| [1] | 1 | SUBROUTINE data_output_ptseries |
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| 2 | |
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| 3 | !------------------------------------------------------------------------------! |
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| 4 | ! Actual revisions: |
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| 5 | ! ----------------- |
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| [60] | 6 | ! Particles-package is now part of the default code. |
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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 60 2007-03-11 11:50:04Z raasch $ |
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| 11 | ! RCS Log replace by Id keyword, revision history cleaned up |
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| 12 | ! |
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| [1] | 13 | ! Revision 1.2 2006/08/22 13:51:13 raasch |
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| 14 | ! Seperate output for particle groups |
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| 15 | ! |
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| 16 | ! Revision 1.1 2006/08/04 14:24:18 raasch |
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| 17 | ! Initial revision |
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| 18 | ! |
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| 19 | ! |
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| 20 | ! Description: |
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| 21 | ! ------------ |
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| 22 | ! Output of particle data timeseries in NetCDF format. |
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| 23 | !------------------------------------------------------------------------------! |
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| 24 | |
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| 25 | USE control_parameters |
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| 26 | USE cpulog |
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| 27 | USE indices |
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| 28 | USE interfaces |
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| 29 | USE netcdf_control |
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| 30 | USE particle_attributes |
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| 31 | USE pegrid |
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| 32 | |
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| 33 | IMPLICIT NONE |
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| 34 | |
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| 35 | |
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| 36 | INTEGER :: i, inum, j, n |
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| 37 | |
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| 38 | REAL, DIMENSION(0:number_of_particle_groups,30) :: pts_value, pts_value_l |
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| 39 | |
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| 40 | |
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| 41 | |
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| 42 | CALL cpu_log( log_point(36), 'data_output_ptseries', 'start' ) |
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| 43 | |
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| 44 | IF ( myid == 0 .AND. netcdf_output ) THEN |
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| 45 | ! |
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| 46 | !-- Open file for time series output in NetCDF format |
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| 47 | dopts_time_count = dopts_time_count + 1 |
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| 48 | CALL check_open( 109 ) |
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| 49 | #if defined( __netcdf ) |
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| 50 | ! |
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| 51 | !-- Update the particle time series time axis |
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| 52 | nc_stat = NF90_PUT_VAR( id_set_pts, id_var_time_pts, & |
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| 53 | (/ simulated_time /), & |
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| 54 | start = (/ dopts_time_count /), count = (/ 1 /) ) |
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| 55 | IF (nc_stat /= NF90_NOERR) CALL handle_netcdf_error( 391 ) |
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| 56 | #endif |
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| 57 | |
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| 58 | ENDIF |
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| 59 | |
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| 60 | pts_value_l = 0.0 |
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| 61 | |
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| 62 | ! |
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| 63 | !-- Calculate or collect the particle time series quantities for all particles |
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| 64 | !-- and seperately for each particle group (if there is more than one group) |
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| 65 | DO n = 1, number_of_particles |
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| 66 | |
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| 67 | pts_value_l(0,1) = number_of_particles ! total # of particles |
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| 68 | pts_value_l(0,2) = pts_value_l(0,2) + & |
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| 69 | ( particles(n)%x - particles(n)%origin_x ) ! mean x |
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| 70 | pts_value_l(0,3) = pts_value_l(0,3) + & |
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| 71 | ( particles(n)%y - particles(n)%origin_y ) ! mean y |
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| 72 | pts_value_l(0,4) = pts_value_l(0,4) + & |
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| 73 | ( particles(n)%z - particles(n)%origin_z ) ! mean z |
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| 74 | pts_value_l(0,5) = pts_value_l(0,5) + particles(n)%z ! mean z (absolute) |
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| 75 | pts_value_l(0,6) = pts_value_l(0,6) + particles(n)%speed_x ! mean u |
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| 76 | pts_value_l(0,7) = pts_value_l(0,7) + particles(n)%speed_y ! mean v |
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| 77 | pts_value_l(0,8) = pts_value_l(0,8) + particles(n)%speed_z ! mean w |
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| 78 | pts_value_l(0,9) = pts_value_l(0,9) + & |
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| 79 | particles(n)%speed_x_sgs ! mean sgsu |
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| 80 | pts_value_l(0,10) = pts_value_l(0,10) + & |
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| 81 | particles(n)%speed_y_sgs ! mean sgsv |
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| 82 | pts_value_l(0,11) = pts_value_l(0,11) + & |
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| 83 | particles(n)%speed_z_sgs ! mean sgsw |
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| 84 | IF ( particles(n)%speed_z > 0.0 ) THEN |
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| 85 | pts_value_l(0,12) = pts_value_l(0,12) + 1.0 ! # of upward moving prts |
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| 86 | pts_value_l(0,13) = pts_value_l(0,13) + & |
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| 87 | particles(n)%speed_z ! mean w upw. |
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| 88 | ELSE |
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| 89 | pts_value_l(0,14) = pts_value_l(0,14) + & |
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| 90 | particles(n)%speed_z ! mean w down |
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| 91 | ENDIF |
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| 92 | pts_value_l(0,15) = number_of_particles |
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| 93 | pts_value_l(0,16) = number_of_particles |
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| 94 | |
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| 95 | ! |
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| 96 | !-- Repeat the same for the respective particle group |
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| 97 | IF ( number_of_particle_groups > 1 ) THEN |
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| 98 | j = particles(n)%group |
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| 99 | |
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| 100 | pts_value_l(j,1) = pts_value_l(j,1) + 1 |
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| 101 | pts_value_l(j,2) = pts_value_l(j,2) + & |
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| 102 | ( particles(n)%x - particles(n)%origin_x ) |
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| 103 | pts_value_l(j,3) = pts_value_l(j,3) + & |
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| 104 | ( particles(n)%y - particles(n)%origin_y ) |
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| 105 | pts_value_l(j,4) = pts_value_l(j,4) + & |
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| 106 | ( particles(n)%z - particles(n)%origin_z ) |
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| 107 | pts_value_l(j,5) = pts_value_l(j,5) + particles(n)%z |
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| 108 | pts_value_l(j,6) = pts_value_l(j,6) + particles(n)%speed_x |
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| 109 | pts_value_l(j,7) = pts_value_l(j,7) + particles(n)%speed_y |
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| 110 | pts_value_l(j,8) = pts_value_l(j,8) + particles(n)%speed_z |
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| 111 | pts_value_l(j,9) = pts_value_l(j,9) + particles(n)%speed_x_sgs |
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| 112 | pts_value_l(j,10) = pts_value_l(j,10) + particles(n)%speed_y_sgs |
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| 113 | pts_value_l(j,11) = pts_value_l(j,11) + particles(n)%speed_z_sgs |
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| 114 | IF ( particles(n)%speed_z > 0.0 ) THEN |
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| 115 | pts_value_l(j,12) = pts_value_l(j,12) + 1.0 |
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| 116 | pts_value_l(j,13) = pts_value_l(j,13) + particles(n)%speed_z |
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| 117 | ELSE |
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| 118 | pts_value_l(j,14) = pts_value_l(j,14) + particles(n)%speed_z |
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| 119 | ENDIF |
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| 120 | pts_value_l(j,15) = pts_value_l(j,15) + 1.0 |
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| 121 | pts_value_l(j,16) = pts_value_l(j,16) + 1.0 |
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| 122 | |
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| 123 | ENDIF |
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| 124 | |
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| 125 | ENDDO |
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| 126 | |
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| 127 | #if defined( __parallel ) |
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| 128 | ! |
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| 129 | !-- Sum values of the subdomains |
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| 130 | inum = number_of_particle_groups + 1 |
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| 131 | |
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| 132 | CALL MPI_ALLREDUCE( pts_value_l(0,1), pts_value(0,1), 14*inum, MPI_REAL, & |
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| 133 | MPI_SUM, comm2d, ierr ) |
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| 134 | CALL MPI_ALLREDUCE( pts_value_l(0,15), pts_value(0,15), inum, MPI_REAL, & |
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| 135 | MPI_MAX, comm2d, ierr ) |
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| 136 | CALL MPI_ALLREDUCE( pts_value_l(0,16), pts_value(0,16), inum, MPI_REAL, & |
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| 137 | MPI_MIN, comm2d, ierr ) |
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| 138 | #else |
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| 139 | pts_value(:,1:16) = pts_value_l(:,1:16) |
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| 140 | #endif |
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| 141 | |
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| 142 | ! |
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| 143 | !-- Normalize the above calculated quantities with the total number of |
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| 144 | !-- particles |
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| 145 | IF ( number_of_particle_groups > 1 ) THEN |
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| 146 | inum = number_of_particle_groups |
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| 147 | ELSE |
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| 148 | inum = 0 |
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| 149 | ENDIF |
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| 150 | |
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| 151 | DO j = 0, inum |
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| 152 | |
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| 153 | IF ( pts_value(j,1) > 0.0 ) THEN |
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| 154 | |
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| 155 | pts_value(j,2:14) = pts_value(j,2:14) / pts_value(j,1) |
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| 156 | IF ( pts_value(j,12) > 0.0 .AND. pts_value(j,12) < 1.0 ) THEN |
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| 157 | pts_value(j,13) = pts_value(j,13) / pts_value(j,12) |
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| 158 | pts_value(j,14) = pts_value(j,14) / ( 1.0 - pts_value(j,12) ) |
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| 159 | ELSEIF ( pts_value(j,12) == 0.0 ) THEN |
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| 160 | pts_value(j,13) = -1.0 |
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| 161 | ELSE |
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| 162 | pts_value(j,14) = -1.0 |
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| 163 | ENDIF |
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| 164 | |
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| 165 | ENDIF |
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| 166 | |
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| 167 | ENDDO |
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| 168 | |
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| 169 | ! |
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| 170 | !-- Calculate higher order moments of particle time series quantities, |
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| 171 | !-- seperately for each particle group (if there is more than one group) |
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| 172 | DO n = 1, number_of_particles |
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| 173 | |
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| 174 | pts_value_l(0,17) = pts_value_l(0,17) + ( particles(n)%x - & |
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| 175 | particles(n)%origin_x - pts_value(0,2) )**2 ! x*2 |
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| 176 | pts_value_l(0,18) = pts_value_l(0,18) + ( particles(n)%y - & |
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| 177 | particles(n)%origin_y - pts_value(0,3) )**2 ! y*2 |
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| 178 | pts_value_l(0,19) = pts_value_l(0,19) + ( particles(n)%z - & |
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| 179 | particles(n)%origin_z - pts_value(0,4) )**2 ! z*2 |
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| 180 | pts_value_l(0,20) = pts_value_l(0,20) + ( particles(n)%speed_x - & |
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| 181 | pts_value(0,6) )**2 ! u*2 |
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| 182 | pts_value_l(0,21) = pts_value_l(0,21) + ( particles(n)%speed_y - & |
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| 183 | pts_value(0,7) )**2 ! v*2 |
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| 184 | pts_value_l(0,22) = pts_value_l(0,22) + ( particles(n)%speed_z - & |
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| 185 | pts_value(0,8) )**2 ! w*2 |
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| 186 | pts_value_l(0,23) = pts_value_l(0,23) + ( particles(n)%speed_x_sgs - & |
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| 187 | pts_value(0,9) )**2 ! u"2 |
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| 188 | pts_value_l(0,24) = pts_value_l(0,24) + ( particles(n)%speed_y_sgs - & |
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| 189 | pts_value(0,10) )**2 ! v"2 |
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| 190 | pts_value_l(0,25) = pts_value_l(0,25) + ( particles(n)%speed_z_sgs - & |
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| 191 | pts_value(0,11) )**2 ! w"2 |
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| 192 | ! |
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| 193 | !-- Repeat the same for the respective particle group |
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| 194 | IF ( number_of_particle_groups > 1 ) THEN |
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| 195 | j = particles(n)%group |
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| 196 | |
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| 197 | pts_value_l(j,17) = pts_value_l(j,17) + ( particles(n)%x - & |
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| 198 | particles(n)%origin_x - pts_value(j,2) )**2 |
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| 199 | pts_value_l(j,18) = pts_value_l(j,18) + ( particles(n)%y - & |
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| 200 | particles(n)%origin_y - pts_value(j,3) )**2 |
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| 201 | pts_value_l(j,19) = pts_value_l(j,19) + ( particles(n)%z - & |
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| 202 | particles(n)%origin_z - pts_value(j,4) )**2 |
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| 203 | pts_value_l(j,20) = pts_value_l(j,20) + ( particles(n)%speed_x - & |
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| 204 | pts_value(j,6) )**2 |
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| 205 | pts_value_l(j,21) = pts_value_l(j,21) + ( particles(n)%speed_y - & |
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| 206 | pts_value(j,7) )**2 |
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| 207 | pts_value_l(j,22) = pts_value_l(j,22) + ( particles(n)%speed_z - & |
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| 208 | pts_value(j,8) )**2 |
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| 209 | pts_value_l(j,23) = pts_value_l(j,23) + ( particles(n)%speed_x_sgs - & |
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| 210 | pts_value(j,9) )**2 |
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| 211 | pts_value_l(j,24) = pts_value_l(j,24) + ( particles(n)%speed_y_sgs - & |
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| 212 | pts_value(j,10) )**2 |
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| 213 | pts_value_l(j,25) = pts_value_l(j,25) + ( particles(n)%speed_z_sgs - & |
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| 214 | pts_value(j,11) )**2 |
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| 215 | ENDIF |
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| 216 | |
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| 217 | ENDDO |
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| 218 | |
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| 219 | pts_value_l(0,26) = ( number_of_particles - pts_value(0,1) / numprocs )**2 |
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| 220 | ! variance of particle numbers |
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| 221 | IF ( number_of_particle_groups > 1 ) THEN |
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| 222 | DO j = 1, number_of_particle_groups |
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| 223 | pts_value_l(j,26) = ( pts_value_l(j,1) - & |
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| 224 | pts_value(j,1) / numprocs )**2 |
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| 225 | ENDDO |
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| 226 | ENDIF |
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| 227 | |
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| 228 | #if defined( __parallel ) |
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| 229 | ! |
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| 230 | !-- Sum values of the subdomains |
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| 231 | inum = number_of_particle_groups + 1 |
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| 232 | |
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| 233 | CALL MPI_ALLREDUCE( pts_value_l(0,17), pts_value(0,17), inum*10, MPI_REAL, & |
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| 234 | MPI_SUM, comm2d, ierr ) |
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| 235 | #else |
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| 236 | pts_value(:,17:26) = pts_value_l(:,17:26) |
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| 237 | #endif |
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| 238 | |
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| 239 | ! |
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| 240 | !-- Normalize the above calculated quantities with the total number of |
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| 241 | !-- particles |
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| 242 | IF ( number_of_particle_groups > 1 ) THEN |
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| 243 | inum = number_of_particle_groups |
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| 244 | ELSE |
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| 245 | inum = 0 |
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| 246 | ENDIF |
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| 247 | |
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| 248 | DO j = 0, inum |
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| 249 | |
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| 250 | IF ( pts_value(j,1) > 0.0 ) THEN |
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| 251 | pts_value(j,17:25) = pts_value(j,17:25) / pts_value(j,1) |
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| 252 | ENDIF |
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| 253 | pts_value(j,26) = pts_value(j,26) / numprocs |
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| 254 | |
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| 255 | ENDDO |
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| 256 | |
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| 257 | #if defined( __netcdf ) |
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| 258 | ! |
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| 259 | !-- Output particle time series quantities in NetCDF format |
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| 260 | IF ( myid == 0 .AND. netcdf_output ) THEN |
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| 261 | DO j = 0, inum |
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| 262 | DO i = 1, dopts_num |
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| 263 | nc_stat = NF90_PUT_VAR( id_set_pts, id_var_dopts(i,j), & |
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| 264 | (/ pts_value(j,i) /), & |
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| 265 | start = (/ dopts_time_count /), & |
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| 266 | count = (/ 1 /) ) |
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| 267 | IF ( nc_stat /= NF90_NOERR ) CALL handle_netcdf_error( 392 ) |
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| 268 | ENDDO |
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| 269 | ENDDO |
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| 270 | ENDIF |
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| 271 | #endif |
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| 272 | |
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| 273 | CALL cpu_log( log_point(36), 'data_output_ptseries','stop', 'nobarrier' ) |
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| 274 | |
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| 275 | END SUBROUTINE data_output_ptseries |
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