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液体火箭反推进再入过程底部热环境与流动特性

郑昊 唐勇 陈湘男 李霁 林志强 石保禄

航空学报2026,Vol.47Issue(8):106-119,14.
航空学报2026,Vol.47Issue(8):106-119,14.DOI:10.7527/S1000-6893.2025.32772

液体火箭反推进再入过程底部热环境与流动特性

Base-region thermal environment and flow characteristics of liquid rocket in retro-propulsion re-entry process

郑昊 1唐勇 2陈湘男 1李霁 1林志强 3石保禄2

作者信息

  • 1. 北京理工大学 空天科学与技术学院,北京 100081
  • 2. 北京理工大学 空天科学与技术学院,北京 100081||北京理工大学(珠海)空天信息学域,珠海 519088
  • 3. 北京理工大学(珠海)空天信息学域,珠海 519088
  • 折叠

摘要

Abstract

Reusable liquid-propellant launch vehicles constitute a pivotal direction for future space transportation sys-tems.During vertical re-entry of a rocket,the aft-mounted engines descend in an irregular configuration facing the freestream.The local thermal environment and flow characteristics are highly complex.A simulation study of the flow over a Falcon 9 v1.2 derived geometry was conducted for four representative re-entry phases:high-altitude powered deceleration,high-altitude aerodynamic deceleration,low-altitude aerodynamic deceleration,and low-altitude powered deceleration.The vehicle thermal environment is markedly transient and non-uniform:plume morphology evolves con-tinuously with altitude and engine operating condition.Powered deceleration phases exhibit substantially stronger flow disturbances and heat-flux maxima than aerodynamic deceleration phases owing to intense plume-freestream cou-pling.Secondary combustion exerts a global thermal influence on the far-field plume at low altitude.Across the four characteristic stages,the peak heat flux persistently localizes at the nozzle lip and the aft-edge of the rocket base,reaching 380 kW/m2,these data constitute a quantitative basis for engine thermal-protection design.

关键词

可重复使用/火箭回收/垂直再入/热环境/流动特性

Key words

reusable/rocket recovery/vertical re-entry/thermal environment/flow characteristics

分类

航空航天

引用本文复制引用

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[J].航空学报,2026,47(8):106-119,14.

基金项目

民用航天技术预先研究项目(D020201) Civil Aerospace Technology Pre-Research Project(D020201) (D020201)

航空学报

1000-6893

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