Boundary conditions and time domain electromagnetic waves

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SUMMARY

The discussion centers on the boundary conditions between lossy and lossless dielectric media in the context of time domain electromagnetic waves. It establishes that the tangential electric field must remain continuous at the interface, yet the equations governing the two media—specifically ET1 = C * exp(-a * t) * sin(b * t) for the lossy medium and ET2 = D * sin(d * t) for the lossless medium—cannot satisfy this condition due to the decay factor in the lossy medium. The conclusion drawn is that there will never be transmission of electromagnetic energy between these two types of media. The participants also explore the implications of using time domain Maxwell wave equations versus frequency domain analysis, emphasizing the necessity of time domain solutions for lossy media.

PREREQUISITES
  • Understanding of Maxwell's equations in both time and frequency domains.
  • Familiarity with concepts of lossy and lossless dielectric media.
  • Knowledge of boundary conditions in electromagnetic theory.
  • Basic proficiency in solving differential equations related to wave propagation.
NEXT STEPS
  • Study the derivation and implications of the wave equation for lossy media, specifically the equation: ∇²E = μσ ∂E/∂t + με ∂²E/∂t².
  • Learn about the continuity conditions at the interface of different media, focusing on electromagnetic boundary conditions.
  • Investigate the role of complex wavenumbers in the analysis of lossy media, particularly in relation to damping.
  • Explore advanced texts such as "Advanced Engineering Electromagnetics" by Constantine A. Balanis for deeper insights into wave behavior in lossy media.
USEFUL FOR

Electromagnetic engineers, physicists, and graduate students specializing in electromagnetics, particularly those focused on wave propagation in complex media and boundary condition analysis.

  • #31
ashade said:
I need the field distributions. A transmission line model won't fit because I'm looking for TE and TM modes on a coaxial cable, semi-infinite, with 2 dielectrics: one lossy and the other lossless. And I need distributions of field because I need to find the best way to place some receivers for a very very specific application.

PS: I didnt say in any moment I want a dumped wave on lossless medium. You said so.

Then what is the difficulty that you are having? Why do you keep complaining that the lossless medium will not allow a damped solution?
 
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  • #32
Born2bwire said:
Then what is the difficulty that you are having? Why do you keep complaining that the lossless medium will not allow a damped solution?

Because dumped and undumped solutions cannot equal for all t. Therefore, continuous tangential electric field is not guarateed in the boundary of both media.
 
  • #33
ashade said:
Because dumped and undumped solutions cannot equal for all t. Therefore, continuous tangential electric field is not guarateed in the boundary of both media.

They are equal because one wave is the source for the other. As I explained previously, a wave that transitions from a lossy to a lossless region has already been attenuated by its passage through the lossy region. A wave that goes from lossless to lossy will become attenuated as it travels into the lossy region. But the wave isn't going to decay until it is traveling in the lossy media. The causality of the problem and the fact that you are working with waves what you are forgetting here. Think of what happens if you were to send a wave pulse down your lossless section of your waveguide and it hits the the lossy dielectric section.

In addition, the analysis of the boundary conditions that I gave in post #19 demonstrates the general case that you are discussing using a plane wave solution. If you convert it from the time-harmonic form to the time domain form the wave solutions match the same conditions that you stipulated in your OP. That is, the left-hand side is dependent upon a sinusoidal function demonstrating the spatial and time phase dependence multiplied by what is equivalently an exponentially decaying function in time (by virtue of the constant dispersion curve relating the wave number with frequency and the phase velocity of the wave). The right hand side will be just a sinusoidal function with a spatial and time dependence.
 

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