
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.
Two point charges 2q and q are placed at vertex A and centre of face CDEF of the cube as shown in figure. The electric flux passing through the cube is : 
Two circular discs of radius \(10\) cm each are joined at their centres by a rod, as shown in the figure. The length of the rod is \(30\) cm and its mass is \(600\) g. The mass of each disc is also \(600\) g. If the applied torque between the two discs is \(43\times10^{-7}\) dyne·cm, then the angular acceleration of the system about the given axis \(AB\) is ________ rad s\(^{-2}\).
