00:01
So, we are given a horizontal disk.
00:03
So, let me draw a horizontal disk.
00:09
This is the horizontal disk and this is its center point.
00:14
The axis passes through its center and vertically.
00:23
So, this is my axis of rotation.
00:27
Axis of rotation.
00:36
We are also given that the disk rotates constant angular velocity.
00:57
Let me say this angular velocity is omega.
01:04
And we calculate omega in radian per second.
01:06
So, this is given to us.
01:09
Now, if we take a point p exactly between the point o and point q.
01:20
Point q is on the rim.
01:24
So, point p is midway between o and q.
01:30
What we can say about this? first, for linear acceleration, we know that the linear acceleration a is r times alpha.
01:53
Where alpha is angular acceleration.
02:05
And also, alpha is change in angular velocity divided by time.
02:17
But here, the angular velocity is constant...