使用CH-LIF/瑞利激光同步技术研究薄反应区的标量混合

Mohy S. Mansour , Norbert Peters , Yung-Cheng Chen
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引用次数: 94

摘要

在高度拉伸的湍流预混甲烷-空气火焰中同时进行了二维CH-LIF/Rayleigh测量。这些火焰属于薄反应区。在这种状态下,Kolmogorov尺度小于层流火焰的预热区厚度,但大于反应区厚度。因此,小涡流可以进入预热区,但不能进入反应区。这些小涡流通过湍流混合扩大了预热区。在卡洛维茨数Ka为23和91的火焰中,观察到薄的反应区和相对厚的湍流预热区。预计预热区的厚度与混合长度尺度lm成比例,混合长度尺度lm是惯性范围内涡流的厚度,其周转时间等于火焰时间。在不同的轴向位置呈现温度/CH图像以及通过反应区的线形图,以说明不同的结构。此外,还给出了温度条件下的概率密度函数(pdf)。目前的数据表明,在高拉伸火焰的早期位置,薄反应区区域的温度相对较低。这归因于燃烧器的热损失。此外,在该区域边缘高度伸展的火焰中,有时会观察到局部熄灭,这可能是由于小涡流被卷入反应区。
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Investigation of scalar mixing in the thin reaction zones regime using a simultaneous CH-LIF/Rayleigh laser technique

Simultaneous two-dimensional CH-LIF/Rayleigh measurements were carried out in highly stretched turbulent premixed stoichiometric methane-air flames. These flames fall into the thin reaction zones regime. In this regime, the Kolmogorov scale is smaller than the preheat zone thickness of a laminar flame, but it is larger than the reaction zone thickness. Therefore, small eddies can penetrate into the preheat zone but not into the reaction zone. These small eddies widen the preheat zone by turbulent mixing.

In the present flames at Karlovitz numbers Ka of 23 and 91, thin reaction zones with relatively thick turbulent preheat zones are being observed. The thickness of the preheat zone is expected to scale with the mixing length scale lm, which is the thickness of an eddy within the inertial range that has a turnover time equal to the flame time.

The temperature/CH images are presented at different axial locations together with line profiles through the reaction zone to illustrate the different structures. In addition probability density functions (PDFs), of temperature conditioned on CH are presented.

The present data show that the temperature in the thin reaction zones' regime at the early positions in the highly stretched flames is relatively low. This is attributed to heat loss to the burner. In addition, in highly stretched flames at the borderline of this regime, local extinction has sometimes been observed, which could be due to entrainment of small eddies into the reaction zone.

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