Questions on Plane Wave Superposition

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SUMMARY

The discussion focuses on the superposition of plane waves, specifically questioning whether all plane waves share the same direction vector, denoted as ##\vec{n}##. The participant proposes that the electric field can be expressed as ##\vec{E}(\vec{x}, t)=\int\mathbf{\mathfrak{E}}(\vec{k}')e^{i\vec{k}'\cdot\vec{x}-i\omega t}d^3k##. Additionally, they seek to understand the relationship between the energy of individual plane waves and their superposition, noting that energy is not a linear quantity. The equations for energy density in terms of electric and magnetic fields are confirmed as ##\frac{\epsilon_0}{2}|\vec{E}|^2## and ##\frac{1}{2\mu_0}|\vec{B}|^2##.

PREREQUISITES
  • Understanding of plane wave propagation and superposition principles
  • Familiarity with vector calculus and integral equations
  • Knowledge of electromagnetic theory, particularly energy density concepts
  • Basic grasp of wave mechanics, including relationships between frequency and wave vector
NEXT STEPS
  • Study the derivation of the superposition principle in wave mechanics
  • Learn about energy density calculations in electromagnetic fields
  • Explore the implications of non-linear energy relationships in wave interactions
  • Investigate the mathematical techniques for evaluating integrals in wave physics
USEFUL FOR

Physicists, electrical engineers, and students studying wave mechanics and electromagnetism will benefit from this discussion, particularly those interested in the mathematical treatment of plane wave superposition and energy density in electromagnetic fields.

andrew chen
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Homework Statement
Starting with the expression for the total energy of arbitrary superposition of plane electromagnetic waves in otherwise empty space, Show that the total number of photons (defined for each plane wave of wave vector ##\vec{k}## and polarization ##\vec{\epsilon}## as its energy divide by ##\hbar ck##) is given by the double integral ##N=\frac{\epsilon_0}{4\pi^2\hbar c}\int d^3x\int d^3x'\frac{\vec{E}(\vec{x}, t)\cdot\vec{E}(\vec{x}', t)+c^2\vec{B}(\vec{x}, t)\cdot\vec{B}(\vec{x}', t)}{|\vec{x}-\vec{x}'|^2}##.
Relevant Equations
##\vec{E}(\vec{x},t)=\mathbf{\mathfrak{E}}e^{ik\vec{n}\cdot\vec{x}}##, ##\vec{B}(\vec{x},t)=\mathbf{\mathfrak{B}}e^{ik\vec{n}\cdot\vec{x}}##, and ##\mathbf{\mathfrak{B}}=\sqrt{\mu\epsilon}\vec{n}{\times}\mathbf{\mathfrak{E}}##
##\frac{1}{|\vec{x}-\vec{x}'|}=\int d^3k\frac{e^{i\vec{k}\cdot(\vec{x}-\vec{x}')}}{k^2}##
First, I have a question about supereposition of the plane waves - whether the direction of all such plane wave is same, i.e. ##\vec{n}## is in some direction. If not, I think it would be ##\vec{E}(\vec{x}, t)=\int\mathbf{\mathfrak{E}}(\vec{k}')e^{i\vec{k}'\cdot\vec{x}-i\omega t}d^3k##. Besides, how to express the energy of such plane wave. I think it would certainly be ##\int d^3x## ##u(\vec{x}, t)##. However, I can't figure out how to relate each specific plane wave's energy to the superposition, for energy isn't linear quantity and ##\omega## also relates to wave vector ##k## by ##\omega = kc##. I think that deriving the equation Jackson wants may require such formula ##\frac{1}{|\vec{x}-\vec{x}'|}=\int d^3k\frac{e^{i\vec{k}\cdot(\vec{x}-\vec{x}')}}{k^2}##. Could someone give me some hints to solve it, tks?
 
Last edited:
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What is the equation for the energy density in terms of electric and magnetic fields?
 
nrqed said:
What is the equation for the energy density in terms of electric and magnetic fields?
It would be ##\frac{\epsilon_0}{2}|\vec{E}|^2## & ##\frac{1}{2\mu_0}|\vec{B}|^2##
 

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