燃烧对模型超燃冲压发动机燃烧室流场的影响

Shuhei Takahashi , Kazunori Wakai , Sadatake Tomioka , Mitsuhiro Tsue , Michikata Kono
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引用次数: 8

摘要

采用实验和数值方法研究了燃烧对带后台阶模型超燃冲压发动机燃烧室流场变化的影响。主气流的马赫数为2.0。冷流总温度为1000k,热流总温度为1800k。氢燃料通过台阶背面的狭缝与主气流平行注入。燃烧模式分为两种模式。一种是弱燃烧(WC)模式,不伴有激波,其流场与冷流相似。另一种是伴随激波的强燃烧(IC)模式,其流场与冷流的流场有很大不同。在IC模式下,激波在台阶后面产生一个大的分离区域,在该区域产生的涡流将燃料卷起。主要的反应区域在激波后面的剪切层,主要气流撞击卷起的燃料,并且由于激波的作用温度相对较高。然后,流场由混合速率控制,导致热量快速释放,从而提高燃烧室中的压力水平,并支持激波。这种被动反馈有效,混合效率和燃烧效率都提高了。另一方面,在WC模式下,反应区扩展到台阶下游的剪切层上,其放热速率低于IC模式。然后,流场由化学反应速率控制,燃烧效率仍然很低。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Effects of combustion on flowfield in a model scramjet combustor

The effects of combustion on the change of the flowfield in a model SCRamjet combustor with a backward step is investigated experimentally and numerically. The main airflow has a Mach number of 2.0. The total temperature is 1000 K for cold flow and 1800 K for hot flow. Hydrogen fuel is injected parallel to the main airflow through a slit on the backward face of the step. The combustion mode is categorized in two modes. One is a weak combustion (WC) mode that is not accompanied by a shock wave, where the flowfield is similar to that in cold flow. Another is an intensive combustion (IC) mode that is accompanied by a shock wave, where the flowfield is much different from that in cold flow. In IC mode, a large separation region is generated behind the step by the shock wave, and the vortex generated at the region rolls the fuel up. The main reacting region is in the shear layer just behind the shock wave, where the main airflow bumps the rolled-up fuel, and the temperature is relatively high due to the shock wave. The flowfield is then controlled by the rate of mixing, leading to fast heat release, which raises the pressure level in the combustor and supports the shock wave. This passive feedback works, and both the mixing efficiency and the combustion efficiency become high. On the other hand, in WC mode, the reacting region spreads over the shear layer downstream of the step, and its heat release rate is lower than that in IC mode. The flowfield is then controlled by the rate of chemical reaction, and the combustion efficiency remains low.

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