Visualizing the Motion of Coins on a Rotating Scale

In summary, the coins on the rod lost contact with the stick and the stick started rotating after the hand was removed.
  • #36
Rahulrj said:
is it correct to write the normal force on the coin at the part of rod with the rod's value of g at that point since they are going to be sticking onto the rod?
I think you mean the rod's value of acceleration at that point.
Yes. If at some point less than 2L/3 from the axis the normal force is zero then the coin must be accelerating faster than the rod, which is not possible. So N>0, which means the coin must be in contact with the rod.
 
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  • #37
haruspex said:
I think you mean the rod's value of acceleration at that point.
Yes. If at some point less than 2L/3 from the axis the normal force is zero then the coin must be accelerating faster than the rod, which is not possible. So N>0, which means the coin must be in contact with the rod.
I am not sure if you got what I meant, for example I am interested in finding acceleration that coin experiences at say L/3
so the equation will be, N - mg = -ma and my doubt is whether if it is correct to write a = g/2? as it is the acceleration rod has at that point
 
  • #38
Rahulrj said:
correct to write a = g/2?
Yes, that must be right. If it were more, it would penetrate the rod; if it were less it would lose contact with the rod, making N zero, so then it would fall at rate g and immediately catch up to the rod again.
 
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  • #39
There is a funny counterintuitive fact: if ##m## is a total mass of all coins then $$|\epsilon|\sim const \,m^{1/3},$$ as ## m\to\infty## where ## \epsilon## is angular acceleration of the rod right after it is released. Other parameters are fixed.
 
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