From the thermodynamic viewpoint the glass transition is a second-order change: there is no latent heat involved, so the entropy varies continuously through the transition. But the transition is not a reversible process. A simulation study of the hard-sphere fluid shows that the statistical entropy, defined in terms of the configuration integral, decreases by 0·20 ± 0·03 Nk when it forms a glass, which indicates that a system of N hard spheres can form about exp (0·2 N) glasses. For the system of N = 256 spheres studied there are about 1022 distinct glasses.
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Robin J. Speedy (1993) studied this question.
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