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Clausius–Clapeyron relation
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Clausius–Clapeyron relation : ウィキペディア英語版
Clausius–Clapeyron relation

The Clausius–Clapeyron relation, named after Rudolf Clausius and Benoît Paul Émile Clapeyron, is a way of characterizing a discontinuous phase transition between two phases of matter of a single constituent. On a pressuretemperature (P–T) diagram, the line separating the two phases is known as the coexistence curve. The Clausius–Clapeyron relation gives the slope of the tangents to this curve. Mathematically,
:\frac = \frac=\frac,
where \mathrmP/\mathrmT is the slope of the tangent to the coexistence curve at any point, L is the specific latent heat, T is the temperature, \Delta v is the specific volume change of the phase transition and \Delta s is the specific entropy change of the phase transition.
== Derivations ==


抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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