Effective interaction between large colloidal particles immersed in a bidisperse suspension of short-ranged attractive colloids

2009 ◽  
Vol 131 (16) ◽  
pp. 164111 ◽  
Author(s):  
A. Jamnik
1999 ◽  
Vol 110 (16) ◽  
pp. 8189-8196 ◽  
Author(s):  
R. H. Gee ◽  
D. Henderson ◽  
A. Kovalenko

2010 ◽  
Vol 82 (1) ◽  
pp. 109-126 ◽  
Author(s):  
Eduardo R.A. Lima ◽  
Evaristo C. Biscaia Jr. ◽  
Mathias Boström ◽  
Frederico W. Tavares

Ion-specific interactions between two colloidal particles are calculated using a modified Poisson-Boltzmann (PB)equationandMonteCarlo(MC)simulations. PBequationspresentgoodresultsofionicconcentration profiles around a macroion, especially for salt solutions containing monovalent ions. These equations include not only electrostatic interactions, but also dispersion potentials originated from polarizabilities of ions and proteins. This enables us to predict ion-specific properties of colloidal systems. We compared results obtained from the modified PB equation with those from MC simulations and integral equations. Phase diagrams and osmotic second virial coefficients are also presented for different salt solutions at different pH and ionic strengths, in agreement with the experimental results observed Hofmeister effects. In order to include the water structure and hydration effect, we have used an effective interaction obtained from molecular dynamics of each ion and a hydrophobic surface combined with PB equation. The method has been proved to be efficient and suitable for describing phenomena where the water structure close to the interface plays an essential role. Important thermodynamic properties related to protein aggregation, essential in biotechnology and pharmaceutical industries, can be obtained from the method shown here.


1998 ◽  
Vol 95 (3) ◽  
pp. 649-655 ◽  
Author(s):  
DAVID GOULDING ◽  
JEAN-PIERRE HANSEN

1998 ◽  
Vol 95 (3) ◽  
pp. 649-655 ◽  
Author(s):  
DAVID GOULDING JEAN-PIERRE HANSEN

2000 ◽  
Vol 112 (24) ◽  
pp. 11107-11108 ◽  
Author(s):  
S. Amokrane ◽  
M. Bouaskarne

2018 ◽  
Vol 32 (18) ◽  
pp. 1840005 ◽  
Author(s):  
Hongru Ma

Colloidal dispersion is composed of particles with size ranging from 1 nm to [Formula: see text]m dispersed in solvents. There are the volume exclusion interaction and other interactions between colloidal particles, of which the former interaction causes the depletion effect. When a big sphere is immersed in the colloidal system of small spheres, there is a depletion layer around the big sphere where the center of small sphere cannot enter. The depletion layers of two big spheres overlap if they are close to each other, increasing the free volume accessed by small spheres and thereby enlarging the entropy of the system. As a result, an effective interaction between the two big spheres is resulted from the change of entropy as a function of their distance, which is referred to as the depletion interaction. This paper first introduces the concept and scenario of the depletion interaction in colloidal systems. Then we briefly introduce various numerical or simulations methods of the depletion interaction of hard sphere systems, such as the acceptance ratio method, Wang–Landau method, and the density functional theory method. Taking the Asakura–Oosawa model as an example, we introduce a useful approximation method, Derjaguin approximation as well as the derivation of some approximate formula for the depletion interaction of different hardcore colloidal systems, such as between a pair of spheres in mono-disperse small spheres, between a hard sphere and a hard wall in a liquid of small spheres, and between a pair of hard spheres in a liquid of thin rods and thin disks.


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