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复杂介质中声波的多次散射建模与分析:在小梁骨中的应用。

Modeling and analysis of multiple scattering of acoustic waves in complex media: application to the trabecular bone.

机构信息

Department of Ultrasound, Institute of Fundamental Technological Research, Polish Academy of Sciences, Pawińskiego 5b Str., 02-106, Warsaw, Poland.

出版信息

J Acoust Soc Am. 2011 Oct;130(4):1908-18. doi: 10.1121/1.3625285.

Abstract

The integral equations that describe scattering in the media with step-rise changing parameters have been numerically solved for the trabecular bone model. The model consists of several hundred discrete randomly distributed elements. The spectral distribution of scattering coefficients in subsequent orders of scattering has been presented. Calculations were carried on for the ultrasonic frequency ranging from 0.5 to 3 MHz. Evaluation of the contribution of the first, second, and higher scattering orders to total scattering of the ultrasounds in trabecular bone was done. Contrary to the approaches that use the μCT images of trabecular structure to modeling of the ultrasonic wave propagation condition, the 3D numerical model consisting of cylindrical elements mimicking the spatial matrix of trabeculae, was applied. The scattering, due to interconnections between thick trabeculae, usually neglected in trabecular bone models, has been included in calculations when the structure backscatter was evaluated. Influence of the absorption in subsequent orders of scattering is also addressed. Results show that up to 1.5 MHz, the influence of higher scattering orders on the total scattered field characteristic can be neglected while for the higher frequencies, the relatively high amplitude interference peaks in higher scattering orders clearly occur.

摘要

对于具有阶跃变化参数的介质中的散射,已经对描述这些散射的积分方程进行了数值求解,该模型由几百个离散随机分布的元素组成。给出了在后续散射阶次中的散射系数的光谱分布。计算是针对从 0.5 到 3 MHz 的超声频率进行的。评估了第一、第二和更高阶散射对骨小梁中超声总散射的贡献。与使用骨小梁结构的 μCT 图像进行超声波传播条件建模的方法相反,应用了由模拟骨小梁空间矩阵的圆柱形元素组成的 3D 数值模型。当评估结构反向散射时,包括了通常在骨小梁模型中忽略的厚骨小梁之间的连接引起的散射。还研究了后续散射阶次的吸收的影响。结果表明,在 1.5MHz 以下,高阶散射对总散射场特性的影响可以忽略不计,而对于较高频率,较高阶次中的相对较高幅度的干涉峰明显出现。

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