For spheres each of mass $M$ and radius $R$ are placed with their centres on the four comers $A, B, C$ and $D$ of a square of side $b$. The spheres $A$ and $B$ are hollow and $C$ and $D$ are solids. The moment of inertia of the system about side $AD$ of square is
Moment of inertia of a hollow sphere of radius $R$ about the diameter passing through $D$ is $I_{A}=\frac{2}{3} M R^{2} \ldots(i)$ Moment of inertia of sol id sphere about diameter $I_{B}=\frac{2}{5} M R^{2} \ldots(i i)$ $\therefore$ Moment of inertia of whole system about side $A D=I_{A}+I_{D}+I_{B}+I_{C} $ $=\frac{2}{3} M R^{2}+\frac{2}{5} M R^{2}+\left(M b^{2}+\frac{2}{3} M R^{2}\right)+\left(M b^{2}+\frac{2}{5} M R^{2}\right)$ $=\frac{32}{15} M R^{2}+2 M b^{2}$
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Top Questions on System of Particles & Rotational Motion
The system of particles refers to the extended body which is considered a rigid body most of the time for simple or easy understanding. A rigid body is a body with a perfectly definite and unchangeable shape.
The distance between the pair of particles in such a body does not replace or alter. Rotational motion can be described as the motion of a rigid body originates in such a manner that all of its particles move in a circle about an axis with a common angular velocity.
The few common examples of rotational motion are the motion of the blade of a windmill and periodic motion.