Visualizing the Motion of Coins on a Rotating Scale

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Homework Help Overview

The problem involves a uniform rigid scale held horizontally, which begins to rotate about its edge when the supporting hand is removed. Coins of negligible mass are placed on the scale, and the discussion centers around the motion of these coins as the scale rotates. Participants are exploring the implications of torque, angular momentum, and the forces acting on the coins during this motion.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the initial conditions of the coins and the scale, questioning how the coins will behave as the scale rotates. Some attempt to reason through the effects of torque and angular momentum, while others explore the implications of the coins' negligible mass on their motion. There is also consideration of the forces acting on the coins and how these relate to their acceleration.

Discussion Status

The discussion is active, with various interpretations being explored regarding the motion of the coins. Some participants suggest calculations related to the acceleration of different points on the scale, while others question the relevance of these calculations to the overall problem. There is no explicit consensus, but several productive lines of reasoning have been presented.

Contextual Notes

Participants are navigating assumptions about the mass of the coins and the effects of gravity on their motion. The problem's setup involves a uniform rod and a chain of coins, with discussions around the implications of treating the coins as having negligible mass versus massless. There are also references to specific options in a multiple-choice context that are under consideration.

  • #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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