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source: palm/trunk/SOURCE/data_output_ptseries.f90 @ 2201

Last change on this file since 2201 was 2101, checked in by suehring, 8 years ago
last commit documented
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File size: 16.9 KB

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[1682]	1	!> @file data_output_ptseries.f90
[2000]	2	!------------------------------------------------------------------------------!
[1036]	3	! This file is part of PALM.
	4	!
[2000]	5	! PALM is free software: you can redistribute it and/or modify it under the
	6	! terms of the GNU General Public License as published by the Free Software
	7	! Foundation, either version 3 of the License, or (at your option) any later
	8	! version.
[1036]	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	!
[2101]	17	! Copyright 1997-2017 Leibniz Universitaet Hannover
[2000]	18	!------------------------------------------------------------------------------!
[1036]	19	!
[263]	20	! Current revisions:
[1]	21	! -----------------
[2001]	22	!
	23	!
[1321]	24	! Former revisions:
	25	! -----------------
	26	! $Id: data_output_ptseries.f90 2101 2017-01-05 16:42:31Z suehring $
	27	!
[2001]	28	! 2000 2016-08-20 18:09:15Z knoop
	29	! Forced header and separation lines into 80 columns
	30	!
[1832]	31	! 1831 2016-04-07 13:15:51Z hoffmann
	32	! curvature_solution_effects moved to particle_attributes
	33	!
[1784]	34	! 1783 2016-03-06 18:36:17Z raasch
	35	! netcdf module name changed + related changes
	36	!
[1683]	37	! 1682 2015-10-07 23:56:08Z knoop
	38	! Code annotations made doxygen readable
	39	!
[1360]	40	! 1359 2014-04-11 17:15:14Z hoffmann
	41	! New particle structure integrated.
	42	!
[1354]	43	! 1353 2014-04-08 15:21:23Z heinze
	44	! REAL constants provided with KIND-attribute
	45	!
[1329]	46	! 1327 2014-03-21 11:00:16Z raasch
	47	! -netcdf output queries
	48	!
[1321]	49	! 1320 2014-03-20 08:40:49Z raasch
[1320]	50	! ONLY-attribute added to USE-statements,
	51	! kind-parameters added to all INTEGER and REAL declaration statements,
	52	! kinds are defined in new module kinds,
	53	! revision history before 2012 removed,
	54	! comment fields (!:) to be used for variable explanations added to
	55	! all variable declaration statements
[1]	56	!
[1319]	57	! 1318 2014-03-17 13:35:16Z raasch
	58	! barrier argument removed from cpu_log,
	59	! module interfaces removed
	60	!
[1037]	61	! 1036 2012-10-22 13:43:42Z raasch
	62	! code put under GPL (PALM 3.9)
	63	!
[826]	64	! 825 2012-02-19 03:03:44Z raasch
	65	! mean/minimum/maximum particle radius added as output quantity,
	66	! particle attributes speed_x\|y\|z_sgs renamed rvar1\|2\|3
	67	!
[1]	68	! Revision 1.1 2006/08/04 14:24:18 raasch
	69	! Initial revision
	70	!
	71	!
	72	! Description:
	73	! ------------
[1682]	74	!> Output of particle data timeseries in NetCDF format.
[1]	75	!------------------------------------------------------------------------------!
[1682]	76	SUBROUTINE data_output_ptseries
	77
[1]	78
[1320]	79	USE control_parameters, &
[1327]	80	ONLY: dopts_time_count, time_since_reference_point
[1320]	81
	82	USE cpulog, &
	83	ONLY: cpu_log, log_point
	84
	85	USE indices, &
[1359]	86	ONLY: nxl, nxr, nys, nyn, nzb, nzt
[1320]	87
	88	USE kinds
	89
[1783]	90	#if defined( __netcdf )
	91	USE NETCDF
	92	#endif
[1320]	93
[1783]	94	USE netcdf_interface, &
	95	ONLY: dopts_num, id_set_pts, id_var_dopts, id_var_time_pts, nc_stat, &
	96	netcdf_handle_error
	97
[1320]	98	USE particle_attributes, &
[1831]	99	ONLY: curvature_solution_effects, grid_particles, number_of_particles,&
	100	number_of_particle_groups, particles, prt_count
[1320]	101
[1]	102	USE pegrid
	103
	104	IMPLICIT NONE
	105
	106
[1682]	107	INTEGER(iwp) :: i !<
	108	INTEGER(iwp) :: inum !<
	109	INTEGER(iwp) :: j !<
	110	INTEGER(iwp) :: jg !<
	111	INTEGER(iwp) :: k !<
	112	INTEGER(iwp) :: n !<
[1]	113
[1682]	114	REAL(wp), DIMENSION(:,:), ALLOCATABLE :: pts_value !<
	115	REAL(wp), DIMENSION(:,:), ALLOCATABLE :: pts_value_l !<
[1]	116
	117
	118	CALL cpu_log( log_point(36), 'data_output_ptseries', 'start' )
	119
[1327]	120	IF ( myid == 0 ) THEN
[1]	121	!
	122	!-- Open file for time series output in NetCDF format
	123	dopts_time_count = dopts_time_count + 1
	124	CALL check_open( 109 )
	125	#if defined( __netcdf )
	126	!
	127	!-- Update the particle time series time axis
[291]	128	nc_stat = NF90_PUT_VAR( id_set_pts, id_var_time_pts, &
	129	(/ time_since_reference_point /), &
[1]	130	start = (/ dopts_time_count /), count = (/ 1 /) )
[1783]	131	CALL netcdf_handle_error( 'data_output_ptseries', 391 )
[1]	132	#endif
	133
	134	ENDIF
	135
[825]	136	ALLOCATE( pts_value(0:number_of_particle_groups,dopts_num), &
	137	pts_value_l(0:number_of_particle_groups,dopts_num) )
	138
[1353]	139	pts_value_l = 0.0_wp
	140	pts_value_l(:,16) = 9999999.9_wp ! for calculation of minimum radius
[1]	141
	142	!
	143	!-- Calculate or collect the particle time series quantities for all particles
	144	!-- and seperately for each particle group (if there is more than one group)
[1359]	145	DO i = nxl, nxr
	146	DO j = nys, nyn
	147	DO k = nzb, nzt
	148	number_of_particles = prt_count(k,j,i)
	149	IF (number_of_particles <= 0) CYCLE
	150	particles => grid_particles(k,j,i)%particles(1:number_of_particles)
	151	DO n = 1, number_of_particles
[1]	152
[1359]	153	IF ( particles(n)%particle_mask ) THEN ! Restrict analysis to active particles
[1]	154
[1359]	155	pts_value_l(0,1) = pts_value_l(0,1) + 1.0_wp ! total # of particles
	156	pts_value_l(0,2) = pts_value_l(0,2) + &
	157	( particles(n)%x - particles(n)%origin_x ) ! mean x
	158	pts_value_l(0,3) = pts_value_l(0,3) + &
	159	( particles(n)%y - particles(n)%origin_y ) ! mean y
	160	pts_value_l(0,4) = pts_value_l(0,4) + &
	161	( particles(n)%z - particles(n)%origin_z ) ! mean z
	162	pts_value_l(0,5) = pts_value_l(0,5) + particles(n)%z ! mean z (absolute)
	163	pts_value_l(0,6) = pts_value_l(0,6) + particles(n)%speed_x ! mean u
	164	pts_value_l(0,7) = pts_value_l(0,7) + particles(n)%speed_y ! mean v
	165	pts_value_l(0,8) = pts_value_l(0,8) + particles(n)%speed_z ! mean w
	166	IF ( .NOT. curvature_solution_effects ) THEN
	167	pts_value_l(0,9) = pts_value_l(0,9) + particles(n)%rvar1 ! mean sgsu
	168	pts_value_l(0,10) = pts_value_l(0,10) + particles(n)%rvar2 ! mean sgsv
	169	pts_value_l(0,11) = pts_value_l(0,11) + particles(n)%rvar3 ! mean sgsw
	170	ENDIF
	171	IF ( particles(n)%speed_z > 0.0_wp ) THEN
	172	pts_value_l(0,12) = pts_value_l(0,12) + 1.0_wp ! # of upward moving prts
	173	pts_value_l(0,13) = pts_value_l(0,13) + &
	174	particles(n)%speed_z ! mean w upw.
	175	ELSE
	176	pts_value_l(0,14) = pts_value_l(0,14) + &
	177	particles(n)%speed_z ! mean w down
	178	ENDIF
	179	pts_value_l(0,15) = pts_value_l(0,15) + particles(n)%radius ! mean rad
	180	pts_value_l(0,16) = MIN( pts_value_l(0,16), particles(n)%radius ) ! minrad
	181	pts_value_l(0,17) = MAX( pts_value_l(0,17), particles(n)%radius ) ! maxrad
	182	pts_value_l(0,18) = pts_value_l(0,18) + 1.0_wp
	183	pts_value_l(0,19) = pts_value_l(0,18) + 1.0_wp
[1]	184	!
[1359]	185	!-- Repeat the same for the respective particle group
	186	IF ( number_of_particle_groups > 1 ) THEN
	187	jg = particles(n)%group
[1]	188
[1359]	189	pts_value_l(jg,1) = pts_value_l(jg,1) + 1.0_wp
	190	pts_value_l(jg,2) = pts_value_l(jg,2) + &
	191	( particles(n)%x - particles(n)%origin_x )
	192	pts_value_l(jg,3) = pts_value_l(jg,3) + &
	193	( particles(n)%y - particles(n)%origin_y )
	194	pts_value_l(jg,4) = pts_value_l(jg,4) + &
	195	( particles(n)%z - particles(n)%origin_z )
	196	pts_value_l(jg,5) = pts_value_l(jg,5) + particles(n)%z
	197	pts_value_l(jg,6) = pts_value_l(jg,6) + particles(n)%speed_x
	198	pts_value_l(jg,7) = pts_value_l(jg,7) + particles(n)%speed_y
	199	pts_value_l(jg,8) = pts_value_l(jg,8) + particles(n)%speed_z
	200	IF ( .NOT. curvature_solution_effects ) THEN
	201	pts_value_l(jg,9) = pts_value_l(jg,9) + particles(n)%rvar1
	202	pts_value_l(jg,10) = pts_value_l(jg,10) + particles(n)%rvar2
	203	pts_value_l(jg,11) = pts_value_l(jg,11) + particles(n)%rvar3
	204	ENDIF
	205	IF ( particles(n)%speed_z > 0.0_wp ) THEN
	206	pts_value_l(jg,12) = pts_value_l(jg,12) + 1.0_wp
	207	pts_value_l(jg,13) = pts_value_l(jg,13) + particles(n)%speed_z
	208	ELSE
	209	pts_value_l(jg,14) = pts_value_l(jg,14) + particles(n)%speed_z
	210	ENDIF
	211	pts_value_l(jg,15) = pts_value_l(jg,15) + particles(n)%radius
	212	pts_value_l(jg,16) = MIN( pts_value(jg,16), particles(n)%radius )
	213	pts_value_l(jg,17) = MAX( pts_value(jg,17), particles(n)%radius )
	214	pts_value_l(jg,18) = pts_value_l(jg,18) + 1.0_wp
	215	pts_value_l(jg,19) = pts_value_l(jg,19) + 1.0_wp
	216	ENDIF
[1]	217
[1359]	218	ENDIF
[1]	219
[1359]	220	ENDDO
	221
	222	ENDDO
	223	ENDDO
[1]	224	ENDDO
	225
[1359]	226
[1]	227	#if defined( __parallel )
	228	!
	229	!-- Sum values of the subdomains
	230	inum = number_of_particle_groups + 1
	231
[622]	232	IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr )
[824]	233	CALL MPI_ALLREDUCE( pts_value_l(0,1), pts_value(0,1), 15*inum, MPI_REAL, &
[1]	234	MPI_SUM, comm2d, ierr )
[622]	235	IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr )
[824]	236	CALL MPI_ALLREDUCE( pts_value_l(0,16), pts_value(0,16), inum, MPI_REAL, &
[825]	237	MPI_MIN, comm2d, ierr )
	238	IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr )
	239	CALL MPI_ALLREDUCE( pts_value_l(0,17), pts_value(0,17), inum, MPI_REAL, &
[1]	240	MPI_MAX, comm2d, ierr )
[622]	241	IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr )
[825]	242	CALL MPI_ALLREDUCE( pts_value_l(0,18), pts_value(0,18), inum, MPI_REAL, &
	243	MPI_MAX, comm2d, ierr )
	244	IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr )
	245	CALL MPI_ALLREDUCE( pts_value_l(0,19), pts_value(0,19), inum, MPI_REAL, &
[1]	246	MPI_MIN, comm2d, ierr )
	247	#else
[825]	248	pts_value(:,1:19) = pts_value_l(:,1:19)
[1]	249	#endif
	250
	251	!
[825]	252	!-- Normalize the above calculated quantities (except min/max values) with the
	253	!-- total number of particles
[1]	254	IF ( number_of_particle_groups > 1 ) THEN
	255	inum = number_of_particle_groups
	256	ELSE
	257	inum = 0
	258	ENDIF
	259
	260	DO j = 0, inum
	261
[1353]	262	IF ( pts_value(j,1) > 0.0_wp ) THEN
[1]	263
[824]	264	pts_value(j,2:15) = pts_value(j,2:15) / pts_value(j,1)
[1353]	265	IF ( pts_value(j,12) > 0.0_wp .AND. pts_value(j,12) < 1.0_wp ) THEN
[1]	266	pts_value(j,13) = pts_value(j,13) / pts_value(j,12)
[1353]	267	pts_value(j,14) = pts_value(j,14) / ( 1.0_wp - pts_value(j,12) )
	268	ELSEIF ( pts_value(j,12) == 0.0_wp ) THEN
	269	pts_value(j,13) = -1.0_wp
[1]	270	ELSE
[1353]	271	pts_value(j,14) = -1.0_wp
[1]	272	ENDIF
	273
	274	ENDIF
	275
	276	ENDDO
	277
	278	!
	279	!-- Calculate higher order moments of particle time series quantities,
	280	!-- seperately for each particle group (if there is more than one group)
[1359]	281	DO i = nxl, nxr
	282	DO j = nys, nyn
	283	DO k = nzb, nzt
	284	number_of_particles = prt_count(k,j,i)
	285	IF (number_of_particles <= 0) CYCLE
	286	particles => grid_particles(k,j,i)%particles(1:number_of_particles)
	287	DO n = 1, number_of_particles
[1]	288
[1359]	289	pts_value_l(0,20) = pts_value_l(0,20) + ( particles(n)%x - &
	290	particles(n)%origin_x - pts_value(0,2) )*2 ! x2
	291	pts_value_l(0,21) = pts_value_l(0,21) + ( particles(n)%y - &
	292	particles(n)%origin_y - pts_value(0,3) )*2 ! y2
	293	pts_value_l(0,22) = pts_value_l(0,22) + ( particles(n)%z - &
	294	particles(n)%origin_z - pts_value(0,4) )*2 ! z2
	295	pts_value_l(0,23) = pts_value_l(0,23) + ( particles(n)%speed_x - &
	296	pts_value(0,6) )*2 ! u2
	297	pts_value_l(0,24) = pts_value_l(0,24) + ( particles(n)%speed_y - &
	298	pts_value(0,7) )*2 ! v2
	299	pts_value_l(0,25) = pts_value_l(0,25) + ( particles(n)%speed_z - &
	300	pts_value(0,8) )*2 ! w2
	301	IF ( .NOT. curvature_solution_effects ) THEN
	302	pts_value_l(0,26) = pts_value_l(0,26) + ( particles(n)%rvar1 - &
	303	pts_value(0,9) )**2 ! u"2
	304	pts_value_l(0,27) = pts_value_l(0,27) + ( particles(n)%rvar2 - &
	305	pts_value(0,10) )**2 ! v"2
	306	pts_value_l(0,28) = pts_value_l(0,28) + ( particles(n)%rvar3 - &
	307	pts_value(0,11) )**2 ! w"2
	308	ENDIF
[1]	309	!
[1359]	310	!-- Repeat the same for the respective particle group
	311	IF ( number_of_particle_groups > 1 ) THEN
	312	jg = particles(n)%group
[1]	313
[1359]	314	pts_value_l(jg,20) = pts_value_l(jg,20) + ( particles(n)%x - &
	315	particles(n)%origin_x - pts_value(jg,2) )**2
	316	pts_value_l(jg,21) = pts_value_l(jg,21) + ( particles(n)%y - &
	317	particles(n)%origin_y - pts_value(jg,3) )**2
	318	pts_value_l(jg,22) = pts_value_l(jg,22) + ( particles(n)%z - &
	319	particles(n)%origin_z - pts_value(jg,4) )**2
	320	pts_value_l(jg,23) = pts_value_l(jg,23) + ( particles(n)%speed_x - &
	321	pts_value(jg,6) )**2
	322	pts_value_l(jg,24) = pts_value_l(jg,24) + ( particles(n)%speed_y - &
	323	pts_value(jg,7) )**2
	324	pts_value_l(jg,25) = pts_value_l(jg,25) + ( particles(n)%speed_z - &
	325	pts_value(jg,8) )**2
	326	IF ( .NOT. curvature_solution_effects ) THEN
	327	pts_value_l(jg,26) = pts_value_l(jg,26) + ( particles(n)%rvar1 - &
	328	pts_value(jg,9) )**2
	329	pts_value_l(jg,27) = pts_value_l(jg,27) + ( particles(n)%rvar2 - &
	330	pts_value(jg,10) )**2
	331	pts_value_l(jg,28) = pts_value_l(jg,28) + ( particles(n)%rvar3 - &
	332	pts_value(jg,11) )**2
	333	ENDIF
	334	ENDIF
[1]	335
[1359]	336	ENDDO
	337	ENDDO
	338	ENDDO
[1]	339	ENDDO
	340
[825]	341	pts_value_l(0,29) = ( number_of_particles - pts_value(0,1) / numprocs )**2
[1]	342	! variance of particle numbers
	343	IF ( number_of_particle_groups > 1 ) THEN
	344	DO j = 1, number_of_particle_groups
[825]	345	pts_value_l(j,29) = ( pts_value_l(j,1) - &
[1]	346	pts_value(j,1) / numprocs )**2
	347	ENDDO
	348	ENDIF
	349
	350	#if defined( __parallel )
	351	!
	352	!-- Sum values of the subdomains
	353	inum = number_of_particle_groups + 1
	354
[622]	355	IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr )
[825]	356	CALL MPI_ALLREDUCE( pts_value_l(0,20), pts_value(0,20), inum*10, MPI_REAL, &
[1]	357	MPI_SUM, comm2d, ierr )
	358	#else
[825]	359	pts_value(:,20:29) = pts_value_l(:,20:29)
[1]	360	#endif
	361
	362	!
	363	!-- Normalize the above calculated quantities with the total number of
	364	!-- particles
	365	IF ( number_of_particle_groups > 1 ) THEN
	366	inum = number_of_particle_groups
	367	ELSE
	368	inum = 0
	369	ENDIF
	370
	371	DO j = 0, inum
	372
[1353]	373	IF ( pts_value(j,1) > 0.0_wp ) THEN
[825]	374	pts_value(j,20:28) = pts_value(j,20:28) / pts_value(j,1)
[1]	375	ENDIF
[825]	376	pts_value(j,29) = pts_value(j,29) / numprocs
[1]	377
	378	ENDDO
	379
	380	#if defined( __netcdf )
	381	!
	382	!-- Output particle time series quantities in NetCDF format
[1327]	383	IF ( myid == 0 ) THEN
[1]	384	DO j = 0, inum
	385	DO i = 1, dopts_num
	386	nc_stat = NF90_PUT_VAR( id_set_pts, id_var_dopts(i,j), &
	387	(/ pts_value(j,i) /), &
	388	start = (/ dopts_time_count /), &
	389	count = (/ 1 /) )
[1783]	390	CALL netcdf_handle_error( 'data_output_ptseries', 392 )
[1]	391	ENDDO
	392	ENDDO
	393	ENDIF
	394	#endif
	395
[825]	396	DEALLOCATE( pts_value, pts_value_l )
	397
[1318]	398	CALL cpu_log( log_point(36), 'data_output_ptseries', 'stop' )
[1]	399
	400	END SUBROUTINE data_output_ptseries

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