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甲烷输运与弛豫性质的计算。II. 热导率、热磁效应、体黏滞系数与核自旋弛豫

Calculation of the transport and relaxation properties of methane. II. Thermal conductivity, thermomagnetic effects, volume viscosity, and nuclear-spin relaxation.

作者信息

Hellmann Robert, Bich Eckard, Vogel Eckhard, Dickinson Alan S, Vesovic Velisa

机构信息

Institut für Chemie, Universität Rostock, D-18059 Rostock, Germany.

出版信息

J Chem Phys. 2009 Mar 28;130(12):124309. doi: 10.1063/1.3098317.

Abstract

Transport properties of pure methane have been calculated in the rigid-rotor approximation using the recently proposed intermolecular potential energy hypersurface [R. Hellmann et al., J. Chem. Phys. 128, 214303 (2008)] and the classical-trajectory method. Results are reported in the dilute-gas limit for the temperature range of 80-1500 K. The calculated thermal conductivity values are in very good agreement with the measured data and correlations. In the temperature range of 310-480 K the calculated values underestimate the best experimental data by 0.5%-1.0%. We suggest that the calculated values are more accurate, especially at low and high temperatures, than the currently available correlations based on the experimental data. Our results also agree well with measurements of thermal transpiration and of the thermomagnetic coefficients. We have shown that although the dominant contribution to the thermomagnetic coefficients comes from the Wjj polarization in the spherical approximation, the contribution of a second polarization, Wj, cannot be neglected nor can a full description of the Wjj polarization. The majority of the volume viscosity measurements around room temperature are consistent with the calculated values but this is not the case at high and low temperatures. However, for nuclear-spin relaxation the calculated values consistently exceed the measurements, which are mutually consistent within a few percent.

摘要

利用最近提出的分子间势能超曲面[R. Hellmann等人,《化学物理杂志》128, 214303 (2008)]和经典轨迹方法,在刚性转子近似下计算了纯甲烷的输运性质。报告了80 - 1500 K温度范围内稀薄气体极限下的结果。计算得到的热导率值与测量数据及关联式非常吻合。在310 - 480 K温度范围内,计算值比最佳实验数据低0.5% - 1.0%。我们认为,与目前基于实验数据的关联式相比,计算值更准确,尤其是在低温和高温下。我们的结果也与热扩散和热磁系数的测量结果吻合良好。我们已经表明,尽管热磁系数的主要贡献来自球近似中的Wjj极化,但第二极化Wj的贡献不可忽略,对Wjj极化的完整描述也不可忽略。室温附近的大多数体黏度测量值与计算值一致,但在高温和低温下并非如此。然而,对于核自旋弛豫,计算值始终超过测量值,测量值在百分之几的范围内相互一致。

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