期刊文献+

深海海底斜坡环境下的声传播 被引量:19

Sound propagation in deep water with a sloping bottom
下载PDF
导出
摘要 海底地形变化对声传播具有很大影响,在南海深海区域海底斜坡环境下进行了一次声传播实验,实验显示倾斜海底环境下声传播损失出现了一些不同于平坦海底环境下的现象,分析并解释了海底地形变化对产生声传播差异的原因.结果表明,海底斜坡对声波的反射增强作用可使斜坡上方的声传播损失减少约5 d B.当声波第一次入射到达的海底位置有较小幅度的山丘(凸起高度小于1/10海深)时,海底小山丘即可对声波有反射遮挡作用,导致在其反射区特定传播距离和深度上出现倒三角声影区,比平坦海底环境下相同影区位置处的传播损失增大约8 d B,影响深度可达海面以下1500 m.而海底斜坡对声波的反射阻挡作用使得从海面反射及水体向下折射的会聚区结构消失,只剩下从水体向上折射的会聚结构.因此,海底地形对深海声传播影响较大,在水下目标探测和性能评估等应用中应予以重视. Variation of bathymetry has a large effect on the sound propagation in deep water. An acoustic propagation experiment is carried out in the South China Sea. Some different propagation phenomena are observed for two different tracks in the flat bottom and the sloping bottom environments. Numerical analysis based on the parabolic equation model RAM(range-dependent acoustic model) is performed to explain the causes of the differences. The experimental and numerical results show that the transmission losses(TLs) decrease down to about 5 d B above the slope due to the reflection of the bottom, with a high-intensity region appearing below the sea surface. When a sea hill with a height of320 m, which is less than 1/10 of water depth, exists in the incident range of sound beams on bottom first time, the sound beams are blocked due to the reflection of the sea hill. Then their propagating directions are changed, which makes an inverted-triangle shadow zone appearing in the reflection area of the sea hill. Compared with the TL results in the flat bottom environment, TLs increase up to about 8 d B in the corresponding area of the first shadow zone, and the abnormal TL effects can reach a maximal depth of 1500 m. Consequently, the shadow amplification effect caused by a small variation of bathymetry in deep water for long-range/large-depth sound propagation should receive enough attention. Furthermore, the convergence-zone structure in the sloping environment is different from that in deep water with flat bottom. The first convergence zone caused by refractions from the water above the axis of sound channel disappears. There are only the sound beams refracted back from water below the axis of sound channel. The numerical simulations show that the reflection-blockage of sound beams caused by the sloping bottom is significant. When the source is located somewhere above the slope, sound beams with large grazing angles can be reflected by the sloping bottom, and only some sound beams with small grazing angles can be refracted in the water without touching the slope and then come into the depth range of the vertical line array(VLA), forming the first part of the convergence zone refracted back from water. As the source moves farther from the VLA, the reflection-blockage of the sloping bottom becomes stronger. Sound beams are all reflected by the slope at a depth of about 3000 m, and they go through below the VLA, which leads to the absence of the first convergence zone caused by refractions from the water above the axis of sound channel. Therefore, the accuracy of bathymetry is meaningful for the sound propagation and target detection in deep water.
出处 《物理学报》 SCIE EI CAS CSCD 北大核心 2016年第1期221-229,共9页 Acta Physica Sinica
基金 国家自然科学基金(批准号:11434012,41561144006,11174312,11404366)资助的课题~~
关键词 深海 海底斜坡 声传播 会聚区 deep water sloping bottom sound propagation convergence zone
  • 相关文献

参考文献2

二级参考文献17

  • 1LI Zhenglin ZHANG Renhe PENG Zhaohui LI Xilu.Anomalous sound propagation due to the horizontal variation of seabed acoustic properties[J].Science China(Physics,Mechanics & Astronomy),2004,47(5):571-580. 被引量:5
  • 2张仁和,何怡,刘红.水平不变海洋声道中的WKBZ简正波方法[J].声学学报,1994,19(1):1-12. 被引量:46
  • 3鄢锦,张仁和.广义相积分简正波理论在双轴海洋声道中的推广与应用[J].声学学报,1997,22(3):209-222. 被引量:6
  • 4Perkins J S, Baer R N. An approximation to the threedimensional parabolic-equation method for acoustic propagation. J. Acoust. Soc. Am., 1982; 72(2): 515-522.
  • 5Lee D,Botseas G, Siegmann W L. Examination of three-dimensional effects using a propagation model with azimuth-coupling capability (FOR3D). J. Acoust. Soc.Am., 1992; 91(6): 3192-3202.
  • 6Jones R M, Riley J P, Georges T M. HARPO-A versatile three-dimensional Hamiltonian ray tracing program for acoustic waves in an ocean with irregular bottom. NOAA Wave Propagation Laboratory Report, 1986.
  • 7iBaer R N. Propagation through a three-dimension eddy including effects on an array. J. Acoust. Soc. Am., 1981;69(1): 70-75.
  • 8Chiu C S, Ehret L L. Computation of sound propagation in a three dimensionally varying ocean: A coupled normal mode approach.In: Computational Acoustics II: Ocean-Acoustic Models and Supercomputing, edited by Lee D,Cakmak A, Vichnevetsky R. Elsevier, Amsterdam, 1990:185-202.
  • 9Lee D, Pierce A D. Parabolic equation development in recent decade. J. Comp. Acoust., 1995; 3(2): 95-173.
  • 10Lee D, Pierce A D, Shange E C. Parabolic equation development in the twentieth century. J. Comp. Acoust., 2000;8(4): 527-637.

共引文献26

同被引文献102

引证文献19

二级引证文献60

相关作者

内容加载中请稍等...

相关机构

内容加载中请稍等...

相关主题

内容加载中请稍等...

浏览历史

内容加载中请稍等...
;
使用帮助 返回顶部