Influence of CNT Length on Dispersion, Localization, and Electrical Percolation in a Styrene-Butadiene-Based Star Block Copolymer.

CNT dispersion CNT length CNT localization ball milling block copolymer carbon nanotubes electrical conductivity mechanical behavior

Journal

Polymers
ISSN: 2073-4360
Titre abrégé: Polymers (Basel)
Pays: Switzerland
ID NLM: 101545357

Informations de publication

Date de publication:
02 Jul 2022
Historique:
received: 03 06 2022
revised: 23 06 2022
accepted: 28 06 2022
entrez: 9 7 2022
pubmed: 10 7 2022
medline: 10 7 2022
Statut: epublish

Résumé

This study followed the approach of dispersing and localizing carbon nanotubes (CNTs) in nanostructured domains of block copolymers (BCPs) by shortening the CNTs via ball milling. The aim was to selectively tune the electrical and mechanical properties of the resulting nanocomposites, e.g., for use as sensor materials. Multiwalled carbon nanotubes (MWCNTs) were ground into different size fractions. The MWCNT length distribution was evaluated via transmission electron microscopy and dynamic light scattering. The nanostructure of the BCPs and the glass transition temperatures of the PB-rich and PS phases were not strongly affected by the addition of CNTs up to 2 wt%. However, AFM and TEM investigations indicated a partial localization of the shortened CNTs in the soft PB-rich phase or at the interface of the PB-rich and PS phase, respectively. The stress-strain behavior of the solution-mixed composites differed little from the mechanical property profile of the neat BCP and was largely independent of CNT amount and CNT size fraction. Significant changes could only be observed for Young's modulus and strain at break and may be attributed to CNT localization and small changes in morphology. For nanocomposites with unmilled CNTs, the electrical percolation threshold was less than 0.1 wt%. As the CNTs were shortened, the resistivity increased and the percolation threshold shifted to higher CNT contents. Composites with CNTs ground for 7.5 h and 13.5 h showed no bulk conductivity but significantly decreased surface resistivity on the bottom side of the films, which could be attributed to a sedimentation process of the grind and thereby highly compressed CNT agglomerates during evaporation.

Identifiants

pubmed: 35808760
pii: polym14132715
doi: 10.3390/polym14132715
pmc: PMC9268902
pii:
doi:

Types de publication

Journal Article

Langues

eng

Subventions

Organisme : Deutsche Forschungsgemeinschaft
ID : STA 1392/1-2

Références

J Phys Chem B. 2006 Aug 17;110(32):15708-18
pubmed: 16898715
Sci Rep. 2016 Mar 11;6:22865
pubmed: 26965728
Nanoscale. 2019 Nov 28;11(44):21394-21403
pubmed: 31674619
Polymers (Basel). 2019 Nov 07;11(11):
pubmed: 31703362

Auteurs

Ulrike Staudinger (U)

Leibniz-Institut für Polymerforschung Dresden e.V., Hohe Str. 6, 01069 Dresden, Germany.

Andreas Janke (A)

Leibniz-Institut für Polymerforschung Dresden e.V., Hohe Str. 6, 01069 Dresden, Germany.

Christine Steinbach (C)

Leibniz-Institut für Polymerforschung Dresden e.V., Hohe Str. 6, 01069 Dresden, Germany.

Uta Reuter (U)

Leibniz-Institut für Polymerforschung Dresden e.V., Hohe Str. 6, 01069 Dresden, Germany.

Martin Ganß (M)

Material Research and Testing Institute (MFPA), the Bauhaus-Universität Weimar, Coudraystraße 9, 99423 Weimar, Germany.

Oliver Voigt (O)

Leibniz-Institut für Polymerforschung Dresden e.V., Hohe Str. 6, 01069 Dresden, Germany.

Classifications MeSH