Moment of Inertia of a Thin Rod about its Center

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The discussion centers on calculating the angular acceleration of a thin rod with two balls attached, focusing on the scenario where one ball detaches. The net torque is determined to be the product of the ball's mass, gravitational acceleration, and the distance from the pivot. The moment of inertia must account for both the rod and the remaining ball, leading to confusion about the role of the rod's mass in the calculations. The correct angular acceleration is derived as 16.333 rad/s², highlighting the importance of including all mass contributions in the moment of inertia. Understanding the dynamics of the system requires careful consideration of how mass distribution affects angular motion.
PsychonautQQ
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Homework Statement


A thin, uniform, 3.8kg bar, 80cm long has two 2.5 kg balls glued on at either end. It is supported horizontally by a thin, horizontal, frictionless axle passing through its centers and perpendicular to the bar. Suddenly the right hand ball becomes detached and falls off, but the other ball remains glued to the bar. Find the angular acceleration of the bar just after the ball falls off.



The Attempt at a Solution


So the net torque will just be m_ball*g*r because each side of the bar will cancel each other out. So if we set
m_ball*g*r = I(alpha) = m_ball*(r^2)*(alpha)

so
g/r = (alpha)
(9.8)/4 = (alpha)
and I get 24.5 which is wrong by a factor of 2/3 (correct answer is 16.333)

The question is asking for the bars angular acceleration and I'm giving It the balls, but wouldn't they be equal?
 
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Isn't it strange that the mass of the bar does not enter the equations? Think for a second that the bar is very massive or is very light; would they behave in exactly the same way under equal torques?
 
PsychonautQQ said:

Homework Statement


A thin, uniform, 3.8kg bar, 80cm long has two 2.5 kg balls glued on at either end. It is supported horizontally by a thin, horizontal, frictionless axle passing through its centers and perpendicular to the bar. Suddenly the right hand ball becomes detached and falls off, but the other ball remains glued to the bar. Find the angular acceleration of the bar just after the ball falls off.



The Attempt at a Solution


So the net torque will just be m_ball*g*r because each side of the bar will cancel each other out.

That is correct, the net torque is that of the weight of the ball.

PsychonautQQ said:
So if we set
m_ball*g*r = I(alpha) = m_ball*(r^2)*(alpha)

The moment of inertia includes also the contribution from the rod. What is it about the centre?


ehild
 
The book claims the answer is that all the magnitudes are the same because "the gravitational force on the penguin is the same". I'm having trouble understanding this. I thought the buoyant force was equal to the weight of the fluid displaced. Weight depends on mass which depends on density. Therefore, due to the differing densities the buoyant force will be different in each case? Is this incorrect?

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