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喷注结构对超声速气-固两相富燃燃气燃烧增强特性

杨鹏年 夏智勋 马立坤 陈斌斌 冯运超 陈兴元

杨鹏年, 夏智勋, 马立坤, 等. 喷注结构对超声速气-固两相富燃燃气燃烧增强特性[J]. 航空动力学报, 2026, 41(1):20240755 doi: 10.13224/j.cnki.jasp.20240755
引用本文: 杨鹏年, 夏智勋, 马立坤, 等. 喷注结构对超声速气-固两相富燃燃气燃烧增强特性[J]. 航空动力学报, 2026, 41(1):20240755 doi: 10.13224/j.cnki.jasp.20240755
YANG Pengnian, XIA Zhixun, MA Likun, et al. Combustion enhancement characteristics of supersonic gas-solid two-phase enriched fuel by injector structure[J]. Journal of Aerospace Power, 2026, 41(1):20240755 doi: 10.13224/j.cnki.jasp.20240755
Citation: YANG Pengnian, XIA Zhixun, MA Likun, et al. Combustion enhancement characteristics of supersonic gas-solid two-phase enriched fuel by injector structure[J]. Journal of Aerospace Power, 2026, 41(1):20240755 doi: 10.13224/j.cnki.jasp.20240755

喷注结构对超声速气-固两相富燃燃气燃烧增强特性

doi: 10.13224/j.cnki.jasp.20240755
基金项目: 国家自然科学基金(12272409,U21B2086); 国防科技大学基石基金计划项目(JS2023-07); 湖南省荷尖人才计划(2022RC1233);湖南省研究生科研创新项目(CX20230058)
详细信息
    作者简介:

    杨鹏年(1996-),男,博士生,主要研究方向为新型固体推进技术。E-mail:yangpengnian@nudt.edu.cn

    通讯作者:

    马立坤(1987-),男,副教授,博士,主要研究方向为新型固体推进技术。E-mail:malikun@nudt.edu.cn

  • 中图分类号: V435

Combustion enhancement characteristics of supersonic gas-solid two-phase enriched fuel by injector structure

  • 摘要:

    针对超声速气-固两相富燃燃气燃烧增强特性,采用数值模拟方法,对比分析了不同喷口形状(圆形、椭圆形、矩形)和喷口布置(单侧与双侧喷注,不同喷注角度)对富燃燃气掺混燃烧的影响规律。研究发现,喷口形状和布置策略对燃烧增强特性具有显著影响。与矩形喷口相比,圆形和椭圆形喷口更有助于富燃燃气在燃烧室内的燃烧释热。此外,增加喷口数量和调整喷口角度能提高穿透深度并促进展向分布,有效扩大富燃燃气与来流空气的接触面积,从而显著提升气相组分的燃烧速度及碳颗粒的燃烧效率。研究还发现,颗粒燃烧过程高度依赖于高温与富氧环境的协同作用,富燃燃气释热的过度集中可能不利于颗粒的加热和点火。因此,创造并维持一个稳定的高温富氧环境,同时确保颗粒能够顺利进入这一理想燃烧区域,对于提升颗粒燃烧效率、优化整体燃烧性能至关重要。

     

  • 图 1  燃烧室壁面压力试验与数值模拟结果对比

    Figure 1.  Comparison of experiment and simulation results of wall pressure along the scramjet combustor

    图 2  喷口形状示意图

    Figure 2.  Schematic of nozzle shapes

    图 3  不同喷口形状下的马赫数、总压恢复系数和总温分布

    Figure 3.  Mach number, total pressure recovery coefficient and total temperature distributions with different nozzle shapes

    图 4  不同喷口形状下富燃燃气的燃烧效率

    Figure 4.  Combustion efficiency distributions of the enriched fuel with different nozzle shapes

    图 5  不同喷口形状下燃烧室中的温度云图

    Figure 5.  Temperature contours in combustors with different nozzle shapes

    图 6  不同喷口形状下的颗粒轨迹

    Figure 6.  Particle trajectory with different nozzle shapes

    图 7  喷口布置示意图

    Figure 7.  Schematic of fuel-jet arrangements

    图 8  不同喷口布置下的马赫数、总压恢复系数和总温分布

    Figure 8.  Mach number, total pressure recovery coefficient and total temperature distributions with different fuel-jet arrangements

    图 9  不同喷口布置下富燃燃气的燃烧效率

    Figure 9.  Combustion efficiency distributions of the enriched fuel with different fuel-jet arrangements

    图 10  不同喷口布置下燃烧室中的温度云图

    Figure 10.  Temperature contours in combustors with different fuel-jet arrangements

    图 11  不同喷口布置下的颗粒轨迹

    Figure 11.  Particle trajectory with different fuel-jet arrangements

    表  1  边界条件

    Table  1.   Boundary conditions

    边界位置 边界类型 总压/MPa 静压/MPa 总温/K
    来流入口 压力入口 1.08 0.093 1660
    燃料喷口 压力入口 1.26 1.010 1 990
    出口 压力出口 0.100 300
    壁面 无滑移壁面
    下载: 导出CSV

    表  2  硼基固体推进剂燃烧的简化组分

    Table  2.   Simplified component of boron-based solid propellant combustion

    相态 组分 质量分数/%
    气相 CO 39.73
    HCl 12.75
    HBO2 0.95
    CO2 0.004
    MgCl2 29.33
    B2O2 3.34
    H2O 0.04
    N2 0.813
    H2 11.62
    B2O3 1.42
    BO2 0.003
    凝相颗粒 B 38.7
    C 27.4
    Al2O3 33.9
    下载: 导出CSV

    表  3  不同喷口形状的燃烧室构型

    Table  3.   Combustion configuration with different nozzle shapes

    工况 喷口布置 喷口形状 喷注角度/(°)
    Case 1 单侧喷注 圆形 60
    Case 2 单侧喷注 椭圆形 60
    Case 3 单侧喷注 矩形 60
    下载: 导出CSV

    表  4  不同喷口布置的燃烧室构型

    Table  4.   Combustion configuration with different fuel-jet arrangements

    工况 喷口布置 喷口形状 喷注角度/(°)
    Case 1 单侧喷注 圆形 60
    Case 4 双侧喷注 圆形 60
    Case 5 双侧喷注 圆形 90
    下载: 导出CSV
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