Detailed Reaction Mechanisms for Low Pressure Premixed n-Heptane Flames
A detailed reaction mechanism of n-heptane combustion has been elaborated and validated by comparison of computed mole fraction profiles with those measured in four premixed flames stabilized on a flat-flame burner under low pressure )6 kPa). in a wide range of equivalence ratios (0.7 - 2.0). As the...
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Published in: | Combustion science and technology Vol. 147; no. 1-6; pp. 61 - 109 |
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Abstract | A detailed reaction mechanism of n-heptane combustion has been elaborated and validated by comparison of computed mole fraction profiles with those measured in four premixed flames stabilized on a flat-flame burner under low pressure )6 kPa). in a wide range of equivalence ratios (0.7 - 2.0). As the MBMS technique was used for species analyses, both stable and active species were considered. The predictions of the model are in good agreement with the experimental results for most stable species. The main active species H. OH and O are fairly well predicted in rich flames while disagreements are observed in the lean and the stoichiometric flames. The intermediate radicals can be grouped in three classes depending on the accuracy of the model predictions: (i) good agreement in Ihe whole range of equivalence ratios, (ii) predicted mole fractions differing from the experimental values by a constant factor in the four flames studied, (iii) difference between computed and measured maximum mole fractions differing from lean to rich flames. In the discussion of the results, the observed disagreements between the model and the experiments have been generally interpreted in term of experimental inaccuracies. However, the modeling of the combustion chemistry for heavy fuel molecules has been carried out so far on the basis of experimental data referring only to stable species and the problems faced with intermediate radicals can result from experimental uncertainties but also from deficiencies in the mechanism or inaccuracies in the kinetic data. |
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AbstractList | The authors develop a detailed reaction mechanism of n-heptane combustion and test it by comparing computed model fraction profiles with those measured in premixed flames stabilized on the flat-flame burner under low prssure. The method was validated in a range of equivalence ratios extending from lean (0.7) to rich (2.0) flames. The mechanism was built upon the addition of an n-heptane consumption submechanism to an H2,C1-C4 submechanism. The main active species, H, OH, and O, are fairly well predicted in rich flames, while in lean and stoichimetric flames, the difference with the experimental results can reach a factor of three. Good agreement of the model with the experimental results is obtained for the active species. (AIAA) A detailed reaction mechanism of n-heptane combustion has been elaborated and validated by comparison of computed mole fraction profiles with those measured in four premixed flames stabilized on a flat-flame burner under low pressure )6 kPa). in a wide range of equivalence ratios (0.7 - 2.0). As the MBMS technique was used for species analyses, both stable and active species were considered. The predictions of the model are in good agreement with the experimental results for most stable species. The main active species H. OH and O are fairly well predicted in rich flames while disagreements are observed in the lean and the stoichiometric flames. The intermediate radicals can be grouped in three classes depending on the accuracy of the model predictions: (i) good agreement in Ihe whole range of equivalence ratios, (ii) predicted mole fractions differing from the experimental values by a constant factor in the four flames studied, (iii) difference between computed and measured maximum mole fractions differing from lean to rich flames. In the discussion of the results, the observed disagreements between the model and the experiments have been generally interpreted in term of experimental inaccuracies. However, the modeling of the combustion chemistry for heavy fuel molecules has been carried out so far on the basis of experimental data referring only to stable species and the problems faced with intermediate radicals can result from experimental uncertainties but also from deficiencies in the mechanism or inaccuracies in the kinetic data. |
Author | DOUTÉ, CHRISTINE DELFAU, JEAN-LOUIS VOVELLE, CHRISTIAN |
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Cites_doi | 10.1002/bbpc.198800219 10.1002/kin.550210805 10.1021/j100308a042 10.1080/00102208608923929 10.1063/1.555759 10.1016/0010-2180(88)90096-X 10.1063/1.555692 10.1063/1.555908 10.1002/kin.550200907 10.1080/00102209708935746 10.1063/1.555783 10.1063/1.555623 10.1002/kin.550190305 10.1063/1.555806 10.1080/00102209708935647 10.1002/kin.550230903 10.1021/j100249a028 10.1021/j100314a019 10.1021/j100325a019 10.1021/j100362a008 10.1021/j100372a054 10.1080/00102209108951771 10.1016/0010-2180(92)90124-8 10.1016/0010-2180(89)90008-4 10.1063/1.555880 10.1002/kin.550030503 10.1002/kin.550270404 10.1080/00102208708960325 10.1021/j100256a043 10.1039/ft9918702361 10.1063/1.444362 10.1002/kin.550200804 10.1021/j100333a028 10.1002/1097-4601(198606)18:6<623::AID-KIN550180603>3.0.CO;2-7 10.1002/kin.550270403 10.1080/00102209408907692 10.1002/kin.550160403 10.1002/kin.550240407 10.1080/00102209508907810 10.1016/0010-2180(93)90131-L 10.1021/j100296a057 10.1021/j100128a013 |
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Keywords | Reaction mechanism Flame structure Premixed flame Combustion Heptane Low pressure |
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References | Homann K.H. (CIT0035) 1983; 87 Slagle I.R. (CIT0051) 1988 CIT0072 CIT0071 CIT0030 Bastin E. (CIT0005) 1988 Tamura T. M. (CIT0053) 1987 CIT0032 CIT0031 CIT0034 CIT0033 Kern R.D. (CIT0038) 1984 Olzmann M. (CIT0045) 1988; 92 Warnatz J. (CIT0064) 1984 Bellimam M. A (CIT0006) 1992 Benesura A. (CIT0007) 1992 CIT0070 Wagner H. Gg. (CIT0061); 76 Kakumoto T. (CIT0036) 1987; 91 Axelsson E. I. (CIT0002) 1986 CIT0039 Timonen R. S. (CIT0054) 1987; 9 Warnatz J. (CIT0065) 1984 CIT0041 CIT0040 CIT0043 CIT0042 CIT0001 Cowart J.S. (CIT0018) 1989 Slagle I.R. (CIT0050) 1986 Westbrook C. K. (CIT0069) 1988 Benson S. W. (CIT0008) 1968 Cvetanovic RJ. (CIT0019) 1987; 16 Chevalier C. (CIT0015) 1992 CIT0003 Mulenko S. A. (CIT0044) 1987; 32 CIT0047 CIT0046 CIT0049 CIT0004 CIT0048 CIT0009 Burcat A (CIT0011) 1989 Coats C. M. (CIT0016) 1979 Warnatz J. (CIT0066) 1988 CIT0052 CIT0010 CIT0012 CIT0055 CIT0014 CIT0058 CIT0057 CIT0059 CIT0017 Warnatz J. (CIT0062) 1981 Chakir A. (CIT0013) 1988 CIT0021 CIT0020 CIT0023 CIT0067 CIT0022 Warnatz J. (CIT0063) 1982 CIT0025 CIT0024 CIT0068 CIT0027 Wagner H. Gg. (CIT0060) 1972; 76 CIT0026 CIT0029 CIT0028 Tsang W. (CIT0056) 1988; 17 |
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Snippet | A detailed reaction mechanism of n-heptane combustion has been elaborated and validated by comparison of computed mole fraction profiles with those measured in... The authors develop a detailed reaction mechanism of n-heptane combustion and test it by comparing computed model fraction profiles with those measured in... |
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SubjectTerms | Applied sciences Chemistry Combustion of liquid fuels Combustion. Flame Energy Energy. Thermal use of fuels Exact sciences and technology Flame Structure Heavy Fuels Laminar Flames Modeling Theoretical studies. Data and constants. Metering |
Title | Detailed Reaction Mechanisms for Low Pressure Premixed n-Heptane Flames |
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