Step 1: Understanding the Concept:
Tangential acceleration \(a_t = r\alpha\). Centripetal acceleration \(a_c = \frac{v^2}{r}\).
Step 2: Apply the condition:
Given \(a_c = \frac13a_t\):
\[ \frac{v^2}{r} = \frac{r\alpha}{3} \Rightarrow v^2 = \frac{r^2\alpha}{3} \]
Step 3: Take the root:
\[ v = r\sqrt{\frac\alpha3} \]
Option (A), \(\frac{r\alpha}{3}\), is an acceleration, not a speed. Options (B) and (D) put r inside the root, which does not give the units of speed when \(\alpha\) is in rad/s\(^2\).
Final Answer:
The speed is \(v = r\sqrt{\frac\alpha3}\), option (C).
\[ \boxed{v = r\sqrt{\frac{\alpha}{3}}} \]