Does This Electromagnetic Wave Satisfy Maxwell's Equations?

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SUMMARY

The discussion centers on determining whether the given electric field E(x,y,t) and magnetic field B(x,y,t) satisfy Maxwell's Equations in free space. The user successfully demonstrates that both fields have zero divergence and applies Ampere's Law and Faraday's Law to derive the relationship between the wave's angular frequency ω and wavenumber k. However, confusion arises regarding the implication that the wave travels faster than the speed of light, c, leading to questions about the definitions of k and ω. Ultimately, the user concludes that the fields can represent a valid electromagnetic wave if the relationship ω/(k√2) equals c.

PREREQUISITES
  • Understanding of Maxwell's Equations and their implications in electromagnetism.
  • Familiarity with vector calculus, particularly curl and divergence operations.
  • Knowledge of wave equations and the relationship between angular frequency and wavenumber.
  • Basic concepts of electromagnetic wave propagation in free space.
NEXT STEPS
  • Study the derivation and implications of Maxwell's Equations in free space.
  • Learn about the relationship between angular frequency and wavenumber in electromagnetic waves.
  • Explore the conditions under which electromagnetic fields can satisfy Maxwell's Equations without representing valid waves.
  • Investigate the physical significance of group velocity and phase velocity in wave mechanics.
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Students and professionals in physics, particularly those specializing in electromagnetism, as well as educators looking to clarify concepts related to Maxwell's Equations and wave propagation.

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Homework Statement



Show whether or not the following functions satisfies Maxwell's Equations in free space. (That is, show whether or not they represent a valid electromagnetic wave).

E(x,y,t)=(0,0,E_0 sin(kx-ky+\omega t))
B(x,y,t)=B_0 (sin(kx-ky+\omega t),sin(kx-ky+\omega t),0)

Homework Equations



\nabla \times E=-\frac{\partial B}{\partial t}
\nabla \times B=\mu_0 \epsilon_0\frac{\partial E}{\partial t}
\nabla \cdot E=0
\nabla \cdot B=0

The Attempt at a Solution



Starting with the easy two, It is clear that these functions have zero divergence.

Then Ampere's Law gives us that 2B_0k=\mu_0 \epsilon_0 \omega E_0
And Faraday tells us that kE_0=\omega B_0

We then elliminate \frac{E_0}{B_0} from these two equations and note that \frac{1}{\mu_0 \epsilon_0}=c^2 to find that \omega=\pm kc\sqrt{2}

Up to this point i am fine. The field clearly satisfies maxwells equations aslong as these conditions are met. My problem is that it seems this implies the field pattern travels at \frac{\omega}{k}=\pm c\sqrt{2}>c (the group velocity of the wave, correct?). This obviously can't be right. I do not know if I'm just interpreting the result wrong, or if somehow this field is invalid for some reason despite satisfying maxwells equations. I've been scouring my textbook and the internet for the last few hours and can't seem to find anything explaining my issue, and would really appreciate some help, thanks.
 
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Is there anything in the question that states that ##k## is the wavenumber in this case or are you just assuming it from the choice of letter?
 
To put it another way, if the relationship between ##k## and ##\omega## is not defined in the question, then it is possible that ##k## is not actually the wave number, but rather some multiple of it, and that might help.
 
No, now i come to think of it there isn't anything stating that k is the wavenumber or that \omega is the angular frequency. If i remember correctly though, i was taught that the coefficients of the spatial variables are always the components of k, and that the time coefficient is always the angular frequency, but this isn't necessarily the case?
If this is the case how would I go about figuring out the speed of this wave? (I've heard that Maxwell's Equations predict that any electromagnetic wave travels at c, so I assume this should be possible to do)

By the way, I also tried substituting the E and B fields into the wave equation itself;
(\nabla^2-\frac{1}{c^2}\frac{\partial}{\partial t})E=0
(\nabla^2-\frac{1}{c^2}\frac{\partial}{\partial t})B=0
And obtained the same results.

Also, is there any way two functions, say E and B, can satisfy Maxwell's Equations without representing a valid electromagnetic wave (and is this perhaps the case?).
Thanks for your help.
 
Sorry I don't have the time and patience to check everything out here, but it seems to me that in this case, the spatial term is ##(x, y, z).(k, -k, 0)## so the magnitude of the wavenumber seems to be ##\sqrt{k^2+k^2+0} = k \sqrt{2}##, so this could be a valid electromagnetic wave if ##\omega/(k\sqrt{2}) = c##.
 
Thats fair enough, Ireally appreciate your time and effort. That makes sense actually. I guess what I said is only true for waves with one spatial compnent! It definitely makes a bit more sense to me now.
 

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