2013
DOI: 10.1039/c3sm51432c
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Phase behaviour of colloids with short-range repulsions plus nonadsorbing polymer chains

Abstract: The colloidal gas-liquid phase behaviour has been studied for aqueous mixtures of well-defined spherical particles with shortranged repulsions mixed with relatively monodisperse poly(ethylene oxide) polymers. We show that our set of experimental phase diagrams are in quantitative agreement with theoretical predictions using generalized free volume theory [G. J. Fleer and R. Tuinier, Phys. Rev. E, 2007, 76, 041802]. The determination of the equilibrium composition of coexisting phases reveals qualitative deviat… Show more

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Cited by 11 publications
(17 citation statements)
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“…Equivalently, added repulsions increase the required depletant concentration for phase coexistence. The latter is in qualitative agreement with computer simulations and experimental results for charged nanoparticles in polymeric solutions [16,32,34,35]. Not surprising, the difference in the phase diagram with respect to the HS cases is more dramatic for larger values of |β | and q Y .…”
Section: Complete Phase Diagrams and Critical Pointssupporting
confidence: 88%
See 1 more Smart Citation
“…Equivalently, added repulsions increase the required depletant concentration for phase coexistence. The latter is in qualitative agreement with computer simulations and experimental results for charged nanoparticles in polymeric solutions [16,32,34,35]. Not surprising, the difference in the phase diagram with respect to the HS cases is more dramatic for larger values of |β | and q Y .…”
Section: Complete Phase Diagrams and Critical Pointssupporting
confidence: 88%
“…However, limited theories are available for dispersed colloidal particles with realistic interactions and added free polymers (acting as depletants). Available approaches focused on short-range repulsive colloids [16,[32][33][34][35]. In real systems, more involved (soft) interactions are often present.…”
Section: Introductionmentioning
confidence: 99%
“…The shaded region indicates the possible extension of the two 20 kDa PEG layers attached to the particle surfaces given by the two extremes, i.e., going from a collapsed state with a spherical diameter of ≈12 nm to a fully extended chain of ≈65 nm. The collapsed state was determined from the previously established empirical relation to estimate the polymer radius of gyration for PEG in water, R g = 6 nm, from the molecular weight . The length of the extended chain was calculated from a monomer length of 0.1464 nm with 20 kDa corresponding to ≈450 monomer units.…”
Section: Resultsmentioning
confidence: 99%
“…The PEG polymers, with a reported molecular weight of 13.3 kg/mol and a polydispersity index of 1.08, were purchased from Polymer Source. We used a previously established empirical relation to estimate the polymer radius of gyration: R g = 47 Å, from the molecular weight 25 . The particles and polymers were prepared by vortex mixing, with salt concentrations in the continuous phase adjusted to 50 mM or 1.5 mM of monovalent salt (NaCl and/or NaN 3 ).…”
Section: Model and Theorymentioning
confidence: 99%