Electric and magnetic waves orthogonal to each other?

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SUMMARY

The discussion centers on the orthogonality of electric (E) and magnetic (B) waves in electromagnetic (E&M) theory, specifically derived from Maxwell's equations. The third Maxwell equation, \nabla \times \vec E = - \partial \vec B / \partial t, establishes that E and B fields are orthogonal to each other and the direction of wave propagation. The conversation also clarifies that while transverse electric (TE) and transverse magnetic (TM) modes exist in waveguides, all light can be classified as transverse electromagnetic (TEM) since E and B are always normal to the propagation direction. The participants emphasize the importance of understanding wave equations and vector relationships in this context.

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  • Understanding of Maxwell's equations, particularly the third equation.
  • Familiarity with electromagnetic wave theory and transverse waves.
  • Basic knowledge of waveguides and their modes (TE, TM, TEM).
  • Experience with vector calculus, including cross products and dot products.
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  • Study the derivation of electromagnetic wave propagation from Maxwell's equations.
  • Learn about waveguide theory and the characteristics of TE, TM, and TEM modes.
  • Explore vector calculus applications in physics, focusing on cross and dot products.
  • Review resources on the wave equation and its solutions in different media.
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Students and professionals in physics, electrical engineering, and anyone studying electromagnetic theory, particularly those interested in wave propagation and waveguide applications.

proton
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In my intro to E&M course, in the section on electromagnetic waves, my textbook just says that electric and magnetic waves are orthogonal to each other, but it doesn't say why. How do we know this? Is it from solving the wave partial differential equation? If so, given that I've tooken a course on intro to DEs that slightly covered PDEs, is it possible for me to solve the wave equation and find out the the E and M waves are orthogonal to each other?
 
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I agree that light is transverse wave, i.e. E and B are all normal to the propagation direction and normal to each other.

However, I saw some definitions about TE, TM and TEM stating that TE is transverse wave where you have only E component normal to the propagation, and so on for TM, TEM. This is meaningless since you would never have E or B NOT normal to the light direction, so all light is TEM.

Am I lost somewhere?
 
You are not talking about waves in free space, but about waves in a waveguide (i.e. guided waves). Propagation of TE and TM modes can be seen as two plane waves reflecting in zig-zag against the walls of the guide. E and B field are orthogonal, but one of them is not orthogonal to the direction of propagation. Try to find a drawing of the shape of electric and magnetic fields in a waveguide.
 
jtbell said:
You get this not from the differential wave equations for \vec E and \vec B, but from the third Maxwell equation, \nabla \times \vec E = - \partial \vec B / \partial t. See

http://farside.ph.utexas.edu/teaching/em/lectures/node48.html

in particular the section beginning with equation 448.

That link doesn't explain why it is k vector dot r vector. My textbooks say that its just k*r, where k and r are scalars
 
Ah yes, after digging a chapter for the waveguides, I got it now.

Thank you, lpfr.
 
Proton, look at eq. 451:

kx(kxE)=const*E

This implies that k and E are orthogonal.
If they were not, the result of the LHS would be another vector that's not parallel with E.

Draw the product of v=kxE, and then kxv, you will see that.Or, another way is using axbxc=b(ac)-c(ab) where ab is scalar product.
 
Last edited:
ok I found another textbook today that derived that E and B are orthogonal in a similar way to the link jtbell provided. I just found it strange that k and r were vectors, but I managed to figure it out.
 

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