恒定雷诺数和不同化学计量的湍流预混火焰分解火焰结构的测量

Armin Soika, Friedrich Dinkelacker, Alfred Leipertz
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引用次数: 87

摘要

为了识别不同的燃烧形式,在网格均匀湍流流场中研究了线稳定预混甲烷-空气火焰。利用平面瑞利散射技术对两个平行激光片进行了三维温度梯度检测。为了详细研究火焰的结构和拓扑结构,在保持湍流雷诺数Ret恒定在87或134的情况下,通过改变火焰的化学计量,从而改变Karlovitz数Ka,研究了湍流运动对不同进程变量c下局部温度梯度的影响。由于热梯度的统计分布近似高斯分布,50%的中位数和分布的宽度是表征火焰响应的合适度量。与层流无应变计算相比,特别是Karlovitz数(Ka=4.6)最高的极细火焰(<0.55)显示火焰厚度减少了约30%。这与预期的燃烧状态相反,但很适合层流应变计算。随后,详细研究了曲率对局部热梯度的影响。结果发现,负弯曲的尖峰(向反应物凹)表明火焰温度曲线变陡,而正弯曲的火焰元素可以通过整个反应过程的延迟来识别。在统计检验方面,考虑了不同反应过程变量c条件下的热梯度分布宽度,发现随着Ka的增加,传播减少与Ret和c无关。基于检测到的火焰的不同曲率半径和扰动频率,我们假设在我们的实验中火焰响应更多地取决于火焰曲率而不是Ka修饰引起的影响。
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Measurement of the resolved flame structure of turbulent premixed flames with constant reynolds number and varied stoichiometry

Wire-stabilized premixed methane-air flames have been studied in a grid-generated homogeneous turbulent flow field in order to identify different burning regimes. The planar Rayleigh scattering technique was used with two parallel laser light sheets, which allows the detection of three-dimensional temperature gradients. For a detailed investigation of the flame structure and topology, the modification of the local temperature gradients at different progress variables c due to the turbulent motion was studied by varying the flame stoichiometry and thereby the Karlovitz number Ka while keeping the turbulent Reynolds number Ret constant at 87 or 134. Because of a nearly Gaussian shaped statistical distribution of the thermal gradients, the 50% median and the width of the distribution are suitable measures used to characterize the flame response. Compared with laminar unstrained calculations, especially very lean flames (<0.55) marked with the highest Karlovitz number (Ka=4.6) revealed a reduction of the flame thickness of about 30%. This is in contrast to the expected burning regime but fits well with laminar strained calculations. Subsequently, detailed investigations were made to examine the influence of curvature on local thermal gradients. It was found that negatively curved cusps (concave toward the reactants) show a steepening of the flame-temperature profile, while positively curved flame elements can be identified by a retardation of the overall reaction process. In terms of a statistical examination, the widths of the thermal gradient distribution conditioned at different reaction progress variables c were regarded, finding a decrease of the spread with increasing Ka independent of Ret and c. Based on different curvature radii and perturbation frequencies of the detected flames, we assume that in our experiments the flame response depends more on flame curvature than on effects caused by modification of Ka.

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