2019
DOI: 10.1063/1.5129575
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Modeling deswelling, thermodynamics, structure, and dynamics in ionic microgel suspensions

Abstract: Ionic microgel particles in a good solvent swell to an equilibrium size determined by a balance of electrostatic and elastic forces. When crowded, ionic microgels deswell owing to a redistribution of microions inside and outside the particles. The concentration-dependent deswelling affects the interactions between the microgels, and consequently the suspension properties. We present a comprehensive theoretical study of crowding effects on thermodynamic, structural, and dynamic properties of weakly cross-linked… Show more

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Cited by 13 publications
(11 citation statements)
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“…A Hertzian interaction potential has often been considered to account for the compressibility of the nanogels in the limit of small deformations. This model has been shown to properly reproduce the observed behavior of fluid nanogel solutions and is the base, together with the Flory–Rehner theory of polymer networks, of Monte Carlo computer simulations used to study the properties of concentrated nanogel solutions. ,, …”
Section: Softness and Collective Behavior In Bulkmentioning
confidence: 99%
“…A Hertzian interaction potential has often been considered to account for the compressibility of the nanogels in the limit of small deformations. This model has been shown to properly reproduce the observed behavior of fluid nanogel solutions and is the base, together with the Flory–Rehner theory of polymer networks, of Monte Carlo computer simulations used to study the properties of concentrated nanogel solutions. ,, …”
Section: Softness and Collective Behavior In Bulkmentioning
confidence: 99%
“…Specifically, variations in temperature, solvent polarity, pH and ionic strength can induce a metamorphosis in morphology and interactions. 5,6 The latter can be achieved rather straightforwardly in poly(N-isopropylacrylamide), PNIPAM, microgels by increasing the temperature slightly above the volume phase transition temperature (VPTT), which is approximately 32 1C. [7][8][9][10] Above the VPTT, the particles form dense homogeneous spheres, while below the VPTT they can be characterized as strongly swollen polymer networks with dangling polymer ends sticking out.…”
Section: Introductionmentioning
confidence: 99%
“…Since only the osmotic pressure and the transport properties D(φ) and η(φ) are required as input characterizing the filtered dispersion, the generalized mBLA method is readily applicable to more complex dispersions of practical relevance. These include dispersions of soft and solvent-permeable colloidal particles such as micro-and nanogels [15,31,43,50,51], and charged rigid colloidal particles, ionic microgels, and proteins [52][53][54][55]. For charged particle dispersions at lower ionic strength, the concentration dependencies of D, η, and Π are distinctly different from those of electrically neutral particles, with accordingly strong differences in the UF performance (see [50,51,54]).…”
Section: Remarks On the Generalized Mbla Methodsmentioning
confidence: 99%