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Experimental study on the detonation propagation behaviors through a small-bore orifice plate in hydrogen-air mixtures
Affiliation:1. State Key Laboratory of Fire Science, University of Science and Technology of China, Hefei, 230027, PR China;2. CAS Key Laboratory of Mechanical Behavior and Design of Materials, Department of Modern Mechanics, University of Science and Technology of China, Hefei, 230026, PR China;3. College of Environment and Resources, Fuzhou University, Fuzhou, 350116, PR China;1. Department of Mechanical Engineering, McGill University, Montréal, Québec H3A 2K6, Canada;2. Department of Mechanical and Industrial Engineering, Concordia University, Montréal, Québec H3G 1M8, Canada;1. Department of Mechanical Engineering, McGill University, Montreal, Quebec H3A 2K6, Canada;2. Department of Mechanical and Industrial Engineering, Concordia University, Montreal, Quebec H3G 1M8, Canada;1. East China University of Science and Technology, Key Laboratory of Coal Gasification and Energy Chemical Engineering of Ministry of Education, Shanghai 200237, China;2. Beijing Institute of Petrochemical Technology, Beijing 102617, China;3. Peking University, College of Engineering, Department of Mechanics and Engineering Science, SKLTCS, Beijing 100871, China
Abstract:In this study, the regimes of detonation transmission through a single orifice plate were investigated systematically in a 6-m length and 90-mm inner diameter round tube. A series of experiments on the detonation propagation mechanisms in hydrogen-air mixtures were performed. A single obstacle with different orifice size (d) from 10 to 60 mm was adopted to study the effects of the induced perturbations on the detonation propagation. Here, the thickness of orifice plate (δ) was fixed at 10.33 mm. Detonation velocity was determined from the time-of-arrival (TOA) of the detonation wave recorded by eight high-speed piezoelectric pressure transducers (PCB102B06). Detonation cellular size was obtained by the smoked foil technique. The characteristic of detonation velocity evolution were quantitatively analyzed after it passes through a single obstacle, and particular attention was paid to the cases for which the blockage ratio (BR) is greater than 0.9, i.e., the cases of small hole diameter of d < 25 mm. The experimental results showed that, in a smooth tube, only super-critical condition and sub-critical condition can be observed. After the orifice plate is introduced into the tube, critical condition occurs. The detonation re-initiation with distinct cellular structures was experimentally observed. Of note is that when the blockage ratio (BR) values in the range of 0.802–0.96, it was easier to detonate at the fuel-lean side. Finally, the critical condition for detonation propagation through an orifice plate was quantified as d/λ > 1 where λ is the detonation cell size.
Keywords:Detonation  Perturbation  Propagation mechanism  Detonation re-initiation  Critical condition
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