2017
DOI: 10.1016/j.ijhydene.2017.07.055
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Non-monotonic behaviors of laminar burning velocities of H2/O2/He mixtures at elevated pressures and temperatures

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Cited by 20 publications
(11 citation statements)
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“…In a rich mixture (φ = 1.8) u S increased with pressure from 0.6 atm until it reached a maximum at about 2 atm, and then decreased with pressure. Dayma et al, 17 Lu et al 18 and Kuznetsov et al 22 confirmed the nonmonotonic behavior of the laminar burning velocity at pressure variation in their research on H 2 -air mixtures with various equivalence ratios. This behavior was assigned by Sun et al 31 and Law 32 1applied to the increasing part of data from Fig.…”
Section: The Laminar Burning Velocities Of H 2 -O 2 -N 2 Flamesmentioning
confidence: 83%
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“…In a rich mixture (φ = 1.8) u S increased with pressure from 0.6 atm until it reached a maximum at about 2 atm, and then decreased with pressure. Dayma et al, 17 Lu et al 18 and Kuznetsov et al 22 confirmed the nonmonotonic behavior of the laminar burning velocity at pressure variation in their research on H 2 -air mixtures with various equivalence ratios. This behavior was assigned by Sun et al 31 and Law 32 1applied to the increasing part of data from Fig.…”
Section: The Laminar Burning Velocities Of H 2 -O 2 -N 2 Flamesmentioning
confidence: 83%
“…In nitrogendiluted H 2 -O 2 mixtures with N 2 concentrations higher than 30 vol% (including H 2 -air) slower flames propagate and a stronger pressure influence on S u is measured (absolute baric coefficients between 0.1 and 0.3). From extended measurements of laminar burning velocity in H 2 -O 2 -N 2 mixtures [14][15][16][17][18] the pressure exponent was found dependent on temperature and dilution degree by nitrogen as well. The data confirm earlier suggestions of Gűnther 19 and Lewis and von Elbe 20 who postulated the baric coefficient as being a function only of flame velocity, not of the system considered and/or the state of the flammable mixture.…”
Section: Introduction *mentioning
confidence: 93%
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