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统一标量波动方程齐次格林函数的单侧表示。

A single-sided representation for the homogeneous Green's function of a unified scalar wave equation.

作者信息

Wapenaar Kees

机构信息

Department of Geoscience and Engineering, Delft University of Technology, Stevinweg 1, 2628 CN Delft, the Netherlands.

出版信息

J Acoust Soc Am. 2017 Jun;141(6):4466. doi: 10.1121/1.4985387.

Abstract

A unified scalar wave equation is formulated, which covers three-dimensional (3D) acoustic waves, 2D horizontally-polarised shear waves, 2D transverse-electric EM waves, 2D transverse-magnetic EM waves, 3D quantum-mechanical waves and 2D flexural waves. The homogeneous Green's function of this wave equation is a combination of the causal Green's function and its time-reversal, such that their singularities at the source position cancel each other. A classical representation expresses this homogeneous Green's function as a closed boundary integral. This representation finds applications in holographic imaging, time-reversed wave propagation and Green's function retrieval by cross correlation. The main drawback of the classical representation in those applications is that it requires access to a closed boundary around the medium of interest, whereas in many practical situations the medium can be accessed from one side only. Therefore, a single-sided representation is derived for the homogeneous Green's function of the unified scalar wave equation. Like the classical representation, this single-sided representation fully accounts for multiple scattering. The single-sided representation has the same applications as the classical representation, but unlike the classical representation it is applicable in situations where the medium of interest is accessible from one side only.

摘要

推导了一个统一的标量波动方程,它涵盖三维(3D)声波、二维水平极化剪切波、二维横向电电磁波、二维横向磁电磁波、三维量子力学波和二维弯曲波。该波动方程的齐次格林函数是因果格林函数及其时间反转的组合,使得它们在源位置的奇点相互抵消。一种经典表示将此齐次格林函数表示为封闭边界积分。这种表示在全息成像、时间反转波传播以及通过互相关进行格林函数检索中得到应用。在这些应用中,经典表示的主要缺点是它需要能够接触到感兴趣介质周围的封闭边界,而在许多实际情况中,介质只能从一侧接触到。因此,为统一标量波动方程的齐次格林函数推导了一种单侧表示。与经典表示一样,这种单侧表示充分考虑了多次散射。单侧表示与经典表示具有相同的应用,但与经典表示不同的是,它适用于感兴趣介质只能从一侧接触到的情况。

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