Related Experiment Video
Updated: Jun 20, 2026

Challenges in Rheological Characterization of Highly Concentrated Suspensions — A Case Study for Screen-printing Silver Pastes
Published on: April 10, 2017
Viscosity of dilute model bead arrays at low shear: inclusion of short range solute-solvent interactions
Stuart A Allison1, Hongxia Pei, Saerom Baek
1Department of Chemistry, Georgia State University, Atlanta, Georgia 30302-4098, USA. sallison@gsu.edu
Abstract:
The intrinsic viscosity, [eta], of certain polymer-solvent systems, such as alkanes in benzene, are "anomalous" in the sense that [eta] for low molecular weight fractions are low and in certain cases negative (Dewan, K. K.; Bloomfield, V. A.; Berget, P. G.; J. Phys. Chem. 1974, 75, 3120). In this work, the theory of the viscosity of a dilute suspension of macromolecules at low shear is formulated that accounts for possible solute-solvent interactions. In doing so, we show that negative intrinsic viscosities are possible and are able to reproduce quite well the known length dependence of [eta] for alkanes in benzene. The coarse grained, solvent continuum, bead model developed here is an extension of previous work (Allison, S. A.; Pei, H. J. Phys. Chem. B 2009, 113, 8056). Following Fixman (Fixman, M. J. Chem. Phys. 1990, 92, 6858), we assume that solute-solvent interactions are short-range in character and can be separated from long-range hydrodynamic interactions between different beads. These interactions are accounted for by introducing three adjustable parameters specific to the transport of small "monomeric" solutes in the solvent of interest. Long range hydrodynamic interactions are accounted for to order a(J)(2)/r(IJ)(3) (a(J) is a bead radius and r(IJ) is an interbead distance). In modeling a macromolecule as an arbitrary array of N beads, the transport of the array is examined numerically in 5 different elementary shear fields. The most computationally demanding component of the procedure involves the inversion of a 12N by 12N matrix. In the present work, we restrict ourselves to systems with a maximum N of about 100. Our procedure is first applied to short rods and rings of from 2 to 10 beads which can be compared with independent results from the literature. Agreement is found to be better than 5%. Modeling macromolecules as wormlike chains, the procedure is then applied first to duplex DNA and then to alkanes in benzene. In both cases, it is possible to obtain excellent agreement between modeling and experiment.
Related Concept Videos
Viscosity of Fluid
Theories of Dissolution: The Danckwerts' Model and Interfacial Barrier Model
Viscosity
The SI unit of viscosity is...
Intermolecular Forces in Solutions
When the strengths of the intermolecular forces of attraction between solute and solvent species in a solution are no different than those present in the separated components, the solution is formed with no accompanying energy change. Such a solution is called an ideal solution. A mixture of ideal gases (or gases such as helium and argon,...
Theories of Dissolution: Diffusion Layer Model
This process starts with a thin layer, saturated with the drug, forming at the interface between the solid and liquid. The solute then diffuses from this layer into the main solution. The Noyes-Whitney equation suggests that the rate of dissolution relies on the diffusion...
Nonideal Two-Component Liquid Solutions

