1 | SUBROUTINE data_output_ptseries |
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2 | |
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3 | !--------------------------------------------------------------------------------! |
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4 | ! This file is part of PALM. |
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5 | ! |
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6 | ! PALM is free software: you can redistribute it and/or modify it under the terms |
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7 | ! of the GNU General Public License as published by the Free Software Foundation, |
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8 | ! either version 3 of the License, or (at your option) any later version. |
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9 | ! |
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10 | ! PALM is distributed in the hope that it will be useful, but WITHOUT ANY |
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11 | ! WARRANTY; without even the implied warranty of MERCHANTABILITY or FITNESS FOR |
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12 | ! A PARTICULAR PURPOSE. See the GNU General Public License for more details. |
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13 | ! |
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14 | ! You should have received a copy of the GNU General Public License along with |
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15 | ! PALM. If not, see <http://www.gnu.org/licenses/>. |
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16 | ! |
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17 | ! Copyright 1997-2014 Leibniz Universitaet Hannover |
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18 | !--------------------------------------------------------------------------------! |
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19 | ! |
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20 | ! Current revisions: |
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21 | ! ----------------- |
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22 | ! |
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23 | ! |
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24 | ! Former revisions: |
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25 | ! ----------------- |
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26 | ! $Id: data_output_ptseries.f90 1329 2014-03-21 11:09:15Z suehring $ |
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27 | ! |
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28 | ! 1327 2014-03-21 11:00:16Z raasch |
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29 | ! -netcdf output queries |
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30 | ! |
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31 | ! 1320 2014-03-20 08:40:49Z raasch |
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32 | ! ONLY-attribute added to USE-statements, |
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33 | ! kind-parameters added to all INTEGER and REAL declaration statements, |
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34 | ! kinds are defined in new module kinds, |
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35 | ! revision history before 2012 removed, |
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36 | ! comment fields (!:) to be used for variable explanations added to |
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37 | ! all variable declaration statements |
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38 | ! |
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39 | ! 1318 2014-03-17 13:35:16Z raasch |
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40 | ! barrier argument removed from cpu_log, |
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41 | ! module interfaces removed |
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42 | ! |
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43 | ! 1036 2012-10-22 13:43:42Z raasch |
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44 | ! code put under GPL (PALM 3.9) |
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45 | ! |
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46 | ! 825 2012-02-19 03:03:44Z raasch |
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47 | ! mean/minimum/maximum particle radius added as output quantity, |
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48 | ! particle attributes speed_x|y|z_sgs renamed rvar1|2|3 |
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49 | ! |
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50 | ! Revision 1.1 2006/08/04 14:24:18 raasch |
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51 | ! Initial revision |
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52 | ! |
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53 | ! |
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54 | ! Description: |
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55 | ! ------------ |
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56 | ! Output of particle data timeseries in NetCDF format. |
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57 | !------------------------------------------------------------------------------! |
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58 | |
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59 | USE cloud_parameters, & |
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60 | ONLY: curvature_solution_effects |
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61 | |
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62 | USE control_parameters, & |
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63 | ONLY: dopts_time_count, time_since_reference_point |
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64 | |
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65 | USE cpulog, & |
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66 | ONLY: cpu_log, log_point |
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67 | |
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68 | USE indices, & |
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69 | ONLY: |
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70 | |
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71 | USE kinds |
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72 | |
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73 | USE netcdf_control |
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74 | |
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75 | USE particle_attributes, & |
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76 | ONLY: number_of_particles, number_of_particle_groups, particles |
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77 | |
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78 | USE pegrid |
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79 | |
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80 | IMPLICIT NONE |
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81 | |
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82 | |
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83 | INTEGER(iwp) :: i !: |
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84 | INTEGER(iwp) :: inum !: |
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85 | INTEGER(iwp) :: j !: |
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86 | INTEGER(iwp) :: n !: |
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87 | |
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88 | REAL(wp), DIMENSION(:,:), ALLOCATABLE :: pts_value !: |
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89 | REAL(wp), DIMENSION(:,:), ALLOCATABLE :: pts_value_l !: |
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90 | |
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91 | |
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92 | CALL cpu_log( log_point(36), 'data_output_ptseries', 'start' ) |
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93 | |
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94 | IF ( myid == 0 ) THEN |
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95 | ! |
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96 | !-- Open file for time series output in NetCDF format |
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97 | dopts_time_count = dopts_time_count + 1 |
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98 | CALL check_open( 109 ) |
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99 | #if defined( __netcdf ) |
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100 | ! |
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101 | !-- Update the particle time series time axis |
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102 | nc_stat = NF90_PUT_VAR( id_set_pts, id_var_time_pts, & |
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103 | (/ time_since_reference_point /), & |
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104 | start = (/ dopts_time_count /), count = (/ 1 /) ) |
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105 | CALL handle_netcdf_error( 'data_output_ptseries', 391 ) |
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106 | #endif |
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107 | |
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108 | ENDIF |
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109 | |
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110 | ALLOCATE( pts_value(0:number_of_particle_groups,dopts_num), & |
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111 | pts_value_l(0:number_of_particle_groups,dopts_num) ) |
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112 | |
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113 | pts_value_l = 0.0 |
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114 | pts_value_l(:,16) = 9999999.9 ! for calculation of minimum radius |
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115 | |
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116 | ! |
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117 | !-- Calculate or collect the particle time series quantities for all particles |
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118 | !-- and seperately for each particle group (if there is more than one group) |
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119 | DO n = 1, number_of_particles |
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120 | |
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121 | pts_value_l(0,1) = number_of_particles ! total # of particles |
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122 | pts_value_l(0,2) = pts_value_l(0,2) + & |
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123 | ( particles(n)%x - particles(n)%origin_x ) ! mean x |
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124 | pts_value_l(0,3) = pts_value_l(0,3) + & |
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125 | ( particles(n)%y - particles(n)%origin_y ) ! mean y |
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126 | pts_value_l(0,4) = pts_value_l(0,4) + & |
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127 | ( particles(n)%z - particles(n)%origin_z ) ! mean z |
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128 | pts_value_l(0,5) = pts_value_l(0,5) + particles(n)%z ! mean z (absolute) |
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129 | pts_value_l(0,6) = pts_value_l(0,6) + particles(n)%speed_x ! mean u |
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130 | pts_value_l(0,7) = pts_value_l(0,7) + particles(n)%speed_y ! mean v |
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131 | pts_value_l(0,8) = pts_value_l(0,8) + particles(n)%speed_z ! mean w |
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132 | IF ( .NOT. curvature_solution_effects ) THEN |
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133 | pts_value_l(0,9) = pts_value_l(0,9) + particles(n)%rvar1 ! mean sgsu |
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134 | pts_value_l(0,10) = pts_value_l(0,10) + particles(n)%rvar2 ! mean sgsv |
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135 | pts_value_l(0,11) = pts_value_l(0,11) + particles(n)%rvar3 ! mean sgsw |
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136 | ENDIF |
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137 | IF ( particles(n)%speed_z > 0.0 ) THEN |
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138 | pts_value_l(0,12) = pts_value_l(0,12) + 1.0 ! # of upward moving prts |
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139 | pts_value_l(0,13) = pts_value_l(0,13) + & |
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140 | particles(n)%speed_z ! mean w upw. |
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141 | ELSE |
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142 | pts_value_l(0,14) = pts_value_l(0,14) + & |
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143 | particles(n)%speed_z ! mean w down |
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144 | ENDIF |
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145 | pts_value_l(0,15) = pts_value_l(0,15) + particles(n)%radius ! mean rad |
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146 | pts_value_l(0,16) = MIN( pts_value_l(0,16), particles(n)%radius ) ! minrad |
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147 | pts_value_l(0,17) = MAX( pts_value_l(0,17), particles(n)%radius ) ! maxrad |
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148 | pts_value_l(0,18) = number_of_particles |
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149 | pts_value_l(0,19) = number_of_particles |
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150 | |
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151 | ! |
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152 | !-- Repeat the same for the respective particle group |
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153 | IF ( number_of_particle_groups > 1 ) THEN |
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154 | j = particles(n)%group |
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155 | |
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156 | pts_value_l(j,1) = pts_value_l(j,1) + 1 |
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157 | pts_value_l(j,2) = pts_value_l(j,2) + & |
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158 | ( particles(n)%x - particles(n)%origin_x ) |
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159 | pts_value_l(j,3) = pts_value_l(j,3) + & |
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160 | ( particles(n)%y - particles(n)%origin_y ) |
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161 | pts_value_l(j,4) = pts_value_l(j,4) + & |
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162 | ( particles(n)%z - particles(n)%origin_z ) |
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163 | pts_value_l(j,5) = pts_value_l(j,5) + particles(n)%z |
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164 | pts_value_l(j,6) = pts_value_l(j,6) + particles(n)%speed_x |
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165 | pts_value_l(j,7) = pts_value_l(j,7) + particles(n)%speed_y |
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166 | pts_value_l(j,8) = pts_value_l(j,8) + particles(n)%speed_z |
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167 | IF ( .NOT. curvature_solution_effects ) THEN |
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168 | pts_value_l(j,9) = pts_value_l(j,9) + particles(n)%rvar1 |
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169 | pts_value_l(j,10) = pts_value_l(j,10) + particles(n)%rvar2 |
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170 | pts_value_l(j,11) = pts_value_l(j,11) + particles(n)%rvar3 |
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171 | ENDIF |
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172 | IF ( particles(n)%speed_z > 0.0 ) THEN |
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173 | pts_value_l(j,12) = pts_value_l(j,12) + 1.0 |
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174 | pts_value_l(j,13) = pts_value_l(j,13) + particles(n)%speed_z |
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175 | ELSE |
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176 | pts_value_l(j,14) = pts_value_l(j,14) + particles(n)%speed_z |
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177 | ENDIF |
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178 | pts_value_l(j,15) = pts_value_l(j,15) + particles(n)%radius |
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179 | pts_value_l(j,16) = MIN( pts_value(j,16), particles(n)%radius ) |
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180 | pts_value_l(j,17) = MAX( pts_value(j,17), particles(n)%radius ) |
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181 | pts_value_l(j,18) = pts_value_l(j,18) + 1.0 |
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182 | pts_value_l(j,19) = pts_value_l(j,19) + 1.0 |
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183 | |
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184 | ENDIF |
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185 | |
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186 | ENDDO |
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187 | |
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188 | #if defined( __parallel ) |
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189 | ! |
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190 | !-- Sum values of the subdomains |
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191 | inum = number_of_particle_groups + 1 |
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192 | |
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193 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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194 | CALL MPI_ALLREDUCE( pts_value_l(0,1), pts_value(0,1), 15*inum, MPI_REAL, & |
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195 | MPI_SUM, comm2d, ierr ) |
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196 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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197 | CALL MPI_ALLREDUCE( pts_value_l(0,16), pts_value(0,16), inum, MPI_REAL, & |
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198 | MPI_MIN, comm2d, ierr ) |
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199 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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200 | CALL MPI_ALLREDUCE( pts_value_l(0,17), pts_value(0,17), inum, MPI_REAL, & |
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201 | MPI_MAX, comm2d, ierr ) |
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202 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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203 | CALL MPI_ALLREDUCE( pts_value_l(0,18), pts_value(0,18), inum, MPI_REAL, & |
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204 | MPI_MAX, comm2d, ierr ) |
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205 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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206 | CALL MPI_ALLREDUCE( pts_value_l(0,19), pts_value(0,19), inum, MPI_REAL, & |
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207 | MPI_MIN, comm2d, ierr ) |
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208 | #else |
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209 | pts_value(:,1:19) = pts_value_l(:,1:19) |
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210 | #endif |
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211 | |
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212 | ! |
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213 | !-- Normalize the above calculated quantities (except min/max values) with the |
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214 | !-- total number of particles |
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215 | IF ( number_of_particle_groups > 1 ) THEN |
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216 | inum = number_of_particle_groups |
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217 | ELSE |
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218 | inum = 0 |
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219 | ENDIF |
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220 | |
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221 | DO j = 0, inum |
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222 | |
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223 | IF ( pts_value(j,1) > 0.0 ) THEN |
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224 | |
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225 | pts_value(j,2:15) = pts_value(j,2:15) / pts_value(j,1) |
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226 | IF ( pts_value(j,12) > 0.0 .AND. pts_value(j,12) < 1.0 ) THEN |
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227 | pts_value(j,13) = pts_value(j,13) / pts_value(j,12) |
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228 | pts_value(j,14) = pts_value(j,14) / ( 1.0 - pts_value(j,12) ) |
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229 | ELSEIF ( pts_value(j,12) == 0.0 ) THEN |
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230 | pts_value(j,13) = -1.0 |
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231 | ELSE |
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232 | pts_value(j,14) = -1.0 |
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233 | ENDIF |
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234 | |
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235 | ENDIF |
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236 | |
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237 | ENDDO |
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238 | |
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239 | ! |
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240 | !-- Calculate higher order moments of particle time series quantities, |
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241 | !-- seperately for each particle group (if there is more than one group) |
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242 | DO n = 1, number_of_particles |
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243 | |
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244 | pts_value_l(0,20) = pts_value_l(0,20) + ( particles(n)%x - & |
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245 | particles(n)%origin_x - pts_value(0,2) )**2 ! x*2 |
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246 | pts_value_l(0,21) = pts_value_l(0,21) + ( particles(n)%y - & |
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247 | particles(n)%origin_y - pts_value(0,3) )**2 ! y*2 |
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248 | pts_value_l(0,22) = pts_value_l(0,22) + ( particles(n)%z - & |
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249 | particles(n)%origin_z - pts_value(0,4) )**2 ! z*2 |
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250 | pts_value_l(0,23) = pts_value_l(0,23) + ( particles(n)%speed_x - & |
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251 | pts_value(0,6) )**2 ! u*2 |
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252 | pts_value_l(0,24) = pts_value_l(0,24) + ( particles(n)%speed_y - & |
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253 | pts_value(0,7) )**2 ! v*2 |
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254 | pts_value_l(0,25) = pts_value_l(0,25) + ( particles(n)%speed_z - & |
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255 | pts_value(0,8) )**2 ! w*2 |
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256 | IF ( .NOT. curvature_solution_effects ) THEN |
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257 | pts_value_l(0,26) = pts_value_l(0,26) + ( particles(n)%rvar1 - & |
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258 | pts_value(0,9) )**2 ! u"2 |
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259 | pts_value_l(0,27) = pts_value_l(0,27) + ( particles(n)%rvar2 - & |
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260 | pts_value(0,10) )**2 ! v"2 |
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261 | pts_value_l(0,28) = pts_value_l(0,28) + ( particles(n)%rvar3 - & |
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262 | pts_value(0,11) )**2 ! w"2 |
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263 | ENDIF |
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264 | ! |
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265 | !-- Repeat the same for the respective particle group |
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266 | IF ( number_of_particle_groups > 1 ) THEN |
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267 | j = particles(n)%group |
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268 | |
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269 | pts_value_l(j,20) = pts_value_l(j,20) + ( particles(n)%x - & |
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270 | particles(n)%origin_x - pts_value(j,2) )**2 |
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271 | pts_value_l(j,21) = pts_value_l(j,21) + ( particles(n)%y - & |
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272 | particles(n)%origin_y - pts_value(j,3) )**2 |
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273 | pts_value_l(j,22) = pts_value_l(j,22) + ( particles(n)%z - & |
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274 | particles(n)%origin_z - pts_value(j,4) )**2 |
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275 | pts_value_l(j,23) = pts_value_l(j,23) + ( particles(n)%speed_x - & |
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276 | pts_value(j,6) )**2 |
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277 | pts_value_l(j,24) = pts_value_l(j,24) + ( particles(n)%speed_y - & |
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278 | pts_value(j,7) )**2 |
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279 | pts_value_l(j,25) = pts_value_l(j,25) + ( particles(n)%speed_z - & |
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280 | pts_value(j,8) )**2 |
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281 | IF ( .NOT. curvature_solution_effects ) THEN |
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282 | pts_value_l(j,26) = pts_value_l(j,26) + ( particles(n)%rvar1 - & |
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283 | pts_value(j,9) )**2 |
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284 | pts_value_l(j,27) = pts_value_l(j,27) + ( particles(n)%rvar2 - & |
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285 | pts_value(j,10) )**2 |
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286 | pts_value_l(j,28) = pts_value_l(j,28) + ( particles(n)%rvar3 - & |
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287 | pts_value(j,11) )**2 |
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288 | ENDIF |
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289 | ENDIF |
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290 | |
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291 | ENDDO |
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292 | |
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293 | pts_value_l(0,29) = ( number_of_particles - pts_value(0,1) / numprocs )**2 |
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294 | ! variance of particle numbers |
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295 | IF ( number_of_particle_groups > 1 ) THEN |
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296 | DO j = 1, number_of_particle_groups |
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297 | pts_value_l(j,29) = ( pts_value_l(j,1) - & |
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298 | pts_value(j,1) / numprocs )**2 |
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299 | ENDDO |
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300 | ENDIF |
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301 | |
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302 | #if defined( __parallel ) |
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303 | ! |
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304 | !-- Sum values of the subdomains |
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305 | inum = number_of_particle_groups + 1 |
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306 | |
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307 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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308 | CALL MPI_ALLREDUCE( pts_value_l(0,20), pts_value(0,20), inum*10, MPI_REAL, & |
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309 | MPI_SUM, comm2d, ierr ) |
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310 | #else |
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311 | pts_value(:,20:29) = pts_value_l(:,20:29) |
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312 | #endif |
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313 | |
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314 | ! |
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315 | !-- Normalize the above calculated quantities with the total number of |
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316 | !-- particles |
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317 | IF ( number_of_particle_groups > 1 ) THEN |
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318 | inum = number_of_particle_groups |
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319 | ELSE |
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320 | inum = 0 |
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321 | ENDIF |
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322 | |
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323 | DO j = 0, inum |
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324 | |
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325 | IF ( pts_value(j,1) > 0.0 ) THEN |
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326 | pts_value(j,20:28) = pts_value(j,20:28) / pts_value(j,1) |
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327 | ENDIF |
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328 | pts_value(j,29) = pts_value(j,29) / numprocs |
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329 | |
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330 | ENDDO |
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331 | |
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332 | #if defined( __netcdf ) |
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333 | ! |
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334 | !-- Output particle time series quantities in NetCDF format |
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335 | IF ( myid == 0 ) THEN |
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336 | DO j = 0, inum |
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337 | DO i = 1, dopts_num |
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338 | nc_stat = NF90_PUT_VAR( id_set_pts, id_var_dopts(i,j), & |
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339 | (/ pts_value(j,i) /), & |
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340 | start = (/ dopts_time_count /), & |
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341 | count = (/ 1 /) ) |
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342 | CALL handle_netcdf_error( 'data_output_ptseries', 392 ) |
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343 | ENDDO |
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344 | ENDDO |
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345 | ENDIF |
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346 | #endif |
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347 | |
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348 | DEALLOCATE( pts_value, pts_value_l ) |
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349 | |
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350 | CALL cpu_log( log_point(36), 'data_output_ptseries', 'stop' ) |
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351 | |
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352 | END SUBROUTINE data_output_ptseries |
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