南京大学学报(自然科学版) ›› 2015, Vol. 51 ›› Issue (7): 96–.

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水下射流噪声数值计算与试验研究

刘永伟1,2*,商德江1,2,李琪1,2,尚大晶1,2,唐锐1,2,张超1,2,肖妍1,2,芦雪松1,2   

  • 出版日期:2015-12-21 发布日期:2015-12-21
  • 作者简介:(1. 哈尔滨工程大学水声技术实验室;2. 哈尔滨工程大学水声工程学院,哈尔滨,150001)
  • 基金资助:
    收稿日期:2015-6-30*通讯联系人:刘永伟,E-mail: liuyongwei3000@hrbeu.edu.cn(b) 2 s

Investigation on calculating and experimental measuring underwater flow noise

LiuYongwei1,2*, ShangDejiang1,2, LiQi1,2, ShangDajing1,2,TangRui1,2,ZhangChao1,2,XiaoYan1,2,LuXuesong   

  • Online:2015-12-21 Published:2015-12-21
  • About author: (1. Acoustic Science and Technology Laboratory, Harbin Engineering University; 2. College of Underwater Acoustic Engineering, Harbin Engineering University, Harbin,15001,China)

摘要: 水下射流噪声所引起的安全性日益受到重视。基于大涡模拟和莱特希尔声类比方程相结合的方法,对一圆形喷嘴的射流噪声开展了数值仿真。采用有限元软件(ANSYS)建立喷嘴和流体的计算模型,利用ANSYS中的Fluent软件进行流场计算,得到随时间变化的射流流场特性,然后对其进行傅利叶分析,导入至ACTRAN软件进行声学计算。经分析发现:射流辐射噪声主要发生在距离喷嘴8~10D(D为喷嘴横截面的最大尺度)的过渡区;而且射流所辐射噪声的指向性是四极子的。基于混响法的原理,建立了一套水下射流噪声测量系统。开展了射流源为重力式水箱的射流噪声试验。经研究发现:水下射流噪声辐射声功率总声级与来流速度的8次方成正比。对于同一类型的喷嘴,射流噪声总声级只取决于射流源的压力,而与喷嘴的截面积无关。试验研究结果与仿真结果吻合较好!研究结果对于指导水下射流结构低噪声设计有较为重要的参考价值。

Abstract: Based on the combination of large eddy simulation theory and Lighthill’s acoustic analogy equation, numerical simulation of underwater flow noise is investigated. The calculation model of nozzle and fluid is built up by finite element software, ANSYS. The property of fluid field is calculated by the software of Fluent in the ANSYS. The property changing with time is gotten and dealt with by FFT, then, introduced into ACTRAN. Therefore, sound field of flow noise is calculated. The flow noise of a circular nozzle is carefully investigated. The diameter of the nozzle is 20 mm, and fluid speed is 10 m/s. The frequency range is from 20 to 5000 Hz. The results demonstrate that sound radiation from flow noise is mainly in transition area. The distance between the nozzle and transition area is in the range from 8 to 10 D. Here, D is maximum dimension of the nozzle. Meanwhile, the directivity of radiated noise in transition area is equivalent to a fourth polar point source. Based on the principle of reverberation method, a measurement system of underwater flow noise is built up. The first kind of nozzle is a steel pipe, and inner diameter is 200 mm. The pipe is placed in a reverberation water pool. The dimension of the pool is 9×6×15 (m3). In the pool, there are two parts: one part is flow area; the other part is test area. In test area, there are 32 hydrophones, which are disposed at different depth. The second kind of nozzle is a circular nozzle with coverage formation. The diameters of circular nozzle are 10 mm, 20 mm, 30 mm, respectively. The nozzle is placed in a reverberation water tank, which is made up by steel plates and supported by separated points at the bottom. The dimension of water tank is 3.6×1.7×9.0(m3). In the top, there are three ducts. The ducts can hinder sound propagation from the tank to the outside, and vice versa. The tank also separated into two parts: one part is flow area; the other part is test area. These actions can protect hydrophones from the knock by the flow. In test area, there are four hydrophones, which are used as a line array to receive the signal induced by the flow. The flow noise source is a tank in high place. And the flow is generated by the gravity. The total sound radiation power level from flow noise is proportional to the 8th power of fluid speed. The results demonstrate that if the nozzle of uniform type, total level of flow noise is only decided by the pressure of flow noise source, and not related to the section area of nozzle. The results are coincided with the simulation.

[1] Ruprecht A, Helmrich T, Aschenbrennert, et al. Simulation of pressure surge in a hydro power plant caused by an elbow draft tube. In: IAHR WG 1 symposium. The behavior of hydraulic machinery under steady oscillatory conditions. Trondheim: 2001: 1-10
[2] Bensow R. E, et al. Large eddy simulation of the viscous flow around submarine hulls. In: 25th symposium on naval hydrodynamics. Canada: 2004: 261-276
[3] 张涛,朱晓军,彭飞等. 近壁面处理对湍流数值计算的影响分析. 海军工程大学学报, 2013, 25(06): 104-108
[4] Stanley,S. A., Sarkar, S. & Mellado, J. P. A study of the flow-field evolution and mixing in a planar turbulent jet using direct numerical simulation. J. Fluid Mech., 2002, 450: 377-407
[5] 范全林,王希麟,张会强等. 圆湍射流拟序结构研究进展. 力学进展, 2002, 02(5): 109-118
[6] Niklas Andersson,lars-erikisson,Lars Davidson. A study of Mach 0.75 jets and their radiated sound using large-eddy simulation. In: 10th AIAA/CEAS Aeroacoustics conference. Manchester: 2004: 1-24
[7] Li X D, Gao J H. Prediction and understanding of three dimensional screech phenomenon from a circular nozzle. In: 13th AIAA/CEAS Aeroacoustics conference. Rome: 2007: 1-19
[8] Groschel E, Renze P, Schroder W, et al. Towards Noise Reduction of Coaxial Jets. In: 13th AIAA/CEAS Aeroacoustics conference. Rome: 2007: 1-18
[9] 王兴,郑刘,周月荣等. 不同喷嘴射流流场结构及噪声. 推进技术, 2011, 32(3): 365-369
[10] 杨洪涛,王从东,张东速等. 高压水射流反射声信号特征值提取方法的研究. 中国机械工程, 2010, 21(20): 2434-2467
[11] 禹言芳,李春晓,孟辉波等. 不同形状喷嘴的射流流动与卷吸特性. 过程工程学报, 2014, 14(4): 549-555
[12] 汤冰,朱旻明,刘明侯. 声激励对圆射流流场结构控制的大涡模拟. 中国科学技术大学学报, 2015, 45(2): 159-167
[13] Smagorinsky J. General circulation experiments with the primitive equations (I): The basic experiment. Monthly Weather Review, 1963, 91(3): 99-165
[14] Lighthill, M.J. On sound generated aerodynamically. Ⅱ. Turbulence as a source of sound. Proc.Roy.Soc., 1954, 1148: 1-32
[15] Goldstein. 气动声学. 闫再友译. 北京: 国防工业出版社, 2014, 78.
[16] 郝宗睿,王乐勤,周忠海. 喷射流场及其辐射声场数值模拟. 哈尔滨工程大学学报,2012, 33(8): 966-971
[17] 尚大晶,李琪,商德江等. 水下声源辐射声功率测量实验研究. 哈尔滨工程大学学报, 2010, 31(7): 938-944
[18] 朱万方. 基于柱塞泵动力源的水射流噪声特性研究. 硕士学位论文. 武汉:华中科技大学, 2012
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