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1.
林旺生  梁国龙  付进  张光普 《物理学报》2013,62(14):144301-144301
浅海低频声场的微观结构特征在于具有可用波导不变量表征的 稳定空间-频率干涉结构.声场兼具标量场和矢量场, 波导条件下二者联合决定声场的全部特性. 本文研究浅海声场空频干涉结构的矢量场特征. 理论分析了声压谱、动能密度谱、声强流谱等矢量场干涉结构的形成机理, 探讨了矢量场干涉结构的波导不变量表征, 数值仿真研究了Pekeris波导中能量和能流密度的干涉特性, 进行了宽带声源辐射矢量声场干涉特性及表征的海上试验.实测结果与理论、仿真分析有较好的一致性. 研究结果表明: 中近程和中远程声场均能模态相干, 有稳定的空频干涉结构, 并且矢量声场空频干涉结构存在多种形式, 除各种能量和能流密度谱图外, 相干系数谱也呈现干涉特征, 这些形式的空频干涉结构均可用波导不变量理论有效表征. 关键词: 矢量声场 干涉结构 波导不变量 浅海低频声场  相似文献   

2.
Pekeris波导中简正波声强流及其互谱信号处理   总被引:7,自引:0,他引:7  
探讨了Pekeris波导中声压场和质点振速场的联合描述,尤其关注垂直声强流的分析.研究表明,由于各阶简正波的干涉作用,水平和垂直声强流均既有有功分量,亦有无功分量.低频声场的垂直声强流的无功分量虽不参与声能的输运,当单个声矢量传感器做适当放置后却可用以判断声源的特定深度.这对于矢量信号处理是有意义的.给出了声压和质点振速联合互谱处理进行目标判别的算法.  相似文献   

3.
波导不变量有两种定义方式,按照干涉条纹斜率的定义适合工程应用,按照简正波频散的定义适合理论分析.在有跃层的波导中,这两种定义方式并不完全一致.由于简正波频散特性差异,按照频散特性定义的波导不变量β会有许多不同的取值,这些β被称为波导不变量的β谱.此时声场干涉结构应该用多个β来描述,而以往的β提取算法只能给出一个最佳估计值,导致一些信息的丢失.借鉴图像处理中的积分投影概念,将声强图像按照角度进行积分投影,以分离不同斜率的条纹成分;然后对投影曲线进行傅里叶变换,以分离不同间距的条纹成分,最终实现各个β谱值的分离.仿真和实验结果表明,β谱分离算法可以从声场干涉结构中有效地提取不同条纹成分的β,并将其映射到二维平面内,具有更强的噪声抑制能力,所以能在更低的信噪比条件下使用.  相似文献   

4.
针对浅海Pekeris环境下声矢量场的干涉特征,基于简正波理论分析了在频率-距离域上声强谱、质点振速自谱、复声强谱和波阻抗谱干涉结构的形成机理,探讨了对干涉结构的波导不变量表征,并进行了宽带辐射声场干涉结构的海上测量试验。仿真研究和海试数据分析均表明,在频率-距离域上,上述4类物理量都会呈现稳定的、可用波导不变量β表征的干涉结构,而复声强独有的纯干涉分量更能体现波导的干涉效应。最后引入多尺度线性滤波器对海试实测LOFAR图进行处理,处理结果表明该滤波器可有效地增强干涉特征,更利于检测和提取干涉图案中的条纹信息。   相似文献   

5.
Pekeris波导中简正波的复声强及其应用   总被引:4,自引:0,他引:4       下载免费PDF全文
余赟  惠俊英  赵安邦  孙国仓  滕超 《物理学报》2008,57(9):5742-5748
在Pekeris波导模型下,关注了简正波的矢量场,讨论了简正波水平复声强和垂直复声强的表述,并分析了其特征.单阶简正波在水平方向是行波,相应的水平复声强仅为有功的;在垂直方向为驻波,相应的垂直复声强仅为无功的.而多阶简正波相互干涉,因此总声场的复声强既有有功分量,也有无功分量,其中只有有功分量参与声能的输运,但无功分量是反映声场信息的重要组成部分.通过对垂直(交互)复声强无功分量和水平交互复声强有功分量的数值分析,对于甚低频率的点源声场,发现当声源深度变化时,上述声场分量的正负号呈有规变化,当接收传感器置 关键词: 目标深度分类 复声强 矢量场 Pekeris波导  相似文献   

6.
利用波导不变量进行运动单线阵的无源测距测速   总被引:4,自引:1,他引:3       下载免费PDF全文
余赟  袁延艺  刘雄厚 《声学学报》2017,42(6):661-668
为克服单线阵难以无源测距、测速的缺点,提出了利用目标辐射低频声场干涉结构和波导不变量的运动单线阵无源测距、测速方法。定义了运动目标的距离距变率比(目标距离与距离变化率的比值),并利用与目标辐射声场的时间-频率干涉结构和波导不变量相关的变量来表征距离距变率比。根据此定义,通过对目标辐射声场的时间-频率干涉结构图进行Radon变换等处理,实现对距离距变率比的估计。利用所估计的距离距变率比,结合平台速度、目标方位角和目标航向角实现对目标距离和速度的同时估计。仿真实验验证了所提方法在测距、测速时的正确性和有效性。结果表明:所提方法在目标航向角较大时有较高的距离、速度估计精度;同时,目标方位估计误差越小,所提方法的距离、速度估计精度越高。   相似文献   

7.
声场干涉结构相似度匹配的目标运动参数估计   总被引:1,自引:0,他引:1       下载免费PDF全文
针对水中运动声源定位问题,建立了一种基于声场干涉结构谱向量相似度匹配的目标运动参数估计方法。结合声场干涉结构水平纵向相关特性,利用目标辐射噪声LOFAR谱图中不同频率的谱值序列,基于两方位-两距离目标运动要素计算方法获取的目标距离解向量,构造声场干涉结构谱向量相似度匹配代价因子,实现目标运动参数估计。仿真数据与试验数据验证结果表明:在绘制的目标运动要素解算结果可视化分布图中可清晰呈现出目标初距、航向和速度结果。该算法实现过程简单、解算效率高,对目标方位误差有较好的鲁棒性。   相似文献   

8.
基于波导不变量的目标运动参数估计及被动测距   总被引:7,自引:0,他引:7  
结合波导不变量的概念推导了中近程目标的干涉条纹方程,它表明在浅海声场中此干涉条纹为一族类双曲线.采用Hough变换对LOFAR图和方位-时间历程进行处理,可以估计反映环境信息的波导不变量β、航向角(φ)以及最近通过距离和航速比r0/v.仿真研究和海试数据分析均表明,低频声场确实存在稳定的干涉结构,结合图像处理手段进行参...  相似文献   

9.
浅海低频声场中目标深度分类方法研究   总被引:2,自引:0,他引:2       下载免费PDF全文
余赟  惠俊英  陈阳  孙国仓  滕超 《物理学报》2009,58(9):6335-6343
分析了浅海甚低频声场中的垂直双水听器的互谱特性,尤其关注了声场中只存在两阶简正波时声压互谱的有功分量.数值计算表明:当两个水听器的深度布放合理时,声压互谱有功分量的正负号分布与水平距离无关,选择合适的水听器深度布放组合,可以用于水面目标、水下目标的双择判决;声速分布对该方法的使用影响不大,海底存在吸收将影响算法的作用距离,但在有效作用距离内,该算法仍有较好的稳健性.运用Pekeris波导有效深度的概念建立了声压互谱有功分量正负号分布特性的近似理论分析并可预报双水听器合理的布放深度.理论分析揭示了双水听器布放深度之和应等于波导有效深度,并且在有效深度限制的波导范围内,整个声场的声压互谱有功分量的正负号分布被分为三个水平区域.理论分析加深了对浅海低频声场特性的理解,对该算法的实际使用有指导意义. 关键词: 目标深度分类 浅海低频声场 声压互谱 有功分量  相似文献   

10.
利用波导不变量的浅海负跃层声源深度判别   总被引:4,自引:1,他引:3       下载免费PDF全文
刘志韬  郭良浩  闫超 《声学学报》2019,44(5):925-933
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。   相似文献   

11.
王朋  郑胜家  黄勇  刘纪元 《声学学报》2015,40(6):789-798
波导不变量是描述海洋波导环境声信号水平距离与频率干涉结构现象的特征参量。运动目标波导不变量测距方法需要已知目标速度值,运动目标速度一般是未知的。针对这一问题,本文提出了一种利用水平线阵估计目标运动速度的浅海波导不变量测距方法。该方法通过不同时刻波束域声信号互谱分析进行声源速度估计,结合HOUGH变换提取的LOFAR图斜率和波导不变量进行运动目标测距。仿真结果表明,该方法能够有效的进行运动目标的距离估计。利用2013年7月浅海实验数据,该方法估计出了发射船的距离,并与GPS测量的距离进行对比,相对误差小于10%。   相似文献   

12.
The paper considers the regular patterns that can be manifested in the behavior of the invariant of the spatial–frequency interference structure of an acoustic field in oceanic waveguides that are homogeneous and inhomogeneous along a track. Using the WKB and adiabatic approximations, an analytic expression is obtained for the invariant that, when certain conditions are fulfilled, reduces to the well-known classical expression independent of the mode numbers, their parity, or the emission frequency. It has been established that the approximate classical expression for the invariant correctly describes the slope of interference lines only in ranges of variation in the grazing angles of modes where the dependence of the cycle length of their corresponding Brillouin waves on the ray parameter is quite smooth and monotonic. The paper studies the formation of the spatial–frequency interference structure of an acoustic field propagating from a shallowwater isovelocity waveguide to a relatively deep-water waveguide with a near-surface sound channel.  相似文献   

13.
The single-element spectrogram for a continuous broadband signal, plotted as a function of range, has been shown to exhibit striated bands of intensity maxima and minima. The slope of the striations is an invariant of the modal interference and is described by a waveguide invariant parameter "beta." The striation pattern is analyzed and modeled in this paper for the beam outputs of a horizontal line array obtained by conventional beamforming. Array beamforming makes it possible to measure the waveguide invariant parameter for weak signals due to the enhancement of signal levels by the array gain over that of a single element. It is shown that the signal beam spectrogram as a function of range exhibits the same striation pattern as that (predicted) for a single element. Specifically, for a broadside signal, the beam striation is identical to that of a single-element plus a constant signal gain. For a nonbroadside target, the signal beam intensity will be modified by a frequency-bearing dependent signal gain due to the signal spread over multiple beams, nevertheless the beam spectrogram retains the same striation pattern (slope) as for a single element. The sidelobe beams (outside the canonical cones containing the signal arrivals) exhibit an entirely different striation pattern as a function of frequency and range. For array processing, it is shown that a fast range-rate, close range target and a distant, slow range-rate interference source will have a different striation pattern (slope) in the corresponding beam spectrograms as a function of time, assuming no prior knowledge of the source ranges. The difference in the striations between the beam spectrograms can be used in array processing to suppress the interference contribution. A 5-7 dB interference suppression is demonstrated using simulated data.  相似文献   

14.
波导不变量反映了水下声场多途传播的干涉结构特征。将波导不变量的提取分析应用于空气中声源产生的水下声场,通过数值仿真分析了波导不变量分布随深度的变化,提出了利用小深度接收声场提取的波导不变量分布来分辨空中和水下声源的方法。分析了空气中声速和风速剖面对该方法的影响,指出在实际海上环境条件下,当出现逆温现象或者当接收器在声源下风方向时,该方法是有效的。   相似文献   

15.
Contour plots of underwater acoustic intensity, mapped in range and frequency, often exhibit striations. It has been claimed that a scalar parameter 'beta', defined in terms of the slope of the striations, is invariant to the details of the acoustic waveguide. In shallow water, the canonical value is β=1. In the present paper, the waveguide invariant is modelled as a distribution rather than a scalar. The effects of shallow water internal waves on the distribution are studied by numerical simulation. Realizations of time-evolving shallow water internal wave fields are synthesized and acoustic propagation simulated using the parabolic equation method. The waveguide invariant distribution is tracked as the internal wave field evolves in time. Both random background internal waves and more event-like solitary internal waves are considered.  相似文献   

16.
Abstract

Contour plots of underwater acoustic intensity, mapped in range and frequency, often exhibit striations. It has been claimed that a scalar parameter ‘beta’, defined in terms of the slope of the striations, is invariant to the details of the acoustic waveguide. In shallow water, the canonical value is β=1. In the present paper, the waveguide invariant is modelled as a distribution rather than a scalar. The effects of shallow water internal waves on the distribution are studied by numerical simulation. Realizations of time-evolving shallow water internal wave fields are synthesized and acoustic propagation simulated using the parabolic equation method. The waveguide invariant distribution is tracked as the internal wave field evolves in time. Both random background internal waves and more event-like solitary internal waves are considered.  相似文献   

17.
Using numerical simulation, an analysis was conducted of the interference structure of a bottomscattered sound field generated by a wideband point source in shallow water under winter and summer conditions. The scattered signals were received from the place where the source was located and were subjected to Fourier transform with a sliding window. The paper demonstrates the possibility of estimating the waveguide invariant for backscattered signals when processing the sound intensity distributions in wide frequency and distance ranges up to the scattering area. A technique is proposed for reconstructing the twodimensional field of internal waves using variations of the interference pattern of reverberation signals. The influence of wind surface waves on the degree of interference band contrast is illustrated.  相似文献   

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