Elsevier

Carbon

Volume 106, September 2016, Pages 64-73
Carbon

Radial collapse of carbon nanotubes for conductivity optimized polymer composites

https://doi.org/10.1016/j.carbon.2016.05.004Get rights and content

Abstract

The optimization of the electronic conduction of carbon nanotube polymer composites is studied by tuning the radial geometry of the carbon nanotubes in a compression cycle. We have investigated the structural evolution of multi-walled carbon nanotubes in a polyamide matrix as a function of applied high pressure. Combining high resolution electron microscopy and small angle neutron scattering experiments, we conclude that the nanotube radial cross-section is irreversibly deformed following applied pressures up to 5 GPa. Studying highly percolated composites we observe that the sample resistivity drastically decreases with pressure up to about 2 GPa with no further change up to the maximum 5 GPa applied pressure. An important hysteresis is observed upon decompression which leads to an enhanced electrical conductivity of the composite in all the studied compression cycles with maximum pressures ranging from 1 to 5 GPa. Modelling the radial collapse of single-walled carbon nanotubes shows that the modified radial geometry can considerably improve the electronic transport properties in contacted carbon nanotube junctions. Our results open opportunities for engineering nanotube composites by controlling the radial collapse.

Introduction

The exceptionally high elastic modulus and tensile strength of carbon nanotubes (CNT) is driving their development as reinforcing agents in next generation composite materials [1], [2], [3]. These properties, together with their electrical and thermal conductance, have been decisive for an emerging industrial interest in CNT in low weight reinforced composites, conductive polymers or advanced nanocomposites with multi-functional features. Nevertheless several challenges need to be tackled before CNT realize their full potential; such as poor dispersion or alignment [4], which together with higher production costs presently prevent CNT to fully compete with carbon fibers. Nevertheless, CNT composites remain attractive as they exhibit very low electric percolation thresholds [5]. Further developments of CNT-based composites, taking advantage of CNT exceptional physical properties, are in all cases needed from synthesis methods and scaling to system design.

Most of the physical properties of CNT rely on their particular geometry: an atomic carbon hollow cylinder with a very high aspect ratio. The circular cross-section constitutes an important characteristic feature, which is determinant for many CNT properties.

The modification of the CNT cross-section geometry constitutes a parameter which up to now has not attracted much attention in the design of CNT composite materials. It is nevertheless known that the radial cross-section adopted by CNT depends on their geometrical parameters (diameter and number of walls) and can be very far from circular [11]. The collapsed structure, also called dog-bone type has been observed in a number of large-diameter single-walled (SWCNT), double-walled (DWCNT) and few-walled (FWCNT) carbon nanotubes at ambient pressure [6], [12], [9], [7], [8], [13], [14]. Some of these observations are summarized in Fig. 1. For very large diameter FWCNT, the collapsed geometry has been proposed as an analogue for graphene nanoribbon structures [15]. The collapsed structure is stabilized through the additional van der Waals interactions provided by the inter-wall interaction which compensates for the involved elastic energies [16]. A number of precautions should be taken when considering published observations of collapsed tubes, such as channelling effects in TEM measurements that can contribute to the tube collapse [12], as well as substrate interactions [7], [17] that can modify the tube cross-section. The existence of a wide region of metastability of collapsed/non-collapsed structures has been predicted [10]. Atomistic calculations [18], [10] (also included in Fig. 1) seem to confirm the experimental trend indicating that at ambient pressure the collapsed tube geometry is governed by the number of walls and the radius of the tube.

Radial collapse of carbon nanotubes can be also obtained by applying pressure. In SWCNT the pressure induced radial collapse has been both theoretically predicted [19], [16], [20], [21] and experimentally observed [22], [23], [24]. There exists as well a number of predictions of pressure induced collapse in MWCNT [25], [26], [27].

There have been a few predictions on the electronic structure evolution of SWCNT subjected to radial deformations [28], [29], [30], [31], [32], [33], [34], [35]: they basically show that both metal-semiconductor and semiconductor-metal transitions are possible, depending on the tube chirality and on the degree of deformation. There have been some experimental confirmations of both a semiconductor to metal transition in SWCNT [36] and of a metal-semiconductor transition in DWCNT [37] upon radial collapse.

There have been many efforts on the optimization of polymer composites [38] and in particular the conductivity of polyamide-MWCNT nanocomposites [39], [5], [40]. In this work we show that the electrical conductivity of polyamide-MWCNT composites can be markedly improved through a high pressure treatment by surpassing the usual pressure limits of hot pressing or extrusion methods. We provide direct evidence of the pressure induced collapse of MWCNT in the compressive process and theoretical understanding of the relation between the geometrical changes of the nanotubes and the modification of the conductivity of the percolated network. Our work shows that the very high compression of MWCNT polymer composites can provide then an additional mechanism for electrical conductivity optimization, beyond the system consolidation.

Section snippets

Experimental methods

Samples were industrial batches of CVD grown MWCNT (Graphistrength ®C100) dispersed in a polyamide PA12 matrix by extrusion at high temperature (Arkema C M1-20 mixture). They consisted of black solid pellets containing perfectly dispersed MWCNT at a concentration of 20% by weight. The nominal moisture content is of 0.10–0.15% by weight. Information of the physical characteristics of the associated nanotubes and composites can be found in different works [41], [42]. The high CNT loading (20% by

Electrical resistivity under high pressure

The electrical resistivity of the initial sample was measured outside the high pressure set-up giving an average value of ∼ 9 Ωcm. The samples were then compressed up to a maximum pressure of 5 GPa. In our high pressure set-up we can measure the variation of the resistivity with pressure only after some initial compression. In fact, some compaction is needed to allow for the electrical conduction between the different parts of the set-up. The variation of the electrical resistivity of the

Discussion

From the different experimental results and theoretical modeling we can now propose a coherent scenario for the full pressure cycle of the composite. The MWCNT geometry distribution is quite large and already at ambient pressure some tubes do not present a perfectly circular cross-section. Pressure application progressively reduces the intertube distance and continues to deform those tubes having the larger internal diameters and the smallest number of walls. As a consequence the electrical

Conclusions

We have shown that the conductivity of commercially available MWCNT polyamide composites can be enhanced by a pressure treatment up to about 1 GPa thanks to the improvement of tube–tube contacts through radial deformation of the tube and/or the intrinsic changes in the tube resistivity due to radial deformation. A further increase of pressure beyond 1 GPa does not improve the final resistivity on decompression. This work points to the possibility of adjusting the pressure treatment for

Acknowledgements

We acknowledge financial support by the ANR program P2N under Contract ANR-11-NANO-025 “TRI-CO”. We are indebted to the Arkema company for providing samples and associated information. We acknowledge technical support of F. Legrand (ILM, Lyon). The transmission electron microscopy studies were conducted at the Laboratorio de Microscopias Avanzadas (LMA) at the Instituto de Nanociencia de Aragon (INA) - Universidad de Zaragoza (Spain). R.A. acknowledges funding from the Spanish Ministerio de

References (62)

  • N.M. Pugno et al.

    Buckling of peapods, fullerenes and nanotubes

    Phys. E Low-dimens. Syst. Nanostruct.

    (2012)
  • A. Charlier et al.

    Metal–semiconductor transitions under uniaxial stress for single- and double-walled carbon nanotubes

    J. Phys. Chem. Solids

    (2001)
  • J. Sandler et al.

    A comparative study of melt spun polyamide-12 fibres reinforced with carbon nanotubes and nanofibres

    Polymer

    (2004)
  • M. Jouni et al.

    Charge carrier transport and low electrical percolation threshold in multiwalled carbon nanotube polymer nanocomposites

    Carbon

    (2014)
  • S. Versavaud et al.

    Influence of injection molding on the electrical properties of polyamide 12 filled with multi-walled carbon nanotubes

    Polymer

    (2014)
  • P. Colomban et al.

    Micro–raman study of the compressive behaviour of advanced pa66 polyamide fibres in a diamond-anvil cell

    Vib. Spectrosc.

    (2005)
  • Z. Jia et al.

    Carbon nanotube-induced structure and phase evolution in polymer-based nanocomposites crystallized at elevated pressures

    Mater. Sci. Eng. B

    (2012)
  • C. Kingston et al.

    Release characteristics of selected carbon nanotube polymer composites

    Carbon

    (2014)
  • B. Arash et al.

    Mechanical properties of carbon nanotube/polymer composites

    Sci. Rep.

    (2014)
  • Y. Zeng et al.

    Design and reinforcement: vertically aligned carbon nanotube-based sandwich composites

    ACS Nano

    (2010)
  • N.G. Chopra et al.

    Fully collapsed carbon nanotubes

    Nature

    (1995)
  • M.F. Yu et al.

    Structure and mechanical flexibility of carbon nanotube ribbons: an atomic-force microscopy study

    J. Appl. Phys.

    (2001)
  • M. Motta et al.

    High performance fibres from “dog bone” carbon nanotubes

    Adv. Mater.

    (2007)
  • J. Xiao et al.

    Collapse and stability of singleand multi-wall carbon nanotubes

    Nanotechnology

    (2007)
  • H. Shima

    Buckling of carbon nanotubes: a state of the art review

    Materials

    (2011)
  • X.H. Zhong et al.

    Structures and characterizations of bundles of collapsed double-walled carbon nanotubes

    Nanotechnology

    (2012)
  • D.H. Choi et al.

    Fabrication and characterization of fully flattened carbon nanotubes: a new graphene nanoribbon analogue

    Sci. Rep.

    (2013)
  • P. Tangney et al.

    Structural transformations of carbon nanotubes under hydrostatic pressure

    Nano Lett.

    (2005)
  • J.C. Blancon et al.

    Electronic transport in individual carbon nanotube bundles under pressure

    J. Appl. Phys.

    (2013)
  • S. Zhang et al.

    Transition states and minimum energy pathways for the collapse of carbon nanotubes

    Phys. Rev. B

    (2006)
  • J.A. Elliott et al.

    Collapse of single-wall carbon nanotubes is diameter dependent

    Phys. Rev. Lett.

    (2004)
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