Laminar flame speed ( S L ) measurements of stoichiometric propane in an oxygen-argon oxidizer were performed in a shock tube at unburned-gas temperatures of 296-1234 K and near-atmospheric pressures. Nonintrusive laser-induced breakdown is used to ignite expanding flames following the reflected-shock passage. Flame propagation is recorded using schlieren imaging in a recently implemented side-wall imaging flame test section (SWIFT). In a refined approach to account for flame distortion and the slight residual motion of the post-reflected-shock gas, an area-averaged formulation of the linear-curvature model (the AA-LC model) is derived for use extrapolating flame data to zero stretch. Measured S L values extracted using the AA-LC model closely agree with previous experimental measurements performed in a conventional kinetics shock tube (CKST) using much smaller flame kernels, providing evidence of the earlier data having been ignition affected. Below the chemistry-affected limit of 1050 K, experimental S L values fall in the range of values simulated with the detailed AramcoMech 3.0 kinetic mechanism and propane-specific mechanisms from NUIG and San Diego but exhibit a stronger temperature dependence than predicted by the mechanisms. Over the wide temperature range of the present data, the ubiquitous power-law form of empirical fit is shown to be inadequate for capturing the S L temperature dependence; a non-Arrhenius form is shown to perform favorably. The uncertainties of flame speed measurements performed in the SWIFT average 3.0% and 4.4% for experiments performed under static and post-reflected-shock conditions, respectively, a reduction from the 5.8% average uncertainty of CKST experiments. This work represents a significant step forward in the development of experimental capabilities for high-temperature flame speed measurements. The present results illustrate the potential value of the shock-tube flame speed method to provide measurements useful for informing kinetic model tuning and validation at conditions for which experimental data were not previously obtainable.& COPY; 2022 The Combustion Institute. Published by Elsevier Inc. All rights reserved.
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Department of Mechanical Engineering, Stanford University, 452 Escondido Mall, Bldg 520, Stanford,CA,94305, United StatesDepartment of Mechanical Engineering, Stanford University, 452 Escondido Mall, Bldg 520, Stanford,CA,94305, United States
Figueroa-Labastida, Miguel
Zheng, Lingzhi
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Department of Mechanical Engineering, Stanford University, 452 Escondido Mall, Bldg 520, Stanford,CA,94305, United StatesDepartment of Mechanical Engineering, Stanford University, 452 Escondido Mall, Bldg 520, Stanford,CA,94305, United States
Zheng, Lingzhi
Ferris, Alison M.
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Department of Mechanical Engineering, Stanford University, 452 Escondido Mall, Bldg 520, Stanford,CA,94305, United StatesDepartment of Mechanical Engineering, Stanford University, 452 Escondido Mall, Bldg 520, Stanford,CA,94305, United States
Ferris, Alison M.
Obrecht, Nicolas
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TotalEnergies OneTech, Solaize,69360, FranceDepartment of Mechanical Engineering, Stanford University, 452 Escondido Mall, Bldg 520, Stanford,CA,94305, United States
Obrecht, Nicolas
Callu, Cyrille
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TotalEnergies OneTech, Solaize,69360, FranceDepartment of Mechanical Engineering, Stanford University, 452 Escondido Mall, Bldg 520, Stanford,CA,94305, United States
Callu, Cyrille
Hanson, Ronald K.
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Department of Mechanical Engineering, Stanford University, 452 Escondido Mall, Bldg 520, Stanford,CA,94305, United StatesDepartment of Mechanical Engineering, Stanford University, 452 Escondido Mall, Bldg 520, Stanford,CA,94305, United States