Glassy and Polymer Dynamics of Elastomers by 1 H-Field-Cycling NMR Relaxometry: Effects of Fillers

H spin-lattice relaxation rate ( ) dispersions were acquired by field-cycling (FC) NMR relaxometry between 0.01 and 35 MHz over a wide temperature range on polyisoprene rubber (IR), either unfilled or filled with different amounts of carbon black, silica, or a combination of both, and sulfur cured....

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Veröffentlicht in:The journal of physical chemistry. B 2021-05, Vol.125 (17), p.4546-4554
Hauptverfasser: Nardelli, Francesca, Martini, Francesca, Carignani, Elisa, Rossi, Elena, Borsacchi, Silvia, Cettolin, Mattia, Susanna, Antonio, Arimondi, Marco, Giannini, Luca, Geppi, Marco, Calucci, Lucia
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Sprache:eng
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Zusammenfassung:H spin-lattice relaxation rate ( ) dispersions were acquired by field-cycling (FC) NMR relaxometry between 0.01 and 35 MHz over a wide temperature range on polyisoprene rubber (IR), either unfilled or filled with different amounts of carbon black, silica, or a combination of both, and sulfur cured. By exploiting the frequency-temperature superposition principle and constructing master curves for the total FC NMR susceptibility, χ″(ω) = ω (ω), the correlation times for glassy dynamics, τ , were determined. Moreover, the contribution of polymer dynamics, χ (ω), to χ″(ω) was singled out by subtracting the contribution of glassy dynamics, χ (ω), well represented by the Cole-Davidson spectral density. Glassy dynamics resulted moderately modified by the presence of fillers, τ values determined for the filled rubbers being slightly different from those of the unfilled one. Polymer dynamics was affected by the presence of fillers in the Rouse regime. A change in the frequency dependence of χ (ω) at low frequencies was observed for all filled rubbers, more pronounced for those reinforced with silica, which suggests that the presence of the filler particles can affect chain conformations, resulting in a different Rouse mode distribution, and/or interchain interactions modulated by translational motions.
ISSN:1520-6106
1520-5207
DOI:10.1021/acs.jpcb.1c00885