Abstract:Chaotic oscillations arising in forced oscillations of a two degree-of-freedom autoparametric system are studied. Statistical analysis of the numerically integrated nonperiodic responses is shown to be a meaningful description of the mean square values and the frequency contents of the responses. Some qualitative experimental results are presented to substantiate the necessity of performing the statistical analysis of the responses even though the system and the input are deterministic.
“…Miles [10] showed that these amplitude and phase modulated motions can themselves bifurcate to chaotic amplitude modulations. No such complex solutions of the amplitude or the averaged equations were found for the subharmonic resonance case investigated by Hatwal et al [6,7].…”
Section: Introductionmentioning
confidence: 94%
“…The autoparametric system for the present study is shown in Figure 1, and its nondimensional equations of motion are given as follows [6,7]: …”
Section: System Description and Equations Of Motionmentioning
confidence: 99%
“…Hatwal etal. [6,7] used the harmonic balance method and direct numerical integration to study a variant of this system at moderately higher levels of excitations, and observed that over some forcing frequencies and amplitudes, the system response was an amplitude and phase modulated harmonic motion. For even higher excitation levels, the response was found to be chaotic.…”
Forced, weakly nonlinear oscillations of a two degree-of-freedom autoparametric vibration absorber system are studied for resonant excitations. The method of averaging is used to obtain first-order approximations to the response of the system. A complete bifurcation analysis of the averaged equations is undertaken in the subharmonic case of internal and external resonance. The "locked pendulum" mode of response is found to bifurcate to coupled-mode motion for some excitation frequencies and forcing amplitudes. The coupled-mode response can undergo Hopf bifurcation to limit cycle motions, when the two linear modes are mistuned away from the exact internal resonance condition. The software packages AUTO and KAOS are used and a numerically assisted study of the Hopf bifurcation sets, and dynamic steady solutions of the amplitude or averaged equations is presented. It is shown that both super-and sub-critical Hopf bifurcations arise and the limit cycles quickly undergo period-doubling bifurcations to chaos. These imply chaotic amplitude modulated motions for the system.
“…Miles [10] showed that these amplitude and phase modulated motions can themselves bifurcate to chaotic amplitude modulations. No such complex solutions of the amplitude or the averaged equations were found for the subharmonic resonance case investigated by Hatwal et al [6,7].…”
Section: Introductionmentioning
confidence: 94%
“…The autoparametric system for the present study is shown in Figure 1, and its nondimensional equations of motion are given as follows [6,7]: …”
Section: System Description and Equations Of Motionmentioning
confidence: 99%
“…Hatwal etal. [6,7] used the harmonic balance method and direct numerical integration to study a variant of this system at moderately higher levels of excitations, and observed that over some forcing frequencies and amplitudes, the system response was an amplitude and phase modulated harmonic motion. For even higher excitation levels, the response was found to be chaotic.…”
Forced, weakly nonlinear oscillations of a two degree-of-freedom autoparametric vibration absorber system are studied for resonant excitations. The method of averaging is used to obtain first-order approximations to the response of the system. A complete bifurcation analysis of the averaged equations is undertaken in the subharmonic case of internal and external resonance. The "locked pendulum" mode of response is found to bifurcate to coupled-mode motion for some excitation frequencies and forcing amplitudes. The coupled-mode response can undergo Hopf bifurcation to limit cycle motions, when the two linear modes are mistuned away from the exact internal resonance condition. The software packages AUTO and KAOS are used and a numerically assisted study of the Hopf bifurcation sets, and dynamic steady solutions of the amplitude or averaged equations is presented. It is shown that both super-and sub-critical Hopf bifurcations arise and the limit cycles quickly undergo period-doubling bifurcations to chaos. These imply chaotic amplitude modulated motions for the system.
“…As can be seen from [10,14], the values of ζ 1 , ζ 2 , , 0 are considered to be sufficiently small. Therefore, we introduce a small parameter ϵ(0 < ≪ 1) and make transform , , , , , ,…”
Section: Introductionmentioning
confidence: 99%
“…The early results of system (1.1) with 0 0 F were traced to [10,14] by Hatwal, Mallik and Ghosh based on the harmonic balance method and direct numerical integration. At moderately higher levels of excitations, they observed that over some forcing frequencies and amplitudes, the system response was amplitude and phase modulated harmonic motion, and for even higher excitation levels, the response was found to be chaotic.…”
Abstract. Based on the method of averaging, in this paper we investigate the continuation of harmonic motions for a weakly forced autoparametric vibrating system which models the dynamics of a forced pendulum positioned on a vertically excited mass. The result shows that when the very weakly force is imposed on the pendulum, a state of dynamic balance (a harmonic motion) is preserving.
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