首页> 外文期刊>The Journal of Chemical Physics >MODELING THE CONCENTRATION DEPENDENCE OF DIFFUSION IN ZEOLITES .2. KINETIC MONTE CARLO SIMULATIONS OF BENZENE IN NA-Y
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MODELING THE CONCENTRATION DEPENDENCE OF DIFFUSION IN ZEOLITES .2. KINETIC MONTE CARLO SIMULATIONS OF BENZENE IN NA-Y

机译:模拟沸石中扩散的浓度相关性; 2。 NA-Y中苯的动力学蒙特卡罗模拟

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摘要

We have performed kinetic Monte Carlo simulations of benzene diffusion in Na-Y at finite loadings for various temperatures to test the analytical theory presented in Paper I, immediately preceding this paper. Our theory and simulations assume that benzene molecules jump among S-II and W sites, located near Na+ ions in 6-rings and in 12-ring windows, respectively. The theory exploits the fact that supercages are identical on average, yielding D-theta = 1/6k(theta)a(theta)(2) = kappa a(theta)(2)/6[tau(1)][1 + K-eq(1-->2)], where k(theta) is the cage-to-cage rate coefficient, K-eq(1-->2) is the W-->S-II equilibrium coefficient, [tau(1)] is the mean W site residence time, and kappa is the transmission coefficient for cage-to-cage motion. The simulations use fundamental rate coefficients calculated at infinite dilution for consistency with the theory in Paper I. Our theory for k(theta), K-eq(1-->2) and [tau(1)] agrees quantitatively with simulation for various temperatures and loadings. The simulated transmission coefficient is nearly 1/2 for all but the highest loadings, qualitatively validating our mean field approximation. Comparison between our theory and experimental data shows excellent qualitative agreement with tracer zero-length column data, but also shows qualitative disagreement with, both pulsed field gradient NMR and frequency response data. (C) 1997 American Institute of Physics. [References: 29]
机译:我们已经完成了在各种温度下有限载荷下Na-Y中苯扩散过程的动力学Monte Carlo模拟,以测试紧接本文之前的论文I中介绍的分析理论。我们的理论和模拟假设苯分子在S-II和W位点之间跳跃,分别位于6环和12环窗口中的Na +离子附近。该理论利用了以下事实:超笼平均相同,得出D-theta = 1 /6kθaaθ(2)=κaθ(2)/ 6 [τ(1)] [1 + K-eq(1-> 2)],其中k(theta)是笼对笼比率系数,K-eq(1-> 2)是W-> S-II平衡系数,[ tau(1)]是W位置的平均停留时间,而kappa是笼到笼运动的传递系数。为了与论文I中的理论一致,该模拟使用在无限稀释下计算的基本速率系数。我们的k(theta),K-eq(1-> 2)和[tau(1)]的理论与各种模拟的定量吻合温度和负载。除最高载荷外,所有情况下的模拟传输系数均接近1/2,从而定性地验证了我们的平均场近似。我们的理论和实验数据之间的比较表明,与示踪剂零长度色谱柱数据的定性非常吻合,但与脉冲场梯度NMR和频率响应数据的定性也不同。 (C)1997美国物理研究所。 [参考:29]

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