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爆轰管内氢氧爆炸过程与碳-铁纳米材料生长研究

赵铁军 刘翼 吴永翔 闫鸿浩 吴林松

方厚林, 卢强, 郭权势, 李国亮, 刘存旭, 陶思昊, 张德志. 水下爆炸冲击波和气泡行为自由面效应的实验研究[J]. 爆炸与冲击, 2024, 44(8): 081444. doi: 10.11883/bzycj-2024-0003
引用本文: 赵铁军, 刘翼, 吴永翔, 闫鸿浩, 吴林松. 爆轰管内氢氧爆炸过程与碳-铁纳米材料生长研究[J]. 爆炸与冲击, 2024, 44(11): 112101. doi: 10.11883/bzycj-2023-0404
FANG Houlin, LU Qiang, GUO Quanshi, LI Guoliang, LIU Cunxu, TAO Sihao, ZHANG Dezhi. Experimental research on the free surface effect of shock wave and bubble behavior of small yield underwater explosion[J]. Explosion And Shock Waves, 2024, 44(8): 081444. doi: 10.11883/bzycj-2024-0003
Citation: ZHAO Tiejun, LIU Yi, WU Yongxiang, YAN Honghao, WU Linsong. Study on hydrogen-oxygen detonation process and the growth of carbon-iron nanomaterials in a detonation tube[J]. Explosion And Shock Waves, 2024, 44(11): 112101. doi: 10.11883/bzycj-2023-0404

爆轰管内氢氧爆炸过程与碳-铁纳米材料生长研究

doi: 10.11883/bzycj-2023-0404
基金项目: 国家自然科学基金(11672068, 12172084);河南省自然科学基金(232300420341);河南省科技攻关项目(242102230015)
详细信息
    作者简介:

    赵铁军(1990- ),男,博士,讲师,tiejun_zhao@henu.edu.cn

    通讯作者:

    闫鸿浩(1974- ),男,博士,教授,yanhh@dlut.edu.cn

  • 中图分类号: O389

Study on hydrogen-oxygen detonation process and the growth of carbon-iron nanomaterials in a detonation tube

  • 摘要: 为研究气相爆轰合成碳-铁纳米材料的爆炸过程,采用氢氧爆炸试验与数值模拟相结合的方式研究了不同氢氧摩尔比(2∶1、3∶1和4∶1)对爆轰参数(爆速、爆温、爆压)峰值时程曲线与碳-铁纳米材料形貌的影响。研究表明:爆轰管内氢氧爆炸包括爆轰波的传播与燃烧波的衰减2个过程,且氢氧摩尔比对爆速、爆温、爆压的峰值时程曲线影响十分显著。随着氢氧摩尔比的提高,爆轰波的爆速、爆温、爆压及其衰减速率均呈减小趋势。氢氧摩尔比通过影响爆轰波的传播与衰减而作用于碳-铁纳米材料形貌的生长。零氧平衡时,样品为碳包铁纳米颗粒,随着氢氧摩尔比的提高,样品中碳纳米管的数量逐渐增多。调整氢氧摩尔比可实现对爆轰波传播与衰减过程的控制,达到气相爆轰控制性制备特定形貌的碳-铁纳米材料的目的。
  • 图  1  气体爆炸合成碳-铁纳米材料所用爆轰管示意图

    Figure  1.  Schematic diagram of the detonation tube used in the synthesis of carbon-iron nanomaterials by gas explosion

    图  2  密闭管道的几何模型

    Figure  2.  Geometry of a closed tube

    图  3  几何模型的网格划分

    Figure  3.  Meshing of geometry

    图  4  氢氧摩尔比为2∶1条件下网格尺寸对速度时程曲线的影响

    Figure  4.  Effect of mesh size on the time-history curves of velocity when the molar ratio of hydrogen to oxygen is 2∶1

    图  5  工况1下爆轰波的传播衰减高速摄影图像与爆速时程曲线

    Figure  5.  Propagation attenuation of the detonation wave, the high-speed photographic image and the time history curve of the detonation velocity under the working condition 1

    图  6  不同时刻速度峰值的速度云图

    Figure  6.  Velocity contours of peak values at different times

    图  7  不同工况下观测点速度、温度和压强的峰值时程曲线

    Figure  7.  Velocity, temperature and pressure history curves at observation points under different working conditions

    图  8  不同工况下样品的 TEM 图像

    Figure  8.  TEM images of the samples under different working conditions

    图  9  不同工况下爆轰波传播到管道中心位置的时间

    Figure  9.  Time required for the detonation wave to propagate to the center of the tube under different working conditions

    表  1  不同网格尺寸的网格数量及其爆速和误差

    Table  1.   The numbers of meshes with different mesh sizes and their detonation velocities and errors

    最大网格尺寸/mm网格数量爆速/(m∙s−1误差/%
    1.0104 492197210.36
    2.027 596187614.73
    2.517 676182017.27
     注:爆速为爆轰波第1次经过观测点时的速度。
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出版历程
  • 收稿日期:  2023-11-10
  • 修回日期:  2023-12-04
  • 网络出版日期:  2024-03-26
  • 刊出日期:  2024-11-15

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