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1.
Acoustic vector sensor consists of pressure and particle velocity sensors,which measure the three-dimensional acoustic particle velocity,as well as the pressure at one location at the same time.By preserving the amplitude and phase information of the pressure and particle velocity,they possess a number of advantages over traditional scalar sensors.Signal-to-noise ratio (SNR) gain (which is often called array gain) is one of such advantages and is always interested by all of us.But it is not unchangeable if the spatial correlation of the noise field varies.Much more important,it is difficult to be given if the noise becomes complex.In this paper,spatial correlation of the vector field of isotropic volume-noise and surface-generated noise has been introduced briefly.Based on the results,the combined SNR output of a vector linear array is investigated and the maximum gain is given in the specified noise.Computer simulation shows that the output of one array in the same noise is not the same in different gestures.And then we find the best gesture through SNR calculation and obtain the biggest gain,which has important meaning to guide how to deploy an array in practice.We also should use the array with respect to the characteristics of the real ambient noise,especially in anisotropic noise field.  相似文献   

2.
Compared to a scalar pressure sensor, a vector sensor can provide a higher signal-to-noise ratio (SNR) signal and more detailed information on the sound field. Study on vector sensors and their applications have become a hot topic. Research on the representation of a vector field is highly relevant for extending the scope of vector sensor technology. This paper discusses the range-frequency distribution of the vector field due to a broadband acoustic source moving in a shallow-water waveguide as the self noise of a surface ship, and the vector extension of the waveguide impulse response measured over a limited frequency range using an active source of known waveform. From theory analysis and numerical simulation, the range-frequency representation of a vector field exhibits an interference structure qualitatively similar to that of the corresponding pressure field but, being quantitatively different, provides additional information on the waveguide, especially through the vertical component. For the range-frequency representation, physical quantities that can better exhibit the interference characteristics of the waveguide are the products of pressure and particle velocity and of the pressure and pressure gradient. An image processing method to effectively detect and isolate the individual striations from an interference structure was reviewed briefly. The representation of the vector impulse response was discussed according to two different measurement systems, also known as particle velocity and pressure gradient. The vector impulse response representation can not only provide additional information from pressure only but even more than that of the range-frequency representation.  相似文献   

3.
It is the traditional belief that sound transmission from water to the air is very weak due to a large contrast between air and water impedances. Recently, the enhanced sound transmission and anomalous transparency of air-water interface have been introduced.Anomalous transparency of air-water interface states that the sound generated by a submerged shallow depth monopole point source localized at depths less than 1/10 sound wavelength, can be transmitted into the air with omni-directional pattern. The generated sound has 35 times higher power compared to the classical ray theory prediction. In this paper, sound transmission through air-water interface for a localized underwater shallow depth source is examined. To accomplish this, two-phase coupled Helmholtz wave equations in two-phase media of air-water are solved by the commercial finite element based COMSOL Multiphysics software. Ratios of pressure amplitudes of different sound sources in two different underwater and air coordinates are computed and analyzed against non-dimensional ratio of the source depth(D) to the sound wavelength(λ). The obtained results are compared with the experimental data and good agreement is displayed.  相似文献   

4.
Most source number estimation methods based on the eigenvalues are decomposed by covariance matrix in MUSIC algorithm. To develop the source number estimation method which has lower signal to noise ratio and is suitable to both correlated and uncorrelated impinging signals, a new source number estimation method called beam eigenvalue method (BEM) is proposed in this paper. Through analyzing the space power spectrum and the correlation of the line array, the covariance matrix is constructed in a new way, which is decided by the line array shape when the signal frequency is given. Both of the theory analysis and the simulation results show that the BEM method can estimate the source number for correlated signals and can be more effective at lower signal to noise ratios than the normal source number estimation methods.  相似文献   

5.
Array calibration is important in engineering practice. In this paper, fast calibration methods for a ULA's gain and phase errors both in far and near fields are proposed. In the far field, using a single sound source without exact orientation, this method horizontally rotates the array exactly once, performs eigen value decomposition for the covariance matrix of received data, then computes the gain and phase error according to the formulas. In the near field, using the same single sound source, it is necessary to rotate the array horizontally at most three times, build equations according to geometric relations, then solve them. Using the formula proposed in this paper, spherical waves are modified into plane waves. Then eigen values decomposition is performed. These two calibration methods were shown to be valid by simulation and are fast, accurate and easy to use. Finally, an analysis of factors influencing estimation precision is given.  相似文献   

6.
Array calibration is important in engineering practice. In this paper, fast calibration methods for a ULA's gain and phase errors both in far and near fields are proposed. In the far field, using a single sound source without exact orientation, this method horizontally rotates the array exactly once, performs eigen value decomposition for the covariance matrix of received data, then computes the gain and phase error according to the formulas. In the near field, using the same single sound source, it is necessary to rotate the array horizontally at most three times, build equations according to geometric relations, then solve them. Using the formula proposed in this paper, spherical waves are modified into plane waves. Then eigen values decomposition is performed. These two calibration methods were shown to be valid by simulation and are fast, accurate and easy to use. Finally, an analysis of factors influencing estimation precision is given.  相似文献   

7.
The aim of the present study is to improve the capabilities and precision of a recently introduced Sea Surface Acoustic Simulator(SSAS) developed based on optimization of the Helmholtz–Kirchhoff–Fresnel(HKF) method. The improved acoustic simulator, hereby known as the Modified SSAS(MSSAS), is capable of determining sound scattering from the sea surface and includes an extended Hall–Novarini model and optimized HKF method. The extended Hall–Novarini model is used for considering the effects of sub-surface bubbles over a wider range of radii of sub-surface bubbles compared to the previous SSAS version. Furthermore, MSSAS has the capability of making a three-dimensional simulation of scattered sound from the rough bubbly sea surface with less error than that of the Critical Sea Tests(CST) experiments. Also, it presents scattered pressure levels from the rough bubbly sea surface based on various incident angles of sound. Wind speed, frequency, incident angle, and pressure level of the sound source are considered as input data, and scattered pressure levels and scattering coefficients are provided. Finally, different parametric studies were conducted on wind speeds, frequencies, and incident angles to indicate that MSSAS is quite capable of simulating sound scattering from the rough bubbly sea surface, according to the scattering mechanisms determined by Ogden and Erskine. Therefore, it is concluded that MSSAS is valid for both scattering mechanisms and the transition region between them that are defined by Ogden and Erskine.  相似文献   

8.
1 Introduction1 New methods of parameter estimation are possible by the appearance of vector transducer. A new method of multi-parameters estimation by single vector transducer was presented in Ref.[1].The correlation of pressure and particle velocity in …  相似文献   

9.
The hydrodynamic performance of a propeller in unsteady inflow was calculated using the surface panel method. The surfaces of blades and hub were discreted by a number of hyperboloidal quadrilateral panels with constant source and doublet distribution. Each panel's corner coordinates were calculated by spline interpolation between the main parameter and the blade geometry of the propeller. The integral equation was derived using the Green Formula. The influence coefficient of the matrix was calculated by the Morino analytic formula. The tangential velocity distribution was calculated with the Yanagizawa method, and the pressure coefficient was calculated using the Bonuli equation. The pressure Kutta condition was satisfied at the trailing edge of the propeller blade using the Newton-Raphson iterative procedure, so as to make the pressure coefficients of the suction and pressure faces of the blade equal at the trailing edge. Calculated results for the propeller in steady inflow were taken as initialization values for the unsteady inflow calculation process. Calculations were carried out from the moment the propeller achieved steady rotation. At each time interval, a linear algebraic equation combined with Kutta condition was established on a key blade and solved numerically. Comparison between calculated results and experimental results indicates that this method is correct and effective.  相似文献   

10.
The water entry problem of an asymmetric wedge with roll motion was analyzed by the method of a modified Logvinovich model (MLM). The MLM is a kind of analytical model based on the Wagner method, which linearizes the free surface condition and body boundary condition. The difference is that the MLM applies a nonlinear Bernoulli equation to obtain pressure distribution, which has been proven to be helpful to enhance the accuracy of hydrodynamic loads. The Wagner condition in this paper was generalized to solve the problem of the water entry of a wedge body with rotational velocity. The comparison of wet width between the MLM and a fully nonlinear numerical approach was given, and they agree well with each other. The effect of angular velocity on the hydrodynamic loads of a wedge body was investigated.  相似文献   

11.
矢量声压振速联合处理是建立在信号的声压和质点振速相位基础上,海洋环境边界对声传播的影响将改变矢量声场声压和质点振速的幅度和相位特性。文章根据南海环境条件和水下目标辐射噪声测量采用矢量简正波理论估算海面非相干偶极子噪声源和水下点声源矢量场的幅度和相位随深度的变化,并对矢量水听器测量系统获取的南海典型深度上的背景噪声数据进行了分析。结果表明:深海背景噪声声压谱级在500 Hz以下基本上不随深度变化,在500 Hz-3 kHz频段浅深度背景噪声声压谱级略高于较深深度的背景噪声声压谱级;背景噪声的垂直质点振速谱级要小于声压和水平质点振速谱级。  相似文献   

12.
在梳理流噪声数值预报方法的基础上,采用流场大涡模拟(large eddy simulation,LES)和声学边界元(boundary element method,BEM)方法在频域内计算预报了船体流噪声谱曲线,求取了其等效声中心.LES计算时选用动力学Smagorinsky-Lilly(dynamic Smagorinsky-Lilly,DSM)亚格子应力模型,流噪声由船体壁面脉动压力和法向速度特性决定,声源节点和声节点变量传递采用一对一的守恒传递方式.结果表明:某型船在航速14 kn时,裸船体流噪声在20 Hz~2 kHz频段内总声源级为133dB;当计算有效频段扩展到20 kHz时,总声源级达143.3 dB.流噪声主要来源于兴波引起的涡量,且主要集中于100 Hz~10 kHz频段.球首尾流区和船体尾涡区对流噪声辐射量贡献明显,特别是球首尾流区,对全频段都有明显的贡献,为水面舰艇流噪声研究提供了一条新的途径.  相似文献   

13.
为研究艇后非均匀流场中大侧斜螺旋桨无空泡负载噪声的分布规律,文章采用“CFD+BEM”法,以SUBOFF潜艇后某大侧斜桨为研究对象,首先稳态计算均匀进流下螺旋桨敞水特性,模拟系数值与实验误差在3%以内,验证了CFD数值计算的可信性。然后采用大涡(LES)模拟,对“艇+桨”进行三维非定常数值模拟,计算得到桨表面声偶极子数据后,通过距离加权平均法映射到声网格节点上,将噪声源直接分布在桨叶表面上进行积分来预报螺旋桨的低频线谱噪声。采用边界元法基于扇声源理论通过FW-H声类比方程分别在1 kHz以内对桨盘面、轴向纵剖面及10倍桨半径球场的噪声进行频域求解。研究表明:桨盘面和轴向纵剖面上声指向均呈8字形,但受螺旋桨自身旋转及大侧斜的存在,指向性不唯一;球场声场显示,轴向声辐射面较大,声辐射强,径向辐射面小且辐射较弱;特征点的计算结果显示,高阶叶频声压级明显比一阶叶频低,这与物理现象相符,将特征点处结果与已发表文献进行对比,吻合性良好,并对存在的差异作出了合理的物理解释。该文为螺旋桨噪声预报介绍了一种可行的新方法。  相似文献   

14.
唐春丽  方开翔 《江苏船舶》2005,22(6):8-9,17
针对某舰壳声纳和导流罩,运用有限元建模计算软件,对1:1实罩建立有限元模型,然后运用声学分析软件,计算某些频率下声源定向发射时的相关数据,主要是水平中性面和垂直中性面的波束宽度变化率和波束高度变化率以及左、右旁瓣高度,结果说明导流罩内加有障板对其声场特性的影响。  相似文献   

15.
基于涡声理论的水下射流噪声预报   总被引:1,自引:0,他引:1  
王春旭  张涛  侯国祥 《船舶力学》2010,14(6):670-677
湍流噪声是潜艇重要的水下噪声源.以水下自由湍射流为例,探讨其噪声机理和预报方法,构造了Powell涡声理论和CFD方法相结合的算法.首先讨论了Powell涡声方程和Howe的涡声方程的解法;作为算例,用CFD软件FLUENT中标准k-ε计算湍射流场,以此作为近场声源;随后,运用Powell涡声和Howe的涡声方程理论对远场噪声谱进行预估,给出了辐射噪声指向性比较,并分析了自由射流场声辐射机理.  相似文献   

16.
泵喷推进器水动力噪声的数值预报   总被引:1,自引:0,他引:1  
泵喷推进器由于其高航速时优异的噪声性能,在核潜艇上已得到广泛应用,对其水动力噪声数值计算方法进行研究具有重要意义。文中首先在利用CFD方法得到固体壁面脉动压力分布的基础上,基于边界元方法完成了静止固体壁面流噪声的计算,结合点源模型并借鉴扇声源理论完成了任意边界条件下旋转声源噪声的计算,并且噪声计算结果与试验值、文献值吻合较好;然后以某泵喷为对象分别计算了泵喷静止部件和旋转部件的水动力噪声,最后对二者声场进行叠加即得到泵喷总噪声。结果表明静止部件噪声宽带总声级在径向最高,旋转部件噪声则在轴向最高;在导叶通过频率及其谐频处,由于叶轮与导管内壁面相互作用区域脉动剧烈,使得导管成为径向测点处噪声的主要贡献者,导叶对总声场的贡献量很小。  相似文献   

17.
针对大型结构体的声辐射问题,提出了一种利用声辐射模态识别声源表面的噪声辐射区域的方法。分析了各阶声辐射模态对声源的辐射声功率的贡献量,找出了对远场辐射声功率贡献最大的几个主要的声辐射模态,然后利用这几个主要的声辐射模态重建声源表面法向振速,通过声源表面法向振速的重建结果实现了声源表面噪声辐射区域的识别。通过对平板声源在几种不同频率下的噪声辐射区域的仿真分析验证了文中方法的正确性。该文方法对于确定特定频率下声源表面的噪声辐射区域,从而进一步进行辐射噪声控制具有积极的意义。  相似文献   

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