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Wearable and flexible thermoelectrics for energy harvesting

Published online by Cambridge University Press:  09 March 2018

Ruoming Tian
Affiliation:
Toyota Physical and Chemical Research Institute, Japan; r.tian@unswalumni.com
Chunlei Wan
Affiliation:
School of Materials Science and Engineering, Tsinghua University, China; wancl@mail.tsinghua.edu.cn
Naoyuki Hayashi
Affiliation:
Fujifilm Corporation, Japan; naoyuki.hayashi@fujifilm.com
Toshiaki Aoai
Affiliation:
Chiba University, Japan; t.aoai@chiba-u.jp
Kunihito Koumoto
Affiliation:
Toyota Physical and Chemical Research Institute, Japan; koumoto@apchem.nagoya-u.ac.jp

Abstract

Conjugated polymers have emerged as potential candidates for thermal-energy harvesting. Their flexible and lightweight nature, as well as scalable processing, make them geometrically versatile for a large variety of applications, including powering wearable electronics that are not available for traditional inorganic materials. However, the long-range structural disorder greatly hinders their electrical conduction, and this far outweighs the induced low thermal conductivity; therefore, the thermoelectric performance needs to be significantly improved to fulfill the requirements of efficient devices. Composites and hybrid thermoelectric materials have been developed to capitalize on the individual strengths of conducting polymers and other components, including carbon nanotubes, graphene, and inorganic nanomaterials. In this article, we present recent advances in conjugated polymers, the associated hybrid thermoelectric composites, and the latest breakthroughs in the development of inorganic–organic hybrid superlattices.

Information

Type
Materials for Energy Harvesting
Copyright
Copyright © Materials Research Society 2018 
Figure 0

Figure 1. Schematics of various synthesis methods for organic-based thermoelectric composites. (a) (Left to right) The random coil-like polyaniline (PANI) molecules become extended chains when treated with m-cresol solvent. After subsequent treatment with a solvent containing dispersed single-walled carbon nanotubes (CNTs), a highly ordered cable-like PANI/CNT composite forms due to synergetic effects and intramolecular conjugation;13 (b) (Left to right) EDOT monomers are dispersed in a reduced graphene oxide (rGO) aqueous solution to form a pie-like PEDOT/rGO composite during in situ polymerization;14 (c) (Left to right) Li-intercalated SnSe powder was exfoliated into nanosheets in water, and then mixed with aqueous PEDOT:PSS. The obtained SnSe/PEDOT:PSS composite was deposited onto a glass substrate by drop casting.16 Note: PEDOT, poly(3,4-ethylenedioxythiophene); PSS, poly(styrene sulfonate); SWNT, single-walled nanotube; EDOT, 3,4-ethylenedioxythiophene.

Figure 1

Figure 2. Thermoelectric properties of a wide range of organic-based composites compiled from data reported in the literature. The plot includes polymer/CNT (carbon nanotube) composites (circle symbols),12,13,17–23,25–31 polymer/graphene composites (square symbols),14,15,32–44 and polymer/inorganic composites (triangle symbols).16,24,45–60 Among these, composites containing poly(3,4-ethylenedioxythiophene) (PEDOT) are shown with hollow symbols, and other polymer materials, including polyaniline, polypyrrole, PVDF, and P3HT, are shown with solid symbols. Power factor (PF) values of organic–inorganic superlattices (A–C)61–63 are also presented (solid diamond) for comparison. The plot shows that the polymer/inorganic composites possess relatively large S as compared to polymer blended with CNTs or graphene. However, their σ (electrical conductivities) need to be significantly enhanced to achieve a large PF. Note: HA, hexylammonium; DMSO, dimethylsulfoxide; NMF, n-methylformamide; TBA, tetrabutyl ammonium; P3HT, poly(3-hexylthiophene); PVDF, poly(vinylidene fluoride); A, electrochemically intercalated TiS2[(HA)(H2O)(DMSO)] superlattice crystal; B, optimized TiS2[(HA)(TBA)] superlattice crystal through heat treatment; C, solution-processed TiS2[(HA)(NMF)] superlattice film.

Figure 2

Figure 3. The configuration and power output of a carbon nanotube (CNT)-based thermoelectric (TE) module fabricated by Fujifilm Corporation.65 (a) Photograph of a CNT-based TE pattern fabricated by stencil printing, and (b) a schematic illustration of a single leg in the pattern. (c) The generated power output at different airflow rates. The inset shows a photograph of the TE module consisting of p-type CNT-based composite material. The TE module can achieve a maximum power output of 120 μW when the hot side is 120°C and the flow rate of the cool air is 3.9 m/s.65

Figure 3

Figure 4. The synthesis of organic-intercalated superlattice materials and thermoelectric performance of the flexible thermoelectric (TE) module. (a) A TiS2[(HA)(DMSO)] superlattice crystal was fabricated by electrochemical intercalation, where the TiS2 crystal and a Pt foil were used as cathode and anode, respectively. Next, the resulting organic-intercalated TiS2 crystal was soaked in water overnight to obtain a TiS2[(HA)(H2O)(DMSO)] superlattice crystal through solvent exchange.61 (b) Synthesis of TiS2/organic superlattice film by the liquid-exfoliation and self-assembly approaches. Specifically, TiS2 powder was mixed with hexylamine and dispersed into a polar solvent (NMF). Then, the mixture was exfoliated into nanosheets by mild sonication. After centrifugation, the obtained supernatant was collected for further film deposition.73 (c) The (top) generated power output and (bottom) power density of (inset) a flexible TE device consisting of p-type poly(3,4-ethylenedioxythiophene):polystyrene sulfonate and n-type TiS2/organic superlattice film.73 The module can generate a maximum voltage output of 33 mV and power density of 250 µW/cm2 at a temperature gradient of 70 K.73 Note: HA, hexylammonium; DMSO, dimethyl sulfoxide; NMF, n-methylformamide; T, temperature. δ+ and δ– in (a) indicate the dipole moments of the polarized polar molecule DMSO. The blue, white, and gray atoms in (b) represent N, H, and C, respectively.