From a circular ring of mass $M$ and radius $R$, an arc corresponding to a $ {{90}^{o}} $ sector is removed. The moment of inertia of the remaining part of the ring about an axis passing through the centre of the ring and perpendicular to the plane of the ring is $k$ times $ M{{R}^{2}} $ . Then the value of $k$ is
The moment of inertia of circular ring $ =M{{R}^{2}} $ The moment of inertia of removed sector $ =\frac{1}{4}M{{R}^{2}} $ The moment of inertia of remaining part $ =M{{R}^{2}}-\frac{1}{4}M{{R}^{2}} $ $ =\frac{3}{4}M{{R}^{2}} $ According to question, the moment of inertia of the remaining part $ =kM{{R}^{2}} $ then $ k=\frac{3}{4} $
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.