Step 1: Apply Clausius–Clapeyron equation.
At constant coverage,
\[
\ln \left(\frac{P_2}{P_1}\right) = \frac{\Delta H_\text{ads}}{R} \left(\frac{1}{T_1} - \frac{1}{T_2}\right)
\]
Given $P_1 = 25$, $P_2 = 30$, $T_1 = 140$, $T_2 = 280$.
Step 2: Substitute values.
\[
\ln \left(\frac{30}{25}\right) = \frac{\Delta H_\text{ads}}{8.314}\left(\frac{1}{140} - \frac{1}{280}\right)
\]
\[
0.182 = \frac{\Delta H_\text{ads}}{8.314}(0.00357)
\]
\[
\Delta H_\text{ads} = \frac{0.182 \times 8.314}{0.00357} = 424.6 \, \text{J mol}^{-1} = 12.0 \, \text{kJ mol}^{-1}
\]
Step 3: Conclusion.
The isosteric enthalpy of adsorption is 12.0 kJ mol$^{-1}$.