U.S. Physics Olympiad F=ma 2008: Problem 12

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Homework Help Overview

The problem involves a uniform disk rotating at a fixed angular velocity, examining the change in kinetic energy when the axis of rotation is shifted from the center to the edge of the disk. The subject area includes concepts of rotational dynamics and moment of inertia.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the moment of inertia for the disk about different axes and how it affects kinetic energy. There are attempts to apply the parallel axis theorem and clarify the correct expressions for moment of inertia.

Discussion Status

Participants are actively engaging with the problem, offering insights into the moment of inertia and its implications for kinetic energy. Some have provided calculations and reasoning, while others are seeking clarification on specific steps and concepts.

Contextual Notes

There appears to be some confusion regarding the application of the parallel axis theorem and the correct moment of inertia for the disk, which is being addressed in the discussion.

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12. A uniform disk rotates at a fixed angular velocity on an axis through its center normal to the plane of the disk, and has kinetic energy E. If the same disk rotates at the same angular velocity about an axis on the edge of the disk (still normal to the plane of the disk), what is its kinetic energy?
(a) 1/2E
(b) 3/2E
(c) 2E
(d) 3E
(e) 4E

Answer: D

Relevant Equations: KE= 1/2 I x w^2, I=MR^2

Attempt at Solving: Io=MR^2, In=4MR^2, thus KE=4 (1/2 I x w^2)= 4E

Can someone please explain why the answer is 3E? I really appreciate your assistance! Thanks!
 
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Hi Rittted, welcome to PF.
Moment of inertia of a uniform disc about an axis through cm perpendicular to the plane is 1/2*M*R^2.
Using theorem of parallel axis, you can find the moment of inertia about an axis on the edge of the disk.
 
Note that for a uniform disk, I = (1/2) m r^2, not m r^2.

Furthermore, the parallel axis theorem may come in handy.

Note that the kinetic energy is linear in I ([itex]E = \tfrac{1}{2} I \omega^2[/itex]) so you only need to show that [itex]I = 3 I_\mathrm{cm}[/itex], where I is the moment of inertia about the axis on the edge, and [itex]I_\mathrm{cm} = \tfrac{1}{2} m r^2[/itex]
 
Thanks for all of the help guys! I really appreciate it!

So I= 1/2mr^2 + mr= 3/2mr^2=3I

and

KE= 3E

Great!
 

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