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Influence of the Graft Length on Nanocomposite Structure and Interfacial Dynamics

Both the dispersion state of nanoparticles (NPs) within polymer nanocomposites (PNCs) and the dynamical state of the polymer altered by the presence of the NP/polymer interfaces have a strong impact on the macroscopic properties of PNCs. In particular, mechanical properties are strongly affected by...

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Autores principales: Genix, Anne-Caroline, Bocharova, Vera, Carroll, Bobby, Dieudonné-George, Philippe, Chauveau, Edouard, Sokolov, Alexei P., Oberdisse, Julian
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9960434/
https://www.ncbi.nlm.nih.gov/pubmed/36839117
http://dx.doi.org/10.3390/nano13040748
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author Genix, Anne-Caroline
Bocharova, Vera
Carroll, Bobby
Dieudonné-George, Philippe
Chauveau, Edouard
Sokolov, Alexei P.
Oberdisse, Julian
author_facet Genix, Anne-Caroline
Bocharova, Vera
Carroll, Bobby
Dieudonné-George, Philippe
Chauveau, Edouard
Sokolov, Alexei P.
Oberdisse, Julian
author_sort Genix, Anne-Caroline
collection PubMed
description Both the dispersion state of nanoparticles (NPs) within polymer nanocomposites (PNCs) and the dynamical state of the polymer altered by the presence of the NP/polymer interfaces have a strong impact on the macroscopic properties of PNCs. In particular, mechanical properties are strongly affected by percolation of hard phases, which may be NP networks, dynamically modified polymer regions, or combinations of both. In this article, the impact on dispersion and dynamics of surface modification of the NPs by short monomethoxysilanes with eight carbons in the alkyl part (C(8)) is studied. As a function of grafting density and particle content, polymer dynamics is followed by broadband dielectric spectroscopy and analyzed by an interfacial layer model, whereas the particle dispersion is investigated by small-angle X-ray scattering and analyzed by reverse Monte Carlo simulations. NP dispersions are found to be destabilized only at the highest grafting. The interfacial layer formalism allows the clear identification of the volume fraction of interfacial polymer, with its characteristic time. The strongest dynamical slow-down in the polymer is found for unmodified NPs, while grafting weakens this effect progressively. The combination of all three techniques enables a unique measurement of the true thickness of the interfacial layer, which is ca. 5 nm. Finally, the comparison between longer (C(18)) and shorter (C(8)) grafts provides unprecedented insight into the efficacy and tunability of surface modification. It is shown that C(8)-grafting allows for a more progressive tuning, which goes beyond a pure mass effect.
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spelling pubmed-99604342023-02-26 Influence of the Graft Length on Nanocomposite Structure and Interfacial Dynamics Genix, Anne-Caroline Bocharova, Vera Carroll, Bobby Dieudonné-George, Philippe Chauveau, Edouard Sokolov, Alexei P. Oberdisse, Julian Nanomaterials (Basel) Article Both the dispersion state of nanoparticles (NPs) within polymer nanocomposites (PNCs) and the dynamical state of the polymer altered by the presence of the NP/polymer interfaces have a strong impact on the macroscopic properties of PNCs. In particular, mechanical properties are strongly affected by percolation of hard phases, which may be NP networks, dynamically modified polymer regions, or combinations of both. In this article, the impact on dispersion and dynamics of surface modification of the NPs by short monomethoxysilanes with eight carbons in the alkyl part (C(8)) is studied. As a function of grafting density and particle content, polymer dynamics is followed by broadband dielectric spectroscopy and analyzed by an interfacial layer model, whereas the particle dispersion is investigated by small-angle X-ray scattering and analyzed by reverse Monte Carlo simulations. NP dispersions are found to be destabilized only at the highest grafting. The interfacial layer formalism allows the clear identification of the volume fraction of interfacial polymer, with its characteristic time. The strongest dynamical slow-down in the polymer is found for unmodified NPs, while grafting weakens this effect progressively. The combination of all three techniques enables a unique measurement of the true thickness of the interfacial layer, which is ca. 5 nm. Finally, the comparison between longer (C(18)) and shorter (C(8)) grafts provides unprecedented insight into the efficacy and tunability of surface modification. It is shown that C(8)-grafting allows for a more progressive tuning, which goes beyond a pure mass effect. MDPI 2023-02-16 /pmc/articles/PMC9960434/ /pubmed/36839117 http://dx.doi.org/10.3390/nano13040748 Text en © 2023 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Genix, Anne-Caroline
Bocharova, Vera
Carroll, Bobby
Dieudonné-George, Philippe
Chauveau, Edouard
Sokolov, Alexei P.
Oberdisse, Julian
Influence of the Graft Length on Nanocomposite Structure and Interfacial Dynamics
title Influence of the Graft Length on Nanocomposite Structure and Interfacial Dynamics
title_full Influence of the Graft Length on Nanocomposite Structure and Interfacial Dynamics
title_fullStr Influence of the Graft Length on Nanocomposite Structure and Interfacial Dynamics
title_full_unstemmed Influence of the Graft Length on Nanocomposite Structure and Interfacial Dynamics
title_short Influence of the Graft Length on Nanocomposite Structure and Interfacial Dynamics
title_sort influence of the graft length on nanocomposite structure and interfacial dynamics
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9960434/
https://www.ncbi.nlm.nih.gov/pubmed/36839117
http://dx.doi.org/10.3390/nano13040748
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