Visualizing the Motion of Coins on a Rotating Scale

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The discussion focuses on the dynamics of coins on a rotating scale after the support is removed. When the scale begins to rotate, the torque varies along its length, causing coins closer to the hinge to experience different forces than those at the end. The key point is that coins of negligible mass may not accelerate with the same force as the rod, leading to some coins appearing to "hang" in the air as they fall under gravity. Calculations reveal that while parts of the rod accelerate faster than gravity, coins not in contact with the rod will fall freely. Ultimately, the conclusion is that the correct visual representation of the scenario involves understanding the differing accelerations experienced by the coins based on their position on the scale.
  • #31
Rahulrj said:
From that fact I can only say 'a' is going to be negative or do you mean a substitution for N?
I get the feeling you do not know how to work with inequalities.
You have a = g-N/m and N≥0. So -N/m≤0. Adding g to each side, g-N/m≤g.
 
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  • #32
haruspex said:
You have a = g-N/m and N≥0. So -N/m≤0. Adding g to each side, g-N/m≤g.

Alternatively ,

since N≥ 0 , m(g - a) ≥ 0 or a≤g
 
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  • #33
haruspex said:
I get the feeling you do not know how to work with inequalities.
You have a = g-N/m and N≥0. So -N/m≤0. Adding g to each side, g-N/m≤g.
I have not had much practice with inequalities so when I come across a problem that requires it, that idea does not strike through although I know how to work out inequalities such as this. Also how would the equation vary if I was to write it for a coin that is placed less than 2/3 L of the rod?
Specifically what in this equation, N-mg=-ma would change?
 
  • #34
Rahulrj said:
what in this equation, N-mg=-ma would change?
Nothing in that equation would change. It would still be true that since N≥0 it must that a ≤ g.
The difference would be that the acceleration of the part of the rod it is on would be < g, implying N > 0.
 
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  • #35
haruspex said:
Nothing in that equation would change. It would still be true that since N≥0 it must that a ≤ g.
The difference would be that the acceleration of the part of the rod it is on would be < g, implying N > 0.
So a more specific value for acceleration cannot be inferred then? or 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?
 
  • #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.
 
  • #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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