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天然气掺氢在管道流动中的氢浓度分布

安永伟, 孙晨, 冀守虎等. 天然气掺氢在管道流动中的氢浓度分布. 力学与实践, 2022, 44(4): 767-775. doi: 10.6052/1000-0879-22-381
引用本文: 安永伟, 孙晨, 冀守虎等. 天然气掺氢在管道流动中的氢浓度分布. 力学与实践, 2022, 44(4): 767-775. doi: 10.6052/1000-0879-22-381
An Yongwei, Sun Chen, Ji Shouhu, et al. Hydrogen concentration distribution in flow of hydrogen blended to natural gas in pipeline. Mechanics in Engineering, 2022, 44(4): 767-775. doi: 10.6052/1000-0879-22-381
Citation: An Yongwei, Sun Chen, Ji Shouhu, et al. Hydrogen concentration distribution in flow of hydrogen blended to natural gas in pipeline. Mechanics in Engineering, 2022, 44(4): 767-775 . doi: 10.6052/1000-0879-22-381

天然气掺氢在管道流动中的氢浓度分布

  • 基金项目:
    中国博士后科学基金(2021M701096), 北京高校卓越青年科学家计划(BJJWZYJH01201910006021), 国家自然科学基金(51875012), 河南省科技攻关(222102220090)资助项目。
详细信息
    作者简介:

    许未晴,副研究员,主要从事氢气产—储—运过程的热物理特性、测量控制及能量转化方面的研究工作。E-mail: weiqing.xu@buaa.edu.cn

    ;

    刘伟,高级工程师,主要从事氢能源高效输送与利用关键技术研究。E-mail: liuwei@spic.com.cn

  • 中图分类号: TK91

HYDROGEN CONCENTRATION DISTRIBUTION IN FLOW OF HYDROGEN BLENDED TO NATURAL GAS IN PIPELINE

  • 天然气掺氢是解决氢气产地与使用地不匹配,进而实现氢气大规模、远距离输送的主要方法。由于氢气的存在会导致在役天然气管道出现氢脆引起安全事故。所以,研究天然气掺氢管路中氢气组分、速度、聚集的规律分析十分必要。本文选用天然气和氢气两种工质,构建T型掺混管路模型和变径管路模型;并基于Fluent软件对T型掺混管路和10种变径掺混管路进行数值模拟研究。结果表明,对于T型掺混管路,在管长是管径35倍处内依然有明显分层,宽度占据1/3管径。对于变径掺混管路,发现变径越靠近掺混中心、直径越窄、高度越低越容易发生氢气富集,氢气摩尔分数最高达到50%~60%,易引起管道的氢脆。研究结果可对天然气掺氢在管道中流动的氢浓度分布和管道变径选取提供参考。

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  • 图 1  掺混管路基本模型

    Figure 1.  Basic model of blending pipeline

    图 2  掺混管路变径模型

    Figure 2.  Variable diameter model of blending pipeline

    图 3  T型掺混模型网格

    Figure 3.  Grid of T-type blending model

    图 4  变径模型网格

    Figure 4.  Grid of variable diameter model

    图 5  气体掺混后速度云图

    Figure 5.  Velocity distribution after gas blending

    图 6  气体掺混后天然气组分摩尔分数云图

    Figure 6.  Mole fraction distribution of natural gas component after gas blending

    图 7  气体掺混后氢气组分摩尔分数云图

    Figure 7.  Mole fraction distribution of hydrogen component after gas blending

    图 8  T型管路掺混后天然气摩尔分数

    Figure 8.  Percentage distribution of natural gas component with T-type pipeline after gas blending

    图 9  T型管路掺混后氢气摩尔分数

    Figure 9.  Percentage distribution of hydrogen component with T-type pipeline after gas blending

    图 10  气体掺混后速度云图

    Figure 10.  Velocity distribution after gas blending

    图 11  气体掺混后天然气组分摩尔分数云图

    Figure 11.  Mole fraction distribution of natural gas component after gas blending

    图 12  气体掺混后氢气组分摩尔分数云图

    Figure 12.  Mole fraction distribution of hydrogen component after gas blending

    图 13  掺混后天然气摩尔分数

    Figure 13.  Percentage distribution of natural gas component after gas blending

    图 14  掺混后氢气摩尔分数

    Figure 14.  Percentage distribution of hydrogen component after gas blending

    表 1  网格无关性说明

    Table 1.  Grid independence specification

    Type Grid feature Number of nodes Number of elements Number of iterations Hydrogen mole fraction at outlet/%
    T-type model sparse 51679 255311 300 4.56
    moderate 99004 510457 268 4.68
    dense 186225 991794 537 4.91
    variable diameter model sparse 52755 260047 318 4.79
    moderate 101075 519109 260 4.76
    dense 189815 1007159 532 4.79
    下载: 导出CSV

    表 2  变径掺混管路几何参数及结果

    Table 2.  Geometric parameters and results of variable diameter type blending pipeline

    NO. s/mm D/mm l/mm x(H2)/%
    1 900 160 100 40~50
    2 1000 160 100 25~30
    3 2000 160 100 25~30
    4 3000 160 100 15~20
    5 3500 160 100 10~15
    6 900 160 200 25~40
    7 900 160 50 45~55
    8 900 240 100 20~40
    9 900 120 100 50~55
    10 900 120 50 50~60
    下载: 导出CSV
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出版历程
收稿日期:  2022-06-27
录用日期:  2022-07-05
刊出日期:  2022-08-08

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