Let State 1 have pressure P1 and volume V1, and State 2 have pressure P2 and volume V2. For an isothermal expansion, V2>V1 and P1>P2.
For expansion from State 1 to State 2:
In a single-stage expansion, the external pressure is constant at the final pressure P2. The magnitude of work is ∣wA∣=P2(V2−V1).
In a multi-stage expansion, the external pressure is reduced in steps, keeping it closer to the internal pressure of the gas. The work done by the gas increases with the number of stages, reaching a maximum for a reversible process (∣wrev∣). Thus, ∣wrev∣>∣wB∣>∣wA∣.
For compression from State 2 to State 1:
In a single-stage compression, the external pressure is constant at the final pressure P1. The magnitude of work is ∣wC∣=P1(V2−V1).
In a multi-stage compression, the external pressure is increased in steps. The work done on the gas decreases with the number of stages, reaching a minimum for a reversible process (∣wrev∣). Thus, ∣wC∣>∣wD∣>∣wrev∣.
Since P1>P2, the single-stage compression work ∣wC∣ is the largest, and the single-stage expansion work ∣wA∣ is the smallest. The reversible work magnitude ∣wrev∣ is the same for both expansion and compression between the same states.
Combining these inequalities, we get:
∣wC∣>∣wD∣>∣wrev∣>∣wB∣>∣wA∣
Therefore, the correct order of the magnitude of work is ∣wC∣>∣wD∣>∣wB∣>∣wA∣.
Answer: ∣wC∣>∣wD∣>∣wB∣>∣wA∣