典型深海声场频率-距离干涉结构分析及实验研究

基于射线理论分析了在典型深海情况下声源与接收水听器位于海水表层时声场频率-距离干涉结构,给出了直达声作用区与影区情况下声场频率-距离干涉结构的近似理论表达式。数值仿真与实验结果表明:在直达声作用区内,由直达声与海面一次反射声形成声场干涉结构,频率域干涉周期为该两条声线到达时间差的倒数;在影区内,由声源-海底-接收器、声源-海面-海底-接收器、声源-海底-海面-接收器和声源-海面-海底-海面-接收器四条声线形成声场干涉结构,声强随着频率具有两种干涉周期,分别随着声源深度、接收水听器深度的增大而减小,并与收发距离有关。本文给出的理论表达式可以较好的解释实验观测到的声场频率-距离干涉结构。      

深海近距离声场频率-距离干涉结构反演海底声学参数

地声反演一般存在多解性的问题,不易有效分离沉积层声速与厚度,本文提出了一种当声源与接收水听器分别位于海面与海底附近时匹配声场干涉周期反演深海沉积层声速与厚度的方法。该声场周期结构由直达波与海底沉积层反射回波干涉形成,其干涉周期受沉积层声速和厚度影响,通过匹配实测与理论计算的声场干涉周期可有效反演沉积层声速和厚度。开展了深海实验验证,利用水听器接收到的近距离船舶噪声的声场干涉条纹,反演得到的实验海域海底沉积层声速与该海域海底表层采样平均值差小于20 m/s。数值仿真与实验结果表明该方法可以有效反演沉积层的声速与厚度。      

利用深海海底声反射区频域干涉结构的声源深度估计方法

提出了一种基于深海海底声反射区声场频域干涉结构特征的水下宽带近海面声源深度估计方法。该方法通过建立深海海底声反射区到达声场结构模型,推导了垂直阵接收信号波束输出幅度谱的近似表达式,利用幅度谱与声源深度和垂直到达角(俯仰角)之间的周期变化关系,将接收信号映射到深度-垂直到达角域中,实现了对宽带声源的深度估计。仿真实验与影响因素分析验证了该原理的正确性,南海实验结果表明:利用阵长为64 m的垂直短阵接收标定深度为50 m和100 m的双弹信号,得到的深度估计结果同实际声源深度吻合较好,估计误差不超过7%,验证了该方法的有效性。     

利用宽带声场频率-掠射角干涉结构的深海直达声区目标深度估计方法

针对典型深海环境中宽带声源的深度分辨问题,通过研究深海声场随频率起伏的干涉结构与垂直线阵频域波束输出图中的干涉结构,给出一种直达声区内可区分多水下目标的宽带声源深度估计方法。该方法以近水面目标的射线声场模型为基础,推导出近海面宽带声源接收声场的波束输出表达式,阐明了频域波束输出图中干涉结构与声源深度的对应关系。然后利用改进的傅里叶变换方法将二维频域波束输出图映射到声源深度-掠射角度域,可实现声源深度信息的有效分离。最后开展了深海实验验证,利用垂直阵接收拖曳声源发射的宽带白噪声信号,拖曳声源深度计算结果与实测声源深度基本一致。数值仿真与实验结果均表明该方法可以在多目标复杂环境下准确估计出水下宽带声源的深度。      

深海海底声反射区多途时延差分析与近海面声源定位

深海海底反射声工作方式下的声场主要由4条一次海底反射声线路径构成。根据4条声线路径到达接收点的时间不同,可以得到6个不同的声线到达时延差值,当声源位于近海面时, 6条声线路径的时延差曲线随接收深度近似呈线性变化。本文基于虚源理论推导了海底声反射区的多途到达时延结构,给出了6条声线路径的时延差曲线随接收深度变化的近似表达式,通过分析时延差曲线与声源水平距离和深度之间的关系,提出了一种利用多途时延差估计深海海底声反射区近海面声源距离与深度的方法,仿真实验与影响因素分析验证了该原理的正确性。南海实验结果表明,当收发距离在10～33 km时,距离估计结果和深度估计结果都同实际声源距离和深度吻合较好,估计误差不超过15%,验证了该方法的有效性。     

高速垂向运动声源声场干涉特性及其可观测性

以高速垂向运动声源宽带连续谱噪声为研究对象,基于射线理论分析了声场干涉现象的产生机理,推导了干涉条纹的轨迹方程,讨论了影响干涉结构特性的因素,揭示了声场干涉结构的特性和规律。理论和仿真结果表明:干涉周期与多途信号时延差成反比关系;减小接收深度或增大接收距离可以提高干涉条纹的可观测性;较大的海面起伏易使干涉条纹形成断点,可观测性降低。湖试数据分析结果表明,干涉条纹主要由直达声-海面反射声干涉条纹构成,干涉条纹宽度和干涉周期随水平距离的增大而增大。该结果可为高速垂向运动声源运动状态分析、环境参数反演等提供参考。     

深海大深度声场垂直相关特性

深海声场垂直相关特性对提高垂直阵阵列增益和水下目标探测性能具有重要意义.基于2014年南中国海实验大跨度垂直阵接收的声信号,分析了深海直达区、影区和会聚区等不同距离下的大深度声场垂直相关特性,并使用射线理论解释了深海垂直相关随空间变化机理.在直达声区内,声场垂直相关半径几乎可以覆盖整个水深,且随着深度增加,直达声和海面反射声到达时间差增加,相关略有下降.在声影区内,声场能量主要来源为经一次海底反射和一到两次海面反射的声线,垂直相关整体偏低.第一会聚区内垂直相关系数随着接收深度的增加而周期性振荡,并且与声能量在深度上的分布具有相似结构,这是高声强区域两组反转声线在垂直方向上周期性干涉的结果.     

深海脉冲信号簇到达结构特征及其在水下声源定位中的应用

为了实现对深海水下声源的定位,对典型深海环境中的脉冲信号到达结构特征进行了理论分析,给出了声源和接收位置位于近海面时到达信号的簇信号形式近似表达式。当声源和接收位置处于近海面深度时,接收到的信号呈簇状结构形式。在提取到达信号中各簇信号到达时间、幅值等特征参数的基础上,提出了一种通过对到达信号中簇信号特征参数匹配搜索进行水下脉冲信号定位的方法,仿真分析了不同距离和不同深度处的簇信号特征,并利用一次南海海域爆炸声源的声传播实验数据进行了实验验证。结果表明:各簇信号对应的到达时间、幅值等特征参数可用于对声源位置的匹配定位;海上实验中利用单水听器得到的水下声源的距离估计结果与实测距离结果较为一致,对实验中2.0 km至90.4 km内声源的距离估计误差不大于8%。      

深海大深度声传播特性及直达声区水下声源距离估计

深海大深度声传播特性对在深海近海底进行水声目标探测和定位具有重要意义。利用一次南海中南部深海不完全声道中的脉冲声传播实验数据,分析了海底附近大深度声传播损失及脉冲多途传播特性,并根据直达波和海底-海面反射波的时延差与收发距离的关系,提出一种利用深海直达声区脉冲多途到达时间进行水下声源距离估计的方法。结果表明:当接收器深度位于南海深海海底附近而声源深度较浅时,直达声区水平宽度可达30 km,传播损失相对影区来说较小,有利于水下声源探测;直达声区的直达波与海底-海面反射波的到达时延差随着收发距离的增大单调减小,可被用于水下声源距离估计。得到水下声源的距离估计结果与实验GPS测量结果较为一致,距离估计均方误差为0.28 km。      

利用波导不变量的浅海负跃层声源深度判别

在夏季负跃层水文条件下,声源激发的声场同时存在折射类和反射类简正波,导致通过分离简正波进行深度判别的方法性能下降甚至失效·提出了一种利用波导不变量判别声源深度的方法。当接收器位于负跃层以下时,水面声源和水下声源的波导不变量数值不同。在本文的仿真条件下,水面声源波导不变量约等于1,当声源位于负跃层以下时,波导不变量大于1.利用频域warping变换从干涉结构中提取与实际距离成线性关系的时域脉冲,可以在未知声源距离的情况下,从声场干涉结构中获得声源激发声场的波导不变量,从而在夏季负跃层水文条件下进行声源深度判别。方法无须声源与接收器存在最近经过距离,可适用于单水听器或水平阵波束形成后输出的LOFAR谱.仿真结果证明,方法可以提取水面目标和水下目标的时延轨迹并计算干涉条纹的波导不变量。最后,对海试实验数据进行分析处理,从水面声源的干涉条纹中提取波导不变量,证明了方法的有效性。      

基于矢量水听器的深海直达波区域声传播特性及其应用

对于深海近水面声源产生的声场, 处于较大深度处的接收器在一定水平距离范围内能接收到直达波. 2014年在某深海海域进行的水声考察实验中, 应用深度为140 m的拖曳声源发射实验信号, 布放在水下3146 m深处的矢量水听器成功地接收到了直达波信号. 本文应用射线理论, 分析了深海直达波区域声场的传播特性, 得出了水平振速与垂直振速的传播损失与声线到达接收点处的掠射角以及收发水平距离之间的关系. 在以上分析的基础上, 提出了一种利用水平振速与垂直振速的能量差估计声源距离的方法, 并结合2014年实验数据对实验中两条航线上8 km范围内的目标声源进行了测距, 测距结果与目标的GPS数据符合得较好.     

The characteristic of sound propagation in deep water and underwater source localization in the direct zone

The multiple-path sound propagation in deep water is conducive to source localization of an underwater target.The transmission losses(TLs) and broadband pulse multiple-path propagation characteristics from a deep receiver is analyzed by using the experimental data from deep water area in the South China Sea(SCS).The results indicate that the width of the direct zone near the bottom of 4300 m water depth is about 30 km.The TLs in the direct zone near the bottom are much less than those in the shadow zone.It is meaningful for underwater sound source detection.Moreover,the time delay between the direct path and the bottomsurface-reflected path for a receiver near the bottom decreases monotonically with the source range.According to the linear relationship between the time delay of multipath and source range,a source localization method is presented to estimate the range of underwater target.The experimental results show that the estimated ranges are consistent with the global position system(GPS) measurements,and the mean square error of the estimation results is less than 0.28 km.     

Illumination of the shadow zone in a two-channel oceanic waveguide with a fine structure of sound speed inhomogeneities

The experimental data on the sound field structure, which were obtained by emitting a continuous pseudonoise signal (a midfrequency of 3.2 kHz) in a two-channel oceanic waveguide, are compared with the calculations performed by the wave program with allowance for the fine structure of the sound speed inhomogeneities. A considerable increase in the intensity of the sound field with a definite angular spectrum is observed in the upper channel in the first shadow zone, and, in the experiment, the increase begins nearer to the sound source than predicted by the wave and ray calculations for a smooth sound speed profile. These features of the field structure are explained by the illumination of the shadow zone by the regular scattering of signals from highly anisotropic fine-structure inhomogeneities of the sound speed profile, which are clearly pronounced in the region of the given oceanic experiment.     

Long-range sound propagation in the region of the subarctic front

The data of two experiments performed in the northwestern Pacific are presented. The propagation path crosses the northern boundary of the subarctic frontal zone. The influence of the frontal zone on the time structure and intensity of the sound field is studied. This influence most clearly manifests itself in the range dependence of the level of the normalized sound field at frequencies of 63–800 Hz. In the region of crossing the boundary of the frontal zone, a change of 1.5–2 dB in the sound field level is observed with localization in distance. In this region, a pronounced increase in the frequency-independent component of the exponential attenuation is also observed (by 0.015 dB/km for explosion-generated signals received at a depth of 600 m). At depths of 150–800 m, a zone of weak variations of the propagation loss is present in the vertical structure of the sound field at the 100-km part of the path in the region of crossing the front. In the experiment with explosion-generated signals, phenomena that are unrelated to the frontal zone are observed as well, namely, the appearance of reverberation forerunners (prereverberation) on separate parts of the path and the presence of bottom-reflected signals on one of the path fractions with a local bottom rise.     

Vertical amplitude phase structure of a low-frequency acoustic field in shallow water

We obtain in integral and analytic form the relations for calculating the amplitude and phase characteristics of an interference structure of orthogonal projections of the oscillation velocity vector in shallow water. For different frequencies and receiver depths, we numerically study the source depth dependences of the effective phase velocities of an equivalent plane wave, the orthogonal projections of the sound pressure phase gradient, and the projections of the oscillation velocity vector. We establish that at low frequencies in zones of interference maxima, independently of source depth, weakly varying effective phase velocity values are observed, which exceed the sound velocity in water by 5–12%. We show that the angles of arrival of the equivalent plane wave and the oscillation velocity vector in the general case differ; however, they virtually coincide in the zone of the interference maximum of the sound pressure under the condition that the horizontal projections of the oscillation velocity appreciably exceed the value of the vertical projection. We give recommendations on using the sound field characteristics in zones with maximum values for solving rangefinding and signal-detection problems.     

Spectrogram and localization of a sound source in shallow water

The paper describes an approach to detecting a sound source and estimating the radial velocity and distance from the receiver, based on repeat Fourier transformation of the interference pattern formed during motion. The obtained spectrogram contains localized domains of the spectral density of single modes. We estimate the localization domain and spectral density distribution and discuss the resolution of moving sound sources. We present the results of a field experiment and consider the interference immunity of the approach for localizing a source using a single receiver.     

利用海底反射信号进行地声参数反演的方法

针对现有反演方法的缺点,提出了一种基于海底反射信号的地声参数高分辨反演方法.它利用短距离声源在不同深度上发射宽带线性调频信号,采用垂直阵进行接收,首先通过匹配滤波方法提取多径到达信息,然后利用海底反射损失曲线,反演海底表层的声速和密度,最后利用浅底层反射信号估计沉积层参数.由于海水中直达波受到内波的强烈影响,选择海底表面反射作为参考,用以可靠地计算浅底层反射的相对到达时间和幅度,从而估计出沉积层的厚度、速度和衰减系数.通过海上实验,验证了利用浅底层反射信号反演参数的有效性. 关键词： 海底参数 反演 浅底层反射信号