Ghorai Pradip Kr, Yashonath S
Solid State and Structural Chemistry Unit and Center for Condensed Matter Theory, Indian Institute of Science, Bangalore-560012, India.
J Phys Chem B. 2005 Mar 10;109(9):3979-83. doi: 10.1021/jp046121t.
Previous work investigating the dependence of self-diffusivity, D, on the size of the guest diffusing within the porous solid such as zeolite has reported the existence of an anomalous maximum in the diffusion coefficient (J. Phys. Chem. 1994, 98, 6368). Two distinct regimes of dependence of D on sigma(gg), diameter of the guest were reported. D proportional to 1/sigma(gg)2, often referred to as linear regime (LR), is found when sigma(gg) is smaller than sigma(v), the diameter of the void. A maximum in D has been observed when sigma(gg) is comparable to sigma(v) and this regime is referred to as anomalous regime (AR). Here we report the intermediate scattering function for a particle from LR and AR in zeolite faujasite. A particle from LR exhibits a biexponential decay while a particle from AR exhibits a single-exponential decay at small k. Variation with k of the full width at half-maximum of the self-part of the dynamic structure factor is nonmonotonic for a particle in the linear regime. In contrast, this variation is monotonic for a particle in the anomalous regime. These results can be understood in terms of the existence of energetic barrier at the bottleneck, the 12-ring window, in the path of diffusion. They provide additional signatures for the linear regime and anomalous regimes and therefore for levitation effect (LE).
此前关于自扩散系数D与在诸如沸石等多孔固体中扩散的客体分子大小之间关系的研究工作报道了扩散系数中存在反常最大值(《物理化学杂志》,1994年,第98卷,6368页)。报道了D对客体分子直径σ(gg)的两种不同依赖关系。当σ(gg)小于孔隙直径σ(v)时,发现D与1/σ(gg)²成正比,这通常被称为线性区域(LR)。当σ(gg)与σ(v)相近时,观察到D出现最大值,此区域被称为反常区域(AR)。在此,我们报道了八面沸石中来自线性区域和反常区域的粒子的中间散射函数。来自线性区域的粒子表现出双指数衰减,而来自反常区域的粒子在小k值时表现出单指数衰减。对于处于线性区域的粒子,动态结构因子自部分半高宽随k的变化是非单调的。相比之下,对于处于反常区域的粒子,这种变化是单调的。这些结果可以通过扩散路径中瓶颈处(12元环窗口)存在能量势垒来理解。它们为线性区域和反常区域提供了额外的特征,因此也为悬浮效应(LE)提供了额外特征。