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海洋中的低频(<1000Hz)声吸收主要决定于海洋的pH值.虽然测得的远程(1000km量级)声传播的绝对幅度相当复杂地依赖于海洋的介质和环境参数,但对不同频率间的相对吸收差的测量能给出有用的信息.此外,沿海面反射声线(RSR)的传播衰减还应附加上海面散射引起的损失.原则上通过比较发射和接收到的声信号的频谱能估算海洋的pH值和表面粗糙度.我们分析了北太平洋750km声传播实验的部分数据.实验结果与理论估算定性地相符,但其测量精度还不足以进行定量的比较(该实验并不是为测量相对吸收差而设计的).估算表明,为了获得0.05的pH测量精度,当信号频率为550±100Hz,传播距离为750km时,对北太平洋(pH≈7.7)和大西洋(pH≈8.0)海域分别需要对100和60个独立测量样本进行平均以消除内波及噪声引起的幅度谱畸变. 相似文献
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声跃层结构变化对深海汇聚区声传播的影响 总被引:1,自引:0,他引:1
根据射线理论建立了线性声速结构条件下的声跃层强度与深海汇聚区关系模型,用最小位移角讨论了海洋环境变化(如声跃层强度变化、声跃层位置变化及季节性跃层生消等)与汇聚区距离和宽度变化的相关性.结果表明,声跃层的结构变化对汇聚区特征影响很大.声跃层强度增大使汇聚区向远离声源的方向变化,跃层强度每增加0.01 s-1对应的汇聚区位移增大约为3.5~5.0 km.声跃层位置变化对汇聚区的影响小于声跃层强度,与两层结构的声速剖面相比,上行结构使汇聚区向靠近声源的方向变化,声跃层上升200 m对应的汇聚区位移减小约为1.0~1.5 km,声跃层越浅,汇聚区距离越近;下行结构使汇聚区向远离声源的方向变化,混合层加深200 m对应的汇聚区位移增大约为1.0~1.5 km,混合层越深,汇聚区距离越远.季节性跃层的生消使近表层有负梯度、零梯度和正梯度的变化.负梯度结构的变化规律与两层结构条件下的声跃层强度变化类似,但对汇聚区的影响程度相对较小;正梯度结构使汇聚区在近表层出现表面声道,梯度值的增强将使汇聚区向靠近声源的方向变化. 相似文献
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海底沉积物声衰减同轴差距衰减测量法与其他测量方法的对比研究 总被引:2,自引:0,他引:2
以精度较高的现场测量Hamilton的原位测量所得数据为标准,对比研究了钱正明的直立同轴衰减测量法、刘强的垂直轴差距衰减测量法和我们课题组的同轴差距衰减测量法等3种研究海底沉积物声衰减的实验室测量方法。通过3种实验测量方法所得数据跟Hamilton原位测量所得数据进行对比,分析了以上实验室方法的优缺点,并分析了声衰减与样品长度和测量频率的关系。同轴差距衰减测量法与直立同轴衰减测量法相比,前者在消除测量仪器和耦合衰减误差方面,以及在实验样品长度方面更合理。同轴差距衰减测量法与垂直轴差距测量法相比,同轴差距衰减测量法在原理上保证了声波传播能量接收的同轴性和同指向性,其实验数据比利用相同实验仪器的垂直轴差距测量法的数据更准确。 相似文献
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应用BELLHOP模式,对声速剖面的声跃层结构变化引起会聚区偏移特征进行了分析。结果表明,声速垂直结构的变化可导致会聚区位置出现不同程度的偏移:跃层强度增加0.01 s-1将使会聚区向远离声源方向偏移1.5~2.0km;跃层厚度增大50m将使会聚区向靠近声源方向偏移0.3~0.5km;跃层位置加深100m将使会聚区向远离声源方向偏移0.5~1.0km。在跃层的三个特征量中,跃层强度起主导作用。跃层强度变化引起的声线在海洋次表层的偏折差异,进而导致进入深海等温层的入射角差异,是使会聚区发生偏移的决定性因素。 相似文献
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Frequency-selective attenuation of sound propagaion and reverberation in shallow waterTXFrequency-selectiveattenuationofsoundp... 相似文献
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针对混响环境非自由声场中声源测量的问题,本文以消声水池和混响水槽为实验环境,以换能器辐射的声场为研究对象,以水听器阵列为测量前端,进行了混响环境非自由声场中声源对象的测量、分析和重构的实验研究。通过单层水听器阵列对非自由声场进行声压分布测量,并对测量结果作声波分离处理,将分离前后的声压分布和在消声水池中测量的声压分布进行比较,给出了声源频率为5 000 Hz和7 000 Hz时,声场重构的误差分析结果。结果表明,基于单层水听器阵列声压测量的声波分离方法,能够较精确地对混响环境中的声场进行重构。 相似文献
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Ji-Xun Zhou Xue-Zhen Zhang Rogers P.H. Simmen J.A. Dahl P.H. Guoliang Jin Zhaohui Peng 《Oceanic Engineering, IEEE Journal of》2004,29(4):988-999
Optimal array-processing techniques in the ocean often require knowledge of the spatial coherence of the reverberation. A mathematical model is derived for the reverberation vertical coherence (RVC) in shallow water (SW). A method for analysis of RVC data is introduced. Measured reverberation cross-correlation coefficients as a function of time and frequency, obtained during the Asian Seas International Acoustic Experiment (ASIAEX) in the East China Sea, are reported. SW reverberation from a single shot provides a continuous spatial sampling of the surrounding sound field up to several tens of kilometers and holds valuable information on the geoacoustic properties of the sea floor over this distance. SW reverberation data can, therefore, be used as the basis for a quick and inexpensive method for geoacoustic inversion and has the obvious advantage that acquiring the data in situ requires only a single platform. This paper considers the use of the vertical coherence of the reverberation as the starting point for such an inversion. Sound speed and attenuation in the sea bottom at the ASIAEX site are obtained over a frequency range of 100-1500 Hz by finding values that provide the best match between the measured and predicted RVC. 相似文献
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A. Kh. Degterev 《Physical Oceanography》2007,17(5):296-302
We propose a numerical model for the evaluation of the three-dimensional scattering of sound in the sea. The model is based
on the construction of ray patterns both for the primary and secondary (scattered) radiation. The intensity of secondary radiation
is expressed via the coefficient of backward volume scattering interpreted as the fraction of backward-scattered acoustic
energy per unit length of the primary ray. It is shown that, in the first approximation, it suffices to consider the secondary
rays repeating the paths of the primary rays in the opposite direction. The attenuation of the intensity of sound along the
paths of the primary and secondary rays is taken into account. The results of numerical analysis of the reverberation signal
as a function of time are presented for various conditions (different depths of immersion of the antenna and widths of the
directional diagram and the presence of sound-scattering layers). The proposed approach can be used for the purposes of modeling
of the surface and bottom reverberation and for the solution of the inverse problems of underwater acoustics.
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Translated from Morskoi Gidrofizicheskii Zhurnal, No. 5, pp. 50–58, September–October, 2007. 相似文献
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Zhaohui Peng Ji-Xun Zhou Dahl P.H. Renhe Zhang 《Oceanic Engineering, IEEE Journal of》2004,29(4):1038-1045
As a part of the Asian Seas International Acoustic Experiment (ASIAEX) in the East China Sea, sound propagation signals from wideband explosive sources were measured using a 32-element vertical line array. Measurements were made as a function of range in two perpendicular tracks. Sea-bed geoacoustic parameters based on a fluid half-space geoacoustic model (sound speed, density, and attenuation) are inverted from the sound propagation in the frequency range 100-500 Hz. The sea-bed sound speed and density were first derived from mode arrival time differences which were obtained using a spatial mode filtering technique. Sea-bed acoustic attenuation was subsequently estimated by comparing measured transmission loss with model results. 相似文献
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为研究小尺度海底沉积物样品的声衰减特性,作者提出了用声学探针测量海底沉积物声波幅值的新方法,对沉积物样品扰动小,两个测量点的距离可小于波长,为海底沉积物微观声衰减测量提供了新手段。作者用小于波长的间隔逐点测量了沉积物的压缩波幅值,数据分析表明沿沉积物柱状样全长的声衰减满足指数衰减模型。目前主要用同轴差距衰减测量法获得海底沉积物声衰减数据,但该方法不能辨识声衰减模型,因此不同海区的测量结果难以建立联系。对此作者又提出用声吸收系数反演的幅值比与声衰减系数反演的R值(两种幅值比的比值)作评价依据,分析了垂直轴差距衰减测量法获得的南海海底沉积物声衰减测量数据,发现部分沉积物样品声衰减的R值远大于1,其声衰减不满足指数衰减模型。在声衰减满足指数衰减模型的条件下,用Hamilton的声衰减和频率经验公式预报的南海沉积物声衰减比与作者用声学探针测量海底沉积物所得的声衰减比对比,通过对R值分析得出Hamilton的声衰减和频率经验公式可以预报南海沉积物声衰减比的范围。作者提出的声学探针测量海底沉积物声衰减的方法的优点是既能获得声衰减数据又能辨识声衰减模型,不同海区测量的沉积物声衰减比可用R值建立联系。 相似文献
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ENSO循环过程中次表层海洋信号的传播和变化 总被引:2,自引:0,他引:2
利用SODA等资料分析了热带太平洋次表层海洋要素的变化特征,结果表明,ENSO循环过程中次表层异常海温信号在赤道外向西传播的路径与温跃层深度的分布有一定关系,10oN附近是气候平均温跃层深度的极小值区域,温跃层在该区域形成了一个从东到西的阻隔带,阻挡了来自赤道地区的ENSO信号继续向北传播,从而转向西传播;而南半球温跃层深度的气候分布不具备这一特征,不利于ENSO信号在南半球的向西传播。进一步的研究还表明,ENSO信号在整个循环过程中,异常海温的主周期是变化的,特别是在沿10oN附近向西传播的过程中,ENSO信号的主周期变化较大。推断西太平洋暖池区域的ENSO信号除了在循环过程中自东太平洋10oN传来的以外,还受其他因素的影响,例如局地的大气变化引起的海温异常,以及来自中高纬度的异常海温信号等因素。 相似文献
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