Step 1: Position, Velocity, and Acceleration.
The displacement of the particle is given by:
\[
x = A \sin \left( 50t + \frac{\pi}{3} \right)
\]
The velocity \( v \) is obtained by differentiating the displacement with respect to time:
\[
v = \frac{dx}{dt} = 50A \cos \left( 50t + \frac{\pi}{3} \right)
\]
The acceleration \( a \) is the derivative of velocity with respect to time:
\[
a = \frac{dv}{dt} = -50^2 A \sin \left( 50t + \frac{\pi}{3} \right)
\]
Step 2: Determining the time when velocity becomes zero (\( t_1 \)).
Velocity becomes zero when the cosine term is zero:
\[
\cos \left( 50t + \frac{\pi}{3} \right) = 0
\]
The general solution is:
\[
50t + \frac{\pi}{3} = \frac{\pi}{2} + n\pi
\]
Solving for \( t \):
\[
50t = \frac{\pi}{2} + n\pi - \frac{\pi}{3}
\]
\[
50t = \frac{3\pi}{6} - \frac{2\pi}{6} + n\pi
\]
\[
50t = \frac{\pi}{6} + n\pi
\]
\[
t_1 = \frac{\pi}{300} + \frac{n\pi}{50}
\]
The smallest positive value occurs when \( n = 0 \):
\[
t_1 = \frac{\pi}{300} \, \text{sec}
\]
Step 3: Determining the time when acceleration becomes zero (\( t_2 \)).
Acceleration becomes zero when the sine term is zero:
\[
\sin \left( 50t + \frac{\pi}{3} \right) = 0
\]
The general solution is:
\[
50t + \frac{\pi}{3} = n\pi
\]
Solving for \( t \):
\[
50t = n\pi - \frac{\pi}{3}
\]
\[
t_2 = \frac{n\pi}{50} - \frac{\pi}{150}
\]
The smallest positive value occurs when \( n = 1 \):
\[
t_2 = \frac{\pi}{75} \, \text{sec}
\]
Final Answer:
\( t_1 = \frac{\pi}{300} \, \text{sec}, \quad t_2 = \frac{\pi}{75} \, \text{sec} \).