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Hard Ball Systems and the Lorentz Gas (Hardcover, 2000 ed.): D. Sza'sz Hard Ball Systems and the Lorentz Gas (Hardcover, 2000 ed.)
D. Sza'sz; L.A. Bunimovich, D. Burago, N. Chernov, E.G.D. Cohen, …
R2,972 Discovery Miles 29 720 Ships in 10 - 15 working days

Hard Ball Systems and the Lorentz Gas are fundamental models arising in the theory of Hamiltonian dynamical systems. Moreover, in these models, some key laws of statistical physics can also be tested or even established by mathematically rigorous tools. The mathematical methods are most beautiful but sometimes quite involved. This collection of surveys written by leading researchers of the fields - mathematicians, physicists or mathematical physicists - treat both mathematically rigourous results, and evolving physical theories where the methods are analytic or computational. Some basic topics: hyperbolicity and ergodicity, correlation decay, Lyapunov exponents, Kolmogorov-Sinai entropy, entropy production, irreversibility. This collection is a unique introduction into the subject for graduate students, postdocs or researchers - in both mathematics and physics - who want to start working in the field.

The Boltzmann Equation - Theory and Applications (Paperback, Softcover reprint of the original 1st ed. 1973): E.G.D. Cohen, W.... The Boltzmann Equation - Theory and Applications (Paperback, Softcover reprint of the original 1st ed. 1973)
E.G.D. Cohen, W. Thirring
R4,479 Discovery Miles 44 790 Ships in 10 - 15 working days

In,1872, Boltzmann published a paper which for the first time provided a precise mathematical basis for a discussion of the approach to equilibrium. The paper dealt with the approach to equilibrium of a dilute gas and was based on an equation - the Boltzmann equation, as we call it now - for the velocity distribution function of such ~ gas. The Boltzmann equation still forms the basis of the kinetic theory of gases and has proved fruitful not only for the classical gases Boltzmann had in mind, but als- if properly generalized - for the electron gas in a solid and the excitation gas in a superfluid. Therefore it was felt by many of us that the Boltzmann equation was of sufficient interest, even today, to warrant a meeting, in which a review of its present status would be undertaken. Since Boltzmann had spent a good part of his life in Vienna, this city seemed to be a natural setting for such a meeting. The first day was devoted to historical lectures, since it was generally felt that apart from their general interest, they would furnish a good introduction to the subsequent scientific sessions. We are very much indebted to Dr. D.

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