火焰曲率和优先扩散对扩散火焰瞬态局部熄灭和重燃行为的影响

Kenji Yoshida, Toshimi Takagi
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引用次数: 33

摘要

对撞击微射流对瞬时H2/ n2 -空气逆流扩散火焰的不稳定应变进行了实验和数值研究。利用激光瑞利散射法进行了二维温度测量,并进行了考虑详细化学动力学的数值计算,注意了与非定常、火焰曲率和优先扩散效应有关的瞬态局部消光和区域。结果表明:(1)微射流撞击处存在瞬态局部火焰熄灭现象。然而,瞬态火焰可以在相当高的拉伸速率下瞬间存活,而稳定火焰则不可能存在。(2)由于微气流撞击引起的局部消光后出现重燃现象。重燃后的温度明显高于原火焰的温度。这种高温是由相对于凹曲率的优先扩散引起的H2物质浓度引起的。实验结果很好地证实了预测的局部瞬态消光和重燃行为。(3)可燃预混气体混合物的形成及其火焰的传播引起重燃。(4)微射流撞击消光后几乎看不到重燃现象。这是由于相对于凸曲率的优先扩散引起H2的稀释。(5)火焰的最高温度不能用拉伸率来解释,而是根据不稳定性和与优先扩散有关的火焰曲率而变化很大。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Transient local extinction and reignition behavior of diffusion flames affected by flame curvature and preferential diffusion

Experimental and numerical studies are made of transient H2/N2-air counterflow diffusion flames unsteadily strained by an impinging micro jet. Two-dimensional temperature measurements by the laser Rayleigh scattering method and numerical computations taking into account detailed chemical kinetics are conducted, paying attention to transient local extinction and reginition in relation to the unsteadiness, flame curvature, and preferential diffusion effects. The results are as follows: (1) Transient local flame extinction is observed where the micro jet impinges. However, the transient flame can survive instantaneously in squite of quite high stretch rate where the steady flame cannot exist. (2) Reignition is observed after the local extinction due to the micro air jet impingement. the temperature after reignition becomes significantly higher than that of the original flame. This high temperature is induced by the concentration of H2 species due to the preferential diffusion in relation to the concave curvature. The predicted behaviors of the local transient extinction and reignition are well confirmed by the experiments. (3) The reignition is induced after the formation of combustible premixed gas mixture and the consequent flame propagation. (4) The reignition is hardly observed after the extinction by micro fuel jet impingement. This is due to the dilution of H2 species induced by the preferential diffusion in relation to the convex curvature. (5) The maximum flame temperature cannot be rationalized by the stretch rate but changes widely, depending on the unsteadiness and the flame curvature in relation with preferential diffusion.

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