Step 1:
We start by applying the Clausius-Clapeyron equation, which is given by:
\[ \ln \left( \frac{P_2}{P_1} \right) = -\frac{\Delta H_{\text{vap}}}{R} \left( \frac{1}{T_2} - \frac{1}{T_1} \right) \]
where $P_1$ and $P_2$ are the initial and final pressures,
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