Shock-initiated ignition of natural gas-air mixtures

Ignition delay times in air for hydrocarbon mixtures that simulate natural gas were measured following the shock heating of such mixtures in reflected shock waves. The onset of ignition was determined by time-resolved absorption of the 3.39 μm He−Ne laser line. Measured induction times ranged from 15–1200 μs over the temperature interval 1200–1850 K at total densities near 3×10 −5 mol/cm 3 , corresponding to a pressure of about 4 atm at 1600 K. It was found that the induction time of a mixture of 1% CH 4 in air is shortened by factors of 3, 9 and 13 for the addition of 0.2% C 3 H 8 , 0.2% C 2 H 6 +0.1% C 3 H 8 and 0.2% C 2 H 6 +0.1% C 3 H 8 +0.1% n -C 4 H 10 , respectively. The temperature variation of the induction times for these fuel mixtures is essentially constant and given by: exp (26000±600 K/T), in agreement with ignition delay studies of CH 4 in O 2 /Ar mixtures. The activation energies for ignition of mixed fuels are thus controlled by the oxidation mechanism of CH 4 . A qualitative interpretation based on changes of initiation and branching rates introduced by the additives is provided to account for the shorter induction times.

[1]  D. Golden,et al.  Reactions of methyl radicals of importance in combustion systems , 1978 .

[2]  P. Pacey,et al.  Arrhenius parameters for the reactions CH3. + C4H10 → CH4 + C4H9. and C2H5. + C4H10 → C2H6 + C4H9. , 1972 .

[3]  P. Roth,et al.  Atom‐Resonanzabsorptionsmessungen beim thermischen Zerfall von Methan hinter Stoßwellen , 1975 .

[4]  J. Dove,et al.  Examination of Possible Non-Arrhenius Behavior in the reactions , 1973 .

[5]  A. Shepp,et al.  Rate of Recombination of Radicals. III. Rate of Recombination of Ethyl Radicals , 1957 .

[6]  P. Roth,et al.  Messungen zur Hochtemperaturpyrolyse von Äthan , 1979 .

[7]  Garry L. Schott,et al.  Further studies of exponential branching rates in reflected-shock heated, nonstoichiometric H2COO2 systems , 1973 .

[8]  Daniel J. Seery,et al.  An experimental and analytical study of methane oxidation behind shock waves , 1970 .

[9]  J. Chao,et al.  Ideal Gas Thermodynamic Properties of Ethane and Propane , 1973 .

[10]  D. R. Stull JANAF thermochemical tables , 1966 .

[11]  W. G. Mallard,et al.  High Temperature Absorption of the 3.39 µm He-Ne Laser Line by Small Hydrocarbons , 1978 .

[12]  A. Burcat,et al.  Shock-tube investigation of comparative ignition delay times for C1-C5 alkanes , 1971 .

[13]  T. Tanzawa,et al.  Thermal decomposition of ethane , 1979 .

[14]  K. Tabayashi,et al.  The early stages of pyrolysis and oxidation of methane , 1979 .

[15]  W. Hase,et al.  The decomposition of chemically activated n–butane, isopentane, neohexane, and n–pentane and the correlation of their decomposition rates with radical recombination rates.†‡ , 1972 .

[16]  W. Tsang Thermal decomposition of 3,4‐dimethylpentene‐1, 2,3,3‐trimethylpentane, 3,3‐dimethylpentane, and isobutylbenzene in a single pulse shock tube , 1969 .

[17]  A. Burcat,et al.  The Effect of Higher Alkanes on the Ignition of Methane-Oxygen-Argon Mixtures in Shock Waves , 1972 .

[18]  S. Tsuchiya,et al.  Temperature Measurement of Argon Gas behind Reflected Shock Wave , 1965 .

[19]  D. Allara,et al.  A computational modeling study of the low-temperature pyrolysis of n-alkanes; mechanisms of propane, n-butane, and n-pentane pyrolyses , 1975 .

[20]  W. Gardiner,et al.  Thermal dissociation rate of ethane at the high pressure limit from 250 to 2500 K , 1979 .

[21]  G. B. Skinner,et al.  Shock-tube investigation of ignition in methane--oxygen--argon mixtures. [Temperature from 1500 to 2150/sup 0/K and pressures of 2 to 10 atm] , 1971 .

[22]  B. Zwolinski,et al.  Ideals gas thermodynamic properties and isomerization of n‐butane and isobutane , 1975 .

[23]  W. Gardiner,et al.  Combustion of methane in fuel-rich mixtures☆ , 1978 .

[24]  G. B. Skinner,et al.  Kinetics of Methane Oxidation , 1972 .

[25]  G. B. Skinner,et al.  Shock tube investigation of ignition inethane-oxygen-argon mixtures , 1971 .