us_int = MAX( 0.5_wp * ( us(jlog,ilog) + us(jlog,ilog-1) ), & |
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| 290 | 0.01_wp ) |
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| 291 | ! |
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| 292 | !-- Neutral solution is applied for all situations, e.g. also for |
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| 293 | !-- unstable and stable situations. Even though this is not exact |
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| 294 | !-- this saves a lot of CPU time since several calls of intrinsic |
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| 295 | !-- FORTRAN procedures (LOG, ATAN) are avoided, This is justified |
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| 296 | !-- as sensitivity studies revealed no significant effect of |
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| 297 | !-- using the neutral solution also for un/stable situations. |
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| 298 | u_int(n) = -usws(jlog,ilog) / ( us_int * kappa + 1E-10_wp ) & |
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| 299 | * log_z_z0_int - u_gtrans |
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| 300 | |
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| 301 | ENDIF |
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| 302 | ! |
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| 303 | !-- Particle above the first grid level. Bi-linear interpolation in the |
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| 304 | !-- horizontal and linear interpolation in the vertical direction. |
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| 305 | ELSE |
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| 306 | |
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| 307 | x = xv(n) + ( 0.5_wp - i ) * dx |
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| 308 | y = yv(n) - j * dy |
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| 309 | aa = x**2 + y**2 |
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| 310 | bb = ( dx - x )**2 + y**2 |
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| 311 | cc = x**2 + ( dy - y )**2 |
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| 312 | dd = ( dx - x )**2 + ( dy - y )**2 |
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| 313 | gg = aa + bb + cc + dd |
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| 314 | |
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| 315 | u_int_l = ( ( gg - aa ) * u(k,j,i) + ( gg - bb ) * u(k,j,i+1) & |
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| 316 | + ( gg - cc ) * u(k,j+1,i) + ( gg - dd ) * & |
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| 317 | u(k,j+1,i+1) ) / ( 3.0_wp * gg ) - u_gtrans |
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| 318 | |
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| 319 | IF ( k == nzt ) THEN |
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| 320 | u_int(n) = u_int_l |
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| 321 | ELSE |
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| 322 | u_int_u = ( ( gg-aa ) * u(k+1,j,i) + ( gg-bb ) * u(k+1,j,i+1) & |
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| 323 | + ( gg-cc ) * u(k+1,j+1,i) + ( gg-dd ) * & |
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| 324 | u(k+1,j+1,i+1) ) / ( 3.0_wp * gg ) - u_gtrans |
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| 325 | u_int(n) = u_int_l + ( zv(n) - zu(k) ) / dz * & |
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| 326 | ( u_int_u - u_int_l ) |
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| 327 | ENDIF |
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| 328 | |
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| 329 | ENDIF |
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| 330 | |
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| 331 | ENDDO |
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| 332 | |
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| 333 | i = ip + block_offset(nb)%i_off |
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| 334 | j = jp |
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| 335 | k = kp + block_offset(nb)%k_off |
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| 336 | ! |
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| 337 | !-- Same procedure for interpolation of the v velocity-component |
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| 338 | DO n = start_index(nb), end_index(nb) |
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| 339 | |
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| 340 | ilog = ( particles(n)%x + 0.5_wp * dx ) * ddx |
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| 341 | jlog = ( particles(n)%y + 0.5_wp * dy ) * ddy |
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| 342 | IF ( constant_flux_layer .AND. zv(n) - zw(nzb_s_inner(jlog,ilog)) < z_p ) THEN |
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| 343 | |
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| 344 | IF ( zv(n) - zw(nzb_s_inner(jlog,ilog)) < z0_av_global ) THEN |
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| 345 | ! |
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| 346 | !-- Resolved-scale horizontal particle velocity is zero below z0. |
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| 347 | v_int(n) = 0.0_wp |
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| 348 | ELSE |
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| 349 | ! |
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| 350 | !-- Determine the sublayer. Further used as index. Please note, |
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| 351 | !-- logarithmus can not be reused from above, as in in case of |
|---|
| 352 | !-- topography particle on u-grid can be above surface-layer height, |
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| 353 | !-- whereas it can be below on v-grid. |
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| 354 | height_p = ( zv(n) - zw(nzb_s_inner(jlog,ilog)) - z0_av_global ) & |
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| 355 | * REAL( number_of_sublayers, KIND=wp ) & |
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| 356 | * d_z_p_z0 |
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| 357 | ! |
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| 358 | !-- Calculate LOG(z/z0) for exact particle height. Therefore, |
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| 359 | !-- interpolate linearly between precalculated logarithm. |
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| 360 | log_z_z0_int = log_z_z0(INT(height_p)) & |
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| 361 | + ( height_p - INT(height_p) ) & |
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| 362 | * ( log_z_z0(INT(height_p)+1) & |
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| 363 | - log_z_z0(INT(height_p)) & |
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| 364 | ) |
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| 365 | ! |
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| 366 | !-- Limit friction velocity. In narrow canyons or holes the |
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| 367 | !-- friction velocity can become very small, resulting in a too |
|---|
| 368 | !-- large particle speed. |
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| 369 | us_int = MAX( 0.5_wp * ( us(jlog,ilog) + us(jlog-1,ilog) ), & |
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| 370 | 0.01_wp ) |
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| 371 | ! |
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| 372 | !-- Neutral solution is applied for all situations, e.g. also for |
|---|
| 373 | !-- unstable and stable situations. Even though this is not exact |
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| 374 | !-- this saves a lot of CPU time since several calls of intrinsic |
|---|
| 375 | !-- FORTRAN procedures (LOG, ATAN) are avoided, This is justified |
|---|
| 376 | !-- as sensitivity studies revealed no significant effect of |
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| 377 | !-- using the neutral solution also for un/stable situations. |
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| 378 | v_int(n) = -vsws(jlog,ilog) / ( us_int * kappa + 1E-10_wp ) & |
|---|
| 379 | * log_z_z0_int - v_gtrans |
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| 380 | |
|---|
| 381 | ENDIF |
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| 382 | |
|---|
| 383 | ELSE |
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| 384 | x = xv(n) - i * dx |
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| 385 | y = yv(n) + ( 0.5_wp - j ) * dy |
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| 386 | aa = x**2 + y**2 |
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| 387 | bb = ( dx - x )**2 + y**2 |
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| 388 | cc = x**2 + ( dy - y )**2 |
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| 389 | dd = ( dx - x )**2 + ( dy - y )**2 |
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| 390 | gg = aa + bb + cc + dd |
|---|
| 391 | |
|---|
| 392 | v_int_l = ( ( gg - aa ) * v(k,j,i) + ( gg - bb ) * v(k,j,i+1) & |
|---|
| 393 | + ( gg - cc ) * v(k,j+1,i) + ( gg - dd ) * v(k,j+1,i+1) & |
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| 394 | ) / ( 3.0_wp * gg ) - v_gtrans |
|---|
| 395 | |
|---|
| 396 | IF ( k == nzt ) THEN |
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| 397 | v_int(n) = v_int_l |
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| 398 | ELSE |
|---|
| 399 | v_int_u = ( ( gg-aa ) * v(k+1,j,i) + ( gg-bb ) * v(k+1,j,i+1) & |
|---|
| 400 | + ( gg-cc ) * v(k+1,j+1,i) + ( gg-dd ) * v(k+1,j+1,i+1) & |
|---|
| 401 | ) / ( 3.0_wp * gg ) - v_gtrans |
|---|
| 402 | v_int(n) = v_int_l + ( zv(n) - zu(k) ) / dz * & |
|---|
| 403 | ( v_int_u - v_int_l ) |
|---|
| 404 | ENDIF |
|---|
| 405 | |
|---|
| 406 | ENDIF |
|---|
| 407 | |
|---|
| 408 | ENDDO |
|---|
| 409 | |
|---|
| 410 | i = ip + block_offset(nb)%i_off |
|---|
| 411 | j = jp + block_offset(nb)%j_off |
|---|
| 412 | k = kp - 1 |
|---|
| 413 | ! |
|---|
| 414 | !-- Same procedure for interpolation of the w velocity-component |
|---|
| 415 | DO n = start_index(nb), end_index(nb) |
|---|
| 416 | |
|---|
| 417 | IF ( vertical_particle_advection(particles(n)%group) ) THEN |
|---|
| 418 | |
|---|
| 419 | x = xv(n) - i * dx |
|---|
| 420 | y = yv(n) - j * dy |
|---|
| 421 | aa = x**2 + y**2 |
|---|
| 422 | bb = ( dx - x )**2 + y**2 |
|---|
| 423 | cc = x**2 + ( dy - y )**2 |
|---|
| 424 | dd = ( dx - x )**2 + ( dy - y )**2 |
|---|
| 425 | gg = aa + bb + cc + dd |
|---|
| 426 | |
|---|
| 427 | w_int_l = ( ( gg - aa ) * w(k,j,i) + ( gg - bb ) * w(k,j,i+1) & |
|---|
| 428 | + ( gg - cc ) * w(k,j+1,i) + ( gg - dd ) * w(k,j+1,i+1) & |
|---|
| 429 | ) / ( 3.0_wp * gg ) |
|---|
| 430 | |
|---|
| 431 | IF ( k == nzt ) THEN |
|---|
| 432 | w_int(n) = w_int_l |
|---|
| 433 | ELSE |
|---|
| 434 | w_int_u = ( ( gg-aa ) * w(k+1,j,i) + & |
|---|
| 435 | ( gg-bb ) * w(k+1,j,i+1) + & |
|---|
| 436 | ( gg-cc ) * w(k+1,j+1,i) + & |
|---|
| 437 | ( gg-dd ) * w(k+1,j+1,i+1) & |
|---|
| 438 | ) / ( 3.0_wp * gg ) |
|---|
| 439 | w_int(n) = w_int_l + ( zv(n) - zw(k) ) / dz * & |
|---|
| 440 | ( w_int_u - w_int_l ) |
|---|
| 441 | ENDIF |
|---|
| 442 | |
|---|
| 443 | ELSE |
|---|
| 444 | |
|---|
| 445 | w_int(n) = 0.0_wp |
|---|
| 446 | |
|---|
| 447 | ENDIF |
|---|
| 448 | |
|---|
| 449 | ENDDO |
|---|
| 450 | |
|---|
| 451 | ENDDO |
|---|
| 452 | |
|---|
| 453 | !-- Interpolate and calculate quantities needed for calculating the SGS |
|---|
| 454 | !-- velocities |
|---|
| 455 | IF ( use_sgs_for_particles .AND. .NOT. cloud_droplets ) THEN |
|---|
| 456 | |
|---|
| 457 | IF ( topography == 'flat' ) THEN |
|---|
| 458 | |
|---|
| 459 | DO nb = 0,7 |
|---|
| 460 | |
|---|
| 461 | i = ip + block_offset(nb)%i_off |
|---|
| 462 | j = jp + block_offset(nb)%j_off |
|---|
| 463 | k = kp + block_offset(nb)%k_off |
|---|
| 464 | |
|---|
| 465 | DO n = start_index(nb), end_index(nb) |
|---|
| 466 | ! |
|---|
| 467 | !-- Interpolate TKE |
|---|
| 468 | x = xv(n) - i * dx |
|---|
| 469 | y = yv(n) - j * dy |
|---|
| 470 | aa = x**2 + y**2 |
|---|
| 471 | bb = ( dx - x )**2 + y**2 |
|---|
| 472 | cc = x**2 + ( dy - y )**2 |
|---|
| 473 | dd = ( dx - x )**2 + ( dy - y )**2 |
|---|
| 474 | gg = aa + bb + cc + dd |
|---|
| 475 | |
|---|
| 476 | e_int_l = ( ( gg-aa ) * e(k,j,i) + ( gg-bb ) * e(k,j,i+1) & |
|---|
| 477 | + ( gg-cc ) * e(k,j+1,i) + ( gg-dd ) * e(k,j+1,i+1) & |
|---|
| 478 | ) / ( 3.0_wp * gg ) |
|---|
| 479 | |
|---|
| 480 | IF ( k+1 == nzt+1 ) THEN |
|---|
| 481 | e_int(n) = e_int_l |
|---|
| 482 | ELSE |
|---|
| 483 | e_int_u = ( ( gg - aa ) * e(k+1,j,i) + & |
|---|
| 484 | ( gg - bb ) * e(k+1,j,i+1) + & |
|---|
| 485 | ( gg - cc ) * e(k+1,j+1,i) + & |
|---|
| 486 | ( gg - dd ) * e(k+1,j+1,i+1) & |
|---|
| 487 | ) / ( 3.0_wp * gg ) |
|---|
| 488 | e_int(n) = e_int_l + ( zv(n) - zu(k) ) / dz * & |
|---|
| 489 | ( e_int_u - e_int_l ) |
|---|
| 490 | ENDIF |
|---|
| 491 | ! |
|---|
| 492 | !-- Needed to avoid NaN particle velocities (this might not be |
|---|
| 493 | !-- required any more) |
|---|
| 494 | IF ( e_int(n) <= 0.0_wp ) THEN |
|---|
| 495 | e_int(n) = 1.0E-20_wp |
|---|
| 496 | ENDIF |
|---|
| 497 | ! |
|---|
| 498 | !-- Interpolate the TKE gradient along x (adopt incides i,j,k and |
|---|
| 499 | !-- all position variables from above (TKE)) |
|---|
| 500 | de_dx_int_l = ( ( gg - aa ) * de_dx(k,j,i) + & |
|---|
| 501 | ( gg - bb ) * de_dx(k,j,i+1) + & |
|---|
| 502 | ( gg - cc ) * de_dx(k,j+1,i) + & |
|---|
| 503 | ( gg - dd ) * de_dx(k,j+1,i+1) & |
|---|
| 504 | ) / ( 3.0_wp * gg ) |
|---|
| 505 | |
|---|
| 506 | IF ( ( k+1 == nzt+1 ) .OR. ( k == nzb ) ) THEN |
|---|
| 507 | de_dx_int(n) = de_dx_int_l |
|---|
| 508 | ELSE |
|---|
| 509 | de_dx_int_u = ( ( gg - aa ) * de_dx(k+1,j,i) + & |
|---|
| 510 | ( gg - bb ) * de_dx(k+1,j,i+1) + & |
|---|
| 511 | ( gg - cc ) * de_dx(k+1,j+1,i) + & |
|---|
| 512 | ( gg - dd ) * de_dx(k+1,j+1,i+1) & |
|---|
| 513 | ) / ( 3.0_wp * gg ) |
|---|
| 514 | de_dx_int(n) = de_dx_int_l + ( zv(n) - zu(k) ) / dz * & |
|---|
| 515 | ( de_dx_int_u - de_dx_int_l ) |
|---|
| 516 | ENDIF |
|---|
| 517 | ! |
|---|
| 518 | !-- Interpolate the TKE gradient along y |
|---|
| 519 | de_dy_int_l = ( ( gg - aa ) * de_dy(k,j,i) + & |
|---|
| 520 | ( gg - bb ) * de_dy(k,j,i+1) + & |
|---|
| 521 | ( gg - cc ) * de_dy(k,j+1,i) + & |
|---|
| 522 | ( gg - dd ) * de_dy(k,j+1,i+1) & |
|---|
| 523 | ) / ( 3.0_wp * gg ) |
|---|
| 524 | IF ( ( k+1 == nzt+1 ) .OR. ( k == nzb ) ) THEN |
|---|
| 525 | de_dy_int(n) = de_dy_int_l |
|---|
| 526 | ELSE |
|---|
| 527 | de_dy_int_u = ( ( gg - aa ) * de_dy(k+1,j,i) + & |
|---|
| 528 | ( gg - bb ) * de_dy(k+1,j,i+1) + & |
|---|
| 529 | ( gg - cc ) * de_dy(k+1,j+1,i) + & |
|---|
| 530 | ( gg - dd ) * de_dy(k+1,j+1,i+1) & |
|---|
| 531 | ) / ( 3.0_wp * gg ) |
|---|
| 532 | de_dy_int(n) = de_dy_int_l + ( zv(n) - zu(k) ) / dz * & |
|---|
| 533 | ( de_dy_int_u - de_dy_int_l ) |
|---|
| 534 | ENDIF |
|---|
| 535 | |
|---|
| 536 | ! |
|---|
| 537 | !-- Interpolate the TKE gradient along z |
|---|
| 538 | IF ( zv(n) < 0.5_wp * dz ) THEN |
|---|
| 539 | de_dz_int(n) = 0.0_wp |
|---|
| 540 | ELSE |
|---|
| 541 | de_dz_int_l = ( ( gg - aa ) * de_dz(k,j,i) + & |
|---|
| 542 | ( gg - bb ) * de_dz(k,j,i+1) + & |
|---|
| 543 | ( gg - cc ) * de_dz(k,j+1,i) + & |
|---|
| 544 | ( gg - dd ) * de_dz(k,j+1,i+1) & |
|---|
| 545 | ) / ( 3.0_wp * gg ) |
|---|
| 546 | |
|---|
| 547 | IF ( ( k+1 == nzt+1 ) .OR. ( k == nzb ) ) THEN |
|---|
| 548 | de_dz_int(n) = de_dz_int_l |
|---|
| 549 | ELSE |
|---|
| 550 | de_dz_int_u = ( ( gg - aa ) * de_dz(k+1,j,i) + & |
|---|
| 551 | ( gg - bb ) * de_dz(k+1,j,i+1) + & |
|---|
| 552 | ( gg - cc ) * de_dz(k+1,j+1,i) + & |
|---|
| 553 | ( gg - dd ) * de_dz(k+1,j+1,i+1) & |
|---|
| 554 | ) / ( 3.0_wp * gg ) |
|---|
| 555 | de_dz_int(n) = de_dz_int_l + ( zv(n) - zu(k) ) / dz * & |
|---|
| 556 | ( de_dz_int_u - de_dz_int_l ) |
|---|
| 557 | ENDIF |
|---|
| 558 | ENDIF |
|---|
| 559 | |
|---|
| 560 | ! |
|---|
| 561 | !-- Interpolate the dissipation of TKE |
|---|
| 562 | diss_int_l = ( ( gg - aa ) * diss(k,j,i) + & |
|---|
| 563 | ( gg - bb ) * diss(k,j,i+1) + & |
|---|
| 564 | ( gg - cc ) * diss(k,j+1,i) + & |
|---|
| 565 | ( gg - dd ) * diss(k,j+1,i+1) & |
|---|
| 566 | ) / ( 3.0_wp * gg ) |
|---|
| 567 | |
|---|
| 568 | IF ( k == nzt ) THEN |
|---|
| 569 | diss_int(n) = diss_int_l |
|---|
| 570 | ELSE |
|---|
| 571 | diss_int_u = ( ( gg - aa ) * diss(k+1,j,i) + & |
|---|
| 572 | ( gg - bb ) * diss(k+1,j,i+1) + & |
|---|
| 573 | ( gg - cc ) * diss(k+1,j+1,i) + & |
|---|
| 574 | ( gg - dd ) * diss(k+1,j+1,i+1) & |
|---|
| 575 | ) / ( 3.0_wp * gg ) |
|---|
| 576 | diss_int(n) = diss_int_l + ( zv(n) - zu(k) ) / dz * & |
|---|
| 577 | ( diss_int_u - diss_int_l ) |
|---|
| 578 | ENDIF |
|---|
| 579 | |
|---|
| 580 | ! |
|---|
| 581 | !-- Set flag for stochastic equation. |
|---|
| 582 | term_1_2(n) = 1.0_wp |
|---|
| 583 | |
|---|
| 584 | ENDDO |
|---|
| 585 | ENDDO |
|---|
| 586 | |
|---|
| 587 | ELSE ! non-flat topography, e.g., buildings |
|---|
| 588 | |
|---|
| 589 | DO n = 1, number_of_particles |
|---|
| 590 | i = particles(n)%x * ddx |
|---|
| 591 | j = particles(n)%y * ddy |
|---|
| 592 | k = ( zv(n) + 0.5_wp * dz * atmos_ocean_sign ) / dz & |
|---|
| 593 | + offset_ocean_nzt ! only exact if eq.dist |
|---|
| 594 | ! |
|---|
| 595 | !-- In case that there are buildings it has to be determined |
|---|
| 596 | !-- how many of the gridpoints defining the particle box are |
|---|
| 597 | !-- situated within a building |
|---|
| 598 | !-- gp_outside_of_building(1): i,j,k |
|---|
| 599 | !-- gp_outside_of_building(2): i,j+1,k |
|---|
| 600 | !-- gp_outside_of_building(3): i,j,k+1 |
|---|
| 601 | !-- gp_outside_of_building(4): i,j+1,k+1 |
|---|
| 602 | !-- gp_outside_of_building(5): i+1,j,k |
|---|
| 603 | !-- gp_outside_of_building(6): i+1,j+1,k |
|---|
| 604 | !-- gp_outside_of_building(7): i+1,j,k+1 |
|---|
| 605 | !-- gp_outside_of_building(8): i+1,j+1,k+1 |
|---|
| 606 | |
|---|
| 607 | gp_outside_of_building = 0 |
|---|
| 608 | location = 0.0_wp |
|---|
| 609 | num_gp = 0 |
|---|
| 610 | |
|---|
| 611 | IF ( k > nzb_s_inner(j,i) .OR. nzb_s_inner(j,i) == 0 ) THEN |
|---|
| 612 | num_gp = num_gp + 1 |
|---|
| 613 | gp_outside_of_building(1) = 1 |
|---|
| 614 | location(num_gp,1) = i * dx |
|---|
| 615 | location(num_gp,2) = j * dy |
|---|
| 616 | location(num_gp,3) = k * dz - 0.5_wp * dz |
|---|
| 617 | ei(num_gp) = e(k,j,i) |
|---|
| 618 | dissi(num_gp) = diss(k,j,i) |
|---|
| 619 | de_dxi(num_gp) = de_dx(k,j,i) |
|---|
| 620 | de_dyi(num_gp) = de_dy(k,j,i) |
|---|
| 621 | de_dzi(num_gp) = de_dz(k,j,i) |
|---|
| 622 | ENDIF |
|---|
| 623 | IF ( k > nzb_s_inner(j+1,i) .OR. nzb_s_inner(j+1,i) == 0 ) THEN |
|---|
| 624 | num_gp = num_gp + 1 |
|---|
| 625 | gp_outside_of_building(2) = 1 |
|---|
| 626 | location(num_gp,1) = i * dx |
|---|
| 627 | location(num_gp,2) = (j+1) * dy |
|---|
| 628 | location(num_gp,3) = k * dz - 0.5_wp * dz |
|---|
| 629 | ei(num_gp) = e(k,j+1,i) |
|---|
| 630 | dissi(num_gp) = diss(k,j+1,i) |
|---|
| 631 | de_dxi(num_gp) = de_dx(k,j+1,i) |
|---|
| 632 | de_dyi(num_gp) = de_dy(k,j+1,i) |
|---|
| 633 | de_dzi(num_gp) = de_dz(k,j+1,i) |
|---|
| 634 | ENDIF |
|---|
| 635 | |
|---|
| 636 | IF ( k+1 > nzb_s_inner(j,i) .OR. nzb_s_inner(j,i) == 0 ) THEN |
|---|
| 637 | num_gp = num_gp + 1 |
|---|
| 638 | gp_outside_of_building(3) = 1 |
|---|
| 639 | location(num_gp,1) = i * dx |
|---|
| 640 | location(num_gp,2) = j * dy |
|---|
| 641 | location(num_gp,3) = (k+1) * dz - 0.5_wp * dz |
|---|
| 642 | ei(num_gp) = e(k+1,j,i) |
|---|
| 643 | dissi(num_gp) = diss(k+1,j,i) |
|---|
| 644 | de_dxi(num_gp) = de_dx(k+1,j,i) |
|---|
| 645 | de_dyi(num_gp) = de_dy(k+1,j,i) |
|---|
| 646 | de_dzi(num_gp) = de_dz(k+1,j,i) |
|---|
| 647 | ENDIF |
|---|
| 648 | |
|---|
| 649 | IF ( k+1 > nzb_s_inner(j+1,i) .OR. nzb_s_inner(j+1,i) == 0 ) THEN |
|---|
| 650 | num_gp = num_gp + 1 |
|---|
| 651 | gp_outside_of_building(4) = 1 |
|---|
| 652 | location(num_gp,1) = i * dx |
|---|
| 653 | location(num_gp,2) = (j+1) * dy |
|---|
| 654 | location(num_gp,3) = (k+1) * dz - 0.5_wp * dz |
|---|
| 655 | ei(num_gp) = e(k+1,j+1,i) |
|---|
| 656 | dissi(num_gp) = diss(k+1,j+1,i) |
|---|
| 657 | de_dxi(num_gp) = de_dx(k+1,j+1,i) |
|---|
| 658 | de_dyi(num_gp) = de_dy(k+1,j+1,i) |
|---|
| 659 | de_dzi(num_gp) = de_dz(k+1,j+1,i) |
|---|
| 660 | ENDIF |
|---|
| 661 | |
|---|
| 662 | IF ( k > nzb_s_inner(j,i+1) .OR. nzb_s_inner(j,i+1) == 0 ) THEN |
|---|
| 663 | num_gp = num_gp + 1 |
|---|
| 664 | gp_outside_of_building(5) = 1 |
|---|
| 665 | location(num_gp,1) = (i+1) * dx |
|---|
| 666 | location(num_gp,2) = j * dy |
|---|
| 667 | location(num_gp,3) = k * dz - 0.5_wp * dz |
|---|
| 668 | ei(num_gp) = e(k,j,i+1) |
|---|
| 669 | dissi(num_gp) = diss(k,j,i+1) |
|---|
| 670 | de_dxi(num_gp) = de_dx(k,j,i+1) |
|---|
| 671 | de_dyi(num_gp) = de_dy(k,j,i+1) |
|---|
| 672 | de_dzi(num_gp) = de_dz(k,j,i+1) |
|---|
| 673 | ENDIF |
|---|
| 674 | |
|---|
| 675 | IF ( k > nzb_s_inner(j+1,i+1) .OR. nzb_s_inner(j+1,i+1) == 0 ) THEN |
|---|
| 676 | num_gp = num_gp + 1 |
|---|
| 677 | gp_outside_of_building(6) = 1 |
|---|
| 678 | location(num_gp,1) = (i+1) * dx |
|---|
| 679 | location(num_gp,2) = (j+1) * dy |
|---|
| 680 | location(num_gp,3) = k * dz - 0.5_wp * dz |
|---|
| 681 | ei(num_gp) = e(k,j+1,i+1) |
|---|
| 682 | dissi(num_gp) = diss(k,j+1,i+1) |
|---|
| 683 | de_dxi(num_gp) = de_dx(k,j+1,i+1) |
|---|
| 684 | de_dyi(num_gp) = de_dy(k,j+1,i+1) |
|---|
| 685 | de_dzi(num_gp) = de_dz(k,j+1,i+1) |
|---|
| 686 | ENDIF |
|---|
| 687 | |
|---|
| 688 | IF ( k+1 > nzb_s_inner(j,i+1) .OR. nzb_s_inner(j,i+1) == 0 ) THEN |
|---|
| 689 | num_gp = num_gp + 1 |
|---|
| 690 | gp_outside_of_building(7) = 1 |
|---|
| 691 | location(num_gp,1) = (i+1) * dx |
|---|
| 692 | location(num_gp,2) = j * dy |
|---|
| 693 | location(num_gp,3) = (k+1) * dz - 0.5_wp * dz |
|---|
| 694 | ei(num_gp) = e(k+1,j,i+1) |
|---|
| 695 | dissi(num_gp) = diss(k+1,j,i+1) |
|---|
| 696 | de_dxi(num_gp) = de_dx(k+1,j,i+1) |
|---|
| 697 | de_dyi(num_gp) = de_dy(k+1,j,i+1) |
|---|
| 698 | de_dzi(num_gp) = de_dz(k+1,j,i+1) |
|---|
| 699 | ENDIF |
|---|
| 700 | |
|---|
| 701 | IF ( k+1 > nzb_s_inner(j+1,i+1) .OR. nzb_s_inner(j+1,i+1) == 0) THEN |
|---|
| 702 | num_gp = num_gp + 1 |
|---|
| 703 | gp_outside_of_building(8) = 1 |
|---|
| 704 | location(num_gp,1) = (i+1) * dx |
|---|
| 705 | location(num_gp,2) = (j+1) * dy |
|---|
| 706 | location(num_gp,3) = (k+1) * dz - 0.5_wp * dz |
|---|
| 707 | ei(num_gp) = e(k+1,j+1,i+1) |
|---|
| 708 | dissi(num_gp) = diss(k+1,j+1,i+1) |
|---|
| 709 | de_dxi(num_gp) = de_dx(k+1,j+1,i+1) |
|---|
| 710 | de_dyi(num_gp) = de_dy(k+1,j+1,i+1) |
|---|
| 711 | de_dzi(num_gp) = de_dz(k+1,j+1,i+1) |
|---|
| 712 | ENDIF |
|---|
| 713 | ! |
|---|
| 714 | !-- If all gridpoints are situated outside of a building, then the |
|---|
| 715 | !-- ordinary interpolation scheme can be used. |
|---|
| 716 | IF ( num_gp == 8 ) THEN |
|---|
| 717 | |
|---|
| 718 | x = particles(n)%x - i * dx |
|---|
| 719 | y = particles(n)%y - j * dy |
|---|
| 720 | aa = x**2 + y**2 |
|---|
| 721 | bb = ( dx - x )**2 + y**2 |
|---|
| 722 | cc = x**2 + ( dy - y )**2 |
|---|
| 723 | dd = ( dx - x )**2 + ( dy - y )**2 |
|---|
| 724 | gg = aa + bb + cc + dd |
|---|
| 725 | |
|---|
| 726 | e_int_l = ( ( gg - aa ) * e(k,j,i) + ( gg - bb ) * e(k,j,i+1) & |
|---|
| 727 | + ( gg - cc ) * e(k,j+1,i) + ( gg - dd ) * e(k,j+1,i+1) & |
|---|
| 728 | ) / ( 3.0_wp * gg ) |
|---|
| 729 | |
|---|
| 730 | IF ( k == nzt ) THEN |
|---|
| 731 | e_int(n) = e_int_l |
|---|
| 732 | ELSE |
|---|
| 733 | e_int_u = ( ( gg - aa ) * e(k+1,j,i) + & |
|---|
| 734 | ( gg - bb ) * e(k+1,j,i+1) + & |
|---|
| 735 | ( gg - cc ) * e(k+1,j+1,i) + & |
|---|
| 736 | ( gg - dd ) * e(k+1,j+1,i+1) & |
|---|
| 737 | ) / ( 3.0_wp * gg ) |
|---|
| 738 | e_int(n) = e_int_l + ( zv(n) - zu(k) ) / dz * & |
|---|
| 739 | ( e_int_u - e_int_l ) |
|---|
| 740 | ENDIF |
|---|
| 741 | ! |
|---|
| 742 | !-- Needed to avoid NaN particle velocities (this might not be |
|---|
| 743 | !-- required any more) |
|---|
| 744 | IF ( e_int(n) <= 0.0_wp ) THEN |
|---|
| 745 | e_int(n) = 1.0E-20_wp |
|---|
| 746 | ENDIF |
|---|
| 747 | ! |
|---|
| 748 | !-- Interpolate the TKE gradient along x (adopt incides i,j,k |
|---|
| 749 | !-- and all position variables from above (TKE)) |
|---|
| 750 | de_dx_int_l = ( ( gg - aa ) * de_dx(k,j,i) + & |
|---|
| 751 | ( gg - bb ) * de_dx(k,j,i+1) + & |
|---|
| 752 | ( gg - cc ) * de_dx(k,j+1,i) + & |
|---|
| 753 | ( gg - dd ) * de_dx(k,j+1,i+1) & |
|---|
| 754 | ) / ( 3.0_wp * gg ) |
|---|
| 755 | |
|---|
| 756 | IF ( ( k == nzt ) .OR. ( k == nzb ) ) THEN |
|---|
| 757 | de_dx_int(n) = de_dx_int_l |
|---|
| 758 | ELSE |
|---|
| 759 | de_dx_int_u = ( ( gg - aa ) * de_dx(k+1,j,i) + & |
|---|
| 760 | ( gg - bb ) * de_dx(k+1,j,i+1) + & |
|---|
| 761 | ( gg - cc ) * de_dx(k+1,j+1,i) + & |
|---|
| 762 | ( gg - dd ) * de_dx(k+1,j+1,i+1) & |
|---|
| 763 | ) / ( 3.0_wp * gg ) |
|---|
| 764 | de_dx_int(n) = de_dx_int_l + ( zv(n) - zu(k) ) / & |
|---|
| 765 | dz * ( de_dx_int_u - de_dx_int_l ) |
|---|
| 766 | ENDIF |
|---|
| 767 | |
|---|
| 768 | ! |
|---|
| 769 | !-- Interpolate the TKE gradient along y |
|---|
| 770 | de_dy_int_l = ( ( gg - aa ) * de_dy(k,j,i) + & |
|---|
| 771 | ( gg - bb ) * de_dy(k,j,i+1) + & |
|---|
| 772 | ( gg - cc ) * de_dy(k,j+1,i) + & |
|---|
| 773 | ( gg - dd ) * de_dy(k,j+1,i+1) & |
|---|
| 774 | ) / ( 3.0_wp * gg ) |
|---|
| 775 | IF ( ( k+1 == nzt+1 ) .OR. ( k == nzb ) ) THEN |
|---|
| 776 | de_dy_int(n) = de_dy_int_l |
|---|
| 777 | ELSE |
|---|
| 778 | de_dy_int_u = ( ( gg - aa ) * de_dy(k+1,j,i) + & |
|---|
| 779 | ( gg - bb ) * de_dy(k+1,j,i+1) + & |
|---|
| 780 | ( gg - cc ) * de_dy(k+1,j+1,i) + & |
|---|
| 781 | ( gg - dd ) * de_dy(k+1,j+1,i+1) & |
|---|
| 782 | ) / ( 3.0_wp * gg ) |
|---|
| 783 | de_dy_int(n) = de_dy_int_l + ( zv(n) - zu(k) ) / & |
|---|
| 784 | dz * ( de_dy_int_u - de_dy_int_l ) |
|---|
| 785 | ENDIF |
|---|
| 786 | |
|---|
| 787 | ! |
|---|
| 788 | !-- Interpolate the TKE gradient along z |
|---|
| 789 | IF ( zv(n) < 0.5_wp * dz ) THEN |
|---|
| 790 | de_dz_int(n) = 0.0_wp |
|---|
| 791 | ELSE |
|---|
| 792 | de_dz_int_l = ( ( gg - aa ) * de_dz(k,j,i) + & |
|---|
| 793 | ( gg - bb ) * de_dz(k,j,i+1) + & |
|---|
| 794 | ( gg - cc ) * de_dz(k,j+1,i) + & |
|---|
| 795 | ( gg - dd ) * de_dz(k,j+1,i+1) & |
|---|
| 796 | ) / ( 3.0_wp * gg ) |
|---|
| 797 | |
|---|
| 798 | IF ( ( k+1 == nzt+1 ) .OR. ( k == nzb ) ) THEN |
|---|
| 799 | de_dz_int(n) = de_dz_int_l |
|---|
| 800 | ELSE |
|---|
| 801 | de_dz_int_u = ( ( gg - aa ) * de_dz(k+1,j,i) + & |
|---|
| 802 | ( gg - bb ) * de_dz(k+1,j,i+1) + & |
|---|
| 803 | ( gg - cc ) * de_dz(k+1,j+1,i) + & |
|---|
| 804 | ( gg - dd ) * de_dz(k+1,j+1,i+1) & |
|---|
| 805 | ) / ( 3.0_wp * gg ) |
|---|
| 806 | de_dz_int(n) = de_dz_int_l + ( zv(n) - zu(k) ) /& |
|---|
| 807 | dz * ( de_dz_int_u - de_dz_int_l ) |
|---|
| 808 | ENDIF |
|---|
| 809 | ENDIF |
|---|
| 810 | |
|---|
| 811 | ! |
|---|
| 812 | !-- Interpolate the dissipation of TKE |
|---|
| 813 | diss_int_l = ( ( gg - aa ) * diss(k,j,i) + & |
|---|
| 814 | ( gg - bb ) * diss(k,j,i+1) + & |
|---|
| 815 | ( gg - cc ) * diss(k,j+1,i) + & |
|---|
| 816 | ( gg - dd ) * diss(k,j+1,i+1) & |
|---|
| 817 | ) / ( 3.0_wp * gg ) |
|---|
| 818 | |
|---|
| 819 | IF ( k == nzt ) THEN |
|---|
| 820 | diss_int(n) = diss_int_l |
|---|
| 821 | ELSE |
|---|
| 822 | diss_int_u = ( ( gg - aa ) * diss(k+1,j,i) + & |
|---|
| 823 | ( gg - bb ) * diss(k+1,j,i+1) + & |
|---|
| 824 | ( gg - cc ) * diss(k+1,j+1,i) + & |
|---|
| 825 | ( gg - dd ) * diss(k+1,j+1,i+1) & |
|---|
| 826 | ) / ( 3.0_wp * gg ) |
|---|
| 827 | diss_int(n) = diss_int_l + ( zv(n) - zu(k) ) / dz *& |
|---|
| 828 | ( diss_int_u - diss_int_l ) |
|---|
| 829 | ENDIF |
|---|
| 830 | ! |
|---|
| 831 | !-- Set flag for stochastic equation. |
|---|
| 832 | term_1_2(n) = 1.0_wp |
|---|
| 833 | |
|---|
| 834 | ELSE |
|---|
| 835 | |
|---|
| 836 | ! |
|---|
| 837 | !-- If wall between gridpoint 1 and gridpoint 5, then |
|---|
| 838 | !-- Neumann boundary condition has to be applied |
|---|
| 839 | IF ( gp_outside_of_building(1) == 1 .AND. & |
|---|
| 840 | gp_outside_of_building(5) == 0 ) THEN |
|---|
| 841 | num_gp = num_gp + 1 |
|---|
| 842 | location(num_gp,1) = i * dx + 0.5_wp * dx |
|---|
| 843 | location(num_gp,2) = j * dy |
|---|
| 844 | location(num_gp,3) = k * dz - 0.5_wp * dz |
|---|
| 845 | ei(num_gp) = e(k,j,i) |
|---|
| 846 | dissi(num_gp) = diss(k,j,i) |
|---|
| 847 | de_dxi(num_gp) = 0.0_wp |
|---|
| 848 | de_dyi(num_gp) = de_dy(k,j,i) |
|---|
| 849 | de_dzi(num_gp) = de_dz(k,j,i) |
|---|
| 850 | ENDIF |
|---|
| 851 | |
|---|
| 852 | IF ( gp_outside_of_building(5) == 1 .AND. & |
|---|
| 853 | gp_outside_of_building(1) == 0 ) THEN |
|---|
| 854 | num_gp = num_gp + 1 |
|---|
| 855 | location(num_gp,1) = i * dx + 0.5_wp * dx |
|---|
| 856 | location(num_gp,2) = j * dy |
|---|
| 857 | location(num_gp,3) = k * dz - 0.5_wp * dz |
|---|
| 858 | ei(num_gp) = e(k,j,i+1) |
|---|
| 859 | dissi(num_gp) = diss(k,j,i+1) |
|---|
| 860 | de_dxi(num_gp) = 0.0_wp |
|---|
| 861 | de_dyi(num_gp) = de_dy(k,j,i+1) |
|---|
| 862 | de_dzi(num_gp) = de_dz(k,j,i+1) |
|---|
| 863 | ENDIF |
|---|
| 864 | |
|---|
| 865 | ! |
|---|
| 866 | !-- If wall between gridpoint 5 and gridpoint 6, then |
|---|
| 867 | !-- then Neumann boundary condition has to be applied |
|---|
| 868 | IF ( gp_outside_of_building(5) == 1 .AND. & |
|---|
| 869 | gp_outside_of_building(6) == 0 ) THEN |
|---|
| 870 | num_gp = num_gp + 1 |
|---|
| 871 | location(num_gp,1) = (i+1) * dx |
|---|
| 872 | location(num_gp,2) = j * dy + 0.5_wp * dy |
|---|
| 873 | location(num_gp,3) = k * dz - 0.5_wp * dz |
|---|
| 874 | ei(num_gp) = e(k,j,i+1) |
|---|
| 875 | dissi(num_gp) = diss(k,j,i+1) |
|---|
| 876 | de_dxi(num_gp) = de_dx(k,j,i+1) |
|---|
| 877 | de_dyi(num_gp) = 0.0_wp |
|---|
| 878 | de_dzi(num_gp) = de_dz(k,j,i+1) |
|---|
| 879 | ENDIF |
|---|
| 880 | |
|---|
| 881 | IF ( gp_outside_of_building(6) == 1 .AND. & |
|---|
| 882 | gp_outside_of_building(5) == 0 ) THEN |
|---|
| 883 | num_gp = num_gp + 1 |
|---|
| 884 | location(num_gp,1) = (i+1) * dx |
|---|
| 885 | location(num_gp,2) = j * dy + 0.5_wp * dy |
|---|
| 886 | location(num_gp,3) = k * dz - 0.5_wp * dz |
|---|
| 887 | ei(num_gp) = e(k,j+1,i+1) |
|---|
| 888 | dissi(num_gp) = diss(k,j+1,i+1) |
|---|
| 889 | de_dxi(num_gp) = de_dx(k,j+1,i+1) |
|---|
| 890 | de_dyi(num_gp) = 0.0_wp |
|---|
| 891 | de_dzi(num_gp) = de_dz(k,j+1,i+1) |
|---|
| 892 | ENDIF |
|---|
| 893 | |
|---|
| 894 | ! |
|---|
| 895 | !-- If wall between gridpoint 2 and gridpoint 6, then |
|---|
| 896 | !-- Neumann boundary condition has to be applied |
|---|
| 897 | IF ( gp_outside_of_building(2) == 1 .AND. & |
|---|
| 898 | gp_outside_of_building(6) == 0 ) THEN |
|---|
| 899 | num_gp = num_gp + 1 |
|---|
| 900 | location(num_gp,1) = i * dx + 0.5_wp * dx |
|---|
| 901 | location(num_gp,2) = (j+1) * dy |
|---|
| 902 | location(num_gp,3) = k * dz - 0.5_wp * dz |
|---|
| 903 | ei(num_gp) = e(k,j+1,i) |
|---|
| 904 | dissi(num_gp) = diss(k,j+1,i) |
|---|
| 905 | de_dxi(num_gp) = 0.0_wp |
|---|
| 906 | de_dyi(num_gp) = de_dy(k,j+1,i) |
|---|
| 907 | de_dzi(num_gp) = de_dz(k,j+1,i) |
|---|
| 908 | ENDIF |
|---|
| 909 | |
|---|
| 910 | IF ( gp_outside_of_building(6) == 1 .AND. & |
|---|
| 911 | gp_outside_of_building(2) == 0 ) THEN |
|---|
| 912 | num_gp = num_gp + 1 |
|---|
| 913 | location(num_gp,1) = i * dx + 0.5_wp * dx |
|---|
| 914 | location(num_gp,2) = (j+1) * dy |
|---|
| 915 | location(num_gp,3) = k * dz - 0.5_wp * dz |
|---|
| 916 | ei(num_gp) = e(k,j+1,i+1) |
|---|
| 917 | dissi(num_gp) = diss(k,j+1,i+1) |
|---|
| 918 | de_dxi(num_gp) = 0.0_wp |
|---|
| 919 | de_dyi(num_gp) = de_dy(k,j+1,i+1) |
|---|
| 920 | de_dzi(num_gp) = de_dz(k,j+1,i+1) |
|---|
| 921 | ENDIF |
|---|
| 922 | |
|---|
| 923 | ! |
|---|
| 924 | !-- If wall between gridpoint 1 and gridpoint 2, then |
|---|
| 925 | !-- Neumann boundary condition has to be applied |
|---|
| 926 | IF ( gp_outside_of_building(1) == 1 .AND. & |
|---|
| 927 | gp_outside_of_building(2) == 0 ) THEN |
|---|
| 928 | num_gp = num_gp + 1 |
|---|
| 929 | location(num_gp,1) = i * dx |
|---|
| 930 | location(num_gp,2) = j * dy + 0.5_wp * dy |
|---|
| 931 | location(num_gp,3) = k * dz - 0.5_wp * dz |
|---|
| 932 | ei(num_gp) = e(k,j,i) |
|---|
| 933 | dissi(num_gp) = diss(k,j,i) |
|---|
| 934 | de_dxi(num_gp) = de_dx(k,j,i) |
|---|
| 935 | de_dyi(num_gp) = 0.0_wp |
|---|
| 936 | de_dzi(num_gp) = de_dz(k,j,i) |
|---|
| 937 | ENDIF |
|---|
| 938 | |
|---|
| 939 | IF ( gp_outside_of_building(2) == 1 .AND. & |
|---|
| 940 | gp_outside_of_building(1) == 0 ) THEN |
|---|
| 941 | num_gp = num_gp + 1 |
|---|
| 942 | location(num_gp,1) = i * dx |
|---|
| 943 | location(num_gp,2) = j * dy + 0.5_wp * dy |
|---|
| 944 | location(num_gp,3) = k * dz - 0.5_wp * dz |
|---|
| 945 | ei(num_gp) = e(k,j+1,i) |
|---|
| 946 | dissi(num_gp) = diss(k,j+1,i) |
|---|
| 947 | de_dxi(num_gp) = de_dx(k,j+1,i) |
|---|
| 948 | de_dyi(num_gp) = 0.0_wp |
|---|
| 949 | de_dzi(num_gp) = de_dz(k,j+1,i) |
|---|
| 950 | ENDIF |
|---|
| 951 | |
|---|
| 952 | ! |
|---|
| 953 | !-- If wall between gridpoint 3 and gridpoint 7, then |
|---|
| 954 | !-- Neumann boundary condition has to be applied |
|---|
| 955 | IF ( gp_outside_of_building(3) == 1 .AND. & |
|---|
| 956 | gp_outside_of_building(7) == 0 ) THEN |
|---|
| 957 | num_gp = num_gp + 1 |
|---|
| 958 | location(num_gp,1) = i * dx + 0.5_wp * dx |
|---|
| 959 | location(num_gp,2) = j * dy |
|---|
| 960 | location(num_gp,3) = k * dz + 0.5_wp * dz |
|---|
| 961 | ei(num_gp) = e(k+1,j,i) |
|---|
| 962 | dissi(num_gp) = diss(k+1,j,i) |
|---|
| 963 | de_dxi(num_gp) = 0.0_wp |
|---|
| 964 | de_dyi(num_gp) = de_dy(k+1,j,i) |
|---|
| 965 | de_dzi(num_gp) = de_dz(k+1,j,i) |
|---|
| 966 | ENDIF |
|---|
| 967 | |
|---|
| 968 | IF ( gp_outside_of_building(7) == 1 .AND. & |
|---|
| 969 | gp_outside_of_building(3) == 0 ) THEN |
|---|
| 970 | num_gp = num_gp + 1 |
|---|
| 971 | location(num_gp,1) = i * dx + 0.5_wp * dx |
|---|
| 972 | location(num_gp,2) = j * dy |
|---|
| 973 | location(num_gp,3) = k * dz + 0.5_wp * dz |
|---|
| 974 | ei(num_gp) = e(k+1,j,i+1) |
|---|
| 975 | dissi(num_gp) = diss(k+1,j,i+1) |
|---|
| 976 | de_dxi(num_gp) = 0.0_wp |
|---|
| 977 | de_dyi(num_gp) = de_dy(k+1,j,i+1) |
|---|
| 978 | de_dzi(num_gp) = de_dz(k+1,j,i+1) |
|---|
| 979 | ENDIF |
|---|
| 980 | |
|---|
| 981 | ! |
|---|
| 982 | !-- If wall between gridpoint 7 and gridpoint 8, then |
|---|
| 983 | !-- Neumann boundary condition has to be applied |
|---|
| 984 | IF ( gp_outside_of_building(7) == 1 .AND. & |
|---|
| 985 | gp_outside_of_building(8) == 0 ) THEN |
|---|
| 986 | num_gp = num_gp + 1 |
|---|
| 987 | location(num_gp,1) = (i+1) * dx |
|---|
| 988 | location(num_gp,2) = j * dy + 0.5_wp * dy |
|---|
| 989 | location(num_gp,3) = k * dz + 0.5_wp * dz |
|---|
| 990 | ei(num_gp) = e(k+1,j,i+1) |
|---|
| 991 | dissi(num_gp) = diss(k+1,j,i+1) |
|---|
| 992 | de_dxi(num_gp) = de_dx(k+1,j,i+1) |
|---|
| 993 | de_dyi(num_gp) = 0.0_wp |
|---|
| 994 | de_dzi(num_gp) = de_dz(k+1,j,i+1) |
|---|
| 995 | ENDIF |
|---|
| 996 | |
|---|
| 997 | IF ( gp_outside_of_building(8) == 1 .AND. & |
|---|
| 998 | gp_outside_of_building(7) == 0 ) THEN |
|---|
| 999 | num_gp = num_gp + 1 |
|---|
| 1000 | location(num_gp,1) = (i+1) * dx |
|---|
| 1001 | location(num_gp,2) = j * dy + 0.5_wp * dy |
|---|
| 1002 | location(num_gp,3) = k * dz + 0.5_wp * dz |
|---|
| 1003 | ei(num_gp) = e(k+1,j+1,i+1) |
|---|
| 1004 | dissi(num_gp) = diss(k+1,j+1,i+1) |
|---|
| 1005 | de_dxi(num_gp) = de_dx(k+1,j+1,i+1) |
|---|
| 1006 | de_dyi(num_gp) = 0.0_wp |
|---|
| 1007 | de_dzi(num_gp) = de_dz(k+1,j+1,i+1) |
|---|
| 1008 | ENDIF |
|---|
| 1009 | |
|---|
| 1010 | ! |
|---|
| 1011 | !-- If wall between gridpoint 4 and gridpoint 8, then |
|---|
| 1012 | !-- Neumann boundary condition has to be applied |
|---|
| 1013 | IF ( gp_outside_of_building(4) == 1 .AND. & |
|---|
| 1014 | gp_outside_of_building(8) == 0 ) THEN |
|---|
| 1015 | num_gp = num_gp + 1 |
|---|
| 1016 | location(num_gp,1) = i * dx + 0.5_wp * dx |
|---|
| 1017 | location(num_gp,2) = (j+1) * dy |
|---|
| 1018 | location(num_gp,3) = k * dz + 0.5_wp * dz |
|---|
| 1019 | ei(num_gp) = e(k+1,j+1,i) |
|---|
| 1020 | dissi(num_gp) = diss(k+1,j+1,i) |
|---|
| 1021 | de_dxi(num_gp) = 0.0_wp |
|---|
| 1022 | de_dyi(num_gp) = de_dy(k+1,j+1,i) |
|---|
| 1023 | de_dzi(num_gp) = de_dz(k+1,j+1,i) |
|---|
| 1024 | ENDIF |
|---|
| 1025 | |
|---|
| 1026 | IF ( gp_outside_of_building(8) == 1 .AND. & |
|---|
| 1027 | gp_outside_of_building(4) == 0 ) THEN |
|---|
| 1028 | num_gp = num_gp + 1 |
|---|
| 1029 | location(num_gp,1) = i * dx + 0.5_wp * dx |
|---|
| 1030 | location(num_gp,2) = (j+1) * dy |
|---|
| 1031 | location(num_gp,3) = k * dz + 0.5_wp * dz |
|---|
| 1032 | ei(num_gp) = e(k+1,j+1,i+1) |
|---|
| 1033 | dissi(num_gp) = diss(k+1,j+1,i+1) |
|---|
| 1034 | de_dxi(num_gp) = 0.0_wp |
|---|
| 1035 | de_dyi(num_gp) = de_dy(k+1,j+1,i+1) |
|---|
| 1036 | de_dzi(num_gp) = de_dz(k+1,j+1,i+1) |
|---|
| 1037 | ENDIF |
|---|
| 1038 | |
|---|
| 1039 | ! |
|---|
| 1040 | !-- If wall between gridpoint 3 and gridpoint 4, then |
|---|
| 1041 | !-- Neumann boundary condition has to be applied |
|---|
| 1042 | IF ( gp_outside_of_building(3) == 1 .AND. & |
|---|
| 1043 | gp_outside_of_building(4) == 0 ) THEN |
|---|
| 1044 | num_gp = num_gp + 1 |
|---|
| 1045 | location(num_gp,1) = i * dx |
|---|
| 1046 | location(num_gp,2) = j * dy + 0.5_wp * dy |
|---|
| 1047 | location(num_gp,3) = k * dz + 0.5_wp * dz |
|---|
| 1048 | ei(num_gp) = e(k+1,j,i) |
|---|
| 1049 | dissi(num_gp) = diss(k+1,j,i) |
|---|
| 1050 | de_dxi(num_gp) = de_dx(k+1,j,i) |
|---|
| 1051 | de_dyi(num_gp) = 0.0_wp |
|---|
| 1052 | de_dzi(num_gp) = de_dz(k+1,j,i) |
|---|
| 1053 | ENDIF |
|---|
| 1054 | |
|---|
| 1055 | IF ( gp_outside_of_building(4) == 1 .AND. & |
|---|
| 1056 | gp_outside_of_building(3) == 0 ) THEN |
|---|
| 1057 | num_gp = num_gp + 1 |
|---|
| 1058 | location(num_gp,1) = i * dx |
|---|
| 1059 | location(num_gp,2) = j * dy + 0.5_wp * dy |
|---|
| 1060 | location(num_gp,3) = k * dz + 0.5_wp * dz |
|---|
| 1061 | ei(num_gp) = e(k+1,j+1,i) |
|---|
| 1062 | dissi(num_gp) = diss(k+1,j+1,i) |
|---|
| 1063 | de_dxi(num_gp) = de_dx(k+1,j+1,i) |
|---|
| 1064 | de_dyi(num_gp) = 0.0_wp |
|---|
| 1065 | de_dzi(num_gp) = de_dz(k+1,j+1,i) |
|---|
| 1066 | ENDIF |
|---|
| 1067 | |
|---|
| 1068 | ! |
|---|
| 1069 | !-- If wall between gridpoint 1 and gridpoint 3, then |
|---|
| 1070 | !-- Neumann boundary condition has to be applied |
|---|
| 1071 | !-- (only one case as only building beneath is possible) |
|---|
| 1072 | IF ( gp_outside_of_building(1) == 0 .AND. & |
|---|
| 1073 | gp_outside_of_building(3) == 1 ) THEN |
|---|
| 1074 | num_gp = num_gp + 1 |
|---|
| 1075 | location(num_gp,1) = i * dx |
|---|
| 1076 | location(num_gp,2) = j * dy |
|---|
| 1077 | location(num_gp,3) = k * dz |
|---|
| 1078 | ei(num_gp) = e(k+1,j,i) |
|---|
| 1079 | dissi(num_gp) = diss(k+1,j,i) |
|---|
| 1080 | de_dxi(num_gp) = de_dx(k+1,j,i) |
|---|
| 1081 | de_dyi(num_gp) = de_dy(k+1,j,i) |
|---|
| 1082 | de_dzi(num_gp) = 0.0_wp |
|---|
| 1083 | ENDIF |
|---|
| 1084 | |
|---|
| 1085 | ! |
|---|
| 1086 | !-- If wall between gridpoint 5 and gridpoint 7, then |
|---|
| 1087 | !-- Neumann boundary condition has to be applied |
|---|
| 1088 | !-- (only one case as only building beneath is possible) |
|---|
| 1089 | IF ( gp_outside_of_building(5) == 0 .AND. & |
|---|
| 1090 | gp_outside_of_building(7) == 1 ) THEN |
|---|
| 1091 | num_gp = num_gp + 1 |
|---|
| 1092 | location(num_gp,1) = (i+1) * dx |
|---|
| 1093 | location(num_gp,2) = j * dy |
|---|
| 1094 | location(num_gp,3) = k * dz |
|---|
| 1095 | ei(num_gp) = e(k+1,j,i+1) |
|---|
| 1096 | dissi(num_gp) = diss(k+1,j,i+1) |
|---|
| 1097 | de_dxi(num_gp) = de_dx(k+1,j,i+1) |
|---|
| 1098 | de_dyi(num_gp) = de_dy(k+1,j,i+1) |
|---|
| 1099 | de_dzi(num_gp) = 0.0_wp |
|---|
| 1100 | ENDIF |
|---|
| 1101 | |
|---|
| 1102 | ! |
|---|
| 1103 | !-- If wall between gridpoint 2 and gridpoint 4, then |
|---|
| 1104 | !-- Neumann boundary condition has to be applied |
|---|
| 1105 | !-- (only one case as only building beneath is possible) |
|---|
| 1106 | IF ( gp_outside_of_building(2) == 0 .AND. & |
|---|
| 1107 | gp_outside_of_building(4) == 1 ) THEN |
|---|
| 1108 | num_gp = num_gp + 1 |
|---|
| 1109 | location(num_gp,1) = i * dx |
|---|
| 1110 | location(num_gp,2) = (j+1) * dy |
|---|
| 1111 | location(num_gp,3) = k * dz |
|---|
| 1112 | ei(num_gp) = e(k+1,j+1,i) |
|---|
| 1113 | dissi(num_gp) = diss(k+1,j+1,i) |
|---|
| 1114 | de_dxi(num_gp) = de_dx(k+1,j+1,i) |
|---|
| 1115 | de_dyi(num_gp) = de_dy(k+1,j+1,i) |
|---|
| 1116 | de_dzi(num_gp) = 0.0_wp |
|---|
| 1117 | ENDIF |
|---|
| 1118 | |
|---|
| 1119 | ! |
|---|
| 1120 | !-- If wall between gridpoint 6 and gridpoint 8, then |
|---|
| 1121 | !-- Neumann boundary condition has to be applied |
|---|
| 1122 | !-- (only one case as only building beneath is possible) |
|---|
| 1123 | IF ( gp_outside_of_building(6) == 0 .AND. & |
|---|
| 1124 | gp_outside_of_building(8) == 1 ) THEN |
|---|
| 1125 | num_gp = num_gp + 1 |
|---|
| 1126 | location(num_gp,1) = (i+1) * dx |
|---|
| 1127 | location(num_gp,2) = (j+1) * dy |
|---|
| 1128 | location(num_gp,3) = k * dz |
|---|
| 1129 | ei(num_gp) = e(k+1,j+1,i+1) |
|---|
| 1130 | dissi(num_gp) = diss(k+1,j+1,i+1) |
|---|
| 1131 | de_dxi(num_gp) = de_dx(k+1,j+1,i+1) |
|---|
| 1132 | de_dyi(num_gp) = de_dy(k+1,j+1,i+1) |
|---|
| 1133 | de_dzi(num_gp) = 0.0_wp |
|---|
| 1134 | ENDIF |
|---|
| 1135 | |
|---|
| 1136 | ! |
|---|
| 1137 | !-- Carry out the interpolation |
|---|
| 1138 | IF ( num_gp == 1 ) THEN |
|---|
| 1139 | ! |
|---|
| 1140 | !-- If only one of the gridpoints is situated outside of the |
|---|
| 1141 | !-- building, it follows that the values at the particle |
|---|
| 1142 | !-- location are the same as the gridpoint values |
|---|
| 1143 | e_int(n) = ei(num_gp) |
|---|
| 1144 | diss_int(n) = dissi(num_gp) |
|---|
| 1145 | de_dx_int(n) = de_dxi(num_gp) |
|---|
| 1146 | de_dy_int(n) = de_dyi(num_gp) |
|---|
| 1147 | de_dz_int(n) = de_dzi(num_gp) |
|---|
| 1148 | ! |
|---|
| 1149 | !-- Set flag for stochastic equation which disables calculation |
|---|
| 1150 | !-- of drift and memory term near topography. |
|---|
| 1151 | term_1_2(n) = 0.0_wp |
|---|
| 1152 | ELSE IF ( num_gp > 1 ) THEN |
|---|
| 1153 | |
|---|
| 1154 | d_sum = 0.0_wp |
|---|
| 1155 | ! |
|---|
| 1156 | !-- Evaluation of the distances between the gridpoints |
|---|
| 1157 | !-- contributing to the interpolated values, and the particle |
|---|
| 1158 | !-- location |
|---|
| 1159 | DO agp = 1, num_gp |
|---|
| 1160 | d_gp_pl(agp) = ( particles(n)%x-location(agp,1) )**2 & |
|---|
| 1161 | + ( particles(n)%y-location(agp,2) )**2 & |
|---|
| 1162 | + ( zv(n)-location(agp,3) )**2 |
|---|
| 1163 | d_sum = d_sum + d_gp_pl(agp) |
|---|
| 1164 | ENDDO |
|---|
| 1165 | |
|---|
| 1166 | ! |
|---|
| 1167 | !-- Finally the interpolation can be carried out |
|---|
| 1168 | e_int(n) = 0.0_wp |
|---|
| 1169 | diss_int(n) = 0.0_wp |
|---|
| 1170 | de_dx_int(n) = 0.0_wp |
|---|
| 1171 | de_dy_int(n) = 0.0_wp |
|---|
| 1172 | de_dz_int(n) = 0.0_wp |
|---|
| 1173 | DO agp = 1, num_gp |
|---|
| 1174 | e_int(n) = e_int(n) + ( d_sum - d_gp_pl(agp) ) * & |
|---|
| 1175 | ei(agp) / ( (num_gp-1) * d_sum ) |
|---|
| 1176 | diss_int(n) = diss_int(n) + ( d_sum - d_gp_pl(agp) ) * & |
|---|
| 1177 | dissi(agp) / ( (num_gp-1) * d_sum ) |
|---|
| 1178 | de_dx_int(n) = de_dx_int(n) + ( d_sum - d_gp_pl(agp) ) * & |
|---|
| 1179 | de_dxi(agp) / ( (num_gp-1) * d_sum ) |
|---|
| 1180 | de_dy_int(n) = de_dy_int(n) + ( d_sum - d_gp_pl(agp) ) * & |
|---|
| 1181 | de_dyi(agp) / ( (num_gp-1) * d_sum ) |
|---|
| 1182 | de_dz_int(n) = de_dz_int(n) + ( d_sum - d_gp_pl(agp) ) * & |
|---|
| 1183 | de_dzi(agp) / ( (num_gp-1) * d_sum ) |
|---|
| 1184 | ENDDO |
|---|
| 1185 | |
|---|
| 1186 | ENDIF |
|---|
| 1187 | e_int(n) = MAX( 1E-20_wp, e_int(n) ) |
|---|
| 1188 | diss_int(n) = MAX( 1E-20_wp, diss_int(n) ) |
|---|
| 1189 | de_dx_int(n) = MAX( 1E-20_wp, de_dx_int(n) ) |
|---|
| 1190 | de_dy_int(n) = MAX( 1E-20_wp, de_dy_int(n) ) |
|---|
| 1191 | de_dz_int(n) = MAX( 1E-20_wp, de_dz_int(n) ) |
|---|
| 1192 | ! |
|---|
| 1193 | !-- Set flag for stochastic equation which disables calculation |
|---|
| 1194 | !-- of drift and memory term near topography. |
|---|
| 1195 | term_1_2(n) = 0.0_wp |
|---|
| 1196 | ENDIF |
|---|
| 1197 | ENDDO |
|---|
| 1198 | ENDIF |
|---|
| 1199 | |
|---|
| 1200 | DO nb = 0,7 |
|---|
| 1201 | i = ip + block_offset(nb)%i_off |
|---|
| 1202 | j = jp + block_offset(nb)%j_off |
|---|
| 1203 | k = kp + block_offset(nb)%k_off |
|---|
| 1204 | |
|---|
| 1205 | DO n = start_index(nb), end_index(nb) |
|---|
| 1206 | ! |
|---|
| 1207 | !-- Vertical interpolation of the horizontally averaged SGS TKE and |
|---|
| 1208 | !-- resolved-scale velocity variances and use the interpolated values |
|---|
| 1209 | !-- to calculate the coefficient fs, which is a measure of the ratio |
|---|
| 1210 | !-- of the subgrid-scale turbulent kinetic energy to the total amount |
|---|
| 1211 | !-- of turbulent kinetic energy. |
|---|
| 1212 | IF ( k == 0 ) THEN |
|---|
| 1213 | e_mean_int = hom(0,1,8,0) |
|---|
| 1214 | ELSE |
|---|
| 1215 | e_mean_int = hom(k,1,8,0) + & |
|---|
| 1216 | ( hom(k+1,1,8,0) - hom(k,1,8,0) ) / & |
|---|
| 1217 | ( zu(k+1) - zu(k) ) * & |
|---|
| 1218 | ( zv(n) - zu(k) ) |
|---|
| 1219 | ENDIF |
|---|
| 1220 | |
|---|
| 1221 | kw = kp - 1 |
|---|
| 1222 | |
|---|
| 1223 | IF ( k == 0 ) THEN |
|---|
| 1224 | aa = hom(k+1,1,30,0) * ( zv(n) / & |
|---|
| 1225 | ( 0.5_wp * ( zu(k+1) - zu(k) ) ) ) |
|---|
| 1226 | bb = hom(k+1,1,31,0) * ( zv(n) / & |
|---|
| 1227 | ( 0.5_wp * ( zu(k+1) - zu(k) ) ) ) |
|---|
| 1228 | cc = hom(kw+1,1,32,0) * ( zv(n) / & |
|---|
| 1229 | ( 1.0_wp * ( zw(kw+1) - zw(kw) ) ) ) |
|---|
| 1230 | ELSE |
|---|
| 1231 | aa = hom(k,1,30,0) + ( hom(k+1,1,30,0) - hom(k,1,30,0) ) * & |
|---|
| 1232 | ( ( zv(n) - zu(k) ) / ( zu(k+1) - zu(k) ) ) |
|---|
| 1233 | bb = hom(k,1,31,0) + ( hom(k+1,1,31,0) - hom(k,1,31,0) ) * & |
|---|
| 1234 | ( ( zv(n) - zu(k) ) / ( zu(k+1) - zu(k) ) ) |
|---|
| 1235 | cc = hom(kw,1,32,0) + ( hom(kw+1,1,32,0)-hom(kw,1,32,0) ) * & |
|---|
| 1236 | ( ( zv(n) - zw(kw) ) / ( zw(kw+1)-zw(kw) ) ) |
|---|
| 1237 | ENDIF |
|---|
| 1238 | |
|---|
| 1239 | vv_int = ( 1.0_wp / 3.0_wp ) * ( aa + bb + cc ) |
|---|
| 1240 | ! |
|---|
| 1241 | !-- Needed to avoid NaN particle velocities. The value of 1.0 is just |
|---|
| 1242 | !-- an educated guess for the given case. |
|---|
| 1243 | IF ( vv_int + ( 2.0_wp / 3.0_wp ) * e_mean_int == 0.0_wp ) THEN |
|---|
| 1244 | fs_int(n) = 1.0_wp |
|---|
| 1245 | ELSE |
|---|
| 1246 | fs_int(n) = ( 2.0_wp / 3.0_wp ) * e_mean_int / & |
|---|
| 1247 | ( vv_int + ( 2.0_wp / 3.0_wp ) * e_mean_int ) |
|---|
| 1248 | ENDIF |
|---|
| 1249 | |
|---|
| 1250 | ENDDO |
|---|
| 1251 | ENDDO |
|---|
| 1252 | |
|---|
| 1253 | DO n = 1, number_of_particles |
|---|
| 1254 | |
|---|
| 1255 | rg(n,1) = random_gauss( iran_part, 5.0_wp ) |
|---|
| 1256 | rg(n,2) = random_gauss( iran_part, 5.0_wp ) |
|---|
| 1257 | rg(n,3) = random_gauss( iran_part, 5.0_wp ) |
|---|
| 1258 | |
|---|
| 1259 | ENDDO |
|---|
| 1260 | |
|---|
| 1261 | DO n = 1, number_of_particles |
|---|
| 1262 | ! |
|---|
| 1263 | !-- Calculate the Lagrangian timescale according to Weil et al. (2004). |
|---|
| 1264 | lagr_timescale = ( 4.0_wp * e_int(n) + 1E-20_wp ) / & |
|---|
| 1265 | ( 3.0_wp * fs_int(n) * c_0 * diss_int(n) + 1E-20_wp ) |
|---|
| 1266 | |
|---|
| 1267 | ! |
|---|
| 1268 | !-- Calculate the next particle timestep. dt_gap is the time needed to |
|---|
| 1269 | !-- complete the current LES timestep. |
|---|
| 1270 | dt_gap = dt_3d - particles(n)%dt_sum |
|---|
| 1271 | dt_particle(n) = MIN( dt_3d, 0.025_wp * lagr_timescale, dt_gap ) |
|---|
| 1272 | |
|---|
| 1273 | ! |
|---|
| 1274 | !-- The particle timestep should not be too small in order to prevent |
|---|
| 1275 | !-- the number of particle timesteps of getting too large |
|---|
| 1276 | IF ( dt_particle(n) < dt_min_part .AND. dt_min_part < dt_gap ) THEN |
|---|
| 1277 | dt_particle(n) = dt_min_part |
|---|
| 1278 | ENDIF |
|---|
| 1279 | |
|---|
| 1280 | ! |
|---|
| 1281 | !-- Calculate the SGS velocity components |
|---|
| 1282 | IF ( particles(n)%age == 0.0_wp ) THEN |
|---|
| 1283 | ! |
|---|
| 1284 | !-- For new particles the SGS components are derived from the SGS |
|---|
| 1285 | !-- TKE. Limit the Gaussian random number to the interval |
|---|
| 1286 | !-- [-5.0*sigma, 5.0*sigma] in order to prevent the SGS velocities |
|---|
| 1287 | !-- from becoming unrealistically large. |
|---|
| 1288 | particles(n)%rvar1 = SQRT( 2.0_wp * sgs_wf_part * e_int(n) + 1E-20_wp ) * & |
|---|
| 1289 | ( rg(n,1) - 1.0_wp ) |
|---|
| 1290 | particles(n)%rvar2 = SQRT( 2.0_wp * sgs_wf_part * e_int(n) + 1E-20_wp ) * & |
|---|
| 1291 | ( rg(n,2) - 1.0_wp ) |
|---|
| 1292 | particles(n)%rvar3 = SQRT( 2.0_wp * sgs_wf_part * e_int(n) + 1E-20_wp ) * & |
|---|
| 1293 | ( rg(n,3) - 1.0_wp ) |
|---|
| 1294 | |
|---|
| 1295 | ELSE |
|---|
| 1296 | ! |
|---|
| 1297 | !-- Restriction of the size of the new timestep: compared to the |
|---|
| 1298 | !-- previous timestep the increase must not exceed 200% |
|---|
| 1299 | |
|---|
| 1300 | dt_particle_m = particles(n)%age - particles(n)%age_m |
|---|
| 1301 | IF ( dt_particle(n) > 2.0_wp * dt_particle_m ) THEN |
|---|
| 1302 | dt_particle(n) = 2.0_wp * dt_particle_m |
|---|
| 1303 | ENDIF |
|---|
| 1304 | |
|---|
| 1305 | ! |
|---|
| 1306 | !-- For old particles the SGS components are correlated with the |
|---|
| 1307 | !-- values from the previous timestep. Random numbers have also to |
|---|
| 1308 | !-- be limited (see above). |
|---|
| 1309 | !-- As negative values for the subgrid TKE are not allowed, the |
|---|
| 1310 | !-- change of the subgrid TKE with time cannot be smaller than |
|---|
| 1311 | !-- -e_int(n)/dt_particle. This value is used as a lower boundary |
|---|
| 1312 | !-- value for the change of TKE |
|---|
| 1313 | |
|---|
| 1314 | de_dt_min = - e_int(n) / dt_particle(n) |
|---|
| 1315 | |
|---|
| 1316 | de_dt = ( e_int(n) - particles(n)%e_m ) / dt_particle_m |
|---|
| 1317 | |
|---|
| 1318 | IF ( de_dt < de_dt_min ) THEN |
|---|
| 1319 | de_dt = de_dt_min |
|---|
| 1320 | ENDIF |
|---|
| 1321 | |
|---|
| 1322 | CALL weil_stochastic_eq(particles(n)%rvar1, fs_int(n), e_int(n), & |
|---|
| 1323 | de_dx_int(n), de_dt, diss_int(n), & |
|---|
| 1324 | dt_particle(n), rg(n,1), term_1_2(n) ) |
|---|
| 1325 | |
|---|
| 1326 | CALL weil_stochastic_eq(particles(n)%rvar2, fs_int(n), e_int(n), & |
|---|
| 1327 | de_dy_int(n), de_dt, diss_int(n), & |
|---|
| 1328 | dt_particle(n), rg(n,2), term_1_2(n) ) |
|---|
| 1329 | |
|---|
| 1330 | CALL weil_stochastic_eq(particles(n)%rvar3, fs_int(n), e_int(n), & |
|---|
| 1331 | de_dz_int(n), de_dt, diss_int(n), & |
|---|
| 1332 | dt_particle(n), rg(n,3), term_1_2(n) ) |
|---|
| 1333 | |
|---|
| 1334 | ENDIF |
|---|
| 1335 | |
|---|
| 1336 | u_int(n) = u_int(n) + particles(n)%rvar1 |
|---|
| 1337 | v_int(n) = v_int(n) + particles(n)%rvar2 |
|---|
| 1338 | w_int(n) = w_int(n) + particles(n)%rvar3 |
|---|
| 1339 | ! |
|---|
| 1340 | !-- Store the SGS TKE of the current timelevel which is needed for |
|---|
| 1341 | !-- for calculating the SGS particle velocities at the next timestep |
|---|
| 1342 | particles(n)%e_m = e_int(n) |
|---|
| 1343 | ENDDO |
|---|
| 1344 | |
|---|
| 1345 | ELSE |
|---|
| 1346 | ! |
|---|
| 1347 | !-- If no SGS velocities are used, only the particle timestep has to |
|---|
| 1348 | !-- be set |
|---|
| 1349 | dt_particle = dt_3d |
|---|
| 1350 | |
|---|
| 1351 | ENDIF |
|---|
| 1352 | ! |
|---|
| 1353 | !-- Store the old age of the particle ( needed to prevent that a |
|---|
| 1354 | !-- particle crosses several PEs during one timestep, and for the |
|---|
| 1355 | !-- evaluation of the subgrid particle velocity fluctuations ) |
|---|
| 1356 | particles(1:number_of_particles)%age_m = particles(1:number_of_particles)%age |
|---|
| 1357 | |
|---|
| 1358 | dens_ratio = particle_groups(particles(1:number_of_particles)%group)%density_ratio |
|---|
| 1359 | |
|---|
| 1360 | IF ( ANY( dens_ratio == 0.0_wp ) ) THEN |
|---|
| 1361 | DO n = 1, number_of_particles |
|---|
| 1362 | |
|---|
| 1363 | ! |
|---|
| 1364 | !-- Particle advection |
|---|
| 1365 | IF ( dens_ratio(n) == 0.0_wp ) THEN |
|---|
| 1366 | ! |
|---|
| 1367 | !-- Pure passive transport (without particle inertia) |
|---|
| 1368 | particles(n)%x = xv(n) + u_int(n) * dt_particle(n) |
|---|
| 1369 | particles(n)%y = yv(n) + v_int(n) * dt_particle(n) |
|---|
| 1370 | particles(n)%z = zv(n) + w_int(n) * dt_particle(n) |
|---|
| 1371 | |
|---|
| 1372 | particles(n)%speed_x = u_int(n) |
|---|
| 1373 | particles(n)%speed_y = v_int(n) |
|---|
| 1374 | particles(n)%speed_z = w_int(n) |
|---|
| 1375 | |
|---|
| 1376 | ELSE |
|---|
| 1377 | ! |
|---|
| 1378 | !-- Transport of particles with inertia |
|---|
| 1379 | particles(n)%x = particles(n)%x + particles(n)%speed_x * & |
|---|
| 1380 | dt_particle(n) |
|---|
| 1381 | particles(n)%y = particles(n)%y + particles(n)%speed_y * & |
|---|
| 1382 | dt_particle(n) |
|---|
| 1383 | particles(n)%z = particles(n)%z + particles(n)%speed_z * & |
|---|
| 1384 | dt_particle(n) |
|---|
| 1385 | |
|---|
| 1386 | ! |
|---|
| 1387 | !-- Update of the particle velocity |
|---|
| 1388 | IF ( cloud_droplets ) THEN |
|---|
| 1389 | ! |
|---|
| 1390 | !-- Terminal velocity is computed for vertical direction (Rogers et |
|---|
| 1391 | !-- al., 1993, J. Appl. Meteorol.) |
|---|
| 1392 | diameter = particles(n)%radius * 2000.0_wp !diameter in mm |
|---|
| 1393 | IF ( diameter <= d0_rog ) THEN |
|---|
| 1394 | w_s = k_cap_rog * diameter * ( 1.0_wp - EXP( -k_low_rog * diameter ) ) |
|---|
| 1395 | ELSE |
|---|
| 1396 | w_s = a_rog - b_rog * EXP( -c_rog * diameter ) |
|---|
| 1397 | ENDIF |
|---|
| 1398 | |
|---|
| 1399 | ! |
|---|
| 1400 | !-- If selected, add random velocities following Soelch and Kaercher |
|---|
| 1401 | !-- (2010, Q. J. R. Meteorol. Soc.) |
|---|
| 1402 | IF ( use_sgs_for_particles ) THEN |
|---|
| 1403 | lagr_timescale = km(kp,jp,ip) / MAX( e(kp,jp,ip), 1.0E-20_wp ) |
|---|
| 1404 | RL = EXP( -1.0_wp * dt_3d / lagr_timescale ) |
|---|
| 1405 | sigma = SQRT( e(kp,jp,ip) ) |
|---|
| 1406 | |
|---|
| 1407 | rg1 = random_gauss( iran_part, 5.0_wp ) - 1.0_wp |
|---|
| 1408 | rg2 = random_gauss( iran_part, 5.0_wp ) - 1.0_wp |
|---|
| 1409 | rg3 = random_gauss( iran_part, 5.0_wp ) - 1.0_wp |
|---|
| 1410 | |
|---|
| 1411 | particles(n)%rvar1 = RL * particles(n)%rvar1 + & |
|---|
| 1412 | SQRT( 1.0_wp - RL**2 ) * sigma * rg1 |
|---|
| 1413 | particles(n)%rvar2 = RL * particles(n)%rvar2 + & |
|---|
| 1414 | SQRT( 1.0_wp - RL**2 ) * sigma * rg2 |
|---|
| 1415 | particles(n)%rvar3 = RL * particles(n)%rvar3 + & |
|---|
| 1416 | SQRT( 1.0_wp - RL**2 ) * sigma * rg3 |
|---|
| 1417 | |
|---|
| 1418 | particles(n)%speed_x = u_int(n) + particles(n)%rvar1 |
|---|
| 1419 | particles(n)%speed_y = v_int(n) + particles(n)%rvar2 |
|---|
| 1420 | particles(n)%speed_z = w_int(n) + particles(n)%rvar3 - w_s |
|---|
| 1421 | ELSE |
|---|
| 1422 | particles(n)%speed_x = u_int(n) |
|---|
| 1423 | particles(n)%speed_y = v_int(n) |
|---|
| 1424 | particles(n)%speed_z = w_int(n) - w_s |
|---|
| 1425 | ENDIF |
|---|
| 1426 | |
|---|
| 1427 | ELSE |
|---|
| 1428 | |
|---|
| 1429 | IF ( use_sgs_for_particles ) THEN |
|---|
| 1430 | exp_arg = particle_groups(particles(n)%group)%exp_arg |
|---|
| 1431 | exp_term = EXP( -exp_arg * dt_particle(n) ) |
|---|
| 1432 | ELSE |
|---|
| 1433 | exp_arg = particle_groups(particles(n)%group)%exp_arg |
|---|
| 1434 | exp_term = particle_groups(particles(n)%group)%exp_term |
|---|
| 1435 | ENDIF |
|---|
| 1436 | particles(n)%speed_x = particles(n)%speed_x * exp_term + & |
|---|
| 1437 | u_int(n) * ( 1.0_wp - exp_term ) |
|---|
| 1438 | particles(n)%speed_y = particles(n)%speed_y * exp_term + & |
|---|
| 1439 | v_int(n) * ( 1.0_wp - exp_term ) |
|---|
| 1440 | particles(n)%speed_z = particles(n)%speed_z * exp_term + & |
|---|
| 1441 | ( w_int(n) - ( 1.0_wp - dens_ratio(n) ) * & |
|---|
| 1442 | g / exp_arg ) * ( 1.0_wp - exp_term ) |
|---|
| 1443 | ENDIF |
|---|
| 1444 | |
|---|
| 1445 | ENDIF |
|---|
| 1446 | |
|---|
| 1447 | ENDDO |
|---|
| 1448 | |
|---|
| 1449 | ELSE |
|---|
| 1450 | |
|---|
| 1451 | DO n = 1, number_of_particles |
|---|
| 1452 | |
|---|
| 1453 | !-- Transport of particles with inertia |
|---|
| 1454 | particles(n)%x = xv(n) + particles(n)%speed_x * dt_particle(n) |
|---|
| 1455 | particles(n)%y = yv(n) + particles(n)%speed_y * dt_particle(n) |
|---|
| 1456 | particles(n)%z = zv(n) + particles(n)%speed_z * dt_particle(n) |
|---|
| 1457 | ! |
|---|
| 1458 | !-- Update of the particle velocity |
|---|
| 1459 | IF ( cloud_droplets ) THEN |
|---|
| 1460 | ! |
|---|
| 1461 | !-- Terminal velocity is computed for vertical direction (Rogers et al., |
|---|
| 1462 | !-- 1993, J. Appl. Meteorol.) |
|---|
| 1463 | diameter = particles(n)%radius * 2000.0_wp !diameter in mm |
|---|
| 1464 | IF ( diameter <= d0_rog ) THEN |
|---|
| 1465 | w_s = k_cap_rog * diameter * ( 1.0_wp - EXP( -k_low_rog * diameter ) ) |
|---|
| 1466 | ELSE |
|---|
| 1467 | w_s = a_rog - b_rog * EXP( -c_rog * diameter ) |
|---|
| 1468 | ENDIF |
|---|
| 1469 | |
|---|
| 1470 | ! |
|---|
| 1471 | !-- If selected, add random velocities following Soelch and Kaercher |
|---|
| 1472 | !-- (2010, Q. J. R. Meteorol. Soc.) |
|---|
| 1473 | IF ( use_sgs_for_particles ) THEN |
|---|
| 1474 | lagr_timescale = km(kp,jp,ip) / MAX( e(kp,jp,ip), 1.0E-20_wp ) |
|---|
| 1475 | RL = EXP( -1.0_wp * dt_3d / lagr_timescale ) |
|---|
| 1476 | sigma = SQRT( e(kp,jp,ip) ) |
|---|
| 1477 | |
|---|
| 1478 | rg1 = random_gauss( iran_part, 5.0_wp ) - 1.0_wp |
|---|
| 1479 | rg2 = random_gauss( iran_part, 5.0_wp ) - 1.0_wp |
|---|
| 1480 | rg3 = random_gauss( iran_part, 5.0_wp ) - 1.0_wp |
|---|
| 1481 | |
|---|
| 1482 | particles(n)%rvar1 = RL * particles(n)%rvar1 + & |
|---|
| 1483 | SQRT( 1.0_wp - RL**2 ) * sigma * rg1 |
|---|
| 1484 | particles(n)%rvar2 = RL * particles(n)%rvar2 + & |
|---|
| 1485 | SQRT( 1.0_wp - RL**2 ) * sigma * rg2 |
|---|
| 1486 | particles(n)%rvar3 = RL * particles(n)%rvar3 + & |
|---|
| 1487 | SQRT( 1.0_wp - RL**2 ) * sigma * rg3 |
|---|
| 1488 | |
|---|
| 1489 | particles(n)%speed_x = u_int(n) + particles(n)%rvar1 |
|---|
| 1490 | particles(n)%speed_y = v_int(n) + particles(n)%rvar2 |
|---|
| 1491 | particles(n)%speed_z = w_int(n) + particles(n)%rvar3 - w_s |
|---|
| 1492 | ELSE |
|---|
| 1493 | particles(n)%speed_x = u_int(n) |
|---|
| 1494 | particles(n)%speed_y = v_int(n) |
|---|
| 1495 | particles(n)%speed_z = w_int(n) - w_s |
|---|
| 1496 | ENDIF |
|---|
| 1497 | |
|---|
| 1498 | ELSE |
|---|
| 1499 | |
|---|
| 1500 | IF ( use_sgs_for_particles ) THEN |
|---|
| 1501 | exp_arg = particle_groups(particles(n)%group)%exp_arg |
|---|
| 1502 | exp_term = EXP( -exp_arg * dt_particle(n) ) |
|---|
| 1503 | ELSE |
|---|
| 1504 | exp_arg = particle_groups(particles(n)%group)%exp_arg |
|---|
| 1505 | exp_term = particle_groups(particles(n)%group)%exp_term |
|---|
| 1506 | ENDIF |
|---|
| 1507 | particles(n)%speed_x = particles(n)%speed_x * exp_term + & |
|---|
| 1508 | u_int(n) * ( 1.0_wp - exp_term ) |
|---|
| 1509 | particles(n)%speed_y = particles(n)%speed_y * exp_term + & |
|---|
| 1510 | v_int(n) * ( 1.0_wp - exp_term ) |
|---|
| 1511 | particles(n)%speed_z = particles(n)%speed_z * exp_term + & |
|---|
| 1512 | ( w_int(n) - ( 1.0_wp - dens_ratio(n) ) * g / & |
|---|
| 1513 | exp_arg ) * ( 1.0_wp - exp_term ) |
|---|
| 1514 | ENDIF |
|---|
| 1515 | |
|---|
| 1516 | ENDDO |
|---|
| 1517 | |
|---|
| 1518 | ENDIF |
|---|
| 1519 | |
|---|
| 1520 | DO n = 1, number_of_particles |
|---|
| 1521 | ! |
|---|
| 1522 | !-- Increment the particle age and the total time that the particle |
|---|
| 1523 | !-- has advanced within the particle timestep procedure |
|---|
| 1524 | particles(n)%age = particles(n)%age + dt_particle(n) |
|---|
| 1525 | particles(n)%dt_sum = particles(n)%dt_sum + dt_particle(n) |
|---|
| 1526 | |
|---|
| 1527 | ! |
|---|
| 1528 | !-- Check whether there is still a particle that has not yet completed |
|---|
| 1529 | !-- the total LES timestep |
|---|
| 1530 | IF ( ( dt_3d - particles(n)%dt_sum ) > 1E-8_wp ) THEN |
|---|
| 1531 | dt_3d_reached_l = .FALSE. |
|---|
| 1532 | ENDIF |
|---|
| 1533 | |
|---|
| 1534 | ENDDO |
|---|
| 1535 | |
|---|
| 1536 | CALL cpu_log( log_point_s(44), 'lpm_advec', 'pause' ) |
|---|
| 1537 | |
|---|
| 1538 | |
|---|
| 1539 | END SUBROUTINE lpm_advec |
|---|
| 1540 | |
|---|
| 1541 | ! Description: |
|---|
| 1542 | ! ------------ |
|---|
| 1543 | !> Calculation of subgrid-scale particle speed using the stochastic model |
|---|
| 1544 | !> of Weil et al. (2004, JAS, 61, 2877-2887). |
|---|
| 1545 | !------------------------------------------------------------------------------! |
|---|
| 1546 | SUBROUTINE weil_stochastic_eq( v_sgs, fs_n, e_n, dedxi_n, dedt_n, diss_n, & |
|---|
| 1547 | dt_n, rg_n, fac ) |
|---|
| 1548 | |
|---|
| 1549 | USE kinds |
|---|
| 1550 | |
|---|
| 1551 | USE particle_attributes, & |
|---|
| 1552 | ONLY: c_0, sgs_wf_part |
|---|
| 1553 | |
|---|
| 1554 | IMPLICIT NONE |
|---|
| 1555 | |
|---|
| 1556 | REAL(wp) :: a1 !< dummy argument |
|---|
| 1557 | REAL(wp) :: dedt_n !< time derivative of TKE at particle position |
|---|
| 1558 | REAL(wp) :: dedxi_n !< horizontal derivative of TKE at particle position |
|---|
| 1559 | REAL(wp) :: diss_n !< dissipation at particle position |
|---|
| 1560 | REAL(wp) :: dt_n !< particle timestep |
|---|
| 1561 | REAL(wp) :: e_n !< TKE at particle position |
|---|
| 1562 | REAL(wp) :: fac !< flag to identify adjacent topography |
|---|
| 1563 | REAL(wp) :: fs_n !< weighting factor to prevent that subgrid-scale particle speed becomes too large |
|---|
| 1564 | REAL(wp) :: sgs_w !< constant (1/3) |
|---|
| 1565 | REAL(wp) :: rg_n !< random number |
|---|
| 1566 | REAL(wp) :: term1 !< memory term |
|---|
| 1567 | REAL(wp) :: term2 !< drift correction term |
|---|
| 1568 | REAL(wp) :: term3 !< random term |
|---|
| 1569 | REAL(wp) :: v_sgs !< subgrid-scale velocity component |
|---|
| 1570 | |
|---|
| 1571 | ! |
|---|
| 1572 | !-- Please note, terms 1 and 2 (drift and memory term, respectively) are |
|---|
| 1573 | !-- multiplied by a flag to switch of both terms near topography. |
|---|
| 1574 | !-- This is necessary, as both terms may cause a subgrid-scale velocity build up |
|---|
| 1575 | !-- if particles are trapped in regions with very small TKE, e.g. in narrow street |
|---|
| 1576 | !-- canyons resolved by only a few grid points. Hence, term 1 and term 2 are |
|---|
| 1577 | !-- disabled if one of the adjacent grid points belongs to topography. |
|---|
| 1578 | !-- Moreover, in this case, the previous subgrid-scale component is also set |
|---|
| 1579 | !-- to zero. |
|---|
| 1580 | |
|---|
| 1581 | a1 = fs_n * c_0 * diss_n |
|---|
| 1582 | ! |
|---|
| 1583 | !-- Memory term |
|---|
| 1584 | term1 = - a1 * v_sgs * dt_n / ( 4.0_wp * sgs_wf_part * e_n + 1E-20_wp ) & |
|---|
| 1585 | * fac |
|---|
| 1586 | ! |
|---|
| 1587 | !-- Drift correction term |
|---|
| 1588 | term2 = ( ( dedt_n * v_sgs / e_n ) + dedxi_n ) * 0.5_wp * dt_n & |
|---|
| 1589 | * fac |
|---|
| 1590 | ! |
|---|
| 1591 | !-- Random term |
|---|
| 1592 | term3 = SQRT( MAX( a1, 1E-20 ) ) * ( rg_n - 1.0_wp ) * SQRT( dt_n ) |
|---|
| 1593 | ! |
|---|
| 1594 | !-- In cese one of the adjacent grid-boxes belongs to topograhy, the previous |
|---|
| 1595 | !-- subgrid-scale velocity component is set to zero, in order to prevent a |
|---|
| 1596 | !-- velocity build-up. |
|---|
| 1597 | |
|---|
| 1598 | !-- This case, set also previous subgrid-scale component to zero. |
|---|
| 1599 | v_sgs = v_sgs * fac + term1 + term2 + term3 |
|---|
| 1600 | |
|---|
| 1601 | END SUBROUTINE weil_stochastic_eq |
|---|
