Total Electrostatic Energy in a system of charges

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Discussion Overview

The discussion revolves around calculating the total electrostatic energy in a system of N fixed charges located at arbitrary positions. Participants explore two primary methods: using Coulomb's law and integrating energy density over volume. The conversation includes comparisons of these methods and their implications for different charge distributions.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants propose using Coulomb's law to calculate total electrostatic energy, while others suggest integrating energy density, noting that both methods may yield the same result under certain conditions.
  • One participant emphasizes the importance of considering the work needed to bring charges from infinity to their locations, which aligns with the Coulomb's law approach.
  • Another participant mentions that for symmetric charge distributions, alternative methods may provide quicker results than direct application of Coulomb's law.
  • It is noted that both methods yield the same result for a single spherical shell of charge, but the equivalence may not hold for collections of point charges due to divergences in energy density integration.
  • One participant highlights that the energy density integration diverges as one approaches point charges, while the Coulomb method provides a finite answer given non-zero separations between charges.
  • A later reply discusses the mathematical details of energy density and its divergence, referencing a source that expands on the contributions of individual charges to the total energy.
  • Another participant expresses interest in examining the mathematical expressions from a referenced source to deepen understanding of the topic.

Areas of Agreement / Disagreement

Participants generally agree that both methods can be valid for calculating electrostatic energy, but they express uncertainty about the conditions under which they are equivalent. There is no consensus on the applicability of these methods to collections of point charges versus continuous charge distributions.

Contextual Notes

Limitations include the divergence of energy density integration at point charges and the dependence on charge distribution symmetry. The discussion does not resolve the mathematical steps or assumptions involved in the equivalence of the two methods.

throneoo
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Suppose there are N charges fixed at arbitrary locations , how do I calculate the total electrostatic energy ?

I can think of two ways.

one being the straightforward coulomb's law :

k=1/(4*pi*ε)

Q=k/2 * ΣiΣj qiqj / |ri-rj| ; i≠j

the other method is to integrate energy density with respect to volume , which would most likely depend on the distribution of the charges.

My questions are, do these methods yield the same result ? If so , how could I show that they are equivalent in both mathematical and physical sense?
 
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throneoo said:
Suppose there are N charges fixed at arbitrary locations , how do I calculate the total electrostatic energy ?
Calculate total energy(work), needed to bring them at their locations, one by one, from the point located at infinity.
 
zoki85 said:
Calculate total energy(work), needed to bring them at their locations, one by one, from the point located at infinity.
Thanks but I want to focus on comparing the two approaches in the OP. Intuitively they seem very different but I see them as valid methods to calculate energy.
 
throneoo said:
Thanks but I want to focus on comparing the two approaches in the OP. Intuitively they seem very different but I see them as valid methods to calculate energy.
If you're dealing with problems having some symmetry of charge distribution, nicely described by mathematical means, than other methods would lead more quickly to the result than straightforward application of Coulomb's law.
 
Both methods give the same result for a single spherical shell of charge – I've just verified this. [For the Coulomb's law method you consider increments of charge being brought from infinity and deposited on the spherical surface.] If I have time, I'll work on a proof for a collection of charges where each charge is spread over a surface or volume of finite linear dimensions. I can see one difficulty though… The equivalence won't hold for a collection of point charges, because the Coulomb method will give a finite answer (provided the charges have non-zero separations) but the energy density integration will blow up because the energy density approaches infinity as one gets close to any charge.
 
Philip Wood said:
Both methods give the same result for a single spherical shell of charge – I've just verified this. [For the Coulomb's law method you consider increments of charge being brought from infinity and deposited on the spherical surface.] If I have time, I'll work on a proof for a collection of charges where each charge is spread over a surface or volume of finite linear dimensions. I can see one difficulty though… The equivalence won't hold for a collection of point charges, because the Coulomb method will give a finite answer (provided the charges have non-zero separations) but the energy density integration will blow up because the energy density approaches infinity as one gets close to any charge.

I've verified them using a sphere and a circular cylinder of finite length, so I'm convinced it would work for any geometry of continuous charge distribution. The equivalence breaks down because point charges have infinite charge densities, unlike that of continuous charge distributions. and what do you mean by the bold?
 
Try evaluating [itex]\int_0^\inf\frac{\epsilon_0}{2}E^2 4\pi r^2 dr[/itex] for [itex]E=\frac{Q}{4 \pi \epsilon_0 r^2}[/itex] and you'll see what I mean by the bold. But you're saying the same thing when you point out that the equivalence breaks down if there are infinite charge densities.
 
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I see. it diverges at r=0.
 
I've just looked this up in my beloved Abraham and Becker (1944 edition!) A&B expand [itex]E^2[/itex] at a point as a sum of [itex]E^2[/itex] terms due to individual charges, plus a sum of terms of the form [itex]\mathbf E_i . \mathbf E_j[/itex]. The first sum goes to infinity owing to the singularities at the charges themselves. But this sum is also independent of the relative positions of the charges. A&B show that it is the second sum that equals the Coulomb-derived energy formula!
 
  • #10
Care to show me a scan of that page? I want to look at the mathematical expressions in detail
 
  • #11
Your every whim is my command...
 

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  • #12
No doubt the original poster has long since achieved understanding and moved on, but I thought the question so interesting that I amused myself by recasting the A&B argument. Attached.
 

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