N2双流体细水雾抑制管道瓦斯爆炸实验研究

余明高 杨勇 裴蓓 牛攀 朱新娜

余明高, 杨勇, 裴蓓, 牛攀, 朱新娜. N2双流体细水雾抑制管道瓦斯爆炸实验研究[J]. 爆炸与冲击, 2017, 37(2): 194-200. doi: 10.11883/1001-1455(2017)02-0194-07
引用本文: 余明高, 杨勇, 裴蓓, 牛攀, 朱新娜. N2双流体细水雾抑制管道瓦斯爆炸实验研究[J]. 爆炸与冲击, 2017, 37(2): 194-200. doi: 10.11883/1001-1455(2017)02-0194-07
Yu Minggao, Yang Yong, Pei Bei, Niu Pan, Zhu Xinna. Experimental study of methane explosion suppression by nitrogen twin-fluid water mist[J]. Explosion And Shock Waves, 2017, 37(2): 194-200. doi: 10.11883/1001-1455(2017)02-0194-07
Citation: Yu Minggao, Yang Yong, Pei Bei, Niu Pan, Zhu Xinna. Experimental study of methane explosion suppression by nitrogen twin-fluid water mist[J]. Explosion And Shock Waves, 2017, 37(2): 194-200. doi: 10.11883/1001-1455(2017)02-0194-07

N2双流体细水雾抑制管道瓦斯爆炸实验研究

doi: 10.11883/1001-1455(2017)02-0194-07
基金项目: 

国家自然科学基金项目 U1361205

国家自然科学基金项目 50974055

国家自然科学基金项目 51604095

河南省教育厅基础研究计划项目 14A620001

河南省科技厅基础与前沿基金项目 152300410100

详细信息
    作者简介:

    余明高(1963-),男,教授,博士生导师

    通讯作者:

    裴蓓, pb128@hpu.edu.cn

  • 中图分类号: O389

Experimental study of methane explosion suppression by nitrogen twin-fluid water mist

  • 摘要: 为了在较低压力下获得较小粒径的细水雾,降低喷雾抑爆系统的运行成本,提高系统的适用性和抑爆效率,自行搭建了尺寸为120 mm×120 mm×840 mm的透明有机玻璃瓦斯爆炸管道实验平台。采用双流体喷嘴将N2和细水雾送入试验管道,通过调节喷雾压力和喷雾时间开展了双流体细水雾抑制瓦斯爆炸实验研究,从火焰速度、瓦斯爆炸超压2个方面探讨双流体细水雾的抑爆有效性。实验结果表明:N2双流体细水雾抑爆效果明显,可以减小瓦斯爆炸强度;随着喷雾时间的延长,爆炸火焰的速度峰值逐渐下降,爆炸超压峰值逐渐下降,平均升压速率逐渐降低;当N2压力为0.4 MPa、喷雾时间为3 s时,速度峰值比不喷雾时下降60.39%,爆炸超压峰值下降37.76%。
  • 图  1  实验系统图

    Figure  1.  Experimental stytem

    图  2  相同时刻火焰锋面位置对比图

    Figure  2.  Comparison of flame front position at the same moment

    图  3  N2双流体细水雾火焰传播速度

    Figure  3.  Flame propagation velocity with N2 twin-fluid

    图  4  N2双流体细水雾火焰速度峰值

    Figure  4.  Peak velocity of flame with N2 twin-fluid

    图  5  N2双流体细水雾压力曲线

    Figure  5.  Pressure curve with N2 twin-fluid

    图  6  N2双流体细水雾爆炸超压峰值

    Figure  6.  Peak explosion pressure with N2 twin-fluid

    表  1  不同压力不同喷雾时间下速度峰值的下降比例

    Table  1.   Decline proportion of the peak velocity under different pressure and at different times

    工况 速度峰值/ (m·s-1) 下降比例/ %
    N2-0.2 MPa-1 s 14.10 17.01
    N2-0.2 MPa-2 s 13.18 22.43
    N2-0.2 MPa-3 s 11.73 30.96
    N2-0.3 MPa-1 s 14.04 17.36
    N2-0.3 MPa-2 s 12.25 27.90
    N2-0.3 MPa-3 s 7.27 57.20
    N2-0.4 MPa-1 s 13.96 17.83
    N2-0.4 MPa-2 s 11.78 30.66
    N2-0.4 MPa-3 s 6.73 60.39
    下载: 导出CSV

    表  2  不同压力不同喷雾时间下超压峰值的下降比例

    Table  2.   Decline proportion of the peak overpressure under different pressure and at different times

    工况 超压峰值/ (104 Pa) 下降比例/ %
    N2-0.2 MPa-1 s 2.978 2 6.68
    N2-0.2 MPa-2 s 2.792 2 12.51
    N2-0.2 MPa-3 s 2.179 3 31.72
    N2-0.3 MPa-1 s 2.917 2 8.59
    N2-0.3 MPa-2 s 2.776 8 12.99
    N2-0.3 MPa-3 s 1.996 3 37.45
    N2-0.4 MPa-1 s 2.814 5 11.81
    N2-0.4 MPa-2 s 2.202 9 30.98
    N2-0.4 MPa-3 s 1.986 4 37.76
    下载: 导出CSV

    表  3  不同压力不同喷雾时间下平均升压速率

    Table  3.   Average pressure rise rate under different pressure and at different times

    工况 平均升压速率/(kPa·s-1)
    N2-0.2 MPa-1 s 495
    N2-0.2 MPa-2s 400
    N2-0.2 MPa-3s 235
    N2-0.3 MPa-1 s 402
    N2-0.3 MPa-2 s 327
    N2-0.3 MPa-3 s 218
    N2-0.4 MPa-1 s 335
    N2-0.4 MPa-2 s 248
    N2-0.4 MPa-3 s 181
    下载: 导出CSV
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出版历程
  • 收稿日期:  2015-08-14
  • 修回日期:  2015-11-03
  • 刊出日期:  2017-03-25

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