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首页> 外文期刊>The Journal of Chemical Physics >MODELING THE CONCENTRATION DEPENDENCE OF DIFFUSION IN ZEOLITES .1. ANALYTICAL THEORY FOR BENZENE IN NA-Y
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MODELING THE CONCENTRATION DEPENDENCE OF DIFFUSION IN ZEOLITES .1. ANALYTICAL THEORY FOR BENZENE IN NA-Y

机译:模拟沸石中扩散的浓度依赖性1。 NA-Y中苯的分析理论

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We have developed an analytical expression for the diffusion coefficient of benzene in Na-Y at finite loadings in terms of fundamental rate coefficients. Our theory assumes that benzene molecules jump among S-II and W sites, located near Na+ ions in 6-rings and in 12-ring windows, respectively. We assume that instantaneous occupancies in different supercages are identical, a mean field approximation yielding D-theta = 1/6k(theta)a(theta)(2) where a(theta) congruent to 11 Angstrom is the mean intercage jump length and 1/k(theta) is the mean supercage residence time, We show that k(theta) = kappa.k(1).P-1, where P-1 is the probability of occupying a W site, k(1) is the total rate of leaving a W site, and kappa is the transmission coefficient for cage-to-cage motion. We assume kappa = 1/2 for all loadings, and derive analytical formulas for the T and theta dependencies of k(1) and P-1, assuming that S-II and W site occupancies are either 0 or 1 and that benzenes do not otherwise interact, Exact expressions for P-1 in the canonical and grand canonical ensembles are related for finite systems with a new correspondence rule. For theta < 2/3, the S-II-->W-->S-II process contributes no loading dependence to k(theta), while the S-II-->W-->W process gives an increasing loading dependence of 1/(2-3 theta), For theta > 2/3, k(theta) initially increases due to enhanced W population, then decreases due to blocking of target W sites. In the article that follows this one we show that our theory agrees quantitatively with simulation, and agrees qualitatively with experiment for low to moderate loadings. (C) 1997 American Institute of Physics. [References: 55]
机译:我们已经根据基本速率系数,针对有限载荷下Na-Y中苯的扩散系数开发了一个解析表达式。我们的理论假设苯分子在S-II和W位点之间跳跃,这些位点分别位于6环和12环窗口中的Na +离子附近。我们假设不同超笼中的瞬时占用是相同的,平均场近似产生D-theta = 1 /6kθaaθ(2),其中aθ等于11埃是平均笼间跳跃长度和1 / k(theta)是平均超笼停留时间,我们证明k(theta)= kappa.k(1).P-1,其中P-1是占据W位置的概率,k(1)是离开W位置的总速率,而kappa是笼对笼运动的传递系数。我们假设所有负载的kappa = 1/2,并推导了k(1)和P-1的T和theta依赖性的分析公式,假设S-II和W的位点占用为0或1,而苯不否则相互作用,规范和大规范合奏中P-1的精确表达式与具有新的对应规则的有限系统相关。对于theta <2/3,S-II-> W-> S-II过程对k(theta)的加载没有依赖性,而S-II-> W-> W过程给出的载荷增加1 /(2-3 theta)的依赖性,对于theta> 2/3,k(theta)最初由于W种群增加而增加,然后由于对目标W站点的阻塞而减少。在此之后的一篇文章中,我们证明了我们的理论在定量上与仿真吻合,在定性上与中低负荷的实验吻合。 (C)1997美国物理研究所。 [参考:55]

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