Hostname: page-component-8448b6f56d-42gr6 Total loading time: 0 Render date: 2024-04-18T18:49:31.826Z Has data issue: false hasContentIssue false

Global stability of base and mean flows: a general approach and its applications to cylinder and open cavity flows

Published online by Cambridge University Press:  23 November 2007

DENIS SIPP
Affiliation:
ONERA, 8 rue des Vertugadins, 92190 Meudon, France
ANTON LEBEDEV
Affiliation:
ONERA, 8 rue des Vertugadins, 92190 Meudon, France

Abstract

This article deals with the first Hopf bifurcation of a cylinder flow, and more particularly with the properties of the unsteady periodic Kármán vortex street regime that sets in for supercritical Reynolds numbers Re > 46. Barkley (Europhys. Lett. vol.75, 2006, p. 750) has recently studied the linear properties of the associated mean flow, i.e. the flow which is obtained by a time average of this unsteady periodic flow. He observed, thanks to a global mode analysis, that the mean flow is marginally stable and that the eigenfrequencies associated with the global modes of the mean flow fit the Strouhal to Reynolds experimental function well in the range 46 < Re < 180. The aim of this article is to give a theoretical proof of this result near the bifurcation. For this, we do a global weakly nonlinear analysis valid in the vicinity of the critical Reynolds number Rec based on the small parameter ε = Rec−1Re−1 ≪ 1. We compute numerically the complex constants λ and μ′ which appear in the Stuart-Landau amplitude equation: dA/dt = ε λA − εμ′ A|A|2. Here A is the scalar complex amplitude of the critical global mode. By analysing carefully the nonlinear interactions yielding the term μ′, we show for the cylinder flow that the mean flow is approximately marginally stable and that the linear dynamics of the mean flow yields the frequency of the saturated Stuart-Landau limit cycle. We will finally show that these results are not general, by studying the case of the bifurcation of an open cavity flow. In particular, we show that the mean flow in this case remains strongly unstable and that the frequencies associated with the eigenmodes do not exactly match those of the nonlinear unsteady periodic cavity flow. It will be demonstrated that two precise conditions must hold for a linear stability analysis of a mean flow to be relevant and useful.

Type
Papers
Copyright
Copyright © Cambridge University Press 2007

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

REFERENCES

Barkley, D. 2006 Linear analysis of the cylinder wake mean flow. Europhys. Lett. 75, 750756.CrossRefGoogle Scholar
Chomaz, J.-M. 2005 Global instabilities in spatially developing flows: Non-normality and nonlinearity. Ann. Rev. Fluid Mech. 37, 357392.CrossRefGoogle Scholar
Davis, T. A. 2004 A column pre-ordering strategy for the unsymmetric-pattern multifrontal method. ACM Trans. Mathe. Softw. 30, 165195.CrossRefGoogle Scholar
Davis, T. A. & Duff, I. 1997 An unsymmetric-pattern multifrontal method for sparse lu factorization. SIAM J. Matrix Anal. Appl. 18, 140158.CrossRefGoogle Scholar
Ding, Y. & Kawahara, M. 1999 Three-dimensional linear stability analysis of incompressible viscous flows using finite element method. Int. J. Num. Meth. Fluids 31, 451479.3.0.CO;2-O>CrossRefGoogle Scholar
Dusek, J., Le Gal, P. & Fraunie, P. 1994 A numerical and theoretical study of the first Hopf bifurcation in a cylinder wake. J. Fluid Mech. 264, 5980.CrossRefGoogle Scholar
Giannetti, F. & Luchini, P. 2007 Structural sensibility of the cylinder wake's first instability. J. Fluid Mech. 581, 167197.CrossRefGoogle Scholar
Hammond, D. A. & Redekopp, L. G. 1997 Global dynamics of symmetric and asymmetric wakes. J. Fluid Mech. 331, 231260.CrossRefGoogle Scholar
Jackson, C. P. 1987 A finite-element study of the onset of vortex shedding in flow past variously shaped bodies. J. Fluid Mech. 182, 2345.CrossRefGoogle Scholar
Koch, W. 1985 Local instability characteristics and frequency determination of self-excited flows. J. Sound Vib. 99, 5383.CrossRefGoogle Scholar
Le Dizès, S., Huerre, P. & Chomaz, J.-M. 1993 Nonlinear stability analysis of slowly-varying medias: Limitations of the weakly nonlinear approach. In Proc. IUTAM Symposium on Bluff-body Wakes, Dynamics and Instabilities, pp. 147152. Springer.CrossRefGoogle Scholar
Monkewitz, P. A., Huerre, P. & Chomaz, J.-M. 1993 Global linear stability analysis of weakly non-parallel shear flows. J. Fluid Mech. 251, 120.CrossRefGoogle Scholar
Pier, B. 2002 On the frequency selection of finite-amplitude vortex shedding in the cylinder wake. J. Fluid Mech. 458, 407417.CrossRefGoogle Scholar
Pier, B. & Huerre, P. 2001 Nonlinear self-sustained structures and fronts in spatially developing wake flows. J. Fluid Mech. 435, 145174.CrossRefGoogle Scholar
Provansal, M., Mathis, C. & Boyer, L. 1987 Bénard–von Kármán instability: Transient and forced regimes. J. Fluid Mech. 182, 122.CrossRefGoogle Scholar
Wesfreid, J., Goujon-Durand, S. & Zielinska, B. J. A. 1996 Global mode behavior of the streamwise velocity in wakes. J. Phys. II Paris 6, 13431357.Google Scholar
Williamson, C. H. K. 1988 Defining a universal and continuous Strouhal–Reynolds number relationship for the laminar vortex shedding of a circular cylinder. Phys. Fluids 31, 27422744.CrossRefGoogle Scholar
Zebib, A. 1987 Stability of a viscous flow past a circular cylindar. J. Engng Math. 21, 155165.CrossRefGoogle Scholar
Zielinska, B., Goujon-Durand, S., Dusek, J. & Wesfreid, J. E. 1997 Strongly nonlinear effect in unstable wakes. Phys. Rev. Lett. 79, 38933896.CrossRefGoogle Scholar