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A Generalized Expression for the Energy Density of Electromagnetic Waves in Media with Strong Temporal Dispersion

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Dan Anderson · 1972

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The study derives a generalized energy density expression for electromagnetic waves in lossless, homogeneous, isotropic media with temporal dispersion that includes higher-order correction terms.

Plain English Summary

Summary written for general audiences

Researchers derived a generalized expression for electromagnetic wave energy density in lossless, homogeneous, isotropic media with temporal dispersion. The expression generalizes the standard form by including higher-order derivatives of dielectric and permeability functions and field amplitudes. Correction terms become important for strong dispersion or broad band signals, as shown with a Gaussian chirp pulse example.

Why This Matters

A third-order expansion is provided, deemed sufficient for most practical purposes. The electric part of the energy density is a quadratic expression in amplitude and its derivatives, enabling detailed treatment of dispersion from higher-order derivatives. The method uses bilinear concomitants and adjoint operators, which the author finds convenient for energy density and flow studies in dispersive media.

Cite This Study
Dan Anderson (1972). A Generalized Expression for the Energy Density of Electromagnetic Waves in Media with Strong Temporal Dispersion.
Show BibTeX
@article{a_generalized_expression_for_the_energy_density_of_electromagnetic_waves_in_medi_g7224,
  author = {Dan Anderson},
  title = {A Generalized Expression for the Energy Density of Electromagnetic Waves in Media with Strong Temporal Dispersion},
  year = {1972},
  
  
}
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Quick Questions About This Study

The study derives a generalized expression for the energy density of electromagnetic waves in lossless, homogeneous, isotropic media with temporal dispersion.
Correction terms are important for strong dispersion and/or broad band signals.
A Gaussian chirp pulse in a simple medium demonstrates the importance of higher-order terms.