2009
DOI: 10.1002/polb.21649
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Dielectric relaxation processes in epoxy resin—ZnO composites

Abstract: Polymer matrix‐ZnO microcomposites were prepared in different filler concentrations. The electrical relaxation dynamics of all samples was examined by means of broadband dielectric spectroscopy (BDS) over a wide temperature range. Two relaxation modes (namely β and γ), observed in the low temperature region, are attributed to the reorientation of small polar groups of the polymer matrix. Glass‐rubber transition (α‐mode) of the polymeric matrix and interfacial polarization phenomena are considered as responsibl… Show more

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Cited by 66 publications
(54 citation statements)
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“…Similar relaxation mechanisms have been previously reported for polymer matrix / inorganic filler composites and have been attributed to polarization phenomena taking place within the reinforcing phase [24][25]27]. Since this relaxation is attributed to the layered silicate itself, its analysis is beyond the scopes of the current work.…”
Section: Resultsmentioning
confidence: 67%
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“…Similar relaxation mechanisms have been previously reported for polymer matrix / inorganic filler composites and have been attributed to polarization phenomena taking place within the reinforcing phase [24][25]27]. Since this relaxation is attributed to the layered silicate itself, its analysis is beyond the scopes of the current work.…”
Section: Resultsmentioning
confidence: 67%
“…For that reason this process can be initially attributed to the alumina filler itself. Such intermediate mechanisms have been observed in polymer matrix/ ceramic filler composites and are attributed to polarization phenomena that take place within the reinforcing phase [24][25]27]. On the other hand, previous studies by us on alumina containing composites embedded in a PU polymer matrix (PU/alumina composites) [28], do not reveal the existence of such mechanism that can be attributed to polarization within the alumina filler.…”
Section: Resultsmentioning
confidence: 67%
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“…Because of the frequency and temperature superposition, loss peaks shift to higher frequencies when temperature is raised (Figures 3 and 4). However, peak shift rate varies from process to process, although in some cases this rate is constant and the relative process appears to be temperature independent [23]. Interfacial polarization follows Arrhenius type behaviour, described by Equation (2): (2) where E A is the activation energy of the process, f 0 pre-exponential factor, k B the Boltzmann constant and T the absolute temperature.…”
Section: Figure 1 Depicts Images From Scanning Electronmentioning
confidence: 99%
“…Here we point out that the same power law behaviour at low frequencies can be produced by a bulk QDC transport process that has fractal transport features [16]. We will also show that loss peak dispersions observed in materials dominated by ion transport cannot be necessarily associated with bulk molecular relaxation mechanisms [28][29][30] as these dispersions are shown to be caused here by interface effects.…”
Section: Response Functionsmentioning
confidence: 78%