开口型管道内瓦斯爆炸冲击波动压的数值模拟

洪溢都; 林柏泉; 朱传杰

doi:10.11883/1001-1455(2016)02-0198-12

开口型管道内瓦斯爆炸冲击波动压的数值模拟

doi: 10.11883/1001-1455(2016)02-0198-12

中国矿业大学安全工程学院煤炭资源与安全开采国家重点实验室, 江苏徐州 221116

基金项目:

国家自然科学基金项目 51204174

中央高校基本科研业务费专项项目 2012QNB01

详细信息

作者简介:
洪溢都(1989—)，男，博士研究生，hongyidu@163.com

中图分类号: O383
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出版历程
- 收稿日期: 2014-08-18
- 修回日期: 2014-10-24
- 刊出日期: 2016-03-25

Simulation on dynamic pressure of premixed methane/air explosion in open-end pipes

State Key Laboratory of Coal Resources and Safe Mining, Faculty of Safety Engineering, China University of Mining and Technology, Xuzhou 221116, Jiangsu, China

摘要

摘要: 为了研究瓦斯爆炸冲击波的动压演化规律，利用数值模拟软件模拟开口型管道内的爆炸。结果表明：动压与流速在时间上存在较好的对应关系，基本同时出现正向和反向的峰值；动压在3个方向上不仅伴随传播距离的增大而不断增大，也伴随传播时间的延长而增大；沿管道方向(火焰传播方向)上的最大动压值是其他2个方向(管道径向)上的数千倍；相比爆炸超压而言，管道径向上的动压对爆炸破坏效应的影响较小，而沿管道方向上的动压造成的破坏效应不能忽视；验证了动压与流速的平方呈正比关系，同时通过分析给出了动压基于管道几何尺寸和流速的经验公式。
- 爆炸力学 /
- 动压 /
- 管道尺寸 /
- 瓦斯爆炸 /
- 开口型管道 /
- 流速
Abstract: In order to study the evolution of dynamic overpressure of deflagration, a simulation was carried out in an open end pipe. It was found that the dynamic pressure was closely correlated with the gas velocity so that they always arrive at the peak value at the same time. In addition, the first positive peak of the dynamic pressure was almost several times greater than that of the second. This may indicate that the blast wave has a greater influence on the dynamic pressure than the flame does. An empirical prediction equation was given to calculate the first and second positive peaks based on the propagation time. Maximum dynamic pressures were increased with the propagation distance in all the three directions (x, y and z), and so was with time. The maximum dynamic pressure value in the x direction was almost several thousand times greater than those in the other two directions. Compared with the explosive overpressure, the influence on the explosive damage by the dynamic pressure in the y and z direction was quite small. Three empirical formulas were given to calculate the maximum dynamic pressures in different directions. The relationship between the dynamic pressure and the square of the gas velocity was verified. An empirical formula of the dynamic overpressure was also given based on the length-diameter ratio and the gas velocity. The results may provide a reference for the study on the gas explosion in the limited spaces.
- mechanics of explosion /
- dynamic pressure /
- pipe size /
- methane/air explosion /
- open-end pipes /
- gas velocity

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图 1 实验管道示意图

Figure 1. Schematic of the experimental pipe

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图 2 爆炸超压数值模拟与实验结果对比

Figure 2. Comparison of explosion overpressure between simulation and experiment

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3a 0.5 m处动压与流速的时间对应关系

3a. Relationship between dynamic pressure and gas velocity at the point of 0.5 m

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3b 2.5 m处动压与流速的时间对应关系

3b. Relationship between dynamic pressure and gas velocity at the point of 2.5 m

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3c 4.5 m处动压与流速的时间对应关系

3c. Relationship between dynamic pressure and gas velocity at the point of 4.5 m

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3d 6.5 m处动压与流速的时间对应关系

3d. Relationship between dynamic pressure and gas velocity at the point of 6.5 m

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3e 8.5 m处动压与流速的时间对应关系

3e. Relationship between dynamic pressure and gas velocity at the point of 8.5 m

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3f 10.5 m处动压与流速的时间对应关系

3f. Relationship between dynamic pressure and gas velocity at the point of 10.5 m

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3g 12.5 m处动压与流速的时间对应关系

3g. Relationship between dynamic pressure and gas velocity at the point of 12.5 m

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3h 14.5 m处动压与流速的时间对应关系

3h. Relationship between dynamic pressure and gas velocity at the point of 14.5 m

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3i 16.5 m处动压与流速的时间对应关系

3i. Relationship between dynamic pressure and gas velocity at the point of 16.5 m

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3j 18.5 m处动压与流速的时间对应关系

3j. Relationship between dynamic pressure and gas velocity at the point of 18.5 m

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图 4 动压的正向峰值与传播距离的关系

Figure 4. Relationship between dynamic pressure peak and propagation distance

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5a 动压在x方向随时间的变化规律

5a. Dynamic pressure in x direction varying with time

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5b 动压在y方向随时间的变化规律

5b. Dynamic pressure in y direction varying with time

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5c 动压在z方向随时间的变化规律

5c. Dynamic pressure in z direction varying with time

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6a 在管道尺寸L/a=16.7时动压与流速的定量关系

6a. Relationship between dynamic pressure and gas velocity behind the shock wave in the pipe with a geometrical size L/a=16.7

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6b 在管道尺寸L/a=25时动压与流速的定量关系

6b. Relationship between dynamic pressure and gas velocity behind the shock wave in the pipe with a geometrical size L/a=25

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6c 在管道尺寸L/a=33.3时动压与流速的定量关系

6c. Relationship between dynamic pressure and gas velocity behind the shock wave in the pipe with a geometrical size L/a=33.3

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6d 在管道尺寸L/a=50时动压与流速的定量关系

6d. Relationship between dynamic pressure and gas velocity behind the shock wave in the pipe with a geometrical size L/a=50

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6e 在管道尺寸L/a=50时动压与流速的定量关系

6e. Relationship between dynamic pressure and gas velocity behind the shock wave in the pipe with a geometrical size L/a=50

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6f 在管道尺寸L/a=62.5时动压与流速的定量关系

6f. Relationship between dynamic pressure and gas velocity behind the shock wave in the pipe with a geometrical size L/a=62.5

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6g 在管道尺寸L/a=66.7时动压与流速的定量关系

6g. Relationship between dynamic pressure and gas velocity behind the shock wave in the pipe with a geometrical size L/a=66.7

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6h 在管道尺寸L/a=75时动压与流速的定量关系

6h. Relationship between dynamic pressure and gas velocity behind the shock wave in the pipe with a geometrical size L/a=75

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6i 在管道尺寸L/a=100时动压与流速的定量关系

6i. Relationship between dynamic pressure and gas velocity behind the shock wave in the pipe with a geometrical size L/a=100

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6j 在管道尺寸L/a=125时动压与流速的定量关系

6j. Relationship between dynamic pressure and gas velocity behind the shock wave in the pipe with a geometrical size L/a=125

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6k 在管道尺寸L/a=187.5时动压与流速的定量关系

6k. Relationship between dynamic pressure and gas velocity behind the shock wave in the pipe with a geometrical size L/a=187.5

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6l 在管道尺寸L/a=250时动压与流速的定量关系

6l. Relationship between dynamic pressure and gas velocity behind the shock wave in the pipe with a geometrical size L/a=250

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7a 偏差曲线方程中二次项系数与管道尺寸拟合关系

7a. Relationship between quadratic coefficient and pipe size

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7b 偏差曲线方程中一次项系数与管道尺寸拟合关系

7b. Relationship between monomial coefficient and pipe size

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7c 偏差曲线方程中常数项与管道尺寸拟合关系

7c. Relationship between constant and pipe size

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表 1 不同网格划分方法下的数值模拟结果与实验结果对比

Table 1. Comparison between experimental data and simulation results by different methods of grid partitioning

测点	p/kPa		ε/%	p/kPa		ε/%
测点	数值模拟(4 cm×4 cm×4 cm)	实验	ε/%	数值模拟(2 cm×2 cm×2 cm)	实验	ε/%
2	213.2	196.5	8.05	202.8	196.5	-3.23
6	199.4	179.2	11.31	186.4	179.2	-3.99
10	141.5	120.6	17.36	110.5	120.6	8.35

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