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Flame Surface Fractal Characteristics in Premixed Turbulent Combustion at High Turbulence Intensities

机译:高湍流强度下预混湍流燃烧的火焰表面分形特征

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Because of the geometrical nature of the wrinkling of the flame surfaces in premixed turbulent combustion, the fractal approach is considered to be one of the most appropriate in power-law subgrid-scale models that are widely used in large eddy simulations. However, the available experimental data in literature on fractal characteristics of the premixed turbulent flame surfaces shows significant discrepancies among data sets, and the several different fractal algorithms used for evaluation may not produce consistent results. In this work, we analyzed premixed turbulent flame front images from an extensive experimental study using three different fractal algorithms and determined the fractal parameters: namely, fractal dimension D, inner cutoff ε_i, and outer cutoff ε_0. These images were obtained using laser-induced fluorescence of OH and Mie scattering on two Bunsen-type burners with diameters of 11.2 and 22.4 mm, with flames of propane-air with equivalence ratios of 0.8 and 1. Nondimensional turbulence intensity u'/S_L (ratio of fluctuating velocity to laminar flame velocity) was from 0.9 to 15, and the Reynolds number, based on the integral length scale, was from 40 to 467. The flame front surface areas were calculated for each set of results and compared with experimental turbulent burning velocities. The three fractal algorithms used for analysis in this work gave significantly different results for the same flame image sets. Further, nondimensional turbulent burning rates computed from the fractal parameters did not agree with the experimental turbulent burning data, except for those fractal results obtained by the box-counting method and only for u'/S_L ≤ 6. Implications of these results for flamelet models are discussed. In addition, the perimeter-ratio approach recently adopted to estimate the wrinkled flame surface area is discussed, and it is argued that the results obtained by the perimeter-ratio approach might not be unique.
机译:由于预混合湍流燃烧中火焰表面起皱的几何性质,分形方法被认为是在大型涡模拟中广泛使用的幂律次网格规模模型中最合适的方法之一。但是,文献中有关预混湍流火焰表面分形特征的可用实验数据显示数据集之间存在显着差异,并且用于评估的几种不同分形算法可能无法产生一致的结果。在这项工作中,我们使用三种不同的分形算法对来自广泛实验研究的预混湍流火焰前像进行了分析,并确定了分形参数:分形维数D,内部截止度ε_i和外部截止度ε_0。这些图像是使用激光诱导的OH荧光和Mie散射在两个直径为11.2和22.4 mm的丙烷气燃烧器上以当量比为0.8和1的丙烷空气火焰获得的。无量纲湍流强度u'/ S_L(脉动速度与层流火焰速度之比)为0.9至15,雷诺数(基于积分长度尺度)为40至467。计算每组结果的火焰前表面积并将其与实验湍流进行比较燃烧的速度。对于相同的火焰图像集,在这项工作中用于分析的三种分形算法给出了明显不同的结果。此外,由分形参数计算出的无量纲湍流燃烧速率与实验湍流燃烧数据不一致,除了那些通过盒数法获得的分形结果并且仅对于u'/ S_L≤6而言。讨论。此外,讨论了最近采用的估计火焰起皱表面积的周长比方法,并认为通过周长比方法获得的结果可能不是唯一的。

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