Scattering of longitudinal waves (sound) by defects in fluids. Rough surface

B. Apostol
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引用次数: 2

Abstract

The classical theory of scattering of longitudinal waves (sound) by small inhomogeneities (scatterers) in an ideal fluid is generalized to a distribution of scatterers and such as to include the effect of the inhomogeneities on the elastic properties of the fluid. The results are obtained by a new method of solving the wave equation with spatial restrictions (caused by the presence of the scatterers), which can also be applied to other types of inhomogeneities (like surface roughness, for instance). A coherent forward scattering is identified for a uniform distribution of scatterers (practically equivalent with a mean-field approach), which is due to the fact that our treatment does not include multiple scattering. The reflected wave is obtained for a half-space (semi-infinite fluid) of uniformly distributed scatterers, as well as the field diffracted by a perfect lattice of scatterers. The same method is applied to a (inhomogeneous) rough surface of a semi-infinite ideal fluid. A perturbation-theoretical scheme is devised, with the roughness function as a perturbation parameter, for computing the waves scattered by the surface roughness. The waves scattered by the rough surface are both waves localized (and propagating only) on the surface (two-dimensional waves) and waves reflected back in the fluid. They exhibit directional effects, slowness, attenuation or resonance phenomena, depending on the spatial characteristics of the roughness function. The reflection coefficients and the energy carried on by these waves are calculated both for fixed and free surfaces. In some cases, the surface roughness may generate waves confined to the surface (damped, rough-surface waves).
纵波(声音)在流体中的散射。粗糙表面
经典的纵波(声音)在理想流体中被小的不均匀性(散射体)散射的理论被推广到散射体的分布,从而包括不均匀性对流体弹性特性的影响。该结果是通过求解具有空间限制(由散射体的存在引起)的波动方程的新方法获得的,该方法也可以应用于其他类型的不均匀性(例如表面粗糙度)。对于均匀分布的散射体(实际上相当于平均场方法),确定了相干前向散射,这是由于我们的处理不包括多重散射。得到了均匀分布的散射体的半空间(半无限流体)反射波,以及由散射体的完美晶格衍射的场。同样的方法也适用于半无限理想流体的(非均匀)粗糙表面。以表面粗糙度函数为扰动参数,设计了一种计算表面粗糙度散射波的微扰理论格式。由粗糙表面散射的波既局限于(且仅传播)表面(二维波),又反射回流体中。它们表现出方向效应、缓慢、衰减或共振现象,这取决于粗糙度函数的空间特征。计算了固定表面和自由表面反射波的反射系数和能量。在某些情况下,表面粗糙度可能产生局限于表面的波(阻尼、粗糙表面波)。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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来源期刊
Central European Journal of Physics
Central European Journal of Physics 物理-物理:综合
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审稿时长
3.3 months
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