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首页> 外文期刊>Journal of propulsion and power >Combustion of Vaporized Kerosene in Supersonic Model Combustors with Dislocated Dual Cavities
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Combustion of Vaporized Kerosene in Supersonic Model Combustors with Dislocated Dual Cavities

机译:具有错位双腔的超音速模型燃烧器中汽化煤油的燃烧

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摘要

Supersonic combustion of vaporized kerosene in a Mach 2.5 model combustor with a total temperature of 1500 K and a total pressure of 1.3 MPa was experimentally investigated for an optimal integration of the cavity-based flameholder and the fuel injection scheme. A novel design of a supersonic model combustor consisting of a two-staged fuel injection system and dislocated dual cavities was proposed to improve the combustor performance, including the combustion efficiency, flame stabilization, combustor "unstart," and heat release distribution. Specifically, a large number of experiments were performed to systematically investigate the effects of fuel injection distribution, which is controlled by varying the injector spacing and the fuel equivalence ratio, on the static pressure distribution, thrust increment, lean blowout limit, wall temperature distribution, and combustor unstart characteristics. The results show that there exists an optimal range of injector spacing to obtain enhanced combustion performance while avoiding the combustion unstart. Furthermore, the equal fuel injection with an overall equivalence ratio of 0.5 for the two injectors was found to result in the optimal static pressure distribution and hence the largest thrust increment.
机译:实验研究了汽化煤油在Mach 2.5模型燃烧器中的超声燃烧,总温度为1500 K,总压力为1.3 MPa,以实现基于腔的火焰保持器和燃料喷射方案的最佳集成。提出了一种由两级燃料喷射系统和错位的双腔组成的超音速模型燃烧室的新颖设计,以改善燃烧室的性能,包括燃烧效率,火焰稳定度,燃烧室“启动”和放热分布。具体而言,进行了大量实验以系统地研究通过改变喷油嘴间距和燃料当量比来控制的喷油分布对静压分布,推力增量,稀薄喷出极限,壁温分布的影响,和燃烧器的启动特性。结果表明,存在最佳的喷射器间距范围,以在不引起燃烧停止的情况下获得增强的燃烧性能。此外,发现两个喷射器的总当量比为0.5的相等燃料喷射导致最佳的静压力分布,从而产生最大的推力增量。

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  • 来源
    《Journal of propulsion and power》 |2014年第5期|1152-1160|共9页
  • 作者单位

    State Key Laboratory of High Temperature Gas Dynamics, Chinese Academy of Sciences, 100190 Beijing, People's Republic of China;

    State Key Laboratory of High Temperature Gas Dynamics, Chinese Academy of Sciences, 100190 Beijing, People's Republic of China;

    State Key Laboratory of High Temperature Gas Dynamics, Chinese Academy of Sciences, 100190 Beijing, People's Republic of China;

    Hong Kong Polytechnic University, Kowloon, Hong Kong, People's Republic of China;

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