Given the relation \(PV^{3/2} = \text{constant}\), the work done \(W\) is defined as:
\[ W = \int P \, dV \]
Substituting \(P = \frac{K}{V^{3/2}}\) from the given relation, where \(K\) is a constant:
\[ W = \int_{V_1}^{V_2} \frac{K}{V^{3/2}} \, dV \]
Upon integration, the work done is calculated as:
\[ W = \left[ -\frac{2K}{V^{1/2}} \right]_{V_1}^{V_2} = 2(P_1V_1 - P_2V_2) \]
- If the work done by the gas is required:
\[ W = 2(P_1V_1 - P_2V_2) \quad \text{(Option 1)} \]
- If the work done on the gas (by an external agent) is required:
\[ W = 2(P_2V_2 - P_1V_1) \quad \text{(Option 2)} \]