×

Chaos in the softening Duffing system under multi-frequency periodic forces. (English) Zbl 1142.70330

Summary: The chaotic dynamics of the softening-spring Duffing system with multi-frequency external periodic forces is studied. It is found that the mechanism for chaos is the transverse heteroclinic tori. The Poincaré map, the stable and the unstable manifolds of the system under two incommensurate periodic forces were set up on a two-dimensional torus. Utilizing a global perturbation technique of Melnikov the criterion for the transverse interaction of the stable and the unstable manifolds was given. The system under more but finite incommensurate periodic forces was also studied. The Melnikov’s global perturbation technique was therefore generalized to higher dimensional systems. The region in parameter space where chaotic dynamics may occur was given. It was also demonstrated that increasing the number of forcing frequencies will increase the area in parameter space where chaotic behavior can occur.

MSC:

70K55 Transition to stochasticity (chaotic behavior) for nonlinear problems in mechanics
70K40 Forced motions for nonlinear problems in mechanics
37N05 Dynamical systems in classical and celestial mechanics
Full Text: DOI

References:

[1] LIU Zeng-rong.Perturbation Method of Chaos[M]. Shanghai: Shanghai Scientific and Technology Education Publishing House, 1994: 7–10. (in Chinese)
[2] Moon F C, Holmes W T. Double Poincare sections of a quasi-periodically forced, chaotic attractor [J].Physics Letters A, 1985,111(4):157–160. · doi:10.1016/0375-9601(85)90565-1
[3] Wiggins S. Chaos in the quasiperiodically forced Duffing oscillator[J].Physics Letters A, 1987,124(3):138–142. · doi:10.1016/0375-9601(87)90240-4
[4] Wiggins S.Global Bifurcations and Chaos–Analytical Methods[M]. New York: Springer-Verlag, 1988: 313–333.
[5] Kayo IDE, Wiggins S. The bifurcation to homoclinic tori in the quasiperiodically forced Duffing oscillator[J].Physica D, 1989,34(1):169–182. · Zbl 0673.58031 · doi:10.1016/0167-2789(89)90232-7
[6] Heagy J, Ditto W L. Dynamics of a two-frequency parametrically driven Duffing oscillator[J].Journal of Nonlinear Science, 1991,1(2):423–455. · Zbl 0794.34028 · doi:10.1007/BF02429848
[7] LU Qi-shao. Principle resonance of a nonlinear system with two-frequency parametric and self-excitations[J].Nonlinear Dynamics, 1991,2(6):419–444. · doi:10.1007/BF00045437
[8] LU Qi-shao, HUANG Ke-lei. Nonlinear dynamics, bifurcation and chaos[A]. In: HUANG Wen-hu, CHEN Bin, WANG Zhao-lin Eds.,New Advances of Common Mechanics (Dynamics, Vibration and Control)[C]. Beijing: Science Press, 1994,11–18. (in Chinese)
[9] Yagasaki K, Sakata M, Kimura K. Dynamics of weakly nonlinear system subjected to combined parametric and external excitation[J].Trans ASME, Journal of Applied Mechanics, 1990,57(1): 209–217. · Zbl 0725.70015 · doi:10.1115/1.2888306
[10] Yagasaki K. Chaos in weakly nonlinear oscillator with parametric and external resonance[J].Trans ASME, Journal of Applied Mechanics, 1991,58(1):244–250. · Zbl 0777.70018 · doi:10.1115/1.2897158
[11] Yagasaki K. Chaotic dynamics of a quasi-periodically forced beam[J].Trans ASME, Journal of Applied Mechanics, 1992,59(1):161–167. · Zbl 0761.73067 · doi:10.1115/1.2899422
[12] CHEN Yu-shu, WANG De-shi. Chaos of the beam with axial-direction excitation[J].Journal of Nonlinear Dynamics, 1993,1(2):124–135. (in Chinese)
[13] Kapitaniak T. Combined bifurcations and transition to chaos in a nonlinear oscillator with two external periodic forces[J].Journal of Sound and Vibration, 1988,121(2):259–268. · Zbl 1235.70123 · doi:10.1016/S0022-460X(88)80028-2
[14] Kapitaniak T. Chaotic distribution of nonlinear systems perturbed by random noise[J].Physical Letters A, 1986,116(6):251–254. · doi:10.1016/0375-9601(86)90588-8
[15] Kapitaniak T. A property of a stochastic response with bifurcation to nonlinear system[J].Journal of Sound and Vibration, 1986,107(1):177–180. · Zbl 1235.70184 · doi:10.1016/0022-460X(86)90292-0
[16] BI Qin-sheng, CHEN Yu-shu, WU Zhi-qiang. Bifurcation in a nonlinear Duffing system with multifrequency external periodic forces[J].Applied Mathematics and mechanics (English Edition), 1998,19(2):121–128. · Zbl 0921.70015 · doi:10.1007/BF02457679
[17] Leung A Y T, Fung C. Construction of chaotic regions[J].Journal of Sound and Vibration, 1989,131(3):445–455. · Zbl 1235.70125 · doi:10.1016/0022-460X(89)91004-3
[18] Stupnicka S, Bajkowski. The 1/2 subharmonic resonance its transition to chaos motion in a nonlinear oscillator[J].IFTR Reports, 1986,4(1):67–72. · Zbl 0628.70020
[19] Dooren R V. On the transition from regular to chaotic behaviour in the Duffing oscillator[J].Journal of Sound and Vibration, 1988,123(2):327–339. · Zbl 1235.70136 · doi:10.1016/S0022-460X(88)80115-9
[20] Yagasaki K. Homoclinic tangles, phase locking, and chaos in a two-frequency perturbation of Duffing equation[J].Journal of Nonlinear Science, 1999,9(1):131–148. · Zbl 0939.34039 · doi:10.1007/s003329900066
This reference list is based on information provided by the publisher or from digital mathematics libraries. Its items are heuristically matched to zbMATH identifiers and may contain data conversion errors. In some cases that data have been complemented/enhanced by data from zbMATH Open. This attempts to reflect the references listed in the original paper as accurately as possible without claiming completeness or a perfect matching.