Issue 0, 1979

Flow turbidity in colloidal kaolinite dispersions

Abstract

The optical transmission and turbidity of a colloidal dispersion of non-spherical particles depends on the number of particles per unit volume and the average extinction cross-section per particle. Laminar shear flow of the dispersion causes preferential orientation of the non-spherical particles and changes the average optical extinction cross-section per particle. The result is a velocity gradient dependence of the optical turbidity.

This paper describes apparatus designed to make accurate flow turbidity measurements with the velocity gradient direction either parallel or at right-angles to the incident light direction.

Results are presented for colloidal kaolinite clay particles dispersed in water and in a range of more viscous water + glycerol mixtures. A semi-empirical expression is developed which relates the turbidity to the velocity gradient by means of a time T and dimensionless parameter p. Values of T derived from the experimental results suggest that T is a relaxation time of an individual kaolinite particle averaged over the distribution of particle sizes in any particular clay fraction. The parameter p is found to be dependent on the polydispersity of the fraction, decreasing with increasing fraction breadth. The linear dependence of T on continuous phase viscosity indicates that the clay particles interact hydrodynamically with the continuous phase. The cubic dependence of T on the equivalent Stokes diameter (ESD) suggests that ESD is proportional to the face diameter of the plate-like kaolinite particles. The use of flow turbidity in colloidal particle size measurement is discussed, and the technique compared with that of flow birefringence.

Article information

Article type
Paper

J. Chem. Soc., Faraday Trans. 2, 1979,75, 767-779

Flow turbidity in colloidal kaolinite dispersions

J. V. Champion, G. H. Meeten and B. R. Moon, J. Chem. Soc., Faraday Trans. 2, 1979, 75, 767 DOI: 10.1039/F29797500767

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