00:01
In this problem, we're going to talk about circular motion.
00:03
So let's say that we have a circular trajectory of radius zr, and we want to describe the dynamics of this trajectory.
00:11
So it can decompose the acceleration of a particle in this trajectory into two components.
00:16
One of them is this intrepital acceleration, and it's equal to omega square times r, where omega is the angular speed.
00:25
And this intrepital acceleration accounts for the change in direction of the trajectory.
00:31
While the tangential acceleration accounts for the change in speed.
00:38
And it's equal to the derivative of the speed with respect to time.
00:45
So in our problem, we have to suppose that we have a ball attached to a string, and the string is one meter long.
01:00
And our goal is to find what is the minimum value of the angular speed, omega -min, such that the ball is able to complete a full circle.
01:17
So we want the ball to complete a full circle.
01:22
And that means that at the top of the trajectory, the forces that act on the ball are the gravitational force and the tension from the string.
01:39
So the total force is t plus m...