轴对称层流扩散火焰中CH, CH*和OH*的实验与计算研究

K.T. Walsh, M.B. Long, M.A. Tanoff, M.D. Smooke
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引用次数: 144

摘要

在这项研究中,我们扩展了之前对轴对称层流扩散火焰的数值和实验相结合的研究结果,其中使用差分拉曼光谱,激光诱导荧光(LIF)和多维火焰模型来生成温度和主要和次要物种的分布。本文概述了测量基态CH (X2II)、激发态CH (A2δ,记为CH*)和激发态OH (A2Σ,记为OH*)的密度并建立模型的方法。CH*和OH*数密度从视距火焰发射测量反卷积。基态CH用线性LIF测量。计算采用GRI Mech 2.11和另一种烃类机理。在这两种情况下,从最近的动力学研究中增加了生成和消耗CH*和OH*的额外反应。碰撞猝灭和自发发射是激发态自由基去激发的主要原因。与我们之前的调查一样,GRI Mech 2.11继续与实验中观察到的总体火焰长度产生非常好的一致性,同时显着低于预测火焰起飞高度。交替动力学方案在预测起飞高度方面更为准确,但对总火焰长度的预测过高。在空间分布和CH自由基的绝对浓度(测量值为4ppm)方面,GRI Mech 2.11预测的基态CH剖面与相应的测量结果非常吻合。激发态种的计算结果与测量结果在空间分布和总体特征上基本一致。对于OH*,测量到的峰值摩尔分数1.3×10−8与计算得到的峰值相当,而对于CH*,测量到的峰值水平2×10−9,两种动力学方案都严重低估了,这表明与火焰中激发态物质相关的形成和破坏动力学需要进一步研究。
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Experimental and computational study of CH, CH*, and OH* in an axisymmetric laminar diffusion flame

In this study, we extend the results of previous combined numerical and experimental investigations of an axisymmetric laminar diffusion flame in which difference Raman spectroscopy, laser-induced fluorescence (LIF), and a multidimensional flame model were used to generate profiles of the temperature and major and minor species. A procedure is outlined by which the number densities of ground-state CH (X2II), excited-state CH (A2δ, denoted CH*), and excited-state OH (A2Σ, denoted OH*) are measured and modeled. CH* and OH* number densities are deconvoluted from line-of-sight flame-emission measurements. Ground-state CH is measured using linear LIF. The computations are done with GRI Mech 2.11 as wel as an alternate hydrocarbon mechanism. In both cases, additional reactions for the production and consumption of CH* and OH* are added from recent kinetic studies. Collisional quenching and spontaneous emission are responsible for the de-excitation of the excited-state radicals.

As with our previous investigations, GRI Mech 2.11 continues to produce very good agreement with the overall flame length observed in the experiments, while significantly under predicting the flame liftoff height. The alternate kinetic scheme is much more accurate in predicting lift-off height but overpredicts the overall flame length. Ground-state CH profiles predicted with GRI Mech 2.11 are in excellent agreement with the corresponding measurements, regarding both spatial distribution and absolute concentration (measured at 4 ppm) of the CH radical. Calculations of the excited-state species show reasonable agreement with the measurements as far as spatial distribution and overall characteristics are concerned. For OH*, the measured peak mole fraction, 1.3×10−8, compared well with computed peaks, while the measured peak level for CH*, 2×10−9, was severely underpredicted by both kinetic schemes, indicating that the formation and destruction kinetics associated with excited-state species in flames require further research.

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