00:01
Hello everyone, we are going to understand this question here given in the question.
00:10
Mass of disk, mass of disc, that is m, radius of disc, radius of disc, that is r.
00:32
So, movement of inertia of disk about the diameter, movement of inertia of disc, about diameter, about center of mass, about center of mass.
01:08
That is represented by i -c -o -m, which is equal to mr -square upon 4.
01:23
So, using the parallel axis theorem, now using parallel axis theorem, we can write i is equal to i -c -o -m plus m into d -square.
01:52
Here, value of d is r...