Y' mass fraction YF r~ Yo YS/Β° Z dimensionless axial coordinate = Z'/Iv Z Parameter defined in Eqs. 9 and 10 Ze Zeldovich number = 0 / Tf 2 Greek Symbols thermal diffusivity /31 temperature perturbation, defined above Eq. 18 3/ 2Zf-1 6 o reduced Damkfhler number, Eq. 18 0 activation temperature = EC
On the oxidation of fuel nitrogen in a diffusion flame
β Scribed by C. V. Sternling; J. O. L. Wendt
- Publisher
- American Institute of Chemical Engineers
- Year
- 1974
- Tongue
- English
- Weight
- 715 KB
- Volume
- 20
- Category
- Article
- ISSN
- 0001-1541
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β¦ Synopsis
Abstract
The kinetic mechanisms of fuel nitrogen conversion to NO and N~2~ in a diffusion flame were investigated. A simple model of a diffusion flame in which the reaction zone has a finite thickness was developed. The purpose of this model was to allow the testing of complex kinetic mechanisms of pollutant formation under conditions where the fuel and oxidant feed rates are controlled by diffusion. A simple kinetic mechanism in which fuel nitrogen was simulated by nitrogen atoms showed the correct functional dependence of nitric oxide emissions on fuel nitrogen content. The model also predicts a significant effect of combustion intensity and temperature on fuel nitrogen conversion. For the hydrogen air diffusion flame the Zeldovich reaction mechanism could account for the production of N~2~ as well as NO.
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Over the temperature range 1950 to 2380 K, the rate constants k(12, ) --(2.0 -+ 0.2) X 108 m3/kgmolesec and k(is) = (5.6 +-0.7) Γ 1010 m3/kgmole-sec have been obtained. The relative contributions of reactions (12') and ( 15) vary markedly with'temperature, with reaction (15) dominating at temperatur