Conservation of Angular Momentum - Two ants on a massless rod

AI Thread Summary
The discussion revolves around a physics problem involving the conservation of angular momentum with two ants on a massless rod. The initial and final angular momentum equations are established, indicating that the second ant must adjust its position to maintain a constant angular velocity as the first ant moves toward the center. The calculations suggest that the second ant needs to move inward as well, but there is a need for clarification on the final expression. Participants confirm the approach and suggest simplifying the equations further. The overall consensus is that the problem is straightforward, but attention to detail is crucial.
HSSN19
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Homework Statement



This is a problem about angular momentum and torque from the physics textbook Don't Panic Volume I. Attached is a screenshot of the problem.

Homework Equations



L = mr2ω

The Attempt at a Solution



The angular momentum must be conserved to keep ω constant.

Initial L = (m1 + m2)(B/4)2ω
Final L= ω(m1(B/4 - \alphat2)2 + m2x)

Therefore, x= [(m1 + m2)(B/4)2 - m1(B/4 - \alphat2)2]/m2

The second ant must move toward the center so that its distance from it is x.

What do you guys think? This is the last problem so I thought it would not be this simple. Is there something missing or should I do something more?

Thanks in advance!
 

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Can you at least state the problem. (Where's the screenshot?)
 
That's odd. I'm sure it was in the attachment... Oh well.

A massless rod of length B is pivoted at its center so that it can rotate in the horizontal plane. Two ants are riding this rod in the locations shown (both B/4 away from the center) and the rod is rotating with angular velocity ω in the counterclockwise direction, viewed from above. If ant 1, mass m1, starts (at t = 0) moving toward the center so that his distance from it is B/4 - \alphat2, what must the second ant, mass m2, do to keep the rod's angular velocity constant?
 
HSSN19 said:
Initial L = (m1 + m2)(B/4)2ω
Final L= ω(m1(B/4 - \alphat2)2 + m2x)
Looks good except that x should be x2.

Looks like you have the right idea. (And that there's not much to it.) Perhaps the expression can be simplified a bit. (If ant 1 moves toward the center, which direction must ant 2 move?)
 
Oh right, forgot the square. Thank you very much!
 
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