火焰光度法测定扩散系数。第3部分。-一氧化氮测定结果

A. Ashton, A. Hayhurst
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引用次数: 4

摘要

利用常压H2+ O2+ N2火焰燃烧气体中扩散的微量一氧化氮,测试了测量气相扩散系数的点源技术。利用空气余辉辐射监测一氧化氮浓度。结果定量地验证了该技术,并在1920 ~ 2520k的温度范围内测量了一氧化氮的扩散系数。这些数据可以用Lennard-Jones(12:6)势或纯排斥性逆幂势函数来解释,以描述一氧化氮分子与主要火焰种的相互作用。对第二势函数有轻微的偏爱。对于Lennard-Jones函数,不可能得到NO的一对唯一的力常数。然而,σ= 3.60 × 10-10 m和(Iµ/k)= 85 k或σ= 3.58 × 10-10 m和(Iµ/k)= 91 k均能较好地计算出扩散系数。对于另一个势函数,排斥力与距离成反比到12次方最适合测量的扩散系数。给出了相应的力常数值。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Flame photometric determinations of diffusion coefficients. Part 3.—Results for nitric oxide
The point-source technique for measuring gas-phase diffusion coefficients has been tested using trace quantities of nitric oxide diffusing in the burnt gases of atmospheric pressure flames of H2+ O2+ N2. The air afterglow emission was used to monitor concentrations of nitric oxide. The results validate quantitatively the technique, and diffusion coefficients for nitric oxide have been measured over the temperature range 1920–2520 K. These data can be accounted for with either a Lennard-Jones (12: 6) potential or a purely repulsive inverse power potential function to describe interactions of a nitric oxide molecule with those of the principal flame species. A slight preference for the second potential function is indicated. With the Lennard-Jones function it is not possible to arrive at one unique pair of force constants for NO. However, either σ= 3.60 × 10–10 m and (Iµ/k)= 85 K or σ= 3.58 × 10–10 m and (Iµ/k)= 91 K can be used to calculate diffusion coefficients with reasonable accuracy. For the other potential function, repulsive forces varying inversely with separation to the 12th power fit the measured diffusion coefficients best. Values of the corresponding force constants are given.
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