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首页> 外文期刊>The journal of physical chemistry, C. Nanomaterials and interfaces >Dynamic Properties of Water Molecules within an Au Nanotube with Different Bulk Densities
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Dynamic Properties of Water Molecules within an Au Nanotube with Different Bulk Densities

机译:具有不同堆积密度的金纳米管中水分子的动力学性质

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Molecular dynamics simulation is used to investigate the dynamic properties of water molecules inside an Au nanotube in different water densities. From the oxygen density profiles, some characteristic peaks appear at specific regions. In order to observe the dynamical behaviors of water molecules in different portions in the Au nanotube, these specific peaks are divided into three regions-I, II, and III-which are 0-4, 4-7, and 7-10 A, respectively, as measured from the center of the tube to the inside wall of the tube. Since the strength of hydrogen bonds between water molecules within regions I and II can overcome the interaction between the Au nanotube and the water molecules within those regions, the major peaks of the region I and II spectra are similar to those of bulk water. However, the strength of hydrogen bonds between water molecules within region III cannot overcome the interaction between the Au nanotube and the water molecules within that region, so the major peak of the region III spectrum shifts to a higher frequency. In addition, the shoulder structure, which can be observed in the spectra of those regions at different densities, exists at high frequency. In the vibration spectra for region I, the shoulders at each different density appears at around 100 cm~(-1), and those of regions II and III at different densities occur around 200 cm~(-1). This is because the shoulder corresponds to O-O stretching intermolecular vibrations of pairs of H-bonded molecules, so the shoulder will gradually appear as the average number of hydrogen bonds increases. Finally, the shoulder in the region I spectrum completely disappears at a bulk density of 0.8 cm~(-1).
机译:分子动力学模拟用于研究金纳米管内部不同水密度下水分子的动力学特性。从氧密度分布图中,某些特征峰出现在特定区域。为了观察金纳米管中不同部分的水分子动力学行为,这些特定的峰分为三个区域-I,II和III-,分别为0-4、4-7和7-10 A,从管子的中心到管子的内壁分别测量。由于区域I和II中水分子之间的氢键强度可以克服金纳米管与这些区域中水分子之间的相互作用,因此区域I和II光谱的主峰与散装水的主峰相似。但是,区域III中水分子之间的氢键强度无法克服Au纳米管与该区域中水分子之间的相互作用,因此区域III光谱的主峰移至更高的频率。另外,在不同密度的那些区域的光谱中可以观察到的肩部结构以高频率存在。在区域I的振动谱中,每个不同密度的肩部出现在100 cm〜(-1)左右,区域II和III的肩部出现在不同密度的200 cm〜(-1)附近。这是因为肩对应于H键合分子对的O-O拉伸分子间振动,因此随着平均氢键数的增加,肩将逐渐出现。最后,区域I光谱中的肩部以0.8 cm〜(-1)的堆积密度完全消失。

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