Seafloor acoustic backscattering strength and properties from published data

N. Chotiros
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引用次数: 3

Abstract

Over the past 50 years, a large number of bottom scattering measurements have been made at a very significant accumulated cost, particularly in the 10 kHz to 1 MHz range. While each measurement is valuable individually, the total collection is more valuable as a whole. The earliest measurements were made in the 1950s using simple sound sources and receivers, such as explosives and omni-directional hydrophones. In the 1960s, a large set of measurements were made with purpose-built sonar equipment by the Applied Research Laboratories of The University of Texas at Austin and others. The results indicated that backscattering strength increased with frequency, but later measurements did not uphold this trend. Another large set of measurements were made in the 1980s by the Applied Physics Laboratory of The University of Washington, which lead to further model development. Since then, many more measurements have been made by numerous institutions and individuals. No one measurement, or program of measurements, has been able to capture the diversity of the seabed. It appears that a database of all the published measurements is needed to fully comprehend the scope of the problem, and the physical processes involved. In parallel with the measurements, a number of models were developed. The earliest ones attempted to link backscattering strength to the sediment type or class, often represented by the mean grain size, in a purely empirical fashion. The earlier data sets appeared to support this approach but the trends are not supported by the database as a whole. Later models were based on physical representations. The seafloor is often modeled as a fluid with volume and roughness scattering mechanisms incorporated. More sophisticated models represented the seafloor as an elastic solid, and more recently as a poro-elastic medium. One objective has been to invert the acoustic backscatter measurements for sediment properties, but the data, so far, shows limited correlation between mean grain size and backscattering strength. The extant database may be used to explore the underlying physics. With respect to the sediment grain size, the scattering regime may be divided into a number of regimes. For grain sizes much smaller than the acoustic wavelength in water, the direct scattering from grains is weak and increases with frequency. This regime is only observed in the laboratory because in the real seafloor, other scattering mechanisms, including seafloor roughness such as sand ripples, and inclusions such as biogenic gas bubbles, and other fauna and flora often dominate the scattering process. In the next regime, where the grain size is of the same order of magnitude as the acoustic wavelength, the backscattering strength is well bounded. In this regime, models and data often agree. Finally, in the regime where the effective grain size is much larger than the acoustic wavelength, there is considerable variability in the data. In this regime, the concept of grain size is no longer useful, because the acoustic scattering is determined by facets rather than grains, and more work is needed to obtain usable relationships.
海底声波后向散射强度和特性
在过去的50年里,以非常高的累积成本进行了大量的底部散射测量,特别是在10 kHz至1 MHz范围内。虽然每一次测量都是有价值的,但作为一个整体,整个收集更有价值。最早的测量是在20世纪50年代进行的,使用的是简单的声源和接收器,比如炸药和全向水听器。在20世纪60年代,德克萨斯大学奥斯汀分校的应用研究实验室和其他机构用专用的声纳设备进行了大量的测量。结果表明,后向散射强度随频率增加而增加,但后来的测量结果并没有维持这一趋势。20世纪80年代,华盛顿大学应用物理实验室进行了另一组大型测量,这导致了进一步的模型开发。从那时起,许多机构和个人进行了更多的测量。没有任何一种测量或测量计划能够捕捉到海底的多样性。似乎需要一个包含所有已发表的测量数据的数据库,以充分理解问题的范围以及所涉及的物理过程。在进行测量的同时,还开发了许多模型。最早的研究试图以纯经验的方式将后向散射强度与沉积物类型或类别联系起来,通常由平均粒度表示。早期的数据集似乎支持这种方法,但整个数据库并不支持这种趋势。后来的模型是基于物理表征的。海底通常被模拟为包含体积和粗糙度散射机制的流体。更复杂的模型将海底描述为弹性固体,最近则将其描述为多孔弹性介质。一个目标是反演沉积物特性的声波后向散射测量,但到目前为止,数据显示平均粒度和后向散射强度之间的相关性有限。现有的数据库可用于探索底层物理。就沉积物粒度而言,散射状态可分为若干状态。对于比声波波长小得多的水中颗粒,颗粒的直接散射较弱,且随频率增加而增加。这种情况只能在实验室中观察到,因为在真实的海底,其他散射机制,包括海底粗糙度,如沙波纹,包裹体,如生物气泡,以及其他动物和植物群通常主导散射过程。在晶粒尺寸与声波波长相同数量级的下一状态下,后向散射强度被很好地限定。在这种情况下,模型和数据往往是一致的。最后,在有效粒径远大于声波波长的情况下,数据存在相当大的变异性。在这种情况下,晶粒尺寸的概念不再有用,因为声散射是由面而不是由晶粒决定的,需要更多的工作来获得可用的关系。
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