Abstract
The fluctuating velocity in the near-wall layer is shown to scale on the fluctuating wall shear stress such that it has the form u '/u 'τ = f (u 'τ y/v) where u 'τ is a velocity based on the r.m.s of the wall shear stress fluctuation and u′ is the r.m.s velocity. The observed dependency on u 'τ y/v which is independent of mean velocity and mean wall shear stress, exhibits a logarithmic region which extends to about 0.1 of the bubble height, and the viscous sublayer is quadratic in behaviour.
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References
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© 2004 Springer Science+Business Media Dordrecht
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Hancock, P.E. (2004). Scaling of the Near-Wall Layer Beneath Reattaching Separated Flow. In: Smits, A.J. (eds) IUTAM Symposium on Reynolds Number Scaling in Turbulent Flow. Fluid Mechanics and its Applications, vol 74. Springer, Dordrecht. https://doi.org/10.1007/978-94-007-0997-3_26
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DOI: https://doi.org/10.1007/978-94-007-0997-3_26
Publisher Name: Springer, Dordrecht
Print ISBN: 978-94-010-3763-1
Online ISBN: 978-94-007-0997-3
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