Rotation: angular momentum and torque

AI Thread Summary
In the discussion on angular momentum and torque, two cases involving a mass attached to a cylindrical post are analyzed. In the first case, where the string passes through a hole at the center, angular momentum is conserved, allowing for the calculation of the final speed of the mass. In the second case, where the string wraps around the post, angular momentum is not conserved due to the torque from the force acting along the string. However, kinetic energy remains conserved since the force is perpendicular to the velocity, resulting in a constant velocity. The discussion emphasizes the importance of understanding conservation laws in different scenarios of rotational motion.
Avi Nandi
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Homework Statement



Mass m is attached to a cylindrical post of rdius R by a string. Initially it is distance r from the centre of the post and is moving tangentially with speed v_{0}.

In case (a) the string passes through a hole in the centre of the post at the top. the string is shortened slowly by drawing it through the hole.

In case (b) the string wraps around at the outside of the post.

What quantities are conserved in each case? Find the final speed of the mass when it heats the post for each case..

The Attempt at a Solution



I am considering the origin of the reference frame on the axis of the cylinder.

Now in the first case i applied angular momentum conservation and the speed in question comes out.

But in the second case angular momentum is not conserved since the force acts along the string which is not passing through the centre and there is a torque in action. Let consider at a certain instant of time length of rope l, velocity of mass v, and distance from the origin r'

angular momentum = mvl/r' and torque = -Fl = -mv^{2} (F= mv^{2}/l)
 
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Hi Avi Nandi! :smile:
Avi Nandi said:
… But in the second case angular momentum is not conserved since the force acts along the string which is not passing through the centre …

Hint: what else might be conserved? :wink:

(and what is the condition for that?)
 
Force is always acting perpendicular to the velocity. So no work is done. Thats why kinetic energy is conserved. Velocity is constant. :) thank you tiny tim. Your help is not tiny at all.
 
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