The penetration depth of atomic radicals in tubes with catalytic surface properties

Domen Paul, M. Mozetič, R. Zaplotnik, A. Vesel, G. Primc, D. Đonlagič
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Abstract

Catalysis of molecular radicals is often performed in interesting experimental configurations. One possible configuration is tubular geometry. The radicals are introduced into the tubes on one side, and stable molecules are exhausted on the other side. The penetration depth of radicals depends on numerous parameters, so it is not always feasible to calculate it. This article presents systematic measurements of the penetration depth of oxygen atoms along tubes made from nickel, cobalt, and copper. The source of O atoms was a surfatron-type microwave plasma. The initial density of O atoms depended on the gas flow and was 0.7, 2.4, and 4.2 〖∙10〗^21 m^(-3) at the flow rates of 50, 300, and 600 sccm, and pressure of 10, 35, and 60 Pa, respectively. The gas temperature remained at room temperature throughout the experiments. The dissociation fraction decreased exponentially along the length of the tubes in all cases. The penetration depths for well-oxidized nickel were 1.2, 1.7, and 2.4 cm, respectively. For cobalt, they were slightly lower at 1.0, 1.3, and 1.6 cm, respectively, while for copper, they were 1.1, 1.3, and 1.7 cm, respectively. The results were explained by gas dynamics and heterogeneous surface association. These data are useful in any attempt to estimate the loss of molecular fragments along tubes, which serve as catalysts for the association of various radicals to stable molecules.
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具有催化表面特性的管中原子自由基的穿透深度
分子自由基的催化通常是在有趣的实验构型中进行的。其中一种可能的配置是管状几何结构。自由基从一侧进入管中,稳定分子从另一侧排出。自由基的穿透深度取决于许多参数,因此计算它并不总是可行的。本文介绍了氧原子沿着由镍、钴和铜制成的管子的穿透深度的系统测量。氧原子的来源是一个表面加速器型微波等离子体。O 原子的初始密度取决于气体流量,在流量为 50、300 和 600 sccm,压力为 10、35 和 60 Pa 时,初始密度分别为 0.7、2.4 和 4.2 〖∙10〗^21 m^(-3)。在整个实验过程中,气体温度始终保持在室温。在所有情况下,解离分数沿管道长度呈指数下降。氧化良好的镍的穿透深度分别为 1.2、1.7 和 2.4 厘米。钴的穿透深度略低,分别为 1.0、1.3 和 1.6 厘米,而铜的穿透深度分别为 1.1、1.3 和 1.7 厘米。气体动力学和异质表面关联可以解释这些结果。这些数据对于估算分子碎片沿管道流失的情况非常有用,因为管道是各种自由基与稳定分子结合的催化剂。
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