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Chen Yushu, Xu Jian (1993)
Periodic response and bifurcation theory of nonlinear Hill systemJ Non Dyn Eng, 1
P. Holmes, D. Rand (1980)
Phase portraits and bifurcations of the non-linear oscillator: ẍ + (α + γx2 + βx + δx3 = 0International Journal of Non-linear Mechanics, 15
M. Feigenbaum (1979)
The universal metric properties of nonlinear transformationsJournal of Statistical Physics, 21
R. Leven, B. Pompe, C. Wilke, B. Koch (1985)
Experiments on periodic and chaotic motions of a parametrically forced pendulumPhysica D: Nonlinear Phenomena, 16
P. Holmes, F. Moon (1983)
Strange Attractors and Chaos in Nonlinear MechanicsJournal of Applied Mechanics, 50
F Takens (1974)
Forced oscillation and bifurcationsComm Math Inst Rijksuniversiteit Utrecht, 3
Stephen Wiggins (1988)
Global Bifurcations and Chaos
J. Guckenheimer, P. Holmes (1983)
Nonlinear Oscillations, Dynamical Systems, and Bifurcations of Vector Fields, 42
YS Chen (1993)
Bifurcation and Chaos Theory of Nonlinear Vibration Systems
V. Bolotin, V. Weingarten, L. Greszczuk, K. Trigoroff, K. Gallegos, E. Cranch (1965)
Dynamic Stability of Elastic SystemsJournal of Applied Mechanics, 32
Lawrence Zavodney, A. Nayfeh, N. Sanchez (1990)
Bifurcations and chaos in parametrically excited single-degree-of-freedom systemsNonlinear Dynamics, 1
MJ Feigenbaum (1979)
The universal metric properties of nonlinear transformJ Stat Phys, 21
Y. Ueda (1978)
Randomly transitional phenomena in the system governed by Duffing's equationJournal of Statistical Physics, 20
M. Soliman, J. Thompson (1989)
Integrity measures quantifying the erosion of smooth and fractal basins of attractionJournal of Sound and Vibration, 135
P Holmes, F Moon (1983)
Strange attractors and chaos in nonlinear mechanicsASME J Appl Mech, 50
Chengzhi Li, C. Rousseau (1990)
Codimension 2 Symmetric Homoclinic Bifurcations and Application to 1:2 ResonanceCanadian Journal of Mathematics, 42
Semi-analytical and semi-numerical method is used to investigate the global bifurcations and chaos in the nonlinear system of a Van der Pol-Duffing-Mathieu oscillator. Semi-analytical and semi-numerical method means that the autonomous system, called Van der Pol-Duffing system, is analytically studied to draw all global bifurcations diagrams in parameter space. These diagrams are called basic bifurcation diagrams. Then fixing parameter in every space and taking parametrically excited amplitude as a bifurcation parameter, we can observe the evolution from a basic bifurcation diagram to chaotic pattern by numerical methods.
Acta Mechanica Sinica – Springer Journals
Published: Aug 25, 2006
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