Angular velocity of suspended rod

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The discussion centers on calculating the angular velocity of a uniform rod when it is released from a horizontal position to a vertical position. One participant suggests using the conservation of energy principle, leading to the formula ω = √(3g/L) for angular velocity. Another participant challenges this approach, arguing that the torque is not constant throughout the motion and that the angular acceleration changes with the angle of the rod. They emphasize the need to integrate the torque to find the correct angular velocity. The debate highlights the importance of considering variable torque and angular acceleration in such problems.
Prathamesh
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Homework Statement


A uniform rod of length L & mass m is suspended through an end. It is shifted through an angle of π/2 radian i.e. made horizontal and then released. Find angular velocity when rod is vertical.[/B]

Homework Equations

The Attempt at a Solution


My attempt to a problem is attached
with this post.

But

Solution says
By energy conservation law
1/2 I ω2= mg L/2
(ω = angular velocity)
Hence
ω=√ (3g/L)

Which one is correct? N why other is wrong?[/B]
 

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but in your soln you have assumed that torque remains constant throughout which is wrong
You must correct it and integerate to get the right answer
 
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Likes Prathamesh and Sahil Dhull
Nope...i ve found the torque acting on the rod when it is in hzt position only... and hence angular acceleration (alpha) also changes with theta...so by putting theta =π/2 i ve found w
 
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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