ABSTRACT

Attraction between two indentical objects uniformly charged in

solution seems intuitively surprising on one hand because we

know that such objects do repel in vacuum and on another hand

because this simple mental picture is still preserved within the

Poisson-Boltzmann (PB) theory [40, 43, 47]. We recall that the PB

theory is a mean field approximation [39] of a primitive model of

electrolytes [16] in which ions are point-like and solvent is simply

a uniform medium of dielectric constant ε. Attraction mechanisms

mediated by counterions require therefore to modify at least one

of the aforementioned assumptions. We will see that one can find

attraction by (a) finding a situation in which two nonuniformly like

charged objects can attract each other even in vacuum, (b) adopting

another theoretical approximation for the samemodel of electrolyte,

and (c) changing the model for the ions.