Cumulative nonlinear distortion of an acoustic wave propagating through non-uniform flow

Author:

Kurosaka M.

Abstract

In this paper we examine how the unsteady flow field radiated from an oscillating body is altered from the result of acoustic theory as the direct consequence of disturbances propagating through the non-uniform flow produced by the presence of the body. Taking the specific example of an oscillating airfoil placed in supersonic flow and having the contour of a parabolic arc, we derive a closed-form representation for the unsteady flow field in terms of the confluent hypergeometric function. The analytical expression reveals explicitly that, though the body shape has a negligible effect in the near field, it inextricably affects the unsteady flow at a large distance, both in its amplitude and phase, and substantially modifies the results of acoustic theory. In addition, we display the relation of this solution to the ‘fundamental solution’ and the other salient physical features connected with disturbances propagating through non-uniform flow. The present results recover Whitham's rule in the limit of zero frequency of oscillation and also include, as another special case, the unsteady solution for a wedge obtained by Carrier and Van Dyke.

Publisher

Cambridge University Press (CUP)

Subject

Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics

Reference29 articles.

1. Van Dyke, M. 1975 Perturbation Methods in Fluid Mechanics , annotated ed.Parabolic Press.

2. Lin, C. C. 1954 J. Math. & Phys. 33,117.

3. Whitham, G. B. 1950 Proc. Roy. Soc. A 201,89.

4. Miles, J. W. 1959 The Potential Theory of Unsteady Supersonic Flow .Cambridge University Press.

5. Temple, G. & Jahn, H. A. 1945 Aero. Res. Counc. R. & M. no. 2140.

Cited by 2 articles. 订阅此论文施引文献 订阅此论文施引文献,注册后可以免费订阅5篇论文的施引文献,订阅后可以查看论文全部施引文献

1. Supersonic cooling by shock–vortex interaction;Journal of Fluid Mechanics;1996-02-10

2. The far field of an oscillating airfoil in supersonic flow;Journal of Fluid Mechanics;1987-10

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