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Mechanisms of excitation and amplitude limitation of self-oscillations and auto-waves. Classification of self-oscillatory systems

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Book cover Nonlinear Oscillations and Waves in Dynamical Systems

Part of the book series: Mathematics and Its Applications ((MAIA,volume 360))

Abstract

The best known mechanism of self-oscillation excitation is so called negative friction (or negative resistance). For definiteness’ sake, we shall speak about negative friction only. Such a character of friction can be achieved by means of feedback. A classical example of a system in which a similar mechanism manifests itself is a well known vacuum tube generator studied by van der Pol [Van der Pol, 1920]. The feedback, resulting in the appearance of a negative friction, is called positive feedback. Negative friction can be both linear and non-linear. The linear negative friction results in self-excitation of oscillations, i.e., in their appearance for as small initial perturbations as wished.

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References

  1. In the western literature this bifurcation, as well as the direct bifurcation (the birth of a stable limit cycle from a stable singular point), is known as the Hopf bifurcation. However, Hopf classified these bifurcations in 1942 [Hopf, 1942], whereas Andronov and Leontovich discovered these bifurcations (though for systems with one degree of freedom only) in 1939 [Andronov, 1939].

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© 1996 Springer Science+Business Media Dordrecht

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Landa, P.S. (1996). Mechanisms of excitation and amplitude limitation of self-oscillations and auto-waves. Classification of self-oscillatory systems. In: Nonlinear Oscillations and Waves in Dynamical Systems. Mathematics and Its Applications, vol 360. Springer, Dordrecht. https://doi.org/10.1007/978-94-015-8763-1_16

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  • DOI: https://doi.org/10.1007/978-94-015-8763-1_16

  • Publisher Name: Springer, Dordrecht

  • Print ISBN: 978-90-481-4670-3

  • Online ISBN: 978-94-015-8763-1

  • eBook Packages: Springer Book Archive

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