爆轰驱动膨胀管性能研究
收稿日期: 2015-04-03
修回日期: 2015-05-08
网络出版日期: 2015-05-14
基金资助
国家自然科学基金(90916028,11402275)
Performance study of a detonation-driven expansion tube
Received date: 2015-04-03
Revised date: 2015-05-08
Online published: 2015-05-14
Supported by
National Natural Science Foundation of China(90916028, 11402275)
超高速流动一般指速度超过5 km/s的流动,由于流动具有高焓高速的特点,模拟超高速流动的地面试验设备面临极大挑战。膨胀管(风洞)是少数几种具备超高速流动模拟能力的地面试验设备之一。中国科学院力学研究所高温气体动力学国家重点实验室(LHD)通过将正向爆轰驱动技术和膨胀管结合在一起,建成了可实现最高速度10 km/s超高速试验气流的爆轰驱动膨胀管(JF-16),并开展了典型模型试验。在此基础上对JF-16进行了改造升级工作,为其设计喷管增加了膨胀风洞运行模式,对其性能进行了相关试验测试研究。同时,对膨胀管相关数值方法进行了介绍,并开展数值模拟对试验状态进行辅助诊断和分析。
周凯 , 汪球 , 胡宗民 , 姜宗林 . 爆轰驱动膨胀管性能研究[J]. 航空学报, 2016 , 37(3) : 810 -816 . DOI: 10.7527/S1000-6893.2015.0128
Hypervelocity(above 5 km/s) test flow is the essential test environment to study reentry physics of space vehicles or capsules. To the date, an expansion tube is one of the few qualified test facilities on the ground. A detonation-driven expansion tube(JF-16) has been built at the State Key Laboratory of High-temperature Gas Dynamics in order to generate relatively steady and clean test flow at high enthalpies. A series of typical model tests has been completed in recent years. Test flow at velocities above 10 km/s has been successfully obtained via JF-16 after upgrade. An expansion tunnel nozzle has been designed for the JF-16 facility. Generally, the test time duration of a shock-expansion tube is extremely shorter as compared to a reflected-shock tunnel of the same scale which results in difficulties in the flow measurement and diagnostics. Numerical simulation is a powerful assistant analysis tool for the study of hypervelocity test flow. Calibration tests as well as numerical simulation are conducted to evaluate the performance of the upgraded test facility.
[1] NEELY A J, MORGAN R G. The superorbital expansion tube concept, experiment and analysis[J]. Aeronautical Journal, 1994, 98(973):97-105.
[2] SCHMISSEUR J, KNIGHT D, LONGO J, et al. Assessment of aerothermodynamic flight prediction tools through ground and flight experimentation:RTO-TR-AVT-136[R]. 2011.
[3] TRIMPI R L. A preliminary theoretical study of the expansion tube, a new device for producing high-enthalpy short-duration hypersonic gas flows:Tech Rep R-133[R]. Washington, D.C.:NASA, 1962.
[4] HOLDEN M S, WADHAMS T P, CANDLER G V. A review of experimental studies in the LENS shock tunnel and expansion tunnel to examine real-gas effects in hypervelocity flows:AIAA-2004-0916[R]. Reston:AIAA,2004.
[5] MACLEAN M, WADHAMS T, HOLDEN M. Integration of CFD and experiments in the CUBRC LENS shock tunnel facilities to understand the physics of hypersonic and hypervelocity flows[C]//4th Symposium on Integrating CFD and Experiments in Aerodynamics. Belgium:Von Karman Institute, 2009:14-16.
[6] JOHN I E, ROBERT J B, ANTHONY C, et al. Dual mode shock-expansion/reflected-shock tunnel:AIAA-1997-0560[R]. Reston:AIAA, 1997.
[7] MACLEAN M, WADHAMS T, HOLDEN M, et al. Numerical and experiment characterization of high enthalpy flow in an expansion tunnel facility:AIAA-2010-1562[R].Reston:AIAA, 2010.
[8] BEN-YAKAR A, HANSON R K. Characterization of expansion tube flows for hypervelocity combustion studies[J]. Journal of Propulsion and Power, 2002, 18(4):943-952.
[9] 高云亮. 超高速流动实验模拟方法及基础气动问题研究[D]. 北京:中国科学院力学研究所, 2008. GAO Y L. Study on hypervelocity flow generation techniques and essential hypersonic phenomena[D]. Beijing:Institute of Mechanics, Chinese Academy of Sciences, 2008(in Chinese).
[10] JIANG Z L, GAO Y L, ZHAO W. Performance study on detonation-driven expansion tube[C]//16th AIAA/DLR/DGLR International Space Planes and Hypersonic Systems and Technologies Conference. Reston:AIAA, 2009.
[11] JIANG Z L, WU B, GAO Y L, et al. Developing the detonation-driven expansion tube for orbital speed experiments[J]. Science China Technological Sciences, 2015, 58(4):695-700.
[12] 武博. 强激波现象与超高速流动实验技术研究[D]. 北京:中国科学院力学研究所, 2012. WU B. Study on the interaction of strong shock wave and the hypervelocity experimental method[D]. Beijing:Institute of Mechanics, Chinese Academy of Sciences, 2012(in Chinese).
[13] HU Z M, WU B, JIANG Z L. Analysis of the test condition of a shock-expansion tube JF-16[C]//The 1st International Symposium on High-temperature Gas Dynamics, 2012:10-13.
[14] HU Z M, WANG C, JIANG Z L, et al. Thermo-chemical nonequlibrium phenomena of the strong shock wave to generate hypersonic test flow[C]//The 5th International Symposium on Physics of Fluids, 2013:15-17.
[15] GRAHAM V C, PRAMOD K S, JOSEPH M B. Advances in computational fluid dynamics methods for hypersonic flows[J]. Journal of Spacecraft and Rockets, 2015, 52(1):17-28.
[16] YU H R. Oxyhydrogen combustion and detonation driven shock tube[J]. Acta Mechanica Sinaca, 1999, 15(2):97-107.
[17] 俞鸿儒, 李斌, 陈宏. 激波管氢氧爆轰驱动技术的发展进程[J]. 力学进展, 2005, 35(3):315-322. YU H R, LI B, CHEN H. The development of gaseous detonation driving technologies for a shock tune[J]. Advances in Mechanics, 2005, 35(3):315-322(in Chinese).
[18] JIANG Z L, ZHAO W, WANG C. Forward-running detonation drivers for high-enthalpy shock tunnels[J]. AIAA Journal, 2002, 40(10):2009-2016.
[19] JIANG Z L, TAKAYAMA K, CHEN Y S. Dispersion conditions for non-oscillatory shock-capturing schemes and its applications[J]. Computational Fluid Dynamics Journal, 1995, 4(2):137-150.
[20] HU Z M, JIANG Z L. Wave dynamic process in cellular detonation reflection from wedges[J]. Acta Mechanica Sinaca, 2007, 23(1):33-41.
[21] MACLEAN M, DUFRENE A, HOLDEN M. Spherical capsule heating in high enthalpy carbon dioxide in LENS-XX expansion tunnel:AIAA-2013-0906[R]. Reston:AIAA,2013.
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