[1682] | 1 | !> @file data_output_ptseries.f90 |
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[1036] | 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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[1818] | 16 | ! Copyright 1997-2016 Leibniz Universitaet Hannover |
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[1036] | 17 | !--------------------------------------------------------------------------------! |
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| 18 | ! |
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[263] | 19 | ! Current revisions: |
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[1] | 20 | ! ----------------- |
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[1784] | 21 | ! |
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[1832] | 22 | ! |
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[1321] | 23 | ! Former revisions: |
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| 24 | ! ----------------- |
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| 25 | ! $Id: data_output_ptseries.f90 1832 2016-04-07 13:28:15Z hellstea $ |
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| 26 | ! |
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[1832] | 27 | ! 1831 2016-04-07 13:15:51Z hoffmann |
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| 28 | ! curvature_solution_effects moved to particle_attributes |
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| 29 | ! |
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[1784] | 30 | ! 1783 2016-03-06 18:36:17Z raasch |
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| 31 | ! netcdf module name changed + related changes |
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| 32 | ! |
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[1683] | 33 | ! 1682 2015-10-07 23:56:08Z knoop |
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| 34 | ! Code annotations made doxygen readable |
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| 35 | ! |
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[1360] | 36 | ! 1359 2014-04-11 17:15:14Z hoffmann |
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| 37 | ! New particle structure integrated. |
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| 38 | ! |
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[1354] | 39 | ! 1353 2014-04-08 15:21:23Z heinze |
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| 40 | ! REAL constants provided with KIND-attribute |
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| 41 | ! |
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[1329] | 42 | ! 1327 2014-03-21 11:00:16Z raasch |
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| 43 | ! -netcdf output queries |
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| 44 | ! |
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[1321] | 45 | ! 1320 2014-03-20 08:40:49Z raasch |
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[1320] | 46 | ! ONLY-attribute added to USE-statements, |
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| 47 | ! kind-parameters added to all INTEGER and REAL declaration statements, |
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| 48 | ! kinds are defined in new module kinds, |
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| 49 | ! revision history before 2012 removed, |
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| 50 | ! comment fields (!:) to be used for variable explanations added to |
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| 51 | ! all variable declaration statements |
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[1] | 52 | ! |
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[1319] | 53 | ! 1318 2014-03-17 13:35:16Z raasch |
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| 54 | ! barrier argument removed from cpu_log, |
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| 55 | ! module interfaces removed |
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| 56 | ! |
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[1037] | 57 | ! 1036 2012-10-22 13:43:42Z raasch |
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| 58 | ! code put under GPL (PALM 3.9) |
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| 59 | ! |
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[826] | 60 | ! 825 2012-02-19 03:03:44Z raasch |
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| 61 | ! mean/minimum/maximum particle radius added as output quantity, |
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| 62 | ! particle attributes speed_x|y|z_sgs renamed rvar1|2|3 |
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| 63 | ! |
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[1] | 64 | ! Revision 1.1 2006/08/04 14:24:18 raasch |
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| 65 | ! Initial revision |
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| 66 | ! |
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| 67 | ! |
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| 68 | ! Description: |
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| 69 | ! ------------ |
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[1682] | 70 | !> Output of particle data timeseries in NetCDF format. |
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[1] | 71 | !------------------------------------------------------------------------------! |
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[1682] | 72 | SUBROUTINE data_output_ptseries |
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| 73 | |
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[1] | 74 | |
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[1320] | 75 | USE control_parameters, & |
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[1327] | 76 | ONLY: dopts_time_count, time_since_reference_point |
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[1320] | 77 | |
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| 78 | USE cpulog, & |
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| 79 | ONLY: cpu_log, log_point |
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| 80 | |
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| 81 | USE indices, & |
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[1359] | 82 | ONLY: nxl, nxr, nys, nyn, nzb, nzt |
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[1320] | 83 | |
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| 84 | USE kinds |
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| 85 | |
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[1783] | 86 | #if defined( __netcdf ) |
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| 87 | USE NETCDF |
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| 88 | #endif |
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[1320] | 89 | |
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[1783] | 90 | USE netcdf_interface, & |
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| 91 | ONLY: dopts_num, id_set_pts, id_var_dopts, id_var_time_pts, nc_stat, & |
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| 92 | netcdf_handle_error |
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| 93 | |
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[1320] | 94 | USE particle_attributes, & |
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[1831] | 95 | ONLY: curvature_solution_effects, grid_particles, number_of_particles,& |
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| 96 | number_of_particle_groups, particles, prt_count |
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[1320] | 97 | |
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[1] | 98 | USE pegrid |
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| 99 | |
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| 100 | IMPLICIT NONE |
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| 101 | |
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| 102 | |
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[1682] | 103 | INTEGER(iwp) :: i !< |
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| 104 | INTEGER(iwp) :: inum !< |
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| 105 | INTEGER(iwp) :: j !< |
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| 106 | INTEGER(iwp) :: jg !< |
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| 107 | INTEGER(iwp) :: k !< |
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| 108 | INTEGER(iwp) :: n !< |
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[1] | 109 | |
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[1682] | 110 | REAL(wp), DIMENSION(:,:), ALLOCATABLE :: pts_value !< |
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| 111 | REAL(wp), DIMENSION(:,:), ALLOCATABLE :: pts_value_l !< |
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[1] | 112 | |
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| 113 | |
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| 114 | CALL cpu_log( log_point(36), 'data_output_ptseries', 'start' ) |
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| 115 | |
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[1327] | 116 | IF ( myid == 0 ) THEN |
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[1] | 117 | ! |
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| 118 | !-- Open file for time series output in NetCDF format |
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| 119 | dopts_time_count = dopts_time_count + 1 |
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| 120 | CALL check_open( 109 ) |
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| 121 | #if defined( __netcdf ) |
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| 122 | ! |
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| 123 | !-- Update the particle time series time axis |
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[291] | 124 | nc_stat = NF90_PUT_VAR( id_set_pts, id_var_time_pts, & |
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| 125 | (/ time_since_reference_point /), & |
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[1] | 126 | start = (/ dopts_time_count /), count = (/ 1 /) ) |
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[1783] | 127 | CALL netcdf_handle_error( 'data_output_ptseries', 391 ) |
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[1] | 128 | #endif |
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| 129 | |
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| 130 | ENDIF |
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| 131 | |
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[825] | 132 | ALLOCATE( pts_value(0:number_of_particle_groups,dopts_num), & |
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| 133 | pts_value_l(0:number_of_particle_groups,dopts_num) ) |
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| 134 | |
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[1353] | 135 | pts_value_l = 0.0_wp |
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| 136 | pts_value_l(:,16) = 9999999.9_wp ! for calculation of minimum radius |
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[1] | 137 | |
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| 138 | ! |
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| 139 | !-- Calculate or collect the particle time series quantities for all particles |
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| 140 | !-- and seperately for each particle group (if there is more than one group) |
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[1359] | 141 | DO i = nxl, nxr |
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| 142 | DO j = nys, nyn |
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| 143 | DO k = nzb, nzt |
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| 144 | number_of_particles = prt_count(k,j,i) |
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| 145 | IF (number_of_particles <= 0) CYCLE |
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| 146 | particles => grid_particles(k,j,i)%particles(1:number_of_particles) |
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| 147 | DO n = 1, number_of_particles |
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[1] | 148 | |
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[1359] | 149 | IF ( particles(n)%particle_mask ) THEN ! Restrict analysis to active particles |
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[1] | 150 | |
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[1359] | 151 | pts_value_l(0,1) = pts_value_l(0,1) + 1.0_wp ! total # of particles |
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| 152 | pts_value_l(0,2) = pts_value_l(0,2) + & |
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| 153 | ( particles(n)%x - particles(n)%origin_x ) ! mean x |
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| 154 | pts_value_l(0,3) = pts_value_l(0,3) + & |
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| 155 | ( particles(n)%y - particles(n)%origin_y ) ! mean y |
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| 156 | pts_value_l(0,4) = pts_value_l(0,4) + & |
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| 157 | ( particles(n)%z - particles(n)%origin_z ) ! mean z |
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| 158 | pts_value_l(0,5) = pts_value_l(0,5) + particles(n)%z ! mean z (absolute) |
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| 159 | pts_value_l(0,6) = pts_value_l(0,6) + particles(n)%speed_x ! mean u |
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| 160 | pts_value_l(0,7) = pts_value_l(0,7) + particles(n)%speed_y ! mean v |
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| 161 | pts_value_l(0,8) = pts_value_l(0,8) + particles(n)%speed_z ! mean w |
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| 162 | IF ( .NOT. curvature_solution_effects ) THEN |
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| 163 | pts_value_l(0,9) = pts_value_l(0,9) + particles(n)%rvar1 ! mean sgsu |
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| 164 | pts_value_l(0,10) = pts_value_l(0,10) + particles(n)%rvar2 ! mean sgsv |
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| 165 | pts_value_l(0,11) = pts_value_l(0,11) + particles(n)%rvar3 ! mean sgsw |
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| 166 | ENDIF |
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| 167 | IF ( particles(n)%speed_z > 0.0_wp ) THEN |
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| 168 | pts_value_l(0,12) = pts_value_l(0,12) + 1.0_wp ! # of upward moving prts |
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| 169 | pts_value_l(0,13) = pts_value_l(0,13) + & |
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| 170 | particles(n)%speed_z ! mean w upw. |
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| 171 | ELSE |
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| 172 | pts_value_l(0,14) = pts_value_l(0,14) + & |
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| 173 | particles(n)%speed_z ! mean w down |
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| 174 | ENDIF |
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| 175 | pts_value_l(0,15) = pts_value_l(0,15) + particles(n)%radius ! mean rad |
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| 176 | pts_value_l(0,16) = MIN( pts_value_l(0,16), particles(n)%radius ) ! minrad |
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| 177 | pts_value_l(0,17) = MAX( pts_value_l(0,17), particles(n)%radius ) ! maxrad |
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| 178 | pts_value_l(0,18) = pts_value_l(0,18) + 1.0_wp |
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| 179 | pts_value_l(0,19) = pts_value_l(0,18) + 1.0_wp |
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[1] | 180 | ! |
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[1359] | 181 | !-- Repeat the same for the respective particle group |
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| 182 | IF ( number_of_particle_groups > 1 ) THEN |
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| 183 | jg = particles(n)%group |
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[1] | 184 | |
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[1359] | 185 | pts_value_l(jg,1) = pts_value_l(jg,1) + 1.0_wp |
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| 186 | pts_value_l(jg,2) = pts_value_l(jg,2) + & |
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| 187 | ( particles(n)%x - particles(n)%origin_x ) |
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| 188 | pts_value_l(jg,3) = pts_value_l(jg,3) + & |
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| 189 | ( particles(n)%y - particles(n)%origin_y ) |
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| 190 | pts_value_l(jg,4) = pts_value_l(jg,4) + & |
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| 191 | ( particles(n)%z - particles(n)%origin_z ) |
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| 192 | pts_value_l(jg,5) = pts_value_l(jg,5) + particles(n)%z |
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| 193 | pts_value_l(jg,6) = pts_value_l(jg,6) + particles(n)%speed_x |
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| 194 | pts_value_l(jg,7) = pts_value_l(jg,7) + particles(n)%speed_y |
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| 195 | pts_value_l(jg,8) = pts_value_l(jg,8) + particles(n)%speed_z |
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| 196 | IF ( .NOT. curvature_solution_effects ) THEN |
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| 197 | pts_value_l(jg,9) = pts_value_l(jg,9) + particles(n)%rvar1 |
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| 198 | pts_value_l(jg,10) = pts_value_l(jg,10) + particles(n)%rvar2 |
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| 199 | pts_value_l(jg,11) = pts_value_l(jg,11) + particles(n)%rvar3 |
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| 200 | ENDIF |
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| 201 | IF ( particles(n)%speed_z > 0.0_wp ) THEN |
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| 202 | pts_value_l(jg,12) = pts_value_l(jg,12) + 1.0_wp |
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| 203 | pts_value_l(jg,13) = pts_value_l(jg,13) + particles(n)%speed_z |
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| 204 | ELSE |
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| 205 | pts_value_l(jg,14) = pts_value_l(jg,14) + particles(n)%speed_z |
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| 206 | ENDIF |
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| 207 | pts_value_l(jg,15) = pts_value_l(jg,15) + particles(n)%radius |
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| 208 | pts_value_l(jg,16) = MIN( pts_value(jg,16), particles(n)%radius ) |
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| 209 | pts_value_l(jg,17) = MAX( pts_value(jg,17), particles(n)%radius ) |
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| 210 | pts_value_l(jg,18) = pts_value_l(jg,18) + 1.0_wp |
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| 211 | pts_value_l(jg,19) = pts_value_l(jg,19) + 1.0_wp |
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| 212 | ENDIF |
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[1] | 213 | |
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[1359] | 214 | ENDIF |
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[1] | 215 | |
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[1359] | 216 | ENDDO |
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| 217 | |
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| 218 | ENDDO |
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| 219 | ENDDO |
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[1] | 220 | ENDDO |
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| 221 | |
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[1359] | 222 | |
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[1] | 223 | #if defined( __parallel ) |
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| 224 | ! |
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| 225 | !-- Sum values of the subdomains |
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| 226 | inum = number_of_particle_groups + 1 |
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| 227 | |
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[622] | 228 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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[824] | 229 | CALL MPI_ALLREDUCE( pts_value_l(0,1), pts_value(0,1), 15*inum, MPI_REAL, & |
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[1] | 230 | MPI_SUM, comm2d, ierr ) |
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[622] | 231 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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[824] | 232 | CALL MPI_ALLREDUCE( pts_value_l(0,16), pts_value(0,16), inum, MPI_REAL, & |
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[825] | 233 | MPI_MIN, comm2d, ierr ) |
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| 234 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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| 235 | CALL MPI_ALLREDUCE( pts_value_l(0,17), pts_value(0,17), inum, MPI_REAL, & |
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[1] | 236 | MPI_MAX, comm2d, ierr ) |
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[622] | 237 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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[825] | 238 | CALL MPI_ALLREDUCE( pts_value_l(0,18), pts_value(0,18), inum, MPI_REAL, & |
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| 239 | MPI_MAX, comm2d, ierr ) |
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| 240 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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| 241 | CALL MPI_ALLREDUCE( pts_value_l(0,19), pts_value(0,19), inum, MPI_REAL, & |
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[1] | 242 | MPI_MIN, comm2d, ierr ) |
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| 243 | #else |
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[825] | 244 | pts_value(:,1:19) = pts_value_l(:,1:19) |
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[1] | 245 | #endif |
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| 246 | |
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| 247 | ! |
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[825] | 248 | !-- Normalize the above calculated quantities (except min/max values) with the |
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| 249 | !-- total number of particles |
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[1] | 250 | IF ( number_of_particle_groups > 1 ) THEN |
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| 251 | inum = number_of_particle_groups |
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| 252 | ELSE |
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| 253 | inum = 0 |
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| 254 | ENDIF |
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| 255 | |
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| 256 | DO j = 0, inum |
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| 257 | |
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[1353] | 258 | IF ( pts_value(j,1) > 0.0_wp ) THEN |
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[1] | 259 | |
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[824] | 260 | pts_value(j,2:15) = pts_value(j,2:15) / pts_value(j,1) |
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[1353] | 261 | IF ( pts_value(j,12) > 0.0_wp .AND. pts_value(j,12) < 1.0_wp ) THEN |
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[1] | 262 | pts_value(j,13) = pts_value(j,13) / pts_value(j,12) |
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[1353] | 263 | pts_value(j,14) = pts_value(j,14) / ( 1.0_wp - pts_value(j,12) ) |
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| 264 | ELSEIF ( pts_value(j,12) == 0.0_wp ) THEN |
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| 265 | pts_value(j,13) = -1.0_wp |
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[1] | 266 | ELSE |
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[1353] | 267 | pts_value(j,14) = -1.0_wp |
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[1] | 268 | ENDIF |
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| 269 | |
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| 270 | ENDIF |
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| 271 | |
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| 272 | ENDDO |
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| 273 | |
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| 274 | ! |
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| 275 | !-- Calculate higher order moments of particle time series quantities, |
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| 276 | !-- seperately for each particle group (if there is more than one group) |
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[1359] | 277 | DO i = nxl, nxr |
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| 278 | DO j = nys, nyn |
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| 279 | DO k = nzb, nzt |
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| 280 | number_of_particles = prt_count(k,j,i) |
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| 281 | IF (number_of_particles <= 0) CYCLE |
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| 282 | particles => grid_particles(k,j,i)%particles(1:number_of_particles) |
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| 283 | DO n = 1, number_of_particles |
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[1] | 284 | |
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[1359] | 285 | pts_value_l(0,20) = pts_value_l(0,20) + ( particles(n)%x - & |
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| 286 | particles(n)%origin_x - pts_value(0,2) )**2 ! x*2 |
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| 287 | pts_value_l(0,21) = pts_value_l(0,21) + ( particles(n)%y - & |
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| 288 | particles(n)%origin_y - pts_value(0,3) )**2 ! y*2 |
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| 289 | pts_value_l(0,22) = pts_value_l(0,22) + ( particles(n)%z - & |
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| 290 | particles(n)%origin_z - pts_value(0,4) )**2 ! z*2 |
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| 291 | pts_value_l(0,23) = pts_value_l(0,23) + ( particles(n)%speed_x - & |
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| 292 | pts_value(0,6) )**2 ! u*2 |
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| 293 | pts_value_l(0,24) = pts_value_l(0,24) + ( particles(n)%speed_y - & |
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| 294 | pts_value(0,7) )**2 ! v*2 |
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| 295 | pts_value_l(0,25) = pts_value_l(0,25) + ( particles(n)%speed_z - & |
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| 296 | pts_value(0,8) )**2 ! w*2 |
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| 297 | IF ( .NOT. curvature_solution_effects ) THEN |
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| 298 | pts_value_l(0,26) = pts_value_l(0,26) + ( particles(n)%rvar1 - & |
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| 299 | pts_value(0,9) )**2 ! u"2 |
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| 300 | pts_value_l(0,27) = pts_value_l(0,27) + ( particles(n)%rvar2 - & |
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| 301 | pts_value(0,10) )**2 ! v"2 |
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| 302 | pts_value_l(0,28) = pts_value_l(0,28) + ( particles(n)%rvar3 - & |
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| 303 | pts_value(0,11) )**2 ! w"2 |
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| 304 | ENDIF |
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[1] | 305 | ! |
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[1359] | 306 | !-- Repeat the same for the respective particle group |
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| 307 | IF ( number_of_particle_groups > 1 ) THEN |
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| 308 | jg = particles(n)%group |
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[1] | 309 | |
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[1359] | 310 | pts_value_l(jg,20) = pts_value_l(jg,20) + ( particles(n)%x - & |
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| 311 | particles(n)%origin_x - pts_value(jg,2) )**2 |
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| 312 | pts_value_l(jg,21) = pts_value_l(jg,21) + ( particles(n)%y - & |
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| 313 | particles(n)%origin_y - pts_value(jg,3) )**2 |
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| 314 | pts_value_l(jg,22) = pts_value_l(jg,22) + ( particles(n)%z - & |
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| 315 | particles(n)%origin_z - pts_value(jg,4) )**2 |
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| 316 | pts_value_l(jg,23) = pts_value_l(jg,23) + ( particles(n)%speed_x - & |
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| 317 | pts_value(jg,6) )**2 |
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| 318 | pts_value_l(jg,24) = pts_value_l(jg,24) + ( particles(n)%speed_y - & |
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| 319 | pts_value(jg,7) )**2 |
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| 320 | pts_value_l(jg,25) = pts_value_l(jg,25) + ( particles(n)%speed_z - & |
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| 321 | pts_value(jg,8) )**2 |
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| 322 | IF ( .NOT. curvature_solution_effects ) THEN |
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| 323 | pts_value_l(jg,26) = pts_value_l(jg,26) + ( particles(n)%rvar1 - & |
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| 324 | pts_value(jg,9) )**2 |
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| 325 | pts_value_l(jg,27) = pts_value_l(jg,27) + ( particles(n)%rvar2 - & |
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| 326 | pts_value(jg,10) )**2 |
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| 327 | pts_value_l(jg,28) = pts_value_l(jg,28) + ( particles(n)%rvar3 - & |
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| 328 | pts_value(jg,11) )**2 |
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| 329 | ENDIF |
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| 330 | ENDIF |
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[1] | 331 | |
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[1359] | 332 | ENDDO |
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| 333 | ENDDO |
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| 334 | ENDDO |
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[1] | 335 | ENDDO |
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| 336 | |
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[825] | 337 | pts_value_l(0,29) = ( number_of_particles - pts_value(0,1) / numprocs )**2 |
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[1] | 338 | ! variance of particle numbers |
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| 339 | IF ( number_of_particle_groups > 1 ) THEN |
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| 340 | DO j = 1, number_of_particle_groups |
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[825] | 341 | pts_value_l(j,29) = ( pts_value_l(j,1) - & |
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[1] | 342 | pts_value(j,1) / numprocs )**2 |
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| 343 | ENDDO |
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| 344 | ENDIF |
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| 345 | |
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| 346 | #if defined( __parallel ) |
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| 347 | ! |
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| 348 | !-- Sum values of the subdomains |
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| 349 | inum = number_of_particle_groups + 1 |
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| 350 | |
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[622] | 351 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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[825] | 352 | CALL MPI_ALLREDUCE( pts_value_l(0,20), pts_value(0,20), inum*10, MPI_REAL, & |
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[1] | 353 | MPI_SUM, comm2d, ierr ) |
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| 354 | #else |
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[825] | 355 | pts_value(:,20:29) = pts_value_l(:,20:29) |
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[1] | 356 | #endif |
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| 357 | |
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| 358 | ! |
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| 359 | !-- Normalize the above calculated quantities with the total number of |
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| 360 | !-- particles |
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| 361 | IF ( number_of_particle_groups > 1 ) THEN |
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| 362 | inum = number_of_particle_groups |
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| 363 | ELSE |
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| 364 | inum = 0 |
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| 365 | ENDIF |
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| 366 | |
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| 367 | DO j = 0, inum |
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| 368 | |
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[1353] | 369 | IF ( pts_value(j,1) > 0.0_wp ) THEN |
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[825] | 370 | pts_value(j,20:28) = pts_value(j,20:28) / pts_value(j,1) |
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[1] | 371 | ENDIF |
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[825] | 372 | pts_value(j,29) = pts_value(j,29) / numprocs |
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[1] | 373 | |
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| 374 | ENDDO |
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| 375 | |
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| 376 | #if defined( __netcdf ) |
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| 377 | ! |
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| 378 | !-- Output particle time series quantities in NetCDF format |
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[1327] | 379 | IF ( myid == 0 ) THEN |
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[1] | 380 | DO j = 0, inum |
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| 381 | DO i = 1, dopts_num |
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| 382 | nc_stat = NF90_PUT_VAR( id_set_pts, id_var_dopts(i,j), & |
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| 383 | (/ pts_value(j,i) /), & |
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| 384 | start = (/ dopts_time_count /), & |
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| 385 | count = (/ 1 /) ) |
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[1783] | 386 | CALL netcdf_handle_error( 'data_output_ptseries', 392 ) |
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[1] | 387 | ENDDO |
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| 388 | ENDDO |
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| 389 | ENDIF |
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| 390 | #endif |
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| 391 | |
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[825] | 392 | DEALLOCATE( pts_value, pts_value_l ) |
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| 393 | |
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[1318] | 394 | CALL cpu_log( log_point(36), 'data_output_ptseries', 'stop' ) |
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[1] | 395 | |
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| 396 | END SUBROUTINE data_output_ptseries |
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