摘要
为探究气粉两相混合体系泄爆特性变化规律,以甲烷-硝酸铵为实验介质,利用自行搭建的不锈钢火焰加速管道开展了泄爆口不同静态动作压力(p_(st))的燃爆实验,着重研究了p_(st)对气粉两相燃爆压力、火焰传播速度和泄爆火焰形态的影响规律。p_(st)由泄爆口阻塞比(θ)和泄爆膜层数(n)决定,θ和n增大的共同作用使p_(st)升高。p_(st)升高将增强管道对气粉和反应产物冲出管外的约束,增大管内流体的黏滞效应,促进管内气粉两相反应,降低未燃气在管外二次爆炸的强度。对爆燃压力进行分析,发现p_(st)从2.97 kPa升高至14.64 kPa时,爆燃压力时程曲线呈含维稳平台的双峰结构。第一压力峰值从5.48 kPa增大至10.20 kPa,维稳时间从6 ms延长至25 ms,第二压力峰值从23.03 kPa减小至9.71 kPa;p_(st)为16.08和24.12 kPa时,破膜前压力多次叠加反射,致使泄爆膜压力时程曲线呈特殊振荡上升的三峰结构。对火焰传播速度进行分析,发现p_(st)升高使火焰的平均传播速度从161.33 m/s降低至67.99 m/s。对泄爆火焰进行分析,发现当n=2时,θ增大将使泄爆火焰结构由簇状转变为射流状;θ=88.9%时,泄爆火焰呈典型的射流状。θ增大和n增大均使火焰亮度逐渐降低,火焰发光区长度减小,破膜至火焰出现时间间隔和火焰持续时间延长。
To investigate the variation law of the blasting characteristics of the gas-powder two-phase mixed system,blast experiments with different outlet static action pressures(p_(st))were carried out in a self-built stainless steel flame acceleration pipeline,and the variation law of p_(st)on two-phase blasting pressure,flame propagation velocity,and blasting flame morphology was emphatically studied.p_(st)is determined by the blasting hole blocking ratio(θ)and the number of blasting film layers(n).The increase ofθand n together increases p_(st).The increase of p_(st)strengthens the constraint of gas powder and reaction products flowing out of the pipe,increases the viscosity effect of the fluid in the pipe,promotes the reaction of gas powder in the pipe,and reduces the degree of secondary explosion of unfired gas outside the pipe.For the pressure-time interval curve analysis,p_(st)increases from 2.97 kPa to 14.64 kPa,and the pressure time interval curve shows a double peak structure with a keep platform.The first pressure peak increases from 5.48 kPa to 10.20 kPa,the keep time extends from 6 ms to 25 ms,and the second pressure peak decreases from 23.03 kPa to 9.71 kPa.When p_(st)is 16.08 and 24.12 kPa,the pressure before the bursting film is superimposed and reflected many times,resulting in the time-history curve of bursting film pressure showing a special oscillating and rising three-peak structure.In the analysis of flame propagation velocity,the increase of p_(st)decreases the average flame propagation velocity from 161.33 m/s to 67.99 m/s.When n=2,the increase ofθmakes the flame structure change from cluster to jet.Whenθ=88.9%,the blasting flame shows a typical jet shape.The increase ofθand n makes the flame brightness gradually decrease,the length of the flame luminescence zone decreases,the time interval from breaking film to flame emergence and the flame duration increase.
作者
朱文艳
汪泉
张军
徐小猛
方敬贤
李雪交
ZHU Wenyan;WANG Quan;ZHANG Jun;XU Xiaomeng;FANG Jingxian;LI Xuejiao(School of Chemical and Blasting Engineering,Anhui University of Science and Technology,Huainan 232001,Anhui,China;Anhui Province Blasting Equipment and Technology Engineering Laboratory,Huainan 232001,Anhui,China;School of Chemical and Blasting Engineering,Joint National-Local Engineering Research Centre for Safe and Precise Coal Mining,Huainan 232001,Anhui,China)
出处
《爆炸与冲击》
EI
CAS
CSCD
北大核心
2024年第7期186-196,共11页
Explosion and Shock Waves
基金
国家自然科学基金(11872002)
煤炭安全精准开采国家地方联合工程研究中心开放基金(EC2023024)。
关键词
泄爆
气粉两相
静态动作压力
爆燃压力
火焰形态
explosion venting
gas-powder two-phase
static action pressure
deflagration pressure
flame pattern