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