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进气温度对脉冲爆震燃烧特性影响

卢恒 张至斌 徐啸 何小民

卢恒, 张至斌, 徐啸, 等. 进气温度对脉冲爆震燃烧特性影响[J]. 航空动力学报, 2025, 40(6):20230821 doi: 10.13224/j.cnki.jasp.20230821
引用本文: 卢恒, 张至斌, 徐啸, 等. 进气温度对脉冲爆震燃烧特性影响[J]. 航空动力学报, 2025, 40(6):20230821 doi: 10.13224/j.cnki.jasp.20230821
LU Heng, ZHANG Zhibin, XU Xiao, et al. Effect of inlet temperatures on pulse detonation combustion characteristics[J]. Journal of Aerospace Power, 2025, 40(6):20230821 doi: 10.13224/j.cnki.jasp.20230821
Citation: LU Heng, ZHANG Zhibin, XU Xiao, et al. Effect of inlet temperatures on pulse detonation combustion characteristics[J]. Journal of Aerospace Power, 2025, 40(6):20230821 doi: 10.13224/j.cnki.jasp.20230821

进气温度对脉冲爆震燃烧特性影响

doi: 10.13224/j.cnki.jasp.20230821
基金项目: 基础加强计划
详细信息
    作者简介:

    卢恒(2000-),男,硕士,主要从事爆震燃烧方面研究

    通讯作者:

    何小民(1971-),男,教授、博士生导师,博士,主要从事航空航天动力燃烧理论和技术方面研究。E-mail:hxm@nuaa.edu.cn

  • 中图分类号: V231.2+2

Effect of inlet temperatures on pulse detonation combustion characteristics

  • 摘要:

    为了获得进气温度对脉冲爆震燃烧特性影响规律,结合试验和理论分析的方法,在爆震点火频率为15~25 Hz、进气温度为300~450 K条件下,对爆震管内燃烧状态、沿程峰值压力、压力波及火焰传播速度进行了研究。研究结果表明:从试验和理论分析结果来看,峰值压力与进气温度呈现反比趋势;进气温度在300 K时,整体火焰传播速度较低,在350 K和400 K最快达到2000 m/s,但400 K无法维持2000 m/s的火焰传播速度。提高进气温度对脉冲爆震燃烧的循环起爆性能具有较大影响,具体表现为在300 K进气温度下,15、20 Hz和25 Hz都能实现稳定起爆,而进气温度提高到350 K以后,15 Hz能稳定起爆,20 Hz出现掉帧现象,而25 Hz只能进行连续燃烧。综合来看,进气温度提高,会降低爆震峰值压力,显著提高连续燃烧概率。

     

  • 图 1  爆震燃烧室结构(单位:mm)

    Figure 1.  Detonation combustion chamber structure (unit:mm)

    图 2  试验系统

    Figure 2.  Experimental system

    图 3  离子探针

    Figure 3.  Ion probe measurement circuit

    图 4  单周期火焰信号

    Figure 4.  Single-cycle flame signal

    图 5  3种燃烧状态火焰信号

    Figure 5.  Flame signals of three combustion states

    图 6  不同进气温度下15 Hz点火频率压力时序图

    Figure 6.  Different inlet temperature 15 Hz ignition frequency pressure sequence diagram

    图 7  压力时序图

    Figure 7.  Pressure time series diagram

    图 8  峰值压力变化

    Figure 8.  Peak pressure change

    图 9  火焰传播速度变化

    Figure 9.  Change of flame propagation velocity

    图 10  火焰信号时序图

    Figure 10.  Flame signal timing diagram

    图 11  爆震波ZND模型

    Figure 11.  Detonation wave ZND model

    图 12  一维爆震燃烧模型[31]

    Figure 12.  One-dimensional detonation combustion model[31]

    图 13  峰值压力随进气温度变化

    Figure 13.  Variation of peak pressure with inlet temperature

    图 14  不同进气温度下火焰持续时间

    Figure 14.  Flame duration of each inlet temperature

    表  1  主要性能参数

    Table  1.   Main technical parameters

    参数 数值
    压力测量范围/kPa 3450
    灵敏度/(mV/kPa) 1.45
    采样频率/kHz ≥500
    反应时间/µs ≤1.0
    反应频率/Hz 0.01
    温度范围/K 200~408
    下载: 导出CSV

    表  2  试验工况

    Table  2.   Experimental conditions

    进气温度T1/K 点火频率/Hz
    300 15
    350 15
    400 15
    450 15
    300 20
    350 20
    300 25
    350 25
    下载: 导出CSV

    表  3  试验设备精度

    Table  3.   Precision of experimental equipment

    测量设备 范围 精度/%
    压力传感器 (压力) 0.014~3450 kPa ±0.1
    压力传感器 (时间) 0~500 kHz ±0.005
    离子探针 −10~10 V ±0.005
    下载: 导出CSV

    表  4  物理量不确定度

    Table  4.   Uncertainty of physical quantity

    物理量 不确定度/%
    压力p/MPa 1.0
    火焰传播速度vf /(m/s) 0.7
    火焰持续时间tfire/ms 0.7
    下载: 导出CSV

    表  5  CJ爆震波压力

    Table  5.   CJ detonation wave pressure

    T1/K CJ爆震波压力/MPa
    300 1.95
    350 1.67
    400 1.46
    450 1.30
    下载: 导出CSV

    表  6  计算结果

    Table  6.   Calculation results

    T1/K vCJ/(m/s)
    式(5) CEA
    300 1853 1963
    350 1874 1858
    400 1894 1852
    450 1914 1847
    下载: 导出CSV
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  • 收稿日期:  2023-12-27
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