Bv. Derjaguin, A THEORY OF THE HETEROCOAGULATION, INTERACTION AND ADHESION OF DISSIMILAR PARTICLES IN SOLUTIONS OF ELECTROLYTES, Progress in Surface Science, 43(1-4), 1993, pp. 60-73
The theory of interaction of charged surfaces in electrolyte solutions
based on computing the energy of overlapping of ionic atmospheres has
up till now been applied only to the symmetrical case of two equally
charged surfaces, or to wetting films with zero charge at their outer
boundary when it is easy to reduce this system to the symmetric one. B
ut there exist many phenomena, for instance coagulation of mixtures of
sols, coacervation, dyeing, flotation, etc., which require considerat
ion of the asymmetric case of unequally charged surfaces. Using the me
thod of '' isodynamic curves '' it is possible to obtain the solution
of the problem for any electrolyte and any constant value of the surfa
ce potentials. The most important property of electric repulsion of su
rfaces having charges of like signs is the existence of a maximum valu
e of the repulsion at a definite gap-width between both surfaces which
is independent of the maximum potentials of both surfaces. This rule
holds strictly being independent of the form of either surface. Divers
e criteria of stability are found theoretically. Two fundamentally dis
tinct cases should be distinguished according to whether the net resul
t of van der Waals' interactions leads to mutual attraction or mutual
repulsion of both bodies-the latter case being impossible when both bo
dies are similar in material. In the former case a modification of Eil
ers and Korff's rule is given, which is adapted to the case when one s
urface remains always strongly charged and the charge of the other one
may acquire any value near to zero. In the other case the adhesion of
surfaces or coagulation is only possible when the charges of both sur
faces have unlike signs and the electrolyte concentration is not very
high. When in addition both surfaces are strongly charged, an equation
is obtained giving the critical concentration below which coagulation
begins. This equation is very similar in form to that deduced by Land
au and myself and includes the modified Hardy-Schulze's and Wolfe-Ostw
ald's rules, but in contrast to it contains the valencies of anions an
d cations symmetrically. Such a reversed Hardy-Schulze's rule is in ac
cordance with the experiments of Frumkin, Gorodetskaja and Titijevskaj
a on adhesion of mercury drops to glass in electrolyte solutions on di
lution. Both these experiments and the theory developed can explain th
e mechanism of the bipolar coacervation. The present theory of interac
tion of unlike surfaces is in accordance with many facts in the fields
of heterocoagulation and mutual coagulation of sol mixtures. For inst
ance, this theory explains the existence of group coagulation in some
cases and disorder coagulation-in other ones, the fixation of dye part
icles prior to the onset of homogeneous coagulation, and many other ph
enomena.