Scattering of Electromagnetic Waves by Many Nano-Wires

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 xˆm = (xm1, xm2) be its center, 1 ≤ m ≤ M , M =   M (a). It is assumed that the poin...

Full description

Bibliographic Details
Main Author: Alexander G. Ramm
Format: Article
Language:English
Published: MDPI AG 2013-07-01
Series:Mathematics
Subjects:
Online Access:http://www.mdpi.com/2227-7390/1/3/89
id doaj-3396a11a2b0f4194999850fe6dc27271
record_format Article
spelling doaj-3396a11a2b0f4194999850fe6dc272712020-11-24T23:48:15ZengMDPI AGMathematics2227-73902013-07-0113899910.3390/math1030089Scattering of Electromagnetic Waves by Many Nano-WiresAlexander G. RammElectromagnetic 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 xˆm = (xm1, xm2) be its center, 1 ≤ m ≤ M , M =   M (a). It is assumed that the points, xˆm, are distributed, so that N (∆)  = (1 / 2πa) * ∫∆ N (xˆ)dxˆ[1 + o(1)], where N (∆) is the number of points, xˆm, in an arbitrary open subset, ∆, of the plane, xoy. The function, N (xˆ) ≥ 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.http://www.mdpi.com/2227-7390/1/3/89metamaterialsrefraction coefficientEM wave scattering
collection DOAJ
language English
format Article
sources DOAJ
author Alexander G. Ramm
spellingShingle Alexander G. Ramm
Scattering of Electromagnetic Waves by Many Nano-Wires
Mathematics
metamaterials
refraction coefficient
EM wave scattering
author_facet Alexander G. Ramm
author_sort Alexander G. Ramm
title Scattering of Electromagnetic Waves by Many Nano-Wires
title_short Scattering of Electromagnetic Waves by Many Nano-Wires
title_full Scattering of Electromagnetic Waves by Many Nano-Wires
title_fullStr Scattering of Electromagnetic Waves by Many Nano-Wires
title_full_unstemmed Scattering of Electromagnetic Waves by Many Nano-Wires
title_sort scattering of electromagnetic waves by many nano-wires
publisher MDPI AG
series Mathematics
issn 2227-7390
publishDate 2013-07-01
description 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 xˆm = (xm1, xm2) be its center, 1 ≤ m ≤ M , M =   M (a). It is assumed that the points, xˆm, are distributed, so that N (∆)  = (1 / 2πa) * ∫∆ N (xˆ)dxˆ[1 + o(1)], where N (∆) is the number of points, xˆm, in an arbitrary open subset, ∆, of the plane, xoy. The function, N (xˆ) ≥ 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.
topic metamaterials
refraction coefficient
EM wave scattering
url http://www.mdpi.com/2227-7390/1/3/89
work_keys_str_mv AT alexandergramm scatteringofelectromagneticwavesbymanynanowires
_version_ 1725486393425133568