[1] | 1 | SUBROUTINE data_output_ptseries |
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| 2 | |
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| 3 | !------------------------------------------------------------------------------! |
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[263] | 4 | ! Current revisions: |
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[1] | 5 | ! ----------------- |
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[826] | 6 | ! |
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[1] | 7 | ! |
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| 8 | ! Former revisions: |
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| 9 | ! ----------------- |
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[3] | 10 | ! $Id: data_output_ptseries.f90 826 2012-02-19 03:41:34Z hoffmann $ |
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[77] | 11 | ! |
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[826] | 12 | ! 825 2012-02-19 03:03:44Z raasch |
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| 13 | ! mean/minimum/maximum particle radius added as output quantity, |
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| 14 | ! particle attributes speed_x|y|z_sgs renamed rvar1|2|3 |
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| 15 | ! |
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[623] | 16 | ! 622 2010-12-10 08:08:13Z raasch |
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| 17 | ! optional barriers included in order to speed up collective operations |
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| 18 | ! |
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[392] | 19 | ! 291 2009-04-16 12:07:26Z raasch |
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| 20 | ! simulated_time in NetCDF output replaced by time_since_reference_point. |
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| 21 | ! Output of NetCDF messages with aid of message handling routine. |
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| 22 | ! |
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[77] | 23 | ! 60 2007-03-11 11:50:04Z raasch |
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| 24 | ! Particles-package is now part of the default code. |
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| 25 | ! |
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[3] | 26 | ! RCS Log replace by Id keyword, revision history cleaned up |
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| 27 | ! |
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[1] | 28 | ! Revision 1.2 2006/08/22 13:51:13 raasch |
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| 29 | ! Seperate output for particle groups |
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| 30 | ! |
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| 31 | ! Revision 1.1 2006/08/04 14:24:18 raasch |
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| 32 | ! Initial revision |
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| 33 | ! |
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| 34 | ! |
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| 35 | ! Description: |
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| 36 | ! ------------ |
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| 37 | ! Output of particle data timeseries in NetCDF format. |
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| 38 | !------------------------------------------------------------------------------! |
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| 39 | |
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[825] | 40 | USE cloud_parameters |
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[1] | 41 | USE control_parameters |
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| 42 | USE cpulog |
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| 43 | USE indices |
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| 44 | USE interfaces |
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| 45 | USE netcdf_control |
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| 46 | USE particle_attributes |
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| 47 | USE pegrid |
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| 48 | |
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| 49 | IMPLICIT NONE |
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| 50 | |
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| 51 | |
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| 52 | INTEGER :: i, inum, j, n |
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| 53 | |
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[825] | 54 | REAL, DIMENSION(:,:), ALLOCATABLE :: pts_value, pts_value_l |
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[1] | 55 | |
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| 56 | |
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| 57 | CALL cpu_log( log_point(36), 'data_output_ptseries', 'start' ) |
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| 58 | |
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| 59 | IF ( myid == 0 .AND. netcdf_output ) THEN |
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| 60 | ! |
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| 61 | !-- Open file for time series output in NetCDF format |
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| 62 | dopts_time_count = dopts_time_count + 1 |
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| 63 | CALL check_open( 109 ) |
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| 64 | #if defined( __netcdf ) |
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| 65 | ! |
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| 66 | !-- Update the particle time series time axis |
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[291] | 67 | nc_stat = NF90_PUT_VAR( id_set_pts, id_var_time_pts, & |
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| 68 | (/ time_since_reference_point /), & |
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[1] | 69 | start = (/ dopts_time_count /), count = (/ 1 /) ) |
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[263] | 70 | CALL handle_netcdf_error( 'data_output_ptseries', 391 ) |
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[1] | 71 | #endif |
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| 72 | |
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| 73 | ENDIF |
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| 74 | |
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[825] | 75 | ALLOCATE( pts_value(0:number_of_particle_groups,dopts_num), & |
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| 76 | pts_value_l(0:number_of_particle_groups,dopts_num) ) |
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| 77 | |
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[1] | 78 | pts_value_l = 0.0 |
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[825] | 79 | pts_value_l(:,16) = 9999999.9 ! for calculation of minimum radius |
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[1] | 80 | |
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| 81 | ! |
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| 82 | !-- Calculate or collect the particle time series quantities for all particles |
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| 83 | !-- and seperately for each particle group (if there is more than one group) |
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| 84 | DO n = 1, number_of_particles |
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| 85 | |
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| 86 | pts_value_l(0,1) = number_of_particles ! total # of particles |
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| 87 | pts_value_l(0,2) = pts_value_l(0,2) + & |
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| 88 | ( particles(n)%x - particles(n)%origin_x ) ! mean x |
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| 89 | pts_value_l(0,3) = pts_value_l(0,3) + & |
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| 90 | ( particles(n)%y - particles(n)%origin_y ) ! mean y |
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| 91 | pts_value_l(0,4) = pts_value_l(0,4) + & |
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| 92 | ( particles(n)%z - particles(n)%origin_z ) ! mean z |
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| 93 | pts_value_l(0,5) = pts_value_l(0,5) + particles(n)%z ! mean z (absolute) |
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| 94 | pts_value_l(0,6) = pts_value_l(0,6) + particles(n)%speed_x ! mean u |
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| 95 | pts_value_l(0,7) = pts_value_l(0,7) + particles(n)%speed_y ! mean v |
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| 96 | pts_value_l(0,8) = pts_value_l(0,8) + particles(n)%speed_z ! mean w |
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[825] | 97 | IF ( .NOT. curvature_solution_effects ) THEN |
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| 98 | pts_value_l(0,9) = pts_value_l(0,9) + particles(n)%rvar1 ! mean sgsu |
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| 99 | pts_value_l(0,10) = pts_value_l(0,10) + particles(n)%rvar2 ! mean sgsv |
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| 100 | pts_value_l(0,11) = pts_value_l(0,11) + particles(n)%rvar3 ! mean sgsw |
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| 101 | ENDIF |
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[1] | 102 | IF ( particles(n)%speed_z > 0.0 ) THEN |
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| 103 | pts_value_l(0,12) = pts_value_l(0,12) + 1.0 ! # of upward moving prts |
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| 104 | pts_value_l(0,13) = pts_value_l(0,13) + & |
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| 105 | particles(n)%speed_z ! mean w upw. |
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| 106 | ELSE |
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| 107 | pts_value_l(0,14) = pts_value_l(0,14) + & |
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| 108 | particles(n)%speed_z ! mean w down |
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| 109 | ENDIF |
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[825] | 110 | pts_value_l(0,15) = pts_value_l(0,15) + particles(n)%radius ! mean rad |
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| 111 | pts_value_l(0,16) = MIN( pts_value_l(0,16), particles(n)%radius ) ! minrad |
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| 112 | pts_value_l(0,17) = MAX( pts_value_l(0,17), particles(n)%radius ) ! maxrad |
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| 113 | pts_value_l(0,18) = number_of_particles |
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| 114 | pts_value_l(0,19) = number_of_particles |
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[1] | 115 | |
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| 116 | ! |
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| 117 | !-- Repeat the same for the respective particle group |
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| 118 | IF ( number_of_particle_groups > 1 ) THEN |
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| 119 | j = particles(n)%group |
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| 120 | |
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| 121 | pts_value_l(j,1) = pts_value_l(j,1) + 1 |
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| 122 | pts_value_l(j,2) = pts_value_l(j,2) + & |
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| 123 | ( particles(n)%x - particles(n)%origin_x ) |
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| 124 | pts_value_l(j,3) = pts_value_l(j,3) + & |
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| 125 | ( particles(n)%y - particles(n)%origin_y ) |
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| 126 | pts_value_l(j,4) = pts_value_l(j,4) + & |
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| 127 | ( particles(n)%z - particles(n)%origin_z ) |
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| 128 | pts_value_l(j,5) = pts_value_l(j,5) + particles(n)%z |
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| 129 | pts_value_l(j,6) = pts_value_l(j,6) + particles(n)%speed_x |
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| 130 | pts_value_l(j,7) = pts_value_l(j,7) + particles(n)%speed_y |
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| 131 | pts_value_l(j,8) = pts_value_l(j,8) + particles(n)%speed_z |
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[825] | 132 | IF ( .NOT. curvature_solution_effects ) THEN |
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| 133 | pts_value_l(j,9) = pts_value_l(j,9) + particles(n)%rvar1 |
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| 134 | pts_value_l(j,10) = pts_value_l(j,10) + particles(n)%rvar2 |
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| 135 | pts_value_l(j,11) = pts_value_l(j,11) + particles(n)%rvar3 |
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| 136 | ENDIF |
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[1] | 137 | IF ( particles(n)%speed_z > 0.0 ) THEN |
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| 138 | pts_value_l(j,12) = pts_value_l(j,12) + 1.0 |
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| 139 | pts_value_l(j,13) = pts_value_l(j,13) + particles(n)%speed_z |
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| 140 | ELSE |
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| 141 | pts_value_l(j,14) = pts_value_l(j,14) + particles(n)%speed_z |
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| 142 | ENDIF |
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[824] | 143 | pts_value_l(j,15) = pts_value_l(j,15) + particles(n)%radius |
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[825] | 144 | pts_value_l(j,16) = MIN( pts_value(j,16), particles(n)%radius ) |
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| 145 | pts_value_l(j,17) = MAX( pts_value(j,17), particles(n)%radius ) |
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| 146 | pts_value_l(j,18) = pts_value_l(j,18) + 1.0 |
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| 147 | pts_value_l(j,19) = pts_value_l(j,19) + 1.0 |
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[1] | 148 | |
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| 149 | ENDIF |
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| 150 | |
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| 151 | ENDDO |
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| 152 | |
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| 153 | #if defined( __parallel ) |
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| 154 | ! |
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| 155 | !-- Sum values of the subdomains |
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| 156 | inum = number_of_particle_groups + 1 |
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| 157 | |
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[622] | 158 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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[824] | 159 | CALL MPI_ALLREDUCE( pts_value_l(0,1), pts_value(0,1), 15*inum, MPI_REAL, & |
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[1] | 160 | MPI_SUM, comm2d, ierr ) |
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[622] | 161 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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[824] | 162 | CALL MPI_ALLREDUCE( pts_value_l(0,16), pts_value(0,16), inum, MPI_REAL, & |
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[825] | 163 | MPI_MIN, comm2d, ierr ) |
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| 164 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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| 165 | CALL MPI_ALLREDUCE( pts_value_l(0,17), pts_value(0,17), inum, MPI_REAL, & |
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[1] | 166 | MPI_MAX, comm2d, ierr ) |
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[622] | 167 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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[825] | 168 | CALL MPI_ALLREDUCE( pts_value_l(0,18), pts_value(0,18), inum, MPI_REAL, & |
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| 169 | MPI_MAX, comm2d, ierr ) |
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| 170 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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| 171 | CALL MPI_ALLREDUCE( pts_value_l(0,19), pts_value(0,19), inum, MPI_REAL, & |
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[1] | 172 | MPI_MIN, comm2d, ierr ) |
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| 173 | #else |
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[825] | 174 | pts_value(:,1:19) = pts_value_l(:,1:19) |
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[1] | 175 | #endif |
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| 176 | |
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| 177 | ! |
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[825] | 178 | !-- Normalize the above calculated quantities (except min/max values) with the |
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| 179 | !-- total number of particles |
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[1] | 180 | IF ( number_of_particle_groups > 1 ) THEN |
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| 181 | inum = number_of_particle_groups |
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| 182 | ELSE |
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| 183 | inum = 0 |
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| 184 | ENDIF |
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| 185 | |
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| 186 | DO j = 0, inum |
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| 187 | |
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| 188 | IF ( pts_value(j,1) > 0.0 ) THEN |
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| 189 | |
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[824] | 190 | pts_value(j,2:15) = pts_value(j,2:15) / pts_value(j,1) |
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[1] | 191 | IF ( pts_value(j,12) > 0.0 .AND. pts_value(j,12) < 1.0 ) THEN |
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| 192 | pts_value(j,13) = pts_value(j,13) / pts_value(j,12) |
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| 193 | pts_value(j,14) = pts_value(j,14) / ( 1.0 - pts_value(j,12) ) |
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| 194 | ELSEIF ( pts_value(j,12) == 0.0 ) THEN |
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| 195 | pts_value(j,13) = -1.0 |
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| 196 | ELSE |
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| 197 | pts_value(j,14) = -1.0 |
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| 198 | ENDIF |
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| 199 | |
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| 200 | ENDIF |
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| 201 | |
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| 202 | ENDDO |
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| 203 | |
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| 204 | ! |
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| 205 | !-- Calculate higher order moments of particle time series quantities, |
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| 206 | !-- seperately for each particle group (if there is more than one group) |
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| 207 | DO n = 1, number_of_particles |
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| 208 | |
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[825] | 209 | pts_value_l(0,20) = pts_value_l(0,20) + ( particles(n)%x - & |
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[1] | 210 | particles(n)%origin_x - pts_value(0,2) )**2 ! x*2 |
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[825] | 211 | pts_value_l(0,21) = pts_value_l(0,21) + ( particles(n)%y - & |
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[1] | 212 | particles(n)%origin_y - pts_value(0,3) )**2 ! y*2 |
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[825] | 213 | pts_value_l(0,22) = pts_value_l(0,22) + ( particles(n)%z - & |
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[1] | 214 | particles(n)%origin_z - pts_value(0,4) )**2 ! z*2 |
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[825] | 215 | pts_value_l(0,23) = pts_value_l(0,23) + ( particles(n)%speed_x - & |
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| 216 | pts_value(0,6) )**2 ! u*2 |
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| 217 | pts_value_l(0,24) = pts_value_l(0,24) + ( particles(n)%speed_y - & |
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| 218 | pts_value(0,7) )**2 ! v*2 |
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| 219 | pts_value_l(0,25) = pts_value_l(0,25) + ( particles(n)%speed_z - & |
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| 220 | pts_value(0,8) )**2 ! w*2 |
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| 221 | IF ( .NOT. curvature_solution_effects ) THEN |
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| 222 | pts_value_l(0,26) = pts_value_l(0,26) + ( particles(n)%rvar1 - & |
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| 223 | pts_value(0,9) )**2 ! u"2 |
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| 224 | pts_value_l(0,27) = pts_value_l(0,27) + ( particles(n)%rvar2 - & |
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| 225 | pts_value(0,10) )**2 ! v"2 |
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| 226 | pts_value_l(0,28) = pts_value_l(0,28) + ( particles(n)%rvar3 - & |
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| 227 | pts_value(0,11) )**2 ! w"2 |
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| 228 | ENDIF |
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[1] | 229 | ! |
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| 230 | !-- Repeat the same for the respective particle group |
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| 231 | IF ( number_of_particle_groups > 1 ) THEN |
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| 232 | j = particles(n)%group |
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| 233 | |
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[825] | 234 | pts_value_l(j,20) = pts_value_l(j,20) + ( particles(n)%x - & |
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[1] | 235 | particles(n)%origin_x - pts_value(j,2) )**2 |
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[825] | 236 | pts_value_l(j,21) = pts_value_l(j,21) + ( particles(n)%y - & |
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[1] | 237 | particles(n)%origin_y - pts_value(j,3) )**2 |
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[825] | 238 | pts_value_l(j,22) = pts_value_l(j,22) + ( particles(n)%z - & |
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[1] | 239 | particles(n)%origin_z - pts_value(j,4) )**2 |
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[825] | 240 | pts_value_l(j,23) = pts_value_l(j,23) + ( particles(n)%speed_x - & |
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| 241 | pts_value(j,6) )**2 |
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| 242 | pts_value_l(j,24) = pts_value_l(j,24) + ( particles(n)%speed_y - & |
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| 243 | pts_value(j,7) )**2 |
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| 244 | pts_value_l(j,25) = pts_value_l(j,25) + ( particles(n)%speed_z - & |
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| 245 | pts_value(j,8) )**2 |
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| 246 | IF ( .NOT. curvature_solution_effects ) THEN |
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| 247 | pts_value_l(j,26) = pts_value_l(j,26) + ( particles(n)%rvar1 - & |
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| 248 | pts_value(j,9) )**2 |
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| 249 | pts_value_l(j,27) = pts_value_l(j,27) + ( particles(n)%rvar2 - & |
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| 250 | pts_value(j,10) )**2 |
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| 251 | pts_value_l(j,28) = pts_value_l(j,28) + ( particles(n)%rvar3 - & |
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| 252 | pts_value(j,11) )**2 |
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| 253 | ENDIF |
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[1] | 254 | ENDIF |
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| 255 | |
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| 256 | ENDDO |
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| 257 | |
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[825] | 258 | pts_value_l(0,29) = ( number_of_particles - pts_value(0,1) / numprocs )**2 |
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[1] | 259 | ! variance of particle numbers |
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| 260 | IF ( number_of_particle_groups > 1 ) THEN |
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| 261 | DO j = 1, number_of_particle_groups |
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[825] | 262 | pts_value_l(j,29) = ( pts_value_l(j,1) - & |
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[1] | 263 | pts_value(j,1) / numprocs )**2 |
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| 264 | ENDDO |
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| 265 | ENDIF |
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| 266 | |
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| 267 | #if defined( __parallel ) |
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| 268 | ! |
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| 269 | !-- Sum values of the subdomains |
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| 270 | inum = number_of_particle_groups + 1 |
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| 271 | |
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[622] | 272 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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[825] | 273 | CALL MPI_ALLREDUCE( pts_value_l(0,20), pts_value(0,20), inum*10, MPI_REAL, & |
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[1] | 274 | MPI_SUM, comm2d, ierr ) |
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| 275 | #else |
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[825] | 276 | pts_value(:,20:29) = pts_value_l(:,20:29) |
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[1] | 277 | #endif |
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| 278 | |
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| 279 | ! |
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| 280 | !-- Normalize the above calculated quantities with the total number of |
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| 281 | !-- particles |
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| 282 | IF ( number_of_particle_groups > 1 ) THEN |
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| 283 | inum = number_of_particle_groups |
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| 284 | ELSE |
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| 285 | inum = 0 |
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| 286 | ENDIF |
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| 287 | |
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| 288 | DO j = 0, inum |
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| 289 | |
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| 290 | IF ( pts_value(j,1) > 0.0 ) THEN |
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[825] | 291 | pts_value(j,20:28) = pts_value(j,20:28) / pts_value(j,1) |
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[1] | 292 | ENDIF |
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[825] | 293 | pts_value(j,29) = pts_value(j,29) / numprocs |
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[1] | 294 | |
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| 295 | ENDDO |
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| 296 | |
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| 297 | #if defined( __netcdf ) |
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| 298 | ! |
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| 299 | !-- Output particle time series quantities in NetCDF format |
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| 300 | IF ( myid == 0 .AND. netcdf_output ) THEN |
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| 301 | DO j = 0, inum |
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| 302 | DO i = 1, dopts_num |
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| 303 | nc_stat = NF90_PUT_VAR( id_set_pts, id_var_dopts(i,j), & |
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| 304 | (/ pts_value(j,i) /), & |
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| 305 | start = (/ dopts_time_count /), & |
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| 306 | count = (/ 1 /) ) |
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[263] | 307 | CALL handle_netcdf_error( 'data_output_ptseries', 392 ) |
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[1] | 308 | ENDDO |
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| 309 | ENDDO |
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| 310 | ENDIF |
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| 311 | #endif |
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| 312 | |
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[825] | 313 | DEALLOCATE( pts_value, pts_value_l ) |
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| 314 | |
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[1] | 315 | CALL cpu_log( log_point(36), 'data_output_ptseries','stop', 'nobarrier' ) |
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| 316 | |
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| 317 | END SUBROUTINE data_output_ptseries |
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