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1.
针对利用侧扫声纳检测海底管道时因其检测声影图像模糊而导致管道悬空高度检测误差过大的问题,提出了侧扫声纳声波掠射角优化设计的思路及方法。阐述了利用侧扫声纳对海底管道进行检测的工作原理,并利用海底管道和海底底质反向散射强度的计算公式探讨了声波在海底的反向散射强度、侧扫声纳声影图像的质量以及声波掠射角的取值这三者之间的关系对海底管道悬空高度h计算精度的影响,从理论上确定声波掠射角最佳取值范围的存在。通过工程实例的现场检测与比对试验,获得了在本试验所处海域环境中利用侧扫声纳检测海底管道时声波掠射角的最佳取值范围,对于类似的海底管道检测工程具有一定的指导意义。  相似文献   

2.
不同粗糙散射理论由于均采用了一定的近似方法,只在特定条件下才具有较好的预测准确性。本文采用PM海浪谱模型,利用积分方程法研究了几种常用粗糙散射理论对海面中频1~20 kHz后向声散射的有效性。仿真结果表明,中频频段相干散射一般远低于非相干散射,平均低约20 dB。四阶小粗糙微扰近似和小斜率近似的预测准确性最好,在频率15 kHz风速小于10 m/s的情况下,24°以上中高掠射角范围的小斜率近似和9°~64°掠射角范围的四阶小粗糙微扰近似的预测误差不超过2 dB。二阶小粗糙微扰近似整体预测精度偏低,特别是在小于20°的小掠射角和大于60°的大掠射角范围。掠射角80°以上的近垂直入射时,小粗糙微扰理论的预测结果偏高,相反Kirchhoff近似只在近垂直入射时才具有较好的准确性,中小掠射角的预测结果偏高。海上测量结果也验证了上述结论。  相似文献   

3.
南海浅海海底沉积物的声衰减   总被引:3,自引:0,他引:3       下载免费PDF全文
刘强  卢博 《海洋学报》2008,30(4):48-55
报道了南海浅海海底沉积物的声衰减性质。给出了测量和计算海底沉积物声衰减的方法。分析讨论了不同频率下的声衰减以及与若干个海底沉积物物理参数的关系,结果表明,同一类型沉积物在高频段时的声衰减要比低频段的声衰减大;同一频段下粗颗粒沉积物的声衰减要比细颗粒的声衰减大;北部湾海底浅层沉积物声衰减在低频100kHz下为80~150dB/m,在高频1MHz下为150~360dB/m;海南岛南部外海海底浅层沉积物声衰减在低频下为66~160dB/m,在高频1MHz下为190~350dB/m;高频段的数据与台湾海峡北部海底表层沉积物声衰减测量分析数据比较接近,而低频段的数据与台湾海峡北部海底表层沉积物声衰减测量分析数据有较大的差别。  相似文献   

4.
为了进行声相关计程仪(ACL)仿真研究,结合K irchhoff近似和R ay le igh-R ice近似散射模型,根据ACL垂直发射波束的特点,在掠射角90°附近,利用已发表的海底散射实验数据与APL-UW散射模型及L am bert公式的理论计算结果相比较,基于K irchhoff近似的散射模型与实验数据具有很好的一致性,仿真结果证明,由于不同类型海底沉积物引起的体积散射在上述情况下是可以被忽略的,这将大大简化进行声相关测速仿真研究的海底建模过程。  相似文献   

5.
多波束反向散射强度数据处理研究   总被引:13,自引:5,他引:8  
在探讨多波束测深系统反向散射强度与海底底质类型的关系基础上,研究影响反向散射强度的各种因素,主要分析了海底地形起伏、中央波束区反射信号对反向散射强度的影响,并给出了消除这些影响的方法;将处理后的“纯”反向散射强度数据镶嵌生成海底声像图,为海底底质类型划分以及地貌解译提供了基础数据和辅助判读依据.  相似文献   

6.
为获得海月水母不同频率下声学特征,在水池条件下,运用鱼探仪对海月水母开展目标强度(TS) 测量实验。结果表明:伞径约为 10 cm 海月水母,姿态角在 60°~ 90°时,单频(120 kHz)条件下,目标强度测量值为–66 ~ –63 dB,接近高通液球模型;宽频(90 kHz~170 kHz)条件下,目标强度测量值为–61 ~ –59 dB, 接近 Mutlu 目标强度和伞径的关系式模型。并进一步分析了相同伞径水母目标强度测量值产生差异的原因, 研究结果将为核电站冷源致灾生物的浅海宽频探测提供参考。  相似文献   

7.
根据2018年4月(春季,绿潮前期)和7月(夏季,绿潮后期) 南黄海营养盐、温度、盐度等水文参数及每日绿潮卫星监测数据,深入分析2018年绿潮的发展规律与营养盐结构特征之间的关系。结果表明:4月25在江苏南通外海首次发现浒苔绿潮,8月中旬在山东半岛近海消亡,其发展区域集中在122°E以西近海,且快速增殖阶段处在35°N以南江苏近海。各组分的营养盐浓度受沿岸径流、冷水团及生物作用等因素影响,均呈现江苏近海高外海以及北部低的特征。对比绿潮发展和营养盐分布呈现3个明显的绿潮−营养盐特征区域:高营养盐−绿潮快速发展区域(35°N以南,122°E 以西,江苏近海);低营养盐−绿潮消亡区域(35°N以北,122°E 以西,山东半岛外海域)及122°E以东外海无绿潮区域。不同特征区营养盐变化表明,江苏近岸较高的营养盐含量(${\rm{NO}}_3^- $-N>6.5 μmol/L, ${\rm{PO}}_4^{3-} $-P>0.27 μmol/L)和丰富来源是浒苔萌发和绿潮快速发展的重要物质基础,为绿潮发展提供了主要的氮、磷生源要素。北部山东半岛南外海较低的营养盐水平(7月,DIN<2 μmol/L, ${\rm{PO}}_4^{3-} $-P<0.03 μmol/L)是限制绿潮继续发展的重要因素。  相似文献   

8.
声波在海底界面的反射和透射是海底散射、海底混响、海底目标探测的重要问题。利用Biot多孔介质声传播理论对声波在水-多孔海底界面上的反射和透射进行了分析,具体给出反射声波的反射系数,3种透射声波的透射系数以及声能透射系数随入射波入射角和频率(10~40 kHz)的变化关系,分析了各种透射波对透射声能的贡献。多孔海底介质参数分别采用Stoll和Chotiros给出的2组参数进行理论计算。  相似文献   

9.
大洋深海硫化物矿调查成就与研究问题   总被引:2,自引:0,他引:2  
1概述 美国、法国和墨西哥《SIAMEKS》国际科考队曾于1978年在东太平洋隆起北纬21&#176;处的考察过程中发现了硫化物矿。早在100多年(1875—1878)前,英国“挑战者”号调查船发现大洋中的铁锰结核和钴锰结壳及磷灰岩。在大洋中脊范围内发现新形式有用矿产-即同热液活动密切有关的硫化物矿,它与结核和结壳不同,不仅埋藏在海底表面,而且还产于大洋基底岩石中。  相似文献   

10.
基于卫星高度计观测的全球中尺度涡的分布和传播特征   总被引:7,自引:0,他引:7  
利用将近12 a的融合高度计资料获得了全球海洋中尺度涡的空间分布和传播特征。结果表明,中尺度涡在副热带海域呈明显的带状分布,反气旋涡和气旋涡的数目相当,但在某些海域它们的数目有很大不同;在40&#176;S-60&#176;N间,大多数涡的运动方向向西,然而在40&#176;-60&#176;S间约有70%的涡向东传播;对于西向传播的涡而言,纬向平均速度随纬度有明显的变化,在赤道附近的西向传播速度为13 cm/s,而在高纬度递减到不足1 cm/s,中尺度涡的传播表现出类似于Rossby波的传播特征。  相似文献   

11.
Sea-surface acoustic backscattering measurements at moderate to high frequencies were performed in the shallow water of the south Yellow Sea, using omnidirectional spherical sources and omnidirectional hydrophones. Sea-surface backscattering data for frequencies in the 6–25 k Hz range and wind speeds of(3.0±0.5)and(4.5±1.0) m/s were obtained from two adjacent experimental sites, respectively. Computation of sea-surface backscattering strength using bistatic transducer is described. Finally, we calculated sea-surface backscattering strengths at grazing angles in the range of 16°–85°. We find that the measured backscattering strengths agree reasonably well with those predicted by using second order small-roughness perturbation approximation method with "PM" roughness spectrum for all frequencies at grazing angles ranged from 40° to 80°. The backscattering strengths varied slightly at grazing angles of 16°–40°, and were much stronger than roughness scattering. It is speculated that scattering from bubbles dominates the backscattering strengths at high wind speeds and small grazing angles. At the same frequencies and moderate to high grazing angles, the results show that the backscattering strengths at a wind speed of(4.5±1.0) m/s were approximately 5 d B higher than those at a wind speed of(3.0±0.5) m/s. However, the discrepancies of backscattering strength at low grazing angles were more than 10 d B. Furthermore the backscattering strengths exhibited no significant frequency dependence at 3 m/s wind speed. At a wind speed of 4.5 m/s, the scattering strengths increased at low grazing angles but decreased at high grazing angles with increasing grazing angle.  相似文献   

12.
Broad-band forward loss and backscattering measurements were made at low to moderate grazing angles in shallow water off San Diego using pulses extending from 1 to 6 kHz in bandwidth. For forward bounce measurements, these large bandwidths achieved time resolutions as small as 0.25 ms, and revealed fine-scale subbottom layering with separations down to approximately 50 cm. The forward loss values show large fluctuations (>10 dB) over translation distances of 20-50 m in some cases or between two measurement runs separated by a few hundred meters in other cases. This observation, along with associated variations in the extent and number of subbottom arrivals, indicates a distinct patchiness in surficial sediment type. Previous measurements made in nearby locales also evidenced strong variations in bottom loss, but lacked the spatial resolution to discern interface reflections from subbottom contributions. Broad-band backscattering strength measured at 20-40° grazing was quite homogeneous over the entire region, probably because the critical angle is below 20°, as inferred from forward loss measurements. Theory suggests that scattering at angles above critical is from subbottom inhomogeneities rather than boundary roughness. The grazing angle and frequency dependence of these backscattering data are relatively weak  相似文献   

13.
Determinations of acoustic scattering strength for sand bottoms have been made at several different shallow-water areas under downward refracting sound propagation conditions in the frequency decade below 1 kHz. The measurements have been made using explosive sources detonated at mid-water depth and bottom-mounted vertical and horizontal hydrophone line arrays as receivers. The ubiquitous presence of multipaths in shallow water prevents a direct-path scattering geometry, and scattering strength must be extracted from the full reverberation field, which complicates the determination of bottom grazing angle dependence of scattering. The major focus of this paper has been the variation of scattering strength with frequency (integrated over participating bottom angles), though estimates of the angular dependence of scattering strength have been made using the vertical receiving array. Typically the integrated scattering strength for sand bottoms reported (and elsewhere) are found to decrease below 1 kHz and in some instances to exhibit a minimum in the several hundred hertz range. Sand bottom scattering strengths below 1 kHz are significantly lower than those predicted by the Mackenzie formula and the limited angular dependence determinations have been found to be consistent with Lambert's law  相似文献   

14.
A two-scale roughness model for bottom backscattering (Novarini and Caruthers) was applied to multibeam sounder data (95 kHz) from Browns Bank (south of Yarmouth, Nova Scotia, Canada). In order to better understand frequency and incident angle dependence of backscattering, acoustic-calibration data (1-6 kHz) were collected from the same area and treated with the same model. The frequency and incident angle dependence of bottom backscattering in the multibeam and acoustic-calibration data were compared. Backscattering due to large-scale roughness was most relevant at near-normal incidence (<7°) and it was more dominant in the low-frequency range, and was strongly dependent on incident angle. Volume scattering was least dependent upon incident angle. It was the dominant factor at the large incident angle. Bragg scattering was the most significant over a very wide frequency range and was more important for high frequency (>5 kHz) and small incidence, but not near-normal incidence  相似文献   

15.
Acoustic backscattering from a sandy seabed was measured at a frequency of 5.5 kHz at a wide range of grazing angles. The measurement system used was the University of Miami's sonar tower, consisting of an omni-directional broadband source and two 16-channel hydrophone receiver arrays. A volume scattering model, which combines a fluid model with reflection/transmission coefficients derived from the Biot theory, is used. This model allows energy penetration into the bottom, calculations of the volume scattering at all grazing angles, and the frequency dependence of the sound speed in the water-saturated sediment. In the model, rather than assume sound-speed correlation length in sedimentary volume, core data were used to assimilate a 3-D fluctuation spectrum of the density. The numerical results showed excellent agreement with the measurement at lower grazing angles. We concluded that the interface roughness scattering was dominant at lower grazing angles, while the volume scattering is dominant at higher grazing angles at the sandy site. The border of the dominance of the interface and volume scattering was the so-called critical angle at this frequency. The frequency dependence of sound speeds is also discussed.  相似文献   

16.
As part of the sediment acoustics experiment 1999 (SAX99), backscattering from a sand sediment was measured in the 20- to 300-kHz range for incident grazing angles from 10/spl deg/ to 40/spl deg/. Measured backscattering strengths are compared to three different scattering models: a fluid model that uses the mass density of the sediment in determining backscattering, a poroelastic model based on Biot theory and an "effective density" fluid model derived from Biot theory. These comparisons rely heavily on the extensive environmental characterization carried out during SAX99. This environmental characterization is most complete at spatial scales relevant to acoustic frequencies from 20 to 50 kHz. Model/data comparisons lead to the conclusions that rough surface scattering is the dominant scattering mechanism in the 20-50-kHz frequency range and that the Biot and effective density fluid models are more accurate than the fluid model in predicting the measured scattering strengths. For 50-150 kHz, rough surface scattering strengths predicted by the Biot and effective density fluid models agree well with the data for grazing angles below the critical angle of the sediment (about 30/spl deg/) but above the critical angle the trends of the models and the data differ. At 300 kHz, data/model comparisons indicate that the dominant scattering mechanism may no longer be rough surface scattering.  相似文献   

17.
Backscattering measurements were performed in shallow water on sand, gravel, and clay bottoms. The equipment included a parametric array that emitted pulses of differential frequencies (8 to 40 kHz) with a 3° directivity. The ranges did not exceed 50 m. The grazing angles varied from 4° to 90°. The bottom backscattering strength does not depend on the emitted pulse type (frequency and length). If one fits a Lambert law to the variations of the backscattering strength versus the grazing angle, the value at the origin fluctuates between-15 and-22 dB without any clear effect from the different bottom types. Statistical tests show that under the experimental measurement conditions: (1) the alternative received signal does not generally follow a normal distribution; (2) among five classical distributions in sonar and radar that have been fitted to the detected-integrated signal (exponential, Weibull, chi-2, log-normal, Rice), the best-fitted law is the log-normal; (3) signals backscattered by separated areas of the same bottom can hardly be regarded as stationary and, even less, homogeneous; and (4) with an anisotropic bottom topography the statistical properties depend on the aspect under which this topography is seen  相似文献   

18.
一种分层海底反向散射模型   总被引:1,自引:1,他引:0  
In order to predict the bottom backscattering strength more accurately, the stratified structure of the seafloor is considered. The seafloor is viewed as an elastic half-space basement covered by a fluid sediment layer with finite thickness. On the basis of calculating acoustic field in the water, the sediment layer, and the basement, four kinds of scattering mechanisms are taken into account, including roughness scattering from the water-sediment interface, volume scattering from the sediment layer, roughness scattering from the sediment-basement interface,and volume scattering from the basement. Then a backscattering model for a stratified seafloor applying to low frequency(0.1–10 kHz) is established. The simulation results show that the roughness scattering from the sediment-basement interface and the volume scattering from the basement are more prominent at relative low frequency(below 1.0 kHz). While with the increase of the frequency, the contribution of them to total bottom scattering gradually becomes weak. And the results ultimately approach to the predictions of the high-frequency(10–100 kHz) bottom scattering model. When the sound speed and attenuation of the shear wave in the basement gradually decrease, the prediction of the model tends to that of the full fluid model, which validates the backscattering model for the stratified seafloor in another aspect.  相似文献   

19.
The propagation of bottom and oceanographic variability through to the variability of acoustic transmissions and reverberation is evaluated with a simple adiabatic model interacting with Gaussian distributed uncertainty in a narrow frequency band. Results show that there is significant sensitivity of time series and reverberation uncertainty to different types of environmental uncertainty. For propagation over uncertain bottoms, it is shown that it is that later part of the time series, corresponding to the highest angle energy reflecting most often off the surface and bottom, that is most sensitive to bottom uncertainty. This implies that the larger reverberation contributions from the highest grazing angles with the largest scattering strength is also the most uncertain. Conversely, it is the lowest angle arrivals which are most sensitive to uncertainty in the sound-speed profile. These behaviors are predicted analytically by the theory [K.D. LePage, in “Impact of Littoral Environmental Variability on Acoustic Predictions and Sonar Performance,” Kluwer, 2002, pp. 353-360].  相似文献   

20.
In this paper, the lowest order small-slope approximation (SSA) scattering cross section for Biot theory is derived. Numerical results are obtained for both backscattering and bistatic scattering using a modified power law spectrum, and these results are compared with those of lowest order perturbation theory (PT). Frequencies ranging from 100 Hz to 3 kHz are used for surfaces with RMS heights h of 0.1 and 1 m and a correlation length l of 10 m. The angle of incidence for the bistatic results is limited to 45/spl deg/. It is found that for the smaller surface height roughness (h = 0.1 m), the SSA and PT give the same results for frequencies up to almost 1 kHz for both backscattering and bistatic scattering. For h = 1 m, the SSA and PT backscatter results are in good agreement at all frequencies for incident grazing angles up to approximately 45/spl deg/. For the bistatic results, the SSA and PT results agree only at low grazing angles of scatter. In the specular region, the results differ significantly.  相似文献   

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