Conservation of Energy and Moment of Inertia

AI Thread Summary
The discussion centers on calculating the angular speed of a thin hoop when it returns to its equilibrium position after being displaced. The potential energy change is expressed as MgR(1-CosB), where R is the radius and B is the angle of displacement. This change in potential energy is set equal to the rotational kinetic energy, leading to the equation MgR(1-CosB) = 1/2 (MR^2)(W^2). The user is confused about the presence of the factor of 2 in their derived formula for angular speed, W = sqrt[(2g/R)(1-CosB)], as their textbook suggests it should not be there. The conversation highlights the importance of correctly applying the conservation of energy principle and the parallel axis theorem in rotational dynamics.
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Homework Statement



(Q) You hang a thin hoop with Radius R over a nail at the rim of the hoop. You displace it to the side through an angle B (Beta) from its equilibrium position and let it go. What is its angular speed when it returns through its equilibrium position?

Homework Equations



Change in Potential energy = Mghcm where hcm is the distance moved by the center of mass.

Rotational Kinetic Energy = 1/2 (IW^2) where W is the angular speed.


The Attempt at a Solution



The distance upward moved by the center of mass = R-RCosB.

Thus, change in potential energy = MgR(1-CosB).

This should be equal to the rotational Kinetic energy which is 1/2(IW^2).

Since this is a hoop(not sure what that means), I = MR^2 (Hope I am correct!)

Thus, MgR(1-CosB) = 1/2 (MR^2)(W^2)
Thus, W = sqrt [(2g/R)(1-CosB)].

Unfortunately, according to my book, the 2 isn't supposed to be there. Can someone please help me figure out why this is so? Thank-you very much!
 
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Thanks a ton! That was really a wake-up call. I can't believe how careless I've been. Thanks again!
 
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