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Influence of the Methane—Zeolite A Interaction Potential on the Concentration Dependence of Self-diffusivity

机译:甲烷-沸石A相互作用势对自扩散浓度依赖性的影响

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Studies on the diffusion of methane in a zeolite structure type LTA (as per IZA nomenclature) have indicated that different types of methane–zeolite potentials exist in the literature in which methane is treated within the united-atom model. One set of potentials, referred to as model A, has a methane oxygen diameter of 3.14 A, while another set of potential parameters, model B, employs a larger value of 3.46 A. Fritzsche and co-workers (1993) have shown that these two potentials lead to two distinctly different energetic barriers for the passage of methane through the eight-ring window in the cation-free form of zeolite A. Here, we compute the variation of the self-diffusivity (D) with loading (c) for these two types of potentials and show that this slight variation in the diameter changes the concentration dependence qualitatively: thus, D decreases monotonically with c for model A, while D increases and goes through a maximum before finally decreasing for model B. This effect and the surprising congruence of the diffusion coefficients for both models at high loadings is examined in detail at the molecular level. Simulations for different temperatures reveal the Arrhenius behaviour of the self-diffusion coefficient. The apparent activation energy is found to vary with the loading. We conclude that beside the cage-to-cage jumps, which are essential for the migration of the guest molecules, at high concentrations migration within the cage and guest–guest interactions with other molecules become increasingly dominant influences on the diffusion coefficient and make the guest–zeolite interaction less important for both model A and model B.
机译:对甲烷在LTA型沸石结构(按照IZA命名法)中的扩散的研究表明,文献中存在不同类型的甲烷-沸石电势,其中在统一原子模型中处理甲烷。一组势能(称为模型A)的甲烷氧直径为3.14 A,而另一组势能参数(模型B)的值更大,为3.46A。Fritzsche和其同事(1993年)表明,这些两个电位导致甲烷以无阳离子形式的沸石A穿过甲烷穿过八环窗口时,产生两个截然不同的高能垒。在此,我们计算自扩散率(D)随载荷(c)的变化。这两种类型的电势,表明直径的这种细微变化从质量上改变了浓度依赖性:因此,对于模型A,D随着c单调下降,而对于模型B D增大并经历最大值,最后减小。在分子水平上详细研究了两种模型在高负荷下的扩散系数令人惊讶的一致性。对不同温度的模拟揭示了自扩散系数的阿伦尼乌斯行为。发现表观活化能随负载而变化。我们得出的结论是,除了保持架到保持架的跃迁(这对于来宾分子的迁移至关重要)外,在高浓度下,在保持架内的迁移以及来宾与客体之间的相互作用与其他分子的相互作用逐渐成为影响扩散系数的主要因素,并使来宾–沸石相互作用对于模型A和模型B都不太重要。

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