Releasing a hollow cylinder on a rotating disk

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Homework Help Overview

The discussion revolves around the dynamics of a hollow cylinder released on a rotating disk, focusing on the conservation of angular momentum and the effects of friction. Participants are analyzing the conditions under which angular momentum is conserved and the implications of slipping versus friction in this context.

Discussion Character

  • Exploratory, Assumption checking, Conceptual clarification

Approaches and Questions Raised

  • Participants are examining the conservation of angular momentum, questioning the role of friction and whether it introduces external torque. There are discussions about the correct interpretation of slipping and the implications for angular velocity.

Discussion Status

The discussion is active, with participants providing feedback on each other's reasoning and clarifying points about the conditions of the problem. Some guidance has been offered regarding the interpretation of angular velocity and the nature of forces involved.

Contextual Notes

There is an ongoing debate about the presence of friction and its impact on the conservation of angular momentum, with some participants suggesting that friction could imply external torque, while others argue it is internal to the system.

archaic
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Homework Statement
A uniform disk has a mass of 3.8 kg and a radius of 0.52 m. The disk is mounted on frictionless bearings and is used as a turntable. The turntable is initially rotating at 50 rpm. A thin-walled hollow cylinder has the same mass and radius as the disk. It is released from rest, just above the turntable, and on the same vertical axis. The hollow cylinder slips on the turntable for 0.20 s until it acquires the same final angular velocity as the turntable. What is the final angular momentum of the system?
Relevant Equations
##L=I\omega##
There is no net external torque since the cylinder is slipping (no friction), so the angular momentum should be conserved.
$$L_f=\frac 12MR^2\omega_i=\frac 12\times3.8\times0.52^2\times50\times\frac{2\pi\times0.52}{60}$$
 
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I think you mean "since the disk is slipping (no friction)".
Your reasoning is right, but you seem to have an extra 0.52 in there.
 
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haruspex said:
I think you mean "since the disk is slipping (no friction)".
Your reasoning is right, but you seem to have an extra 0.52 in there.
Right, I should have the velocity in radians per second. Thank you.
 
haruspex said:
I think you mean "since the disk is slipping (no friction)".
The hollow cylinder slips on the turntable
 
archaic said:
The hollow cylinder slips on the turntable
Yes, but with friction, or they would not converge to the same angular velocity.
 
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archaic said:
Right, I should have the velocity in radians per second. Thank you.
I'm not sure how that is a response to my post. What do you have as the answer now?
 
haruspex said:
I'm not sure how that is a response to my post. What do you have as the answer now?
$$\frac 12\times3.8\times0.52^2\times50\times\frac{2\pi}{60}$$
haruspex said:
Yes, but with friction, or they would not converge to the same angular velocity.
This actually bothered me a bit. I went with conservation of angular momentum since I saw no other way of doing the problem. Doesn't friction imply a net external torque on the disk and the cylinder?
 
archaic said:
Doesn't friction imply a net external torque on the disk and the cylinder?
The system, the angular momentum of which is conserved, is the turntable plus the hollow cylinder. There is no external torque acting on the system; friction is internal. This is the rotational equivalent of a one dimensional inelastic collision where two blocks collide and stick together after the collision.
 

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