A particle at rest starts moving with a constant angular acceleration of $4\ \text{rad}/\text{s}^2$ in a circular path. At what time the magnitudes of its tangential acceleration and centripetal acceleration will be equal?
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When tangential and centripetal accelerations are equal, the total acceleration vector makes a $45^\circ$ angle with the velocity vector. Setting $\omega^2 = \alpha$ is the fastest direct condition for this scenario.
Step 1: Understanding the Question:
A particle is undergoing circular motion with a constant angular acceleration. We need to find the specific time when the tangential acceleration equals the centripetal (radial) acceleration in magnitude.
Step 2: Key Formula or Approach:
The formula for tangential acceleration is $a_t = r\alpha$.
The formula for centripetal acceleration is $a_c = r\omega^2$.
The kinematic equation for angular velocity is $\omega = \omega_0 + \alpha t$.
Step 3: Detailed Explanation:
The problem states that the magnitudes of the two accelerations are equal:
$$a_c = a_t$$
$$r\omega^2 = r\alpha$$
Cancel the radius $r$ from both sides:
$$\omega^2 = \alpha$$
We are given the angular acceleration $\alpha = 4\ \text{rad}/\text{s}^2$:
$$\omega^2 = 4 \implies \omega = 2\ \text{rad}/\text{s}$$
Since the particle starts from rest, its initial angular velocity $\omega_0 = 0$. Using the kinematic equation to find the time $t$:
$$\omega = \omega_0 + \alpha t$$
$$2 = 0 + 4t$$
$$t = \frac{2}{4} = 0.5\ \text{s}$$
Step 4: Final Answer:
The required time is $0.5\ \text{s}$, matching option (A).