Questions about EM wave in material

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SUMMARY

This discussion focuses on the analysis of electromagnetic (EM) wave propagation in materials and the calculation of induced current density. To determine current density, one must utilize Maxwell's Equations rather than kinematic equations, and the relationship involves charge density multiplied by velocity (ρv). The ability of EM waves to propagate is influenced by material properties, with good conductors like gold, silver, copper, and aluminum effectively preventing RF and microwave waves from propagating due to their high conductivity. Additionally, the thickness of the material relative to the wavelength plays a critical role in wave attenuation.

PREREQUISITES
  • Maxwell's Equations
  • Poisson's Equation
  • Computational electromagnetic solvers (e.g., method of moments, finite difference time-domain, finite element method)
  • Understanding of material properties (permittivity and permeability)
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  • Study Maxwell's Equations in detail
  • Explore Poisson's Equation applications in electrostatics
  • Research computational electromagnetic solvers and their methodologies
  • Investigate the effects of material thickness on EM wave propagation
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Physicists, electrical engineers, and materials scientists interested in electromagnetic wave behavior in various materials and the computational methods used to analyze these phenomena.

kirk404
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How can I find the induced current density by EM wave in a material?
Should I have ma = Fbinding + Fdriving + Fdamping like treating it as a spring?
Then the current density should be charge density of the material x velocity (ρv), isn't it?
Is there any condition the EM wave cannot propagate?
Thank you very much!
 
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You would not use kinematic equations, you would use Maxwell's Equations and model the behavior of the charges in the bulk by the permittivity and permeability. This is a rather complex process though. If you are talking about the electrostatic case, then we use Poisson's Equation to find the potential, charge, and electric field distributions. If we are talking about electromagnetic waves, then we would use the full Maxwell Equations. The process to find the charge and current densities depend upon the material and geometry of the specific problem. This can be done in closed form for a small set of problems but in general we use computational electromagnetic solvers like the method of moments, finite difference time-domain, or finite element method to solve for the current and charge distributions.

As for preventing wave propagation, any loss in the material would cause this (dependent upon the thickness of the material with respect to the wavelength). In general, any good conductor, like gold, silver, copper, aluminium, have high enough conductivities that most RF and microwave electromagnetic waves are prevented from propagating. Low frequency waves (say kilohertz and below) will take a rather thick block of even a good conductor to extinguish. And for frequencies in the Terahertz range and above, there are additional physics like plasmonics and quantum that dictate the transparency of the material.
 

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