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Reaction propagation modes in millimeter-scale tubes for ethylene/oxygen mixtures
Authors:Ming-Hsun Wu  Chan-Yu Wang
Affiliation:1. Department of Mechanical and Aerospace Engineering, Princeton University, Princeton, NJ 08544-5263, USA;2. Department of Mechanical and Aerospace Engineering, West Virginia University, Morgantown, WV 26506-6106, USA;3. Institute for Nuclear and Energy Technologies, Karlsruhe Institute of Technology, Kaiserstrasse 12, 76131 Karlsruhe, Germany;4. Department of Applied Mechanics, Chalmers University of Technology, 41296 Göteborg, Sweden;5. Center for Combustion Energy, Tsinghua University, Beijing 100084, China;6. Department of Physics, Umeå University, 90187 Umeå, Sweden;1. Department of Mechanical Engineering, University College London, London WC1E 7JE, United Kingdom;2. Lab. of Fluid Dynamics and Technical Flows, University of Magdeburg “Otto von Guericke”, Universitätsplatz 2, D-39106 Magdeburg, Germany;1. Dept. Ingeniería Térmica y de Fluidos, Universidad Carlos III de Madrid, 28911 Leganés, Spain;2. Department of Energy, CIEMAT, Avda. Complutense 40, 28040 Madrid, Spain
Abstract:Effects of tube diameter and equivalence ratio on reaction front propagations of ethylene/oxygen mixtures in capillary tubes were experimentally analyzed using high speed cinematography. The inner diameters of the tubes investigated were 0.5, 1, 2 and 3 mm. The flame was ignited at the center of the 1.5 m long smooth tube under ambient pressure and temperature before propagated towards the exits in the opposite directions. A total of five reaction propagation scenarios, including deflagration-to-detonation transition followed by steady detonation wave transmission (DDT/C–J detonation), oscillating flame, steady deflagration, galloping detonation and quenching flame, were identified. DDT/C–J detonation mode was observed for all tubes for equivalence ratios in the vicinity of stoichiometry. The velocity for the steady detonation wave propagation was approximately Chapman–Jouguet velocity for 1, 2, and 3 mm I.D. tubes; however, a velocity deficit of 5% was found for the case in 0.5 mm I.D. tube. For leaner mixtures, an oscillating flame mode was found for tubes with diameters of 1 to 3 mm, and the reaction front travelled in a steady deflagrative flame mode with velocities around 2–3 m/s when the mixture equivalence ratio becomes even leaner. Galloping detonation wave propagation was the dominant mode for the fuel lean regime in the 0.5 mm I.D. tube. For rich mixtures beyond the detonation limits, a fast flame followed by flame quenching was observed.
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