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纳机电矢量水听器根据鱼类听觉器官侧线设计,是一种新型微纳结合的纤毛式水声矢量探测仿生结构。以往关于纳机电矢量水听器的定向研究都是基于单个水听器的,方位角出现了左右舷模糊,波束图的主瓣宽度较宽。为提高水听器的性能,改进了其敏感单元和封装方式,经国防科技工业一级测量站标定,其频率响应范围为20~2 000 Hz,灵敏度为-165 dB。为解决左右舷模糊,采用二元阵进行定向,水听器的两路输出信号被校准一致后,在某开阔水域进行了纳机电矢量水听器二元阵的实验研究,验证了纳机电矢量水听器二元阵水平沿X轴放置时能够唯一确定目标的方位角,但是俯仰角出现了左右舷模糊;对低频信号的定向能力较强;具有可靠的跟踪水下运动目标能力。 相似文献
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在多波束回声声纳系统中,高分辨处理算法例如MUSIC、ESPRIT,被广泛应用于海底地形的测绘。在应用高分辨算法时,一条均匀线阵是必要条件。然而,由于系统覆盖范围/分辨率的需求以及安装空间的限制,在多波束系统中经常会采用特殊形状的接收阵列,这使得高分辨算法无法直接应用。同时回波信号的短时平稳特性使得难以估计出协方差矩阵,这也增加了高分辨算法在多波束系统中的应用难度。本文首先介绍一种基于多角度子阵波束形成的ESPRIT算法,该算法能降低高分辨算法对信噪比、样本点数和计算能力的要求。仿真表明此算法能提供更好的分辨力。接着提出一种将基于多角度子阵波束形成的ESPRIT算法与虚拟阵列变换相结合的高分辨底检测算法,并针对高分辨底检测算法在U型阵上的应用进行了探讨。计算机仿真和试验数据处理结果验证了文章所提高分辨底检测算法的有效性。 相似文献
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针对传统三维声呐硬件系统复杂、计算量庞大的特点,本文设计了一种基于垂直线阵的水下三维成像系统。相比于传统二维面阵成像声呐,垂直线阵成像声呐阵元数较少,硬件电路较简单。但是,垂直线阵扫面时间过长的缺点使得系统成像速率较慢,无法满足实时成像的需求。为解决此问题,本文提出了一种多频率发射波束形成算法,该算法通过优化垂直阵列的发射过程,有效地减少了系统发射阵列的波束发射次数,从而缩短了系统扫描时间,提升了成像速度。系统硬件部分由发射模块、接收模块、电源模块以及显示模块4个部分组成。系统通过FPGA控制120路信号的同步采样,在波束形成计算中使用并行子阵分级波束形成算法再次提高了系统的运算速率。为了验证系统的性能指标,本文先后对系统进行了波束形成仿真测试以及水下环境的实际成像测试。经测试,本文设计的垂直线阵三维声呐成像效果接近同等指标的二维面阵成像声呐,系统成像帧率较高,满足了三维声呐低功耗、小型化、实时成像的需求。 相似文献
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大太阳天顶角下水色卫星叶绿素遥感探测能力研究 总被引：2，自引：2，他引：0
本文利用考虑地球曲率的矢量辐射传输模型PCOART-SA,对大太阳天顶角下叶绿素浓度的卫星遥感探测极限能力进行了模拟研究。结果表明:太阳-传感器几何参数,尤其是太阳天顶角对叶绿素浓度变化的探测极限能力影响较大;大太阳天顶角下,卫星对叶绿素浓度变化的探测能力下降十几倍。在典型陆架水体（叶绿素浓度为1 μg/L）,低太阳天顶角（30°）时,叶绿素浓度变化探测极限为0.012 8 μg/L（约为原浓度的1.2%）,而大太阳天顶角（80°）时,探测极限为0.136 μg/L（约为原浓度的13.6%）。相比于太阳天顶角,观测天顶角增大造成的叶绿素浓度探测能力衰减较小。叶绿素浓度越高,吸收作用越强,对卫星遥感器的辐射探测灵敏度、定标及大气校正精度的要求越高。 相似文献
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《Oceanic Engineering, IEEE Journal of》2008,33(2):182-197
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The problem of tracking the directions-of-arrival (DOAs) of multiple moving sonar targets with an array of passive sensors is complicated by sensor movement. An algorithm for the joint tracking of source DOAs and sensor positions is presented to address this problem. Initial maximum-likelihood estimates of source DOAs and sensor positions are refined by Kalman filtering. Spatio-temporally correlated array movement is considered. Source angle dynamics are used to achieve correct data association. The new technique is capable of performing well for the difficult cases of sources that cross in angle as well as for fully coherent sources. Computer simulations show that the approach is robust in the presence of array motion modeling uncertainty and effectively reduces dependence on expensive and possibly unreliable hardware 相似文献
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程国胜 《数字海洋与水下攻防》2019,2(1):86-94
工程中矢量物理量的测量,例如水中目标的磁场、电场的测量,通常测量传感器的姿态角是任意或随机的,因此需要对传感器平台的姿态角进行测量,并由此将矢量物理量的测量数据修正到确定的参照坐标系。 分析了文献中通常使用的修正算法,即根据传感器平台姿态角测量值直接引用欧拉角旋转变换公式,分析表明这一算法存在原理性误差。 在此基础上,推导出了合理的变换计算式,可以直接应用在任意姿态下矢量物理量的测量数据修正计算,以及类似的坐标变换计算中。 相似文献
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Aperture extension is achieved in this novel ESPRIT-based two-dimensional angle estimation scheme using a uniform rectangular array of vector hydrophones spaced much farther apart than a half-wavelength. A vector hydrophone comprises two or three spatially co-located, orthogonally oriented identical velocity hydrophones (each of which measures one Cartesian component of the underwater acoustical particle velocity vector-field) plus an optional pressure hydrophone. Each incident source's directions-of-arrival are determined from the source's acoustical particle velocity components, which are extracted by decoupling the data covariance matrix's signal-subspace eigenvectors using the lower dimensional eigenvectors obtainable by ESPRIT. These direction-cosine estimates are unambiguous but have high variance; they are used as coarse references to disambiguate the cyclic phase ambiguities in ESPRIT's eigenvalues when the intervector-hydrophone spacing exceeds a half-wavelength. In one simulation scenario, the estimation standard deviation decreases with increasing intervector-hydrophone spacing up to 12 wavelengths, effecting a 97% reduction in the estimation standard deviation relative to the half-wavelength case. This proposed scheme and the attendant vector-hydrophone array outperform a uniform half-wavelength spaced pressure-hydrophone array with the same aperture and slightly greater number of component hydrophones by an order of magnitude in estimation standard deviation. Other simulations demonstrate how this proposed method improves underwater acoustic communications link performance. The virtual array interpolation technique would allow this proposed algorithm to be used with irregular array geometries 相似文献
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Feng Lu Milios E. Stergiopoulos S. Dhanantwari A. 《Oceanic Engineering, IEEE Journal of》2003,28(3):552-563
In real-time towed-array systems, performance degradation of array gain occurs when a line array that is not straight is assumed straight in the beamforming process. In this paper, a new method is proposed for array shape estimation. The novelty of this method is that it accounts for the variations in the tow ship's speed, which are typical during course alterations. The procedure consists of two steps. First, we solve for the tow-point induced motion in the time domain based on the constraints from the tow-point compass-sensor readings and from a discretized Paidoussis equation. At each time instance, the shape estimate is solved from a linear system of equations. We also show that this solution is equivalent to a previous frequency-domain solution while the new approach is much simpler. In the second step, we use the tail compass-sensor data to adjust the overall array shape. By noting that variations in the ship speed lead to a distortion in the normalized time axis, we first register the predicted tail displacement with the tail sensor readings along the time axis. Then, distortions in the estimated array shape over its length can be compensated accordingly. We also model a slow-changing bias between sensor zeros and remove systematic sensor errors. The effectiveness of the new algorithm is demonstrated with simulations and real sea-trial data. 相似文献
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Dosso S.E. Brooke G.H. Kilistoff S.J. Sotirin B.J. McDonald V.K. Fallat M.R. Collison N.E. 《Oceanic Engineering, IEEE Journal of》1998,23(4):365-379
Array element localization (AEL) surveys are often required to accurately localize acoustic instruments (transponders or sensors) in the ocean. These are typically based on transmitting or recording acoustic signals from or at a set of well-known positions. A significant limiting factor in many AEL surveys is the uncertainty inherent in these “known” positions. In this paper, an inversion algorithm is developed which properly treats both transponder and sensor positions as unknowns, subject to available a priori information in the form of position estimates and uncertainties. The algorithm essentially consists of an iterative linearized inversion of the raytracing equations employing the method of regularization. The approach is applied to independently localize transponders and vertical line array (VLA) sensors that form part of a three-dimensional sensor array in the Arctic Ocean. Confidence limits estimated via Monte Carlo simulation indicate that transponders and sensors are localized to less than 1 m in three dimensions. The VLA sensor motion, monitored over a seven-week period, appears to be predominately driven by tidal currents and is consistent with historical current measurements for the region 相似文献
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Underwater acoustic transient signals are generated mechanically at known positions along a wharf. These signals are received by a wide aperture planar array of four underwater acoustic sensors, whose positions relative to the wharf are unknown. A method is described that enables the positions of the sensors to be estimated from accurate differential time-of-arrival measurements (with 0.1 /spl mu/s precision) as the signal wavefronts traverse the array. A comparison of the estimated positions with the nominal positions of the first three sensors, which form a 20-m-wide aperture horizontal line array, reveals a 2-cm displacement of the middle sensor from the line array axis. This slight bowing of the line array results in overranging (bias error of 3%) when the wavefront curvature method is used with the nominal collinear sensor positions to locate a static source of active sonar transmissions at a range of 59.2 m. The use of the spherical intersection method coupled with the estimated sensor positions of the line array provides an order of magnitude improvement in the range estimate (within 0.3% of the actual value). However, systematic ranging errors are observed when the sound propagation medium becomes nonstationary. Next, the differences in the arrival times of the direct path and boundary-reflected path signals at the middle sensor of the wide aperture line array are estimated using the differential phase residue of the analytic signal at the sensor output. These multipath delays are used to estimate the range and depth of the source. Although the average value of the multipath range estimates is within 0.5% of the actual value, the variance of the range estimates is 50 times larger when compared with the results of the spherical intersection and wavefront curvature methods. The multipath delay data are also processed to provide a reliable estimate of the temporal variation in the water depth enabling the tidal variation to be observed. 相似文献
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We consider the role played by the sensor locations in the optimal performance of an array of acoustic vector sensors, First we derive an expression for the Cramer-Rao bound on the azimuth and elevation of a single far-field source for an arbitrary acoustic vector-sensor array in a homogeneous wholespace and show that it has a block diagonal structure, i.e., the source location parameters are uncoupled from the signal and noise strength parameters. We then derive a set of necessary and sufficient geometrical constraints for the two direction parameters, azimuth and elevation, to be uncoupled from each other. Ensuring that these parameters are uncoupled minimizes the bound and means they are the natural or “canonical” location parameters for the model. We argue that it provides a compelling array design criterion. We also consider a bound on the mean-square angular error and its asymptotic normalization, which are useful measures in three-dimensional bearing estimation problems. We derive an expression for this bound and discuss it in terms of the sensors' locations. We then show that our previously derived geometrical conditions are also sufficient to ensure that this bound is independent of azimuth. Finally, we extend those conditions to obtain a set of geometrical constraints that ensure the optimal performance is isotropic 相似文献