Gonzalez Jorge, Devi R Nandini, Wright Paul A, Tunstall David P, Cox Paul A
School of Chemistry, University of St. Andrews, St. Andrews, Fife, United Kingdom.
J Phys Chem B. 2005 Nov 24;109(46):21700-9. doi: 10.1021/jp052590z.
(2)H wide-line NMR has been used, in conjunction with molecular dynamics simulations where appropriate, to follow the reorientation of the monoaromatic compounds benzene, toluene, and p-xylene within the one-dimensional channels of the alpha- and beta-polymorphs of aluminum methylphosphonate, Al(2)(CH(3)PO(3))(3). Variable-temperature, static, (2)H NMR spectra of adsorbed d(6)-benzene, d(3)-, d(5)-, and d(8)-toluenes, and d(3),d(3)-p-xylene were matched by line shape simulation. The motion of p-xylene in both polymorphs is approximated by the long axis of the molecule describing a cone within the channels, the half-angle of which is greater for the slightly wider channels in AlMePO-beta (27-30 degrees cf. 18-19 degrees). The (2)H NMR of d(3)-toluene is simulated using a similar model, whereas the signal from aromatic deuterons in d(5)- and d(8)-toluenes is simulated by a ring undergoing 2pi/3 flips around the para axis. The reorientation of benzene shows the largest differences between the two pore structures. In AlMePO-beta it tumbles with little restriction, although at low temperatures the spectral details are better matched by allowing the molecule to spend a greater proportion of its time closer to the wall. In AlMePO-alpha the much broader line shape arises from constrained motion within the strongly triangular channels. Molecular dynamics simulations of benzene in the two structures confirm the differences. They support a model for benzene in AlMePO-alpha where its motion is restricted to rotations about its 6-fold axis and 2pi/3 jumps between symmetry-related sites in the pores, so that the plane of the aromatic ring remains approximately parallel to the c-axis.
(2)宽线核磁共振已与分子动力学模拟(在适当情况下)结合使用,以跟踪单芳香族化合物苯、甲苯和对二甲苯在甲基膦酸铝α和β多晶型物的一维通道内的重新取向,即Al(2)(CH(3)PO(3))(3)。通过线形模拟匹配了吸附的d(6)-苯、d(3)-、d(5)-和d(8)-甲苯以及d(3),d(3)-对二甲苯的变温静态(2)H核磁共振谱。在两种多晶型物中,对二甲苯的运动可近似为分子的长轴在通道内描绘一个圆锥,对于AlMePO-β中稍宽的通道,其半角更大(27 - 30度,相比之下AlMePO-α中为18 - 19度)。d(3)-甲苯的(2)H核磁共振谱使用类似模型进行模拟,而d(5)-和d(8)-甲苯中芳香族氘核的信号则通过环围绕对位轴进行2π/3翻转来模拟。苯的重新取向在两种孔结构之间显示出最大差异。在AlMePO-β中,它几乎不受限制地翻滚,尽管在低温下,通过允许分子在更靠近壁的位置花费更大比例的时间,光谱细节能得到更好的匹配。在AlMePO-α中,更宽的线形是由强三角形通道内的受限运动引起的。两种结构中苯的分子动力学模拟证实了这些差异。它们支持AlMePO-α中苯的一种模型,即其运动限于围绕其六重轴的旋转以及孔中对称相关位点之间的2π/3跳跃,使得芳香环平面大致保持与c轴平行。