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脉冲爆震外涵加力燃烧室推力特性

谢俊杰 郑龙席 卢杰 王凌羿 谭汶昊

谢俊杰, 郑龙席, 卢杰, 等. 脉冲爆震外涵加力燃烧室推力特性[J]. 航空动力学报, 2025, 40(1):20220448 doi: 10.13224/j.cnki.jasp.20220448
引用本文: 谢俊杰, 郑龙席, 卢杰, 等. 脉冲爆震外涵加力燃烧室推力特性[J]. 航空动力学报, 2025, 40(1):20220448 doi: 10.13224/j.cnki.jasp.20220448
XIE Junjie, ZHENG Longxi, LU Jie, et al. Thrust characteristics of pulse detonation duct burner[J]. Journal of Aerospace Power, 2025, 40(1):20220448 doi: 10.13224/j.cnki.jasp.20220448
Citation: XIE Junjie, ZHENG Longxi, LU Jie, et al. Thrust characteristics of pulse detonation duct burner[J]. Journal of Aerospace Power, 2025, 40(1):20220448 doi: 10.13224/j.cnki.jasp.20220448

脉冲爆震外涵加力燃烧室推力特性

doi: 10.13224/j.cnki.jasp.20220448
详细信息
    作者简介:

    谢俊杰(1997-),男,硕士生,研究方向为脉冲爆震燃烧与流动

    通讯作者:

    郑龙席(1971-),男,教授、博士生导师,博士,主要从事新概念发动机研究。E-mail:zhenglx@nwpu.edu.cn

  • 中图分类号: V231.2

Thrust characteristics of pulse detonation duct burner

  • 摘要:

    为了得到不同喷管与脉冲爆震外涵加力燃烧室相互作用机理,提高脉冲爆震外涵加力燃烧室增推性能,对无喷管、带七种收敛喷管、七种收扩喷管和五种二次流喷管的脉冲爆震外涵加力燃烧室进行了数值计算。结果表明:收敛喷管会反射压缩波,减缓高压工质的排出,提高轴向力增益;收扩喷管会在收敛段的基础上进一步加速气流,但在一个循环的某些时间内会使外界激波进入扩张段而造成部分推力损失;二次流喷管可以调节喷管扩张段工质参数,但也会带来一定的掺混损失。三种工况下采用二次流喷管时轴向力增益提升率最高,依次为22.11%、15.06%和15.23%。

     

  • 图 1  脉冲爆震外涵加力燃烧室数值计算模型与网格

    Figure 1.  Numerical calculation model and grid of pulse detonation duct burner

    图 2  喷管数值计算模型

    Figure 2.  Numerical calculation model of nozzle

    图 3  二次流喷管计算模型

    Figure 3.  Numerical calculation model of fluidic nozzle

    图 4  工况1下无喷管时总压与静温云图

    Figure 4.  Total pressure and static temperature contour without nozzle under condition 1

    图 5  不同工况下脉冲爆震外涵加力燃烧室轴向力的变化

    Figure 5.  Variation of axial force in pulse detonation duct burner under different conditions

    图 6  单次计算周期随收敛比的变化

    Figure 6.  Variation of single calculation time with convergence ratio

    图 7  工况1下装有C1喷管后总压与静温变化云图

    Figure 7.  Total pressure and static temperature contour with C1 nozzle under condition 1

    图 8  轴向力增益随收敛比的变化

    Figure 8.  Axial force gain with different convergent nozzles

    图 9  单次计算周期随扩张比的变化

    Figure 9.  Variation of single calculation time with divergence ratio

    图 10  工况1下装有CD1喷管后总压与静温变化云图

    Figure 10.  Total pressure and static temperature contour with CD1 nozzle under condition 1

    图 11  工况1下马赫数随时间的变化

    Figure 11.  Mach number contour with convergent divergent nozzle under condition 1

    图 12  轴向力增益随扩张比的变化

    Figure 12.  Axial force gain under different working conditions with different convergent divergent nozzles

    图 13  工况1下装有二次流喷管后总压与静温变化云图

    Figure 13.  Total pressure and static temperature contour with fluidic nozzle under condition 1

    图 14  工况1下二次流喷管中马赫数的变化

    Figure 14.  Mach number contour with fluidic nozzle under condition 1

    图 15  不同工况轴向力增益随二次流喷管参数的变化

    Figure 15.  Variation of axial force gain under different working conditions with fluidic nozzle parameters

    表  1  网格尺寸验证结果

    Table  1.   Grid size verification results

    网格尺寸/mm CEA 计算结果 数值计算结果
    静压峰值/MPa 波速/(m/s) 静压峰值/MPa 波速/(m/s) DDT距离/m DDT时间/ms
    1.0 1.987 1797.7 1.87 1812.1 0.7733 2.95
    0.5 2.02 1853.2 0.7715 2.85
    0.2 2.04 1856.7 0.7711 2.87
    下载: 导出CSV

    表  2  喷管结构参数

    Table  2.   Nozzle structure parameters

    喷管类型 喷管编号 收敛段长度
    Lc/mm
    扩张段长度
    Ld/mm
    入口直径
    Din/mm
    喉部直径
    Dthroat/mm
    出口直径
    Dout/mm
    收敛比 扩张比
    收敛喷管 C1 40 0 62 36 0 0.3371 0
    C2 40 62 38 0.3757
    C3 40 62 40 0.4162
    C4 40 62 42 0.4589
    C5 40 62 44 0.5036
    C6 40 62 46 0.5505
    C7 40 62 48 0.5994
    收扩喷管 CD1 40 80.00 62 40 45 0.4162 1.2656
    CD2 40 80.00 62 40 50 0.4162 1.5625
    CD3 40 80.00 62 40 55 0.4162 1.8902
    CD4 40 90.94 62 40 60 0.4162 2.2500
    CD5 40 119.66 62 40 65 0.4162 2.6406
    CD6 40 150.40 62 40 70 0.4162 3.0625
    CD7 40 183.47 62 40 75 0.4162 3.5156
    下载: 导出CSV

    表  3  典型外涵入口工况

    Table  3.   Typical bypass inlet conditions

    工况 入口总压/MPa 入口总温/K
    1 0.3012 416.5
    2 0.3863 444.5
    3 0.4713 485.5
    下载: 导出CSV
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  • 收稿日期:  2022-06-22
  • 网络出版日期:  2024-08-21

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