Moment of inertia of big drop is $I=\frac{2}{5} M R^{2}$
When small droplets are formed from big drop volume of liquid remain same
$n \frac{4}{3} \pi r^{3}=\frac{4}{3} \pi R^{3}$
$\Rightarrow n^{1 / 3} r=R$ as $n=8 \Rightarrow r=\frac{R}{2}$
Mass of each small droplet $=\frac{M}{8}$
$\therefore$ Moment of inertia of each small droplet
$=\frac{2}{5}\left[\frac{M}{8}\right]\left[\frac{R}{2}\right]^{2}$
$=\frac{1}{32}\left[\frac{2}{5} M R^{2}\right]=\frac{I}{32}$
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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.