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Applied Mathematics and Nonlinear Sciences
Volume 5 (2020): Issue 1 (January 2020)
Open Access
On the existence of periodic solution and the transition to chaos of Rayleigh-Duffing equation with application of gyro dynamic
Mohamed El-Borhamy
Mohamed El-Borhamy
and
Nahla Mosalam
Nahla Mosalam
| Mar 30, 2020
Applied Mathematics and Nonlinear Sciences
Volume 5 (2020): Issue 1 (January 2020)
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Published Online:
Mar 30, 2020
Page range:
93 - 108
Received:
Aug 06, 2019
Accepted:
Nov 09, 2019
DOI:
https://doi.org/10.2478/amns.2020.1.00010
Keywords
Nonlinear Ordinary Differential Equations
,
Stability Theory
,
Periodic Solutions
,
Bifurcation
,
Chaotic Dynamic
,
Gyroscope
© 2020 Mohamed El-Borhamy et al., published by Sciendo
This work is licensed under the Creative Commons Attribution 4.0 International License.
Fig. 1
Motion of Lagrange’s gyroscope represented by a cylindrical body mounted on a vibrating base with periodic excitation(d(t) = do sinωt).
Fig. 2
Existence of stable limit cycle with α = 10, β = 1, c = 0.1, e = 0.05, Γ = 1 and ω = 3.
Fig. 3
Solution and phase plane in case of a stable motion at α = 10, β = 1, c = 0.5, e = 0.2, Γ = 1 and ω = 3.
Fig. 4
Bifurcation diagrams in case of c = 0.5, ω = 1, e = 0 (left) and e = 0.1 (right).
Fig. 5
Chaos diagrams in case of c = 0.5, ω = 1, e = 0 at Γ=0.522,1,25 and 50 from to left to right.
Fig. 6
Chaos diagrams in case of c = 0.5, ω = 1, e = 0.1 at Γ=0.529,1,25 and 50 from to left to right.