Step 1: Understanding the Concept:
For circular motion with constant angular acceleration \(\alpha\) starting from rest, \(\omega = \alpha t\). Tangential acceleration is \(a_t = r\alpha\) and centripetal acceleration is \(a_c = \omega^2 r\).
Step 2: Set them equal:
\[ r\alpha = \omega^2 r = \alpha^2t^2 r \Rightarrow \alpha t^2 = 1 \]
Step 3: Solve:
\[ t = \frac{1}{\sqrt\alpha} = \frac{1}{\sqrt4} = 0.5\ \text{s} \]
Step 4: Check:
At \(t = 0.5\) s, \(\omega = 4\times0.5 = 2\) rad/s, so \(a_c = 4r\) and \(a_t = 4r\). They are equal. At 0.2 s, \(a_c = 0.64r < a_t\), so option (A) is not it. Option (C).
Final Answer:
Equating r alpha with alpha squared t squared r gives t = 0.5 s.
\[ \boxed{\text{(C) }0.5\ \text{s}} \]