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首页> 外文期刊>The Journal of Chemical Physics >ABSOLUTE HCO CONCENTRATION MEASUREMENTS IN METHANE/AIR FLAME USING INTRACAVITY LASER SPECTROSCOPY
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ABSOLUTE HCO CONCENTRATION MEASUREMENTS IN METHANE/AIR FLAME USING INTRACAVITY LASER SPECTROSCOPY

机译:用吸入激光光谱法对甲烷/火焰中的HCO进行绝对测量

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摘要

Intracavity laser absorption spectroscopy was used to measure the absorption spectra of a premixed, flat methane/air flame at a total pressure of 30 Torr. The spectra were measured in the spectral range of 16 000-16 300 cm(-1). A flat flame burner was placed inside the cavity of a broadband dye laser pumped by a cw argon-ion laser. The spectrum of the laser output was measured by a high resolution spectrograph (with a spectral resolution of 0.003 nm). The spectrum of HCO radicals ((A) over tilde (2)A''<--(X) over tilde(2)A' transition) was measured with a high signal-to-noise ratio at different positions above the burner, providing the first quantitative measurement of the absolute concentrations of the HCO radical in flames. The linewidths of the individual rotational lines in the spectrum can be closely fitted by the equation Gamma=X+ZN(2)(N+1)(2), where X=0.37+/-0.03 cm(-1) and Z=(8 +/-0.5) 10(-6). The rotational temperature of the HCO radicals was evaluated from the spectra, but the error and the data scatter are relatively high since the lines with a high rotational quantum number N are strongly superimposed with Lines from different branches. The ''hot band,'' which can be assigned to the transition (0,0,1)-(0,9,1), was observed in spectra measured at high temperature. The value nu(3)''=1859 cm(-1) is evaluated from the position of this ''hot band.'' The concentration profile of the HCO radical has a maximum value of about 1.2x10(13) molecules/cm(3) which is in reasonable agreement with computer simulation results, when the uncertainties of the absorption cross section and of the rate constants for HCO reactions an taken into account. The relatively strong lines of the CH2 radical spectrum (the (b) over tilde(1)B(1)<--(a) over tilde(1)A(1) transition) were also recorded in the studied wavelength range. The spectra of these two radicals can be measured simultaneously which is advantageous in combustion diagnostics. (C) 1997 American Institute of Physics. [References: 50]
机译:腔内激光吸收光谱法用于在30 Torr的总压力下测量预混合的扁平甲烷/空气火焰的吸收光谱。在16 000-16 300 cm(-1)的光谱范围内测量光谱。将平焰燃烧器放置在由连续氩离子激光器泵浦的宽带染料激光器的腔体内。激光输出的光谱通过高分辨率光谱仪(光谱分辨率为0.003nm)测量。在燃烧器上方的不同位置以高信噪比测量HCO自由基的光谱((A)超过波浪线((2)A''<-(X)超过波浪线(2)A')。提供火焰中HCO自由基绝对浓度的首次定量测量。光谱中各个旋转线的线宽可以通过方程Gamma = X + ZN(2)(N + 1)(2)来拟合,其中X = 0.37 +/- 0.03 cm(-1)和Z = (8 +/- 0.5)10(-6)。从光谱评估了HCO自由基的旋转温度,但是由于具有高旋转量子数N的线与来自不同分支的线强烈叠加,因此误差和数据散布相对较高。在高温下测得的光谱中观察到了可分配给跃迁(0,0,1)-(0,9,1)的``热带''。值nu(3)''= 1859 cm(-1)是从该“热带”的位置评估的。HCO自由基的浓度曲线的最大值约为1.2x10(13)分子/ cm (3)在考虑吸收截面和HCO反应速率常数的不确定性的情况下,与计算机模拟结果合理吻合。在研究的波长范围内,还记录了CH2自由基光谱的相对较强的线(在tilde(1)B(1)<-(a)在tilde(1)A(1)过渡上的(b))。这两个自由基的光谱可以同时测量,这在燃烧诊断中是有利的。 (C)1997美国物理研究所。 [参考:50]

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