Instabilities of the Ginzburg-Landau equation: periodic solutions
Authors:
Paul K. Newton and Lawrence Sirovich
Journal:
Quart. Appl. Math. 44 (1986), 49-58
MSC:
Primary 35Q20; Secondary 58F21
DOI:
https://doi.org/10.1090/qam/840442
MathSciNet review:
840442
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Abstract: The evolution of spatially periodic unstable solutions to the Ginzburg-Landau equation is considered. These solutions are shown to remain pointwise bounded (Lagrange stable). The first step in the route to chaos is limit cycle behavior. This is treated by perturbation theory and shown to result in a factorable form. Agreement between the perturbation result and an exact numerical integration is shown to be excellent.
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A. C. Newell and J. A. Whitehead, Finite bandwidth, finite amplitude convection, J. Fluid Mech. 38, 279 (1969)
K. Stewartson and J. T. Stuart, A non-linear instability theory for a wave system in plane Poiseuille flow, J. Fluid Mech. 48, 529 (1971)
R. C. DiPrima, W. Eckhaus, and L. A. Segel, Non-linear wave-number interaction in near-critical two dimensional flows, J. Fluid Mech. 49, 705 (1971)
D. J. Benney and G. J. Roskes, Wave instabilities, Stud. Appl. Math. 48, 377 (1969)
A. Davey and K. Stewartson, On three-dimensional packets of surface waves, Proc. Roy. Soc. London A338, 101 (1974)
T. B. Benjamin and J. E. Feir, The disintegration of wave trains on deep water, J. Fluid Mech. 27, 417 (1967)
H. Hasimoto and H. Ono, Nonlinear modulation of gravity waves, J. Phys. Soc. Japan 33, 805 (1972)
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A. Thyagaraja, in Nonlinear waves, ed. L. Debnath, Chapter 17: “Recurrence Phenomena and the Number of Effective Degrees of Freedom in Nonlinear Wave Motions,” Cambridge, 1983
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© Copyright 1986
American Mathematical Society