The moment of inertia for a solid sphere along its diameter is
$I_{\text {diameter }}=\frac{2}{5} M R^{2}$
Moment of inertia about a tangent touching to its surface,
$I_{\text {tangent }}=I_{\text {diameter }}+M R^{2}$
(using theorem of parallel axes)
$=\frac{2}{5} M R^{2}+M R^{2}$$=\frac{7}{5} M R^{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.