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