Vasudevan Venkatesh, Hanson Ronald K, Bowman Craig T, Golden David M, Davidson David F
High Temperature Gasdynamics Laboratory, Mechanical Engineering Department, Stanford University, Stanford, California 94305, USA.
J Phys Chem A. 2007 Nov 22;111(46):11818-30. doi: 10.1021/jp075638c. Epub 2007 Oct 25.
We have studied the reaction between CH and N2, (1) CH + N2 --> products, in shock tube experiments using CH and NCN laser absorption. CH was monitored by continuous-wave, narrow-line-width laser absorption at 431.1 nm. The overall rate coefficient of the CH + N2 reaction was measured between 1943 and 3543 K, in the 0.9-1.4 atm pressure range, using a CH perturbation approach. CH profiles recorded upon shock-heating dilute mixtures of ethane in argon and acetic anhydride in argon were perturbed by the addition of nitrogen. The perturbation in the CH concentration was principally due to the reaction between CH and N2. Rate coefficients for the overall reaction were inferred by kinetically modeling the perturbed CH profiles. A least-squares, two-parameter fit of the current overall rate coefficient measurements was k1 = 6.03 x 1012 exp(-11150/T [K]) (cm3 mol-1 s-1). The uncertainty in k1 was estimated to be approximately +/-25% and approximately +/-35% at approximately 3350 and approximately 2100 K, respectively. At high temperatures, there are two possible product channels for the reaction between CH and N2, (1a) CH + N2 --> HCN + N and (1b) CH + N2 --> H + NCN. The large difference in the rates of the reverse reactions enabled inference of the branching ratio of reaction 1, k1b/(k1b + k1a), in the 2228-2905 K temperature range by CH laser absorption in experiments in a nitrogen bath. The current CH measurements are consistent with a branching ratio of 1 and establish NCN and H as the primary products of the CH + N2 reaction. A detailed and systematic uncertainty analysis, taking into account experimental and mechanism-induced contributions, yields a conservative lower bound of 0.70 for the branching ratio. NCN was also detected by continuous-wave, narrow-line-width laser absorption at 329.13 nm. The measured NCN time histories were used to infer the rate coefficient of the reaction between H and NCN, H + NCN --> HCN + N, and to estimate an absorption coefficient for the NCN radical.
我们利用CH和NCN激光吸收在激波管实验中研究了CH与N₂之间的反应:(1) CH + N₂ → 产物。通过431.1 nm处的连续波、窄线宽激光吸收监测CH。采用CH微扰方法,在1943至3543 K温度范围、0.9 - 1.4 atm压力范围内测量了CH + N₂反应的总包速率系数。在氩气中乙烷稀释混合物以及氩气中乙酸酐的激波加热过程中记录的CH分布曲线,因添加氮气而受到微扰。CH浓度的微扰主要归因于CH与N₂之间的反应。通过对微扰后的CH分布曲线进行动力学建模推断出总包反应的速率系数。当前总包速率系数测量值的最小二乘二参数拟合结果为k1 = 6.03 x 10¹² exp(-11150/T [K]) (cm³ mol⁻¹ s⁻¹)。k1的不确定度估计在约3350 K时约为±25%,在约2100 K时约为±35%。在高温下,CH与N₂反应存在两个可能的产物通道:(1a) CH + N₂ → HCN + N和(1b) CH + N₂ → H + NCN。通过在氮气浴实验中利用CH激光吸收,根据逆反应速率的巨大差异推断出2228 - 2905 K温度范围内反应(1)的分支比k1b/(k1b + k1a)。当前的CH测量结果与分支比为1一致,并确定NCN和H为CH + N₂反应的主要产物。考虑到实验和机理引起的贡献进行的详细系统不确定度分析得出分支比的保守下限为0.70。还通过329.13 nm处的连续波、窄线宽激光吸收检测到了NCN。测量得到的NCN时间历程用于推断H与NCN反应H + NCN → HCN + N的速率系数,并估计NCN自由基的吸收系数。