掺氢比对甲烷-氧气爆轰特性的影响

倪靖 潘剑锋 姜超 陈祥 张顺

倪靖, 潘剑锋, 姜超, 陈祥, 张顺. 掺氢比对甲烷-氧气爆轰特性的影响[J]. 爆炸与冲击, 2020, 40(4): 042102. doi: 10.11883/bzycj-2019-0237
引用本文: 倪靖, 潘剑锋, 姜超, 陈祥, 张顺. 掺氢比对甲烷-氧气爆轰特性的影响[J]. 爆炸与冲击, 2020, 40(4): 042102. doi: 10.11883/bzycj-2019-0237
NI Jing, PAN Jianfeng, JIANG Chao, CHEN Xiang, ZHANG Shun. Effects of hydrogen-blending ratio on detonation characteristics of premixed methane-oxygen gas[J]. Explosion And Shock Waves, 2020, 40(4): 042102. doi: 10.11883/bzycj-2019-0237
Citation: NI Jing, PAN Jianfeng, JIANG Chao, CHEN Xiang, ZHANG Shun. Effects of hydrogen-blending ratio on detonation characteristics of premixed methane-oxygen gas[J]. Explosion And Shock Waves, 2020, 40(4): 042102. doi: 10.11883/bzycj-2019-0237

掺氢比对甲烷-氧气爆轰特性的影响

doi: 10.11883/bzycj-2019-0237
基金项目: 国家自然科学基金(91641113)
详细信息
    作者简介:

    倪 靖(1996- ),男,硕士研究生,a1437407300@163.com

    通讯作者:

    潘剑锋(1978- ),男,博士,教授,mike@ujs.edu.cn

  • 中图分类号: O382

Effects of hydrogen-blending ratio on detonation characteristics of premixed methane-oxygen gas

  • 摘要: 含氢多组分燃料由于其优良的燃烧特性逐渐成为研究关注的重点。为了对掺氢燃料的爆轰特性作进一步的研究,设计了长3 000 mm、管径30 mm的圆柱形半封闭燃烧室,对不同初压下的CH4-2O2、6CH4-H2-12.5O2、3CH4-H2-6.5O2(掺氢比分别为0%、5.1%、9.5%)3种预混合气的爆轰特性进行了实验研究,并采用烟熏膜、离子探针和压力传感器分别探测胞格结构、火焰位置和内部压力。结果表明,甲烷/氧气掺氢后可以有效提高爆轰波的传播速度,且掺氢浓度越高,传播速度越快;同时,氢气的掺入可减少管道出口处的速度亏损并在初始压力较低时加速火焰和激波的耦合,降低胞格尺寸,提高爆轰敏感性。
  • 图  1  实验系统

    Figure  1.  Experimental system

    图  2  点火系统等效R-L-C电路[17]

    Figure  2.  An equivalent R-L-C circuit of the ignition system[17]

    图  3  CH4-2O2激波与火焰的相互作用过程

    Figure  3.  Time evolution of shock-flame interaction for CH4-2O2

    图  4  6CH4-H2-12.5O2激波与火焰的相互作用过程

    Figure  4.  Time evolution of shock-flame interaction for 6CH4-H2-12.5O2

    图  5  3CH4-H2-6.5O2激波与火焰的相互作用过程

    Figure  5.  Time evolution of shock-flame interaction for 3CH4-H2-6.5O2

    图  6  不同初压下管道中各点火焰速度与CJ速度的比值

    Figure  6.  Ratios of flame velocity to CJ velocity at each point in the pipeline under different initial pressures

    图  7  不同掺氢比下爆轰波稳定传播平均速度随初压的变化

    Figure  7.  Average velocity of steady propagation of detonation wave varying with initial pressure at different hydrogen-blending ratios

    图  8  不同掺氢比、不同初始压力下管道中各点压力峰值的分布情况

    Figure  8.  Distribution of the pressure peak at each point in the pipeline under different hydrogen-blending ratios and different initial pressures

    图  9  初始压力为20.0 kPa时3种气体的胞格结构

    Figure  9.  Cellular structures of three gases at the initial pressure of 20.0 kPa

    图  10  初始压力为30.0 kPa时3种气体的胞格结构

    Figure  10.  Cellular structures of three gases at the initial pressure of 30.0 kPa

    图  11  初始压力为40.0 kPa时3种气体的胞格结构

    Figure  11.  Cellular structures of three gases at the initial pressure of 40.0 kPa

    图  12  不同掺氢比下胞格尺寸随初始压力的变化

    Figure  12.  Change of cell size with initial pressure at different hydrogen-blending ratios

    表  1  实验气体组分

    Table  1.   Experimental gas compositions

    气体编号气体配比氢气摩尔分数/%
    #1CH4-2O20
    #26CH4-H2-12.5O25.1
    #33CH4-H2-6.5O29.5
    下载: 导出CSV

    表  2  爆轰胞格尺寸$\lambda $与初始压力p0之间的拟合关系参数

    Table  2.   Parameters for fitting relationship between detonation cell size λ and initial pressure p0

    掺氢比/%C/mmb
    0688.229 571.149 81
    5.1515.502 931.096 92
    9.5977.119 241.347 64
    下载: 导出CSV
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出版历程
  • 收稿日期:  2019-06-13
  • 修回日期:  2019-09-30
  • 刊出日期:  2020-04-01

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