Since the flywheel accelerates uniformly from rest, we can also solve this using average angular velocity.
The final angular velocity after 10 seconds is $\omega = \omega_0 + \alpha t = 0 + 0.5 \times 10 = 5\ \text{rad/sec}$.
Because the acceleration is constant, the average angular velocity over the interval is the mean of the initial and final values: $\omega_{avg} = \frac{\omega_0 + \omega}{2} = \frac{0+5}{2} = 2.5\ \text{rad/sec}$.
Angular displacement equals average angular velocity multiplied by time: $\theta = \omega_{avg} \times t = 2.5 \times 10 = 25$ radians.
This confirms the same result through a different route.
\[\boxed{25\ \text{radians}}\]