首页> 外文期刊>The Journal of Chemical Physics >Electric conductivities of 1:1 electrolytes in liquid methanol along the liquid-vapor coexistence curve up to the critical temperature.I.NaCI,KCI,and CsCI solutions
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Electric conductivities of 1:1 electrolytes in liquid methanol along the liquid-vapor coexistence curve up to the critical temperature.I.NaCI,KCI,and CsCI solutions

机译:液态甲醇中1:1电解质的电导率沿着液态蒸汽共存曲线达到临界温度.NaCl,KCI和CsCI溶液

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The molar conductivities A of NaCl,KCl,and CsCl in liquid methanol were measured in the concentration range of(0.3-2.0)X10~-3 mol dm~-3 and the temperature range of 60-240 deg C along the liquid-vapor coexistence curve.The temperature range corresponds to the solvent density range of(2.78-1.55)rho,where rho_c=0.2756 g cm~-3 is the critical density of methanol.The concentration dependence of A at each temperature and density(pressure)has been analyzed by the Fuoss-Chen-Justice equation to obtain the limiting molar conductivity LAMBDA~0 and the molar association constant K_A.For all the electrolytes studied,LAMBDA~0 increased almost linearly with decreasing density at densities above 2.0_rho_c,while the opposite tendency was observed at lower densities.The relative contribution of the nonhydrodynamic effect on the translational friction coefficient zeta was estimated in terms of LAMBDA zeta/zeta,where the residual friction coefficient LAMBDA zeta is the difference between zeta and the Stokes friction coefficient zeta.At densities above 2.0_rho_c,LAMBDA zeta/zeta increased with decreasing density though zeta and LAMBDA zeta decrease,and the tendencies are common for all the ions studied.The density dependences of zeta and LAMBDA zeta/zeta were explained well by the Hubbard-Onsager(HO)dielectric friction theory based on the sphere-in-continuum model.At densities below 2.0_rho-c,however,the experimental results cannot be explained by the HO theory.
机译:在(0.3-2.0)X10〜-3 mol dm〜-3的浓度范围内以及沿液体蒸气的温度范围为60-240℃下测量NaCl,KCl和CsCl在液态甲醇中的摩尔电导率A温度范围对应于(2.78-1.55)rho的溶剂密度范围,其中rho_c = 0.2756 g cm〜-3是甲醇的临界密度.A在各个温度和浓度(压力)下的浓度依赖性用Fuoss-Chen-Justice方程分析得出极限摩尔电导率LAMBDA〜0和摩尔缔合常数K_A。对于所有研究的电解质,当密度大于2.0_rho_c时,LAMBDA〜0随密度的降低几乎呈线性增加,而相反非流体力学效应对平移摩擦系数zeta的相对贡献是根据LAMBDA zeta / zeta估算的,其中残余摩擦系数LAMBDA zeta是zeta与St之间的差密度大于2.0_rho_c时,虽然zeta和LAMBDA zeta降低,但LAMBDA zeta / zeta随密度的降低而增加,并且所有研究离子的趋势都相同。很好地解释了zeta和LAMBDA zeta / zeta的密度依赖性。通过基于连续球模型的Hubbard-Onsager(HO)介电摩擦理论。然而,在密度低于2.0_rho-c时,HO理论无法解释实验结果。

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