Disk falling while rotating round a point

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Homework Help Overview

The problem involves a disk of mass m and radius R that rotates around a point O on its circumference while falling from a vertical to a horizontal position. Participants are discussing the velocities and accelerations of the disk at the horizontal position.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to apply energy conservation to find the angular velocity and subsequently the velocities and accelerations at the horizontal position. Some participants confirm the calculations, while one points out a typographical error regarding terminology.

Discussion Status

Contextual Notes

Participants are working within the constraints of the problem statement and the equations provided, with an emphasis on ensuring clarity in terminology and calculations.

Karol
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Homework Statement


The disk of mass m and radius R is at position (a), upwards. it is free to rotate round point O on it's circumference.
If falls and reaches state (b), horizontal position.
What are the velocities and accelerations in position (b)

Homework Equations


Moment of inertia of a disk: ##I=\frac{1}{2}mR^2##
Torque of rigid body: ##M=I\alpha##
Energy of a rigid body: ##E=\frac{1}{2}I\omega^2##
Centripetal acceleration: ##a_{cen}=\frac{v^2}{R}=\omega^2 R##

The Attempt at a Solution


The angular velocity ω is from energy conservation:
$$mgR=mR^2\left( \frac{1}{2}+1 \right)\omega^2\; \rightarrow \omega^2=\frac{4g}{3R}$$
COM's velocity is ##v_{cm}=\omega R=\sqrt{\frac{4g}{3R}}R=2\sqrt{\frac{gR}{3}}##
The radial velocity from the circular motion:
$$a_{cen}=\omega^2 R=\frac{4g}{3}$$
Tangential acceleration is from the gravity:
$$M=I\alpha\rightarrow mgR=\frac{3}{2}mR^2\alpha\rightarrow\alpha=\frac{2g}{3R}$$
$$a_{tan}=R\alpha=\frac{2g}{3}$$
 

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One typo... where you wrote radial velocity you meant radial acceleration.
 
Thanks
 

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