For the specified process where \( PV^2 = \text{constant} \), the work done by the gas during expansion is calculated via the integral: \[ W = \int_{V_1}^{V_2} P \, dV \] Given \( P = \frac{\text{constant}}{V^2} \), the work done is computed as: \[ W = \int_{V_1}^{V_2} \frac{C}{V^2} dV \] With limits \( V_1 = 1 \, \text{L} \) and \( V_2 = 2 \, \text{L} \), and the relation \( P_1 V_1^2 = P_2 V_2^2 \), the work done is determined. The pressure at \( V_2 \) is derived from the initial state: \[ P_1 V_1^2 = P_2 V_2^2 \] Consequently, the work performed by the gas is approximately 10.1 J.