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温度相关动力学(195-798 K)和 H 原子产率(298-498 K)来自(1)CH(2)与乙炔、乙烯和丙烯的反应。

Temperature dependent kinetics (195-798 K) and H atom yields (298-498 K) from reactions of (1)CH(2) with acetylene, ethene, and propene.

机构信息

School of Chemistry, University of Leeds, Leeds, LS2 9JT, United Kingdom.

出版信息

J Phys Chem A. 2010 Sep 9;114(35):9413-24. doi: 10.1021/jp102276j.

Abstract

The rate coefficients for the removal of the excited state of methylene, (1)CH(2) (a(1)A(1)), by acetylene, ethene, and propene have been studied over the temperature range 195-798 K by laser flash photolysis, with (1)CH(2) being monitored by laser-induced fluorescence. The rate coefficients of all three reactions exhibit a negative temperature dependence that can be parametrized as k((1)CH(2)+C(2)H(2)) = (3.06 +/- 0.11) x 10(-10) T ((-0.39+/-0.07)) cm(3) molecule(-1) s(-1), k((1)CH(2)+C(2)H(4)) = (2.10 +/- 0.18) x 10(-10) T ((-0.84+/-0.18)) cm(3) molecule(-1) s(-1), k((1)CH(2)+C(3)H(6)) = (3.21 +/- 0.02) x 10(-10) T ((-0.13+/-0.01)) cm(3) molecule(-1) s(-1), where the errors are statistical at the 2sigma level. Removal of (1)CH(2) occurs by chemical reaction and electronic relaxation to ground state triplet methylene. The H atom yields from the reactions of (1)CH(2) with acetylene, ethene, and propene have been determined by laser-induced fluorescence over the temperature range 298-498 K. For the reaction with propene, H atom yields are close to the detection limit, but for acetylene and ethene, the fraction of H atom production is approximately 0.88 and 0.71, respectively, at 298 K, rising to unity by 398 K, with the balance of the reaction with acetylene presumed to be electronic relaxation. Experimental constraints limit studies to a maximum of 1 Torr of bath gas; master equation calculations using an approach that allows treatment of intermediates with deep energy wells have been carried out to explore the role of collisional stabilization for the reaction of (1)CH(2) with acetylene. Stabilization is calculated to be insignificant under the experimental conditions, but does become significant at higher pressures. Between pressures of 100 and 1000 Torr, propyne and allene are formed in similar amounts with a slight preference for propyne. At higher pressures propyne formation becomes about a factor two greater than that of allene, and above 10(5) Torr (300 < T (K) < 600) cyclopropene formation starts to become significant. The implications of temperature-dependent (1)CH(2) relaxation on the roles of (1)CH(2) in chemical mechanisms for soot formation are discussed.

摘要

甲叉基(1)CH(2)(a(1)A(1))的激发态被乙炔、乙烯和丙烯去除的速率系数在 195-798 K 的温度范围内通过激光闪光光解进行了研究,其中(1)CH(2) 通过激光诱导荧光进行监测。所有三种反应的速率系数都表现出负的温度依赖性,可以参数化为 k((1)CH(2)+C(2)H(2)) = (3.06 +/- 0.11) x 10(-10) T ((-0.39+/-0.07)) cm(3) molecule(-1) s(-1),k((1)CH(2)+C(2)H(4)) = (2.10 +/- 0.18) x 10(-10) T ((-0.84+/-0.18)) cm(3) molecule(-1) s(-1),k((1)CH(2)+C(3)H(6)) = (3.21 +/- 0.02) x 10(-10) T ((-0.13+/-0.01)) cm(3) molecule(-1) s(-1),其中误差在 2sigma 水平上是统计性的。(1)CH(2) 的去除是通过化学反应和电子弛豫到基态三重态甲叉基发生的。在 298-498 K 的温度范围内,通过激光诱导荧光测定了(1)CH(2)与乙炔、乙烯和丙烯反应的 H 原子产率。对于与丙烯的反应,H 原子产率接近检测极限,但对于乙炔和乙烯,在 298 K 时 H 原子生成的比例分别约为 0.88 和 0.71,到 398 K 时上升到 1,而与乙炔的反应的平衡假定为电子弛豫。实验限制将研究限制在最大 1 托的浴气中;使用允许处理深能阱中间体的方法进行了主方程计算,以探索(1)CH(2)与乙炔反应中碰撞稳定化的作用。在实验条件下,稳定化被计算为不重要,但在较高压力下变得重要。在 100 到 1000 托之间的压力下,丙炔和丙二烯以相似的量形成,丙炔略有偏好。在较高的压力下,丙炔的形成大约是丙二烯的两倍,高于 10(5)托(300 < T (K) < 600)时,环丙烯的形成开始变得显著。讨论了温度依赖的(1)CH(2)弛豫对(1)CH(2)在烟灰形成的化学机制中的作用的影响。

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