凹腔燃烧室中粉末燃料流动特性大涡模拟研究-金属燃料推进剂技术专栏

  • 胡颖 ,
  • 董佳欣 ,
  • 王正阳 ,
  • 李超 ,
  • 任全彬
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  • 1. 西北工业大学
    2. 航天动力技术研究院

收稿日期: 2025-09-29

  修回日期: 2026-01-23

  网络出版日期: 2026-07-06

基金资助

陕西省青年科技新星

Large Eddy Simulation Study on the Flow Characteristics of Powder Fuel in a Cavity Combustor

  • HU Ying ,
  • DONG Jia-Xin ,
  • WANG Zheng-Yang ,
  • LI Chao ,
  • REN Quan-Bin
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Received date: 2025-09-29

  Revised date: 2026-01-23

  Online published: 2026-07-06

摘要

基于大涡模拟气固两相数值模型,本文对超声速流场内粉末燃料的掺混特性开展了详细研究。研究表明颗粒在超声速流场的流动行为具有显著的尺寸依赖性,在分布粒径条件下,较小颗粒会附着壁面并进入凹腔,较大颗粒则更接近主流区。进入凹腔前缘的颗粒驻留时间(约1 ms)显著长于绕过凹腔的颗粒(约0.4 ms)。对于2 μm和5 μm颗粒,其运动轨迹覆盖凹腔内低速回流区,通过再循环机制延长驻留时间。小尺寸颗粒(2 μm、5 μm)会引发剪切层轮廓的显著脉动,且更易受流场涡结构影响:其质量分数在喷射点附近达到约0.9,但向下游快速减小;主流区质量分数分布呈现明显不连续性(通常为0.1-0.3),且分布宽度大于大尺寸颗粒。相比之下,大尺寸颗粒(20 μm、40 μm)形成的剪切层轮廓更为平滑。增加喷射速度虽能略微提升颗粒射流穿透深度,但对总体颗粒驻留时间影响甚微。提高来流马赫数会缩短颗粒驻留时间,同时使颗粒射流发生偏转,促使更多颗粒进入凹腔。

本文引用格式

胡颖 , 董佳欣 , 王正阳 , 李超 , 任全彬 . 凹腔燃烧室中粉末燃料流动特性大涡模拟研究-金属燃料推进剂技术专栏[J]. 航空学报, 0 : 1 -0 . DOI: 10.7527/S1000-6893.2026.32849

Abstract

Based on a large eddy simulation (LES) gas-solid two-phase numerical model, this paper conducts a detailed investigation of the mixing characteristics of powder fuel in a supersonic flow field. The study reveals that the flow behavior of particles in the supersonic flow field exhibits significant size dependency. Under distributed particle size conditions, smaller particles tend to adhere to the wall and enter the cavity, while larger particles remain closer to the mainstream region. The residence time of particles entering the leading edge of the cavity (approximately 1 ms) is significantly longer than that of particles bypassing the cavity (approximately 0.4 ms). For 2 μm and 5 μm particles, their trajectories cover the low-speed recirculation zone within the cavity, extending the residence time through a recirculation mechanism. Small-sized particles (2 μm, 5 μm) cause significant fluctuations in the shear layer profile and are more susceptible to the flow field vortex structures: their mass fraction reaches about 0.9 near the injection point but decreases rapidly downstream; the mass fraction distribution in the mainstream region shows obvious discontinuity (typically 0.1–0.3), with a wider distribution compared to larger particles. In contrast, larger particles (20 μm, 40 μm) form a smoother shear layer profile. Increasing the injection velocity slightly enhances the penetration depth of the particle jet but has minimal impact on the overall particle residence time. Increasing the incoming Mach number reduces the particle residence time and causes deflection of the particle jet, driving more particles into the cavity.

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