Abstract

We study the adsorption–desorption transition of polyelectrolyte chains onto planar, cylindrical and spherical surfaces with arbitrarily high surface charge densities by massive Monte Carlo computer simulations. We examine in detail how the well known scaling relations for the threshold transition—demarcating the adsorbed and desorbed domains of a polyelectrolyte near weakly charged surfaces—are altered for highly charged interfaces. In virtue of high surface potentials and large surface charge densities, the Debye–Hückel approximation is often not feasible and the nonlinear Poisson–Boltzmann approach should be implemented. At low salt conditions, for instance, the electrostatic potential from the nonlinear Poisson–Boltzmann equation is smaller than the Debye–Hückel result, such that the required critical surface charge density for polyelectrolyte adsorption increases. The nonlinear relation between the surface charge density and electrostatic potential leads to a sharply increasing critical surface charge density with growing ionic strength, imposing an additional limit to the critical salt concentration above which no polyelectrolyte adsorption occurs at all. We contrast our simulations findings with the known scaling results for weak critical polyelectrolyte adsorption onto oppositely charged surfaces for the three standard geometries. Finally, we discuss some applications of our results for some physical–chemical and biophysical systems.

Highlights

  • In contrast to neutral polymers confined near interfaces [100,101,102], the adsorption of PE chains onto oppositely charged surface is controlled by an additional length scale, the Debye screening length, lD = 1 k

  • We present the results of computer simulations for the width of the adsorbed PE layer w obtained with the nonlinearly treated ES potential, see equations (A23) and (A33) for the spherical and cylindrical surfaces, respectively

  • We carried out extensive computer simulations to unravel the properties of electrostatically driven adsorption of flexible PE chains onto oppositely charged surfaces of arbitrarily high surface charge densities

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Summary

Introduction

The adsorption of charged polymers or polyelectrolytes (PEs) onto oppositely charged planar and curved interfaces [1,2,3,4,5,6] attracted the attention of a large number of theoretical [7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25,26,27,28,29,30,31,32,33,34], experimental [35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,53], and computer simulations [54,55,56,57,58,59,60,61,62,63,64,65,66,67,68,69,70,71,72,73,74,75,76,77,78,79] groups over the last decades. The electrostatic (ES) polymer-surface attraction is comparatively weak and the transition between adsorbed and desorbed chain conformations is governed by the interplay of the PE-surface attraction and the entropic penalty of chain confinement in the vicinity of the interface [2, 5], see figure 1 In this weak coupling limit the transition is quantified in terms of the critical surface charge density sc via its dependence on the reciprocal Debye screening length, κ. In contrast to neutral polymers confined near interfaces [100,101,102], the adsorption of PE chains onto oppositely charged surface is controlled by an additional length scale, the Debye screening length, lD = 1 k.

Model and approximations
Adsorption onto planar surfaces
Adsorption onto curved surfaces
Discussion and conclusions
Planar geometry We start with the solution for the dimensionless ES potential
Spherical geometry
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