[1] | 1 | SUBROUTINE data_output_ptseries |
---|
| 2 | |
---|
[1036] | 3 | !--------------------------------------------------------------------------------! |
---|
| 4 | ! This file is part of PALM. |
---|
| 5 | ! |
---|
| 6 | ! PALM is free software: you can redistribute it and/or modify it under the terms |
---|
| 7 | ! of the GNU General Public License as published by the Free Software Foundation, |
---|
| 8 | ! either version 3 of the License, or (at your option) any later version. |
---|
| 9 | ! |
---|
| 10 | ! PALM is distributed in the hope that it will be useful, but WITHOUT ANY |
---|
| 11 | ! WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS FOR |
---|
| 12 | ! A PARTICULAR PURPOSE. See the GNU General Public License for more details. |
---|
| 13 | ! |
---|
| 14 | ! You should have received a copy of the GNU General Public License along with |
---|
| 15 | ! PALM. If not, see <http://www.gnu.org/licenses/>. |
---|
| 16 | ! |
---|
[1310] | 17 | ! Copyright 1997-2014 Leibniz Universitaet Hannover |
---|
[1036] | 18 | !--------------------------------------------------------------------------------! |
---|
| 19 | ! |
---|
[263] | 20 | ! Current revisions: |
---|
[1] | 21 | ! ----------------- |
---|
[1359] | 22 | ! New particle structure integrated. |
---|
[1329] | 23 | ! |
---|
[1321] | 24 | ! Former revisions: |
---|
| 25 | ! ----------------- |
---|
| 26 | ! $Id: data_output_ptseries.f90 1359 2014-04-11 17:15:14Z hoffmann $ |
---|
| 27 | ! |
---|
[1354] | 28 | ! 1353 2014-04-08 15:21:23Z heinze |
---|
| 29 | ! REAL constants provided with KIND-attribute |
---|
| 30 | ! |
---|
[1329] | 31 | ! 1327 2014-03-21 11:00:16Z raasch |
---|
| 32 | ! -netcdf output queries |
---|
| 33 | ! |
---|
[1321] | 34 | ! 1320 2014-03-20 08:40:49Z raasch |
---|
[1320] | 35 | ! ONLY-attribute added to USE-statements, |
---|
| 36 | ! kind-parameters added to all INTEGER and REAL declaration statements, |
---|
| 37 | ! kinds are defined in new module kinds, |
---|
| 38 | ! revision history before 2012 removed, |
---|
| 39 | ! comment fields (!:) to be used for variable explanations added to |
---|
| 40 | ! all variable declaration statements |
---|
[1] | 41 | ! |
---|
[1319] | 42 | ! 1318 2014-03-17 13:35:16Z raasch |
---|
| 43 | ! barrier argument removed from cpu_log, |
---|
| 44 | ! module interfaces removed |
---|
| 45 | ! |
---|
[1037] | 46 | ! 1036 2012-10-22 13:43:42Z raasch |
---|
| 47 | ! code put under GPL (PALM 3.9) |
---|
| 48 | ! |
---|
[826] | 49 | ! 825 2012-02-19 03:03:44Z raasch |
---|
| 50 | ! mean/minimum/maximum particle radius added as output quantity, |
---|
| 51 | ! particle attributes speed_x|y|z_sgs renamed rvar1|2|3 |
---|
| 52 | ! |
---|
[1] | 53 | ! Revision 1.1 2006/08/04 14:24:18 raasch |
---|
| 54 | ! Initial revision |
---|
| 55 | ! |
---|
| 56 | ! |
---|
| 57 | ! Description: |
---|
| 58 | ! ------------ |
---|
| 59 | ! Output of particle data timeseries in NetCDF format. |
---|
| 60 | !------------------------------------------------------------------------------! |
---|
| 61 | |
---|
[1320] | 62 | USE cloud_parameters, & |
---|
| 63 | ONLY: curvature_solution_effects |
---|
| 64 | |
---|
| 65 | USE control_parameters, & |
---|
[1327] | 66 | ONLY: dopts_time_count, time_since_reference_point |
---|
[1320] | 67 | |
---|
| 68 | USE cpulog, & |
---|
| 69 | ONLY: cpu_log, log_point |
---|
| 70 | |
---|
| 71 | USE indices, & |
---|
[1359] | 72 | ONLY: nxl, nxr, nys, nyn, nzb, nzt |
---|
[1320] | 73 | |
---|
| 74 | USE kinds |
---|
| 75 | |
---|
[1] | 76 | USE netcdf_control |
---|
[1320] | 77 | |
---|
| 78 | USE particle_attributes, & |
---|
[1359] | 79 | ONLY: grid_particles, number_of_particles, number_of_particle_groups, & |
---|
| 80 | particles, prt_count |
---|
[1320] | 81 | |
---|
[1] | 82 | USE pegrid |
---|
| 83 | |
---|
| 84 | IMPLICIT NONE |
---|
| 85 | |
---|
| 86 | |
---|
[1320] | 87 | INTEGER(iwp) :: i !: |
---|
| 88 | INTEGER(iwp) :: inum !: |
---|
| 89 | INTEGER(iwp) :: j !: |
---|
[1359] | 90 | INTEGER(iwp) :: jg !: |
---|
| 91 | INTEGER(iwp) :: k !: |
---|
[1320] | 92 | INTEGER(iwp) :: n !: |
---|
[1] | 93 | |
---|
[1320] | 94 | REAL(wp), DIMENSION(:,:), ALLOCATABLE :: pts_value !: |
---|
| 95 | REAL(wp), DIMENSION(:,:), ALLOCATABLE :: pts_value_l !: |
---|
[1] | 96 | |
---|
| 97 | |
---|
| 98 | CALL cpu_log( log_point(36), 'data_output_ptseries', 'start' ) |
---|
| 99 | |
---|
[1327] | 100 | IF ( myid == 0 ) THEN |
---|
[1] | 101 | ! |
---|
| 102 | !-- Open file for time series output in NetCDF format |
---|
| 103 | dopts_time_count = dopts_time_count + 1 |
---|
| 104 | CALL check_open( 109 ) |
---|
| 105 | #if defined( __netcdf ) |
---|
| 106 | ! |
---|
| 107 | !-- Update the particle time series time axis |
---|
[291] | 108 | nc_stat = NF90_PUT_VAR( id_set_pts, id_var_time_pts, & |
---|
| 109 | (/ time_since_reference_point /), & |
---|
[1] | 110 | start = (/ dopts_time_count /), count = (/ 1 /) ) |
---|
[263] | 111 | CALL handle_netcdf_error( 'data_output_ptseries', 391 ) |
---|
[1] | 112 | #endif |
---|
| 113 | |
---|
| 114 | ENDIF |
---|
| 115 | |
---|
[825] | 116 | ALLOCATE( pts_value(0:number_of_particle_groups,dopts_num), & |
---|
| 117 | pts_value_l(0:number_of_particle_groups,dopts_num) ) |
---|
| 118 | |
---|
[1353] | 119 | pts_value_l = 0.0_wp |
---|
| 120 | pts_value_l(:,16) = 9999999.9_wp ! for calculation of minimum radius |
---|
[1] | 121 | |
---|
| 122 | ! |
---|
| 123 | !-- Calculate or collect the particle time series quantities for all particles |
---|
| 124 | !-- and seperately for each particle group (if there is more than one group) |
---|
[1359] | 125 | DO i = nxl, nxr |
---|
| 126 | DO j = nys, nyn |
---|
| 127 | DO k = nzb, nzt |
---|
| 128 | number_of_particles = prt_count(k,j,i) |
---|
| 129 | IF (number_of_particles <= 0) CYCLE |
---|
| 130 | particles => grid_particles(k,j,i)%particles(1:number_of_particles) |
---|
| 131 | DO n = 1, number_of_particles |
---|
[1] | 132 | |
---|
[1359] | 133 | IF ( particles(n)%particle_mask ) THEN ! Restrict analysis to active particles |
---|
[1] | 134 | |
---|
[1359] | 135 | pts_value_l(0,1) = pts_value_l(0,1) + 1.0_wp ! total # of particles |
---|
| 136 | pts_value_l(0,2) = pts_value_l(0,2) + & |
---|
| 137 | ( particles(n)%x - particles(n)%origin_x ) ! mean x |
---|
| 138 | pts_value_l(0,3) = pts_value_l(0,3) + & |
---|
| 139 | ( particles(n)%y - particles(n)%origin_y ) ! mean y |
---|
| 140 | pts_value_l(0,4) = pts_value_l(0,4) + & |
---|
| 141 | ( particles(n)%z - particles(n)%origin_z ) ! mean z |
---|
| 142 | pts_value_l(0,5) = pts_value_l(0,5) + particles(n)%z ! mean z (absolute) |
---|
| 143 | pts_value_l(0,6) = pts_value_l(0,6) + particles(n)%speed_x ! mean u |
---|
| 144 | pts_value_l(0,7) = pts_value_l(0,7) + particles(n)%speed_y ! mean v |
---|
| 145 | pts_value_l(0,8) = pts_value_l(0,8) + particles(n)%speed_z ! mean w |
---|
| 146 | IF ( .NOT. curvature_solution_effects ) THEN |
---|
| 147 | pts_value_l(0,9) = pts_value_l(0,9) + particles(n)%rvar1 ! mean sgsu |
---|
| 148 | pts_value_l(0,10) = pts_value_l(0,10) + particles(n)%rvar2 ! mean sgsv |
---|
| 149 | pts_value_l(0,11) = pts_value_l(0,11) + particles(n)%rvar3 ! mean sgsw |
---|
| 150 | ENDIF |
---|
| 151 | IF ( particles(n)%speed_z > 0.0_wp ) THEN |
---|
| 152 | pts_value_l(0,12) = pts_value_l(0,12) + 1.0_wp ! # of upward moving prts |
---|
| 153 | pts_value_l(0,13) = pts_value_l(0,13) + & |
---|
| 154 | particles(n)%speed_z ! mean w upw. |
---|
| 155 | ELSE |
---|
| 156 | pts_value_l(0,14) = pts_value_l(0,14) + & |
---|
| 157 | particles(n)%speed_z ! mean w down |
---|
| 158 | ENDIF |
---|
| 159 | pts_value_l(0,15) = pts_value_l(0,15) + particles(n)%radius ! mean rad |
---|
| 160 | pts_value_l(0,16) = MIN( pts_value_l(0,16), particles(n)%radius ) ! minrad |
---|
| 161 | pts_value_l(0,17) = MAX( pts_value_l(0,17), particles(n)%radius ) ! maxrad |
---|
| 162 | pts_value_l(0,18) = pts_value_l(0,18) + 1.0_wp |
---|
| 163 | pts_value_l(0,19) = pts_value_l(0,18) + 1.0_wp |
---|
[1] | 164 | ! |
---|
[1359] | 165 | !-- Repeat the same for the respective particle group |
---|
| 166 | IF ( number_of_particle_groups > 1 ) THEN |
---|
| 167 | jg = particles(n)%group |
---|
[1] | 168 | |
---|
[1359] | 169 | pts_value_l(jg,1) = pts_value_l(jg,1) + 1.0_wp |
---|
| 170 | pts_value_l(jg,2) = pts_value_l(jg,2) + & |
---|
| 171 | ( particles(n)%x - particles(n)%origin_x ) |
---|
| 172 | pts_value_l(jg,3) = pts_value_l(jg,3) + & |
---|
| 173 | ( particles(n)%y - particles(n)%origin_y ) |
---|
| 174 | pts_value_l(jg,4) = pts_value_l(jg,4) + & |
---|
| 175 | ( particles(n)%z - particles(n)%origin_z ) |
---|
| 176 | pts_value_l(jg,5) = pts_value_l(jg,5) + particles(n)%z |
---|
| 177 | pts_value_l(jg,6) = pts_value_l(jg,6) + particles(n)%speed_x |
---|
| 178 | pts_value_l(jg,7) = pts_value_l(jg,7) + particles(n)%speed_y |
---|
| 179 | pts_value_l(jg,8) = pts_value_l(jg,8) + particles(n)%speed_z |
---|
| 180 | IF ( .NOT. curvature_solution_effects ) THEN |
---|
| 181 | pts_value_l(jg,9) = pts_value_l(jg,9) + particles(n)%rvar1 |
---|
| 182 | pts_value_l(jg,10) = pts_value_l(jg,10) + particles(n)%rvar2 |
---|
| 183 | pts_value_l(jg,11) = pts_value_l(jg,11) + particles(n)%rvar3 |
---|
| 184 | ENDIF |
---|
| 185 | IF ( particles(n)%speed_z > 0.0_wp ) THEN |
---|
| 186 | pts_value_l(jg,12) = pts_value_l(jg,12) + 1.0_wp |
---|
| 187 | pts_value_l(jg,13) = pts_value_l(jg,13) + particles(n)%speed_z |
---|
| 188 | ELSE |
---|
| 189 | pts_value_l(jg,14) = pts_value_l(jg,14) + particles(n)%speed_z |
---|
| 190 | ENDIF |
---|
| 191 | pts_value_l(jg,15) = pts_value_l(jg,15) + particles(n)%radius |
---|
| 192 | pts_value_l(jg,16) = MIN( pts_value(jg,16), particles(n)%radius ) |
---|
| 193 | pts_value_l(jg,17) = MAX( pts_value(jg,17), particles(n)%radius ) |
---|
| 194 | pts_value_l(jg,18) = pts_value_l(jg,18) + 1.0_wp |
---|
| 195 | pts_value_l(jg,19) = pts_value_l(jg,19) + 1.0_wp |
---|
| 196 | ENDIF |
---|
[1] | 197 | |
---|
[1359] | 198 | ENDIF |
---|
[1] | 199 | |
---|
[1359] | 200 | ENDDO |
---|
| 201 | |
---|
| 202 | ENDDO |
---|
| 203 | ENDDO |
---|
[1] | 204 | ENDDO |
---|
| 205 | |
---|
[1359] | 206 | |
---|
[1] | 207 | #if defined( __parallel ) |
---|
| 208 | ! |
---|
| 209 | !-- Sum values of the subdomains |
---|
| 210 | inum = number_of_particle_groups + 1 |
---|
| 211 | |
---|
[622] | 212 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
---|
[824] | 213 | CALL MPI_ALLREDUCE( pts_value_l(0,1), pts_value(0,1), 15*inum, MPI_REAL, & |
---|
[1] | 214 | MPI_SUM, comm2d, ierr ) |
---|
[622] | 215 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
---|
[824] | 216 | CALL MPI_ALLREDUCE( pts_value_l(0,16), pts_value(0,16), inum, MPI_REAL, & |
---|
[825] | 217 | MPI_MIN, comm2d, ierr ) |
---|
| 218 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
---|
| 219 | CALL MPI_ALLREDUCE( pts_value_l(0,17), pts_value(0,17), inum, MPI_REAL, & |
---|
[1] | 220 | MPI_MAX, comm2d, ierr ) |
---|
[622] | 221 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
---|
[825] | 222 | CALL MPI_ALLREDUCE( pts_value_l(0,18), pts_value(0,18), inum, MPI_REAL, & |
---|
| 223 | MPI_MAX, comm2d, ierr ) |
---|
| 224 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
---|
| 225 | CALL MPI_ALLREDUCE( pts_value_l(0,19), pts_value(0,19), inum, MPI_REAL, & |
---|
[1] | 226 | MPI_MIN, comm2d, ierr ) |
---|
| 227 | #else |
---|
[825] | 228 | pts_value(:,1:19) = pts_value_l(:,1:19) |
---|
[1] | 229 | #endif |
---|
| 230 | |
---|
| 231 | ! |
---|
[825] | 232 | !-- Normalize the above calculated quantities (except min/max values) with the |
---|
| 233 | !-- total number of particles |
---|
[1] | 234 | IF ( number_of_particle_groups > 1 ) THEN |
---|
| 235 | inum = number_of_particle_groups |
---|
| 236 | ELSE |
---|
| 237 | inum = 0 |
---|
| 238 | ENDIF |
---|
| 239 | |
---|
| 240 | DO j = 0, inum |
---|
| 241 | |
---|
[1353] | 242 | IF ( pts_value(j,1) > 0.0_wp ) THEN |
---|
[1] | 243 | |
---|
[824] | 244 | pts_value(j,2:15) = pts_value(j,2:15) / pts_value(j,1) |
---|
[1353] | 245 | IF ( pts_value(j,12) > 0.0_wp .AND. pts_value(j,12) < 1.0_wp ) THEN |
---|
[1] | 246 | pts_value(j,13) = pts_value(j,13) / pts_value(j,12) |
---|
[1353] | 247 | pts_value(j,14) = pts_value(j,14) / ( 1.0_wp - pts_value(j,12) ) |
---|
| 248 | ELSEIF ( pts_value(j,12) == 0.0_wp ) THEN |
---|
| 249 | pts_value(j,13) = -1.0_wp |
---|
[1] | 250 | ELSE |
---|
[1353] | 251 | pts_value(j,14) = -1.0_wp |
---|
[1] | 252 | ENDIF |
---|
| 253 | |
---|
| 254 | ENDIF |
---|
| 255 | |
---|
| 256 | ENDDO |
---|
| 257 | |
---|
| 258 | ! |
---|
| 259 | !-- Calculate higher order moments of particle time series quantities, |
---|
| 260 | !-- seperately for each particle group (if there is more than one group) |
---|
[1359] | 261 | DO i = nxl, nxr |
---|
| 262 | DO j = nys, nyn |
---|
| 263 | DO k = nzb, nzt |
---|
| 264 | number_of_particles = prt_count(k,j,i) |
---|
| 265 | IF (number_of_particles <= 0) CYCLE |
---|
| 266 | particles => grid_particles(k,j,i)%particles(1:number_of_particles) |
---|
| 267 | DO n = 1, number_of_particles |
---|
[1] | 268 | |
---|
[1359] | 269 | pts_value_l(0,20) = pts_value_l(0,20) + ( particles(n)%x - & |
---|
| 270 | particles(n)%origin_x - pts_value(0,2) )**2 ! x*2 |
---|
| 271 | pts_value_l(0,21) = pts_value_l(0,21) + ( particles(n)%y - & |
---|
| 272 | particles(n)%origin_y - pts_value(0,3) )**2 ! y*2 |
---|
| 273 | pts_value_l(0,22) = pts_value_l(0,22) + ( particles(n)%z - & |
---|
| 274 | particles(n)%origin_z - pts_value(0,4) )**2 ! z*2 |
---|
| 275 | pts_value_l(0,23) = pts_value_l(0,23) + ( particles(n)%speed_x - & |
---|
| 276 | pts_value(0,6) )**2 ! u*2 |
---|
| 277 | pts_value_l(0,24) = pts_value_l(0,24) + ( particles(n)%speed_y - & |
---|
| 278 | pts_value(0,7) )**2 ! v*2 |
---|
| 279 | pts_value_l(0,25) = pts_value_l(0,25) + ( particles(n)%speed_z - & |
---|
| 280 | pts_value(0,8) )**2 ! w*2 |
---|
| 281 | IF ( .NOT. curvature_solution_effects ) THEN |
---|
| 282 | pts_value_l(0,26) = pts_value_l(0,26) + ( particles(n)%rvar1 - & |
---|
| 283 | pts_value(0,9) )**2 ! u"2 |
---|
| 284 | pts_value_l(0,27) = pts_value_l(0,27) + ( particles(n)%rvar2 - & |
---|
| 285 | pts_value(0,10) )**2 ! v"2 |
---|
| 286 | pts_value_l(0,28) = pts_value_l(0,28) + ( particles(n)%rvar3 - & |
---|
| 287 | pts_value(0,11) )**2 ! w"2 |
---|
| 288 | ENDIF |
---|
[1] | 289 | ! |
---|
[1359] | 290 | !-- Repeat the same for the respective particle group |
---|
| 291 | IF ( number_of_particle_groups > 1 ) THEN |
---|
| 292 | jg = particles(n)%group |
---|
[1] | 293 | |
---|
[1359] | 294 | pts_value_l(jg,20) = pts_value_l(jg,20) + ( particles(n)%x - & |
---|
| 295 | particles(n)%origin_x - pts_value(jg,2) )**2 |
---|
| 296 | pts_value_l(jg,21) = pts_value_l(jg,21) + ( particles(n)%y - & |
---|
| 297 | particles(n)%origin_y - pts_value(jg,3) )**2 |
---|
| 298 | pts_value_l(jg,22) = pts_value_l(jg,22) + ( particles(n)%z - & |
---|
| 299 | particles(n)%origin_z - pts_value(jg,4) )**2 |
---|
| 300 | pts_value_l(jg,23) = pts_value_l(jg,23) + ( particles(n)%speed_x - & |
---|
| 301 | pts_value(jg,6) )**2 |
---|
| 302 | pts_value_l(jg,24) = pts_value_l(jg,24) + ( particles(n)%speed_y - & |
---|
| 303 | pts_value(jg,7) )**2 |
---|
| 304 | pts_value_l(jg,25) = pts_value_l(jg,25) + ( particles(n)%speed_z - & |
---|
| 305 | pts_value(jg,8) )**2 |
---|
| 306 | IF ( .NOT. curvature_solution_effects ) THEN |
---|
| 307 | pts_value_l(jg,26) = pts_value_l(jg,26) + ( particles(n)%rvar1 - & |
---|
| 308 | pts_value(jg,9) )**2 |
---|
| 309 | pts_value_l(jg,27) = pts_value_l(jg,27) + ( particles(n)%rvar2 - & |
---|
| 310 | pts_value(jg,10) )**2 |
---|
| 311 | pts_value_l(jg,28) = pts_value_l(jg,28) + ( particles(n)%rvar3 - & |
---|
| 312 | pts_value(jg,11) )**2 |
---|
| 313 | ENDIF |
---|
| 314 | ENDIF |
---|
[1] | 315 | |
---|
[1359] | 316 | ENDDO |
---|
| 317 | ENDDO |
---|
| 318 | ENDDO |
---|
[1] | 319 | ENDDO |
---|
| 320 | |
---|
[825] | 321 | pts_value_l(0,29) = ( number_of_particles - pts_value(0,1) / numprocs )**2 |
---|
[1] | 322 | ! variance of particle numbers |
---|
| 323 | IF ( number_of_particle_groups > 1 ) THEN |
---|
| 324 | DO j = 1, number_of_particle_groups |
---|
[825] | 325 | pts_value_l(j,29) = ( pts_value_l(j,1) - & |
---|
[1] | 326 | pts_value(j,1) / numprocs )**2 |
---|
| 327 | ENDDO |
---|
| 328 | ENDIF |
---|
| 329 | |
---|
| 330 | #if defined( __parallel ) |
---|
| 331 | ! |
---|
| 332 | !-- Sum values of the subdomains |
---|
| 333 | inum = number_of_particle_groups + 1 |
---|
| 334 | |
---|
[622] | 335 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
---|
[825] | 336 | CALL MPI_ALLREDUCE( pts_value_l(0,20), pts_value(0,20), inum*10, MPI_REAL, & |
---|
[1] | 337 | MPI_SUM, comm2d, ierr ) |
---|
| 338 | #else |
---|
[825] | 339 | pts_value(:,20:29) = pts_value_l(:,20:29) |
---|
[1] | 340 | #endif |
---|
| 341 | |
---|
| 342 | ! |
---|
| 343 | !-- Normalize the above calculated quantities with the total number of |
---|
| 344 | !-- particles |
---|
| 345 | IF ( number_of_particle_groups > 1 ) THEN |
---|
| 346 | inum = number_of_particle_groups |
---|
| 347 | ELSE |
---|
| 348 | inum = 0 |
---|
| 349 | ENDIF |
---|
| 350 | |
---|
| 351 | DO j = 0, inum |
---|
| 352 | |
---|
[1353] | 353 | IF ( pts_value(j,1) > 0.0_wp ) THEN |
---|
[825] | 354 | pts_value(j,20:28) = pts_value(j,20:28) / pts_value(j,1) |
---|
[1] | 355 | ENDIF |
---|
[825] | 356 | pts_value(j,29) = pts_value(j,29) / numprocs |
---|
[1] | 357 | |
---|
| 358 | ENDDO |
---|
| 359 | |
---|
| 360 | #if defined( __netcdf ) |
---|
| 361 | ! |
---|
| 362 | !-- Output particle time series quantities in NetCDF format |
---|
[1327] | 363 | IF ( myid == 0 ) THEN |
---|
[1] | 364 | DO j = 0, inum |
---|
| 365 | DO i = 1, dopts_num |
---|
| 366 | nc_stat = NF90_PUT_VAR( id_set_pts, id_var_dopts(i,j), & |
---|
| 367 | (/ pts_value(j,i) /), & |
---|
| 368 | start = (/ dopts_time_count /), & |
---|
| 369 | count = (/ 1 /) ) |
---|
[263] | 370 | CALL handle_netcdf_error( 'data_output_ptseries', 392 ) |
---|
[1] | 371 | ENDDO |
---|
| 372 | ENDDO |
---|
| 373 | ENDIF |
---|
| 374 | #endif |
---|
| 375 | |
---|
[825] | 376 | DEALLOCATE( pts_value, pts_value_l ) |
---|
| 377 | |
---|
[1318] | 378 | CALL cpu_log( log_point(36), 'data_output_ptseries', 'stop' ) |
---|
[1] | 379 | |
---|
| 380 | END SUBROUTINE data_output_ptseries |
---|