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首页> 外文期刊>Journal of Fluid Mechanics >Ignition, flame structure and near-wall burning in transverse hydrogen jets in supersonic crossflow
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Ignition, flame structure and near-wall burning in transverse hydrogen jets in supersonic crossflow

机译:超声速横流中横向氢射流的点火,火焰结构和近壁燃烧

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We have investigated the properties of transverse sonic hydrogen jets in high-temperature supersonic crossflow at jet-to-crossflow momentum flux ratios J between 0.3 and 5.0. The crossflow was held fixed at a Mach number of 2.4, 1400 K and 40 kPa. Schlieren and OH* chemiluminescence imaging were used to investigate the global flame structure, penetration and ignition points; OH planar laser-induced fluorescence imaging over several planes was used to investigate the instantaneous reaction zone. It is found that J indirectly controls many of the combustion processes. Two regimes for low (<1) and high (>3) J are identified. At low J, the flame is lifted and stabilizes in the wake close to the wall possibly by autoignition after some partial premixing occurs; most of the heat release occurs at the wall in regions where OH occurs over broad regions. At high J, the flame is anchored at the upstream recirculation region and remains attached to the wall within the boundary layer where OH remains distributed over broad regions; a strong reacting shear layer exists where the flame is organized in thin layers. Stabilization occurs in the upstream recirculation region that forms as a consequence of the strong interaction between the bow shock, the jet and the boundary layer. In general, this interaction - which indirectly depends on J because it controls the jet penetration - dominates the fluid dynamic processes and thus stabilization. As a result, the flow field may be characterized by a flame structure characteristic of multiple interacting combustion regimes, from (non-premixed) flamelets to (partially premixed) distributed reaction zones, thus requiring a description based on a multi-regime combustion formulation.
机译:我们研究了横向超声声氢射流在高温超声速横流中的特性,射流与横流的动量通量比J在0.3和5.0之间。错流保持固定,马赫数为2.4、1400 K和40 kPa。 Schlieren和OH *化学发光成像用于研究整体火焰结构,穿透和着火点。使用OH平面激光诱导的在多个平面上的荧光成像来研究瞬时反应区。发现J间接地控制了许多燃烧过程。确定了低(<1)和高(> 3)J的两种情况。在低J值下,部分预混发生后,火焰可能会通过自燃而升起并稳定在靠近壁的尾流处。大部分的热量释放发生在宽阔区域中发生OH的区域的壁上。在高J值处,火焰被锚固在上游的再循环区域,并保持附着在边界层内的壁上,在该边界层上OH仍然分布在较宽的区域内。在火焰组织成薄层的情况下,存在一个强大的反应性剪切层。由于弓形激波,射流和边界层之间的强烈相互作用,在上游的再循环区域中形成了稳定作用。通常,这种相互作用-间接取决于J,因为它控制射流的穿透-主导了流体动力学过程,从而稳定了流体。结果,流场的特征在于从(非预混的)小火焰到(部分预混的)分布的反应区域的多个相互作用的燃烧状态的火焰结构特征,因此需要基于多区域燃烧公式进行描述。

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