We study the structure and linear viscoelasticity of interacting polymer nanocomposites based on mixtures of poly(ethylene oxide) and fumed silica particles. The filler is dispersed within the polymer using two different techniques which lead to different dispersion states. The analysis of the dynamic response of our systems highlights the formation of a stress-bearing network above a critical volume fraction, Φc. Extending a two-phase model used to describe weakly interacting systems, we show that above Φc the melt-state elasticity of the composites arises from the independent contributions of a polymer–particle network and a viscous matrix. We also find that, although Φc depends on the initial state of dispersion, the network elasticity scales with volume fraction following a universal power-law, with an exponent ν ≈ 1.8. Such a scaling law has been recently predicted for the stress-bearing mechanism governed by polymer-mediated interactions.
Universal Features of the Melt Elasticity of Interacting Polymer Nanocomposites / Capuano, Guglielmo; Filippone, Giovanni; Romeo, Giovanni; Acierno, Domenico. - In: LANGMUIR. - ISSN 0743-7463. - 28:(2012), pp. 5458-5463. [10.1021/la205105m]
Universal Features of the Melt Elasticity of Interacting Polymer Nanocomposites
CAPUANO, GUGLIELMO;FILIPPONE, GIOVANNI;ROMEO, GIOVANNI;ACIERNO, DOMENICO
2012
Abstract
We study the structure and linear viscoelasticity of interacting polymer nanocomposites based on mixtures of poly(ethylene oxide) and fumed silica particles. The filler is dispersed within the polymer using two different techniques which lead to different dispersion states. The analysis of the dynamic response of our systems highlights the formation of a stress-bearing network above a critical volume fraction, Φc. Extending a two-phase model used to describe weakly interacting systems, we show that above Φc the melt-state elasticity of the composites arises from the independent contributions of a polymer–particle network and a viscous matrix. We also find that, although Φc depends on the initial state of dispersion, the network elasticity scales with volume fraction following a universal power-law, with an exponent ν ≈ 1.8. Such a scaling law has been recently predicted for the stress-bearing mechanism governed by polymer-mediated interactions.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.