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Spatial and Temporal Characteristics of OH in Turbulent Opposed-Jet Double Flames

机译:湍流对流双火焰中OH的时空特征

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摘要

Simultaneous high repetition-rate, two-point hydroxyl (OH) time-series measurements with associated PLIF/PIV measurements are employed to investigate spatio–temporal scales and flame-velocity interactions in turbulent opposed jets sustaining methane-air double flames. For a fuel-side equivalence ratio, ϕ B = 1.2, a rich premixed flame exists on the fuel side while a diffusion flame exists on the air side of the stagnation plane. The bulk Reynolds number (Re) and strain rate (SR) can be adjusted to generate flames at ϕ B = 1.2 with both well separated and completely merged flame fronts. Simultaneous PLIF/PIV measurements highlight distinct spatial OH structures of the premixed and diffusive fronts corresponding to variations in the flow field. The self-propagating tendency of the rich premixed front causes large-scale wrinkling, thereby enhancing the OH contour length by 15% as compared to the diffusive front. Two-point OH time-series measurements are implemented to quantify both spatial and temporal fluctuations via study of radial length and time scales. In general, these integral length and time scales follow similar trends and reach a minimum at the axial location of peak [OH]. In comparison to merged double flames having higher Re and SR, greater OH fluctuations are observed in the rich-premixed front as compared to the diffusive front for a well separated double flame. Because of the developing turbulence, the OH length scales exhibit reduced axial gradients across the reaction zone for higher Re in comparison to lower Re. A stochastic time-series simulation, using a state relationship based on a joint mixture fraction and progress variable, is utilized to extract estimated scalar time scales from those of measured OH. The simulations indicate that the hydroxyl fluctuations in double flames are only twice those of the underlying conserved scalar.
机译:同时进行高重复率,两点羟基(OH)时间序列测量和相关的PLIF / PIV测量,以研究维持甲烷-空气双火焰的相对湍流喷射中的时空尺度和火焰-速度相互作用。对于燃料侧当量比ϕ B = 1.2,在燃料侧存在浓的预混火焰,而在停滞平面的空气侧存在扩散火焰。可以调整整体雷诺数(Re)和应变率(SR),以在ϕ B = 1.2时产生火焰,且火焰前部相互独立且完全合并。同时进行PLIF / PIV测量可突出显示与流场变化相对应的预混和扩散前沿的不同空间OH结构。丰富的预混合前沿的自蔓延趋势导致大规模起皱,因此与扩散前沿相比,OH轮廓长度增加了15%。通过研究径向长度和时间尺度,实施了两点OH时间序列测量以量化空间和时间波动。通常,这些积分长度和时间尺度遵循相似的趋势,并且在峰值[OH]的轴向位置达到最小值。与具有较高的Re和SR的合并双火焰相比,与良好分离的双火焰的扩散前沿相比,在富预混合前沿中观察到更大的OH波动。由于湍流的发展,与较低的Re相比,对于较高的Re,OH长度标度在整个反应区上呈现出减小的轴向梯度。利用基于联合混合分数和进度变量的状态关系的随机时间序列模拟,从测量的OH的标量时间标度中提取估计的标量时间标度。模拟表明,双火焰中的羟基波动仅是基本保守标量的羟基波动的两倍。

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