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Combustion, Explosion and Shock Waves

2023 year, number 5

EFFECT OF THE IGNITION POSITION AND OBSTACLE ON VENTED METHANE-AIR DEFLAGRATION

J.-L. Li1, J. Guo2, X.-X. Sun3, F.-Q. Yang2
1School of Safety Engineering, China University of Mining and Technology, Xuzhou, PR China
2College of Environment and Safety Engineering, Fuzhou University, Fuzhou, PR China
3State Key Laboratory of Fire Science, University of Science and Technology of China, Hefei, PR China
Keywords: methane-air mixture, vented explosion, obstacle, overpressure, flame

Abstract

In this study, explosion venting of front, centrally, and rear ignited 9% methane-air mixtures has been conducted in a 1-m3 rectangular vessel with and without cylinders placed parallel to the venting direction. Three pressure peaks P1, P2, and Pext caused by vent failure, flame-acoustic interaction, and external explosion, respectively, can be distinguished. The pressure peak P1 appears in all the tests and is insensitive to the ignition position, but the existence of obstacles increases its value. The pressure peak P2 only appears in the centrally and front ignited explosions without obstacles. The pressure peak Pext can be observed in the rear ignition tests and is strengthened by the cylinders. The duration of the Helmholtz oscillations is longer in front ignition tests, whereas addition of cylinders had a minor effect on their frequency. This study also validates the ability of FLACS in predicting a vented methane-air explosion by comparing the simulated pressure--time histories and flame propagations with experimental results. FLACS can basically predict the shape of overpressure curves. If cylinders exist, the simulation results ensure better agreement with the experimental data because FLACS cannot simulate the flame-acoustic-interaction-induced pressure peak P2. The performance of FLACS is satisfactory in rear ignition tests because it calculates Pext and obstacles' effect on Pext exactly. The flame behavior simulated by FLACS is similar to that in experiments, but the effect of the Taylor instability on the flame is not sufficiently considered.