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...
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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 |
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1725486393425133568 |