潜艇激发的海面辐聚辐散场是其重要的尾流水动力特征,是重要的非声探测源。本文采用CFD技术对Suboff模型在层化流体环境中激发的自由表面散度场(辐聚辐散场)进行数值模拟研究,并在层化水池内采用PIV技术对数值仿真结果进行了验证。研究结果表明:仿真计算得到的散度场尾迹开角和最大强度与实验值相符合;随着内Froude数的增大,潜艇尾迹表面辐聚辐散场开角逐渐双e指数递减过渡到线性递减。
The surface divergence field excited by submarine is an important hydrodynamic characteristic of wake and is an important source of non-acoustic detection. In this paper, CFD was used to numerically simulate the free surface divergence field excited by Suboff model in a stratified fluid environment, and PIV technology was used to verify the numerical simulation results in a stratified pool. The results show that the Kelvin angle and the maximum intensity of the divergence wake calculated by simulation are in good agreement with the experimental values. With the increase of the internal Froude number, the Kelvin angle of divergence field on the submarine wake surface gradually decreases from double e exponent function to decrease linear function.
2022,44(15): 60-65 收稿日期:2022-01-14
DOI:10.3404/j.issn.1672-7649.2022.15.013
分类号:O352
作者简介:侯建军(1973-),男,博士,副教授,研究方向为舰艇运动力学与军事航海
参考文献:
[1] 崔国恒, 于德新. 非声探潜技术现状及其对抗措施[J]. 火力与指挥控制, 2007, 32(12)
CUI Guoheng, YU Dexin. Status quo of non-acoustics antisubmarine detecting technology and its countermeasures[J]. Fire Control and Command Control, 2007, 32(12)
[2] 韩晶, 赵朝方. 海洋遥感技术在探测潜艇中的应用[J]. 装备环境工程, 2008, 5(3): 67–70
[3] 陈允锋, 刘伟. 非声探潜新技术浅析[J]. 光纤与电缆及其应用技术, 2016, 6(6): 29–36
[4] 张军, 张效慈, 赵峰. 源于水动力学的潜艇尾迹非声探测技术研究进展[J]. 船舶力学, 2003, 7(2): 121–128
[5] WREN G G, MAY D. Detection of submerged vessels using remote sensing techniques[J]. Australian Defense Force, 1997, 127: 8–15
[6] REED A M. MILGRAM J H. Ship wakes and their radar images[J]. Annu Rev Fluid Mech, 2002(34): 469–502
[7] GONG B, HUANG W G, CHEN P. Study on the SAR imaging simulation of Kelvin ship wake[J]. Marine Science Bulletin, 2013, 32(2): 208–213
[8] YEUNG R W, NGUYEN T C. Waves generated by a moving source in a two-layer ocean of finite depth[J]. Journal of Engineering Mathematics, 1999(35): 85–107
[9] GAYEN B, TAYLOR R J, and SARKAR S. Large eddy simulation of a stratified boundary layer under an oscillatory current. Journal[J]. Journal. Fluid Mech, 2010, 643: 233–266
[10] 陈圣涛, 王慧丽, 王运鹰, 等. 舰船气泡尾流特性的数值模拟和实验研究[J]. 船舶力学, 2012, 16(4): 342–348
[11] 陈雄, 杨智惠, 韩玉阁. 温度分层海水中潜艇尾流数值模拟[J]. 声学技术, 2016, 35(3): 118–121
[12] 万鹏程, 傅慧萍. 舰船气泡尾流数值模拟[J]. 上海交通大学学报, 2013, 47(2): 193–197
[13] BUICK J M, MARTIN A J, COSGROVE J A, et al. Comparison of a lattice Boltzmann simulation of steep internal waves and laboratory measurements using particle image velocimetry[J]. European Journal of Mechanics B/Fluids, 2003, 22: 27–38
[14] KRAFT W N. Experimental investigation of a stratified buoyant wave. [M]. United Sates: Texas A & M University, 2004.
[15] 李广年, 李磊, 谢永和. PIV技术在旋转流场测试中的应用[J]. 中国造船, 2011, 52: 145–149
[16] 李广年, 张国平, 陆林章. 大型空泡水筒中螺旋桨尾流场2D-PIV测量[J]. 船舶力学, 2009(5): 682–687
[17] 黄少锋, 张志荣, 赵峰. 自由面肥大船粘性绕流场的数值模拟[J]. 船舶力学, 2008(1): 46–53
[18] 代钦, 赵莉莉. 近自由表面翼型尾流速度场的PIV测量及POD分析[J]. 水动力学研究与进展A辑, 2008, 23(2): 196–203
[19] FELLI M, PEREIRA F, CALCAGNO G. A modular Stereo-PIV probe for underwater applications configurations and measurement performance[C] // Proceedings of 5th International Symposium on Particle Image Velocimetry. Busan, Korea, 2003.
[20] 王志博, 姚惠之, 张楠. 指挥台围壳对潜艇尾流影响的计算研究[J]. 船舶力学, 2009, 13(2): 197–202
[21] 李茂华, 龚杰. 三维PIV应用于船舶精细流场测试研究进展[J]. 中国舰船研究, 2015, 10(1): 58–67
[22] 熊莉芳, 林源, 李世武. K-ε湍流模型及其在FLUENT软件中的应用[J]. 工业加热, 2007, 4(36): 13–15
[23] ALIN N, BENSOW R E, FUREBY C. Current capabilities of DES and LES for submarines at straight course[J]. Journal of Ship Research, 2010, 54(3): 184–196