Page 160 - 《爆炸与冲击》2023年第2期
P. 160

第 43 卷    第 2 期                   爆    炸    与    冲    击                       Vol. 43, No. 2
                2023 年 2 月                    EXPLOSION AND SHOCK WAVES                          Feb., 2023

               DOI:10.11883/bzycj-2022-0174


                    破膜压力对氢-空气预混气体燃爆特性的影响                                                            *


                                          杜赛枫 ,张    凯 ,陈    昊 ,郭    进 ,段在鹏    2
                                                        1
                                                               1
                                                                       1
                                                1
                                       (1. 福州大学环境与安全工程学院,福建 福州 350116;
                                          2. 福州大学经济与管理学院,福建 福州 350116)
                  摘要: 利用自主设计的         5.00 m  长矩形管道,对氢气体积分数为         30%  的氢气-空气预混气体进行了不同破膜压力
               (p v )下的系列燃爆实验,重点研究了        p v 对管道内外火焰传播行为及爆炸超压的影响。实验结果表明:管道内的火焰传
               播行为受   p v 影响显著。在靠近泄爆口的压力传感器所监测的压力-时间曲线上,可以观察到                            3  个压力峰值(p b 、p out 、
               p ext ),分别对应于铝膜破裂、燃烧混合物泄放以及外部爆炸,大多数情况下,p b 为最大压力峰值。管道内部最大超压随
               着  p v 升高而增大,但最大内部超压出现的位置受            p v 的影响。管道外部火焰传播行为与           p v 有关,但不同  p v 下外部火焰
               的最大长度无明显差异。最大外部超压与               p v 之间呈现非单调变化规律。
                  关键词: 氢气;破膜压力;火焰传播;爆炸超压;外部爆炸
                  中图分类号: O382.1   国标学科代码: 1303520   文献标志码: A

                          Effects of vent burst pressure on explosion characteristics
                                          of premixed hydrogen-air gases

                                                      1
                                          1
                                                                 1
                                                                          1
                                DU Saifeng , ZHANG Kai , CHEN Hao , GUO Jin , DUAN Zaipeng 2
                       (1. College of Environment and Safety Engineering, Fuzhou University, Fuzhou 350116, Fujian, China;
                           2. School of Economics and Management, Fuzhou University, Fuzhou 350116, Fujian, China)
               Abstract:  By using a self-designed 5.00-m-long duct with a cross-section of 0.30 m × 0.30 m, a seris of experiments were
               performed on premixed hydrogen-air gases in which volume fraction of hydrogen was 30%. And the effects of vent burst
               pressure (p ) on the flame propagation and pressure-time histories in the duct were experimentally iveatigated. The explosion
                       v
               flames were recorded by a high-speed camera at a frequency of 2.5 kHz. Five piezoelectric pressure transducers were employed
               to record the internal and external overpressure. The duct had been evacuated using a vacuum pump before the experiment, and
               the premixed hydrogen-air gases with volume fraction of 30% was prepared according to Dalton’s law of partial pressure. The
               variation of the vent burst pressure was achieved by changing the thickness of the aluminum foil which was used as vent cover.
               The results show that the first three stages of the flame structure in the duct are hemispherical, finger-shaped and tulip flame,
               respectively. p  has a significant effect on the structure of tulip flame and its subsequent development. Three pressure peaks (p , b
                         v
               p ,  p )  can  be  distinguished  from  the  pressure-time  histories  monitored  by  the  pressure  transducer  near  the  vent,
               out
                   ext
               corresponding  to  three  different  generation  mechanisms:  burst  of  the  aluminum  film,  venting  of  burned  mixtures,  and  the
               external explosion, respectively. The three pressure peaks increase with an increase in p . p is the dominant pressure peak in
                                                                               v  b
               most  cases.  The  maximum  internal  overpressure  increases  as  p   increases,  and  the  position  where  the  maximum  internal
                                                              v
               overpressure was measured depended on p . The maximum internal overpressure was obtained at the center of the duct (PT2)
                                              v
               when p ≤42 kPa, but near the open end of the duct (PT3) if p >42 kPa. When the flame reached the vent, it ejected from the
                    v
                                                            v
                 *  收稿日期: 2022-04-24;修回日期: 2022-10-11
                   基金项目: 国家社会科学基金(17CGL049)
                   第一作者: 杜赛枫(1997- ),男,硕士研究生,1095290649@qq.com
                   通信作者: 段在鹏(1985- ),男,博士,副教授,duanzaipeng@163.com


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