00:01
Hi, everybody.
00:01
So for this one, we need to find a, the speed of hanging mass.
00:07
Okay.
00:08
And as it strikes the floor, and that's what this second image right here is showing.
00:14
Okay.
00:16
You see how this mass? so what i'm going to call is we're going to call this part one.
00:21
And actually, let's do that in a different color.
00:25
Let's do that in green.
00:27
So we got one and we got two.
00:31
So for this, for this first one, which we have as one here, okay? we know that the mass is just going to focus on mge, okay? and that is because it's hanging with gravity and your kinetic energy initial is going to be zero.
00:54
Okay, because it's not moving.
00:55
And for potential energy of two and so what we can do is potential energy of two is just going to be zero because it's flying down okay and your kinetic energy of two is going to equal to one half mass times velocity squared and that's this one right here and your one plus one half the inertia and the velocity squared, your rotational velocity, which is this one right here, okay? because you have this wheel that's moving.
01:34
And now we can keep going to just make it look nicer.
01:38
We have nv squared plus one half.
01:42
Substitute capital m, r, okay, r squared times velocity squared.
01:51
Squared, okay? and what we can also do is sub in here for the rotational velocity divided by r squared, okay? and we can keep going.
02:07
And what i'm going to do is we can cross these bad boys out.
02:14
Perfect.
02:16
And now we're going to use a law of conservation.
02:19
So law conservation, we have k1.
02:21
Plus kinetic energy plus potential energy equals kinetic energy, second system, second one, okay? and so here we have zero plus mgh equals one half mb squared plus one half capital mr...