Direct numerical simulation of the Ekman layer: a step in Reynolds number, and cautious support for a log law with a shifted origin
Direct numerical simulation of the Ekman layer: a step in Reynolds number, and cautious support for a log law with a shifted origin
Results at Ekman Reynolds numbers Re ranging from 1000 to 2828 expand the DNS contribution to the theory of wall-bounded turbulence. An established spectral method is used, with rules for domain size and grid resolution at each Reynolds number derived from the theory. The Re increase is made possible by better computers and by optimizing the grid in relation to the wall shear-stress direction. The boundary-layer thickness in wall units ?+ varies here by a factor of about 5.3, and reaches values near 5,000, or 22 times the minimum at which turbulence has been sustained. An equivalent channel Reynolds number, based on the pressure gradient in wall units, would reach about Re? = 1250. The principal goal of the analysis, the impartial identification of a log law, is summarized in the local ‘Karman Measure’ d(ln z+)/dU+. The outcome differs from that for Hoyas & Jim´enez and for Hu, Morfey & Sandham in channel-flow DNS at similar Reynolds numbers, for reasons unknown: here, the law of the wall is gradually established up to a z+ around 400, with little statistical scatter. To leading order, it is consistent with the experiments of ¨Osterlund et al. in boundary layers. With the traditional expression, a logarithmic law is not present, in that the Karman Measure drifts from about 0.41 at z+ ? 70 to the 0.37-0.38 range for z+ ? 500, with Re = 2828. However, if a virtual origin is introduced with a shift of a+ = 7.5 wall units, the data support a long logarithmic layer with ? = 0.38 a good fit to d(ln[z++a+])/dU+. A determination of the Karman constant from the variation of the skin-friction coefficients with Reynolds numbers also yields values near 0.38. The uncertainty is about ±0.01. These values are close to the boundary-layer experiments, but well below the accepted range of [0.40,0.41] and the experimental pipe-flow results near 0.42. The virtual-origin concept is also controversial, although non-essential at transportation or atmospheric Reynolds numbers. Yet, this series may reflect some success in verifying the law of the wall and investigating the logarithmic law by DNS, redundantly and with tools more impartial than the visual fit of a straight line to a velocity profile.
three-dimensional turbulent boundary layers, near-wall similarity, direct numerical simulation
Spalart, Philippe R.
8b92da5d-561c-4c7d-be1f-97f27de7c2a3
Coleman, Gary N.
ea3639b9-c533-40d7-9edc-3c61246b06e0
Johnstone, Roderick
8ac02aa2-776b-4f80-b44d-1a5cf8682f21
31 October 2008
Spalart, Philippe R.
8b92da5d-561c-4c7d-be1f-97f27de7c2a3
Coleman, Gary N.
ea3639b9-c533-40d7-9edc-3c61246b06e0
Johnstone, Roderick
8ac02aa2-776b-4f80-b44d-1a5cf8682f21
Spalart, Philippe R., Coleman, Gary N. and Johnstone, Roderick
(2008)
Direct numerical simulation of the Ekman layer: a step in Reynolds number, and cautious support for a log law with a shifted origin.
Physics of Fluids, 20 (10).
(doi:10.1063/1.3005858).
Abstract
Results at Ekman Reynolds numbers Re ranging from 1000 to 2828 expand the DNS contribution to the theory of wall-bounded turbulence. An established spectral method is used, with rules for domain size and grid resolution at each Reynolds number derived from the theory. The Re increase is made possible by better computers and by optimizing the grid in relation to the wall shear-stress direction. The boundary-layer thickness in wall units ?+ varies here by a factor of about 5.3, and reaches values near 5,000, or 22 times the minimum at which turbulence has been sustained. An equivalent channel Reynolds number, based on the pressure gradient in wall units, would reach about Re? = 1250. The principal goal of the analysis, the impartial identification of a log law, is summarized in the local ‘Karman Measure’ d(ln z+)/dU+. The outcome differs from that for Hoyas & Jim´enez and for Hu, Morfey & Sandham in channel-flow DNS at similar Reynolds numbers, for reasons unknown: here, the law of the wall is gradually established up to a z+ around 400, with little statistical scatter. To leading order, it is consistent with the experiments of ¨Osterlund et al. in boundary layers. With the traditional expression, a logarithmic law is not present, in that the Karman Measure drifts from about 0.41 at z+ ? 70 to the 0.37-0.38 range for z+ ? 500, with Re = 2828. However, if a virtual origin is introduced with a shift of a+ = 7.5 wall units, the data support a long logarithmic layer with ? = 0.38 a good fit to d(ln[z++a+])/dU+. A determination of the Karman constant from the variation of the skin-friction coefficients with Reynolds numbers also yields values near 0.38. The uncertainty is about ±0.01. These values are close to the boundary-layer experiments, but well below the accepted range of [0.40,0.41] and the experimental pipe-flow results near 0.42. The virtual-origin concept is also controversial, although non-essential at transportation or atmospheric Reynolds numbers. Yet, this series may reflect some success in verifying the law of the wall and investigating the logarithmic law by DNS, redundantly and with tools more impartial than the visual fit of a straight line to a velocity profile.
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Submitted date: 17 December 2007
Published date: 31 October 2008
Keywords:
three-dimensional turbulent boundary layers, near-wall similarity, direct numerical simulation
Organisations:
Aerodynamics & Flight Mechanics
Identifiers
Local EPrints ID: 63836
URI: http://eprints.soton.ac.uk/id/eprint/63836
ISSN: 1070-6631
PURE UUID: 7dfc494b-41e2-4633-bbb3-8db389c5a42e
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Date deposited: 05 Jan 2009
Last modified: 15 Mar 2024 11:43
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Author:
Philippe R. Spalart
Author:
Gary N. Coleman
Author:
Roderick Johnstone
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