The continuous spectrum of the Orr-Sommerfeld equation. Part 1. The spectrum and the eigenfunctions
- 12 July 1978
- journal article
- research article
- Published by Cambridge University Press (CUP) in Journal of Fluid Mechanics
- Vol. 87 (1) , 33-54
- https://doi.org/10.1017/s0022112078002918
Abstract
It is shown that the Orr-Sommerfeld equation, which governs the stability of any mean shear flow in an unbounded domain which approaches a constant velocity in the far field, has a continuous spectrum. This result applies to both the temporal and the spatial stability problem. Formulae for the location of this continuum in the complex wave-speed plane are given. The temporal continuum eigenfunctions are calculated for two sample problems: the Blasius boundary layer and the two-dimensional laminar jet. The nature of the eigenfunctions, which are very different from the Tollmien-Schlichting waves, is discussed. Three mechanisms are proposed by which these continuum modes could cause transition in a shear flow while bypassing the usual linear Tollmien-Schlichting stage.Keywords
This publication has 28 references indexed in Scilit:
- Linear stability of Poiseuille flow in a circular pipeJournal of Fluid Mechanics, 1980
- Higher eigenstates in boundary-layer stability theoryJournal of Fluid Mechanics, 1976
- A numerical study of the temporal eigenvalue spectrum of the Blasius boundary layerJournal of Fluid Mechanics, 1976
- Accurate solution of the Orr–Sommerfeld stability equationJournal of Fluid Mechanics, 1971
- Spectrum of Eigenvalues of the Orr Sommerfeld Equation for Blasius FlowPhysics of Fluids, 1971
- The stability of steady and time-dependent plane Poiseuille flowJournal of Fluid Mechanics, 1968
- Stability of Pipe Poiseuille FlowPhysics of Fluids, 1968
- On the behaviour of small disturbances in plane Couette flowJournal of Fluid Mechanics, 1964
- Elementary Nuclear TheorySoil Science, 1948
- III. An experimental investigation of the circumstances which determine whether the motion of water shall be direct or sinuous, and of the law of resistance in parallel channelsProceedings of the Royal Society of London, 1883