| 1 | SUBROUTINE data_output_ptseries |
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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: data_output_ptseries.f90 1310 2014-03-14 08:01:56Z suehring $ |
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| 27 | ! |
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| 28 | ! 1036 2012-10-22 13:43:42Z raasch |
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| 29 | ! code put under GPL (PALM 3.9) |
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| 30 | ! |
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| 31 | ! 825 2012-02-19 03:03:44Z raasch |
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| 32 | ! mean/minimum/maximum particle radius added as output quantity, |
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| 33 | ! particle attributes speed_x|y|z_sgs renamed rvar1|2|3 |
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| 34 | ! |
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| 35 | ! 622 2010-12-10 08:08:13Z raasch |
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| 36 | ! optional barriers included in order to speed up collective operations |
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| 37 | ! |
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| 38 | ! 291 2009-04-16 12:07:26Z raasch |
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| 39 | ! simulated_time in NetCDF output replaced by time_since_reference_point. |
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| 40 | ! Output of NetCDF messages with aid of message handling routine. |
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| 41 | ! |
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| 42 | ! 60 2007-03-11 11:50:04Z raasch |
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| 43 | ! Particles-package is now part of the default code. |
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| 44 | ! |
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| 45 | ! RCS Log replace by Id keyword, revision history cleaned up |
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| 46 | ! |
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| 47 | ! Revision 1.2 2006/08/22 13:51:13 raasch |
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| 48 | ! Seperate output for particle groups |
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| 49 | ! |
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| 50 | ! Revision 1.1 2006/08/04 14:24:18 raasch |
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| 51 | ! Initial revision |
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| 52 | ! |
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| 53 | ! |
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| 54 | ! Description: |
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| 55 | ! ------------ |
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| 56 | ! Output of particle data timeseries in NetCDF format. |
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| 57 | !------------------------------------------------------------------------------! |
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| 58 | |
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| 59 | USE cloud_parameters |
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| 60 | USE control_parameters |
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| 61 | USE cpulog |
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| 62 | USE indices |
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| 63 | USE interfaces |
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| 64 | USE netcdf_control |
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| 65 | USE particle_attributes |
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| 66 | USE pegrid |
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| 67 | |
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| 68 | IMPLICIT NONE |
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| 69 | |
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| 70 | |
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| 71 | INTEGER :: i, inum, j, n |
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| 72 | |
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| 73 | REAL, DIMENSION(:,:), ALLOCATABLE :: pts_value, pts_value_l |
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| 74 | |
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| 75 | |
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| 76 | CALL cpu_log( log_point(36), 'data_output_ptseries', 'start' ) |
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| 77 | |
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| 78 | IF ( myid == 0 .AND. netcdf_output ) THEN |
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| 79 | ! |
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| 80 | !-- Open file for time series output in NetCDF format |
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| 81 | dopts_time_count = dopts_time_count + 1 |
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| 82 | CALL check_open( 109 ) |
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| 83 | #if defined( __netcdf ) |
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| 84 | ! |
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| 85 | !-- Update the particle time series time axis |
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| 86 | nc_stat = NF90_PUT_VAR( id_set_pts, id_var_time_pts, & |
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| 87 | (/ time_since_reference_point /), & |
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| 88 | start = (/ dopts_time_count /), count = (/ 1 /) ) |
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| 89 | CALL handle_netcdf_error( 'data_output_ptseries', 391 ) |
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| 90 | #endif |
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| 91 | |
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| 92 | ENDIF |
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| 93 | |
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| 94 | ALLOCATE( pts_value(0:number_of_particle_groups,dopts_num), & |
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| 95 | pts_value_l(0:number_of_particle_groups,dopts_num) ) |
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| 96 | |
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| 97 | pts_value_l = 0.0 |
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| 98 | pts_value_l(:,16) = 9999999.9 ! for calculation of minimum radius |
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| 99 | |
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| 100 | ! |
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| 101 | !-- Calculate or collect the particle time series quantities for all particles |
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| 102 | !-- and seperately for each particle group (if there is more than one group) |
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| 103 | DO n = 1, number_of_particles |
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| 104 | |
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| 105 | pts_value_l(0,1) = number_of_particles ! total # of particles |
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| 106 | pts_value_l(0,2) = pts_value_l(0,2) + & |
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| 107 | ( particles(n)%x - particles(n)%origin_x ) ! mean x |
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| 108 | pts_value_l(0,3) = pts_value_l(0,3) + & |
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| 109 | ( particles(n)%y - particles(n)%origin_y ) ! mean y |
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| 110 | pts_value_l(0,4) = pts_value_l(0,4) + & |
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| 111 | ( particles(n)%z - particles(n)%origin_z ) ! mean z |
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| 112 | pts_value_l(0,5) = pts_value_l(0,5) + particles(n)%z ! mean z (absolute) |
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| 113 | pts_value_l(0,6) = pts_value_l(0,6) + particles(n)%speed_x ! mean u |
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| 114 | pts_value_l(0,7) = pts_value_l(0,7) + particles(n)%speed_y ! mean v |
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| 115 | pts_value_l(0,8) = pts_value_l(0,8) + particles(n)%speed_z ! mean w |
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| 116 | IF ( .NOT. curvature_solution_effects ) THEN |
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| 117 | pts_value_l(0,9) = pts_value_l(0,9) + particles(n)%rvar1 ! mean sgsu |
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| 118 | pts_value_l(0,10) = pts_value_l(0,10) + particles(n)%rvar2 ! mean sgsv |
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| 119 | pts_value_l(0,11) = pts_value_l(0,11) + particles(n)%rvar3 ! mean sgsw |
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| 120 | ENDIF |
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| 121 | IF ( particles(n)%speed_z > 0.0 ) THEN |
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| 122 | pts_value_l(0,12) = pts_value_l(0,12) + 1.0 ! # of upward moving prts |
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| 123 | pts_value_l(0,13) = pts_value_l(0,13) + & |
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| 124 | particles(n)%speed_z ! mean w upw. |
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| 125 | ELSE |
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| 126 | pts_value_l(0,14) = pts_value_l(0,14) + & |
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| 127 | particles(n)%speed_z ! mean w down |
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| 128 | ENDIF |
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| 129 | pts_value_l(0,15) = pts_value_l(0,15) + particles(n)%radius ! mean rad |
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| 130 | pts_value_l(0,16) = MIN( pts_value_l(0,16), particles(n)%radius ) ! minrad |
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| 131 | pts_value_l(0,17) = MAX( pts_value_l(0,17), particles(n)%radius ) ! maxrad |
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| 132 | pts_value_l(0,18) = number_of_particles |
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| 133 | pts_value_l(0,19) = number_of_particles |
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| 134 | |
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| 135 | ! |
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| 136 | !-- Repeat the same for the respective particle group |
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| 137 | IF ( number_of_particle_groups > 1 ) THEN |
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| 138 | j = particles(n)%group |
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| 139 | |
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| 140 | pts_value_l(j,1) = pts_value_l(j,1) + 1 |
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| 141 | pts_value_l(j,2) = pts_value_l(j,2) + & |
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| 142 | ( particles(n)%x - particles(n)%origin_x ) |
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| 143 | pts_value_l(j,3) = pts_value_l(j,3) + & |
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| 144 | ( particles(n)%y - particles(n)%origin_y ) |
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| 145 | pts_value_l(j,4) = pts_value_l(j,4) + & |
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| 146 | ( particles(n)%z - particles(n)%origin_z ) |
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| 147 | pts_value_l(j,5) = pts_value_l(j,5) + particles(n)%z |
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| 148 | pts_value_l(j,6) = pts_value_l(j,6) + particles(n)%speed_x |
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| 149 | pts_value_l(j,7) = pts_value_l(j,7) + particles(n)%speed_y |
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| 150 | pts_value_l(j,8) = pts_value_l(j,8) + particles(n)%speed_z |
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| 151 | IF ( .NOT. curvature_solution_effects ) THEN |
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| 152 | pts_value_l(j,9) = pts_value_l(j,9) + particles(n)%rvar1 |
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| 153 | pts_value_l(j,10) = pts_value_l(j,10) + particles(n)%rvar2 |
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| 154 | pts_value_l(j,11) = pts_value_l(j,11) + particles(n)%rvar3 |
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| 155 | ENDIF |
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| 156 | IF ( particles(n)%speed_z > 0.0 ) THEN |
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| 157 | pts_value_l(j,12) = pts_value_l(j,12) + 1.0 |
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| 158 | pts_value_l(j,13) = pts_value_l(j,13) + particles(n)%speed_z |
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| 159 | ELSE |
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| 160 | pts_value_l(j,14) = pts_value_l(j,14) + particles(n)%speed_z |
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| 161 | ENDIF |
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| 162 | pts_value_l(j,15) = pts_value_l(j,15) + particles(n)%radius |
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| 163 | pts_value_l(j,16) = MIN( pts_value(j,16), particles(n)%radius ) |
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| 164 | pts_value_l(j,17) = MAX( pts_value(j,17), particles(n)%radius ) |
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| 165 | pts_value_l(j,18) = pts_value_l(j,18) + 1.0 |
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| 166 | pts_value_l(j,19) = pts_value_l(j,19) + 1.0 |
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| 167 | |
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| 168 | ENDIF |
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| 169 | |
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| 170 | ENDDO |
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| 171 | |
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| 172 | #if defined( __parallel ) |
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| 173 | ! |
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| 174 | !-- Sum values of the subdomains |
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| 175 | inum = number_of_particle_groups + 1 |
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| 176 | |
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| 177 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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| 178 | CALL MPI_ALLREDUCE( pts_value_l(0,1), pts_value(0,1), 15*inum, MPI_REAL, & |
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| 179 | MPI_SUM, comm2d, ierr ) |
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| 180 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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| 181 | CALL MPI_ALLREDUCE( pts_value_l(0,16), pts_value(0,16), inum, MPI_REAL, & |
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| 182 | MPI_MIN, comm2d, ierr ) |
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| 183 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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| 184 | CALL MPI_ALLREDUCE( pts_value_l(0,17), pts_value(0,17), inum, MPI_REAL, & |
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| 185 | MPI_MAX, comm2d, ierr ) |
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| 186 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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| 187 | CALL MPI_ALLREDUCE( pts_value_l(0,18), pts_value(0,18), inum, MPI_REAL, & |
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| 188 | MPI_MAX, comm2d, ierr ) |
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| 189 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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| 190 | CALL MPI_ALLREDUCE( pts_value_l(0,19), pts_value(0,19), inum, MPI_REAL, & |
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| 191 | MPI_MIN, comm2d, ierr ) |
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| 192 | #else |
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| 193 | pts_value(:,1:19) = pts_value_l(:,1:19) |
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| 194 | #endif |
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| 195 | |
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| 196 | ! |
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| 197 | !-- Normalize the above calculated quantities (except min/max values) with the |
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| 198 | !-- total number of particles |
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| 199 | IF ( number_of_particle_groups > 1 ) THEN |
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| 200 | inum = number_of_particle_groups |
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| 201 | ELSE |
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| 202 | inum = 0 |
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| 203 | ENDIF |
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| 204 | |
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| 205 | DO j = 0, inum |
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| 206 | |
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| 207 | IF ( pts_value(j,1) > 0.0 ) THEN |
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| 208 | |
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| 209 | pts_value(j,2:15) = pts_value(j,2:15) / pts_value(j,1) |
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| 210 | IF ( pts_value(j,12) > 0.0 .AND. pts_value(j,12) < 1.0 ) THEN |
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| 211 | pts_value(j,13) = pts_value(j,13) / pts_value(j,12) |
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| 212 | pts_value(j,14) = pts_value(j,14) / ( 1.0 - pts_value(j,12) ) |
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| 213 | ELSEIF ( pts_value(j,12) == 0.0 ) THEN |
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| 214 | pts_value(j,13) = -1.0 |
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| 215 | ELSE |
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| 216 | pts_value(j,14) = -1.0 |
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| 217 | ENDIF |
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| 218 | |
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| 219 | ENDIF |
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| 220 | |
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| 221 | ENDDO |
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| 222 | |
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| 223 | ! |
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| 224 | !-- Calculate higher order moments of particle time series quantities, |
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| 225 | !-- seperately for each particle group (if there is more than one group) |
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| 226 | DO n = 1, number_of_particles |
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| 227 | |
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| 228 | pts_value_l(0,20) = pts_value_l(0,20) + ( particles(n)%x - & |
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| 229 | particles(n)%origin_x - pts_value(0,2) )**2 ! x*2 |
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| 230 | pts_value_l(0,21) = pts_value_l(0,21) + ( particles(n)%y - & |
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| 231 | particles(n)%origin_y - pts_value(0,3) )**2 ! y*2 |
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| 232 | pts_value_l(0,22) = pts_value_l(0,22) + ( particles(n)%z - & |
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| 233 | particles(n)%origin_z - pts_value(0,4) )**2 ! z*2 |
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| 234 | pts_value_l(0,23) = pts_value_l(0,23) + ( particles(n)%speed_x - & |
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| 235 | pts_value(0,6) )**2 ! u*2 |
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| 236 | pts_value_l(0,24) = pts_value_l(0,24) + ( particles(n)%speed_y - & |
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| 237 | pts_value(0,7) )**2 ! v*2 |
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| 238 | pts_value_l(0,25) = pts_value_l(0,25) + ( particles(n)%speed_z - & |
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| 239 | pts_value(0,8) )**2 ! w*2 |
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| 240 | IF ( .NOT. curvature_solution_effects ) THEN |
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| 241 | pts_value_l(0,26) = pts_value_l(0,26) + ( particles(n)%rvar1 - & |
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| 242 | pts_value(0,9) )**2 ! u"2 |
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| 243 | pts_value_l(0,27) = pts_value_l(0,27) + ( particles(n)%rvar2 - & |
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| 244 | pts_value(0,10) )**2 ! v"2 |
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| 245 | pts_value_l(0,28) = pts_value_l(0,28) + ( particles(n)%rvar3 - & |
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| 246 | pts_value(0,11) )**2 ! w"2 |
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| 247 | ENDIF |
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| 248 | ! |
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| 249 | !-- Repeat the same for the respective particle group |
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| 250 | IF ( number_of_particle_groups > 1 ) THEN |
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| 251 | j = particles(n)%group |
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| 252 | |
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| 253 | pts_value_l(j,20) = pts_value_l(j,20) + ( particles(n)%x - & |
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| 254 | particles(n)%origin_x - pts_value(j,2) )**2 |
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| 255 | pts_value_l(j,21) = pts_value_l(j,21) + ( particles(n)%y - & |
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| 256 | particles(n)%origin_y - pts_value(j,3) )**2 |
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| 257 | pts_value_l(j,22) = pts_value_l(j,22) + ( particles(n)%z - & |
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| 258 | particles(n)%origin_z - pts_value(j,4) )**2 |
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| 259 | pts_value_l(j,23) = pts_value_l(j,23) + ( particles(n)%speed_x - & |
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| 260 | pts_value(j,6) )**2 |
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| 261 | pts_value_l(j,24) = pts_value_l(j,24) + ( particles(n)%speed_y - & |
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| 262 | pts_value(j,7) )**2 |
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| 263 | pts_value_l(j,25) = pts_value_l(j,25) + ( particles(n)%speed_z - & |
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| 264 | pts_value(j,8) )**2 |
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| 265 | IF ( .NOT. curvature_solution_effects ) THEN |
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| 266 | pts_value_l(j,26) = pts_value_l(j,26) + ( particles(n)%rvar1 - & |
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| 267 | pts_value(j,9) )**2 |
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| 268 | pts_value_l(j,27) = pts_value_l(j,27) + ( particles(n)%rvar2 - & |
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| 269 | pts_value(j,10) )**2 |
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| 270 | pts_value_l(j,28) = pts_value_l(j,28) + ( particles(n)%rvar3 - & |
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| 271 | pts_value(j,11) )**2 |
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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 | pts_value_l(0,29) = ( number_of_particles - pts_value(0,1) / numprocs )**2 |
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| 278 | ! variance of particle numbers |
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| 279 | IF ( number_of_particle_groups > 1 ) THEN |
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| 280 | DO j = 1, number_of_particle_groups |
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| 281 | pts_value_l(j,29) = ( pts_value_l(j,1) - & |
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| 282 | pts_value(j,1) / numprocs )**2 |
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| 283 | ENDDO |
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| 284 | ENDIF |
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| 285 | |
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| 286 | #if defined( __parallel ) |
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| 287 | ! |
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| 288 | !-- Sum values of the subdomains |
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| 289 | inum = number_of_particle_groups + 1 |
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| 290 | |
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| 291 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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| 292 | CALL MPI_ALLREDUCE( pts_value_l(0,20), pts_value(0,20), inum*10, MPI_REAL, & |
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| 293 | MPI_SUM, comm2d, ierr ) |
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| 294 | #else |
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| 295 | pts_value(:,20:29) = pts_value_l(:,20:29) |
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| 296 | #endif |
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| 297 | |
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| 298 | ! |
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| 299 | !-- Normalize the above calculated quantities with the total number of |
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| 300 | !-- particles |
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| 301 | IF ( number_of_particle_groups > 1 ) THEN |
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| 302 | inum = number_of_particle_groups |
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| 303 | ELSE |
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| 304 | inum = 0 |
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| 305 | ENDIF |
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| 306 | |
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| 307 | DO j = 0, inum |
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| 308 | |
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| 309 | IF ( pts_value(j,1) > 0.0 ) THEN |
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| 310 | pts_value(j,20:28) = pts_value(j,20:28) / pts_value(j,1) |
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| 311 | ENDIF |
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| 312 | pts_value(j,29) = pts_value(j,29) / numprocs |
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| 313 | |
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| 314 | ENDDO |
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| 315 | |
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| 316 | #if defined( __netcdf ) |
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| 317 | ! |
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| 318 | !-- Output particle time series quantities in NetCDF format |
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| 319 | IF ( myid == 0 .AND. netcdf_output ) THEN |
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| 320 | DO j = 0, inum |
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| 321 | DO i = 1, dopts_num |
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| 322 | nc_stat = NF90_PUT_VAR( id_set_pts, id_var_dopts(i,j), & |
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| 323 | (/ pts_value(j,i) /), & |
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| 324 | start = (/ dopts_time_count /), & |
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| 325 | count = (/ 1 /) ) |
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| 326 | CALL handle_netcdf_error( 'data_output_ptseries', 392 ) |
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| 327 | ENDDO |
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| 328 | ENDDO |
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| 329 | ENDIF |
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| 330 | #endif |
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| 331 | |
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| 332 | DEALLOCATE( pts_value, pts_value_l ) |
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| 333 | |
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| 334 | CALL cpu_log( log_point(36), 'data_output_ptseries','stop', 'nobarrier' ) |
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| 335 | |
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| 336 | END SUBROUTINE data_output_ptseries |
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