共查询到17条相似文献，搜索用时 109 毫秒
1.
对于组合式纵振压电水声换能器，当采取增加它的辐射面积、减小辐射盖板的厚度和降低机械Q值等方法来提高它的辐射功率并展宽其工作频带时，实验观测到换能器的辐射面不再作纯等幅纵振动，而耦合有弯曲振动。因此存在节线区域，它们一般呈圆线状， 相似文献
2.
对于组合式纵振压电水声换能器,当采取增加它的辐射面积、减小辐射盖板的厚度和降低机械Q值等方法来提高它的辐射功率并展宽其工作频带时,实验观测到换能器的辐射面不再作纯等幅纵振动,而耦合有弯曲振动。因此存在节线区域,它们一般呈圆线状,称为辐射面的波节线。通过Al_2O_3粉末法可以测量这些波节线的分布及大小。 相似文献
3.
本文介绍在设计夹心换能器纵振动的谐振频率计算中，由振子的厚度等效于基波的半波长出发，导出纵向振动换能器的频率方程。使谐振频率计算更加简便。实验表明，该方法计算方便，精确，适用于设计夹心换能器纵向振动的谐振频率计算。 相似文献
4.
利用溢流式换能器的液腔振动和径向振动耦合原理获得较宽的频率响应;采用声反射系统使换能器在垂直方向形成高指向性,换能器的方向性能指数增加２２ｄＢ。 相似文献
5.
运用表观弹性法,采用二次径向谐振频率计算表观弹模量,设计高度与直径可比拟,谐振频率不满足压电晶片和金属圆片最低径向谐振频率方程的多维耦合振动复合电振子。用本方法设计垂直探鱼仪的换能器和提高优质单胞藻饲料多不饱和脂肪酸含量的超声辐射仪换能器。计算结果表明,理论与值与实验值相符合。这种方法简单,方地压电晶片的径向谐振频率低于换能器揩能器谐振频率的多维耦合振动复合压电振的设计。 相似文献
6.
本文介绍利用表观弹性法,设计纵向振动与径向振动相耦合的朗芝万型换能器,该换能器用于大深度声遥测触底指示仪上,实验表明,理论计算值与实验值相符合,计算方法简单、方便。 相似文献
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在复杂的水声信道中 ,实现高速率的数据传输 ,水声换能器的带宽是一个重要的技术问题。实验中 ,为了拓宽换能器的带宽 ,我们利用圆柱形压电换能器的径向振动与液腔振动相耦合原理研制自由溢流式换能器和利用纵向振动与前盖板弯曲振动相耦合原理研制纵向振动复合棒换能器。本文介绍适应于复杂的水声信道中 ,进行高速率数据传输的两种宽频带换能器的研制 相似文献
9.
利用多孔结构增加换能器频带宽度，是换能器设计方面的一个新的理论问题。本文指出，换能器辐射块钻孔引起等效质量的减少，是导致频带变宽的主要原因．对园台形辐射块钻孔的换能器，用一般解析法求其振速分布是困难的。本文采用有限元方法求其振速的数值解，并算出了换能器的等效质量及带宽变化。该计算方法同样适用于辐射块前端或中间沿轴向钻孔的复合式和夹心式压电换能器等效质量的计算。 相似文献
10.
本文介绍利用圆柱形换能器水平无方向性和换能器的近场波束特性，采用压电陶瓷圆柱的径向振动和壁厚振动不同振动模式，设计适宜于声波对海洋生物影响实验使用的换能器。 相似文献
11.
P. Cobo C. Ranz A. Fernández M. Cuesta D.K. Anthony M. Siguero 《Marine Geophysical Researches》2005,26(2-4):87-95
Vertical resolution is of fundamental importance in sonar exploration and is directly related to the duration of the acoustic
pulse generated by the transducer. The shorter the radiated pulse, the higher the vertical resolution. Many sub-bottom profiling
sonar systems use piezoelectric transducers because they are reversible and well understood. Piezoelectric projectors are
normally resonant transducers, which are intrinsically narrowband. A piezoelectric transducer is usually driven by a tone-burst.
However, it is possible to use Fourier techniques to find a pre-compensated electrical driving function so that the transducer
radiates a prescribed wider band acoustic waveform. This technique can be applied to synthesize zero-phase cosine-magnitude,
Gaussian, and bionic pulses, with a conventional sandwich transducer. Zero-phase cosine-magnitude waveforms provide minimum
length pulses (and therefore maximum resolution) within a prescribed frequency band.The aim of this paper is to illustrate
the synthesis of wideband acoustic pulses using an underwater piezoelectric projector. The conventional acoustic waveform
radiated when a Tonpiltz transducer is transiently excited using a “click” and allows its frequency response function to be
measured. This function is used to design the electrical signal which then drives the transducer so that it radiates the shortest
pulse compatible with its mechanical response. The significant resolution enhancement of the waveform shaping process is illustrated
by its application to a sediment wedge model. 相似文献
12.
Decarpigny J.-N. Hamonic B. Wilson O.B. Jr. 《Oceanic Engineering, IEEE Journal of》1991,16(1):107-122
The difficulties that dominate low-frequency projector design problems in sonar and oceanographic applications are discussed. These are related to the size of the projector, the low radiation resistance, the acoustic interaction effects in arrays, and the requirements due to deep submergence. Low-frequency projectors are described and compared, and future trends associated with transducer shapes and dimensions and with the type of active materials used for the driving part are analyzed. The different modeling approaches are discussed, and an insight into the respective advantages and disadvantages of classical equivalent circuit models and numerical models-mainly those using the finite-element method-is provided. Several modeling examples are briefly introduced 相似文献
14.
Long-range underwater acoustic systems, such as those used in ocean acoustic tomography, require low-frequency signals covering a broad frequency band. To meet this requirement, a novel design based on a tunable narrow-band high-efficiency sound projector has been used. The projector transmits a frequency sweep signal by mechanically tuning a resonator tube (or organ pipe) to match the frequency and phase of a reference signal. The resonator tube projector consists of a symmetrical pressure-balanced Tonpilz driver placed between two coaxially mounted tubes. The Tonpilz acoustic driver is composed of two pistons separated by preloaded ceramic stacks. The resonant tube is a simple, efficient, narrow-band, medium-output projector that operates at any ocean depth. Both projector tubes have slots (or vents) which are progressively covered or uncovered by sliding coaxial tubular sleeves. The frequency varies with the sleeve position. A computer-controlled electromechanical actuator moves the cylindrical sleeves along the tubes, keeping the projector in resonance at the instantaneous frequency of a swept frequency signal. The actuator smoothly tunes the resonator tube frequency in a bandwidth of 200 to 300 Hz during a 135-s transmission. A computer synthesizes the linear frequency-modulated signal; compares the phase between transmitted and reference signals; and, using a phase-lock loop (PLL) system, keeps the resonator tube frequency in resonance with the driver frequency. The estimated PLL precision is better than 3/spl deg/ phase error. The system was analyzed by means of finite element analysis and electrical equivalent circuit simulation. The projector prototype was first tested at the Woods Hole Oceanographic Institution (WHOI) dock in Woods Hole, MA and later in the Pacific Ocean during a voyage of the R/V "Point Sur" in November 2001. 相似文献
15.
Towed linear arrays of hydrophones are used in various applications, for example, seismic prospecting. Tow cable vibration is capable of causing output in the towed array system. Since one of the factors limiting acoustic sensitivity is self-noise, the general objective of this analysis is to investigate the nature of longitudinal and transverse cable vibrations, with the aim of minimizing vibration transmitted to the array. The equations of transverse cable motion are derived and solved for a single-póint excitation and for distributed-vortex excitation. The response to vortex-shedding excitation along the first 150 ft of array-end cable is quantitatively evaluated and compared with actual tow-trial measurements. Two types of longitudinal vibration are analyzed, one caused by direct excitation along the cable axis, and one caused indirectly by transverse cable vibration. Fluid drag and hysteretic damping are included in the analysis. 相似文献
16.
Bjerrum-Niese C. Bjorno L. Pinto M.A. Quellec B. 《Oceanic Engineering, IEEE Journal of》1996,21(2):143-149
The paper discusses the development of a simulation tool to model high data-rate acoustic communication in shallow water. The simulation tool is able to generate synthetic time series of signals received at a transducer array after transmission across a shallow-water communication channel. The simulation tool is suitable for testing advanced signal processing techniques for message recovery. A channel model has been developed based on the physical aspects of the acoustic channel. Special emphasis has been given to fluctuations of the signal transmission caused by time-varying multipath effects. At shorter ranges, the temporal variations are dominated by acoustic scattering from the moving sea surface. Therefore, the channel model produces a coherence function which may be interpreted as a time-varying reflection coefficient for the surface scattered acoustical path. A static, range-independent ray model identifies the significant multipaths, and the surface path is modulated with the time-varying reflection coefficient. The advantages and limitations of the channel model are discussed and assumptions necessary to overcome the limitations are emphasised. Based on the assumptions, an algorithm has been developed and implemented to model how a binary message will be modulated when transmitted by a transducer, is distorted in the channel and finally is received by a transducer array 相似文献
