Equating the initial and final internal energies, with the same additive constant,soThis is cooling in free expansion of a van der Waals gas. The gas cools because separating attractive particles raises their potential energy at the expense of kinetic energy. The excluded-volume coefficient cancels from this caloric model. The result assumes a homogeneous equilibrium gas with and positive ; a two-phase final state would require a coexistence calculation rather than this homogeneous formula. The ideal-gas limit has no temperature change.
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