Please wait a minute...
Chin. Phys. B, 2019, Vol. 28(1): 014302    DOI: 10.1088/1674-1056/28/1/014302
ELECTROMAGNETISM, OPTICS, ACOUSTICS, HEAT TRANSFER, CLASSICAL MECHANICS, AND FLUID DYNAMICS Prev   Next  

Effects of rough surface on sound propagation in shallow water

Ruo-Yun Liu(刘若芸)1,2, Zheng-Lin Li(李整林)1
1 State Key Laboratory of Acoustics, Institute of Acoustics, Chinese Academy of Sciences, Beijing 100190, China;
2 University of Chinese Academy of Sciences, Beijing 100190, China
Abstract  

Underwater acoustic applications depend critically on the prediction of sound propagation, which can be significantly affected by a rough surface, especially in shallow water. This paper aims to investigate how randomly fluctuating surface influences transmission loss (TL) in shallow water. The one-dimension wind-wave spectrum, Monterey-Miami parabolic equation (MMPE) model, Monte Carlo method, and parallel computing technology are combined to investigate the effects of different sea states on sound propagation. It is shown that TL distribution properties are related to the wind speed, frequency, range, and sound speed profile. In a homogenous waveguide, with wind speed increasing, the TLs are greater and more dispersive. For a negative thermocline waveguide, when the source is above the thermocline and the receiver is below that, the effects of the rough surface are the same and more significant. When the source and receiver are both below the thermocline, the TL distributions are nearly the same for different wind speeds. The mechanism of the different TL distribution properties in the thermocline environment is explained by using ray theory. In conclusion, the statistical characteristics of TL are affected by the relative roughness of the surface, the interaction strength of the sound field with the surface, and the changes of propagating angle due to refraction.

Keywords:  surface fluctuation      shallow water      transmission loss      statistical characteristics  
Received:  07 August 2018      Revised:  17 October 2018      Accepted manuscript online: 
PACS:  43.30.+m (Underwater sound)  
  43.30.Hw (Rough interface scattering)  
Fund: 

Project supported by the National Natural Science Foundation of China (Grant Nos. 11434012, 11874061, and 41561144006).

Corresponding Authors:  Zheng-Lin Li     E-mail:  lzhl@mail.ioa.ac.cn

Cite this article: 

Ruo-Yun Liu(刘若芸), Zheng-Lin Li(李整林) Effects of rough surface on sound propagation in shallow water 2019 Chin. Phys. B 28 014302

[1] Luo J and Badiey M 2005 J. Acoust. Soc. Am. 118 2038
[2] Al-Kurd A 1996 J. Acoust. Soc. Am. 100 2703
[3] Wang X H, Peng Z H and Li Z L 2007 Tech. Acoust. 26 551 (in Chinese)
[4] Li Z L 2001 The Effect of Internals Waves, Surface Fluctuation and Bottom Roughness on Matched Field Source Localization in Shallow Water (Ph. D. dissertation) (Beijing: Graduate University of Chinese Academy of Sciences) (in Chinese)
[5] Park C, Seong W, Gerstoft P and Hodgkiss W S 2011 J. Acoust. Soc. Am. 129 98
[6] Karjadi E A, Badiey M, Kirby J T and Bayindir C 2012 IEEE J. Ocean. Eng. 37 112
[7] Badiey M, Mu Y K, Simmen J A and Forsythe S E 2000 IEEE J. Ocean. Eng. 25 492
[8] Yang T C 2006 J. Acoust. Soc. Am. 120 2595
[9] Dahl P H 1996 J. Acoust. Soc. Am. 100 748
[10] Tindle C T and Deane G B 2005 J. Acoust. Soc. Am. 117 2783
[11] Dahl P H 2001 IEEE J. Ocean. Eng. 26 141
[12] Siderius M and Porter M B 2008 J. Acoust. Soc. Am. 124 137
[13] Eckart C 1953 J. Acoust. Soc. Am. 25 566
[14] Urick R and Hoover R 1956 J. Acoust. Soc. Am. 28 1038
[15] Kuperman W A and Ingenito F 1977 J. Acoust. Soc. Am. 61 1178
[16] Weston D E and Ching P A 1989 J. Acoust. Soc. Am. 86 1530
[17] Zou Z G and Badiey M 2018 IEEE J. Ocean. Eng. 43 1187
[18] Smith K B and Tappert F D 1993 UMPE: University Miami Parabolic Equation Model (Version 1.0)
[19] Neumann G and Pierson W J 1966 Principle of Physical Oceanography (Englewood Cliffs: Prentice Hall) p. 351
[20] Smith K B 2001 J. Comput. Acoust. 9 243
[21] Hardin R H and Tappert F D 1973 SIAM Rev. 15 423
[22] Tappert F D and Lan N 1985 J. Acoust. Soc. Am. 77 S101
[23] Thomson D J and Chapman N R 1983 J. Acoust. Soc. Am. 74 1848
[24] Lusk E and Gropp W 1995 Adv. Parallel Computing 10 265
[25] Li F H and Zhang R H 2000 Acta Acust. 25 297 (in Chinese)
[1] Exact solutions of a (2+1)-dimensional extended shallow water wave equation
Feng Yuan(袁丰), Jing-Song He(贺劲松), Yi Cheng(程艺). Chin. Phys. B, 2019, 28(10): 100202.
[2] Propagation of acoustic waves in a fluid-filled pipe with periodic elastic Helmholtz resonators
Dian-Long Yu(郁殿龙), Hui-Jie Shen(沈惠杰), Jiang-Wei Liu(刘江伟), Jian-Fei Yin(尹剑飞), Zhen-Fang Zhang(张振方), Ji-Hong Wen(温激鸿). Chin. Phys. B, 2018, 27(6): 064301.
[3] Fully nonlinear (2+1)-dimensional displacement shallow water wave equation
Feng Wu(吴锋), Zheng Yao(姚征), Wanxie Zhong(钟万勰). Chin. Phys. B, 2017, 26(5): 054501.
[4] Optimized design and fabrication of nanosecond response electro–optic switch based on ultraviolet-curable polymers
Zhao Xu-Liang (赵旭亮), Yue Yuan-Bin (岳远斌), Liu Tong (刘通), Sun Jian (孙健), Wang Xi-Bin (王希斌), Sun Xiao-Qiang (孙小强), Chen Chang-Ming (陈长鸣), Zhang Da-Ming (张大明). Chin. Phys. B, 2015, 24(4): 044101.
[5] Modified (2+1)-dimensional displacement shallow water wave system and its approximate similarity solutions
Liu Ping(刘萍) and Fu Pei-Kai(付培凯) . Chin. Phys. B, 2011, 20(9): 090203.
[6] Statistical characteristics of meso-scale vortex effects on the track of a tropical cyclone
Luo Zhe-Xian(罗哲贤), Sun Zhi-An(孙治安), and Ping Fan(平凡) . Chin. Phys. B, 2011, 20(4): 049201.
No Suggested Reading articles found!