To better understand how the dynamics of a folded flame propagating from the closed end of a semiinfinite tube is affected by the blast flow of unburned mixture and the flame-driven acoustics, we study a one-dimensional, unsteady model in which (1) the folded flame is modeled as a planar, markedly s
Transition to detonation in a flame jet
โ Scribed by I.O. Moen; D. Bjerketvedt; T. Engebretsen; A. Jenssen; B.H. Hjertager; J.R. Bakke
- Publisher
- Elsevier Science
- Year
- 1989
- Tongue
- English
- Weight
- 1005 KB
- Volume
- 75
- Category
- Article
- ISSN
- 0010-2180
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โฆ Synopsis
The results of an experimental and numerical investigation of flame-jet ignition of an acetylene-air cloud contained in a 2 m diameter plastic bag, 8 m long, are reported. The flame jet is produced by an acetylene-air flame in a 0.66 m diameter tube, 11 m long. The composition of the mixture was varied to obtain the critical composition for initiation of detonation in the cloud, with and without obstacles at the end of the tube. Numerical calculations were used to characterize the flame jet. Transition to detonation in the flame jet from an open tube was observed for acetylene-air mixtures with more than 7.9% C2H2. The mechanism of transition observed on the high-speed film records is analogous to that seen in similar laboratory experiments, with a localized explosion somewhere in the turbulent flame jet leading to the onset of detonation. Transition was facilitated by placing various obstacles at the exit of the tube. With an orifice plate with 50 nun diameter holes, initiation of detonation in a 7.0% C2H2 mixture occurs uniformly across the flame jet a short distance downstream of the plate. With a circular central obstacle in the tube exit, transition to detonation was observed in a 5.6% C2H2 mixture. From the results of this investigation, it is concluded that the phenomena of hot gas jet initiation of detonation seen in laboratory experiments with fuel-oxygen mixtures also occur in fuel-air mixtures provided the jet is large enough. The size of the jet can be reduced significantly if obstacles and/or nearby physical boundaries are present to perturb the turbulent flame jet.
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