To solve for the change in Gibbs free energy (\( \Delta G \)) when the volume of an ideal gas is reduced isothermally, we use the formula for isothermal processes:
\[ \Delta G = nRT \ln \left( \frac{V_2}{V_1} \right) \]
Where:
\( n = 2.0 \, \text{mol}, \quad R = 8.314 \, \text{J mol}^{-1} \text{K}^{-1}, \quad T = 300 \, \text{K}
\[ \Delta G = 2.0 \, \text{mol} \times 8.314 \, \text{J mol}^{-1} \text{K}^{-1} \times 300 \, \text{K} \times \ln \left( \frac{1}{2} \right) \]
\[ \Delta G = 2.0 \times 8.314 \times 300 \times (-0.6931) \, \text{J} \]
\[ \Delta G \approx -3458.66 \, \text{J} = -3.45866 \, \text{kJ} \]
\[ \Delta G = -3.46 \, \text{kJ} \]
Finally, we confirm that the calculated value, \( -3.46 \, \text{kJ} \), falls within the provided range of \( -3.44 \, \text{kJ} \) to \( -3.46 \, \text{kJ} \).