The displacement \( x(t) \) of a particle undergoing simple harmonic motion is given by the equation:
\[
x(t) = A \cos(\omega t)
\]
where:
- \( A \) is the amplitude of the oscillation,
- \( \omega = \frac{2\pi}{T} \) is the angular frequency, and
- \( T \) is the time period of the motion.
Here, we are given that:
- \( A = 4 \) cm
- \( T = 4 \) s
- We need to find the displacement after \( t = \frac{1}{3} \) seconds.
Step 1: Calculate the angular frequency \( \omega \)
\[
\omega = \frac{2\pi}{T} = \frac{2\pi}{4} = \frac{\pi}{2} \, \text{rad/s}
\]
Step 2: Substitute values into the displacement equation
\[
x(t) = 4 \cos\left(\frac{\pi}{2} \times \frac{1}{3}\right)
\]
\[
x(t) = 4 \cos\left(\frac{\pi}{6}\right)
\]
\[
x(t) = 4 \times \frac{\sqrt{3}}{2} = 2\sqrt{3} \, \text{cm}
\]
Final Answer:
Therefore, the distance of the particle after \( \frac{1}{3} \) seconds is approximately:
\[
\boxed{2 \, \text{cm}}
\]