Finding Angular Speed of Hoop Using Energy Methods

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SUMMARY

The discussion centers on calculating the angular speed of a thin hoop when displaced and released from an angle β. The key equation derived is ω = √((2*g*(1 - cosβ))/R), where R is the radius of the hoop and g is the acceleration due to gravity. A discrepancy arises with a textbook solution that omits the factor of 2, leading to ω = √((g*(1 - cosβ))/R). The moment of inertia used is I = MR², applicable for thin-walled hollow cylinders, but the axis of rotation must be considered through the center of mass, necessitating the use of the parallel axis theorem for accurate calculations.

PREREQUISITES
  • Understanding of angular motion and energy conservation principles
  • Familiarity with moment of inertia calculations for thin-walled hollow cylinders
  • Knowledge of the parallel axis theorem
  • Basic trigonometry, specifically the cosine function
NEXT STEPS
  • Review the parallel axis theorem and its applications in rotational dynamics
  • Study energy conservation in rotational motion, focusing on kinetic and potential energy relationships
  • Explore the derivation of angular speed formulas for various shapes and mass distributions
  • Practice problems involving angular motion of hoops and cylinders in different configurations
USEFUL FOR

Physics students, mechanical engineers, and educators seeking to deepen their understanding of rotational dynamics and energy methods in mechanics.

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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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