The total energy is given by \( \text{Total energy} = \frac{-GMm}{2(2R)} \). Upon adding energy \( \frac{10^4R}{6} \), the equation becomes \( \frac{-GMm}{4R} + \frac{10^4R}{6} = \frac{-GMm}{2r} \), where \( r \) denotes the new radius of revolution and \( g = \frac{GM}{R^2} \). Substituting \( g \) and \( m = 10^3\, \text{kg} \), we get \( -\frac{mgR}{4} + \frac{10^4R}{6} = -\frac{mgR^2}{2r} \). This simplifies to \( -\frac{10^3 \times 10 \times R}{4} + \frac{10^4R}{6} = -\frac{10^3 \times 10 \times R^2}{2r} \). Further simplification leads to \( -\frac{1}{4} + \frac{1}{6} = -\frac{R}{2r} \). Solving for \( r \) yields \( r = 6R \).

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:
