Special Topics in Electromagnetics
eBook - ePub

Special Topics in Electromagnetics

Kun-Mu Chen

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  1. 228 pages
  2. English
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eBook - ePub

Special Topics in Electromagnetics

Kun-Mu Chen

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About This Book

A primary resource for graduate teaching and research in advanced electromagnetic materials, Special Topics in Electromagnetics covers some new methods for treating the interaction of electromagnetic field with materials, as well as biological applications and radar identification using electromagnetic waves. This book supplements its content with detailed mathematical derivation and covers some practical applications.

Contents:

  • General Maxwell's Equations and Solutions
  • Vector Wave Functions and Applications
  • Dyadic Green's Functions and Applications
  • Biomedical Application of Electromagnetic Waves
  • Radar Target Identification with Extinction-Pulse (E-Pulse) Method


Readership: Graduate and research students and working professionals interested in the field of electromagnetics.

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Information

Publisher
WSPC
Year
2013
ISBN
9789814412193
Chapter 1
General Maxwell’s Equations and Solutions
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Modified Maxwell’s Equations with Magnetic Source Terms
Conventional Maxwell’s equations which express the relations between the field vectors, the electric field
images
and the magnetic induction
images
, and the source current density
images
and charge density ρ are usually written in the following form :
images
where the displacement vector
images
and the magnetic field
images
are defined by
images
with
images
as the polarization density,
images
as the magnetization density, and Δ0 and Ό0 are permittivity and permeability of the free space.
The source current density
images
and source charge density ρ are related by the equation of continuity:
images
In a simple medium,
images
Where Δ and Ό are the permittivity and permeability of the medium.
The Maxwell’s equations expressed in Eqs. (1.1) to (1.4) are not symmetrical mathematically. Equations (1.1) and (1.2) are different in form and so are Eqs. (1.3) and (1.4) as the result. Why? Because the elementary source for the electric field
images
is different from that of the magnetic field
images
. Eq. (1.3) implies that
images
field starts from or terminates at an electric charge ρ. However, Eq. (1.4) implies that
images
field does not start from or terminate at a magnetic charge. This is due to the fact that there exists no real magnetic charge (or magnetic monopole). In fact, the smallest unit of the magnetic source is a magnetic dipole which is actually an infinitesimal current loop. The situation is depicted in Fig. 1a. This is the conventional thinking even though there are some reports on the discovery of magnetic monopoles. If these reports are verified in the future, it would not alter the following derivation of t...

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