TEM mode propagation between 2 infinite conductor plates

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SUMMARY

The discussion centers on the propagation of the Transverse Electromagnetic (TEM) mode between two infinite conductor plates separated by a dielectric, as described in Jackson's "Classical Electrodynamics." The user attempts to solve the wave equation with boundary conditions that require the electric field (##\vec E##) to be perpendicular to the conductor surfaces and the magnetic field (##\vec B##) to be parallel. The user derives expressions for the electric field (##\vec E=-\frac{V}{d}e^{-ikz}\hat y##) and magnetic field (##\vec H=\sqrt{\frac{\varepsilon}{\mu}}\frac{V}{a}e^{-ikz}\hat x##), but is confused about the presence of current in the plates, which seems contradictory to their understanding of capacitive behavior.

PREREQUISITES
  • Understanding of TEM mode propagation in transmission lines
  • Familiarity with Maxwell's equations and boundary conditions
  • Knowledge of wave equations in dielectric media
  • Basic concepts of electrostatics and current flow in conductors
NEXT STEPS
  • Study the derivation of TEM mode propagation in parallel plate transmission lines
  • Learn about boundary conditions for electromagnetic fields in conductors
  • Explore the role of surface currents in electromagnetic theory
  • Review Jackson's "Classical Electrodynamics," particularly Chapter 8 on wave propagation
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Students and professionals in electrical engineering, particularly those studying electromagnetic theory, transmission line design, and wave propagation in dielectric media.

fluidistic
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Homework Statement


I am trying to solve a problem from Jackson's book (in chapter 8). I must describe the propagation of a TEM mode through a transmission line that consists of two infinite conductor plates that are parallel to each other and separated by a distance a. There's a dielectric between the 2 plates.

At first I did not know how to start the problem. Maybe solve the wave equation with boundary conditions that ##\vec E## must be perpendicular to the conductor surfaces and ##\vec B## must be parallel to it and both fields should have no component in the z direction, the direction of propagation. On the top of this, since it's a TEM, Jackson's demonstrate that in a hollow cylinder the fact that ##E_z## and ##B_z## vanish implies that these fields satisfy electrostatics Maxwell equations and I believe it is also the case for the exercise I'm dealing with. This is also confirmed by page 14 of http://www.ece.msstate.edu/~donohoe/ece4333notes3.pdf for the particular set up I'm facing in this problem.

Homework Equations


Not sure...

The Attempt at a Solution


Following the document linked above I reach that ##\vec E=-\frac{V}{d}e^{-ikz}\hat y## and ##\vec H=\sqrt{\frac{\varepsilon}{\mu}}\frac{V}{a}e^{-ikz}\hat x##.
So I see no propagation, no time dependence... However in the document I linked above one read
The current directions in the two plates correspond to the direction of propagation assumed for the waves.
which confuses me even more. How come there is a current in the plates? They seemed to act like a capacitor to me and as far as I know there is no current in the plates... What I am missing?

I've also found another solution to the problem but it did not convince me since the guy assumes time dependence of the fields and for some unknown reason to me, he assumes from the start that the current in the plates if of the form ##\vec K=(z,t)=K_0\mu e^{i(kz-\omega t)}\hat x##. See http://www-personal.umich.edu/~pran/jackson/P506/P506W02HW02.pdf.

So which answer is correct? Thank you.
 
Still stuck at the very same point in this problem. I don't know which solution is correct and whether there is some time dependence on the fields.
 

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