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The rough favourabl...
The rough favourable pressure gradient turbulent boundary layer
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- Cal, Raúl Bayoán (författare)
- Portland State University
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- Brzek, Brian (författare)
- Rensselaer Polytechnic Institute
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- Johansson, Gunnar, 1945 (författare)
- Chalmers tekniska högskola,Chalmers University of Technology
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- Castillo, Luciano (författare)
- Rensselaer Polytechnic Institute
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(creator_code:org_t)
- 2009
- 2009
- Engelska.
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Ingår i: Journal of Fluid Mechanics. - 0022-1120 .- 1469-7645. ; 641, s. 129-155
- Relaterad länk:
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http://publications.... (primary) (free)
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https://research.cha...
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https://doi.org/10.1...
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Abstract
Ämnesord
Stäng
- Laser Doppler anemometry measurements of the mean velocity and Reynolds stresses are carried Out for a rough-surface favourable pressure gradient turbulent boundary layer. The experimental data is compared with smooth favourable pressure gradient and rough zero-pressure gradient data. The velocity and Reynolds stress profiles are normalized using various scalings Such as the friction velocity and free stream velocity. In the velocity profiles, the effects of roughness are removed when using the friction velocity. The effects of pressure gradient are not absorbed. When using the free stream velocity, the scaling is more effective absorbing the pressure gradient effects. However, the effects of roughness are almost removed, while the effects of pressure gradient are still observed on the outer flow, when the mean deficit velocity profiles are normalized by the U(infinity)delta(*)/delta scaling. Furthermore, when scaled with U(infinity)(2), the component of the Reynolds stress augments due to the rough Surface despite the imposed favourable pressure gradient; when using the friction velocity scaling it u(*)(2), it is dampened. It becomes 'flatter' in the inner region mainly due to the rough Surface, which destroys the coherent structures of the flow and promotes isotropy. Similarly, the pressure gradient imposed on the flow decreases the magnitude of the Reynolds stress profiles especially on the and - components for the u(*)(2) or U(infinity)(2) scaling. These effects are reflected in the boundary layer parameter delta(*)/delta, which increase due to roughness, but decrease due to the favourable pressure gradient. Additionally, the pressure parameter Lambda found not to be in equilibrium, describes the development of the turbulent boundary layer, with no influence of the roughness linked to this parameter. These measurements are the first with an extensive number of downstream locations (11). This makes it possible to compute the required x-dependence for the production term and the wall shear stress from the full integrated boundary layer equation. The finding indicates that the skin friction coefficient depends oil the favourable pressure gradient condition and surface roughness.
Ämnesord
- TEKNIK OCH TEKNOLOGIER -- Maskinteknik -- Strömningsmekanik och akustik (hsv//swe)
- ENGINEERING AND TECHNOLOGY -- Mechanical Engineering -- Fluid Mechanics and Acoustics (hsv//eng)
Nyckelord
- favourable pressure gradient
- boundary layers
- Roughness
Publikations- och innehållstyp
- art (ämneskategori)
- ref (ämneskategori)
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