How Does Mass Redistribution Affect Angular Velocity?

AI Thread Summary
When the thread holding two masses on a rotating rod breaks, the masses slide to the ends, affecting the system's angular velocity. Angular momentum, defined as L=Iω, is conserved in this scenario, where I is the moment of inertia and ω is the angular velocity. As the masses move outward, the moment of inertia increases, which leads to a decrease in angular velocity to conserve angular momentum. The discussion emphasizes that while rotational energy is a factor, the conservation of angular momentum is the key principle at play. Understanding these dynamics is essential for analyzing the effects of mass redistribution on angular velocity.
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The figure attached shows two masses held together by a thread on a rod that is rotating about its center with angular velocity w. If the thread breaks, the masses will slide out to the ends of the rod. How will that affect the rod's angular velocity. Will it increase, decrease, or remain unchanged? Explain.

My attempt:

w= V/R

Neither of the two variables change, wouldn't it remain unchanged?

Thanks!
 

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How do you know that neither variable changes? What do you consider a conserved quantity, and why ?
 
Radius remains the same. Velocity will change I guess. It has something to do with angular momentum may be?
Can you guide me here?
 
Radius remains the same ? I read that the masses will slide to the ends of the rod ? What is it that we call radius here ?
 
Hint: Rotational energy is conserved, but what happens to the moment of inertia of the system?

The rotational energy is ##E=\frac{1}{2}I\omega^{2}##, where ##I## is the moment of inertia and ##\omega## the angular velocity.

EDIT: Just to be sure, let's rather say that angular momentum, ##L=I\omega## is the quantity that is conserved... The answer is same, anyway.
 
Last edited:
hilbert2 said:
Hint: Rotational energy is conserved, but what happens to the moment of inertia of the system?

The rotational energy is ##E=\frac{1}{2}I\omega^{2}##, where ##I## is the moment of inertia and ##\omega## the angular velocity.

EDIT: Just to be sure, let's rather say that angular momentum, ##L=I\omega## is the quantity that is conserved... The answer is same, anyway.
Yes, you must use angular momentum here, not energy - for two reasons.
First, we don't know whether there is friction. Second, we don't know how much KE there is in the radial motion.
 
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