The response of a turbulent boundary layer to a step change in surface roughness. Part 2. Rough-to-smooth

Author:

Antonia R. A.,Luxton R. E.

Abstract

An experimental study of the structure of the internal layer which grows down-stream from a rough-to-smooth surface change shows it to be essentially different from that studied by Antonia & Luxton (1971 b) for the case of a smooth-to-rough perturbation. The rate of growth of the internal layer is less than that for the smooth-to-rough step and it appears that the more intense initial rough-wall flow dictates the rate of diffusion of the disturbance for a considerable distance. Inside the internal layer the mixing lengthIis increased relative to the equilibrium distributionI=KY.A turbulent energy budget shows that the advection is comparable with the production or dissipation, whilst there seems to be some diffusion of energy into the internal-layer region close to the wall. The boundary layer, as a whole, recovers much more slowly following a rough-to-smooth change than following a smooth-to-rough change, and at the last measuring station (16 boundary-layer thicknesses from the start of the smooth surface) the distributions of mean velocity and Reynolds shear stress are far from self-preserving.

Publisher

Cambridge University Press (CUP)

Subject

Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics

Reference22 articles.

1. Luxton, R. E. , Swenson, G. G. BE Chadwick, B. S. 1967 The Collection and Processing of Field Data (ed. E. F. Bradley & O. T. Denmead ),p.497.Interscience.

2. Badrinarayanan, M. A. & RAO, K. N. 1968 Aero. Soc. of India, Joint Technical Sessions, Bangalore.

3. Antonia, R. A. & Luxton, R. E. 1971 J. Fluid Mech. 48,721.

4. Makita, H. 1968 M. Eng. thesis,University of Tokyo.

5. Tani, I. 1968 Proc. Computation of Turbulent Boundary Layers, Afosr-IFP-Stanford University .

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