The work done on the disc is:
\[
W = F \cdot d = 4 \times 2 \pi \times 0.5 = 4 \pi \, \text{J}
\]
The work done on the disc is also equal to the change in rotational kinetic energy:
\[
K = \frac{1}{2} I \omega^2
\]
For a solid disc, the moment of inertia \( I \) is \( \frac{1}{2} m r^2 \), so:
\[
K = \frac{1}{2} \times \frac{1}{2} \times 2 \times (0.5)^2 \times \omega^2 = \frac{1}{4} \times \omega^2
\]
Equating the work and kinetic energy:
\[
4 \pi = \frac{1}{4} \times \omega^2
\]
Solving for \( \omega \):
\[
\omega = 16 \, \text{rad/s}
\]
Thus, the angular velocity acquired by the disc is \( 16 \, \text{rad/s} \).