| 1 | SUBROUTINE lpm_advec (ip,jp,kp) |
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| 2 | |
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| 3 | !--------------------------------------------------------------------------------! |
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| 4 | ! This file is part of PALM. |
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| 5 | ! |
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| 6 | ! PALM is free software: you can redistribute it and/or modify it under the terms |
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| 7 | ! of the GNU General Public License as published by the Free Software Foundation, |
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| 8 | ! either version 3 of the License, or (at your option) any later version. |
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| 9 | ! |
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| 10 | ! PALM is distributed in the hope that it will be useful, but WITHOUT ANY |
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| 11 | ! WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS FOR |
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| 12 | ! A PARTICULAR PURPOSE. See the GNU General Public License for more details. |
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| 13 | ! |
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| 14 | ! You should have received a copy of the GNU General Public License along with |
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| 15 | ! PALM. If not, see <http://www.gnu.org/licenses/>. |
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| 16 | ! |
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| 17 | ! Copyright 1997-2014 Leibniz Universitaet Hannover |
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| 18 | !--------------------------------------------------------------------------------! |
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| 19 | ! |
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| 20 | ! Current revisions: |
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| 21 | ! ------------------ |
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| 22 | ! |
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| 23 | ! |
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| 24 | ! Former revisions: |
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| 25 | ! ----------------- |
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| 26 | ! $Id: lpm_advec.f90 1370 2014-04-24 06:06:17Z maronga $ |
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| 27 | ! |
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| 28 | ! 1369 2014-04-24 05:57:38Z raasch |
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| 29 | ! usage of module interfaces removed |
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| 30 | ! |
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| 31 | ! 1359 2014-04-11 17:15:14Z hoffmann |
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| 32 | ! New particle structure integrated. |
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| 33 | ! Kind definition added to all floating point numbers. |
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| 34 | ! |
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| 35 | ! 1322 2014-03-20 16:38:49Z raasch |
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| 36 | ! REAL constants defined as wp_kind |
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| 37 | ! |
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| 38 | ! 1320 2014-03-20 08:40:49Z raasch |
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| 39 | ! ONLY-attribute added to USE-statements, |
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| 40 | ! kind-parameters added to all INTEGER and REAL declaration statements, |
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| 41 | ! kinds are defined in new module kinds, |
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| 42 | ! revision history before 2012 removed, |
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| 43 | ! comment fields (!:) to be used for variable explanations added to |
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| 44 | ! all variable declaration statements |
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| 45 | ! |
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| 46 | ! 1314 2014-03-14 18:25:17Z suehring |
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| 47 | ! Vertical logarithmic interpolation of horizontal particle speed for particles |
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| 48 | ! between roughness height and first vertical grid level. |
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| 49 | ! |
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| 50 | ! 1036 2012-10-22 13:43:42Z raasch |
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| 51 | ! code put under GPL (PALM 3.9) |
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| 52 | ! |
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| 53 | ! 849 2012-03-15 10:35:09Z raasch |
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| 54 | ! initial revision (former part of advec_particles) |
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| 55 | ! |
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| 56 | ! |
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| 57 | ! Description: |
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| 58 | ! ------------ |
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| 59 | ! Calculation of new particle positions due to advection using a simple Euler |
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| 60 | ! scheme. Particles may feel inertia effects. SGS transport can be included |
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| 61 | ! using the stochastic model of Weil et al. (2004, JAS, 61, 2877-2887). |
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| 62 | !------------------------------------------------------------------------------! |
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| 63 | |
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| 64 | USE arrays_3d, & |
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| 65 | ONLY: de_dx, de_dy, de_dz, diss, e, u, us, usws, v, vsws, w, z0, zu, & |
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| 66 | zw |
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| 67 | |
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| 68 | USE cpulog |
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| 69 | |
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| 70 | USE pegrid |
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| 71 | |
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| 72 | USE control_parameters, & |
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| 73 | ONLY: atmos_ocean_sign, cloud_droplets, dt_3d, dt_3d_reached_l, dz, & |
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| 74 | g, kappa, molecular_viscosity, prandtl_layer, topography, & |
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| 75 | u_gtrans, v_gtrans, simulated_time |
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| 76 | |
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| 77 | USE grid_variables, & |
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| 78 | ONLY: ddx, dx, ddy, dy |
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| 79 | |
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| 80 | USE indices, & |
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| 81 | ONLY: nzb, nzb_s_inner, nzt |
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| 82 | |
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| 83 | USE kinds |
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| 84 | |
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| 85 | USE particle_attributes, & |
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| 86 | ONLY: block_offset, c_0, density_ratio, dt_min_part, grid_particles, & |
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| 87 | iran_part, log_z_z0, number_of_particles, number_of_sublayers, & |
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| 88 | particles, particle_groups, offset_ocean_nzt, & |
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| 89 | offset_ocean_nzt_m1, sgs_wfu_part, sgs_wfv_part, sgs_wfw_part, & |
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| 90 | use_sgs_for_particles, vertical_particle_advection, z0_av_global |
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| 91 | |
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| 92 | USE statistics, & |
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| 93 | ONLY: hom |
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| 94 | |
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| 95 | IMPLICIT NONE |
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| 96 | |
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| 97 | INTEGER(iwp) :: agp !: |
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| 98 | INTEGER(iwp) :: gp_outside_of_building(1:8) !: |
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| 99 | INTEGER(iwp) :: i !: |
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| 100 | INTEGER(iwp) :: ip !: |
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| 101 | INTEGER(iwp) :: j !: |
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| 102 | INTEGER(iwp) :: jp !: |
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| 103 | INTEGER(iwp) :: k !: |
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| 104 | INTEGER(iwp) :: kp !: |
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| 105 | INTEGER(iwp) :: kw !: |
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| 106 | INTEGER(iwp) :: n !: |
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| 107 | INTEGER(iwp) :: nb !: |
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| 108 | INTEGER(iwp) :: num_gp !: |
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| 109 | |
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| 110 | INTEGER(iwp), DIMENSION(0:7) :: start_index !: |
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| 111 | INTEGER(iwp), DIMENSION(0:7) :: end_index !: |
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| 112 | |
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| 113 | REAL(wp) :: aa !: |
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| 114 | REAL(wp) :: bb !: |
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| 115 | REAL(wp) :: cc !: |
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| 116 | REAL(wp) :: d_sum !: |
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| 117 | REAL(wp) :: d_z_p_z0 !: |
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| 118 | REAL(wp) :: dd !: |
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| 119 | REAL(wp) :: de_dx_int_l !: |
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| 120 | REAL(wp) :: de_dx_int_u !: |
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| 121 | REAL(wp) :: de_dy_int_l !: |
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| 122 | REAL(wp) :: de_dy_int_u !: |
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| 123 | REAL(wp) :: de_dt !: |
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| 124 | REAL(wp) :: de_dt_min !: |
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| 125 | REAL(wp) :: de_dz_int_l !: |
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| 126 | REAL(wp) :: de_dz_int_u !: |
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| 127 | REAL(wp) :: diss_int_l !: |
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| 128 | REAL(wp) :: diss_int_u !: |
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| 129 | REAL(wp) :: dt_gap !: |
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| 130 | REAL(wp) :: dt_particle_m !: |
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| 131 | REAL(wp) :: e_int_l !: |
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| 132 | REAL(wp) :: e_int_u !: |
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| 133 | REAL(wp) :: e_mean_int !: |
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| 134 | REAL(wp) :: exp_arg !: |
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| 135 | REAL(wp) :: exp_term !: |
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| 136 | REAL(wp) :: gg !: |
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| 137 | REAL(wp) :: height_int !: |
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| 138 | REAL(wp) :: height_p !: |
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| 139 | REAL(wp) :: lagr_timescale !: |
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| 140 | REAL(wp) :: location(1:30,1:3) !: |
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| 141 | REAL(wp) :: random_gauss !: |
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| 142 | REAL(wp) :: u_int_l !: |
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| 143 | REAL(wp) :: u_int_u !: |
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| 144 | REAL(wp) :: us_int !: |
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| 145 | REAL(wp) :: v_int_l !: |
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| 146 | REAL(wp) :: v_int_u !: |
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| 147 | REAL(wp) :: vv_int !: |
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| 148 | REAL(wp) :: w_int_l !: |
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| 149 | REAL(wp) :: w_int_u !: |
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| 150 | REAL(wp) :: x !: |
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| 151 | REAL(wp) :: y !: |
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| 152 | REAL(wp) :: z_p !: |
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| 153 | |
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| 154 | REAL(wp), DIMENSION(1:30) :: d_gp_pl !: |
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| 155 | REAL(wp), DIMENSION(1:30) :: de_dxi !: |
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| 156 | REAL(wp), DIMENSION(1:30) :: de_dyi !: |
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| 157 | REAL(wp), DIMENSION(1:30) :: de_dzi !: |
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| 158 | REAL(wp), DIMENSION(1:30) :: dissi !: |
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| 159 | REAL(wp), DIMENSION(1:30) :: ei !: |
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| 160 | |
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| 161 | REAL(wp), DIMENSION(number_of_particles) :: dens_ratio !: |
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| 162 | REAL(wp), DIMENSION(number_of_particles) :: de_dx_int !: |
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| 163 | REAL(wp), DIMENSION(number_of_particles) :: de_dy_int !: |
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| 164 | REAL(wp), DIMENSION(number_of_particles) :: de_dz_int !: |
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| 165 | REAL(wp), DIMENSION(number_of_particles) :: diss_int !: |
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| 166 | REAL(wp), DIMENSION(number_of_particles) :: dt_particle !: |
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| 167 | REAL(wp), DIMENSION(number_of_particles) :: e_int !: |
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| 168 | REAL(wp), DIMENSION(number_of_particles) :: fs_int !: |
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| 169 | REAL(wp), DIMENSION(number_of_particles) :: log_z_z0_int !: |
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| 170 | REAL(wp), DIMENSION(number_of_particles) :: u_int !: |
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| 171 | REAL(wp), DIMENSION(number_of_particles) :: v_int !: |
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| 172 | REAL(wp), DIMENSION(number_of_particles) :: w_int !: |
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| 173 | REAL(wp), DIMENSION(number_of_particles) :: xv !: |
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| 174 | REAL(wp), DIMENSION(number_of_particles) :: yv !: |
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| 175 | REAL(wp), DIMENSION(number_of_particles) :: zv !: |
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| 176 | |
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| 177 | REAL(wp), DIMENSION(number_of_particles, 3) :: rg !: |
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| 178 | |
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| 179 | CALL cpu_log( log_point_s(44), 'lpm_advec', 'continue' ) |
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| 180 | |
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| 181 | ! |
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| 182 | !-- Determine height of Prandtl layer and distance between Prandtl-layer |
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| 183 | !-- height and horizontal mean roughness height, which are required for |
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| 184 | !-- vertical logarithmic interpolation of horizontal particle speeds |
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| 185 | !-- (for particles below first vertical grid level). |
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| 186 | z_p = zu(nzb+1) - zw(nzb) |
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| 187 | d_z_p_z0 = 1.0_wp / ( z_p - z0_av_global ) |
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| 188 | |
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| 189 | start_index = grid_particles(kp,jp,ip)%start_index |
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| 190 | end_index = grid_particles(kp,jp,ip)%end_index |
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| 191 | |
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| 192 | xv = particles(1:number_of_particles)%x |
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| 193 | yv = particles(1:number_of_particles)%y |
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| 194 | zv = particles(1:number_of_particles)%z |
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| 195 | |
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| 196 | DO nb = 0, 7 |
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| 197 | |
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| 198 | i = ip |
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| 199 | j = jp + block_offset(nb)%j_off |
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| 200 | k = kp + block_offset(nb)%k_off |
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| 201 | |
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| 202 | ! |
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| 203 | !-- Interpolate u velocity-component |
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| 204 | DO n = start_index(nb), end_index(nb) |
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| 205 | ! |
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| 206 | !-- Interpolation of the u velocity component onto particle position. |
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| 207 | !-- Particles are interpolation bi-linearly in the horizontal and a |
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| 208 | !-- linearly in the vertical. An exception is made for particles below |
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| 209 | !-- the first vertical grid level in case of a prandtl layer. In this |
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| 210 | !-- case the horizontal particle velocity components are determined using |
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| 211 | !-- Monin-Obukhov relations (if branch). |
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| 212 | !-- First, check if particle is located below first vertical grid level |
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| 213 | !-- (Prandtl-layer height) |
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| 214 | IF ( prandtl_layer .AND. particles(n)%z < z_p ) THEN |
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| 215 | ! |
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| 216 | !-- Resolved-scale horizontal particle velocity is zero below z0. |
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| 217 | IF ( particles(n)%z < z0_av_global ) THEN |
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| 218 | u_int(n) = 0.0_wp |
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| 219 | ELSE |
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| 220 | ! |
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| 221 | !-- Determine the sublayer. Further used as index. |
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| 222 | height_p = ( particles(n)%z - z0_av_global ) & |
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| 223 | * REAL( number_of_sublayers, KIND=wp ) & |
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| 224 | * d_z_p_z0 |
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| 225 | ! |
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| 226 | !-- Calculate LOG(z/z0) for exact particle height. Therefore, |
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| 227 | !-- interpolate linearly between precalculated logarithm. |
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| 228 | log_z_z0_int(n) = log_z_z0(INT(height_p)) & |
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| 229 | + ( height_p - INT(height_p) ) & |
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| 230 | * ( log_z_z0(INT(height_p)+1) & |
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| 231 | - log_z_z0(INT(height_p)) & |
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| 232 | ) |
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| 233 | ! |
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| 234 | !-- Neutral solution is applied for all situations, e.g. also for |
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| 235 | !-- unstable and stable situations. Even though this is not exact |
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| 236 | !-- this saves a lot of CPU time since several calls of intrinsic |
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| 237 | !-- FORTRAN procedures (LOG, ATAN) are avoided, This is justified |
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| 238 | !-- as sensitivity studies revealed no significant effect of |
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| 239 | !-- using the neutral solution also for un/stable situations. |
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| 240 | !-- Calculated left and bottom index on u grid. |
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| 241 | us_int = 0.5_wp * ( us(j,i) + us(j,i-1) ) |
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| 242 | |
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| 243 | u_int = -usws(j,i) / ( us_int * kappa + 1E-10_wp ) & |
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| 244 | * log_z_z0_int(n) |
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| 245 | |
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| 246 | ENDIF |
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| 247 | ! |
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| 248 | !-- Particle above the first grid level. Bi-linear interpolation in the |
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| 249 | !-- horizontal and linear interpolation in the vertical direction. |
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| 250 | ELSE |
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| 251 | |
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| 252 | x = xv(n) + ( 0.5_wp - i ) * dx |
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| 253 | y = yv(n) - j * dy |
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| 254 | aa = x**2 + y**2 |
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| 255 | bb = ( dx - x )**2 + y**2 |
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| 256 | cc = x**2 + ( dy - y )**2 |
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| 257 | dd = ( dx - x )**2 + ( dy - y )**2 |
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| 258 | gg = aa + bb + cc + dd |
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| 259 | |
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| 260 | u_int_l = ( ( gg - aa ) * u(k,j,i) + ( gg - bb ) * u(k,j,i+1) & |
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| 261 | + ( gg - cc ) * u(k,j+1,i) + ( gg - dd ) * & |
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| 262 | u(k,j+1,i+1) ) / ( 3.0_wp * gg ) - u_gtrans |
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| 263 | |
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| 264 | IF ( k == nzt ) THEN |
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| 265 | u_int(n) = u_int_l |
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| 266 | ELSE |
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| 267 | u_int_u = ( ( gg-aa ) * u(k+1,j,i) + ( gg-bb ) * u(k+1,j,i+1) & |
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| 268 | + ( gg-cc ) * u(k+1,j+1,i) + ( gg-dd ) * & |
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| 269 | u(k+1,j+1,i+1) ) / ( 3.0_wp * gg ) - u_gtrans |
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| 270 | u_int(n) = u_int_l + ( zv(n) - zu(k) ) / dz * & |
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| 271 | ( u_int_u - u_int_l ) |
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| 272 | ENDIF |
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| 273 | ENDIF |
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| 274 | |
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| 275 | ENDDO |
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| 276 | |
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| 277 | i = ip + block_offset(nb)%i_off |
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| 278 | j = jp |
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| 279 | k = kp + block_offset(nb)%k_off |
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| 280 | ! |
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| 281 | !-- Same procedure for interpolation of the v velocity-component |
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| 282 | DO n = start_index(nb), end_index(nb) |
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| 283 | IF ( prandtl_layer .AND. particles(n)%z < z_p ) THEN |
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| 284 | |
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| 285 | IF ( particles(n)%z < z0_av_global ) THEN |
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| 286 | ! |
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| 287 | !-- Resolved-scale horizontal particle velocity is zero below z0. |
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| 288 | v_int(n) = 0.0_wp |
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| 289 | ELSE |
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| 290 | ! |
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| 291 | !-- Neutral solution is applied for all situations, e.g. also for |
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| 292 | !-- unstable and stable situations. Even though this is not exact |
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| 293 | !-- this saves a lot of CPU time since several calls of intrinsic |
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| 294 | !-- FORTRAN procedures (LOG, ATAN) are avoided, This is justified |
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| 295 | !-- as sensitivity studies revealed no significant effect of |
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| 296 | !-- using the neutral solution also for un/stable situations. |
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| 297 | !-- Calculated left and bottom index on v grid. |
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| 298 | us_int = 0.5_wp * ( us(j,i) + us(j-1,i) ) |
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| 299 | |
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| 300 | v_int = -vsws(j,i) / ( us_int * kappa + 1E-10_wp ) & |
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| 301 | * log_z_z0_int(n) |
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| 302 | ENDIF |
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| 303 | ELSE |
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| 304 | x = xv(n) - i * dx |
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| 305 | y = yv(n) + ( 0.5_wp - j ) * dy |
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| 306 | aa = x**2 + y**2 |
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| 307 | bb = ( dx - x )**2 + y**2 |
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| 308 | cc = x**2 + ( dy - y )**2 |
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| 309 | dd = ( dx - x )**2 + ( dy - y )**2 |
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| 310 | gg = aa + bb + cc + dd |
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| 311 | |
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| 312 | v_int_l = ( ( gg - aa ) * v(k,j,i) + ( gg - bb ) * v(k,j,i+1) & |
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| 313 | + ( gg - cc ) * v(k,j+1,i) + ( gg - dd ) * v(k,j+1,i+1) & |
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| 314 | ) / ( 3.0_wp * gg ) - v_gtrans |
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| 315 | |
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| 316 | IF ( k == nzt ) THEN |
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| 317 | v_int(n) = v_int_l |
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| 318 | ELSE |
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| 319 | v_int_u = ( ( gg-aa ) * v(k+1,j,i) + ( gg-bb ) * v(k+1,j,i+1) & |
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| 320 | + ( gg-cc ) * v(k+1,j+1,i) + ( gg-dd ) * v(k+1,j+1,i+1) & |
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| 321 | ) / ( 3.0_wp * gg ) - v_gtrans |
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| 322 | v_int(n) = v_int_l + ( zv(n) - zu(k) ) / dz * & |
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| 323 | ( v_int_u - v_int_l ) |
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| 324 | ENDIF |
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| 325 | ENDIF |
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| 326 | |
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| 327 | ENDDO |
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| 328 | |
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| 329 | i = ip + block_offset(nb)%i_off |
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| 330 | j = jp + block_offset(nb)%j_off |
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| 331 | k = kp-1 |
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| 332 | ! |
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| 333 | !-- Same procedure for interpolation of the w velocity-component |
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| 334 | DO n = start_index(nb), end_index(nb) |
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| 335 | |
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| 336 | IF ( vertical_particle_advection(particles(n)%group) ) THEN |
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| 337 | |
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| 338 | x = xv(n) - i * dx |
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| 339 | y = yv(n) - j * dy |
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| 340 | aa = x**2 + y**2 |
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| 341 | bb = ( dx - x )**2 + y**2 |
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| 342 | cc = x**2 + ( dy - y )**2 |
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| 343 | dd = ( dx - x )**2 + ( dy - y )**2 |
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| 344 | gg = aa + bb + cc + dd |
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| 345 | |
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| 346 | w_int_l = ( ( gg - aa ) * w(k,j,i) + ( gg - bb ) * w(k,j,i+1) & |
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| 347 | + ( gg - cc ) * w(k,j+1,i) + ( gg - dd ) * w(k,j+1,i+1) & |
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| 348 | ) / ( 3.0_wp * gg ) |
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| 349 | |
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| 350 | IF ( k == nzt ) THEN |
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| 351 | w_int(n) = w_int_l |
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| 352 | ELSE |
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| 353 | w_int_u = ( ( gg-aa ) * w(k+1,j,i) + & |
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| 354 | ( gg-bb ) * w(k+1,j,i+1) + & |
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| 355 | ( gg-cc ) * w(k+1,j+1,i) + & |
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| 356 | ( gg-dd ) * w(k+1,j+1,i+1) & |
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| 357 | ) / ( 3.0_wp * gg ) |
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| 358 | w_int(n) = w_int_l + ( zv(n) - zw(k) ) / dz * & |
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| 359 | ( w_int_u - w_int_l ) |
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| 360 | ENDIF |
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| 361 | |
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| 362 | ELSE |
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| 363 | |
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| 364 | w_int(n) = 0.0_wp |
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| 365 | |
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| 366 | ENDIF |
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| 367 | |
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| 368 | ENDDO |
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| 369 | |
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| 370 | ENDDO |
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| 371 | |
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| 372 | !-- Interpolate and calculate quantities needed for calculating the SGS |
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| 373 | !-- velocities |
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| 374 | IF ( use_sgs_for_particles ) THEN |
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| 375 | |
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| 376 | IF ( topography == 'flat' ) THEN |
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| 377 | |
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| 378 | DO nb = 0,7 |
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| 379 | |
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| 380 | i = ip + block_offset(nb)%i_off |
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| 381 | j = jp + block_offset(nb)%j_off |
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| 382 | k = kp + block_offset(nb)%k_off |
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| 383 | |
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| 384 | DO n = start_index(nb), end_index(nb) |
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| 385 | ! |
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| 386 | !-- Interpolate TKE |
|---|
| 387 | x = xv(n) - i * dx |
|---|
| 388 | y = yv(n) - j * dy |
|---|
| 389 | aa = x**2 + y**2 |
|---|
| 390 | bb = ( dx - x )**2 + y**2 |
|---|
| 391 | cc = x**2 + ( dy - y )**2 |
|---|
| 392 | dd = ( dx - x )**2 + ( dy - y )**2 |
|---|
| 393 | gg = aa + bb + cc + dd |
|---|
| 394 | |
|---|
| 395 | e_int_l = ( ( gg-aa ) * e(k,j,i) + ( gg-bb ) * e(k,j,i+1) & |
|---|
| 396 | + ( gg-cc ) * e(k,j+1,i) + ( gg-dd ) * e(k,j+1,i+1) & |
|---|
| 397 | ) / ( 3.0_wp * gg ) |
|---|
| 398 | |
|---|
| 399 | IF ( k+1 == nzt+1 ) THEN |
|---|
| 400 | e_int(n) = e_int_l |
|---|
| 401 | ELSE |
|---|
| 402 | e_int_u = ( ( gg - aa ) * e(k+1,j,i) + & |
|---|
| 403 | ( gg - bb ) * e(k+1,j,i+1) + & |
|---|
| 404 | ( gg - cc ) * e(k+1,j+1,i) + & |
|---|
| 405 | ( gg - dd ) * e(k+1,j+1,i+1) & |
|---|
| 406 | ) / ( 3.0_wp * gg ) |
|---|
| 407 | e_int(n) = e_int_l + ( zv(n) - zu(k) ) / dz * & |
|---|
| 408 | ( e_int_u - e_int_l ) |
|---|
| 409 | ENDIF |
|---|
| 410 | ! |
|---|
| 411 | !-- Needed to avoid NaN particle velocities |
|---|
| 412 | IF ( e_int(n) == 0.0_wp ) THEN |
|---|
| 413 | e_int(n) = 1.0E-20_wp |
|---|
| 414 | ENDIF |
|---|
| 415 | ! |
|---|
| 416 | !-- Interpolate the TKE gradient along x (adopt incides i,j,k and |
|---|
| 417 | !-- all position variables from above (TKE)) |
|---|
| 418 | de_dx_int_l = ( ( gg - aa ) * de_dx(k,j,i) + & |
|---|
| 419 | ( gg - bb ) * de_dx(k,j,i+1) + & |
|---|
| 420 | ( gg - cc ) * de_dx(k,j+1,i) + & |
|---|
| 421 | ( gg - dd ) * de_dx(k,j+1,i+1) & |
|---|
| 422 | ) / ( 3.0_wp * gg ) |
|---|
| 423 | |
|---|
| 424 | IF ( ( k+1 == nzt+1 ) .OR. ( k == nzb ) ) THEN |
|---|
| 425 | de_dx_int(n) = de_dx_int_l |
|---|
| 426 | ELSE |
|---|
| 427 | de_dx_int_u = ( ( gg - aa ) * de_dx(k+1,j,i) + & |
|---|
| 428 | ( gg - bb ) * de_dx(k+1,j,i+1) + & |
|---|
| 429 | ( gg - cc ) * de_dx(k+1,j+1,i) + & |
|---|
| 430 | ( gg - dd ) * de_dx(k+1,j+1,i+1) & |
|---|
| 431 | ) / ( 3.0_wp * gg ) |
|---|
| 432 | de_dx_int(n) = de_dx_int_l + ( zv(n) - zu(k) ) / dz * & |
|---|
| 433 | ( de_dx_int_u - de_dx_int_l ) |
|---|
| 434 | ENDIF |
|---|
| 435 | ! |
|---|
| 436 | !-- Interpolate the TKE gradient along y |
|---|
| 437 | de_dy_int_l = ( ( gg - aa ) * de_dy(k,j,i) + & |
|---|
| 438 | ( gg - bb ) * de_dy(k,j,i+1) + & |
|---|
| 439 | ( gg - cc ) * de_dy(k,j+1,i) + & |
|---|
| 440 | ( gg - dd ) * de_dy(k,j+1,i+1) & |
|---|
| 441 | ) / ( 3.0_wp * gg ) |
|---|
| 442 | IF ( ( k+1 == nzt+1 ) .OR. ( k == nzb ) ) THEN |
|---|
| 443 | de_dy_int(n) = de_dy_int_l |
|---|
| 444 | ELSE |
|---|
| 445 | de_dy_int_u = ( ( gg - aa ) * de_dy(k+1,j,i) + & |
|---|
| 446 | ( gg - bb ) * de_dy(k+1,j,i+1) + & |
|---|
| 447 | ( gg - cc ) * de_dy(k+1,j+1,i) + & |
|---|
| 448 | ( gg - dd ) * de_dy(k+1,j+1,i+1) & |
|---|
| 449 | ) / ( 3.0_wp * gg ) |
|---|
| 450 | de_dy_int(n) = de_dy_int_l + ( zv(n) - zu(k) ) / dz * & |
|---|
| 451 | ( de_dy_int_u - de_dy_int_l ) |
|---|
| 452 | ENDIF |
|---|
| 453 | |
|---|
| 454 | ! |
|---|
| 455 | !-- Interpolate the TKE gradient along z |
|---|
| 456 | IF ( zv(n) < 0.5_wp * dz ) THEN |
|---|
| 457 | de_dz_int(n) = 0.0_wp |
|---|
| 458 | ELSE |
|---|
| 459 | de_dz_int_l = ( ( gg - aa ) * de_dz(k,j,i) + & |
|---|
| 460 | ( gg - bb ) * de_dz(k,j,i+1) + & |
|---|
| 461 | ( gg - cc ) * de_dz(k,j+1,i) + & |
|---|
| 462 | ( gg - dd ) * de_dz(k,j+1,i+1) & |
|---|
| 463 | ) / ( 3.0_wp * gg ) |
|---|
| 464 | |
|---|
| 465 | IF ( ( k+1 == nzt+1 ) .OR. ( k == nzb ) ) THEN |
|---|
| 466 | de_dz_int(n) = de_dz_int_l |
|---|
| 467 | ELSE |
|---|
| 468 | de_dz_int_u = ( ( gg - aa ) * de_dz(k+1,j,i) + & |
|---|
| 469 | ( gg - bb ) * de_dz(k+1,j,i+1) + & |
|---|
| 470 | ( gg - cc ) * de_dz(k+1,j+1,i) + & |
|---|
| 471 | ( gg - dd ) * de_dz(k+1,j+1,i+1) & |
|---|
| 472 | ) / ( 3.0_wp * gg ) |
|---|
| 473 | de_dz_int(n) = de_dz_int_l + ( zv(n) - zu(k) ) / dz * & |
|---|
| 474 | ( de_dz_int_u - de_dz_int_l ) |
|---|
| 475 | ENDIF |
|---|
| 476 | ENDIF |
|---|
| 477 | |
|---|
| 478 | ! |
|---|
| 479 | !-- Interpolate the dissipation of TKE |
|---|
| 480 | diss_int_l = ( ( gg - aa ) * diss(k,j,i) + & |
|---|
| 481 | ( gg - bb ) * diss(k,j,i+1) + & |
|---|
| 482 | ( gg - cc ) * diss(k,j+1,i) + & |
|---|
| 483 | ( gg - dd ) * diss(k,j+1,i+1) & |
|---|
| 484 | ) / ( 3.0_wp * gg ) |
|---|
| 485 | |
|---|
| 486 | IF ( k == nzt ) THEN |
|---|
| 487 | diss_int(n) = diss_int_l |
|---|
| 488 | ELSE |
|---|
| 489 | diss_int_u = ( ( gg - aa ) * diss(k+1,j,i) + & |
|---|
| 490 | ( gg - bb ) * diss(k+1,j,i+1) + & |
|---|
| 491 | ( gg - cc ) * diss(k+1,j+1,i) + & |
|---|
| 492 | ( gg - dd ) * diss(k+1,j+1,i+1) & |
|---|
| 493 | ) / ( 3.0_wp * gg ) |
|---|
| 494 | diss_int(n) = diss_int_l + ( zv(n) - zu(k) ) / dz * & |
|---|
| 495 | ( diss_int_u - diss_int_l ) |
|---|
| 496 | ENDIF |
|---|
| 497 | |
|---|
| 498 | ENDDO |
|---|
| 499 | ENDDO |
|---|
| 500 | |
|---|
| 501 | ELSE ! non-flat topography, e.g., buildings |
|---|
| 502 | |
|---|
| 503 | DO n = 1, number_of_particles |
|---|
| 504 | |
|---|
| 505 | i = particles(n)%x * ddx |
|---|
| 506 | j = particles(n)%y * ddy |
|---|
| 507 | k = ( zv(n) + 0.5_wp * dz * atmos_ocean_sign ) / dz & |
|---|
| 508 | + offset_ocean_nzt ! only exact if eq.dist |
|---|
| 509 | ! |
|---|
| 510 | !-- In case that there are buildings it has to be determined |
|---|
| 511 | !-- how many of the gridpoints defining the particle box are |
|---|
| 512 | !-- situated within a building |
|---|
| 513 | !-- gp_outside_of_building(1): i,j,k |
|---|
| 514 | !-- gp_outside_of_building(2): i,j+1,k |
|---|
| 515 | !-- gp_outside_of_building(3): i,j,k+1 |
|---|
| 516 | !-- gp_outside_of_building(4): i,j+1,k+1 |
|---|
| 517 | !-- gp_outside_of_building(5): i+1,j,k |
|---|
| 518 | !-- gp_outside_of_building(6): i+1,j+1,k |
|---|
| 519 | !-- gp_outside_of_building(7): i+1,j,k+1 |
|---|
| 520 | !-- gp_outside_of_building(8): i+1,j+1,k+1 |
|---|
| 521 | |
|---|
| 522 | gp_outside_of_building = 0 |
|---|
| 523 | location = 0.0_wp |
|---|
| 524 | num_gp = 0 |
|---|
| 525 | |
|---|
| 526 | IF ( k > nzb_s_inner(j,i) .OR. nzb_s_inner(j,i) == 0 ) THEN |
|---|
| 527 | num_gp = num_gp + 1 |
|---|
| 528 | gp_outside_of_building(1) = 1 |
|---|
| 529 | location(num_gp,1) = i * dx |
|---|
| 530 | location(num_gp,2) = j * dy |
|---|
| 531 | location(num_gp,3) = k * dz - 0.5_wp * dz |
|---|
| 532 | ei(num_gp) = e(k,j,i) |
|---|
| 533 | dissi(num_gp) = diss(k,j,i) |
|---|
| 534 | de_dxi(num_gp) = de_dx(k,j,i) |
|---|
| 535 | de_dyi(num_gp) = de_dy(k,j,i) |
|---|
| 536 | de_dzi(num_gp) = de_dz(k,j,i) |
|---|
| 537 | ENDIF |
|---|
| 538 | |
|---|
| 539 | IF ( k > nzb_s_inner(j+1,i) .OR. nzb_s_inner(j+1,i) == 0 ) & |
|---|
| 540 | THEN |
|---|
| 541 | num_gp = num_gp + 1 |
|---|
| 542 | gp_outside_of_building(2) = 1 |
|---|
| 543 | location(num_gp,1) = i * dx |
|---|
| 544 | location(num_gp,2) = (j+1) * dy |
|---|
| 545 | location(num_gp,3) = k * dz - 0.5_wp * dz |
|---|
| 546 | ei(num_gp) = e(k,j+1,i) |
|---|
| 547 | dissi(num_gp) = diss(k,j+1,i) |
|---|
| 548 | de_dxi(num_gp) = de_dx(k,j+1,i) |
|---|
| 549 | de_dyi(num_gp) = de_dy(k,j+1,i) |
|---|
| 550 | de_dzi(num_gp) = de_dz(k,j+1,i) |
|---|
| 551 | ENDIF |
|---|
| 552 | |
|---|
| 553 | IF ( k+1 > nzb_s_inner(j,i) .OR. nzb_s_inner(j,i) == 0 ) THEN |
|---|
| 554 | num_gp = num_gp + 1 |
|---|
| 555 | gp_outside_of_building(3) = 1 |
|---|
| 556 | location(num_gp,1) = i * dx |
|---|
| 557 | location(num_gp,2) = j * dy |
|---|
| 558 | location(num_gp,3) = (k+1) * dz - 0.5_wp * dz |
|---|
| 559 | ei(num_gp) = e(k+1,j,i) |
|---|
| 560 | dissi(num_gp) = diss(k+1,j,i) |
|---|
| 561 | de_dxi(num_gp) = de_dx(k+1,j,i) |
|---|
| 562 | de_dyi(num_gp) = de_dy(k+1,j,i) |
|---|
| 563 | de_dzi(num_gp) = de_dz(k+1,j,i) |
|---|
| 564 | ENDIF |
|---|
| 565 | |
|---|
| 566 | IF ( k+1 > nzb_s_inner(j+1,i) .OR. nzb_s_inner(j+1,i) == 0 ) & |
|---|
| 567 | THEN |
|---|
| 568 | num_gp = num_gp + 1 |
|---|
| 569 | gp_outside_of_building(4) = 1 |
|---|
| 570 | location(num_gp,1) = i * dx |
|---|
| 571 | location(num_gp,2) = (j+1) * dy |
|---|
| 572 | location(num_gp,3) = (k+1) * dz - 0.5_wp * dz |
|---|
| 573 | ei(num_gp) = e(k+1,j+1,i) |
|---|
| 574 | dissi(num_gp) = diss(k+1,j+1,i) |
|---|
| 575 | de_dxi(num_gp) = de_dx(k+1,j+1,i) |
|---|
| 576 | de_dyi(num_gp) = de_dy(k+1,j+1,i) |
|---|
| 577 | de_dzi(num_gp) = de_dz(k+1,j+1,i) |
|---|
| 578 | ENDIF |
|---|
| 579 | |
|---|
| 580 | IF ( k > nzb_s_inner(j,i+1) .OR. nzb_s_inner(j,i+1) == 0 ) & |
|---|
| 581 | THEN |
|---|
| 582 | num_gp = num_gp + 1 |
|---|
| 583 | gp_outside_of_building(5) = 1 |
|---|
| 584 | location(num_gp,1) = (i+1) * dx |
|---|
| 585 | location(num_gp,2) = j * dy |
|---|
| 586 | location(num_gp,3) = k * dz - 0.5_wp * dz |
|---|
| 587 | ei(num_gp) = e(k,j,i+1) |
|---|
| 588 | dissi(num_gp) = diss(k,j,i+1) |
|---|
| 589 | de_dxi(num_gp) = de_dx(k,j,i+1) |
|---|
| 590 | de_dyi(num_gp) = de_dy(k,j,i+1) |
|---|
| 591 | de_dzi(num_gp) = de_dz(k,j,i+1) |
|---|
| 592 | ENDIF |
|---|
| 593 | |
|---|
| 594 | IF ( k > nzb_s_inner(j+1,i+1) .OR. nzb_s_inner(j+1,i+1) == 0 ) & |
|---|
| 595 | THEN |
|---|
| 596 | num_gp = num_gp + 1 |
|---|
| 597 | gp_outside_of_building(6) = 1 |
|---|
| 598 | location(num_gp,1) = (i+1) * dx |
|---|
| 599 | location(num_gp,2) = (j+1) * dy |
|---|
| 600 | location(num_gp,3) = k * dz - 0.5_wp * dz |
|---|
| 601 | ei(num_gp) = e(k,j+1,i+1) |
|---|
| 602 | dissi(num_gp) = diss(k,j+1,i+1) |
|---|
| 603 | de_dxi(num_gp) = de_dx(k,j+1,i+1) |
|---|
| 604 | de_dyi(num_gp) = de_dy(k,j+1,i+1) |
|---|
| 605 | de_dzi(num_gp) = de_dz(k,j+1,i+1) |
|---|
| 606 | ENDIF |
|---|
| 607 | |
|---|
| 608 | IF ( k+1 > nzb_s_inner(j,i+1) .OR. nzb_s_inner(j,i+1) == 0 ) & |
|---|
| 609 | THEN |
|---|
| 610 | num_gp = num_gp + 1 |
|---|
| 611 | gp_outside_of_building(7) = 1 |
|---|
| 612 | location(num_gp,1) = (i+1) * dx |
|---|
| 613 | location(num_gp,2) = j * dy |
|---|
| 614 | location(num_gp,3) = (k+1) * dz - 0.5_wp * dz |
|---|
| 615 | ei(num_gp) = e(k+1,j,i+1) |
|---|
| 616 | dissi(num_gp) = diss(k+1,j,i+1) |
|---|
| 617 | de_dxi(num_gp) = de_dx(k+1,j,i+1) |
|---|
| 618 | de_dyi(num_gp) = de_dy(k+1,j,i+1) |
|---|
| 619 | de_dzi(num_gp) = de_dz(k+1,j,i+1) |
|---|
| 620 | ENDIF |
|---|
| 621 | |
|---|
| 622 | IF ( k+1 > nzb_s_inner(j+1,i+1) .OR. nzb_s_inner(j+1,i+1) == 0)& |
|---|
| 623 | THEN |
|---|
| 624 | num_gp = num_gp + 1 |
|---|
| 625 | gp_outside_of_building(8) = 1 |
|---|
| 626 | location(num_gp,1) = (i+1) * dx |
|---|
| 627 | location(num_gp,2) = (j+1) * dy |
|---|
| 628 | location(num_gp,3) = (k+1) * dz - 0.5_wp * dz |
|---|
| 629 | ei(num_gp) = e(k+1,j+1,i+1) |
|---|
| 630 | dissi(num_gp) = diss(k+1,j+1,i+1) |
|---|
| 631 | de_dxi(num_gp) = de_dx(k+1,j+1,i+1) |
|---|
| 632 | de_dyi(num_gp) = de_dy(k+1,j+1,i+1) |
|---|
| 633 | de_dzi(num_gp) = de_dz(k+1,j+1,i+1) |
|---|
| 634 | ENDIF |
|---|
| 635 | |
|---|
| 636 | ! |
|---|
| 637 | !-- If all gridpoints are situated outside of a building, then the |
|---|
| 638 | !-- ordinary interpolation scheme can be used. |
|---|
| 639 | IF ( num_gp == 8 ) THEN |
|---|
| 640 | |
|---|
| 641 | x = particles(n)%x - i * dx |
|---|
| 642 | y = particles(n)%y - j * dy |
|---|
| 643 | aa = x**2 + y**2 |
|---|
| 644 | bb = ( dx - x )**2 + y**2 |
|---|
| 645 | cc = x**2 + ( dy - y )**2 |
|---|
| 646 | dd = ( dx - x )**2 + ( dy - y )**2 |
|---|
| 647 | gg = aa + bb + cc + dd |
|---|
| 648 | |
|---|
| 649 | e_int_l = ( ( gg - aa ) * e(k,j,i) + ( gg - bb ) * e(k,j,i+1) & |
|---|
| 650 | + ( gg - cc ) * e(k,j+1,i) + ( gg - dd ) * e(k,j+1,i+1) & |
|---|
| 651 | ) / ( 3.0_wp * gg ) |
|---|
| 652 | |
|---|
| 653 | IF ( k == nzt ) THEN |
|---|
| 654 | e_int(n) = e_int_l |
|---|
| 655 | ELSE |
|---|
| 656 | e_int_u = ( ( gg - aa ) * e(k+1,j,i) + & |
|---|
| 657 | ( gg - bb ) * e(k+1,j,i+1) + & |
|---|
| 658 | ( gg - cc ) * e(k+1,j+1,i) + & |
|---|
| 659 | ( gg - dd ) * e(k+1,j+1,i+1) & |
|---|
| 660 | ) / ( 3.0_wp * gg ) |
|---|
| 661 | e_int(n) = e_int_l + ( zv(n) - zu(k) ) / dz * & |
|---|
| 662 | ( e_int_u - e_int_l ) |
|---|
| 663 | ENDIF |
|---|
| 664 | ! |
|---|
| 665 | !-- Needed to avoid NaN particle velocities |
|---|
| 666 | IF ( e_int(n) == 0.0_wp ) THEN |
|---|
| 667 | e_int(n) = 1.0E-20_wp |
|---|
| 668 | ENDIF |
|---|
| 669 | ! |
|---|
| 670 | !-- Interpolate the TKE gradient along x (adopt incides i,j,k |
|---|
| 671 | !-- and all position variables from above (TKE)) |
|---|
| 672 | de_dx_int_l = ( ( gg - aa ) * de_dx(k,j,i) + & |
|---|
| 673 | ( gg - bb ) * de_dx(k,j,i+1) + & |
|---|
| 674 | ( gg - cc ) * de_dx(k,j+1,i) + & |
|---|
| 675 | ( gg - dd ) * de_dx(k,j+1,i+1) & |
|---|
| 676 | ) / ( 3.0_wp * gg ) |
|---|
| 677 | |
|---|
| 678 | IF ( ( k == nzt ) .OR. ( k == nzb ) ) THEN |
|---|
| 679 | de_dx_int(n) = de_dx_int_l |
|---|
| 680 | ELSE |
|---|
| 681 | de_dx_int_u = ( ( gg - aa ) * de_dx(k+1,j,i) + & |
|---|
| 682 | ( gg - bb ) * de_dx(k+1,j,i+1) + & |
|---|
| 683 | ( gg - cc ) * de_dx(k+1,j+1,i) + & |
|---|
| 684 | ( gg - dd ) * de_dx(k+1,j+1,i+1) & |
|---|
| 685 | ) / ( 3.0_wp * gg ) |
|---|
| 686 | de_dx_int(n) = de_dx_int_l + ( zv(n) - zu(k) ) / & |
|---|
| 687 | dz * ( de_dx_int_u - de_dx_int_l ) |
|---|
| 688 | ENDIF |
|---|
| 689 | |
|---|
| 690 | ! |
|---|
| 691 | !-- Interpolate the TKE gradient along y |
|---|
| 692 | de_dy_int_l = ( ( gg - aa ) * de_dy(k,j,i) + & |
|---|
| 693 | ( gg - bb ) * de_dy(k,j,i+1) + & |
|---|
| 694 | ( gg - cc ) * de_dy(k,j+1,i) + & |
|---|
| 695 | ( gg - dd ) * de_dy(k,j+1,i+1) & |
|---|
| 696 | ) / ( 3.0_wp * gg ) |
|---|
| 697 | IF ( ( k+1 == nzt+1 ) .OR. ( k == nzb ) ) THEN |
|---|
| 698 | de_dy_int(n) = de_dy_int_l |
|---|
| 699 | ELSE |
|---|
| 700 | de_dy_int_u = ( ( gg - aa ) * de_dy(k+1,j,i) + & |
|---|
| 701 | ( gg - bb ) * de_dy(k+1,j,i+1) + & |
|---|
| 702 | ( gg - cc ) * de_dy(k+1,j+1,i) + & |
|---|
| 703 | ( gg - dd ) * de_dy(k+1,j+1,i+1) & |
|---|
| 704 | ) / ( 3.0_wp * gg ) |
|---|
| 705 | de_dy_int(n) = de_dy_int_l + ( zv(n) - zu(k) ) / & |
|---|
| 706 | dz * ( de_dy_int_u - de_dy_int_l ) |
|---|
| 707 | ENDIF |
|---|
| 708 | |
|---|
| 709 | ! |
|---|
| 710 | !-- Interpolate the TKE gradient along z |
|---|
| 711 | IF ( zv(n) < 0.5_wp * dz ) THEN |
|---|
| 712 | de_dz_int(n) = 0.0_wp |
|---|
| 713 | ELSE |
|---|
| 714 | de_dz_int_l = ( ( gg - aa ) * de_dz(k,j,i) + & |
|---|
| 715 | ( gg - bb ) * de_dz(k,j,i+1) + & |
|---|
| 716 | ( gg - cc ) * de_dz(k,j+1,i) + & |
|---|
| 717 | ( gg - dd ) * de_dz(k,j+1,i+1) & |
|---|
| 718 | ) / ( 3.0_wp * gg ) |
|---|
| 719 | |
|---|
| 720 | IF ( ( k+1 == nzt+1 ) .OR. ( k == nzb ) ) THEN |
|---|
| 721 | de_dz_int(n) = de_dz_int_l |
|---|
| 722 | ELSE |
|---|
| 723 | de_dz_int_u = ( ( gg - aa ) * de_dz(k+1,j,i) + & |
|---|
| 724 | ( gg - bb ) * de_dz(k+1,j,i+1) + & |
|---|
| 725 | ( gg - cc ) * de_dz(k+1,j+1,i) + & |
|---|
| 726 | ( gg - dd ) * de_dz(k+1,j+1,i+1) & |
|---|
| 727 | ) / ( 3.0_wp * gg ) |
|---|
| 728 | de_dz_int(n) = de_dz_int_l + ( zv(n) - zu(k) ) /& |
|---|
| 729 | dz * ( de_dz_int_u - de_dz_int_l ) |
|---|
| 730 | ENDIF |
|---|
| 731 | ENDIF |
|---|
| 732 | |
|---|
| 733 | ! |
|---|
| 734 | !-- Interpolate the dissipation of TKE |
|---|
| 735 | diss_int_l = ( ( gg - aa ) * diss(k,j,i) + & |
|---|
| 736 | ( gg - bb ) * diss(k,j,i+1) + & |
|---|
| 737 | ( gg - cc ) * diss(k,j+1,i) + & |
|---|
| 738 | ( gg - dd ) * diss(k,j+1,i+1) & |
|---|
| 739 | ) / ( 3.0_wp * gg ) |
|---|
| 740 | |
|---|
| 741 | IF ( k == nzt ) THEN |
|---|
| 742 | diss_int(n) = diss_int_l |
|---|
| 743 | ELSE |
|---|
| 744 | diss_int_u = ( ( gg - aa ) * diss(k+1,j,i) + & |
|---|
| 745 | ( gg - bb ) * diss(k+1,j,i+1) + & |
|---|
| 746 | ( gg - cc ) * diss(k+1,j+1,i) + & |
|---|
| 747 | ( gg - dd ) * diss(k+1,j+1,i+1) & |
|---|
| 748 | ) / ( 3.0_wp * gg ) |
|---|
| 749 | diss_int(n) = diss_int_l + ( zv(n) - zu(k) ) / dz *& |
|---|
| 750 | ( diss_int_u - diss_int_l ) |
|---|
| 751 | ENDIF |
|---|
| 752 | |
|---|
| 753 | ELSE |
|---|
| 754 | |
|---|
| 755 | ! |
|---|
| 756 | !-- If wall between gridpoint 1 and gridpoint 5, then |
|---|
| 757 | !-- Neumann boundary condition has to be applied |
|---|
| 758 | IF ( gp_outside_of_building(1) == 1 .AND. & |
|---|
| 759 | gp_outside_of_building(5) == 0 ) THEN |
|---|
| 760 | num_gp = num_gp + 1 |
|---|
| 761 | location(num_gp,1) = i * dx + 0.5_wp * dx |
|---|
| 762 | location(num_gp,2) = j * dy |
|---|
| 763 | location(num_gp,3) = k * dz - 0.5_wp * dz |
|---|
| 764 | ei(num_gp) = e(k,j,i) |
|---|
| 765 | dissi(num_gp) = diss(k,j,i) |
|---|
| 766 | de_dxi(num_gp) = 0.0_wp |
|---|
| 767 | de_dyi(num_gp) = de_dy(k,j,i) |
|---|
| 768 | de_dzi(num_gp) = de_dz(k,j,i) |
|---|
| 769 | ENDIF |
|---|
| 770 | |
|---|
| 771 | IF ( gp_outside_of_building(5) == 1 .AND. & |
|---|
| 772 | gp_outside_of_building(1) == 0 ) THEN |
|---|
| 773 | num_gp = num_gp + 1 |
|---|
| 774 | location(num_gp,1) = i * dx + 0.5_wp * dx |
|---|
| 775 | location(num_gp,2) = j * dy |
|---|
| 776 | location(num_gp,3) = k * dz - 0.5_wp * dz |
|---|
| 777 | ei(num_gp) = e(k,j,i+1) |
|---|
| 778 | dissi(num_gp) = diss(k,j,i+1) |
|---|
| 779 | de_dxi(num_gp) = 0.0_wp |
|---|
| 780 | de_dyi(num_gp) = de_dy(k,j,i+1) |
|---|
| 781 | de_dzi(num_gp) = de_dz(k,j,i+1) |
|---|
| 782 | ENDIF |
|---|
| 783 | |
|---|
| 784 | ! |
|---|
| 785 | !-- If wall between gridpoint 5 and gridpoint 6, then |
|---|
| 786 | !-- then Neumann boundary condition has to be applied |
|---|
| 787 | IF ( gp_outside_of_building(5) == 1 .AND. & |
|---|
| 788 | gp_outside_of_building(6) == 0 ) THEN |
|---|
| 789 | num_gp = num_gp + 1 |
|---|
| 790 | location(num_gp,1) = (i+1) * dx |
|---|
| 791 | location(num_gp,2) = j * dy + 0.5_wp * dy |
|---|
| 792 | location(num_gp,3) = k * dz - 0.5_wp * dz |
|---|
| 793 | ei(num_gp) = e(k,j,i+1) |
|---|
| 794 | dissi(num_gp) = diss(k,j,i+1) |
|---|
| 795 | de_dxi(num_gp) = de_dx(k,j,i+1) |
|---|
| 796 | de_dyi(num_gp) = 0.0_wp |
|---|
| 797 | de_dzi(num_gp) = de_dz(k,j,i+1) |
|---|
| 798 | ENDIF |
|---|
| 799 | |
|---|
| 800 | IF ( gp_outside_of_building(6) == 1 .AND. & |
|---|
| 801 | gp_outside_of_building(5) == 0 ) THEN |
|---|
| 802 | num_gp = num_gp + 1 |
|---|
| 803 | location(num_gp,1) = (i+1) * dx |
|---|
| 804 | location(num_gp,2) = j * dy + 0.5_wp * dy |
|---|
| 805 | location(num_gp,3) = k * dz - 0.5_wp * dz |
|---|
| 806 | ei(num_gp) = e(k,j+1,i+1) |
|---|
| 807 | dissi(num_gp) = diss(k,j+1,i+1) |
|---|
| 808 | de_dxi(num_gp) = de_dx(k,j+1,i+1) |
|---|
| 809 | de_dyi(num_gp) = 0.0_wp |
|---|
| 810 | de_dzi(num_gp) = de_dz(k,j+1,i+1) |
|---|
| 811 | ENDIF |
|---|
| 812 | |
|---|
| 813 | ! |
|---|
| 814 | !-- If wall between gridpoint 2 and gridpoint 6, then |
|---|
| 815 | !-- Neumann boundary condition has to be applied |
|---|
| 816 | IF ( gp_outside_of_building(2) == 1 .AND. & |
|---|
| 817 | gp_outside_of_building(6) == 0 ) THEN |
|---|
| 818 | num_gp = num_gp + 1 |
|---|
| 819 | location(num_gp,1) = i * dx + 0.5_wp * dx |
|---|
| 820 | location(num_gp,2) = (j+1) * dy |
|---|
| 821 | location(num_gp,3) = k * dz - 0.5_wp * dz |
|---|
| 822 | ei(num_gp) = e(k,j+1,i) |
|---|
| 823 | dissi(num_gp) = diss(k,j+1,i) |
|---|
| 824 | de_dxi(num_gp) = 0.0_wp |
|---|
| 825 | de_dyi(num_gp) = de_dy(k,j+1,i) |
|---|
| 826 | de_dzi(num_gp) = de_dz(k,j+1,i) |
|---|
| 827 | ENDIF |
|---|
| 828 | |
|---|
| 829 | IF ( gp_outside_of_building(6) == 1 .AND. & |
|---|
| 830 | gp_outside_of_building(2) == 0 ) THEN |
|---|
| 831 | num_gp = num_gp + 1 |
|---|
| 832 | location(num_gp,1) = i * dx + 0.5_wp * dx |
|---|
| 833 | location(num_gp,2) = (j+1) * dy |
|---|
| 834 | location(num_gp,3) = k * dz - 0.5_wp * dz |
|---|
| 835 | ei(num_gp) = e(k,j+1,i+1) |
|---|
| 836 | dissi(num_gp) = diss(k,j+1,i+1) |
|---|
| 837 | de_dxi(num_gp) = 0.0_wp |
|---|
| 838 | de_dyi(num_gp) = de_dy(k,j+1,i+1) |
|---|
| 839 | de_dzi(num_gp) = de_dz(k,j+1,i+1) |
|---|
| 840 | ENDIF |
|---|
| 841 | |
|---|
| 842 | ! |
|---|
| 843 | !-- If wall between gridpoint 1 and gridpoint 2, then |
|---|
| 844 | !-- Neumann boundary condition has to be applied |
|---|
| 845 | IF ( gp_outside_of_building(1) == 1 .AND. & |
|---|
| 846 | gp_outside_of_building(2) == 0 ) THEN |
|---|
| 847 | num_gp = num_gp + 1 |
|---|
| 848 | location(num_gp,1) = i * dx |
|---|
| 849 | location(num_gp,2) = j * dy + 0.5_wp * dy |
|---|
| 850 | location(num_gp,3) = k * dz - 0.5_wp * dz |
|---|
| 851 | ei(num_gp) = e(k,j,i) |
|---|
| 852 | dissi(num_gp) = diss(k,j,i) |
|---|
| 853 | de_dxi(num_gp) = de_dx(k,j,i) |
|---|
| 854 | de_dyi(num_gp) = 0.0_wp |
|---|
| 855 | de_dzi(num_gp) = de_dz(k,j,i) |
|---|
| 856 | ENDIF |
|---|
| 857 | |
|---|
| 858 | IF ( gp_outside_of_building(2) == 1 .AND. & |
|---|
| 859 | gp_outside_of_building(1) == 0 ) THEN |
|---|
| 860 | num_gp = num_gp + 1 |
|---|
| 861 | location(num_gp,1) = i * dx |
|---|
| 862 | location(num_gp,2) = j * dy + 0.5_wp * dy |
|---|
| 863 | location(num_gp,3) = k * dz - 0.5_wp * dz |
|---|
| 864 | ei(num_gp) = e(k,j+1,i) |
|---|
| 865 | dissi(num_gp) = diss(k,j+1,i) |
|---|
| 866 | de_dxi(num_gp) = de_dx(k,j+1,i) |
|---|
| 867 | de_dyi(num_gp) = 0.0_wp |
|---|
| 868 | de_dzi(num_gp) = de_dz(k,j+1,i) |
|---|
| 869 | ENDIF |
|---|
| 870 | |
|---|
| 871 | ! |
|---|
| 872 | !-- If wall between gridpoint 3 and gridpoint 7, then |
|---|
| 873 | !-- Neumann boundary condition has to be applied |
|---|
| 874 | IF ( gp_outside_of_building(3) == 1 .AND. & |
|---|
| 875 | gp_outside_of_building(7) == 0 ) THEN |
|---|
| 876 | num_gp = num_gp + 1 |
|---|
| 877 | location(num_gp,1) = i * dx + 0.5_wp * dx |
|---|
| 878 | location(num_gp,2) = j * dy |
|---|
| 879 | location(num_gp,3) = k * dz + 0.5_wp * dz |
|---|
| 880 | ei(num_gp) = e(k+1,j,i) |
|---|
| 881 | dissi(num_gp) = diss(k+1,j,i) |
|---|
| 882 | de_dxi(num_gp) = 0.0_wp |
|---|
| 883 | de_dyi(num_gp) = de_dy(k+1,j,i) |
|---|
| 884 | de_dzi(num_gp) = de_dz(k+1,j,i) |
|---|
| 885 | ENDIF |
|---|
| 886 | |
|---|
| 887 | IF ( gp_outside_of_building(7) == 1 .AND. & |
|---|
| 888 | gp_outside_of_building(3) == 0 ) THEN |
|---|
| 889 | num_gp = num_gp + 1 |
|---|
| 890 | location(num_gp,1) = i * dx + 0.5_wp * dx |
|---|
| 891 | location(num_gp,2) = j * dy |
|---|
| 892 | location(num_gp,3) = k * dz + 0.5_wp * dz |
|---|
| 893 | ei(num_gp) = e(k+1,j,i+1) |
|---|
| 894 | dissi(num_gp) = diss(k+1,j,i+1) |
|---|
| 895 | de_dxi(num_gp) = 0.0_wp |
|---|
| 896 | de_dyi(num_gp) = de_dy(k+1,j,i+1) |
|---|
| 897 | de_dzi(num_gp) = de_dz(k+1,j,i+1) |
|---|
| 898 | ENDIF |
|---|
| 899 | |
|---|
| 900 | ! |
|---|
| 901 | !-- If wall between gridpoint 7 and gridpoint 8, then |
|---|
| 902 | !-- Neumann boundary condition has to be applied |
|---|
| 903 | IF ( gp_outside_of_building(7) == 1 .AND. & |
|---|
| 904 | gp_outside_of_building(8) == 0 ) THEN |
|---|
| 905 | num_gp = num_gp + 1 |
|---|
| 906 | location(num_gp,1) = (i+1) * dx |
|---|
| 907 | location(num_gp,2) = j * dy + 0.5_wp * dy |
|---|
| 908 | location(num_gp,3) = k * dz + 0.5_wp * dz |
|---|
| 909 | ei(num_gp) = e(k+1,j,i+1) |
|---|
| 910 | dissi(num_gp) = diss(k+1,j,i+1) |
|---|
| 911 | de_dxi(num_gp) = de_dx(k+1,j,i+1) |
|---|
| 912 | de_dyi(num_gp) = 0.0_wp |
|---|
| 913 | de_dzi(num_gp) = de_dz(k+1,j,i+1) |
|---|
| 914 | ENDIF |
|---|
| 915 | |
|---|
| 916 | IF ( gp_outside_of_building(8) == 1 .AND. & |
|---|
| 917 | gp_outside_of_building(7) == 0 ) THEN |
|---|
| 918 | num_gp = num_gp + 1 |
|---|
| 919 | location(num_gp,1) = (i+1) * dx |
|---|
| 920 | location(num_gp,2) = j * dy + 0.5_wp * dy |
|---|
| 921 | location(num_gp,3) = k * dz + 0.5_wp * dz |
|---|
| 922 | ei(num_gp) = e(k+1,j+1,i+1) |
|---|
| 923 | dissi(num_gp) = diss(k+1,j+1,i+1) |
|---|
| 924 | de_dxi(num_gp) = de_dx(k+1,j+1,i+1) |
|---|
| 925 | de_dyi(num_gp) = 0.0_wp |
|---|
| 926 | de_dzi(num_gp) = de_dz(k+1,j+1,i+1) |
|---|
| 927 | ENDIF |
|---|
| 928 | |
|---|
| 929 | ! |
|---|
| 930 | !-- If wall between gridpoint 4 and gridpoint 8, then |
|---|
| 931 | !-- Neumann boundary condition has to be applied |
|---|
| 932 | IF ( gp_outside_of_building(4) == 1 .AND. & |
|---|
| 933 | gp_outside_of_building(8) == 0 ) THEN |
|---|
| 934 | num_gp = num_gp + 1 |
|---|
| 935 | location(num_gp,1) = i * dx + 0.5_wp * dx |
|---|
| 936 | location(num_gp,2) = (j+1) * dy |
|---|
| 937 | location(num_gp,3) = k * dz + 0.5_wp * dz |
|---|
| 938 | ei(num_gp) = e(k+1,j+1,i) |
|---|
| 939 | dissi(num_gp) = diss(k+1,j+1,i) |
|---|
| 940 | de_dxi(num_gp) = 0.0_wp |
|---|
| 941 | de_dyi(num_gp) = de_dy(k+1,j+1,i) |
|---|
| 942 | de_dzi(num_gp) = de_dz(k+1,j+1,i) |
|---|
| 943 | ENDIF |
|---|
| 944 | |
|---|
| 945 | IF ( gp_outside_of_building(8) == 1 .AND. & |
|---|
| 946 | gp_outside_of_building(4) == 0 ) THEN |
|---|
| 947 | num_gp = num_gp + 1 |
|---|
| 948 | location(num_gp,1) = i * dx + 0.5_wp * dx |
|---|
| 949 | location(num_gp,2) = (j+1) * dy |
|---|
| 950 | location(num_gp,3) = k * dz + 0.5_wp * dz |
|---|
| 951 | ei(num_gp) = e(k+1,j+1,i+1) |
|---|
| 952 | dissi(num_gp) = diss(k+1,j+1,i+1) |
|---|
| 953 | de_dxi(num_gp) = 0.0_wp |
|---|
| 954 | de_dyi(num_gp) = de_dy(k+1,j+1,i+1) |
|---|
| 955 | de_dzi(num_gp) = de_dz(k+1,j+1,i+1) |
|---|
| 956 | ENDIF |
|---|
| 957 | |
|---|
| 958 | ! |
|---|
| 959 | !-- If wall between gridpoint 3 and gridpoint 4, then |
|---|
| 960 | !-- Neumann boundary condition has to be applied |
|---|
| 961 | IF ( gp_outside_of_building(3) == 1 .AND. & |
|---|
| 962 | gp_outside_of_building(4) == 0 ) THEN |
|---|
| 963 | num_gp = num_gp + 1 |
|---|
| 964 | location(num_gp,1) = i * dx |
|---|
| 965 | location(num_gp,2) = j * dy + 0.5_wp * dy |
|---|
| 966 | location(num_gp,3) = k * dz + 0.5_wp * dz |
|---|
| 967 | ei(num_gp) = e(k+1,j,i) |
|---|
| 968 | dissi(num_gp) = diss(k+1,j,i) |
|---|
| 969 | de_dxi(num_gp) = de_dx(k+1,j,i) |
|---|
| 970 | de_dyi(num_gp) = 0.0_wp |
|---|
| 971 | de_dzi(num_gp) = de_dz(k+1,j,i) |
|---|
| 972 | ENDIF |
|---|
| 973 | |
|---|
| 974 | IF ( gp_outside_of_building(4) == 1 .AND. & |
|---|
| 975 | gp_outside_of_building(3) == 0 ) THEN |
|---|
| 976 | num_gp = num_gp + 1 |
|---|
| 977 | location(num_gp,1) = i * dx |
|---|
| 978 | location(num_gp,2) = j * dy + 0.5_wp * dy |
|---|
| 979 | location(num_gp,3) = k * dz + 0.5_wp * dz |
|---|
| 980 | ei(num_gp) = e(k+1,j+1,i) |
|---|
| 981 | dissi(num_gp) = diss(k+1,j+1,i) |
|---|
| 982 | de_dxi(num_gp) = de_dx(k+1,j+1,i) |
|---|
| 983 | de_dyi(num_gp) = 0.0_wp |
|---|
| 984 | de_dzi(num_gp) = de_dz(k+1,j+1,i) |
|---|
| 985 | ENDIF |
|---|
| 986 | |
|---|
| 987 | ! |
|---|
| 988 | !-- If wall between gridpoint 1 and gridpoint 3, then |
|---|
| 989 | !-- Neumann boundary condition has to be applied |
|---|
| 990 | !-- (only one case as only building beneath is possible) |
|---|
| 991 | IF ( gp_outside_of_building(1) == 0 .AND. & |
|---|
| 992 | gp_outside_of_building(3) == 1 ) THEN |
|---|
| 993 | num_gp = num_gp + 1 |
|---|
| 994 | location(num_gp,1) = i * dx |
|---|
| 995 | location(num_gp,2) = j * dy |
|---|
| 996 | location(num_gp,3) = k * dz |
|---|
| 997 | ei(num_gp) = e(k+1,j,i) |
|---|
| 998 | dissi(num_gp) = diss(k+1,j,i) |
|---|
| 999 | de_dxi(num_gp) = de_dx(k+1,j,i) |
|---|
| 1000 | de_dyi(num_gp) = de_dy(k+1,j,i) |
|---|
| 1001 | de_dzi(num_gp) = 0.0_wp |
|---|
| 1002 | ENDIF |
|---|
| 1003 | |
|---|
| 1004 | ! |
|---|
| 1005 | !-- If wall between gridpoint 5 and gridpoint 7, then |
|---|
| 1006 | !-- Neumann boundary condition has to be applied |
|---|
| 1007 | !-- (only one case as only building beneath is possible) |
|---|
| 1008 | IF ( gp_outside_of_building(5) == 0 .AND. & |
|---|
| 1009 | gp_outside_of_building(7) == 1 ) THEN |
|---|
| 1010 | num_gp = num_gp + 1 |
|---|
| 1011 | location(num_gp,1) = (i+1) * dx |
|---|
| 1012 | location(num_gp,2) = j * dy |
|---|
| 1013 | location(num_gp,3) = k * dz |
|---|
| 1014 | ei(num_gp) = e(k+1,j,i+1) |
|---|
| 1015 | dissi(num_gp) = diss(k+1,j,i+1) |
|---|
| 1016 | de_dxi(num_gp) = de_dx(k+1,j,i+1) |
|---|
| 1017 | de_dyi(num_gp) = de_dy(k+1,j,i+1) |
|---|
| 1018 | de_dzi(num_gp) = 0.0_wp |
|---|
| 1019 | ENDIF |
|---|
| 1020 | |
|---|
| 1021 | ! |
|---|
| 1022 | !-- If wall between gridpoint 2 and gridpoint 4, then |
|---|
| 1023 | !-- Neumann boundary condition has to be applied |
|---|
| 1024 | !-- (only one case as only building beneath is possible) |
|---|
| 1025 | IF ( gp_outside_of_building(2) == 0 .AND. & |
|---|
| 1026 | gp_outside_of_building(4) == 1 ) THEN |
|---|
| 1027 | num_gp = num_gp + 1 |
|---|
| 1028 | location(num_gp,1) = i * dx |
|---|
| 1029 | location(num_gp,2) = (j+1) * dy |
|---|
| 1030 | location(num_gp,3) = k * dz |
|---|
| 1031 | ei(num_gp) = e(k+1,j+1,i) |
|---|
| 1032 | dissi(num_gp) = diss(k+1,j+1,i) |
|---|
| 1033 | de_dxi(num_gp) = de_dx(k+1,j+1,i) |
|---|
| 1034 | de_dyi(num_gp) = de_dy(k+1,j+1,i) |
|---|
| 1035 | de_dzi(num_gp) = 0.0_wp |
|---|
| 1036 | ENDIF |
|---|
| 1037 | |
|---|
| 1038 | ! |
|---|
| 1039 | !-- If wall between gridpoint 6 and gridpoint 8, then |
|---|
| 1040 | !-- Neumann boundary condition has to be applied |
|---|
| 1041 | !-- (only one case as only building beneath is possible) |
|---|
| 1042 | IF ( gp_outside_of_building(6) == 0 .AND. & |
|---|
| 1043 | gp_outside_of_building(8) == 1 ) THEN |
|---|
| 1044 | num_gp = num_gp + 1 |
|---|
| 1045 | location(num_gp,1) = (i+1) * dx |
|---|
| 1046 | location(num_gp,2) = (j+1) * dy |
|---|
| 1047 | location(num_gp,3) = k * dz |
|---|
| 1048 | ei(num_gp) = e(k+1,j+1,i+1) |
|---|
| 1049 | dissi(num_gp) = diss(k+1,j+1,i+1) |
|---|
| 1050 | de_dxi(num_gp) = de_dx(k+1,j+1,i+1) |
|---|
| 1051 | de_dyi(num_gp) = de_dy(k+1,j+1,i+1) |
|---|
| 1052 | de_dzi(num_gp) = 0.0_wp |
|---|
| 1053 | ENDIF |
|---|
| 1054 | |
|---|
| 1055 | ! |
|---|
| 1056 | !-- Carry out the interpolation |
|---|
| 1057 | IF ( num_gp == 1 ) THEN |
|---|
| 1058 | ! |
|---|
| 1059 | !-- If only one of the gridpoints is situated outside of the |
|---|
| 1060 | !-- building, it follows that the values at the particle |
|---|
| 1061 | !-- location are the same as the gridpoint values |
|---|
| 1062 | e_int(n) = ei(num_gp) |
|---|
| 1063 | diss_int(n) = dissi(num_gp) |
|---|
| 1064 | de_dx_int(n) = de_dxi(num_gp) |
|---|
| 1065 | de_dy_int(n) = de_dyi(num_gp) |
|---|
| 1066 | de_dz_int(n) = de_dzi(num_gp) |
|---|
| 1067 | ELSE IF ( num_gp > 1 ) THEN |
|---|
| 1068 | |
|---|
| 1069 | d_sum = 0.0_wp |
|---|
| 1070 | ! |
|---|
| 1071 | !-- Evaluation of the distances between the gridpoints |
|---|
| 1072 | !-- contributing to the interpolated values, and the particle |
|---|
| 1073 | !-- location |
|---|
| 1074 | DO agp = 1, num_gp |
|---|
| 1075 | d_gp_pl(agp) = ( particles(n)%x-location(agp,1) )**2 & |
|---|
| 1076 | + ( particles(n)%y-location(agp,2) )**2 & |
|---|
| 1077 | + ( zv(n)-location(agp,3) )**2 |
|---|
| 1078 | d_sum = d_sum + d_gp_pl(agp) |
|---|
| 1079 | ENDDO |
|---|
| 1080 | |
|---|
| 1081 | ! |
|---|
| 1082 | !-- Finally the interpolation can be carried out |
|---|
| 1083 | e_int(n) = 0.0_wp |
|---|
| 1084 | diss_int(n) = 0.0_wp |
|---|
| 1085 | de_dx_int(n) = 0.0_wp |
|---|
| 1086 | de_dy_int(n) = 0.0_wp |
|---|
| 1087 | de_dz_int(n) = 0.0_wp |
|---|
| 1088 | DO agp = 1, num_gp |
|---|
| 1089 | e_int(n) = e_int(n) + ( d_sum - d_gp_pl(agp) ) * & |
|---|
| 1090 | ei(agp) / ( (num_gp-1) * d_sum ) |
|---|
| 1091 | diss_int(n) = diss_int(n) + ( d_sum - d_gp_pl(agp) ) * & |
|---|
| 1092 | dissi(agp) / ( (num_gp-1) * d_sum ) |
|---|
| 1093 | de_dx_int(n) = de_dx_int(n) + ( d_sum - d_gp_pl(agp) ) * & |
|---|
| 1094 | de_dxi(agp) / ( (num_gp-1) * d_sum ) |
|---|
| 1095 | de_dy_int(n) = de_dy_int(n) + ( d_sum - d_gp_pl(agp) ) * & |
|---|
| 1096 | de_dyi(agp) / ( (num_gp-1) * d_sum ) |
|---|
| 1097 | de_dz_int(n) = de_dz_int(n) + ( d_sum - d_gp_pl(agp) ) * & |
|---|
| 1098 | de_dzi(agp) / ( (num_gp-1) * d_sum ) |
|---|
| 1099 | ENDDO |
|---|
| 1100 | |
|---|
| 1101 | ENDIF |
|---|
| 1102 | |
|---|
| 1103 | ENDIF |
|---|
| 1104 | ENDDO |
|---|
| 1105 | ENDIF |
|---|
| 1106 | |
|---|
| 1107 | DO nb = 0,7 |
|---|
| 1108 | i = ip + block_offset(nb)%i_off |
|---|
| 1109 | j = jp + block_offset(nb)%j_off |
|---|
| 1110 | k = kp + block_offset(nb)%k_off |
|---|
| 1111 | |
|---|
| 1112 | DO n = start_index(nb), end_index(nb) |
|---|
| 1113 | ! |
|---|
| 1114 | !-- Vertical interpolation of the horizontally averaged SGS TKE and |
|---|
| 1115 | !-- resolved-scale velocity variances and use the interpolated values |
|---|
| 1116 | !-- to calculate the coefficient fs, which is a measure of the ratio |
|---|
| 1117 | !-- of the subgrid-scale turbulent kinetic energy to the total amount |
|---|
| 1118 | !-- of turbulent kinetic energy. |
|---|
| 1119 | IF ( k == 0 ) THEN |
|---|
| 1120 | e_mean_int = hom(0,1,8,0) |
|---|
| 1121 | ELSE |
|---|
| 1122 | e_mean_int = hom(k,1,8,0) + & |
|---|
| 1123 | ( hom(k+1,1,8,0) - hom(k,1,8,0) ) / & |
|---|
| 1124 | ( zu(k+1) - zu(k) ) * & |
|---|
| 1125 | ( zv(n) - zu(k) ) |
|---|
| 1126 | ENDIF |
|---|
| 1127 | |
|---|
| 1128 | ! kw = particles(n)%z / dz |
|---|
| 1129 | kw = kp-1 ! ok for ocean??? ( + offset_ocean_nzt_m1 ???) |
|---|
| 1130 | |
|---|
| 1131 | IF ( k == 0 ) THEN |
|---|
| 1132 | aa = hom(k+1,1,30,0) * ( zv(n) / & |
|---|
| 1133 | ( 0.5_wp * ( zu(k+1) - zu(k) ) ) ) |
|---|
| 1134 | bb = hom(k+1,1,31,0) * ( zv(n) / & |
|---|
| 1135 | ( 0.5_wp * ( zu(k+1) - zu(k) ) ) ) |
|---|
| 1136 | cc = hom(kw+1,1,32,0) * ( zv(n) / & |
|---|
| 1137 | ( 1.0_wp * ( zw(kw+1) - zw(kw) ) ) ) |
|---|
| 1138 | ELSE |
|---|
| 1139 | aa = hom(k,1,30,0) + ( hom(k+1,1,30,0) - hom(k,1,30,0) ) * & |
|---|
| 1140 | ( ( zv(n) - zu(k) ) / ( zu(k+1) - zu(k) ) ) |
|---|
| 1141 | bb = hom(k,1,31,0) + ( hom(k+1,1,31,0) - hom(k,1,31,0) ) * & |
|---|
| 1142 | ( ( zv(n) - zu(k) ) / ( zu(k+1) - zu(k) ) ) |
|---|
| 1143 | cc = hom(kw,1,32,0) + ( hom(kw+1,1,32,0)-hom(kw,1,32,0) ) * & |
|---|
| 1144 | ( ( zv(n) - zw(kw) ) / ( zw(kw+1)-zw(kw) ) ) |
|---|
| 1145 | ENDIF |
|---|
| 1146 | |
|---|
| 1147 | vv_int = ( 1.0_wp / 3.0_wp ) * ( aa + bb + cc ) |
|---|
| 1148 | ! |
|---|
| 1149 | !-- Needed to avoid NaN particle velocities. The value of 1.0 is just |
|---|
| 1150 | !-- an educated guess for the given case. |
|---|
| 1151 | IF ( vv_int + ( 2.0_wp / 3.0_wp ) * e_mean_int == 0.0_wp ) THEN |
|---|
| 1152 | fs_int(n) = 1.0_wp |
|---|
| 1153 | ELSE |
|---|
| 1154 | fs_int(n) = ( 2.0_wp / 3.0_wp ) * e_mean_int / & |
|---|
| 1155 | ( vv_int + ( 2.0_wp / 3.0_wp ) * e_mean_int ) |
|---|
| 1156 | ENDIF |
|---|
| 1157 | |
|---|
| 1158 | ENDDO |
|---|
| 1159 | ENDDO |
|---|
| 1160 | |
|---|
| 1161 | DO n = 1, number_of_particles |
|---|
| 1162 | |
|---|
| 1163 | rg(n,1) = random_gauss( iran_part, 5.0_wp ) |
|---|
| 1164 | rg(n,2) = random_gauss( iran_part, 5.0_wp ) |
|---|
| 1165 | rg(n,3) = random_gauss( iran_part, 5.0_wp ) |
|---|
| 1166 | |
|---|
| 1167 | ENDDO |
|---|
| 1168 | |
|---|
| 1169 | DO n = 1, number_of_particles |
|---|
| 1170 | ! |
|---|
| 1171 | !-- Calculate the Lagrangian timescale according to Weil et al. (2004). |
|---|
| 1172 | lagr_timescale = ( 4.0_wp * e_int(n) ) / & |
|---|
| 1173 | ( 3.0_wp * fs_int(n) * c_0 * diss_int(n) ) |
|---|
| 1174 | |
|---|
| 1175 | ! |
|---|
| 1176 | !-- Calculate the next particle timestep. dt_gap is the time needed to |
|---|
| 1177 | !-- complete the current LES timestep. |
|---|
| 1178 | dt_gap = dt_3d - particles(n)%dt_sum |
|---|
| 1179 | dt_particle(n) = MIN( dt_3d, 0.025_wp * lagr_timescale, dt_gap ) |
|---|
| 1180 | |
|---|
| 1181 | ! |
|---|
| 1182 | !-- The particle timestep should not be too small in order to prevent |
|---|
| 1183 | !-- the number of particle timesteps of getting too large |
|---|
| 1184 | IF ( dt_particle(n) < dt_min_part .AND. dt_min_part < dt_gap ) THEN |
|---|
| 1185 | dt_particle(n) = dt_min_part |
|---|
| 1186 | ENDIF |
|---|
| 1187 | |
|---|
| 1188 | ! |
|---|
| 1189 | !-- Calculate the SGS velocity components |
|---|
| 1190 | IF ( particles(n)%age == 0.0_wp ) THEN |
|---|
| 1191 | ! |
|---|
| 1192 | !-- For new particles the SGS components are derived from the SGS |
|---|
| 1193 | !-- TKE. Limit the Gaussian random number to the interval |
|---|
| 1194 | !-- [-5.0*sigma, 5.0*sigma] in order to prevent the SGS velocities |
|---|
| 1195 | !-- from becoming unrealistically large. |
|---|
| 1196 | particles(n)%rvar1 = SQRT( 2.0_wp * sgs_wfu_part * e_int(n) ) * & |
|---|
| 1197 | ( rg(n,1) - 1.0_wp ) |
|---|
| 1198 | particles(n)%rvar2 = SQRT( 2.0_wp * sgs_wfv_part * e_int(n) ) * & |
|---|
| 1199 | ( rg(n,2) - 1.0_wp ) |
|---|
| 1200 | particles(n)%rvar3 = SQRT( 2.0_wp * sgs_wfw_part * e_int(n) ) * & |
|---|
| 1201 | ( rg(n,3) - 1.0_wp ) |
|---|
| 1202 | |
|---|
| 1203 | ELSE |
|---|
| 1204 | ! |
|---|
| 1205 | !-- Restriction of the size of the new timestep: compared to the |
|---|
| 1206 | !-- previous timestep the increase must not exceed 200% |
|---|
| 1207 | |
|---|
| 1208 | dt_particle_m = particles(n)%age - particles(n)%age_m |
|---|
| 1209 | IF ( dt_particle(n) > 2.0_wp * dt_particle_m ) THEN |
|---|
| 1210 | dt_particle(n) = 2.0_wp * dt_particle_m |
|---|
| 1211 | ENDIF |
|---|
| 1212 | |
|---|
| 1213 | ! |
|---|
| 1214 | !-- For old particles the SGS components are correlated with the |
|---|
| 1215 | !-- values from the previous timestep. Random numbers have also to |
|---|
| 1216 | !-- be limited (see above). |
|---|
| 1217 | !-- As negative values for the subgrid TKE are not allowed, the |
|---|
| 1218 | !-- change of the subgrid TKE with time cannot be smaller than |
|---|
| 1219 | !-- -e_int(n)/dt_particle. This value is used as a lower boundary |
|---|
| 1220 | !-- value for the change of TKE |
|---|
| 1221 | |
|---|
| 1222 | de_dt_min = - e_int(n) / dt_particle(n) |
|---|
| 1223 | |
|---|
| 1224 | de_dt = ( e_int(n) - particles(n)%e_m ) / dt_particle_m |
|---|
| 1225 | |
|---|
| 1226 | IF ( de_dt < de_dt_min ) THEN |
|---|
| 1227 | de_dt = de_dt_min |
|---|
| 1228 | ENDIF |
|---|
| 1229 | |
|---|
| 1230 | particles(n)%rvar1 = particles(n)%rvar1 - fs_int(n) * c_0 * & |
|---|
| 1231 | diss_int(n) * particles(n)%rvar1 * dt_particle(n) / & |
|---|
| 1232 | ( 4.0_wp * sgs_wfu_part * e_int(n) ) + & |
|---|
| 1233 | ( 2.0_wp * sgs_wfu_part * de_dt * & |
|---|
| 1234 | particles(n)%rvar1 / & |
|---|
| 1235 | ( 2.0_wp * sgs_wfu_part * e_int(n) ) + & |
|---|
| 1236 | de_dx_int(n) & |
|---|
| 1237 | ) * dt_particle(n) / 2.0_wp + & |
|---|
| 1238 | SQRT( fs_int(n) * c_0 * diss_int(n) ) * & |
|---|
| 1239 | ( rg(n,1) - 1.0_wp ) * & |
|---|
| 1240 | SQRT( dt_particle(n) ) |
|---|
| 1241 | |
|---|
| 1242 | particles(n)%rvar2 = particles(n)%rvar2 - fs_int(n) * c_0 * & |
|---|
| 1243 | diss_int(n) * particles(n)%rvar2 * dt_particle(n) / & |
|---|
| 1244 | ( 4.0_wp * sgs_wfv_part * e_int(n) ) + & |
|---|
| 1245 | ( 2.0_wp * sgs_wfv_part * de_dt * & |
|---|
| 1246 | particles(n)%rvar2 / & |
|---|
| 1247 | ( 2.0_wp * sgs_wfv_part * e_int(n) ) + & |
|---|
| 1248 | de_dy_int(n) & |
|---|
| 1249 | ) * dt_particle(n) / 2.0_wp + & |
|---|
| 1250 | SQRT( fs_int(n) * c_0 * diss_int(n) ) * & |
|---|
| 1251 | ( rg(n,2) - 1.0_wp ) * & |
|---|
| 1252 | SQRT( dt_particle(n) ) |
|---|
| 1253 | |
|---|
| 1254 | particles(n)%rvar3 = particles(n)%rvar3 - fs_int(n) * c_0 * & |
|---|
| 1255 | diss_int(n) * particles(n)%rvar3 * dt_particle(n) / & |
|---|
| 1256 | ( 4.0_wp * sgs_wfw_part * e_int(n) ) + & |
|---|
| 1257 | ( 2.0_wp * sgs_wfw_part * de_dt * & |
|---|
| 1258 | particles(n)%rvar3 / & |
|---|
| 1259 | ( 2.0_wp * sgs_wfw_part * e_int(n) ) + & |
|---|
| 1260 | de_dz_int(n) & |
|---|
| 1261 | ) * dt_particle(n) / 2.0_wp + & |
|---|
| 1262 | SQRT( fs_int(n) * c_0 * diss_int(n) ) * & |
|---|
| 1263 | ( rg(n,3) - 1.0_wp ) * & |
|---|
| 1264 | SQRT( dt_particle(n) ) |
|---|
| 1265 | |
|---|
| 1266 | ENDIF |
|---|
| 1267 | u_int(n) = u_int(n) + particles(n)%rvar1 |
|---|
| 1268 | v_int(n) = v_int(n) + particles(n)%rvar2 |
|---|
| 1269 | w_int(n) = w_int(n) + particles(n)%rvar3 |
|---|
| 1270 | |
|---|
| 1271 | ! |
|---|
| 1272 | !-- Store the SGS TKE of the current timelevel which is needed for |
|---|
| 1273 | !-- for calculating the SGS particle velocities at the next timestep |
|---|
| 1274 | particles(n)%e_m = e_int(n) |
|---|
| 1275 | ENDDO |
|---|
| 1276 | |
|---|
| 1277 | ELSE |
|---|
| 1278 | ! |
|---|
| 1279 | !-- If no SGS velocities are used, only the particle timestep has to |
|---|
| 1280 | !-- be set |
|---|
| 1281 | dt_particle = dt_3d |
|---|
| 1282 | |
|---|
| 1283 | ENDIF |
|---|
| 1284 | ! |
|---|
| 1285 | !-- Store the old age of the particle ( needed to prevent that a |
|---|
| 1286 | !-- particle crosses several PEs during one timestep, and for the |
|---|
| 1287 | !-- evaluation of the subgrid particle velocity fluctuations ) |
|---|
| 1288 | particles(1:number_of_particles)%age_m = particles(1:number_of_particles)%age |
|---|
| 1289 | |
|---|
| 1290 | dens_ratio = particle_groups(particles(1:number_of_particles)%group)%density_ratio |
|---|
| 1291 | |
|---|
| 1292 | IF ( ANY( dens_ratio == 0.0_wp ) ) THEN |
|---|
| 1293 | DO n = 1, number_of_particles |
|---|
| 1294 | |
|---|
| 1295 | ! |
|---|
| 1296 | !-- Particle advection |
|---|
| 1297 | IF ( dens_ratio(n) == 0.0_wp ) THEN |
|---|
| 1298 | ! |
|---|
| 1299 | !-- Pure passive transport (without particle inertia) |
|---|
| 1300 | particles(n)%x = xv(n) + u_int(n) * dt_particle(n) |
|---|
| 1301 | particles(n)%y = yv(n) + v_int(n) * dt_particle(n) |
|---|
| 1302 | particles(n)%z = zv(n) + w_int(n) * dt_particle(n) |
|---|
| 1303 | |
|---|
| 1304 | particles(n)%speed_x = u_int(n) |
|---|
| 1305 | particles(n)%speed_y = v_int(n) |
|---|
| 1306 | particles(n)%speed_z = w_int(n) |
|---|
| 1307 | |
|---|
| 1308 | ELSE |
|---|
| 1309 | ! |
|---|
| 1310 | !-- Transport of particles with inertia |
|---|
| 1311 | particles(n)%x = particles(n)%x + particles(n)%speed_x * & |
|---|
| 1312 | dt_particle(n) |
|---|
| 1313 | particles(n)%y = particles(n)%y + particles(n)%speed_y * & |
|---|
| 1314 | dt_particle(n) |
|---|
| 1315 | particles(n)%z = particles(n)%z + particles(n)%speed_z * & |
|---|
| 1316 | dt_particle(n) |
|---|
| 1317 | |
|---|
| 1318 | ! |
|---|
| 1319 | !-- Update of the particle velocity |
|---|
| 1320 | IF ( cloud_droplets ) THEN |
|---|
| 1321 | exp_arg = 4.5_wp * dens_ratio(n) * molecular_viscosity / & |
|---|
| 1322 | ( particles(n)%radius )**2 * & |
|---|
| 1323 | ( 1.0_wp + 0.15_wp * ( 2.0_wp * particles(n)%radius & |
|---|
| 1324 | * SQRT( ( u_int(n) - particles(n)%speed_x )**2 + & |
|---|
| 1325 | ( v_int(n) - particles(n)%speed_y )**2 + & |
|---|
| 1326 | ( w_int(n) - particles(n)%speed_z )**2 ) & |
|---|
| 1327 | / molecular_viscosity )**0.687_wp & |
|---|
| 1328 | ) |
|---|
| 1329 | |
|---|
| 1330 | exp_term = EXP( -exp_arg * dt_particle(n) ) |
|---|
| 1331 | ELSEIF ( use_sgs_for_particles ) THEN |
|---|
| 1332 | exp_arg = particle_groups(particles(n)%group)%exp_arg |
|---|
| 1333 | exp_term = EXP( -exp_arg * dt_particle(n) ) |
|---|
| 1334 | ELSE |
|---|
| 1335 | exp_arg = particle_groups(particles(n)%group)%exp_arg |
|---|
| 1336 | exp_term = particle_groups(particles(n)%group)%exp_term |
|---|
| 1337 | ENDIF |
|---|
| 1338 | particles(n)%speed_x = particles(n)%speed_x * exp_term + & |
|---|
| 1339 | u_int(n) * ( 1.0_wp - exp_term ) |
|---|
| 1340 | particles(n)%speed_y = particles(n)%speed_y * exp_term + & |
|---|
| 1341 | v_int(n) * ( 1.0_wp - exp_term ) |
|---|
| 1342 | particles(n)%speed_z = particles(n)%speed_z * exp_term + & |
|---|
| 1343 | ( w_int(n) - ( 1.0_wp - dens_ratio(n) ) * & |
|---|
| 1344 | g / exp_arg ) * ( 1.0_wp - exp_term ) |
|---|
| 1345 | ENDIF |
|---|
| 1346 | |
|---|
| 1347 | ENDDO |
|---|
| 1348 | |
|---|
| 1349 | ELSE |
|---|
| 1350 | |
|---|
| 1351 | DO n = 1, number_of_particles |
|---|
| 1352 | |
|---|
| 1353 | !-- Transport of particles with inertia |
|---|
| 1354 | particles(n)%x = xv(n) + particles(n)%speed_x * dt_particle(n) |
|---|
| 1355 | particles(n)%y = yv(n) + particles(n)%speed_y * dt_particle(n) |
|---|
| 1356 | particles(n)%z = zv(n) + particles(n)%speed_z * dt_particle(n) |
|---|
| 1357 | ! |
|---|
| 1358 | !-- Update of the particle velocity |
|---|
| 1359 | IF ( cloud_droplets ) THEN |
|---|
| 1360 | |
|---|
| 1361 | exp_arg = 4.5_wp * dens_ratio(n) * molecular_viscosity / & |
|---|
| 1362 | ( particles(n)%radius )**2 * & |
|---|
| 1363 | ( 1.0_wp + 0.15_wp * ( 2.0_wp * particles(n)%radius * & |
|---|
| 1364 | SQRT( ( u_int(n) - particles(n)%speed_x )**2 + & |
|---|
| 1365 | ( v_int(n) - particles(n)%speed_y )**2 + & |
|---|
| 1366 | ( w_int(n) - particles(n)%speed_z )**2 ) / & |
|---|
| 1367 | molecular_viscosity )**0.687_wp & |
|---|
| 1368 | ) |
|---|
| 1369 | |
|---|
| 1370 | exp_term = EXP( -exp_arg * dt_particle(n) ) |
|---|
| 1371 | ELSEIF ( use_sgs_for_particles ) THEN |
|---|
| 1372 | exp_arg = particle_groups(particles(n)%group)%exp_arg |
|---|
| 1373 | exp_term = EXP( -exp_arg * dt_particle(n) ) |
|---|
| 1374 | ELSE |
|---|
| 1375 | exp_arg = particle_groups(particles(n)%group)%exp_arg |
|---|
| 1376 | exp_term = particle_groups(particles(n)%group)%exp_term |
|---|
| 1377 | ENDIF |
|---|
| 1378 | particles(n)%speed_x = particles(n)%speed_x * exp_term + & |
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| 1379 | u_int(n) * ( 1.0_wp - exp_term ) |
|---|
| 1380 | particles(n)%speed_y = particles(n)%speed_y * exp_term + & |
|---|
| 1381 | v_int(n) * ( 1.0_wp - exp_term ) |
|---|
| 1382 | particles(n)%speed_z = particles(n)%speed_z * exp_term + & |
|---|
| 1383 | ( w_int(n) - ( 1.0_wp - dens_ratio(n) ) * g / & |
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| 1384 | exp_arg ) * ( 1.0_wp - exp_term ) |
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| 1385 | ENDDO |
|---|
| 1386 | |
|---|
| 1387 | ENDIF |
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| 1388 | |
|---|
| 1389 | DO n = 1, number_of_particles |
|---|
| 1390 | ! |
|---|
| 1391 | !-- Increment the particle age and the total time that the particle |
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| 1392 | !-- has advanced within the particle timestep procedure |
|---|
| 1393 | particles(n)%age = particles(n)%age + dt_particle(n) |
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| 1394 | particles(n)%dt_sum = particles(n)%dt_sum + dt_particle(n) |
|---|
| 1395 | |
|---|
| 1396 | ! |
|---|
| 1397 | !-- Check whether there is still a particle that has not yet completed |
|---|
| 1398 | !-- the total LES timestep |
|---|
| 1399 | IF ( ( dt_3d - particles(n)%dt_sum ) > 1E-8_wp ) THEN |
|---|
| 1400 | dt_3d_reached_l = .FALSE. |
|---|
| 1401 | ENDIF |
|---|
| 1402 | |
|---|
| 1403 | ENDDO |
|---|
| 1404 | |
|---|
| 1405 | CALL cpu_log( log_point_s(44), 'lpm_advec', 'pause' ) |
|---|
| 1406 | |
|---|
| 1407 | END SUBROUTINE lpm_advec |
|---|
