Ar. Gerson, The role of fuzzy interfaces in the nucleation, growth and agglomeration of aluminum hydroxide in concentrated caustic solutions, PROG CRYST, 43(2-3), 2001, pp. 187-220
Fundamental crystal growth theory relies on classical concepts of monomeric
addition at step sites on crystal surfaces. The nucleation and growth of c
rystalline aluminium hydroxide from concentrated caustic solutions does not
follow classical crystal growth mechanistic pathways. Numerous techniques
including static and dynamic light scattering, small angle X-ray and neutro
n scattering, cryovitirification transmission electron microscopy, rheology
and atomic force microscopy have been employed in the study of aluminium.
hydroxide crystallisation from concentrated caustic solutions. The observat
ions from these techniques have been interpreted on the basis polymer cryst
al growth theory, thermodynamic phase inversions analysis and entropically
driven insolubility.
The experimental observations can be interpreted on the basis that aluminiu
m hydroxide nuclei and crystals are surrounded by a diffuse interface which
grades in density from the crystalline aluminium hydroxide particle core t
o the surrounding solution. A mechanism for the nucleation and growth mecha
nisms of aluminium. hydroxide has been proposed: initial solution formation
of a loose polymeric network; clustering of this network followed by gradu
al densification to form amorphous nuclei; further densification of the cor
e of the nuclei to form crystallites and gradual densification but not crys
tallisation of the still amorphous diffuse interface.
The presence of this diffuse interface enables the slow agglomeration behav
iour of aluminium hydroxides particles in concentrated caustic liquors to b
e explained. In liquors of very high ionic strength (in this case up to 6 M
NaOH) particulate agglomeration would be expected to be rapid due to the s
mall double layer thickness as predicted by DLVO theory. During rapid growt
h the diffuse interface inhibits the sufficiently close approach of the den
se part of the particles to the point where attractive inter-particulate va
n der Waals forces would dominate and agglomeration would take place. As su
persaturation is depleted and the growth rate of the diffuse interface decr
eases but densification is still occurring the particles can approach more
closely and agglomeration will occur. Thus it is probable that the observed
agglomeration behaviour is supersaturation. and growth rate related.