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Applied Mathematics and Nonlinear Sciences
Volume 3 (2018): Issue 2 (July 2018)
Open Access
Intermittent transition to chaos in vibroimpact system
V.A. Bazhenov
V.A. Bazhenov
,
O.S. Pogorelova
O.S. Pogorelova
and
T.G. Postnikova
T.G. Postnikova
| Dec 01, 2018
Applied Mathematics and Nonlinear Sciences
Volume 3 (2018): Issue 2 (July 2018)
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Published Online:
Dec 01, 2018
Page range:
475 - 486
Received:
Aug 29, 2018
Accepted:
Nov 29, 2018
DOI:
https://doi.org/10.2478/AMNS.2018.2.00037
Keywords
vibroimpact system
,
chaotic behaviour
,
route to chaos
,
intermittency
,
continuous wavelet transform
,
surface of wavelet coefficients
© 2018 V.A. Bazhenov et al., published by Sciendo
This work is licensed under the Creative Commons Attribution-NonCommercial-NoDerivatives 4.0 License.
Fig. 1
Vibroimpact system model
Fig. 2
Amplitude-frequency response in wide range of excitation frequency
Fig. 3
Floquet multipliers behaviour at DE region
Fig. 4
The largest Lyapunov exponent dependence on control parameter
Fig. 5
Bifurcation diagram
Fig. 6
Time series and wavelet surface projection for intermittency under ω = 6.076 rad⋅s-1 (Color online)
Fig. 7
Time series and wavelet surface projection for intermittency under ω = 6.13 rad⋅s-1 (Color online)
Fig. 8
Time series and wavelet surface projection for intermittency under ω = 6.13 rad⋅s-1 (region inside red oval at Fig. 7)
Fig. 9
Surface of wavelet coefficients for intermittency under ω = 6.13 rad⋅s-1 (Color online)
Fig. 10
Phase trajectories and Poincare maps for the regions of chaotic and periodic motions under intermittency (ω = 6.13 rad⋅s-1)
Fig. 11
Time series and wavelet surface projection for chaotic regime under ω = 6.2 rad⋅s-1 (Color online)
Fig. 12
Phase trajectories and Poincare map for chaotic motion under ω = 6.2 rad⋅s-1
Fig. 13
Surface of wavelet coefficients for chaotic motion under ω = 6.2 rad⋅s-1 (Color online)