00:01
In this problem, we're looking at a basketball, which we model as a hollow spherical shell, which is rolling down an incline into a valley and then back up an incline on the other side.
00:12
It's starting at a height h -0, and there is an added strangeness to this problem of the incline it's rolling down, has enough friction to keep it from slipping, but the incline it's rolling up at the end has no friction.
00:30
So it will slip.
00:33
So the way to solve this is going to be to pull out our energy equations.
00:38
E equals mgh0.
00:41
And then at the bottom, it will get a velocity that we can use to figure out how high it's going to go up the other side.
00:48
So be 1 1āmv squared, i'll call that v1, plus it's rolling.
00:56
So that'll be 1 half i omega squared.
01:01
And we know that that, the moment of inertia of a holosphere is two -thirds m r squared, so we can just plug that in.
01:09
M.
01:09
V squared plus one -half times two -thirds, mr -squared.
01:19
And then the angular velocity, we can change into v squared over r -squared.
01:27
That will cancel out...