The time period of the disc is \(2 \pi \sqrt{(3 r / 2 g )}\)
We know that the time period of an object,
\(T =2 \pi \sqrt{(I / mgL )}\)
where,
\(I=\) moment of inertia from the suspended point
\(L =\) distance of its centre from suspended point \(= r\)
we know that, the moment of inertia of disc about its centre \(= mr ^2 / 2\)
using parallel axis theoram the moment of inertia from a point in its periphery,
\(I = mr ^2+ mr ^2 / 2=3 mr ^2 / 2\)
putting the values in the above equation we get,
\(2 \pi \sqrt{\left(3 mr ^2 / 2 mgr \right)}\)
\(=2 \pi \sqrt{(3 r / 2 g )}\)
therefore, the time period of the disc is \(2 \pi \sqrt{(3 r / 2 g )}\)