A chaotic crisis between chaotic saddle and attractor in forced Duffing oscillators

被引:14
作者
Hong, Ling [1 ]
Xu, Jianxue [1 ]
机构
[1] Department of Engineering Mechanics, Sch. of Civil Engineering/Mechanics, Xi'an Jiaotong University
关键词
Chaotic saddle; Crisis; Fractal basin boundary; Generalized cell mapping system; Global analysis;
D O I
10.1016/S1007-5704(02)00107-7
中图分类号
学科分类号
摘要
We investigate crises in forced Duffing oscillators by the generalized cell mapping digraph method to efficiently complete the global analysis of non-linear systems, which includes global transient analysis through digraphic algorithms based on a strictly theoretical correspondence between generalized cell mappings and digraphs. A process of generalized cell mapping method is developed to refine persistent and transient self-cycling sets. The refining procedures of persistent and transient self-cycling sets are respectively given on the basis of their definitions in the cell state space. A chaotic boundary crisis and a chaotic interior crisis are discovered. A chaotic boundary crisis owing to a collision between chaotic attractor and saddle occurs in its basin boundary possessing a fractal structure. In such a case the chaotic attractor together with its basin of attraction is suddenly destroyed as the parameter passes through the critical value, and the chaotic saddle also undergoes an abrupt enlargement in its size. Namely, the chaotic attractor is converted into an incremental portion of the chaotic saddle after the collision. For a chaotic interior crisis, there is a sudden increase in the size of a chaotic attractor as the parameter passes through the critical value. For the chaotic interior crisis, it is demonstrated that the chaotic attractor collides with a chaotic saddle in its basin interior when the crisis occurs. This chaotic saddle is an invariant and non-attracting set. The origin and evolution of the chaotic saddle are investigated as well. © 2003 Elsevier B.V. All rights reserved.
引用
收藏
页码:313 / 329
页数:16
相关论文
共 15 条
  • [1] Grebogi C., Ott E., Yorke J.A., Crises, sudden changes in chaotic attractors, and transient chaos, Physica D, 7, pp. 181-200, (1983)
  • [2] Grebogi C., Ott E., Yorke J.A., Critical exponents of chaotic transients in nonlinear dynamical systems, Phys. Rev. Lett., 57, pp. 1284-1287, (1986)
  • [3] Thompson J.M.T., Stewart H.B., Nonlinear Dynamics and Chaos, (1986)
  • [4] Thompson J.M.T., Stewart H.B., Ueda Y., Safe, explosive, and dangerous bifurcations in dissipative dynamical systems, Phys. Rev. E, 49, pp. 1019-1027, (1994)
  • [5] Lai Y.C., Grebogi C., Yorke J.A., Sudden change in the size of chaotic attractors: How does it occur?, Applied Chaos, pp. 441-455, (1992)
  • [6] Abraham R.H., Stewart H.B., A chaotic blue sky catastrophe in forced relaxation oscillations, Physica D, 19, pp. 294-400, (1986)
  • [7] Stewart H.B., A chaotic saddle catastrophe in forced oscillators, Dynamical Systems Approaches to Nonlinear Problems in Systems and Circuits, pp. 138-149, (1988)
  • [8] Ueda Y., Explosion of strange attractors exhibited by Duffing's equation, Nonlinear Dynamics, pp. 422-434, (1980)
  • [9] Hsu C.S., Cell-to-cell Mapping: A Method of Global Analysis for Nonlinear Systems, (1987)
  • [10] Hsu C.S., Global analysis by cell mapping, Int. J. Bifurcat. Chaos, 2, 4, pp. 727-771, (1992)