Question:

A ball rolls without slipping. The radius of gyration of the ball about an axis passing through its center of mass is $K$. If radius of the ball be $R,$ then the fraction of total energy associated with its rotational energy will be

Updated On: Jun 20, 2022
  • $\frac{K^2}{K^2 +R^2}$
  • $\frac{R^2}{K^2 +R^2}$
  • $\frac{K^2 +R^2}{R^2}$
  • $\frac{K^2}{R^2}$
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The Correct Option is A

Solution and Explanation

In rolling without slipping, total energy of ball is the sum of its translational and rotational energy.
Kinetic energy of rotation
$K_{rot}=\frac{1}{2}I\omega^2=\frac{1}{2}MK^2\frac{v^2}{R^2}$
where $K$ is radius of gyration.
Kinetic energy of translation,
$K_{\text{trans}}=\frac{1}{2}Mv^2$
Thus, total energy
$E=K_{rot}+K_{\text{trans}}$
$=\frac{1}{2}MK^2\frac{V^2}{R^2}+\frac{1}{2}Mv^2$
$=\frac{1}{2}Mv^2\left(\frac{K62}{R^2}+1\right)$
$=\frac{1}{2}\frac{Mv^2}{R^2}(K^2+R^2)$
Hence $\frac{K_{rot}}{K_{trans}}=\frac{\frac{1}{2}MK^2\frac{v^2}{R^2}}{\frac{1}{2}\frac{Mv^2}{R^2}(K^2+R^2)}$
$=\frac{K^2}{K^2+R^2}$
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Concepts Used:

System of Particles and Rotational Motion

  1. 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.
  2. 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.
  3. The few common examples of rotational motion are the motion of the blade of a windmill and periodic motion.