[1] | 1 | SUBROUTINE data_output_ptseries |
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| 2 | |
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[1036] | 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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[1310] | 17 | ! Copyright 1997-2014 Leibniz Universitaet Hannover |
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[1036] | 18 | !--------------------------------------------------------------------------------! |
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| 19 | ! |
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[263] | 20 | ! Current revisions: |
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[1] | 21 | ! ----------------- |
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[1329] | 22 | ! |
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[1354] | 23 | ! |
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[1321] | 24 | ! Former revisions: |
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| 25 | ! ----------------- |
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| 26 | ! $Id: data_output_ptseries.f90 1354 2014-04-08 15:22:57Z witha $ |
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| 27 | ! |
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[1354] | 28 | ! 1353 2014-04-08 15:21:23Z heinze |
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| 29 | ! REAL constants provided with KIND-attribute |
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| 30 | ! |
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[1329] | 31 | ! 1327 2014-03-21 11:00:16Z raasch |
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| 32 | ! -netcdf output queries |
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| 33 | ! |
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[1321] | 34 | ! 1320 2014-03-20 08:40:49Z raasch |
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[1320] | 35 | ! ONLY-attribute added to USE-statements, |
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| 36 | ! kind-parameters added to all INTEGER and REAL declaration statements, |
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| 37 | ! kinds are defined in new module kinds, |
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| 38 | ! revision history before 2012 removed, |
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| 39 | ! comment fields (!:) to be used for variable explanations added to |
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| 40 | ! all variable declaration statements |
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[1] | 41 | ! |
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[1319] | 42 | ! 1318 2014-03-17 13:35:16Z raasch |
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| 43 | ! barrier argument removed from cpu_log, |
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| 44 | ! module interfaces removed |
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| 45 | ! |
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[1037] | 46 | ! 1036 2012-10-22 13:43:42Z raasch |
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| 47 | ! code put under GPL (PALM 3.9) |
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| 48 | ! |
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[826] | 49 | ! 825 2012-02-19 03:03:44Z raasch |
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| 50 | ! mean/minimum/maximum particle radius added as output quantity, |
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| 51 | ! particle attributes speed_x|y|z_sgs renamed rvar1|2|3 |
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| 52 | ! |
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[1] | 53 | ! Revision 1.1 2006/08/04 14:24:18 raasch |
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| 54 | ! Initial revision |
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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 | ! Output of particle data timeseries in NetCDF format. |
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| 60 | !------------------------------------------------------------------------------! |
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| 61 | |
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[1320] | 62 | USE cloud_parameters, & |
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| 63 | ONLY: curvature_solution_effects |
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| 64 | |
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| 65 | USE control_parameters, & |
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[1327] | 66 | ONLY: dopts_time_count, time_since_reference_point |
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[1320] | 67 | |
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| 68 | USE cpulog, & |
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| 69 | ONLY: cpu_log, log_point |
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| 70 | |
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| 71 | USE indices, & |
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| 72 | ONLY: |
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| 73 | |
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| 74 | USE kinds |
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| 75 | |
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[1] | 76 | USE netcdf_control |
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[1320] | 77 | |
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| 78 | USE particle_attributes, & |
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| 79 | ONLY: number_of_particles, number_of_particle_groups, particles |
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| 80 | |
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[1] | 81 | USE pegrid |
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| 82 | |
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| 83 | IMPLICIT NONE |
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| 84 | |
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| 85 | |
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[1320] | 86 | INTEGER(iwp) :: i !: |
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| 87 | INTEGER(iwp) :: inum !: |
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| 88 | INTEGER(iwp) :: j !: |
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| 89 | INTEGER(iwp) :: n !: |
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[1] | 90 | |
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[1320] | 91 | REAL(wp), DIMENSION(:,:), ALLOCATABLE :: pts_value !: |
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| 92 | REAL(wp), DIMENSION(:,:), ALLOCATABLE :: pts_value_l !: |
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[1] | 93 | |
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| 94 | |
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| 95 | CALL cpu_log( log_point(36), 'data_output_ptseries', 'start' ) |
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| 96 | |
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[1327] | 97 | IF ( myid == 0 ) THEN |
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[1] | 98 | ! |
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| 99 | !-- Open file for time series output in NetCDF format |
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| 100 | dopts_time_count = dopts_time_count + 1 |
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| 101 | CALL check_open( 109 ) |
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| 102 | #if defined( __netcdf ) |
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| 103 | ! |
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| 104 | !-- Update the particle time series time axis |
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[291] | 105 | nc_stat = NF90_PUT_VAR( id_set_pts, id_var_time_pts, & |
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| 106 | (/ time_since_reference_point /), & |
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[1] | 107 | start = (/ dopts_time_count /), count = (/ 1 /) ) |
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[263] | 108 | CALL handle_netcdf_error( 'data_output_ptseries', 391 ) |
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[1] | 109 | #endif |
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| 110 | |
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| 111 | ENDIF |
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| 112 | |
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[825] | 113 | ALLOCATE( pts_value(0:number_of_particle_groups,dopts_num), & |
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| 114 | pts_value_l(0:number_of_particle_groups,dopts_num) ) |
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| 115 | |
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[1353] | 116 | pts_value_l = 0.0_wp |
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| 117 | pts_value_l(:,16) = 9999999.9_wp ! for calculation of minimum radius |
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[1] | 118 | |
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| 119 | ! |
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| 120 | !-- Calculate or collect the particle time series quantities for all particles |
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| 121 | !-- and seperately for each particle group (if there is more than one group) |
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| 122 | DO n = 1, number_of_particles |
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| 123 | |
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| 124 | pts_value_l(0,1) = number_of_particles ! total # of particles |
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| 125 | pts_value_l(0,2) = pts_value_l(0,2) + & |
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| 126 | ( particles(n)%x - particles(n)%origin_x ) ! mean x |
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| 127 | pts_value_l(0,3) = pts_value_l(0,3) + & |
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| 128 | ( particles(n)%y - particles(n)%origin_y ) ! mean y |
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| 129 | pts_value_l(0,4) = pts_value_l(0,4) + & |
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| 130 | ( particles(n)%z - particles(n)%origin_z ) ! mean z |
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| 131 | pts_value_l(0,5) = pts_value_l(0,5) + particles(n)%z ! mean z (absolute) |
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| 132 | pts_value_l(0,6) = pts_value_l(0,6) + particles(n)%speed_x ! mean u |
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| 133 | pts_value_l(0,7) = pts_value_l(0,7) + particles(n)%speed_y ! mean v |
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| 134 | pts_value_l(0,8) = pts_value_l(0,8) + particles(n)%speed_z ! mean w |
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[825] | 135 | IF ( .NOT. curvature_solution_effects ) THEN |
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| 136 | pts_value_l(0,9) = pts_value_l(0,9) + particles(n)%rvar1 ! mean sgsu |
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| 137 | pts_value_l(0,10) = pts_value_l(0,10) + particles(n)%rvar2 ! mean sgsv |
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| 138 | pts_value_l(0,11) = pts_value_l(0,11) + particles(n)%rvar3 ! mean sgsw |
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| 139 | ENDIF |
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[1353] | 140 | IF ( particles(n)%speed_z > 0.0_wp ) THEN |
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| 141 | pts_value_l(0,12) = pts_value_l(0,12) + 1.0_wp ! # of upward moving prts |
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[1] | 142 | pts_value_l(0,13) = pts_value_l(0,13) + & |
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| 143 | particles(n)%speed_z ! mean w upw. |
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| 144 | ELSE |
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| 145 | pts_value_l(0,14) = pts_value_l(0,14) + & |
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| 146 | particles(n)%speed_z ! mean w down |
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| 147 | ENDIF |
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[825] | 148 | pts_value_l(0,15) = pts_value_l(0,15) + particles(n)%radius ! mean rad |
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| 149 | pts_value_l(0,16) = MIN( pts_value_l(0,16), particles(n)%radius ) ! minrad |
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| 150 | pts_value_l(0,17) = MAX( pts_value_l(0,17), particles(n)%radius ) ! maxrad |
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| 151 | pts_value_l(0,18) = number_of_particles |
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| 152 | pts_value_l(0,19) = number_of_particles |
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[1] | 153 | |
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| 154 | ! |
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| 155 | !-- Repeat the same for the respective particle group |
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| 156 | IF ( number_of_particle_groups > 1 ) THEN |
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| 157 | j = particles(n)%group |
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| 158 | |
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| 159 | pts_value_l(j,1) = pts_value_l(j,1) + 1 |
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| 160 | pts_value_l(j,2) = pts_value_l(j,2) + & |
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| 161 | ( particles(n)%x - particles(n)%origin_x ) |
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| 162 | pts_value_l(j,3) = pts_value_l(j,3) + & |
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| 163 | ( particles(n)%y - particles(n)%origin_y ) |
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| 164 | pts_value_l(j,4) = pts_value_l(j,4) + & |
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| 165 | ( particles(n)%z - particles(n)%origin_z ) |
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| 166 | pts_value_l(j,5) = pts_value_l(j,5) + particles(n)%z |
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| 167 | pts_value_l(j,6) = pts_value_l(j,6) + particles(n)%speed_x |
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| 168 | pts_value_l(j,7) = pts_value_l(j,7) + particles(n)%speed_y |
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| 169 | pts_value_l(j,8) = pts_value_l(j,8) + particles(n)%speed_z |
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[825] | 170 | IF ( .NOT. curvature_solution_effects ) THEN |
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| 171 | pts_value_l(j,9) = pts_value_l(j,9) + particles(n)%rvar1 |
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| 172 | pts_value_l(j,10) = pts_value_l(j,10) + particles(n)%rvar2 |
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| 173 | pts_value_l(j,11) = pts_value_l(j,11) + particles(n)%rvar3 |
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| 174 | ENDIF |
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[1353] | 175 | IF ( particles(n)%speed_z > 0.0_wp ) THEN |
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| 176 | pts_value_l(j,12) = pts_value_l(j,12) + 1.0_wp |
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[1] | 177 | pts_value_l(j,13) = pts_value_l(j,13) + particles(n)%speed_z |
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| 178 | ELSE |
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| 179 | pts_value_l(j,14) = pts_value_l(j,14) + particles(n)%speed_z |
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| 180 | ENDIF |
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[824] | 181 | pts_value_l(j,15) = pts_value_l(j,15) + particles(n)%radius |
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[825] | 182 | pts_value_l(j,16) = MIN( pts_value(j,16), particles(n)%radius ) |
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| 183 | pts_value_l(j,17) = MAX( pts_value(j,17), particles(n)%radius ) |
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[1353] | 184 | pts_value_l(j,18) = pts_value_l(j,18) + 1.0_wp |
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| 185 | pts_value_l(j,19) = pts_value_l(j,19) + 1.0_wp |
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[1] | 186 | |
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| 187 | ENDIF |
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| 188 | |
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| 189 | ENDDO |
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| 190 | |
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| 191 | #if defined( __parallel ) |
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| 192 | ! |
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| 193 | !-- Sum values of the subdomains |
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| 194 | inum = number_of_particle_groups + 1 |
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| 195 | |
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[622] | 196 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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[824] | 197 | CALL MPI_ALLREDUCE( pts_value_l(0,1), pts_value(0,1), 15*inum, MPI_REAL, & |
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[1] | 198 | MPI_SUM, comm2d, ierr ) |
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[622] | 199 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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[824] | 200 | CALL MPI_ALLREDUCE( pts_value_l(0,16), pts_value(0,16), inum, MPI_REAL, & |
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[825] | 201 | MPI_MIN, comm2d, ierr ) |
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| 202 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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| 203 | CALL MPI_ALLREDUCE( pts_value_l(0,17), pts_value(0,17), inum, MPI_REAL, & |
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[1] | 204 | MPI_MAX, comm2d, ierr ) |
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[622] | 205 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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[825] | 206 | CALL MPI_ALLREDUCE( pts_value_l(0,18), pts_value(0,18), inum, MPI_REAL, & |
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| 207 | MPI_MAX, comm2d, ierr ) |
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| 208 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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| 209 | CALL MPI_ALLREDUCE( pts_value_l(0,19), pts_value(0,19), inum, MPI_REAL, & |
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[1] | 210 | MPI_MIN, comm2d, ierr ) |
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| 211 | #else |
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[825] | 212 | pts_value(:,1:19) = pts_value_l(:,1:19) |
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[1] | 213 | #endif |
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| 214 | |
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| 215 | ! |
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[825] | 216 | !-- Normalize the above calculated quantities (except min/max values) with the |
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| 217 | !-- total number of particles |
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[1] | 218 | IF ( number_of_particle_groups > 1 ) THEN |
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| 219 | inum = number_of_particle_groups |
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| 220 | ELSE |
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| 221 | inum = 0 |
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| 222 | ENDIF |
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| 223 | |
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| 224 | DO j = 0, inum |
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| 225 | |
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[1353] | 226 | IF ( pts_value(j,1) > 0.0_wp ) THEN |
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[1] | 227 | |
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[824] | 228 | pts_value(j,2:15) = pts_value(j,2:15) / pts_value(j,1) |
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[1353] | 229 | IF ( pts_value(j,12) > 0.0_wp .AND. pts_value(j,12) < 1.0_wp ) THEN |
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[1] | 230 | pts_value(j,13) = pts_value(j,13) / pts_value(j,12) |
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[1353] | 231 | pts_value(j,14) = pts_value(j,14) / ( 1.0_wp - pts_value(j,12) ) |
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| 232 | ELSEIF ( pts_value(j,12) == 0.0_wp ) THEN |
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| 233 | pts_value(j,13) = -1.0_wp |
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[1] | 234 | ELSE |
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[1353] | 235 | pts_value(j,14) = -1.0_wp |
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[1] | 236 | ENDIF |
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| 237 | |
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| 238 | ENDIF |
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| 239 | |
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| 240 | ENDDO |
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| 241 | |
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| 242 | ! |
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| 243 | !-- Calculate higher order moments of particle time series quantities, |
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| 244 | !-- seperately for each particle group (if there is more than one group) |
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| 245 | DO n = 1, number_of_particles |
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| 246 | |
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[825] | 247 | pts_value_l(0,20) = pts_value_l(0,20) + ( particles(n)%x - & |
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[1] | 248 | particles(n)%origin_x - pts_value(0,2) )**2 ! x*2 |
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[825] | 249 | pts_value_l(0,21) = pts_value_l(0,21) + ( particles(n)%y - & |
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[1] | 250 | particles(n)%origin_y - pts_value(0,3) )**2 ! y*2 |
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[825] | 251 | pts_value_l(0,22) = pts_value_l(0,22) + ( particles(n)%z - & |
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[1] | 252 | particles(n)%origin_z - pts_value(0,4) )**2 ! z*2 |
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[825] | 253 | pts_value_l(0,23) = pts_value_l(0,23) + ( particles(n)%speed_x - & |
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| 254 | pts_value(0,6) )**2 ! u*2 |
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| 255 | pts_value_l(0,24) = pts_value_l(0,24) + ( particles(n)%speed_y - & |
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| 256 | pts_value(0,7) )**2 ! v*2 |
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| 257 | pts_value_l(0,25) = pts_value_l(0,25) + ( particles(n)%speed_z - & |
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| 258 | pts_value(0,8) )**2 ! w*2 |
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| 259 | IF ( .NOT. curvature_solution_effects ) THEN |
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| 260 | pts_value_l(0,26) = pts_value_l(0,26) + ( particles(n)%rvar1 - & |
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| 261 | pts_value(0,9) )**2 ! u"2 |
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| 262 | pts_value_l(0,27) = pts_value_l(0,27) + ( particles(n)%rvar2 - & |
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| 263 | pts_value(0,10) )**2 ! v"2 |
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| 264 | pts_value_l(0,28) = pts_value_l(0,28) + ( particles(n)%rvar3 - & |
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| 265 | pts_value(0,11) )**2 ! w"2 |
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| 266 | ENDIF |
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[1] | 267 | ! |
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| 268 | !-- Repeat the same for the respective particle group |
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| 269 | IF ( number_of_particle_groups > 1 ) THEN |
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| 270 | j = particles(n)%group |
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| 271 | |
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[825] | 272 | pts_value_l(j,20) = pts_value_l(j,20) + ( particles(n)%x - & |
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[1] | 273 | particles(n)%origin_x - pts_value(j,2) )**2 |
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[825] | 274 | pts_value_l(j,21) = pts_value_l(j,21) + ( particles(n)%y - & |
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[1] | 275 | particles(n)%origin_y - pts_value(j,3) )**2 |
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[825] | 276 | pts_value_l(j,22) = pts_value_l(j,22) + ( particles(n)%z - & |
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[1] | 277 | particles(n)%origin_z - pts_value(j,4) )**2 |
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[825] | 278 | pts_value_l(j,23) = pts_value_l(j,23) + ( particles(n)%speed_x - & |
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| 279 | pts_value(j,6) )**2 |
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| 280 | pts_value_l(j,24) = pts_value_l(j,24) + ( particles(n)%speed_y - & |
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| 281 | pts_value(j,7) )**2 |
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| 282 | pts_value_l(j,25) = pts_value_l(j,25) + ( particles(n)%speed_z - & |
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| 283 | pts_value(j,8) )**2 |
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| 284 | IF ( .NOT. curvature_solution_effects ) THEN |
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| 285 | pts_value_l(j,26) = pts_value_l(j,26) + ( particles(n)%rvar1 - & |
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| 286 | pts_value(j,9) )**2 |
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| 287 | pts_value_l(j,27) = pts_value_l(j,27) + ( particles(n)%rvar2 - & |
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| 288 | pts_value(j,10) )**2 |
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| 289 | pts_value_l(j,28) = pts_value_l(j,28) + ( particles(n)%rvar3 - & |
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| 290 | pts_value(j,11) )**2 |
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| 291 | ENDIF |
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[1] | 292 | ENDIF |
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| 293 | |
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| 294 | ENDDO |
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| 295 | |
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[825] | 296 | pts_value_l(0,29) = ( number_of_particles - pts_value(0,1) / numprocs )**2 |
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[1] | 297 | ! variance of particle numbers |
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| 298 | IF ( number_of_particle_groups > 1 ) THEN |
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| 299 | DO j = 1, number_of_particle_groups |
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[825] | 300 | pts_value_l(j,29) = ( pts_value_l(j,1) - & |
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[1] | 301 | pts_value(j,1) / numprocs )**2 |
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| 302 | ENDDO |
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| 303 | ENDIF |
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| 304 | |
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| 305 | #if defined( __parallel ) |
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| 306 | ! |
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| 307 | !-- Sum values of the subdomains |
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| 308 | inum = number_of_particle_groups + 1 |
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| 309 | |
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[622] | 310 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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[825] | 311 | CALL MPI_ALLREDUCE( pts_value_l(0,20), pts_value(0,20), inum*10, MPI_REAL, & |
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[1] | 312 | MPI_SUM, comm2d, ierr ) |
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| 313 | #else |
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[825] | 314 | pts_value(:,20:29) = pts_value_l(:,20:29) |
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[1] | 315 | #endif |
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| 316 | |
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| 317 | ! |
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| 318 | !-- Normalize the above calculated quantities with the total number of |
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| 319 | !-- particles |
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| 320 | IF ( number_of_particle_groups > 1 ) THEN |
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| 321 | inum = number_of_particle_groups |
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| 322 | ELSE |
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| 323 | inum = 0 |
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| 324 | ENDIF |
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| 325 | |
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| 326 | DO j = 0, inum |
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| 327 | |
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[1353] | 328 | IF ( pts_value(j,1) > 0.0_wp ) THEN |
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[825] | 329 | pts_value(j,20:28) = pts_value(j,20:28) / pts_value(j,1) |
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[1] | 330 | ENDIF |
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[825] | 331 | pts_value(j,29) = pts_value(j,29) / numprocs |
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[1] | 332 | |
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| 333 | ENDDO |
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| 334 | |
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| 335 | #if defined( __netcdf ) |
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| 336 | ! |
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| 337 | !-- Output particle time series quantities in NetCDF format |
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[1327] | 338 | IF ( myid == 0 ) THEN |
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[1] | 339 | DO j = 0, inum |
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| 340 | DO i = 1, dopts_num |
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| 341 | nc_stat = NF90_PUT_VAR( id_set_pts, id_var_dopts(i,j), & |
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| 342 | (/ pts_value(j,i) /), & |
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| 343 | start = (/ dopts_time_count /), & |
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| 344 | count = (/ 1 /) ) |
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[263] | 345 | CALL handle_netcdf_error( 'data_output_ptseries', 392 ) |
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[1] | 346 | ENDDO |
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| 347 | ENDDO |
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| 348 | ENDIF |
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| 349 | #endif |
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| 350 | |
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[825] | 351 | DEALLOCATE( pts_value, pts_value_l ) |
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| 352 | |
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[1318] | 353 | CALL cpu_log( log_point(36), 'data_output_ptseries', 'stop' ) |
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[1] | 354 | |
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| 355 | END SUBROUTINE data_output_ptseries |
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