2004
DOI: 10.1142/s0218127404010990
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Global Dynamics of a Duffing Oscillator With Delayed Displacement Feedback

Abstract: This paper presents a systematic study on the dynamics of a controlled Duffing oscillator with delayed displacement feedback, especially on the local bifurcations of periodic motions with respect to the time delay. The study begins with the analysis of the stability switches of the trivial equilibrium of the system with various parametric combinations and gives the critical values of time delay, where the trivial equilibrium may change its stability. It shows that as the time delay increases from zero to the p… Show more

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Cited by 46 publications
(36 citation statements)
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“…In the region III (antidashed zone), quasiperiodic oscillations resulting from a secondary Hopf bifurcation take place when crossing from region II to region III. It is worthy to notice that a similar equation to (7) was studied numerically, and it was shown that as the delay gain is increased, the system undergoes a secondary Hopf bifurcations [12,13,17]. Figure 3(c) indicates that by increasing the frequency Ω, the Hopf and the secondary Hopf bifurcation curves overlap giving birth to regions (dashed region IV in Figure 3(c)) on which a stable trivial steady state and a stable limit cycle coexist.…”
Section: Nontrivial Solutionsmentioning
confidence: 94%
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“…In the region III (antidashed zone), quasiperiodic oscillations resulting from a secondary Hopf bifurcation take place when crossing from region II to region III. It is worthy to notice that a similar equation to (7) was studied numerically, and it was shown that as the delay gain is increased, the system undergoes a secondary Hopf bifurcations [12,13,17]. Figure 3(c) indicates that by increasing the frequency Ω, the Hopf and the secondary Hopf bifurcation curves overlap giving birth to regions (dashed region IV in Figure 3(c)) on which a stable trivial steady state and a stable limit cycle coexist.…”
Section: Nontrivial Solutionsmentioning
confidence: 94%
“…As it can be seen from this figure, the bifurcation value of this limit cycle is τ = π/2. Instead of employing the system (9a) and (9b), to obtain the relation between the amplitude of the periodic solution, R, and time delay, τ, as done in [12], we will take advantage from this modulation system to determine the region of existence of this periodic motion born by Hopf bifurcation.…”
Section: Nontrivial Solutionsmentioning
confidence: 99%
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