2006
DOI: 10.1063/1.2374886
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Thermosensitive core-shell particles as model systems for studying the flow behavior of concentrated colloidal dispersions

Abstract: We report on a comprehensive investigation of the flow behavior of colloidal thermosensitive core-shell particles at high densities. The particles consist of a solid core of poly͑styrene͒ onto which a network of cross-linked poly͑N-isopropylacrylamide͒ is affixed. Immersed in water the shell of these particles will swell if the temperature is low. Raising the temperature above 32°C leads to a volume transition within this shell which leads to a marked shrinking of the shell. The particles have well-defined cor… Show more

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Cited by 105 publications
(160 citation statements)
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“…The typical entropy change for deformed grafted chains is $10 3 times smaller than for free chains [18]. The estimated order of $10 6 monomers in the grafted layer agrees with the value $3 Â 10 6 based on the known composition of our system [9]. To conclude, we have presented a kinetic model that can account for spontaneous dimer dissociation which, combined with light-scattering experiments, provides a robust protocol for quantifying the dissociation rate and the reversible association (dimerization) energy of mutually attractive Brownian molecules and nanoparticles.…”
supporting
confidence: 74%
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“…The typical entropy change for deformed grafted chains is $10 3 times smaller than for free chains [18]. The estimated order of $10 6 monomers in the grafted layer agrees with the value $3 Â 10 6 based on the known composition of our system [9]. To conclude, we have presented a kinetic model that can account for spontaneous dimer dissociation which, combined with light-scattering experiments, provides a robust protocol for quantifying the dissociation rate and the reversible association (dimerization) energy of mutually attractive Brownian molecules and nanoparticles.…”
supporting
confidence: 74%
“…As this value is mostly independent of the surface chemistry [14], we take it here as the width of the effective well. Furthermore, this value is much larger than the molecular roughness of the PNIPAM shell, which is of the order of 1 nm [9,10], such that the attractive hydrophobic force dominates over repulsive entropic protrusion forces which are much shorter-ranged [14]. There is now only one free parameter in our model, the depth of the effective attraction well, V min , i.e., the binding energy of the dimers.…”
mentioning
confidence: 99%
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