Abstract

Electromagnetic wave scattering by many parallel to the z−axis, thin, impedance, parallel, infinite cylinders is studied asymptotically as a → 0. Let Dm be the cross-section of the m−th cylinder, a be its radius and x ^ m = (x m1 , x m2 ) be its center, 1 ≤ m ≤ M , M = M (a). It is assumed that the points, x ^ m , are distributed, so that N(Δ)= 1 2πa ∫ Δ N ( x ^ )d x ^ [1+o(1)] where N (∆) is the number of points, x ^ m , in an arbitrary open subset, ∆, of the plane, xoy. The function, N( x ^ ) ≥0 , is a continuous function, which an experimentalist can choose. An equation for the self-consistent (effective) field is derived as a → 0. A formula is derived for the refraction coefficient in the medium in which many thin impedance cylinders are distributed. These cylinders may model nano-wires embedded in the medium. One can produce a desired refraction coefficient of the new medium by choosing a suitable boundary impedance of the thin cylinders and their distribution law.

Highlights

  • There is a large literature on electromagnetic (EM) wave scattering by an array of parallel cylinders

  • Electromagnetic wave scattering by many parallel to the z−axis, thin, circular, of radius a, infinite cylinders, on the boundary of which an impedance boundary condition holds, is studied in this paper asymptotically as a → 0

  • One sees from formula (19) that it is sufficient to find one number, Q, in order to solve the scattering problem, (11)–(13), for one thin cylinder

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Summary

Introduction

There is a large literature on electromagnetic (EM) wave scattering by an array of parallel cylinders (see, e.g., [1], where there are many references given, and [2]). Our results include formulas for the solution to the scattering problem, the derivation of the equation for the effective field in the medium obtained by embedding many thin perfectly conducting cylinders and a formula for the refraction coefficient in this limiting medium. This formula shows that by choosing a suitable distribution of the cylinders, one can change the refraction coefficient, for example, one can make it smaller than the original one.

EM Wave Scattering by One Thin Perfectly Conducting Cylinder
Wave Scattering by Many Thin Cylinders
Conclusions

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