The moment of inertia of a disc about its diameter is \( I_{\text{disc}} = \frac{1}{4} M R^2 \), where \( M \) is the disc's mass and \( R \) is its radius.
Step 1: Moment of inertia of the solid sphere about PQ
The moment of inertia of a solid sphere about its center is \( I_{\text{sphere}} = \frac{2}{5} M R^2 \). Applying the parallel axis theorem for rotation about point \( P \), with distance \( d=R \), the moment of inertia is \( I_{\text{sphere, PQ}} = I_{\text{sphere}} + M d^2 = \frac{2}{5} M R^2 + M R^2 = \frac{7}{5} M R^2 \).
Step 2: Moment of inertia of the spherical shell about PQ
The moment of inertia of a spherical shell about its center is \( I_{\text{shell}} = \frac{2}{3} M R^2 \). Using the parallel axis theorem for rotation about PQ, the moment of inertia is \( I_{\text{shell, PQ}} = \frac{2}{3} M R^2 + M R^2 = \frac{5}{3} M R^2 \).
Step 3: Moment of inertia of the system about PQ
The total moment of inertia of the system is the sum of individual moments of inertia: \( I_{\text{total}} = I_{\text{disc, PQ}} + I_{\text{sphere, PQ}} + I_{\text{shell, PQ}} = \frac{1}{4} M R^2 + \frac{7}{5} M R^2 + \frac{5}{3} M R^2 \).
Step 4: Simplifying the total moment of inertia
With a common denominator of 60, the total moment of inertia simplifies to \( I_{\text{total}} = \frac{15}{60} M R^2 + \frac{84}{60} M R^2 + \frac{100}{60} M R^2 = \frac{199}{60} M R^2 \).
Step 5: Comparing with the given moment of inertia
Given that the moment of inertia about PQ is \( \frac{x}{15} I \), where \( I = \frac{1}{4} M R^2 \), we have \( \frac{x}{15} I = \frac{199}{60} M R^2 \). Substituting \( I = \frac{1}{4} M R^2 \) yields \( \frac{x}{60} = \frac{199}{60} \), thus \( x = 199 \).
The value of \( x \) is 199.