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The continuous spectrum of the Orr-Sommerfeld equation. Part 2. Eigenfunction expansions

Published online by Cambridge University Press:  20 April 2006

Harold Salwen
Affiliation:
Department of Physics and Engineering Physics, Stevens Institute of Technology, Hoboken, N. J. 07030
Chester E. Grosch
Affiliation:
Department of Oceanography and Department of Mathematics, Old Dominion University, Norfolk, Va. 23508

Abstract

The expansion of an arbitrary two-dimensional solution of the linearized stream-function equation in terms of the discrete and continuum eigenfunctions of the Orr-Sommerfeld equation is discussed for flows in the half-space, y ε [0, ∞). A recent result of Salwen is used to derive a biorthogonality relation between the solution of the linearized equation for the stream function and the solutions of the adjoint problem.

For the case of temporal stability, the orthogonality relation obtained is equivalent to that of Schensted for bounded flows. This relationship is used to carry out the formal solution of the initial-value problem for temporal stability. It is found that the vorticity of the disturbance at t = 0 is the proper initial condition for the temporal stability problem. Finally, it is shown that the set consisting of the discrete eigen-modes and continuum eigenfunctions is complete.

For the spatial stability problem, it is shown that the continuous spectrum of the Orr-Sommerfeld equation contains four branches. The biorthogonality relation is used to derive the formal solution to the boundary-value problem of spatial stability. It is shown that the boundary-value problem of spatial stability requires the stream function and its first three partial derivatives with respect to x to be specified at x = 0 for all t. To be applicable to practical problems, this solution will require modification to eliminate disturbances originating at x = ∞ and travelling upstream to x = 0.

For the special case of a constant base flow, the method is used to calculate the evolution in time of a particular initial disturbance.

Type
Research Article
Copyright
© 1981 Cambridge University Press

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References

Berger, S. A. & Aroesty, J. 1977 ‘e9’: Stability theory and boundary layer transition. R-1898-ARRA. Rand Corporation.
Coddington, E. A. & Levinson, N. 1955 Theory of Ordinary Differential Equations. McGraw-Hill.
Corner, D., Houston, D. J. R. & Ross, M. A. S. 1976 Higher eigenstates in boundary-layer stability theory. J. Fluid Mech. 77, 81.Google Scholar
DiPrima, R. C. & Habetler, G. J. 1969 A completeness theorem for nonself-adjoint eigenvalue problems in hydrodynamic stability. Arch. Rat. Mech. 34, 218.Google Scholar
Friedman, A. 1969 Partial Differential Equations. Holt, Rinehart and Winston.
Grosch, C. E. & Salwen, H. 1975 The continuous spectrum of the Orr-Sommerfeld equation. Bull. Am. Phys. Soc. 20, 1423.Google Scholar
Grosch, C. E. & Salwen, H. 1978a The continuous spectrum of the Orr—Sommerfeld equation. 1. The spectrum and the eigenfunctions. J. Fluid Mech. 87, 33.Google Scholar
Grosch, C. E. & Salwen, H. 1978b The spatial continuum revisited. Bull. Am. Phys. Soc. 23, 525.Google Scholar
Gustavsson, L. H. 1979 On the initial value problem for boundary layer flows. Phys. Fluids 22, 1602.Google Scholar
Haupt, O. 1912 Über die Entwicklung einer willkurliehen Funktion nach den Eigenfunktionen des Turbulenzproblems. Sber. Bayer. Akad. Wiss. 2, 289.Google Scholar
Jordinson, R. 1971 Spectrum of eigenvalues of the Orr—Sommerfeld equation for Blasius flow, Phys. Fluids 14, 177.Google Scholar
Lighthill, M. J. 1960 Fourier Analysis and Generalized Functions. Cambridge University Press.
Mack, L. M. 1976 A numerical study of the temporal eigenvalue spectrum of the Blasius boundary layer. J. Fluid Mech. 73, 497.Google Scholar
Murdock, J. W. & Stewartson, K. 1977 Spectrum of the Orr—Sommerfeld equation. Phys. Fluids 20, 1404.Google Scholar
Obremski, H. J., Morkovin, M. J. & Landahl, M. 1969 A portfolio of stability characteristics of incompressible boundary layers. AGAR Dograph no. 134.Google Scholar
Reid, W. H. 1965 The stability of parallel flows. In Basic Developments in Fluid Dynamics (ed. M. Holt). Academic.
Salwen, H. 1979 Expansions in spatial or temporal eigenmodes of the linearized Navier—Stokes equations. Bull. Am. Phys. Soc. 24, 74.Google Scholar
Schensted, I. V. 1960 Contributions to the theory of hydrodynamic stability. Ph.D. dissertation, University of Michigan.
Yudovich, V. I. 1965 Stability of steady flows of viscous incompressible fluids. Soviet Phys. Dokl. 10, 293.Google Scholar