Signal Propagation and Detection in Lossy Media

  • Henning F. Harmuth
  • Raouf N. Boules
  • Malek G. M. Hussain

Abstract

We start with the modified Maxwell equations of Section 1.1. They were written in Section 2.1 for Cartesian coordinates and planar TEM waves. The polarization was extracted by Eqs.(2.1–16), (2.1–17) and Eqs.(2.1–18), (2.1–19) were obtained. We can use these equations here but we leave out the indices i and 1 since we consider waves in one medium rather than at the boundary of two mediums:
$$\frac{{\partial E}}{{\partial y}} + \mu \frac{{\partial H}}{{\partial t}} + sH = 0$$
$$\frac{{\partial E}}{{\partial y}} + \in \frac{{\partial E}}{{\partial t}} + \sigma H = 0$$

Keywords

Permeability Dioxide Microwave Attenuation Ferrite 

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Copyright information

© Springer Science+Business Media New York 1999

Authors and Affiliations

  • Henning F. Harmuth
    • 1
  • Raouf N. Boules
    • 2
  • Malek G. M. Hussain
    • 3
  1. 1.Formerly of the Catholic University of AmericaUSA
  2. 2.Towson UniversityTowsonUSA
  3. 3.Kuwait UniversityKuwait

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