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2023
DOI: 10.1016/j.ast.2023.108269
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Effects of the quantity and arrangement of reactive jet obstacles on flame acceleration and transition to detonation: A numerical study

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Cited by 10 publications
(2 citation statements)
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“…Hence, the upper-wall shock hot spot at 13.385 ms, which, over time, causes a detonation to detonation-induced combustion wave moves fast, and, finally, the de to the local explosion and the leading shock wave merge. This mecha can be similar to the one described by Wang et al [42]. They observed hot spot at the flame tip, which promptly consumed the surroundin leading to the initiation of a detonation.…”
Section: Effects Of Inhomogeneity On the Fa And Ddt In Lean Mixturessupporting
confidence: 87%
“…Hence, the upper-wall shock hot spot at 13.385 ms, which, over time, causes a detonation to detonation-induced combustion wave moves fast, and, finally, the de to the local explosion and the leading shock wave merge. This mecha can be similar to the one described by Wang et al [42]. They observed hot spot at the flame tip, which promptly consumed the surroundin leading to the initiation of a detonation.…”
Section: Effects Of Inhomogeneity On the Fa And Ddt In Lean Mixturessupporting
confidence: 87%
“…Saeid et al [34] studied the spatial height ratio (S/H) of the obstacle spacing to the pipe diameter; they found that in inhomogeneous mixtures, detonation could not be triggered in the tube when the S/H was equal to 10 and that the DDT time was considerably reduced when the S/H was reduced to 2.5. Wang et al [35] investigated the effect of the number of jet obstacles on the DDT process, speculated that there existed an optimal number of jet obstacles, and concluded that the optimal number of jet obstacles may vary with changes in channel size and obstacle spacing. Coates et al [36] compared the influences of obstacles of different shapes on flame acceleration and found that rectangular obstacles induced the largest flame acceleration.…”
Section: Introductionmentioning
confidence: 99%