Interaction of phase-locked modes: a new mechanism for the rapid growth of three-dimensional disturbances

Author:

Wu Xuesong,Stewart Philip A.

Abstract

In this paper, we have identified a new mechanism which can promote rapid growth of three-dimensional disturbances. The mechanism involves the interaction between a planar mode and an oblique mode, or a pair of oblique modes, which are phase-locked in the sense that they have the same phase speed. This allows a powerful nonlinear interaction to take place within the common critical layer(s). The disturbance is not required to form a subharmonic resonant triad, and hence the mechanism operates under much less restrictive conditions than does subharmonic resonance (although it is somewhat less powerful). We show that the quadratic interaction between the planar mode and the oblique modes drives an exceptionally large forced mode with the difference frequency, which in turn interacts with the planar mode to contribute the dominant nonlinear effect. This interaction can cause the oblique modes to grow super-exponentially provided that their magnitude is sufficiently small. As a result of the super-exponential growth, the oblique mode may soon become strong enough to produce a feedback effect on the planar mode, so that the interactions eventually become fully coupled. This subsequent stage takes slightly different forms depending on whether a single or a pair of oblique modes is present. Both cases are investigated. Particular attention is paid to symmetric plane shear layers, e.g. a planar wake or jet, for which subharmonic resonance of sinuous modes is inactive.

Publisher

Cambridge University Press (CUP)

Subject

Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics

Reference38 articles.

1. Wu, X. 1993b On critical-layer and diffusion-layer nonlinearity in the three-dimensional stage of boundary-layer transition.Proc. R. Soc. Lond. A443,95–106.

2. Wu, X. 1995 Viscous effects on fully coupled resonant triad interactions: an analytical approach.J. Fluid Mech. 292,377–407.

3. Williamson, C. H. K. & Prasad, A. 1993b Acoustic forcing of oblique wave resonance in the far wake.J. Fluid Mech. 256,315–341.

4. Wundrow, D. W. , Hultgren, L. S. & Goldstein, M. E. 1994 Interaction of oblique stability waves with a nonlinear planar wave.J. Fluid Mech. 262,343–372.

5. Williamson, C. H. K. & Prasad, A. 1993a A new mechanism for oblique wave resonance in the ‘natural’ far wake.J. Fluid Mech. 256,269–313.

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