In an isothermal expansion of an ideal gas, the temperature remains constant. The work done \( W \) during such an expansion is given by the formula:
\[
W = \int_{V_1}^{V_2} P \, dV
\]
Using the ideal gas law \( P = \frac{nRT}{V} \), where \( n \) is the number of moles of gas, \( R \) is the gas constant, and \( T \) is the temperature, we get:
\[
W = \int_{V_1}^{V_2} \frac{nRT}{V} \, dV
\]
Since the temperature is constant (\( T = {constant} \)), the work done becomes:
\[
W = nRT \ln \left( \frac{V_2}{V_1} \right)
\]
This is the correct expression for the work done during an isothermal expansion.
- Zero work would apply only if there is no volume change, which is not the case in this scenario.
- \( P\Delta V \) is the work formula for an ideal gas in an isobaric process, not an isothermal process.
- \( nC_v \Delta T \) represents the heat or work done in an isochoric process (constant volume), not an isothermal one.
Thus, the correct answer is \( nRT \ln \left( \frac{V_2}{V_1} \right) \).