Finding Angular Speed of Hoop Using Energy Methods

AI Thread Summary
The discussion revolves around calculating the angular speed of a thin hoop when displaced and released from an angle β. The key equation used is the conservation of energy, equating kinetic energy to gravitational potential energy. The derived formula for angular speed is ω = √((2*g*(1 - cosβ))/R), but there is a discrepancy with the book's formula, which lacks the factor of 2. The error is attributed to the moment of inertia being incorrectly applied, as the hoop's axis of rotation is not through its center of mass. The parallel axis theorem is suggested as a solution to correct the moment of inertia calculation.
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Homework Statement



You hang a thin hoop using radius R over a nail at the rim of a the hoop. You displace it to the side (within the plane of the hoop) through angle β from its equilibrium position and let it go. Using U = M*g*y(center of mass), what is the angular speed when it returns to its equilibrium position

Homework Equations



ycm = R - R*cosβ

K = U → 0.5*I*ω^2 = M*g*y(center of mass), where I = MR^2 for thin walled and hollow cylinders.

The Attempt at a Solution



0.5*I*ω^2 = M*g*ycm

0.5*M*R^2*ω^2 = M*g*(R - R*cosβ)

ω = √((2*g*(1 - cosβ))/R)

But my book, which seems to never be wrong, has everything but the 2,
ω = √((g*(1 - cosβ))/R)

I just can't see how I could be wrong.
 
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