Translational kinetic energy, $K_{T}=\frac{1}{2} m v^{2}$ Rotational kinetic energy $V_{1}$ $K_{R}=\frac{1}{2} I \omega^{2}=\frac{1}{2} \times \frac{2}{5} m R^{2} \times \frac{v^{2}}{R^{2}}$ $=\frac{1}{5} m v^{2}$ $\frac{K_{T}}{K_{R}}=\frac{\frac{1}{2} m v^{2}}{\frac{1}{5} m v^{2}}$ $=\frac{5}{2}=2.5$
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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.