00:01
So in this case we have this pulley rotated about its center and it weighs 40 kilograms.
00:06
It has a radius of 0 .2 meters and we have a force that's applied that's always acting tangential.
00:13
So whether it's actually a force that's moving on here or maybe a cable that is unwrapping around here, but it's always a tangential force.
00:22
And we're asked to figure out, what are we asked to figure out? the magnitude of velocity of the tangential velocity on the point of the rim after the rim after the disk has spun through 0 .2 revolutions and that is 1 .5, 1 .427 radiance.
00:42
So again, we need to remember to convert our angle from revolutions to radians.
00:48
Now, we know from kinematics that the velocity, angular velocity squared, equals the initial angular velocity square plus two times the angular acceleration minus the change in angle.
01:04
And since i'm just going to measure the start as initial angle at zero, then this is just the change in angle.
01:12
For a uniform disk, j, and i'm going to use j here instead of i, that's from more of an engineering point of view because in mechanical engineering, i is an area moment and j is a mass moment.
01:25
And those things get really, really confused later on in higher level classes.
01:33
And so an area moment has units of length to the fourth.
01:41
And so when you start talking about beams in engineering, you're going to see i a lot.
01:47
And then you're going to see j a lot in dynamics class because to distinguish the two, engineers we use j for the mass moment.
01:58
So i'm going to use j.
02:01
And that's 0 .800 kilogram meter squared.
02:05
So the angular acceleration, so it just, you know, torque equals j times the angle of acceleration because it's the angle of acceleration is the torque divided by j...