Volume 47 Issue 8
Aug.  2018
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Wang Weidong, Wen Ming, Wang Diankai, Qing Zexu. Influence of key parameters on laser-induced hot core in air[J]. Infrared and Laser Engineering, 2018, 47(8): 806002-0806002(6). doi: 10.3788/IRLA201847.0806002
Citation: Wang Weidong, Wen Ming, Wang Diankai, Qing Zexu. Influence of key parameters on laser-induced hot core in air[J]. Infrared and Laser Engineering, 2018, 47(8): 806002-0806002(6). doi: 10.3788/IRLA201847.0806002

Influence of key parameters on laser-induced hot core in air

doi: 10.3788/IRLA201847.0806002
  • Received Date: 2018-03-07
  • Rev Recd Date: 2018-04-07
  • Publish Date: 2018-08-25
  • In order to understand the phenomenon of plasma hot core evolution in air deposited by nanosecond-pulsed laser energy, a high-resolution schlieren system was set up by using two cameras with different resolution. The experimental results obtained from schlieren system showed a good illustration of the initial moment of laser energy deposition, and then the law of the two key parameters of pulse energy and lens focal length on the evolution of laser-induced plasma hot core were studied. The experimental results show that the higher the energy of laser deposition, the larger the size of the plasma hot core, but there may be saturation of the laser energy deposition. In addition, the higher the laser energy and the shorter the focal length of lens, the later the external air penetrates the plasma core after laser energy deposition, which means the plasma core can maintain a steady state of high temperature and low density for a long time, and provides sufficient reaction time for the relevant research on plasma active flow control from the laser energy.
  • [1] Hong Junwu, Chen Xiaodong, Zhang Yulun, et al. The primary numerical research of active control technology in flow[J]. Acta Aerodynamica Sinica, 2005, 23(4):402-407. (in Chinese)洪俊武, 陈晓东, 张玉伦, 等. 主动流动控制技术的初步数值研究[J]. 空气动力学学报, 2005, 23(4):402-407.
    [2] Udagawa K, Kawaguchi K, Saito S, et al. Experimental study on supersonic flow control by MHD interaction[R]. 39th Plasmadynamics Lasers Conference, AIAA 2008-4222, 2008.
    [3] Shneider M N, Macheret S O, et al. Virtual shapes in supersonic flow control with energy addition[J]. Journal of Propulsion and Power, 2008, 24(5):900-915.
    [4] Michael Atkinson, Jonathan Poggie, Jose Camberos. Numerical investigation of oblique shock-wave/turbulent boundary-layer interaction control using plasma actuators[C]//49th AIAA Aerospace Sciences Meeting and Exhibit, AIAA 2011-3427, 2011.
    [5] Yan H, Gaitonde D. Control of edney IV interaction by energy pulse[C]//44th AIAA Aerospace Sciences Meeting and Exhibit, AIAA 2006-562, 2006.
    [6] Radziemski L J, Loree T R, Cremers D A, et al. Time-resolved laser-induced breakdown spectrometry of aerosols[J]. Analytical Chemistry, 1983, 55(8):1246-1252.
    [7] Hugo S, Mayo V, Rafael N, et al. Temporal evolution of the shock wave and hot core air in laser induced plasma[J]. Applied Physics Letters, 2000, 77(20):3158-3160.
    [8] Jebens D S, Lakkaraju H S, Mckay C P, et al. Time resolved simulation of lightning by lip[J]. Geophysical Research Letters, 1992, 19(3):273-276.
    [9] Erdem E, Zare-Behtash H, Kontis K, et al. Single pulse laser energy deposition in quiescent air and hypersonic flows[C]//18th AIAA/3AF International Space Planes and Hypersonic Systems and Technologies Conference, AIAA-2012-5870, 2012.
    [10] Qing Z X, Hong Y J, Wang D K, et al. Experimental and numerical study of nanosecond pulsed laser energy asymmetric deposition in quiescent air[J]. Journal of Propulsion Technology, 2017, 38(7):1661-1668.
    [11] Schlein E, Zheltovodov A A, Pimonov E A, et al. Study of the bow shock interaction with laser-pulse-heated air bubbles[C]//39th AIAA Fluid Dynamics Conference and Exhibit,AIAA 2009-3568, 2009.
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Influence of key parameters on laser-induced hot core in air

doi: 10.3788/IRLA201847.0806002
  • 1. State Key Laboratory of Laser Propulsion & Application,Space Engineering University,Beijing 101416,China

Abstract: In order to understand the phenomenon of plasma hot core evolution in air deposited by nanosecond-pulsed laser energy, a high-resolution schlieren system was set up by using two cameras with different resolution. The experimental results obtained from schlieren system showed a good illustration of the initial moment of laser energy deposition, and then the law of the two key parameters of pulse energy and lens focal length on the evolution of laser-induced plasma hot core were studied. The experimental results show that the higher the energy of laser deposition, the larger the size of the plasma hot core, but there may be saturation of the laser energy deposition. In addition, the higher the laser energy and the shorter the focal length of lens, the later the external air penetrates the plasma core after laser energy deposition, which means the plasma core can maintain a steady state of high temperature and low density for a long time, and provides sufficient reaction time for the relevant research on plasma active flow control from the laser energy.

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