Potential energy of point charges

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Discussion Overview

The discussion revolves around the potential energy of a system of three identical point charges arranged at the corners of a square. Participants explore the implications of symmetry in energy distribution as the charges move to infinity, questioning the published solution that suggests each charge attains equal kinetic energy. The conversation includes numerical simulations and methods for analyzing the system's dynamics.

Discussion Character

  • Debate/contested
  • Mathematical reasoning
  • Experimental/applied

Main Points Raised

  • One participant expresses confusion regarding the notion of symmetry in the energy distribution of the charges, particularly questioning how symmetry applies when the charges are not equidistant from each other.
  • Another participant suggests that the middle charge may end up with more than 1/3 of the total energy, while the other two charges share the remaining energy, indicating a potential discrepancy in the published solution.
  • A numerical simulation conducted by a participant indicates that the energy distribution among the charges is not equal, with one charge receiving approximately 1.061 times the energy of the others.
  • Participants discuss the challenges of deriving velocity from force as a function of distance, with one expressing uncertainty about the integration process needed to analyze the system.
  • Another participant describes a numerical integration approach to simulate the system's behavior, emphasizing the iterative nature of the method and mentioning various numerical techniques that could be employed.

Areas of Agreement / Disagreement

Participants generally disagree on the implications of symmetry in energy distribution, with multiple competing views on how energy is shared among the charges. The discussion remains unresolved regarding the correct interpretation of the energy dynamics in the system.

Contextual Notes

Participants note the limitations of the published solution and the need for numerical methods to explore the system's behavior, highlighting the complexity of the interactions as the charges move apart.

BobFroehlich
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I am puzzled by the solution to a problem in electrical potential. The situation involves three identical point charges (same charge, same mass) each one placed at a corner of a square. The charges are released simultaneously and the problem is to find the maximum speed attained by each of them.

The published solution of the problem states that by symmetry each will end up with the same kinetic energy when the charges have moved to infinity. So the procedure is to calculate the potential energy of the configuration, divide that by 3, set that equal to one-half m v squared, and solve for v, where v is the speed of one charge.

I am having trouble seeing the notion of “symmetry” here since the charges are not equidistant from each other. I also pose the argument that what if a fourth charge were to be included, one that would be orders of magnitude away from the original 3 and would consequently experience far less force due to the other particles. Would the individual charges each still have 1/4 the potential energy of the assembly of four? The only rationale I can muster is that the symmetry is not local symmetry but symmetry at infinity, and I have difficulty picturing that. Hope you can help me sort this out.
 
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I agree that the notion of symmetry seems a little... well, odd to me.

It seems like the middle particle would end up with more than 1/3 of the total energy, whereas the two others would end up with the same value splitting the difference.

In fact, I would argue that this can't possibly be right. Because this would certainly lead to different behavior then three particles arranged on the vertices of an equilateral triangle, and that would certainly give a 3-way split of energy.

Perhaps you could simulate this numerically and look at asymptotic behavior to get a feel for what actually happens.
 
When I simulate it numerically, it appears that the one particle ends up with around 1.061 times the individual energies of the other two. So you have 1-1.061-1 as ar as energy distribution goes.

That's out to 10000 seconds. It was about the same for 1000 seconds; I can give you more data if you want.
 
Thanks for your analysis - it seems to confirm my hunch. I was trying to do that myself. I know how to get v from F(t), but am unsure how to get v when I know F(r); I suspect a double integration. How did you do the analysis?
 
When you do a numerical integration like I did, you don't have to get v = v(t) in closed form... that's the point of the approximation.

You just use a scheme like:

dx = vdt => delta(x) ~= v delta(t) => x' = x + v delta(t)
dv = adt => delta(v) ~= a delta(t) => v' = v + a delta(t)
a = F/m where F = f(x, v, t).

This is notoriously easy to iterate on a computer. There are several methods, the simplest of which is Euler's method, though better schemes - such as Runge Kutta or more stable methods - exist.
 

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