贫预混扩散复合火焰在接近熄灭极限时的火焰结构

T. Kawanami, Y. Yahagi
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引用次数: 0

摘要

对逆流中形成的稀薄预混扩散复合火焰的熄灭和火焰结构进行了实验和数值研究。灭绝界限可分为两个区域。一种是扩散火焰优势消光区(DF- de),其消光极限下LPF侧等效比(φL)随DF侧燃料浓度的增加而线性减小(χU)。另一个是稀薄预混火焰优势消光区(LPF-DE),其中χU对消光φL的影响随χU的增大而增大。在这两个区域,火焰结构及其φL依赖性有很大差异。在DF- de中,温度分布与φL无关,温度峰位于DF附近。由于DF的温度比LPF高,所以LPF的热支撑比DF高。两个反应区之间的温度梯度随φL的增大而减小,而层流燃烧速度(SL)和燃烧气体宽度(WB)与φL无关。另一方面,在LPF- de中,温度分布不对称,温度峰向LPF侧倾斜。即与DF侧相比,LPF侧的温度梯度非常陡。由于LPF的温度比DF高,所以DF的热支撑比LPF高。无论φL大小,两个反应区之间的温度梯度都是恒定的,而SL和WB随φL的增大而增大。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Flame structure of lean premixed and diffusion combined flames near extinction limit
Extinction and flame structure of lean premixed and diffusion combined flames formed in a counter flow are investigated experimentally and numerically. The extinction limits can be divided into two regions. One is a diffusion flame dominant extinction region (DF-DE) in which equivalence ratio of LPF side (φL) at extinction limit is decreasing linearly with increasing fuel concentration of DF side (χU). The other is a lean premixed flame dominant extinction region (LPF-DE) in which effect of χU on extinction φL is increasing with increasing χU. In these two regions, the flame structures and its φL dependence are different greatly. In the DF-DE, the temperature has symmetrical profile regardless of φL and the temperature peak is located near DF. Since DF has higher temperature than LPF, LPF is thermally supported than DF. Temperature gradients between two reaction zones are decreasing with increasing φL, while laminar burning velocity (SL) and burnt gas width (WB) are constant regardless of φL. On the other hand, in the LPF-DE, the temperature has asymmetrical profile and the temperature peak leans to the LPF side. That is, the temperature gradient of LPF side is very steep compared with the DF side. Since LPF has higher temperature than DF, DF is thermally supported than LPF. Temperature gradients between two reaction zones are constant regardless of φL, while SL and WB are increasing with increasing φL.
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