| 1 | SUBROUTINE data_output_ptseries |
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| 2 | |
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| 3 | !------------------------------------------------------------------------------! |
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| 4 | ! Current revisions: |
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| 5 | ! ----------------- |
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| 6 | ! mean particle radius added as output quantity. |
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| 7 | ! particle attributes speed_x|y|z_sgs renamed rvar1|2|3. |
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| 8 | ! |
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| 9 | ! Former revisions: |
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| 10 | ! ----------------- |
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| 11 | ! $Id: data_output_ptseries.f90 824 2012-02-17 09:09:57Z raasch $ |
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| 12 | ! |
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| 13 | ! 622 2010-12-10 08:08:13Z raasch |
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| 14 | ! optional barriers included in order to speed up collective operations |
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| 15 | ! |
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| 16 | ! 291 2009-04-16 12:07:26Z raasch |
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| 17 | ! simulated_time in NetCDF output replaced by time_since_reference_point. |
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| 18 | ! Output of NetCDF messages with aid of message handling routine. |
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| 19 | ! |
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| 20 | ! 60 2007-03-11 11:50:04Z raasch |
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| 21 | ! Particles-package is now part of the default code. |
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| 22 | ! |
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| 23 | ! RCS Log replace by Id keyword, revision history cleaned up |
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| 24 | ! |
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| 25 | ! Revision 1.2 2006/08/22 13:51:13 raasch |
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| 26 | ! Seperate output for particle groups |
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| 27 | ! |
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| 28 | ! Revision 1.1 2006/08/04 14:24:18 raasch |
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| 29 | ! Initial revision |
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| 30 | ! |
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| 31 | ! |
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| 32 | ! Description: |
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| 33 | ! ------------ |
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| 34 | ! Output of particle data timeseries in NetCDF format. |
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| 35 | !------------------------------------------------------------------------------! |
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| 36 | |
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| 37 | USE control_parameters |
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| 38 | USE cpulog |
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| 39 | USE indices |
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| 40 | USE interfaces |
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| 41 | USE netcdf_control |
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| 42 | USE particle_attributes |
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| 43 | USE pegrid |
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| 44 | |
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| 45 | IMPLICIT NONE |
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| 46 | |
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| 47 | |
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| 48 | INTEGER :: i, inum, j, n |
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| 49 | |
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| 50 | REAL, DIMENSION(0:number_of_particle_groups,30) :: pts_value, pts_value_l |
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| 51 | |
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| 52 | |
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| 53 | |
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| 54 | CALL cpu_log( log_point(36), 'data_output_ptseries', 'start' ) |
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| 55 | |
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| 56 | IF ( myid == 0 .AND. netcdf_output ) THEN |
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| 57 | ! |
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| 58 | !-- Open file for time series output in NetCDF format |
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| 59 | dopts_time_count = dopts_time_count + 1 |
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| 60 | CALL check_open( 109 ) |
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| 61 | #if defined( __netcdf ) |
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| 62 | ! |
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| 63 | !-- Update the particle time series time axis |
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| 64 | nc_stat = NF90_PUT_VAR( id_set_pts, id_var_time_pts, & |
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| 65 | (/ time_since_reference_point /), & |
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| 66 | start = (/ dopts_time_count /), count = (/ 1 /) ) |
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| 67 | CALL handle_netcdf_error( 'data_output_ptseries', 391 ) |
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| 68 | #endif |
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| 69 | |
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| 70 | ENDIF |
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| 71 | |
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| 72 | pts_value_l = 0.0 |
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| 73 | |
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| 74 | ! |
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| 75 | !-- Calculate or collect the particle time series quantities for all particles |
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| 76 | !-- and seperately for each particle group (if there is more than one group) |
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| 77 | DO n = 1, number_of_particles |
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| 78 | |
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| 79 | pts_value_l(0,1) = number_of_particles ! total # of particles |
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| 80 | pts_value_l(0,2) = pts_value_l(0,2) + & |
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| 81 | ( particles(n)%x - particles(n)%origin_x ) ! mean x |
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| 82 | pts_value_l(0,3) = pts_value_l(0,3) + & |
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| 83 | ( particles(n)%y - particles(n)%origin_y ) ! mean y |
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| 84 | pts_value_l(0,4) = pts_value_l(0,4) + & |
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| 85 | ( particles(n)%z - particles(n)%origin_z ) ! mean z |
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| 86 | pts_value_l(0,5) = pts_value_l(0,5) + particles(n)%z ! mean z (absolute) |
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| 87 | pts_value_l(0,6) = pts_value_l(0,6) + particles(n)%speed_x ! mean u |
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| 88 | pts_value_l(0,7) = pts_value_l(0,7) + particles(n)%speed_y ! mean v |
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| 89 | pts_value_l(0,8) = pts_value_l(0,8) + particles(n)%speed_z ! mean w |
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| 90 | pts_value_l(0,9) = pts_value_l(0,9) + particles(n)%rvar1 ! mean sgsu |
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| 91 | pts_value_l(0,10) = pts_value_l(0,10) + particles(n)%rvar2 ! mean sgsv |
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| 92 | pts_value_l(0,11) = pts_value_l(0,11) + particles(n)%rvar3 ! mean sgsw |
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| 93 | IF ( particles(n)%speed_z > 0.0 ) THEN |
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| 94 | pts_value_l(0,12) = pts_value_l(0,12) + 1.0 ! # of upward moving prts |
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| 95 | pts_value_l(0,13) = pts_value_l(0,13) + & |
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| 96 | particles(n)%speed_z ! mean w upw. |
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| 97 | ELSE |
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| 98 | pts_value_l(0,14) = pts_value_l(0,14) + & |
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| 99 | particles(n)%speed_z ! mean w down |
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| 100 | ENDIF |
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| 101 | pts_value_l(0,15) = pts_value_l(0,15) + particles(n)%radius |
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| 102 | pts_value_l(0,16) = number_of_particles |
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| 103 | pts_value_l(0,17) = number_of_particles |
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| 104 | |
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| 105 | ! |
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| 106 | !-- Repeat the same for the respective particle group |
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| 107 | IF ( number_of_particle_groups > 1 ) THEN |
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| 108 | j = particles(n)%group |
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| 109 | |
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| 110 | pts_value_l(j,1) = pts_value_l(j,1) + 1 |
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| 111 | pts_value_l(j,2) = pts_value_l(j,2) + & |
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| 112 | ( particles(n)%x - particles(n)%origin_x ) |
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| 113 | pts_value_l(j,3) = pts_value_l(j,3) + & |
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| 114 | ( particles(n)%y - particles(n)%origin_y ) |
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| 115 | pts_value_l(j,4) = pts_value_l(j,4) + & |
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| 116 | ( particles(n)%z - particles(n)%origin_z ) |
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| 117 | pts_value_l(j,5) = pts_value_l(j,5) + particles(n)%z |
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| 118 | pts_value_l(j,6) = pts_value_l(j,6) + particles(n)%speed_x |
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| 119 | pts_value_l(j,7) = pts_value_l(j,7) + particles(n)%speed_y |
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| 120 | pts_value_l(j,8) = pts_value_l(j,8) + particles(n)%speed_z |
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| 121 | pts_value_l(j,9) = pts_value_l(j,9) + particles(n)%rvar1 |
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| 122 | pts_value_l(j,10) = pts_value_l(j,10) + particles(n)%rvar2 |
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| 123 | pts_value_l(j,11) = pts_value_l(j,11) + particles(n)%rvar3 |
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| 124 | IF ( particles(n)%speed_z > 0.0 ) THEN |
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| 125 | pts_value_l(j,12) = pts_value_l(j,12) + 1.0 |
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| 126 | pts_value_l(j,13) = pts_value_l(j,13) + particles(n)%speed_z |
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| 127 | ELSE |
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| 128 | pts_value_l(j,14) = pts_value_l(j,14) + particles(n)%speed_z |
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| 129 | ENDIF |
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| 130 | pts_value_l(j,15) = pts_value_l(j,15) + particles(n)%radius |
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| 131 | pts_value_l(j,16) = pts_value_l(j,16) + 1.0 |
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| 132 | pts_value_l(j,17) = pts_value_l(j,17) + 1.0 |
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| 133 | |
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| 134 | ENDIF |
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| 135 | |
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| 136 | ENDDO |
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| 137 | |
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| 138 | #if defined( __parallel ) |
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| 139 | ! |
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| 140 | !-- Sum values of the subdomains |
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| 141 | inum = number_of_particle_groups + 1 |
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| 142 | |
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| 143 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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| 144 | CALL MPI_ALLREDUCE( pts_value_l(0,1), pts_value(0,1), 15*inum, MPI_REAL, & |
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| 145 | MPI_SUM, comm2d, ierr ) |
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| 146 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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| 147 | CALL MPI_ALLREDUCE( pts_value_l(0,16), pts_value(0,16), inum, MPI_REAL, & |
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| 148 | MPI_MAX, comm2d, ierr ) |
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| 149 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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| 150 | CALL MPI_ALLREDUCE( pts_value_l(0,17), pts_value(0,17), inum, MPI_REAL, & |
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| 151 | MPI_MIN, comm2d, ierr ) |
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| 152 | #else |
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| 153 | pts_value(:,1:17) = pts_value_l(:,1:17) |
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| 154 | #endif |
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| 155 | |
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| 156 | ! |
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| 157 | !-- Normalize the above calculated quantities with the total number of |
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| 158 | !-- particles |
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| 159 | IF ( number_of_particle_groups > 1 ) THEN |
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| 160 | inum = number_of_particle_groups |
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| 161 | ELSE |
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| 162 | inum = 0 |
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| 163 | ENDIF |
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| 164 | |
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| 165 | DO j = 0, inum |
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| 166 | |
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| 167 | IF ( pts_value(j,1) > 0.0 ) THEN |
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| 168 | |
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| 169 | pts_value(j,2:15) = pts_value(j,2:15) / pts_value(j,1) |
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| 170 | IF ( pts_value(j,12) > 0.0 .AND. pts_value(j,12) < 1.0 ) THEN |
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| 171 | pts_value(j,13) = pts_value(j,13) / pts_value(j,12) |
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| 172 | pts_value(j,14) = pts_value(j,14) / ( 1.0 - pts_value(j,12) ) |
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| 173 | ELSEIF ( pts_value(j,12) == 0.0 ) THEN |
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| 174 | pts_value(j,13) = -1.0 |
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| 175 | ELSE |
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| 176 | pts_value(j,14) = -1.0 |
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| 177 | ENDIF |
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| 178 | |
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| 179 | ENDIF |
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| 180 | |
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| 181 | ENDDO |
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| 182 | |
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| 183 | ! |
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| 184 | !-- Calculate higher order moments of particle time series quantities, |
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| 185 | !-- seperately for each particle group (if there is more than one group) |
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| 186 | DO n = 1, number_of_particles |
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| 187 | |
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| 188 | pts_value_l(0,18) = pts_value_l(0,18) + ( particles(n)%x - & |
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| 189 | particles(n)%origin_x - pts_value(0,2) )**2 ! x*2 |
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| 190 | pts_value_l(0,19) = pts_value_l(0,19) + ( particles(n)%y - & |
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| 191 | particles(n)%origin_y - pts_value(0,3) )**2 ! y*2 |
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| 192 | pts_value_l(0,20) = pts_value_l(0,20) + ( particles(n)%z - & |
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| 193 | particles(n)%origin_z - pts_value(0,4) )**2 ! z*2 |
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| 194 | pts_value_l(0,21) = pts_value_l(0,21) + ( particles(n)%speed_x - & |
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| 195 | pts_value(0,6) )**2 ! u*2 |
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| 196 | pts_value_l(0,22) = pts_value_l(0,22) + ( particles(n)%speed_y - & |
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| 197 | pts_value(0,7) )**2 ! v*2 |
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| 198 | pts_value_l(0,23) = pts_value_l(0,23) + ( particles(n)%speed_z - & |
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| 199 | pts_value(0,8) )**2 ! w*2 |
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| 200 | pts_value_l(0,24) = pts_value_l(0,24) + ( particles(n)%rvar1 - & |
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| 201 | pts_value(0,9) )**2 ! u"2 |
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| 202 | pts_value_l(0,25) = pts_value_l(0,25) + ( particles(n)%rvar2 - & |
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| 203 | pts_value(0,10) )**2 ! v"2 |
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| 204 | pts_value_l(0,26) = pts_value_l(0,26) + ( particles(n)%rvar3 - & |
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| 205 | pts_value(0,11) )**2 ! w"2 |
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| 206 | ! |
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| 207 | !-- Repeat the same for the respective particle group |
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| 208 | IF ( number_of_particle_groups > 1 ) THEN |
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| 209 | j = particles(n)%group |
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| 210 | |
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| 211 | pts_value_l(j,18) = pts_value_l(j,18) + ( particles(n)%x - & |
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| 212 | particles(n)%origin_x - pts_value(j,2) )**2 |
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| 213 | pts_value_l(j,19) = pts_value_l(j,19) + ( particles(n)%y - & |
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| 214 | particles(n)%origin_y - pts_value(j,3) )**2 |
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| 215 | pts_value_l(j,20) = pts_value_l(j,20) + ( particles(n)%z - & |
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| 216 | particles(n)%origin_z - pts_value(j,4) )**2 |
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| 217 | pts_value_l(j,21) = pts_value_l(j,21) + ( particles(n)%speed_x - & |
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| 218 | pts_value(j,6) )**2 |
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| 219 | pts_value_l(j,22) = pts_value_l(j,22) + ( particles(n)%speed_y - & |
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| 220 | pts_value(j,7) )**2 |
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| 221 | pts_value_l(j,23) = pts_value_l(j,23) + ( particles(n)%speed_z - & |
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| 222 | pts_value(j,8) )**2 |
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| 223 | pts_value_l(j,24) = pts_value_l(j,24) + ( particles(n)%rvar1 - & |
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| 224 | pts_value(j,9) )**2 |
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| 225 | pts_value_l(j,25) = pts_value_l(j,25) + ( particles(n)%rvar2 - & |
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| 226 | pts_value(j,10) )**2 |
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| 227 | pts_value_l(j,26) = pts_value_l(j,26) + ( particles(n)%rvar3 - & |
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| 228 | pts_value(j,11) )**2 |
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| 229 | ENDIF |
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| 230 | |
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| 231 | ENDDO |
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| 232 | |
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| 233 | pts_value_l(0,27) = ( number_of_particles - pts_value(0,1) / numprocs )**2 |
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| 234 | ! variance of particle numbers |
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| 235 | IF ( number_of_particle_groups > 1 ) THEN |
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| 236 | DO j = 1, number_of_particle_groups |
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| 237 | pts_value_l(j,27) = ( pts_value_l(j,1) - & |
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| 238 | pts_value(j,1) / numprocs )**2 |
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| 239 | ENDDO |
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| 240 | ENDIF |
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| 241 | |
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| 242 | #if defined( __parallel ) |
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| 243 | ! |
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| 244 | !-- Sum values of the subdomains |
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| 245 | inum = number_of_particle_groups + 1 |
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| 246 | |
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| 247 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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| 248 | CALL MPI_ALLREDUCE( pts_value_l(0,18), pts_value(0,18), inum*10, MPI_REAL, & |
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| 249 | MPI_SUM, comm2d, ierr ) |
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| 250 | #else |
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| 251 | pts_value(:,18:27) = pts_value_l(:,18:27) |
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| 252 | #endif |
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| 253 | |
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| 254 | ! |
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| 255 | !-- Normalize the above calculated quantities with the total number of |
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| 256 | !-- particles |
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| 257 | IF ( number_of_particle_groups > 1 ) THEN |
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| 258 | inum = number_of_particle_groups |
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| 259 | ELSE |
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| 260 | inum = 0 |
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| 261 | ENDIF |
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| 262 | |
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| 263 | DO j = 0, inum |
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| 264 | |
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| 265 | IF ( pts_value(j,1) > 0.0 ) THEN |
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| 266 | pts_value(j,18:26) = pts_value(j,18:26) / pts_value(j,1) |
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| 267 | ENDIF |
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| 268 | pts_value(j,27) = pts_value(j,27) / numprocs |
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| 269 | |
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| 270 | ENDDO |
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| 271 | |
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| 272 | #if defined( __netcdf ) |
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| 273 | ! |
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| 274 | !-- Output particle time series quantities in NetCDF format |
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| 275 | IF ( myid == 0 .AND. netcdf_output ) THEN |
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| 276 | DO j = 0, inum |
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| 277 | DO i = 1, dopts_num |
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| 278 | nc_stat = NF90_PUT_VAR( id_set_pts, id_var_dopts(i,j), & |
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| 279 | (/ pts_value(j,i) /), & |
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| 280 | start = (/ dopts_time_count /), & |
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| 281 | count = (/ 1 /) ) |
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| 282 | CALL handle_netcdf_error( 'data_output_ptseries', 392 ) |
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| 283 | ENDDO |
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| 284 | ENDDO |
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| 285 | ENDIF |
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| 286 | #endif |
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| 287 | |
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| 288 | CALL cpu_log( log_point(36), 'data_output_ptseries','stop', 'nobarrier' ) |
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| 289 | |
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| 290 | END SUBROUTINE data_output_ptseries |
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