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Conical quarl swirl stabilized non-premixed flames: flame and flow field interaction

机译:锥形夸脱旋流稳定的非预混火焰:火焰与流场相互作用

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摘要

The flame-flow field interaction is studied in non-premixed methane swirl flames stabilized in quartz quarl via simultaneous measurements of the flow field using a stereo PIV and OH-PLIF at 5 KHz repetition rate. Under the same swirl intensity, two flames with different fuel jet velocity were investigated. The time-averaged flow field shows a unique flow pattern at the quarl exit, where two recirculation vortices are formed; a strong recirculation zone formed far from the quarl exit and a larger recirculation zone extending inside the quarl. However, the instantaneous images show that, the flow pattern near the quarl exit plays a vital role in the spatial location and structure of the reaction zone. In the low fuel jet velocity flame, a pair of vortical structures, located precisely at the corners of the quarl exit, cause the flame to roll up into the central region of low speed flow, where the flame sheet then tracks the axial velocity fluctuations. The vorticity field reveals a vortical structure surrounding the reaction zones, which reside on a layer of low compressive strain adjacent to that vortical structure. In the high fuel jet velocity flame, initially a laminar flame sheet resides at the inner shear layer of the main jet, along the interface between incoming fresh gas and high temperature recirculating gas. Further downstream, vortex breakdown alters the flame sheet path toward the central flame region. The lower reaction zones show good correlation to the regions of maximum vorticity and track the regions of low compressive strain associated with the inner shear layer of the jet flow. In both flames the reactions zones conform the passage of the large structure while remaining inside the low speed regions or at the inner shear layer.
机译:通过使用立体声PIV和OH-PLIF以5 KHz重复频率同时测量流场,研究了在石英夸克中稳定的非预混合甲烷旋流火焰中的火焰流场相互作用。在相同的旋流强度下,研究了两种具有不同燃料喷射速度的火焰。时间平均流场显示了在夸脱出口处的独特流型,在该处形成了两个回流涡流。远离燃烧室出口形成的强回流区和在燃烧室内部延伸的较大回流区。然而,瞬时图像表明,在夸脱出口附近的流动模式在反应区的空间位置和结构中起着至关重要的作用。在低燃料喷射速度的火焰中,一对精确位于燃烧室出口拐角处的涡旋结构使火焰卷入低速流动的中心区域,然后火焰片跟踪轴向速度波动。旋涡场揭示了围绕反应区的旋涡结构,该旋涡结构位于与该旋涡结构相邻的低压缩应变层上。在高燃料喷射速度的火焰中,最初,层流火焰片沿着进入的新鲜气体与高温再循环气体之间的界面位于主喷射流的内部剪切层上。在更下游,涡流破坏改变了火焰片流向中央火焰区域的路径。较低的反应区与最大涡度的区域具有良好的相关性,并跟踪与射流内部剪切层相关的低压缩应变的区域。在两个火焰中,反应区都与大型结构的通道相符,同时保留在低速区域内或内部剪切层。

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