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Two-color, two-photon laser-induced polarization spectroscopy (LIPS) measurements of atomic hydrogen in near-adiabatic, atmospheric pressure hydrogen/air flames

机译:接近绝热的大气压氢气/空气火焰中原子氢的双色,两光子激光诱导偏振光谱(LIPS)测量

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Two-color, two-photon laser-induced polarization spectroscopy (LIPS) of atomic hydrogen has been demonstrated and applied in atmospheric pressure hydrogen/air flames. Fundamental and frequency-doubled beams from a single 486-nm dye laser were used in the experiments. The 243-nm pump beam in the measurements was tuned to the two-photon n = 1 → n = 2 resonance of the hydrogen atom. The 486-nm probe beam was tuned to the single-photon n = 2 → n = 4 resonance of the hydrogen atom. Measurements were performed in an atmospheric pressure H_2/air flame stabilized on a near-adiabatic, flat-flame calibration burner (the Hencken burner). For the range of pump beam intensities used, the LIPS signal was found to be nearly proportional to the square of the pump beam intensity over a wide range of flame equivalence ratios. Spectral lineshapes were recorded at flame equivalence ratios ranging from 0.85 to 2.10. Vertical H-atom number density distribution profiles were measured in the Hencken burner. The vertical H-atom number density profiles measured along the burner centerline for various flame equivalence ratios were compared with the results of a numerical flame calculation using the UNICORN (Unsteady Ignition and Combustion with Reactions) code. Good agreement between theory and experiment was obtained for stoichiometric and rich flame conditions. For flames with equivalence ratios greater than 1.5, the H-atom concentration was substantially above the adiabatic equilibrium value, even at 50 mm above the burner surface. The slow approach to the adiabatic equilibrium H-atom concentration value can be explained by assuming partial equilibrium in the postflame gases; the H-atom concentration is proportional to the O_2 concentration which requires significant residence time to decrease to its very low equilibrium concentration. These results suggest that the use of the Hencken burner as a radical measurement technique calibration source may be of questionable value for equivalence ratios greater than 1.5 and less than 0.8.
机译:原子氢的两色,两光子激光诱导的偏振光谱(LIPS)已被证明并应用于常压氢/空气火焰中。实验中使用了来自单个486 nm染料激光器的基本光束和倍频光束。测量中的243 nm抽运光束被调谐到氢原子的双光子n = 1→n = 2共振。将486 nm探测光束调谐到氢原子的单光子n = 2→n = 4共振。在接近绝热的平焰标定燃烧器(Hencken燃烧器)上稳定的大气压H_2 /空气火焰中进行测量。对于所使用的泵浦光束强度范围,发现LIPS信号在很宽的火焰当量比范围内几乎与泵浦光束强度的平方成正比。在火焰当量比为0.85至2.10范围内记录光谱线形。在Hencken燃烧器中测量垂直H原子数密度分布曲线。将沿燃烧器中心线测量的各种火焰当量比的垂直H原子数密度分布图与使用UNICORN(非稳态点火和反应燃烧)代码的火焰数值计算结果进行了比较。对于化学计量和浓火焰条件,理论与实验之间取得了良好的一致性。对于当量比大于1.5的火焰,即使在燃烧器表面上方50 mm处,H原子浓度也基本上高于绝热平衡值。假设绝热后气体中存在部分平衡,可以解释达到绝热平衡H原子浓度值的缓慢方法。 H原子浓度与O_2浓度成正比,这需要大量的停留时间才能降低到非常低的平衡浓度。这些结果表明,对于大于1.5且小于0.8的当量比,使用Hencken燃烧器作为自由基测量技术的校准源可能具有可疑的价值。

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