00:01
We know that the applied force causes a torque, which gives the pulley an angular acceleration.
00:05
We know that the applied force varies with time, and if this is the case, so will the angular acceleration.
00:12
We can say that in order to find the angular velocity, we can integrate the variable acceleration to solve for this, and then we can then say the speed of a point on the rim is the tangential velocity of the rim of the wheel.
00:29
So we can set this up and say that sigma tau equaling the radius times the force tension, and this would be equalling the moment of inertia multiplied by the angular acceleration.
00:43
So we find that the angular acceleration would simply be equaling the radius times the force tension, which is, again, varying with time.
00:53
And this would be divided by the moment of inertia.
00:55
From the definition of the angular acceleration, the angular acceleration is going to be equalling the derivative of the angular velocity with respect to time t.
01:06
So we can then say that we can integrate from rather omega initial to omega final times d omega...