The torque \( \tau \) acting on the disc is given by:
\[
\tau = F \times r
\]
Where:
- \( F = 4 \, \text{N} \) (force applied),
- \( r = 0.5 \, \text{m} \) (radius of the disc).
Thus:
\[
\tau = 4 \times 0.5 = 2 \, \text{N.m}
\]
Now, the angular acceleration \( \alpha \) is given by the relation:
\[
\alpha = \frac{\tau}{I}
\]
Where \( I \) is the moment of inertia of a solid disc:
\[
I = \frac{1}{2} M R^2
\]
For this disc:
- \( M = 2 \, \text{kg} \) (mass of the disc),
- \( R = 0.5 \, \text{m} \) (radius of the disc).
So, the moment of inertia is:
\[
I = \frac{1}{2} \times 2 \times (0.5)^2 = 0.25 \, \text{kg.m}^2
\]
Now, the angular acceleration is:
\[
\alpha = \frac{2}{0.25} = 8 \, \text{rad/s}^2
\]
Finally, the angular velocity \( \omega \) at the end of 2 seconds is given by:
\[
\omega = \alpha \times t
\]
Substituting the values:
\[
\omega = 8 \times 2 = 16 \, \text{rad/s}
\]
Thus, the angular velocity acquired by the disc is 16 rad/s.