To solve this problem, we need to match the types of isothermal processes from List-I with the corresponding expressions for work done from List-II.
- Reversible expansion:
- In a reversible isothermal expansion, the work done is given by the formula: \(w = -nRT \ln \frac{V_f}{V_i}\), where \(n\) is the number of moles, \(R\) is the gas constant, \(T\) is the temperature, and \(V_f\) and \(V_i\) are the final and initial volumes, respectively.
- Therefore, the match is with option 2: \(w = -nRT \ln \frac{V_f}{V_i}\).
- Free expansion:
- In a free expansion, no work is done because the process occurs without any external pressure change.
- The work done, \(w\), is zero. So, it matches with option 1: \(w = 0\).
- Irreversible expansion:
- In an irreversible expansion against a constant external pressure, the work done is given by \(w = -P_{\text{ext}} (V_f - V_i)\).
- Thus, it matches with option 4: \(w = -P_{\text{ext}} (V_f - V_i)\).
- Irreversible compression:
- Similar to irreversible expansion, but since it's compression, the volume change \((V_i - V_f)\) is considered as positive work done by the surroundings.
- So, it matches with option 3: \(w = -P_{\text{ext}} (V_i - V_f)\).
Therefore, the correct matching order is 2, 1, 3, 4, corresponding to the option 2, 1, 3, 4.