Iop Concise Physics
2 total works
Modern Analytical Electromagnetic Homogenization
by Tom G. Mackay and Akhlesh Lakhtakia
Published 1 July 2015
Electromagnetic homogenization is the process of estimating the effective electromagnetic properties of composite materials in the long-wavelength regime, wherein the length scales of nonhomogeneities are much smaller than the wavelengths involved. This is a bird's-eye view of currently available homogenization formalisms for particulate composite materials. It presents analytical methods only, with focus on the general settings of anisotropy and bianisotropy.
The authors largely concentrate on `effective' materials as opposed to `equivalent' materials, and emphasize the fundamental (but sometimes overlooked) differences between these two categories of homogenized composite materials. The properties of an `effective' material represents those of its composite material, regardless of the geometry and dimensions of the bulk materials and regardless of the orientations and polarization states of the illuminating electromagnetic fields. In contrast, the properties of `equivalent' materials only represent those of their corresponding composite materials under certain restrictive circumstances.
The authors largely concentrate on `effective' materials as opposed to `equivalent' materials, and emphasize the fundamental (but sometimes overlooked) differences between these two categories of homogenized composite materials. The properties of an `effective' material represents those of its composite material, regardless of the geometry and dimensions of the bulk materials and regardless of the orientations and polarization states of the illuminating electromagnetic fields. In contrast, the properties of `equivalent' materials only represent those of their corresponding composite materials under certain restrictive circumstances.
Infinite-Space Dyadic Green Functions in Electromagnetism
by Muhammad Faryad and Akhlesh Lakhtakia
Published 6 August 2018
In any linear system, the input and the output are connected by means of a linear operator. When the input can be notionally represented by a function that is null valued everywhere except at a specific location in spacetime, the corresponding output is called the Green function in field theories. Dyadic Green functions are commonplace in electromagnetics, because both the input and the output are vector functions of space and time. This book provides a survey of the state-of-the-art knowledge of infinite space dyadic Green functions.