液体火箭反推进再入过程底部热环境与流动特性研究

  • 郑昊 ,
  • 唐勇 ,
  • 陈湘男 ,
  • 李霁 ,
  • 林志强 ,
  • 石保禄
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  • 1. 北京理工大学空天科学与技术学院
    2. 北京理工大学

收稿日期: 2025-09-10

  修回日期: 2025-12-10

  网络出版日期: 2025-12-15

基金资助

民用航天技术预先研究项目

Study on Thermal Environment and Flow Field Characteristics of Resuable Liquid Rocket under Retro-propulsion

  • ZHENG Hao ,
  • TANG Yong ,
  • CHEN Xiang-Nan ,
  • LI Ji ,
  • LIN Zhi-Qiang ,
  • SHI Bao-Lu
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Received date: 2025-09-10

  Revised date: 2025-12-10

  Online published: 2025-12-15

摘要

可重复使用液体火箭是未来航天运输系统的重要发展方向,火箭垂直再入过程中底部发动机以非规则构型迎风下降,局部热环境和流动特性十分复杂。针对猎鹰9号v1.2的构型设计箭体,根据再入过程的特点选取了高空动力减速、高空气动减速、低空气动减速、低空动力减速等四个典型阶段,开展了发动机迎风再入绕流气动特性仿真研究。结果表明,再入过程箭体热环境呈高度瞬态、非均匀特征,羽流结构随高度和发动机工况发生显著变化;动力减速阶段因燃气-来流强耦合,其流动紊乱程度与热流峰值均显著高于气动减速阶段;二次燃烧对低空远场羽流的热影响具有全域性;四个典型阶段中,最大热流始终集中于喷管出口外沿及箭体底部边缘区域,峰值可达380kW/m2,为发动机热防护设计提供支撑。

本文引用格式

郑昊 , 唐勇 , 陈湘男 , 李霁 , 林志强 , 石保禄 . 液体火箭反推进再入过程底部热环境与流动特性研究[J]. 航空学报, 0 : 1 -0 . DOI: 10.7527/S1000-6893.2025.32772

Abstract

Reusable liquid-propellant launch vehicles constitute a pivotal direction for future space transportation systems. During vertical reentry, the aft-mounted engines descend in an irregular configuration facing the freestream, engendering highly localized and complex thermal environments. A simulation study of the flow over a Falcon 9 v1.2 derived geometry was conducted for four representative reentry phases: high-altitude powered deceleration, high-altitude aerodynamic deceleration, low-altitude aerodynamic deceleration, and low-altitude powered deceleration. Results demonstrate that the vehicle thermal environment is markedly transient and non-uniform: plume morphology evolves continuously with altitude and engine operating condition; powered phases exhibit substantially stronger flow disturbances and heat-flux maxima than aerodynamic phases owing to intense plume–freestream coupling; secondary combustion exerts a global thermal influence on the far-field plume at low altitude. Across all phases, peak heat flux consistently localizes at the nozzle-exit lip and the outer rim of the aft heat shield, reaching 380 kW/m2, thereby identifying these regions as critical for thermal protection.

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