首页> 外文会议>Proceedings of the Combustion Institute >TIME-RESOLVED LASER-INDUCED INCANDESCENCE FOR SOOT PARTICLE SIZING DURING ACETYLENE PYROLYSIS REHIND SHOCK WAVES
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TIME-RESOLVED LASER-INDUCED INCANDESCENCE FOR SOOT PARTICLE SIZING DURING ACETYLENE PYROLYSIS REHIND SHOCK WAVES

机译:乙炔热解后重击波中烟尘颗粒尺寸的时间分辨激光致死

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Time-resolved laser-induced incandescence (LII) and continuous wave (CW) laser extinction were applied for the sizing of soot particles originated from acetylene pyrolysis behind reflected shock waves. The LII technique is based on a fast heating of particles by a short laser pulse and on the time-resolved observation of the particle thermal emission. The time history of this emission is a measure for the particle cooling, which provides information about the particle size. Additionally, the soot formation was measured by a cw-laser-extinction technique, which provides information about induction times and total soot concentration. Three groups of experiments with mixtures of 5% C_2H_2 diluted in Ar at average temperatures of around 1840 K, 1900 K, and 2020 K at pressures of about 2.8 bar were performed. For the individual experiments within each group, the delay time between shock-induced heating of the C_2H_2/Ar mixture and the LII laser pulse was varied between 200μs and 1000μs in steps of 100μs. The analysis of the LII data results in particle mean radii between 1.8 nm and 10 nm of a log-normal size distribution. Higher temperatures and longer reaction times yield bigger particles. In combination with the extinction data, the soot yield was found to be between 5% and 16% at the maximum reaction time of 1000μs. The induction times for the soot-particle formation were found to be within the range of previous studies.
机译:时间分辨激光诱导的白炽(LII)和连续波(CW)激光消光施加用于源自反射冲击波的乙炔热解的烟灰颗粒的尺寸。 LII技术基于短的激光脉冲的颗粒的快速加热,并在颗粒热排放的时间分辨观察中。该发射的时间历史是颗粒冷却的措施,其提供有关粒径的信息。另外,通过CW激光 - 消光技术测量烟灰形成,其提供有关诱导时间和总烟灰浓度的信息。在约2.8巴的压力下,在约1840k,1900k和2020k的平均温度下,在AR中稀释的三组实验。在约2.8巴的压力下,在AR中稀释的5%C_2H_2。对于每组内的个体实验,C_2H_2 / AR混合物的冲击诱导的加热与LII激光脉冲之间的延迟时间在100μs的步骤之间变化。 LII数据的分析导致粒子平均半径在1.8nm和10nm之间的逻辑正常尺寸分布之间。较高的温度和更长的反应时间产生更大的颗粒。结合消光数据,发现烟灰产量在最大反应时间为1000μs的5%和16%之间。发现烟灰粒子形成的诱导时间在先前的研究范围内。

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