In an irreversible isothermal expansion of 2 moles of an ideal gas, work done (W) is found to be (-P\(_{ext}\)V). If the same isothermal expansion is carried out reversibly, the work done will be:
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When dealing with isothermal processes, remember that the work done in reversible and irreversible processes are related by a factor of \( 2.303 \) in the case of isothermal expansion.
For an irreversible expansion, the work done \( W \) is given by:
\[
W = -P_{ext} \Delta V
\]
For a reversible expansion, the work done is given by:
\[
W = -nRT \ln \left( \frac{V_f}{V_i} \right)
\]
For the same isothermal expansion, the relationship between irreversible and reversible work done is:
\[
W_{reversible} = W_{irreversible} \times 2.303
\]
Thus:
\[
W_{reversible} = -2.303 \times W_{irreversible} = -2.303 \times (-1 \cdot 2RT) = -1.386 RT
\]