Abstract

Peter Debye and Erich Huckel had developed a theory for the ionic activity coefficients in dilute solutions of strong electrolytes some 95 years ago [1]. Their limiting law still stands and is confirmed as close to reality in many experiments. In a previous article [2], it is shown that these limiting activity coefficients arise because the electrical contribution in the electrochemical potential of ionic species is overestimated traditionally with a factor 2. The smaller value removes inconsistencies in the models and complies better with the basic electrostatic principles. In this article further evidence is given in support of this alternative description. As consequence the dilute activity coefficients become unity, e.g. are removed, which means that the electrochemical potential of ions in dilute solutions is expressed directly in concentration, instead of activity, which simplifies modelling in such dilute solutions.

Highlights

  • The behavior of a strong electrolyte in the limit of high dilution is given by the formulae due to Debye and Hückel [1]

  • Peter Debye and Erich Hückel had developed a theory for the ionic activity coefficients in dilute solutions of strong electrolytes some 95 years ago [1]

  • As consequence the dilute activity coefficients become unity, e.g. are removed, which means that the electrochemical potential of ions in dilute solutions is expressed directly in concentration, instead of activity, which simplifies modelling in such dilute solutions

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Summary

Introduction

The behavior of a strong electrolyte in the limit of high dilution is given by the formulae due to Debye and Hückel [1]. This publication gives a discussion and additional information in support of the theory

Thermodynamics
Debye-Hückel Model
Electro-Capillarity
Linear Superposition Principle
Assembly of Charges
Cyclotron
Modelling the Electrical Interaction Term
Electrical Work in an Electrochemical Cell
Semi-Permeable Membrane
Extrapolation to Standard States at Infinite Dilution
Summary
Discussion
Full Text
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