Hoshina Taka-Aki, Tanaka Kensuke, Tsuchihashi Noriaki, Ibuki Kazuyasu, Ueno Masakatsu
Department of Molecular Science and Technology, Faculty of Engineering, Doshisha University, Kyo-Tanabe, Kyoto 610-0321, Japan.
J Chem Phys. 2004 Nov 15;121(19):9517-25. doi: 10.1063/1.1797211.
The molar conductivities Lambda of KBr and KI in dilute methanol solutions were measured along the liquid-vapor coexistence curve up to the critical temperature (240 degrees C). The concentration dependence of Lambda in each condition was analyzed by the Fuoss-Chen-Justice equation to obtain the limiting molar conductivities and the molar association constants. Using the present data together with the literature ones, the validity of the Hubbard-Onsager (HO) dielectric friction theory based on the sphere-in-continuum model was examined for the translational friction coefficients zeta of the halide ions (the Cl(-), Br(-), and I(-) ions) in methanol in the density range of 2.989rho(c)> or =rho> or =1.506rho(c), where rho(c)=0.2756 g cm(-3) is the critical density of methanol. For all the halide ions studied, the friction coefficient decreased with decreasing density at rho>2.0rho(c), while the nonviscous contribution Deltazeta/zeta increased; Deltazeta was defined as the difference between zeta and the friction coefficient estimated by the Stokes law. The density dependence of zeta and Deltazeta/zeta were well reproduced by the HO theory at rho>2.0rho(c). The HO theory also explained the ion-size dependence of Deltazeta/zeta which decreased with ion-size at rho>2.0rho(c). At rho<2.0rho(c), on the other hand, the HO theory could not explain the density and the ion-size dependences of zeta and Deltazeta/zeta. These results indicated that the application limit of the HO theory lied about rho=2.0rho(c) which is the same as the application limit observed for the alkali metal ions. The present results were also compared with the results in subcritical aqueous solutions.
在稀甲醇溶液中,沿着液 - 气共存曲线直至临界温度(240℃)测量了溴化钾(KBr)和碘化钾(KI)的摩尔电导率Λ。通过福斯 - 陈 - 贾斯蒂斯方程分析了每种条件下Λ的浓度依赖性,以获得极限摩尔电导率和摩尔缔合常数。结合当前数据和文献数据,在甲醇密度范围为2.989ρ(c)≥ρ≥1.506ρ(c)(其中ρ(c)=0.2756 g cm⁻³是甲醇的临界密度)内,检验了基于连续介质中球体模型的哈伯德 - 昂萨格(HO)介电摩擦理论对卤离子(Cl⁻、Br⁻和I⁻离子)平移摩擦系数ζ的有效性。对于所有研究的卤离子,在ρ>2.0ρ(c)时,摩擦系数随密度降低而减小,而非粘性贡献Δζ/ζ增加;Δζ定义为ζ与由斯托克斯定律估算的摩擦系数之间的差值。在ρ>2.0ρ(c)时,HO理论很好地再现了ζ和Δζ/ζ的密度依赖性。HO理论还解释了在ρ>2.0ρ(c)时Δζ/ζ随离子大小的减小而减小的离子大小依赖性。另一方面,在ρ<2.0ρ(c)时,HO理论无法解释ζ和Δζ/ζ的密度和离子大小依赖性。这些结果表明,HO理论的应用极限约为ρ = 2.0ρ(c),这与碱金属离子观察到的应用极限相同。还将当前结果与亚临界水溶液中的结果进行了比较。