The torque \( \tau \) acting on the disc is calculated as \( \tau = F \times r \), where \( F = 4 \, \text{N} \) and \( r = 0.5 \, \text{m} \). This yields \( \tau = 4 \times 0.5 = 2 \, \text{N.m} \). The angular acceleration \( \alpha \) is determined by \( \alpha = \frac{\tau}{I} \), with \( I \) being the moment of inertia of a solid disc. The moment of inertia formula is \( I = \frac{1}{2} M R^2 \). For this disc, \( M = 2 \, \text{kg} \) and \( R = 0.5 \, \text{m} \), resulting in \( I = \frac{1}{2} \times 2 \times (0.5)^2 = 0.25 \, \text{kg.m}^2 \). Therefore, the angular acceleration is \( \alpha = \frac{2}{0.25} = 8 \, \text{rad/s}^2 \). The angular velocity \( \omega \) after 2 seconds is given by \( \omega = \alpha \times t \). Substituting the values, \( \omega = 8 \times 2 = 16 \, \text{rad/s} \). The disc acquires an angular velocity of 16 rad/s.