The total energy (E) of an object rolling without slipping is given by:
$E = \frac{1}{2}mv_{cm}^2 + \frac{1}{2}I\omega^2$
where:
For pure rolling, $v_{cm} = R\omega$, where $R$ is the radius. Thus, $\omega = \frac{v_{cm}}{R}$. Substituting this into the energy equation:
$E = \frac{1}{2}mv_{cm}^2 + \frac{1}{2}I\left(\frac{v_{cm}}{R}\right)^2$
$E = \frac{1}{2}mv_{cm}^2\left(1 + \frac{I}{mR^2}\right)$
From the graph, we see that when $v_{cm}^2 = 4$, $E = 3$. Since the mass is 1 kg:
$3 = \frac{1}{2}(1)(4)\left(1 + \frac{I}{mR^2}\right)$
$3 = 2\left(1 + \frac{I}{mR^2}\right)$
$1 + \frac{I}{mR^2} = \frac{3}{2}$
$\frac{I}{mR^2} = \frac{1}{2}$
This means $I = \frac{1}{2}mR^2$, which is the moment of inertia of a disc.
The correct answer is (C) disc.
A uniform circular disc of radius \( R \) and mass \( M \) is rotating about an axis perpendicular to its plane and passing through its center. A small circular part of radius \( R/2 \) is removed from the original disc as shown in the figure. Find the moment of inertia of the remaining part of the original disc about the axis as given above.