Asymptotic solutions of the Helmholtz equation: generalised Friedlander-Keller ray expansions of fractional order

Applications of a WKBJ-type `ray ansatz' to obtain asymptotic solutions of the Helmholtz equation in the high{frequency limit are now standard, and underpin the construction of `geometrical optics' ray diagrams in many electromagnetic, acoustic and elastic reflection, transmission and othe...

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Main Author: Tew, R.H.
Format: Article
Published: Cambridge University Press 2020
Online Access:https://eprints.nottingham.ac.uk/52013/
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author Tew, R.H.
author_facet Tew, R.H.
author_sort Tew, R.H.
building Nottingham Research Data Repository
collection Online Access
description Applications of a WKBJ-type `ray ansatz' to obtain asymptotic solutions of the Helmholtz equation in the high{frequency limit are now standard, and underpin the construction of `geometrical optics' ray diagrams in many electromagnetic, acoustic and elastic reflection, transmission and other scattering problems. These applications were subsequently extended by Keller to include other types of rays - called `diffracted' rays - to provide an accessible and impressively accurate theory which is relevant in wide-ranging sets of circumstances. Friedlander and Keller then introduced a modified ray ansatz to extend yet further the scope of ray theory and its applicability to certain other classes of diffraction problems (tangential ray incidence upon an obstructing boundary, for instance), and did so by the inclusion of an extra term proportional to a power of the wavenumber within the exponent of the initial ansatz. Our purpose here is to generalise this further still by the inclusion of several such terms, ordered in a natural sequence in terms of strategically-chosen fractional powers of the large wavenumber, and to derive a systematic sequence of boundary value problems for the coefficient phase functions that arise within this generalised exponent, as well as one for the leading-order amplitude occurring as a pre-exponential factor. One particular choice of fractional power is considered in detail, and waves with specified radially-symmetric or planar wavefronts are then analysed, along with a boundary value problem typifying two-dimensional radiation whereby arbitrary phase and amplitude variations are specified on a prescribed boundary curve. This theory is then applied to the scattering of plane and cylindrical waves at curved boundaries with small-scale perturbations to their underlying profile.
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spelling nottingham-520132020-05-04T19:36:16Z https://eprints.nottingham.ac.uk/52013/ Asymptotic solutions of the Helmholtz equation: generalised Friedlander-Keller ray expansions of fractional order Tew, R.H. Applications of a WKBJ-type `ray ansatz' to obtain asymptotic solutions of the Helmholtz equation in the high{frequency limit are now standard, and underpin the construction of `geometrical optics' ray diagrams in many electromagnetic, acoustic and elastic reflection, transmission and other scattering problems. These applications were subsequently extended by Keller to include other types of rays - called `diffracted' rays - to provide an accessible and impressively accurate theory which is relevant in wide-ranging sets of circumstances. Friedlander and Keller then introduced a modified ray ansatz to extend yet further the scope of ray theory and its applicability to certain other classes of diffraction problems (tangential ray incidence upon an obstructing boundary, for instance), and did so by the inclusion of an extra term proportional to a power of the wavenumber within the exponent of the initial ansatz. Our purpose here is to generalise this further still by the inclusion of several such terms, ordered in a natural sequence in terms of strategically-chosen fractional powers of the large wavenumber, and to derive a systematic sequence of boundary value problems for the coefficient phase functions that arise within this generalised exponent, as well as one for the leading-order amplitude occurring as a pre-exponential factor. One particular choice of fractional power is considered in detail, and waves with specified radially-symmetric or planar wavefronts are then analysed, along with a boundary value problem typifying two-dimensional radiation whereby arbitrary phase and amplitude variations are specified on a prescribed boundary curve. This theory is then applied to the scattering of plane and cylindrical waves at curved boundaries with small-scale perturbations to their underlying profile. Cambridge University Press 2020-02 Article PeerReviewed Tew, R.H. (2020) Asymptotic solutions of the Helmholtz equation: generalised Friedlander-Keller ray expansions of fractional order. European Journal of Applied Mathematics, 31 (1). ISSN 1469-4425 https://www.cambridge.org/core/journals/european-journal-of-applied-mathematics/article/asymptotic-solutions-of-the-helmholtz-equation-generalised-friedlanderkeller-ray-expansions-of-fractional-order/9E162EEF38941D0A01F69909CD01676E doi:10.1017/S095679251800044X doi:10.1017/S095679251800044X
spellingShingle Tew, R.H.
Asymptotic solutions of the Helmholtz equation: generalised Friedlander-Keller ray expansions of fractional order
title Asymptotic solutions of the Helmholtz equation: generalised Friedlander-Keller ray expansions of fractional order
title_full Asymptotic solutions of the Helmholtz equation: generalised Friedlander-Keller ray expansions of fractional order
title_fullStr Asymptotic solutions of the Helmholtz equation: generalised Friedlander-Keller ray expansions of fractional order
title_full_unstemmed Asymptotic solutions of the Helmholtz equation: generalised Friedlander-Keller ray expansions of fractional order
title_short Asymptotic solutions of the Helmholtz equation: generalised Friedlander-Keller ray expansions of fractional order
title_sort asymptotic solutions of the helmholtz equation: generalised friedlander-keller ray expansions of fractional order
url https://eprints.nottingham.ac.uk/52013/
https://eprints.nottingham.ac.uk/52013/
https://eprints.nottingham.ac.uk/52013/