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Slow Passage Through Resonance and Resonance Tongues

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Nonlinear Resonances

Part of the book series: Springer Series in Synergetics ((SSSYN))

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Abstract

In Chap. 11 the autoresonance phenomenon due to a slow variation of frequency of the driving force or the slow variation of a parameter of nonlinear systems is described. Two other interesting effects that can be realizable in the case of slowly varying a parameter are the slow passage through resonance and resonance tongues. For example, consider a linear or a nonlinear system driven by a periodic external force with a fixed frequency ω f. Assume that the amplitude of oscillation is maximum at ω f = ω f,max with a value A max. Suppose ω is allowed to vary slowly with time and write \(\omega _{\mathrm{f}}(t) =\omega +\epsilon t\), ε ≪ 1. In a typical case when ω is fixed at a value smaller than ω f,max then the amplitude of oscillation varies with time, reaches a maximum value at a certain time t′ such that \(\omega _{\mathrm{f}}(t) =\omega +\epsilon t' <\omega _{\mathrm{f,max}}\) and then decreases. The new resonance frequency ω f(t) is lower than the frequency ω f,max. This is termed as slow passage through resonance and is a transient phenomenon. Such a passing through has been found to occur in systems exhibiting parametric resonance also.

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Rajasekar, S., Sanjuan, M.A.F. (2016). Slow Passage Through Resonance and Resonance Tongues. In: Nonlinear Resonances. Springer Series in Synergetics. Springer, Cham. https://doi.org/10.1007/978-3-319-24886-8_13

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