Fractal Morphology and Breakage of DLCA and RLCA Aggregates.

Latex aggregates, formed in 1 M McIlvaine buffer solution and 0.2 M NaCl solution, have been characterized in terms of aggregate size distribution and fractal morphology. This was achieved using three sizing techniques (image analysis, laser scattering, and electrical sensing) in which size distributions and fractal properties of the aggregates were measured. Estimates of fractal dimensions were made using the two-slope method based on dimensional analysis and the small-angle light scattering method. Aggregate suspensions were prepared using both water and a mixture of heavy water/ water as the solvent. The latter essentially eliminated sedimentation, which was observed after one day of aggregation when water alone was used as a solvent. Latex aggregates formed by diffusion-limited colloid aggregation (DLCA) and reaction-limited colloid aggregation (RLCA) had fractal dimensions close to 1.8 and 2.1, respectively. As observed through image analysis, DLCA aggregates possessed a loose tenuous structure, whereas RLCA aggregates were more compact. Disruption of both DLCA and RLCA aggregates has been investigated in laminar flow and turbulent capillary flow. The shear forces introduced by a laminar shear device with a shear rate up to 1711 s(-1) were unable to bring about aggregate breakup; shearing facilitates aggregate growth in the case of DLCA. However, latex aggregates were significantly disrupted after passage through a turbulent capillary tube at 95209 s(-1). Copyright 2000 Academic Press.

[1]  E. Pefferkorn,et al.  Modes of spontaneous and provoked cluster fragmentation , 1992 .

[2]  P. Ayazi Shamlou,et al.  Processing of Solid–Liquid Suspensions , 1993 .

[3]  R. C. Ball,et al.  Universality in colloid aggregation , 1989, Nature.

[4]  Andrew Harrison,et al.  Fractals in Chemistry , 1995 .

[5]  G. C. Paul,et al.  Characterisation of mycelial morphology using image analysis. , 1998, Advances in biochemical engineering/biotechnology.

[6]  E. Pefferkorn,et al.  Dynamics of latex aggregation. Modes of cluster growth , 1989 .

[7]  Huang,et al.  Limits of the fractal dimension for irreversible kinetic aggregation of gold colloids. , 1985, Physical review letters.

[8]  P. Elving,et al.  Preparation of Buffer Systems of Constant Ionic Strength , 1956 .

[9]  Ángel V. Delgado,et al.  Particle Size Distribution of Inorganic Colloidal Dispersions: A comparison of different techniques , 1991 .

[10]  W. Russel,et al.  Floc structure and growth kinetics for rapid shear coagulation of polystyrene colloids , 1991 .

[11]  J. Hunt Self-similar particle-size distributions during coagulation: theory and experimental verification , 1982, Journal of Fluid Mechanics.

[12]  David Avnir,et al.  The Fractal approach to heterogeneous chemistry : surfaces, colloids, polymers , 1989 .

[13]  V. Oles Shear-induced aggregation and breakup of polystyrene latex particles , 1992 .

[14]  A. Friboulet,et al.  Editorial: Whither catalytic antibodies? , 1998 .

[15]  E. Pefferkorn,et al.  Aggregation/fragmentation processes in unstable latex suspensions , 1990 .

[16]  M Al-Rubeai,et al.  Estimation of disruption of animal cells by turbulent capillary flow , 1993, Biotechnology and bioengineering.

[17]  D. Cannell,et al.  Restructuring of colloidal silica aggregates. , 1986, Physical review letters.

[18]  D. Shaw,et al.  Introduction to colloid and surface chemistry , 1970 .

[19]  Bruce E. Logan,et al.  Fractal dimensions of aggregates determined from steady-state size distributions , 1991 .

[20]  G. C. Paul,et al.  Characterising latex particles and fractal aggregates using image analysis , 1999 .