超声速横流中反应与非反应射流的数值模拟

IF 5 Q2 ENERGY & FUELS
Michael Ullman, Shivank Sharma, Venkat Raman
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引用次数: 0

摘要

超声速横流中的典型射流研究已被广泛用于研究与各种应用相关的基础物理。虽然大多数JISC的工作都考虑了气体注入,但液体注入也具有实际意义,并引入了额外的多尺度物理,如雾化和蒸发,使流动动力学复杂化。为了促进对这些复杂现象的进一步理解,这项工作提出了反应和非反应JISC构型的多相模拟,自由流马赫数约为4.5。采用流体体积方案实现自适应网格细化,以高分辨率捕捉液体破碎和湍流混合过程。结果比较了射流动量比和自由流温度对射流侵彻、混合和燃烧动力学的影响。对于相似的射流动量比,反应和非反应情况下的射流侵彻和混合特性相似。混合分析表明,涡度和湍流动能(TKE)强度在急流切变层中达到峰值,其中涡旋拉伸是所有情况下主要的湍流产生机制。在自由流温度较低的情况下,热释放可以忽略不计,而在自由流温度较高的情况下,化学反应主要沿着船头激波和射流尾流的边界层进行。蒸发冷却使初级雾化区的化学反应在喷射高度处淬灭,使得x/d=20后几种产物的流量趋于平稳。由于局部温度和压力升高,最终产物物质的大量集中只在弓形激波沿线和远下游的边界层中观察到,在那里较低的流速抵消了长时间点火延迟的影响。这些因素的综合作用导致区域出口的燃烧效率较低。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Numerical simulation of reacting and non-reacting liquid jets in supersonic crossflow
Canonical jet in supersonic crossflow (JISC) studies have been widely used to study fundamental physics relevant to a variety of applications. While most JISC works have considered injection of gases, liquid injection is also of practical interest and introduces additional multi-scale physics, such as atomization and evaporation, that complicate the flow dynamics. To facilitate further understanding of these complex phenomena, this work presents multiphase simulations of reacting and non-reacting JISC configurations with freestream Mach numbers of roughly 4.5. Adaptive mesh refinement is implemented with a volume of fluid scheme to capture the liquid breakup and turbulent mixing at high resolution. The results compare the effects of the jet momentum ratio and freestream temperature on the jet penetration, mixing, and combustion dynamics. For similar jet momentum ratios, the jet penetration and mixing characteristics are similar for the reacting and non-reacting cases. Mixing analyses reveal that vorticity and turbulent kinetic energy (TKE) intensities peak in the jet shear layers, where vortex stretching is the dominant turbulence-generation mechanism for all cases. Cases with lower freestream temperatures yield negligible heat release, while cases with elevated freestream temperatures exhibit chemical reactions primarily along the leading bow shock and within the boundary layer in the jet wake. The evaporative cooling quenches the chemical reactions in the primary atomization zone at the injection height, such that the flow rates of several product species plateau after x/d=20. Substantial concentrations of final product species are only observed along the bow shock—due to locally elevated temperature and pressure—and in the boundary layer far downstream—where lower flow velocities counteract the effects of prolonged ignition delays. This combination of factors leads to low combustion efficiency at the domain exit.
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