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NMR investigations of hexamethyldisilane confined in controlled pore glasses: Pore size distribution and molecular dynamics studies

机译:限制在受控孔玻璃中的六甲基乙硅烷的NMR研究:孔径分布和分子动力学研究

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In this work, the melting-point depression and molecular dynamics of hexamethyldisilane confined within five controlled pore glasses, with mean diameters ranging from 7.9 to 23.9 run, are studied by high-field (9.4 T) nuclear magnetic resonance (NMR), and the results are discussed with reference to the bulk substance. The melting-point depression in pores with radius R follows the simplified Gibbs-Thompson equation DeltaT = k(p)/(R - s) with a k(rho) value of 74 K . nm and an value of I nm. To our knowledge, this is the first time the k(rho) value of hexamethyldisilane is reported. Proton spin-lattice relaxation times (T), spin-spin relaxation times (T-2), and diflusivities (D) are reported as a function of temperature. The confinement in the pores gives rise to substantial changes in the molecular dynamics and the phase behavior. The line-shape measurements reveal a two-phase system assigned to a relatively mobile component at the pore walls and a crystalline solid at the center of the pores. However, the T, measurements show that the mobile phase also embraces a minor component attributed to nonfrozen liquid in pockets or micropores. The diffusivity of the major narrowline component is approximately three orders of magnitude larger than that in the plastic bulk phase, reflecting fast diffusion of mobile molecules. Below the melting region, T, of the narrow line is significantly shorter than T-1 of the broad line, suggesting that the molecular reorientation is more hindered close to the surface than at the center of the pore. [References: 24]
机译:在这项工作中,通过高场(9.4 T)核磁共振(NMR)研究了平均直径范围从7.9到23.9 run的五个受控孔玻璃中的六甲基乙硅烷的熔点降低和分子动力学。将参考散装物质讨论结果。半径为R的孔中的熔点降低遵循简化的Gibbs-Thompson方程DeltaT = k(p)/(R-s),k(rho)值为74K。 nm和I nm的值。据我们所知,这是首次报告六甲基乙硅烷的k(rho)值。据报道,质子自旋晶格弛豫时间(T),自旋自旋弛豫时间(T-2)和扩散性(D)是温度的函数。孔中的封闭引起分子动力学和相行为的实质性变化。线形测量显示出两相系统,该两相系统分配给孔壁处相对易移动的组分,并分配给孔中心的结晶固体。然而,T 1测量表明流动相还包含归因于袋或微孔中未冻结液体的微量成分。主要窄线成分的扩散率比塑料本体相的扩散率大约大三个数量级,反映了移动分子的快速扩散。在熔融区域下方,窄线的T明显短于宽线的T-1,这表明靠近表面的分子重新定向比在孔的中心更受阻碍。 [参考:24]

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