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Titlebook: Equilibrium Statistical Physics; Phases of Matter and Marc Baus,Carlos F. Tejero Textbook 20081st edition Springer-Verlag Berlin Heidelberg

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51#
發(fā)表于 2025-3-30 09:29:47 | 只看該作者
Franco Basile PhD,Rudolph K. Mignonous (second-order) or where the order parameter of a continuous phase transition vanishes (Fig. 10.1). Such a thermodynamical state is called a critical state, or a critical point (CP), and its variables will be distinguished here by a subscript c. In the immediate vicinity of a CP, there occur a nu
52#
發(fā)表于 2025-3-30 14:56:45 | 只看該作者
Christos Kravvaritis,Marilena Mitrouliquilibrium. In the various examples of coexistence considered in Sects. 9.1 and 9.2, the average densities of the phases are uniform, i.e., the conditions of mechanical equilibrium and chemical equilibrium at a given temperature have been derived from the free energy of each bulk phase (in the therm
53#
發(fā)表于 2025-3-30 20:19:57 | 只看該作者
https://doi.org/10.1007/978-3-319-04720-1 been considered to be perfect although, in practice, many bulk phases exhibit defects, i.e., domains where this order departs from the one originally postulated. Such defects are usually very stable, because the free energy cost to remove them easily exceeds the thermal energy, and prevent the syst
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