A solid sphere of mass M, radius R has moment of inertia 'I' about its diameter. It is recast into a disc of thickness 't' whose moment of inertia about an axis passing through its edge and perpendicular to its plane remains 'I'. Radius of the disc will be
Show Hint
Mass cancels out completely when recasting shapes! Setting up the raw coefficients directly ($\frac{2}{5}R^2 = \frac{3}{2}R'^2$) lets you cross-multiply and take the square root to isolate the new radius fraction in seconds.
The moment of inertia of a solid sphere about its diameter is:
$$I_{\text{sphere}} = \frac{2}{5}MR^2$$
Let the radius of the recast disc be $R'$. The moment of inertia of a flat disc about its central axis perpendicular to its plane is $\frac{1}{2}MR'^2$. Applying the parallel axis theorem ($I = I_{\text{cm}} + Md^2$) to find the moment of inertia about its edge axis ($d = R'$):
$$I_{\text{disc}} = \frac{1}{2}MR'^2 + MR'^2 = \frac{3}{2}MR'^2$$
Since the moment of inertia remains unchanged ($I_{\text{sphere}} = I_{\text{disc}}$):
$$\frac{2}{5}MR^2 = \frac{3}{2}MR'^2$$
$$\frac{2}{5}R^2 = \frac{3}{2}R'^2 \implies R'^2 = \frac{4}{15}R^2$$
$$R' = \frac{2R}{\sqrt{15}}$$
Final Answer:
The radius of the disc will be $\frac{2R}{\sqrt{15}}$, which corresponds to option (C).