Electric and magnetic waves orthogonal to each other?

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Discussion Overview

The discussion centers on the relationship between electric and magnetic fields in electromagnetic waves, specifically addressing the orthogonality of these fields. Participants explore the theoretical basis for this orthogonality, referencing Maxwell's equations and the wave equation, while also discussing implications in different contexts such as free space and waveguides.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions the basis for the orthogonality of electric and magnetic fields, suggesting it may be derived from solving the wave partial differential equation.
  • Another participant asserts that the orthogonality is derived from the third Maxwell equation, providing a link to further reading.
  • A participant expresses confusion regarding the definitions of TE, TM, and TEM modes, arguing that all light should be classified as TEM since E and B are always normal to the direction of propagation.
  • In response, another participant clarifies that TE and TM modes refer to guided waves in waveguides, where the fields can be oriented differently compared to free space.
  • One participant notes a discrepancy in their understanding of the relationship between the wave vector and the electric field, referencing a specific equation that implies orthogonality.
  • Another participant confirms their understanding after reviewing additional material on waveguides.
  • A later reply discusses the implications of vector products in demonstrating the orthogonality of the wave vector and the electric field.
  • One participant mentions finding another textbook that supports the orthogonality of E and B fields, noting confusion about vector representations in the equations.

Areas of Agreement / Disagreement

Participants express differing views on the definitions and implications of TE, TM, and TEM modes, indicating a lack of consensus on these classifications. There is also ongoing exploration of the mathematical basis for the orthogonality of electric and magnetic fields, with some participants agreeing on certain points while others raise questions.

Contextual Notes

Participants reference various equations and concepts from Maxwell's equations and wave theory, but there are indications of differing interpretations and understandings of these concepts, particularly in the context of waveguides versus free space.

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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You get this not from the differential wave equations for [itex]\vec E[/itex] and [itex]\vec B[/itex], but from the third Maxwell equation, [itex]\nabla \times \vec E = - \partial \vec B / \partial t[/itex]. See

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

in particular the section beginning with equation 448.
 
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 [itex]\vec E[/itex] and [itex]\vec B[/itex], but from the third Maxwell equation, [itex]\nabla \times \vec E = - \partial \vec B / \partial t[/itex]. 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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