We know that angular momentum of the body is given by $L=I \omega$ or $L=I\times \frac{2 \pi}{\tau}$ or $L \propto \frac{1}{T}$ $\Rightarrow \frac{L_1}{L_2}=\frac{T_2}{T_1}$ $\frac{L}{L_2}=\frac{2T}{T} (As ,T_2=2T)$ so,$L_2=\frac{L}{2}$ Thus, on doubling the time period, angular momentum of body becomes half.
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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.