
The moment of inertia of a hollow sphere about its diameter axis is defined as: \( I_{\text{sphere}} = \frac{2}{3} MR^2 = M k_1^2 \), where \(k_1\) represents the hollow sphere's radius of gyration.
The moment of inertia of a solid cylinder about its diameter axis is expressed as: \( I_{\text{cylinder}} = \frac{1}{12} M(4R^2) + \frac{1}{4} MR^2 + M(2R)^2 = \frac{67}{12} MR^2 = M k_2^2 \).
The ratio of the radii of gyration is calculated as: \( \frac{k_1}{k_2} = \sqrt{\frac{\frac{2}{3}}{\frac{67}{12}}} = \sqrt{\frac{8}{67}} \).
Consequently, \(x\) equals 67.