Consider two different paths in which the volume of an ideal gas doubles isothermally:
(i) Reversible expansion (work done = \( w_{\text{rev}} \))
(ii) Irreversible expansion, with the external pressure equal to the final pressure of the gas (work done = \( w_{\text{irrev}} \))
Here,
\[
\dfrac{w_{\text{rev}}}{w_{\text{irrev}}} = ?
\]