๐”– Bobbio Scriptorium
โœฆ   LIBER   โœฆ

Viscosity of a Dilute Suspension of Sodium Montmorillonite in a Electrostatically Stable Condition

โœ Scribed by Y. Adachi; K. Nakaishi; M. Tamaki


Publisher
Elsevier Science
Year
1998
Tongue
English
Weight
133 KB
Volume
198
Category
Article
ISSN
0021-9797

No coin nor oath required. For personal study only.

โœฆ Synopsis


mally observed for the suspension of charged colloid, is one The viscosity of a dilute suspension of sodium montmorillonite source of the electroviscous effect; the viscosity of the suspenunder dispersed conditions was measured as a function of electrosion exceeds that of an uncharged suspension.

lyte concentration using a capillary viscometer. Analyses were fo-It is known that there are three distinctive regimes of cused on the evaluation of electroviscous effects. The absence of electroviscous effect for the solution of macroions or the particle expansion due to swelling was confirmed by the Stokes suspension of charged colloidal particles when the fluid is diameter measured by photon correlation spectroscopy (PCS). The set in motion (2). The primary effect is caused by the resisintrinsic viscosity obtained was found to increase with an increase tance of ionic atmosphere against fluid distortion of shear. of reciprocal Debye length (k 01 ) which demonstrated the evidence It can be detected as an increment of the intrinsic viscosity.

of a primary electroviscous effect. By extrapolating this relation to k 01 ร… 1 nm, we obtained the intrinsic viscosity [h] free from the The secondary effect is the additional energy dissipation electroviscous effect. Using this value, the shape factor and size of genarated due to the overlapping of diffuse double layers of the montmorillonite sheet were estimated. The estimated size was colloidal particles when two charged particles are conveyed slightly smaller than that obtained from PCS. The viscosity data to a close position by an external fluid motion. This effect also suggested the importance of the multiparticle interaction is still significant even in the dilute suspension and is proporwhich appeared in accordance with an increment in double layer tional to the second power of the volume fraction of colloidal thickness. At lower electrolyte concentration, we found a larger particles. Therefore, the effect can be detected as an incre-Huggins' coefficient, which is an index of the degree of pair interacment of the Huggins' coefficient from that estimated for an tion, and we found that the multiparticle interaction appeared at uncharged colloidal dispersion. Because this effect demona lower volume fraction of clay sheets. แญง 1998 Academic Press strates shear dependency, it has been regarded as one of the


๐Ÿ“œ SIMILAR VOLUMES


Shear-Induced Diffusivity in a Dilute Bi
โœ Isidro E. Zarraga; David T. Leighton Jr. ๐Ÿ“‚ Article ๐Ÿ“… 2001 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 175 KB

In this paper we calculate the shear-induced self and gradient diffusivities in a dilute bidisperse suspension of hard spheres. Unlike the interaction of identical spheres, the center of mass of a pair of unequally sized spheres does not translate with the imposed shear flow and hence the radial and

Sedimentation Velocity and Potential in
โœ Huan J. Keh; Yung C. Liu ๐Ÿ“‚ Article ๐Ÿ“… 1997 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 606 KB

The sedimentation of a charged composite particle composed biomedical, and environmental engineering and science. of a solid core and a surrounding porous shell in an electrolyte This problem is more complex than that of uncharged colloisolution is analytically studied. In the solvent-permeable and

Hydrodynamic Interactions and Mean Settl
โœ Shing Bor Chen; Aiping Cai ๐Ÿ“‚ Article ๐Ÿ“… 1999 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 159 KB

A theoretical investigation is conducted to study hydrodynamic interactions among porous spheres under creeping flow conditions. The particles may differ in size and permeability. Based on the Brinkman equation governing the fluid flow inside the particle, the flow field, and the drag force and torq