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A critical-layer analysis of the resonant triad in boundary-layer transition: nonlinear interactions

Published online by Cambridge University Press:  26 April 2006

Reda R. Mankbadi
Affiliation:
NASA Lewis Research Center, Cleveland, OH 44135, USA
Xuesong Wu
Affiliation:
Department of Mathematics, Imperial College, 180 Queens Gate, London SW7 2BZ, UK
Sang Soo Lee
Affiliation:
Sverdrup Technology, Inc., Lewis Research Center Group, Cleveland, OH 44135, USA

Abstract

A systematic theory is developed to study the nonlinear spatial evolution of the resonant triad in Blasius boundary layers. This triad consists of a plane wave at the fundamental frequency and a pair of symmetrical, oblique waves at the subharmonic frequency. A low-frequency asymptotic scaling leads to a distinct critical layer wherein nonlinearity first becomes important, and the critical layer's nonlinear, viscous dynamics determine the development of the triad.

The plane wave initially causes double-exponential growth of the oblique waves. The plane wave, however, continues to follow the linear theory, even when the oblique waves’ amplitude attains the same order of magnitude as that of the plane wave. However, when the amplitude of the oblique waves exceeds that of the plane wave by a certain level, a nonlinear stage comes into effect in which the self-interaction of the oblique waves becomes important. The self-interaction causes rapid growth of the phase of the oblique waves, which causes a change of the sign of the parametric-resonance term in the oblique-waves amplitude equation. Ultimately this effect causes the growth rate of the oblique waves to oscillate around their linear growth rate. Since the latter is usually small in the nonlinear regime, the net outcome is that the self-interaction of oblique waves causes the parametric resonance stage to be followed by an ‘oscillatory’ saturation stage.

Type
Research Article
Copyright
© 1993 Cambridge University Press

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References

Benney, D. J. & Bergeron, R. F. 1969 A new class of nonlinear waves in parallel flows. Stud. Appl. Maths 48, 181204.Google Scholar
Bodonyi, R. J. & Smith, F. T. 1981 The upper branch stability of the Blasius boundary layer, including non-parallel flow effects. Proc. R. Soc. Lond. A 375, 6592.Google Scholar
Brown, P., Brown, S. N. & Smith, F. T. 1993 (In preparation.)
Corke, T. C. & Mangano, R. A. 1989 Resonant growth of three-dimensional modes in transitioning Blasius boundary layers. J. Fluid Mech. 209, 93150.Google Scholar
Craik, A. D. D. 1971 Non-linear resonant instability in boundary layers. J. Fluid Mech. 50, 393413.Google Scholar
Craik, A. D. D. 1985 Wave Interactions and Fluid Flow. Cambridge University Press.
Drazin, P. G. & Reid, W. H. 1981 Hydrodynamic Stability. Cambridge University Press.
Goldstein, M. E. & Choi, W. W. 1989 Nonlinear evolution of interacting oblique waves on two-dimensional shear layers. J. Fluid Mech. 207, 97120.(See also Corrigendum, J. Fluid Mech. 216, 659–663.)Google Scholar
Goldstein, M. E. & Durbin, P. A. 1986 Nonlinear critical layers eliminate the upper branch of spatially growing Tollmien-Schlichting waves. Phys. Fluids 29, 23442345.Google Scholar
Goldstein, M. E., Durbin, P. A. & Leib, S. J. 1987 Roll-up of vorticity in adverse-pressure gradient boundary layers. J. Fluid Mech. 183, 325342.Google Scholar
Goldstein, M. E. & Leib, S. J. 1988 Nonlinear roll-up of externally excited free shear layers. J. Fluid Mech. 191, 481515.Google Scholar
Goldstein, M. E. & Lee, S. S. 1992 Fully coupled resonant-triad interaction in an adverse-pressure-gradient boundary layer. J. Fluid Mech. 245, 523551.Google Scholar
Hall, P. & Smith, F. T. 1991 On strongly nonlinear vortex/wave interactions in boundary-layer transition. J. Fluid Mech. 227, 641.Google Scholar
Herbert, T. 1983 Subharmonic three-dimensional disturbances in unstable plane shear flows. AIAA Paper 83–1759.
Herbert, T. 1988 Secondary instability of boundary layers. Ann. Rev. Fluid Mech. 20, 487526.Google Scholar
Kachanov, Yu. S. 1984 Development of spatial wave packets in boundary layer. In Laminar—Turbulent Transition (ed. V. V. Kozlov), Proc. Second IUTAM Symp. Novosibirsk, pp. 115123. Springer.
Kachanov, Yu. S., Kozlov, V. V. & Levchenko, V. Ya. 1978 Nonlinear development of a wave in a boundary layer. Fluid Dyn. 12, 383390.Google Scholar
Kachanov, Yu. S. & Levchenko, V. Ya. 1984 The resonant interaction of disturbances at laminar-turbulent transition in a boundary layer. J. Fluid Mech. 138, 209247.Google Scholar
Klebanoff, P. S., Tidstrom, K. D. & Sargent, L. M. 1962 The three-dimensional nature of boundary-layer instability. J. Fluid Mech. 12, 134.Google Scholar
Kleiser, L. & Zang, T. A. 1991 Numerical simulation of transition in wall-bounded shear flows. Ann. Rev. Fluid Mech. 23, 495537.Google Scholar
Knapp, C. F. & Roache, P. J. 1968 A combined visual and hot wire anemometer investigation of boundary-layer transition. AIAA J. 6, 2936.Google Scholar
Lin, C. C. 1955 The Theory of Hydrodynamic Stability. Cambridge University Press.
Lin, C. C. 1957 On the instability of laminar flow and transition to turbulence. IUTAM Symposium Freiburg/BR, p. 144.
Mankbadi, R. R. 1990 Critical-layer nonlinearity in the resonance growth of three-dimensional waves in boundary layer. NASA TM-103639.
Mankbadi, R. R. 1991a Detuned triad interaction in boundary-layer instability. Bull. Am. Phys. Soc. JD6, 36, 2713.Google Scholar
Mankbadi, R. R. 1991b Subharmonic route to boundary-layer transition: critical-layer non-linearity. In Forum on Turbulent Flows (ed. M. J. Morris et al.), ASME FED, vol. 112, pp. 7581.
Mankbadi, R. R. 1993 The nonlinear interaction of frequency-detuned modes in boundary-layer transition. AIAA-93-0341.
Maslowe, S. A. 1986 Critical layers in shear flows. Ann. Rev. Fluid Mech. 18, 405432.Google Scholar
Raetz, G. S. 1959 A new theory of the cause of transition in fluid flows. Northrop Corp. Rep. NOR- 59–383, Hawthorne, California.
Reid, W. H. 1965 The stability of parallel flows. In Basic Developments in Fluid Dynamics (ed. M. Holt), pp. 249308. Academic.
Saric, W. S., Kozlov, V. V. & Levchenko, V. Ya. 1984 Forced and unforced subharmonic resonance in boundary layer transition. AIAA Paper 84–0007.
Smith, F. T. & Stewart, P. A. 1987 The resonant-triad nonlinear interaction in boundary-layer transition. J. Fluid Mech. 179, 227252.Google Scholar
Usher, J. R. & Craik, A. D. D. 1975 Nonlinear wave interactions in shear flows. Part 2. Third-order theory. J. Fluid Mech. 70, 437461.Google Scholar
Wu, X. 1992 The nonlinear evolution of high-frequency resonant-triad waves in an oscillatory Stokes layer at high Reynolds number. J. Fluid Mech. 245, 553597.Google Scholar
Wu, X. 1993 On the critical-layer and diffusion-layer nonlinearity in the three-dimensional stability of boundary layer transition. Proc. R. Soc. Lond. (to appear.)Google Scholar
Wu, X., Lee, S. S. & Cowley, S. J. 1993 On the weakly nonlinear three-dimensional instability of shear layers to pairs of oblique waves: the Stokes layer as a paradigm. J. Fluid Mech. 253, 681721.Google Scholar