Concept:
For rotational motion with constant angular acceleration,
\[
\theta = \omega_0 t + \frac{1}{2}\alpha t^2
\]
Since the wheel starts from rest,
\[
\omega_0 = 0
\]
\[
\theta = \frac{1}{2}\alpha t^2
\]
Step 1: Angular displacement in the first \(2\) seconds.
\[
\theta_1 = \frac{1}{2}\alpha (2)^2
\]
\[
\theta_1 = 2\alpha \qquad ...(1)
\]
Step 2: Angular displacement in the first \(4\) seconds.
\[
\theta' = \frac{1}{2}\alpha (4)^2
\]
\[
\theta' = 8\alpha \qquad ...(2)
\]
Step 3: Angular displacement in the next \(2\) seconds.
\[
\theta_2 = \theta' - \theta_1
\]
\[
\theta_2 = 8\alpha - 2\alpha
\]
\[
\theta_2 = 6\alpha
\]
Step 4: Find the required ratio.
\[
\frac{\theta_2}{\theta_1} = \frac{6\alpha}{2\alpha}
\]
\[
\frac{\theta_2}{\theta_1} = 3
\]
Thus,
\[
\boxed{\frac{\theta_2}{\theta_1} = 3}
\]