EM Wave - basic question on energy conservation in a wave

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Discussion Overview

The discussion revolves around the energy conservation in electromagnetic (EM) waves, particularly focusing on the behavior of electric and magnetic field components as they oscillate. Participants explore the relationship between field strength and energy at points where the fields are zero, and how this relates to the concept of photons.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions how energy is related to the points in an EM wave oscillation where both electric and magnetic fields are zero, seeking clarification on energy conservation in this context.
  • Another participant provides the energy density formula for the electromagnetic field, noting that while energy density is not conserved, the total energy of the EM field is conserved over a region of space.
  • A participant explains that the energy associated with EM waves is propagating and not localized at points where fields are zero, drawing an analogy to kinetic and potential energy in a wave on a string.
  • One participant expresses confusion about treating light as both an EM wave and a photon, acknowledging a conceptual mistake and appreciating the clarification provided by others.
  • A later reply emphasizes that a photon is not a localizable entity and that it is more accurate to consider electromagnetism as a field phenomenon rather than a point-particle-like object.

Areas of Agreement / Disagreement

Participants express various viewpoints on the nature of energy in EM waves and the relationship between classical field theory and quantum descriptions of light. There is no consensus on the interpretation of energy at points where the fields are zero, and the discussion remains unresolved regarding the implications of these concepts.

Contextual Notes

Participants highlight the complexity of relating classical electromagnetic wave behavior to quantum descriptions, indicating potential limitations in understanding energy localization and conservation in different contexts.

mgkii
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I've searched threads and can't find easy explanation - sorry if I'm missing something basic / have a basic understanding error!

In the classic picture of an EM wave with the Electric and Magnetic components oscillating at 90 degrees to each other, both components cross the middle axis at the same point. If this means that both the components are at Zero "something" that relates to the strength of the field, is that something related to energy? If so, then where does that energy "hide" at the points in the oscillations that are not at their maximum? If it's not related to energy, then how do we use the strength of that field to do work?

Thank you
Matt
 
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The energy density (!) of the free electromagnetic field is (in SI units)
$$u=\frac{\epsilon_0}{2} \vec{E}^2 + \frac{1}{2 \mu_0} \vec{B}^2.$$
It's not a conserved quantity. Only the total energy for a free em. field
$$E=\int_{\mathbb{R}^3} \mathrm{d}^3 x u(t,\vec{x})$$
is conserved.
 
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mgkii said:
Summary:: where does the energy "hide" (wrong word I know!) at the points in an EM wave oscillation where the two field components cross the axis and are zero.

I've searched threads and can't find easy explanation - sorry if I'm missing something basic / have a basic understanding error!

In the classic picture of an EM wave with the Electric and Magnetic components oscillating at 90 degrees to each other, both components cross the middle axis at the same point. If this means that both the components are at Zero "something" that relates to the strength of the field, is that something related to energy? If so, then where does that energy "hide" at the points in the oscillations that are not at their maximum? If it's not related to energy, then how do we use the strength of that field to do work?

Thank you
Matt

The energy associated with any wave is propagating. In the simple case of a pulse moving along a string, the kinetic energy and elastic potential energy of the wave moves along the string, so that a particular section of the string is distrurbed for a short time, then returns to its equilibrium position, and the energy is now manifest at a different part of the string.

The case of EM waves is similar. The total energy of a pulse of EM radiation is associated with the electric and magnetic fields over the region of space where the fields are non-zero. This region changes as the wave propagates. There is no particular significance of the points in space within this region where the fields happen to be zero instantaneously as the wave moves through.

PS I see @vanhees71 has expressed this somewhat more mathematically.
 
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Thank you! I have a feeling I'm making a rookie mistake of trying to treat light as an EM wave and a photon at the same time... In my head I am following the EM diagram and thinking "at that point there where the E & M components cross the axis, where is the <whatever> in the photon?" The string analogy quickly dispels that thought!

Much appreciated all.
 
Light is an electromagnetic wave with the relevant frequencies in a certain range, our eyes are sensitive to. A photon is a one-particle Fock state of the electromagnetic quantum field. It is not localizable to begin with, i.e., it is completely wrong to think of it in terms as a point-particle-like object. You cannot even define a position for a photon in the strict sense but only probabilities for being detected at a given point at a given time.

In almost all cases it's much closer to the true picture to think about electromagnetism as field phenomenon. It's also amazing how far you get with the completely classical field picture as described by Maxwell's equations.
 

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