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Titlebook: Nonlinear Dynamics; Integrability, Chaos M. Lakshmanan,S. Rajasekar Textbook 2003 Springer-Verlag Berlin Heidelberg 2003 Analysis.Chaos.Pot

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31#
發(fā)表于 2025-3-26 22:22:09 | 只看該作者
M. Lakshmanan,S. Rajasekars are confined to the Fe-rich corner. Contrary to that the present compilation covers the composition range of all evaluated systems as much as possible.978-3-540-88154-4Series ISSN 1615-1844 Series E-ISSN 1616-9522
32#
發(fā)表于 2025-3-27 01:22:36 | 只看該作者
33#
發(fā)表于 2025-3-27 06:37:01 | 只看該作者
s are confined to the Fe-rich corner. Contrary to that the present compilation covers the composition range of all evaluated systems as much as possible.978-3-540-88154-4Series ISSN 1615-1844 Series E-ISSN 1616-9522
34#
發(fā)表于 2025-3-27 10:30:21 | 只看該作者
What is Nonlinearity?,anging their positions continuously. Oceans, rivers, clouds etc. again change their state continuously. Crystals grow and chemicals interact. Even inanimate objects like furniture, buildings, sculptures, etc. change their physical state, perhaps more slowly and over a longer period of time. Change i
35#
發(fā)表于 2025-3-27 14:18:14 | 只看該作者
36#
發(fā)表于 2025-3-27 18:17:20 | 只看該作者
37#
發(fā)表于 2025-3-28 00:55:41 | 只看該作者
38#
發(fā)表于 2025-3-28 03:19:55 | 只看該作者
Chaos in Dissipative Nonlinear Oscillators and Criteria for Chaos,presented by difference equations, where the time variable varies in discrete steps. In the present chapter we shall study the bifurcations phenomena and chaotic solutions of continuous time (flow) dynamical systems described by ordinary differential equations, by making use of our earlier understan
39#
發(fā)表于 2025-3-28 09:47:10 | 只看該作者
Chaos in Nonlinear Electronic Circuits, (5.1)), it requires much computer power and enormous time to scan the entire parameters space, particularly, if more than one control parameters are involved, in order to understand the rich variety of bifurcations and chaotic phenomena. In this connection, . studies of nonlinear oscillators throug
40#
發(fā)表于 2025-3-28 11:56:59 | 只看該作者
Chaos in Conservative Systems,ime bounded motions of such systems are described by attractors. A bounded trajectory starting from an arbitrary initial condition approaches an attractor asymptotically (in the limit . → ∞). The attractor may be an equilibrium point or a periodic orbit or even a chaotic orbit. Further, a dissipativ
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