LES and RANS for turbulent flow over arrays of wall-mounted obstacles

Large-eddy simulation (LES) has been applied to calculate the turbulent flow over staggered wall-mounted cubes and staggered random arrays of obstacles with area density 25%, at Reynolds numbers between 5 × 10^3 and 5 10^6, based on the free stream velocity and the obstacle height. Re = 5 × 10^3 dat...

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Bibliographic Details
Main Authors: Xie, Zheng-Tong (Author), Castro, Ian P. (Author)
Format: Article
Language:English
Published: 2006.
Subjects:
Online Access:Get fulltext
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100 1 0 |a Xie, Zheng-Tong  |e author 
700 1 0 |a Castro, Ian P.  |e author 
245 0 0 |a LES and RANS for turbulent flow over arrays of wall-mounted obstacles 
260 |c 2006. 
856 |z Get fulltext  |u https://eprints.soton.ac.uk/30157/1/LES_and_RANS_for_turbulent_flow_ovr_arrays_of_wall_mounted_obstacles.pdf 
520 |a Large-eddy simulation (LES) has been applied to calculate the turbulent flow over staggered wall-mounted cubes and staggered random arrays of obstacles with area density 25%, at Reynolds numbers between 5 × 10^3 and 5 10^6, based on the free stream velocity and the obstacle height. Re = 5 × 10^3 data were intensively validated against direct numerical simulation (DNS) results at the same Re and experimental data obtained in a boundary layer developing over an identical roughness and at a rather higher Re. The results collectively confirm that Reynolds number dependency is very weak, principally because the surface drag is predominantly form drag and the turbulence production process is at scales comparable to the roughness element sizes. LES is thus able to simulate turbulent flow over the urban-like obstacles at high Re with grids that would be far too coarse for adequate computation of corresponding smooth-wall flows. Comparison between LES and steady Reynolds-averaged Navier-Stokes (RANS) results are included, emphasising that the latter are inadequate, especially within the canopy region. 
655 7 |a Article