Conservation of Energy and Moment of Inertia

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SUMMARY

The discussion focuses on the conservation of energy in a system involving a thin hoop with radius R, displaced at an angle Beta from its equilibrium position. The change in potential energy is calculated as MgR(1-CosB), which is set equal to the rotational kinetic energy, represented by 1/2(IW^2). The moment of inertia for the hoop is confirmed as I = MR^2, leading to the derived angular speed W = sqrt[(2g/R)(1-CosB)]. The participant seeks clarification on the presence of the factor of 2 in their equation, which is contradicted by their textbook.

PREREQUISITES
  • Understanding of potential energy and its calculation in rotational systems
  • Familiarity with rotational kinetic energy equations
  • Knowledge of moment of inertia, specifically for a thin hoop
  • Basic grasp of angular motion and its equations
NEXT STEPS
  • Review the conservation of energy principles in rotational dynamics
  • Study the derivation of the moment of inertia for various shapes, focusing on hoops and cylinders
  • Learn about the parallel axis theorem and its applications in rotational motion
  • Examine the implications of angular displacement on potential and kinetic energy transformations
USEFUL FOR

Students studying physics, particularly those focusing on mechanics and rotational dynamics, as well as educators seeking to clarify concepts related to energy conservation in rotational systems.

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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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