1. 中国航天空气动力技术研究院,北京,100074
2. 中国科学技术大学 工程与材料科学实验中心,合肥,230026
3. 北京动力机械研究所,北京,100074
卢洪波(1985—),男,博士研究生,研究员,研究方向:冲压发动机流动/燃烧特征与试验技术. E-mail:finlhb_0605@163.com
林键*(1984—),男,博士研究生,高级工程师,研究方向:气动热测量技术与脉冲风洞技术. E-mail:naoh52@sohu.com
纸质出版:2024
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卢洪波, 林键, 金熠, 等. 马赫数10条件下冲压发动机内氢气燃烧特性试验[J]. 空气动力学学报, 2024, 42(4): 27−36.
LU Hongbo, LIN Jian, JIN Yi, et al. Hydrogen combustion experiments of a fullpath scramjet at a Mach 10 condition of high enthalpy shock tunnel[J]. 2024, 42(4): 27-36.
卢洪波, 林键, 金熠, 等. 马赫数10条件下冲压发动机内氢气燃烧特性试验[J]. 空气动力学学报, 2024, 42(4): 27−36. DOI: 10.7638/kqdlxxb-2023.0134
LU Hongbo, LIN Jian, JIN Yi, et al. Hydrogen combustion experiments of a fullpath scramjet at a Mach 10 condition of high enthalpy shock tunnel[J]. 2024, 42(4): 27-36. DOI: 10.7638/kqdlxxb-2023.0134.
针对高马赫数超燃冲压发动机面临的高效燃烧组织挑战,本文提出了一种凹腔后缘激波强化的高马赫数超声速燃烧组织技术,并设计了一套燃烧室采用双侧对称布置凹腔结构的三维发动机试验模型。采用OH
*
基化学发光光谱诊断与壁面测压相结合的试验手段,在自由活塞驱动激波风洞的名义
Ma
= 10流场中,对凹腔上游横向氢气射流的燃烧特性进行了研究,并讨论了模拟流场的重复性,给出了氢气燃烧演化特征、火焰稳定结构及释热特性。不同车次的总压等流场参数表明试验流场具有较高的重复性,可保障氢气燃烧特性的可复现性。通过观察试验过程中OH
*
基动态发光特征发现,在高焓激波风洞发动机试验中采用燃料提前喷注的方法使发动机流道在空气主流到来之前充盈大量的氢气,进而在主流到达发动机内的瞬间形成所谓“激波管流动-燃烧”效应,使来流空气与氢气接触面发生自点火与剧烈燃烧,产生显著不同于发动机正常工作情况下的点火与燃烧机制,但随着主流趋于平稳,“激波管流动-燃烧”效应消失,在高总温气流的自点火效应与凹腔后缘的X型激波耦合作用下,火焰稳定在凹腔上游近壁面区的氢气射流尾迹区和凹腔后缘附近的全流场中。通过分析壁面压力分布特征发现,凹腔后缘的X型激波实现了燃烧的强化与火焰的稳定,并获得了最显著的释热压升。这些结果表明高马赫数冲压发动机可利用凹腔后缘X型激波强化燃烧和稳定火焰。
To explore how to improve the performance of scramjet engines operating at a flight Mach number around 10
we proposed a method to achieve combustion enhancement by means of the cavity-aft-shock
and designed the three-dimensional scramjet article with a both-side-symmetrically-configured cavity combustion chamber. Using a combination of the excited OH
*
chemiluminescenc
e visualization and wall pressure measurement
burning characteristics of the hydrogen jet injected upstream of the cavity in a highly supersonic crossflow of the scramjet combustor were experimentally studied at the nominal condition of
Ma
= 10 in a free-piston driven high enthalpy shock tunnel. The repeatability of the simulated flow field was discussed
and the evolution characteristics of hydrogen combustion
flame-stabilization structure
and heat release profiles were given. Across all experimental cases
the stagnation parameters of the freestream flow remained constant with low standard deviation
allowing for effective analysis of hydrogen combustion characteristics. The evolving features of OH
*
chemiluminescence indicate that the so-called "shock tube flow-combustion" in the engine article is formed at the initial stage of the crossflow establishment due to the employment of the fuel injection before the arrival of the highly supersonic crossflow
leading to the autoignition at the contact interface of the high temperature crossflow with the injected hydrogen
while the flame ultimately anchors at the jet wake of the bodyside wall and the whole flow path around the cavity aft due to the coupling interaction of the autoignition in high total temperature crossflow and cavity-aft X-type shock pattern. The OH
*
luminosity and wall pressure distribution features within the effective test time demonstrate that the combustion enhancement is associated with the cavity-aft X-type shock patterns
which generate the drastic heat release-induced pressure rise. The results are useful to promote combustion efficiency of high Mach number scramjet engines by means of cavity configuration presented in this paper.
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