00:01
Hi everyone.
00:01
We're going to take another look at circular motion.
00:05
Okay, this time we're going to take a look at a wheel that is rolling without slipping.
00:11
So here's our wheel.
00:15
Okay, we've got an axle here, and the velocity of the axle goes like this.
00:23
And then we're going to consider point a up here, point b over here, and point c over here.
00:33
And we want to find the velocity at those points with respect to the axle.
00:41
Okay, so this would make it seem like the wheel is spinning in place.
00:49
So velocity with respect to the axle.
01:00
This looks like it's spinning in place.
01:03
Looks like it is spinning in place.
01:14
And so, and it's going to be spinning in place with angular velocity omega.
01:23
Okay.
01:24
And b is equal to omega -r.
01:33
And so we also have the v -axil is equal to omega -r.
01:42
All right.
01:44
So, b at a is omega -r, but that's just the omega -of -the -axil.
01:54
So v at the axle, sorry, v at a is equal to v at the axle.
02:04
V at a equals b at the axle.
02:11
Okay.
02:12
And now if the wheel is spinning this way, then at point a, it will be going like this.
02:24
Point b will be going like this.
02:27
And point c, the velocities will be going like that.
02:31
So at point a, it'll be equal to the velocity of the axle, and the direction, you can say it's directed to the right.
02:47
We can do the same thing at b.
02:50
That's going to be omega -r.
02:53
So v at b is v of the axle, but this time it is directed down.
03:03
And then v at c is also omega r.
03:10
So v at c is equal to the velocity of the axle.
03:16
And this one is going to be directed to the left.
03:25
Directed to the left.
03:27
All right.
03:28
So that's when we look with respect to the axle.
03:31
Let's look at what happens with respect to the ground.
03:38
So we'll draw our wheel just so we have it for reference.
03:43
Okay.
03:43
Here's our v -axil.
03:48
Okay, we've got our, sorry, that's a up there, b over here, c over here...