00:01
Okay, so for this problem, we want to draw a free body diagram for a ball that is hanging from a string in two cases in part a, where the acceleration of this ball on a string on a train.
00:14
Part a, acceleration is zero, and then in part b, where it is equal to some constant.
00:20
So again, we're working with part a just to write an equation form what i just said.
00:25
The acceleration is going to be equal to zero.
00:28
So in other words, our ball that is hanging from a string on this train, of course, the omnipresent force, it's going to be gravity, it's going to be directed downward.
00:43
However, the ball is just sitting there hanging from the string.
00:46
It's not going anywhere.
00:47
So we know that the total net force is going to have to be equal to zero.
00:50
And that is intuitively going to be counterbalanced by the tension on the string, and that's supposed to be these two vectors are supposed to be equal to one another.
01:04
So again, in this part of the problem, r that force is equal to zero, because there's no acceleration.
01:16
Okay, contrast this with what is going on in part b, where the acceleration is equal to some non -zero constant.
01:27
So we'll just call that some constant a...