The moment of inertia of a disc of mass $M$ and radius $R$ about an axis, which is tangential to the circumference of the disc and parallel to its diameter is
The moment of inertia of a disc about its
diameter (i.e. $z$ axis) is $I_{0}=\frac{MR^{2}}{4}$$\therefore$ According to parallel axis theorem, moment of inertia about the required axis (i.e. z' axis) is
$I=I_{0}+MR^{2}$$=\frac{MR^{2}}{4}+MR^{2}=\frac{5MR^{2}}{4}$
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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.