1 | SUBROUTINE flow_statistics |
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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 1997-2012 Leibniz University 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: flow_statistics.f90 1116 2013-03-26 18:49:55Z heinze $ |
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27 | ! |
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28 | ! 1115 2013-03-26 18:16:16Z hoffmann |
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29 | ! ql is calculated by calc_liquid_water_content |
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30 | ! |
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31 | ! 1111 2013-03-08 23:54:10Z raasch |
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32 | ! openACC directive added |
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33 | ! |
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34 | ! 1053 2012-11-13 17:11:03Z hoffmann |
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35 | ! additions for two-moment cloud physics scheme: |
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36 | ! +nr, qr, qc, prr |
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37 | ! |
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38 | ! 1036 2012-10-22 13:43:42Z raasch |
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39 | ! code put under GPL (PALM 3.9) |
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40 | ! |
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41 | ! 1007 2012-09-19 14:30:36Z franke |
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42 | ! Calculation of buoyancy flux for humidity in case of WS-scheme is now using |
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43 | ! turbulent fluxes of WS-scheme |
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44 | ! Bugfix: Calculation of subgridscale buoyancy flux for humidity and cloud |
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45 | ! droplets at nzb and nzt added |
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46 | ! |
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47 | ! 801 2012-01-10 17:30:36Z suehring |
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48 | ! Calculation of turbulent fluxes in advec_ws is now thread-safe. |
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49 | ! |
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50 | ! 743 2011-08-18 16:10:16Z suehring |
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51 | ! Calculation of turbulent fluxes with WS-scheme only for the whole model |
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52 | ! domain, not for user-defined subregions. |
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53 | ! |
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54 | ! 709 2011-03-30 09:31:40Z raasch |
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55 | ! formatting adjustments |
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56 | ! |
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57 | ! 699 2011-03-22 17:52:22Z suehring |
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58 | ! Bugfix in calculation of vertical velocity skewness. The added absolute value |
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59 | ! avoid negative values in the root. Negative values of w'w' can occur at the |
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60 | ! top or bottom of the model domain due to degrading the order of advection |
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61 | ! scheme. Furthermore the calculation will be the same for all advection |
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62 | ! schemes. |
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63 | ! |
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64 | ! 696 2011-03-18 07:03:49Z raasch |
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65 | ! Bugfix: Summation of Wicker-Skamarock scheme fluxes and variances for all |
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66 | ! threads |
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67 | ! |
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68 | ! 678 2011-02-02 14:31:56Z raasch |
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69 | ! Bugfix in calculation of the divergence of vertical flux of resolved scale |
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70 | ! energy, pressure fluctuations, and flux of pressure fluctuation itself |
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71 | ! |
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72 | ! 673 2011-01-18 16:19:48Z suehring |
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73 | ! Top bc for the horizontal velocity variances added for ocean runs. |
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74 | ! Setting the corresponding bottom bc moved to advec_ws. |
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75 | ! |
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76 | ! 667 2010-12-23 12:06:00Z suehring/gryschka |
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77 | ! When advection is computed with ws-scheme, turbulent fluxes are already |
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78 | ! computed in the respective advection routines and buffered in arrays |
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79 | ! sums_xx_ws_l(). This is due to a consistent treatment of statistics with the |
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80 | ! numerics and to avoid unphysical kinks near the surface. |
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81 | ! So some if requests has to be done to dicern between fluxes from ws-scheme |
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82 | ! other advection schemes. |
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83 | ! Furthermore the computation of z_i is only done if the heat flux exceeds a |
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84 | ! minimum value. This affects only simulations of a neutral boundary layer and |
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85 | ! is due to reasons of computations in the advection scheme. |
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86 | ! |
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87 | ! 624 2010-12-10 11:46:30Z heinze |
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88 | ! Calculation of q*2 added |
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89 | ! |
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90 | ! 622 2010-12-10 08:08:13Z raasch |
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91 | ! optional barriers included in order to speed up collective operations |
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92 | ! |
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93 | ! 388 2009-09-23 09:40:33Z raasch |
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94 | ! Vertical profiles of potential density and hydrostatic pressure are |
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95 | ! calculated. |
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96 | ! Added missing timeseries calculation of w"q"(0), moved timeseries q* to the |
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97 | ! end. |
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98 | ! Temperature gradient criterion for estimating the boundary layer height |
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99 | ! replaced by the gradient criterion of Sullivan et al. (1998). |
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100 | ! Output of messages replaced by message handling routine. |
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101 | ! |
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102 | ! 197 2008-09-16 15:29:03Z raasch |
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103 | ! Spline timeseries splptx etc. removed, timeseries w'u', w'v', w'q' (k=0) |
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104 | ! added, |
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105 | ! bugfix: divide sums(k,8) (e) and sums(k,34) (e*) by ngp_2dh_s_inner(k,sr) |
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106 | ! (like other scalars) |
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107 | ! |
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108 | ! 133 2007-11-20 10:10:53Z letzel |
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109 | ! Vertical profiles now based on nzb_s_inner; they are divided by |
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110 | ! ngp_2dh_s_inner (scalars, procucts of scalars) and ngp_2dh (staggered |
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111 | ! velocity components and their products, procucts of scalars and velocity |
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112 | ! components), respectively. |
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113 | ! |
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114 | ! 106 2007-08-16 14:30:26Z raasch |
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115 | ! Prescribed momentum fluxes at the top surface are used, |
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116 | ! profiles for w*p* and w"e are calculated |
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117 | ! |
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118 | ! 97 2007-06-21 08:23:15Z raasch |
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119 | ! Statistics for ocean version (salinity, density) added, |
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120 | ! calculation of z_i and Deardorff velocity scale adjusted to be used with |
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121 | ! the ocean version |
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122 | ! |
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123 | ! 87 2007-05-22 15:46:47Z raasch |
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124 | ! Two more arguments added to user_statistics, which is now also called for |
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125 | ! user-defined profiles, |
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126 | ! var_hom and var_sum renamed pr_palm |
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127 | ! |
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128 | ! 82 2007-04-16 15:40:52Z raasch |
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129 | ! Cpp-directive lcmuk changed to intel_openmp_bug |
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130 | ! |
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131 | ! 75 2007-03-22 09:54:05Z raasch |
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132 | ! Collection of time series quantities moved from routine flow_statistics to |
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133 | ! here, routine user_statistics is called for each statistic region, |
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134 | ! moisture renamed humidity |
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135 | ! |
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136 | ! 19 2007-02-23 04:53:48Z raasch |
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137 | ! fluxes at top modified (tswst, qswst) |
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138 | ! |
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139 | ! RCS Log replace by Id keyword, revision history cleaned up |
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140 | ! |
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141 | ! Revision 1.41 2006/08/04 14:37:50 raasch |
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142 | ! Error removed in non-parallel part (sums_l) |
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143 | ! |
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144 | ! Revision 1.1 1997/08/11 06:15:17 raasch |
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145 | ! Initial revision |
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146 | ! |
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147 | ! |
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148 | ! Description: |
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149 | ! ------------ |
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150 | ! Compute average profiles and further average flow quantities for the different |
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151 | ! user-defined (sub-)regions. The region indexed 0 is the total model domain. |
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152 | ! |
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153 | ! NOTE: For simplicity, nzb_s_inner and nzb_diff_s_inner are being used as a |
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154 | ! ---- lower vertical index for k-loops for all variables, although strictly |
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155 | ! speaking the k-loops would have to be split up according to the staggered |
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156 | ! grid. However, this implies no error since staggered velocity components are |
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157 | ! zero at the walls and inside buildings. |
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158 | !------------------------------------------------------------------------------! |
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159 | |
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160 | USE arrays_3d |
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161 | USE cloud_parameters |
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162 | USE control_parameters |
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163 | USE cpulog |
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164 | USE grid_variables |
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165 | USE indices |
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166 | USE interfaces |
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167 | USE pegrid |
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168 | USE statistics |
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169 | |
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170 | IMPLICIT NONE |
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171 | |
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172 | INTEGER :: i, j, k, omp_get_thread_num, sr, tn |
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173 | LOGICAL :: first |
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174 | REAL :: dptdz_threshold, height, pts, sums_l_eper, sums_l_etot, ust, & |
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175 | ust2, u2, vst, vst2, v2, w2, z_i(2) |
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176 | REAL :: dptdz(nzb+1:nzt+1) |
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177 | REAL :: sums_ll(nzb:nzt+1,2) |
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178 | |
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179 | CALL cpu_log( log_point(10), 'flow_statistics', 'start' ) |
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180 | |
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181 | ! |
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182 | !-- To be on the safe side, check whether flow_statistics has already been |
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183 | !-- called once after the current time step |
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184 | IF ( flow_statistics_called ) THEN |
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185 | |
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186 | message_string = 'flow_statistics is called two times within one ' // & |
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187 | 'timestep' |
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188 | CALL message( 'flow_statistics', 'PA0190', 1, 2, 0, 6, 0 ) |
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189 | |
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190 | ENDIF |
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191 | |
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192 | !$acc update host( km, kh, e, pt, qs, qsws, rif, shf, ts, u, v, w ) |
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193 | |
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194 | ! |
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195 | !-- Compute statistics for each (sub-)region |
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196 | DO sr = 0, statistic_regions |
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197 | |
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198 | ! |
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199 | !-- Initialize (local) summation array |
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200 | sums_l = 0.0 |
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201 | |
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202 | ! |
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203 | !-- Store sums that have been computed in other subroutines in summation |
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204 | !-- array |
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205 | sums_l(:,11,:) = sums_l_l(:,sr,:) ! mixing length from diffusivities |
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206 | !-- WARNING: next line still has to be adjusted for OpenMP |
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207 | sums_l(:,21,0) = sums_wsts_bc_l(:,sr) ! heat flux from advec_s_bc |
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208 | sums_l(nzb+9,pr_palm,0) = sums_divold_l(sr) ! old divergence from pres |
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209 | sums_l(nzb+10,pr_palm,0) = sums_divnew_l(sr) ! new divergence from pres |
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210 | |
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211 | ! |
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212 | !-- Copy the turbulent quantities, evaluated in the advection routines to |
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213 | !-- the local array sums_l() for further computations |
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214 | IF ( ws_scheme_mom .AND. sr == 0 ) THEN |
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215 | |
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216 | ! |
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217 | !-- According to the Neumann bc for the horizontal velocity components, |
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218 | !-- the corresponding fluxes has to satisfiy the same bc. |
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219 | IF ( ocean ) THEN |
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220 | sums_us2_ws_l(nzt+1,:) = sums_us2_ws_l(nzt,:) |
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221 | sums_vs2_ws_l(nzt+1,:) = sums_vs2_ws_l(nzt,:) |
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222 | ENDIF |
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223 | |
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224 | DO i = 0, threads_per_task-1 |
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225 | ! |
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226 | !-- Swap the turbulent quantities evaluated in advec_ws. |
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227 | sums_l(:,13,i) = sums_wsus_ws_l(:,i) ! w*u* |
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228 | sums_l(:,15,i) = sums_wsvs_ws_l(:,i) ! w*v* |
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229 | sums_l(:,30,i) = sums_us2_ws_l(:,i) ! u*2 |
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230 | sums_l(:,31,i) = sums_vs2_ws_l(:,i) ! v*2 |
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231 | sums_l(:,32,i) = sums_ws2_ws_l(:,i) ! w*2 |
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232 | sums_l(:,34,i) = sums_l(:,34,i) + 0.5 * & |
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233 | ( sums_us2_ws_l(:,i) + sums_vs2_ws_l(:,i) + & |
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234 | sums_ws2_ws_l(:,i) ) ! e* |
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235 | DO k = nzb, nzt |
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236 | sums_l(nzb+5,pr_palm,i) = sums_l(nzb+5,pr_palm,i) + 0.5 * ( & |
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237 | sums_us2_ws_l(k,i) + & |
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238 | sums_vs2_ws_l(k,i) + & |
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239 | sums_ws2_ws_l(k,i) ) |
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240 | ENDDO |
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241 | ENDDO |
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242 | |
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243 | ENDIF |
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244 | |
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245 | IF ( ws_scheme_sca .AND. sr == 0 ) THEN |
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246 | |
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247 | DO i = 0, threads_per_task-1 |
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248 | sums_l(:,17,i) = sums_wspts_ws_l(:,i) ! w*pt* from advec_s_ws |
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249 | IF ( ocean ) sums_l(:,66,i) = sums_wssas_ws_l(:,i) ! w*sa* |
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250 | IF ( humidity .OR. passive_scalar ) sums_l(:,49,i) = & |
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251 | sums_wsqs_ws_l(:,i) !w*q* |
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252 | ENDDO |
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253 | |
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254 | ENDIF |
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255 | ! |
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256 | !-- Horizontally averaged profiles of horizontal velocities and temperature. |
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257 | !-- They must have been computed before, because they are already required |
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258 | !-- for other horizontal averages. |
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259 | tn = 0 |
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260 | |
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261 | !$OMP PARALLEL PRIVATE( i, j, k, tn ) |
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262 | #if defined( __intel_openmp_bug ) |
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263 | tn = omp_get_thread_num() |
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264 | #else |
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265 | !$ tn = omp_get_thread_num() |
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266 | #endif |
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267 | |
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268 | !$OMP DO |
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269 | DO i = nxl, nxr |
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270 | DO j = nys, nyn |
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271 | DO k = nzb_s_inner(j,i), nzt+1 |
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272 | sums_l(k,1,tn) = sums_l(k,1,tn) + u(k,j,i) * rmask(j,i,sr) |
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273 | sums_l(k,2,tn) = sums_l(k,2,tn) + v(k,j,i) * rmask(j,i,sr) |
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274 | sums_l(k,4,tn) = sums_l(k,4,tn) + pt(k,j,i) * rmask(j,i,sr) |
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275 | ENDDO |
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276 | ENDDO |
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277 | ENDDO |
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278 | |
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279 | ! |
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280 | !-- Horizontally averaged profile of salinity |
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281 | IF ( ocean ) THEN |
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282 | !$OMP DO |
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283 | DO i = nxl, nxr |
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284 | DO j = nys, nyn |
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285 | DO k = nzb_s_inner(j,i), nzt+1 |
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286 | sums_l(k,23,tn) = sums_l(k,23,tn) + & |
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287 | sa(k,j,i) * rmask(j,i,sr) |
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288 | ENDDO |
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289 | ENDDO |
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290 | ENDDO |
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291 | ENDIF |
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292 | |
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293 | ! |
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294 | !-- Horizontally averaged profiles of virtual potential temperature, |
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295 | !-- total water content, specific humidity and liquid water potential |
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296 | !-- temperature |
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297 | IF ( humidity ) THEN |
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298 | !$OMP DO |
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299 | DO i = nxl, nxr |
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300 | DO j = nys, nyn |
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301 | DO k = nzb_s_inner(j,i), nzt+1 |
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302 | sums_l(k,44,tn) = sums_l(k,44,tn) + & |
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303 | vpt(k,j,i) * rmask(j,i,sr) |
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304 | sums_l(k,41,tn) = sums_l(k,41,tn) + & |
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305 | q(k,j,i) * rmask(j,i,sr) |
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306 | ENDDO |
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307 | ENDDO |
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308 | ENDDO |
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309 | IF ( cloud_physics ) THEN |
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310 | !$OMP DO |
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311 | DO i = nxl, nxr |
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312 | DO j = nys, nyn |
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313 | DO k = nzb_s_inner(j,i), nzt+1 |
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314 | sums_l(k,42,tn) = sums_l(k,42,tn) + & |
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315 | ( q(k,j,i) - ql(k,j,i) ) * rmask(j,i,sr) |
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316 | sums_l(k,43,tn) = sums_l(k,43,tn) + ( & |
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317 | pt(k,j,i) + l_d_cp*pt_d_t(k) * ql(k,j,i) & |
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318 | ) * rmask(j,i,sr) |
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319 | ENDDO |
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320 | ENDDO |
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321 | ENDDO |
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322 | ENDIF |
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323 | ENDIF |
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324 | |
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325 | ! |
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326 | !-- Horizontally averaged profiles of passive scalar |
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327 | IF ( passive_scalar ) THEN |
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328 | !$OMP DO |
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329 | DO i = nxl, nxr |
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330 | DO j = nys, nyn |
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331 | DO k = nzb_s_inner(j,i), nzt+1 |
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332 | sums_l(k,41,tn) = sums_l(k,41,tn) + q(k,j,i) * rmask(j,i,sr) |
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333 | ENDDO |
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334 | ENDDO |
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335 | ENDDO |
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336 | ENDIF |
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337 | !$OMP END PARALLEL |
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338 | ! |
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339 | !-- Summation of thread sums |
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340 | IF ( threads_per_task > 1 ) THEN |
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341 | DO i = 1, threads_per_task-1 |
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342 | sums_l(:,1,0) = sums_l(:,1,0) + sums_l(:,1,i) |
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343 | sums_l(:,2,0) = sums_l(:,2,0) + sums_l(:,2,i) |
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344 | sums_l(:,4,0) = sums_l(:,4,0) + sums_l(:,4,i) |
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345 | IF ( ocean ) THEN |
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346 | sums_l(:,23,0) = sums_l(:,23,0) + sums_l(:,23,i) |
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347 | ENDIF |
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348 | IF ( humidity ) THEN |
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349 | sums_l(:,41,0) = sums_l(:,41,0) + sums_l(:,41,i) |
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350 | sums_l(:,44,0) = sums_l(:,44,0) + sums_l(:,44,i) |
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351 | IF ( cloud_physics ) THEN |
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352 | sums_l(:,42,0) = sums_l(:,42,0) + sums_l(:,42,i) |
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353 | sums_l(:,43,0) = sums_l(:,43,0) + sums_l(:,43,i) |
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354 | ENDIF |
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355 | ENDIF |
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356 | IF ( passive_scalar ) THEN |
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357 | sums_l(:,41,0) = sums_l(:,41,0) + sums_l(:,41,i) |
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358 | ENDIF |
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359 | ENDDO |
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360 | ENDIF |
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361 | |
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362 | #if defined( __parallel ) |
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363 | ! |
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364 | !-- Compute total sum from local sums |
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365 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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366 | CALL MPI_ALLREDUCE( sums_l(nzb,1,0), sums(nzb,1), nzt+2-nzb, MPI_REAL, & |
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367 | MPI_SUM, comm2d, ierr ) |
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368 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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369 | CALL MPI_ALLREDUCE( sums_l(nzb,2,0), sums(nzb,2), nzt+2-nzb, MPI_REAL, & |
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370 | MPI_SUM, comm2d, ierr ) |
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371 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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372 | CALL MPI_ALLREDUCE( sums_l(nzb,4,0), sums(nzb,4), nzt+2-nzb, MPI_REAL, & |
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373 | MPI_SUM, comm2d, ierr ) |
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374 | IF ( ocean ) THEN |
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375 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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376 | CALL MPI_ALLREDUCE( sums_l(nzb,23,0), sums(nzb,23), nzt+2-nzb, & |
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377 | MPI_REAL, MPI_SUM, comm2d, ierr ) |
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378 | ENDIF |
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379 | IF ( humidity ) THEN |
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380 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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381 | CALL MPI_ALLREDUCE( sums_l(nzb,44,0), sums(nzb,44), nzt+2-nzb, & |
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382 | MPI_REAL, MPI_SUM, comm2d, ierr ) |
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383 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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384 | CALL MPI_ALLREDUCE( sums_l(nzb,41,0), sums(nzb,41), nzt+2-nzb, & |
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385 | MPI_REAL, MPI_SUM, comm2d, ierr ) |
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386 | IF ( cloud_physics ) THEN |
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387 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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388 | CALL MPI_ALLREDUCE( sums_l(nzb,42,0), sums(nzb,42), nzt+2-nzb, & |
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389 | MPI_REAL, MPI_SUM, comm2d, ierr ) |
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390 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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391 | CALL MPI_ALLREDUCE( sums_l(nzb,43,0), sums(nzb,43), nzt+2-nzb, & |
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392 | MPI_REAL, MPI_SUM, comm2d, ierr ) |
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393 | ENDIF |
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394 | ENDIF |
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395 | |
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396 | IF ( passive_scalar ) THEN |
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397 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
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398 | CALL MPI_ALLREDUCE( sums_l(nzb,41,0), sums(nzb,41), nzt+2-nzb, & |
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399 | MPI_REAL, MPI_SUM, comm2d, ierr ) |
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400 | ENDIF |
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401 | #else |
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402 | sums(:,1) = sums_l(:,1,0) |
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403 | sums(:,2) = sums_l(:,2,0) |
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404 | sums(:,4) = sums_l(:,4,0) |
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405 | IF ( ocean ) sums(:,23) = sums_l(:,23,0) |
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406 | IF ( humidity ) THEN |
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407 | sums(:,44) = sums_l(:,44,0) |
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408 | sums(:,41) = sums_l(:,41,0) |
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409 | IF ( cloud_physics ) THEN |
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410 | sums(:,42) = sums_l(:,42,0) |
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411 | sums(:,43) = sums_l(:,43,0) |
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412 | ENDIF |
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413 | ENDIF |
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414 | IF ( passive_scalar ) sums(:,41) = sums_l(:,41,0) |
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415 | #endif |
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416 | |
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417 | ! |
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418 | !-- Final values are obtained by division by the total number of grid points |
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419 | !-- used for summation. After that store profiles. |
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420 | sums(:,1) = sums(:,1) / ngp_2dh(sr) |
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421 | sums(:,2) = sums(:,2) / ngp_2dh(sr) |
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422 | sums(:,4) = sums(:,4) / ngp_2dh_s_inner(:,sr) |
---|
423 | hom(:,1,1,sr) = sums(:,1) ! u |
---|
424 | hom(:,1,2,sr) = sums(:,2) ! v |
---|
425 | hom(:,1,4,sr) = sums(:,4) ! pt |
---|
426 | |
---|
427 | |
---|
428 | ! |
---|
429 | !-- Salinity |
---|
430 | IF ( ocean ) THEN |
---|
431 | sums(:,23) = sums(:,23) / ngp_2dh_s_inner(:,sr) |
---|
432 | hom(:,1,23,sr) = sums(:,23) ! sa |
---|
433 | ENDIF |
---|
434 | |
---|
435 | ! |
---|
436 | !-- Humidity and cloud parameters |
---|
437 | IF ( humidity ) THEN |
---|
438 | sums(:,44) = sums(:,44) / ngp_2dh_s_inner(:,sr) |
---|
439 | sums(:,41) = sums(:,41) / ngp_2dh_s_inner(:,sr) |
---|
440 | hom(:,1,44,sr) = sums(:,44) ! vpt |
---|
441 | hom(:,1,41,sr) = sums(:,41) ! qv (q) |
---|
442 | IF ( cloud_physics ) THEN |
---|
443 | sums(:,42) = sums(:,42) / ngp_2dh_s_inner(:,sr) |
---|
444 | sums(:,43) = sums(:,43) / ngp_2dh_s_inner(:,sr) |
---|
445 | hom(:,1,42,sr) = sums(:,42) ! qv |
---|
446 | hom(:,1,43,sr) = sums(:,43) ! pt |
---|
447 | ENDIF |
---|
448 | ENDIF |
---|
449 | |
---|
450 | ! |
---|
451 | !-- Passive scalar |
---|
452 | IF ( passive_scalar ) hom(:,1,41,sr) = sums(:,41) / & |
---|
453 | ngp_2dh_s_inner(:,sr) ! s (q) |
---|
454 | |
---|
455 | ! |
---|
456 | !-- Horizontally averaged profiles of the remaining prognostic variables, |
---|
457 | !-- variances, the total and the perturbation energy (single values in last |
---|
458 | !-- column of sums_l) and some diagnostic quantities. |
---|
459 | !-- NOTE: for simplicity, nzb_s_inner is used below, although strictly |
---|
460 | !-- ---- speaking the following k-loop would have to be split up and |
---|
461 | !-- rearranged according to the staggered grid. |
---|
462 | !-- However, this implies no error since staggered velocity components |
---|
463 | !-- are zero at the walls and inside buildings. |
---|
464 | tn = 0 |
---|
465 | #if defined( __intel_openmp_bug ) |
---|
466 | !$OMP PARALLEL PRIVATE( i, j, k, pts, sums_ll, sums_l_eper, sums_l_etot, & |
---|
467 | !$OMP tn, ust, ust2, u2, vst, vst2, v2, w2 ) |
---|
468 | tn = omp_get_thread_num() |
---|
469 | #else |
---|
470 | !$OMP PARALLEL PRIVATE( i, j, k, pts, sums_ll, sums_l_eper, sums_l_etot, tn, ust, ust2, u2, vst, vst2, v2, w2 ) |
---|
471 | !$ tn = omp_get_thread_num() |
---|
472 | #endif |
---|
473 | !$OMP DO |
---|
474 | DO i = nxl, nxr |
---|
475 | DO j = nys, nyn |
---|
476 | sums_l_etot = 0.0 |
---|
477 | DO k = nzb_s_inner(j,i), nzt+1 |
---|
478 | ! |
---|
479 | !-- Prognostic and diagnostic variables |
---|
480 | sums_l(k,3,tn) = sums_l(k,3,tn) + w(k,j,i) * rmask(j,i,sr) |
---|
481 | sums_l(k,8,tn) = sums_l(k,8,tn) + e(k,j,i) * rmask(j,i,sr) |
---|
482 | sums_l(k,9,tn) = sums_l(k,9,tn) + km(k,j,i) * rmask(j,i,sr) |
---|
483 | sums_l(k,10,tn) = sums_l(k,10,tn) + kh(k,j,i) * rmask(j,i,sr) |
---|
484 | sums_l(k,40,tn) = sums_l(k,40,tn) + p(k,j,i) |
---|
485 | |
---|
486 | sums_l(k,33,tn) = sums_l(k,33,tn) + & |
---|
487 | ( pt(k,j,i)-hom(k,1,4,sr) )**2 * rmask(j,i,sr) |
---|
488 | |
---|
489 | IF ( humidity ) THEN |
---|
490 | sums_l(k,70,tn) = sums_l(k,70,tn) + & |
---|
491 | ( q(k,j,i)-hom(k,1,41,sr) )**2 * rmask(j,i,sr) |
---|
492 | ENDIF |
---|
493 | |
---|
494 | ! |
---|
495 | !-- Higher moments |
---|
496 | !-- (Computation of the skewness of w further below) |
---|
497 | sums_l(k,38,tn) = sums_l(k,38,tn) + w(k,j,i)**3 * rmask(j,i,sr) |
---|
498 | |
---|
499 | sums_l_etot = sums_l_etot + & |
---|
500 | 0.5 * ( u(k,j,i)**2 + v(k,j,i)**2 + & |
---|
501 | w(k,j,i)**2 ) * rmask(j,i,sr) |
---|
502 | ENDDO |
---|
503 | ! |
---|
504 | !-- Total and perturbation energy for the total domain (being |
---|
505 | !-- collected in the last column of sums_l). Summation of these |
---|
506 | !-- quantities is seperated from the previous loop in order to |
---|
507 | !-- allow vectorization of that loop. |
---|
508 | sums_l(nzb+4,pr_palm,tn) = sums_l(nzb+4,pr_palm,tn) + sums_l_etot |
---|
509 | ! |
---|
510 | !-- 2D-arrays (being collected in the last column of sums_l) |
---|
511 | sums_l(nzb,pr_palm,tn) = sums_l(nzb,pr_palm,tn) + & |
---|
512 | us(j,i) * rmask(j,i,sr) |
---|
513 | sums_l(nzb+1,pr_palm,tn) = sums_l(nzb+1,pr_palm,tn) + & |
---|
514 | usws(j,i) * rmask(j,i,sr) |
---|
515 | sums_l(nzb+2,pr_palm,tn) = sums_l(nzb+2,pr_palm,tn) + & |
---|
516 | vsws(j,i) * rmask(j,i,sr) |
---|
517 | sums_l(nzb+3,pr_palm,tn) = sums_l(nzb+3,pr_palm,tn) + & |
---|
518 | ts(j,i) * rmask(j,i,sr) |
---|
519 | IF ( humidity ) THEN |
---|
520 | sums_l(nzb+12,pr_palm,tn) = sums_l(nzb+12,pr_palm,tn) + & |
---|
521 | qs(j,i) * rmask(j,i,sr) |
---|
522 | ENDIF |
---|
523 | ENDDO |
---|
524 | ENDDO |
---|
525 | |
---|
526 | ! |
---|
527 | !-- Computation of statistics when ws-scheme is not used. Else these |
---|
528 | !-- quantities are evaluated in the advection routines. |
---|
529 | IF ( .NOT. ws_scheme_mom .OR. sr /= 0 ) THEN |
---|
530 | !$OMP DO |
---|
531 | DO i = nxl, nxr |
---|
532 | DO j = nys, nyn |
---|
533 | sums_l_eper = 0.0 |
---|
534 | DO k = nzb_s_inner(j,i), nzt+1 |
---|
535 | u2 = u(k,j,i)**2 |
---|
536 | v2 = v(k,j,i)**2 |
---|
537 | w2 = w(k,j,i)**2 |
---|
538 | ust2 = ( u(k,j,i) - hom(k,1,1,sr) )**2 |
---|
539 | vst2 = ( v(k,j,i) - hom(k,1,2,sr) )**2 |
---|
540 | |
---|
541 | sums_l(k,30,tn) = sums_l(k,30,tn) + ust2 * rmask(j,i,sr) |
---|
542 | sums_l(k,31,tn) = sums_l(k,31,tn) + vst2 * rmask(j,i,sr) |
---|
543 | sums_l(k,32,tn) = sums_l(k,32,tn) + w2 * rmask(j,i,sr) |
---|
544 | ! |
---|
545 | !-- Perturbation energy |
---|
546 | |
---|
547 | sums_l(k,34,tn) = sums_l(k,34,tn) + 0.5 * & |
---|
548 | ( ust2 + vst2 + w2 ) * rmask(j,i,sr) |
---|
549 | sums_l_eper = sums_l_eper + & |
---|
550 | 0.5 * ( ust2+vst2+w2 ) * rmask(j,i,sr) |
---|
551 | |
---|
552 | ENDDO |
---|
553 | sums_l(nzb+5,pr_palm,tn) = sums_l(nzb+5,pr_palm,tn) & |
---|
554 | + sums_l_eper |
---|
555 | ENDDO |
---|
556 | ENDDO |
---|
557 | ENDIF |
---|
558 | ! |
---|
559 | !-- Horizontally averaged profiles of the vertical fluxes |
---|
560 | |
---|
561 | !$OMP DO |
---|
562 | DO i = nxl, nxr |
---|
563 | DO j = nys, nyn |
---|
564 | ! |
---|
565 | !-- Subgridscale fluxes (without Prandtl layer from k=nzb, |
---|
566 | !-- oterwise from k=nzb+1) |
---|
567 | !-- NOTE: for simplicity, nzb_diff_s_inner is used below, although |
---|
568 | !-- ---- strictly speaking the following k-loop would have to be |
---|
569 | !-- split up according to the staggered grid. |
---|
570 | !-- However, this implies no error since staggered velocity |
---|
571 | !-- components are zero at the walls and inside buildings. |
---|
572 | |
---|
573 | DO k = nzb_diff_s_inner(j,i)-1, nzt_diff |
---|
574 | ! |
---|
575 | !-- Momentum flux w"u" |
---|
576 | sums_l(k,12,tn) = sums_l(k,12,tn) - 0.25 * ( & |
---|
577 | km(k,j,i)+km(k+1,j,i)+km(k,j,i-1)+km(k+1,j,i-1) & |
---|
578 | ) * ( & |
---|
579 | ( u(k+1,j,i) - u(k,j,i) ) * ddzu(k+1) & |
---|
580 | + ( w(k,j,i) - w(k,j,i-1) ) * ddx & |
---|
581 | ) * rmask(j,i,sr) |
---|
582 | ! |
---|
583 | !-- Momentum flux w"v" |
---|
584 | sums_l(k,14,tn) = sums_l(k,14,tn) - 0.25 * ( & |
---|
585 | km(k,j,i)+km(k+1,j,i)+km(k,j-1,i)+km(k+1,j-1,i) & |
---|
586 | ) * ( & |
---|
587 | ( v(k+1,j,i) - v(k,j,i) ) * ddzu(k+1) & |
---|
588 | + ( w(k,j,i) - w(k,j-1,i) ) * ddy & |
---|
589 | ) * rmask(j,i,sr) |
---|
590 | ! |
---|
591 | !-- Heat flux w"pt" |
---|
592 | sums_l(k,16,tn) = sums_l(k,16,tn) & |
---|
593 | - 0.5 * ( kh(k,j,i) + kh(k+1,j,i) ) & |
---|
594 | * ( pt(k+1,j,i) - pt(k,j,i) ) & |
---|
595 | * ddzu(k+1) * rmask(j,i,sr) |
---|
596 | |
---|
597 | |
---|
598 | ! |
---|
599 | !-- Salinity flux w"sa" |
---|
600 | IF ( ocean ) THEN |
---|
601 | sums_l(k,65,tn) = sums_l(k,65,tn) & |
---|
602 | - 0.5 * ( kh(k,j,i) + kh(k+1,j,i) ) & |
---|
603 | * ( sa(k+1,j,i) - sa(k,j,i) ) & |
---|
604 | * ddzu(k+1) * rmask(j,i,sr) |
---|
605 | ENDIF |
---|
606 | |
---|
607 | ! |
---|
608 | !-- Buoyancy flux, water flux (humidity flux) w"q" |
---|
609 | IF ( humidity ) THEN |
---|
610 | sums_l(k,45,tn) = sums_l(k,45,tn) & |
---|
611 | - 0.5 * ( kh(k,j,i) + kh(k+1,j,i) ) & |
---|
612 | * ( vpt(k+1,j,i) - vpt(k,j,i) ) & |
---|
613 | * ddzu(k+1) * rmask(j,i,sr) |
---|
614 | sums_l(k,48,tn) = sums_l(k,48,tn) & |
---|
615 | - 0.5 * ( kh(k,j,i) + kh(k+1,j,i) ) & |
---|
616 | * ( q(k+1,j,i) - q(k,j,i) ) & |
---|
617 | * ddzu(k+1) * rmask(j,i,sr) |
---|
618 | |
---|
619 | IF ( cloud_physics ) THEN |
---|
620 | sums_l(k,51,tn) = sums_l(k,51,tn) & |
---|
621 | - 0.5 * ( kh(k,j,i) + kh(k+1,j,i) ) & |
---|
622 | * ( ( q(k+1,j,i) - ql(k+1,j,i) )& |
---|
623 | - ( q(k,j,i) - ql(k,j,i) ) ) & |
---|
624 | * ddzu(k+1) * rmask(j,i,sr) |
---|
625 | ENDIF |
---|
626 | ENDIF |
---|
627 | |
---|
628 | ! |
---|
629 | !-- Passive scalar flux |
---|
630 | IF ( passive_scalar ) THEN |
---|
631 | sums_l(k,48,tn) = sums_l(k,48,tn) & |
---|
632 | - 0.5 * ( kh(k,j,i) + kh(k+1,j,i) ) & |
---|
633 | * ( q(k+1,j,i) - q(k,j,i) ) & |
---|
634 | * ddzu(k+1) * rmask(j,i,sr) |
---|
635 | ENDIF |
---|
636 | |
---|
637 | ENDDO |
---|
638 | |
---|
639 | ! |
---|
640 | !-- Subgridscale fluxes in the Prandtl layer |
---|
641 | IF ( use_surface_fluxes ) THEN |
---|
642 | sums_l(nzb,12,tn) = sums_l(nzb,12,tn) + & |
---|
643 | usws(j,i) * rmask(j,i,sr) ! w"u" |
---|
644 | sums_l(nzb,14,tn) = sums_l(nzb,14,tn) + & |
---|
645 | vsws(j,i) * rmask(j,i,sr) ! w"v" |
---|
646 | sums_l(nzb,16,tn) = sums_l(nzb,16,tn) + & |
---|
647 | shf(j,i) * rmask(j,i,sr) ! w"pt" |
---|
648 | sums_l(nzb,58,tn) = sums_l(nzb,58,tn) + & |
---|
649 | 0.0 * rmask(j,i,sr) ! u"pt" |
---|
650 | sums_l(nzb,61,tn) = sums_l(nzb,61,tn) + & |
---|
651 | 0.0 * rmask(j,i,sr) ! v"pt" |
---|
652 | IF ( ocean ) THEN |
---|
653 | sums_l(nzb,65,tn) = sums_l(nzb,65,tn) + & |
---|
654 | saswsb(j,i) * rmask(j,i,sr) ! w"sa" |
---|
655 | ENDIF |
---|
656 | IF ( humidity ) THEN |
---|
657 | sums_l(nzb,48,tn) = sums_l(nzb,48,tn) + & |
---|
658 | qsws(j,i) * rmask(j,i,sr) ! w"q" (w"qv") |
---|
659 | sums_l(nzb,45,tn) = sums_l(nzb,45,tn) + ( & |
---|
660 | ( 1.0 + 0.61 * q(nzb,j,i) ) * & |
---|
661 | shf(j,i) + 0.61 * pt(nzb,j,i) * & |
---|
662 | qsws(j,i) ) |
---|
663 | IF ( cloud_droplets ) THEN |
---|
664 | sums_l(nzb,45,tn) = sums_l(nzb,45,tn) + ( & |
---|
665 | ( 1.0 + 0.61 * q(nzb,j,i) - & |
---|
666 | ql(nzb,j,i) ) * shf(j,i) + & |
---|
667 | 0.61 * pt(nzb,j,i) * qsws(j,i) ) |
---|
668 | ENDIF |
---|
669 | IF ( cloud_physics ) THEN |
---|
670 | ! |
---|
671 | !-- Formula does not work if ql(nzb) /= 0.0 |
---|
672 | sums_l(nzb,51,tn) = sums_l(nzb,51,tn) + & ! w"q" (w"qv") |
---|
673 | qsws(j,i) * rmask(j,i,sr) |
---|
674 | ENDIF |
---|
675 | ENDIF |
---|
676 | IF ( passive_scalar ) THEN |
---|
677 | sums_l(nzb,48,tn) = sums_l(nzb,48,tn) + & |
---|
678 | qsws(j,i) * rmask(j,i,sr) ! w"q" (w"qv") |
---|
679 | ENDIF |
---|
680 | ENDIF |
---|
681 | |
---|
682 | ! |
---|
683 | !-- Subgridscale fluxes at the top surface |
---|
684 | IF ( use_top_fluxes ) THEN |
---|
685 | sums_l(nzt:nzt+1,12,tn) = sums_l(nzt:nzt+1,12,tn) + & |
---|
686 | uswst(j,i) * rmask(j,i,sr) ! w"u" |
---|
687 | sums_l(nzt:nzt+1,14,tn) = sums_l(nzt:nzt+1,14,tn) + & |
---|
688 | vswst(j,i) * rmask(j,i,sr) ! w"v" |
---|
689 | sums_l(nzt:nzt+1,16,tn) = sums_l(nzt:nzt+1,16,tn) + & |
---|
690 | tswst(j,i) * rmask(j,i,sr) ! w"pt" |
---|
691 | sums_l(nzt:nzt+1,58,tn) = sums_l(nzt:nzt+1,58,tn) + & |
---|
692 | 0.0 * rmask(j,i,sr) ! u"pt" |
---|
693 | sums_l(nzt:nzt+1,61,tn) = sums_l(nzt:nzt+1,61,tn) + & |
---|
694 | 0.0 * rmask(j,i,sr) ! v"pt" |
---|
695 | |
---|
696 | IF ( ocean ) THEN |
---|
697 | sums_l(nzt,65,tn) = sums_l(nzt,65,tn) + & |
---|
698 | saswst(j,i) * rmask(j,i,sr) ! w"sa" |
---|
699 | ENDIF |
---|
700 | IF ( humidity ) THEN |
---|
701 | sums_l(nzt,48,tn) = sums_l(nzt,48,tn) + & |
---|
702 | qswst(j,i) * rmask(j,i,sr) ! w"q" (w"qv") |
---|
703 | sums_l(nzt,45,tn) = sums_l(nzt,45,tn) + ( & |
---|
704 | ( 1.0 + 0.61 * q(nzt,j,i) ) * & |
---|
705 | tswst(j,i) + 0.61 * pt(nzt,j,i) * & |
---|
706 | qswst(j,i) ) |
---|
707 | IF ( cloud_droplets ) THEN |
---|
708 | sums_l(nzt,45,tn) = sums_l(nzt,45,tn) + ( & |
---|
709 | ( 1.0 + 0.61 * q(nzt,j,i) - & |
---|
710 | ql(nzt,j,i) ) * tswst(j,i) + & |
---|
711 | 0.61 * pt(nzt,j,i) * qswst(j,i) ) |
---|
712 | ENDIF |
---|
713 | IF ( cloud_physics ) THEN |
---|
714 | ! |
---|
715 | !-- Formula does not work if ql(nzb) /= 0.0 |
---|
716 | sums_l(nzt,51,tn) = sums_l(nzt,51,tn) + & ! w"q" (w"qv") |
---|
717 | qswst(j,i) * rmask(j,i,sr) |
---|
718 | ENDIF |
---|
719 | ENDIF |
---|
720 | IF ( passive_scalar ) THEN |
---|
721 | sums_l(nzt,48,tn) = sums_l(nzt,48,tn) + & |
---|
722 | qswst(j,i) * rmask(j,i,sr) ! w"q" (w"qv") |
---|
723 | ENDIF |
---|
724 | ENDIF |
---|
725 | |
---|
726 | ! |
---|
727 | !-- Resolved fluxes (can be computed for all horizontal points) |
---|
728 | !-- NOTE: for simplicity, nzb_s_inner is used below, although strictly |
---|
729 | !-- ---- speaking the following k-loop would have to be split up and |
---|
730 | !-- rearranged according to the staggered grid. |
---|
731 | DO k = nzb_s_inner(j,i), nzt |
---|
732 | ust = 0.5 * ( u(k,j,i) - hom(k,1,1,sr) + & |
---|
733 | u(k+1,j,i) - hom(k+1,1,1,sr) ) |
---|
734 | vst = 0.5 * ( v(k,j,i) - hom(k,1,2,sr) + & |
---|
735 | v(k+1,j,i) - hom(k+1,1,2,sr) ) |
---|
736 | pts = 0.5 * ( pt(k,j,i) - hom(k,1,4,sr) + & |
---|
737 | pt(k+1,j,i) - hom(k+1,1,4,sr) ) |
---|
738 | |
---|
739 | !-- Higher moments |
---|
740 | sums_l(k,35,tn) = sums_l(k,35,tn) + pts * w(k,j,i)**2 * & |
---|
741 | rmask(j,i,sr) |
---|
742 | sums_l(k,36,tn) = sums_l(k,36,tn) + pts**2 * w(k,j,i) * & |
---|
743 | rmask(j,i,sr) |
---|
744 | |
---|
745 | ! |
---|
746 | !-- Salinity flux and density (density does not belong to here, |
---|
747 | !-- but so far there is no other suitable place to calculate) |
---|
748 | IF ( ocean ) THEN |
---|
749 | IF( .NOT. ws_scheme_sca .OR. sr /= 0 ) THEN |
---|
750 | pts = 0.5 * ( sa(k,j,i) - hom(k,1,23,sr) + & |
---|
751 | sa(k+1,j,i) - hom(k+1,1,23,sr) ) |
---|
752 | sums_l(k,66,tn) = sums_l(k,66,tn) + pts * w(k,j,i) * & |
---|
753 | rmask(j,i,sr) |
---|
754 | ENDIF |
---|
755 | sums_l(k,64,tn) = sums_l(k,64,tn) + rho(k,j,i) * & |
---|
756 | rmask(j,i,sr) |
---|
757 | sums_l(k,71,tn) = sums_l(k,71,tn) + prho(k,j,i) * & |
---|
758 | rmask(j,i,sr) |
---|
759 | ENDIF |
---|
760 | |
---|
761 | ! |
---|
762 | !-- Buoyancy flux, water flux, humidity flux, liquid water |
---|
763 | !-- content, rain drop concentration and rain water content |
---|
764 | IF ( humidity ) THEN |
---|
765 | IF ( cloud_physics .OR. cloud_droplets ) THEN |
---|
766 | pts = 0.5 * ( vpt(k,j,i) - hom(k,1,44,sr) + & |
---|
767 | vpt(k+1,j,i) - hom(k+1,1,44,sr) ) |
---|
768 | sums_l(k,46,tn) = sums_l(k,46,tn) + pts * w(k,j,i) * & |
---|
769 | rmask(j,i,sr) |
---|
770 | IF ( .NOT. cloud_droplets ) THEN |
---|
771 | pts = 0.5 * & |
---|
772 | ( ( q(k,j,i) - ql(k,j,i) ) - & |
---|
773 | hom(k,1,42,sr) + & |
---|
774 | ( q(k+1,j,i) - ql(k+1,j,i) ) - & |
---|
775 | hom(k+1,1,42,sr) ) |
---|
776 | sums_l(k,52,tn) = sums_l(k,52,tn) + pts * w(k,j,i) * & |
---|
777 | rmask(j,i,sr) |
---|
778 | IF ( icloud_scheme == 0 ) THEN |
---|
779 | sums_l(k,54,tn) = sums_l(k,54,tn) + ql(k,j,i) * & |
---|
780 | rmask(j,i,sr) |
---|
781 | sums_l(k,75,tn) = sums_l(k,75,tn) + qc(k,j,i) * & |
---|
782 | rmask(j,i,sr) |
---|
783 | IF ( precipitation ) THEN |
---|
784 | sums_l(k,73,tn) = sums_l(k,73,tn) + nr(k,j,i) * & |
---|
785 | rmask(j,i,sr) |
---|
786 | sums_l(k,74,tn) = sums_l(k,74,tn) + qr(k,j,i) * & |
---|
787 | rmask(j,i,sr) |
---|
788 | sums_l(k,76,tn) = sums_l(k,76,tn) + prr(k,j,i) *& |
---|
789 | rmask(j,i,sr) |
---|
790 | ENDIF |
---|
791 | ELSE |
---|
792 | sums_l(k,54,tn) = sums_l(k,54,tn) + ql(k,j,i) * & |
---|
793 | rmask(j,i,sr) |
---|
794 | ENDIF |
---|
795 | ELSE |
---|
796 | sums_l(k,54,tn) = sums_l(k,54,tn) + ql(k,j,i) * & |
---|
797 | rmask(j,i,sr) |
---|
798 | ENDIF |
---|
799 | ELSE |
---|
800 | IF( .NOT. ws_scheme_sca .OR. sr /= 0 ) THEN |
---|
801 | pts = 0.5 * ( vpt(k,j,i) - hom(k,1,44,sr) + & |
---|
802 | vpt(k+1,j,i) - hom(k+1,1,44,sr) ) |
---|
803 | sums_l(k,46,tn) = sums_l(k,46,tn) + pts * w(k,j,i) * & |
---|
804 | rmask(j,i,sr) |
---|
805 | ELSE IF ( ws_scheme_sca .AND. sr == 0 ) THEN |
---|
806 | sums_l(k,46,tn) = ( 1.0 + 0.61 * hom(k,1,41,sr) ) * & |
---|
807 | sums_l(k,17,tn) + & |
---|
808 | 0.61 * hom(k,1,4,sr) * sums_l(k,49,tn) |
---|
809 | END IF |
---|
810 | END IF |
---|
811 | ENDIF |
---|
812 | ! |
---|
813 | !-- Passive scalar flux |
---|
814 | IF ( passive_scalar .AND. ( .NOT. ws_scheme_sca & |
---|
815 | .OR. sr /= 0 ) ) THEN |
---|
816 | pts = 0.5 * ( q(k,j,i) - hom(k,1,41,sr) + & |
---|
817 | q(k+1,j,i) - hom(k+1,1,41,sr) ) |
---|
818 | sums_l(k,49,tn) = sums_l(k,49,tn) + pts * w(k,j,i) * & |
---|
819 | rmask(j,i,sr) |
---|
820 | ENDIF |
---|
821 | |
---|
822 | ! |
---|
823 | !-- Energy flux w*e* |
---|
824 | !-- has to be adjusted |
---|
825 | sums_l(k,37,tn) = sums_l(k,37,tn) + w(k,j,i) * 0.5 * & |
---|
826 | ( ust**2 + vst**2 + w(k,j,i)**2 )& |
---|
827 | * rmask(j,i,sr) |
---|
828 | ENDDO |
---|
829 | ENDDO |
---|
830 | ENDDO |
---|
831 | ! |
---|
832 | !-- For speed optimization fluxes which have been computed in part directly |
---|
833 | !-- inside the WS advection routines are treated seperatly |
---|
834 | !-- Momentum fluxes first: |
---|
835 | IF ( .NOT. ws_scheme_mom .OR. sr /= 0 ) THEN |
---|
836 | !$OMP DO |
---|
837 | DO i = nxl, nxr |
---|
838 | DO j = nys, nyn |
---|
839 | DO k = nzb_diff_s_inner(j,i)-1, nzt_diff |
---|
840 | ust = 0.5 * ( u(k,j,i) - hom(k,1,1,sr) + & |
---|
841 | u(k+1,j,i) - hom(k+1,1,1,sr) ) |
---|
842 | vst = 0.5 * ( v(k,j,i) - hom(k,1,2,sr) + & |
---|
843 | v(k+1,j,i) - hom(k+1,1,2,sr) ) |
---|
844 | ! |
---|
845 | !-- Momentum flux w*u* |
---|
846 | sums_l(k,13,tn) = sums_l(k,13,tn) + 0.5 * & |
---|
847 | ( w(k,j,i-1) + w(k,j,i) ) & |
---|
848 | * ust * rmask(j,i,sr) |
---|
849 | ! |
---|
850 | !-- Momentum flux w*v* |
---|
851 | sums_l(k,15,tn) = sums_l(k,15,tn) + 0.5 * & |
---|
852 | ( w(k,j-1,i) + w(k,j,i) ) & |
---|
853 | * vst * rmask(j,i,sr) |
---|
854 | ENDDO |
---|
855 | ENDDO |
---|
856 | ENDDO |
---|
857 | |
---|
858 | ENDIF |
---|
859 | IF ( .NOT. ws_scheme_sca .OR. sr /= 0 ) THEN |
---|
860 | !$OMP DO |
---|
861 | DO i = nxl, nxr |
---|
862 | DO j = nys, nyn |
---|
863 | DO k = nzb_diff_s_inner(j,i)-1, nzt_diff |
---|
864 | ! |
---|
865 | !-- Vertical heat flux |
---|
866 | sums_l(k,17,tn) = sums_l(k,17,tn) + 0.5 * & |
---|
867 | ( pt(k,j,i) - hom(k,1,4,sr) + & |
---|
868 | pt(k+1,j,i) - hom(k+1,1,4,sr) ) & |
---|
869 | * w(k,j,i) * rmask(j,i,sr) |
---|
870 | IF ( humidity ) THEN |
---|
871 | pts = 0.5 * ( q(k,j,i) - hom(k,1,41,sr) + & |
---|
872 | q(k+1,j,i) - hom(k+1,1,41,sr) ) |
---|
873 | sums_l(k,49,tn) = sums_l(k,49,tn) + pts * w(k,j,i) * & |
---|
874 | rmask(j,i,sr) |
---|
875 | ENDIF |
---|
876 | ENDDO |
---|
877 | ENDDO |
---|
878 | ENDDO |
---|
879 | |
---|
880 | ENDIF |
---|
881 | |
---|
882 | |
---|
883 | ! |
---|
884 | !-- Density at top follows Neumann condition |
---|
885 | IF ( ocean ) THEN |
---|
886 | sums_l(nzt+1,64,tn) = sums_l(nzt,64,tn) |
---|
887 | sums_l(nzt+1,71,tn) = sums_l(nzt,71,tn) |
---|
888 | ENDIF |
---|
889 | |
---|
890 | ! |
---|
891 | !-- Divergence of vertical flux of resolved scale energy and pressure |
---|
892 | !-- fluctuations as well as flux of pressure fluctuation itself (68). |
---|
893 | !-- First calculate the products, then the divergence. |
---|
894 | !-- Calculation is time consuming. Do it only, if profiles shall be plotted. |
---|
895 | IF ( hom(nzb+1,2,55,0) /= 0.0 .OR. hom(nzb+1,2,68,0) /= 0.0 ) THEN |
---|
896 | |
---|
897 | sums_ll = 0.0 ! local array |
---|
898 | |
---|
899 | !$OMP DO |
---|
900 | DO i = nxl, nxr |
---|
901 | DO j = nys, nyn |
---|
902 | DO k = nzb_s_inner(j,i)+1, nzt |
---|
903 | |
---|
904 | sums_ll(k,1) = sums_ll(k,1) + 0.5 * w(k,j,i) * ( & |
---|
905 | ( 0.25 * ( u(k,j,i)+u(k+1,j,i)+u(k,j,i+1)+u(k+1,j,i+1) & |
---|
906 | - 0.5 * ( hom(k,1,1,sr) + hom(k+1,1,1,sr) ) & |
---|
907 | ) )**2 & |
---|
908 | + ( 0.25 * ( v(k,j,i)+v(k+1,j,i)+v(k,j+1,i)+v(k+1,j+1,i) & |
---|
909 | - 0.5 * ( hom(k,1,2,sr) + hom(k+1,1,2,sr) ) & |
---|
910 | ) )**2 & |
---|
911 | + w(k,j,i)**2 ) |
---|
912 | |
---|
913 | sums_ll(k,2) = sums_ll(k,2) + 0.5 * w(k,j,i) & |
---|
914 | * ( p(k,j,i) + p(k+1,j,i) ) |
---|
915 | |
---|
916 | ENDDO |
---|
917 | ENDDO |
---|
918 | ENDDO |
---|
919 | sums_ll(0,1) = 0.0 ! because w is zero at the bottom |
---|
920 | sums_ll(nzt+1,1) = 0.0 |
---|
921 | sums_ll(0,2) = 0.0 |
---|
922 | sums_ll(nzt+1,2) = 0.0 |
---|
923 | |
---|
924 | DO k = nzb+1, nzt |
---|
925 | sums_l(k,55,tn) = ( sums_ll(k,1) - sums_ll(k-1,1) ) * ddzw(k) |
---|
926 | sums_l(k,56,tn) = ( sums_ll(k,2) - sums_ll(k-1,2) ) * ddzw(k) |
---|
927 | sums_l(k,68,tn) = sums_ll(k,2) |
---|
928 | ENDDO |
---|
929 | sums_l(nzb,55,tn) = sums_l(nzb+1,55,tn) |
---|
930 | sums_l(nzb,56,tn) = sums_l(nzb+1,56,tn) |
---|
931 | sums_l(nzb,68,tn) = 0.0 ! because w* = 0 at nzb |
---|
932 | |
---|
933 | ENDIF |
---|
934 | |
---|
935 | ! |
---|
936 | !-- Divergence of vertical flux of SGS TKE and the flux itself (69) |
---|
937 | IF ( hom(nzb+1,2,57,0) /= 0.0 .OR. hom(nzb+1,2,69,0) /= 0.0 ) THEN |
---|
938 | |
---|
939 | !$OMP DO |
---|
940 | DO i = nxl, nxr |
---|
941 | DO j = nys, nyn |
---|
942 | DO k = nzb_s_inner(j,i)+1, nzt |
---|
943 | |
---|
944 | sums_l(k,57,tn) = sums_l(k,57,tn) - 0.5 * ( & |
---|
945 | (km(k,j,i)+km(k+1,j,i)) * (e(k+1,j,i)-e(k,j,i)) * ddzu(k+1) & |
---|
946 | - (km(k-1,j,i)+km(k,j,i)) * (e(k,j,i)-e(k-1,j,i)) * ddzu(k) & |
---|
947 | ) * ddzw(k) |
---|
948 | |
---|
949 | sums_l(k,69,tn) = sums_l(k,69,tn) - 0.5 * ( & |
---|
950 | (km(k,j,i)+km(k+1,j,i)) * (e(k+1,j,i)-e(k,j,i)) * ddzu(k+1) & |
---|
951 | ) |
---|
952 | |
---|
953 | ENDDO |
---|
954 | ENDDO |
---|
955 | ENDDO |
---|
956 | sums_l(nzb,57,tn) = sums_l(nzb+1,57,tn) |
---|
957 | sums_l(nzb,69,tn) = sums_l(nzb+1,69,tn) |
---|
958 | |
---|
959 | ENDIF |
---|
960 | |
---|
961 | ! |
---|
962 | !-- Horizontal heat fluxes (subgrid, resolved, total). |
---|
963 | !-- Do it only, if profiles shall be plotted. |
---|
964 | IF ( hom(nzb+1,2,58,0) /= 0.0 ) THEN |
---|
965 | |
---|
966 | !$OMP DO |
---|
967 | DO i = nxl, nxr |
---|
968 | DO j = nys, nyn |
---|
969 | DO k = nzb_s_inner(j,i)+1, nzt |
---|
970 | ! |
---|
971 | !-- Subgrid horizontal heat fluxes u"pt", v"pt" |
---|
972 | sums_l(k,58,tn) = sums_l(k,58,tn) - 0.5 * & |
---|
973 | ( kh(k,j,i) + kh(k,j,i-1) ) & |
---|
974 | * ( pt(k,j,i-1) - pt(k,j,i) ) & |
---|
975 | * ddx * rmask(j,i,sr) |
---|
976 | sums_l(k,61,tn) = sums_l(k,61,tn) - 0.5 * & |
---|
977 | ( kh(k,j,i) + kh(k,j-1,i) ) & |
---|
978 | * ( pt(k,j-1,i) - pt(k,j,i) ) & |
---|
979 | * ddy * rmask(j,i,sr) |
---|
980 | ! |
---|
981 | !-- Resolved horizontal heat fluxes u*pt*, v*pt* |
---|
982 | sums_l(k,59,tn) = sums_l(k,59,tn) + & |
---|
983 | ( u(k,j,i) - hom(k,1,1,sr) ) & |
---|
984 | * 0.5 * ( pt(k,j,i-1) - hom(k,1,4,sr) + & |
---|
985 | pt(k,j,i) - hom(k,1,4,sr) ) |
---|
986 | pts = 0.5 * ( pt(k,j-1,i) - hom(k,1,4,sr) + & |
---|
987 | pt(k,j,i) - hom(k,1,4,sr) ) |
---|
988 | sums_l(k,62,tn) = sums_l(k,62,tn) + & |
---|
989 | ( v(k,j,i) - hom(k,1,2,sr) ) & |
---|
990 | * 0.5 * ( pt(k,j-1,i) - hom(k,1,4,sr) + & |
---|
991 | pt(k,j,i) - hom(k,1,4,sr) ) |
---|
992 | ENDDO |
---|
993 | ENDDO |
---|
994 | ENDDO |
---|
995 | ! |
---|
996 | !-- Fluxes at the surface must be zero (e.g. due to the Prandtl-layer) |
---|
997 | sums_l(nzb,58,tn) = 0.0 |
---|
998 | sums_l(nzb,59,tn) = 0.0 |
---|
999 | sums_l(nzb,60,tn) = 0.0 |
---|
1000 | sums_l(nzb,61,tn) = 0.0 |
---|
1001 | sums_l(nzb,62,tn) = 0.0 |
---|
1002 | sums_l(nzb,63,tn) = 0.0 |
---|
1003 | |
---|
1004 | ENDIF |
---|
1005 | |
---|
1006 | ! |
---|
1007 | !-- Calculate the user-defined profiles |
---|
1008 | CALL user_statistics( 'profiles', sr, tn ) |
---|
1009 | !$OMP END PARALLEL |
---|
1010 | |
---|
1011 | ! |
---|
1012 | !-- Summation of thread sums |
---|
1013 | IF ( threads_per_task > 1 ) THEN |
---|
1014 | DO i = 1, threads_per_task-1 |
---|
1015 | sums_l(:,3,0) = sums_l(:,3,0) + sums_l(:,3,i) |
---|
1016 | sums_l(:,4:40,0) = sums_l(:,4:40,0) + sums_l(:,4:40,i) |
---|
1017 | sums_l(:,45:pr_palm,0) = sums_l(:,45:pr_palm,0) + & |
---|
1018 | sums_l(:,45:pr_palm,i) |
---|
1019 | IF ( max_pr_user > 0 ) THEN |
---|
1020 | sums_l(:,pr_palm+1:pr_palm+max_pr_user,0) = & |
---|
1021 | sums_l(:,pr_palm+1:pr_palm+max_pr_user,0) + & |
---|
1022 | sums_l(:,pr_palm+1:pr_palm+max_pr_user,i) |
---|
1023 | ENDIF |
---|
1024 | ENDDO |
---|
1025 | ENDIF |
---|
1026 | |
---|
1027 | #if defined( __parallel ) |
---|
1028 | |
---|
1029 | ! |
---|
1030 | !-- Compute total sum from local sums |
---|
1031 | IF ( collective_wait ) CALL MPI_BARRIER( comm2d, ierr ) |
---|
1032 | CALL MPI_ALLREDUCE( sums_l(nzb,1,0), sums(nzb,1), ngp_sums, MPI_REAL, & |
---|
1033 | MPI_SUM, comm2d, ierr ) |
---|
1034 | #else |
---|
1035 | sums = sums_l(:,:,0) |
---|
1036 | #endif |
---|
1037 | |
---|
1038 | ! |
---|
1039 | !-- Final values are obtained by division by the total number of grid points |
---|
1040 | !-- used for summation. After that store profiles. |
---|
1041 | !-- Profiles: |
---|
1042 | DO k = nzb, nzt+1 |
---|
1043 | sums(k,3) = sums(k,3) / ngp_2dh(sr) |
---|
1044 | sums(k,8:11) = sums(k,8:11) / ngp_2dh_s_inner(k,sr) |
---|
1045 | sums(k,12:22) = sums(k,12:22) / ngp_2dh(sr) |
---|
1046 | sums(k,23:29) = sums(k,23:29) / ngp_2dh_s_inner(k,sr) |
---|
1047 | sums(k,30:32) = sums(k,30:32) / ngp_2dh(sr) |
---|
1048 | sums(k,33:34) = sums(k,33:34) / ngp_2dh_s_inner(k,sr) |
---|
1049 | sums(k,35:39) = sums(k,35:39) / ngp_2dh(sr) |
---|
1050 | sums(k,40) = sums(k,40) / ngp_2dh_s_inner(k,sr) |
---|
1051 | sums(k,45:53) = sums(k,45:53) / ngp_2dh(sr) |
---|
1052 | sums(k,54) = sums(k,54) / ngp_2dh_s_inner(k,sr) |
---|
1053 | sums(k,55:63) = sums(k,55:63) / ngp_2dh(sr) |
---|
1054 | sums(k,64) = sums(k,64) / ngp_2dh_s_inner(k,sr) |
---|
1055 | sums(k,65:69) = sums(k,65:69) / ngp_2dh(sr) |
---|
1056 | sums(k,70:pr_palm-2) = sums(k,70:pr_palm-2)/ ngp_2dh_s_inner(k,sr) |
---|
1057 | ENDDO |
---|
1058 | |
---|
1059 | !-- Upstream-parts |
---|
1060 | sums(nzb:nzb+11,pr_palm-1) = sums(nzb:nzb+11,pr_palm-1) / ngp_3d(sr) |
---|
1061 | !-- u* and so on |
---|
1062 | !-- As sums(nzb:nzb+3,pr_palm) are full 2D arrays (us, usws, vsws, ts) whose |
---|
1063 | !-- size is always ( nx + 1 ) * ( ny + 1 ), defined at the first grid layer |
---|
1064 | !-- above the topography, they are being divided by ngp_2dh(sr) |
---|
1065 | sums(nzb:nzb+3,pr_palm) = sums(nzb:nzb+3,pr_palm) / & |
---|
1066 | ngp_2dh(sr) |
---|
1067 | sums(nzb+12,pr_palm) = sums(nzb+12,pr_palm) / & ! qs |
---|
1068 | ngp_2dh(sr) |
---|
1069 | !-- eges, e* |
---|
1070 | sums(nzb+4:nzb+5,pr_palm) = sums(nzb+4:nzb+5,pr_palm) / & |
---|
1071 | ngp_3d(sr) |
---|
1072 | !-- Old and new divergence |
---|
1073 | sums(nzb+9:nzb+10,pr_palm) = sums(nzb+9:nzb+10,pr_palm) / & |
---|
1074 | ngp_3d_inner(sr) |
---|
1075 | |
---|
1076 | !-- User-defined profiles |
---|
1077 | IF ( max_pr_user > 0 ) THEN |
---|
1078 | DO k = nzb, nzt+1 |
---|
1079 | sums(k,pr_palm+1:pr_palm+max_pr_user) = & |
---|
1080 | sums(k,pr_palm+1:pr_palm+max_pr_user) / & |
---|
1081 | ngp_2dh_s_inner(k,sr) |
---|
1082 | ENDDO |
---|
1083 | ENDIF |
---|
1084 | |
---|
1085 | ! |
---|
1086 | !-- Collect horizontal average in hom. |
---|
1087 | !-- Compute deduced averages (e.g. total heat flux) |
---|
1088 | hom(:,1,3,sr) = sums(:,3) ! w |
---|
1089 | hom(:,1,8,sr) = sums(:,8) ! e profiles 5-7 are initial profiles |
---|
1090 | hom(:,1,9,sr) = sums(:,9) ! km |
---|
1091 | hom(:,1,10,sr) = sums(:,10) ! kh |
---|
1092 | hom(:,1,11,sr) = sums(:,11) ! l |
---|
1093 | hom(:,1,12,sr) = sums(:,12) ! w"u" |
---|
1094 | hom(:,1,13,sr) = sums(:,13) ! w*u* |
---|
1095 | hom(:,1,14,sr) = sums(:,14) ! w"v" |
---|
1096 | hom(:,1,15,sr) = sums(:,15) ! w*v* |
---|
1097 | hom(:,1,16,sr) = sums(:,16) ! w"pt" |
---|
1098 | hom(:,1,17,sr) = sums(:,17) ! w*pt* |
---|
1099 | hom(:,1,18,sr) = sums(:,16) + sums(:,17) ! wpt |
---|
1100 | hom(:,1,19,sr) = sums(:,12) + sums(:,13) ! wu |
---|
1101 | hom(:,1,20,sr) = sums(:,14) + sums(:,15) ! wv |
---|
1102 | hom(:,1,21,sr) = sums(:,21) ! w*pt*BC |
---|
1103 | hom(:,1,22,sr) = sums(:,16) + sums(:,21) ! wptBC |
---|
1104 | ! profile 24 is initial profile (sa) |
---|
1105 | ! profiles 25-29 left empty for initial |
---|
1106 | ! profiles |
---|
1107 | hom(:,1,30,sr) = sums(:,30) ! u*2 |
---|
1108 | hom(:,1,31,sr) = sums(:,31) ! v*2 |
---|
1109 | hom(:,1,32,sr) = sums(:,32) ! w*2 |
---|
1110 | hom(:,1,33,sr) = sums(:,33) ! pt*2 |
---|
1111 | hom(:,1,34,sr) = sums(:,34) ! e* |
---|
1112 | hom(:,1,35,sr) = sums(:,35) ! w*2pt* |
---|
1113 | hom(:,1,36,sr) = sums(:,36) ! w*pt*2 |
---|
1114 | hom(:,1,37,sr) = sums(:,37) ! w*e* |
---|
1115 | hom(:,1,38,sr) = sums(:,38) ! w*3 |
---|
1116 | hom(:,1,39,sr) = sums(:,38) / ( abs( sums(:,32) ) + 1E-20 )**1.5 ! Sw |
---|
1117 | hom(:,1,40,sr) = sums(:,40) ! p |
---|
1118 | hom(:,1,45,sr) = sums(:,45) ! w"vpt" |
---|
1119 | hom(:,1,46,sr) = sums(:,46) ! w*vpt* |
---|
1120 | hom(:,1,47,sr) = sums(:,45) + sums(:,46) ! wvpt |
---|
1121 | hom(:,1,48,sr) = sums(:,48) ! w"q" (w"qv") |
---|
1122 | hom(:,1,49,sr) = sums(:,49) ! w*q* (w*qv*) |
---|
1123 | hom(:,1,50,sr) = sums(:,48) + sums(:,49) ! wq (wqv) |
---|
1124 | hom(:,1,51,sr) = sums(:,51) ! w"qv" |
---|
1125 | hom(:,1,52,sr) = sums(:,52) ! w*qv* |
---|
1126 | hom(:,1,53,sr) = sums(:,52) + sums(:,51) ! wq (wqv) |
---|
1127 | hom(:,1,54,sr) = sums(:,54) ! ql |
---|
1128 | hom(:,1,55,sr) = sums(:,55) ! w*u*u*/dz |
---|
1129 | hom(:,1,56,sr) = sums(:,56) ! w*p*/dz |
---|
1130 | hom(:,1,57,sr) = sums(:,57) ! ( w"e + w"p"/rho )/dz |
---|
1131 | hom(:,1,58,sr) = sums(:,58) ! u"pt" |
---|
1132 | hom(:,1,59,sr) = sums(:,59) ! u*pt* |
---|
1133 | hom(:,1,60,sr) = sums(:,58) + sums(:,59) ! upt_t |
---|
1134 | hom(:,1,61,sr) = sums(:,61) ! v"pt" |
---|
1135 | hom(:,1,62,sr) = sums(:,62) ! v*pt* |
---|
1136 | hom(:,1,63,sr) = sums(:,61) + sums(:,62) ! vpt_t |
---|
1137 | hom(:,1,64,sr) = sums(:,64) ! rho |
---|
1138 | hom(:,1,65,sr) = sums(:,65) ! w"sa" |
---|
1139 | hom(:,1,66,sr) = sums(:,66) ! w*sa* |
---|
1140 | hom(:,1,67,sr) = sums(:,65) + sums(:,66) ! wsa |
---|
1141 | hom(:,1,68,sr) = sums(:,68) ! w*p* |
---|
1142 | hom(:,1,69,sr) = sums(:,69) ! w"e + w"p"/rho |
---|
1143 | hom(:,1,70,sr) = sums(:,70) ! q*2 |
---|
1144 | hom(:,1,71,sr) = sums(:,71) ! prho |
---|
1145 | hom(:,1,72,sr) = hyp * 1E-4 ! hyp in dbar |
---|
1146 | hom(:,1,73,sr) = sums(:,73) ! nr |
---|
1147 | hom(:,1,74,sr) = sums(:,74) ! qr |
---|
1148 | hom(:,1,75,sr) = sums(:,75) ! qc |
---|
1149 | hom(:,1,76,sr) = sums(:,76) ! prr (precipitation rate) |
---|
1150 | |
---|
1151 | hom(:,1,pr_palm-1,sr) = sums(:,pr_palm-1) |
---|
1152 | ! upstream-parts u_x, u_y, u_z, v_x, |
---|
1153 | ! v_y, usw. (in last but one profile) |
---|
1154 | hom(:,1,pr_palm,sr) = sums(:,pr_palm) |
---|
1155 | ! u*, w'u', w'v', t* (in last profile) |
---|
1156 | |
---|
1157 | IF ( max_pr_user > 0 ) THEN ! user-defined profiles |
---|
1158 | hom(:,1,pr_palm+1:pr_palm+max_pr_user,sr) = & |
---|
1159 | sums(:,pr_palm+1:pr_palm+max_pr_user) |
---|
1160 | ENDIF |
---|
1161 | |
---|
1162 | ! |
---|
1163 | !-- Determine the boundary layer height using two different schemes. |
---|
1164 | !-- First scheme: Starting from the Earth's (Ocean's) surface, look for the |
---|
1165 | !-- first relative minimum (maximum) of the total heat flux. |
---|
1166 | !-- The corresponding height is assumed as the boundary layer height, if it |
---|
1167 | !-- is less than 1.5 times the height where the heat flux becomes negative |
---|
1168 | !-- (positive) for the first time. |
---|
1169 | z_i(1) = 0.0 |
---|
1170 | first = .TRUE. |
---|
1171 | |
---|
1172 | IF ( ocean ) THEN |
---|
1173 | DO k = nzt, nzb+1, -1 |
---|
1174 | IF ( first .AND. hom(k,1,18,sr) < 0.0 & |
---|
1175 | .AND. abs(hom(k,1,18,sr)) > 1.0E-8) THEN |
---|
1176 | first = .FALSE. |
---|
1177 | height = zw(k) |
---|
1178 | ENDIF |
---|
1179 | IF ( hom(k,1,18,sr) < 0.0 .AND. & |
---|
1180 | abs(hom(k,1,18,sr)) > 1.0E-8 .AND. & |
---|
1181 | hom(k-1,1,18,sr) > hom(k,1,18,sr) ) THEN |
---|
1182 | IF ( zw(k) < 1.5 * height ) THEN |
---|
1183 | z_i(1) = zw(k) |
---|
1184 | ELSE |
---|
1185 | z_i(1) = height |
---|
1186 | ENDIF |
---|
1187 | EXIT |
---|
1188 | ENDIF |
---|
1189 | ENDDO |
---|
1190 | ELSE |
---|
1191 | DO k = nzb, nzt-1 |
---|
1192 | IF ( first .AND. hom(k,1,18,sr) < 0.0 & |
---|
1193 | .AND. abs(hom(k,1,18,sr)) > 1.0E-8 ) THEN |
---|
1194 | first = .FALSE. |
---|
1195 | height = zw(k) |
---|
1196 | ENDIF |
---|
1197 | IF ( hom(k,1,18,sr) < 0.0 .AND. & |
---|
1198 | abs(hom(k,1,18,sr)) > 1.0E-8 .AND. & |
---|
1199 | hom(k+1,1,18,sr) > hom(k,1,18,sr) ) THEN |
---|
1200 | IF ( zw(k) < 1.5 * height ) THEN |
---|
1201 | z_i(1) = zw(k) |
---|
1202 | ELSE |
---|
1203 | z_i(1) = height |
---|
1204 | ENDIF |
---|
1205 | EXIT |
---|
1206 | ENDIF |
---|
1207 | ENDDO |
---|
1208 | ENDIF |
---|
1209 | |
---|
1210 | ! |
---|
1211 | !-- Second scheme: Gradient scheme from Sullivan et al. (1998), modified |
---|
1212 | !-- by Uhlenbrock(2006). The boundary layer height is the height with the |
---|
1213 | !-- maximal local temperature gradient: starting from the second (the last |
---|
1214 | !-- but one) vertical gridpoint, the local gradient must be at least |
---|
1215 | !-- 0.2K/100m and greater than the next four gradients. |
---|
1216 | !-- WARNING: The threshold value of 0.2K/100m must be adjusted for the |
---|
1217 | !-- ocean case! |
---|
1218 | z_i(2) = 0.0 |
---|
1219 | DO k = nzb+1, nzt+1 |
---|
1220 | dptdz(k) = ( hom(k,1,4,sr) - hom(k-1,1,4,sr) ) * ddzu(k) |
---|
1221 | ENDDO |
---|
1222 | dptdz_threshold = 0.2 / 100.0 |
---|
1223 | |
---|
1224 | IF ( ocean ) THEN |
---|
1225 | DO k = nzt+1, nzb+5, -1 |
---|
1226 | IF ( dptdz(k) > dptdz_threshold .AND. & |
---|
1227 | dptdz(k) > dptdz(k-1) .AND. dptdz(k) > dptdz(k-2) .AND. & |
---|
1228 | dptdz(k) > dptdz(k-3) .AND. dptdz(k) > dptdz(k-4) ) THEN |
---|
1229 | z_i(2) = zw(k-1) |
---|
1230 | EXIT |
---|
1231 | ENDIF |
---|
1232 | ENDDO |
---|
1233 | ELSE |
---|
1234 | DO k = nzb+1, nzt-3 |
---|
1235 | IF ( dptdz(k) > dptdz_threshold .AND. & |
---|
1236 | dptdz(k) > dptdz(k+1) .AND. dptdz(k) > dptdz(k+2) .AND. & |
---|
1237 | dptdz(k) > dptdz(k+3) .AND. dptdz(k) > dptdz(k+4) ) THEN |
---|
1238 | z_i(2) = zw(k-1) |
---|
1239 | EXIT |
---|
1240 | ENDIF |
---|
1241 | ENDDO |
---|
1242 | ENDIF |
---|
1243 | |
---|
1244 | hom(nzb+6,1,pr_palm,sr) = z_i(1) |
---|
1245 | hom(nzb+7,1,pr_palm,sr) = z_i(2) |
---|
1246 | |
---|
1247 | ! |
---|
1248 | !-- Computation of both the characteristic vertical velocity and |
---|
1249 | !-- the characteristic convective boundary layer temperature. |
---|
1250 | !-- The horizontal average at nzb+1 is input for the average temperature. |
---|
1251 | IF ( hom(nzb,1,18,sr) > 0.0 .AND. abs(hom(nzb,1,18,sr)) > 1.0E-8 & |
---|
1252 | .AND. z_i(1) /= 0.0 ) THEN |
---|
1253 | hom(nzb+8,1,pr_palm,sr) = ( g / hom(nzb+1,1,4,sr) * & |
---|
1254 | hom(nzb,1,18,sr) * & |
---|
1255 | ABS( z_i(1) ) )**0.333333333 |
---|
1256 | !-- so far this only works if Prandtl layer is used |
---|
1257 | hom(nzb+11,1,pr_palm,sr) = hom(nzb,1,16,sr) / hom(nzb+8,1,pr_palm,sr) |
---|
1258 | ELSE |
---|
1259 | hom(nzb+8,1,pr_palm,sr) = 0.0 |
---|
1260 | hom(nzb+11,1,pr_palm,sr) = 0.0 |
---|
1261 | ENDIF |
---|
1262 | |
---|
1263 | ! |
---|
1264 | !-- Collect the time series quantities |
---|
1265 | ts_value(1,sr) = hom(nzb+4,1,pr_palm,sr) ! E |
---|
1266 | ts_value(2,sr) = hom(nzb+5,1,pr_palm,sr) ! E* |
---|
1267 | ts_value(3,sr) = dt_3d |
---|
1268 | ts_value(4,sr) = hom(nzb,1,pr_palm,sr) ! u* |
---|
1269 | ts_value(5,sr) = hom(nzb+3,1,pr_palm,sr) ! th* |
---|
1270 | ts_value(6,sr) = u_max |
---|
1271 | ts_value(7,sr) = v_max |
---|
1272 | ts_value(8,sr) = w_max |
---|
1273 | ts_value(9,sr) = hom(nzb+10,1,pr_palm,sr) ! new divergence |
---|
1274 | ts_value(10,sr) = hom(nzb+9,1,pr_palm,sr) ! old Divergence |
---|
1275 | ts_value(11,sr) = hom(nzb+6,1,pr_palm,sr) ! z_i(1) |
---|
1276 | ts_value(12,sr) = hom(nzb+7,1,pr_palm,sr) ! z_i(2) |
---|
1277 | ts_value(13,sr) = hom(nzb+8,1,pr_palm,sr) ! w* |
---|
1278 | ts_value(14,sr) = hom(nzb,1,16,sr) ! w'pt' at k=0 |
---|
1279 | ts_value(15,sr) = hom(nzb+1,1,16,sr) ! w'pt' at k=1 |
---|
1280 | ts_value(16,sr) = hom(nzb+1,1,18,sr) ! wpt at k=1 |
---|
1281 | ts_value(17,sr) = hom(nzb,1,4,sr) ! pt(0) |
---|
1282 | ts_value(18,sr) = hom(nzb+1,1,4,sr) ! pt(zp) |
---|
1283 | ts_value(19,sr) = hom(nzb+1,1,pr_palm,sr) ! u'w' at k=0 |
---|
1284 | ts_value(20,sr) = hom(nzb+2,1,pr_palm,sr) ! v'w' at k=0 |
---|
1285 | ts_value(21,sr) = hom(nzb,1,48,sr) ! w"q" at k=0 |
---|
1286 | |
---|
1287 | IF ( ts_value(5,sr) /= 0.0 ) THEN |
---|
1288 | ts_value(22,sr) = ts_value(4,sr)**2 / & |
---|
1289 | ( kappa * g * ts_value(5,sr) / ts_value(18,sr) ) ! L |
---|
1290 | ELSE |
---|
1291 | ts_value(22,sr) = 10000.0 |
---|
1292 | ENDIF |
---|
1293 | |
---|
1294 | ts_value(23,sr) = hom(nzb+12,1,pr_palm,sr) ! q* |
---|
1295 | ! |
---|
1296 | !-- Calculate additional statistics provided by the user interface |
---|
1297 | CALL user_statistics( 'time_series', sr, 0 ) |
---|
1298 | |
---|
1299 | ENDDO ! loop of the subregions |
---|
1300 | |
---|
1301 | ! |
---|
1302 | !-- If required, sum up horizontal averages for subsequent time averaging |
---|
1303 | IF ( do_sum ) THEN |
---|
1304 | IF ( average_count_pr == 0 ) hom_sum = 0.0 |
---|
1305 | hom_sum = hom_sum + hom(:,1,:,:) |
---|
1306 | average_count_pr = average_count_pr + 1 |
---|
1307 | do_sum = .FALSE. |
---|
1308 | ENDIF |
---|
1309 | |
---|
1310 | ! |
---|
1311 | !-- Set flag for other UPs (e.g. output routines, but also buoyancy). |
---|
1312 | !-- This flag is reset after each time step in time_integration. |
---|
1313 | flow_statistics_called = .TRUE. |
---|
1314 | |
---|
1315 | CALL cpu_log( log_point(10), 'flow_statistics', 'stop' ) |
---|
1316 | |
---|
1317 | |
---|
1318 | END SUBROUTINE flow_statistics |
---|