Numerical Simulation of External Flow Field Self-excited Oscillating Pulsed Cavitation Jet of Dual Chamber Nozzle
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摘要: 以单腔室自激振荡脉冲喷嘴为基础,采用串联方式建立双腔室自激振荡脉冲喷嘴,应用FLUENT软件对其外部流场进行数值模拟,分析入射压力、靶距、腔长比、腔径比的改变对外部流场的影响。结果表明:当入射压力在1.1 MPa~4.4 MPa间变化时,空化程度随着压力增大而减小,同时压力每增加一倍时,靶面处最大速度增长约20~76 m/s;当靶距在100 mm~400 mm范围内变化时,空化程度随靶距增大而增大,但当靶距达到400 mm时,会因靶距太远气泡在空中溃灭空化程度骤减;当腔长比为0.67时或腔径比为1.2时,腔室内的涡环结构对称性好,有利于脉冲和空化的产生;同时具有较高的动能,当腔长与腔径同时取最佳值时,脉冲性最佳具有较好的清洗效果。Abstract: In single-chamber self-oscillation pulse basis nozzle, a double-chamber self-excited oscillation pulse nozzle was established in series, The FLUENT software was used to simulate the external flow field, and the effects of changes in incident pressure, target distance, cavity length ratio and cavity diameter ratio on the external flow field were analyzed. The results show that when the incident pressure varies between 1.1 MPa and 4.4 MPa, the degree of cavitation decreases with the increase of pressure, and the maximum velocity at the target surface increases about 20~76 m/s every time the pressure is doubled; When the target distance varies from 100 mm to 400 mm, the degree of cavitation increases with the increase of the target distance. However, when the target distance reaches 400 mm, the degree of cavitation in the air collapses rapidly due to the target distance. When the cavity length ratio is 0.67 or the cavity diameter ratio is 1.2, the vortex ring structure in the chamber has good symmetry, which is beneficial to the generation of pulse and cavitation. At the same time, it has high kinetic energy. When the cavity length and the cavity diameter are taken its optimal values at the same time, the pulse quality is optimal and has a good cleaning effect.
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Key words:
- dual chamber /
- cavitation jets /
- numerical analysis /
- cavitation model /
- cavitation nozzle
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表 1 不同腔长腔径结构参数
mm 腔长 腔径 腔径 腔径 腔径 腔径 20 60 80 100 120 140 40 60 80 100 120 140 60 60 80 100 120 140 80 60 80 100 120 140 100 60 80 100 120 140 -
[1] Knapp R T, Daily J W, Hammit F G. Cavitation[M]. New York:McGraw-Hill, 1970 [2] 于秀芳.低压大流量自激脉冲空化射流打击特性研究[D].济南: 山东大学, 2016 http://cdmd.cnki.com.cn/Article/CDMD-10422-1016165060.htmYu X F. Study on the strike characteristics of jet low-pressure high-flow self-excited pulse cavitation[D]. Ji'nan: Shandong University, 2016(in Chinese) http://cdmd.cnki.com.cn/Article/CDMD-10422-1016165060.htm [3] 汪朝晖, 胡亚男, 饶长健, 等.自激振荡脉冲喷嘴空化效应及其射流形态的数值分析[J].机械工程学报, 2017, 28(13):1535-1541 http://d.old.wanfangdata.com.cn/Periodical/zgjxgc201713004Wang Z H, Hu Y N, Rao C J, et al. Numerical analysis of cavitation effects of self-excited oscillation pulse nozzles and jet forms[J]. China Mechanical Engineering, 2017, 28(13):1535-1541(in Chinese) http://d.old.wanfangdata.com.cn/Periodical/zgjxgc201713004 [4] Sou A, Biçer B, Tomiyama A. Numerical simulation of incipient cavitation flow in a nozzle of fuel injector[J]. Computers & Fluids, 2014, 103:42-48 http://cn.bing.com/academic/profile?id=bff56a3346745571a53722473e712271&encoded=0&v=paper_preview&mkt=zh-cn [5] Suh H K, Lee C S. Effect of cavitation in nozzle orifice on the diesel fuel atomization characteristics[J]. International Journal of Heat and Fluid Flow, 2008, 29(4):1001-1009 doi: 10.1016/j.ijheatfluidflow.2008.03.014 [6] 方珍龙, 康勇, 王晓川, 等.腔径比对亥姆赫兹自振射流性能影响[J].浙江大学学报(工学版), 2016, 50(11):2100-2106 doi: 10.3785/j.issn.1008-973X.2016.11.009Fang Z L, Kang Y, Wang X C, et al. Numerical investigation of cavity diameter ratio influence on Helmholtz oscillation waterjet[J]. Journal of Zhejiang University (Engineering Science), 2016, 50(11):2100-2106(in Chinese) doi: 10.3785/j.issn.1008-973X.2016.11.009 [7] 汪朝晖, 胡亚男, 廖振方, 等.基于自激振荡脉冲效应的雾化喷嘴出口流道空化特性研究[J].机械工程学报, 2016, 52(14):204-212 http://d.old.wanfangdata.com.cn/Periodical/jxgcxb201614023Wang Z H, Hu Y N, Liao Z F, et al. Cavitation characteristics study on the outlet channel of atomization nozzle based on the self-excited oscillating pulse effects[J]. Journal of Mechanical Engineering, 2016, 52(14):204-212(in Chinese) http://d.old.wanfangdata.com.cn/Periodical/jxgcxb201614023 [8] 王乐勤, 王循明, 徐如良, 等.自激振荡脉冲喷嘴结构参数配比试验研究[J].工程热物理学报, 2004, 25(6):956-958 doi: 10.3321/j.issn:0253-231X.2004.06.016Wang L Q, Wang X M, Xu R L, et al. Experimental study on structural parameters optimized design of the self-excited oscillation pulsed jet nozzle[J]. Journal of Engineering Thermophysics, 2004, 25(6):956-958(in Chinese) doi: 10.3321/j.issn:0253-231X.2004.06.016 [9] Kubota A, Kato H, Yamaguchi H. A new modelling of cavitating flows:a numerical study of unsteady cavitation on a hydrofoil section[J]. Journal of Fluid Mechanics, 1992, 240:59-96 doi: 10.1017/S002211209200003X [10] 赵权, 文国军, 王玉丹, 等.脉冲来流下自激振荡喷嘴仿真研究[J].矿山机械, 2016, 44(12):20-24 http://d.old.wanfangdata.com.cn/Periodical/ksjx201612005Zhao Q, Wen G J, Wang Y D, et al. Simulation and study on self-excited oscillation nozzle in upstream pulsed flow[J]. Mining & Processing Equipment, 2016, 44(12):20-24(in Chinese) http://d.old.wanfangdata.com.cn/Periodical/ksjx201612005 [11] Fang Z L, Kang Y, Yang X F, et al. The influence of collapse wall on self-excited oscillation pulsed jet nozzle performance[C]//Proceedings of the 26th IAHR Symposium on Hydraulic Machinery and Systems. Beijing: IOP, 2012: 1-6 https://www.researchgate.net/publication/258613883_The_influence_of_collapse_wall_on_self-excited_oscillation_pulsed_jet_nozzle_performance [12] 韩健, 蔡腾飞, 潘岩, 等.风琴管喷嘴和赫姆霍兹喷嘴射流特性分析[J].煤矿安全, 2017, 48(7):134-137 http://d.old.wanfangdata.com.cn/Periodical/mkaq201707036Han J, Cai T F, Pan Y, et al. Study on jet's characteristics of organ nozzle and Helmholtz nozzle[J]. Safety in Coal Mines, 2017, 48(7):134-137(in Chinese) http://d.old.wanfangdata.com.cn/Periodical/mkaq201707036 [13] 焦磊, 吴大转, 王乐勤, 等.两种喷嘴喷射性能的试验研究[J].工程热物理学报, 2006, 27(6):962-964 doi: 10.3321/j.issn:0253-231X.2006.06.020Jiao L, Wu D Z, Wang L Q, et al. Experiment study on the spurting characteristic of two types of jet[J]. Journal of Engineering Thermophysics, 2006, 27(6):962-964(in Chinese) doi: 10.3321/j.issn:0253-231X.2006.06.020 [14] Alehossein H, Qin Z. Numerical analysis of Rayleigh-Plesset equation for cavitating water jets[J]. International Journal for Numerical Methods in Engineering, 2007, 72(7):780-807 doi: 10.1002/(ISSN)1097-0207 [15] 唐川林, 吴霞, 胡东.串联型脉冲喷嘴的实验研究[J].湖南工业大学学报, 2007, 21(4):60-64 http://d.old.wanfangdata.com.cn/Periodical/zzgxyxb200704014Tang C L, Wu X, Hu D. The experimental study on the series pulsed nozzle[J]. Journal of Hunan University of Technology, 2007, 21(4):60-64(in Chinese) http://d.old.wanfangdata.com.cn/Periodical/zzgxyxb200704014 [16] 邓嵘, 李向东, 丰波.双腔室自振脉冲喷嘴数值分析与实验研究[J].机械科学与技术, 2017, 36(12):1816-1822 http://journals.nwpu.edu.cn/jxkxyjs/CN/abstract/abstract6881.shtmlDeng R, Li X D, Feng B. Numerical analysis and experimental research of a dual chamber self-excited oscillation pulsed jet nozzle[J]. Mechanical Science and Technology for Aerospace Engineering, 2017, 36(12):1816-1822(in Chinese) http://journals.nwpu.edu.cn/jxkxyjs/CN/abstract/abstract6881.shtml [17] Zwart P J, Gerber A G, Belamri T. A two-phase flow model for predicting cavitation dynamics[C]//Proceedings of the Fifth International Conference on Multiphase Flow. Yokohama, Japan: ICMF, 2004: 1-11