DC and AC Conductivity of Carbon ...
Document type :
Article dans une revue scientifique
DOI :
Permalink :
Title :
DC and AC Conductivity of Carbon Nanotubes−Polyepoxy Composites
Author(s) :
Barrau, Sophie [Auteur]
Centre interuniversitaire de recherche et d'ingénierie des matériaux [CIRIMAT]
Demont, Philippe [Auteur]
Centre interuniversitaire de recherche et d'ingénierie des matériaux [CIRIMAT]
Peigney, Alain [Auteur]
Centre interuniversitaire de recherche et d'ingénierie des matériaux [CIRIMAT]
Laurent, Christophe [Auteur]
Centre interuniversitaire de recherche et d'ingénierie des matériaux [CIRIMAT]
Lacabanne, Colette [Auteur]
Centre interuniversitaire de recherche et d'ingénierie des matériaux [CIRIMAT]

Centre interuniversitaire de recherche et d'ingénierie des matériaux [CIRIMAT]
Demont, Philippe [Auteur]
Centre interuniversitaire de recherche et d'ingénierie des matériaux [CIRIMAT]
Peigney, Alain [Auteur]
Centre interuniversitaire de recherche et d'ingénierie des matériaux [CIRIMAT]
Laurent, Christophe [Auteur]
Centre interuniversitaire de recherche et d'ingénierie des matériaux [CIRIMAT]
Lacabanne, Colette [Auteur]
Centre interuniversitaire de recherche et d'ingénierie des matériaux [CIRIMAT]
Journal title :
Macromolecules
Abbreviated title :
Macromolecules
Volume number :
36
Pages :
5187-5194
Publisher :
American Chemical Society (ACS)
Publication date :
2003-07
English keyword(s) :
Electrical Conductivity
Carbon Nanotubes
Epoxy
Composites
Carbon Nanotubes
Epoxy
Composites
HAL domain(s) :
Chimie/Matériaux
English abstract : [en]
The dc and ac conductivities of carbon nanotubes−polyepoxy composites have been investigated from 20 to 110 °C in the frequency range 10-2−106 Hz as a function of the conductive weight fraction p ranging from 0.04 to 2.5 ...
Show more >The dc and ac conductivities of carbon nanotubes−polyepoxy composites have been investigated from 20 to 110 °C in the frequency range 10-2−106 Hz as a function of the conductive weight fraction p ranging from 0.04 to 2.5 wt %. The frequency dependence of the measured conductivity obeys the universal dynamic response (UDR): a dc plateau followed, above a critical frequency ωc, by the ωs power law with exponent s 0.6−1. The dc conductivity follows a percolation scaling law: σdc (p − pc)t with pc = 0.3 wt % and t = 1.4−1.8, according to the temperature. σdc reached 10-4 S/cm for 2.5 wt % CNTs content and increases with increasing temperature. Considering a biased random walk in three dimensions approach, we may explain the scaling law of ωc with p and its proportionality to σdc. The universality of ac conduction in carbon nanotubes−polymer composites is examined by the construction of master curves.Show less >
Show more >The dc and ac conductivities of carbon nanotubes−polyepoxy composites have been investigated from 20 to 110 °C in the frequency range 10-2−106 Hz as a function of the conductive weight fraction p ranging from 0.04 to 2.5 wt %. The frequency dependence of the measured conductivity obeys the universal dynamic response (UDR): a dc plateau followed, above a critical frequency ωc, by the ωs power law with exponent s 0.6−1. The dc conductivity follows a percolation scaling law: σdc (p − pc)t with pc = 0.3 wt % and t = 1.4−1.8, according to the temperature. σdc reached 10-4 S/cm for 2.5 wt % CNTs content and increases with increasing temperature. Considering a biased random walk in three dimensions approach, we may explain the scaling law of ωc with p and its proportionality to σdc. The universality of ac conduction in carbon nanotubes−polymer composites is examined by the construction of master curves.Show less >
Audience :
Non spécifiée
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Submission date :
2020-02-18T07:17:10Z
2020-02-19T07:57:44Z
2020-02-19T08:13:36Z
2023-03-24T12:52:45Z
2020-02-19T07:57:44Z
2020-02-19T08:13:36Z
2023-03-24T12:52:45Z