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 | ! |
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7 | ! |
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8 | ! Former revisions: |
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9 | ! ----------------- |
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10 | ! $Id: data_output_ptseries.f90 623 2010-12-10 08:52:17Z letzel $ |
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11 | ! |
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12 | ! 622 2010-12-10 08:08:13Z raasch |
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13 | ! optional barriers included in order to speed up collective operations |
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14 | ! |
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15 | ! 291 2009-04-16 12:07:26Z raasch |
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16 | ! simulated_time in NetCDF output replaced by time_since_reference_point. |
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17 | ! Output of NetCDF messages with aid of message handling routine. |
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18 | ! |
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19 | ! 60 2007-03-11 11:50:04Z raasch |
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20 | ! Particles-package is now part of the default code. |
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21 | ! |
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22 | ! RCS Log replace by Id keyword, revision history cleaned up |
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23 | ! |
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24 | ! Revision 1.2 2006/08/22 13:51:13 raasch |
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25 | ! Seperate output for particle groups |
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26 | ! |
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27 | ! Revision 1.1 2006/08/04 14:24:18 raasch |
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28 | ! Initial revision |
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29 | ! |
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30 | ! |
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31 | ! Description: |
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32 | ! ------------ |
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33 | ! Output of particle data timeseries in NetCDF format. |
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34 | !------------------------------------------------------------------------------! |
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35 | |
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36 | USE control_parameters |
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37 | USE cpulog |
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38 | USE indices |
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39 | USE interfaces |
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40 | USE netcdf_control |
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41 | USE particle_attributes |
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42 | USE pegrid |
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43 | |
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44 | IMPLICIT NONE |
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45 | |
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46 | |
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47 | INTEGER :: i, inum, j, n |
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48 | |
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49 | REAL, DIMENSION(0:number_of_particle_groups,30) :: pts_value, pts_value_l |
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50 | |
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51 | |
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52 | |
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53 | CALL cpu_log( log_point(36), 'data_output_ptseries', 'start' ) |
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54 | |
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55 | IF ( myid == 0 .AND. netcdf_output ) THEN |
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56 | ! |
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57 | !-- Open file for time series output in NetCDF format |
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58 | dopts_time_count = dopts_time_count + 1 |
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59 | CALL check_open( 109 ) |
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60 | #if defined( __netcdf ) |
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61 | ! |
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62 | !-- Update the particle time series time axis |
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63 | nc_stat = NF90_PUT_VAR( id_set_pts, id_var_time_pts, & |
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64 | (/ time_since_reference_point /), & |
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65 | start = (/ dopts_time_count /), count = (/ 1 /) ) |
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66 | CALL handle_netcdf_error( 'data_output_ptseries', 391 ) |
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67 | #endif |
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68 | |
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69 | ENDIF |
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70 | |
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71 | pts_value_l = 0.0 |
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72 | |
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73 | ! |
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74 | !-- Calculate or collect the particle time series quantities for all particles |
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75 | !-- and seperately for each particle group (if there is more than one group) |
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76 | DO n = 1, number_of_particles |
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77 | |
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78 | pts_value_l(0,1) = number_of_particles ! total # of particles |
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79 | pts_value_l(0,2) = pts_value_l(0,2) + & |
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80 | ( particles(n)%x - particles(n)%origin_x ) ! mean x |
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81 | pts_value_l(0,3) = pts_value_l(0,3) + & |
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82 | ( particles(n)%y - particles(n)%origin_y ) ! mean y |
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83 | pts_value_l(0,4) = pts_value_l(0,4) + & |
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84 | ( particles(n)%z - particles(n)%origin_z ) ! mean z |
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85 | pts_value_l(0,5) = pts_value_l(0,5) + particles(n)%z ! mean z (absolute) |
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86 | pts_value_l(0,6) = pts_value_l(0,6) + particles(n)%speed_x ! mean u |
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87 | pts_value_l(0,7) = pts_value_l(0,7) + particles(n)%speed_y ! mean v |
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88 | pts_value_l(0,8) = pts_value_l(0,8) + particles(n)%speed_z ! mean w |
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89 | pts_value_l(0,9) = pts_value_l(0,9) + & |
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90 | particles(n)%speed_x_sgs ! mean sgsu |
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91 | pts_value_l(0,10) = pts_value_l(0,10) + & |
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92 | particles(n)%speed_y_sgs ! mean sgsv |
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93 | pts_value_l(0,11) = pts_value_l(0,11) + & |
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94 | particles(n)%speed_z_sgs ! mean sgsw |
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95 | IF ( particles(n)%speed_z > 0.0 ) THEN |
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96 | pts_value_l(0,12) = pts_value_l(0,12) + 1.0 ! # of upward moving prts |
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97 | pts_value_l(0,13) = pts_value_l(0,13) + & |
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98 | particles(n)%speed_z ! mean w upw. |
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99 | ELSE |
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100 | pts_value_l(0,14) = pts_value_l(0,14) + & |
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101 | particles(n)%speed_z ! mean w down |
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102 | ENDIF |
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103 | pts_value_l(0,15) = number_of_particles |
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104 | pts_value_l(0,16) = number_of_particles |
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105 | |
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106 | ! |
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107 | !-- Repeat the same for the respective particle group |
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108 | IF ( number_of_particle_groups > 1 ) THEN |
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109 | j = particles(n)%group |
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110 | |
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111 | pts_value_l(j,1) = pts_value_l(j,1) + 1 |
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112 | pts_value_l(j,2) = pts_value_l(j,2) + & |
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113 | ( particles(n)%x - particles(n)%origin_x ) |
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114 | pts_value_l(j,3) = pts_value_l(j,3) + & |
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115 | ( particles(n)%y - particles(n)%origin_y ) |
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116 | pts_value_l(j,4) = pts_value_l(j,4) + & |
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117 | ( particles(n)%z - particles(n)%origin_z ) |
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118 | pts_value_l(j,5) = pts_value_l(j,5) + particles(n)%z |
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119 | pts_value_l(j,6) = pts_value_l(j,6) + particles(n)%speed_x |
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120 | pts_value_l(j,7) = pts_value_l(j,7) + particles(n)%speed_y |
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121 | pts_value_l(j,8) = pts_value_l(j,8) + particles(n)%speed_z |
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122 | pts_value_l(j,9) = pts_value_l(j,9) + particles(n)%speed_x_sgs |
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123 | pts_value_l(j,10) = pts_value_l(j,10) + particles(n)%speed_y_sgs |
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124 | pts_value_l(j,11) = pts_value_l(j,11) + particles(n)%speed_z_sgs |
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125 | IF ( particles(n)%speed_z > 0.0 ) THEN |
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126 | pts_value_l(j,12) = pts_value_l(j,12) + 1.0 |
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127 | pts_value_l(j,13) = pts_value_l(j,13) + particles(n)%speed_z |
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128 | ELSE |
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129 | pts_value_l(j,14) = pts_value_l(j,14) + particles(n)%speed_z |
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130 | ENDIF |
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131 | pts_value_l(j,15) = pts_value_l(j,15) + 1.0 |
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132 | pts_value_l(j,16) = pts_value_l(j,16) + 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), 14*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(0,15), pts_value(0,15), 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(0,16), pts_value(0,16), 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(:,1:16) = pts_value_l(:,1:16) |
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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,2:14) = pts_value(j,2:14) / 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(0,17) = pts_value_l(0,17) + ( 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(0,18) = pts_value_l(0,18) + ( 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(0,19) = pts_value_l(0,19) + ( 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(0,20) = pts_value_l(0,20) + ( particles(n)%speed_x - & |
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195 | pts_value(0,6) )**2 ! u*2 |
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196 | pts_value_l(0,21) = pts_value_l(0,21) + ( particles(n)%speed_y - & |
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197 | pts_value(0,7) )**2 ! v*2 |
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198 | pts_value_l(0,22) = pts_value_l(0,22) + ( particles(n)%speed_z - & |
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199 | pts_value(0,8) )**2 ! w*2 |
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200 | pts_value_l(0,23) = pts_value_l(0,23) + ( particles(n)%speed_x_sgs - & |
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201 | pts_value(0,9) )**2 ! u"2 |
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202 | pts_value_l(0,24) = pts_value_l(0,24) + ( particles(n)%speed_y_sgs - & |
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203 | pts_value(0,10) )**2 ! v"2 |
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204 | pts_value_l(0,25) = pts_value_l(0,25) + ( particles(n)%speed_z_sgs - & |
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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,17) = pts_value_l(j,17) + ( 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,18) = pts_value_l(j,18) + ( 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,19) = pts_value_l(j,19) + ( 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,20) = pts_value_l(j,20) + ( particles(n)%speed_x - & |
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218 | pts_value(j,6) )**2 |
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219 | pts_value_l(j,21) = pts_value_l(j,21) + ( particles(n)%speed_y - & |
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220 | pts_value(j,7) )**2 |
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221 | pts_value_l(j,22) = pts_value_l(j,22) + ( particles(n)%speed_z - & |
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222 | pts_value(j,8) )**2 |
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223 | pts_value_l(j,23) = pts_value_l(j,23) + ( particles(n)%speed_x_sgs - & |
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224 | pts_value(j,9) )**2 |
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225 | pts_value_l(j,24) = pts_value_l(j,24) + ( particles(n)%speed_y_sgs - & |
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226 | pts_value(j,10) )**2 |
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227 | pts_value_l(j,25) = pts_value_l(j,25) + ( particles(n)%speed_z_sgs - & |
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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(0,26) = ( 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,26) = ( 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(0,17), pts_value(0,17), 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(:,17:26) = pts_value_l(:,17:26) |
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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,17:25) = pts_value(j,17:25) / pts_value(j,1) |
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267 | ENDIF |
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268 | pts_value(j,26) = pts_value(j,26) / 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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