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The classical equations of motion for a finite chain of particles with a nearest-neighbor Lennard-Jones interaction are solved numerically and, for a broad class of initial conditions, Planck-like distributions are obtained for the time averages of the energies of the normal modes. For physical values of the parameters in the problem, the action constant entering such a distribution turns out to be of the order of magnitude of Planck's constant.
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Galgani et al. (1972) studied this question.
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