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基于500 Hz OH-PLIF技术的超声速燃烧室火焰结构

叶家伟 张顺平 于欣

叶家伟, 张顺平, 于欣. 基于500 Hz OH-PLIF技术的超声速燃烧室火焰结构[J]. 航空动力学报, 2020, 35(12): 2593-2601. doi: 10.13224/j.cnki.jasp.2020.12.013
引用本文: 叶家伟, 张顺平, 于欣. 基于500 Hz OH-PLIF技术的超声速燃烧室火焰结构[J]. 航空动力学报, 2020, 35(12): 2593-2601. doi: 10.13224/j.cnki.jasp.2020.12.013
YE Jiawei, ZHANG Shunping, YU Xin. Flame structure in supersonic combustion chamber based on 500 Hz OH-PLIF technology,[J]. Journal of Aerospace Power, 2020, 35(12): 2593-2601. doi: 10.13224/j.cnki.jasp.2020.12.013
Citation: YE Jiawei, ZHANG Shunping, YU Xin. Flame structure in supersonic combustion chamber based on 500 Hz OH-PLIF technology,[J]. Journal of Aerospace Power, 2020, 35(12): 2593-2601. doi: 10.13224/j.cnki.jasp.2020.12.013

基于500 Hz OH-PLIF技术的超声速燃烧室火焰结构

doi: 10.13224/j.cnki.jasp.2020.12.013
基金项目: 国家自然科学基金青年科学基金(11904396)

Flame structure in supersonic combustion chamber based on 500 Hz OH-PLIF technology,

  • 摘要: 针对超声速燃烧室火焰驻留时间短和高湍流度的特点,利用500 Hz高频OH-PLIF(planar laser induced fluorescence)技术,研究了氢燃料超声速燃烧室火焰结构,结合壁面压力,获得了点火、稳焰以及熄火过程的规律。结果表明:隔离段入口来流马赫数为2的情况下,氢气当量比0.1和0.3,在火花塞点火下,2 ms均能点燃并获得PLIF火焰图像,其中当量比为0.1凹槽内存在爆燃现象,火焰达到稳定燃烧状态较慢(约65 ms)。稳焰过程中,当量比为0.3燃烧相对不充分,燃烧区域更靠近下壁面,燃烧位置和火核位置变化较大。当量比为0.1和0.3,熄火时间均在6 ms内,其中当量比为0.1熄火时火焰是从凹腔中部传播到凹腔前缘位置熄灭并伴随有一个短暂火焰增强的过程,并且在传播至凹腔前缘时已接近熄灭,当量比为0.3在熄灭前则是慢慢变弱,最终在凹腔前缘至喷氢位置间熄灭。

     

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出版历程
  • 收稿日期:  2020-04-25
  • 刊出日期:  2020-12-28

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