Abstract

Like-charged macromolecules repel in electrolyte solutions that contain small (i.e. point-like) monovalent co- and counterions. Yet, if the mobile ions of one species are spatially extended instead of being point-like, the interaction may turn attractive. This effect can be captured within the mean-field Poisson-Boltzmann framework if the charge distribution within the spatially extended ions is accounted for. This has been demonstrated recently for rod-like ions. In the present work, we consider an electrolyte solution that is composed of monovalent point-like salt ions and uniformly charged spherical colloids, sandwiched between two planar like-charged surfaces. Minimization of the mean-field free energy yields an integral-differential equation for the electrostatic potential that we solve numerically within the linear Debye-Huckel limit. The free energy, which we calculate from the potential, indeed predicts attractive in- teractions for sufficiently large spherical colloids. We derive an approximate analytical expression for the critical colloid size, above which attraction between like-charged surfaces starts to emerge. (doi: 10.5562/cca1824)

Highlights

  • Interactions between like-charged macromolecules in electrolyte solutions are of fundamental importance in biological and biotechnological systems

  • We focus on the Debye-Hückel regime where the charge densities on both the extended planar surfaces and on the surfaces of the spherical colloids are small

  • The oscillations in Ψ (x) are accompanied by overcharging where the charge of the spherical colloids over-compensates the charges on the planar surfaces

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Summary

Introduction

Interactions between like-charged macromolecules in electrolyte solutions are of fundamental importance in biological and biotechnological systems. We consider an additional system of spatially extended ions, namely spherical colloids that carry a uniform surface charge density.

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