2019
DOI: 10.1103/physrevlett.123.187802
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Direct Observation of Dynamic Tube Dilation in Entangled Polymer Blends: A Combination of Neutron Scattering and Dielectric Techniques

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Cited by 9 publications
(13 citation statements)
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“…Figure shows the results obtained for the normalized chain dynamic structure factor S ( Q , t )/ S ( Q ,0) corresponding to long chains in the blend with the 18-arm star additive (ϕ L = 0.5). The results corresponding to the blends with the 8-arm star additive, and with the short linear additivethat were previously reportedare also included here for comparison. We have also included in the figure as a reference (dashed lines) the fitting curves describing the S ( Q , t )/ S ( Q ,0) data, corresponding to the pure PI-80k sample .…”
Section: Resultsmentioning
confidence: 99%
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“…Figure shows the results obtained for the normalized chain dynamic structure factor S ( Q , t )/ S ( Q ,0) corresponding to long chains in the blend with the 18-arm star additive (ϕ L = 0.5). The results corresponding to the blends with the 8-arm star additive, and with the short linear additivethat were previously reportedare also included here for comparison. We have also included in the figure as a reference (dashed lines) the fitting curves describing the S ( Q , t )/ S ( Q ,0) data, corresponding to the pure PI-80k sample .…”
Section: Resultsmentioning
confidence: 99%
“…The results corresponding to the blends with the 8-arm star additive, and with the short linear additivethat were previously reportedare also included here for comparison. We have also included in the figure as a reference (dashed lines) the fitting curves describing the S ( Q , t )/ S ( Q ,0) data, corresponding to the pure PI-80k sample . These fitting curves correspond to a de Gennes-like model for S ( Q , t )/ S ( Q ,0) with a value of the effective tube of d 0 = 64 Å (see ref for the details), which will be explained in detail in Section .…”
Section: Resultsmentioning
confidence: 99%
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“…[1][2][3][4][5][6] This gives rise to questions as how much the microscopic relaxation dynamics of a polymeric material, which decides its dynamic mechanical properties and phase stability, can be modified after loading of an additive, in particular when that additive has a similar molecular structure as the polymer chains. [7] In previous experimental studies of some miscible polymer blends, dynamical heterogeneity was observed, indicated by a broad glass transition temperature and/or thermo-rheological complexity. [8][9][10][11][12][13] This thermo-rheological complexity of certain miscible polymer blends was attributed to either differences in the component's parameters to ε AA = 0.80, ε BB = 2.0, and ε AB = 1.6 (note that the resulting interaction energies are negative at the potential minima), with oligomer and polymer monomers being categorized as the fast (A) and slow (B) component, respectively.…”
Section: The Relaxation Spectra Of the Components In Polymer Blends Dmentioning
confidence: 96%