首页> 外文会议>International Conference of Computational Methods in Sciences and Engineering 2003 (ICCMSE 2003); Sep 12-16, 2003; Kastoria, Greece >ACCURATE THERMOPHYSICAL PROPERTIES OF NEAT GLOBULAR GASES AND THEIR BINARY MIXTURES DETERMINED BY MEANS OF AN ISOTROPIC TEMPERATURE-DEPENDENT POTENTIAL
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ACCURATE THERMOPHYSICAL PROPERTIES OF NEAT GLOBULAR GASES AND THEIR BINARY MIXTURES DETERMINED BY MEANS OF AN ISOTROPIC TEMPERATURE-DEPENDENT POTENTIAL

机译:用各向同性的温度相关势确定的精确球状气体及其二元混合物的热物理性质

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摘要

We present results on self-consistent calculations of second pVT- virial coefficients B(T), viscosity data η(T) and diffusion coefficients ρD for heavy globular gases (BF_3, CF_4, SiF_4, CCl_4, SiCl_4, SF_6, MoF_6, WF_6, UF_6, C(CH_3)_4, and Si(CH_3)_4) and their binary mixtures with globular gases, and Ar, Kr, and Xe, respectively. The calculations are performed mainly in the temperature range between 200 and 900K by means of isotropic n-6 potentials with explicitly temperature-dependent separation r_m(T) and potential well-depth ε(T). In the case of the pure gases the potential parameters at T = 0 K (ε, r_m n) and the enlargement of the first level radii δ are obtained solving an ill-posed problem of minimizing the squared deviations between experimental and calculated values normalized to their relative experimental error. The temperature dependence of the potential is a result of the influence of vibrational excitation on binary interactions. The interaction potential of the binary mixtures are obtained with simple combination rules from the potential parameters of the neat gases. In all cases we observe excellent reproduction of the experimental thermophysical properties of the neat gases and the binary mixtures.
机译:我们给出了重球状气体(BF_3,CF_4,SiF_4,CCl_4,SiCl_4,SF_6,MoF_6,WF_6, UF_6,C(CH_3)_4和Si(CH_3)_4)以及它们与球状气体以及Ar,Kr和Xe的二元混合物。这些计算主要是在200至900K的温度范围内,通过各向同性的n-6电位进行的,这些电位具有明显的温度相关距离r_m(T)和势阱深度ε(T)。在纯气体的情况下,获得了T = 0 K(ε,r_m n)处的势能参数和第一级半径δ的增大,从而解决了不适当地使实验值与计算值之间的平方偏差标准化为最小的不适定问题。它们的相对实验误差。电位的温度依赖性是振动激发对二元相互作用的影响的结果。二元混合物的相互作用势可以通过简单的组合规则从净气的势参数中获得。在所有情况下,我们都观察到纯净气体和二元混合物的实验热物理性质的出色再现。

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