## Abstract Chemical kinetic simulations that more accurately consider reaction conditions behind reflected shock waves in a high pressure shock tube have been conducted by accounting for (1) timeβdependent temperature and pressure variations in contrast to assuming constant temperature and pressur
N2O Dissociation behind reflected shock waves
β Scribed by S. Charles Baber; Anthony M. Dean
- Publisher
- John Wiley and Sons
- Year
- 1975
- Tongue
- English
- Weight
- 898 KB
- Volume
- 7
- Category
- Article
- ISSN
- 0538-8066
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β¦ Synopsis
The dissociation of NzO/Ar mixtures, with and without added CO, has been studied by monitoring both infrared and ultraviolet emissions behind reflected shock waves. Initial temperatures ranged from 1850 to 2535"K, and the total concentrations were 1.94-2.40 X 10'8 molecule/cm3. The infrared emission, corrected if necessary for CO, was observed to decay exponentially, and an apparent rate constant k,,, was obtained. Addition of CO had no effect upon k,, and all the data can be described by the following Arrhenius parameters (in units of cm3/molecule.sec): log A = -9.31 f 0.12 and EA = 219.1 =t 5.2 kJ/mole. Ultraviolet emission data, in runs with added CO, indicate that the atomic oxygen concentration reached a constant value at t < 600 psec for To > 2050'K.
Numerical integration of the mechanism (1) N Z O + M + N z + O + M allowed comparison of calculated and observed parameters relating to both infrared and ultraviolet data. A consistent fit to these data was obtained with k, = 1.3 X 10-9 exp (-238 kJ/RT) and kz = ks = 1.91 X lo-" exp (-105 kJ/RT).
The concentration of atomic oxygen produced by N 2 0 dissociation is shown to be a sensitive function of kl through ka. Upper limits are also set for the rate constants of the following reactions:
(4)
(5)
In trodurtion
The dissociation of nitrous oxide behind shock waves has been extensively studied [l-81, and there is general agreement that the mechanism is (1) NzO + M -+ N:, + 0 + M NZO + 0 -+ 2 N 0 5 2 0 + 0 + Nz + 0 2
( 2 )
π SIMILAR VOLUMES
The thermal decomposition of acetylene has been studied in the temperature and pressure regimes of 1900-2500 K and 0.3-0.55 atm using a shock tube coupled to a time-of-flight mass spectrometer. A series of mixtures varying from 1.0-6.2% CzHz diluted in a Ne-Ar mixture yielded a carbon atom density r
The pyrolysis of benzene was studied in the temperature and pressure range of 1400-2200K and 0.25-0.81 arm using a shock tube coupled to a time-of-flight mass spectrometer. The mixtures employed were 2.1 and 5% benzene diluted with neon, which yielded a carbon atom density range of (1.6-7.9) x 1017
Time histories of OH, H 2 O, and 306.8 nm absorbance were measured behind reflected shock waves in mixtures of 1% n-butanol in Ar. Reflected shock conditions covered temperatures (T 5 ) from 1274 to 1439 K and pressures (P 5 ) near 1.5 atm. OH was measured using laser absorption of the R 1 (5) line
## Abstract The homogeneous thermal isomerization of cyclopropane to propene was studied in the presence of large excesses (99.6%β99.8%) of argon or helium diluent. Reaction temperatures ranged from 1038Β°β1208Β°K, and total gas pressures were varied from 533 to 5097 torr. The comparativeβrate single
Self-ignition of stoichiometric airlike argon mixtures of monocyclic and bicyclic small-ring hydrocarbons was investigated behind reflected shock waves at 1200-1600 K and 0.6 + 0.1 MPa. The reactivity of small-ring hydrocarbons has been found to be determined by the properties of their thermal decom