For an isothermal, reversible expansion of an ideal gas, the product of pressure and volume remains constant: \[ P_1 V_1 = P_2 V_2. \] Given \( V_1 = V \) and \( V_2 = 2V \), we have: \[ P V = P_2 \cdot 2V. \] Solving for \( P_2 \): \[ P_2 = \frac{P}{2}. \] Thus, the final pressure is: \[ \boxed{\frac{P}{2}}. \]