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Extinction limit extension of unsteady counterflow diffusion flames affected by velocity change

机译:速度变化影响非定常逆流扩散火焰的消光极限扩展

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The unsteady extinction limit of (CH_4 + N_2)/air diffusion flames was investigated in terms of the time history of the strain rate and initial strain rates. A spatially locked flame in an opposed-jet counterflow burner was perturbed using linear velocity variation, and time-dependent flame luminosity and unsteady extinction limits were measured with a high-speed intensified CCD (ICCD) camera. In addition, the transient maximum flame temperature and hydroxyl (OH) radical were measured as a function of time using Rayleigh scattering and OH laser-induced fluorescence, respectively. In this experiment, unsteady flames survive at strain rates that are much higher than the extinction limit of steady flames and unsteady extinction limits increase as the slope of the strain rate increases or as the initial strain rate decreases. We found that the equivalent strain rate represents well the unsteady behavior in the outer convective-diffusive layer of the flame. By using the equivalent strain rate, we were able to accurately estimate the contribution of the unsteady effect in the outer convective-diffusive layer to the extinction limit extension, and we also identified the unsteady effect in the inner diffusive-reactive layer of the flame. Consequently, the extension of unsteady extinction limits results from the unsteady effects of both the convective-diffusive layer and the diffusive-reactive layer. The former effect is dominant at the beginning of the velocity change, and the latter effect is dominant near the extinction limit.
机译:根据应变速率和初始应变速率的时间历程,研究了(CH_4 + N_2)/空气扩散火焰的非稳态熄灭极限。使用线性速度变化扰动对置射流逆流燃烧器中的空间锁定火焰,并使用高速增强CCD(ICCD)相机测量随时间变化的火焰光度和不稳定熄灭极限。此外,使用瑞利散射和OH激光诱导的荧光分别测量了瞬时最大火焰温度和羟基(OH)自由基随时间的变化。在该实验中,不稳定火焰以比稳定火焰的消光极限高得多的应变率生存,并且随着应变率的斜率增加或初始应变率降低,不稳定消光极限增加。我们发现当量应变率很好地表示了火焰在外部对流扩散层中的不稳定行为。通过使用等效应变率,我们能够准确地估计外部对流扩散层中的非稳态效应对消光极限扩展的贡献,并且还确定了火焰内部扩散反应层中的非稳态效应。因此,不稳定消光极限的扩展是由对流扩散层和扩散反应层两者的不稳定影响引起的。前者在速度变化开始时占主导地位,而后者在消光极限附近占主导地位。

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