Volume 46 Issue 12
Jan.  2018
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Article Navigation >  Infrared and Laser Engineering  > 2017  >  46(12): 1205001-1205001(6)

Li Xudong, Zhou Yiping, Yan Renpeng, Pan Hu, Chen Deying, Zhou Zhongxiang. Study on laser for applications in high-speed planar laser induced fluorescence[J]. Infrared and Laser Engineering, 2017, 46(12): 1205001-1205001(6). doi: 10.3788/IRLA201746.1205001
Citation: Li Xudong, Zhou Yiping, Yan Renpeng, Pan Hu, Chen Deying, Zhou Zhongxiang. Study on laser for applications in high-speed planar laser induced fluorescence[J]. Infrared and Laser Engineering, 2017, 46(12): 1205001-1205001(6). doi: 10.3788/IRLA201746.1205001
shu

Study on laser for applications in high-speed planar laser induced fluorescence

doi: 10.3788/IRLA201746.1205001
  • 1.

    Department of Physics,College of Science,Harbin Institute of Technology,Harbin 150001,China;

  • 2.

    National Key Laboratory of Science and Technology on Tunable Laser,Harbin Institute of Technology,Harbin 150080,China

  • Received Date: 2017-04-10
  • Rev Recd Date: 2017-05-20
  • Publish Date: 2017-12-25
  • Planar laser induced fluorescence (PLIF) is a significant method to study the characteristics of flow field and combustion, owing to the advantages of non-conduction, high spatial and temporal resolutions. In comparison with existing low-speed PLIF, high-speed PLIF has a lot of advantages. High-speed PLIF with repetition rate higher than 10 kHz is necessary to study turbulent and reacting flows in order to capture the dynamics that governs the underlying physics in the fields such as supersonic and hypersonic flows, combustion and plasma physics. The lack of laser sources with high repetition rate and high pulse energy significantly limits the development of high-speed PLIF. A comprehensive overview for the development and the latest achievements of high-speed PLIF and the employed laser sources was given in this article. The characteristics of different laser sources were compared, and the pulse-burst technique was believed to be a promising source for high-speed PLIF technique. The development of pulse-burst laser used as the laser source in high-speed PLIF was predicted.
  • [1] Su Tie, Chen Shuang, Yang Furong, et al. Investigation of temperature of transient combustion using two-line PLIF[J]. Infrared and Laser Engineering, 2014, 43(6):1750-1754. (in Chinese)苏铁, 陈爽, 杨富荣, 等. 双色平面激光诱导荧光瞬态燃烧场测温实验[J]. 红外与激光工程, 2014, 43(6):1750-1754.
    [2] Zhang Zhenrong, Wang Sheng, Li Guohua, et al. Exciting laser beam shaping in planar laser-induced fluorescence experiment[J]. Chinese Optics, 2013, 6(3):359-364. (in Chinese)张振荣, 王晟, 李国华, 等. 平面激光诱导荧光实验中激励激光的光束整形[J]. 中国光学, 2013, 6(3):359-364.
    [3] Wang Sheng, Zhang Zhenrong, Shao Jun, et al. Denoising of PLIF images for flow parameter measurement[J]. Optics and Precision Engineering, 2013, 21(7):1858-1864. (in Chinese)王晟, 张振荣, 邵珺, 等. 瞬态流场定量测量中平面激光诱导荧光图像的降噪[J]. 光学精密工程, 2013, 21(7):1858-1864.
    [4] Gao Jing, Yu Feng, Kuang Hongshen, et al. Generation of super continuum spectra from acousto-optic Q-switched nanosecond fiber lasers[J]. Optics and Precision Engineering, 2014, 22(5):1138-1142. (in Chinese)高静, 于峰, 匡鸿深, 等. 纳秒声光调Q光纤激光器产生超连续谱[J]. 光学精密工程, 2014, 22(5):1138-1142.
    [5] Wang Zijian, Jin Guangyong, Yu Yongji, et al. 2.1m optical parametric oscillator based on high-repetition Q-switch Nd:YVO4 laser[J]. Infrared and Laser Engineering, 2015, 44(9):2638-2642. (in Chinese)王子健, 金光勇, 于永吉,等. 高重频声光调Q Nd:YVO4激光器2.1m光参量振荡器[J]. 红外与激光工程, 2015, 44(9):2638-2642.
    [6] Pan Qikun. Progress of mid-infrared solid-state laser[J]. Chinese Optics, 2015, 8(4):557-566. (in Chinese)潘其坤. 中红外固体激光器研究进展[J]. 中国光学, 2015, 8(4):557-566.
    [7] Kaminski C, Hult J, Alden M. High repetition rate planar laser induced fluorescence of OH in a turbulent non-premixed flame[J]. Applied Physics B, 1999, 68(4):757-760.
    [8] Gashi S, Hult J, Jenkins K W, et al. Curbature and wrinkling of premixed flame kernels-comparisons of OH PLIF and DNS data[J]. Proceedings of the Combustion Institute, 2005, 30(1):809-817.
    [9] Miller J D, Engel S R, Troger J W, et al. Characterization of a CH planar laser-induced fluorescence imaging system using a kHz-rate multimode-pumped optical parametric oscillator[J]. Applied Optics, 2012, 51(14):2589-2599.
    [10] Paa W, Mller D, Stafast H, et al. Flame turbulences recorded at 1 kHz using planar laser induced fluorescence upon hot band excitation of OH radicals[J]. Applied Physics B, 2007, 86(1):1-5.
    [11] Hedman T, Cho K, Pfeil M, et al. High speed OH PLIF applied to multiphase combustion(Review)[J]. Combustion, Explosion, and Shock Waves, 2016, 52(1):1-13.
    [12] Boeck L, Mvel R, Fiala T, et al. High-speed OH-PLIF imaging of deflgration-to-detonation transition in H2-air mixtures[J]. Experiments in Fluids, 2016, 57(6):105.
    [13] Johchi A, Naka Y, Shimura M, et al. Investigati on on rapid consumption of fine scale unburned mixture islands in turbulent flame via 10 kHz simultaneous CH-OH PLIF and SPIV[J]. Proceedings of the Combustion Institute, 2015, 35(3):3663-3671.
    [14] Wu P, Lempert W R, Miles R B, et al. Megahertz pulse-burst laser and visualization of shock-wave/boundary-layer interaction[J]. Journal of AIAA, 2000, 38(4):672-679.
    [15] Jiang N, Webster M, Lempert W, et al. MHz-rate NO PLIF imaging in a Mach 10 hypersonic wind tunnel[J]. Applied Optics, 2010, 50(4):A20-28.
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    [18] Slipchenko M, Miller J, Roy S, et al. All-diode-pumped quasi-continuous burst-mode laser for extended high-speed planar imaging[J]. Optics Express, 2013, 21(1):681-689.
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Study on laser for applications in high-speed planar laser induced fluorescence

doi: 10.3788/IRLA201746.1205001
  • 1. Department of Physics,College of Science,Harbin Institute of Technology,Harbin 150001,China;
  • 2. National Key Laboratory of Science and Technology on Tunable Laser,Harbin Institute of Technology,Harbin 150080,China
  • Received Date: 2017-04-10
  • Rev Recd Date: 2017-05-20
  • Publish Date: 2017-12-25

Abstract: Planar laser induced fluorescence (PLIF) is a significant method to study the characteristics of flow field and combustion, owing to the advantages of non-conduction, high spatial and temporal resolutions. In comparison with existing low-speed PLIF, high-speed PLIF has a lot of advantages. High-speed PLIF with repetition rate higher than 10 kHz is necessary to study turbulent and reacting flows in order to capture the dynamics that governs the underlying physics in the fields such as supersonic and hypersonic flows, combustion and plasma physics. The lack of laser sources with high repetition rate and high pulse energy significantly limits the development of high-speed PLIF. A comprehensive overview for the development and the latest achievements of high-speed PLIF and the employed laser sources was given in this article. The characteristics of different laser sources were compared, and the pulse-burst technique was believed to be a promising source for high-speed PLIF technique. The development of pulse-burst laser used as the laser source in high-speed PLIF was predicted.

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