How to show that Electric and Magnetic fields are transverse

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SUMMARY

This discussion focuses on demonstrating that electric and magnetic fields are transverse in the context of plane wave solutions as described in classical electromagnetism. The plane wave solutions are given by the equations $$ \textbf{E}(\vec{x}, t) = Re[\vec{E_0}e^{-i(\vec{k} \cdot \vec{x} - \omega t)}] $$ and $$ \textbf{B}(\vec{x}, t) = Re[\vec{B_0}e^{-i(\vec{k} \cdot \vec{x} - \omega t)}] $$, where the divergence conditions from Maxwell's equations lead to the requirements $$\vec{k} \cdot \textbf{E} = 0$$ and $$\vec{k} \cdot \textbf{B} = 0$$. The discussion clarifies that the complex amplitude vectors $$\vec{E_0}$$ and $$\vec{B_0}$$ must satisfy these conditions, leading to the conclusion that both components of the amplitude vectors must individually be orthogonal to the wave vector $$\vec{k}$$.

PREREQUISITES
  • Understanding of Maxwell's equations
  • Familiarity with plane wave solutions in electromagnetism
  • Knowledge of vector calculus, specifically divergence
  • Basic concepts of complex numbers and their application in physics
NEXT STEPS
  • Study the implications of Maxwell's equations on wave propagation
  • Explore the mathematical derivation of plane wave solutions in electromagnetism
  • Learn about the physical significance of complex amplitude vectors in wave mechanics
  • Investigate the relationship between wave vectors and polarization in electromagnetic waves
USEFUL FOR

Students of physics, particularly those studying electromagnetism, as well as educators and researchers looking to deepen their understanding of wave behavior in electric and magnetic fields.

leonardthecow
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Homework Statement


This isn't necessarily a problem, but a question I have about a certain step taken in showing that the electric and magnetic fields are transverse.

In Jackson, Griffiths, and my professor's written notes, each claims the following. Considering plane wave solutions of the form $$ \textbf{E}(\vec{x}, t) = Re[\vec{E_0}e^{-i(\vec{k} \cdot \vec{x} - \omega t)}] \\ \textbf{B}(\vec{x}, t) = Re[\vec{B_0}e^{-i(\vec{k} \cdot \vec{x} - \omega t)}]$$ since the Maxwell equations demand that the divergences of both E and B are zero, this in turn demands that $$\vec{k} \cdot \textbf{E} = 0 \\ \vec{k} \cdot \textbf{B} = 0.$$

Homework Equations



See above, plus the fact that ##\vec{E_0}## and ##\vec{B_0}## are complex functions.

The Attempt at a Solution


[/B]
This has to just be my missing something stupid; I just don't see how the plane wave solutions and the Maxwell equations imply that condition (where the wave vector dotted into the E and B fields is zero). Even doing the divergence out for, say, the x component of the E field, you would have something like $$ (\nabla \cdot \textbf{E})_x = \partial_x ({E_0}_xe^{-i(k_x x - \omega t)}) = \partial_x {E_0}_x - ik_x {E_0}_xe^{-i(k_x x - \omega t)}$$ which, combined with the other components would give you $$ \nabla \cdot \vec{E_0} - i\vec{k} \cdot \textbf{E} = 0 $$ which clearly isn't what any of the textbooks are saying is the case. Is it just that the divergence of the complex function ##\vec{E_0}## is zero? If so, why is that the case? Where am I going wrong here? Thanks!
 
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##\vec E_0## is an amplitude, a constant for the plane waves you describe.
 
Ah okay, I buy that, thanks! Related question though; ##\vec{E_0}## is defined as $$\vec{E_0}=\textbf{A}_1 + i\textbf{A}_2,$$ where ##\textbf{A}_2## and ##\textbf{A}_2## are in ##\mathbb{R}^3##. In a later proof, my professor makes the claim that $$\vec{k} \cdot \textbf{A}_1 = \vec{k} \cdot \textbf{A}_2 = 0.$$ Now, just by simple substitution into ##\vec{k} \cdot \vec{E_0} = 0## would this not imply only that ##\vec{k} \cdot \textbf{A}_1 = - \vec{k} \cdot \textbf{A}_2##? I don't see why we would assume that both dot products are individually zero.
 
Well, if ##\vec k## is real, then ##
\vec{k} \cdot \vec{E_0} = \vec{k} \cdot ( \textbf{A}_1 + i\textbf{A}_2) = 0 + i 0## implies ##\vec{k} \cdot \textbf{A}_1 = \vec{k} \cdot \textbf{A}_2 = 0 ## and you are in business. Is ##\vec k_0## real ? why (or: why not) ?
 

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