Work done in an irreversible isothermal process is given by $w = -P_{ext}\Delta V$. We compare the magnitudes $|w|$.
1. For Expansion ($V_1 \to V_2$):
Single stage ($w_A$): $P_{ext} = P_2$. Magnitude $|w_A| = P_2(V_2 - V_1)$.
Multi-stage ($w_B$): $P_{ext}$ decreases in steps. The area under the path is larger than the single rectangle of $w_A$. Thus, $|w_B|>|w_A|$.
2. For Compression ($V_2 \to V_1$):
Single stage ($w_C$): $P_{ext} = P_1$. Magnitude $|w_C| = P_1(V_2 - V_1)$. Since $P_1>P_2$, $|w_C|$ is very large.
Multi-stage ($w_D$): $P_{ext}$ increases in steps. The area required is less than the single large rectangle of $w_C$ but still more than the reversible work. Thus, $|w_C|>|w_D|$.
3. General relationship:
Work done on the system (compression) is always of greater magnitude than work done by the system (expansion) for the same state change. Specifically:
$$ |w_{comp, single}|>|w_{comp, multi}|>|w_{rev}|>|w_{exp, multi}|>|w_{exp, single}| $$
Assigning the given variables:
$$ |w_C|>|w_D|>|w_B|>|w_A| $$
This matches option 3.