离子-离子关联在导出德拜-赫克尔方程时通过线性化Poisson-Boltzmann方程而丢失
Gabriel M Silva1, Xiaodong Liang1, Georgios M Kontogeorgis1
1Center for Energy Resources Engineering, Department of Chemical and Biochemical Engineering, Technical University of Denmark, Kgs. Lyngby, Denmark.
The Journal of chemical physics
|January 19, 2024
概括
离子关联常数来自Poisson-Boltzmann方程的差异,解释了稀释溶液中德拜-赫克尔限制定律的偏差.
科学领域:
- 物理化学 物理化学
- 电化学 电化学 电化学
- 解决方案理论 解决方案理论
背景情况:
- 德拜-赫克尔限制定律为电解质行为提供了一个基本模型.
- 了解离子-离子相互作用对于准确预测溶液性质至关重要.
- 需要更高阶的静电理论来捕捉复杂的现象,如离子协会.
研究的目的:
- 将离子关联常数归因于Poisson-Boltzmann完全方程和线性方程之间的差异.
- 为德拜-赫克尔限制定律的负偏差提供理论基础.
- 在严格的理论框架内引入埃贝林关联常数.
主要方法:
- 对Poisson-Boltzmann方程的分析近似解的导数.
- 从近似的解决方案计算赫尔姆霍尔茨自由能量和活动系数.
- 与质量作用定律原理进行比较,以导出关联常数.
主要成果:
- 离子关联常数与完整的和线性化的Poisson-Boltzmann方程之间的差异直接相关.
- 衍生模型成功地解释了德拜-赫克尔限制定律的负偏差.
- 通过这种理论方法得到了埃贝林关联常数.
结论:
- 静电离子-离子相互作用模型忽略了更高阶效应,错过了离子协会的贡献.
- 离子联结是一种关键的物理现象,可以解释稀释电解质溶液中的偏差.
- 这项工作弥合了简化模型和复杂的静电理论之间的差距.
更多相关视频
相关概念视频
Factors Affecting Activity Coefficient
800
The extended Debye-Hückel equation indicates that the activity coefficient of an ion in an aqueous solution at 25°C depends on three partially interdependent properties: the ionic strength of the solution, the charge of the ion, and the ion size.
The activity coefficient value for an ion is close to one when the solution has almost zero ionic strength, i.e., when the solution shows close to ideal behavior. As the ionic strength of the solution increases from 0 to 0.1 mol/L, a...
The activity coefficient value for an ion is close to one when the solution has almost zero ionic strength, i.e., when the solution shows close to ideal behavior. As the ionic strength of the solution increases from 0 to 0.1 mol/L, a...
800
Poisson's And Laplace's Equation
2.9K
The electric potential of the system can be calculated by relating it to the electric charge densities that give rise to the electric potential. The differential form of Gauss's law expresses the electric field's divergence in terms of the electric charge density.
2.9K
The de Broglie Wavelength
25.9K
In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
25.9K
The Bohr Model
53.9K
Following the work of Ernest Rutherford and his colleagues in the early twentieth century, the picture of atoms consisting of tiny dense nuclei surrounded by lighter and even tinier electrons continually moving about the nucleus was well established. This picture was called the planetary model since it pictured the atom as a miniature “solar system” with the electrons orbiting the nucleus like planets orbiting the sun. The simplest atom is hydrogen, consisting of a single proton as...
53.9K
Potential Due to a Polarized Object
410
A neutral atom consists of a positively charged nucleus surrounded by a negatively charged electron cloud. When placed in an external electric field, the external electric force pulls the electrons and nucleus apart, opposite to the intrinsic attraction between the nucleus and the electrons. The opposing forces balance each other with a slight shift between the center of masses of the nucleus and the electron cloud, resulting in a polarized atom. On the other hand, a few molecules, like water,...
410
The Quantum-Mechanical Model of an Atom
42.3K
Shortly after de Broglie published his ideas that the electron in a hydrogen atom could be better thought of as being a circular standing wave instead of a particle moving in quantized circular orbits, Erwin Schrödinger extended de Broglie’s work by deriving what is now known as the Schrödinger equation. When Schrödinger applied his equation to hydrogen-like atoms, he was able to reproduce Bohr’s expression for the energy and, thus, the Rydberg formula governing hydrogen spectra.
42.3K


