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用于稀薄气体李雅普诺夫指数之和的博戈柳博夫-博恩-格林-柯克伍德-伊冯层级方法。

Bogoliubov-Born-Green-Kirkwood-Yvon hierarchy methods for sums of Lyapunov exponents for dilute gases.

作者信息

Dorfman J. R., Latz Arnulf, Van Beijeren Henk

机构信息

Institute for Physical Science and Technology and Department of Physics, University of Maryland, College Park, Maryland 20742.

出版信息

Chaos. 1998 Jun;8(2):444-454. doi: 10.1063/1.166325.

Abstract

We consider a general method for computing the sum of positive Lyapunov exponents for moderately dense gases. This method is based upon hierarchy techniques used previously to derive the generalized Boltzmann equation for the time-dependent spatial and velocity distribution functions for such systems. We extend the variables in the generalized Boltzmann equation to include a new set of quantities that describe the separation of trajectories in phase space needed for a calculation of the Lyapunov exponents. The method described here is especially suitable for calculating the sum of all of the positive Lyapunov exponents for the system, and may be applied to equilibrium as well as nonequilibrium situations. For low densities we obtain an extended Boltzmann equation, from which, under a simplifying approximation, we recover the sum of positive Lyapunov exponents for hard-disk and hard-sphere systems, obtained before by a simpler method. In addition we indicate how to improve these results by avoiding the simplifying approximation. The restriction to hard-sphere systems in d dimensions is made to keep the somewhat complicated formalism as clear as possible, but the method can be easily generalized to apply to gases of particles that interact with strong short-range forces. (c) 1998 American Institute of Physics.

摘要

我们考虑一种计算中等密度气体正李雅普诺夫指数之和的通用方法。该方法基于先前用于推导此类系统随时间变化的空间和速度分布函数的广义玻尔兹曼方程的层级技术。我们将广义玻尔兹曼方程中的变量进行扩展,以纳入一组新的量,这些量描述了计算李雅普诺夫指数所需的相空间中轨迹的分离。这里描述的方法特别适用于计算系统所有正李雅普诺夫指数之和,并且可应用于平衡和非平衡情况。对于低密度情况,我们得到一个扩展的玻尔兹曼方程,在一个简化近似下,从中我们恢复了之前通过更简单方法得到的硬磁盘和硬球系统的正李雅普诺夫指数之和。此外,我们指出了如何通过避免简化近似来改进这些结果。限制在d维硬球系统是为了尽可能清晰地呈现有点复杂的形式体系,但该方法可以很容易地推广到适用于与强短程力相互作用的粒子气体。(c)1998美国物理研究所。

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