The Lorenz Equations: Bifurcations, Chaos, and Strange Attractors
The Lorenz Equations: Bifurcations, Chaos, and Strange Attractors
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DOI:
10.1007/978-1-4612-5767-7
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发表时间:
1982-12
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影响因子:
--
通讯作者:
C. Sparrow
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文献类型:
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作者:
C. Sparrow
The Lorenz equations, named after Ed Lorenz who first introduced them as a model of a two-dimensional convection [21], have been important for a number of different reasons at various times in the past 20 years or so. Initially they were remarkable just because they are a simple threedimensional nonlinear system of autonomous ordinary differential equa tions showing chaotic behaviour; though many such systems are now known (as described elsewhere in this volume), in 1963 such systems were almost unheard of. So much so, in fact, that, despite the beauty of Lorenz's original paper, and the remarkable progress he made in understanding the behaviour of his system, the paper (and the ideas) were largely ignored for nearly ten years. Also, of course, the equations were of importance because of their connection with the problem from which they were derived: here was the hope that turbulent phenomena could be modelled by simple finite-dimensional systems, but this aspect too was largely ignored.In the 1970s, with the burgeoning interest in dynamical systems (and the wider acceptance of the notion of chaotic behaviour), the Lorenz equations featured in many papers. In several cases, important types of behaviour were first investigated in the Lorenz equations although these behaviours have since been recognised as typical of many systems. For instance Manneville and Pomeau's work on intermittence [24] and the Henon map [18] both appeared in papers on the Lorenz system. At the same time, a specific geometric model of the equations in a small range of parameter values was developed. This work was led by Williams [38, 39] and Guckenheimer [14, 17], though the range of parameter values in question was actually that studied by Lorenz in his original paper. This geometric