Premixed fuel and air were burned at atmospheric pressure and 1750 K in a jet-stirred combustor. A water-cooled stainless-steel probe was used to sample stable species over an equivalence ratio range of 1.3-2.0. In general, the major stable species measured showed good agreement with a model consist
Benzene destruction in fuel-rich jet-stirred reactor combustion
โ Scribed by Craig B. Vaughn; Jack B. Howard; John P. Longwell
- Publisher
- Elsevier Science
- Year
- 1991
- Tongue
- English
- Weight
- 770 KB
- Volume
- 87
- Category
- Article
- ISSN
- 0010-2180
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โฆ Synopsis
Benzene destruction was studied using a jet-stirred reactor burning premixed C2H2, C6H6, H2, 02, N 2 mixtures at 1 atm, 1630 K, a fuel equivalence ratio of 2.2, a C/H ratio of 0.5, and residence times of 5-6 ms. Stable species concentrations were measured by water-cooled probe sampling and gas chromatography. A set of equations relating the concentrations of radical species to those of measured stable species were solved to determine radical concentrations under the range of experimental conditions, c6a 6 formation and destruction occur simultaneously in combustion, but in this study, the destruction was enhanced relative to formation by adding C6H 6 to the fuel, thereby reducing the sensitivity of the net destruction rate to the formation kinetics. The net C6H 6 destruction rates predicted by the model are within 90% of the experimental values. According to the model, the largest contribution to C6H 6 destruction under these conditions is H abstraction, largely by H atom, OH and CH3, and the C6H 5 formed is destroyed by both addition and unimolecular destruction reactions.
๐ SIMILAR VOLUMES
Dynamics of combustion processes of n-heptane and i-octane have been studied with varying temperature and pressure by means of a jet stirred flow reactor (JSFR), in the range 450-850K and 1-12 atm. Periodic or damped oscillatory cool flames, multistage ignitions, "'jumps," and slow combustion have