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Ultrasonic field patterns and broadband imaging-simulations in transversely isotropic media

机译:横观各向同性介质中的超声场模式和宽带成像模拟

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摘要

Thorough application of NDE — and imaging techniques in anisotropic media has to overcome those inherent problems like beam splitting, beam distortion and deviation between wave propagation direction and energy flow, known as beam skewing. A theory of elastic wave propagation in transversely isotropic media which properly accounts for these effects has been presented previously [1], an overview has been presented at last year’s conference [2]. Analytic expressions have been derived characterizing the propagation of Gaussian Wave Packets (GWPs) in these media thus making possible the simulation of real pulse propagation. In order to provide information from a practical point of view the theory has been evaluated to yield field patterns of GWPs in unidirectional graphite-epoxy as well as centrifugally cast stainless steel. The plane wave spectral decomposition of Green’s dyadic and triadic functions, also presented last year, has been used to derive the algorithm of forward-backward-propagation of elastic wavefields yielding a simple solution to the inverse problem, the so-called elastodynamic holography. With this basic imaging technique, field distributions of GWPs are propagated forth and back; for comparison, the conventional isotropic algorithm [3] is also applied, resulting in field distributions which differ both in intensity and position. Finally the simulations, being evaluated in frequency domain, are performed at multiple frequencies thus in principle making up a mode-matched FT-SAFT [4], neglecting the vector scattering amplitudes.
机译:在各向异性介质中彻底使用NDE和成像技术必须克服那些固有的问题,例如光束分裂,光束畸变以及波传播方向与能量流之间的偏差(称为光束偏斜)。先前已经提出了适当地解释这些影响的横波各向同性介质中弹性波传播的理论[1],在去年的会议上也做了概述[2]。已经推导出了解析表达式,表征了高斯波包(GWP)在这些介质中的传播,从而使真实脉冲传播的仿真成为可能。为了从实际角度提供信息,已对该理论进行了评估,以产生单向石墨-环氧树脂以及离心铸造不锈钢中的GWP的场模式。去年同样提出的格林的二元和三元函数的平面波谱分解已被用于推导弹性波场的向前-向后传播算法,从而产生了反问题的简单解决方案,即所谓的弹性动力学全息图。利用这种基本的成像技术,GWP的场分布前后传播。为了进行比较,还应用了传统的各向同性算法[3],从而导致强度和位置都不同的场分布。最后,在频域上进行评估的仿真是在多个频率上执行的,因此原则上构成了模式匹配的FT-SAFT [4],而忽略了矢量散射幅度。

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