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Microstructure Sources of Sound Backscattering in a Stratified Flow

机译:分层流动中声音反向散射的微观结构源

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Investigation of sound-scattering mechanisms is of key importance in the development of adequate algorithms for remote diagnostics of the ocean. According to modern concepts, the basic mechanism responsible for the generation of scattering inhomogeneities is assumed to be a turbulent microstructure with an intrinsic scale on the order of the sound wavelength λ. In this case, maximum scattering intensity is expressed in terms of the spectral fluctuation density of sound speed, which is taken at the doubled wavenumber 2k_0 = 4π/λ of the incident sound wave [1-3]. Since natural stratified flows are known to be inhomogeneous in depth, such a regularity must be valid only at certain horizons in which there exists the developed turbulence. However, from the data of full-scale tests performed in ocean, it follows that the vertical cross-section profiles of scattering strongly correlate with the spectral density of temperature fluctuations in the entire range of probed depths [4, 5]. This implies that the mechanism underlying the formation of the sound-scattering microstructure may be of non-turbulent origin.
机译:声音散射机制的研究对于开发用于海洋远程诊断的适当算法至关重要。根据现代概念,负责产生散射不均匀性的基本机理被假定为湍流微结构,其固有尺度为声波长λ的数量级。在这种情况下,最大散射强度以声速的频谱波动密度表示,在入射声波的两倍波数2k_0 =4π/λ处获得[1-3]。由于已知自然分层流在深度上是不均匀的,因此这种规律性仅在存在已发展湍流的某些层级才有效。然而,从在海洋中进行的全面测试数据来看,散射的垂直截面轮廓与整个探测深度范围内的温度波动谱密度密切相关[4,5]。这意味着,声散射微结构形成的基础机制可能是非湍流起源的。

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