2018
DOI: 10.1080/23311916.2018.1469377
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Numerical simulation of detonation wave propagation and quenching process in in-line crimped-ribbon flame arrester

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Cited by 8 publications
(4 citation statements)
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“…Thus, Δ T 1 , Δ T 2 , and c p are independent of the flame detonation velocity v and the length l . 25 Hence, Equation (2) can be updated to λeffl/δitalichV. …”
Section: Methodsmentioning
confidence: 99%
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“…Thus, Δ T 1 , Δ T 2 , and c p are independent of the flame detonation velocity v and the length l . 25 Hence, Equation (2) can be updated to λeffl/δitalichV. …”
Section: Methodsmentioning
confidence: 99%
“…Considering the simulation accuracy, calculation amount and application scope, this study used the re‐normalization group (RNG) k‐ε model as the turbulence model 28,29 and used the eddy breakup (EBU), Arrhenius model, to simulate the chemical reaction of mine gas combustion in the pipe. Moreover, the chemical reaction was regarded as a single‐step reaction in the simulation 30‐32 …”
Section: Methodsmentioning
confidence: 99%
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“…A study using a crimped ribbon flame arrester was conducted by several scientists, and they varied the length of the arrester (see a brief review from Wang et al, 2018b). Sun et al (2018) numerically investigated detonation wave propagation and quenching in an in-line crimped-ribbon flame arrester, offering key insights into initiation, quenching rules, and the impact of structural parameters on propagation. Moreover, the parameters used to assess the flame arrester's effectiveness are the propagation velocity of the combustion wave, shock wave pressure, reinitiation distance, and detonation cell size.…”
Section: Introductionmentioning
confidence: 99%