首页> 外文会议>European research conference on molten salts >Mutual Diffusion Coefficients of the Systems (Rb,Ag)Cl and (AIk,Ag)NO_3 with Alk=Li, Na, K, Rb, and Cs, Measured with Interferometric Methods
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Mutual Diffusion Coefficients of the Systems (Rb,Ag)Cl and (AIk,Ag)NO_3 with Alk=Li, Na, K, Rb, and Cs, Measured with Interferometric Methods

机译:用干涉方法测量的系统(RB,Ag)Cl和(Aik,Ag)Cl和(Aik,Ag)NO_3的互扩散系数NO_3,用干涉方法测量

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Mutual diffusion coefficients of the systems (Rb,Ag)Cl and (Alk,Ag)NO_3 with Alk = Li, Na, K, Rb, and Cs are reported. Experiments in the nitrate systems were performed with either holographic real-time interferometry or Savart interferometry under free-diffusion boundary conditions. Initial diffusion boundaries were created using a flowing junction cell or bottom layer cells. Mutual diffusion coefficients in the system (Rb,Ag)Cl were measured with digital image holography, a newly developed interferometric technique. Some experiments were performed with Savart interferometry as an internal consistency check. In the nitrate systems diffusion data were collected in a temperature range from the melting points of the mixtures up to 603 K over the whole accessible concentration range. The D values are considered to be accurate to +-1-3 %. The results have been correlated using Arrhenius-type equations. Furthermore the concentration dependence of the mutual diffusion coefficient at 573 K is discussed. The data are fitted to parabolas of the form D = a_2x-2~2 + a_1x_2 + a_0. where x_2 denotes the mole fraction of the silver nitrate. For all systems, except (Li,Ag)NO_3, parameters a_2, a_1 and a_0 show a clear linear proportionality to the radii of the alkali ions. Trace diffusion coefficients are extrapolated and discussed. Mutual diffusion coefficients in the system (Rb,Ag)Cl with x_(AgCl) = 0.61 were measured in a temperature range between 573 K and 748 K. The results show an Arrhenius behaviour with D = (1.37 +- 0.10) m~2s~(-1) exp(-(20.7 +- 0.4) kJ mol~(-1)/(RT)).
机译:报道了具有Alk = Li,Na,K,Rb和Cs的系统(RB,Ag)Cl和(Al Ag)NO_3的互扩散系数。在自由扩散边界条件下通过全息实时干涉测量法或Savart干涉测量法进行硝酸盐系统的实验。使用流动的结电池或底层细胞创建初始扩散边界。用数字图像全息术测量系统(RB,AG)CL中的互扩散系数,新开发的干涉技术。用萨维特干涉测量法进行一些实验,作为内部一致性检查。在硝酸盐系统中,在从混合物的熔点的温度范围内收集在整个可接近的浓度范围内的混合物的熔点中的温度范围内收集。 D值被认为是准确到+ -1-3%。结果与Arhenius型方程相关。此外,讨论了在573k处的互扩散系数的浓度依赖性。数据适用于表单D = A_2X-2〜2 + A_1X_2 + A_0的抛物线。其中X_2表示银硝酸盐的摩尔分数。对于所有系统,除了(Li,Ag)No_3,参数A_2,A_1和A_0显示碱离子的半径的明显线性比例。跟踪扩散系数是外推和讨论的。在573k和748k的温度范围内测量系统(Rb,Ag)Cl中的互散分数= 0.61。结果显示了D =(1.37 + - 0.10)m〜2s的Arhenius行为〜(-1)exp( - (20.7±0.4)kj mol〜(-1)/(rt))。

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