I have two problems regarding rotational motion.
1) Use conservation of energy to determine the angular speed of the spool shown in Figure P8.36 after the 3.00 kg bucket has fallen 4.35 m, starting from rest. The light string attached to the bucket is wrapped around the spool and does not slip as it unwinds.
I initially set it up to solve it as a conservation of energy problem by setting PE = mgh = (3)(9.81)(4.35) = 128.0205
I then equated this to (1/2)(mbucket)(vfinal(bucket) + (1/2)(Ispool(wspool2)
I then was unsure where to proceed, so if anyone could help me out that'd be great.
I did however see another means of solving it (or so I think) not using conservation of energy.
I solved for the torque of the spool by (0.6)(3)(9.81) = (r)(Fbucket) = 17.658
I then solved for the angular acceleration by 17.658 = (5)(0.6)2(a) and got a = 9.81
Since the circumference = 2(pi)(r), I got the circumference = 2(pi)(0.6) = that many meters / rotation
The bucket fell 4.35m, so that = 1.153873337 rotations, which = 7.25 radians, the change in theta.
I then used the equation w2 = wi2(a)(change in theta) to get (2)(9.81)(7.25) = w2
So w = 11.92665, however this answer was wrong (by less than 10%).
2) A potter's wheel having a radius 0.48 m and a moment of inertia 12.7 kg·m2 is rotating freely at 47 rev/min. The potter can stop the wheel in 5.5 s by pressing a wet rag against the rim and exerting a radially inward force of 70 N. Find the effective coefficient of kinetic friction between the wheel and the wet rag.
I solved for a by dividing wi by the time, then multiplied a by I to get the force of friction, -5.455175723.
I then set uk = (Ffric)(FN) = (-5.455175723) / (-70) = .07793, but this was wrong.
Any help would be greatly appreciated, thanks!
Nick