A closed-form solution of deep tunnel subject to an internal pressure and to an axisymmetrical time-dependent temperature ยฎeld is presented. The material is supposed to have a thermal-softening behaviour, the cohesion decreasing with the temperature. The thermal expansion generates plastic zones wit
Modeling the thermal De-NOx process: Closing in on a final solution
โ Scribed by J. A. Miller; P. Glarborg
- Book ID
- 101250962
- Publisher
- John Wiley and Sons
- Year
- 1999
- Tongue
- English
- Weight
- 171 KB
- Volume
- 31
- Category
- Article
- ISSN
- 0538-8066
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โฆ Synopsis
We have extended our previous kinetic model for the Thermal De-NO x Process to include recent information about the branching fraction โฃ 1 (T) of the NH 2 ฯฉ NO reaction,
2 where โฃ 1 (T) ฯญ k 1b /(k 1a ฯฉ k 1b ). The values of the rate coefficients k 1a (T) and k 1b (T) used in the model are 20 ฯช2.65 3 k ฯญ 2.77 ฯซ 10 T exp(ฯช1258/RT) cm /mole-sec. 1a 10 0.425 3 k ฯญ 2.29 ฯซ 10 T exp(814/RT) cm /mole-sec. and 1b
These two rate coefficients combine to give values of the total rate coefficient and branching fraction that are in excellent agreement with experiments over a wide range of temperatures, 300 K ฯฝ T ฯฝ 1400 K for k 1 ฯญ k 1a ฯฉ k 1a and 300 K ฯฝ T ฯฝ 2000 K for โฃ 1 (T). The smaller values of โฃ 1 (T) in the Thermal De-NO x temperature window, 1100 K ฯฝ T ฯฝ 1400 K, used in the model allow us to reduce the value of the NNH lifetime to 1.5 ฯซ 10 ฯช8 sec, which is consistent both with the upper limit set by experiment and with the best theoretical predictions. We compare the model predictions with the experiments of Kasuya et al. and discuss the results in some detail.
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