Undergrad Waveguide Question: TE & TM Waves Explained

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The discussion clarifies the distinction between transverse electric (TE) and transverse magnetic (TM) waves in waveguides, noting that waveguides do not support transverse electromagnetic (TEM) waves. When a monochromatic plane wave enters a waveguide, it can excite multiple TE and TM modes, resulting in a combination of guided waves that aligns with the incident wave. Additionally, while a laser beam can pass through a waveguide without significant interaction, its output can be characterized as a superposition of plane waves, particularly in a resonant cavity where stable modes are present. The conversation also touches on the utility of Fourier analysis in understanding these wave interactions. Overall, the complexities of wave behavior in waveguides and lasers are acknowledged, emphasizing the intricate nature of electromagnetic wave propagation.
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I am a little confused about the difference between TE and TM waves in a waveguide. Let's say a monochromatic plane wave is incident on a wave guide. Then will this result in both TE and TM waves such that the sum of the guided waves at the entrance of the waveguide agrees with the plane wave?
 
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pierce15 said:
I am a little confused about the difference between TE and TM waves in a waveguide.
This issue is that a waveguide does not support transverse electromagnetic (TEM) waves, where both E and B are perpendicular to the direction of propagation. So the waves that propagate must have a component of the electromagnetic field parallel to the direction of propagation. Waves for which the electric field is perpendicular to the direction of propagation are called transverse electric (TE); these waves have a component of the magnetic field along the direction of propagation. Likewise waves for which the magnetic field is perpendicular to the propagation direction are TM, and these waves have a component of E along the propagation direction. But it is also possible for a wave in a waveguide to have components of both E and B along the propagation direction, for example:

pierce15 said:
Then will this result in both TE and TM waves such that the sum of the guided waves at the entrance of the waveguide agrees with the plane wave?
Yep. In general it will excite many TE and TM modes. The wave will have E and B in all directions, including along the direction of propagation.

EDIT: note that in general there will be a wave reflected from the waveguide as well, which complicates things a little. But conceptually you have the right idea. Actually performing these kinds of calculations can be fairly messy and not so insightful, in my experience (from many years ago...).

jason
 
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Thanks, that helps.

An unrelated question, but one that started when I was thinking about this: is it possible to characterize the light coming out of a laser beam as a superposition of plane waves (i.e. Fourier transform of some function)? Or to handle it in some other way while still thinking about E and B?

My intuition is that if you shine a laser into a hollow cavity it seems like it would pass right through without exciting any TE or TM modes, if the width of the laser beam is less than the waveguide radius (assuming circular cylinder).
 
Yes, Fourier analysis can be useful for these types of systems.

Reagarding the laser beam, for all practical purposes the waveguide has essentially no effect. If you have ever looked through a metal pipe you know that optical frequencies have no trouble propagating. If you want the exact answer, then the waveguide will have a small effect - the extent of which depends on the details of the beam shape ans the size of the waveguide. I suspect it will be unmeasurable in many cases, though.
 
pierce15 said:
Thanks, that helps.

An unrelated question, but one that started when I was thinking about this: is it possible to characterize the light coming out of a laser beam as a superposition of plane waves (i.e. Fourier transform of some function)? Or to handle it in some other way while still thinking about E and B?

Within a resonant cavity, the EM field consists of stable modes: both longitudinal and transverse. The laser output consists of coupling the internal modes to the outside via a partially reflecting mirror. The usual way to describe the emitted field is to decompose the emitted beam in terms of the cavity modes- most laser output is a single transverse mode (e.g. a Gaussian beam), but higher-order modes (Laguerre-Gaussian or Hermite-Gaussian, depending on the cavity cross-section) are possible as well. Other, more complicated cavities (unstable resonators, for example) have different eigenmodes.

https://courses.engr.illinois.edu/ece455/Files/Galvinlectures/02_CavityModes.pdf

One helpful fact is that the Fourier transform of a Gaussian function is another Gaussian- making it trivial to perform some basic optical analysis.
 
Thanks to both of you.
 
I do not have a good working knowledge of physics yet. I tried to piece this together but after researching this, I couldn’t figure out the correct laws of physics to combine to develop a formula to answer this question. Ex. 1 - A moving object impacts a static object at a constant velocity. Ex. 2 - A moving object impacts a static object at the same velocity but is accelerating at the moment of impact. Assuming the mass of the objects is the same and the velocity at the moment of impact...

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