Screening of strongly charged macroparticles in liquid electrolyte solutions

A modified Poisson-Boltzmann model has been proposed which makes it possible to describe the screening of strongly charged macroparticles in liquid electrolyte Z:Z solutions in the case when parameter B = ZeQ(0)/epsilonRTmuch greater than1 (Q(0) is the surface electric charge, T is the temperature, epsilon is the solution permittivity, and Z is the valence of ions) provided that the solution is dilute: kappaR equivalent to (8piZ(2)e(2)n(i0)/epsilonT)(1/2)Rmuch less than1 (n(i0) is the equilibrium number density of ions). It is assumed that the charge Q(0) of a macroparticle appears as a result of adsorption of ions of a certain polarity on its surface. Quantitative criteria of division of dissolved ions into capable and incapable of adsorption are formulated. For aqueous solutions, the adsorption mechanism always leads to values of Bmuch greater than1. It is shown that the charge inversion effect predicted by other authors on the basis of different models must be observed for such solutions for all Zgreater than or equal to1. The effect of Brownian movement of macroparticles on their screening is considered. It is shown that viscous forces emerging during such movement lead to peripheral destruction ("washing out") of the screening ionic shell of macroparticles and, as a result, to violation of their electroneutrality. This results in the emergence of two types of oppositely charged compound particles with small radii close to R and with radii much larger than R, the charge polarity of the latter being opposite to the polarity of Q(0) . It is found that both types of ions of compound particles obey the "law of distribution" of the mean energy of their electric field, expressed by formula (29). The problem of ionic screening of gas bubbles accompanied by the formation of bubstons (bubbles stabilized by ions) is considered separately. It is shown that the bubston radius R in pure water and in aqueous solutions of electrolytes is equal to 14 nm irrespective of the ion number density n(i0). The value of n(i0) determines the number density n(b) of bubstons themselves, which are formed spontaneously under equilibrium conditions. (C) 2003 MAIK "Nauka/Interperiodica".