The work done by the applied force is converted into rotational kinetic energy of the disc. The torque \( \tau \) acting on the disc is given by:
 
 \[
 \tau = F \cdot R
 \]
 
 Where:
 - \( F = 4 \, \text{N} \) is the force,
 - \( R = 0.5 \, \text{m} \) is the radius of the disc.
 
 The angular acceleration \( \alpha \) is given by:
 
 \[
 \alpha = \frac{\tau}{I}
 \]
 
 Where \( I \) is the moment of inertia of the disc, and for a solid disc:
 
 \[
 I = \frac{1}{2} m R^2
 \]
 
 Substituting values:
 
 \[
 I = \frac{1}{2} \times 2 \times 0.5^2 = 0.5 \, \text{kg m}^2
 \]
 
 Now, calculate the torque:
 
 \[
 \tau = 4 \times 0.5 = 2 \, \text{N m}
 \]
 
 Thus, the angular acceleration is:
 
 \[
 \alpha = \frac{2}{0.5} = 4 \, \text{rad/s}^2
 \]
 
 The angular velocity \( \omega \) at the end of 2 seconds is:
 
 \[
 \omega = \alpha t = 4 \times 2 = 8 \, \text{rad/s}
 \]
 
 Thus, the angular velocity acquired by the disc at the end of 2 seconds is 16 rad/s.