戊-3-烯-2-基自由基与氧分子之间反应的实验和计算研究:随着温度的升高,从纯粹的稳定转变为纯粹的分解

IF 3.1 3区 化学 Q2 CHEMISTRY, PHYSICAL
Timo T. Pekkanen, László Valkai, Satya P. Joshi, György Lendvay, Petri Heinonen, Raimo S. Timonen and Arkke J. Eskola
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引用次数: 3

摘要

我们使用激光光解光电离质谱法、量子化学计算和主方程模拟来研究(E/Z)-戊-3-烯-2-基a共振稳定烃自由基与分子氧之间的反应动力学。时间分辨实验在伪一阶条件(过量[O2])下,在较宽的温度范围(240-750 K)和相对较低的压力(0.4-7 Torr)下进行。在大多数实验中使用氦气,但在一些测量中使用氮气来研究较重的对撞机对所研究反应动力学的影响。利用MESMER程序中最近实现的轨迹拟合功能,直接使用实验轨迹来优化主方程模型中的参数。低温下(T <300k),反应进行无阻碍重组反应生成过氧基加合物,自由基轨迹为单指数。在326 ~ 376 K范围内,反应物与过氧加合物达到平衡,自由基轨迹呈多指数分布。有趣的是,在500 K以上的温度下,再次观察到单指数衰减,尽管反应比低温时慢得多。主方程模拟表明,在低温和高温下,自由基衰变速率由单个特征值控制。在低温下,这个特征值对应于重组反应,在高温下对应于双分子产物的现象学形成。在低温和高温之间(确切的温度阈值取决于[O2]),存在一个避免交叉的区域,其中速率系数从一个特征曲线“跳跃”到另一个特征曲线。虽然化学显著特征值在高温(600 K, 0.01 bar, 850 K, 100 bar)下不能很好地与内能弛豫特征值分离,但我们观察到,主方程模型产生的许多baris - widom速率系数在1500 K以下有效。我们的模拟预测了高温下最重要的反应通道是(E/Z)-五-1,3-二烯和羟基的形成。采用实验约束的主方程模型模拟了多种条件下的标题反应。为了便于在自燃和燃烧模型中使用我们的结果,对最重要的反应通道给出了修正的阿伦尼乌斯表示。
本文章由计算机程序翻译,如有差异,请以英文原文为准。

An experimental and computational study of the reaction between pent-3-en-2-yl radicals and oxygen molecules: switching from pure stabilisation to pure decomposition with increasing temperature†

An experimental and computational study of the reaction between pent-3-en-2-yl radicals and oxygen molecules: switching from pure stabilisation to pure decomposition with increasing temperature†

We have used laser-photolysis–photoionization mass spectrometry, quantum chemical calculations, and master equation simulations to investigate the kinetics of the reaction between (E/Z)-pent-3-en-2-yl a resonance-stabilised hydrocarbon radical, and molecular oxygen. The time-resolved experiments were performed over a wide temperature range (240–750 K) at relatively low pressures (0.4–7 Torr) under pseudo-first-order conditions (excess [O2]). Helium bath gas was used in most experiments, but nitrogen was employed in a few measurements to investigate the effect of a heavier collider on the kinetics of the studied reaction. The experimental traces were directly used to optimise parameters in the master equation model using the recently implemented trace fitting feature in the MESMER program. At low temperatures (T < 300 K), the reaction proceeds by barrierless recombination reactions to form peroxyl adducts, and the radical traces are single-exponential. Between 326 K and 376 K, equilibration between the reactants and the peroxyl adducts is observed, and the radical traces are multi-exponential. Interestingly, at temperatures above 500 K, single-exponential decays were again observed, although the reaction is much slower than at low temperatures. The master equation simulations revealed that at both low and high temperatures, the radical decay rate is governed by a single eigenvalue. At low temperatures, this eigenvalue corresponds to recombination reactions, and at high temperatures to the phenomenological formation of bimolecular products. Between low and high temperatures (the exact temperature thresholds depend on [O2]), there is a region of avoided crossing in which the rate coefficient “jumps” from one eigencurve to the other. Although chemically significant eigenvalues are not well separated from internal energy relaxation eigenvalues at elevated temperatures (600 K at 0.01 bar, 850 K at 100 bar), we observed that many of the Bartis–Widom rate coefficients produced by the master equation model were valid up to 1500 K. Our simulations predict that the most important reaction channel at high temperatures is the formation of (E/Z)-penta-1,3-diene and hydroperoxyl. The experimentally constrained master equation model was used to simulate the title reaction over a wide range of conditions. To facilitate the use of our results in autoignition and combustion models, modified Arrhenius representations are given for the most important reaction channels.

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来源期刊
Faraday Discussions
Faraday Discussions 化学-物理化学
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期刊介绍: Discussion summary and research papers from discussion meetings that focus on rapidly developing areas of physical chemistry and its interfaces
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