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Geometric influence on the propagation of the quasi-detonations in a stoichiometric H_2-O_2 mixture

机译:几何影响对化学计量H_2-O_2混合物中的准爆炸繁殖的影响

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Combustion wave propagation was studied experimentally in an obstructed narrow channel filled with stoichiometric H-2-O-2 mixtures using a simultaneous schlieren and soot foil technique. The propagation modes uncovered were classified as fast-flames, discontinuous detonation, and continuous detonation. In this study blockage ratio (BR) was found to have a strong effect on the detonation limit. For BRs of 33% and 66%, the ratio of the obstacle opening and detonation cell size (d/lambda) at the detonation limit was found to be 0.6 and 6.0, respectively. This order of magnitude change in the detonation limit was found to be governed by a change in propagation mechanism associated with the discontinuous detonation mode. For all BRs the discontinuous mode is characterized by detonation failure, as it diffracts through the obstacle opening, and then re-initiation. For the low BR obstacles detonation re-initiation is driven by the generation of a detonation Mach stem that propagates along the top and bottom walls following oblique reflection of the decoupled detonation leading shock wave. For the high BR obstacles shock reflection off the top and bottom walls does not produce a detonation wave, instead a detonation is initiated at the proceeding obstacle face following a roughly normal reflection of the leading shock. These propagation mechanisms are not governed by obstacle BR, but rather the obstacle height and spacing is the key parameter as they control the strength of the shock at the point of reflection.
机译:通过使用同时Schlieren和烟灰箔技术在填充有化学计量的H-2-O-2混合物的阻塞窄通道中实验研究燃烧波传播。未覆盖的传播模式被归类为快速火焰,不连续的爆轰和连续爆炸。在该研究中,发现封闭率(BR)对爆轰极限产生了强烈影响。对于33%和66%的BRS,发现爆震限制下的障碍物开口和爆炸细胞尺寸(D / Lambda)的比例分别为0.6和6.0。发现爆震限制中的这种级别变化顺序由与不连续爆震模式相关联的传播机制的变化来控制。对于所有BRS,不连续模式的特征在于爆轰失败,因为它通过障碍物开口衍射,然后重新启动。对于低BR障碍物,爆炸重新启动通过产生沿着顶次和底壁传播的爆炸马蹄杆驱动,这在倾斜的爆轰引导波浪的倾斜反射之后传播。对于高BR障碍物的障碍物,顶壁的冲击反射不会产生爆轰波,而是在主导冲击大致正常反射之后在进行障碍物面上启动爆炸。这些传播机制不受障碍物BR管辖,而是障碍物高度和间距是控制反射点处的冲击强度的关键参数。

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