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STUDIES OF THE KINETICS AND MECHANISM OF GAS-SURFACE REACTIONS ON METAL AND METAL OXIDE SURFACES.

机译:气体在金属和金属氧化物表面上的反应动力学和机理的研究。

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摘要

The coadsorption of SO(,2) and CO on Pt is studied by using Flash Desorption Mass Spectrometry (FDMS) and Auger Electron Spectroscopy (AES). We find that: (1) SO(,2) chemisorbs on clean Pt with an initial sticking probability of unity and with at least three first order, coverage independent binding states with E(,d) of 7, 11 and 23 kcal mole('-1) respectively. (2) CO adsorbs on clean Pt with an initial sticking probability of 0.6 and with at least two first order and coverage dependent binding states with E(,d) around 18 and 22 kcal mole('-1) respectively. (3) In the coadsorption experiments, the surface reaction proceeds between the adsorbed species to form a complex which dissociates to form CO(,2) and sulfur. The sulfur diffuses into the bulk of the Pt foil. The complex formation modifies the surface bonding. The E(,d) for CO is decreased while the E(,d) of the two low temperature binding states for SO(,2) are increased. (4) The CO(,2) FDMS shows that there are at least two first order and coverage dependent binding states with E(,d) around 13 and 16 kcal mole('-1) respectively. (5) When the surface is saturated with SO(,2) ((theta) = 1) adsorption of CO is completely inhibited. However, if the surface is saturated with CO ((theta) = 0.67) appreciable amounts of SO(,2) can still be adsorbed. The observed reduction in Pt activity is simply due to blocking of the sites. (6) The kinetics of the surface reacton for this system are characteristic of a Langmuir-Hinshelwood mechanism. The rate-determining step is the first order desorption of CO(,2) from a surface complex. (7) The energy change for the formation of the complex {('O) (,S) ('O) (,C) ('O)} (ad.) from the SO(,2)(ad.) and CO(ad.) molecules is calculated to be (DELTA)E = -31 kcal mole('-1).;Moreover, the stability of the AlO(,2) molecule is studied by using a 60(DEGREES) sector magnetic mass spectrometer. We find that: (11) The AlO(,2) molecules exist as a minor vapor species evaporating from the Al(,2)O(,3) surface. The atomization enthalpy of AlO(,2) is found to be.;(DIAGRAM, TABLE OR GRAPHIC OMITTED...PLEASE SEE DAI).;This leads to a heat of formation for AlO(,2) of.;In addition, the Reaction Probability technique is used to study the kinetics and mechanism of the dissociation reaction of In(,2)O on W and on Al(,2)O(,3). We find that: (8) In atoms chemisorb on both a clean W surface and an oxidized W surface with an initial sticking probability of unity and with a first order, coverage dependent binding state. The E(,d) decreases with increasing coverage up to (theta) = 0.25 and (theta) = 0.125 for W(clean) and W(oxidized) respectively. In the zero coverage limit, the E(,d) are 92 and 65 kcal mole('-1) for In on W(clean) and on W(oxidized) respectively. (9) In(,2)O is chemisorbed on an oxidized W surface with a first order, coverage dependent binding state. At high coverage, the interaction among the In(,2)O molecules and the surface is rather complicated. The adsorbed In(,2)O molecules can either desorb from the surface as In(,2)O or undergo dissociation to form In and O atoms. The O atoms react with W immediately to form tungsten oxides. The desorption of In is the rate-determining step of this system. (10) In atoms also chemisorb on Al(,2)O(,3) with an E(,d) of 56 kcal mole('-1) in the limit of zero coverage. In(,2)O is chemisorbed on Al(,2)O(,3). The E(,d) of desorption in the zero coverage limit is 44 kcal mole('-1). The desorption of In is the rate-determining step of the In(,2)O on Al(,2)O(,3) system.;(DIAGRAM, TABLE OR GRAPHIC OMITTED...PLEASE SEE DAI).
机译:SO(,2)和CO在Pt上的共吸附是通过使用快速脱附质谱(FDMS)和俄歇电子能谱(AES)研究的。我们发现:(1)SO(,2)在干净的Pt上化学吸附,其初始粘附概率为1,并且具有至少三个一阶,覆盖独立的结合状态,其E(,d)为7、11和23 kcal摩尔( '-1)。 (2)CO吸附在干净的Pt上的初始粘附概率为0.6,并且具有至少两个与E(,d)分别依赖于18和22 kcal mole('-1)的一级和覆盖依赖性结合态。 (3)在共吸附实验中,表面反应在被吸附物质之间进行,形成复合物,该复合物解离形成CO(,2)和硫。硫扩散到Pt箔的主体中。复合物形成改变了表面结合。 CO的E(,d)降低,而SO(,2)的两个低温结合态的E(,d)升高。 (4)CO(,2)FDMS显示至少有13个和16 kcal mole('-1)附近的E(,d)具有两个依赖于一阶和覆盖的结合状态。 (5)当表面用SO(,2)(θ= 1)饱和时,完全抑制了CO的吸附。但是,如果表面被CO饱和(θ= 0.67),仍然可以吸附相当数量的SO(,2)。观察到的Pt活性降低仅是由于位点的封闭。 (6)该系统表面反应的动力学是Langmuir-Hinshelwood机理的特征。速率确定步骤是从表面络合物一级解吸CO(,2)。 (7)从SO(,2)(ad。)形成复合物{('O)(,S)('O)(,C)('O)}(ad。)的能量变化CO(ad。)分子的计算值为ΔE= -31 kcal mole('-1)。此外,使用60(DEGREES)扇形磁质量研究了AlO(,2)分子的稳定性光谱仪。我们发现:(11)AlO(,2)分子以从Al(,2)O(,3)表面蒸发的少量蒸气形式存在。发现AlO(,2)的雾化焓为(;省略了图表,表格或图形...请参见DAI);;这导致AlO(,2)的形成热;反应概率技术用于研究In(,2)O在W和Al(,2)O(,3)上解离反应的动力学和机理。我们发现:(8)在原子上,化学吸附在干净的W表面和氧化的W表面上,其初始粘着概率为1,并且具有第一级,取决于覆盖范围的结合状态。对于W(纯净)和W(氧化),E(d)随覆盖率的增加而降低,分别达到θ= 0.25和θ= 0.125。在零覆盖极限下,In在W(纯净)和W(氧化)上的E(,d)分别为92和65 kcal mole('-1)。 (9)In(,2)O以一阶覆盖率依赖性结合态化学吸附在氧化的W表面上。在高覆盖率下,In(,2)O分子与表面之间的相互作用相当复杂。吸附的In(,2)O分子可以作为In(,2)O从表面解吸,也可以解离形成In和O原子。 O原子立即与W反应形成氧化钨。 In的解吸是该系统的速率确定步骤。 (10)在零覆盖范围内,原子中的E(,d)也以56 kcal mole('-1)的E(,d)化学吸附在Al(,2)O(,3)上。 In(,2)O化学吸附在Al(,2)O(,3)上。零覆盖范围内的解吸E(d)为44 kcal mole('-1)。 In的解吸是Al(,2)O(,3)系统上In(,2)O的速率确定步骤。(图,图表或图形省略...请参见DAI)。

著录项

  • 作者

    HO, PIN.;

  • 作者单位

    University of Illinois at Chicago.;

  • 授予单位 University of Illinois at Chicago.;
  • 学科 Chemistry Physical.
  • 学位 Ph.D.
  • 年度 1981
  • 页码 179 p.
  • 总页数 179
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 遥感技术;
  • 关键词

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