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Effect of shock structure on stabilization and blow-off of hydrogen jet flames

机译:冲击结构对氢射流火焰稳定和喷吹的影响

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Under-expanded hydrogen jet has characteristic shock structure immediately downstream of the nozzle exit. The shock structure depends on the ratio p(Ex)/p(A), i.e. the ratio of nozzle exit to ambient pressure, and the distributions of velocity and concentration in an under-expanded hydrogen jet depend on characteristics of the shock structure. Therefore, the shock structure should affect the blow-off behaviour of under-expanded hydrogen jet flame. Since this issue has not been investigated in detail, this study aims to close this knowledge gap. The effect of changes in shock structure on lift-off length and blow-off conditions for non-premixed turbulent hydrogen free jet flame has been experimentally investigated. The shock structure was varied by using three types of nozzles: convergent, straight and divergent nozzles. Inlet diameters of nozzles change from 0.31 to 1.04 mm and outlet diameters from 0.34 to 1.7 mm. The static pressure and the ratio of cross-section area at the nozzle inlet to that at the outlet were varying parameters in this study. Hydrogen was horizontally spouted through a nozzle to atmosphere. The maximum static pressure in a nozzle was 13.2 MPa. The experiments revealed that when the hydrogen jet had sequential shock cell structures, which occurred in the range of p(Ex)/p(A) smaller than 2.45, a higher mass flow rate of hydrogen was needed for the stabilization of a jet flame than that for p(Ex)/p(A) larger than 2.45 and that when closed to the ideal expansion (p(Ex)/p(A) = 1), the mass flow rate for stable flame became maximum. In addition, it was observed that the lift-off length of stable flames followed with sequential shock cell structures were almost the same when the minimum cross-section area of used nozzles was constant. However, when hydrogen jet had a shock structure with single Mach disk, the lift-off lengths and the minimum mass flow rate required for the stable jet flame were decreasing with the decrease of the cross-sectional area ratio of the nozzle exit to inlet. (C) 2020 Hydrogen Energy Publications LLC. Published by Elsevier Ltd. All rights reserved.
机译:膨胀不足的氢气射流在喷嘴出口的下游具有特征性的冲击结构。冲击结构取决于比率p(Ex)/ p(A),即喷嘴出口与环境压力的比率,并且在膨胀不足的氢射流中速度和浓度的分布取决于冲击结构的特性。因此,冲击结构将影响膨胀不足的氢射流火焰的喷射行为。由于尚未对此问题进行详细调查,因此本研究旨在缩小这一知识差距。实验研究了冲击结构变化对非预混湍流无氢射流火焰的升空长度和升空条件的影响。通过使用三种类型的喷嘴来改变冲击结构:会聚喷嘴,笔直喷嘴和发散喷嘴。喷嘴的入口直径从0.31变为1.04 mm,出口直径从0.34变为1.7 mm。在这项研究中,静压和喷嘴入口处与出口处的横截面积之比是变化的参数。通过喷嘴将氢气水平喷出到大气中。喷嘴中的最大静压力为13.2MPa。实验表明,当氢射流具有连续的冲击池结构(发生在p(Ex)/ p(A)小于2.45的范围内)时,稳定射流火焰所需的氢气质量流量要高于氢流量。当p(Ex)/ p(A)大于2.45且接近理想膨胀(p(Ex)/ p(A)= 1)时,稳定火焰的质量流量变为最大。此外,可以观察到,当使用的喷嘴的最小横截面面积恒定时,稳定火焰的升起长度以及相继的冲击腔结构随后将几乎相同。然而,当氢射流具有单个马赫盘的冲击结构时,稳定的射流火焰所需的升起长度和最小质量流率随着喷嘴出口与入口的截面积比的减小而减小。 (C)2020 Hydrogen Energy Publications LLC。由Elsevier Ltd.出版。保留所有权利。

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