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高温下沿共存曲线的水和有机溶剂的自扩散系数。

Self-diffusion coefficients for water and organic solvents at high temperatures along the coexistence curve.

作者信息

Yoshida Ken, Matubayasi Nobuyuki, Nakahara Masaru

机构信息

Institute for Chemical Research, Kyoto University, Uji, Kyoto 611-0011, Japan.

出版信息

J Chem Phys. 2008 Dec 7;129(21):214501. doi: 10.1063/1.3006420.

Abstract

The self-diffusion coefficients D for water, benzene, and cyclohexane are determined by using the pulsed-field-gradient spin echo method in high-temperature conditions along the liquid branch of the coexistence curve: 30-350 degrees C (1.0-0.58 g cm(-3)), 30-250 degrees C (0.87-0.56 g cm(-3)), and 30-250 degrees C (0.77-0.48 g cm(-3)) for water, benzene, and cyclohexane, respectively. The temperature and density effects are separated and their origins are discussed by examining the diffusion data over a wide range of thermodynamic states. The temperature dependence of the self-diffusion coefficient for water is larger than that for organic solvents due to the large contribution of the attractive hydrogen-bonding interaction in water. The density dependence is larger for organic solvents than for water. The difference is explained in terms of the van der Waals picture that the structure of nonpolar organic solvents is determined by the packing effect due to the repulsion or exclusion volumes. The dynamic solvation shell scheme [K. Yoshida et al., J. Chem. Phys. 127, 174509 (2007)] is applied for the molecular interpretation of the translational dynamics with the aid of molecular dynamics simulation. In water at high temperatures, the velocity relaxation is not completed before the relaxation of the solvation shell (mobile-shell type) as a result of the breakdown of the hydrogen-bonding network. In contrast, the velocity relaxation of benzene is rather confined within the solvation shell (in-shell type).

摘要

通过脉冲场梯度自旋回波方法,在共存曲线的液相分支上的高温条件下,测定了水、苯和环己烷的自扩散系数D:水为30 - 350℃(1.0 - 0.58 g·cm⁻³),苯为30 - 250℃(0.87 - 0.56 g·cm⁻³),环己烷为30 - 250℃(0.77 - 0.48 g·cm⁻³)。通过研究广泛热力学状态下的扩散数据,分离了温度和密度效应并讨论了其起源。由于水中吸引性氢键相互作用的巨大贡献,水的自扩散系数对温度的依赖性大于有机溶剂。有机溶剂的密度依赖性大于水。这种差异根据范德华图像来解释,即非极性有机溶剂的结构由排斥或排除体积引起的堆积效应决定。借助分子动力学模拟,应用动态溶剂化壳层方案[K. Yoshida等人,《化学物理杂志》127, 174509 (2007)]对平动动力学进行分子解释。在高温水中,由于氢键网络的破坏,速度弛豫在溶剂化壳层弛豫之前未完成(移动壳层类型)。相比之下,苯的速度弛豫相当局限于溶剂化壳层内(壳层内类型)。

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