00:01
So here we are going to use the centripetal acceleration or centripetal force.
00:06
So here we have the centripetal force is mv squared over r is equal to the force which is a hundred or the tension here.
00:20
Now remember v and this is for r2 and v2 remember that v2 is going to be to omega 2 over, sorry, omega 2 times r2.
00:37
So if we plug that in here, we'll get that m omega 2 squared, r2 squared divided by r2 is going to be equal to the tension.
00:49
So we have m omega 2 squared, r2 is going to be the tension.
00:56
Now we need to find our second omega 2.
00:58
We note the mass of the object.
01:02
And we know it's, and we need to look for its radius.
01:06
So now we still need to find the angular velocity.
01:09
So here we're going to use a conservation of angular momentum.
01:12
Here we have l1 is going to equal l2, so the angular momentum before is equal to the angular momentum after.
01:20
So the angular momentum before is going to be one, or sorry, mr squared, or i omega, where i, the moment of inertia, is equal to m, then the r1, squared and then times omega 1...