For a phase change $(1 \rightarrow 2)$ at constant equilibrium, Clausius-Clapeyron relation is $$\frac{dP}{dT} = \frac{\Delta H_{\text{vap}}}{T \Delta V},$$ where $\Delta H_{\text{vap}} = L \text{ (latent heat)},$ and $\Delta V = V_2 - V_1$.
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