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Lecture 2 Notes, Electromagnetic Theory II

Lecture 2 Notes, Electromagnetic Theory IIDr. Christopher S. Baird, of Massachusetts Lowell1. Dispersion introduction - An Electromagnetic wave with an arbitrary wave-shape can be thought of as a superposition of single-frequency plane If the dielectric material responds in the exact same way to plane waves of any frequency, then each component of the wave-shape will travel at the same speed, and the overall wave-shape will be If the dielectric material responds differently to plane waves of different frequencies ( the material's dielectric constant is frequency dependent), then the various components of a wave-shape will travel at different speeds.

Lecture 2 Notes, Electromagnetic Theory II Dr. Christopher S. Baird, faculty.uml.edu/cbaird University of Massachusetts Lowell 1. Dispersion Introduction - An electromagnetic wave with an arbitrary wave-shape can be thought of as a superposition of single-frequency plane waves.

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