Behavior of Electromagnetic Waves in Different Media and by Ali Akdagli

By Ali Akdagli

This complete quantity completely covers wave propagation behaviors and computational suggestions for electromagnetic waves in numerous advanced media. The bankruptcy authors describe strong and complex analytic and numerical how you can clear up their particular electromagnetic difficulties for complicated media and geometries besides. This ebook may be of curiosity to electromagnetics and microwave engineers, physicists and scientists.

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2007). , New York, USA. Stuchly, S. , Sibbald, C. L. and Anderson, J. M. (1994). A new aperture admittance model for open-ended waveguides, IEEE Transactions on Microwave Theory and Techniques 42(2): 192–198. Weir, W. B. (1974). Automatic measurement of complex dielectric constant and permeability at microwave frequencies, Proceedings of the IEEE 62(1): 33–36. Wolfram Research, Inc. (2008). Mathematica v. , Champaign, Illinois, USA. , Liu, L. and Jiang, Z. (1987). Measurement of the dielectric properties of biological substances using an improved open-ended coaxial line resonator method, IEEE Transactions on Microwave Theory and Techniques MTT-35(12): 1424–1428.

Ferrite cylinder of radius r and tensor permeability μ The ferrite cylinders are used in many microwave nonreciprocal devices such as circulators, isolators and phase shifters. The nonreciprocal properties can be controlled 34 Behaviour of Electromagnetic Waves in Different Media Will-be-set-by-IN-TECH and Structures 8 by the direction and value of bias magnetization field. For the ferrite cylinder case the constitutive equations are expressed as follows: D = ε 0 ε f E, (9) B = μ0 μE, (10) We assume that tensor μ has the following dyadic form: μ = μ (iρ iρ + i ϕ i ϕ ) + jμ a (iρ i ϕ − i ϕ iρ ) + 1iz iz (11) γMs i with μ = 1 + δ2 −1 , μ a = δ2 −1 , δ = γH f , p = f , Hi denotes internal bias magnetic field intensity, Ms saturated magnetization and γ gyromagnetic coefficient of the ferrite.

K). In the homogeneous region around the investigated post configuration we define the artificial cylindrical or spherical surface S . The aim of analysis is to determine the relation between incident and scattered fields in the outer region on the surface S . In the first step we assume that objects are illuminated by an unknown incident field F inc (0) defined in global coordinate system. Depending on the formulation of the method these fields are defined as infinite series of cylindrical or spherical eigenfunctions with unknown coefficients.

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