The centripetal force is supplied by tension (T), where \( T = mv^2/r \). When r and m are constant, T is directly proportional to \( v^2 \). If \( T_2 \) equals 4\( T_1 \), then \( v_2^2 \) equals 4\( v_1^2 \).
Given \( v_1 = 10 \) rpm, then \( v_2 = \sqrt{4 \times 10^2} = 20 \) rpm.

A body of mass $100 \;g$ is moving in a circular path of radius $2\; m$ on a vertical plane as shown in the figure. The velocity of the body at point A is $10 m/s.$ The ratio of its kinetic energies at point B and C is: (Take acceleration due to gravity as $10 m/s^2$)

A sportsman runs around a circular track of radius $ r $ such that he traverses the path ABAB. The distance travelled and displacement, respectively, are:
