The Clapeyron–Clausius equation describes the relationship between pressure and temperature during phase transitions, such as melting (fusion), vaporization, or sublimation.
When a solid and liquid are in equilibrium, and their vapour pressures are measured at two different temperatures, this equation allows us to compute the latent heat of fusion.
The integrated form of the Clausius–Clapeyron equation is:
\[
\ln\left(\frac{P_2}{P_1}\right) = -\frac{\Delta H_{\text{fus}}}{R} \left( \frac{1}{T_2} - \frac{1}{T_1} \right)
\]
Where:
$P_1, P_2$ = vapour pressures at temperatures $T_1$ and $T_2$ respectively (in Kelvin)
$\Delta H_{\text{fus}}$ = latent heat of fusion
$R$ = universal gas constant
By rearranging this equation, we can solve for $\Delta H_{\text{fus}}$ if the vapour pressures and corresponding temperatures are known.
Other options like Nernst Heat Theorem, Maxwell’s equations, and Van Laar equations do not directly apply to phase transition calculations involving vapour pressure and latent heat.
Hence, the correct method for such a calculation is the Clapeyron–Clausius equation.