Some chemical kinetics issues in reburning: The branching fraction of the HCCO+NO reaction

James A. Miller , Joseph L. Durant , Peter Glarborg
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引用次数: 26

Abstract

We have determined theoretically some critical kinetic parameters in the mechanism of NOx reburning under flow-reactor conditions. Specifically, using a variety of electronic-structure methods to investigate the potential energy surfaces and the maximum free-energy method of Quack and Troe to determine the resulting rate coefficients, we have deduced the values of k2 and k3 for the reactions HCNO+O a3HCO+NO (R2) and HCNO+OH a3HCOH+NO (R3) to be k2≈7×1013 cm3/mole s and k3≈2×1013 cm3/mole s independent of temperature for 300 K<T<2700 K. With such fast reactions converting HCNO to NO, a critical parameter in the reburn mechanism is α(T)=k1b(T)/k1(T), the branching fraction of the HCCO+NO reaction, HCCO+NO a3HCNO+CO (R1a) -a3HCN+CO2 (R1b) -a3NONC+CO (R1c) Again using PES information from a variety of electronic-structure methods (including the QCISD barrier heights of Nguyen et al.), we have used the statistical-theoretical methodology of Miller, Parrish, and Brown to determine α(T)=0.985 exp (−T/1748), valid for 300 K<T<2000 K. Using a value of k1=k1a+k1b+k1c=2.4×1013 cm3/mole s independent of temperature (consistent with experiment), we have determined modified Arrhenius expressions for k1a and k1b, k1a=1.17×1011 T0.65 cm3/mole s and k1b=1.45×1016 T−0.968 exp(−648/RT) cm3/mole s for 300 K<T<2000 K. Reaction (R1c) never contributes as much as 1% to the total rate coefficient. Our predictions for α(T) disagree with an experimental determination at T=700 K, but they are only slightly smaller than those used in modeling for 1000 K<T<1400 K.

The theoretical analyses and the reburn mechanism are discussed in detail.

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再燃烧中的一些化学动力学问题:HCCO+NO反应的分支分数
从理论上确定了流动反应器条件下NOx再燃机理的几个关键动力学参数。具体来说,利用各种电子结构方法研究势能面,并利用Quack和Troe的最大自由能法确定所得的速率系数,我们推导出HCNO+O a3HCO+NO (R2)和HCNO+OH a3HCOH+NO (R3)反应的k2和k3值分别为k2≈7×1013 cm3/mol s和k3≈2×1013 cm3/mol s,与温度无关,为300 K<T<2700 K。由于这种快速反应将HCNO转化为NO,再燃烧机制的一个关键参数是α(T)=k1b(T)/k1(T), HCCO+NO反应的分支分数,HCCO+NO a3hno +CO (R1a) -a3HCN+CO2 (R1b) -a3NONC+CO (R1c)。再次使用来自各种电子结构方法的PES信息(包括Nguyen等人的QCISD势垒高度),我们使用Miller, Parrish和Brown的统计理论方法确定α(T)=0.985 exp(−T/1748)。有效值为300 K<T<2000 K。利用与温度无关的k1=k1a+k1b+k1c=2.4×1013 cm3/mol s(与实验一致),我们确定了k1a和k1b的修正Arrhenius表达式,k1a=1.17×1011 T0.65 cm3/mol s, k1b=1.45×1016 T - 0.968 exp(- 648/RT) cm3/mol s (300 K<T<2000 K)。反应(R1c)对总速率系数的贡献从不超过1%。我们对α(T)的预测与T=700 K时的实验结果不一致,但它们仅略小于1000 K<T<1400 K时的模型。详细讨论了理论分析和再燃机理。
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