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Premixed turbulent flame front structureinvestigation by Rayleigh scattering in the thinreaction zone regime

机译:稀反应区状态下瑞利散射对预混湍流火焰前部结构的研究

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Premixed turbulent flames of methane–air and propane–air stabilized on a bunsen type burner werestudied using planar Rayleigh scattering and particle image velocimetry. The fuel–air equivalence ratiorange was from lean 0.6 to stoichiometric for methane flames, and from 0.7 to stoichiometric for propaneflames. The non-dimensional turbulence rms velocity, u'/SL, covered a range from 3 to 24, correspondingto conditions of corrugated flamelets and thin reaction zones regimes. Flame front thickness increasedslightly with increasing non-dimensional turbulence rms velocity in both methane and propane flames,although the flame thickening was more prominent in propane flames. The probability density functionof curvature showed a Gaussian-like distribution at all turbulence intensities in both methane and propaneflames, at all sections of the flame.The value of the term Dk, the product of molecular diffusivity evaluated at reaction zone conditions andthe flame front curvature, has been shown to be smaller than the magnitude of the laminar burning velocity.This finding questions the validity of extending the level set formulation, developed for corrugatedflames region, into the thin reaction zone regime by increasing the local flame propagation by addingthe term Dk to laminar burning velocity.
机译:在本生型燃烧器上稳定的甲烷-空气和丙烷-空气的预混湍流是 使用平面瑞利散射和粒子图像测速技术进行了研究。燃油-空气当量比 甲烷火焰的范围从稀薄的0.6到化学计量的,丙烷的范围从0.7到化学计量的 火焰。无量纲湍流均方根速度u'/ SL覆盖3至24的范围,对应 应对波纹状小火焰和薄反应区的要求。火焰前壁厚度增加 在甲烷和丙烷火焰中,随着无量纲湍流均方根速度的增加而略有增加, 尽管在丙烷火焰中火焰增厚更为明显。概率密度函数 的曲率在甲烷和丙烷的所有湍流强度下均呈高斯状分布 火焰,在火焰的所有部分。 术语Dk的值,是在反应区条件下评估的分子扩散率的乘积, 已经证明火焰前曲率小于层状燃烧速度的大小。 这一发现对扩展针对瓦楞纸的水平设定配方的有效性提出质疑 火焰区域,通过增加局部火焰传播而进入稀薄的反应区状态 术语Dk为层流燃烧速度。

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