Hydrodynamic Stability Without Eigenvalues

Fluid flows that are smooth at low speeds become unstable and then turbulent at higher speeds. This phenomenon has traditionally been investigated by linearizing the equations of flow and testing for unstable eigenvalues of the linearized problem, but the results of such investigations agree poorly in many cases with experiments. Nevertheless, linear effects play a central role in hydrodynamic instability. A reconciliation of these findings with the traditional analysis is presented based on the "pseudospectra" of the linearized problem, which imply that small perturbations to the smooth flow may be amplified by factors on the order of 105 by a linear mechanism even though all the eigenmodes decay monotonically. The methods suggested here apply also to other problems in the mathematical sciences that involve nonorthogonal eigenfunctions.

[1]  W. Thomson,et al.  XXI. Stability of fluid motion (continued from the May and June numbers).—Rectilineal motion of viscous fluid between two parallel planes , 1887 .

[2]  H. Squire On the Stability for Three-Dimensional Disturbances of Viscous Fluid Flow between Parallel Walls , 1933 .

[3]  HYDRODYNAMIC STABILITY AND THE INVISCID LIMIT , 1961 .

[4]  H. Kreiss Über Die Stabilitätsdefinition Für Differenzengleichungen Die Partielle Differentialgleichungen Approximieren , 1962 .

[5]  [On the sternal reflex in severe pathological conditions of the cerebral hemispheres with signs of somnolence and coma]. , 1962, Neurologia, neurochirurgia i psychiatria polska.

[6]  Tosio Kato Perturbation theory for linear operators , 1966 .

[7]  M. R. Head,et al.  Some observations on skin friction and velocity profiles in fully developed pipe and channel flows , 1969, Journal of Fluid Mechanics.

[8]  General Solution for Perturbed Plane Couette Flow , 1971 .

[9]  S. Orszag Accurate solution of the Orr–Sommerfeld stability equation , 1971, Journal of Fluid Mechanics.

[10]  T. Ellingsen,et al.  Stability of linear flow , 1975 .

[11]  M. Landahl Wave Breakdown and Turbulence , 1975 .

[12]  H. J. Landau,et al.  Loss in unstable resonators , 1976 .

[13]  M. Landahl A note on an algebraic instability of inviscid parallel shear flows , 1980, Journal of Fluid Mechanics.

[14]  D. J. Benney,et al.  A New Mechanism For Linear and Nonlinear Hydrodynamic Instability , 1981 .

[15]  L. Gustavsson Energy growth of three-dimensional disturbances in plane Poiseuille flow , 1981, Journal of Fluid Mechanics.

[16]  R. Breidenthal,et al.  Structure in turbulent mixing layers and wakes using a chemical reaction , 1981, Journal of Fluid Mechanics.

[17]  Lennart S. Hultgren,et al.  Algebraic growth of disturbances in a laminar boundary layer , 1981 .

[18]  Sheila E. Widnall,et al.  A flow-visualization study of transition in plane Poiseuille flow , 1982, Journal of Fluid Mechanics.

[19]  Anthony T. Patera,et al.  Secondary instability of wall-bounded shear flows , 1983, Journal of Fluid Mechanics.

[20]  Luis P. Bernal,et al.  Streamwise vortex structure in plane mixing layers , 1986, Journal of Fluid Mechanics.

[21]  W. O. Criminale,et al.  Evolution of wavelike disturbances in shear flows : a class of exact solutions of the Navier-Stokes equations , 1986, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

[22]  J. Lasheras,et al.  Three-dimensional instability of a plane free shear layer: an experimental study of the formation and evolution of streamwise vortices , 1988, Journal of Fluid Mechanics.

[23]  Steven A. Orszag,et al.  Instability mechanisms in shear-flow transition , 1988 .

[24]  Brian F. Farrell,et al.  Optimal excitation of perturbations in viscous shear flow , 1988 .

[25]  Brian F. Farrell,et al.  Optimal Excitation of Baroclinic Waves , 1989 .

[26]  M. Nishioka,et al.  Origin of the peak-valley wave structure leading to wall turbulence , 1989, Journal of Fluid Mechanics.

[27]  W. Kerner Large-scale complex eigenvalue problems , 1989 .

[28]  Kenneth S. Breuer,et al.  The evolution of a localized disturbance in a laminar boundary layer. Part 1. Weak disturbances , 1990, Journal of Fluid Mechanics.

[29]  P. Moin,et al.  Structure of turbulence at high shear rate , 1990, Journal of Fluid Mechanics.

[30]  A. Johansson,et al.  Direct simulation of turbulent spots in plane Couette flow , 1991, Journal of Fluid Mechanics.

[31]  B. G. B. Klingmann On transition due to three-dimensional disturbances in plane Poiseuille flow , 1992, Journal of Fluid Mechanics.

[32]  Kathryn M. Butler,et al.  Three‐dimensional optimal perturbations in viscous shear flow , 1992 .

[33]  Nils Tillmark,et al.  Experiments on transition in plane Couette flow , 1992, Journal of Fluid Mechanics.

[34]  Lloyd N. Trefethen,et al.  How Fast are Nonsymmetric Matrix Iterations? , 1992, SIAM J. Matrix Anal. Appl..

[35]  L. Trefethen,et al.  Stability of the method of lines , 1992, Spectra and Pseudospectra.

[36]  Lloyd N. Trefethen,et al.  A Hybrid GMRES Algorithm for Nonsymmetric Linear Systems , 1992, SIAM J. Matrix Anal. Appl..

[37]  D. Henningson,et al.  A mechanism for bypass transition from localized disturbances in wall-bounded shear flows , 1993, Journal of Fluid Mechanics.

[38]  Stiffness of ODEs , 1993 .

[39]  S. C. Reddy,et al.  Energy growth in viscous channel flows , 1993, Journal of Fluid Mechanics.

[40]  Dan S. Henningson,et al.  Pseudospectra of the Orr-Sommerfeld Operator , 1993, SIAM J. Appl. Math..

[41]  P. Ioannou,et al.  Optimal excitation of three‐dimensional perturbations in viscous constant shear flow , 1993 .

[42]  Kathryn M. Butler,et al.  Optimal perturbations and streak spacing in wall‐bounded turbulent shear flow , 1993 .