Mathematical Explanation of Faraday Cage Theory - Reflected/Transmitted Waves

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SUMMARY

The discussion focuses on the mathematical explanation of Faraday cage theory, specifically relating hole size to reflected and transmitted waves using electromagnetic theory. Key methods include treating the cage as an infinite sheet with periodic holes to analyze Floquet modes, and modeling holes as rectangular waveguides to evaluate evanescent modes and power loss. The conversation emphasizes that for electrically small holes, the mesh behaves like a solid Perfect Electric Conductor (PEC) sheet, with induced currents influenced by the phase shift between current sources. The size of the holes is determined by the minimum phase shift permissible before reflection becomes significant.

PREREQUISITES
  • Electromagnetic theory fundamentals
  • Understanding of Floquet modes
  • Knowledge of evanescent wave behavior
  • Familiarity with Perfect Electric Conductor (PEC) properties
NEXT STEPS
  • Explore the mathematical derivation of Floquet modes in periodic structures
  • Study the characteristics of evanescent waves in waveguides
  • Investigate the impact of hole size on electromagnetic wave reflection and transmission
  • Learn about the applications of wire grid polarizers in electromagnetic systems
USEFUL FOR

Physicists, electrical engineers, and researchers in electromagnetic theory, particularly those interested in the design and analysis of Faraday cages and related structures.

MisterX
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I was looking for a mathematical explanation of a Faraday cage. In particular I was seeking something that relates hole size to the reflected and transmitted waves, using electromagnetic theory. This might also relate to a wire grid polarizer. Would anyone be able to help me?
 
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There are several ways of doing it, depending on how much you want to simplify and approximate.

For example, you can treat the cage as an infinite sheet with periodic holes. There are many methods, some analytic but generally more computational, that can solve for an infinite periodic mesh and find the Floquet modes that describe the transmission and reflection characteristics (EDIT: Remembered the word!).

You could also treat the holes as rectangular waveguides of a very small thickness. You could find the evanescent mode at your frequency for your given hole size and then approximate the power loss in the transmission. This would ignore the coupling between the holes that the above method takes into account. The loss of the evanescent mode depends upon the size of the hole.

Then there is the hand-wavy explanation. The gridded mesh, if the size of the holes are electrically small, behaves like a solid PEC sheet. This is realized from the fact that for an infinite PEC sheet, the induced currents from a plane wave are constant magnitude, lie in the same direction, and only differ in phase. A rectangular mesh therefore can support a superposition of currents that run in normal directions, so by decomposing any incident wave into the superposition of two plane waves we can see how the induced currents can be supported. The rule for the holes comes about because the ideal PEC sheet has a continuous distribution of currents whereas the mesh has a discrete stepping in the phase shift between current sources. So the hole size is dictated by the minimum phase shift that we can allow before we consider the reflection of the plane wave to be unsupportable.
 
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