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      Optimization of thermoelectric properties of carbon nanotube veils by defect engineering

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          Abstract

          Defect engineering of CNT veils, by stretching and heat-repairing, is shown to be a method for optimising thermoelectric performances, as thermal conductivity can be reduced without significantly affecting Seebeck voltage and electrical conductivity.

          Abstract

          Carbon nanotubes (CNTs), with their combination of excellent electrical conductivity, Seebeck coefficient, mechanical robustness and environmental stability are highly desired as thermoelectric (TE) materials for a wide range of fields including Internet of Things, health monitoring and environmental remediation solutions. However, their high thermal conductivity ( κ) is an obstacle to practical TE applications. Herein, we present a novel method to reduce the κ of CNT veils, by introducing defects, while preserving their Seebeck coefficient and electrical conductivity. Solid-state drawing of a CNT veil embedded within two polycarbonate films generates CNT veil fragments of reducing size with increasing draw ratio. A successive heat treatment, at above the polycarbonate glass-to-rubber transition temperature, spontaneously reconnects the CNT veils fragments electrically but not thermally. Stretching to a draw ratio of 1.5 and heat repairing at 170 °C leads to a dramatic 3.5-fold decrease in κ (from 46 to 13 W m −1 K −1), in contrast with a decrease in electrical conductivity of only 26% and an increase in Seebeck coefficient of 10%. To clarify the mechanism of reduction in thermal conductivity, a large-scale mesoscopic simulation of CNT veils under uniaxial stretching has also been used. This work shows that defect engineering can be a valuable strategy to optimize TE properties of CNT veils and, potentially, other thermoelectric materials.

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          Most cited references63

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          Ultralow thermal conductivity and high thermoelectric figure of merit in SnSe crystals.

          The thermoelectric effect enables direct and reversible conversion between thermal and electrical energy, and provides a viable route for power generation from waste heat. The efficiency of thermoelectric materials is dictated by the dimensionless figure of merit, ZT (where Z is the figure of merit and T is absolute temperature), which governs the Carnot efficiency for heat conversion. Enhancements above the generally high threshold value of 2.5 have important implications for commercial deployment, especially for compounds free of Pb and Te. Here we report an unprecedented ZT of 2.6 ± 0.3 at 923 K, realized in SnSe single crystals measured along the b axis of the room-temperature orthorhombic unit cell. This material also shows a high ZT of 2.3 ± 0.3 along the c axis but a significantly reduced ZT of 0.8 ± 0.2 along the a axis. We attribute the remarkably high ZT along the b axis to the intrinsically ultralow lattice thermal conductivity in SnSe. The layered structure of SnSe derives from a distorted rock-salt structure, and features anomalously high Grüneisen parameters, which reflect the anharmonic and anisotropic bonding. We attribute the exceptionally low lattice thermal conductivity (0.23 ± 0.03 W m(-1) K(-1) at 973 K) in SnSe to the anharmonicity. These findings highlight alternative strategies to nanostructuring for achieving high thermoelectric performance.
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            Thermal properties of graphene and nanostructured carbon materials.

            Recent years have seen a rapid growth of interest by the scientific and engineering communities in the thermal properties of materials. Heat removal has become a crucial issue for continuing progress in the electronic industry, and thermal conduction in low-dimensional structures has revealed truly intriguing features. Carbon allotropes and their derivatives occupy a unique place in terms of their ability to conduct heat. The room-temperature thermal conductivity of carbon materials span an extraordinary large range--of over five orders of magnitude--from the lowest in amorphous carbons to the highest in graphene and carbon nanotubes. Here, I review the thermal properties of carbon materials focusing on recent results for graphene, carbon nanotubes and nanostructured carbon materials with different degrees of disorder. Special attention is given to the unusual size dependence of heat conduction in two-dimensional crystals and, specifically, in graphene. I also describe the prospects of applications of graphene and carbon materials for thermal management of electronics.
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              Highly stretchable, integrated supercapacitors based on single-walled carbon nanotube films with continuous reticulate architecture.

              Highly stretchable, integrated, single-walled carbon nanotube (SWCNT) film supercapacitors are prepared by combining directly grown SWCNT films with continuous reticulate architecture with polydimethylsiloxane with enhanced prestrain. The performance of the prepared stretchable supercapacitors remains nearly unchanged even during the stretching process under 120% strain. Copyright © 2013 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.
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                Author and article information

                Contributors
                Journal
                MHAOAL
                Materials Horizons
                Mater. Horiz.
                Royal Society of Chemistry (RSC)
                2051-6347
                2051-6355
                August 29 2023
                2023
                : 10
                : 9
                : 3601-3609
                Affiliations
                [1 ]Department of Aeronautics, Imperial College London, Exhibition Road, London, SW7 2AZ, UK
                [2 ]School of Engineering and Materials Science, Queen Mary University of London, London, E1 4NS, UK
                [3 ]Department of Materials, University of Manchester, Manchester, M13 9PL, UK
                [4 ]National Graphene Institute, University of Manchester, M13 9PL, UK
                [5 ]School of Physical and Chemical Sciences, Queen Mary University of London, London, E1 4NS, UK
                [6 ]Henry Royce Institute for Advanced Materials, University of Manchester, Manchester, M13 9PL, UK
                [7 ]Department of Mechanical Engineering, University of Alabama, 7th Avenue, Tuscaloosa, AL 35487, USA
                Article
                10.1039/D3MH00525A
                fe0aeaf0-7926-4e99-a7f2-dbd4f296714d
                © 2023

                http://creativecommons.org/licenses/by-nc/3.0/

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