2012
DOI: 10.1524/zpch.2012.0258
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Coarse-Graining of Ionic Microgels: Theory and Experiment

Abstract: In this work, we discuss the statistical mechanics of many-body systems consisting of electrically charged microgels, and we show that their collective behavior is determined by an interplay between the screened electrostatic and the elastic contributions to their effective interaction potential. The former is derived by means of a statistical-mechanical approach due to Denton [A. R. Denton, Phys. Rev. E 67, 011804 (2003)], and it includes the screened electrostatic potential between penetrable spheres and the… Show more

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Cited by 45 publications
(79 citation statements)
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“…U dd 100k B T , captures the small microgels 9 behavior. This estimate is consistent with scaling arguments of the Hertzian model as a function of particle size [52,53] with respect to the large microgels.…”
Section: Model and Theorysupporting
confidence: 88%
See 1 more Smart Citation
“…U dd 100k B T , captures the small microgels 9 behavior. This estimate is consistent with scaling arguments of the Hertzian model as a function of particle size [52,53] with respect to the large microgels.…”
Section: Model and Theorysupporting
confidence: 88%
“…U dd 100k B T , captures the small microgels 9 behavior. This estimate is consistent with scaling arguments of the Hertzian model as a function of particle size [52,53] with respect to the large microgels.Numerical calculation of the effective potential Microgel configurations are built as disordered, fully-bonded networks generated as in Ref. [8,40] using ≈ 5000 monomers of diameter σ m in a spherical confinement of radius Z = 25 σ m and crosslinker concentration c = 5%.…”
supporting
confidence: 88%
“…The resulting effective pair potential, obtained by coarse-graining the electrolyte degrees of freedom, has been used to predict the phase behaviour of uniform ionic microgel suspensions. [14][15][16] Recently, it has been shown that this formalism is in good agreement with experimental data of particle microstructure, when adding the elastic repulsion. 16 Here, we extend the study to the more general case of core-shell microgel structures and analyse the effect of the shell extension on the ion penetration inside the microgel, the effective charge of the particles, and on the electrostatic effective interaction between pairs of particles.…”
Section: Introductionsupporting
confidence: 56%
“…By applying the HNC closure equation given in Eq. (16) to the microgel-ion correlations and assuming that g m+ (r) ≈ g m− (r) ≈ 1, it is a simple task to show that then the HNC closure reduces to e −c mi (r)−βV mi (r) = 1 and, hence, to the Random Phase approximation. 44 The screening of the microgel bare charge can be estimated using the internal net particle charge, Z in , which can be calculated by integration of the ionic density profiles inside the particle …”
Section: Resultsmentioning
confidence: 99%
“…Under from an experimental viewpoint surprisingly general conditions, a h is unequivocally determined from the measurement of a single-particle transport property such as the translational diffusion coefficient D t 0 or the intrinsic viscosity [η]. The definition of the HRM includes also spherical particles with fuzzy hydrodynamic structure and no sharp outer boundary, and with a soft pair potential such as for weakly cross-linked ionic microgels [1, 27,28]. For spherical particles having excluded volume interactions only with a h < a, the HRM reduces to the so-called spherical annulus model.…”
Section: Introductionmentioning
confidence: 99%