When a particle moves in a circular path, in half the period of revolution it covers a semi-circular path. Let’s consider the motion of the particle:
- The total distance covered by the particle in half the period is half the circumference of the circle.
Thus, the distance \( d \) covered is:
\[
d = \pi R
\]
- The displacement, which is the straight-line distance between the initial and final position of the particle, is the diameter of the circle. Therefore, the displacement \( s \) is:
\[
s = 2R
\]
Hence, the displacement is \( 2R \) and the distance covered is \( \pi R \).