How would you Calculate the Energy in an EM field?

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Discussion Overview

The discussion revolves around calculating the energy in an electromagnetic field produced by a particle, specifically an electron. Participants explore theoretical aspects, mathematical approaches, and implications of energy density in electromagnetic fields.

Discussion Character

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

Main Points Raised

  • One participant suggests squaring the electric field to calculate energy density, integrating over all space, but notes this leads to an infinite result.
  • Another participant argues that while the energy may be infinite, it diminishes with distance, making it negligible at far distances, using a geometric analogy involving circles.
  • A later reply introduces the inverse square law as a relevant concept, implying a need for further exploration of this principle.
  • Some participants express uncertainty about the integral's role in addressing the infinite energy issue, with one suggesting that the result should be finite, like pi, despite being conceptually infinite.
  • Another participant emphasizes that the electric field of a charge does not radiate energy but rather stores it, and highlights the distinction between self-energy and radiated energy.

Areas of Agreement / Disagreement

Participants exhibit disagreement regarding the interpretation of energy in electromagnetic fields, particularly concerning the implications of infinity and the behavior of energy at varying distances from the charge. No consensus is reached on the correct approach to calculating this energy.

Contextual Notes

Participants reference mathematical concepts and physical laws, but there are unresolved assumptions about the nature of point charges and the implications of integrating over infinite space.

Ryan Reed
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How would you calculate the energy in an electromagnetic field produced by a particle such as an electron?
 
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I'd square it. Energy density is E2 times a constant depending on your units. Then integrate over all space. Of course you get infinity.
 
But as it goes out, the energy would get smaller and smaller, getting to the point where even though it's infinite, the energy would be so much smaller the farther you go away, it couldn't reach the next decimal place. Think about it like this, a circle with certain dimensions will have a definite volume, even though numbers are infinitely dividable and if you add the radius each time you change the angle until you get to 360 degrees, it will be infinity since 360 can be divided infinitely, but this doesn't happen.
 
Ryan Reed said:
But as it goes out, the energy would get smaller and smaller, getting to the point where even though it's infinite, the energy would be so much smaller the farther you go away,

have you heard of the inverse square law ?
do a google search and have a read :smile:
 
I don't know what to say. Integrals take care of this. That's why we use them,
 
Vanadium 50 said:
I don't know what to say. Integrals take care of this. That's why we use them,
What I mean by this is the answer should be something like pi, infinitely long, not infinitely large. Pi is infinitely long, but will never go above 3.14
 
I know that's what you meant. This whole conversation has an Alice-In-Wonderland aspect, with you - who doesn't know how to do the integral - telling me - who does - that he is wrong, based on your feelings. That's why I don't know what to say.
 
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Ryan Reed said:
But as it goes out, the energy would get smaller and smaller, getting to the point where even though it's infinite, the energy would be so much smaller the farther you go away,

Try going in the other direction, closer and closer to the charge. If the charge is a mathematical point with zero size, what happens?
 
  • #10
Ryan Reed said:
But as it goes out,
What do you mean "as it goes out"? The E field of a charge does not radiate energy, it stores energy. The energy that is there does not go anywhere without a B field also.

As was pointed out earlier, the self energy of a classical point charge is infinite, but it does not radiate.
 
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