Kinetic energy of sphere
$K_{r_{0}}=\frac{1}{2} I \omega^{2}$
$\therefore$ Moment of inertia of sphere,
$I=\frac{2}{5} M R^{2}$
$\therefore$ Rotational kinetic energy of sphere
$K_{r_{0}}=\frac{1}{2} M R^{2} \omega^{2}$
Total energy of sphere
$K_{r_{0}} =\frac{1}{2} I \omega^{2}+\frac{1}{2} M v^{2} $
$=\frac{1}{2} \times \frac{2}{5} M R^{2} \omega^{2}+\frac{1}{2} M R^{2} \omega^{2} $
$=M R^{2} \omega^{2}\left(\frac{1}{5}+\frac{1}{2}\right) $
$=\frac{7}{10} M R^{2} \omega^{2}$
Total energy of sphere $K_{t_0}=\frac{7}{10} M R^{2} \omega^{2}$
$\frac{K_{r_{0}}}{K_{t_{0}}}=\frac{\frac{1}{5} M R^{2} \omega^{2}}{\frac{7}{10} M R^{2} \omega^{2}}=\frac{2}{7}$
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Top Questions on System of Particles & Rotational Motion
The system of particles refers to the extended body which is considered a rigid body most of the time for simple or easy understanding. A rigid body is a body with a perfectly definite and unchangeable shape.
The distance between the pair of particles in such a body does not replace or alter. Rotational motion can be described as the motion of a rigid body originates in such a manner that all of its particles move in a circle about an axis with a common angular velocity.
The few common examples of rotational motion are the motion of the blade of a windmill and periodic motion.