横向射流影响缓燃向爆震转捩过程的试验研究

doi:10.7527/S1000-6893.2017.121412

流体力学与飞行力学

本期目录 | 过刊浏览 | 高级检索

前一篇 | 后一篇

横向射流影响缓燃向爆震转捩过程的试验研究

彭瀚, 黄玥, 刘晨, 邢菲, 栾振业

厦门大学航空航天学院, 厦门 361005

收稿日期:2017-05-12 修回日期:2017-06-27 出版日期:2018-02-15 发布日期:2017-06-27
通讯作者: 黄玥,E-mail:154552879@qq.com E-mail:huangyue@xmu.edu.cn
基金资助:
国家自然科学基金（51406171）；中央高校基本科研业务费专项资金（20720150094）；福建省自然科学基金（2015J05111）；航空科学基金（20152868006）

Experimental study of effects of fluidic obstacle parameters on deflagration-to-detonation transition

PENG Han, HUANG Yue, LIU Chen, XING Fei, LUAN Zhenye

School of Aerospace Engineering, Xiamen University, Xiamen 361005, China

Received:2017-05-12 Revised:2017-06-27 Online:2018-02-15 Published:2017-06-27
Supported by:
National Natural Science Foundation of China (51406171); the Fundamental Research Funds for the Central Universities (20720150094); Natural Science Foundation of Fujian Province (2015J05111); Aeronautical Science Foundation of China(20152868006)

摘要/Abstract

摘要： 为探究横向射流对缓燃转爆震过程的影响，在高为20 mm，深为6 mm，总长为810 mm的矩形通道内进行了横向射流加速起爆的单爆试验。采用甲烷和氧气的预混气为反应物，点火源为点火能量为50 mJ的弱火花塞点火。垂直于主流的横向喷射孔径为1 mm，喷射介质为与反应物同浓度的混气。试验主要研究射流延迟时间、射流位置、射流数量和射流分布形式对起爆特性的影响。结果显示，射流各喷射位置下均存在相应的最佳射流延迟喷射时间使得预混气的起爆时间最短。射流位置分别位于距点火区90、270 mm处的平行双射流和90、180 mm处的交错射流均具有最短的起爆时间，约为1 ms。

关键词: 横向射流, 缓燃转爆震, 射流位置, 多股射流, 单次爆震试验

Abstract: To investigate the effect of jet in cross flow on the process of Deflagration-to-Detonation Transition (DDT), an single-shot detonation experiment is conducted in a rectangular channel with a height of 20 mm, a depth of 6 mm, and a total length of 810 mm. The premixed methane/oxygen mixture is the reactant, which is ignited by a 50 mJ spark plug. The diameter of the injector of jet in cross flow is 1 mm, and the injection gas is the same concentration premixed mixture. The effect of the jet delay time, the jet location, the quantity and jet distribution pattern on detonation initiation are studied by a series of tests. The results show that there exits at various injection locations the corresponding optimal jet delay time to minimize the DDT time. The DDT time of the parallel double jets located 90 and 270 mm away from the ignition zone and the staggered jets located at 90 and 180 mm away from the ignition zone is the shortest, about 1 ms.

Key words: jet in cross flow, deflagration-to-detonation, jet flow location, multiple jet flow, single-shot detonation test

中图分类号:

V231.2

彭瀚, 黄玥, 刘晨, 邢菲, 栾振业. 横向射流影响缓燃向爆震转捩过程的试验研究[J]. 航空学报, 2018, 39(2): 121412-121412.

PENG Han, HUANG Yue, LIU Chen, XING Fei, LUAN Zhenye. Experimental study of effects of fluidic obstacle parameters on deflagration-to-detonation transition[J]. ACTA AERONAUTICAET ASTRONAUTICA SINICA, 2018, 39(2): 121412-121412.

参考文献

[1] KAILASANATH K. Review of propulsion applications of detonation waves[J]. AIAA Journal, 2015, 38(9):1698-1708.[2] PANDEY K M, DEBNATH P. Review on recent advances in pulse detonation engines[J]. Journal of Combustion, 2016(5):4193034.[3] AUSTIN J M, SHEPHERD J E. Detonations in hydrocarbon fuel blends[J]. Combustion & Flame, 2003, 132(1):73-90.[4] 严传俊, 范玮. 脉冲爆震发动机原理及关键技术[M]. 西安:西北工业大学出版社, 2005:9-14. YAN C J, FAN W. Principle and key technologies of pulse detonation engine[M]. Xi'an:Northwestern Polytechnical University Press, 2005:9-14(in Chinese).[5] 黄玥, 唐豪, 李建中, 等. 煤油/空气小尺寸脉冲爆震发动机实验研究[J]. 航空学报, 2009, 30(11):2015-2022. HUANG Y, TANG H, LI J Z, et al. Experimental investigation on small-scale pulse detonation engine with kerosene/air[J]. Acta Aeronautica et Astronautica Sinica, 2009, 30(11):2015-2022(in Chinese).[6] BAZHENOVA T V, GOLUB V V. Use of gas detonation in a controlled frequency mode[J]. Combustion, Explosion and Shock Waves, 2003, 39(4):365-381.[7] LEE J H S. The detonation phenomenon[M]. Cambridge:Cambridge University Press, 2008:267-271.[8] COOPER M, JACKSON S, AUSTIN J, et al. Direct experimental impulse measurements for detonations and deflagrations[J]. Journal of Propulsion and Power, 2002, 18(5):1033-1041.[9] LEE S Y, CONRAD C, WATTS J, et al. Deflagration to detonation transition study using simultaneous schlieren and OH PLIF images[C]//36th AIAA/ASME/SAE/ASEE Joint Propulsion Conference and Exhibit. Reston, VA:AIAA, 2000:3217.[10] TEODORCZYK A, DROBNIAK P, DABKOWSKI A. Fast turbulent deflagration and DDT of hydrogen-air mixtures in small obstructed channel[J]. International Journal of Hydrogen Energy, 2009, 34(14):5887-5893.[11] PAXSON D, SCHAUER F, Hopper D. Performance impact of deflagration to detonation transition enhancing obstacles[C]//47th AIAA Aerospace Sciences Meeting Including the New Horizons Forum and Aerospace Exposition. Reston, VA:AIAA, 2012:502.[12] 邓君香, 严传俊, 郑龙席, 等. 障碍物对脉冲爆震发动机性能影响的数值模拟[J]. 航空学报, 2009, 30(4):614-621. DENG J X, YAN C J, ZHENG L X, et al. Numerical simulation of effect of obstacles on pulse detonation engine performances[J]. Acta Aeronautica et Astronautica Sinica, 2009, 30(4):614-621(in Chinese).[13] AHMED K A, FORLITI D J. Fluidic flame stabilization in a planar combustor using a transverse slot jet[J]. AIAA Journal, 2009, 47(11):2770-2775.[14] KNOX B W, FORLITI D J, STEVENS C A, et al. Unsteady flame speed control and deflagration-to-detonation transition enhancement using fluidic obstacles[C]//48th AIAA Aerospace Sciences Meeting Including the New Horizons Forum and Aerospace Exposition. Reston, VA:AIAA, 2010:151.[15] KNOX B, FORLITI D, STEVENS C, et al. A comparison of fluidic and physical obstacles for deflagration-to-detonation transition[C]//49th AIAA Aerospace Sciences Meeting Including the New Horizons Forum and Aerospace Exposition. Reston, VA:AIAA, 2011:587.[16] MCGARRY J, AHMED K. Laminar deflagrated flame interaction with a fluidic jet flow for deflagration-to-detonation flame acceleration[C]//51st AIAA/SAE/ASEE Joint Propulsion Conference. Reston, VA:AIAA, 2015:4096.[17] CHAMBERS J, MCGARRY J, AHMED K. Fluidic jet augmentation of a deflagrated turbulent flame for deflagration-to-detonation[C]//54th AIAA Aerospace Sciences Meeting. Reston, VA:AIAA, 2016:0443.[18] 白桥栋, 翁春生. 射流对爆轰波传播过程影响的理论研究[J]. 弹道学报, 2013, 25(3):83-87. BAI Q D, WENG C S. Theoretical study of influence of jet flow on propagation of detonation wave[J]. Journal of Ballistics, 2013, 25(3):83-87(in Chinese).[19] 王永佳, 范玮, 张扬, 等. 流体障碍物对爆震燃烧起爆性能影响的实验研究[J]. 推进技术, 2017, 38(3):646-652. WANG Y J, FAN W, ZHANG Y, et al. Experimental study for effects of fluidic obstacles on detonation initiation performance[J]. Journal of Propulsion Technology, 2017, 38(3):646-652(in Chinese).[20] LIU C, HUANG Y, YANG W, et al. Study on effects of fluidic obstacle on flame acceleration and deflagration-to-detonation transition[C]//21st AIAA International Space Planes and Hypersonics Technologies Conference. Reston, VA:AIAA, 2017:2261.[21] SCHWER D A, KAILASANATH K. Effect of low pressure ratio on exhaust plumes of rotating detonation engines[C]//50th AIAA/ASME/SAE/ASEE Joint Propulsion Conference. Reston, VA:AIAA, 2014:3901.

E-mail：hkxb@buaa.edu.cn

关于我们

期刊社服务

专业学科

封面文章

友情链接

主管单位：中国科学技术协会主办单位：中国航空学会北京航空航天大学

横向射流影响缓燃向爆震转捩过程的试验研究

Experimental study of effects of fluidic obstacle parameters on deflagration-to-detonation transition

PDF (PC)

可视化

摘要/Abstract

引用本文

使用本文

参考文献

相关文章 4

编辑推荐

Metrics

本文评价

[1]	舒博文, 黄江涛, 高正红, 刘刚, 何成军, 夏露. 二元激波矢量喷管矢量性能敏感性分析[J]. 航空学报, 2023, 44(13): 127831-127831.
[2]	邓甜, 李佳周, 陈伟. 黏性液体横向射流破碎机理[J]. 航空学报, 2022, 43(3): 125130-125130.
[3]	邓甜, 李佳周, 陈伟. 剪切气流中无黏液体横向射流破碎机理[J]. 航空学报, 2021, 42(7): 124464-124464.
[4]	丁阳, 常海萍, 杜治能. 多排反向射流角气膜冷却特性研究[J]. 航空学报, 2013, 34(11): 2472-2481.